KGRKJGETMRETU895U-589TY5MIGM5JGB5SDFESFREWTGR54TY
Server : Apache/2.4.62
System : FreeBSD fbsdweb2.web.rcn.net 14.1-RELEASE FreeBSD 14.1-RELEASE releng/14.1-n267679-10e31f0946d8 GENERIC amd64
User : www ( 80)
PHP Version : 8.3.8
Disable Function : NONE
Directory :  /domains/shockphysics/

Upload File :
current_dir [ Writeable ] document_root [ Writeable ]

 

Current File : /domains/shockphysics/APS_SCCM_1981to2005.xls
��ࡱ�>��	�����B�D�F�H�J�L�N�������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������	

 !"#$%&'()*+,-./0123456789:;<=>?@AC����DEFGHIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~�R�������� �F������Workbook��������	\
SummaryInformation(�����DocumentSummaryInformation8������������	�%�����\pStephen Walley                                                                                               B�a=���=��s�L8X@�"��1���Verdana1���Verdana1���Verdana1���Verdana1���Verdana"�"#,##0;\-"�"#,##0"�"#,##0;[Red]\-"�"#,##0"�"#,##0.00;\-"�"#,##0.00#"�"#,##0.00;[Red]\-"�"#,##0.005*0_-"�"* #,##0_-;\-"�"* #,##0_-;_-"�"* "-"_-;_-@_-,)'_-* #,##0_-;\-* #,##0_-;_-* "-"_-;_-@_-=,8_-"�"* #,##0.00_-;\-"�"* #,##0.00_-;_-"�"* "-"??_-;_-@_-4+/_-* #,##0.00_-;\-* #,##0.00_-;_-* "-"??_-;_-@_-��� � ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� � � �+�� �� �)�� �� �,�� �� �*�� �� �	�� �� ������������������`�:_APS SCCM 1981to2005.txt���ai�  
] 1903-1906 (Zhuang S.,  Ravichandran G., Grady D.E. J Influence of interface scattering on shock waves in heterogeneous solids Zhugin Y.N. Z The behaviour of a-quartz under high dynamic and static pressures: New results and views Zou G.,  Meng J., Cui Q. J Study of the Raman spectra of Bi2Ti4O11 at high temperature and pressure FZucker J.M.,  Barra A.J.,  Zerkle D.K.,  Kaneshige M.J., Dickson P.M. > Thermal decomposition models for high explosive compositions Zurek A.K., Follansbee P.S. 9 Microstructural effects on spall fracture in 1008 steel Zurek A.K., Hunter D.A. ? Dynamic testing and characterization of pre-fractured ceramic bZurek A.K.,  Embury J.D.,  Kelly A.,  Thissell W.R.,  Gustavsen R.L.,  Vorthman J.E., Hixson R.S. E Microstructure of depleted uranium under uniaxial strain conditions &Zwitter D.E.,  Kuklja M.M., Kunz A.B. V A computation of the frequency dependent dielectric function for energetic materials 4Zybin S.V.,  Elert M.L.,  Harrison J.A., White C.T. R Atomistic modeling of orientation dependence of shock wave properties in diamond $Zybin S.V.,  Elert M.L., White C.T. D Molecular dynamics study of non-reacting shock waves in anthracene 	 306-309 7Zybin S.V.,  Zhakhovskii V.V.,  Elert M.L., White C.T. S Molecular dynamics studies of orientation dependence of shock structure in solids 	 310-315 IZybin S.V.,  Zhakhovskii V.V.,  Bringa E.M.,  Abarzhi S.I., Remington B. \ Molecular dynamics simulations of the Richtmyer-Meshkov instability in shock loaded solids 	 437-441 J Database on material properties studied in experiments using shock waves ^Zhernokletov M.V.,  Lebedeva T.S.,  Medvedev A.B.,  Mochalov M.A.,  Shuykin A.N., Fortov V.E. L Thermodynamic parameters and equation of state of low-density SiO2 aerogel ~Zhernokletov M.V.,  Ilkaev R.I.,  Kirshanov S.I.,  Lebedeva T.S.,  Mikhaylov A.L.,  Mochalov M.A.,  Shuikin A.N., Fortov V.E. ~ Experimental measurement of compressibility and temperature in shock-compressed liquid xenon in pressure range up to 350 GPa /Zhiembetov A.K.,  Mikhaylov A.L., Smirnov G.S. ? Experimental study of explosive fragmentation of metals melts R Fragmentation properties of cerium and copper M1 on dynamic volumetric expansion 	 694-697 bZhmodik S.M.,  Verkhovtseva N.V.,  Nesterenko V.F.,  Chikov B.M.,  Airijant E., Nemirovskaya N.A. < Shock induced gold redistribution in quartz-pyrite mixture  Zhou G.-Q.,  Tang Z.P., Yang G. T Numerical study of laser-induced two-dimensional shock waves in metallic materials !Zhou G.-Q.,  Tang Z.P., Li X.-Z. o Experimental study of spalling strength and the hydro-elastic-viscoplastic constitutive equations with damage %Zhou M.,  Clifton R.J., Needleman A. E The role of material inhomogeneities in the localization of strains +Zhou X.M.,  Hu J.B.,  Jing F.Q., Wang J.G. W Sound velocity measurement for 4.2Ni2.45Fe0.35Co0.05MnW alloy under shock compression 	 109-113 )Zhou G.,  Yun S.R.,  Huang F.L., Ding J. � Theoretical research on mechanisms by which carbon in explosives is synthesized into ultrafine diamond in detonation processes: 'Gaslike-liquid-solid-graphitization' model Zhou M., Zhai J. N Modelling of micromechanical fracture using a cohesive finite element method 	 623-628 Zhu J.S., Fan Z.M. R Effects of lateral expansion and artificial viscosity on steady detonation waves %Zhuang S.,  Liu C.,  Wang C., Sun C. K Dynamic fracture of iron under shock loading induced by pulsed laser beam E Quasitemperature distribution in shocked energetic molecular solids Zhang L., Jin X. 5 Predicting of fragment number and size distribution 2Zhang H.,  Patanella A.,  Espinosa H.D., Pae K.D. $ Dynamic friction of nano-materials /Zhang F.,  Thibault P.A.,  Link R., Gonor A.L. Y Momentum transfer during shock interaction with metal particles in condensed explosives 	 934-937 bZhang Y.,  Mashimo T.,  Fukuoka K.,  Kikuchi M.,  Sekine T.,  Kobayashi T.,  Chau R., Nellis W.J. R Hugoniot measurement of GGG (Gd3Ga5O12) in the pressure range up to over 100 GPa 	 127-128 Zhang D.Z. < Shock dispersion in composite material with polymer binder Zhang D., Feng R. E Polycrystal modeling to determine the strengths of shocked ceramics HZhang L.,  Zybin S.V.,  van�Duin A.C.T.,  Dasgupta S., Goddard�III W.A. a Shock induced decomposition and sensitivity of energetic materials by ReaxFF molecular dynamics T Thermal decomposition of energetic materials by ReaxFF reactive molecular dynamics 6Zhao S.D.,  Ling Z.,  Shen L.T.,  Chen S.X., Bai Y.L. 5 An experimental approach to evolution of spallation Zhao F.,  Sun C.-W., Wei T.-Z. E A developed unified criterion for the initiation of bare explosives  1361-1364 -Zhao J.,  Winey J.M.,  Gupta Y.M., Perger W. P Elastic properties of molecular crystals using density functional calculations /Zhao J.,  Winey J.M.,  Gupta Y.M., Perger W.F. < First-principles studies of RDX crystals under compression $Zhao S.,  Germann T.C., Strachan A. t Molecular dynamics simulations of shock-induced chemical, mechanical, and thermal processes in Ni/Al nanolaminates Zheng L., Luo S.-N. O Simulated structure modifications on silica subjected to UV-laser irradiation  Zhernokletov M.V., Simakov G.I. L Studies of shock-compressed graphite behavior in reshock and release waves RZhernokletov M.V.,  Trunin R.F.,  Gudarenko L.F.,  Trushchin V.D., Gushchina O.N. 5 High pressure equation of state for HF, CF4, and F2 > Constitutive relations for the plastic deformation of metals 1 Surface energy and the size of diamond crystals 3 Constitutive relations for titanium and Ti-6Al-4V � Dislocation mechanics based constitutive equation incorporating dynamic recovery and applied to thermomechanical shear instability Z Application of Eyring's thermal activation theory to constitutive equations for polymers D Thermal activation constitutive model for polymers applied to PTFE Zerilli F.J., Kuklja M.M. 6 Ab initio 0K isotherm for organic molecular crystals 2 Equation of state of FOX-7 from first principles %Zerwekh W.D.,  Marsh S.P., Tan T.-H. # Phase detonated shock tube (PFST)  1877-1880 ;Zha C.-S.,  Hemley R.J.,  Mao H.-K.,  Duffy T.S., Meade C. 2 Brillouin scattering of silica glass to 57.5 GPa ;Zhakhovskii V.V.,  Zybin S.V.,  Abarzhi S.I., Nishihara K. ^ Atomistic dynamics of the Richtmyer-Meshkov instability in cylindrical and planar geometries Zhang K.,  Xi J., Gao J. = Research on wave formation in multilayer explosive cladding AZhang Y.,  Morosin B.,  Graham R.A.,  Hubbard C.R., Stewart J.M. y Shock induced solid state reaction and phase transition: X-ray profile studies on shock modified Fe3O4 and ZrO2 powders 0Zhang B.P.,  Zheng Y.L.,  Peng Q.Y., Xiong Y.M. Q Dynamic behavior of tungsten sintered alloys at high strain rates up to 105 s-1 1Zhang B.-P.,  Xiong Y.-M.,  Yang C., Jiang C.-L. [ The influence of tungsten-atom transition on the mechanical properties of tungsten alloys $Zhang S.,  Vohra Y.K., Brister K.E. N Synchrotron X-ray and laser induced fluorescence in diamond at high pressure /Zhang R.-Q.,  Kang Q.,  Tang W.-H., Jing F.-Q. ' Equation of state (EOS) for 93W alloy 	 105-107 Zhang Z.,  Huan S., Lu F.-Y. Y Lagrangian analysis method of flow field in detonation reaction zone of high explosives Zhang J.-H., Ding J. ^ X-ray diffraction technique with VISAR support for study of shock-compressed single crystals 4Zaretsky E.,  Levi-Hevroni D.,  Ofer D., Shvarts D. ; Lateral sample motion in the plate-rod impact experiments 4 X-ray diffraction on shock-strained single crystal I Spatial evolution of three-wave structure in shocked potassium chloride 8Zaretsky E.B.,  Kanel G.I.,  Razorenov S.V., Baumung K. K Anomalous high-temperature shock-induced strengthening of two superalloys 	 645-648 &Zaretsky E.,  Herrmann B., Shvarts D. 5 Dynamic response of high temperature uranium phases aZaug J.M.,  Farber D.L.,  Craig I.M.,  Blosch L.L.,  Shuh D.K.,  Hansen D.W., Aracne-Ruddle C.M. Y Quasi-dynamic pressure and temperature <  initiated b <-> d solid phase transitions in HMX Zavattieri P.D., Espinosa H.D. > Ballistic penetration of multi-layered ceramic/steel targets :Zeigler F.J.,  McGlaun J.M.,  Thompson S.L., Trucano T.G. L Computations of hypervelocity impact uding the CTH shock wave physics code !Zeinert P.,  Bless S.J., Beno T. K Comminuted particles originating from catastrophic failure of a glass bar 	 900-902 /Zelepugin S.A.,  Nikulichev V.B., Ivanova O.V. _ Numerical simulation of superfast shock-induced chemical reaction in titanium-silicon mixture Zelepugin S.A., Dorokhov N.S. R Failure of a long rod projectile obliquely interacting with a three-layer target  1407-1410 
Zerilli F.J. . Shock induced molecular excitation in solids Zerilli F.J., Armstrong R.W. | Dislocation mechanics based constitutive relations for materials dynamics modelling: Slip and deformation twinning in iron ( Shock Waves in Condensed Matter   1987 a Dislocation mechanics based constitutive relations for dynamic straining to tensile instability N Modeling shock waves with dislocation mechanics based constitutive relations 	 257-260 Zerilli F.J., Jones H.D. < New equation of state models for hydrodynamic applications / A new global hydrogen equation of state model Young J.A., Wirth B.D. U The interaction of dislocations and radiation-induced obstacles at high strain-rate 2Yu L.H.,  Nellis W.J.,  Meyers M.A., Vecchio K.S. & Shock synthesis of niobium silicides ,Yuan G.,  Zhou G.-Q.,  Tang Z.P., Wang L.L. F An analytical model for laser-supported detonation waves on a target  1899-1902 Yun S.-R.,  Hou X.-F., Lu M. X Experimental determination of two-dimensional strain of liners under explosive loading 	 625-638 Yun S.,  Hou X., Lu M. .Yun S.-R.,  Sun Y.-F.,  Chang J.-Y., Wu F.-Y. Q Experimental investigation of phase conversion of boron nitride under explosion !Yun S.R.,  Huang Z.P., Shun Y.F. S Pressure measurement in a recovery tube for superhard BN synthesized by explosion >Yunoshev A.S.,  Silvestrov V.V.,  Kalinin A.A., Palyanov Y.N. B Shock-wave synthesis and HPHT sintering of cubic silicon nitride 3Zahariev F.,  Hu A.,  Hooper J.,  Woo T., Zhang F. A Ab initio based simulations of high-pressure phases of nitrogen @Zakaria M.,  Wu X.,  Loretto M.H.,  Millett J.C.F., Bourne N.K. G Defect analysis in Ti-based alloys deformed at different strain rates =Zakraysek A.J.,  Sutherland G.T.,  Sandusky H.D., Strange D. ^ A new gun facility dedicated to preforming shock physics and terminal ballistics experiments 
Zang J.M. q Sound speed and thermal property measurements of inert materials: Laser spectroscopy and the diamond anvil cell  73-78 2Zang J.M.,  Howard W.M.,  Fried L.E., Hansen D.W. > Detonation product EOS studies: Using ISLS to refine Cheetah Zaretsky E. ) Dislocation dynamics behind shock front O Mechanism and kinetics of phase transformation in KCl under shock compression Zaretsky E., Kaluzhny M. G Fracture threshold and shock induced strengthening of stainless steel )Yoo C.S.,  Holmes N.C.,  Ross M., See E. 3 Shock temperature measurements of iron to 350 GPa Yoo C.S., Holmes N.C. " Shock initiation of nitromethane  1567-1570 $Yoo C.S.,  Holmes N.C., Souers P.C. J Time-resolved temperatures of shocked and detonating energetic materials Yoo Y.-H., Kum O. d Numerical simulation of long rod interaction with multi-layered ceramic materials at oblique angle &Yoshida M.,  Fujiwara S., Kusakabe M. Y A new method for the evaluation of the Gruneisen parameter from Lagrangian gage records $Yoshida M.,  Tanaka K., Fujiwara S. [ A computational study of a shock collision fixture for high-pressure recovery experiments Yoshida M., Thadhani N.N. v Study of shock induced solid state reactions by recovery experiments and measurements of Hugoniot and sound velocity 	 585-592 Yoshinaka A., Zhang F. : Shock initiation and detonability of liquid nitromethane 5Yoshinaka A.C.,  Zhang F.,  Petel O.E., Higgins A.J. I Initiation of detonation in multiple shock-compressed liquid explosives You S.,  Horie Y., Hwang M. ] Modeling of shock-induced chemical reactions in powder mixtures 2: Continuum mixture theory Young D.A., Grover R. O Theory of the iron equation of state and melting curve to very high pressures G Theory of the carbon phase diagram at high pressures and temperatures Young D.A. $ The periodic law at high pressures  45-52 Young R.D. . Generalized hydrodynamic penetration process 	Young C. A Electromagnetic gauge measurement of dynamic tensile fracturing Young R., Silling S. O Experimental technique to obtain material response at strain rates to 105 s-1  1647-1650 (Young R.D.,  Littlefield D.L., Horie Y. ( Investigation of anomalous penetration  1821-1824 A Probing the shock induced reaction threshold of powder mixtures *Young D.A.,  Barbee�III T.W., Rogers F.J. 4 Simulation of shaped-charge with SPH rezone method Yao J. 2 A fast three-dimensional lighting time algorithm &Yarger F.L.,  Prieto F.E., Loske A.M. 0 Underwater shock waves in medical applications OYazaki A.,  Kishimura H.,  Hironaka Y.,  Saito F.,  Nakamura K.G., Kondo K.-I. ^ Transition from expansion to shock compression in laser irradiated silicon by multiple shots $Yaziv D.,  Bless S.J., Rosenberg Z. - Shock fracture and recompaction of ceramics 	 425-430 1Yaziv D.,  Yeshurun Y.,  Partom Y., Rosenberg Z. ; Shock structure and precursor delay in commercial alumina %Yaziv D.,  Cox P.A., Riegel�III J.P. _ Modified integral theory of impact to model long rod penetration at normal and oblique impact 7Yelkin V.M.,  Kozlov E.A.,  Kakshina E.V., Moreva Y.S. V Two-phase (g,a) equation of state for cerium and features of its dynamic compression OYenice K.M.,  Lee S.A.,  Venkateswaran U.D.,  Williamson�III W., Dubowski J.J. S Photoluminescence study of CdTe-Cd1-xMnxTe multiple quantum well at high pressure )Yeshurun Y.,  Rosenberg G., Rosenberg Z. M Measurements of compressive and tensile waves in a shock loaded pyrex glass 	 431-435 Yoh J.J., McClelland M.A. [ Simulating the thermal response of high explosives on time scales of days to microseconds $Yoneda A.,  Spetzler H., Getting I. T Implication of the complete travel time equation of state for a new pressure scale  1609-1612 $Yoo C.S.,  Furrer J.J., Duvall G.E. N Absorption spectra and reactions of carbon disulfide under shock compression #Yoo C.S.,  Gupta Y.M., Duvall G.E. M Electronic and chemical changes of carbon disulfide under shock compression 	 675-682 	Yoo C.S. d Shock induced absorption changes of anthracene in comparison with changes at static high pressures Yoo C.S.,  Holmes N.C., See E. n Shock induced optical changes in Al2O3 at 200 GPa: Implications for shock temperature measurements in metals Yagi T.,  Kondo T., Syono Y. r High pressure in situ X-ray diffraction study of MnO to 137 GPa and comparison with shock compression experiment &Yakovlev I.V.,  Pai V.V., Kuzmin G.E. ] Approximate estimate of loading parameters in composites for the case of strong shock waves Yakushev V.V. h Electrical effects in polarized polymer films under high velocity impact: Application to impact gauges  1069-1073 Yakushev V.V., Yakusheva T.I. 8 Electrical conductivity of shock-compressed PVDF films ,Yamakata M.,  Yagi T.,  Utsumi W., Fukai Y. h Electrical conductivity and crystal structure of iron hydride under high pressure and high temperature Yamamoto H., Sawaoka A.B. } Microstructure and superconducting critical temperature of dynamically consolidated YBa2Cu3O7-x without post heat treatment  Yang G.,  Tang Z.P., Zhou G.-Q. ? Non-Fourier thermoelastic response of metal induced by lasers 1Yang W.,  Ahrens T.J.,  Miller G.H., Petach M.B. % Jet ejecta mass upon oblique impact Yang W.-B., Ahrens T.J. 0 Oblique impact jetting of geological materials /Yang W.,  Chen G.,  Anderson W.W., Ahrens T.J. 6 Shock compression and isentropic release of rh<  yolite  1115-1118 +Yang Y.,  Gould R.D.,  Horie Y., Iyer K.R. Z New evidence concerning the shock-induced chemical reaction mechanism in a Ni/Al mixture Yano K.,  Horie Y., Tang Z.P. Q Calculation of nonequilibrium velocities in powder mixtures under shock loading Yano K., Horie Y. E Particle velocity dispersion in shock compression of solid mixtures E Discrete-element modeling of shock-induced phase transition in iron  Yano K.,  Horie Y., Greening D. 5 Mechanistic model of hot-spot: A unifying framework ]Yao B.,  Ding B.Z.,  Li D.J.,  Hu Z.Q.,  Su W.H.,  Geng Y.Z.,  Hu A.G.,  Lou T.P., Yang J.H. 8 A discussion on a new phase in polycrystalline diamond #Yao J.,  Gunger M.E., Matuska D.A. 'Wright T.W.,  Ramesh K.T., Molinari A. O Status of statistical modeling for damage from nucleation and growth of voids 	 690-693 JWright M.,  Williams P.,  Richardson J.,  Edmonds E.,  Jones A., Drake R. I UK marginal initiation characterisation test (MICT) for high explosives .Wu Y.H.,  Onomichi M.,  Sasaki S., Shimizu H. P High-pressure Raman studies of liquids and solids of some fluorinated methanes Wu T.-C., Bassett W.A. ^ Measuring deviatoric stress in the diamond anvil cell using two X-ray diffraction geometries  1625-1628 Wu Q.,  Tan H., Jing F.-Q. N A thermodynamic model for prediction of shock adiabatics of porous materials Xia H.,  Xia Q., Ruoff A.L. . Equation of state of BP to megabar pressures Xia Q.,  Xia H., Ruoff A.L. @ New high pressure phases of the III-IV compounds AlN, GaN, InN (Xu K.,  Yu D.-Y.,  Xu Y.-X., Zeng X.-F. Q Effect of charge diameter on detonation pressure measured by aquarium technique 	 573-577 5Xu D.-P.,  Tong X.,  Su W.-H.,  Xiao L.-Z., Li S.-T. k Structure and magnetic properties of CdS nanocrystalline materials synthesized under high static pressure Xu Y., Espinosa H.D. , Damage quantification in confined ceramics Xu X., Thadhani N.N. k Investigation of shock-induced chemical reactions in Ni-Ti powder mixtures using instrumented experiments &Xue Q.,  Nesterenko V.F., Meyers M.A. W Self-organization of adiabatic shear bands in titanium, Ti-6Al-4V and stainless steel "Xue Q.,  Gray�III G.T., Chen S.R. O Influence of shock prestraining on shear localization in 316L stainless steel %Xue Q.,  Cerreta E.K., Gray�III G.T. � Influence of explosive-driven shock prestraining on the microstructural evolution and shear localization of 304 and 316L stainless steels GYagi T.,  Hishinuma T.,  Yamakata M.,  Uchida T.,  Utsumi W., Fukai Y. U Formation and structure of iron hydride under the condition of the Earth's interior W Vibrational spectroscopic studies of reduced-sensitivity RDX under static compression (Wood S.M.,  Gupta Y.M., Pangilinan G.I. R Time-resolved Raman measurements in shocked Z-cut, a-quartz subjected to tension  1571-1574 'Wood B.P.,  Trainor R.J., Keinigs R.K. C Shock compression experimental capabilities of the ATLAS facility Woody D.,  Davis J., Coffey S. [ Real time imaging of shear bands induced by low velocity shocks during impact of crystals Woody D.L., Davis J.J. H The effect of low velocity impact on various inert crystalline samples %Woody D.L.,  Davis J.J., Deiter J.S. : Plastic flow generated solid state metal/metal reactions Y Recovery studies of impact-induced metal/polymer reactions in titanium based composites 	 667-669 Woody D., Davis J.J. ` The effect of variation of aluminum particle size and polymer on the performance of explosives 	 942-945 %Woody D.L.,  Dokhan A., Johnson C.E. Y Performance comparisons of nanoaluminum, coated microaluminum and their bimodal mixture 0Woolsey N.C.,  Wark J.S.,  Blyth W.J., Riley D. ) Sub-nanosecond powder x-ray diffraction Woolsey N.C., Wark J.S. ^ Simulated X-ray streak camera data of in situ diffraction from laser-shocked single crystals  1919-1922 /Woolsey N.C.,  Cauble R.,  Lee R.W., Wark J.S. V In situ X-ray diffraction from uniform radiation driven shocks in crystalline solids HWorkman A.,  Meziere Y.J.E.,  Millett J.C.F.,  Bourne N.K., Wallwork A. H Shear stress in nickel and Ni-60Co under one-dimensional shock loading (Wright N.G.,  McMahon M.I., Nelmes R.J. L Microstructural aspects of reconstructive phase transitions under pressure &Wright S.I.,  Bingert J.F., Zernow L. F Microtextural characterization of copper shaped charge jet fragments 5Wright T.W.,  Schoenfeld S.E.,  Ramesh K.T., Wu X.Y. H Progress in computational models for damage from shear bands and voids W Hugoniot and wave-profile measurements on shock-loaded stainless steel (21Cr-6Ni-9Mn) Wise J.L., Kipp M.E. @ Time-resolved penetration response of ceramic and steel plates &Wise J.L.,  Kerley G.I., Trucano T.G. 6 Shock-vaporization studies on zinc and porous carbon  Wise S.,  Bless S.J., Brar N.S. 1 Shock compression of chemically bonded ceramics Wise J.L., Grady D.E. M Dynamic, multiaxial impact response of confined and unconfined ceramic rods NWise J.L.,  Jones S.C.,  Hall C.A.,  Reinhart W.D.,  Hickman R.J., Gluth J.W. X Effects of annealing and preheating on the impact response of selected braze materials 	 686-689 Wisniewski R., Molinar G.F. B High pressure transducer with ceramic free rod as active element  1685-1686 Witczak Z. � The effect of hydrostatic pressurization on the microstructure and mechanical properties of the L12 Cu-modified titanium trialuminide (Witczak Z.,  Jemielniak R., Szczepek J.  The apparatus for mechanical testing of materials under high hydrostatic pressure with the in situ acoustic emission analyzer  1601-1604 0Wittman C.,  Lopatin C.,  Perron P., Swenson J. 4 Strain rate dependency of copper recrystallization GWixom M.R.,  Fechner W.B.,  Maynard R.L.,  Schmerberg N.W., Mayer F.J. ( Shock processing in spherical geometry Wixom M.R. V Shock recovery experiments on high nitrogen content, high molecular weight compounds Wixom M.W. 9 An electroluminescent fiber optic shock pressure sensor Wong M.K.W., Gupta Y.M. O Response of lateral piezoresistance gauges in fused silica shocked to 60 kbar V Dynamic inclusion analyses of lateral piezoresistive gauges under shock wave loading Wong P.T.T. E High pressure FT-IR spectroscopy for biomedical and cancer research Wong M.K.W. < Experiments and analysis of lateral piezoresistance gauges  1735-1738 Wong C.P., Gump J.C. B Shock-induced changes in the absorption spectrum of nitromethane  1563-1566 CWiney J.M.,  Dreger Z.A.,  Gruzdkov Y.A.,  Jensen B.J., Gupta Y.M. Q Equation of state and temperature measurements for shocked ammonium perchlorate Winey J.M., Gupta Y.M. 0 Anisotropic modeling for shock single crystals 	 367-372 Winfree N.A., Kerley G.I. 0 Equation of state model for tributyl phosphate KWinfree N.A.,  Chhabildas L.C.,  Reinhart W.D.,  Carroll D.E., Kerley G.I. L EOS data of Ti6Al4V to impact velocities of 10.4 km/s on a three-stage gun Winkler W.D., Stilp A.J. P Spallation behavior of TiB2, SiC, and B4C under planar impact tensile stresses O Pressure induced macro- and micromechanical phenomena in planar impacted TiB2 Winkler W.-D., Nahme H. I A simple recovery technique for shock wave studies of brittle materials  1663-1666 (Winter R.E.,  Markland L.S., Prior S.D. 3 Modelling shock initiation of HMX-based explosive OWinter R.E.,  Taylor P.,  Carley D.J.,  Barlow A.J.,  Pragnell H., Markland L. l A flash X-ray technique to measure strain distribution at interfaces sliding at high pressure and velocity NWinter R.E.,  Smeeton V.S.,  De'Ath J.,  Taylor P.,  Markland L., Barlow A.J. H Metallography of sub-surface flows generated by shock-induced friction HWinter R.E.,  Whiteman G.,  Haining G.S.,  Salisbury D.A., Tsembelis K. 8 Measurement of equation of state of silicone elastomer Winter R.E., Harris E.J. < Stress-induced resistivity of padded lateral stress gauges 'Wise J.L.,  Chhabildas L.C., Asay J.R.   Shock compression of beryllium 	 417-421 
Wise J.L. ` Refractive index and equation of state of a shock-com<  pressed aqueous solution of zinc chloride Wise J.L., Chhabildas L.C. U Laser interferometer measurements of refractive index in shock compressed materials 	 441-454 Wise J.L., Mikkola D.E. K Analysis of CsI shock-wave data in terms of high-temperature dissociation  73-75 Williams P.E. C The influence of the reaction rate of explosives on blast effects Williamson R.L., Berry R.A. X Microlevel numerical modeling of the shock wave induced consolidation of metal powders 	 341-346 ;Williamson D.L.,  Morosin B.,  Venturini E.L., Graham R.A. 3 Mossbauer study of shock-synthesised zinc ferrite 	 809-814 Williamson R.L., Wright R.N. i A particle-level numerical simulation of the dynamic consolidation of a metal matrix composite material =Williamson D.,  Palmer S.,  Grantham S.,  Proud W., Field J. " Mechanical properties of PBS9501 	 816-819 ,Williamson D.M.,  Palmer S.J.P., Proud W.G. , Fracture studies of PBX simulant materials 'Willmott G.R.,  Proud W.G., Field J.E.   Shock properties of kimberlite Wills J.M., Eriksson O. _ Theoretical studies of the crystal structure of rare earths and actinides at zero temperature &Wilson C.R.,  duvall G.E., Ogilvie K. F The resisitivity of liquid carbon disulfide during shock compression 	 296-298 Wilson K.R. 6 Molecular dynamics of chemical reactions in solution  27-34 Wilson W.H., Holloway D.C. F Relationship between wavefront curvature and surface tensile strains Wilson W.H. T Experimental study of reaction and stress growth in projectile impacted explosives 8Wilson W.H.,  Forbes J.W.,  Liddiard T.P., Doherty R.M. 4 Sensitivity studies of a new energetic formulation IWilson W.H.,  Forbes J.W.,  Gustavson P.K.,  Lemar E.R., Sutherland G.T. ; Detonation properties of the non-ideal explosive PBXW-123 hWilson J.N.,  Hashemi J.,  James D.,  G�ven N.,  Dallas T.,  Kuhrts K.,  Combs B.,  Hale M., Willson G. \ Metallurgical analysis and computer simulation of a solid steel sphere under shock loading $Winey J.M.,  Gupta Y.M., Casey K.G. IWhite C.T.,  Barrett J.J.C.,  Mintmire J.W.,  Elert M.L., Robertson D.H. V Molecular dynamics study of chemistry from strong shock waves interacting with voids $White A.,  Zerilli F.J., Jones H.D. A An ab initio method for estimating equation of state parameters 7White C.T.,  Robertson D.H.,  Swanson D.R., Elert M.L. B Critical widths in molecular dynamics simulations of detonations White S.J. ^ Direct comparison of a range of strain-rate dependent strength models on Taylor impact tests 
Whitley V.H. ( Optical absorption measurements of RDX $Whitlock R.R.,  Wark J.S., Kiehn G. 8 Streaked X-ray diffraction from laser-shocked crystals Whitlock R.R., Wark J.S. J Plasticity in shocked single crystals viewed by pulsed x-ray diffraction Whitworth N.J., Maw J.R. = Modelling shock desensitisation of heterogeneous explosives C Modelling 'hot-spot' initiation in heterogeneous solid explosives Whitworth N.J. Z Development of a simple model of 'hot-spot' initiation in heterogeneous solid explosives 5Wicks A.L.,  Kaiser M.A.,  Wilson L.T., Swantek S.D. Y Experimentally derived bar dispersion and transducer selection for split Hopkinson bars 
Wiegand D.A. F Mechanical failure properties of composite plastic bonded explosives R The influence of confinement on the mechanical properties of energetic materials Wiegand D., Reddingius B. Z Mechanical properties of plastic bonded composites as a function of hydrostatic pressure 	 812-815 
Wilkerson S. o A numerical formulation using the boundary integral method for three-dimensional bubble dynamics calculations (Williams W.D.,  Fogelson D.J., Lee L.M. % Carbon piezoresistive stress gauges 3Williams F.L.,  Lee Y.K.,  Morosin B., Graham R.A. R Catalytic activity of shock modified ZnO for CO oxidation and methanol synthesis 	 791-796 Williams Q., Jeanloz R. N Measurement and analysis of 3 GPa shock wave profiles in annealed OFE copper I Measurement and analysis of three 1.5 GPa shock-wave profiles in copper 'Warnes R.H.,  Paisley D.L., Tonks D.L. 9 Hugoniot and spall data from the laser-driven miniflyer DWebb A.W.,  Qadri S.B.,  Skelton E.F.,  Moulton N.E., Vanderah T.A. $ Compressibility of Ti2Ba2CaCu2O8+d 7Webb A.W.,  Osofsky M.S.,  Skelton E.F., Vanderah T.A. b Pressure dependence of resistivity for normal-state '123'-superconducting copper oxide compounds Weerasooriya T. < Modeling flow behavior of 93W-5Ni-2Fe tungsten heavy alloy A Modeling flow behavior of 93W-5Ni-2Fe due to sudden rate change i Modeling compressive flow behavior of a tungsten heavy alloy at different strain rates and temperatures Wei D.,  Zhang F., Woo T.K. R Ab initio molecular dynamics simulations of molecular collisions of nitromethane /Weidner D.J.,  Wang Y.,  Meng Y., Vaughan M.T. A Deviatoric stress measurements at high pressure and temperature XWeinstein B.A.,  Ritter T.M.,  Stair K.,  Choi-Feng C.,  Devane G.,  Kim H.M., Wie C.R. d Strain relaxation in highly mismatched heterostructures under high-pressure/temperature conditions MWeir S.T.,  Nellis W.J.,  Kramer M.J.,  Seaman C.L.,  Early E.A., Maple M.B. G Shock induced defects and flux pinning in YBa2Cu3O7-d + Ag composites 	 563-565 'Weir S.T.,  Nellis W.J., Mitchell A.C. B Electrical conductivity of hydrogen shocked to megabar pressures 	 881-883 
Weirick L.J. I Shock characterization of epoxy - 42 volume percent glass microballoons Weirick L.J., Navarro M.J. % Shock characterization of TOAD pins QWerdiger M.,  Eliezer S.,  Moshe e.,  Henis Z.,  Dekel E.,  Horovitz Y., Arad B. : Al and Cu dynamic strength at a strain rate of 5.108 s-1 Wester M., Prentice J.K. I The development of a multiple mesh capability for an Eulerian hydrocode i Molecular dynamics simulation of ejection induced by reflection of shock wave at free surface of metals #Wang J.-H.,  Duan W.-S., Pan Y.-S. A Molecular dynamics investigation of shock wave in one dimension  1067-1070 "Wang W.,  Jin X.-G., Rosenberg Z. ] Improved analytical model for the piezoresistive response of lateral manganin stress gauges Wang W., Tang Z. : A study on the propagation of macroscopic phase boundary Wang W., Tang Z.P. 7 A one-dimensional phase transition constitutive model !Wang Y.,  Ahuja R., Johansson B. M Calculated Hugoniot curves of porous metals: Copper, nickel, and molybdenum &Wang W.,  Tang Z.,  Gong P., Horie Y. ) Discrete element method modeling of gas Wang W.,  Tang Z., Horie Y. S Discrete element method simulation of nonlinear visc����������������������������������������������������������������������������������������������������������������������������������oelastic stress wave problems 	 371-373 'Wang S.,  Yang Y.,  Sun Z., Dlott D.D. s Shock-induced chemical reaction propagation in nanoenergetic materials observed with nanometer spatial resolution ?Wark J.S.,  Whitlock R.R.,  Hauer A.,  Swain J.E., Solone P.J. ; Short-pulse X-ray diffraction from laser-shocked crystals 	 781-786 8Wark J.S.,  Whitlock R.R.,  Kiehn G.,  Smith R., Lin Z. A Simulation of transient x-ray diffraction from shocked crystals IWark J.S.,  Woolsey N.C.,  Riley D.,  Blyth W.,  Whitlock R.R., Keihn G. x Direct measurements of compressive and tensile strain during shock breakout by use of sub-nanosecond x-ray diffraction BWark J.S.,  Belak J.F.,  Collins G.W.,  Colvin J.D.,  Davies H.M.,  Duchaineau M.,  Eggert J.H.,  Germann T.C.,  Hawreliak J.,  Higginbotham A.,  Holian B.L.,  Kadau K.,  Kalantar D.H.,  Lomdahl P.S.,  Lorenzana H.E.,  Meyers M.A.,  Remington B.A.,  Rosolankova K.,  Rudd R.E.,  Schneider M.S.,  Sheppard J., Stolken J.S. A Picosecond X-ray diffraction from laser-shocked copper and iron 	 286-291 Warnes R.H., Tonks D.L. h Comparison of detonation velocities and average vibrational motion of atom pairs in organic explosives -Walker J.D.,  Anderson�Jr. C.E., Lankford J. O Numerical simulations of split Hopkinson pressure bar compression experiments Walker J.D., Anderson�Jr. C.E. E The influence of projectile nose shape on the shock phase of impact + Multi-material velocities for mixed cells  1773-1776 Walker J.D<  . # Incoherence of shaped charge jets  1869-1872 Walker J.D., Young R.D. I Deformation mechanisms of powder particles during dynamic consolidation N An analytic penetration model for a Drucker-Prager yield surface with cutoff Walker J.D., Thacker B.H. ' Yield surfaces for anisotropic plates 0Walker J.D.,  Dannemann K.A., Anderson�Jr. C.E. : Anisotropic failure model development and implementation S New directions and new challenges in analytical modeling of penetration mechanics  1273-1278 
Wallace D.C.  37-49 ) Overdriven shocks in solids and liquids HWallwork A.,  Meziere Y.J.E.,  Millett J.C.F.,  Bourne N.K., Workman A. 8 Spallation in NiTi under one-dimensional shock loading 	 682-685 Walsh J.M. b On the problem of the oblique interaction of a detonation wave with an explosive-metal interface 
Walters C.T. 4 Laser generation of 100 kbar shock waves in solids 
Walters W.P.   Shaped charges and shock waves  1053-1060 Walters W.P., Summers R.L. a An analytical expression for the velocity difference between jet particles from a shaped charge  1861-1864 ! Shaped charge jet particulation  1873-1876 Wang J. " Asymmetric supersonic collisions 	 661-666 %Wang S.L.,  Meyers M.A., Graham R.A. = Shock consolidation of IN-100 nickel-base superalloy powder 	 731-736 Wang Z.-X.,  Li H., Zhu J.-S. Z Numerical simulation of one dimensional unsteady detonation by method of characteristics Wang J.-H., Zhang J.-G. Voltz C.,  Buy F., Roy G. Y Iron damage and spalling behavior below and above shock induced a to e phase transition 	 678-683 von�Holle W.G. ` Temperature measurements of shocked translucent materials by time-resolved infrared radiometry 	 287-291 _ Shock wave diagnostics by time-resolved infrared radiometry and non-linear Raman spectroscopy 	 283-291 %Vong T.S.,  Leyrat J.P., Pujols H.C. G Impact effects of a two-parts high velocity jet on homogeneous target 5Vorobiev O.Y.,  Antoun T.H.,  Lomov I.N., Glenn L.A. < A strength and damage model for rock under dynamic loading %Vorobiev O.,  Cowler M., Birnbaum N. A A modular material modeling architecture for nonlinear dynamics Vorthman J.E. L Facilities for the study of shock induced decomposition of high explosives 	 680-684 Vorthman J., Wackerle J. 9 Multiple-wave effects on explosives decomposition rates DVorthman J.E.,  Hixson R.S.,  Anderson W.W.,  Fritz J.N., Shaw M.S. + Release isentropes in overdriven PBX 9502 AVos W.L.,  Finger L.W.,  Hemley R.J.,  Mao H.-K., Yoder�Jr. H.S. + Phase behavior of H2-H2O at high pressure !Vrel D.,  Huang X.S., Mashimo T. 9 Shock compression recovery experiments on some dioxides 4Vukuturi S.,  Perger W.F.,  Dreger Z.A., Gupta Y.M. 7 First-principles vibrational study of pentaerythritol Wackerle J., Anderson A.D. L Burning topology in the shock-induced reaction of heterogeneous explosives Wackerle J., Stacy H.L. , Refractive index of shocked alkali halides I Shock-induced heating, phase transitions, and opacity in alkali halides ,Wakabayashi K.,  Nakamura K.G., Kondo K.-I. f Shock-induced orientation of benzen molecules studied by nanosecond time-resolved Raman spectroscopy <Wakatsuki M.,  Takano K.J.,  Kagi H.,  Yuino T., Kumagai S. T Real-time evaluation of pressure using the pressure effect on EMF of thermocouples  1695-1698 Walker F.E., Karo A.M. :Venkateswaran C.,  Jeyabalan K.,  Jaya N.V., Natarajan S. C High pressure studies of Y0.8Ba2.2Cu3O6+y and Y0.8Sr0.2Ba2Cu3O6+y 	 685-686 )Venturini E.L.,  Morosin B., Graham R.A. + Paramagnetic defects in shock-loaded TiO2  77-81 K Magnetic properties of shock-synthesised and furnace-reacted zinc ferrite 	 815-820 )Venturini E.L.,  Graham R.A., Morosin B. D Static magnetization and microwave loss in shock-modified ferrites 7Venturini E.L.,  Graham R.A.,  Ginley D.S., Morosin B. X Effects of shock modification on superconductivity in Tl2Ca2Ba2Cu3Oy and Bi2CaSr2Cu2Ox 7Vidal P.,  Cowperthwaite M.,  Presles H.-N., Bouton E. e A study of the curvature of a two-dimensional detonation wave at an explosive-confinement interface FVignjevic R.,  Millett J.C.F.,  Bourne N.K.,  Meziere Y., Lukyanov A. E The behaviour of a carbon-fibre epoxy composite under shock loading CVildanov V.G.,  Gorshkov M.M.,  Slobodenjukov V.M., Rushkovan E.H. L Shock compression of low initial density quartz at pressures up to 100 GPa Visscher P.B., Holian B.L. ` Vibrational relaxation rates in molecular fluids via equilibrium simulation: Thermal softening 1Vitello P.,  Fried L.E.,  Pudliner B., McAbee T. H Sparse partial equilibrium tables in chemically resolved reactive flow Vitello P., Souers P.C. / The piecewise linear reactive flow rate model �Vogan W.S.,  Anderson W.W.,  Grover M.,  King N.S.P.,  Lamoreaux S.K.,  Morley K.B.,  Rigg P.A.,  Stevens G.D.,  Turley W.D., Buttler W.T. Z A new spin on an old technology: Piezoelectric ejecta diagnostics for shock environments Vogler T.J., Asay J.R. O A distributional model for elastic-plastic behavior of shock-loaded materials 2Vohra Y.K.,  McCauley T.S.,  Gu G., Vagarali S.S. 9 Isotopically pure 12C diamond anvil at megabar pressure Voltz C., Roy G. ] Study of spalling for high purity iron below and aobe shock induced a to e phase transition Vandersall K.S., Thadhani N.N. 9 Shock compression synthesis of B1-type tantalum nitride T Dynamic densification of Mo-Si powder compacts for reactive solid state processing X Shock compression of Mo-Si powder mixtures using recovery and instrumented experiments EVandersall K.S.,  Forbes J.W.,  Tarver C.M.,  Urtiew P.A., Garcia F. H Re-shock experiments in LX-17 to investigate reacted equation of state � Investigation of shock-induced chemical reactions in Mo-Si powder mixtures using instrumented experiments with PVDF stress gauges fVandersall K.S.,  Murty S.S.,  Chidester S.K.,  Forbes J.W.,  Garcia F.,  Greenwood D.W., Tarver C.M. t Investigation of Steven impact test using a transportation hook projectile with gauged experiments and 3D modeling 7Vandersall K.S.,  Tarver C.M.,  Garcia F., Urtiew P.A. ] Shock initiation experiments on PBX9501 explosive at 150�C for ignition and growth modeling &Vantine H.C.,  Chan J., Erickson L.M. # Thin pulse initiation of PBX-9404 	 558-562 (Vassiliou J.K.,  Otto J.W., Porter R.F. - The equation of state of d-TaN0.8 to 72 GPa 6Vaughan B.A.M.,  Murray N.H.,  Proud W.G., Field J.E. 2 Spall strength of ceramic in a multilayer system 4Vecchio K.S.,  Andrade U.,  Meyers M.A., Meyer L.W. H Microstructural evolution in high strain, high strain-rate deformation Vecchio K.S., Gray�III G.T. F Effects of shock loading on a solid-solution strengthened superalloy 
Vecchio K.S. C Electron microscopy of shock synthesized silicides and aluminides ,Vedantam K.,  Bajaj D.,  Brar N.S., Hill S. 9 Johnson-Cook strength models for mild and DP 590 steels WVeeser L.R.,  Gray�III G.T.,  Vorthman J.E.,  Rodriguez P.J.,  Hixson R.S., Hayes D.B. . High pressure response of a high-purity iron FVenkateswaran U.D.,  Mak C.-L.,  Bak J.,  Sooryakumar R., Jonker B.T. E Pressure-induced enhancement of exchange interactions in Zn1-xCoxSe � In situ X-ray diffraction study of the phase transition from graphite to hexagonal diamond under high pressures and high temperatures Vaidya R.U., Zurek A.K. A Dynamic mechanical deformation of a SiCp/Al-Li (8090) composite 4Vaidya R.U.,  Song S.G.,  Zurek A.K., Gray�III G.T. � The effect of structural defects in SiC particles on the static and dynamic mechanical response of a 15 volume percent SiC/6061-Al matrix composite Valone S.M. = Non-Newtonian viscosity effects at shocked fluid interfaces I Particle-velocity dependent rate constants from transition-state theory Valone S.M., Kapila V. L Nonequilibrium atomistic polymer simulations under shear and shock loading  Valyanskaya T.V., Stepanov G.N. M Superconductivity at 12 K in silicon u< nder low temperature pressure release Van�Camp P.E., Van�Doren V.E. 3 Theoretical high pressure study of boronphosphide mvan�der�Heijden A.E.D.M.,  Bouma R.H.B.,  Carton E.P.,  Pacheco M.M.,  Meuken B.,  Webb R., Zevenbergen J.F. p Processing, application and characterization of (ultra)fine and nanometric materials in energetic compositions  1121-1126 cvan�Duin A.C.T.,  Zybin S.V.,  Chenoweth K.,  Zhang L.,  Han S.-P.,  Strachan A., Goddard�III W.A. f Reactive force fields based on quantum mechanics for applications to materials at extreme conditions #van�Hinsberg M.G.E., Schouten J.A. 1 The phase diagram of nitrogen clathrate hydrate "van�Thiel M.,  Ree F.H., Sayer J. g Equilibrium shock and release properties of post deformation mixtures of PBX-9404 LX-14, RDX, and TNT 	 883-889 #van�Thiel M.,  Ree F.H., Grover R. 3 Three phase carbon EOS with electronic excitation 
van�Thiel M. c Thermodynamic properties and hydrodynamic response of high-density high-temperature CHNO mixtures  79-86 van�Thiel M., Ree F.H. L Lindemann melting law for anisentropic crystals: Graphite to liquid carbon - Unlike pair interactions in N2-H2O mixtures ,Urlin V.D.,  Mochalov M.A., Mikhailova O.L. j Quasi-isentropic compression of liquid xenon up to the density of 20 g/cm3 under the pressure of 700 GPa (Urtiew P.A.,  Tarver C.M., Simpson R.L. 4 Shock initiation of 2,4-dinitroimidazole (2,4-DNI) 3Urtiew P.A.,  Tarver C.M.,  Forbes J.W., Garcia F. 5 Shock sensitivity of LX-04 at elevated temperatures 3Urtiew P.A.,  Forbes J.W.,  Tarver C.M., Garcia F. 3 Calibration of manganin pressure gauges at 250 �C 3Urtiew P.A.,  Forbes J.W.,  Garcia F., Tarver C.M. & Shock initiation of UF-TATB at 250�C tUrtiew P.A.,  Forbes J.W.,  Tarver C.M.,  Vandersall K.S.,  Garcia F.,  Greenwood D.W.,  Hsu P.C., Maienschein J.L. P Shock sensitivity of LX-04 containing delta-phase HMX at elevated temperatures  Usuba S.,  Kondo K., Sawaoka A. n Status of electromagnetic mass-accelerator development and prospect of application to high-pressure research GUtkin A.V.,  Kanel G.I.,  Baumung K.,  Karow H.U.,  Rusch D., Licht V. 7 Ion beam diagnostics by methods of shock-wave physics  1891-1894 $Utkin A.V.,  Kanel G.I., Baumung K. E Experimental observations of state of matter heated by the ion beam CUtkin A.V.,  Kanel G.I.,  Razorenov S.V.,  Bogach A.A., Grady D.E. R Elastic moduli and dynamic yield strength of metals near the melting temperature 6Utkin A.V.,  Kanel G.I.,  Bogach A.A., Razorenov S.V. ] Macrokinetics of the energy release in high explosives containing nano-size boron particles 9Utkin A.V.,  Kolesnikov S.A.,  Pershin S.V., Fortov V.E. l Reaction zone transformation for steady-state detonation of high explosives under initial density increase 	 938-941 5Utkin A.V.,  Sosikov V.A.,  Bogach A.A., Fortov V.E. # Tension of liquids by shock waves 'Utkin A.V.,  Sosikov V.A., Fortov V.E. 8 Tension of ethyl alcohol and hexadecane by shock waves 	 896-899 0Utsumi W.,  Yamakata M.,  Yagi T., Shimomura O. r Model simulation of chemical reaction in a diatomic crystal. 1: Energy exchange in rapid exothermic dissociation Tse J.S., Klug D.D. N Molecular dynamics studies of high pressure phase transitions and structures 7Tsembelis K.,  Millett J.C.F.,  Proud W.G., Field J.E. ; The shock Hugoniot properties of cement paste up to 5 GPa &Tsembelis K.,  Proud W.G., Field J.E. Q The principal Hugoniot and dynamic strength of dolerite under shock compression > The dynamic strength of cement paste under shock compression  1414-1417 8Tsembelis K.,  Proud W.G.,  Willmott G.R., Cross D.L.A. G The shock Hugoniot properties of cement paste and mortar up to 18 GPa Tsembelis K., Proud W.G. ( The dynamic behavior of micro-concrete  1496-1499 (Tsou P.,  Griffiths D.J., Buettner D.J. J Structural influence on hypervelocity intact capture in underdense media 0Tsuji K.,  Yamamoto Y.,  Katayama Y., Koyama N. E Amorphization from quenched high-pressure phase in III-IV compounds +Tsukinovsky D.,  Zaretsky E., Rutkevich I. C Polyurethane in plane impact with velocities from 10 to 400 m/sec Tunison K.S., Gupta Y.M. N Elastic precursor decay in shocked pure LiF crystals: Role of surface damage 'Tyler C.,  Millett J.C.F., Bourne N.K. 9 Spallation in Ti6Al4V: Stress measurements and recovery 	 674-677 Uchino M., Mashimo T. ' Hugoniot measurements of zinc sulfide 	 975-976 >Ueno M.,  Yoshida M.,  Onodera A.,  Shimomura O., Takemura K. K Equation of state and pressure-induced phase transition of III-V nitrides #Ulivi L.,  Barocchi F., Pratesi G. E Brillouin scattering from fluid and solid hydrogen at high pressure 	 869-872 9Urakawa S.,  Ohno H.,  Igawa N.,  Kondo T., Shimomura O. @ Synchrotron radiation study on the phase relations of KAlSi3O8 +Urlin V.D.,  Mochalov M.A., Mikhailov O.L. H Quasi-isentropic compression of liquid argon at pressure up to 500 GPa  55-56 I Studies of laser-driven flyer acceleration using optical fiber coupling > Investigation of the dynamic behavior of laser-driven flyers  1655-1658 (Trott B.D.,  Fenton G.K., Ebersole H.N. 1 Hugoniot equation of state of liquid propellant X High-speed optical studies of the driving plasma in laser acceleration of flyer plates Trott W.M., Asay J.R. u Investigation of microscale shock phenomena using a line-imaging optically recording velocity interferometer system 7Trott W.M.,  Knudson M.D.,  Chhabildas L.C., Asay J.R. � Measurements of spatially resolved velocity variations in shock compressed heterogeneous materials using a line-imaging velocity interferometer 	 993-998 0Trott W.M.,  Setchell R.E., Farnsworth�Jr. A.V. y Investigation of the effects of target material strength on the efficiency of acceleration of thick laser-driven flyers 9Trott W.M.,  Chhabildas L.C.,  Baer M.R., Caste�eda J.N. k Investigation of dispersive waves in low-density sugar and HMX using line-imaging velocity interferometry d Development of laser-driven flyer techniques for equation of state studies of microscale materials Trucano T.G., Grady D.E. O Intermediate velocity penetration of steel spheres into deep aluminum targets 4Trucano T.G.,  Barker L.M.,  Asay J.R., Kerley G.I. Q Numerical studies of the dynamic isentropic loading of solid molecular hydrogen 	 461-465 *Trucano T.G.,  Asay J.R., Chhabildas L.C. > Hydrocode benchmarking of 1-D shock vaporization experiments Trucano T.G., Chhabildas L.C. < Calculations supporting hypervelocity launcher development  1639-1642 Trunin R.F., Simakov G.V. > The peculiarities of porous metal compression in shock waves PTrunin R.F.,  Zhernokletov M.V.,  Simakov G.V.,  Gudarenko L.F., Gushchina O.N. ` Shock compression of highly porous samples of copper, iron, nickel and their equation of state Tsai D.H., Trevino S.F. C Shock wave evolution of the mechanical threshold stress in copper : Reverse plasticity effects in free-surface wave profiles 7Tonks D.L.,  Hixson R.S.,  Johnson J.N., Gray�III G.T. Y Dislocation drag contribution to high-rate plastic deformation in shock-loaded tantalum 7 Shock wave plasticity in molybdenum at 293K and 1673K _Tonks D.L.,  Hixson R.,  Gustavsen R.L.,  Vorthman J.E.,  Kelly A.,  Zurek A.K., Thissell W.R. , Spallation studies on shock loaded uranium >Tonks D.L.,  Vorthman J.E.,  Hixson R.,  Kelly A., Zurek A.K. 4 Spallation studies on shock-loaded U-6 wt. pct. Nb 'Tonks D.L.,  Zurek A.K., Thissell W.R. + Void coalescence model for ductile damage *Tonks D.L.,  Thissell W.R., Schwartz D.S. R Modeling incipient copper damage data from the tensile Hopkinson bar and gas gun FTonks D.L.,  Henrie B.L.,  Trujillo C.P.,  Holtkamp D., Thissell W.R. < Roughness of ductile damage paths in shock loaded tantalum 	 670-673 FTowler M.D.,  Hines R.I.,  Allan N.L.,  Braithwaite M., Mackrodt W.C. Q Equations of state for polar solids at high pressures and elevated temperatures <  Townsend D., Bourne N.K. 2 Measurements of the conductivity of shocked PMMA  1267-1270 *Trainor R.J.,  Holmes N.C., Anderson R.A. 8 Ultrahigh pressure laser-driven shock wave experiments 	 145-154 %Tran P.X.,  Brenner D.W., White C.T. D Nonlinear dynamics of chains interacting with a steady shock front Tranchet J.Y., Cagnoux J. f A model of plasticity with strain-hardening for shock-wave behavior of non porous and porous alumina ETrebinski R.,  Wlodarczyk E.,  Cudzilo S.,  Paszula J., Trzcinski W. 5 Investigations into the detonative synthesis of bBN Trevino S.F., Tsai D.H. c Model simulation of chemical reaction in a diatomic crystal. 2: Kinetics of equilibrium chemistry Trott W.M., Meeks K.D. F Acceleration of thin foil targets using fiber-coupled optical pulses Trott W.M. c Quasi-isentropic and shock compression measurements of iron response by direct laser illumination  1425-1428 +Timofeev B.B.,  Egorov B.V., Zvorykin L.O. H Hydrodynamic theory of shock induced anomalous mass transfer in solids *Titov V.M.,  Anisichkin V.F., Malkov I.Y. : Diamond synthesis from dynamically loaded organic matter %Togaya M.,  Sugiyama S., Mizuhara E.  Melting line of graphite Tokheim R.E., Lutze A.B. B Characterization of thermomechanical response of porous vanadium 	 246-250 
Tokheim R.E. S Analysis of electrical noise from shock loading a steel flatpack soil stress gage 	 559-564 )Tokheim R.E.,  Erlich D.C., Kobayashi T. 5 Characterization of spall in Kevlar/Epoxy composite > Interpretation of quartz-gage response in radiation problems  1715-1718 Tokheim R.E., Williams G.C. W Computed and observed experimental double pulse phenomena in aluminum PRS experiments =Tokheim R.E.,  Erlich D.C.,  Curran D.R.,  Tobin M., Eder D. 8 Aerogel algorithm for shrapnel penetration experiments 1Tollier L.,  Cottet F.,  Boustie M., Ansart J.P. Y Experimental and numerical studies of Ti-6Al-4V spallation by laser and impact loadings %Tollier L.,  Bartnicki E., Fabbro R. S Experimental and numerical study of laser-driven spallation with VISAR diagnostic Tomar V., Zhou M. ; Molecular dynamics simulation of shock induced detonation _ Molecular dynamics modeling of shock wave propagation in fcc-Al, a-Fe2O3 and their interfaces >Tong X.,  Xu D.-P.,  Su W.-H.,  Xiao L.-Z.,  Li S.-T., Han L. o Study on surface photovoltage spectra of CdS nanocrystalline materials synthesized under high static pressure Tonks D.L. J Constitutive relation for 6061T6 aluminum under shock loading conditions 	 347-351 Y Relation between shock strength and strain-rate plasticity at maximum deviatoric stress 	 ElseiverTonks D.L., Johnson J.N. Thissell W.R.,  Henrie B.L.,  Cerreta E.K.,  Anderson W.A.,  Atchison W.L.,  Cochrane J.C.,  Kaul A.M.,  Keinigs R.K.,  Ladish J.S.,  Lindemuth I.R.,  Oro D.M.,  Paisley D.,  Reinovsky R.,  Rodriguez G.,  Salazar M.A.,  Stokes J.L.,  Taylor A.J.,  Tonks D.L., Zurek A.K. Y Metallurgical characterization of Atlas cylindrically convergent spallation experiments Thoma K.,  Klee C., Ludwig D. B Theoretical investigation of the wave shaping in a shaped charge �Thomas R.J.,  Boley M.S.,  Chandrasekhar H.R.,  Chandrasekhar M.,  Parks C.,  Ramdas A.K.,  Han J.,  Kobayashi M., Gunshor R.L. v Raman and photo-modulated reflectivity studies of ZnTe/InAs semiconductor heterostructure under hydrostatic pressure Thomas J.N. T Influence of plasticity models upon the outcome of simulated hypervelocity impacts  1785-1788 HThomas K.A.,  Martin E.S.,  Kennedy J.E.,  Garcia I.A., Foster�Jr. J.C. > Transient detonation processes in a plastic bonded explosive Thompson W.E., Predebon W.W. Z An investigation of incipient fracture in shock-loaded lamellar cobalt-aluminum eutectic 	 451-455 Thompson D.G., Wright W.J. 4 Mechanical properties from PBX 9501 pressing study KThornhill T.F.,  Reinhart W.D.,  Chhabildas L.C.,  Grady D.E., Wilson L.T. 1 Cylinder fragmentation using gas gun techniques >Thornhill T.F.,  Vogler T.J.,  Reinhart W.D., Chhabildas L.C. E Polycrystalline aluminum oxynitride Hugoniot and optical properties .Thornhill T.F.,  Chhabildas L.C., Vogler T.J. * Tube fragmentation of multiple materials 	 666-669 Thyer A.M., W Byers B. J Quantitative computer analysis of low velocity detonation in AN and ANFO (Tierney T.E.,  Swift D.C., Johnson R.P. N Novel techniques for laser-irradiation driven, dynamic materials experiments OTierney T.E.,  Swift D.C.,  Luo S.-N.,  Niemczura J.,  Gammel J.T., Peralta P. .Ternovoi V.Y.,  Pyalling A.A., Filimonov A.S. � Quasi-isentropic plane compression of matter at megabar pressures by using a layered system to diminish first shock wave intensity  1243-1245 ZTernovoi V.Y.,  Kvitov S.V.,  Nikolaev D.N.,  Pyalling A.A.,  Filimonov A.S., Fortov V.E. W Experimental study of transition of Jupiter and Saturn atmosphere to conducting state  1492-1495 Thadhani N.N. = Shock induced chemical synthesis of intermetallic compounds 	 503-510 'Thadhani N.N.,  Dunbar E., Graham R.A. P Characteristics of shock-compressed configuration of Ti and Si powder mixtures DThadhani N.N.,  Subramanian V.,  Russell R.,  Savage D., Gupta Y.M. Z The effect of pulse duration on shock-induced chemical reaction in Ti-Si powder mixtures ZThadhani N.N.,  Vandersall K.S.,  Russell R.T.,  Graham R.A.,  Holman G.T., Anderson M.U. U Shock compression of Al+Fe2O3 powder mixtures of different volumetric distributions )Thakur A.M.,  Thadani N.N., Schwarz R.B. L Martensitic transformation in NiTi alloys induced by tensile stress pulses Tham R.H., Stilp A.J. F Dynamic strength calculations of W-alloys based on grain deformation (Thissell W.R.,  Zurek A.K., Addessio F. d Mechanical properties and failure mechanisms of carbon fiber reinforced epoxy laminated composites 5Thissell W.R.,  Zurek A.K.,  Tonks D.L., Hixson R.S. o Experimental quantitative damage measurements and void growth model predictions in the spallation of tantalum nThissell W.R.,  Zurek A.K.,  Macdougall D.A.S.,  Miller D.,  Everett R.,  Geltmacher A.,  Brooks R., Tonks D. P The effect of material cleanliness in dynamic damage evolution in 10100 copper 3Thissell W.R.,  Tonks D.L.,  Schwartz D., House J. ] Dynamic failure resistance of two tantalum materials with different melt practice sequences WTasker D.G.,  Goforth J.H.,  Oona H.,  Fowler C.M.,  King J.C.,  Herrera D., Torres D. X Advances in isentropic compression experiments (ICE) using high explosive pulsed power �Tasker D.G.,  Goforth J.H.,  Oona H.,  Rigg P.A.,  Dennis-Koller D.,  King J.,  Torres D.,  Herrera D.,  Sena F.,  Abeyta F., Tabaka L. 7 Results from isentropic compression experiments (ICE) Taylor J.W.  Thunder in the mountains  3-15 Taylor P.A. R The effects of grain size on the shock sensitivity of porous granular explosives Taylor P.A., Dodson B.W. 5 Simulation of lattice damage due to dynamic loading 	 287-292 &Taylor P.A.,  Boslough M.B., Horie Y. @ Modeling of shock-induced chemistry in nickel-aluminum systems 0 Shock-induced atomic-scale structure in metals `Taylor P.E.,  Gilbert P.H.,  Kernthaler C.,  Lee L.M.,  Smith E.A.,  Reeder S.T., Anderson M.U. ( Quartz gauge response in ion radiation FTaylor P.,  Salisbury D.A.,  Markland L.S.,  Winter R.E., Andrew M.I. 9 Reaction of shocked but undetonated HMX-based explosive &Taylor P.,  Cook I.T., Salisbury D.A. W Development of an explosively driven sustained shock generator for shock wave studies CTaylor E.A.,  Tsembelis K.,  Chapman D.,  Proud W.G., Cockell C.S. < Hugoniot properties of dry Yorkshire sandstone up to 8 GPa  1488-1491 9Ternovoi V.Y.,  Fortov V.E.,  Kvitov S.V., Nikolaev D.N. 6 Experimental study of lead critical point parameters ]Ternovoi V.Y.,  Filimonov A.S.,  Fortov V.E.,  Lomosonov O.V.,  Nikolaev D.N., Pyalling A.A. C Investigation of tin thermodynamics in near critical point region ZTernovoi V.Y.,  Filimonov A.S.,  Fortov V.E.,  Kvitov S.V.,  Nikolaev D.N., Pyalling A.A. L Liquid-vapor phase boundaries deter<  mination by dynamic experimental method KTernovoi V.Y.,  Filimonov A.S.,  Pyalling A.A.,  Mintsev V.B., Fortov V.E. F Thermophysical properties of helium under multiple shock compression )Tarver C.M.,  Erickson L.M., Parker N.L. q Shock initiation, detonation wave propagation and metal acceleration measurements and calculations for RX-26-AF Tarver C.M., Maiden D.E. h Experimental measurements and numerical simulations of metal spallation by detonating solid explosives Tarver C.M. 7 The structure of detonation waves in solid explosives 	 311-315 (Tarver C.M.,  Simpson R.L., Urtiew P.A. 3 Shock initiation on an e-Cl-20-estane formulation D Chemical reaction and equilibration mechanisms in detonation waves ` Next generation experiments and models for shock initiation and detonation of solid explosives 	 873-877 3Tarver C.M.,  Forbes J.W.,  Urtiew P.A., Garcia F. & Shock sensitivity of LX-04 at 150 �C 0 What is a shock wave to an explosive molecule?  42-49 3Tarver C.M.,  Forbes J.W.,  Garcia F., Urtiew P.A. U Manganin gauge and reactive flow modeling study of the shock initiation of PBX 9501 3 On the existence of pathological detonation waves 3 Detonation reaction zones in condensed explosives  1026-1029 $Tashiro S.,  Mashimo T., Nishida M. G Consolidation of tantalum nitride system powders by shock compression  1295-1298 Tasker D.G., Lee R.J. O High current electrical conduction of pressed condensed detonating explosives 	 923-928 &Tasker D.G.,  Granholm R.H., Lee R.J. o The fast measurement of electrical conductivity structure within the detonation zone of a condensed explosive Tasker D.G., Baker R.N. u A new, unbiased method for analyzing streak data, the calibration of the NSWC expanded large scale gap test (ELSGT) ATasker D.G.,  Dick R.D.,  Wilson W.H.,  Lee R.J., Gustavson P.K. P Response of wet, saturated, and dry riverbed sands to high strain rate loading %Tasker D.G.,  Dick R.D., Wilson W.H. O Mechanical properties of explosives under high deformation loading conditions @Tang Z.P.,  Li X.Z.,  Zhou G.Q.,  Lin S.B.,  Li D.H., Wang W.Q. m Experimental investigation of shear stress effects on shock-induced phase transition in InSb single crystal Tang J., Endo S. ~ X-ray study of the transitions among the rutile, a-PbO2 and baddeleyite phases of TiO2 at high pressure and high temperature 0Tang W.-H.,  Zhang R.-Q.,  Jing F.-Q., Hu J.-B. M Restudy on the thermal relaxation at interfaces following shock compression Tang P.K., Scannapieco A.J.  Modeling cylinder test #Tang Z.P.,  Horie Y., Psakhie S.G. V Discrete meso-element dynamic simulation of shock response of reactive porous solids > Apparent spectral radiance at shocked metal/window interface $Tang P.K.,  Hixson R.S., Fritz J.N. 2 Modeling PBX 9501 overdriven release experiments Tang Z.P.,  Liu W., Horie Y. D Numerical investigation of pore collapse under dynamic compression .Tang Z.P.,  Liu W.,  Wang W.,  Chen L., Hu X. L 3D discrete meso-element method and its application to spherical collision Tang Z.P., Wang W.W. J Discrete element modeling for shock processes of heterogeneous materials 	 679-684 Tang Z., Xu J. _ A combined DEM/FEM multiscale method and structure failure simulation under laser irradiation ,Tang Z.,  Tang X.,  Zhang X.,  Hu H., Xu W. ` Abnormal spall behavior observed in pure iron and FeMnNi alloy undergoing a-e phase transition 	 662-665 Tanguay V., Higgins A.J. r Comparison of critical conditions for initiation of porous PETN by shock waves transmitted from solids and gases $Taniguchi T.,  Kondo K., Sawaoka A. 3 Shock wave profiles in powder compacts of a Al2O3 	 773-778 (Tao W.C.,  Tarver C.M., Breithaupt D.R. H Fundamental chemical interactions in metal filled composite explosives #Tappan B.C.,  Son S.F., Moore D.S. [ Nano-aluminum reaction with nitrogen in the burn front of oxygen-free energetic materials  1022-1025 0Takayama K.,  Saito K.,  Obara T., Kameshima N. U High pressure generation by underwater shock wave focusing in an ellipsoidal cavity Takemura K. 1 High-pressure X-ray diffraction study of barium 0Takizawa H.,  Yamazaki K.,  Endo T., Shimada M. Y High-pressure synthesis and magnetic properties of T1-xT'xGe4(T,T':3d transition metal) 3Tamura H.,  Ueda K.,  Sawaoka A.B., Igenbergs E.B. 4 Microprojectile acceleration by plasma accelerator Tamura S., Horie Y. G Discrete meso-element simulation of chemical reactions in shear bands ?Tan T.H.,  Fritz J.N.,  Marsh S.P.,  McQueen R.G., Steele R.D. E Characterization of simple explosively driven particle acceleration 	 665-667 Tan T.-H., Marsh S.P. > Plasma production from shock compression of condensed matter %Tanaka K.,  Fujiwara S., Kusakabe M. , 2-D simulations of shock recovery fixtures . Calculations of liquid plane-wave generators KTanaka K.,  Fujiwara S.,  Sellam M.,  Presles H.N.,  Brochet C., Cheret R. 7 Calculations of overdriven detonation in nitromethane Tanaka K., Ookouchi T. 8 Impact of dryice projectiles on elastic plastic bodies ; High-speed impact of dry-ice projectiles onto thin plates  1853-1856 `Tanaka K.,  Noda K.,  Hyodo Y.,  Nakamura H.,  Kosaka K.,  Nakayama T.,  Katayama M., Takeba A. < XDT in HTPB propellant from steel flyer plate impact tests 
Tanaka K. B Shock compression of solid with voids by gridless Lagrangian SPH  1117-1120 Tang Z.P., Gupta Y.M. * Shock response of CdS/BAMO:THF composite 	 305-307 %Tang Z.P.,  Bellamy P.M., Gupta Y.M. L Stress dependence of the current ramping observed in shorted quartz gauges 	 609-610 1Tang P.K.,  Seitz W.L.,  Stacy H.L., Wackerle J. < A study of the contribution of slow reaction in detonation 
Tang P.K. > A study of the impact of reaction rates on equation of state Syed I.H., Brar N.S. A Strain rate sensitivity of graphite/polymer laminate composites f High strain rate compression and tension characterization of high strength (automotive) sheet steels FSyono Y.,  Goto T.,  Wang W.K.,  Iwasaki H.,  Ohshima S., Wakiyama T. - Shock synthesis experiments of Nb-Si system  87-91 Syono Y., Goto T. J Shock wave facilities for high pressure experiments at Tohoku University 	 701-705 	Syono Y. S Shock-induced phase transitions in solids: Their understanding at atomistic level _Syono Y.,  Nagoshi M.,  Kikuchi M.,  Tokiwa A.,  Aoyagi E.,  Suzuki T.,  Kusaba K., Fukuoka K. ? Shock loading effects on high Tc superconductor Bi-Sr-Ca-Cu-O CSyono Y.,  Taguchi H.,  Fukai Y.,  Atou T.,  Kusaba K., Fukuoka K. H Shock compression of VH0.50, NbH0.75, and TaH0.50: A comparative study 0Syono Y.,  Hikosaka H.,  Kikuchi M., Fukuoka K. @ Shock-synthesis of a metastable tetragonal phase of EuBa2Cu3Oy 8Syono Y.,  Noguchi Y.,  Fukuoka K.,  Kusuba K., Atou T. Q Shock induced phase transition of MnO and several other transition metal oxides 	 151-154 &Szarzynski S.,  Martinez E., Heuz� O. [ Experimental study of the detonation initiation of pure nitromethane by a reflected shock 	 899-901 Tagi Y. ~ Recent advances in high pressure and high temperature in situ X-ray studies using sintered diamond and synchrotron radiation  1621-1624 =Takarabe K.,  Takumi M.,  Minomura S.,  Nakagawa T., Ohta K. < Resonant tunneling in triple barriers diode under pressure GTakarabe K.,  Hitomi S.,  Mori Y.,  Minomura S.,  Niwa E., Masumoto K. 2 Pressure effects on optical properties of AgGaS2 KTakarabe K.,  Shirase N.,  Minomura S.,  Kato H.,  Watanabe Y., Matsuda K. 7 Electron emission spectra of DX center under pressure KTakashima K.,  Tonda H.,  Nishida M.,  Hagino S.,  Suzuki M., Takeshita T. D Preparation of oxide superconducting coils by explosive compaction < Detonation Hugoniots produced by piston-driven simulations Swanson D.R., White C.T. = Steady flow detonations from molecular dynamics simulations 3Sweeney M.A.,  Perry F.C.,  Asay J.R., Widner M.M. / Shock effects in particle beam fusion targets 	 188-192 Swegle J.W., Grady D.E. C Shock vis<  cosity and the calculation of steady shock wave profiles 	 353-357 Swegle J.W. < A numerical study of Rayleigh-Taylor instability in solids L Heterogeneous deformation model for the high pressure strength of aluminum T Irreversible phase transitions and wave propagation in silicate geologic materials 
Swegle J. 3 Non-steady wave profiles and the fourth-power law 	 249-252 Swenson C.A., Anderson M.S. H Equations of state for the alkali metals, with generalizations to NaCl 
Swenson C.A. 3 Shock wave overtake measurements on cesium iodide 	 135-144 Swift R.P. E Shock attenuation in saturated rock using an effective stress model Swift D.C.  Shear banding in Ti-6Al-V Swift R.P., Snell C.M. E Source conditions for exploding wire stress wave impact experiments  1671-1674 0 Ab fere initio equations of state for aluminum . Ab fere initio equations of state for solids  23-26 6 Ab initio polymorphic equations of state for silicon Swift D.C., Braithwaite M. > Temperature-dependent reactive flow for non-ideal explosives 2Swift D.C.,  Paisley D.L.,  Kyrala G.A., Hauer A. I Simultaneous VISAR and TXD measurements on shocks in beryllium crystals  1192-1195 "Swift D.,  Paisley D., Knudson M. H Equation of state measurements for beryllium in the ICF capsule regime Swift D.C., Ruiz C.R. > Laser-induced Mach waves for ultra high pressure experiments  1297-1300 NSwitzer L.L.,  Vandersall K.S.,  Chidester S.K.,  Greenwood D.W., Tarver C.M. _ Threshold studies of heated HMX-based energetic material targets using the Steven impact test a Measurement of ultrasonic wave velocities in silica glass at high temperature and high pressure *Sun C.,  Zhao F.,  Wen S.,  Li Q., Liu C. A High velocity flyers accelerated by multi-stage explosive slabs Sundaram S., Clifton R.J. I Flow behavior of soda-lime glass at high pressures and high shear rates Surh M.P., Runge K.J. ) Theoretical phase diagrams for solid H2 Sutherland G.T. I Multiple stress-time profiles in the Navy explosive PBXN-110 (PBXW-113) FSutherland G.T.,  Forbes J.W.,  Lemar E.R.,  Ashwell K.D., Baker R.N. L Multiple stress-time profiles in a RDX/AP/Al/HTPB plastic bonded explosive pSutherland G.T.,  Lemar E.R.,  Forbes J.W.,  Anderson E.,  Miller P.,  Ashwell K.D.,  Baker R.N., Liddiard T.P. l Shock wave and detonation wave response of selected HMX based research explosives with HTPB binder systems HSutherland G.T.,  Ashwell K.D.,  O'Connor J.H.,  Baker R.N., Lemar E.R. 5 Shock response of several plastic bonded explosives ;Sutherland G.T.,  Gustavson P.K.,  Lemar E.R., O'Connor J. * Shock response of the explosive PBXN-103 Sutherland G.T., Burns J. < Explosive response model evaluation using the explosive H6 4 Stress growth measurements for the explosive IRX-4 E Shock response of a mock explosive containing sugar and HTPB binder 	 808-811 rSuzuki I.,  Kumazawa M.,  Inouye Y.,  Ohno I.,  Oda H.,  Sasaki K.,  Sugawara T.,  Syono Y.,  Kumagai H., Suda N. x Elasticity measurements on the material analogous to iron in the inner core of the Earth by FT-ultrasonic spectroscopy Svendsen B., Ahrens T.J. , Thermal history of shock compressed solids ,Swallowe G.M.,  Field J.E., Hutchinson C.D. K Impact experiments on thin layers of polymers and intermediate explosives 	 891-898 (Swanson R.W.,  Straub G.K., Holian B.L. B Molecular dynamics study of sodium using a model pseudopotential 	 241-245 &Swanson D.R.,  Elert M.L., White C.T. Stout R.B., Anderson G.A. * Dislocation kinetics behind shear shocks Stout R.B. D Microcrack dependent discontinuity conditions across a shock front 0Strachan A.,  van�Duin A.C.T., Goddard�III W.A. \ Initial chemical events in the energetic material RDX under shock loading: Role of defects RStraight J.W.,  Idar D.J.,  Smith L.,  Osborn M.A.,  Viramontes L.E., Chavez P.J. O Measuring the energy release of low amplitude impact of high explosive events ;Strassburger E.,  Patel P.,  McCauley J.W., Templeton D.W. � High-speed photographic study of wave propagation and impact damage in fused silica and AlON using the edge-on impact (EOI) method 	 892-895 Straub G.K. @ The overlap of electron core states for very high compressions  85-93 'Straub G.K.,  Wills J.M., Wallace D.C. ) Elastic moduli of copper under pressure P Extrapolation of the shear modulus to high compressions and negative pressures Streletz G.J., MacFarland L.H. ? A new browser for the visualization of equation of state data AStrutt A.J.,  Vecchio K.S.,  Yu L.-H.,  Meyers M.A., Graham R.A. Stuivinga M., Carton E.P. 1 Shock wave compacted, melt infiltrated ceramics )Stuivinga M.,  Verbeek H.J., Carton E.P. = Planar compaction of ceramic powders with mining explosives 	 745-750 @Su W.-H.,  Yu R.-C.,  Xu D.-P.,  Li X.-Z.,  Zhang Z., Kuo K.-H. � Formation of six new orthorhombic approximants of decagonal quasicrystals in Al70Co15Ni10Tb5 alloy by quenching under high-static pressure #Su D.,  Santare M.H., Gazonas G.A. N Numerical modeling of wave propagation in anisotropically microcracked media Subramanian V., Thadhani N.N. O Reaction behavior of shock compressed aluminum and iron-oxide powder mixtures Sudenkov Y. r Influence of the structural levels on the elastic-plastic hardening of metals under submicrosecond shock loading 	 627-629 Suito K., Miyoshi M. 4Stevens G.D.,  Vesser L.R.,  Rigg P.A., Hixson R.S. 2 Suitability of magnesium oxide as a VISAR window  1353-1356 Stevenson D.J. a The role of high pressure experiment and theory in our understanding of gaseous and icy planets Stewart S.T., Ahrens T.J. & Shock wave propagation in porous ice B A new H2O ice Hugoniot: Implications for planetary impact events  1478-1483 )Stewart S.T.,  Ahrens T.J., O'Keefe J.D. : Impact-induced melting of near-surface water ice on Mars  1484-1487 dStewart D.S.,  Thomas K.A.,  Clarke S.,  Mallett H.,  Martin E.,  Martinez M.,  Munger A., Saenz J. J On the initiation mechanism in exploding bridgewire and laser detonators 3Stewart D.S.,  Lambert D.E.,  Yoo S., Wescott B.L. N Experimental validation of detonation shock dynamics in condensed explosives  1018-1021 aStewart S.T.,  Kennedy G.B.,  Senft L.E.,  Furlanetto M.R.,  Obst A.W.,  Payton J.R., Seifter A. I Post-shock temperature and free surface velocity measurements of basalt $Stiel L.I.,  Rotondi P., Baker E.L. 7 Optimization of parameters for JCZ3 equation of state Stiel L.I., Baker E.L. @ Detonation energies of explosives by optimized JCZ3 procedures U Optimized JCZ3 procedures for detonation properties at highly overdriven conditions %Stiel L.I.,  Baker E.L., Capellos C. M JAGUAR analyses of experimental detonation values for aluminized explosives G Study of detonation and cylinder velocities for aluminized explosives [Stilp A.J.,  Hohler V.,  Schneider E.,  Tham R.,  H�lsewig M.,  Kuscher G., Junckermann W. / Impact facilities at the Ernst-Mach Institute 	 711-712 Stixrude L., Cohen R.E. D First principles investigation of bcc, fcc, and hcp phases of iron nStokes J.,  Fulton R.D.,  Morgan D.V.,  Obst A.W.,  Oro D.M.,  Oona H.,  Anderson W.,  Chandler E.A., Egan P. ` Material failure and pattern growth in shock-driven aluminum cylinders at the Pegasus facility Q Molecular dynamics and experimental study of shock polarization of nitromethane Soulard L., Crouzet B. A Molecular dynamics analysis of a liquid explosive reaction zone 
Stacey F. S Thermodynamic relationships and the properties of iron at Earth's core conditions ?Stacy H.L.,  Steitz W.L.,  Wackerle J.,  Polcyn M., Esparza E. 2 Contained high explosive firing facility (CHEFF)  1675-1678 +Staehler J.M.,  Predebon W.W., Pletka B.J. ? The response of a high purity alumina to plate impact testing PStahl D.B.,  Gehr R.J.,  Harper R.W.,  Rupp T.D.,  Sheffield S.A., Robbins D.L. E Flyer velocity characteristics of the laser-driven miniflyer system Stapleton B.S., Gupta Y.M. H Response of single crystal calcite shocked to 40 kbar along the c-<  axis Stassis C. k Inelastic neutron scattering of g-iron and the determination of the elastic constants by lattice dynamics ,Staudhammer K.P.,  Johnson K.A., Olinger B. N 1.2 Mbar shock loaded 304 stainless steel: Residual structure and properties Staudhammer K.P., Johnson K.A. > Mach stem characterization in Mbar designs using RSR powders 	 737-742 Staudhammer K.P. 7 Temperature effects in shock consolidation of powders Steele R.D., Tan T.-H.  Fast shock tube assemblies Steinberg D.J., Sharp�Jr. R.W. m Interpretation of shock-wave data for beryllium and uranium with an elastic-viscoplastic constitutive model 	 367-371 Steinberg D.J. 3 A rate dependent constitutive model for beryllium 6 Computer studies of the dynamic strength of ceramics 4 A rate-dependent constitutive model for molybdenum / Modeling release behavior in shocked tantalum .Stepanov G.N.,  Gavriliuk A.G., Lyubutin I.S. = Mossbauer study of HSTHF for Sn119 in NdFeO3 under pressure  1481-1484 )Sterer E.,  Pasternak M.P., .Taylor R.D. : Pressure induced metallization of the Mott insulator VI2  1453-1456 V Effects of temperature on an ISL-PVDF shock sensor between +20 deg. C and -40 deg. C 	 891-892 (Solie D.J.,  Johnson J.B., Barrett S.A. 7 The response of natural snow to explosive shock waves Solv� G., Cagnoux J. 9 The behavior of pyrex glass against a shaped-charge jet >Somayazulu M.S.,  Ramachandran H.S.,  Sharma S.M., Sikka S.K. K Phase transition in potassium titanyl phosphate (KTP) under high pressure *Somayazulu M.S.,  Sharma S.M., Sikka S.K. N Molecular dynamical calculations of a-quartz: Implications for shock results !Son S.F.,  Asay B.W., Bdzil J.B. A Inert plug formation in the DDT of granular energetic materials 	Son S.F.  The combustion of explosives  1059-1064 Son S.F., Berghout H.L. * Flame spread across surfaces of PBX 9501  1014-1017 Song I., Thadhani N.N. J Effects of shock processing parameters on synthesis of nickel aluminides Song S., Gray�III G.T. 1 Omega phase formation in shock-loaded zirconium 9Song H.,  Bless S.J.,  Brar N.S.,  Simha C.H., Jang S.D. - Shock properties of Al2O3 and ZrO2 ceramics &Song S.G.,  Gray�III G.T., Lopez M.F. 7 Deformation response of zirconium after shock-loading Sorber S.S., Winter R.E. E The effect of precursor shocks on the growth to detonation of EDC37 FSorenson D.S.,  Minich R.W.,  Romero J.L.,  Tunnell T.W., Malone R.M. N Ejecta particle size distributions for shock-loaded tin and aluminum targets Sorrell F.Y., Kuo T.-M. 1 Dynamic response of moist soil to shock loading Souers P.C., Garza R. , Size effect and detonation front curvature Soulard L., Bauer F. ^ Applications of standardized PVDF shock gauges for shock pressure measurements in explosives Soulard L. D Shock polar calculation using Gauss' principle of least constraint P Shock polar calculation of inert nitromethane by molecular dynamics simulation / Characterization of HMX particles in PBX 9501 NSkidmore C.B.,  Phillips D.S.,  Asay B.W.,  Idar D.J.,  Howe P.M., Bolme D.S. = Microstructural effects in PBX 9501 damaged by shear impact .Skripnyak V.A.,  Skripnyak E.G., Zhukova Y.V. S Computer simulation of the propagation of short shock pulses in ceramic materials .Skripnyak E.G.,  Skripnyak V.A., Nazarov M.N. \ Mechanical behaviour of nanostructured materials at high strain rates: Computer simulation NSkripnyak V.A.,  Skripnyak E.G.,  Garkushin G.V.,  Kolobov Y.R., Dudarev E.F. � Influence of martensitic transformation on the spall strength and the shear strength of NiTi under shock wave loading in the temperature range from 213 K to 413 K 	 658-661 Skryl Y., Kuklja M.M. C Numerical simulation of the vacancy diffusion in shocked crystals M Numerical simulation of diffusion of electrons and holes in shocked silicon #Skryl Y.,  Belak A.A., Kuklja M.M. K Numerical simulation of shock induced polarization in binary electrolytes GSmilowitz L.B.,  Henson B.F.,  Asay B.W.,  Dickson P.M., Robinson J.M. 2 Kinetics of the b-d phase transition in PBX 9501 _Smilowitz L.,  Henson B.F.,  Asay B.W.,  Dickson P.M.,  Oschwald D.M.,  Romero J.J., Parker G. < Morphology changes during thermal decomposition of PBX9501 bSmilowitz L.,  Henson B.F.,  Sandstrom M.M.,  Asay B.W.,  Oschwald D.M.,  Romero J.J., Novak A.M. F Fast internal temperature measurements in PBX9501 thermal explosions Smith R.W., Srolovitz D.J. T Computer simulation of impact induced fracture and fragmentation in brittle solids +Smugeresky J.E.,  McCabe T.J., Graham R.A. i Effect of powder particle size and shape on the microstructure of explosively compacted stainless steel Soga S.,  Kondo K., Sawaoka A. 4 Shock compaction of TiN/TiC solid solution powders 3Solie D.J.,  Johnson J.B.,  Dutta P.K., Kalafut J. Sikka S.K., Gupta S.C. * Shock induced amorphization of materials 	 145-150 #Silvera I.F.,  Chen N., Moshary F. L Orientational order in the solid hydrogens: The boomerang phase line in HD ESilvestri M.R.,  Schroeder J.,  Persans P.D.,  Hwang L.W., Zhao X.S. F Optical high pressure studies of ternary semiconducting nanocrystals Silvestrov V.V., Gorshkov N.N. K Effect of strain rate on the tensile strength of copper shaped charge jet Simha C.H.M., Bless S.J. E Carbon piezoresistive gauges in one-dimensional stress measurements  1037-1039 &Simha C.H.M.,  Bless S.J., Bedford A. . Modelling precursor decay in AD-99.5 alumina 	 231-234 1 What is the peak stress in ceramic bar impacts? Simonenko V.A. D Shock compression of condensed matter up to gigabar pressure range  41-47 &Simonsen I.K.,  Horie Y., Graham R.A. & Shock synthesis of nickel aluminides 	 743-748 (Simpson R.L.,  Urtiew P.A., Tarver C.M. 4 Shock initiation of 1,3,3-trinitroazetidine (TNAZ) Singh A.K. n The effect of stress anisotropy on the lattice strains measured with an X-ray difraction opposed anvil setup  1629-1632 `Sinitsyna L.M.,  Novikov S.A.,  Gray�III G.T.,  Cerreta E.,  Henrie B.,  Lopez M., Yablinsky C. L Substructure evolution in energetic-driven spherically shock-loaded copper !Sitaud B.,  P�r� J., Th�venin T. 5 Melting curve determination for cerium up to 30 GPa XSiviour C.R.,  Williamson D.M.,  Grantham S.G.,  Palmer S.J.P.,  Proud W.G., Field J.E. * Split Hopkinson bar measurements of PBXs 	 804-807 Siviour C.R., Proud W.G. ? Measurements of strain propagation in Hopkinson bar specimens  1293-1296 �Skelton E.F.,  Moulton N.E.,  Kim C.C.,  Qadri S.B.,  Webb A.W.,  Wolf S.A.,  Osofsky M.S.,  Berkley D.D.,  Lechter W.T., Liebenberg D.H. 0 Effects of pressure on high Tc superconductors 4Skidmore C.B.,  Phillips D.S.,  Son S.F., Asay B.W. J A computer model for the evolution of impact damage in brittle materials Shimizu H., Sasaki S. � New method of high-pressure Brillouin studies for elastic properties of molecular single crystals grown in a diamond-anvil cell =Shishkova N.V.,  Malyshev E.N.,  Shepel V.M., Mikheenko P.N. _ Influence of pressure and temperature of deformation on phase composition of yttrium ceramics JShkuratov S.I.,  Talantsev E.F.,  Baird J.,  Altgilbers L.L., Stults A.H. z Transverse explosive shock-wave compression of Nd2Fe14B high-energy hard ferromagnets: Induced magnetic phase transition 	 282-285 VShkuratov S.I.,  Talantsev E.F.,  Baird J.,  Temkin H.,  Altgilbers L.L., Stults A.H. � Longitudinal shock wave depolarization of Pb(Zr52Ti48)O3 polycrystalline ferroelectrics and their utilization in explosove pulsed power mShon J.W.,  Ree F.H.,  Viecelli J.A.,  van�Thiel M.,  Young D.A.,  Schmidt R.D.,  Hrubesh L.H., Vantine H.C. D Hugoniots of aerogels involving carbon and resorcinal formaldehyde :Shor A.,  Zaretsky E.,  Ohtera K.,  Sasoh A., Takayama K. 8 Dynamic mechanical properties of aluminum alloys GIGAS PShotnikova M.A.,  Strokina T.I.,  Krylov N.A.,  Mescheryakov Y.I., Divakov A.K. ; Formation of rotation in titanium alloys at shock loading Shpatakovskaya G.V. P Generalized statistical model: Scott correction at <  any temperature and density Shrader J.E., Bjorkman M.D. G High temperature phase transformation on the titanium alloy Ti-6Al-4V 	 310-314 	Shuda Z. 8 The surface impurity distribution on synthetic diamond 8Shunin V.M.,  Nabatov S.S.,  Yakushev V.V., Volkov A.P. U High-speed spherical solid registration by the use of piezoelectric composite films Sikka S.K. B Shock Hugoniot equation of state   electron band theory approach  71-84 )Sikka S.K.,  Sharma S.M., Chidambaram R. T Steric constraints: A powerful criterion to predict the onset of phase transitions 6 Description of a new 63-mm diameter gas gun facility 	 565-570 Sheffield S.A. / Onset of shock-induced reaction in liquid CS2 Sheffield S.A., Alcon R.R. + Shock induced reaction in several liquids . In-situ magnetic gauge measurements in Kel-F JSheffield S.A.,  Gustavsen R.L.,  Alcon R.R.,  Graham R.A., Anderson M.U. > Particle velocity and stress measurements in low density HMX ,Sheffield S.A.,  Gustavsen R.L., Alcon R.R. H Observations of shock-induced reaction in liquid bromoform up to 11GPa 8 Hugoniot and initiation measurements on TNAZ explosive ; Porous HMX initiation studies: Sugar as an inert simulant (Sheffield S.A.,  Davis L.L., Engelke R. W Detonation properties of nitromethane, deuterated nitromethane, and bromonitromethane X In situ magnetic gauging technique used at LANL: Method and shock information obtained  1043-1048 PSheffield S.A.,  Davis L.L.,  Baer M.R.,  Engelke R.,  Alcon R.R., Renlund A.M. < Hugoniot and shock initiation studies of isopropyl nitrate HSheffield S.A.,  Gustavsen R.L.,  Alcon R.R.,  Robbins D.L., Stahl D.B. B High pressure Hugoniot and reaction rate measurements in PBX9501 ZSheffield S.A.,  Dattelbaum D.M.,  Alcon R.R.,  Robbins D.L.,  Stahl D.B., Gustavsen R.L. F Shock-induced chemical reaction in organic and silicon based liquids Shen X.A., Gupta Y.M. R Time-resolved luminescence measurements in ruby shocked along the crystal A-axis 	 893-895 
Sherman D.M. K Electronic structure, entropy and the high-pressure stability of bcc iron =Shibue T.,  Nakayama E.,  Natsumura T.,  Tanaka T., Asano T. 2 Numerical simulation of impact penetration tests  1789-1792 WShigemori K.,  Ichinose D.,  Irifune T.,  Otani K.,  Shiota T.,  Sakaiya T., Azechi H. ` Measurements of sound velocity of laser-irradiated iron foils relevant to Earth Core condition  1480-1483 
Shimamura S. O Chemistry of energetic materials under shock caused by electronic excitations 	 639-645 Sharma J., Coffey C.S. T Nature of ignition sites and hot spots studied by using an atomic force microscope `Sharma J.,  Hoover S.M.,  Coffey C.S.,  Tompa A.S.,  Sandusky H.W.,  Armstrong R.W., Elban W.L. C Structure of crystal defects in damaged RDX as revealed by an AFM ISharma J.,  Coffey C.S.,  Armstrong R.W.,  Elban W.L., Lanzerotti M.Y.D. r Nanostructure of porosity (and entrapped solvent effects) in laboratory-grown crystals of RDX as revealed by AFM CSharma J.,  Coffey C.S.,  Armstrong R.W.,  Elban W.L., Hoover S.M. � Sub-molecular fracture steps in shock-shattered RDX crystals and follow-on nano-indentation evaluation of early state plasticity Shaw M.S., Johnson J.D. > A slow reaction rate in detonations due to carbon clustering 
Shaw M.S. v Direct Monte Carlo simulation of chemical equilibrium composition of molecular fluid mixtures under shock conditions @ Chemical equilibrium in high pressure molecular fluid mixtures R An equation of state for detonation products incorporating small carbon clusters � A theoretical equation of state for detonation products with chemical equilibrium composition of the surface of small carbon clusters V A hybrid Monte Carlo method for equilibrium equation of state of detonation products < Direct simulation of detonation products equation of state Shaw M.S., Tymczak C.J. � Theoretical N2 Hugoniot using MondoSCF density functional quantum energies and a very efficient Monte Carlo reweighting scheme  Sheffield S.A., Bloomquist D.D. 3 Low pressure Hugoniot cusp in polymeric materials  57-61 Sheffield S.A., Fisk G.A. F Particle velocity measurements in laser irradiated foils using ORVIS 1Sheffield S.A.,  Rogers�Jr. J.W., Caste�eda J.N. O Velocity measurements of laser-driven flyers backed by high impedance windows 	 541-546 Sheffield S.A., Dugan D.W. NSetchell R.E.,  Chhabildas L.C.,  Furnish M.D.,  Montgomery S.T., Holman G.T. R Dynamic electromechanical characterization of the ferroelectric ceramic PZT 95/5 	 781-784 @Setchell R.E.,  Montgomery S.T.,  Chhabildas L.C., Furnish M.D. e The effects of shock stress and field strength on shock-induced depoling of normally poled PZT 95/5 O Recent progress in understanding the shock response of ferroelectric ceramics 	 191-196 9Setchell R.E.,  Tuttle B.A.,  Voigt J.A., Venturini E.L. N Effects of initial porosity in the shock response of normally poled PZT 95/5 (Setchell R.E.,  Tuttle B.A., Voigt J.A. ; Microstructural effects on the shock repsonse of PZT 95/5 	 180-183 :Setchell R.E.,  Montgomery S.T.,  Cox D.E., Anderson M.U. W Dielectric properties of PZT 95/5 during shock compression under high electric fields 	 278-281 Sewell T.D. L Monte Carlo calculations of the physical properties of RDX, b-HMX and TATB 2Sewell T.D.,  Bedrov D.,  Menikoff R., Smith G.D.  Elastic properties of HMX Sewell T.D., Menikoff R. F Complete equation of state for b-HMX and implications for initiation 3Shahinpoor M.,  Asay J.R.,  Dixon W.R., Hawke R.S. 7 Effects of barrel joints on hypervelocity projectiles CShaner J.W.,  Hixson R.S.,  Winkler M.A.,  Boness D.A., Brown J.M.  Birch's law for fluid metals Shaner J.W. = Role of d-electrons in phase transitions and thermodynamics ^Sharma J.,  Hoffsommer J.C.,  Glover D.J.,  Coffey C.S.,  Santiago F.,  Stolovy A., Yasuda S. r Comparative study of molecular fragmentation in sub-initiated TATB caused by impact, UV, heat and electron beams 5Sharma J.,  Forbes J.W.,  Coffey C.S., Liddiard T.P. H The nature of reaction sites and sensitization centers in TATB and TNT Sharma S.M., Gupta Y.M. U Relating the ruby R-line spectra to deformation under shock amd hydrostatic loading 	 887-892 
Sharma J. 
Sekine T. ' Shock transformation in boron nitride Sekine T., Ahrens T.J. + Equation of state of heated glassy carbon MSekine T.,  Maruyama Y.,  Nagata M.,  Mizutani N.,  Kitagawa H., Inoguchi H. 2 Shock-induced phase transformation of fullerites 4Sekine T.,  Tashiro S.,  Kobayashi T., Matsumura T. = The NIRIM two-stage light gas gun: Performance test results Sekine T., Kobayashi T. ] Shock-induced phase transition of 6H polytype SiC and an implication for post-diamond phase R Shock-induced process during compression of graphite perpendicular to the c-axis 8 Shock-induced cubic silicon nitride and its properties  1113-1118 HSekine T.,  Hirata N.,  Yamaguchi A.,  Kobayashi T.,  He H., Tang Z.-P. T Shock flattening of spheres in porous media: Implications for flattened chondrules <Selezenev A.A.,  Berezhko P.G.,  Ganchuk N.S., Kreknin D.A. O Molecular dynamics simulation of shock wave interaction with defects in solid \Selezenev A.A.,  Golubev V.K.,  Aleinikov A.Y.,  Butnev O.I.,  Barabanov R.A., Voronin B.L. C Molecular dynamics simulation of shock wave compression of metals 	 374-377 MSelim F.A.,  Wells D.P.,  Harmon J.F.,  Kwofie J.,  Lancaster G., Jones J.L. ` Measurements of dynamic structural changes in laser-shocked materials by positron annihilation LSenf H.,  Hornemann U.,  Rothenh�usler H.,  Scharpf F.,  Poth A., Pfrang W. \ Experimental and numerical investigations concerning the dynamics of penetration processes 	 539-543 Seo M.S., Ryu J. M Explosively driven ferroelectric generator for compact pulsed power systems  1313-1316 Setchell R.E. + Sandia 25 meter compressed helium/air gun Setchell R.E., Taylor P.A. I Dynamic and static compressibility of porous gr<  anular hexanitrostilbene 	 871-876 C Visible emission from granular explosives during shock initiation 1 Response of PVDF gauges to structured waveforms [ Influence of a rare gas on the vibrational spectrum of a diatomic system at high pressure  1487-1490 2Schuster S.H.,  England R.,  Koik V., Wagner M.H. | 1- and 2-dimensional calculations of the effect of high pressure EOS models on the energy partitioning in cratering events 8Schwartz A.J.,  Cazamias J.U.,  Fiske P.S., Minich R.W. = Grain size and pressure effects on spall strength in copper 9Schwarz R.B.,  Kasiraj P.,  Vreeland�Jr. T., Ahrens T.J. F The effect of shock duration on the dynamic consolidation of powders Schwarz O.J., Horie Y. K Stress fluctuation and order generation in shearing of granular materials 
Seaman L. B Development of computational models for microstructural features 	 118-129 Seaman L., Keough D.D. = Lagrangian analysis with an emphasis on unloading phenomena 5 Determining a soil model from wave propagation data 	 627-632 YSeaman C.L.,  Early E.A.,  Maple M.B.,  Nellis W.J.,  Holt J.B.,  Kamegai M., Smith G.S. Y Superconducting and microstructural properties of shock compacted high Tc oxide powders )Seaman L.,  Boustie M., de�Resseguier T. J Use of the Steinberg and Carroll-Holt model concepts in ductile fracture Seaman L., Curran D.R. 0 Inertia and temperature effects in void growth Secco R.A. ; High pressure measurements of viscosities of Fe-S liquids D Load cycling and pressure efficiency in a large volume cubic press  1593-1596 : High pressure DSC signal amplification using thermopiles  1691-1694 Segletes S.B., Walters W.P. % Comments on the Gr�neisen parameter Segletes S.B. , Vibrational stiffness of an atomic lattice TSeifter A.,  Stewart S.T.,  Furlanetto M.R.,  Kennedy G.B.,  Payton J.R., Obst A.W. 1 Post-shock temperature measurements of aluminum Seitz W.L. ) Short-duration shock initiation of TATB "Sekine T.,  Akaishi M., Setaka N. C Shock-induced oxidation-reduction reaction in the system Fe-Fe2O3 J Twinning, texture and constitutive relations for explosively formed jets ,Schiferl S.K.,  Davidson R.F., Maudlin P.J. 3 Effects of anisotropy on dynamic tensile behavior �Schirber J.E.,  Samara G.A.,  Morosin B.,  Assink R.,  Loy O.,  Wang H.,  Williams J.,  Murphy D.,  Kortan A.R.,  Rossiensky M.,  Zhou O.,  Zhu Q.,  Kniaz K., Fischer J.E. - Role of pressure in the study of fullerenes (Schloessin H.H.,  Secco R.A., Spal R.D. O On pressure figures in single crystals, mechanical strength and high stresses 4Schmalz R.F.,  Fedosejevs R.,  Sigel R., Teng Y.-L. ( Laser-driven shock waves in plexiglass 	 535-539 
Schmidt R.M. ! Boeing shock physics laboratory 	 634-638 'Schmidt S.C.,  Moore D.S., Shaner J.W. 4 Raman spectroscopies in shock-compressed materials 	 293-302 4Schmidt S.C.,  Moore D.S.,  Shaw M.S., Johnson J.D. > Vibrational spectroscopy of shock compressed fluid N2 and O2 K Coherent anti-Stokes Raman spectroscopy of shock-compressed liquid oxygen Schmitt D.R., Ahrens T.J. - Emission spectra of shock compressed solids &Schmitt D.,  Svendsen B., Ahrens T.J. ' Shock induced radiation from minerals 	 261-265 4Schmitt M.J.,  Kopp R.A.,  Moore D.S., McGrane S.D. G Analysis of laser-driven shocks in confined and unconfined geometries 
Schmitt R.G. 2 Toward a new paradigm for reactive flow modeling Schneider H., Jung I. G Structural deformation of experimentally shock-loaded periclase (MgO) 	 140-144 USchneider M.S.,  Gregori F.,  Kad B.K.,  Kalantar D.H.,  Remington B.A., Meyers M.A. F Laser-induced shock compression of copper and copper aluminum alloys Schonberg W.P., Ebrahim A.R. [ A shock physics based model of a oblique impact of a thin plate by a spherical projectile Schott G.L. G Measured Hugoniot states of a two-element fluid, O2 + N2 near 2 Mg/m3 !Schouten J.A., Scheerboom M.I.M. Savic P., Celebonovic V. 2 Dense matter theory: A simple classical approach :Savinykh A.S.,  Kanel G.I.,  Razorenov S.V., Rajendran A. J Compressive fracture of brittle materials under divergent impact loading 	 888-891 =Saw C.K.,  Zaug J.M.,  Farber D.L.,  Weeks B.L., Aracne C.M. g Using simultaneous time-resolved SHG and XRD diagnostics to examine phase transitions of HMX and TATB 	 856-859 Saw C.K., Tarver C.M. < Binder/HMX interaction in PBX9501 at elevated temperatures Sawaoka A., Kondo K. 6 Shock wave facility at Tokyo Institute of Technology 	 696-700 
Sawaoka A.B. 9 The role of shock wave compression in materials science  51-56 Sawaoka A.B., Akashi T. A A new concept of dynamic sintering utilizing post shock heating 2Sawaoka A.B.,  Kunishige H.,  Tamura H., Horie Y. Q Heterogeneous shock compression mechanism of diamond powders in a metal capsule 8Sawaoka A.B.,  Dan K.,  Tamura H.,  Horie Y., Yamada K. q Local rapid quenching in a powder mixture and its utilization to synthesize novel compounds in the B-C-N system &Sawas O.,  Brar N.S., Ramamurthy A.C. S High strain rate characterization of plastics using polymeric split Hopkinson bar $Sawas O.,  Brar N.S., Brockman R.A. I High strain rate characterization of low-density low-strength materials 
Scheidler M. ? Formulas for the pressure and bulk modulus in uniaxial strain > Response of nonlinear elastic solids to oblique plate impact J Universal relations for pressure-shear waves in nonlinear elastic solids Scheidler M., Gazonas G. W Analytical and computational study of one-dimensional impact of graded elastic solids S Universal relations for acceleration wave speeds in nonlinear viscoelastic solids y Approximate universal relations between shock and acceleration wave speeds for oblique plate impact of inelastic solids Schiferl S.K. ^ Effects of pressure on the orientational ordering and phase transitions in solid C60 and C70 N From ferroelectric to quantum paraelectric KTa1-xNbxO3 (KTN): A model system 	 176-179 %Samsonov D.,  Zhdanov S., Morfill G. 5 Shock waves and solitons in complex (dusty) plasmas 	Sanai M. C Two examples of industrial applications of shock physics research 	 463-467 MSander R.,  Blais N.,  Engelke R.,  Dattelbaum D.,  Sheffield S., McInroy R. 1 Shock-induced chemistry in polydimethylsiloxane *	

 !"#$%&'()*+,-./0123456789:;<=>?@ABCE����FGHIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~�Sandstrom F.W.,  Persson P.A., Olinger B. \ Isothermal and shock compression of high density ammonium nitrate and ammonium perchlorate  1409-1412 9Sandstrom F.W.,  Abernathy R.L.,  Leone M.G., Banks M.L. Q Diameter effect and detonation front curvature of ideal and nonideal explosives *Sandusky H.W.,  Elban W.L., Liddiard T.P.  Compaction of porous beds ' Shock Waves in Condense Matter - 1983 Sandusky H.W., Bernecker R.R. ? Shock reactivity experiments on a porous composite propellant E Gun-launched impact initiation of the composite propellant PBXN-103 Sandusky H.W., Chambers G.P. 8 Shock reactivity of the liquid propellant Otto Fuel II ) Instrumentation of slow cook-off events .Sandusky H.W.,  Granholm R.H., Yakaboski O.N. 4 Deformation around cavities from compressive loads Sandusky H.W., Granholm R.H. 6 Prompt reaction of aluminum in detonating explosives Sano Y., Sano T. M Thermal properties of close-packed iron determined using Hugoniot functions Sarracino R.S., Guest A. @ Measured and predicted strains in the near zone of a blasthole Sasaki S., Shimizu H. 7 High-pressure Brillouin study of liquid and solid N2O LSatapathy S.,  Cazamias J.,  Bless S.,  Monfredo�Gee R.,  Meyer L., Brar N. 3 Dynamic strength of tungsten-nickel-cobalt alloys Saumon D., Guillot T. N Shock compression of deuterium at Mbar pressures and the interior of Jupiter = Thermodynamic limits of the index of refraction of hydrogen 5 Refractive index of diamond anvils at high pressure -Ruoff A.L.,  Luo H.,  Xia H., Vanderborgh C. + 5 mm X-ray appertures and their metrology  1633-1636 BRupp T.D.,  Gehr R.J.,  Stahl D.B.,  Sheffield S.A., Robbins D.L. B Temperature controlled vessel for equation of state measurements <  RRupp T.D.,  Gehr R.J.,  Bucholtz S.M.,  Robbins D.L.,  Stahl D.B., Sheffield S.A. V Stereo camera system for calibration and analysis of small laser-driven flyer plates !Russell R.,  Bless S.J., Beno T. / Impact induced failure zones in Homalite bars $Rutkevich I.,  Zaretsky E., Mond M. & Stability of strong shocks in metals (Ruuskanen P.R.,  Kiiski A.A., Heczko O. = Microstructure of dynamically compacted amorphous materials )Rycerz Z.A.,  Jacobs P.W.M., Hooton I.E. ( Molecular dynamics study of detonation -Salansky N.,  Mar H.,  Hawken D., Kleiman Y. > Basic features of dynamic phase transition in finite samples 6Salisbury D.A.,  Winter R.E.,  Taylor P., Harris E.J. , The response of foams to shock compression )Salisbury D.A.,  Giles A.R., Winter R.E. 0 Transmission of shocks along thin-walled tubes Salisbury D.A., Markland L. J Assessment and application of a PVDF gauge strain compensation technique $Salisbury D.,  Winter R., Biddle L. t A study on the effect of electrical energy imput on detonation failure in wedges of the TATB-based explosive EDC35  1010-1013 Saltz D., G�len S.C. 2 A study of the liquefaction shock wave structure %Salyer T.R.,  Khalsa N.S., Hill L.G. 8 An automated test bed for VISAR probe characterization Samara G.A., Bauer F. 9 Hydrostatic pressure studies of PVDF and its copolymers Samara G.A. Z The effects of pressure on the b molecular relaxation process in polyvinylidene fluoride 6Samara G.A.,  Hansen L.V.,  Morosin B., Schirber J.E. G Further considerations of the adiabatic exponent in steady detonation ' Do JCZ and BKW EoS need modification? j Large-scale molecular dynamics simulations of shock wave in Laves crystals and icosahedral quasicrystals 	 378-381 H Constant volume specific heat capacity of the CJ state of nitromethane 0 Shock waves and solitary waves in bcc crystals 	 302-305 (Rothman S.R.,  Evans A.M., Freeman N.J. ; Copper shock Hugoniot experiments using high power lasers Rothman S.D., Evans A.M. 9 High accuracy EOS experiments using the AWE Helen laser |Rothman S.D.,  Evans A.M.,  Graham P.,  Parker K.W.,  Palmer J.,  Jalinaud T.,  Davis J.-P.,  Asay J.,  Knudson M., Hall C. \ Measurements of the equation of state of lead under varying conditions by multiple methods =Rothman S.D.,  Parker K.W.,  Davis J.-P.,  Palmer J., Maw J. E Isentropic compression of lead and lead alloy using the 'Z' machine Rottenkolber E., Arnold W. 9 An analytic model of close-range blast fragment loading  1403-1406 
Rottler J.S. \ Multigroup radiation transport in one-dimensional Lagrangian radiation-hydrodynamics codes O Radiation diffusion in the three-dimensional radiation-hydrodynamics code CTH Rubin M.B. - Analysis of weak shocks in 6061-T6 aluminum "Rubin M.B.,  Elata D., Attia A.V. a Modeling added compressibility of porosity and the thermomechanical response of wet porous rock HRudakov F.M.,  Hastings J.B.,  Dowell D.H.,  Schmerge J.F., .Weber P.M. J Megavolt electron beams for ultrafast time-resolved electron diffraction  1287-1292 Ruggiero A., Bonora N. M Ductile damage prediction in Taylor impact cylinder test using CDM approach \ On the presence of the elastic precursor in re-shock experiment: An unorthodox explanation Ruoff A.L. - High pressure as a probe of the solid state  13-34 ) Implications of experiments on hydrogen Ruoff A.L., Ghandehari K. Rosenberg Z., Brar N.S. - Hysteresis of lateral piezoresistive gauges  1707-1710 l On the correlation between dynamic compressive strengths of strong ceramics and their indentation hardness Rosenberg Z., Ginzburg A. Q On the source for failure of commercial manganin gauges at high shock pressures ;Rosenberg Z.,  Dekel E.,  Hohler V.,  Stilp A.J., Weber K. d Penetration of tungsten alloy rods into composite ceramic targets: Experiments and 2-D simulations B Review on lateral stress measurements with piezoresistive gauges  1033-1037 ;Rosenberg Z.,  Bourne N.K.,  Gray�III G.T., Millett J.C.F. B On the measurement of shear-strength in quasi-isentropic loading Rosenberg Z., Dekel E. / On the entrance phase in long rod penetration  1310-1313 %Rosenberg Z.,  Ginzburg A., Dekel E. G More on the use of commercial carbon resistors as low pressure gauges +Rosenberg Z.,  Bourne N.K., Millett J.C.F. a Calibration of commercial gauges of varying geometry to measure the lateral component of stress �Rosolankov� K.,  Kalantar D.H.,  Belak J.F.,  Bringa E.M.,  Caturia M.J.,  Hawreliak J.,  Holian B.L.,  Kadau K.,  Lomdahl P.S.,  Germann T.C.,  Ravelo R.,  Sheppard J., Wark J.S. h X-ray diffraction from shocked crystals: Experiments and predictions of molecular dynamics simulations Ross M., Nellis W.J. Q Equation of state experiments and theory relevant to modeling the major planets 	 226-230 Ross M. q A review of some recent theoretical calculations of phase transitions and comparisons with experimental results (Ross M.,  Mao H.K.,  Bell P.M., Xu J.A. P The equation of state of dense argon: A comparison of shock and static studies = The dissociation of dense liquid nitrogen and shock cooling Roth J. x Correlation of impulsive strain effects in rocks with detonation parameters of the strain-generating explosive charges 	 475-479 =Romain J.P.,  Hallouin M.,  Gerland M.,  Cottet F., Marty L. H a to e phase transition in iron induced by laser generated shock waves Romain J.P., Zagouri D. W Laser shock studies using an electromagnetic gauge for particle velocity measurements 0Romain J.P.,  Bauer F.,  Zagouri D., Boustie M. A Measurements of laser induced shock pressures using PVDF gauges  1915-1918 Romero V., Williams P.E. ' Blast waves from non-ideal explosives tRosen M.D.,  Phillion D.W.,  Price R.H.,  Campbell E.M.,  Obenschain S.P.,  Whitlock R.R.,  McLean E.A., Ripin B.H. k Creation of ultra high pressure shocks by the collision of laser accelerated disks: Experiment and theory &Rosenberg G.,  Yaziv D., Mayseless M. N Electromagnetic gauge for measuring the radial particle velocity in 2-D flow 	 495-499 
Rosenberg G. @ RAFAEL Terminal Ballistics Laboratory: Facility and capability 	 706-710 *Rosenberg Z.,  Mayseless M., Rosenberg G. P Measurement of the radial displacement in 2D flow by embedded constantan wires Rosenberg Z., Partom Y. l Direct measurement of temperature in shock-loaded polymethylmethacrylate with very thin copper thermistors b On the lateral stress measurement in shock loaded targets with transverse piezoresistance gauges 	 525-530 
Rosenberg Z. h Determination of dynamic yield strengths with manganin gauges embedded in impulsively-loaded long rods 9Rosenberg G.,  Lopatin C.M.,  Rajendran A.M., Bless S.J. = Electrically driven expanding ring generator set up at UDRI %Rosenberg Z.,  Brar N.S., Bless S.J. W Determination of the strength of shock loaded ceramics using double impact techniques Rosenberg G., Curran D.R. N Two dimensional compression shock waves generated by plate impact techniques 4 The response of ceramic materials to shock loading 	 439-446 ` Shear strength of titanium diboride under shock loading measured by transverse manganin gauges 3Roberson S.,  Davis R.F.,  Joshi V.S., Fienello D. / Shock compaction of molybdenum nitride powder 	 643-646 7Robertson D.H.,  Brenner D.W.,  Elert M.L., White C.T. P Simulations of chemically-sustained shock fronts in a model energetic material Robertson D.H. 3 Molecular dynamics simulations of shock processes *Robertson D.H.,  Brenner D.W., White C.T. u Effects of crystal orientation on the properties of a chemically sustained shock wave in a model energetic material 9Robertson D.H.,  Barrett J.J.C.,  Elert M.L., White C.T. J Self-similar behavior from molecular dynamics simulations of detonations Robinson A.C. ? An analytical model for Rayleigh-Taylor instability in solids CRobinson A.C.,  Vaughan C.T.,  Fang H.E.,  Diegert C.F., Cho K.-S. J Hydrocode development on the NCUBE and the Connection Machine Hypercubes Robinson C<  .M. 3 Modelling of laser spall experiments in aluminium  1359-1362 ; A multi-phase equation of state for solid and liquid lead K Material properties on a phase boundary of a multiphase equation of state 	 274-277 )Rodriguez G.,  Roberts J.P., Taylor A.J. k Electromagnetically-driven cylindrical 2D shockwave profile measurements in water with laser shadowgraphy 5Rodriguez G.,  Clarke S.A.,  Taylor A.J., Forsman A. s Diagnosis of ultrafast laser-heated metal surfaces and plasma expansion with absolute displacement interferometry  1401-1404 Roessig K.M., Foster�Jr. J.C. R Experimental simulations of dynamic stress bridging in plastic bonded explosives 
Roessig K.M. 2 Mesoscale mechanics of plastic bonded explosives 	 973-978 *Roessig K.M.,  Gonthier K.A., Klomfass A. @ Modeling of low pressure compaction and mesoscale localization 	 800-803 :Rohde R.W.,  Wise J.L.,  Byrne J.G., Panchanadeeswaran S. f Microstructural-hardness correlations in shock-loaded and quasi-statically deformed 6061-T6 aluminum  North Holland9 Shock wave propagation process in epoxy syntactic foams 9Ribeiro J.,  G�is J.,  Campos J.,  Plaksin I., Mendes R. l Investigation of collapse and jet formation of hollow glass micro spheres in inert and energetic materials  1021-1024 7Ribeiro J.B.,  Mendes R.L.,  Plaksin L.Y., Campos J.A. P Features of the shock and detonation waves in cylindrical explosive compaction Rice B.M., Trevino S.F. B Monte Carlo calculations of the properties of solid nitromethane Richmond C.T. A Gap test modeling to predict wedge tests initiation of PBXN-103 8 Modeling the asymmetric burning of ultrafine particles Riedel W.,  Nahme H., Thoma K. d Equation of state properties of modern composite materials: Modeling shock, release and spallation Rigg P.A., Gupta Y.M. y X-ray diffraction measurements to determine longitudinal and transverse lattice deformation in shocked lithium fluoride  1051-1056 CRigg P.A.,  Anderson W.W.,  Olson R.T.,  Buttler W.T., Hixson R.S. J Investigation of ejecta production in tin using plate impact experiments Rightley M. n Calibration and validation of high explosives equations of state with an experimental cylinder test database Rimer N.,  Cherry J.T., Lie K. J Simulation of particle velocity records from small scale explosive tests &Riou C.,  Cottentot C.E., Boussuge M. 8 New experimental approach of impact on silicon carbide #Ripley R.C.,  Zhang F., Lien F.-S. H Shock interaction of metal particles in condensed explosive detonation PRobbins D.L.,  Gehr R.J.,  Harper R.W.,  Rupp T.D.,  Sheffield S.A., Stahl D.B. + Laser-driven miniflyer induced gold spall |Robbins D.L.,  Kelly A.M.,  Alexander D.J.,  Hanrahan R.J.,  Snow R.C.,  Gehr R.J.,  Rupp T.D.,  Sheffield S.A., Stahl D.B. 7 Dynamic properties of shock loaded thin uranium foils *Robbins D.L.,  Sheffield S.A., Alcon R.R. ; Magnetic particle velocity measurements of shocked Teflon uReisman D.B.,  Forbes J.W.,  Tarver C.M.,  Garcia F.,  Cauble R.C.,  Hall C.A.,  Asay J.R.,  Struve K., Furnish M.D. 6 Isentropic compression of LX-04 on the Z accelerator uRemington B.A.,  Hawreliak J.,  Lorenz K.T.,  Lorenzana H.E.,  McNaney J.M.,  Pollaine S.M.,  Swift D.C., Yaakobi B. - Materials response under extreme conditions 	 765-770 !Remiot C.,  Chapron P., Demay B. Y A flash X-ray radiography diagnostic for studying surface phenomena under shock loading  1763-1766 $Remiot C.,  Mexmain J.M., Bonnet L. J Precise method to determine points on isentropic release curve on copper Remo J.L., Furnish M.D. 4 High intensity X-ray coupling to meteorite targets  1410-1413 Renero C., Prieto F.E. = Reduced variables and universality in high pressure physics % Shock Hugoniot for porous materials *Renlund A.M.,  Sheffield S.A., Trott W.M. W Time-resolved infrared spectral photography studies of shock-induced chemistry in CS2 	 237-242 Renlund A.M., Trott W.M. < Spectroscopic studies of shocked and detonating explosives 	 547-552 R Raman spectroscopic studies of shock-compressed nitromethane and nitromethane-d3 
Renlund A.M. M Reactive wave growth in shock-compressed thermally degraded high explosives Resnyansky A.D., Gray�III G.T. T Numerical simulations of the influence of loading pulse shape on SHPB measurements .Resnyansky A.D.,  Bourne N.K., Millett J.C.F. D Experiment and theory for the characterization of porous materials Resnyansky A.D., Bourne N.K. d Factors influencing the shape of the fracture wave induced by the rod impact of a brittle material , Shock compression of dry and hydrated sand  1474-1477 9Ribeiro J.,  Plaksin I.,  Campos J.,  Mendes R., G�is J. Z Process of shock attenuation inside a hollow glass microsphere/polymeric composite media /Ribeiro J.,  Campos J.,  Plaksin I., Mendes R. MReed R.P.,  Greenwoll J.I.,  Bauer F.,  Lee L.M.,  Davies F.W., Johnson D.J. @ Pulsed radiation response of stressed PVDF shock stress gauges  1743-1746 *Reed E.J.,  Joannopoulos J.D., Fried L.E. k Hugoniot constraint molecular dynamics study of a transformation to a metastable phase in shocked silicon 7Reed E.J.,  Manaa M.R.,  Joannopoulos J.D., Fried L.E. T Electronic excitations, vibrational spectra, and chemistry in nitromethane and HMX 	 385-390 7Reed E.J.,  Fried L.E.,  Manaa M.R., Joannopoulos J.D. Q A method for tractable dynamical studies of single and double shock compression +Reed E.J.,  Soljacic M., Joannopoulos J.D. / The color of shock waves in photonic crystals  1307-1312 4Reed E.J.,  Soljacic M.,  Gee R., Joannopoulos J.D. S Prediction of coherent optical radiation from shock waves in polarizable crystals  1345-1348 =Reho J.H.,  Moore D.S.,  Funk D.J.,  Fisher G.L., Rabie R.L. k Ultrafast spectroscopic investigation of shock compressed glycidyl azide polymer and nitrocellulose films  1219-1222 -Reinhart W.D.,  Chhabildas L.C., Wilson L.T. O Dynamic yield strength and spall strength determination for AerMet 100 steels ;Reinhart W.D.,  Chhabildas L.C.,  Winfree N.A., Grady D.E. * Dynamic properties of tributyl phosphate <Reinhart W.D.,  Chhabildas L.C.,  Trott W.M., Dandekar D.P. D Investigating multi-dimensional effects in single-crystal sapphire Reinhart W.D., Chhabildas L.C. 9 Dynamic strength of AD995 alumina at Mbar stress levels 	 759-764 > Response to unloading and reloading of shock compressed PMMA Reinovsky R.E., Trainor R.J. P Hydrodynamic and material properties experiments using pulsed power techniques wReinovsky R.E.,  Anderson W.E.,  Atchison W.L.,  Faehl R.J.,  Keinigs R.K.,  Lindemuth I.R.,  Thompson M.C., Taylor A. _ Shock-wave and material properties experiments using the Los Alamos Atlas pulsed power system � Hugoniot elastic limit and spall strength of aluminum and copper single crystals over a wide range of strain rates and temperatures 9Razorenov S.V.,  Savinykh A.S.,  Kanel G.I., Shakun S.N. [ Sub-microsecond yield and tensile strengths of metals and alloys at elevated temperatures 9Razorenov S.V.,  Kanel G.I.,  Savinykh A.S., Fortov V.E. C Large tensions and strength of iron in different structure states 	 650-653 Reaugh J.E. = Computer simulation and analysis of the expanding ring test 	 395-399 @ Computer simulations of the explosive consolidation of powders @ The influence of target strength model on computed perforation  1797-1800 E Computer simulations to study the high-pressure deflagration of HMX 1Redmer R.,  Juranek H.,  Nettelmann N., Holst B. - Warm dense hydrogen in the chemical picture 5Ree F.H.,  Nellis W.J.,  van�Thiel M., Mitchell A.C. U Experimental and theoretical studies on shock compression of liquid carbon monoxide ERee F.H.,  Nellis W.J.,  Trainor R.J.,  Mitchell A.C., Boslough M.B. Q Theoretical and experimental studies of shock-compressed benzene and polybutene 	Ree F.H. @ Phase changes and chemistry at high pressures and temperatures Ree F.H., Calef D.F. 2 Theoretical Hugoniot of liquid hydrogen fluoride Ree F.H., van�Thiel M. T Effective like- and<   unlike-pair interactions at high pressure and high temperature / One- and multi-component theories of mixtures Ree F.H., Choi Y. E Stability of the face-centered-cubic phase of heavy rare gas solids Ree F.H., Glosli J.N. J Modeling high pressure and high temperature phase changes in bulk carbon JReed R.P.,  Graham R.A.,  Moore L.M.,  Lee L.M.,  Fogelson D.J., Bauer F. , The Sandia standard for PVDF shock sensors Reed R.P., Greenwoll J.I. W Characteristics and pulsed radiation response of non-ideal quartz shock stress gauges  1711-1714 'Rajendran A.M.,  Grove D.J., Bar-On E. 3 Response of thin sheet due to debris cloud impact Rajendran A.M. . Modeling the shock response of AD995 alumina Rajendran A.M., Grove D.J. G Determination of Rajendran-Grove ceramic constitutive model constants Rajendran A.M., Walsh K.P. k Modeling of in-situ ballistic measurements using the Rajendran-Grove and Johnson-Holmquist ceramic models (Ramamurthy A.C.,  Bless S.J., Brar N.S. 5 Stresses in painted steel coupons from stone impact  1091-1094 ;Randles P.W.,  Libersky L.D.,  Carney T.C., Sandstrom F.W. 2 SPH simulation of fragmentation in the MK82 bomb Ranga�Rao M.P.  Spherical shocks in solids 	 681-685 Ranga�Rao M.P., Ramu A. * Study of shock propagation due to impact #Rao R.S.,  Godwal B.K., Sikka S.K. 3 On the primitive hexagonal and w phases of carbon Rasky D.J., McHenry M.R. A Construction of porous Hugoniots from solid material properties 3Ravelo R.,  Holian B.L.,  Germann T.C., Lomdahl P. ? Directional dependence in shock-induced melting of fcc metals 	 270-273 .Ravichandran G.,  Chang S.N., Nemat-Nasser S. < Elasto-plastic behavior of a partially stabilized zirconia 9Ravichandran G.,  Rosakis A.J.,  Hodowany J., Rosakis P. Q On the conversion of plastic work into heat during high strain rate deformation 	 557-562 Ravindran P., Asokamani R. Y Electronic structure and pressure induced superconductivity in Ge, Sn and Pb tellurides RRazorenov S.V.,  Bogatch A.A.,  Kanel G.I.,  Utkin A.V.,  Fortov V.E., Grady D.E. O Elastic-plastic deformation and spall fracture of metals at high temperatures PRazorenov S.V.,  Kanel G.I.,  Utkin A.V.,  Bogach A.A.,  Burkins M., Gooch W.A. c Dynamic strength and edge effects at spall fracture for titanium alloys of varying oxygen content 5Razorenov S.V.,  Kanel G.I.,  Baumung K., Bluhm H.J. ( The dynamic behavior of a filled glass 	 884-887 5Radousky H.B.,  Mitchell A.C.,  Nellis W.J., Ross M. + Shock temperature measurements in ammonia 	 467-472 Radousky H.B. ' Shock-induced cooling in dense fluids 3Rae P.J.,  Goldrein H.T.,  Palmer S.J.P., Proud W. * Moir� interferometry studies of PBX 9501 8Rae P.J.,  Gray�III G.T.,  Dattelbaum D.M., Bourne N.K. - The Taylor impact response of PTFE (Teflon) Rae P.J., Brown E.N. 5 The Taylor impact and large strain response of PEEK  1399-1302 wRaevsky V.A.,  Aprelkov O.N.,  Igonin V.V.,  Ignatova O.N.,  Knyazev V.N.,  Lebedev A.I.,  Sinitsyna S.N., Yukina N.A. K Heterogeneous deformation of copper in shock waves a subgrain scale level 	 761-764 Raftenberg M.N. E Tensile damage effects in steel plate perforation by a tungsten rod G Application of a brittle damage model to normal plate-on-plate impact 	 862-865 ARagan C.E.,  Diven B.C.,  Rich M.,  Robinson E.E., Teasdale W.A. 4 Shock compression measurements at pressures >1 TPa 	 169-173 Ragan C.E. & Nuclear-explosive-driven experiments 	 644-647 ARagan C.E.,  Diven B.C.,  Rich M.,  Teasdale W.A., Robinson E.E. ( Precise ultrahigh-pressure experiments 6Raghupathy R.,  Gazonas G.A.,  Molinari J.F., Zhou F. ] Numerical convergence of the cohesive element approach in dynamic fragmentation simulations 	 654-657 Raiser G., Clifton R.J. C Failure waves in uniaxial compression of an aluminosilicate glass Rajendran A.M., Bless S.J. X Use of the Bodner-Partom model viscoplastic constitutive model to describe HY100 steel 	 383-388 (Rajendran A.M.,  Grove D.J., Bless S.J. 2 A new yield function based dynamic failure model /Rajendran A.M.,  Dietenberger M.A., Grove D.J. ; Results from the recently developed dynamic failure model 'Rajendran A.M.,  Brar N.S., Khobaib M. E Effects of dynamic pre-strain on the subsequent tensile flow stress = The measurement of hot-spots in granulated ammonium nitrate $Proud W.G.,  Kirby I.J., Field J.E. C The nature, number and evolution of hot-spots in ammonium nitrate  1017-1020 #Proud W.G.,  Wang J., Cross D.L.A. F The effect of sample roughness and planarity on gauge response times  1203-1206 Pr�mmer R. 6 Explosive welding of tin, uranium and thorium copper 	 467-469 #Pruzan P.,  Chervin J.C., Canny B. l Determination of the ice VII-VIII transition line at high pressure and low temperature by Raman scattering 4Pruzan P.,  Chervin J.C.,  Canny B., Kuyumchev A.A. A Transformation of CS2 to a polymer at 10 GPa: An infrared study .Psakhie S.G.,  Korostelev S.Y., Vorobyov V.I. ^ Formation of nanocrystalline structure by shock wave propagation through amorphous materials 	 157-159 .Pyalling A.A.,  Ternovoi V.Y., Filimonov A.S. w Temperature measurements of single and double shock compressed liquid nitrogen in overtaking shock wave configuration /Qadri S.B.,  Skelton E.F.,  Webb A.W., Hu J.Z. ' Pressure induced polymorphism of ZnTe >Qadri S.B.,  Skelton E.F.,  Webb A.W.,  Hu J.Z., Furdyna J.K. 1 Pressure induced phase transition of Zn1-xCoxSe "Quidot M.,  Racimor P., Chabin P. 1 Constitutive models for PBX at high strain rate (Rabie R.L.,  Vorthman J.E., Dienes J.K. D Three-dimensional computer modeling of a shock recovery experiment Rabie R., Dick J.J. H Equation of state and crushing dynamics of low-density silica aerogels 0Radchenko A.V.,  Kobenko S.V., Krivosheina M.N. i Effect of oriented elastic and strength characteristics on the impact fracture of anisotropic materials &Radford D.D.,  Proud W.G., Field J.E. O The deviatoric response of three dense glasses under shock loading conditions )Radford D.D.,  Willmott G.R., Field J.E. C The effect of structure on failure front velocities in glass rods (Radford D.D.,  Tsembelis K., Proud W.G. ^ Time evolution of pressure fields generated in impact of cylindrical projectiles with plates  1805-1808 ,Prakash A.,  McCormick A.V., Zachariah M.R. 2 Thermo-kinetic study of sore-shell nanothermites  1006-1009 3Predebon W.W.,  O'Donoghue P.E., Anderson�Jr. C.E. M Gap closure and opening between preformed fragments during explosive launch /Predebon W.W.,  Anderson�Jr. C.E., Walker J.D. > Inclusion of equivalent plastic strain in Eulerian wavecodes Prentice J.K. M Methodology and applications of the HULL hydrocode Eulerian/Lagrangian link Prentice J.K., Kipp M.E. F Modeling of rate dependent brittle fracture in an Eulerian hydrocode 'Prentice J.K.,  Fikani M.K., Fuka M.Z. 4 TOLTEC: A multidimensional solid dynamics wavecode 7Prentice H.J.,  Grantham S.G.,  Proud W.G., Field J.E. N Three-dimensional penetration measurements using digital speckle photography Prentice H.J., Proud W.G. o Three-dimensional dynamic deformation measurements using stereoscopic imaging and digital speckle photography (Preston D.L.,  Tonks D.L., Wallace D.C. E The rate dependence of the saturation flow stress of Cu and 1100 Al bPrice R.H.,  Rosen M.D.,  Banner D.L.,  Holmes N.C.,  Kobierecki M.,  Zickuhr J.R., Ahlstrom H.G. N Time and space resolved measurements of the dynamics of laser fusion targets 	 155-163 &Prieto F.E.,  Loske A.M., Yarger F.L. S Study of pressure transducers and electrodes for underwater shock wave generators  1723-1726 Pritchard D.S. R Further investigation of stresses and strains in targets impacted by penetrators ( Shock waves in condensed matter - 1983 I Fuzzy logic applied to shaped charge jet penetration of glass composite %Proud W.G.,  Bourne N.K., Field J.E. 6 Shock-induced luminescence in polymethylmethacrylate Proud W.G., Field J.E. - Shock-induced reaction in hyd<  rogen peroxide Proud W.G. X Mesoscale probing of CRZ structure in PBX: DW oscillations from ignition up to failure  1002-1005 *Plohr J.N.,  Clements B.E., Addessio F.L. I Dynamically driven phase transformations in damaged composite materials 	 266-269 Plohr B.J., Plohr J.Y.N. F Simplified shock conditions for large-strain thermo-visco-plasticity Podlesak M. V Investigation of electrical shock conductivity in a polymer shock compression switch ,Podurets A.M.,  Barenboim A.I., Trunin R.F. S X-ray flash diffraction study of shock phase transitions in zirconium and bismuth 	 231-233 Poirier J.-P., Shankland T.J. 3 Dislocation theory of melting for iron, revisited Polishchuk A.Y., Fortov V.E. u New theoretical approach in calculation of laser beam and particle beam ranges in shock-compressed condensed matter 	 781-783 Polishchuk A.Y. P Kinetic and optical properties of condensed matter in ultra strong laser field  1895-1987 Pollock R. X Comments on 'Thermodynamic properties of nonideal strongly degenerate hydrogen plasma' 	 123-124 0Poole C.P.,  Farach H.A.,  Owens F.J., Pinto J. 7 Compression induced aligned radicals in nitroanilines 	 647-649 OPorowski S.,  Jun J.,  Krukowski S.,  Bockowski M.,  Tedenac J.C., Record M.C. O High pressure differential thermal analysis (DTA) and crystal growth of a-HgS LPorowski S.,  Lojkowski W.,  Molodov D.A.,  Shvindlerman L.S., Gottstein G. M Effect of high pressure on grain boundary migration in aluminium bicrystals [Postnov V.I.,  Nikolaev D.N.,  Ternovoi V.J.,  Filimonov A.S.,  Fortov V.E., Yakushev V.V. W The opportunity of the use of sapphire at multiple shock-wave compression of hydrogen ;Postnov V.I.,  Fortov V.E.,  Yakushev V.V., Yakusheva T.I. l Electrical conductivity investigation of graphite-diamond transition under multiple shock-wave compression Prakash A. 9 Deviatoric strength of silicon carbide subject to shock Pickup I.M., Bourne N.K. . The failure of aluminium nitride under shock *Pickup I.M.,  Millett J.C.F., Bourne N.K. N The shock behaviour of a SiO2-Li2O transparent glass-ceramic armour material Piekutowski A.J. ' Distribution of mass in debris clouds 	 953-956 .Pinheiro L.M.V.,  Calado A.R.T., Viana C.A.N. I Pressure effects on Menschutkin reactions in butan-1-ol and pentan-1-ol iPiza�a C.,  Murr L.E.,  Anchondo I.A.,  Pi�a C.Y.,  Baquera M.T.,  Tamoria T.L.,  Chen H.C., Cytron S.J. � DRX-induced solid-state flow and projectile-target mixing during [001] single-crystal tungsten rod penetration into steel targets  1395-1398 lPlaksin I.Y.,  Shutov V.I.,  Gerasimov V.M.,  Gerasimenko V.F.,  Morozov V.G.,  Karpenko I.I., Sokolov S.S. } Evolution of explosion in TATB HE in the process of its expansion into a free space followed by impact against hard barrier <Plaksin I.,  Campos J.,  Mendonca M.,  Mendes R., Gois J.C. 4 Interaction of double corner turning effect in PBX 9Plaksin I.,  Campos J.,  Mendes R.,  Ribeiro J., Gois J. G Mechanism of detonation wave propagation in PBX with energetic binder /Plaksin I.,  Campos J.,  Ribeiro J., Mendes R. * Detonation phenomena of PBX microsamples 	 918-921 `Plaksin I.,  Campos J.,  Ribeiro J.,  Mendes R.,  G�is J.,  Portugal A.,  Sim�es P., Pedroso L. 5 Detonation meso-scale tests for energetic materials 	 922-925 `Plaksin I.,  Campos J.,  Direito J.,  Mendes R.,  Sim�es P.,  Portugal A.,  Ribeiro J., G�is J. R Coarse explosive particles of PBX as a dominant factor of detonation instability UPlaksin I.,  Campos J.,  Mendes R.,  Ribeiro J.,  Direito J.,  Braga D., Coffey C.S. 3 Effect of shear stress in shock initiation of PBX WPlaksin I.,  Direito J.,  Coffey C.S.,  Campos J.,  Ribeiro J.,  Mendes R., Kennedy J. > Detonation propagation in shock-compressed liquid explosives Petel O.E., Higgins A.J. G Comparison of failure thickness and critical diameter of nitromethane 	 994-997 5Petel O.E.,  Higgins A.J.,  Yoshinaka A.C., Zhang F. N Effect of shock precompression on the critical diameter of liquid explosives 
 998-1001 FPeterson P.D.,  Mang J.T.,  Fletcher M.A.,  Olinger B.W., Roemer E.L. D Influence of pressing parameters on the microstructure of PBX 9501 	 796-799 Petit J., Hereil P.L. 2 Characterization of recovered shocked Armco iron ,Petit J.,  Kazeev M.,  Levit P., Tolstov Y. U Electromagnetic cylindrical compression test under large strain at high strain rate (Petrovic J.J.,  Olinger B.W., Roof R.B. ? Behavior of Si3N4 powder subjected to explosive shock loading Petrovsky V.P., Ostrik A.V. j Experimental methods of investigating composite structures strength against unstationary loading effects 1Petrovtsev A.V.,  Bychenkov V.A., Kovalenko G.V. u Numerical simulation of elastic-viscous-plastic properties: Polymorphous transformations and spall fracture in iron 	 591-594 .Petrovtsev A.V.,  Zhugin Y.N., Kovalenko G.V. H Modeling polymorphic transformations of quartzite in dynamic processes ZPetrovtsev A.V.,  Dremov V.V.,  Vildanov V.G.,  Gorshkov M.M.,  Zahikin V.T., Zhugin Y.N. / Equation of state and phase diagram of quartz .Peyronneau J.,  Poirier J.-P., Shankland T.J. a Electrical conductivity of perovskite-magnesiow�stite as a function of pressure and temperature  1465-1468 Phillips L., Oran E.S. H Molecular dynamics simulations of shocks in imperfect crystal lattices Phillips L. B Shock compression of a 2D model of DT embedded in a plastic foam EPhillips D.S.,  Schwarz R.B.,  Skidmore C.B.,  Hiskey M.A., Son S.F. , Some observations on the structure of TATB Pickup I.M., Barker A.K. $ Damage kinetics in silicon carbide 	 513-516 G Structural changes in ammonium perchlorate under compression to 5 GPa ;Peiris S.M.,  Pangilinan G.I.,  Zerilli F.J., Russell T.P. ^ Structural studies and EOS of diaminodinitroethylene (DADNE, FOX-7) under static compression *Pelak R.A.,  Rightley P., Hammerberg J.E. + Friction in high-speed impact experiments 4 Erratum: Friction in high-speed impact experiments P�nicaud M. - A theoretical equation of state for uranium >Peralta P.,  Swift D.,  Loomis E.,  Lim C.-H., McClellan K.J. K Characterization of laser-driven shocked NiAl monocrystals and bicrystals 	 601-604 Pereira C.M., Chaudhri M.M. P Optical and Raman studies of explosives under varying pressure and temperature 1Perevalova V.P.,  Kaminskii P.P., Kuznetsov V.M. I Equation of state (EOS) and bulk modulus under pressure of noble metals Perez M., Costeraste J. B Infrared method for postshock temperature measurements of solids 	Perez M. V The 'MIVAR': A ramp-wave generator material fabricated by the plasma spray technique [ Residual temperature measurements of shocked copper and iron plates by infrared pyrometry -Perger W.F.,  Zhao J.,  Blanco M., Pandey R. b First-principles intermolecular binding energies in molecular crystals with optimized basis sets /Perger W.F.,  Zhao J.,  Winey J.M., Gupta Y.M. z First-principles studies of PETN single crystal unit cell volumes and vibrational frequencies under hydrostatic pressure Perry F.C. G Investigations of hydrodynamic stability using electron and ion beams 	 639-643 G Dynamic heterogeneous response of aluminum and copper to stress waves Perry F.C., Noack D.D. G Heterogeneous response of aluminum and lithium niobate to shock waves 	 655-660 &Persson P.A.,  Ward R., Thadhani N.N. H Shock induced reaction synthesis (SRS) assisted compaction of ceramics BPetel O.E.,  Tanguay V.,  Higgins A.J.,  Yoshinaka A.C., Zhang F. > Calibration of DSD parameters for LX-07 from rate-stick data - Failure diameter of confined explosive rods 	 829-832 +Partom Y.,  Anderson�Jr. C.E., Orphal D.L. I Further investigation of the target resistance penetration parameter Rt  1129-1132 H Hydro-reactive computations with a temperature dependent reaction rate 	 460-463 # Long-rod moving-plate interaction  More on D(k) for PBX-9502 SPartouche-Sebban D.,  P�lissier J.-L.,  Anderson W.W.,  Hixson R.S., Holtkamp D.B. I Characterization of sapphire for <  optical pyrometry in shock experiments  1289-1292 Partouche-Sebban D. T High-speed multi-wavelength pyrometry and emissivity measurement of shocked metals  1293-1298 
Passman S.L. ' Models for penetration of thin plates APasternak M.P.,  Hearne G.,  Sterer E.,  Taylor R.D., Jeanloz R. a High pressure metallization of Mott insulators: Magnetic, structural, and electronic properties 
Pastine D.J. - Radio emissions from unequilibrated sources 	 861-864 GPatel D.,  Temkin H.,  Menoni C.S.,  Logan R.A.,  Coblentz D., Tome C. f Enhanced characteristics of InGaAsP buried quaternary lasers with pressure in the diamond anvil cell Patel M.V., Streitz F.H. G Simulations of rapid pressure-induced solidification in molten metals 	 298-301 &Patterson J.,  Lagutchev A., Dlott D. = Shock compression of molecules with 1.5 Angstrom resolution $Paul W.,  Burnett J.H., Cheong H.M. 2 Role of high pressures in semiconductor research CPauler D.K.,  Kress J.D.,  Lightfoot J.M.,  Woods L., Russell B.G. H Decomposition of nitroplasticizer in plastic bonded explosive PBX 9501 OPavlovskii A.I.,  Tatsenko O.M.,  Platonov V.V.,  Volkov A.A., Markevtsev I.M. J Investigation of ruby luminescence R-line by isentropic megabar pressure ,Peiris S.M.,  Pangilinan G.I., Russell T.P. A The laser-induced decomposition of TATB at static high pressure 6 Adhesion studies between HMX and EDC37 binder system jPalmour�III H.,  Kim K.Y.,  Batchelor A.D.,  Hare T.M.,  Goudey G.T.,  More K.L.,  Linse V.D., Adair J.H. R Influence of dynamic pressure on sinterability of shock-consolidated TiC powders Pangilinan G.I., Russell T.P. d Real-time changes induced by pulsed laser heating in ammonium perchlorate at static high pressures 0Panov V.,  Vignjevic R.,  Bourne N., Millett J. ; Material failure modelling in metals at high strain rates 	 646-649 Pappu S., Murr L.E. G Microstructural and computer simulation studies on some EFP materials 7Paris V.E.,  Zaretsky E.B.,  Kanel G.I., Savinykh A.S. V Diagnostics of ductility, failure and compaction of ceramics under shock compression 	 747-750 Paris V.E., Zaretsky E.B. S Study of compressive failure of alumina in impact experiments with divergent flow 	 880-883 'Parkash V.,  Freund L.B., Clifton R.J. ' Plane strain fracture in plate impact +Parker L.J.,  Ladouceur H.D., Russell T.P. R Teflon and Teflon/Al (nanocrystalline) decomposition chemistry at high pressures EParker G.R.,  Asay B.W.,  Dickson P.M.,  Henson B.F., Smilowitz L.B. : Effect of thermal damage on the permeability of PBX 9501 RParker G.R.,  Dickson P.M.,  Asay B.W.,  Smilowitz L.B.,  Henson B.F., Perry W.L. V Understanding the mechanisms leading to gas permeation in thermally damaged PBX 9501 #Partom Y.,  Yaziv D., Rosenberg Z. 9 Shock release of 2024-T351 aluminum in the 10 GPa range 	 387-391 Partom Y., Rosenberg Z. % More on the precursor decay anomaly 
Partom Y. = Modeling the crossover in reaction rate for micronized TATB B Understanding the Swegle-Grady (strain rate goes as s4) relation 	 317-319 Partom Y., Yaziv D. J Penetration of L/D=10 and 20 tungsten alloy projectiles into RHA targets  1801-1804 0 Accounting for the penetration entrance effect Y Shock induced sub-detonation chemical reactions in 1,3,5-triamino-2,4,6-trinitrobenzene Ovidko I.A. T On dislocation ensemble evolution in fcc metals under high strain rate deformation 	 461-463 : On new mechanism for plastic flow in shock loaded solids Owens F.J. m Electron paramagnetic resonance study of shock-induced reactions of some small molecules in the solid state Owens F.J., Politzer P. o Molecular orbital calculation of indices of impact and shock induced reactivity in trinitroaromatic molecules 	 857-861 H Effect of shock and hydrostatic pressure on H bonding in water and ice Owens F.J., Iqbal Z. t Microwave absorption measurement of flux trapping in shocked processed high temperature superconductor YBa2Cu3O7-y 	 599-601 %Owens F.J.,  Iqbal Z., Thadhani N.N. _ Magnetic field dependent microwave absorption in the shocked 85K superconductor Bi-Sr-Ca-Cu-O 9Oxby T.,  Perger W.F.,  Zhao J.,  Winey J.M., Gupta Y.M. E Calculating elastic constants of molecular crystals using CRYSTAL98 5Pahl R.J.,  Trott W.M.,  Snedigar S., Caste�eda J.N. c Evaluation of aluminum participation in the development of reactive waves in shokc compressed HMX 	 990-993 
Paisley D.L. R Laser-driven miniature flyer plates for shock initiation of secondary explosives &Paisley D.L.,  Warnes R.H., Kopp R.A. | Laser-driven flat plate impacts to 100 GPa with sub-nanosecond pulse duration and resolution for material property studies 	 825-828 BPaisley D.L.,  Swift D.C.,  Johnson R.P.,  Kopp R.A., Kyrala G.A. ` Laser-launched flyer plates and direct laser shocks for dynamic material property measurements "Pak H.-R.,  Horie Y., Graham R.A. Q Synthesis of nickel-aluminum alloys by shock compression of composite particles 	 761-766 *Palanivel B.,  Kalpana G., Rajagopalan M. / Physical properties of thorium under pressure ,Palmer S.J.P.,  Williamson D.M., Proud W.G. Z Two-variable feature of Gr�neisen function observed in experimental porous Hugoniot data ,Oh K.-H.,  Yang Y.-J.,  Kim H.-J., Kim H.W. 2 A simple model for multiple shock Hugoniot state  Oh K.-H.,  Kim H.-J., Lee H.-W. 6 Behavior of Gr�neisen g in the multiple shock region DOhno I.,  Hanayama Y.,  Kimura M.,  Suzuki I.,  Oda H., Kumazawa M. N Pressure derivatives of elastic constants of iron by cavity resonance method <Oinuma S.,  Tanaka K.,  Iida M.,  Nakayama Y., Matsunaga T. - Diamonds recovered from detonation products 3Oleynik I.I.,  Zybin S.V.,  Elert M.L., White C.T. I Nanoscale molecular dynamics simulation of shock compression of silicon 4 Shear stresses in shock-compressed covalent solids `Oleynik I.I.,  Conroy M.,  Zybin S.V.,  Zhang L.,  van�Duin A.C.,  Goddard�III W.A., White C.T. v Energetic materials at high compression: First-principles density functional theory and reactive force field studies Olson M.A., Kimsey K.D. K Calculation of elastic-plastic wave propagation on the Connection Machine *Orphal D.L.,  Kozhushko A.A., Sinani A.B. ` Possible detection of failure wave velocity in SiC using hypervelocity penetration experiments -Orphal D.L.,  Walker J.D., Anderson�Jr. C.E. 6 Ballistic response of fabrics: Model and experiments Orphal D.L., Anderson�Jr. C.E. J Crater diameter for L/D=1 like-material impacts on semi-infinite targets  1347-1350 HOrphal D.L.,  Behner T.,  Hohler V.,  Anderson�Jr. C.E., Templeton D.W. ; Failure wave in DEDF and sodalime glass during rod impact  1391-1394 OOsher J.E.,  Chau H.H.,  Gathers G.R.,  Lee R.S.,  Pomykal G.W., Weingart R.C. r Shock-wave studies using plastic flyers driven by an electric gun for hypervelocity impact on selected materials 5Osher J.E.,  Chau H.H.,  Gathers G.R., Weingart R.C. S Characteristics of flyer impact for one-dimensional shock-wave study applications �stmark H. ANiska H.M.,  Charron A.E.,  Schulz T.J.,  Perger W.F., Kunz A.B. ? Dynamic simulation of a crystal lattice under impulse loading 'Norwood F.R.,  Graham R.A., Sawaoka A. L Numerical simulation of a sample recovery fixture for high velocity impact 	 837-842 Novikov S.A., Pushkov V.A. V Study of steel crack resistance under dynamic loading and temperature range 20-300�C ;Novikov S.A.,  Pushkov V.A.,  Sinitsyn V.A., Gray�III G.T. W Crack resistance of aluminium composite under shock loading at different temperatures 	 455-457 Nunziato J.W. : Initiation and growth-to-detonation in reactive mixtures 	 581-588 Nutt G.L., Hallquist J.O. & Calibration of piezoresistive gauges Nutt G.L., Erickson L.M. - Reactive flow Lagrange analysis in RX-26-AF AO'Donoghue P.E.,  Anderson�Jr. C.E.,  Renick J.D., O'Kelley D.K. U Flyer plate impact of dry soils: A comparison of analytic and numerical predictions BO'Donoghu<  e P.E.,  Friesenhahn G.J.,  Anderson�Jr. C.E., Parr C.H. L Anisotropic model development for shock wave propagation computer programs �Obst A.W.,  Alrick K.R.,  Anderson W.W.,  Boboridis K.,  Buttler W.T.,  Lamoreaux S.K.,  Marshall B.R.,  Montgomery S.L.,  Payton J.R., Wilke M.D. : Ellipsometry in the study of dynamic material properties Ogilvie K., Duvall G.E. 8 Time resolved spectroscopy of shock compressed liquids 	 292-295 Ogorodnikov V.A., Ivanov A.G. 7 On the nature of scale effect in high-rate fracturing 4Ogura T.,  Nakamura K.G.,  Takenaka H., Kondo K.-I. F Shock temperature of NaCl measured with wide-band optical radiometry  1215-1218 Oh K.-H., Persson P.-A. < Full range Hugoniot equation of state for porous materials 	Oh K.-H. K Graphical construction of P-Up porous Hugoniots from solid Hugoniot curve S Comparison of high energy shock states for reactant material and product material 0Oh K.-H.,  Jhung K.S.,  Kim I.H., Persson P.-A. G K-shell photoabsorption edge spectroscopy in shock compressed plasmas   Shock waves and plasma physics  53-58 Nguyen J.H., Holmes N.C. 1 Iron sound velocities in shock wave experiments 1 Shock induced birefringence in lithium fluoride HNguyen J.H.,  Orlikowski D.,  Streitz F.H.,  Holmes N.C., Moriarty J.A. V Specifically prescribed dynamic thermodynamic paths and resolidification experiments  1225-1230 Nichols�III A.L. ` Coupled thermal/chemical/mechanical modeling of insensitive explosives in thermal environments 3 Nonequilibrium detonation of composite explosives -Nichols�III A.L.,  Tarver C.M., McGuire E.M. 4 ALE3D statistical hot spot model results for LX-17 5 Statistical hot spot model for explosive detonation 	 465-470 Nicholson D.W. 4 Shock induced temperature rise in a titanium plate %Nicol M.,  Johnson S.W., Holmes N.C. O Shock-chemistry of benzene studied by spectra from and behind the shock front 	 471-476 Nikkel�Jr. D.J., Lassila D.H. V The effect of the constitutive response on the predicted temperatures in copper jets  1857-1860 MNikolaev D.N.,  Filimonov A.S.,  Fortov V.E.,  Lomonosov I.V., Ternovoi V.Y. 5 Mechanical properties of preshocked sapphire driver JNikolaev D.N.,  Fortov V.E.,  Filimonov A.S.,  Kvitov S.V., Ternovoi V.Y. B SiO2-aerogel plasma properties in the energy range up to 65 kJ/g -Nikolaev D.N.,  Ternovoi V.Y., Pyalling A.A. M Nickel critical point parameters from shock experiments with porous samples  59-62 >Nikolaev D.N.,  Emelyanov A.A.,  Pyalling A.A., Ternovoi V.Y. h Study of near-critical point thermodynamics of molybdenum by isentropic expansion and isobaric heating pNiles A.M.,  Garcia F.,  Greenwood D.W.,  Forbes J.W.,  Tarver C.M.,  Chidester S.K.,  Garza R.G., Switzer L.L. ] Measurement of low level explosive reaction in gauged multi-dimensional Steven impact tests 	 886-889 V Incubation time and growth pattern of martensite under a short duration stress pulse 	 181-184 Nemes J.A., Eftis J. N Use of viscoplastic constitutive theory for simulating spallation thresholds ^Nemtchinov I.V.,  Shulov V.V.,  Artemieva N.A.,  Ivanov B.A.,  Kosarev I.B., Trubetskaya I.A. 2 Light flashes caused by impacts against the Moon 	 957-960 Nesterenko V.F. b The modifications of superconducting properties of Y-Ba-Cu-O and Bi-Sr-Ca-Cu-O using shock waves +Nesterenko V.F.,  Bondar M.P., Ershov I.V. 6 Instability of plastic flow at dynamic pore collapse 9Nesterenko V.F.,  Meyers M.A.,  Chen H.C., LaSalvia J.C. ? Chemical reactions in controlled high-strain-rate shear bands P Controlled high rate strain shear bands in inert and reactant porous materials 	 609-614 ? Solitons, shock waves in strongly nonlinear particulate media 5Nesterenko V.F.,  Indrakanti S.S.,  Brar S., Gu Y.B. I Long rod penetration test of hot isostatically pressed Ti-based targets 2Nesterenko V.,  Maple M.B.,  Taylor B.J., Gu Y.B. ] Modification of magnesium diboride properties using shock loading and hot isotatic pressing  1114-1117 INeumeier J.J.,  Nellis W.J.,  Maple M.B.,  Torikachvili M.S., Sales B.C. I Superconductivity of A15-phase Nb3Si synthesized by Mbar shock pressure Neuwald P. 8 Explosively driven combustion of shock-dispersed fuels 	 976-981 (Newlander C.D.,  Stone S.F., Burns J.B. S Measurement and analysis of pulsed laser generated stress waves in epoxy and PMMA 8Newlander C.D.,  Cherest J.A.,  Lilly M.C., Eisler R.D. ! Wave propagation in polymers. 2 .Ng A.,  Pareniuk D.,  Celliers P., DaSilva L. 5 Reflectivity measurements on shock-unloading solids Ng A. : Recent experiments in laser-driven shock waves in solids eNg A.,  da�Silva L.,  Godwal B.K.,  Chiu G.,  Cottet F.,  Richardson M.C.,  Jaanimagi P.A., Lee Y.T. C Plastic deformation rate and initiation of crystalline explosives !Narayanan V.,  Lu X., Hanagud S. D Shock-induced chemical reactions in structural energetic materials �Nazarov D.V.,  Mikhaylov A.L.,  Fedorov A.V.,  Manachkin S.F.,  Urlin V.D.,  Menshikh A.V.,  Finyushin S.A.,  Davydov V.A., Filinov E.V. _ Characterization of optically transparent window materials for isentropic compression studies /Negreskul S.I.,  Psakhie S.G., Korostelev S.Y. R The simulation of explosive compaction of powders by the element dynamics method /Nellis W.J.,  Ross M.,  van�Thiel M., Brown N. 8 The shock compression of liquid H2 to 10 GPa (100kbar) 	 223-225 Nellis W.J. 3 Shocked fluids at high densities and temperatures  31-40 SNellis W.J.,  Moss W.C.,  Radousky H.B.,  Mitchell A.C.,  Maple M.B., McElfresh M. @ Properties of niobium recovered from megabar dynamic pressures 	 719-724  Nitrogen at high pressure  43-49 'Nellis W.J.,  Gourdin W.H., Maple M.B. 0 Shock-induced melting and rapid solidification ]Nellis W.J.,  Koch R.,  Davidson H.,  Hunter J.W.,  Brocius W.F.,  Marshall A., Geballe T.H. ? Micron thin niobium films recovered from Mbar shock pressures HNellis W.J.,  Mitchell A.C.,  Erskine D.J.,  McCandless P.C., Weir S.T. L Energy gap of molecular hydrogen from electrical conductivity measurements 	 111-112 ^ Fluids at high shock pressures and temperatures and some thoughts about future possibilities PNellis W.J.,  Weir S.T.,  Hinsey N.A.,  Balachandran U.,  Kramer M.J., Raman R. 0 Disks of YBa2Cu3O7 shocked to 10 GPa pressures Nellis W.J., Mitchell A.C. 8 Molecular and planetary fluids at high shock pressures  13-19 J Sensitivity and accuracy of Hugoniot measurements at ultrahigh pressures Nelmes R.J., McMahon M.I. ; Powder diffraction studies of structures at high pressure 4Nemat-Nasser S.,  Sano Y.,  Chang S.N., Meyers M.A. 3 Initiation of PETN powder by pulse laser ablation 	 995-998 4Nagayama K.,  Ebisuzaki H.,  Kubota S., Nakahara M. ( Pulse laser ignition of preheated PETN  1005-1008 /Nagayama K.,  Mori Y.,  Motegi Y., Nakahara M. C Shock Hugoniot compression data for several bio-related materials  1547-1550 Nahme H.,  Hohler V., Stilp A. F Elastic plastic behavior of shock-loaded Fe-SiO2 composite materials R Determination of the dynamic material properties of shock loaded silicon-nitride 	 765-768 Nahme H.,  Hiltl M., Arnold W. j Dynamic properties and microstructural response to shock loading of Armco iron at different temperatures  Nahme H.,  Stilp A.J., Weber K. I Shock wave reflection behavior in double-layer meteoroid bumper systems 	 941-944 Nahme H., Lach E. p Determination of the mechanical behavior of nitrogen alloyed steel (P900) at strain rates 10-3<de/dt<2*106 s-1 	Nahme H. A Spall plane formation near spall threshold for different metals 
Naimark O.B. d Mesodefects collective properties and self-similar regularity of shocked condensed matter behavior Nakamura A., Mashimo T. ' Shock-induced phase transition of AlN (Nakamura Y.,  Fujishiro I., Kawakami H. f Estimation of refractive index and density of lubricants under high pressure by Brillouin scattering ,Nakamura K.G.,  Wakabayashi K., Kondo K.-I. ~ Transient bond scission of PTFE under laser-induced shock compression <  studied by nanosecond time-resolved Raman spectroscopy %Nakamura K.G.,  Matsuda A., Kondo K. x Liquid-solid phase transition of benzene under shock compression studied by time-resolved nonlinear Raman spectroscopy $Nakano S.,  Fujioka H., Fukunaga O. 0 High pressure synthesis of cubic boron nitride Namjoshi S.A., Thadhani N.N. H Reaction synthesis of shock densified titanium-silicon powder mixtures Namkung J., Coffey C.S. OMurphy M.J.,  Simpson R.L.,  Urtiew P.A.,  Souers P.C.,  Garcia F., Garza R.G. Z Reactive flow model development for PBXW-126 using modern nonlinear optimization methods 	 417-420 
Murr L.E. w Examination of microstructural development by shock waves in condensed matter: Theoretical and practical consequences ;Murr L.E.,  Pradhan-Advani M.,  Niou C.S., Schoenlein L.H. | Correlating critical process parameters and microstructures in explosively fabricated ceramic/metal matrix superconductors (Murray N.H.,  Bourne N.K., Rosenberg Z. % Precursor decay in several aluminas 5Murray N.H.,  Bourne N.K.,  Field J.E., Rosenberg Z. ) Symmetrical Taylor impact of glass bars 8Murray N.H.,  Millett J.C.F.,  Proud W.G., Rosenberg Z. D Issues surrounding lateral stress measurements in alumina ceramics $Murri W.J.,  Curran D.R., Seaman L. + Fracture model for high energy propellant 	 460-464 Murri W.J. B Shock wave facilities at Poulter Laboratory of SRI International 	 652-656 /Myers S.A.,  Koch C.C.,  Horie Y., Graham R.A. 7 TEM of nickel aluminides produced by shock compaction 	 755-759 �Nagao H.,  Nakamura K.G.,  Kondo K.,  Ozaki N.,  Ono T.,  Takamatsu K.,  Tanaka K.A.,  Nagai K.,  Nakai M.,  Wakabayashi K.,  Okada K., Yoshida M. B Equation of state of diamond under shock compression up to 2 TPa Nagayama K. f Universal description of solids at high pressures and temperatures based on the Gr�neisen assumption j Statistical mechanical interpretation of new thermal variables of Gr�neisen equation of state for solids � Simple method of calculating Gr�neisen parameter and cold potential energy function for solids based on the Slater, D-M, and free volume theories Nagayama K., Mori Y. < Anomaly in the temperature calculation of shocked polymers 0Nagayama K.,  Mori Y.,  Shimada K., Nakahara M. 8 Water shock Hugoniot measurement up to less than 1 GPa #Nagayama K.,  Inou K., Nakahara M. D A method to estimate the yield of an underground nuclear explosion 2Moss W.C.,  Mitchell A.C.,  Heinle R., Fritz J.N. l Particle velocity measurements near underground nuclear explosions using axially symmetric magnetic gauges 1Moss W.C.,  Clarke D.B.,  White J.W., Young D.A. ? Sonoluminescence, shock waves, and micro-thermonuclear fusion 	 453-458 Moulard H., Bauer F. . Lagrangian analysis of the PVDF shock sensor %Mowrey R.C.,  Elert M.L., White C.T. < Quantum dynamics of energy transfer under shock conditions /Mukundan T.,  Constantinou C.P., Chaudhri M.M. q Mass spectrometric and spectroscopic investigations of the chemical sensitization of nitrocompounds by an amine *Mulder A.,  Michels J.P.J., Schouten J.A. K Monte Carlo calculations on the orientational behaviour of solid nitrogen &Mulford R.N.,  Dick J.J., Pettit D.R. L Shock initiation of PETN crystals: Optical absorption and emission studies *Mulford R.N.,  Sheffield S.A., Alcon R.R. , Preshock desensitization of PBX explosives  1405-1408 Mulford R.N., Alcon R.R. 7 Shock initiation of PBX-9502 at elevated temperatures Mulford R.N., Romero J.A. J Sensitivity of the TATB-based explosive PBX-9502 after thermal expansion Mulford R.N., Swift D.C. @ Reactive flow models for the desensitization of high explosive 	 895-898 A Mesoscale modelling of shock initiation in HMX-based explosives Mulford R., Swift D. Q Reactive flow in nitromethane using a quasiharmonic unreacted equation of state 1 Modelling temperatures of reacting nitromethane CMullin S.A.,  Littlefield D.L.,  Chhabildas L.C., Piekutowski A.J. g Computational simulations of experimental impact data obtained at 7 to 11 km/s with aluminum and zinc  1817-1820 -Murata K.,  Takahashi K.,  Kato Y., Murai K. U Development of pressure gauge using PVDF copolymer for underwater shock measurement I Monoclinic to tetragonal conversion of zirconia under shock compression )Morosin B.,  Venturini E.L., Graham R.A. = X-ray diffraction studies of shock-synthesised zinc ferrite 	 797-801 GMorosin B.,  Graham R.A.,  Venturini E.L.,  Carr M.J., Williamson D.L. 5 Shock-induced chemical synthesis of barium ferrites HMorosin B.,  Graham R.A.,  Venturini E.L.,  Ginley D.S., Hammetter W.F. b Shock-induced chemical synthesis of phases similar to the high temperature superconductor oxides 'Morosin B.,  Graham R.A., Pollack S.S. < X-ray diffraction line broadening in shock modified Pyrite SMorosin B.,  Venturini E.L.,  Holman G.T.,  Newcomer P.N.,  Dunn R.G., Graham R.A.  Shock-induced defects in HgO &Morris C.E.,  Fritz J.N., Holian B.L. 9 Quasi-elastic high-pressure waves in 2024 Al and copper 	 382-386 Morris C.E.   Shock Wave Physics Group (M-6) 	 616-620 'Morris C.E.,  McQueen R.G., Marsh S.P. 5 Mach disc formation in cylindrical recovery systems *Morris C.E.,  Winkler M.A., Mitchell A.C. B Ti-6%Al-4%V alloy wave profile measurements in the shadow region HMorris C.E.,  Loughran E.D.,  Mortensen G.F.,  Gray�III G.T., Shaw M.S. , Shock induced dissociation of polyethylene 3Morris J.P.,  Glenn L.A.,  Antoun T.H., Lomov I.N. w Numerical investigation into the performance of a rarefaction shock wave cutter for offshore oil-gas platform removal 3Morris J.P.,  Glenn L.A.,  Heuze F.E., Bonner M.P. f Simulations of underground structures subjected to dynamic loading using the distinct element method  1470-1473 +Moss G.L.,  Netherwood�Jr. P.H., Seaman L. S Nucleation threshold stresses for the dynamic fracture of a low-alloy Ni-Cr steel 	 446-450 Moss W.C., Glenn L.A. E A Bauschinger effect model suitable for use in large computer codes 
Moss W.C. 7 Using the Hugoniot to approximate the release adiabat 	 157-162 0Morgado J.,  Dur�es L.,  Campos J., Portugal A. , Iron oxide/aluminum fast thermite reaction Mori Y., Nagayama K. � Sensitive detection of shock front and free surface velocity history for polymeric materials by new inclined-prism method in 1 GPa pressure region Z Measurement of the slope of shock velocity-particle velocity Hugoniot curve for polymers P Anomalous shock properties of polymeric materials around 0.5 GPa stress region � Evolution of stress relaxation structures for several polymers subjected to plane shock compression around 0.5 GPa shock stress measured by PVDF gauge l Nonlinearity of polyethylene Hugoniot up to 1 GPa and its interpretation by Gr�neisen parameter estimation -Mori A.,  Tamaru K.,  Hokamoto K., Fujita M. C Underwater explosive welding: Discussion based on weldable window M�ri N. 8 Electrical and magnetic properties of Ce monopnictides  1477-1480 Moriarty J.A. V High-pressure ion-thermal properties of metals from ab initio interatomic potentials 	 101-106 d First-principles equations of state for aluminum, copper, and lead in the pressure range 1-10 Mbar @ First-principles pressure-temperature phase diagrams in metals �Moriarty J.A.,  Benedict L.X.,  Glosli J.N.,  Hood R.Q.,  Orlikowski D.A.,  Patel M.V.,  S�derlind P.,  Streitz F.H.,  Tang M., Yang L.H. 9 Quantum-based atomistic simulation of transition metals 	 403-408 3Moritoh T.,  Kawai N.,  Nakamura K.G., Kondo K.-I. P Projectile acceleration aiming at velocities above 9 km/s by a compact gas gun  1204-1207 Morosin B., Graham R.A. # Shock-induced inorganic chemistry  4-13 s Crystallographic properties of lithium niobate shock-loaded from 3.7 to 20 GPa and preserved for post-shock study 	 330-334 J X-ray diffraction line broadening studies on shock-loaded TiO2 and Al2O3 	 355-362 'Morosin B.,  Graham R.A., Hellman J.R. i Temporal profiles of explosively-generated pressures in solids measured by an optical f<  iber-based gauge  1199-1202 Montgomery S.T. p Analysis of transitions between ferroelectric and antiferroelectric states under conditions of uniaxial strain 	 179-184 -Montgomery S.T.,  Graham R.A., Anderson M.U. W Return to the shorted and shunted quartz gauge problem: Analysis with the SUBWAY code  1025-1028 HMontgomery S.T.,  Brannon R.M.,  Robbins J.,  Setchell R.E., Zeuch D.H. ~ Simulation of the effects of shock stress and electrical field strength on shock-induced depoling of normally poled PZT 95/5 CMoore D.S.,  Schmidt S.C.,  Shaner J.W.,  Shampine D.L., Holt W.T. ^ Coherent anti-Stokes Raman scattering in benzene and nitromethane shock-compressed to 11 GPa 	 207-211 Moore D.S., Schmidt S.C. C Experimental molecular spectroscopy in shock-compressed materials  35-42 Moore L.M., Graham R.A. k Response of standardized PVDF piezoelectric polymer gauges to direct shock pressures between 8 and 32 GPa 4Moore D.S.,  Schmidt S.C.,  Shaw M.S., Johnson J.D. 8 Vibrational spectroscopy of shock-compressed liquid CO �Moore D.S.,  Gahagan K.T.,  Buelow S.J.,  Rabie R.L.,  Funk D.J.,  Sheffield S.A.,  Davis L.L.,  Lippert T.,  Brand H., Nicholson J.W. X Time- and space-resolved optical probing of the shock rise time in thin aluminum films  1003-1006 [Moore D.S.,  Funk D.J.,  Gahagan K.T.,  Reho J.H.,  Fisher G.L.,  McGrane S.D., Rabie R.L. F Sub-picosecond laser-driven shocks in metals and energetic materials  1333-1338 %Moore D.S.,  McGrane S.D., Funk D.J. S Ultrafast spectroscopic investigation of shock compressed energetic polymer films  1285-1288 Moran B., Goldwire�Jr. H.C. X Effect of source modelling on the inferred yield from an underground nuclear explosion 	 645-647 Morano E.O., Shepherd J.E. ? Effect of reaction rate periodicity on detonation propagation 	 446-449 	 184-187 *Mitchell A.C.,  Nellis W.J., Trainor R.J. D The Lawrence Livermore National Laboratory two-stage light gas-gun 	 613-615 Mitchell A.C.,  Nellis W.J.,  Holmes N.C.,  Ross M.,  Repp G.W.,  Heinle R.A.,  Valk T.C.,  Rego J.,  Graham W.B., Olness R.J. ` Shock impedance match experiments in aluminum and molybdenum between 0.1   2.5 TPa (1-25 Mbar) hMitchell A.C.,  Nellis W.J.,  Holmes N.C.,  Erskine D.J.,  McCandless P.C.,  Ravizza D.L., Cassidy L.D. L Equation of state data of shock compressed liquid CO2 and synthetic Uranus AMochalov M.A.,  Glukhodedov V.D.,  Kirshanov S.I., Lebedeva T.S. k Electric conductivity of liquid argon, krypton and xenon under shock compression up to pressure of 90 GPa %Mock�Jr. W.,  Holt W.H., Kerley G.I. # Shock and recovery of PTFE powder Mock�Jr. W., Holt W.H. @ Impact initiation of rods of pressed PTFE and aluminum powders 2Molinar G.F.,  Ehrlich C.,  Houck J., Cresto P.C. G Elastic distortions of a multi-mode piston-cylinder unit up to 28 MPa  1589-1592 'Molinari V.G.,  Mostacci D., Sumini M. ^ Particle density and temperature distribution in the early stage of laser-plasma interaction Molinari V.G., Teodori F. ? Energy propagation from a spherically symmetric particle flow Molinari V., Teodori F. r Analysis of the slowing of a high energy proton shot through a target in the frame of the Fokker-Planck equation &Molinari V.,  Mostacci D., Teodori F. � Analysis of the slowing down of high energy proton shots through matter via a Monte Carlo simulation of the Fokker Planck equation  1466-1469 ,Molodets A.M.,  Molodets M.A., Nabatov S.S. . Free energy and shock compression of diamond *Monat J.E.,  Carney J.R., Pangilinan G.I. C Novel optical fiber-based gauge for measuring transient pressures  1281-1284 9Monat J.E.,  Carney J.R.,  Whitley V.H., Pangilinan G.I. HMilman Y.V.,  Gooch W.,  Timofeeva I.I.,  Chugunova S.I., Gridneva I.V. K Pressure induced phase transition in ceramic materials during indentation Milne A.M., Bourne N.K. E Experimental and numerical study of temperatures in cavity collapse 	 914-917 )Milne A.M.,  Bourne N.K., Millett J.C.F. ? On the unreacted Hugoniots of three plastic bonded explosives VMilyavskiy V.V.,  Utkin A.V.,  Zaretsky E.B.,  Zhuk A.Z.,  Yakushev V.V., Fortov V.E.  Hugoniot of C60 fullerite ^Ming L.C.,  Manghnani M.H.,  Balogh J.,  Qadri S.B.,  Skelton E.F.,  Webb A.W., Jamieson J.C. C Static P-T-V measurements on MgO: Comparison with shock wave data Minich R.W. @ Optimal velocity amplification in a system of colliding plates 1Minich R.W.,  Kumar M.,  Schwarz A., Cazamias J. . Scaling, microstructure and dynamic fracture Minnaar K., Zhou M. 3 Characterization of impact in composite laminates  1208-1211 Minomura S. Y High pressure studies of lattice and electronic structures of Si/Si1-xGex superlattices :Mintmire J.W.,  Robertson D.H.,  Brenner D.W., White C.T. f Molecular dynamics simulations of pressure wave effects at voids in a model condensed-phase material GMintmire J.W.,  Robertson D.H.,  Elert M.L.,  Brenner D.W., White C.T. A Molecular dynamics of void collapse mechanisms in shocked media 	 969-972 ]Mintsev V.B.,  Ternovoi V.Y.,  Gryaznov V.K.,  Pyalling A.A.,  Fortov V.E., Iosilevskii I.L. 3 Electrical conductivity of shock compressed xenon Mishin G., Yushchenkova N. - Nonlinear processes in shock waves in gases 	 741-743 MMishra A.,  Martin M.,  Gregori F.,  Asaro R.J.,  Meyers M.A., Thadhani N.N. 2 Reverse Taylor tests on ultrafine grained copper Missionnier M., Heuz� O. P Modeling of shock waves with multiple phase transitions in condensed materials 	 262-265 (Mitchell A.C.,  Nellis W.J., Monahan B. 4 Enhanced performance of a two-stage, light gas-gun K Piezoresistant response of rolled ytterbium foils to double-shock loading Miller A.R. 3 Explosive synthesis of a Y-Ba-Cu-O superconductor Miller P.J., Guirguis R.H. _ Effects of late chemical reactions on the energy partition in non-ideal underwater explosions Miller P.J., Sutherland G.T. $ Reac����������������������������������������������������������������������������������������������������������������������������������tion rate modeling of PBXN-110 Miller P.J., Lindfors A.J. X Shock loading and reactive flow modeling studies of void induced AP/Al/HTPB propellant Miller J.S., Pangilinan G.I. ? Measurements of aluminum combustion in energetic formulations +Millett J.C.F.,  Bourne N.K., Rosenberg Z. Y Shear stress measurements in copper, iron and mild steel under shock loading conditions M An investigation of the a-e phase transition in shock loaded EN3 mild steel <Millett J.C.F.,  Galbraith S.D.,  Rosenberg Z., Bourne N.K. d Direct measurements of strain in the B1/B2 phase transformation in shock loaded potassium chloride > Measurements of strain in a shock loaded, high-density glass 8Millett J.C.F.,  Tsembelis K.,  Bourne N.K., Field J.E. ) The shock Hugoniot of two igneous rocks 8Millett J.C.F.,  Bourne N.K.,  Gray�III G.T., Cooper G. * On the shock response of polychloroprene Millett J.C.F., Bourne N.K. ` The shear strength of potassium chloride above the B1-B2 phase transition during shock loading ;Millett J.C.F.,  Bourne N.K.,  Gray�III G.T., Stevens G.S. 7 On the shock response of the shape memory alloy, NiTi 9Millett J.C.F.,  Jones i.P.,  Bourne N.K., Gray�III G.T. N The effect of microstructure on the shock behaviour of g-titanium aluminides ,Millett J.C.F.,  Gray�III G.T., Bourne N.K. C Longitudinal and lateral stress measurements in shock loaded PEEK C Lateral stress measurements in pure tungsten during shock loading GMilman V.Y.,  Nemoshkalenko V.V.,  Zhalko-Titarenko A.V., Antonov V.N. 8 Equation of state of transition fcc metals up to 1 TPa  1109-1112  Meyer�Jr. H.W., Schoenfeld S.E. 8 Effects of damage criteria on the onset of penetration  1343-1346 8Meyers M.A.,  Thadhani N.H.,  Erlich D.C., DeCarli P.S. < Martensitic transformation induced by tensile stress waves $Meyers M.A.,  Wang S.L., Gupta B.B. A Mechanical and thermal response of sohck-consolidated Mar-M 200 Meyers M.A., Kuriyama S. 4 Modeling of instability at the tip of a shear band 	 321-328 %Meyers M.A.,  Yu<   L.-H., Vecchio K.S.  Shock synthesis of silicides &Meyers M.A.,  Benson D.J., Shang S.S. ; Energy expenditure and limitations in shock consolidation &Meyers M.A.,  Xue Q., Nesterenko V.F. 6 Evolution in the patterning of adiabatic shear bands ?Meyers M.A.,  Perez-Prado M.T.,  Xue Q.,  Xu Y., McNelley T.R. N Microstructural evolution in adiabatic shear localization in stainless steel Meyers M.A.,  Gregori F.,  Kad B.K.,  Schneider M.S.,  Kalantar D.H.,  Remington B.A.,  Wark J.S.,  Boehly T., Ravichandran G. R Plastic deformation in laser-induced shock compression of monocrystalline copper EMeziere Y.,  Akhavan J.,  Stevens G.S.,  Millett J.C.F., Bourne N.K. 8 The shock Hugoniot of hydroxy-terminated polybutadiene HMeziere Y.J.E.,  Millett J.C.F.,  Bourne N.K.,  Wallwork A., Workman A. Z Longitudinal and lateral stress measurements in NiTi under one-dimensional shock loading Mikhailov A.I., Osipov R.S. ? Interface instabilities between shock-compressed metal layers Mikkola D.E., Wright R.N. ( Metallurgical effects of shock loading  98-117 ` Dislocation generation and its relation to the dynamic plastic response of shock loaded metals 
Milella P.P. ~ On the dependence of the yield strength of metals on temperature and strain rate: The mechanical equation of the solid state 	 642-645 Miller M.D. I Wave propagation and long-time behavior on the driven Sine-Gordon chain 	 281-286 Miller S.A. * Compaction wave profiles in granular HMX $ Pore collapse and hot spots in HMX % Detonation wave profile in PBX 9501 	 986-989 4Menoni C.S.,  Patel D.,  Hafich M.J., Robinson G.Y. H Band offsets in InGaP/InAlP multiple quantum wells using high pressure 8Merritt C.D.,  Huston A.L.,  Justus B.L., Campillo A.J. 5 Ultrafast shock induced uniaxial strain in a liquid !Merzhievsky L.A., Tyagelsky A.V. 0 Modelling of shock compression of porous media Mescheryakov Y.I. T Mesoscopical effects and particle velocity distribution in shock compressed solids  1065-1070 ; Macro-meso energy exchange in dynamically deformed steels  Mescheryakov Y.I., Divakov A.K. F Shock-induced mesoscopic processes and dynamic strength of materials MMescheryakov Y.I.,  Zhigacheva N.I.,  Petrov Y.A.,  Divakov A.K., Cline C.F. d Comparative analysis of uniaxial strain shock tests and Taylor tests for armor and maraging steels 'Meserole C.A.,  Fisher G.L., Funk D.J. f Synthesis of ideal iron film samples for shock physics experiments using ultrafast X-ray diffraction 3Meshcheryakov Y.I.,  Atroshenko S.A., Divakov A.K. k Role of shock-induced particle distribution in processes of dynamic localization during backside spalling FMeshcheryakov Y.,  Atroshenko S.A.,  Vasilkov V.B., Chernyshenko A.I. ] Criteria of transition from translational to rotational motion of media under shock loading 	 407-410 Meshcheryakov Y.I. D Kinetics of microstructure and strain rate dependence of materials 	 623-625 AMeshcheryakov Y.I.,  Divakov A.K.,  Zhigacheva N.I., Petrov Y.A. a Shock-induced a-w phase transition and mechanisms of spallation in shock loaded titanium alloys Meuken D., Carton E.P.   Explosive welding and cladding  1110-1113 uMeyer�Jr. H.W.,  Abeln T.,  Bingert S.,  Bruchey W.J.,  Brannon R.M.,  Chhabildas L.C.,  Dienes J.K., Middleditch J. 2 Crack behavior of ballistically impacted ceramic � Crystal-structure studies of III-V and group IV semiconductors using angle-dispersive diffraction techniques with an image-plate detector ~ Crystal-structure studies of II-VI semiconductors using angle-dispersive diffraction techniques with an image-plate detector McQueen R.G., Fritz J.N. � Some techniques and results from high-pressure shock-wave experiments utilizing the radiation from shocked transparent materials 	 193-207 'McQueen R.G.,  Fritz J.N., Morris C.E. < The velocity of sound behind strong shock waves in 2024 Al McQueen R.G., Marsh S.P. 6 High explosive systems for equation-of-state studies McQueen R.G., Isaak D.G. > Bromoform (CHBr3)   A very high-pressure shock-wave analyzer 
McQueen R.G. 4 The velocity of sound behind strong shocks in SiO2 6Meenakshi S.,  Godwal B.K.,  Rao R.S., Vijayakumar V. 3 On tetragonal distortion in indium under pressure 	Mehta S. A Theoretical melt curves of aluminium, copper, tantalum and lead 	 258-261 Meier J.K., Kerrisk J.F. . An introduction to the fast shock tube (FST) Meir G., Clifton R.J. ; Dislocation mobility in high purity LiF from 100K to 300K 	 303-307 ;Meisel L.V.,  Scanlon R.D.,  Johnson M.A., Lanzerotti Y.D. j Self-affine analysis on curved reference surfaces: Self-affine fractal characterization of a TNT surface &Mello M.C.,  Prakash V., Clifton R.J. G Multi-point interferometer for monitoring two-dimensional wave motion "Mendes R.,  Plaksin I., Campos J. ) Single and two initiation points of PBX /Mendes R.,  Plaksin I.,  Campos J., Ribeiro J. & Double slapper initiation of the PBX Menikoff R., Lackner K.S. B Generating strong shock waves with a supersonic peristaltic pump Menikoff R. 0 Numerical anomalies mimicking physical effects 	 253-258 Menikoff R., Kober E. P Equation of state and Hugoniot locus for porous materials: P-a model revisited " Compaction waves in granular HMX OMazavet S.,  Kress J.D.,  Collins L.A.,  Wood W.W.,  Johnson J.D., Blottiau P. K Density functional calculation of the Hugoniot of shocked liquid nitrogen @Mazevet S.,  Kress J.D.,  Magee N.H.,  Keady J.J., Collins L.A. E Quantum molecular dynamics calculations of Rosseland mean opacities 	 293-297 Mazor A.,  Partom Y., Barak G. F Equation of state of gold in the high-temperature low-density regime McCammon C. X High pressure in situ investigation of cubanite (CuFe2S3): Structural phase transition 9McClellan K.J.,  Swift D.C.,  Paisley D.L., Koskelo A.C. - Dynamic properties of nickel-aluminum alloy qMcCluskey C.W.,  Wilke M.D.,  Anderson W.W.,  Byers M.E.,  Holtkamp D.B.,  Rigg P.A.,  Furnish M.D., Romero V.T. @ Discrete layer verification of the LiF window spall diagnostic "McDaniel O.,  Moore C., Tindol S.  Laser ordnance initiation *McDonald R.,  Tanner W.G., Alexander W.M. q A study using molecular dynamics of the shock waves produced in an aluminum thin film via hypervelocity impacts  1769-1772 UMcDonald S.A.,  Bourne N.K.,  Withers P.J.,  Millett J.C.F.,  Bennett K., Milne A.M. W The shock response, simulation and microstructural determination of an inert simulant +McGlaun J.M.,  Zeigler F.J., Thompson S.L. R CTH: A three-dimensional, large deformation deformation, shock wave physics code %McGrane S.D.,  Moore D.S., Funk D.J. b Measurement of shocked thin polymer film Hugoniot properties with ultrafast dynamic ellipsometry  1181-1186 McGregor N.M., Sutherland G.T. > Plate impact experiments on a porous Teflon-aluminum mixture 
McMahan A.K. 3 The a-b transition on T=0 high pressure beryllium 	 340-344 McMahan A.K., Skriver H.L. D Positron annihilation and pressure-induced electron s-d transition 	 107-112 5McMahon M.I.,  Nelmes R.J.,  Wright N.G., Allan D.R. L An internal damage model for viscoelastic-viscoplastic energetic materials Matheson E.R., Rosenberg J.T. U A mechanistic study of delayed detonation in impact damaged solid rocket propellant 	 464-467 Matheson E.R., Nguyen D.Q. W A rate-dependent viscoelastic damage model for simulation of solid propellant impacts GMathews A.R.,  Boat R.M.,  Hemsing W.F.,  Warnes R.H., Whittemore G.R. ' Full field Fabry-Perot interferometer %Mathieu D.,  Simonetti P., Martin P. N A model to study the electronic response to an impact in energetic materials %Mathieu D.,  Martin P., Simonetti P. T Nonadiabatic simulation of valence electrons in solids under sustained shock waves (Matsuda A.,  Nakamura K.G., Kondo K.-I. ^ Time-resolved Raman spectroscopy of benzene derivatives under laser-driven shock compression 
Matsui M. B Molecular dynamics study of iron at Earth's inner core < condition Mattsson A.E. , Equation of state for a high-density glass (Maw J.R.,  Whitworth N.J., Holland R.B. @ Multiple shock compression of polyurethane and syntactic foams Maw J.R., Giles A.R. < Numerical modelling of spallation in 2D hydrodynamic codes 	 295-298 Maw J.R., Whitworth N.J. T Shock compression and the equation of state of fully dense and porous polyurethane 	Maw J.R. 4 Lagrangian analysis of EDC37 shock initiation data  1027-1030 K A characteristics code for analysis of isentropic compression experiments KMayer F.J.,  Maynard R.L.,  Musinski D.L.,  Schmerberg N.W., Benjamin R.J. Z Recent developments in microshell-tipped optical fibers as high pressure shock detectors 	 547-551 $Mayseless M.,  Harvey W.B., Hetz A. R A computational study of non-porous and porous liners in explosively-formed jets )Mayseless M.,  Luttwak G., Birnbaum N.K. 0 Numerical simulations of rod-plate interaction  1133-1136 # New LANL gas driven two-stage gun  1643-1646 Martinez E., Servas J.M. A Sound velocity Doppler laser interferometry measurements on TiN  1200-1203 &Martinez A.R.,  Hooks D.E., Dick J.J. C Longitudinal and lateral ytterbium gauge measurements in PBX 9501 	 792-795 Martynov A.I., Batsanov S.S. 7 The calculation of dimensions of the steady Mach wave 	 677-680 FMas E.M.,  Clements B.E.,  Blumenthal W.R.,  Cady C.M., Gray�III G.T. v Applying micromechanics to finite element simulations of split Hopkinson pressure bar experiments in high explosives OMas E.M.,  Clements B.E.,  Blumenthal W.R.,  Cady C.M.,  Gray�III G.T., Liu C. & A viscoelastic model for PBX binders 	 661-664 &Mas E.M.,  Clements B.E., George D.C. * Direct numerical simulations of PBX 9501 2Mas E.M.,  Clements B.E.,  Ionita A., Peterson P. \ Finite element method calculations on statistically consistent microstructures of PBX 9501 Mashimo T. W Measurements of the combined compression-shear shock waves of over 20 GPa in sapphire 0 Shock yielding properties of brittle materials :Mashimo T.,  Kodama M.,  Kusaba K.,  Fukuoka K., Syono Y. Y Hugoniot measurement study of the partially stabilised and stabilised zirconia ceramics ; Shock compression of ceramic materials: Yielding property Mashimo T., Uchino M. - Shock compression behavior of boron carbide 	 531-533 $Mashimo T.,  Nakamura M., Uchino M. H Measurement of shock-wave structure of LiF single crystal by the VISAR <Mashimo T.,  Tsumoto K.,  Noguchi Y.,  Fukuoka K., Syono Y. Y Hugoniot measurement of alumina single crystal in the pressure range up to over 100 GPa 	 101-103 &Mason T.A.,  Henrie B.L., Thomas K.A. 7 Damage progression in explosively loaded polycrystals +Matheson E.R.,  Drumheller D.S., Baer M.R. b A coupled damage and reaction model for simulating energetic material response to impact hazards N Structural characterization of energetic materials by small angle scattering ?Mang J.T.,  Skidmore C.B.,  Son S.F.,  Hjelm R.P., Rieker T.P. b An optical microscopy and small-angle scattering study of porosity in thermally treated PBX 9501 Mang J.T., Hjelm R.P. � SANS and contrast variation measurement of the different contributions to the total surface area in PBX 9501 as a function of pressing intensity WMangeant C.,  Lassalle F.,  L'Eplattenier P.,  H�reil P.-L.,  Bergues D., Avrillaud G. N SYRINX project: HPP generators devoted to isentropic compression experiments  1173-1176 "Mao H.-K.,  Hemley R.J., Mao A.L. 2 Recent design of ultrahigh-pressure diamond cell  1613-1616 Margolin L.G. C Calculations of cratering experiments with the bedded crack model 	 465-469 )Margolin L.G.,  Smith B.W., DeVault G.P. 1 A micromechanical model of porous-brittle solid 	 329-333 &Marlin P.,  Penazzi L., Bensoussan P. J Laser-induced shock waves in aluminum with PVDF and quartz stress gauges $Marom H.,  Sherman D., Rosenberg Z. : On the inelastic response of alumina under shock loading $Marsh S.P.,  McQueen R.G., Tan T.H.  Acceleration of metal plates 	 985-987 Marsh S.P., Tan T.-H. " Hypervelocity plate acceleration  1033-1039 Marston P.L., Pullen G.L. > Cavitation in water induced by the reflection of shock waves 	 515-519 Marston P.L., Unger B.T. ; Rapid cavitation induced by the reflection of shock waves 	 401-405 
Marston P.L. \ Wavefront geometries giving transverse cusp and hyperbolic umbilic foci in acoustic shocks &Martin M.,  Hanagud S., Thadhani N.N. L Dynamic mechanical behavior of nickel-aluminum reinforced epoxy composites EMartin E.S.,  Thomas K.A.,  Clarke S.A.,  Kennedy J.E., Stewart D.S. D Measurements of the DDT process in exploding bridgewire detonators IMartinez A.R.,  Sheffield S.A.,  Whitehead M.C.,  Olivas H.D., Dick J.J. 5Lutz S.S.,  Turley W.D.,  Rightley P.M., Primas L.E. % Gated IR images of shocked surfaces  1239-1242 Lynch C.S., Charest J.A. ; Practical considerations on the piezofilm gauge technique Lyzenga G.A., Ahrens T.J. ( One-dimensional isentropic compression 
Lyzenga G.A. A Optical pyrometry at high shock pressure and its interpretation 	 268-276 Mabire C., H�reil P.L. 9 Shock induced polymorphic transition and melting of tin 3 Shock induced melting of lead: Experimental study :Maienschein J.L.,  Urtiew P.A.,  Garcia F., Chandler J.B. 6 Effect of microvoids on the shock initiation of PETN 7Mailhot C.,  Yang L.H.,  McMahan A.K., Barbee�III T.W.  Polymeric nitrogen Maillet J.-B., Bernard S. / Uniaxial Hugoniostat: Method and applications Maillet J.-B.  MD simulations of hot spots 	 379-384 DMaillet J.-B.,  Crouzet B.,  Matignon C.,  Mondelain L., Soulard L. % Multiscale simulation of detonation Main J.A., Gazonas G.A. > Impulsive loading of cellular media in sandwich construction Majewski P. 2 Effects of thin glue bonds on shock waves in LiF 	 500-504 $Majewski P.,  Gupta Y.M., Seaman L. > Tension-recompression response of shock loaded polycarbonate 	 407-413 Makhov M.N. B Explosion heat and metal acceleration ability of high explosives Maksimov I.L. N Thermomagnetic shock wave and magnetic flux penetration into superconductors *Malaise F.,  Tranchet J.-Y., Collombet F. ^ Effects of a dynamic confinement on the penetration resistance of ceramics against long rods Malkov I.Y., Titiov V.M. 7 Structure and properties of detonation soot particles )Mandell D.A.,  Holian K.S., Henninger R. B MESA: A 3-D Eulerian hydrocode for penetration mechanics studies Mandell D.A., Wingate C.A. L Numerical simulations of glass impacts using smooth particle hydrodynamics @Mang J.T.,  Skidmore C.B.,  Howe P.M.,  Hjelm R.P., Rieker T.P. Lucht R.A., Charest J.A. H Calibration and use of a rugged new piezoresistive pressure transducer Lugovoy P.Z., Gouliaev V.I. C Propagation of shock wave fronts in anisotropic layered materials Lundblad E.G. 6 High pressure synthesis of diamond in Sweden in 1953 Luo H., Ruoff A.L. . X-ray diffraction study of sulfur to 212 GPa  43-48 !Luo H.,  Greene R.G., Ruoff A.L. D X-ray diffraction and Raman scattering studies of C6H5Cl to 60 GPa G On the ultimate yield strength of diamond: Finite elasticity approach 2 High-pressure Raman scattering studies of sulfur ILuo S.-N.,  Swift D.C.,  Tierney T.,  Xia K.,  Tschauner O., Asimow P.D. k Time-resolved X-ray diffraction investigation of superheating-melting of crystals under ultrafast heating $Luo S.-N.,  Ahrens T.J., Swift D.C. & Melting at the limit of superheating 	 172-175 
Luo S.-N. D Limit of superheating and supercooling in solid-liquid transitions 	 252-257 Luther G.G., Vesser L. T A microwave interferometer to measure particle and shock velocities simultaneously Luther G.G., Warthen B.J. 8 Microwave interferometry to elucidate shock properties  1755-1758 Luttwak G. / Numerical simulation of water jet penetration !Luttwak G.,  Florie K., Venis A. * Numerical simulation of soft body impact   Second order discrete rezoning  1777-1780 %Luttwak G.,  Rosenberg Z., Kivity Y. <  ( Long rod penetration in oblique impact Luttwak G., Mayseless M. f Three dimensional numerical simulations of the effect of cyclic perturbations on liner accelerations (Luttwak G.,  Cowler M.S., Birnbaum N.K. 4 Virtual memory techniques in Eulerian calculations d Comparing Lagrangian Godunov and pseudo-viscosity schemes for multi-dimensional impact simulations 7 Interface tracking in Eulerian and MMALE calculations Luttwak G., Falcovitz J. = Staggered mesh Godunov schemes for Lagrangian hydrodynamics / Plate impact recovery experiments of ceramics %Lopatin C.M.,  Bless S.J., Brar N.S. / Dynamic unloading behavior of soda lime glass &Lopatin C.,  Wittman C., Holmquist T. 9 Dynamic compressive properties of an explosive simulant 	 495-496 Lorenz B., Orgzall I. @ Optical absorption studies of sulfur at pressures up to 20 GPa Louro L.H.L., Meyers M.A. = Stress-wave induced fragmentation in alumina-based ceramics , Shock Compression of Condensed Matter 1989 (Louzada K.L.,  Stewart S.T., Weiss B.P. l Shock demagnetization of pyrrhotite (Fe1-xS, xd"0.13) and implications for the Martian crust and meteorites  1476-1479 VLoveday J.S.,  Wilson R.M.,  Nelmes R.J.,  Besson J.M.,  Klotz S.,  Hamel G., Hull S. U Crystal structure studies with the Paris-Edinburgh cell: Neutron scattering aspects 	 413-416 Lowe C.A., Greenaway M.W. ) The dynamic compaction of microfine HMX L�wer T., Sigel R. L Uniform shock waves driven by thermal radiation from laser-heated cavities Lu F.,  Huan S., Ding J. a Viscoplasticity and porosity effects on the shock propagation in PMMA and porous aluminum oxide  1013-1016 Lu X., Hanagud S.V. V Structural phase transitions and equation of state of aluminum from first principles Lu X., Hanagud S. u High pressure & high temperature equation of state and magnetic phase transitions of hematite from first principles Lubyatinsky S.N., Loboiko B.G. @ Reaction zone measurements in detonating aluminized explosives G Density effect on detonation reaction zone length in solid explosives 	 743-746 �Lubyatinsky S.N.,  Batalov S.V.,  Garmashev A.Y.,  Israelyan V.G.,  Kostitsyn O.V.,  Loboiko B.G.,  Pashentsev V.A.,  Sibilev V.A.,  Smirnov E.B., Filin V.P. F Detonation propagation in 180� ribs of an insensitive high explosive LLubyatinsky S.N.,  Loboiko B.G.,  Filin V.P.,  Kostitsin O.V., Smirnov E.B. * Steady 2D detonations and the DSD theory A Study of sensitivity and repeatability of piezoelectric sensors  1195-1198 VLoboyko B.G.,  Alekseev A.V.,  Litvinov B.V.,  Sumin V.D.,  Taybinov N.P., Filin V.P. H Investigation of explosives mechanic impact sensitivity on the samples BLojkowski W.,  Porowski S.,  Rebkin E.I.,  Straumal B.B., Gust W. b Pressure effect on grain boundary dewetting and premelting transition in a Fe-6 at.%Si bicrystal  1205-1208 +Lomonosov I.V.,  Bushman A.V., Fortov V.E. 8 Equations of state for metals at high energy densities 4 Wide-range multi-phase equation of state of metals 	 121-124 <Lomonosov I.V.,  Bushman A.V.,  Fortov V.E., Khishenko K.V. 4 Caloric equations of state of structural materials Lomonosov I.V., Fortov V.E. � Look into the liquid phase of metal from the equation of state: Is there an agreement between shock-wave and isobaric-expansion data?  51-54 ?Lomonosov I.V.,  Fortov V.E.,  Khishchenko K.V., Levashov P.R.   Shock wave stability in metals \ Phase diagrams and thermodynamic properties of metals at high pressures, high temperatures = Theoretical investigation of shock wave stability in metals GLomonosov I.V.,  Fortov V.E.,  Kim V.V.,  Matveichev A.V., Ostrik A.V. L Influence of equation of state on results of hypervelocity impact modeling Lomov I.N., Kondaurov V.I. T Fracture of brittle material with initial porosity under high energy density flows %Lomov I.N.,  Antoun T.H., Glenn L.A. K Explosion in the granite field: Hardening and softening behavior in rocks 2Lomov I.N.,  Antoun T.H.,  Wagoner J., Rambo J.T. = Three-dimensional simulation of the Baneberry nuclear event  1462-1465 Lomov I., Liu B. y Approximation of multifluid mixture response for simulation of sharp and diffuse material interfaces on a Eulerian grid Long K.S.,  Young D., Lee F.H. / A new full-range equation of state for copper 	 213-217 Longy F., Cagnoux J. g Pressure-induced grain fining and noncrystallization of crystal structure in Eu2+ activated Sr-borate *Liu H.,  Liu W.,  Guan Z.,  Sun S., Su W. N Crystallization of amorphous SrB4O7 under high pressure and high temperature Liu J., Vohtra Y.K. R Calibration and fluorescence intensities of Sm:doped YAG to ultra high pressures  1681-1684 RLiu F.-S.,  Chen X.-M.,  Chen P.-S.,  Chen J.-X.,  Tan H.,  Gou Q.-Q., Jing F.-Q. ; Equation of state and conductivity of shocked heavy water Liu L.-Q., Katsabanis P.D. D A constitutive model for predicting rock fragmentation by blasting Liu C., Ahrens T.J. / Stress wave attenuation in shock damaged rock Liu C.L., Ahrens T.J. 4 Wave generations from confined explosions in rocks Liu Z.,  Nagano S., Itoh S. 4 Overdriven detonation phenomenon in high explosive  Liu C.,  Ahrens T.J., Brar N.S. ) Vitreous Ge02 response to shock loading Liu W.,  Tang Z.P., Liu Y. j Discrete meso-element simulation of the failure behavior of short-fiber composites under dynamic loading 3 Penetration depth time history measurement method  1039-1042 Liu C. ) Fracture of the PBX 9501 high explosive 	 786-791  Liu B.T.,  Lomov I., Glenn L.A. Q Numerical modeling of mixing and venting from explosions in undergound chambers  1472-1475 'Llorca F.,  Juanicotena A., Dambrun C. � Modeling of the high strain and high strain rate behavior of tantalum: Application to the dynamic expansion of a spherical shell Llorca F., Buy F. g The contribution of the expanding shell test to the modeling of elastoplasticity at high strain rates Llorca F.,  Buy F., Farre J. 7 Experimental analysis of shock wave effects in copper 	 638-641 Llorca F., Roy G. ; Metallurgical investigation of dynamic damage in tantalum !Lloyd A.,  Borg J.P., Downs T.J. - Liquid breakup under one-dimensional strain 	 634-637 (Lloyd C.E.,  Greenaway M.W., Proud W.G. \ Study on the synthesis process of CeTbO3 compound under high pressure and high temperature .Li X.-Z.,  Tang Z.-P.,  Zhou G.-Q., Lin S.-B. 5 Thermal effects in laser induced strong shock waves  1907-1910 Liang Y.-M., Zhao H.-Y. C Two methods for measuring shock relations with improved EMV gauge !Liang D.,  Chou P.C., Hashemi J. 5 Shock and shear effects in explosives due to impact 7Libersky L.D.,  Randles P.W.,  Bourne N., Vignjevic R. ] Simulation of void collapse in ammonium nitrate using a meshfree Lagrangian particle method Libersky L.D., Randles P.W. 0 Shocks and discontinuities in particle methods Liddiard T.P., Forbes J.W. I Shock waves in fresh water generated by detonation of pentolite spheres 	 578-582 ,Lindfors A.J.,  Finnegan S.A., Boteler J.M. L A study of shock-induced reactivity in a porous pyrotechnic powder mixture 2Littlefield D.L.,  Anderson�Jr. C.E., Skaggs S.R. 4 Analysis of penetration of steel and Al2O3 targets  1793-1796 $Littlefield D.L., Anderson�Jr. C.E. E A study of zoning requirements for 2-D and 3-D long-rod penetration #Littlefield D.L., Cour-Palais B.G. V Scaling relationships for evaluation of performance of advanced space debris shields Littlefield D.L. E Optimization of the performance of segmented-telescopic penetrators L An algorithm for modeling contact in three-dimensional Eulerian hydrocodes Littlefield D.L., Baker E.L. P Implementation of a high explosive equation of state into a Eulerian hydrocode �Litvinov B.V.,  Zeldovich V.I.,  Purygin N.P.,  Khomskaya I.V.,  Buzanov V.I.,  Kheifetz A.E.,  Rinkevich O.S.,  Frolova N.Y., Sobyanina < G.A. � Non-one-dimensional and quasi-spherical loading of metal balls by shock-waves having up to 3 Mbar pressure, with the investigation of the preserved samples 	 981-983 9Liu W.-N.,  Liu H.-J.,  Feng Y.-C.,  Sun S.-L., Su W.-H. Q Picosecond laser induced shock wave pressure measurements in Al, C-Si, and GaAs 	 343-345 LLevashov P.R.,  Fortov V.E.,  Khishchenko K.V.,  Lomov I.N., Lomonosov I.V.  Shock wave data base ?Levashov P.R.,  Fortov V.E.,  Khishchenko K.V., Lomonosov I.V. % Equation of state for liquid metals ^ Analysis of isobaric expansion data based on soft-sphere equation of state for liquid metals  71-74 6Levashov P.R.,  Filinov V.S.,  Fortov V.E., Bonitz M. J Thermodynamic properties of nonideal strongly degenerate hydrogen plasma w Authors' reply to R. Pollock's comments on 'Thermodynamic properties of nonideal strongly degenerate hydrogen plasma' 	 125-126 ?Levashov P.R.,  Khishchenko K.V.,  Lomonosov I.V., Fortov V.E. R Database on shock-wave experiments and equations of state available via internet !Levy A.,  Barak G., Ashkenazi J. c Thermodynamics of 3d metals   Band structure effects and their disappearance at high temperatures Li C.H., Clifton R.J. G Dynamic stress-strain curves at plastic shear strain rates of 105 s-1 	 360-366 Li W. I Simplified equation of state P=P(r,E) and P=P(r,T) for condensed matter 	 167-173 Li H., Wang Z. E Free Lagrange method for two dimensional hydro-elastic-plastic flow !Li X.-Z.,  Tang Z.P., Zhou G.-Q. H Mechanism of the shock-induced phase transition in CdS single crystals Li X.-J., Zhang K. @ Explosive welding of multilayer amorphous ribbons into a plate :Li D.J.,  Feng J.,  Ding B.Z.,  Yao B.,  Hu Z.Q., Su W.H. _ The high pressure amorphization and the computer simulation of the pressure-quenching process 9Li D.J.,  Guo M.,  Hu Z.Q.,  Ding B.Z.,  Yao B., Su W.H. : Pressure-induced amorphization mechanism of Cd-Sb system 5Li M.M.,  Strachan D.J.,  Tamargo M., Weinstein B.A. > Pressure-induced instability of deep acceptor states in ZnSe Li H.,  Su W.,  Li L., Wang Y. � A method of parameterising hydrocode kinetic models for non-ideal explosives based on the variation of detonation velocity with charge diameter 	 917-922 Leiper G.A., Hackett A. 6 Radial motion in unconfined axisymmetric detonations .Leitsin V.N.,  Skripnyak V.A., Dmitrieva M.A. l Three-scale model for numerical simulation of mechano-chemical processes in shock-compressed powder bodies  1093-1096 2Lemar E.R.,  Forbes J.W.,  Erkman J.O., Watt J.W. . NSWC/WO light gas gun and explosive facility 	 663-667 $Lemar E.R.,  Forbes J.W., Watt J.W. T Unreacted Hugoniot and shock initiation studies of composition B-3 and PBXW-109(I) 	 539-541 1Lemar E.R.,  Forbes J.W.,  Tasker D.F., Bur A.J. F Polyvinylidene fluoride transducer for dynamic pressure measurements 	 503-508 Lemar E.R., Forbes J.W. 7 Detonation wave curvature of cast Comp B and PBXN-111 *Lemar E.R.,  Forbes J.W., Sutherland G.T. > Detonation wave velocity and curvature of IRX-4 and PBXN-110 +Lemar E.R.,  Forbes J.W., Cowperthwaite M. n Oblique shock wave calculations for detonation waves in brass confined and bare PBXN-111 cylindrical charges +Lemberg V.F.,  Psakhie S.G., Zolnikov K.P. D Thermodynamic properties of simple metals under shock wave loading  75-78 Lemberg V.F., Psakhie S.G. ] The search for the conditions necessary to initiate chemical reaction by particle collision BLemke R.W.,  Knudson M.D.,  Davis J.-P.,  Bliss D.E., Harjes J.C. u Self-consistent 2D magneto-hydrodynamic simulations of magnetically driven flyer plate experiments on the Z-machine  1175-1180 "Le�n G.C.,  Romo S.R., Tchijov V. 6 A kinetic model of multiple phase transitions in ice $Lettieri T.,  Kelley J., Ehrlich C. Q Investigation of annular forces using an oscillating, gas-operated piston gauge  1605-1608 #Leung K.P.,  Yao S.S., Alfano R.R. ? Enhancement of detonation properties by electric energy input 	 865-868 )Lee L.M.,  Montgomery S.T., Jilbert P.H. . Multi-element quartz shock gauge development Lee R.J., Joshi V.S. k Use of high-speed photography to augment split Hopkinson pressure bar measurements of energetic materials 	 860-863 �Lee K.K.M.,  Benedetti L.R.,  Mackinnon A.,  Hicks D.,  Moon S.J.,  Loubeyre P.,  Occelli F.,  Dewaele A.,  Collins G.W., Jeanloz R. u Taking thin diamonds to their limit: Coupling static-compression and laser-shock techniques to generate dense water =Lee K.-Y.,  Kennedy J.E.,  Asay B.W.,  Son S.F., Martin E.S. e Preparation and characterization of fine-particle NTO and its formulation with aluminum nanopowders 	 855-858 @Lee J.S.,  Hokamoto K.,  Raghukandan K.,  Yamashita K., Itoh S. Z Development of an underwater dynamic compaction technique for making Al-based composites  1106-1109 Lee R.J., Gustavson P.K. w Electrical conductivity as a real-time probe of secondary combustion of solid-fuel additives in detonating explosives �Lee R.J.,  Mock�Jr. W.,  Carney J.R.,  Holt W.H.,  Pangilinan G.I.,  Gamache R.M.,  Boteler J.M.,  Bohl D.G.,  Drotar J., Lawrence G.W.  Reactive materials studies 	 169-174 0Lee P.R.,  Curtis J.P.,  Mills J.T., Lynch N.J. Q On the detonation of an explosive by the shock resulting from projectile impact 2L�ger J.M.,  Haines J.,  Atouf A., Tomaszewski P. k Phase transitions in several metal dioxides as studied by angle dispersive X-ray diffraction up to 50 GPa Legrand M. H Interface instabilities occurring during an explosive driven implosion $Legrand B.,  Blanco E., Martinez E. h Validation of a multitechnical device aimed to reach the temperature of a material under shock loading  1191-1194 Leiper G.A., Kirby I.J. N Studies of the Bauer piezoelectric polymer gauge (PVF2) under impact loading 	 497-502 ALee M.P.,  Wang G.M.,  Sung P.H.,  Chang W.L.,  Lee Y.L., Lin K. ? The attenuation of shock waves in PU foam and its application 	 687-692 =Lee R.J.,  Tasker D.G.,  Forbes J.W.,  Beard B.C., Sharma J. E Shock ignition of an explosive due to electrostatic discharge (ESD) .Lee L.M.,  Hyndman D.A.,  Reed R.P., Bauer F. ) PVDF applications in shock measurements Lee R.J., Tasker D.G. V Factors affecting the sensitivity of energetic materials to electrostatic initiation $Lee W.M.,  Demske D.L., Miller P.J. q Optically measured temperature profile of a condensed aluminum-water medium undergoing a fast chemical reaction ?Lee L.M.,  Johnson D.E.,  Bauer F.,  Reed R.P., Greenwoll J.I. O Piezoelectric polymer PVDF application under soft x-ray induced shock loading !Lee I.-Y.S.,  Wen X., Dlott D.D. ` Ultrafast spectroscopy of temperature and pressure jump and shock waves in molecular materials  1543-1546 ILee I.-Y.S.,  Hare D.E.,  Hill J.R.,  Franken J.,  Suzuki H., Dlott D.D. 0 Ultrafast spectroscopy of the first nanosecond Lee W.H., Clancy S.P. G A strong shock tube problem calculated by different numerical schemes Lee R.J., Forbes J.W. N PVDF transducer response from an electrical discharge in an aluminized solid  1089-1092 5Lee J.,  Kuk J.H.,  Song S.-Y.,  Cjoi K.Y., Lee J.W. 8 Detonation in an aluminized explosive and its modeling 	 369-372 Lee M., Bless S.J. S A discrete impact model for effect of yaw angle on penetration by rod projectiles ULee J.H.S.,  Goroshin S.,  Yoshinaka A.,  Romano M.,  Jiang J.,  Hooton I., Zhang F. < Attempts to initiate detonations in metal-sulphur mixtures .Lee J.J.,  Jiang J.,  Choong K.H., Lee J.H.S. g Effect of diethylenetriamine and triethylamine sensitization on the critical diameter of nitromethane ,Lee J.,  Kuk J.-H.,  Kim C.-H., Hwang E.-H. hLawrence R.J.,  Mehlhorn T.A.,  Haill T.A.,  Budge K.G.,  Trucano T.G.,  Cochrane K.R., MacFarlane J.J. @ Analysis of radiation-driven jetting experiments on NOVA and Z &Lawrence R.J.,  Grady D.E., Hall C.A. N The response of ceramic powders to high-level quasi-isentropic dynamic loads <   1213-1216 @Lawrence R.J.,  Reinhart W.D.,  Chhabildas L.C., Thornhill T.F. 2 Hypervelocity impact flash at 6, 11, and 25 km/s "Leal B.,  Presles H.N., Baudin G. 0 Shock initiation of detonation in nitromethane 	 687-690 )Lebedev T.S.,  Korchin V.A., Burtny P.A. H Petrovelocity PT-modeling and elastic inhomogeneity of the lithosphere 
Lebedev T.S. S Problem of geophysical application of the results of experimental PT-petrophysics Lebedev T.S., Savenko B.Y. ; Features of PT-changes of remanent magnetization of rocks 	 811-814 )Lebedev A.I.,  Aprelkov O.N.,  Arinin V.A.,  Bulannikov A.S.,  Burtsev V.V.,  Golubev V.A.,  Davydov N.B.,  Zhernokletov M.V.,  Ignatova O.N.,  Igonin V.V.,  Makarov Y.M.,  Manachkin S.F.,  Mochalov M.A.,  Nadezhin S.S.,  Nizovtsev P.N.,  Raevsky V.A.,  Sinitsyna S.N.,  Solovev V.P., Fadeev L.A. ^ Perturbaton method for study of shear strength of materials at pressures up to about 300 GPa &Lecume S.,  Spyckerelle C., Sommer F. K Structure of pristine crystal defects revealed by AFM and microtomography (Lee L.M.,  Fogelson D.J., Williams W.D. ) Dynamic stress transducer qualification Lee L.M., Forrestal M.J. A Experimental determination of applied forces during penetration 3Lee Y.K.,  Williams F.L.,  Graham R.A., Morosin B. 9 Specific surface measurements of shock modified powders !Lee C.K.B.,  Baker J., Peyton S. X The effect of equilibrium modeling of saturated quartz in energy coupling calculations 2Lee E.L.,  van�Thiel M.,  Green L.G., Mitchell A. G Detonation product EOS: The region above the Chapman-Jouguet pressure 1Lee L.M.,  Williams W.D.,  Graham R.A., Bauer F. 2 Numerical method for shock front Hugoniot states (Lange M.A.,  Ahrens T.J., Boslough M.B. ( Cratering and spall fracture in Gabbro Lanzerotti M.Y.D., Pinto J. C Chemical reaction of energetic materials during high acceleration 	 909-916 )Lanzerotti M.Y.D.,  Pinto J.J., Wolfe A. ) Fracture surface topography of cast TNT 4Lanzerotti M.Y.D.,  Autera J.,  Pinto J., Sharma J. Y Crystal growth of energetic materials during high acceleration using an ultracentrifuge 	 489-491 )Lanzerotti M.Y.D.,  Autera J., Sharma J. 1 Crystal growth of TNAZ during high acceleration Lanzerotti Y., Sharma J. ] Mechanical properties of energetic materials during high acceleration in an ultracentrifuge 	 595-597 E Mechanical behavior of energetic materials during high acceleration 	 853-855 4Lanzerotti Y.,  Capellos C.,  Travers B., Sharma J. E Mechanical behavior of TNAZ/CAB explosives during high acceleration 	 783-785 'Lanzerotti Y.,  Sharma J., Capellos C. H Mechanical behavior of TNAZ/Hytemp explosives during high acceleration -Last H.R.,  Garrett�Jr. R.K., Rajendran A.M. N A comparative study of high strain rate behavior of three martensitic steels Laverty R., Gazonas G. L Transient stress optimization of elastic and viscoelastic composite strips Lawrence W. : Measurement problems in high velocity impact experiments 	 534-538 8 Measurements of penetration using instrumented targets Lawrence R.J. / Stand-off shields for hypervelocity particles @ The equivalence of simple models for radiation-induced impulse Lawrence W., Franz R.E. : Designing a cutting charge to cut the shaped charge jets < Analytic models for hypervelocity particle shield analysis  1837-1840 4Lawrence R.J.,  Asay J.R.,  Trucano T.G., Hall C.A. / Analysis of radiation-driven explosive flyers P Analysis of the interaction of short-pulse high-fluence radiation with targets  1185-1188 2 Fracture initiation using tailored-pulse loading 	 470-474 Kutepov A., Kutepova S. 8 The ab initio study of structural stability of uranium Kuznetsov N.M.  Stability of shock waves 	 229-232 Kuznetsov N.M., Oleinik I.I. W Numerical simulation of relaxation phenomena in xenon compressed by strong shock wave Kwiatkowski C.S., Gupta Y.M. R Optical measurements to probe inelastic deformation in shocked brittle materials 	 641-644 2L'Eplattenier P.,  Avrillaud G., Vanpoperynghe J. ` 0D modelisation of the magnetic flux compression scheme for isentropic compression experiments  1188-1191 %Labaste J.L.,  Doucet M., Joubert P. = Shocks induced by laser driven flyer plates. 1: Experiments  1213-1215 &Labaste J.-L.,  Brisset D., Doucet M. R Investigation of driving plasma materials for laser acceleration of flyer plates  1189-1192 %Laber M.W.,  Brar N.S., Rosenberg Z. # Shock response of 5083-0 aluminum Ladd A.J.C. A Molecular dynamics studies of plastic flow at high strain rates 	 267-280 2Laine L.,  Ranestad �.,  Sandvik A., Snekkevik A. 4 Numerical simulation of anti-tank mine detonations 4Laity P.R.,  Siviour C.R.,  Church P.D., Proud W.G. = High strain rate characterisation of a polymer bonded sugar 	Lalle P. M Use of glass as window in interferometric measurements of particle velocity 	 751-758 3 Us-Up relation from isothermal equations of state Lalle P., Courchinoux R.  Melting on the Hugoniot 	 207-210 Lambourn B.D. N An interpretation of particle velocity histories during growth to detonation , An improved EOS for non-reacted explosives 7Lambrakos S.G.,  Oran E.S.,  Boris J.P., Guirguis R.H. O Molecular dynamics simulation of shock-induced detonation in energetic solids .Landwehr A.,  B�ttner M.,  Hahn W., Winter R. 0 The effect of high pressure on model membranes Lane J.M.D., Marder M. PKubota S.,  Ogata Y.,  Wada Y.,  Katoh K.,  Saburi T.,  Yoshida M., Nagayama K. 5 Observation of shock initiation process in gap test  1085-1088 CKudoh Y.,  Nagase T.,  Ohta S.,  Sasaki S.,  Kanzaki M., Tanaka M. L Crystal structure and compressibility of superhydrous phase B, Mg2Si6H8O36 Kudoh Y., Kanzaki M. J On the symmetry of the CaSiO3 perovskite quenched from 15 GPa and 1500�C % High pressure study on wollastonite )Kuk J.H.,  Lee J.,  Song S.-Y., Cho Y.S. K Numerical modeling of an underwater explosion for an aluminized explosive Kuklja M.M., Kunz A.B. 3 Modeling of shock compression of RDX with defects Kuklja M.M. M How point and line defects affect detonation properties of energetic solids 	 454-459 *Kuklja M.M.,  Rashkeev S.N., Zerilli F.J. W Ab initio calculations of the electronic structure of 1,1-diamino-2,2-dinitroethylene [ The atomic and electronic structure of defects in 1,1-diamino-2,2-dinitroethylene (FOX-7) 1Kumaran S.U.,  Lim C.T.,  Ong K.C.G., Tan G.E.B. X Effects of different nose-shaped projectiles on the high speed perforation of concrete &Kunishige H.,  Horie Y., Sawaoka A.B. c Numerical and experimental studies of chemically reacting powder mixtures under shock compression 
Kunz A.B. B Theory of spectroscopy of point defects in solids: Cr impuritues .Kupershtokh A.L.,  Ershov A.P., Medvedev D.A. 4 Coagulation of carbon clusters in detonation front 6Kuroyama Y.,  Itoh K.,  Liu Z.Y.,  Fujita M., Itoh S. ; A new apparatus for direct transformation from hBN to cBN 	 615-617  Kusaba K.,  Syono Y., Matsui Y. d Molecular dynamics calculation of rutile-fluorite phase transition induced by uniaxial compression Kusaba K., Weidner D.J. , Structure of high pressure phase I in ZnTe %Kuscher G.F.,  Hohler V., Stilp A.J. 8 Non-linear propagation of elasto-plastic waves in rods 	 377-382 Kusubov A.S., Swift R.P. <Kozlov E.A.,  Buslova E.S.,  Boboedova V.A., Gorbachev D.M. g Macrokinetics of a�e phase transition for some steels under different conditions of explosive loading �Kozlov E.A.,  Litvinov B.V.,  Kabin I.G.,  Matushkin N.D.,  Abakshin E.V.,  Muakin V.K.,  Chinkova R.H.,  Gornovaya I.K.,  Kuropatenko V.F.,  Sapozhnikov A.T., Sapozhnikova G.N. � The acquisition and investigation of submicrocrystal structure materials in experiments on loading of metal spheres by spherically converging shock waves 	 535-537 Kozlov E.A., Zhukov A.V. - Phase transitions in spherical stress waves *Kozlov E.A.,  Feldman V.I., Sazonova L.V. � Crystallochemical<   structure of rock-forming minerals and peculiarities, sequence and completeness of physicochemical transformations in weak and strong shock waves 0Kraichikov S.S.,  Dremov V.V., Sapozhnikov P.A. L Molecular dynamics investigation into influence of nano-particles in spall 	 399-402 Kraidenov V.F., Itskevich E.S. 7 The thermopower of HTC superconductors under pressure EKress J.D.,  Bickham S.R.,  Collins L.A.,  Holian B.L., Goedecker S. A Tight-binding molecular dynamics of shock waves in hydrocarbons &Kress J.D.,  Mazevet S., Collins L.A. P Density-functional molecular dynamics simulations of shocked molecular liquids 4Kress J.D.,  Mazevet S.,  Collins L.A., Blottiau P. E Quantum molecular dynamics simulations of shocked molecular liquids Kroupa J.L., Rajendran A.M. e The use of Grady-Kipp type fragmentation model to describe the impact behavior of ceramic materials DKr�ger L.,  Kanel G.I.,  Razorenov S.V.,  Meyer L., Bezrouchko G.S. f Yield and strength properties of the Ti-6-22-22S alloy over a wide strain rate and temperature range 0Kubota S.,  Nagayama K.,  Shimada H., Matsui K. < Numerical simulation of laser initiation of thin explosive 	 468-471 < Pressure calculation of reacting explosive by mixture rule pKonrad C.H.,  Chhabildas L.C.,  Boslough M.B.,  Piekutowski A.J.,  Poorman K.L.,  Mullin S.A., Littlefield D.L. : Dependence of debris cloud formation on projectile shape  1845-1848 ~Konrad C.H.,  Reinhart W.D.,  Chhabildas L.C.,  Mann G.A.,  Mosher D.A.,  Kipp M.E.,  Trucano T.G.,  Summers R.M., Peery J.S. : Experimental bench mark data for ALEGRA code validations )Koritskaya S.V.,  Trunin I.R., Arnold W. S Calculated experimental investigation of the Armco iron deformation in shock wave Korth G.E., Williamson R.L. 5 Impact shock generator from explosive-driven plates )Korth G.E.,  Williamson R.L., Rabin B.H. G Metal matrix composites from dynamic consolidation of powder mixtures /Kos K.,  Millett J.C.F.,  Bourne N.K., Deas D. K Lateral stress measurements and shear strength of an alumina-filled epoxy 3Koskelo A.,  Greenfield S.,  Greening D., Smith D. * New windows into shocks at the mesoscale !Kotelnikov A.D., Montgomery D.C. @ Numerical study of shock propagation in inhomogeneous material SKotulski J.D.,  Anderson M.U.,  Brock B.C.,  Gomez J.,  Graham R.A., Vittitoe C.N. D Determination of equivalent circuit for PVDF shock-pressure gauges  1739-1742 5Kovar F.R.,  Trigger K.R.,  Guymon L.G., Harvey J.R. : High explosive detonations in varying oxygen atmospheres 	 563-567 %Kowalski E.,  Tauscher B., Ludwig H. 3 Autoxiation of linolenic acid under high pressure &Kowalski P.M.,  Mazevet S., Saumon D. A The free-free opacity in warm, dense, and weakly ionized helium 	 123-126 Kozhevnikov V.F. L An acoustical study of prewetting phenomena in a compressed metallic vapor Kozhushko A., Maiboroda V. 1 Steady supersonic penetration of a porous media Kozlov E.A. � Experimental check of E.I. Zababahin hypothesis concerning limitation of energy calculation in the spherically converging shock-wave front in the medium with phase transitions 	 169-171 "Kober E.M.,  Bdzil J.B., Son S.F. H Modeling DDT in granular explosives with a multi-dimensional hydrocode �Koenig M.,  Benuzzi-Mounaix A.,  Grandjouan N.,  Malka V.,  Bouquet S.,  Fleury X.,  Marchet B.,  Stehl� C.,  Michaut C.,  Chi�ze J.P.,  Batani D.,  Henry E., Hall T. 4 Radiative shock experiments using high power laser dKoenig M.,  Benuzzi-Mounaix A.,  Ozaki N.,  Ravasio A.,  Vinci T.,  Lepape S.,  Tanaka K., Riley D. 8 High energy density physics on LULI2000 laser facility GKolesnikov S.A.,  Utkin A.V.,  Ananin A.V.,  Pershin S.V., Fortov V.E. O Reaction zone of steady-state detonation waves in dinitrodiazapentane and RDX QKoller D.D.,  Rigg P.A.,  Gray�III G.T.,  Jensen B.J.,  Hayes D.B., Maestas J.D. ) Low pressure Hugoniot for U-Nb (6 wt.%) tKoller D.D.,  Hixson R.S.,  Gray�III G.T.,  Rigg P.A.,  Addessio L.B.,  Cerreta E.K.,  Maestas J.D., Yablinsky C.A. 8 Explosively driven shock induced damage in OFHC copper 	 599-602 Kondaurov V.I., Lomov I.N. V Application of the Godunov-type methods for solution of the condensed matter problem #Kondo K.,  Ahrens T.J., Sawaoka A. M Electrical and optical measurements on fused quartz under shock compression 	 299-303 )Kondo K.,  Sawaoka A.,  Sato K., Ando M. : Shock compression and phase transformation of AlN and BP 	 325-329 	Kondo K. 2 Phase transformation of AlN by shock compression 6 Shock compaction method for nanocrystalline ceramics 	 609-612 * Shock compression of carbons and diamond Kondo K.-I. T Window problem and complementary method for shock-temperature measurements of iron  1555-1558 QKondo K.,  Hironaka Y.,  Ito H.,  Sugiura H.,  Ozaki S.,  Takeba A., Katayama M. B A trial of the three-stage light gas gun with a preheating stage >Kondo K.,  Fatyanov O.V.,  Hironaka Y.,  Moritoh T., Ozaki S. F Performance of the three-stage light gas gun with a preheating stage R Two mechanisms of explosive initiation by the impact of a cylindrical projectile ; Homogeneous mechanisms for detonation of heterogeneous HE )Kline K.,  Horie Y.,  Dick J.J., Wang W. ) Impact response of PBX 9501 below 2 GPa 9Kline K.L.,  Armstrong R.W.,  Kramer M.P., Richards D.W. I Comparative model X-ray diffraction characteristics of RDX and aluminum VKlotz S.,  Besson J.M.,  Hamel G.,  Nelmes R.J.,  Loveday J.S.,  Wilson R.M., Hull S. Z Crystal structure studies to 10 GPa with the Paris-Edinburgh cell: High pressure aspects  1577-1580 6Klug D.D.,  Svensson E.C.,  Montfrooij W., Sears V.F. 3 Low-frequency modes in high-density amorphous ice =Kmetyk L.N.,  Chhabildas L.C.,  Boslough M.B., Lawrence R.J. B Effect of phase change in a debris cloud on a backwall structure  1829-1832 HKnapp I.,  Millett J.C.F.,  Gray�III G.T.,  Bourne N.K., Meziere Y.J.E. 8 The shock Hugoniot of the intermetallic compound Ni3Al %Knudson M.D.,  Gupta Y.M., Kunz A.B. ` Transformation mechanism and kinetics for the pressure-induced phase transition in shocked CdS 	 255-260 Knudson M.D., Gupta Y.M. N Use of stimulated emission to measure R-line shifts in shocked ruby crystals LKnudson M.D.,  Hanson D.L.,  Bailey J.E.,  Hall C.A.,  Deeney C., Asay J.R. ? Equation of state measurements in liquid deuterium to 100 GPa  81-86 \Kobayashi T.,  Shoji M.,  Deol R.S.,  Buchan N.,  Heuberger W.,  Jakubowicz A., Roentgen P. w Pressure dependence of photoluminescence in GaInP grown on misoriented (100) GaAs by metalorganic vapor phase epitaxy  1495-1498 AKobayashi T.,  Sekine T.,  Fatyanov O.V.,  Takazawa E., Zhu Q.Y. H Shock temperatures of soda-lime glass measured by an optical pyrometer Kobayashi T., Sekine T. J Spectroscopic studies of some aromatic compounds under shock compression  Kobayashi T.,  Sekine T., He H. @ Vibrational spectra of nitro compounds under shock compression I High-pressure crystalline transformations and amorphization in a-quartz  39-42 *Kingsbury S.J.,  Tsembelis K., Proud W.G. > The dynamic properties of the Atlanta Stone Mountain granite  1454-1457 'Kinoshita T.,  Kawamura K., Mashimo T. I MD simulation of dislocation behavior in KCl under uniaxial compression Kipp M.E., Davison L. 9 Analyses of ductile flow and fracture in two dimensions Kipp M.E., Grady D.E. 9 Flaw nucleation and energetics of dynamic fragmentation A An application of geometric statistics to dynamic fragmentation 	 435-439 'Kipp M.E.,  Setchell R.E., Taylor P.A. 7 Homogeneous reactive kinetics applied to granular HNS 9 Shock compression and release in high-strength ceramics 3 Elastic wave dispersion in high-strength ceramics 
Kipp M.E. + Target response to debris cloud incidence  1849-1852 +Kipp M.E.,  Chhabildas L.C., Reinhart W.D. 7 Elastic shock response and spall strength of concrete 7Kipp M.E.,  Chhabildas L.C.,  Reinhart W.D., Wong M.K. 6 Polyurethane foam impact experiments and simulations Kirby I.J., Chan S.K. ^ Analysis of<   VOD-diameter data using an analytical two-dimensional non-ideal detonation model 9Kirkpatrick S.W.,  Curran D.R.,  Erlich D.C., Klopp R.W. Z Three-dimensional analyses of plate impact experiments with circular and star geometries 
 AmsterdamDKishimura H.,  Kawano H.,  Hironaka Y.,  Nakamura K.G., Kondo K.-I. � Transient lattice response to the interaction between pulse-laser and semiconductors probed by time-resolved X-ray diffraction Klee C.,  Kroh M., Ludwig D. C Experiments on the attenuation of shock waves in condensed matter 	 486-490 /Klein B.,  Frage N.,  Zaretsky E., Dariel M.P. F Dynamic response of titanium carbide-steel, ceramic-metal composites Klevert P. : Shock to detonation transition in homogeneous explosives Klimenko V.Y. . Multiprocess model of detonation (Version 3) W Equations of state and physical-chemical transformations of shocked organic compounds dKhishchenko K.V.,  Fortov V.E.,  Lomonosov I.V.,  Pavlovskii M.N.,  Simakov G.V., Zhernokletov M.V. T Shock compression, adiabatic expansion and multi-phase equation of state of carbon Kiiski A.A., Ruuskanen P.R. B Wear resistance coatings of steel made with shock wave technique  1659-1662 +Kiiski A.A.,  Deribas A.A., Shtertser A.A. G Study on explosive compaction of fine copper, iron and nickel powders ;Kikuchi M.,  Syono Y.,  Shimoda N.,  Fukuoka K., Hiraga K. F Redox reaction on oxide-metal interface boundary under shock loading ;Kikuchi M.,  Kawamata S.,  Okuda K.,  Fukuoka K., Syono Y. e Evaluation of shock-compacted Bi2Sr2CaCu2O8+d by X-ray diffraction and magnetic torque measurements 
Killian B.G. � Numerical methods developed for the simulation of coupled high-energy gas flows and stress wave propagation in geologic materials Kim K., Oh S.I. J Dynamic compaction of elastic-visco-plastic poeous materials under shock 	 376-380 PKim K.Y.,  Palmour�III H.,  Batchelor A.D.,  Kanda H.,  Akaishi M., Fukunaga O. Q Effects of dynamic vs. static compaction on the sinterability of alumina powder Kim K. = Particle size dependent reaction rate in shocked explosives Kim H., Dlott D.D. ; Blast and shock wave dynamics in complex molecular solids 8Kim I.H.,  Jhung K.S.,  Oh K.-H.,  Hahn K.B., Hong S.H. $ Shock induced chemistry of dry air ; Shock compression of proteins: The energy landscape model  1448-1453 GKim V.V.,  Fortov V.E.,  Lomonosov I.V.,  Matveichev A.V., Ostrik A.V. 8 3D computer modeling of high-velocity impact phenomena King T.R., Shively J.H.  Nonlinear Hugoniots  47-50 'King�Jr. H.E.,  Cook R.L., Herbst C.A. C Density scaling of viscosity measured via diamond cell viscometry  1055-1058 3Kingma K.J.,  Hemley R.J.,  Veblen D.R., Mao H.-K. | Effect of processing induced microstructural bias of phase distribution on spall strength of two-phase TiB2-Al2O3 ceramics jKennedy J.,  Plaksin I.,  Thomas K.,  Martin E.,  Lee K.-Y.,  Akinci A.,  Asay B.,  Campos J., Direito J. 3 Instrumented Floret tests of detonation spreading  1500-1503 Kerley G.I. + Theoretical equations of state for metals 	 208-212 Kerley G.I., Switendick A.C. A Theory of molecular dissociation in shocked nitrogen and oxygen  95-100 Kerley G.I., Wise J.L. / Shock-induced vaporization of porous aluminum % Theory of calcite equation of state 	 613-616 - A new multiphase equation of state for iron *Kerr J.H.,  Christiansen E.L., Crews J.L. 6 Hydrocode modeling of advanced debris shield designs  1167-1170 $Kerr S.,  Kirkpatrick D., Garden S. F Measurement of particle velocity using a mutual inductance technique Kerrisk J.F., Meier J.K. < Comparisons between fast shock tube calculations and tests IKesler G.,  Karow H.U.,  Baumung K.,  Fortov V.E.,  Kanel G.I., Licht V. 4 High-power light ion beams and intense shock waves  1887-1890 Khantouleva T.A. = Non-local theory of high-rate processes in structured media T Nonlocal theory of macro-meso-level energy exchange in the shock compressed matter Khantuleva T.A. Q Shock waves propagation in scope of the nonlocal theory of dynamical plasticity %Khasainov B.,  Victorov S., Heuz� O. ^ A comparison of two approaches for fast and accurate hydrodynamic simulations of detonations 7Khasainov B.A.,  Kuhl A.L.,  Victorov S.B., Neuwald P. < Model of non-premixed combustion of aluminium-air mixtures 	 449-452 /Khishchenko K.V.,  Lomonosov I.V., Fortov V.E. U Equations of state for organic compounds over wide range of densities and pressures /Khishchenko K.V.,  Fortov V.E., Lomonosov I.V. I High temperature, high pressure equation of state for polymer materials ' The reshock and release waves in PTFE Karger N., L�demann H.-D. G Self diffusion in liquid hydrogen fluoride at pressures up to 600 MPa  1321-1324 6Karo A.M.,  Walker F.E.,  Cunningham W.G., Hardy J.R. y Theoretical studies of shock dynamics in two-dimensional structures V. Microscopic constraints on shock-induced signals  92-96 )Kaschner G.C.,  Gray�III G.T., Chen S.R. Q The influence of texture and impurities on the mechanical behavior of zirconium 9Kasiraj P.,  Vreeland�Jr. T.,  Schwarz R.B., Ahrens T.J. < Mechanical properties of a shock consolidated steel powder >Katayama Y.,  Koyama N.,  Tsuji K.,  Oyanagi H., Shimomura O. 7 EXAFS study of isolated selenium chain under pressure 	 477-480 "Katayama Y.,  Koyama N., Tsuji K. ? Optical absorption of isolated selenium chains under pressure RKawai N.,  Atou T.,  Ito S.,  Yubuta K.,  Kikuchi M.,  Nakamura K.G., Kondo K.-I. M The amorphization and disproportionation of mullite under shock compression 	 248-251 2Keck J.D.,  Hamkey D.L.,  Graham R.A., Morosin B. e Shock-induced chemical and structural modification of zirconia, lead oxide and their mixed products  82-86 Keller C.E. 7 Utility of shock models for underground nuclear tests 	 485-487 Keller A.R., Zhou M. Z Experimental characterization of the dynamic failure resistance of TiB2/Al2O3 composites 	 795-798 (Kelley J.M.,  Joshi V.S., Guirguis R.H. 5 Mechanical behavior of explosives at high pressures 	 864-867 MKennedy J.E.,  Lee K.-Y.,  Son S.F.,  Martin E.S.,  Asay B.W., Skidmore C.B. > Second-harmonic generation and the shock sensitivity of TATB =Kennedy G.,  Ferranti L.,  Russell R.,  Zhou M., Thadhani N. u Influence of microstructural bias on the Hugoniot elastic limit and spall strength of two-phase TiB2+Al2O3 ceramics (Kennedy G.,  Ferranti L., Thadhani N.N. S Estimation of the spall fracture kinetics from the free-surface velocity profiles 5Kanel G.I.,  Razorenov S.V.,  Utkin A.V., Grady D.E. 7 The spall strength of metals at elevated temperatures 	 503-506 KKanel G.I.,  Baumung K.,  Rush D.,  Singer J.,  Razorenov S.V., Utkin A.V. / Melting of shock compressed metals in release 	 155-158 ^Kanel G.I.,  Razorenov S.V.,  Utkin A.V.,  Dudin S.N.,  Mintsev V.B.,  Bless S., Simha C.H.M. T Investigation of mechanical properties of ceramics using axi-symmetric shock waves �Kanel G.I.,  Fortov V.E.,  Khishchenko K.V.,  Utkin A.V.,  Razorenov S.V.,  Lomonosov I.V.,  Mehlhorn T.,  Asay J.R., Chhabildas L.C. a Thin foil acceleration method for measuring the unloading isentropes of shock-compressed matter 3Kanel G.I.,  Razorenov S.V.,  Baumung K., Bluhm H. � Anomalous behavior of aluminum near the melting temperature: Transition in the rate controlling mechanism of yielding and realization of superheated solid states under tension RKanel G.I.,  Bogach A.A.,  Razorenov S.V.,  Savinykh A.S.,  Chen Z., Rajendran A. = A study of the failure wave phenomenon in brittle materials Kanel G.I. + Failure waves in shock-compressed glasses 	 870-875 DKanel G.I.,  Razorenov S.V.,  Savinykh A.S.,  Rajendran A., Chen Z. R A study of failure wave phenomenon on glasses at peak stresses exceeding the HEL 	 876-879 ;Kaneshige M.J.,  Renlund A.M.,  Schmitt R.G., Erikson W.W. N Development of scalable cook-off models using real-time in situ measurements Kani K.,  Yamada T., Abe M. F Hugoniot and electric resistivity measurements on amorphous<   selenium 3Kanomata T.,  Kawashima T.,  Yoshide H., Kaneko T. G Pressure effect on the Curie temperatures of MnRuAs, MnPdAs and MnRhP  1469-1472 2Kanzleiter R.,  Atchison W.,  Bowers R., Guzik J. T Simulated, theoretical and experimental shock trajectories in cylindrical geometry #Karakhanov S.M., Bordzilovsky S.A.  1193-1197 �Kalantar D.H.,  Allen A.M.,  Gregori F.,  Kad B.,  Kumar M.,  Lorenz K.T.,  Loveridge A.,  Meyers M.A.,  Pollaine S.,  Remington B.A., Wark J.S. D Laser driven high pressure, high strain-rate materials experiments �Kalantar D.H.,  Collins G.W.,  Colvin J.D.,  Davies H.M.,  Eggert J.H.,  Hawreliak J.,  Lorenzana H.E.,  Meyers M.A.,  Rosolankova K.,  Schneidler M.S.,  Sheppard J.,  St�lken J.S., Wark J.S. I Direct observation of the a-e transition in shocked single crystal iron 	 240-243 *Kalpana G.,  Palanivel B., Rajagopalan M. F Band structure and superconductivity of bcc tellurium under pressure 	 673-676 Kamegai M. I Numerical analysis of Hopkinson bar experiments on dislocation dynamics )Kamegai M.,  Klein L.S., Rosenkilde C.E. a Computer simulation of the effect of free surface reflection on shock wave propagation in water &Kamegai M.,  Walton O.R., Taylor A.G. P Micro-scale simulation of dynamic compaction of oxide and metal powder mixture 
Kamm J.R. P A simple hydrodynamic model for jetting from tubular hypervelocity penetrators  1825-1828 Kandasamy R., Brar N.S. N Flow stress and material model study at high strain rate and low temperature  1031-1034 Kane J.O., Smith R.F. Q Modeling non-equilibrium phase transitions in isentropically compressed bismuth 	 244-247 1Kaneko T.,  Kanomata T.,  Kawashima T., Yasui H. L Pressure effect on the Curie temperature and exchange striction of YMn2Ge2  1473-1476 )Kanel G.I.,  Rasorenov S.V., Fortov V.E. D The failure waves and spallations in homogeneous brittle materials MKanel G.I.,  Razorenov S.V.,  Utkin A.V.,  Baumung K.,  Karow H.U., Licht V. 2 Spallations near the ultimate strength of solids  1043-1046 )Kanel G.I.,  Utkin A.V., Tolstikova Z.G. > Response of the high-filled elastomers to shock-wave loading  1123-1126 Kanel G.I., Utkin A.V. : Dynamic characterization of shape memory titanium alloys 	 581-584 Joshi V.S., Carney T.C. L Modeling of bullet penetration in explosively welded composite armor plate  1387-1390 8Jouet R.J.,  Granholm R.H.,  Sandusky H.W., Warren A.D. b Preparation and shock reactivity analysis of novel perfluoroalkyl-coated aluminum nanocomposites  1527-1530 Juanicotena A., Szarzynski S. G Investigation of dynamic friction induced by shock loading conditions Jung J.,  Jhung K.S., Kim I. P Helmholtz free energy equation of state applied to carbon at megabar pressures )Justus B.L.,  Huston A.L., Campillo A.J. F Temperature measurements of shocked water using a fluorescence probe *Justus B.L.,  Merritt C.D., Campillo A.J. O Efficient photogeneration of triplets in shock compressed 2,4-dinitrostilbene HJyoti G.,  Joshi K.D.,  Gupta S.C.,  Sikka S.K.,  Dey G.K., Banerjee S. K The orientation relations between the a and w phases of shocked zirconium 	 227-230 EJyoti G.,  Gupta S.C.,  Ahrens T.J.,  Kossakovski D., Beauchamp J.L. 7 Mass spectrometer calibration of cosmic dust analyzer 4Kadau K.,  Germann T.C.,  Lomdahl P.S., Holian B.L. f Shock-induced structural phase transformations studied by large-scale molecular-dynamics simulations BKadau K.,  Germann T.C.,  Lomdahl P.S.,  Holian B.L., Cherne F.J. : Atomistic simulations of shock-induced phase transitions 	 229-234 7 Atomistic simulation of shock-induced melting in iron 	 236-239 TKagi H.,  Wakatsuki M.,  Hayakawa S.,  Nakamura F.,  Gohshi Y.,  Kanda H., isoya J. x Characterization of trace nickel in synthetic diamond and its relationship to the abundance of substitutional nitrogen 5Kaiser M.A.,  Wilson L.T.,  Wicks A.L., Swantek S.D. / Experimental techniques for the Hopkinson bar cKalantar D.H.,  Remington B.A.,  Colvin J.D.,  Gold D.M.,  Mikaelian K.O.,  Weber S.V., Wiley L.G. + Shock compressed solids on the NOVA laser C Impact surface VISAR measurements in CdS shocked along the c-axis QJones H.D.,  Zerilli F.J.,  Holt W.H.,  Mock�Jr. W.,  Miller P.J., Lindfors A.J. ' Equation of state for porous mixtures ; Theoretical equation of state for water at high pressures = Equation of state for liquid nitromethane at high pressures Jordan J.L., Thadhani N.N. R Shock compaction and synthesis of the titanium-silicon ternary carbide (Ti3SiC2) Q Effect of shock-activation on post-shock reaction synthesis of ternary ceramics [Jordan J.L.,  Sekine T.,  Kobayashi T.,  Li X.,  Thadhani N.N.,  El-Raghy T., Barsoum M.W. ^ Hugoniot measurements of high pressure phase stability of titanium-silicon carbide (Ti3SiC2) aJordan J.L.,  Dick R.D.,  Ferranti L.,  Thadhani N.N.,  Austin R.A.,  McDowell D.L., Benson D.J. [ Equation of state of aluminum-iron oxide (Fe2O3)-epoxy composite: Modeling and experiment 	 157-160 2Joshi V.S.,  Grebe H.A.,  Thadhani N.N., Iqbal Z. E Effect of packing density on shock consolidation of diamond powders  1251-1253 (Joshi V.S.,  Thadhani N.N., Graham R.A. i Mechanistic study of shock-induced solid-state chemistry in Ti- and Ta-based carbide and boride systems  1299-1302 :Joshi V.S.,  Thadhani N.N.,  Graham R.A., Holman�Jr. G.T. : Shock compression of quartz and aluminum powder mixtures OJoshi K.D.,  Suresh N.,  Jyoti G.,  Kulshreshtha S.K.,  Gupta S.C., Sikka S.K. } Shock wave induced phase transitions from the trigonal phase to the coexisting amorphous and orthorhombic phases in a-FePO4 &Joshi V.S.,  Persson P.-A., Brower K. N Shock-induced grain burning in mixtures of ammonium	

 !"#$%&'()*+,-./0123456789:;<=>?@ABCDEG����HIJKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~� perchlorate and aluminum &Joshi V.S.,  Banks M.L., Krebsbach K. ? Explosive bonding of plates with diffusion barrier interfaces Joshi V.S., Lee R.J. s Resolving mechanical response of plastic bonded explosives at high strain rate using split Hopkinson pressure bar Joshi V.S., Imam M.A. e Interpretation of the stress histories from shock impact tests on snow using embedded stress gauges Johnson K.A., Medina W.J. P Shock compaction of high-temperature superconducting YBa2Cu3O7 ceramic powders 
Johnson J.D.  Carbon in detonations 	 697-704 SJohnson J.B.,  Brown J.A.,  Gaffney E.S.,  Blaisdell G.L.,  Sturm M., Barrett S.A.  Shock wave studies of snow 	 107-110 Johnson J.D., Shaw M.S. 1 The influence of a slow rate on detonation flow Johnson J.N., Tonks D.L. J Dynamic plasticity in transition from thermal activation to viscous drag 	 371-378 Johnson G.R., Holmquist T.J. D An improved computational constitutive model for brittle materials 7Johnson J.N.,  Hixson R.S.,  Tonks D.L., Gray�III G.T. 8 Shock compression and quasielastic release in tantalum A Micromechanical strength effects in shock compression of solids 2Johnson D.E.,  Lee L.M.,  Hedemann M.A., Bauer F. H PVDF measurement of soft X-ray induced shock and filter debris impulse  1911-1914 4Johnson J.N.,  Hixson R.S.,  Tonks D.L., Zurek A.K. 2 Rate-dependent spallation properties of tantalum *Johnson D.E.,  Davies F.W., Hedemann M.A. ] Characterization and reduction of prompt electrical noise on the Saturn PRS X-ray simulator ( The features of the principal Hugoniot Johnson J.N., Dick J.J.  Spallation studies in estane 9Johnson G.R.,  Stryk R.A.,  Beissel S.R., Holmquist T.J. n Conversion of finite elements into meshless particles for penetration computations involving ceramic targets  1287-1290 %Johnson J.N.,  Dolan D.H., Howe P.M. > EOS of mixtures: Phase transformation and explosive reaction 	Jonas J. 5 High pressure NMR studies of proteins and membranes Jones H.D. I Theoretical equation of state for liquid nitromethane at high pressures 	 103-106 Jones H.D., Zerilli F.J. # Analytic equation of state for H6 Jones S.D., Gupta Y.M. Jevais J.R., Zerah G. M A new fluid integral equation application to the equation of state of xenon 	 119-124 /Jhung K.S.,  Ki<  m I.H.,  Oh K.-H., Jhung K.H.C. 9 Universal description of energetics of condensed matter 	 329-332 #Jiang J.,  Goroshin S., Lee J.H.S. 6 Shock wave induced chemical reaction in Mn+S mixture 'Jiao T.,  Clifton R.J., Grunschel S.E. + High strain rate response of an elastomer Jin G. ( Shock Hugoniot measurement on tungsten @Jin X.,  Zhang H.,  Che R.,  Zhou L.,  Zhao Q.,  Liu J., Xiu L. K Isothermal equations of state for nanometer and micrometer nickel powders  99-102 KJin Z.Q.,  Chen K.H.,  Li J.,  Zeng H.,  Liu P.,  Wang Z.L., Thadhani N.N. E Shock compaction of exchange-coupled nanocomposite magnetic powders  1102-1105 EJin Z.Q.,  Li J.,  Thadhani N.N.,  Wang Z.L.,  Vedantam T., Liu J.P. ` Shock compression of FePt and FePt/Fe3Pt nanoparticles: Exchange-coupled nanocomposite magnets Jing F.-Q. & Shock wave physics research in China  33-44 $John R.,  Antoun T., Rajendran A.M. @ Effect of strain rate and size on tensile strength of concrete *John�Jr. H.J.,  Hudson�III F.E., Robbs R. : High strain rate testing of AP/Al/HTPB solid propellants John�Jr. H.J., Alamo M.F. 1 High strain rate testing of HMX-based explosive 
Johnson J.N. # Spallation by ductile void growth 	 438-441 1 Calculated shock pressures in the aquarium test 	 568-572 &Johnson J.D.,  Shaw M.S., Holian B.L.   Dense molecular thermodynamics  27-30 %Johnson M.L.,  Nicol M., Holmes N.C. : Molecular emission spectra from shock-decomposed benzene <Johnson K.A.,  Staudhammer K.P.,  Elliott N.E., Medina W.J. \ Strain and ambient temperature microstructural effects in shock loaded 304 stainless steel ) Hot-spot reaction in unsustained shocks (Johnson J.B.,  Brown J.A., Gaffney E.S. D Shock synthesis and processing of high temperature superconductors 	 575-578 -Itoh S.,  Natamitsu Y.,  Liu Z.Y., Fujita M. = On von Neumann reflection of shock wave in condensed matter 9Itoh S.,  Liu Z.,  Nakamura Y.,  Nagano S., Nadamitsu Y. i The irregular reflection from the symmetrical collision of two plane detonation waves in high explosive .Itskevich E.S.,  Voronovsky A.N., Dizhur E.M. ` Investigations of quasi-particle spectra using electron-topological transitions under pressure hIvanov D.S.,  Zhigilei L.V.,  Bringa E.M.,  De�Koning M.,  Remington B.A.,  Caturia M.J., Pollaine S.M. l Molecular dynamics simulations of shocks including electronic heat conduction and electron-phonon coupling 2Iyer K.R.,  Bennett L.S.,  Sorrell F.Y., Horie Y. 3 Solid state chemical reactions at the shock front Iyer K., Dandekar D. J Computational design study for recovery of shock damaged silicon carbide 	 866-869 Jackson I. I Viscoelastic relaxation in iron and the shear modulus of the Inner Core %James H.R.,  Cook M.D., Haskins P.J. W The effect of impact angle on the initiation threshold of bare and covered explosives 'James H.R.,  McElrue D.H., Winter R.E.  Recovery of uranium fragments  1302-1305 James H.R. O The role of tip geometry in the initiation of explosives by shaped charge jet 	 993-997 G Estimaton of two-dimensional initiation thresholds from pop plot data  1081-1084 aJarmakani H.,  McNaney J.M.,  Schneider M.S.,  Orlikowski D.,  Nguyen J.H.,  Kad B., Meyers M.A. R Dynamic response of copper subjected to quasi-isentropic, gas-gun driven loading 
Jayaraman A. 6 Recent developments in static high pressure research  13-36 Jeanloz R., Grover R. . Birch-Murnaghan and Us-up equations of state `Jensen B.J.,  Rigg P.A.,  Knudson M.D.,  Hixson R.S.,  Gray�III G.T.,  Sencer B.H., Cherne F.J. - Dynamic compression of iron single crystals 	 232-235 M Experimental study of laser shock-released states of iron into a LiF window )Huston A.L.,  Justus B.L., Campillo A.J. � Spectral shifts in the fluorescence of anthracene and lifetime changes in crystal violet under laser driven shock compression: Probes of pressure and viscosity 	 243-248 Hutchens G.J. 1 Approximate blast theory: Application to solids 	 442-445 Hwang M.,  Horie Y., You S. R Modeling of shock-induced chemical reactions in powder mixtures 1: The VIR model 7Hwang L.W.,  Schroeder J.,  Silvestri M.R., Zhao X.-S. N Optical effects in II-VI semiconductor nanocrystal colloids at high pressure Hyndman D.A., Gaffney E.S. 9 Calibration of PVDF transducers at stresses below 1 MPa 	 809-811 2Idar D.J.,  Peterson P.D.,  Scott P.D., Funk D.J. M Low strain rate compression measurements of PBXN-9, PBX 9501, and mock 9501 EIdar D.J.,  Straight J.W.,  Osborn M.A.,  Coulter W.L., Buntain G.A. * Low amplitude impact of damaged PBX 9501 �Idar D.J.,  Thompson D.G.,  Gray�III G.T.,  Blumenthal W.R.,  Cady C.M.,  Peterson P.D.,  Roemer E.L.,  Wright W.J., Jacquez B.L. n Influence of polymer molecular weight, temperature, and strain rate on the mechanical properties of PBX 9501 IIkazaki F.,  Kamiya K.,  Uchida K.,  Kawamura M.,  Gotoh A., Fujiwara S. B Shock modified silicon nitride and its sintering characteristics Ilkaev R.I.,  Fortov V.E.,  Bulannikov A.S.,  Burtsev V.V.,  Golubev V.A.,  Golubkov A.N.,  Davydov N.B.,  Zhernokletov M.V.,  Kirshanov S.I.,  Manachkin S.F.,  Medvedev A.B.,  Mikhaylov A.L.,  Mochalov M.A.,  Orlov V.D.,  Khrustalev V.V., Yaroshenko V.V. W Quasi-isentropic compressibility of gaseous deuterium in pressure range up to 300 GPa $Ionita A.,  Mas E.M., Clements B.E. C Two-scale FEM in the dynamic response of a heterogeneous material wIqbal Z.,  Thadhani N.N.,  Chawla N.,  Rao K.V.,  Skumryev S.,  Ramakrishna B.L.,  Sharma R.,  Eckhardt H., Owens F.J. Hu J.-B.,  Tan H., Jing F.-Q. - Shock-induced phase transition of bromoform Huan S., Ding J. 2 Probe for two-dimensional flow field measurement 	 593-595 Huan S.,  Yang W., Ding J. M Experimental calibration for the dynamic tensile coefficient of metal foils 	 361-364 Huan S.,  Lu F.-Y., Ding J. I Attenuation of two-dimensional axisymmetric shock waves in porous Al2O3 	 261-264 Huang Z.-P., Zhang H.-P. ( A study of electromagnetic stress gage 	 233-236 .Huang S.,  Ding F.,  Jing F.,  Dong Y., Li Z. < Dynamic quasi-isentropic compression of oxygen free copper Huang F.,  Bai C., Ding J. B Mechanical response of a composite propellant to dynamic loading 	 491-494 -Huang S.,  Jin X.,  Li Z.,  Wang X., Guan K. I Experimental measurements of 2169 stainless steel under dynamic loading Huang Y.K. < Notes on two general models for the inquiry of shock waves  Huang X.S.,  Ono M., Mashimo T. l Preparation of metastable alloy bulk material in Fe-Cu system by mechanical alloying and shock compression #Huang X.,  Kuramoto K., Mashimo T. c Nonequilibrium bulk material in W-Ag system prepared by mechanical alloying and shock compression Huang H., Asay J.R. C Compressive strength of shocked aluminum for stresses of 4-22 GPa 5Huang W.,  Patterson J.E.,  Lagutchev A., Dlott D.D. D Shock compression spectroscopy with high time and space resolution  1265-1270 Huang F., Zhang L. a DOP test evaluation of the ballistic performance of armor ceramics against long rod penetration  1383-1386 Hudson�III L.C. c Computational studies of sympathetic detonation between two axially adjacent, cased charges of H6 'Huffman A.R.,  Brown J.M., Carter N.L. K Temperature dependence of shock-induced microstructures in tectosilicates �Huser G.,  Benuzzi-Mounaix A.,  Koenig M.,  Faral B.,  Grandjouan N.,  Henry E.,  Vinci T.,  Batani D.,  Tomasini T.,  Telaro B., Guyot F. ] Wavelength shift of the ruby luminescence R-lines due to shock compression along the c-axis H�rz F. U Morphology and chemistry of projectile residue in small experimental impact craters 	 481-484 Hostler S.R., Brennen C.E. K Measurements and simulation of wave propagation in agitated granular beds Houser B., Ingalls R. = Pressure-induced transition in Rb.31WO3 as measured by XAFS &Howard W.M.,  Souers P.C., Fried L.E. C Kinetic calculations of explosives with slow-burning constituents &Howard W.M.,  Fried L.E., Souers P.C. - Modeling of non-ideal aluminized explosives <  5Howard W.M.,  Fried L.E.,  Souers P.C., Vitello P.A. d Calculation of chemical detonation waves with hydrodynamics and a thermochemical equation of state Howard W.M., Molitoris J.D. / Modeling propagation of shock waves in metals Howe P.M., Benson D.J. 9 Progress in the development of a shock initiation model ?Hoy D.E.P.,  Akaishi M.,  Park J.K.,  Horie Y., Whitfield J.K. . Shock compression of aluminum nitride powder Hrbek G.M. � Invariant functional forms for the second, third, and fourth order Birch-Murnaghan equation of state for materials subjected to hydrodynamic shock u Physical interpretation of mathematically invariant K(r,P) type equations of state for hydrodynamically driven flow ` Invariant functional forms for K(r,P) type equations of state for hydrodynamically driven flow "Hsieh A.J.,  Akkala S., Brar N.S. G High strain rate behavior of coextruded polycarbonate/PMMA composites Hsiung L.L. P On the micromechanisms of shock-induced martensitic transformation in tantalum 	 228-231 (Hu J.,  Mao H.-K.,  Shu J., Hemley R.J. X High-pressure energy dispersive X-ray diffraction technique with synchrotron radiation 	 441-444 9Hu B.-Y.,  Dong Q.-D.,  Han C.-S.,  Wang D.-S., Hu H.-B. I Microanalysis of adiabatic shear fracture in explosive-filled cylinders  1229-1132 ]Homae T.,  Okamoto A.,  Nakamura K.G.,  Kondo K.-I.,  Yoshida M.,  Hirabayashi K., Niwase K. � Cooling rate threshold in transformation of C60 fullerene to amorphous diamond and highly disordered carbon in SCARQ experiments ]Hongo T.,  Kawai N.,  Nakamura K.G.,  Atou T.,  Yubuta K.,  Kusaba K.,  Kikuchi M., Kondo K. < Phase transition of MnF2 by shock compression up to 33 GPa 	 224-227 &Hooks D.E.,  Dick J.J., Martinez A.R. 0 Shock experiments on explosive single crystals Hoover W.G., Moran B. 0 Dynamic and stress intensity in elastic strips ?Hoover W.G.,  Moran B.,  Holian B.L.,  Posch H.A., Bestiale S. 1 Computer simulation of nonequilibrium processes Hopkins A., Brar N.S. A Hugoniot and shear strength of titanium-6-4 under shock loading 	Horie Y. + Glass transition in shock loaded ceramics 	 315-319 C Some thermodynamical influences of defects in shock-loaded solids 	 369-373 >Horie Y.,  Hoy D.E.P.,  Simonsen I.,  Graham R.A., Morosin B. - Shock-wave synthesis of titanium aluminides 	 749-754 Horie Y., Kipp M.E. ] Modeling of chemical reactions in the mixture of Al-Ni powders under shock-wave compression : Shock compaction of ceramic powders in reactive mixtures 	 479-485 O Computational modeling of shock-induced chemical reactions in powder mixtures CHorie Y.,  Tang Z.P.,  Anderson M.U.,  Graham R.A., Sheffield S.A. S Discrete meso-element dynamic analysis of stress profiles in HMX explosive powder Horie Y., Yano K. L Nonequilibrium fluctuations in shock compression of polycrystalline a-iron +Horie Y.,  Hamate Y.,  Greening D., Dey T. p Reactive burn modeling of solid explosives with a statistical treatment of hot spots in two spatial dimensions $Horioka K.,  Aizawa T., Tsuchida M. X Ion-beam driven shock device using accelerated high density plasmoid by phased Z-pinch 	 993-996 Horn P., Gupta Y.M. #Holmes N.C.,  Nellis W.J., Ross M. . Sound velocities in shocked liquid deuterium QHolt W.H.,  Mock W.,  Soper W.G.,  Coffey C.S.,  Ramachandran V., Armstrong R.W. D Shear banding in titanium via reverse-ballistic impact experiments ( Shock Waves in Condensed Matter   1989 DHolt W.H.,  Mock�Jr. W.,  Clark J.B.,  Zerilli F.J., Armstrong R.W. s Gas-gun reverse ballistic impact deformation and fracture of armco iron Taylor specimens of differing grain sizes  1193-1196 CHolt W.H.,  Mock�Jr. W.,  Anderson M.U.,  Holman G.T., Graham R.A. � Effect of particle morphology on input and propagated stress wave profiles for two highly porous polytetrafluoroethylene powders 2Holt W.H.,  Wilson L.T.,  Mock�Jr. W., Simpson B. 9 Dynamic properties of a shock loaded tungsten composite 4Holt W.H.,  Mock�Jr. W.,  Santiago F., Gamache R.M. H Experiment to capture gaseous products from shock-decomposed materials  1196-1199 (Holt W.H.,  Mock�Jr. W., Armstrong R.W. M Crystal structure effects on surface fractures of impacted superalloy cubes �Holtkamp D.B.,  Clark D.A.,  Crain M.D.,  Furnish M.D.,  Gallegos C.H.,  Garcia L.A.,  Hammon D.L.,  Hemsing W.F.,  Shinas M.A., Thomas K.A. ? Development of a non-radiographic spall and damage diagnostic <Holtkamp D.B.,  Clark D.A.,  Ferm E.N.,  Gallegos R.A.,  Hammon D.,  Hemsing W.F.,  Hogan C.E.,  Holmes V.H.,  King N.S.P.,  Liljestrand R.,  Lopez R.P.,  Merrill F.E.,  Morris C.L.,  Morley K.B.,  Murray M.M.,  Pazuchanics P.D.,  Prestridge K.P.,  Quintana J.P.,  Saunders A.,  Schafer T.,  Shinas M.A., Stacy H.L. a A survey of high explosive-induced damage and spall in selected metals using proton radiography 	 477-482  Holtz M.,  Sauncy T., Zallen R. 8 Pressure-Raman studies of implantation disordered GaAs &Holtz M.,  Solin S.A., Pinnavaia T.J. > Pressure-Raman studies of layered alumino-silicate compounds  1539-1542 G Spall wave-profile and shock-recovery experiments on depleted uranium EHixson R.S.,  Vorthman J.E.,  Zurek A.K.,  Anderson W.W., Tonks D.L. # Spall response of U-Nb (6%) alloy HHixson R.S.,  Gray�III G.T.,  Rigg P.A.,  Addessio L.B., Yablinsky C.A. 6 Dynamic damage investigations using triangular waves 	 469-472 Hoffman N.M., Swift D.C. b Predictions of the microstructural contribution to instability seeding in beryllium ICF capsules ;Hokamoto K.,  Fujita M.,  Tanaka S.-I.,  Ayabe M., Itoh S. d Possibility of making polycrystalline diamond using high-temperature shock consolidation technique Holian B.L. 7 Modeling shockwave deformation via molecular dynamics Holian K.S. 0 Hydrocode simulations of hypervelocity impacts P Shockwave-induced plasticity via large-scale nonequilibrium molecular dynamics 	 173-177 GHolian B.L.,  Germann T.C.,  Lomdahl P.S.,  Hammerberg J.E., Ravelo R. ? Shock waves and their aftermath: A view from the atomic scale  35-41 =Holland K.G.,  Chhabildas L.C.,  Reinhart W.D., Furnish M.D. - Experiments on CERCOM SiC rods under impact -Holman�Jr. G.T.,  Graham R.A., Anderson M.U. 6 Shock response of porous 2Al + Fe2O3 powder mixtures FHolmes N.C.,  Trainor R.J.,  Anderson R.A.,  Veeser L.R., Reeves G.A. 9 Impedance-match experiments using high intensity lasers 	 160-163 Holmes N.C. H High energy laser facilities at Lawrence Livermore National Laboratory 	 648-651 GHolmes N.C.,  Mitchell A.C.,  Nellis W.J.,  Graham W.B., Walrafen G.E. % Raman spectroscopy of shocked water 	 307-308 Holmes B.S. , Measuring pressure from short laser pulses 7Holmes N.C.,  Nellis W.J.,  Graham W.B., Walrafen G.E. 	 191-200 Holmes B.S., Aidun J.B. 6 Piezoresistant response of vapor-deposited ytterbium 	 519-524 Holmes N.C., See E.F. : Shock compression of low-density microcellular materials ( Shock compression of low-density foams R Shock recovery experiments on sandstone under dry and water-saturated conditions  1251-1254 Hirai H., Kondo K.-I. O Amorphous diamond from C60 fullerene by shock compression and rapid quenching Hirai H., Kondo K. ~ A wide variety of carbon behavior: Amorphous diamond fabricated from C60 fullerence by shock compression and rapid quenching 	 675-680 IHiroe T.,  Matsuo H.,  Fujiwara K.,  Tanoue T.,  Yoshide M., Fujiwara S. N A production of cylindrical imploding shocks in solid by exploding wire rows  1667-1670 QHiroe T.,  Matsuo H.,  Fujiwara K.,  Sakai S.,  Abe T.,  Yoshida M., Fujiwara S. L Generation of cylindrical imploding shocks in solid using a high explosive ,Hiroe T.,  Fujiwara K.,  Abe T., Yoshida M. N Rapid expansion and fracture of metallic cylinders driven by explosive loads 	 465-468 !Hironaka Y.,  Nicol M., Kondo K. , Shock induced polarization in some liquids [Hironaka Y.,  Saito F.,  Yazaki A.,  Fujimoto Y.,  Nakamura K.G.,  Kondo K.-I., Yoshida M. M Pump-probe X-ray diffractio<  n for condensed matter in picosecond time domain @Hironaka Y.,  Saito F.,  Yazaki A.,  Nakamura K.G., Kondo K.-I. J Picosecond time-resolved X-ray diffraction: Estimation of local pressure +Hirosaki Y.,  Murata K.,  Kato Y., Itoh S. G Effect of void size on the detonation pressure of emulsion explosives 	 930-933 6Hixson R.S.,  Bellamy P.M.,  Duvall G.E., Wilson C.R. : Effect of shock waves on the absorption spectrum of ruby 	 282-286 Hixson R.S., Fritz J.N.  Shock compression of iron  69-70 'Hixson R.S.,  McQueen R.G., Fritz J.N. K The shock Hugoniot of 316 stainless steel and sound velocity measurements 	 105-108 7Hixson R.S.,  Johnson J.N.,  Gray�III G.T., Price J.D. I Effects of interfacial bonding on spallation in metal-matrix composites 	 555-558 UHixson R.S.,  Vorthman J.E.,  Gustvsen R.L.,  Zurek A.K.,  Thissell W.R., Tonks D.L. [ A new temperature-dependent equation of state for inert, reactive and composite materials 	Heuz� O. D A complete equation of state for detonation products in hydrocodes 	 450-453 @Heuz� O.,  Martinez E.,  Szarzynski S.,  Mulford R., Swift D.C. ? Reactive flow in nitromethane using the CW2 equation of state X Building of equations of state with numerous phase transitions: Application to bismuth 	 212-215 (Hicks D.L.,  Norwood F.R., Trucano T.G. 0 TOODY-WONDY calculations of penetration events 	 544-547 BHiggins A.J.,  Jett� F.X.,  Yoshinaka A.C.,  Lee J.H.S., Zhang F. 7 Detonation initiation in preshocked liquid explosives  1023-1026 Hild F., Denoual C. G A probabilistic model for the dynamic fragmentation of brittle solids Hilfi H., Brar N.S. c Evaluation of Johnson-Cook model constants for aluminum based particulate metal matrix composites >Hill L.G.,  Seitz W.L.,  Kramer J.F.,  Murk D.M., Medina R.S. E Wedge test data for three new explosives: LAX112, 2,4-DNI, and TNAZ 1Hill L.G.,  Seitz W.L.,  Forest C.A., Harry H.H. F High explosive corner turning performance and the LANL mushroom test 	 751-754 =Hill L.G.,  Bdzil J.B.,  Davis W.C.,  Engelke R., Frost D.L. i Front curvature analysis and detonation shock dynamics calibration for pure and sensitized nitromethane 	 813-816 
Hill L.G. ' Development of the LANL sandwich test Hill L.G., Aslam T.D. Q The LANL detonation-confinement test: Prototyope development and sample results K Burning crack networks and combustion bootstrapping in cookoff explosions Hiltl M., Nahme H. _ Macro- and micromechanical response of a shock-loaded glass-ceramic at different temperatures Hiltl M., Hornemann U. t Structural deformations on fluorophlogopite crystals of a pre-heated and experimentally shocked mica glass-ceramic BHiltl M.,  Swift R.P.,  Hagelberg C.R.,  Carney T.C., Nellis W.J. SHenson B.F.,  Smilowitz L.,  Asay B.W.,  Romero J.J.,  Oschwald D.M., Dickson P.M. M Measurement of the specific area of HMX and PBX 9501 by physical adsorption AHenson B.G.,  Smilowitz L.,  Romero J.,  Asay B.W., Dickson P.M. [ Measurement of temperature and ignition time during fast compression and flow in PBX 9501 *Herbold E.B.,  Nesterenko V.F., Daraio C. � Influence of controlled viscous dissipation on the propagation of strongly nonlinear waves in stainless steel based phononic crystals  1523-1526 Hereil P.L., Doubax F. A Shock induced polymorphic phase transition in a low-alloy steel (Hereil P.L.,  Lassalle F., Avrillaud G. W GEPI: An ICE generator for dynamic material characterisation and hypervelocity impact H�reil P.-L., Mabire C. 8 Temperature measurement of TiN under shock compression  1235-1238 Herrmann W. 3 On constitutive modelling for the shock physicist 	 346-359 8 Elastic-plastic constitutive equations at large strain KHerrmann B.,  Venkert A.,  Kimmel G.,  Landau A.,  Shvarts D., Zaretsky E. U Formation and morphology of twinning in titanium under high strain rate deformation @Herrmann B.,  Landau A.,  Shvarts D.,  Favorsky V., Zaretsky E. V Modeling of uranium alloy response in plane impact and reverse ballistic experiments  1306-1309 AHerrmann B.,  Venkert A.,  Favorsky V.,  Shvarts D., Zaretsky E. A U-0.75Ti and Ti6Al4V in planar and ballistic impact experiments 4Herrmann B.,  Favorsky V.,  Zaretsky E., Shvarts D. l Critical plastic strain as a criterion for failure in ballistic impact experiments of U/Ti and Ti64 alloys )Hertel E.S.,  Chhabildas L.C., Hill S.A. # Whipple bumper shield simulations !Hertel�Jr. E.S., Chhabildas L.C. ` Projectile shape influence on ballistic limit curves as determined by computational simulation  1179-1182 $Heuz� O.,  Goutelle J.C., Baudin G. #Hebert D.,  Bertron I., Garnier H. [ Mie-Gr�neisen EOS based on second order Birch-Murnaghan isotherm and Steinberg parameters Held M. < Critical area for the initiation of high explosive charges 	 555-557  Fragment generators @ Profile of detonation front by longitudinal gaps in HE charges 	 667-670 \ Analytical initiation criteria of high explosives at different projectile or jet densities 3Hellman J.R.,  Kuroda K.,  Heuer A.H., Graham R.A. E Microstructural characterization of shock-modified zirconia powders Hemley R.J., Mao H.K. . Static compression to multimegabar pressures  27-38 Hemley R.J., Mao H.-K. . New findings in static high-pressure science  17-26 IHemsing W.F.,  Mathews A.R.,  Warnes R.H.,  George M.J., Whittemore G.R. $ VISAR: Line imaging interferometer ,Henninger R.J.,  Maudlin P.J., Harstad E.N. : Differential sensitivity theory applied to the MESA code  1781-1784 X Differential sensitivity theory applied to the MESA2D code for multi-material problems -Henninger R.J.,  Maudlin P.J., Rightley M.L. I Accuracy of differential sensitivity for one-dimensional shock problems Henninger R.J., Maudlin P.J. : Code differentiation for hydrodynamic model optimization Henninger R.J. 0 Sensitivities for Taylor test model parameters 'Henrie B.L.,  Mason T.A., Bingert J.F. b Investigating incipiently spalled tantalum through multiple section planes and serial sectioning 0Hensel F.,  Hohl G.F.,  Pilgrim W.C., Winter R. U Metal-nonmetal transition and the dynamic structure factor of expanded fluid metals @Henson B.F.,  Funk D.J.,  Dickson P.M.,  Fugard C.S., Asay B.W. M Surface temperature measurements of heterogeneous explosives by IR emission 7Henson B.F.,  Asay B.W.,  Smilowitz L.B., Dickson P.M. @ Ignition chemistry in HMX from thermal explosion to detonation -Hayek M.,  Hasson A.,  Bransky I., Halevy D. d Derivation of the dynamics of an explosively driven ring from magnetically induced electric signal Hayek M., Luttwak G. " Mach stem formation in plexiglas Hayes D.B., Grady D.E. @ A thermal-viscous model for heterogeneous yielding in aluminum 	 412-416 &Hayes D.B.,  Kipp M.E., Nunziato J.W. K Application of mixture theory to shock initiation of porous HNS explosive %Hayes D.,  Hixson R.S., McQueen R.G. � High pressure elastic properties, solid-liquid phase boundary and liquid equation of state from release wave measurements in shock-loaded copper Hayes D., Hall C. Z Correcting free surface effects by integrating the equations of motion backward in space  1177-1180 UHayes D.B.,  Gray�III G.T.,  hixson R.S.,  Zurek A.K.,  Vorthman J.E., Anderson W.W. A Precursor suppression by shear stress relaxation in U-Nb(6-wt%) 4Hayes D.B.,  Gray�III G.T.,  Hall C.A., Hixson R.S. : Elastic-plastic behavior of U6Nb under ramp wave loading .He H.-L.,  Jin X.-G.,  Chen P.-X., Wang W.-K. ? Shock induced crystallization of metallic glass Fe40Ni40P12B8 	 625-627 He Y.-H., Ding J. ; The shape of detonation front and the detonation velocity  1365-1368 /He H.-L.,  Jin X.-G.,  Jing F.-Q., Ahrens T.J. A Characteristic of dynamic tensile fracture in augite-peridotite %He H.-L.,  Shi S.-C.,  Tan H., Xu K. 1 Shock compression of ZnO+a-Fe2O3 powder mixture 	 721-723  He H.,  kobayashi T., Sekine T. D Time-resolved measurement of the launch of laser-driven foil plate  1339-1342 ^He H.L.,  Boustie M.,  Arrigoni M.<  ,  de�Ress�guier T.,  Auroux E.,  Deleignies M., Gatulle M. K Hugoniot measurement of water from the impact of laser driven mini-flyers 6Hearne G.R.,  Sterer E.,  Pasternak M.P., Taylor R.D. o Pressure dependence of the electronic and magnetic properties of the layered antiferromagnetic insulator FeI2  1461-1464 Harvey W.B., McQueen R.G. ) Perturbations in high-velocity gas flow Haskins P.J., Cook M.D. 0 Short range interactions in diatomic molecules 	 113-118 K Many-body contributions to the short range potentials for helium and neon H The origin and computation of many-body forces in the repulsive region  67-70 : Monte Carlo simulation of 3-body effects in dense helium N Molecular dynamics studies of shock initiation in a model energetic material  1341-1344 S Molecular dynamics studies of thermal and shock initiation in energetic materials � Shock-induced reactions in energetic materials, studied by molecular dynamics with directly evaluated quantum mechanical potentials &Haskins P.J.,  Cook M.D., Briggs R.I. Q The effect of additives on the detonation characteristics of a liquid explosive 	 890-893 0Haskins P.J.,  Cook M.D.,  Flower H., Wood A.D. , Ab initio prediction of impact sensitivity 
Hatano T. S Temperature dependence of shock-induced plasticity: A molecular dynamics approach Hatt D.J., Waschl J.A. & A study of laser-driven flyer plates  1221-1224 ?Hatton P.D.,  Crain J.,  Ackland G.J.,  Clark S.J., Piltz R.O. 5 Metastable structures of tetrahedral semiconductors 1Hatton P.D.,  Crain J.,  Kawamura H., Akahama Y. Q Comparative studies of rotating anode and synchrotron-based image plate systems  1699-1702 THawke R.S.,  Brooks A.L.,  Mitchell A.C.,  Fowler C.M.,  Peterson D.R., Shaner J.W. ) Railguns for equation-of-state research 	 179-183 Hawke R.S. ; Railgun development for EOS applications: A status report 	 643-648 �Hawreliak J.,  Rosolankova K.,  Belak J.F.,  Collins G.,  Colvin J.,  Davies H.M.,  Eggert J.H.,  Germann T.C.,  Holian B.,  Kalantar D.H.,  Kadau K.,  Lomdahl P.,  Lorenzana H.E.,  Sheppard J.,  St�lken J.S., Wark J.S. S Shock induced a-e phase change in iron: Analysis of MD simulations and experiment 	 220-223 < Optical extinction of sapphire shock-loaded to 250-260 GPa  1231-1234 gHare D.E.,  Reisman D.B.,  Garcia F.,  Green L.G.,  Forbes J.W.,  Furnish M.D.,  Hall C., Hickman R.J. . The isentrope of unreacted LX-04 to 170 kbar MHare D.E.,  Vandersall K.S.,  Garcia F.,  Davis J.-P.,  Hall C., Forbes J.W. Q Isentropic compression data on LX-04 explosive at 150�C using the Z accelerator  1315-1318 ]Harrach R.J.,  Lee Y.T.,  Trainor R.J.,  Holmes N.C.,  Rosen M.D.,  Banner D.L., Olness R.J. l Contrasts in one- and two-dimensional hydrocode calculations of laser-generated shockwaves in disk targets 	 164-168 %Harrach R.J.,  Sz�ke A., Howard W.M. + Inertial effects in laser-driven ablation 	 335-337 
Harrach D.J. a High pressure, energy and impulse loading of the wall in a 1 GJ laboratory microfusion facility lHarrigan J.J.,  Hung Y.-C.,  Tan P.J.,  Bourne N.K.,  Withers P.J.,  Reid S.R.,  Millett J.C.F., Milne A.M. / High-rate compaction of aluminium alloy foams  1519-1522 Harris P., Presles H.N. L Reflection of a laser-generated optical signal from a shock front in water 6Harris E.J.,  Salisbury D.A.,  Taylor P., Winter R.E. E Characterization of the SATURN air lens and its use in foam studies %Harris E.J.,  Taylor P., Winter R.E. C The response of polyurethane foam to explosively generated shocks 	 659-662 Harris E.J., Winter R.E. I Calculating the resistance of lateral manganin gauges in a steel matrix 'Harry H.H.,  Uher K.J., Hagelberg S.I. A The poly-rho test as a tool for screening explosive performance 	 977-980 +Harstad E.N.,  Maudlin P.J., McKirgan J.B. / Anisotropic failure modeling for HY-100 steel 'Harstad E.N.,  Addessio F.L., Zuo Q.H. 2 A strength model for materials with phase change 	 216-219 OHartman J.K.,  Wise J.L.,  Graham R.A.,  Johnson R.O.,  Clark G.E., Burns T.J. ? Microwave dielectric constant of shock-loaded lithium niobate ?Hammond R.I.,  Church P.D.,  Grief A.,  Proud W.G., Field J.E. Y Dependence of measured lateral stress on thickness of protective 'padding' around gauge (Hammond R.I.,  Winter R.E., Harris E.J. A Measurement of strength of EN3B mild steel using lateral gauges GHan C.-S.,  Liu G.-Z.,  Dong Y.-B.,  Feng J.-P.,  Wang D.-S., Hu H.-B. R Expansion movement and fracture of a cylindrical shell due to internal explosion 	 357-360 
Handley C.A. Z Lagrangian analysis of velocity gauge data to determine reaction rate histories in EDC37 %Hanfland M.,  Hemley R.J., Mao H.-K. Y Synchrotron infrared measurements of pressure-induced transformations in solid hydrogen 	 873-876 Hanson D.L., Matzen M.K. 0 Study of ion-beam driven shock waves in metals 7Hanson D.L.,  Struve K.W.,  Spielman R.B., Seaman J.F. r Application of piezoelectric stress gauges to the measurement of fast rise time multimegampere electric currents  1719-1722 �Hanson D.L.,  Asay J.R.,  Hall C.A.,  Knudson M.D.,  Bailey J.E.,  Fleming K.J.,  Johnston R.R.,  Clark B.F.,  Bernard M.A.,  Anderson W.W., Rothman S.D. - Progress on deuterium EOS measurements on Z _Hanson D.L.,  Johnston R.R.,  Knudson M.D.,  Asay J.R.,  Hall C.A.,  Bailey J.E., Hickman R.J. V Advanced cryogenic system capabilities for precision shock physics measurements on Z  1141-1144 0Harada T.,  Kanomata T.,  Yoshida H., Kaneko T. ? Pressure effect on transport properties of M3-xCoxGaC (x<0.3)  1441-1444 Hardy R.J., Karo A.M. 9 Stress and energy flux in the vicinity of a shock front 	 161-164 #Hardy R.J.,  Root S., Swanson D.R. 1 Continuum properties from molecular simulations 	 363-366 J Two dimensional continuum properties from molecular dynamics simulations #Hare D.E.,  Webb D.J., Holmes N.C. a Imaging shocked sapphire at 200-460 kbar: The effect of crystal orientation on optical emission /Hare D.E.,  Webb D.J.,  Lee S.-H., Holmes N.C. !Hambir S.A.,  Kim H., Dlott D.D. 9 Ultrafast dynamics of nanoshocks in molecular materials 	 945-950 +Hamilton D.C.,  Mitchell A.C., Nellis W.J. J Electrical conductivity measurements in shock compressed liquid nitrogen Hamilton D.C., Ree F.H. i Chemical equilibrium calculations for the high pressure and temperature dissociation of liquid nitrogen OHamilton D.C.,  Nellis W.J.,  Holmes N.C.,  Radousky H.B.,  Ree F.H., Nicol M. b Electrical conductivity and equation of state measurements on planetary fluids at high pressures  99-101 �Hammel B.A.,  Cauble R.,  Celliers P.,  DaSilva L.B.,  Dittrich T.R.,  Griswold D.,  Haan S.W.,  Holmes N.,  Landen O.L.,  Orzechowski T., Perry T.S. 8 Shock physics with the NOVA laser for ICF applications  1281-1285 Hammerberg J.E. = The Riemann problem for a model nonlinear elastic continuum 	 169-172 -Hammerberg J.E.,  Preston D.L., Wallace D.C. 4 A new model of rate dependent elastic-plastic flow )Hammerberg J.E.,  Holian B.L., Zhou S.J. 2 Studies of sliding friction in compressed copper Hammerberg J.E., Pepin J. 4 An analytic solution to a driven interface problem uHammerberg J.E.,  Kyrala G.A.,  Oro D.M.,  Fulton R.D.,  Anderson W.E.,  Obst A.W.,  Oona H.,  Stokes J., Wilke M.D. - A Pegasus dynamic liner friction experiment ,Hammerberg J.E.,  Germann T.C., Holian B.L.  Shock waves in dusty plasmas EHammerberg J.E.,  Ravelo R.,  Germann T.C.,  Kress J.D., Holian B.L. 1 Sliding friction at compressed Ta/Al interfaces *Hammerberg J.E.,  Ravelo B., Germann T.C. 4 High density sliding of Ta/Al and Al/Al interfaces 8Hammetter W.P.,  Hellman J.R.,  Graham R.A., Morosin B. X Energy release and transformation of shock-modified zirconia upon annealing to 1550 �C 4Hammetter W.F.,  Graham R.A.,  Morosin B., Horie Y. g Effects of shock modificatio<  n on the self-propagating high temperature synthesis of nickel aluminides 	 431-434 8 On the shock discontinuities in titanium and zirconium 	 131-134 BHaberman K.S.,  Bennett J.G.,  Asay B.W.,  Henson B.F., Funk D.J. c Modeling, simulation and experimental verification of constitutive models for energetic materials Hablot O., Soulard L. % Shock decomposition of nitromethane 	 857-860 cHackenberg R.,  Swift D.,  Bourne N.,  Gray�III G.T.,  Paisley D.,  Thoma D.,  Cooley J., Hauer A. . Dynamic properties of nickel-titanium alloys PHagelberg C.R.,  Swift R.P.,  Carney T.C.,  Greening D.,  Hiltl M., Nellis W.J. 2 Modeling shock recovery experiments of sandstone  1275-1278 +Hall C.A.,  Chhabildas L.C., Reinhart W.D. h Shock Hugoniot and release states in concrete mixtures with different aggregate sizes form 3 to 23 GPa qHall C.A.,  Asay J.R.,  Trott W.M.,  Knudson M.,  Fleming K.J.,  Bernard M.A.,  Clark B.F.,  Hauer A., Kyrala G. < Aluminum Hugoniot measurements on the Sandia Z accelerator  1171-1174 WHall C.A.,  Asay J.R.,  Knudson M.D.,  Hayes D.B.,  Lemke R.L.,  Davis J.P., Deeney C. _ Recent advances in quasi-isentropic compression experiments (ICE) on the Sandia Z accelerator  1163-1168 uHall C.A.,  Baer M.R.,  Gustavsen R.L.,  Hooks D.E.,  Orler E.B.,  Dattelbaum D.M.,  Sheffield S.A., Sutherland G.T. J A study of polymer materials subjected to isentropic compression loading  1311-1314  Hamashima H.,  Kato Y., Itoh S. 9 Determination of JWL parameters for non-ideal explosive Hamate Y., Horie Y. M A statistical approach on mechanistic modeling of high-explosive detonation ? Development of a mechanistic burn modeling of high explosives [Hamaya N.,  Sakamoto Y.,  Fujihisa H.,  Fujii Y.,  Takemura K.,  Kikegawa T., Shimomura O. : Rietveld analysis of high pressure phase of praseodymium 1Hambir S.A.,  Franken J.,  Hill J.R., Dlott D.D. W Ultrafast vibrational spectroscopy of shocks in molecular materials: The first 100 ps "Gupta S.C.,  Ahrens T.J., Yang W. ; Shock induced vaporization of anhydrite CaSO4 and calcite  1259-1262 $Gupta S.C.,  Love S.G., Ahrens T.J. L Shock temperatures in calcite: Implication for shock induced decomposition a The coupling between shock waves and condensed matter: Continuum mechanics to quantum mechanics Gustavsen R.L., Sheffield S.A. 6 Unreacted Hugoniots for porous and liquid explosives ,Gustavsen R.L.,  Sheffield S.A., Alcon R.R. R Response of inclined electromagnetic particle velocity gauges in shocked liquids  1703-1706 ` Low pressure shock initiation of porous HMX for two grain size distributions and two densities 2 Detonation wave profiles in HMX based explosives cGustavsen R.L.,  Sheffield S.A.,  Alcon R.R.,  Hill L.G.,  Winter R.E.,  Salisbury D.A., Taylor P. V Initiation of EDC-37 measured with embedded electromagnetic particle velocity gauges WGustavsen R.L.,  Sheffield S.A.,  Alcon R.R.,  Winter R.E.,  Taylor P., Salisbury D.A. ; Double shock initiation of the HMX based explosive EDC-37 TGustavsen R.L.,  Sheffield S.A.,  Alcon R.R.,  Forbes J.W.,  Tarver C.M., Garcia F. ~ Embedded electromagnetic gauge measurements and modeling of shock initiation in the TATB based explosives LX-17 and PBX 9502 v Shock initiation of 'virgin' and 'recycled' PBX 9502 measured with embedded electromagnetic particle velocity gauges pGustavsen R.L.,  Dattelbaum D.M.,  Orler E.B.,  Hooks D.E.,  Alcon R.R.,  Sheffield S.A.,  Hall C.E., Baer M.R. \ Isentropic compression of nitroplasticized estane to about 35 kbar on the Sandia Z-Machine *Gustavson P.K.,  Tasker D.G., Forbes J.W. ; Underwater shock wave measurements using PVDF transducers 	 905-908 Gutkin M.Y., Ovidko I.A. > Rotational effect and amorphization in shock loaded crystals 	 401-404 <Gyanchandani J.S.,  Gupta S.C.,  Sikka S.K., Chidambaram R. 0 On the valence transition in shocked ytterbium Guirguis R.H., Landsberg A.M.  Convective detonations 	 926-929 Guirguis R.H., Kelley J.M. 7 Role of radiation in surface burning of melt cast TNT Guirguis R.H., Joshi V.S. @ An ignition model for liquid-solid powder hypergolic reactions 2Gump J.C.,  Wong C.P.,  Zerilli F.J., Peiris S.M. 8 High-pressure structural study of epsilon HNIW (CL-20) !Gump J.,  Parker L., Peiris S.M. U HMX (beta phase): Laser-ignited reaction kinetics and isothermal equations of state 	 967-972 Gump J.C., Peiris S.M. C Comparison of reaction kinetics of I-RDX and RDX at high pressure  1069-1072 #Gupta Y.M.,  Murri W.J., Henley D. H Large amplitude compression and shear wave propagation in an elastomer Gupta Y.M., Murri W.J. 5 Piezoelectric shear stress gage for dynamic loading Gupta Y.M. 2 Analysis and modeling of piezoresistive response Gupta S.C., Gupta Y.M. T Response of ytterbium foils oriented parallel and perpendicular to the shock front 	 237-238 D Piezoelectric response of manganin foils: Experiments and analysis 	 509-511 F Piezoresistance response of manganin foils: Experiments and analysis ( Shock waves in condensed matter - 1985 
 Y. Gupta %Gupta S.C.,  Gupta Y.M., Williams M. C Piezoresistance response of ytterbium foils in shocked liquid CS2 	 601-603 � Progress in understanding shock deformation in condensed materials at the atomic/molecular level: Recent experimental developments  15-26 Gupta S.C. P Band structure calculations to predict phase transformations at high pressures 	 157-163 nGupta S.C.,  Agarwal R.G.,  Gyanchandani J.S.,  Roy S.,  Suresh N.,  Sikka S.K.,  Kakodkar A., Chidambaram R. / A single stage gas gun for shock wave studies #Gupta S.C.,  Suresh N., Sikka S.K. 3 On 5f band occupation in shock compressed thorium ^ Shock wave experiments at different length scales: Recent achievements and future challenges �Gryaznov V.K.,  Kulish M.,  Mintsev V.B.,  Fortov V.E.,  Sharkov B.,  Golubev A.,  Fertman A.,  Mescheryakov N.,  Hoffmann D.H.H.,  Stetter M.,  St�cki C., Gardes D. @ About masurements of stopping power behind intense shock waves 	 879-882 Grzegory I. E Crystal growth of III-N semiconductors under high nitrogen pressure 	 561-564 PGrzegory I.,  Krukowski S.,  Jun J.,  Bockowski M.,  Wroblewski M., Porowski S. : Stability of indium nitride at N2 pressure up to 20 kbar Gu G., Vohra Y.K. 6 Mo-Re and Ti-V alloys at extreme static compressions 	 473-476 Gu Z., Jin X. = Temperature dependence on shock response of stainless steel ,Gu Y.-B.,  Nesterenko V.F., Indrakanti S.S. X Ballistic testing and high-strain-rate properties of hot isostatically pressed Ti6Al4V  1294-1297 #Gu Y.-B.,  Nesterenko V.F., Cai J. W Shear localization and patterning of shear bands in PTFE and its mixtures with metals RGudarenko L.F.,  Gushchina O.N.,  Zhernokletov M.V.,  Medvedev A.B., Simakov G.V. W Shock compression and isentropic expansion of tungsten, nickel and tin porous samples Gudarenko L.F., Kudelkin V.G. e Construction of wide-range equations of state through 'merging' local equations using mixture model 	 127-130 Gu�ry J.F. T Damage models with intermediate configuration large strain formulation and results  1157-1160 Gu�ry J.-F., Seaman L. ; Simulations of microfractures in solid rocket propellants Guirguis R.H., Oran E.S. K Numerical studies of laser-induced shock structure in condensed materials 	 351-352 Guirguis R. , Munroe/channel effect and weak detonations Guirguis R.H.  1-D detonability 	 377-380 ( Energy release in non-ideal explosives 	 381-384 $Guirguis R.,  McKeown R., Kelley J. M A closed water-filled cylinder test for characterizing non-ideal explosives 	 871-874 # Ignition due to macroscopic shear 3Grignon F.,  Benson D.,  Vecchio K.S., Meyers M.A. S Explosive welding of aluminum to aluminum: Analysis, computations and experiments  1098-1101 cGrigsby W.,  Bowes B.T.,  Dalton D.A.,  Bless S.,  Downer M.C.,  Taleff E.,  Colvin J., Ditmire T. I Diagnosis of Mbar laser produced shocks in tin using short pulse probes  1337-1340 -Grinfeld M.A.,  Schoenfeld S.E., Wri<  ght T.W. K Failure fronts in brittle materials and their morphological instabilities 	 858-861  Grote D.L.,  Park S.W., Zhou M. J An experimental characterization of the dynamic impact failure of mortar  1271-1274 Grove D.J., Rajendran A.M. 8 Simulation of flyer plate-rod target impact experiment 0Grove D.J.,  Rajrendran A.M., Dietenberger M.A. : Numerical simulation of a double flyer impact experiment 	 365-368 Grove J.W. 5 Irregular shock refractions at a material interface 3Grove D.J.,  Rajendran A.M.,  Bar-On E., Brar N.S. # Damage evolution in a ceramic rod e Modeling of Kipp-Grady plate impact experiments on ceramics using the Rajendran-Grove ceramic model Grove D.J., Rajrendran A.M. V Effects of pulverized material strength on penetration resistance of ceramic targets Q A comparison between scalar and multi-plane microcracking ceramic damage models J Modeling of microcrack density based on damage evolution in ceramic rods Grover R.W. , Why linear Birch and Us-up expansions work 	 139-142 Grover R.,  Ree F., Holmes N. 3 Equation-of-state from SiO2-aerogel Hugoniot data zGrun J.,  Manka C.K.,  Hoffman C.A.,  Meyer J.R.,  Glembocki O.J.,  Qadri S.B.,  Skelton E.F.,  Donnelly D., Covington B. ; Athermal annealing of neutron-transmutation-doped silicon 	 981-984 Gruzdkov Y.A., Gupta Y.M. F Mechanism of chemical decomposition in a shocked condensed explosive 	 813-818 &Gruzdkov Y.A.,  Gupta Y.M., Dick J.J. G Time-resolved absorption spectroscopy in shocked PETN single crystals 	 461-464 �Gray�III G.T.,  Cerreta E.,  Yablinsky C.A.,  Addessio L.B.,  Henrie B.L.,  Sencer B.H.,  Burkett M.,  Maudlin P.J.,  Maloy S.A.,  Trujillo C.P., Lopez M.F. � Influence of shock prestraining and grain size on the dynamic-tensile-extrusion response of copper: Experiments and simulation Grebenkin K.F. # Semiconductor model of detonation 	 982-985 >Grebyonkin K.F.,  Zherebtsov A.I.,  Popova V.V., Taranik M.V. 5 P,V,E,T equation of state for TATB-based explosives (Greeff G.W.,  Trinkle D.R., Albers R.C. D Alpha-omega transition in titanium: Equation of state and kinetics DGreeff C.W.,  Rigg P.A.,  Knudson M.D.,  Hixson R.S., Gray�III G.T. > Modeling dynamic phase transitions in titanium and zirconium 	 209-212 6Greeff C.W.,  Graf M.J.,  Boettger J.C., Johnson J.D. 0 High accuracy equations of state for standards  89-94 1Green L.G.,  Lee E.L.,  Breithaupt D., Walton J. 3 The equation of state of PETN detonation products 	 507-510 EGreenaway M.W.,  Gifford M.J.,  Proud W.G.,  Field J.E., Goveas S.G. X An investigation into the initiation of hexanitrostilbene by laser-driven flyer plates Greenaway M.W., Field J.E. 0 The development of a laser-driven flyer system (Greenaway M.W.,  Laity P.R., Pelikan V. L X-ray microtomography of sugar and HMX granular beds undergoing compaction Greene R.G., Ruoff A.L. < Optical effects of fine ceramic powder in solidified gases !Greene R.G.,  Luo H., Ruoff A.L. 0 High pressure Raman and EDXD study of diaspore  1535-1538 +Greenfield S.R.,  Swift D.C., Koskelo A.C. 9 Transient interferometric studies of shocked bicrystals  1269-1272 Greening D.R., Koskelo A. 2 Calculation of grain boundary shock interactions YGreenwood D.,  Forbes J.,  Garcia F.,  Vandersall K.,  Urtiew P.,  Green L., Erickson L. B Improvements in the signal fidelity of the manganin stress gauge  1157-1159 %Gran J.K.,  Holmes B.S., Curran D.R. B Measurement of explosive blast loads with flatpack stress gauges Granholm R.H., Sandusky H.W. 6 Small-scale shock reactivity and internal blast test Grantham S.G., Proud W.G. ) Digital speckle X-ray flash photography 	 803-806 'Grantham S.G.,  Proud W.G., Field J.E. : Internal displacements in cement during ballistic impact  1335-1338 ?Grantham S.G.,  Braithwaite C.H.,  Proud W.G., Williamson D.M. > Displacement maps in Taylor impact using speckle radiography  1333-1336 Gratz A.J., Nellis W.J. # Microstructures of shocked quartz 	 203-205 Gray�III G.T., Follansbee P.S. u Influence of peak pressure on the substructure evolution and mechanical properties of shock-loaded 6061-T6 aluminum Gray�III G.T. + Shock recovery experiments: An assessment 	 407-414 )Gray�III G.T.,  Hixson R.S., Morris C.E. ) Bauschinger effect during shock loading U Influence of peak pressure and temperature on the shock-loading reponse of tantalum  1103-1106 . Shock loading response of advanced materials  1161-1164 *Gray�III G.T.,  Hixson R.S., Johnson J.N. m Dynamic deformation and fracture response of a 6061-T6 Al   50 vol. % Al2O3 continuous reinforced composite 7Gray�III G.T.,  Blumenthal W.R.,  Idar D.J., Cady C.M. R Influence of temperature on the high strain-rate mechanical behavior of PBX 9501 	 583-586 IGray�III G.T.,  Bourne N.K.,  Zocher M.A.,  Maudlin P.J., Millett J.C.F. ^ Influence of crystallographic anisotropy on the Hopkinson fracture 'spallation' of zirconium HGray�III G.T.,  Bourne N.K.,  Millett J.C.F.,  Lopez M.F., Vecchio K.S. S Influence of microstructural anisotropy on the spallation of 1080 eutectoid steel 9Gray�III G.T.,  Bourne N.K.,  Millett J.C.F., Lopez M.F. � Influence of shock-wave profile shape ('Taylor-wave' versus square-topped) on the shock-hardening and spallation response of 316L stainless steel i Shock profile studies on selected silicon carbide ceramics with application to dynamic yield mechanisms = Spall properties of Solenhofen limestone and Dresser basalt N Fragmentation of expanding cylinders and the statistical theory of N.F. Mott U Analytic solutions and constitutive relations for shock propagation in porous media 3 The statistical fragmentation theory of N.F. Mott 	 455-460 0 Solutions of spall and fragmentation of solids 	 623-626 'Graf M.J.,  Greeff C.W., Boettger J.C. H High-pressure Debye-Waller and Gr�neisen parameters of gold and copper Graham R.A. ' The electrical-to-chemical connection  52-56 Graham R.A., Webb D.M. N Fixtures for controlled explosive loading and preservation of powder samples `Graham R.A.,  Morosin B.,  Horie Y.,  Venturini E.L.,  Boslough M.,  Carr M.J., Williamson D.L. 6 Chemical synthesis under high pressure shock loading 	 693-711 Graham R.A., Carr M.J. H Analytical electron microscopy study of shock synthesised zinc ferrite 	 803-808 M Shock-induced temperature distributions in powder compact recovery fixtures 	 831-836 G Shock compression of solids as a physical-chemical-mechanical process  11-18 $Graham R.A.,  Morosin B., Bush D.M. a Shock-induced melting of a KCl:LiCl eutectic powder as determined from electrochemical response !Graham R.A.,  Lee L.M., Bauer F. O Response of Bauer piezoelectric polymer stress gauges (PVDF) to shock loading 6Graham R.A.,  Anderson M.U.,  Bauer F., Setchell R.E. x Piezoelectric polarization of the ferroelectric polymer PVDF from 10 MPa to 10 GPa: Studies of loading path dependence  Bridgman's concern  3-12 Y Ballography: A billion nanosecond history of the Bee Bluff impact crater of south Texas  1462-1467 4Graham R.A.,  Martin M.,  Thadhani N.N., Morosin B. L Quartz and hydrous iron oxides from the Bee Bluff structure of south Texas  1468-1471 P Modeling energy dissipation induced by quasi-static compaction of granular HMX 	 289-292 Gonthier K.A., Son S.F. A Modeling compaction induced energy localization in granular HMX Goto T., Syono Y. ' Shock-induced phase transition in GaP 	 320-324 Gourdin W.H., Weinland S.L. 3 Hugoniot measurements on unsintered metal powders  99-104 
Gourdin W.H. V Prediction of microstructural modification in dynamically consolidated metal powders = Dynamic compaction of a monosized spherical tungsten powder 	 725-730 [ Metallurgical effects on the constitutive and fragmentation behavior of OFHC copper rings 	 351-354 *Gourdin W.H.,  Weinland S.L., Boling R.M. N Electromagnetic ri< ng expansion as a high-rate test: Experimental development Gourdin W.H., Lassila D.H. Y Deformation behavior of pre-shocked copper as a function of strain rate and temperature I Multiple mechanisms in the thermally activated plastic flow of tantalum 5Goveas S.G.,  Millett J.C.F.,  Bourne N.K., Knapp I. V One-dimensional shock and detonation characterization of ultrafine hexanitrostilbene Grady D.E. 3 Fragment size prediction in dynamic fragmentation 	 456-459 O Nonhydrostatic effects in stress-wave induced phase transformation of calcite D Temperature and deformation microstructure in the shock transition 	 363-367 K High pressure release wave measurements and phase transformation in CaCO3 	 589-593 > A strain-rate dependent spall mechanism transition in metals Grady D.E., Furnish M.D. P Hugoniot and release properties of a water-saturated high silica content grout 1 Shock wave properties of high-strength ceramics 	 455-458 D Impact strength and indentation hardness of high-strength ceramics ) Shock-wave properties of brittle solids  9-20 	Grady D. U Differential Hugoniot and experimental estimate of the Gr�neisen parameter for SiO2 O Impact response of single crystal potassium chloride at elevated temperatures 5Goncharov A.F.,  Struzhkin V.V.,  Ruf T., Syassen K. R Effect of pressure on coupled phonon and crystal-field excitations in NdBa2Cu3O7 ,Goncharov A.F.,  Struzhkin V.V., Syassen K. � Superconductivity-induced phonon self-energy effects and electronic Raman scattering in YBa2Cu3O7-x single crystals under pressure Gong Z.,  Tan H., Jing F. O Shock wave equation of state and shock induced phase transition of Halloysite 	 167-170 Gong Z.,  Li X., Jing F. U The possible composition and thermal structure of the Earth's lower mantle and core  1401-1405 %Gong Z.,  Dai F.,  Zhang L., Jing F. M An empirical material constant and equation of state on the solids Hugoniot .Gong Z.,  Dai F.,  Fei Y.,  Zhang L., Jing F. | Equation of state, phase stability of (Mg0.92Fe0.08)SiO3 perovskite from shock wave study and its geophysical implications  1444-1447 .Gong Z.,  Yu H.,  Deng L.,  Zhang L., Yang J. H Variations of thermal pressure for solids along the principal Hugoniot ,Gong Z.,  He L.,  Fei Y.,  Yang J., Jing F. p Sound velocity of (Mg0.92,Fe0.08)SiO3 perovskite up to 140 GPa shock pressure and its geophysical implications  1458-1461 Gonor A.L. i High-pressure vaporization and boiling of condensed material: A generalized Clausius-Clapeyron equation  63-66 !Gonor A.,  Hooton I., Narayan S. E Steady-state model of heterogeneous detonation with inert particles 	 423-426 Gonor A.L., Hooton L.E. t Shock wave diffraction over an inclusion in condensed matter and hot spot generation at the particle surface in HE 	 955-958 Gonor A., Hooton I. � On the origin of a maximum peak pressure on the target outside of the stagmation point upon normal impact of a blunt projectile and with underwater explosion  1379-1382 2Gonthier K.A.,  Menikoff R.,  Son S.F., Asay B.W. u High pressure spectroscopic study of the action of N-ethylamines and water on the 2-nitropropane/nitric acid system  1265-1268 KGoel B.,  Baumann K.,  H�bel W.,  Vorobiev O.Y.,  Shutov A.V., Fortov V.E. > Numerical analysis of foil acceleration experiments at KALIF BGogulya M.F.,  Dolgoborodov A.Y.,  Brazhnikov M.A., Dushenok S.A. , Shock wave initiation of liquid explosives 	 903-906 PGogulya M.F.,  Dolgoborodov A.Y.,  Brazhnikov M.A.,  Makhov M.N., Arkhipov V.I. 9 Aluminised explosive compositions based on NQ and BTNEN 	 962-965 Gogulya M.F., Brazhnikov M.A. c Some aspects of shock-induced radiation of transparent media and its transformation with pressure  1329-1332 !Gois J.C.,  Campos J., Mendes R. A Extinction and initiation of detonation of NM-PMMA-GMB mixtures .Gois J.C.,  Campos J.,  Plaksin I., Mendes R. H Failure and re-initiation detonation phenomena in NM/PMMA-GMB mixtures  Gois J.,  Campos J., Plaksin I. ` Effect of glass microballoons on failure and reaction regime of nitromethane/PMMA-GMB mixtures 	 898-901 sGold D.M.,  Celliers P.M.,  Collins G.W.,  DaSilva L.B.,  Cauble R.C.,  Kalantar D.H.,  Weber S.V., Remington B.A. R Optical interferometry diagnostics in laser-driven equation of state experiments CGolden J.,  Williams F.,  Morosin B.,  Venturini E.L., Graham R.A. 0 Catalytic activity of shock-loaded TiO2 powder  72-76 GGoldenberg A.,  Britan A.,  Ben-Dor G.,  Igra O.,  Hariton I., Glam B. T Dynamics of the load-transfer in a single straight chain of disks: FEM simulations 	 201-204 *Goldrein H.T.,  Synnergren P., Proud W.G. C Three-dimensional displacement measurements ahead of a projectile  1095-1098 7Goldrein H.T.,  Grantham S.G.,  Proud W.G., Field J.E. q The study of internal deformation fields in granular materials using 3D digital speckle X-ray flash photography $Golkov R.,  Kleiman D., Zaretsky E. 9 Dynamic fracture studies using sleeved Taylor specimens 	 519-522 9Gilmore M.R.,  Foster�Jr. J.C.,  Wilson L.L., Jones S.E.  The generalized Taylor test  1331-1334 (Ginzburg A.,  Rosenberg Z., Birnboim A. P The measurement of very short stress signals with piezoresistive stress gauges Ginzburg A., Rosenberg Z. X Using reverberation techniques to study the properties of shock loaded soda-lime glass 	 529-531 Glaesemann K.R., Fried L.E. 4 Recent advances in modeling Hugoniots with Cheetah 	 515-518 :Glam B.,  Britan A.,  Ben-Dor G.,  Igra O., Goldenberg A. 2 Dynamics of the contact stress in granular media  1261-1264 (Glancy B.C.,  Krall A.D., Sandusky H.W. ; Microwave interferometric applications in SDT/DDT studies (Glancy B.C.,  Sandusky H.W., Krail A.D. P Microwave interferometric hot spot density measurements in energetic materials Glenn L.A. = Shock attenuation in an inertial confinement fusion reactor 	 510-514 &Glenn H.D.,  Rambo J.T., Terhune R.W. " Calculational study of Baneberry 0 Seismic verification of underground explosions 	 613-620 *Glenn H.D.,  Stubbs T.F., Kalinowski J.A. 8 Ground motion measurements for the QUESO nuclear event 	 639-644 5 Performance analysis of the two-stage light gas gun *Glenn L.A.,  Latter A.L., Martinelli E.A. ! Multistage gasdynamic launchers 	 977-984 ( Partially decoupled explosion cavities c The influence of rock material models on seismic discrimination of underground nuclear explosions 	 343-346 5 Optimization studies of a three-stage light gas gun F On improving the penetration of commercial shaped charge perforators :Glushak B.L.,  Novikov S.A.,  Sinitsyna L.M., Yukina N.A. I Peculiarities of metal balls deformation by quasi-spherical shock waves 	 513-515 <Gobin C.,  Lucas H.,  Marteau P.,  Hebert P., Petitet J.-P. )Germann T.C.,  Holian B.L., Lomdahl P.S. G Plastic deformation in shock waves via molecular dynamics simulations 
Germann T.C. o Large-scale molecular dynamics simulations of shock-induced plasticity, phase transformations, and detonation ,Germann T.C.,  Hammerberg J.E., Holian B.L. J Large-scale molecular dynamics simulations of ejecta formation in copper EGerward L.,  Olsen J.S.,  Benedict U.,  Dancausse J.-P., Heathman S. Y High-pressure X-ray diffraction studies of ThS2, US2, and other AnX2 and AnXY compounds Getting I.C., Spetzler H.A. > Gas-charged piston-cylinder apparatus for pressures to 4 GPa  1581-1584 Ghose J., Roy A.  Optical studies on Rh2O3 (Gifford M.J.,  Luebcke P.E., Field J.E. \ A mechanism for the deflagration-to-detonation transition in ultrafine granular explosives &Gifford M.J.,  Proud W.G., Field J.E. @ Observations on type II deflagration-to-detonation transitions 	 878-881 Giles A.R., Maw J.R. N Modelling the temperature and strain rate dependence of spallation in metals 	 243-246 Gilev S.D., Trubachev A.M. W Shock-induced conduction waves in solids and their applications in high power systems N A study of semiconductor-metal transition in shocked monocrystalline silicon <  	 777-780 Gilman J.J. ) Dynamics at detonation fronts in solids  The plastic wave myth 	 387-389 Gilman J.J., Armstrong R.W. ) Shear-induced polymerization of benzene # Strain induced chemical reactions  1349-1352 , Topology of phase changes via bond-bending 	 215-219 F Deformation potentials and plasmon energies: Measures of sensitivity 	 313-316 2 Plasmon diagnosis of shock and detonation fronts 	 809-812  Mechanical states of solids  36-41 - Cohesion in ball lightning and Cook plasmas  1257-1260 / Bond modulus and stability of covalent solids 	 855-857 ,Gilmore M.R.,  Foster�Jr. J.C., Wilson L.L. v Thermal cook-off experiments of the HMX-based high explosive LX-04 to characterize violence with varying confinement aGarmasheva N.V.,  Filin V.P.,  Loboiko B.G.,  Averin A.N.,  Mathieu D.,  Simonetti P., Belmas R. ? Modeling and prediction of sensitivity in energetic materials 	 439-441 .Garrett G.R.,  Chhabildas L.C., Reinhart W.D.  Shock compression of liquids  81-84 -Garrett�Jr. R.K.,  Rajendran A.M., Last H.R. 3 Modeling spall in HY100, HY130, and AF1410 steels *Gathers G.R.,  Mitchell A.C., Holmes N.C. J Hugoniot measurements in vanadium using the LLNL two-stage light-gas gun  89-90 Gathers G.R., Mitchell A.C. U Hugoniot measurements in aluminum to 420 GPa using the LLNL two-stage light-gas gun 	 151-155 JGathers G.R.,  Osher J.E.,  Chau H.H.,  Weingart R.C.,  Lee C.G., Diaz E. ; Release isentrope measurements with the LLNL electric gun 	 175-178 5Gathers G.R.,  Chau H.H.,  Osher J.E., Weingart R.C. ; Hugoniot measurements with the LLNL electric gun facility J Hugoniot measurements on a slurry of finely divided tungsten and plastic  83-85 HGautier L.,  Belmas R.,  Bry A.,  Poullain D.,  Picart D., Le�Gallic C. ? Influence of thermal cycles on a TATB composition sensitivity 0Gefken P.,  Curran D.,  Nesterenko V.F., Cai J. � The explosive spherical cavity expansion for characterization of SiC-N ceramic dynamic behavior and post shock damage using RUS method 	 619-622 RGehr R.J.,  Bucholtz S.M.,  Rupp T.D.,  Robbins D.L.,  Stahl D.B., Sheffield S.A. S Line ORVIS particle velocity measurements on the laser-driven miniflyer apparatus  1163-1166 Gerin-Roze J. " Unusual self-similar compression  1515-1518 #Germain-Lacour M., de�Gliniasty M.  Ramp-wave generators studies 	 481-485 :German V.N.,  Mikhailov A.L.,  Osipov R.S., Tsyganov V.A. ; Structural transitions in solids under shock-wave loading 	 247-250 b Ultrafast time-resolved 2D spatial interferometry for shock wave characterization in metal films  1351-1354 Gailly B., Petit J. 9 Influence of the microstructure on armor steel spalling +Galbraith S.D.,  Rosenberg Z., Bourne N.K. T The determination of the reverse phase transition b2-b1 stress in shock loaded KCl 	 219-222 DGallagher K.G.,  Bass J.D.,  Ahrens T.J.,  Fitzner M., Abelson J.R. v Shock temperature of stainless steel and a high pressure-high temperature constraint on thermal diffusivity of Al2O3 &Gallagher K.G.,  Yang W., Ahrens T.J. 1 Free-surface light emission from shocked Teflon  1551-1554 PGamache R.M.,  Drotar J.T.,  Lee R.J.,  Callahan J.H.,  Evans T.W., Turner N.H. � Study of secondary reactions from explosives detonated within a bombproof and shock tube system via visible spectrometry and gas and solids collection &Gammel J.T.,  Swift D., Tierney�IV T. 1 Shock response of iron on nanosecond timescales  1385-1388 /Gang Y.,  Sun C.-W.,  Ghang-Quan Z., Tang Z.P. K Measurements of laser induced stress waves by eddy-current velocity gauge 	 925-927  Gao J.-X.,  Bai R.-S., Cheng C. 3 Measurement of temperature in shock-loaded solids 	 639-642 Gao X.-Z., Ding J. Y Shock Hugoniot of porous materials in the completely and incompletely compacted regions -Gao J.-X.,  Deng R.-G.,  Xu X.-H., Rao X.-L. 9 Effect of shock wave activation on nitriding of Sm2Fe17 Garcia B.O., Chavez D.J. ' Shock compression of liquid hydrazine VGarcia F.,  Forbes J.W.,  Tarver C.M.,  Urtiew P.A.,  Greenwood D.W., Vandersall K.S. Z Pressure wave measurements from thermal cook-off of an HMX-based high explosive PBX 9501 	 882-885 FGarcia F.,  Vandersall K.S.,  Forbes J.W.,  Tarver C.M., Greenwood D. b Pressure wave measurements resulting from thermal cook-off of the HMX based high explosive LX-04 G An ultrafast X-ray diffraction apparatus for the study of shock waves &Furnish M.D.,  Grady D.E., Brown J.M. H Analysis of shock wave structure in single-crystal olivine using VISAR 	 595-599 
Furnish M.D. B Dynamic compression and release experiments on Indiana limestone 	 625-628 ?Furnish M.D.,  Chhabildas L.C.,  Steinberg D.J., Gray�III G.T. , Dynamic behavior of fully dense molybdenum (Furnish M.D.,  Gray�III G.T., Remo J.L. > Dynamical behavior of octahedrite from the Henbury meteorite /Furnish M.D.,  Chhabildas L.C., Steinberg D.J.   Dynamical behavior of tantalum  1099-1102 Furnish M.D., Ito E. = Experimental measurements of shock properties of stishovite  93-96 >Furnish M.D.,  Lassila D.H.,  Chhabildas L.C., Steinberg D.J. Y Dynamic material properties of refractory metals: Tantalum and tantalum/tungsten alloys Furnish M.D., Chhabildas L.C. 4 Alumina strength degradation in the elastic regime @Furnish M.D.,  Chhabildas L.C.,  Setchell R.E., Montgomery S.T. F Dynamic electromechanical characterization of axially poled PZT 95/����������������������������������������������������������������������������������������������������������������������������������5 ZFurnish M.D.,  Robbins J.,  Trott W.M.,  Chhabildas L.C.,  Lawrence R.J., Montgomery S.T. @ Multi-dimensional validation impact tests on PZT 95/5 and ALOX 	 205-208 MFurnish M.D.,  Trott W.M.,  Mason J.,  Podsednik J.,  Reinhart W.D., Hall C. N Assessing mesoscale material response via high-resolution line-imaging VISAR IFurnish M.D.,  Reinhart W.D.,  Trott W.M.,  Chhabildas L.C., Vogler T.J. ^ Variability in dynamic properties of tantalum: Spall, Hugoniot elastic limit and attenuation Gaeta P.J., Dandekar D.P. ( Shock response of Kennertium grade W-2 	 269-272 Gaffney E.S., Brown J.A. G Comparative response of alluvium to Hopkinson bar and gas gun loading 	 621-626 
Gaffney E.S. D Generation of 2 MHz plane-strain sine waves by 3D quartz composite >Gahagan K.T.,  Reho J.H.,  Moore D.S.,  Funk D.J., Rabie R.L. ;Frost D.L.,  Goroshin S.,  Levine J.,  Ripley R., Zhang F. Y Critical conditions for ignition of aluminum particles in cylindrical explosive charges 	 972-975 'Frutschy K.J.,  Clifton R.J., Mello M. Q High-temperature pressure-shear plate impact studies on OFHC copper and pure WC 	 463-466 Fu R.,  Lindfors A., Davis J.  Scaling for internal blast  1440-1443 )Fuchs B.E.,  Droughton J., Persson P.-A. / Modifications to Oh-Persson equation of state 3Fugelso E.,  Jacobson J.D.,  Karpp R.R., Jensen R. ; Radiographic study of impact in polymer-bonded explosives 	 607-611 +Fujishiro I.,  Nakamura Y., Yamanokuchi H. s Evaluation of temperature dependence on ruby fluorescence at high pressure by viscosity measurement of lubricants  1059-1062 Fuka M.Z., Prentice J.K. : Interactive mesh generation in solid dynamics hydrocodes 	 297-300 #Fukunaga O.,  Iizuka M., Sugano T. P Formation pressure temperature region of diamond using alloy solvent catalysts -Funamori N.,  Yagi T.,  Uchida T., Utsumi W. ? Stability field of the orthorhombic perovskite type of MgSiO3 	 791-794 2Funk D.J.,  Laabs G.W.,  Peterson P.D., Asay B.W. � Measurement of the stress/strain response of energetic materials as a function of strain rate and temperature: PBX 9501 and mock 9501 �Funk D.J.,  Asay B.W.,  Bennett B.I.,  Bowman J.D.,  Boat R.M.,  Dickson P.M.,  Henson B.F.,  Hull L.M.,  Idar D.J.,  Laabs G.W.,  London R.K.,  Mace J.L.,  Morgan G.L.,  Murk D.M.,  Rabie R.L.,  Ragan C.E.,  Satcy H.L., Yuan V.W. I Dynamic measurement of temperature using neutron resonance spectroscopy MFunk D.J.,  Moore D.S.,  Reho J.H.,  Gahagan K.T.,  McGrane S.D., Rabie R.L. Y Ultrafast measurement of the optical properties of shocked nickel and laser hea<  ted gold  1227-1230 tFunk D.J.,  Meserole C.A.,  Hof D.E.,  Fisher G.L.,  Roberts J.,  Taylor A.J.,  Lee H.J.,  Workman J., McCulloch Q. / Shock compaction of alumina/zirconia ceramics  1263-1266 Fried L.E., Tarver C. A Molecular dynamics simulation of shocks in porous TATB crystals Fried L.E., Howard W.M. 5 The equation of state of HF under shock compression #Fried L.E.,  Reed E.J., Manaa M.R. < Simulations of fluid nitromethane under extreme conditions 1Fried L.E.,  Goldman N.,  Kuo I.F.W., Mundy C.J. 2 Chemistry of H2O and HF under extreme conditions  18-25 Fritz J.N., McQueen R.G.  Reflected shocks in SiO2 5Fritz J.N.,  Morris C.E.,  Hixson R.S., McQueen R.G. E Liquid sound speeds at pressure from the optical analyzer technique 	 149-152 Fritz J.N. D Overtaking wave interaction, reflected shock or reflected release? Fritz J.N., Kennedy J.E. @ Air cushion effect in the short-pulse initiation of explosives 4 The isotope effect on the Hugoniot of polyethylene A Waves at high pressure and explosive products equation of state 	 239-244 bFroeschner K.E.,  Chau H.,  Dittbenner G.,  Lee R.S.,  Mikkelson K.,  Steinberg D., Weingart R.C. 2 Shock Hugoniot experiments using an electric gun 	 174-178 6Froeschner K.E.,  Lee R.S.,  Chau H.H., Weingart R.C. / Shock Hugoniot measurements on Ta to 0.78 TPa 
Froger A. | A reaction zone enthalpy balance model to simulate shock-to-detonation transition and unsteady detonation wave propagation !Frost D.L.,  Aslam T., Hill L.G. | Application of detonation shock dynamics to the propagation of a detonation in nitromethane in a packed inert particle bed oFrost D.L.,  Zhang F.,  McCahan S.,  Murray S.B.,  Higgins A.J.,  Slanik M.,  Casas-Cordero M., Ornthanalai C. H Near-field impulse effects from detonation of heterogeneous explosives 	 946-949 JFrost D.L.,  Goroshin S.,  Janidlo S.,  Pryszlak J.,  Levine J., Zhang F. I Fragmentation of reactive metallic particles during impact with a plate 	 451-454 <Foster�Jr. J.C.,  Christopher F.R.,  Wilson L.L., Osborn J. F Mechanical ignition of combustion in condensed phase high explosives (Foster�Jr. J.C.,  Glenn J.G., Gunger M. { Meso-scale origins of the low-pressure equation of state and high rate mechanical properties of plastic bonded explosives EFoster�Jr. J.C.,  Jones S.E.,  Toness O.,  DeAngelis R.J., Rule W.K. L An analytical estimate for mass loss from a high velocity rigid penetrator  1125-1128 *Foster�Jr. J.C.,  Gilmore M., Wilson L.L. ~ The use of the Taylor test in exploring and validating the large-strain, high-strain-rate constitutive response of materials  1318-1322 *Fourney W.L.,  Barker D.B., Holloway D.C. 2 Mechanisms of fragmentation in brittle materials 	 153-158 $Fourney W.L.,  Wang X.J., Dick R.D. + Crush zone size dependence on charge size 	 597-600 6Fowler C.M.,  Peterson D.R.,  Hawke R.S., Brooks A.L. ' Rail gun development for EOS research 	 686-690 Fowler C.M.  Magnetic flux compression  53-64 Fowles G.R.  Shock wave stability 	 520-524 $Frachet V.,  Elias P., Martineau J. d Matter ejection from shocked materials: A physical model to understand the effects of free surface Frachet V., Mercier P. I Shaped charge virtual priming centers determination by image processing  1865-1858 Frank A.M., Gathers G.R. 1 Shock pressure determination in detonator wires Frank A.M. ! Mechanisms of EBW HE initiation Frank A.M., Chau H.H. ! Six-mm, plave wave shock driver  1651-1654 Frank A.M., Trott W.M. g Investigation of thin laser-driven flyer plates using streak imaging and stop motion microphotography  1209-1212 
Frankel M.J. > Pressure dependent vibronic relaxation in shocked explosives 	 593-597 %Franken J.,  Hambir S.A., Dlott D.D. D Picosecond vibrational spectroscopy of shocked energetic materials &Freim J.,  McKittrick J., Nellis W.J. 8 Impulse time integral function and Lagrangian analysis 	 189-192 E Lagrangian analysis, data covariance, and the impulse time integral 	 317-324 Q Isentrope energy, Hugoniot temperature, and the Mie-Gruneisen equation of state  31-34 %Forrestal M.J.,  Luk V.K., Brar N.S. D Perforation of aluminum armor plates with conical-nose projectiles 	 951-953 wFortov V.E.,  Bushman A.V.,  Filimonov A.S.,  Kvitov S.V.,  Kulish M.I.,  Lebedev M.E.,  Polischuk A.Y., Ternovoi V.Y. C Optical properties of dense plasma in shock and rarefaction waves oFortov V.E.,  Efremov V.P.,  Kanel G.I.,  Morosov P.V.,  Demidov B.A.,  Lomonosov I.V.,  Ni A.L., Vorobev O.Y. k Theoretical and experimental investigation of shock waves generated by high energy charged particle beams (Fortov V.E.,  Kostin V.V., Vorobev O.Y. R Generation of extreme states in condensed matter with high energy particle beams  1883-1886 PFortov V.E.,  Lebedev M.,  Dyabilin K.,  Vorobev O.,  Smirnov V., Grabovskij E. C Generation of shock waves by soft X-radiation from Z-pinch plasma iFortov V.E.,  Ternovoi V.Y.,  Kvitov S.V.,  Mintsev V.B.,  Nikolaev D.N.,  Pyalling A.A., Filimonov A.S. � Thermodynamic properties and electrical conductivity of hydrogen at multiple shock compression up to 150 GPa pressure ionization kFortov V.E.,  Yakushev V.V.,  Kagan K.L.,  Lomonosov I.V.,  Postnov V.I.,  Yakusheva T.I., Kuryanchik A.N. D Abnormal electric conductivity of lithium at high dynamic pressure 	 237-240 �Fortov V.E.,  Gryaznov V.K.,  Ilkaev R.I.,  Mikhaylov A.I.,  Mintsev V.B.,  Mochalov M.A.,  Pyalling A.A.,  Ternovoi V.Y., Zhernokletov M.V. O Pressure ionization of condensed matter under intense shock waves at megabars 	 135-140 Fortov V.E. 1 Intense shock waves and nonideal plasma physics  3-17 +Foster�Jr. J.C.,  Maudlin P.J., Jones S.E. F On the Taylor test: A continuum analysis of plastic wave propagation (Florence A.L.,  Cizek J.C., Keller C.E. < Laboratory experiments on explosions in geologic materials Fogel M.B. 4 Yield strength modeling of shock damaged materials 	 489-492 ZFogelson D.J.,  Lee L.M.,  Gilbert D.W.,  Conley W.R.,  Graham R.A.,  Reed R.P., Bauer F. T Fabrication of standardized piezoelectric polymer shock gauges by the Bauer method 	 615-618 Foiles S.M. ` DFT calculations of structural and thermodynamic properties of molten Sn: Zero-pressure isobar Follansbee P.S., Gray�III G.T. 8 Threshold stress measurements in shock-deformed copper 	 371-376 Follansbee P.S. o High strain rate deformation mechanisms in copper and implications for behavior during shock wave deformation 	 249-254 + The HEL and rate-dependent yield behavior 0 Shear stress prediction in shock loaded copper Foltz M.F., Maienschein J.L. V Phase transitions in ammonium perchlorate to 26 GPa and 700K in a diamond anvil cell 	 239-242 Forbes J.W., Elban W.L. � Comparison of axial longitudinal velocity measurements determined ultrasonically and by a weak shock velocity technique on an aluminized melt cast explosive 	 583-587 :Forbes J.W.,  Tasker D.G.,  Granholm R.H., Gustavson P.K. F Direct observation of shocked explosive crystals immersed in liquids %Forbes J.W.,  Lemar E.R., Baker R.N. ' Detonation wave curvature of PBXN-111  1389-1392 Forbes J.W., Lemar E.R. B Detonation wave velocity and curvature of brass encased PBXN-111 7Forbes J.W.,  Glancy B.C.,  Liddiard T.P., Wilson W.H. ` Aquarium test evaluation of a pyrotechnic's ability to perform work in microsecond time frames Forbes J.W. O The history of the APS Topical Group on Shock Compression of Condensed Matter aForbes J.W.,  Souers P.C.,  Urtiew P.A.,  Vandersall K.S.,  Garcia F.,  Greenwood D.W., Green L. = Pressure wave measurements in cylinders of detonating LX-17 	 902-905 Forest C.A. 5 SPH simulation of high density hydrogen compression QField J.E.,  Tsembelis K.,  Brar N.S.,  Proud W.G.,  Dandekar D.P., Rosenberg Z. C Issues related to lateral stress measurements in alumina ceramics ;Fietz W.H.,  Metzger J.,  Weber T.,  Grube K., Ludwig H.A. � Dependence of the intrinsic dTc/dp of YBa2Cu3Ox on the oxygen co<  ntent and the additive Tc increase by pressure-induced oxygen ordering 	 703-706 zFilin V.P.,  Loboyko B.G.,  Averin A.N.,  Litvinov B.V.,  Korotkikh I.G.,  Alekseev A.V.,  Belenovsky Y.A., Taibinov N.P. � On the mechanism of influence of explosive compounds: Destruction process on sensitivity of these compounds to mechanic impact CFilinov V.S.,  Levashov P.R.,  Bonitz M.,  Fortov V.E., Ebeling W. 9 On phase transition in strongly coupled hydrogen plasma CFischer R.P.,  Grun J.,  Mignogna R.,  Donnelly D.W., Covington B. T Athermal annealing of semiconductors using shock waves generated by a laser-plasma IFiske P.S.,  Nellis W.J.,  Lorenzana H.,  Lipp M.,  Kikuchi M., Syono Y. o Generation of pseudotachylites in shock experiments: Implications for impact cratering products and processes  1163-1165 7Flater P.J.,  House J.W.,  De�Angelis R.J., Nixon M.E. \ Damage characterization in copper deformed under hydrostatic stress: Experimental analysis 
Fleming K.J. ] Analysis of a high intensity X-ray source using a specialized Doppler interferometer system 2Flinn J.E.,  Korth G.E.,  Wright R.N., Green R.C. + Dynamic consolidation of aluminum powders 	 713-718 $Flinn J.E.,  Korth G.E., Doyle T.E. O Particle interaction and bonding for dynamically consolidated Fe-40Ni powders Flock R.A., Fowles G.R. 1 Explosive phase transition in superheated Freon 	 273-276 Flock R.A. @ Measurement of 'thin film' Gr�neisen using x-cut quartz gauges 	 763-766 Flock R.A., Liu D.T. ? Numerical analysis of 'thin film' Gr�neisen test measurements nFedorov A.V.,  Mikhailov A.L.,  Nazarov D.V.,  Finyushin S.A.,  Menshikh A.V.,  Davydov V.A., Govorunova T.A. P Study of detonation wave structure in solid and liquid tetranitromethane (TNM) 	 964-967 %Fellows J.,  Haskins P.J., Cook M.D. a A study of deflagration-to-detonation transition in a model A-B system using molecular dynamics 	 391-394 $Feng K.K.,  Jones D.E.G., Chan S.K. = Shock initiation of bubble sensitized commercial explosives 	 691-694 Feng R., Gupta Y.M. X Effect of epoxy bond response on combined compression-shear wave propagation in solids Feng S.S., Wang H.F. Z A simple method of determining the attenuation of the shock pressure in porous materials 	 963-966 Feng R.,  Gupta Y.M., Yuan G. Q Dynamic strength and inelastic deformation of ceramics under shock wave loading 	 483-488 eFerm E.N.,  Morris C.L.,  Quintana J.P.,  Pazuchanic P.,  Stacy H.,  Zumbro J.D.,  Hogan G., King N. [ Proton radiography examination of unburned regions in PBX 9502 corner turning experiments 	 966-969 �Ferm E.N.,  Dennison S.,  Lopez R.,  Prestridge K.,  Quintana J.P.,  Espinoza C.,  Hogan G.,  King N.,  Lopez J.D.,  Merrill F.,  Morley K.,  Morris C.L.,  Pazuchanics P.,  Saunders A.,  Baker S.A.,  Liljestrand R., Thompson R.T. C Proton radiography experiments on shocked high explosive products Ferm E.N., Mariam F. { Proton radiography observations of the failure of a detonation wave to propagate to the end of a conical explosive charge 	 968-971 ,Ferranti�Jr. L.,  Thadhani N.N., House J.W. N Dynamic mechanical behavior characterization of epoxy-cast Al+Fe2O3 mixtures MFerreira A.,  Yu L.H.,  Thadhani N.N.,  Chang S.N.,  Chang S.S., Meyers M.A. Z Shock compaction, synthesis, and chemically assisted bonding of aluminides and silicides Ferreira A., Costa�Junior A.M. C Analytical model for compaction of powder by means of shock waves Ferrel R., Romero V. E First results of reaction propagation rates in HMX at high pressure #Farnsworth�Jr. A.V., Lawrence R.J. E Numerical and analytical analysis of thin laser-driven flyer plates 	 821-824 Farnsworth�Jr. A.V. # Laser acceleration of thin flyers 0Farnsworth�Jr. A.V.,  Trott W.M., Setchell R.E. 4 A computational study of laser driven flyer plates  1355-1358 XFarrell J.P.,  Batchelor K.,  Dudnikov V.,  Srinivasan-Rao T.,  Smedley J., McDonald J. g Laser triggered synchronizable X-ray system for real time study of shock waves in condensed materials  1185-1187 Fast L., S�derlind P. : Crystal structure of actinide metals at high compression 3Fatyanov O.V.,  Nicol M.F.,  Ogura T., Kondo K.-I.  Equation of state for CCl4 	 117-120 3Fatyanov O.V.,  Ogura T.,  Nicol M.F., Kondo K.-I. O Precise time-resolved mid-infrared radiometry of shocked carbon tetrachloride +Fedorov A.V.,  Menshikh A.V., Yagodin N.B. A On detonation wave front structure of condensed high explosives IFedorov A.V.,  Zotov E.V.,  Krasovsky G.B.,  Menshikh A.V., Yagodin N.B. C Detonation front in homogeneous and heterogeneous high explosives 
Fedorov A.V. m Experimental investigation of heterogeneous high explosive decomposition mechanism in detonation wave front 	 910-913 �Fedorov A.V.,  Mikhailov A.L.,  Finyushin S.A.,  Nazarov D.V.,  Menshikh A.V.,  Davydov V.A.,  Govorunova T.A.,  Filinov E.V.,  Yukina N.A., Khokhlov A.A. E Recording of dispersion of elastic wave velocity in natural uranium }Fedorov A.V.,  Mikhailov A.L.,  Finyushin S.A.,  Nazarov D.V.,  Menshikh A.V.,  Davydov V.A.,  Govorunova T.A., Filinov E.V. = Study of relaxation of elastic precursor in natural uranium \Fedorov A.V.,  Mikhailov A.L.,  Nazarov D.V.,  Finyushin S.A.,  Menshikh A.V., Davydov V.A. 4 Shock wave initiation of mixture liquid explosives 	 960-963 m Prediction of pressure induced structural phase transitions and internal mode frequency changes in solid N2 Etters R.D., Kuchta B. h New methods for calculating phase transitions in simple molecular crystals: Application to N2O and CO2 %Evans A.M.,  Graham P., Rothman S.D. [ Recent results from materials properties experiments using the AWE high power laser HELEN $Evans D.J.,  Milne A.M., Softley I. ; The burning rate of aluminium particles in cylinder tests Ewart L., Dandekar D.P. b Relationship between the shock response and microstructural features of titanium diboride (TiB2)  1201-1204 Fahrenthold E.P. A Shock physics simulation using a hybrid particle-element method &Fanget A.,  Hereil P.L., Sibeaud J.M. X The influence of shock induced polymorphic transition in steel on 2D waves propagation  1087-1090 #Fanget A.,  Hereil P.L., Martin C. U Influence of the polymorphic transition and damage in steel on 2D waves propagation 	 235-238 
Fanget A. r Stability analysis of numerical solutions of wave propagation when pseudoviscosity is replaced by real viscosity !Fanget A.,  Trumel H., Dragon A.  A coupled viscoelastic-viscoplastic finite strain model for the dynamic behaviour of particulate composites: Numerical issues 	 179-182 <Faral B.,  Fabbro R.,  Virmont J.,  Cottet F., Romain J.-P. q Generation of ultrahigh pressures obtained in colliding foil experiments: Importance of two-dimensional effects 	 761-763 /Faral B.,  Fabbro R.,  Cottet F., Romain J.-P. v X-UV and visible emission of very high shocks (100 Mbar) in gold obtained by impedance mismatch in laser experiments mFaral B.,  Koenig M.,  Boudenne J.M.,  Batani D.,  Benuzzi A.,  Bossi S.,  Temporal M.,  Atzeni S., L�wer T. N EOS impedance matching experiments at high pressure with smoothed laser beam 	 943-946 BFarber D.L.,  Esposito A.P.,  Zaug J.M.,  Raugh J.E., Aracne C.M. Erlich D.C., Gran J.K. L Effect of static transverse prestress on dynamic tensile failure in metals 	 355-358 Erlich D.C., Schmidt C.G. * Rod impact experiments on thin specimens Erlich D.C., Seaman L. 5 Biaxial strain deformation and fracture of polymers , Shock Compression of Condensed Matter-1991 Erlich D.C., Curran D.R. { An experimental technique for studying shock propagation in large-scale samples of snow and other highly porous materials #Erskine D.J.,  Green L., Tarver C. 8 VISAR wave profile measurements in supra-compressed HE 	 717-720 
Erskine D.J. L Calculation of the refractive index change in dissociating shocked benzene 	 883-886 Erskine D.J., Nellis W.J. E Shock-induced martensitic transformation of highly ordered graphite 	 185-186 Erskine D. 7 Opacity measurements in<  shock-generated argon plasmas $ High pressure Hugoniot of sapphire M Increase of the dynamic range of catchup experiments by high-pass filtering 	 959-962 Erskine D.J., Holmes N.C. % White light velocity interferometry  1003-1005 < Increase in velocimeter depth of focus through astigmatism  1007-1009 * Improved shock-detecting pin arrangement  1105-1108 (Escobar J.C.,  Clifton R.J., Yang S.-Y. > Stress-wave induced martensitic phase transformation in NiTi 	 267-270 Espinosa H.D. > High strain rate modeling of ceramics and ceramic composites 	 721-724  Espinosa H.D.,  Mello M., Xu Y. \ A desensitized displacement interferometer applied to fast moving particles in a continuum  1011-1014 6Espinosa H.D.,  Yuan G.,  Dwivedi S., Zavattieri P.D. O Numerical study of penetration in ceramic targets with a multiple-plane model 	 901-904 Espinosa H.D., Zavattieri P.D. N Modeling of ceramic microstructures: Dynamic damage initiation and evolution 	 333-338 -Etters R.D.,  Kobashi K., Chandrasekharan V. Z Molecular dynamics study of reaction zone properties in chemically sustained shock waves 	 183-186 9Elert M.L.,  Barrett J.J.C.,  Robertson D.H., White C.T. i Molecular dynamics investigation of the effects of variation in energy release on detonation initiation &Elert M.L.,  Swanson D.R., White C.T. G Molecular dynamics simulation of shock-induced chemistry in acetylene 	 283-286 "Elert M.L.,  Zybin S., White C.T. K Molecular dynamics modeling of impact-induced shock waves in hydrocarbons  1406-1409 $Elert M.L.,  Zybin S.V., White C.T. C Molecular dynamics study of shock-induced chemistry in anthracene 	 323-326 Elias P., Chapron P. W Experimental techniques for measuring mass ejection from shock-loaded metallic sample 	 645-650 !Elias P.,  Chapron P., Mondot M. X Experimental study of the slowing down of shock-induced matter ejection into argon gas Eloy J.-F., Delpuech A. m Experimental study of photon-phonon interactions in an explosive by laser probe mass spectrometry (LPMS-25) Emery M.H., Gardner J.H. K Laser driven shock instabilities in multimaterial, layered, solid targets !Endo S.,  Takenaka I., Arashi H. * A new phase transition in TiO2 at 80 GPa Epstein J.S., Deason V.A. O Dynamic moir� interferometry: A review of research in weak shock environments Eremets M.i., Utjuzh A.N. L Optical nonmagnetic low-temperature hydrostatic pressure cells up to 3 GPa  1597-1600 8Erickson L.M.,  Palmer H.G.,  Parker N.L., Vantine H.C. f Free-surface velocity measurements of plates driven by reacting and detonating RX-03-BB and PBX-9404 	 553-557 Erickson L. ? Lawrence Livermore National Laboratory single-stage 101mm gun &Erlich D.C.,  Shockey D.A., Seaman L. @ Symmetric rod impact technique for dynamic yield determination 	 402-406 Erlich D.C., Shockey D.A. Q Dynamic flow curve of 4340 steel as determined by the symmetric rod impact test $ Eight beam Perot-Fabry velocimeter  1751-1754 Duvall G.E. 5 Shock wave research: Yesterday, today, and tomorrow  1-12 9Duvall G.E.,  Granholm R.H.,  Bellamy P.M., Hegland J.E. Q Effects of temperature on the UV-visible spectrum of dynamically compressed CS2 	 213-219 ! Three blind men and an elephant Eakins D.E., Thadhani N.N. D Investigation of shock-induced reactions in a Ni+Al powder mixture )Eatwell M.,  Millett J.C.F., Bourne N.K. c Lateral stress measurements in a shock loaded silicon carbide: Shear strength and delayed failure 6Eatwell M.,  Millett J.C.F.,  Bourne N.K., Meziere Y. D The behaviour of a glass-fibre epoxy composite during plate impact 3Eden G.,  Carden M.H.,  Collyer A.M., Smith C.P.M. ; Shock wave propagation in a 3-D quartz phenolic composite 	 217-220 +Edwards M.R.,  Bourne N.K., Millett J.C.F. P The effect of orientation on the spall strength of the aluminium alloy 7010-T6 	 523-526 +Edwards M.R.,  Millett J.C.F., Bourne N.K. x Quasistatic and shock induced mechanical response of an aluminium-zinc-magnesium alloy as a function of heat treatment 	 557-560 (Efros B.,  Shishkova N., Beigelzimer Y. V Structural and phase transitions in metastable systems at deformation under pressure 3Eggert J.H.,  Hemley R.J.,  Mao H.K., Feldman J.L. J Rotation-vibration and intermolecular dynamics of hydrogen and deuterium ;Egorov L.A.,  Barenboim A.I.,  Mokhova V.V., Samoilov A.I. � X-ray diffraction studies of the structures of dynamically compressed beryllium, aluminum, lithium fluoride, potassium chloride, and silicon dioxide Ek D.R., Asay J.R. P The stress and strain-rate dependence of spall strength in two aluminum alloys 	 413-418 &Elert M.L.,  Brenner D.W., White C.T. C Some one-dimensional molecular dynamics simulations of detonation 	 275-278 9Elert M.L.,  Robertson D.H.,  Barrett J.J.C., White C.T. ; The dynamic response of porous calcium carbonate minerals 	 309-313 2 The role of distention in reacting porous solids )Drummond N.D.,  Swift D.C., Ackland G.J. % Ab initio model of porous periclase  1436-1439 
Duba A.G.  Iron: What is melt? 	 923-926 XDudin S.V.,  Fortov V.E.,  Gryaznov V.K.,  Mintsev V.B.,  Shilkin N.S., Ushnurtsev A.E. X Investigation of shock compressed plasma parameters by interaction with magnetic field Duffy T.S., Ahrens T.J. 4 Hugoniot sound velocities and finite strain theory I Free surface velocity profiles in molybdenum shock compressed at 1400�C  1079-1082 B Shock compression and release of polycrystalline magnesium oxide  1107-1110 EDunbar E.,  Graham R.A.,  Holman G.T.,  Anderson M.U., Thadhani N.N. L Time-resolved pressure measurements in chemically reacting powder mixtures Dunn J.E., Grady D.E. 7 Strain rate dependence in steady, plastic shock waves 	 359-364 
Dunn J.E. @ The evolution of plastic strain in steady, plastic shock waves Dunn J.E., Fosdick R. d A dissipation principle and its consequences for structured shock waves in thermoelastic materials 	 215-218 7 Implications and origins of shock structure in solids  21-32 FDunn J.,  Price D.F.,  Moon S.J.,  Cauble R.C.,  Springer P.T., Ng A. > 1-10 Mbar laser-driven shocks using the JANUS laser facility Duprey K.E., Clifton R.J. @ Dynamic constitutive response of tantalum at high strain rates 	 475-478 0 Pressure-shear response of thin tantalum foils !Dur�es L.,  Campos J., Gois J.C. A New equation of state for the detonation products of explosives 	 385-388 #Dur�es L.,  Campos J., Portugal A. 6 Reaction path of energetic materials using Thor code <Dur�es L.,  Santos R.,  Correia A.,  Campos J., Portugal A. O Thermal behavior of Fe2O3/Al thermite mixtures in air and vacuum environments 	 956-959 !Durand M.,  Lalle P., Andriot P. A Pressure waves in medicine: From tissue injury to drug delivery  1431-1435 Drake R.P., Reighard A.B. D Context and theory for planar radiative shock experiments in xenon  1417-1420 4Dreger Z.A.,  Gruzdkov Y.A.,  Gupta Y.M., Dick J.J. E Time-resolved emission spectroscopy in shocked PETN single crystals Dremin A.N., Babare L.V. 0 The shock wave chemistry of organic substances  27-41 Dremin A.N., Molodets A.M. ) Metal spall and fracture micromechanism 	 415-420 (Dremin A.N.,  Orlov A.V., Molodets A.M. U Influence of temperature on the electrical conductivity of glass under shock effect ?Dremov V.V.,  Kutepov A.L.,  Petrovtsev A.V., Sapozhnikov A.T. - Equation of state and phase diagram of iron  87-90 .Dremov V.V.,  Sapozhnikov A.T., Smirnova M.A. d Wide range equation of state of water taking into account evaporation, dissociation and ionization ,Dremov V.V.,  Sapozhnikov P.A., Bringa E.M. j Molecular dynamics simulation of interaction between shock wave and high-symmetry intergranular boundary Drennov O.B., Mikhailov A.L. a About formation of contact boundary between two metals in unsteady conditions of oblique impact >Drennov O.B.,  Mikhaylov A.L.,  Nizovtsev P.N., Raevskii V.A. < t Growth of perturbations on metals interfaces at oblique collision with supersonic velocity of contact point motion <Drennov O.B.,  Davydov A.I.,  Mikhaylov A.L., Raevskii V.A. l Shear instability at the 'explosion product-metal' interface for sliding detonation of an explosive charge � Stabilization of wave formation on a contact boundary of metal layers at an oblique impact during Kelvin-Helmholtz instability development  1375-1378 (Drickamer H.G.,  Lang J.M., Dreger Z.A. 0 Recent high pressure photoluminescence studies  1491-1494 Drumheller D.S. L A theory for the shock-loading response of an alumina-filled epoxy mixture 	 527-528 Drumheller D.S., Grady D.E. 	 265-268 Ding J. . A description of shock wave in the year 1637 Ding J.-L., Hayes D. / Phase transformation rate in shock-loaded KCl Dionne J.P., Lee J.H.S. ? Modeling the detonation structure of heterogeneous explosives 	 317-320 2Divakov A.K.,  Khantuleva T.A., Mescheryakov Y.I. S Kinetics of mesostructure and reloading behavior of dynamically compressed solids 	 553-556 Dlott D.D. ; Ultrafast vibrational energy transfer in molecular solids 	 709-718 .Dobler E.A.,  Gryadunov A.N., Shteinberg A.S. D On the possible gas detonation explosion of BaO2/Zr powder mixture 	 635-638 Dodson B.W., Graham R.A. ! Shock-induced organic chemistry  42-51 Dodson B.W. T An exploratory study of reactivity in organic compounds subjected to shock loading  62-66 Dodson B.W., Venturini E.L. * Shock-induced defects in cadmium sulfide 	 335-339 Dodson B.W., Taylor P.A. 8 Monte Carlo simulation of shock-induced lattice damage 	 395-396 ;Dodson B.W.,  Arnold�Jr. C.,  Venturini E.L., Lenahan P.M. X Post-shock chemical and ESR analysis of acrylamide and selected anthracene derivatives 	 423-425 .Dodson B.W.,  Venturini E.L., Rogers�Jr. J.W. I Subthreshold generation of free radicals in shock-loaded organic solids 	 897-901 Dodson B.W., Bosclough M.S. 1 Techniques for recovery of shock-loaded samples 	 767-769 fDoherty R.M.,  Forbes J.W.,  Lawrence G.W.,  Deiter J.S.,  Baker R.N.,  Ashwell K.D., Sutherland G.T. E Detonation velocity of melt-cast ADN and ADN/nano-diamond cylinders Dolan D.H., Gupta Y.M. H Time-dependent freezing of water under multiple shock wave compression 	 167-171 "Dolgoborodov A.Y., Marshakov V.N. N Investigation of shock wave impulse influence on solid propellant combustion 	 868-871 1Dong Q.-D.,  Zhang J.-C.,  Liu G.Z., Jiang H.-Z. 5 Fusion produced by implosion of spherical explosive Doukas A.G. G Shock initiation of PETN crystals: Steric effects due to plastic flow 	 349-352 3Dick R.D.,  Williams J.D.,  Young C., Lottero R.E. , Blast pressure measurement from explosives &Dick R.D.,  Fourney W.L., Weaver T.A. R Effects of open joints and weak layers on wave propagation in geologic materials *Dick J.J.,  Whitehead M.C., Martinez A.R. ^ Crystal orientation dependence of elastic precursor strength in pentaerythritol tetranitrate (Dick R.D.,  Fourney W.L., Williams J.D. 2 Response of NTS tuff to high strain rate loading 	 153-156 < Orientation-dependent shock response of explosive crystals 	 815-818 *Dick R.D.,  Armstrong R.W., Williams J.D. 5 Split Hopkinson pressure bar tests on pure tantalum 	 471-474 Dick J.J., von�Dreele R.B. } Determination of the response of pentaerythritol tetranitrate to static high pressure up to 4.28 GPa by neutron diffraction %Dick R.D.,  Chang P.C., Fourney W.L. @ High strain rate loading of polymeric foams and solid plastics l Stress-strain response of PBX 9501 below 1 GPa from embedded magnetic gauge data using Lagrangian analysis 	 683-686 Dick J.J., Martinez A.R. 3 Elastic precursor decay in HMX explosive crystals 	 817-820 >Dickson P.M.,  Asay B.W.,  Henson B.F.,  Fugard C.S., Wong J. [ Measurement of phase change and thermal decomposition kinetics during cookoff of PBX 9501 	 837-840 EDickson P.M.,  Parker G.R.,  Smilowitz L.B.,  Zucker J.M., Asay B.W. 8 Frictional heating and ignition of energetic materials 7Dienes J.K.,  Middleditch J.,  Zuo Q.H., Kershner J.D. 5 On the role of crack orientation in brittle failure 	 447-450 /Dietenberger M.A.,  Rajendran A.M., Grove D.J. P A use of microphysical fracture model to describe ceramic material upon impact 	 457-460 .Dietenberger M.A.,  Antoun T., Rajendran A.M. g Simulation of uniaxial stress-strain curves for arbitrary strain rates and confining stress histories Delpuech A., Menil A. > Raman scattering temperature measurement behind a shock wave %Delpuech A.,  Mentil A., Pouligny B. [ Raman scattering temperature measurement behind a shock wave: A study of solid explosives 	 877-882 Demmie P.N. I Modeling and simulation of explosively driven electromechanical devices #Demol G.,  Goutelle J.C., Mazel P. h CHARME: A reactive model for pressed explosivves using pore and grain size distributions as parameters Demol G., Sandusky H.W. J Physical and chemical microstructural damage in pressed CL-20 explosives 'Demske D.L.,  Forbes J.W., Tasker D.G. o High current electrical resistance of PBX-9404 and dielectric breakdown measurements of naval high explosives ;Demske D.,  Brazell N.,  Farley W.E.,  Pogue E., Warnes R. E Intense electron beam detonation of insensitive energetic materials 	 773-776 $Denoual C.,  Cottenot C.E., Hild F. ? Analysis of the degradation mechanisms in an impacted ceramic Denoual C., Diani J.M. 3 Cavitation in compressible viscoplastic materials ,Derbenev I.V.,  Dremov V.V., Nikitenko Y.R. C Molecular dynamics simulation of hot spots in energetic materials 	 569-572 Deribas A. x Use of explosive energy for the production of multilayered composites from high Tc superconductive ceramics and metals Desgreniers S., Legault R. 6 High density crystalline structures of copper oxides 	Dey T.N. @ Effective stress model for partially and fully saturated rocks Dey T.N., Johnson J.N. 2 Shear band formation in plastic bonded explosive 
Dick J.J. @ Plane shock intiation on gamma-irradiated PETN single crystals B Pop plot and Arrhenius parameters for <110> PETN single crystals 	 903-907 ) Stress-strain histories in shocked PMMA &Dick J.J.,  Pettit D.R., Spencer W.J. A Crystal orientation effects in PETN explosive with 4 GPa shocks 	 713-715 !Dick J.J.,  Garcia E., Shaw D.C. E Isentropic compression experiments on dynamic solidification in tin $Davison L.,  Webb D.M., Graham R.A. > Analysis of capsules for recovery of shock compressed matter  67-71 Davison L. 1 Numerical modeling of dynamic material response 	 181-186 Davison D. W Sensing the threshold for initiation of high explosives in hydrodynamics calculations > Traditional analysis of nonlinear wave propagation in solids  20-25 )de�Resseguier T.,  Cottet F., Migault A. @ A 1D model for glass dynamic behaviour under explosive loading  1071-1074 0de�Ress�guier T.,  Berterretche P., Hallouin M. G Evidence of anisotropic wave propagation in laser shock-loaded quartz Dear J.P., Field J.E. Z An investigation of the shock structures and conditions for jetting during liquid impact 	 667-672 /Deas D.,  Millett J.C.F.,  Bourne N.K., Kos K. 4 The shock Hugoniot of two alumina-epoxy composites 	 693-696 &Deas D.,  Millett J.C.F., Bourne N.K. C The shock induced equation of state of two ferroelectric ceramics 	 851-854 %Deb S.K.,  Meenakshi S., Godwal B.K. 2 High pressure Raman studies on p-dichlorobenzene  1531-1534 
DeCarli P.S. 3 Were carbonados synthesized by an ancient impact? 	 757-760 7 More on the possibility of impact origin of carbonado ?DeCarli P.S.,  Bowden E.,  Sharp T.G.,  Jones A.P., Price G.D. J Evidence for kinetic effects on shock wave propagation in tectosilicates  1381-1384 0DeCarli P.S.,  Weaver C.A.,  Xie Z., Sharp T.G. \ Meteorite studies illuminate phase transition behavior of minerals under shock compression  1427-1430 Dehn J. + Modeling armor that uses interface defeat <  ADein J.,  Tokheim R.,  Curran D.,  Chau H.,  Weingart R., Lee R. 4 Aluminum damage simulation in high-velocity impact 	 171-174 Dekel E., Rosenberg Z. > More on the transition from rigid to eroding-rod penetration  1327-1330 l Shock wave synthesis of titanium silicide. 1: Effects of impact velocity, milling time and compact density  1094-1097 7Daswani J.M.,  Gupta S.C.,  Sikka S.K., Chidambaram R. M Theoretical analysis of the isostructural transition in zirconium at 53 GPa uDattelbaum D.M.,  Robbins D.L.,  Sheffield S.A.,  Orler E.B.,  Gustavsen R.L.,  Alcon R.R.,  Lloyd J.M., Chavez P.J. O Quasistatic and shock compressive response of fluorinated polymers: Kel-F 800 Davidson R.F., Walsh M.L. 3 Constitutive modeling for hypervelocity cratering  1159-1162 7Davies F.W.,  Smith E.A.,  Martinez A.A., Gaffney E.S. " Wave propagation in jointed rock 3Davies F.W.,  Reeder D.L.,  Johnson D.E., Lee L.M. d The derivation of material properties from measurements of radiation induced stress-time histories  1273-1276 #Davis J.F.,  Furlong J.R., Alme M. G Ceramics behavior at stress levels characteristic of ballistic impact Davis J.J. _ The effect of an electric field on the high strain rate properties of polymethyl methacrylate  1131-1134 Davis L.L., Brower K.R. ? A study of organic reactions driven by shock waves in liquids Davis J.J., Lindfors A.J. R Inert Hugoniot for a porous titanium-Teflon mixture: Experiment and calculations + Shock initiation chemistry of nitroarenes 	 699-702 %Davis J.J.,  Woody D.L., Miller P.J. ; Shock and impact initiation of a porous incendiary device (Davis L.L.,  Sheffield S.A., Engelke R. , Detonation properties of bromonitromethane 	 785-788 Davis L.L., Hill L.G.  ANFO cylinder tests 	 165-168 NDavis J.-P.,  Hayes D.B.,  Asay J.R.,  Watts P.W.,  Flores P.A., Reisman D.B. Y Investigation of liquid-solid phase transition using isentropic compression experiments 	 221-224 Davis J.J., Miller P.J. L Effect of metal particle size on blast performance of RDX-based explosives 	 950-953 Davis J.-P., Hayes D.B. / Response of ceramics under shock wave loading 	 729-732 Dandekar D.P., Bartkowski P. ! Shock response of AD995 alumina f Experimental technique to measure tensile impedance of a material under plane shock wave propagation 9 Shock, release, and tension response of soda lime glass Dandekar D.P., Spletzer S.V.  Shock response of Ti-6Al-4V Dandekar D.P., Grady D.E. B Shock equation of state and dynamic strength of tungsten carbide 	 783-786 H A re-examination of two-step lateral stress history in silicon carbide 	 731-734 Dandekar D.P., Prakash V. : Effect of shock induced shear on spall strength of SiC-N Dandrea R.G., Ashcroft N.W. 7 Theory of the high temperature shocked metallic state  57-69 EDaniels W.B.,  Lipp M.,  Strachan D.,  Yoo C.,  Zhang H.M., Yu Z.-H. R Nonlinear optics probes of ultraviolet energy levels of solids at high pressures  1499-1502 
Daniels W.B. B Use- and diamond-friendly method of rounding diamond anvil edges  1617-1618 +Danker G.R.,  Newlander C.D., Colella N.J. L Analytical modeling of dynamic tensile behavior in loaded Vamac elastomers 	 213-216 0Dannemann K.A.,  Lankford�Jr. J., Nicholls A.E. d The mechanism of strain rate strengthening during dynamic compression of closed-cell aluminum foam MDannemann K.A.,  Lankford�Jr. J.,  Nicholls A.E.,  Vaidyanathan R., Green C. T Dynamic compression of aluminum foam processes by a freeform fabrication technique MDanson C.,  Bann R.,  Hardie D.,  Pepler D.,  Ross I.,  Sails S., Woolsey N. 9 Uniform focal profiles suitable for laser driven shocks "Daraio C.,  Nesterenko V., Jin S. 2 Strongly nonlinear waves in 3D phononic crystals 3Daraio C.,  Nesterenko V.F.,  Herbold E.B., Jin S. = Strongly nonlinear waves in polymer based phononic crystals &Das K.,  Bandyopadhyay A., Gupta Y.M. [ The importance of material properties for cratering and penetration in geologic materials 	 945-948 &Curran D.R.,  Seaman L., Tokheim R.E. 0 Fragmentation models based on void coalescence $ Dynamic fracture and fragmentation  11-16 N Comparison of mesomechanical and continuum granular flow models for ceramics 	 315-318 -Cygan R.T.,  Boslough M.B., Kirkpatrick R.J. K Experimentally shocked quartz, NMR spectroscopy, and shock wave barometry > NMR spectroscopy of experimentally shocked silicate minerals 	 633-636 P NMR spectroscopic examination of shocked sandstone from Meteor Crater, Arizona 5Czerski H.,  Greenaway M.W.,  Proud W.G., Field J.E. 9 Monitoring phase change in HMX during dropweight impact J Links between the morphology of RDX crystals and their shock sensitivity d'Almeida T., Gupta Y.M. ; X-ray diffraction measurements in KCl shocked along [100] 	 113-116 
Dallman J.C. * Absorption spectra of shocked liquid CS2 	 231-235 &Dally J.W.,  Dick R.D., Williams J.D. " Dynamic loading with a short bar 	 755-758 Damamme G. / The divergent quasistationary detonation wave W A new method to simulate shocks, detonations and transitions from shock to detonation 	 575-577 CDan K.,  Tamura H.,  Sawaoka A.B.,  Mori T.,  Hwang M.D., Horie Y. \ Microstructures of single-crystal copper rods shock-treated by a rod-in-cylinder technique  1225-1228 Dandekar D.P., Lamothe R.M. A Shock, re-shock, and release behavior of a phenolic resin FF-17 	 125-128 Dandekar D.P., Lopatin C.M. 2 Shock response of SiC/2014-T4 aluminum composite 	 365-369 %Dandekar D.P.,  Gaeta P.J., Horie Y. A Double shock and release experiments in PMMA and Z-cut sapphire Dandekar D.P., Hankin M. G Deformation of a polyvinyl based elastomer subjected to shock loading Dandekar D.P. = Effect of shock re-shock on spallation of titanium diboride p Using mesoscale modeling to investigate the role of material heterogeneity in geologic and planetary materials  1453-1457 :Crepeau J.,  Needham C.,  Caipen T.,  Grady D., Harper F. T First principles calculations of the interaction of blast waves with aqueous foams &Crockett S.,  Chisholm E., Wallace D. d A comparison of theory and experiment of the bulk sound velocity in aluminum using a two-phase EOS :Crockett S.D.,  Greeff C.W.,  Johnson J.D., Burakovsky L. A Testing of a liquid equation of state model against copper data )Cross D.L.A.,  Dandekar D.P., Proud W.G.  Spall behaviour of PMMA 	 655-658 qCross D.L.A.,  Chapman D.J.,  Tsembelis K.,  Proud W.G.,  Borg J.P.,  Lloyd A.,  Schwalbe L.,  Cogar J., Ward A. - Experimental Hugoniot data of porous silica ,Crouzet B.,  Partouche-Sebban D., Carion N. 2 Temperature measurements in shocked nitromethane  1253-1256 eCunningham B.,  Vandersall K.S.,  Niles A.M.,  Greenwood D.W.,  Garcia F.,  Forbes J.W., Wilson W.H. < Carbon resistor pressure gauge calibration at low stresses  1137-1140 Curran D.R. I Stress and temperature-driven nucleation of microscopic voids in metals 	 135-139 Curran D.R., Seaman L. W Computational models for nucleation, growth, and coalescence of adiabatic shear bands ( Shock Waves in Condensed Matter - 1985 	 315-320 I Application of micromechanical failure models to shock physics problems 	 321-326 I Incubation times and rate-dependent toughness for macrocrack initiation 	 305-308 N Appropriate material softening and failure models for numerical calculations 	 395-398 #Curran D.R.,  Seaman L., Cooper T. _ A micromechanical model for granular material and application to penetration of ceramic armor 7 Computer models of dynamic fracture and fragmentation &Curran D.R.,  Cooper T., Tokheim R.E. 3 Model for hot spots in porous frictional material L Generation of ultra-high pressure shocks in 0.26 mm wavelength experiments 	 531-534 Cottet F., Boustie M. a Spall measurements in metallic targets using shock waves induced by short duration laser pulses +Counihan P.J.,  Crawford A., Thadhani N.N. a Nanostructure formation by dynamic densification and recrystallization of amor<  phous Ti-Si alloy #Cour-Palais B.G., Piekutowski A.J. - The multi-shock hypervelocity impact shield 	 979-982 Cour-Palais B.G. C Spacecraft outer thermal blankets as hypervelocity impact bumpers  1175-1178 &Courchinoux R.,  Chapron P., Elias P. b Particle velocity profiles measured by LDI through a LiF window in loading-unloading experiments 	 771-774 Courchinoux R., Lalle P. ( Unreacted Hugoniot of ammonium nitrate  1397-1400 B Dynamic properties of water: Sound velocity and refractive index  61-64 HCouturier S.,  Boustie M.,  de�R�ss�guier T.,  Hallouin M., Romain J.P. i Laser driven shock pressure measurements by VF2/VF3 and PVDF gages for pulses of 2.5ns up to 1012 w/cm2  1097-1100 Cowperthwaite M., Gupta Y.M. ; Investigation of shear induced reaction in composition B3 	 863-869 Cowperthwaite M. ? An analytic analysis for the tension-recompression experiment 	 585-588 Cowperthwaite M., Vidal P. A Shock-change equations for classical two-dimensional detonation 	 255-258 @ One-dimensional flows with straight particle velocity contours 	 245-248 B A new approach to the Wood and Kirkwood axial detonation problem  1357-1360 	Cox G.A. ; A multiphase equation of state and strength model for tin 	 208-211 Coyne�Jr. P.J., Elban W.L. @ A strain rate sensitivity prediction for porous bed compaction 	 147-150 7Crawford P.,  Rainey K.,  Rightley P., Hammerberg J.E. f A novel experimental technique for the study of high-speed friction under elastic loading conditions Crawford D.A. N High speed observation of fragment impact initiation of nitromethane charges OCook M.D.,  Haskins P.J.,  Briggs R.I.,  Stennett C.,  Fellows J., Cheese P.J. B Fragment impact characterization of melt-cast and PBX explosives  1047-1050 NCook M.D.,  Stennett C.,  Haskins P.J.,  Briggs R.I.,  Wood A.D., Cheese P.J. S The role of binders in controlling the cook-off violence of HMX/HTPB compositions 	 952-955 &Cooper T.,  Rosenberg G., Curran D.R. f Utilization of shock wave concepts to improve ballistics modeling for armor penetration by long rods RCooper G.A.,  Longbottom A.W.,  Bourne N.K.,  Milne A.M.,  Murray I., Hollands R. C Plate impact study of the shock to detonation transition in a PBX :Cooper G.A.,  Millett J.C.F.,  Bourne N.K., Dandekar D.P. + Delayed failure in a shock loaded alumina 	 847-850 Corey E.M., Young D.A. 0 A new prototype equation of state data library  43-46 ?Corley J.,  Riedel W.,  Hiermaier S.,  Weidemaier P., Thoma K. � A combined experimental computational approach to assessing the high strain rate response of high explosive simulants and other viscoelastic composite materials :Cornelius A.L.,  Schilling J.S.,  Endstra T., Mydosh J.A. T High pressure studies on the ferromagnetic dense Kondo systems CeRh3B2 and UCu2Ge2  1457-1460 5Cortecuisse S.,  Cansell F.,  Fabre D., Petitet J.P. C Raman spectroscopy of nitromethane under pressure and temperature 	 295-297 *Cosculluela A.,  Cagnoux J., Collombet F. N Two types of experiment for studying uniaxial dynamic compression of alumina 	 951-954 Cottet F., Romain J.P. 1 Twinning in iron by laser generated shock waves 	 130-134 #Cottet F.,  Fabbro R., Romain J.P. U Experiments and simulation of laser-driven shock wave evolution in aluminum targets GCottet F.,  Hallouin M.,  Romain J.P.,  Fabbro R.,  Faral B., P�pin H. 9 Crystal failure and crack formation during plastic flow CCogar J.R.,  Robinson N.,  Tsembelis K.,  Proud W.G., Cross D.L.A. 3 Shock Hugoniot data for low density silica powder  1090-1093 Cohen R.E., Gong Z. . Melting and melt structure at high pressures 	 379-382 3Cohen R.E.,  Stixrude L., Papaconstantopoulos D.A. v An accurate tight-binding model for iron at high pressures: Towards high temperature simulations of the Earth's core �Collins G.W.,  DaSilva L.B.,  Celliers P.,  Budil K.S.,  Cauble R.,  Gold D.,  Foord M.,  Stewart R.,  Holmes N.C.,  Ross M.,  Hammel B.A.,  Kilkenny J.D.,  Wallace R.J., Ng A. . Equation of state measurements of D2 on NOVA  55-60 Colvin J.D., Kalantar D.H. \ Scaling of pressure with intensity in laser-driven shocks and effects of hot X-ray preheat  1413-1416 �Conrad C.H.,  Trott W.M.,  Hall C.A.,  Lash J.S.,  Dukart R.J.,  Clark B.,  Hanson D.L.,  Chandler G.A.,  Fleming K.J.,  Trucano T.G.,  Chhabildas L.C., Asay J.R. A Use of Z-pinch sources for high pressure shock wave experiments 
 997-1000 Constantinou C.P., Gupta Y.M. J The UV/visible absorption spectra of shocked nitromethane-amine mixtures  1559-1562 Cook M.D., Haskins P.J. 1 Short range interactions of detonation products 	 271-274 %Cook M.D.,  Haskins P.J., James H.R. k An investigation of projectile and barrier geometry effects on impact initiation of a secondary explosive 	 675-678 Cook W.H., Rajendran A.M. ( Modeling impact damage in AD85 alumina l An investigation of the response of secondary explosives to conical-tipped projectiles and oblique impacts  1421-1424 9 Projectile impact initiation of a homogeneous explosive f The development of a new Arrhenius-basd burn model for both homogeneous and heterogeneous explosives MCook M.D.,  Haskins P.J.,  Briggs R.I.,  Cheese P.,  Stennett C., Fellows J. n Validation of an advanced material model for simulating the impact and shock response of composite materials Clements B.E. + Damage evolution in viscoelastic polymers Clements B.E., Mas E.M. ] Modeling high explosives with the method of cells and Mori-Tanaka effective medium theories 	 427-430 (Clements B.E.,  Mas E.M., Gray�III G.T. > Investigation of the observed anisotropic fracture in steels 'Clements B.E.,  Mas E.M., Maudlin P.J. e Developments toward a continuum-level non-spherical void growth model using a micro-mechanics basis , Low-pressure equation of state of polymers  57-60 AClements B.E.,  Mas E.M.,  Plohr J.N.,  Ionita A., Addessio F.L. > Dynamic response of PBX9501 through the b-d phase transition 	 204-207 
Clifton R.J. / Re-examination of the precursor decay anomaly 	 407-411 + Plate impact facility at Brown University 	 661-662 B Pressure shear impact and the dynamic plastic response of metals 	 105-111 1Clifton R.J.,  Raiser G.,  Ortiz M., Espinosa H. ) A soft recovery experiment for ceramics 	 437-440 #Clifton R.J.,  Mello M., Brar N.S. 5 Effect of shear on failure waves in soda lime glass Clifton R.J., Bhate N. : Bridging length scales in dynamic plasticity simulations  19-26 ,Clifton R.J.,  Jearanaisilawong P., Jiao T. 9 Hgih strain rate response of an epoxy and a vinyl ester Cochran S.G., Tarver C.M. d Modeling particle size and initial temperature events on shock initiation of TATB-based explosives 	 593-596 Coffey C.S. 8 Compressive waves and shock waves in anharmonic solids %Coffey C.S.,  Davis J.J., Woody D.L. = Energy localization in rapidly deforming crystalline solids 	 253-256 E Microscopic processes of plastic deformation during shock or impact  1181-1184 I Energy dissipation and the initiation of explosives during plastic flow 	 807-810 Coffey C.S., Sharma J. a Variation of thermal and cold curve contributions to thermodynamic functions along the Hugoniot Chisholm E., Wallace D. U Estimating the viscosity coefficient of liquid metals from vibration-transit theory Chitanvis S.M. / Hotspot mechanisms in shock-melted explosives J Preliminary results from an asymptotic analysis of the Forest Fire model 	 511-514 6Cho Y.S.,  Baek S.H.,  Lee J.,  Choi K.Y., Song S.-Y. % Interaction of two bubbles in water Choi C.S.,  Lee S.W., Kim K. I Temperature rise in hot spots in porous explosives due to finite strain <Christiansen E.L.,  Crews J.L.,  Kerr J.H., Chhabildas L.C. O Hypervelocity impact testing above 10 km/s of advanced orbital debris shields Chronister E.L., Baer B.J. S An optical study of pentacene in p-terphenyl at high pressure and low temperature  1507-1510 Chung D.-T. 9 The effect of the specimen shape on dynamic flow s< tress $Church P.,  Townsley R., Millett J. B Consideration of stress gauges in the modelling of plate impacts  1083-1086 7Church P.D.,  Proud W.G.,  Andrews T.D., Goldthorpe B. N The spall strength measurement and modelling of AQ80 iron and copper systems 	 487-490 7Church P.D.,  Andrews T.,  Bourne N.K., Millett J.C.F. ! Spallation in the alloy Ti6Al4V @Church P.D.,  Grief A.,  Tsembelis K.,  Proud W.G., Murray N.H. A Experiment and simulation of the lateral gauge in glass targets ACinnamon J.D.,  Palazotto A.N.,  Brar N.S.,  Kennan Z., Bajaj D. H Johnson-Cook strength model constants for Vascomax 300 and 1080 steels 	 709-712 
Clayton J.D. L Plasticity and spall in high density polycrystals: Modeling and simulation 	 311-314 Clegg R.A., Hayhurst C.J. v Numerical modelling of the compressive and tensile response of brittle materials under high pressure dynamic loading %Clegg R.A.,  Hayhurst C.J., Nahme H. 4 Shock loading and release behavior of x-cut quartz 	 601-605 4Chhabildas L.C.,  Carr M.J.,  Kunz S.C., Morosin B. ( Shock-recovery experiments on PZT 95/5 	 785-790 Chhabildas L.C., Barker L.M. 2 Dynamic quasi-isentropic compression of tungsten 	 111-114 % Pressure-shear loading of materials 	 579-584 8Chhabildas L.C.,  Barker L.M.,  Asay J.R., Trucano T.G. ? Spall strength measurements on shock-loaded refractory metals )Chhabildas L.C.,  Hertel E.S., Hill S.A. - Whipple bumper shield tests at over 10 km/s 	 991-994 RChhabildas L.C.,  Barker L.M.,  Asay J.R.,  Trucano T.G.,  Kerley G.I., Dunn J.E. % Launch capabilities to over 10 km/s  1025-1031 ;Chhabildas L.C.,  Boslough M.B.,  Reinhart W.D., Hall C.A. D Debris cloud characterization at impact velocities of 5 to 11 km/s  1841-1844 9Chhabildas L.C.,  Kmetyk L.N.,  Reinhart W.D., Hall C.A.   Launch capabilities to 16 km/s  1197-1200 ;Chhabildas L.C.,  Furnish M.D.,  Reinhart W.D., Grady D.E.  Impact of AD995 alumina rods .Chhabildas L.C.,  Furnish M.D., Reinhart W.D. > Shock induced melting in aluminum: Wave profile measurements  97-100 EChhabildas L.C.,  Trott W.M.,  Reinhart W.D.,  Cogar J.R., Mann G.A. > Incipient spall studies in tantalum: Microstructural effects 'Chidester S.K.,  Tarver C.M., Lee C.G. 4 Impact initiation of new and aged solid explosives 8Chidester S.K.,  Tarver C.M.,  DePiero A.H., Garza R.G. _ Single and multiple impact ignition of new and aged high explosives in the Steven impact test 	 663-666 =Chidester S.K.,  Vandersall K.S.,  Switzer L.L., Tarver C.M. \ LX-04 violence measurements: Steven tests impacted by projectiles shot from a howitzer gun  1049-1052 *Chijioke A.D.,  Nellis W.J., Silvera I.F. G Isotherms reduced from isentropes and Hugoniots up to several 100 GPa  49-53 &Chisholm E.,  Crockett S., Wallace D. 7 Shear localization in granular and comminuted alumina 	 607-610 !Chen G.Q.,  Ahrens T.J., Hide R. ; Theory of shock magnetization of asteroids Gaspra and Ida 	 929-932 (Chen T.,  Thadhani N.N., Hampikian J.M. = Shock compaction and strengthenning of nanocrystalline NiAl 	 733-736 $Chen Q.,  Cao L.,  Gong Z., Jing F. I Hugoniots and shock temperature of dense helium under shock compression <Chen X.-F.,  Gong Z.,  Fei Y.,  Zhang L.,  Deng L., Jing F. r A new evidence of the stability of (Mg,Fe)SiO3 perovskite at lower mantle conditions: Shock recovery experiments .Cheng J.-Y.,  Zhou G.-Q.,  Tang Z.P., Li X.Z. n A unified theory of collective dislocation motion including both thermal activation and viscous drag effects fCheret R.,  Andriot P.,  Chapron P.,  Le�Drean C.,  Lezaud J.M.,  Loichot R.,  Martineau J., Olive F. F Shock wave experiments using explosives and light gas-gun facilities 	 626-630 
Cheret R. C Critical propagation velocities of a steady autonomous detonation 	 511-513 
Ch�ret R. , The life and work of Pierre Henri Hugoniot  11-19 ACherne F.J.,  Baskes M.I.,  Germann T.C.,  Ravelo R.J., Kadau K. T Shock Hugoniot and melt curve for a modified embedded atom method model of gallium %Cherne F.J.,  Kadau K., Germann T.C. R A molecular dynamics study of solid gallium using a modified embedded atom model PChesnut G.N.,  Streetman B.D.,  Schiferl D.,  Anderson W.W.,  Nicol M., Meng Y. X Static X-ray diffraction of cerium: The standard approach and the magic-angle approach (Chesnut G.N.,  Anderson W.W., Casson J. 9 Static X-ray diffracton study of cerium to 300 kilobars 'Chhabildas L.C.,  Wise J.L., Asay J.R. + Reshock and release behavior of beryllium 	 422-426 Chhabildas L.C. ; The Sandia shock thermodynamics applied research facility 	 621-625 Chhabildas L.C., Grady D.E. ) Shock loading behaviour of fused quartz 	 175-179 : The response of PVF2 stress gauges to shock wave loading 	 797-800 . A simple approach to piezofilm stress gauges 	 897-900 Charest J.A., Lilly M.D. 8 PFV2 stress gauges for non-planar wave applications. 1  1731-1734 Charest J.A., Mace J.L. 2 Outputs of shock-loaded small piezoceramic disks  1153-1156 Chartagnac P.F. F Determination of mean and deviatoric stresses in shock loaded solids 	 397-401 Chartagnac P. 5 A pragmatic approach to sequential dynamic loadings 	 923-930 NChartagnac P.,  Decaso P.,  Jimenez B.,  Bouchu M.,  Cavailler C., Delavel J. : Dynamic behaviour of PVF2 gauges in the 0-600 kbar range 	 893-896 -Charters A.C.,  Menna T.L., Piekutowski A.J. S High velocity penetration of semi-infinite steel by continuous and segmented rods 	 931-934 MChau H.,  Dittbenner G.,  Mikkelsen K.,  Weingart R.,  Froeschner K., Lee R. 4 Performance of a 100 kV, 78 kJ electric gun system 	 691-695 .Chemerys V.T.,  Raychenko A.I., Karpinos B.S. [ Impact interaction of projectile with conducting wall at the presence of electric current  1314-1317 Chen D. ] Numerical simulation and analysis of single/two-stage gas gun for shock compression studies 	 649-651 Chen X.-R., Chen B.-Y. C A study of the mechanism of pressure-casting charge of explosives 	 737-740 *Chen D.,  Feng J.,  Wang J.-G., Liu G.-L. * Terminal effects of high velocity impact Chen S.-H. ( Component Hugoniot in mixture material  69-72 >Chen G.,  Stump N.A.,  Haire R.G.,  Burns J.B., Peterson J.R. 5 A luminescence study of B-type Eu2O3 under pressure 	 359-362 ;Chen J.H.,  Iwasaki H.,  Kikegawa T.,  Yaoita K., Tsuji K. ? Crystal structure of the high pressure phase of bismuth BiIII Chen A.L., Yu P.Y. P Near-IR absorption measurements of the transition metal iodides under pressure )Chen H.C.,  Meyers M.A., Nesterenko V.F. % Bar impact tests on alumina (AD995) 	 787-790 Celebonovic V., Schulz H.J. K The electrical conductivity of the organic conductors under high pressure  1449-1452 OCerreta E.,  Gray�III G.T.,  Henrie B.L.,  Brown D.W.,  Hixson R.S., Rigg P.A. x The influence of peak stress on the mechanical behavior and the substructural evolution in shock-prestrained zirconium 	 541-544 PCerreta E.,  Gray�III G.T.,  Lawson A.C.,  Morris C.E.,  Hixson R.S., Rigg P.A. g The influence of interstitial oxygen on the alpha to omega phase transition in titanium and zirconium HChakravarty A.,  Gifford M.J.,  Greenaway M.W.,  Proud W.G., Field J.E. < Factors affecting shock sensitivity of energetic materials (Chakravarty A.,  Proud W.G., Field J.E. / Small scale gap testing of novel compositions 	 935-938 <Chambers G.,  Sandusky H.,  Zerilli F.,  Rye K., Tussing R. U Pressure measurements on a deforming surface in response to an underwater explosion 2Chambers G.P.,  Lee R.J.,  Oxby T.J., Perger W.F. 9 Electromagnetic properties of pre-detonating explosives 	 890-897 !Chandra U.,  Mudgal P., Kumar M. t Study of phase transformations on nanocrystalline (La,Sr)(Mn,Fe)O3 systems by high-pressure M�ssbauer spectroscopy 	 200-203 6Chang S.N.,  Meyers M.A.,  Thadhani N.N., Erlich D.C. R Martensitic transformations induced by tensile stress pulse in an Fe-Ni-Mn alloy <Chang S.N.,  Chung D.-T.,  Ravichandran G., Nemat-Nasser S. <  F Plate impact experiments on Mg-PSZ and improved target configuration 	 389-392 Chang S.N., Choi J.H. 5 High strain rate response of a tungsten heavy alloy 	 415-418 (Chapman D.J.,  Tsembelis K., Proud W.G. / The behaviour of dry sand under shock loading  1445-1448 "Chapron P.,  Elias P., Laurent B. j Experimental determination of the pressure inducing melting in release for shock-loaded metallic samples 	 171-173 Charest J.A., Lynch C.S. KCarroll D.E.,  Chhabildas L.C.,  Reinhart W.D.,  Winfree N.A., Kerley G.I. F Computational characterization of three-stage gun flier plate launch 	 307-310 ECart E.J.,  Lee R.J.,  Gustavson P.K.,  Coffey C.S., Sutherland G.T. 5 The role of shear in shock initiation of explosives ACart E.J.,  Granholm R.H.,  Joshi V.S.,  Sandusky H.W., Lee R.J. R Measurement of ignition and reaction parameters in non-ideal energetic materials  1045-1048 )Carton E.P.,  Stuivinga M., Verbeek H.J. 1 Crack prevention in shock compaction of powders 	 549-552 V Shock compaction of combustion synthesized ceramics in the cylindrical configuration 'Carton E.P.,  Stuivinga M., Boluijt A. # TiC by SHS and dynamic compaction  1127-1130 Carton E.P., Stuivinga M. 5 Scale-up method for the shock compaction of powders  1086-1089 + Explosive forming of aerospace components Case S., Horie Y. ? Modelling the shock response of polycrystals at the mesoscale $Casey W.H.,  Carr M.J., Graham R.A. @ Crystal defects and the dissolution kinetics of shocked rutile Catanach R.A., Hill L.G. L Diameter effect curve and detonation front curvature measurements for ANFO 	 906-909 7Caulder S.M.,  Buess M.L.,  Garroway A.N., Miller P.J. d NQR line broadening due to crystal lattice imperfections and its relationship to shock sensitivity 	 929-934 &Cazalis B.,  Boissi�re C., Sibille G. G Shocks induced by laser driven flyer plates. 2: Numerical simulations  1217-1220 @Cazamias J.U.,  Bless S.J.,  Hari�Manoj�Simha C., Hartnett T.M. : Dynamic failure of a transparent polycrystalline ceramic 	 611-614 Cazamias J.U. Q The effects of shear banding in 6-4 titanium on round and square Taylor impacts 	 587-590 'Cazamias J.U.,  Fiske P.S., Bless S.J. $ The Hugoniot elastic limit of ALON JCazamias J.U.,  Reinhart W.D.,  Konrad C.H.,  Chhabildas L.C., Bless S.J. Z Collapse of hollow cylinders of PTFE and aluminum particles mixtures using Hopkinson bar Calef D.F. G Theoretical approaches to chemical dynamics in high compressed fluids 	 457-462 'Callen B.W.,  Lamb F.K., Sullivan J.D. F Insensitive interval in the evolution of shock waves from explosions ECampbell E.M.,  Holmes N.C.,  Libby S.B.,  Remington B.A., Teller E. F High energy-density physics: From nuclear testing to the superlasers  21-27 *Campbell E.M.,  Cauble R., Remington B.A. ? High energy density science on the National Ignition Facility  3-11 Campillo A.J., Schoen P.E. < Reflective probing of laser generated kbar shocks in water 	 347-350 $Cansell F.,  Fabre D., Petitet J.P. R Raman study of benzene phase transition under high pressure and high temperature >Cao B.Y.,  Meyers M.A.,  Nesterenko V.F.,  Benson D., Xu Y.B. T Shear localization-martensitic transformation interactions in Fe-Cr-Ni monocrystal aCao B.Y.,  Meyers M.A.,  Lassila D.H.,  Schneider M.S.,  Xu Y.B.,  Kalantar D.H., Remington B.A. Q Defect substructures in plate impacted and laser shocked monocrystalline copper  1145-1148 %Card�o P.A.,  Gois J.C., Campos J.A. . Thermal decomposition of energetic materials 	 853-856 =Carney J.R.,  Ladouceur H.D.,  Russell T.P., Pangilinan G.I. S A new method for determining material thermal properties at static high pressures  1143-1146 7Carney J.R.,  Miller J.S.,  Gump J.C., Pangilinan G.I. K Atmospheric effects on the combustion of detonating aluminized explosives 	 948-951 Carr M.J., Beauchamp E.K. s Transmission electron microscopical characterization of hot pressed shocked and unshocked aluminum nitride powder 0Carr M.J.,  Hills C.R.,  Graham R.A., Wise J.L. } The effects of microstructure on the hardness and deformation mode of shock-loaded 6061 aluminum and JBK-75 stainless steel 	 335-338 Butkovich T.R., Burton D.E. = Underground explosive fracture and permeability enhancement Buy F., Llorca F. e Shock wave effects in copper: Design of an experimental device for post recovery mechanical testing 	 319-322 B The expanding shell test: Numerical simulation of the experiment Buy F., Voltz C. H Shock loading influence on the mechanical behavior of high purity iron 	 533-536 Buy F.,  Voltz C., Llorca F. s Thermodynamically based equation of state for shock wave studies: Application to the design of experiments on tin  41-44 3Buzaud E.,  Hereil P.L.,  Pontiroli C., Lambert P. 9 Modeling the shock compression of concrete under 20 GPa Byers�Brown W., Horton T.V. c Analytical representation of high density fluid equations of state based on statistical mechanics Byers�Brown W., Braithwaite M. � Analytical representation of the adiabatic equation for detonation products based on statistical mechanics and intermolecular forces 	 325-328 = 	

 !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGI����JKLMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~�Williamsburg equation of state for detonation product fluid  73-76 d Entropy production in ZND detonation with realistic equations of state for explosives and products 	 353-356 LCady C.M.,  Gray�III G.T.,  Liu C.,  Trujillo C.P.,  Jacquez B.L., Mukai T. d Compressive properties of a closed-cell aluminum foam as a function of strain rate and temperature :Cagliostro D.J.,  Warnes R.H.,  Johnson N.L., Fujita R.K. ^ Spall measurements in shock-loaded hemispherical shells from free-surface velocity histories 	 367-370 Cagnoux J. ? Shock-wave compression of a borosilicate glass up to 170 kbar 	 392-396 Cagnoux J., Longy F. 4 Is the dynamic strength of alumina rate-dependent? 	 293-296 M Spherical waves in pure alumina: Effects of grain size on flow and fracture Cai H.,  Tang Z.P., Yang B. C Inverse method and consistency examination for Lagrangian anlysis 	 973-976 Cai J., Nesterenko V.F. 	 321-324 Bukowinski M.S.T. < Accurate self-consistent-field isotherms for NaCl to 30GPa 	 218-222 Bundy F.P. > A history of the science and technology of diamond synthesis 	 495-498 Buravova S. 2 Surface erosion under impact action of particles  1007-1010 Burchell M.J., Thomson R. D Intact hypervelocity particle capture in aerogel in the laboratory  1155-1158 ?Burchell M.J.,  Leliwa-Kopystynki J.,  Vaughan B., Zarnecki J. ; Comparison of H2O and CO2 ices under hypervelocity impact 	 949-952 Burchell M.J. 6 Microbial life and shock compression: Life or death?  1439-1444 Burkett M.W., Rabern D.A. W Stress fields generated by kinetic energy projectile interaction with ceramic targets 	 947-950 7Burkett M.W.,  Clancy S.P.,  Maudlin P.J., Holian K.S. n Modeling anisotropic plasticity: 3D Eulerian hydrocode simulations of high strain rate deformation processes 	 279-282 i Coupled plasticity and damage modeling and their applications in a three-dimensional Eulerian hydrocode 	 529-532 YBurley S.J.,  Bourne N.K.,  Fung V.,  Hollands R.,  Millett J.C.F.,  Milne A.M., Wood A. ; Advances in the understanding of the large-scale gap test 	 944-947 %Burns T.J.,  Grady D.E., Costin L.S. 5 On a criterion for thermo-plastic shear instability  372-37 Burns T.J. 6 Dynamic instability in adiabatic thermoplastic shear 	 145-146 7 A mechanism for high strain rate shear band formation ( Shock waves in Condensed Matter - 1989 	 345-348 4Burnside N.J.,  Son S.F.,  Asay B.W., Skidmore C.B. 3 Particle characterization of pressed granular HMX Burt J.A., Gupta Y.M. M Time-resolved ruby luminescence measurements under shock compression at 77K 	 695-697 dBushman A.V.,  Efremov V.P.,  Fortov V.E.,  Kanel G.I.,  Lomonosov I.V.,  Ternovoi V.Y., Utkin A.V. = Equation of state of composites under high energy densities  79-82 Q Shock and recovery of PTFE above and below the<   phase II to phase III transition 	 196-199 :Brown W.T.,  Schmidt M.F.,  Dzwilewski P.T., Samaras T.M. K Electromagnetic radiation from the detonation of metal encased explosives  1037-1040 Browning R.V. G Microstructural model of mechanical initiation of energetic materials 	 405-408 Browning J.S., Montoya J.L. / Hypervelocity impact tests of optical sensors . Shock Compression of Condensed Matter - 1995  1113-1116 Browning R.V., Scammon R.J. h Mechanical strength model for plastic bonded granular materials at high strain rates and large strains 	 277-280 G Microstructural model of ignition for time-varying loading conditions 	 987-990 :Browning R.V.,  Peterson P.D.,  Roemer E.L., Scammon R.J. 9 Grit particle enhanced non-shock ignition of explosives 	 921-924 XBrowning R.V.,  Peterson P.D.,  Roemer E.L.,  Oldenborg M.R.,  Thompson D.G., Deluca R. G Experimental study of grit particle enhancement in non-shock ignition  1041-1044 >Brusso J.A.,  Mikkola D.E.,  Bloom G.,  Lee R.S., Vonholle W. c Use of electric gun experiments to study the shock deformation behavior of 21-6-9 stainless steel 	 375-378 EBucholtz S.M.,  Gehr R.J.,  Rupp T.D.,  Sheffield S.A., Robbins D.L. 3 Temperature controller system for gas gun targets  1245-1248 Budge K.G. G ALE shock calculations using a stabilized serendipity rezoning scheme WBudin A.,  Bogomaz A.,  Kolikov V.,  Kuprin A.,  Leontiev V.,  Rutberg P., Shirokov N. I Investigation of heavy current discharges with high initial gas density 	 937-939 HBuelow S.J.,  Anderson J.E.,  Aiken A.C.,  Arrington�Jr. C.A., Jones B. I Mass spectral studies of shocked salts and nitrocellulose polymer films  1377-1380 Bukiet B., Menikoff R. 4 Sharp shock model for propagating detonation waves 	 259-262 
Bukiet B. , Solving curved detonation Riemann problems < Ceramic bar impact experiments for improved material model 	 727-730 Brar N.S., Rajendran A.M. 0 Confined alumina bar-on-bar impact experiments 	 843-846 &Braue W.,  Schneider H., Hornemann U. g Shock-wave induced formation of 'diaplectic' glasses of mullite 2Al2O3:1SiO2 composition: a TEM study 	 725-728 &Brenner D.W.,  Elert M.L., White C.T. W Incorporation of reactive dynamics in simulations of chemically-sustained shock waves 
Brenner D.W. = Molecular potentials for simulating shock-induced chemistry 	 115-121 Briggs M., Ferm E.N. r Axial VISAR velocity measurements of the non-planar acceleration of a plate from a penetrating shaped charge jet  1371-1374 -Britan A.,  Elperin T.,  Igra O., Jiang J.P. @ Head-on collision of a planar shock wave with a granular layer Brown W.T. e Numerical modeling of oblique impact hypervelocity impact using two-dimensional plane strain models 	 529-533 Brown J.M., Shaner J.W. P Rarefaction velocities in shocked tantalum and the high pressure melting point  91-94 'Brown J.M.,  Furnish M.D., Boness D.A. ) Sound velocities for San Carlos olivine 	 119-122 9Brown J.A.,  Gaffney E.S.,  Blaisdell G.L., Johnson J.B. B Techniques for gas gun studies of shock wave attenuation in snow 	 657-660 A A computational study of shock propagation in Indiana limestone 	 629-632 1Brown J.M.,  Slutsky L.J.,  Abramson E., Zaug J. f Sound velocities, elastic constants, thermal diffusivity, and structural relaxation at high pressure  35-38 Brown C.A., Russell T.P. = Time resolved emission studies of aluminum/water combustion 	 909-912 !Brown J.,  Curtis J.P., Lee P.R. ` Ab initio determination of the V of D of an octol from the statistics of its crystal structure 	 333-336 UBrown E.N.,  Rae P.J.,  Trujillo C.P.,  Dattelbaum D.M.,  Gray�III G.T., Bourne N.K.  1511-1514 'Braithwaite M.,  Sims C.E., Allan N.L. W Thermodynamic representations for solid/melt systems at high pressure and temperature 	 185-188 *Braithwaite C.H.,  Proud W.G., Field J.E. L The shock Hugoniot properties of quartz feldspathic gneiss and amphibolite  1435-1438 4Brannon P.J.,  Morris R.W.,  Konrad C.H., Asay J.R. H Shock-induced luminescence from X-cut quartz and Z-cut lithium niobate 	 303-306 Brannon R.M., Chhabildas L.C. $ Shock-induced vaporization of zinc 	 201-206 
Brannon R.M. / A consistent kinetics probability (CKP) model 	 301-304 ;Brannon R.M.,  Montgomery S.T.,  Aidun J.B., Robinson A.C. > Macro- and meso-scale modeling of PZT ferroelectric ceramics 	 197-200 9Bransky I.,  Hayek M.,  Halevy D.,  Miller S., Kivity Y. N Determination of dynamic mechanical properties from explosively driven rings 	 389-393 Brar N.S., Gupta Y.M. B Piezoresistance response of different batches of ytterbium foils 	 513-518 - Phase transition in shocked ytterbium foils 	 151-153 %Brar N.S.,  Bless S.J., Rosenberg Z. @ Factors affecting ballistic efficiency of alumina and sapphire 	 955-957 %Brar N.S.,  Rosenberg Z., Bless S.J. \ Applying Steinberg s model to the Hugoniot elastic limit of porous boron carbide specimens 	 467-470 Brar N.S., Rosenberg Z. L On the possibility of fracto-emission in ceramics during shock compression  1759-1762  Shock Hugoniot of 1215 steel 	 101-104 5Brar N.S.,  Espinosa H.D.,  Yuan G., Zavattieri P.D. D Experimental study of interface defeat in confined ceramic targets #Brar N.S.,  Hopkins A., Laber M.W. + Laser shock peening of titanium 6-4 alloy 
Brar N.S. = Failure waves in glass and ceramics under shock compression 	 601-606 Brar N.S., Joshi V.S. S Dynamic characterization of compliant/brittle materials using split Hopkinson bar 'Brar N.S.,  Proud W.G., Rajendran A.M. A Surface fracture zones in shock-loaded polycrystalline ceramics 	 493-496 K Simultaneous manganin gauge and VISAR measurements of shock wave profiles 	 849-852 Bourne N.K., Townsend D. / Variations in the conductivity of shocked KCl 	 109-112 ,Bourne N.K.,  Gray�III G.T., Millett J.C.F. - On the failure of shocked titanium diboride 	 589-592 5Bourne N.K.,  Millett J.C.F.,  Barnes N., Belcher I. L The deviatoric response of an epoxy resin to one-dimensional shock loading 	 649-652 6Bourne N.K.,  Millett J.C.F.,  Gray�III G.T., Mort P. < On the strength behaviour of Kel-F-800 and estane polymers 	 653-656 Bourne N.K., Gray�III G.T. - On the failure of boron carbide under shock 	 775-778 Bourne N.K., Vecchio K.S. ) Dynamic loading of a designer composite 	 689-692 Bourne N.K., Cooper G.A. . New insights into shock propagation in glass +Bourne N.K.,  Rosenberg Z., Millett J.C.F. 5 Propagation of waves through a float glass laminate Bourne N.K. 1 Mesoscale modelling of the response of aluminas $Boustie M.,  Cottet F., Romain J.P. a Spalling due to a strong shock wave decay process in solid targets irradiated by a pulsed laser DBoustie M.,  Seymarc C.,  Auroux E.,  de�Ress�guier T., Romain J.P. b Coating debonding induced by confined laser shock interpreted in terms of shock wave propagation /Bouyer V.,  Baudin G.,  Le�Gallic C., Herv� P. Q Emission spectroscopy applied to shock to detonation transition in nitromethane  1223-1226 Bovenkerk H.P. < The commercialization of high pressure synthesized diamond #Boyle V.M.,  Frey R.B., Bines A.L. 3 Parallel/oblique impact on thin explosive samples 	 819-822 ,Bragov A.M.,  Lomunov A.K., Sergeichev I.V. 1 High-speed behavior of some shape memory alloys <Bragov A.M.,  Lomunov A.K.,  Sergeichev I.V., Gray�III G.T. = Dynamic behaviour of birch and sequoia at high strain rates Z Optical measurements of shock-induced chemical reactions in mixed aluminum-nickel powder 	 767-772 8Boslough M.B.,  Cygan R.T.,  Venturini E.L., Morosin B. J Shock-chemistry in natural materials and evolution of planetary surfaces 	 381-386 Boslough M.B. i Thermochemical model for shock induced chemical reactions in porous thermite: The heat detonation model P Postshock spectral radiance measurements in nickel and nickel/aluminum powders <  	 617-620 wBoslough M.B.,  Chhabildas L.C.,  Reinhart W.D.,  Hall C.A.,  Miller J.M.,  Hickman R.,  Mullin S.A., Littlefield D.L. M PVDF gauge characterization of hypervelocity-impact-generated debris clouds  1833-1836 Boslough M.B., Crawford D.A. Y Impact-generated atmospheric plumes: Observations of Jupiter and implications for Earth  1187-1190 ,Botcher T.R.,  Ladouceur H.D., Russell T.P. 7 Pressure dependent laser induced decomposition of RDX 	 989-992 Boteler J.M., Lindfors A.J. 7 Shock loading studies of AP/Al/HTPB based propellants 	 767-770 
Boteler J.M. 7 Compression-shear study of glass reinforced polyester 	 537-540 (Boteler J.M.,  Rajandran A.M., Grove D. 2 Shock wave profiles in polymer matrix composites 	 563-566 Bouchu M., Guillamot J.-Y. = Application of PVF2 active gage as an initiation diagnostic 	 553-558 Bourasseau E., Maillet J.-B. Q Parameter optimization for charge equilibration method in molecular simulations 	 565-568 Bourcier R.J., Chhabildas L.C. + High velocity erosion of metal interfaces 	 741-744 5Bourne N.K.,  Rosenberg Z.,  Crouch I.G., Field J.E. R Microstructural variations in seven aluminas and their effect on impact response 	 769-772 Bourne N.K., Rosenberg Z. ) The dynamic response of soda-lime glass 	 567-572 S Fractoemission and its effect upon noise in gauges placed near ceramic interfaces  1053-1056 'Bourne N.K.,  Rosenberg Z., Field J.E. a Melting along the Hugoniots of KBr and CaBr: Optical pyrometry-rarefaction overtake experiments ) Heat capacity of shocked alkali halides  85-88 Boness D.A. g Metastability in shocked iron: Controversy with regard to sound velocity and temperature measurements  77-80 1Boness D.A.,  Brown J.M.,  Morgan M., Madamba J. � Disagreement between shock and static temperature data: Calculation of argon optical transmittance in laser-heated diamond anvil cells 	 173-176 &Bonora N.,  Ruggiero A., Milella P.P. ( Fracture energy effect on spall signal 	 439-442 CBonora N.,  Ruggiero A.,  Flater P.J.,  House J.W., DeAngelis R.J. ^ On the role of material post-necking stress-strain curve in the simulaiton of dynamic impact 	 701-704 =Boogerd P.,  Verbeek H.J.,  Stuivinga M., van�der�Steen A.C. 6 Shock wave equation of state for metals and ceramics  89-92 #Bordzilovsky S.A., Karakhanov S.M. A Electrical resistivity of PTFE layers under dynamic compression 	 801-804 6Bordzilovsky S.A.,  Karakhanov S.M., Merzhievsky L.A. O Shock response of a unidirectional composite at various orientation of fibers 	 545-548 
Borg J.P. [ Estimating the break-up diameter of an impulsively driven initially smooth fluid cylinder 	 715-718 UBorg J.P.,  Schwalbe L.,  Cogar J.,  Chapman D.J.,  Tsembelis K.,  Ward A., Lloyd A. 5 Dynamic compaction modeling of porous silica powder  37-40 HBorodina T.I.,  Fortov V.E.,  Milyavskiy V.V.,  Zharkov A.S., Zhuk A.Z. < Shock wave synthesis of carbyne from graphite: New results  1082-1085 /Borschevsky A.O.,  Gorshkov M.M., Tarasov A.M. C The twofold quartzite shock adiabat under pressures of 55-150 GPa  95-98 Boslough M.B., Ahrens T.J. Q A method of determining points on the principal isentropes of molecular liquids 	 236-240 9 Particle velocity experiments in anorthosite and gabbro 'Boslough M.B.,  Graham R.A., Webb D.M. KBocquillon C.,  Bogicevic C.,  Clerc F.,  L�ger J.M.,  Fabre C., Rassat A. O Synthesis of diamond at high pressure and high temperature from C60 fullerene 	 647-650 Bodner S.R., Rajendran A.M. F On the strain rate and temperature dependence of hardening of copper 	 499-502 Boehler R. > The phase diagram of iron to 2 Mbar: New static measurements + High-precision grinding of diamond anvils  1619-1620 Boettger J.C., Wallace D.C. 8 A model for the shock-induced phase transition in iron 	 129-132 =Boettger J.C.,  Honnell K.G.,  Mori Y.,  Niiya N., Mizuno T. 3 Theoretical equation of state for beryllium oxide  33-36 Bogach A.A. E Analysis of temperature influence on the dynamic fracture of metals 	 223-226 NBokarev V.P.,  Temnitsky I.N.,  Bondarev Y.M.,  Mardashev Y.S., Batsanov S.S. W Effect of explosion on the catalytic properties of stochiometric inorganic substances 	 827-829 vBoley M.S.,  Thomas R.J.,  Chandrasekhar M.,  Chandrasekhar H.R.,  Ram-Mohan L.R.,  Samarth N.,  Luo H., Furdyna J.K. � Hydrostatic pressure studies of optical transitions in the photoluminescence spectra of Zn1-xCdxSe thick epilayers and Zn1-xCdxSe/ZnSe strained layer multiple quantum wells 	 203-206 IBoley M.S.,  Chandrasekhar M.,  Chandrasekhar H.R.,  Wu Y., Boolchand P. u Hydrostatic pressure studies of the Raman-active phonon modes in the bulk high-temperature superconductor YBa2Cu4O8 	 681-684 TBolis C.,  Berthe L.,  Boustie M.,  Arrigoni M.,  He H.L.,  Jeandin M., Barradas S. v VISAR pull-back signals as a diagnostic for the laser adherence test applied to copper coating on aluminum substrate  1373-1376 &Boness D.A.,  Brown J.M., Shaner J.W. % Rarefaction studies in shocked lead Boness D.A., Brown J.M. M Time-resolved optical spectroscopy of shock-compressed fluid alkali halides 	 863-866 Boness D., Brown J.M. Q The effect of shock rise time on strength of alumina in 1D stress and 1D strain 	 711-714 Bless S., Chau R. $ Tensile failure of tungsten alloys Bloom G.H. 6 Gr�neisen parameter measurements for high explosives 	 588-592 FBloom G.,  Chau H.,  Glaser R.,  Honodel C.,  Lee R.S., Weingart R.C. D Improvements in thin-pulse shock initiation threshold measurements GBloom G.,  Duncan A.,  Honodel C.,  Lee R.,  von�Holle W., Weingart R. h Changes in the particle size distribution of LX-17 samples induced by 3.5 ti 11 GPa planar shock waves 	 569-571  Bloomquist D.D., Sheffield S.A. X Shock-compression temperature rise determined from resistivity of embedded metal foils 	 304-308 Blumenthal W.R., Gray�III G.T. M Characterization of shock-loaded aluminum-infiltrated boron carbide cermets 	 393-396 KBlumenthal W.R.,  Abeln S.P.,  Cannon D.D.,  Gray�III G.T., Carpenter R.W. R Influence of strain rate and temperature on the mechanical behavior of beryllium 	 411-414 `Blumenthal W.R.,  Gray�III G.T.,  Idar D.J.,  Holmes M.D.,  Scott P.D.,  Cady C.M., Cannon D.D. _ Influence of temperature and strain rate on the mechanical behavior of PBX 9502 and Kel-F 800 	 671-674 DBlumenthal W.R.,  Cady C.M.,  Lopez M.F.,  Gray�III G.T., Idar D.J. j Influence of temperature and strain rate on the compressive behavior of PMMA amnd polycarbonate polymers (Blumenthal W.R.,  Brown D.W., Tom� C.N. A Evolution of crystallographic texture and strength in beryllium 	 525-528 (Bock W.J.,  Urbanczyk W., Wisniewski R. X Fiber-optic pressure sensor using an electronically scanned white-light interferometer  1687-1690 }Bockowski M.,  Grzegory I.,  Wr�blewski M.,  Witek A.,  Jun J.,  Krukowski S.,  Porowski S.,  Ayral-Marin R.M., Tedenac J.C. M Combustion synthesis of AlN at high pressure of nitrogen and argon mixtures  1255-1258 K Reflectometric detection of shock wave propagation within a concrete wall Billingsley J.P. M Energetic materials shock sensitivity relevance to specific heat properties 	 429-432 ( The Hugoniot elastic limit decay limit 	 199-202 b HMX and HNS shock sensitivity correlation with specific heat and reactive temperature magnitudes 	 899-902  The HEL upper limit 	 735-738 Binggeli N., Chelikowsky J.R. 3 is simulated 'amorphous' silica really amorphous? 	 397-400 Birnboim A., Rosenberg Z. 8 The response of shocked quartz gauge to impact loading Bjorkman M.D., Shrader J.E. X Shock wave propagation in beryllium at small impact stresses and elevated temperatures 	 432-436 Bjorkman M.D., Holsapple K.A. P Plane hypervelocity impact and source similitude dependence on a Tillotson EOS 	 195-198 Bless S.J. , Hypervelocity impact response of Ti and Be 	 548-552 J Impact physics facilities at the University of Dayton Research Institute < 	 668-673 Bless S.J., Paisley D.L. ) Dynamic tensile fracture of OFHC copper $Bless S.J.,  Yaziv D., Rosenberg Z. ) Spall zones in polycrystalline ceramics ! Shock Waves in Condensed Matter 	 419-424 %Bless S.J.,  Brar N.S., Rosenberg Z. 5 Strength of soda lime glass under shock compression & Shock Waves in Condensed Matter 1987 	 309-312 = Failure of ceramic and glass rods under dynamic compression Bless S.J., Brar N.S. J Load/unload hysteresis in ceramics measured by a reverberation technique 	 483-486 ' Impact induced fracture of glass bars  1813-1816 , Penetration mechanics of non-circular rods  1119-1122 Bless S.J., Satapathy S. 1 Penetration of thick targets by yawed long rods 	 933-936 Bless S.J., Cazamias J. Z Using the penetration-velocity relationship to correct for variations in target hardness  1291-1293 Bless S.J., Bourne N.K. K Participation of aluminum in two-dimensional shock initiation experiments 	 573-576 Bernecker R.R. / Shock initiation of some aqueous HMX mixtures 	 695-698 . Hugoniots of some elastomeric binder systems 	 137-140 & Observations on the Hugoniot for HMX 	 141-144 Bernecker R.R., Simpson R.L. E Further observations on HMX particle size and buildup to detonation 	 719-722 Bernhard R.P., H�rz F. Z Fragmentation history of glass projectiles impacting aluminum targets at 0.5 to 1.5 km/s  1147-1150 Bernhard R.P., Christiansen E. d Analysis of microstructures and projectile residues in hypervelocity impacts on fused silica glass Berry R.A., Williamson R.L. K A multiphase mixture for the shock induced consolidation of metal powders 	 335-340  Bessette G.C., Littlefield D.L. J Analysis of transverse loading in long-rod penetrators by oblique plates 	 937-940 \Bessette G.C.,  Lawrence R.J.,  Chhabildas L.C.,  Reinhart W.D.,  Thornhill T.F., Saul W.V. K Multi-dimensional hydrocode analyses of penetrating hypervelocity impacts  1323-1326 mBesson J.M.,  Pruzan P.,  Klotz S.,  Hamel G.,  Silvi B.,  Nelmes R.J.,  Loveday J.S.,  Wilson R.M., Hull S. e Interatomic distance in D2O VIII under high pressure from neutron scattering measurements to 10 GPa ,Bezruchko G.S.,  Kanel G.I., Razorenov S.V. E Measurements of sound speed in zinc in the negative pressure region :Bezruchko G.S.,  Razorenov S.V.,  Kanel G.I., Fortov V.E. A Influence of temperature upon the a to w transition in titanium 	 192-195 %Bhate N.,  Clifton R.J., Phillips R. g Atomistic simulations of the motion of an edge dislocation in aluminum using the embedded atom method 	 339-342 5Bickham S.R.,  Lenosky T.,  Collins L.A., Kress J.D. * Simulations of shock-compressed hydrogen  45-48 Biele J.K. 5 Sounding experiments of high pressure gas discharge 	 891-894 	 259-260 Bennett B.I., Liberman D.A. 2 Quantum mechanical effects on the shock Hugoniot  49-52 2Bennett L.S.,  Iyer K.R.,  Sorrell F.Y., Horie Y. 7 Shock induced exothermic reactions in powder mixtures 	 605-608 Beno T.,  Bless S., Nichols S. ; New phenomena observed in plate impacts onto alumina bars 	 839-842 Benson D.A., Baer M.R. . Grain burning experiments with HMX explosive Benson D.J., Nellis W.J. ? Numerical simulation of the shock compaction of copper powder Benson A.K. y Inversion of compressional elastic wave data as a fnction of off set to recover bulk modulus, shear modulus and density -Benson D.J.,  Nesterenko V.F., Jonsdottir F. ; Micromechanics of shock deformation of granular materials 	 603-606 � Characterizing subsurface lithology with elastic parameter contrasts from the decomposition and inversion of the elastic wave equation  1283-1286 Benson A.K., Wu J. � Predicting elastic properties of porous fluid-filled rocks by inverting the BGG equation: Applications to seismic and borehole data  1291-1294 !Benson D.J.,  Do I., Meyers M.A. < Computational modeling of the shock compression of powders  1087-1092 �Benuzzi-Mounaix A.,  Huser G.,  Koenig M.,  Faral B.,  Grandjouan N.,  Batani D.,  Henry E.,  Tomasini M.,  Marchet B.,  Hall T.,  Boustie M.,  de�Ress�guier T.,  Hallouin M., Guyot F. H Experimental study of highly compressed iron using laser driven shocks  83-86 $Berghout H.L.,  Son S.F., Asay B.W. : Measurement of convective burn rates in gaps of PBX 9501 Bergmann O.R. b Industrial uses of explosive pressure: From rock blasting to metal bonding and synthetic diamond 	 429-433 Bergstresser T., Becker S. D Temperature measurement of isentropically accelerated flyer plates  1169-1172 @Bernecker R.R.,  Clairmont�Jr. A.R.,  Sandusky H.W., Smith M.S. $ Piezoelectric polymer shock gauges  1183-1186 4Baumung K.,  Singer J.,  Razorenov S.V., Utkin A.V. d Hydrodynamic proton beam-target interaction experiments using an improved line-imaging velocimeter  1015-1018 /Baumung K.,  Kanel G.I.,  M�ller G., Singer J. a Measurement of the adhesive strength of 200 mm thick turbine blade coatings by a dynamic method  1207-1210 ABeard B.C.,  Sharma J.,  Sandusky H.W.,  Glancy B.C., Elban W.L. N Dislocation density variation in shocked single crystal ammonium perchlorate 	 571-574 $Bedrov D.,  Smith G.D., Sewell T.D. ` Molecular dynamics simulations of HMX crystal polymorphs using a flexible molecule force field 	 403-406 *Beissel S.R.,  Gerlach C.A., Johnson G.R. ] Three-dimensional impact simulations by conversion of finite elements to meshfree particles 	 193-196 	Belak J. < Computer simulation of molecular response at a shock front  1063-1066 X Molecular dynamics simulation of high strain rate void nucleation and growth in copper 	 211-214 Belgaumkar B.M. K Shock induced instability due to crack-like defects in a solid propellant 	 598-602  American Institute of Physcs.Belgelzimer Y.E.,  Efros B.M., Shishkova N.V. ) Metal fracture at hydrostatic extrusion  1051-1054 Bell P.M.,  Xu J., Mao H.K. | Static compression of gold and copper ad calibration of the ruby pressure scale to pressures to 1.8 Megabars (static, RNO) 	 125-130 ;Beloshenko V.A.,  Slobodina V.G.,  Grinjov V.G., Prut E.V. L New method of processing compositions based on high molecular polyethylene  1029-1030 Benedict U. ? Updated diagrams of high-pressure phase relations in f-metals 	 241-244 %Benham R.A.,  Weirick L.J., Lee L.M. : Calibration of thin-foil manganin gauge in ALOX material  1061-1064 7Benjamin R.F.,  McQueen R.G.,  Marsh S.P., Shaner J.W. @ Results on Richtmyer-Meshkov instabilities in condensed fluids 2Baudin G.,  Le�Gallic C.,  Davoine F., Bouinot P. d Experimental method to determine the detonation characteristics of a very non-ideal high explosive 	 940-943 	Bauer F. J Behavior of ferroelectric ceramics and PVF2 polymers under shock loading 	 251-267  ISL shock wave facilities 	 674-679 r Piezoelectric and electric properties of PVF2 polymers under shock wave action: Application to shock transducers ( Shock Waves in Condensed Matter - 1983 	 225-228 a Ferroelectric properties and shock response of a poled PVF2 polymer and of VF2/C2F3H copolymers 	 483-496 Bauer F., Moulard H. R State-of-the-art in the research work of piezoelectric PVDF polymer shock gauges 	 627-630 Bauer F., Lichtenberger A. C Use of PVDF shock gauges for stress measurements in Hopkinson bar 	 631-634 Bauer F., Graham R.A. C Behaviour of VF2/VF3 piezoelectric copolymers under shock loading 	 793-796 KBauer F.,  Graham R.A.,  Anderson M.U.,  Lefebvre H.,  Lee L.M., Reed R.P. U Response of the piezoelectric polymer PVDF to shock compression greater than 10 GPa 	 887-890 6 High pressure applications of ferroelectric polymers  1727-1730 #Bauer F.,  Moulard H., Graham R.A. k Piezoelectric response of ferroelectric polymers under shock loading: Nanosecond piezoelectric PVDF gauge  1073-1076 UBauer F.,  Isner-Brown P.,  Moulard H.,  Couturier S.,  De�Resseguier T., Boustie M. Z Piezoelectric P(VDF-TrFE) thick copolymers: Response in current mode under shock loading  1077-1080 <  !Bauer F.,  Moulard H., Samara G. B Advances in ferroelectric polymers for shock compression sensors U Advances in PVDF shock sensors: Applications to polar materials and high explosives  1023-1028 P PVDF gauge piezoelectric response under two-stage light gas gun impact loading  1149-1152 6 PVDF shock compression sensors in shock wave physics  1121-1124 KBarrett W.H.,  Greenwoll J.I.,  Smith C.W.,  Johnson D.E., De�la�Cruz C.F. � Noise measurements in shunted, shorted, and fully electroded quartz gauges in the Saturn plasma radiation source X-ray simulator  1029-1032 9Barrett J.J.C.,  Robertson D.H.,  Elert M.L., White C.T. C Detonation Hugoniot for ozone from molecular dynamics simulations 	 329-331 Bartkowski T., Dandekar D.P. = Spall strengths of sintered and hot pressed silicon carbide 	 535-538 Bartkowski P.T., Dandekar D.P. 7 Recompression of PMMA following shock induced tension ,Bartkowski P.T.,  Dandekar D.P., Grove D.J. 1 Spallation of hot pressed boron carbide ceramic 	 779-782 9Barzhkin V.V.,  Lyapin A.G.,  Popova S.B., Voloshin R.N. M Amorphization of high pressure phases: Application to silicon and germanium 	 249-250 Bashkirov A.G., Orlov A.V. C Shock wave structure for some non-analytical-in-velocity closures 
Bass R.C. K Measurements and calculations of shock propagation in dry desert alluvium 	 633-637 6Bassett W.A.,  Weathers M.S.,  Wu T.-C., Holmquist T. ) Equation of state of SiC up to 68.4 GPa 	 145-148 Bassett W.A., Weathers M.S. V Fullerence structures produced from melted diamond at high pressure by laser heating J Thermodynamic significance of a high-pressure/temperature bcc iron phase 	 915-918 VBatalov S.V.,  Averin A.N.,  Batalova I.A.,  Loboiko B.G.,  Litvinov B.V., Filin V.P. 7 On the mechanism of diamond formation from explosives 	 753-755 )Batkov Y.V.,  Novikov S.A., Fishman N.D. 4 Shear stresses in polymers under shock compression 	 577-580 GBatkov Y.V.,  Knyazev V.N.,  Novikov S.A.,  Raveski V.A., Fishman N.D. 5 Shear strength of aluminum at shockless compression 	 501-504 Batsanov S.S. % Perspectives on inorganic chemistry ( Shock Waves in Condensed Matter - 1981  1-3 2 Inorganic synthesis under shock-wave compression  14-26 V The material point method and simulation of wave propagation in heterogeneoous media 	 187-192 :Bardenhagen S.G.,  Brydon A.D.,  Williams T.O., Collet C. p Coupling grain scale and bulk mechanical response for PBXs using numerical simulations of real microstructures 	 479-482 Bardo R.D., Jones W.H. H A theoretical calculation of the 0 K isotherm for shocked nitromethane 	 621-624 Bardo R.D. = Rate-determining steps for ignition of shocked nitromethane 	 843-856 � Theoretical study of the coupling of electrons and lattice wave packets in superconducting metastable states formed at high shock pressures 	 595-598 J Theoretical prediction of novel molecular solids formed at high pressure 	 209-216 Bardwell S., Parpart-Henke U. : The use of strong shock waves for isentropic compression 	 331-333 Barker L.M. 3 High-pressure quasi-isentropic impact experiments 	 217-224 2Barker L.M.,  Trucano T.G.,  Wise J.L., Asay J.R. T Experimental technique for measuring the isentrope of hydrogen to several megabars 	 455-459 )Barker L.M.,  Trucano T.G., Munford J.W. 8 Metal surface gouging by hypervelocity sliding contact 	 753-756 8Barker L.M.,  Chhabildas L.C.,  Trucano T.G., Asay J.R. ' Gas-accelerated plate stability study 	 989-991 ' The accuracy of VISAR instrumentation 	 833-836 G The development of the VISAR and its use in shock compression science  11-17 C Multi-beam VISARs for simultaneous velocity vs. time measurements 
 999-1002 1Barlow A.J.,  Winter R.E.,  Carley D., Taylor P. C Hydrocode modelling and analysis of a dynamic friction experiment 	 521-524 (Barnes N.,  Bourne N.K., Millett J.C.F. & The shock Hugoniot of an epoxy resin 	 135-138 ;Barrett J.J.C.,  Brenner D.W.,  Robertson D.H., White C.T. 2 Detonation of solid O3: Effects of void collapse 	 191-194 'Baker E.L.,  Schimel B., Grantham W.J. P Numerical optimization of ignition and growth reactive flow modeling for PAX2A 	 409-412 Bakhralh S.M.,  Volodina N.A.,  Drennov O.B.,  Goreva T.A.,  Mikhailov A.L.,  Nizovtsev P.N.,  Spiridonov V.F., Shuvalova E.V. � Numerical simulation and experimental study of coating stabilizing effect on shear instability growth in oblique impact of metal slabs  1363-1366 ?Balagansky I.A.,  Balagansky A.I.,  Razorenov S.V., Utkin A.V. 2 Evolution of shock waves in silicon carbide rods 	 835-838 
Ball G.J. * Numerical simulation of dynamic friction  1503-1506 <Ballard P.,  Fournier J.,  Fabbro R.,  Frelat J., Castex L. + Residual stresses induced by laser shocks 	 341-344 7Bandak F.A.,  Armstrong R.W.,  Douglas A.S., Tsai D.H. 4 Nanodislocation structures for shock strengthening &Bandyopadhyay A.,  Das K., Gupta Y.M. I Shock wave synthesis of titanium silicide. 2: Effect of ceramic fillers  1079-1081 4Bar-On E.,  Rajendran A.M.,  Bless S.J., Grove D.J. 5 Modeling of dynamic fracture in a solid cone target 	 939-942 Bar-on E., Yankelevsky D.Z. _ Using Maxwell-Boltzmann's statistics for microcracks distribution function in a failure model  1165-1168 5Bar-on E.,  Partom Y.,  Rubin M.B., Yankelevsky D.Z. ( On the HEL and the 'ramping' above HEL 	 739-742 Barbee�III T.W. 2 Phonons and metastability in compressed nitrogen 	 163-166 Barbieri F., Patuelli C. h Recovery of copper after shock-loading by means of Fourier analysis of x-ray diffraction line profiles 	 453-456 @Bardenhagen S.G.,  Harstad E.N.,  Foster�Jr. J.C., Maudlin P.J. 7 Viscoelastic models for polymeric composite materials 	 327-330 PBardenhagen S.G.,  Harstad E.N.,  Maudlin P.J.,  Gray�III G.T., Foster�Jr. J.C. 4 Viscoelastic models for explosive binder materials /Bardenhagen S.G.,  Greening D.R., Roessig K.M. F Initial free-surface velocities imparted by grazing detonation waves 	 919-922 Backofen J.E., Weickert C.A. � Effect of an inert material's thickness and properties on the ratio of energies imparted by a detonation's first and second propulsion stages 	 954-957 F Obtaining the Gurney energy constant for a two-step propulsion model 	 958-961 Backofen J.E. x Additional information showing that a cylinder's material and geometry affect measuring an explosive's Gurney velocity 	 445-448 b Modeling a material's instantaneous velocity during acceleration driven by a detonation gas-push 	 936-939 (Badding J.V.,  Nesting D.C., Baron R.B. I In situ study of the solubility of hydrogen in rhenium at high pressure  1317-1320 
Baer M.R. T A mixture model for shock compression of porous multi-component reactive materials  1247-1250 #Baer M.R.,  Hertel E.S., Bell R.L. 6 Multidimensional DDT modeling of energetic materials 	 433-436 M Computational modeling of heterogeneous reactive materials at the mesoscale  27-33 Baer M.R., Trott W.M. G Mesoscale descriptions of shock-loaded heterogeneous porous materials 	 713-716 7 Mesoscale studies of shock loaded tin sphere lattices 	 517-520 Baer B.J., Yoo C.-S. n Vibrational spectra of dense molecular fluids in a laser-heated DAC: Implications to shock-compressed fluids  1249-1252 DBaer M.R.,  Hall C.A.,  Gustavsen R.L.,  Hooks D.E., Sheffield S.A. R Isentropic compression experiments for mesoscale studies of energetic composites  1307-1310 $Bahl K.L.,  Lee R.S., Weingart R.C. Q Velocity of spherically-diverging detonation waves in RX-26-AF, LX-17 and LX-10 	 559-562 Bai C., Ding J. c A numerical study of hot spot formation and ignition of composite propellants under shock loading 	 291-294 Bai C.,  Huang F., Ding J. 6 Behavior of ammonium perchlorate under shock loading ,Atou T.,  Kikuchi M.,  Fukuoka K., Syona Y. � Shock induced phase transition of scandium sesquioxide: Geometric factor governing high pressure transitions on rare earth sesquiox<  ides 	 331-334 FAtroshenko S.A.,  Zhigachieva N.I.,  Meshcheryakov Y.I., Tomilin M.G. D The method of visualisation of dynamic deformation modes in metals 	 611-613 Attia A.V. E Numerical simulation of shock response of fluid-filled porous rocks 	 637-640 "Attia A.V.,  Moran B., Glenn L.A. = Comparative yield estimation via shock hydrodynamic methods 	 281-284 3Atwood A.I.,  Curran P.O.,  Price C.F., Wiknich J. @ Quasi-static compaction studies of a porous pyrotechnic powder 	 745-748 $Auroux E.,  Boustie M., Romain J.P. o Improvement of the laser spallation technique using an amplifying layer: Experimental and numerical technique  1211-1214 �Avdonin V.V.,  Postnov V.I.,  Kagan K.L.,  Shakhray D.V.,  Shestakov A.F.,  Nikolaev R.K.,  Sidorov N.S.,  Kveder V.V.,  Osipyan Y.A., Fortov V.E. \ Conductivity of C60 fullerene crystals under multi-step dynamic compression up to 300 kbar 	 189-191 ;Averin A.B.,  Dremov V.V.,  Samarin S.I., Sapozhnikov A.T. / Equation of state and phase diagram of carbon  65-68 sAverin A.N.,  Alekseev A.V.,  Batalov S.V.,  Loboiko B.G.,  Litvinov B.V.,  Sumin V.D.,  Filin V.P., Yagnakov A.N. m Investigation into low-temperatures influence on high explosive compounds sensitivity to shock-wave impacts 	 847-849 {Averin A.N.,  Batalov S.V.,  Belenovsky Y.A.,  Kostitsyn O.V.,  Loboiko B.C.,  Pestrechikhin V.A.,  Sumin V.D., Filin V.P. ? Studying properties of explosives exposed to organic solvents 	 917-920 MAverkov O.N.,  Gryadobitov S.P.,  Kozlov E.A.,  Lupilin G.A., Matushkin N.D. � A solid state calorimeter for measuring the internal energy increment of metal samples, capable of surviving explosive loading 	 859-862 Backofen J.E., Weickert C. 2Asay B.W.,  Laabs G.W.,  Peterson P.D., Funk D.J. Q Measurement of strain and temperature fields during dynamic shear of explosives @Asay B.W.,  Henson B.F.,  Dickson P.M.,  Fugard C.S., Funk D.J. b Direct measurement of strain field evolution during dynamic deformation of an energetic material 	 567-570 
Asay J.R. 9 Isentropic compression experiments on the Z accelerator 	 261-266 Asay J.R.,  Hall C.A.,  Holland K.G.,  Bernard M.A.,  Stygar W.A.,  Spielman R.B.,  Rosenthal S.E.,  McDaniel D.H., Hayes D.B. 7 Isentropic compression of iron with the Z accelerator  1151-1154 ) Shock wave paradigms and new challenges  26-35 <Asay B.,  Dickson P.,  Henson B.,  Smilowitz L., Tellier L. X Effect of temperature profile on reaction violence in heated and self-ignited PBX 9501  1065-1068 Y Wave structure studies in condensed matter physics: Single crystals to magnetic effects  3-10 1Asay B.W.,  Son S.F.,  Busse J.R., Oschwald D.M. _ Observations on the mechanism of reaction propagation in metastable intermolecular composites 	 827-830 =Asay B.W.,  Tasker D.G.,  King J.C.,  Sanders V.E., Son S.F. W Electrical conductivity measurements in reacting metastable intermolecular composites 	 927-930 2Ashuach Y.,  Rosenberg Z.,  Dekel E., Ginzburg A. > More on the strength of materials under high shock pressures  1241-1244 #Aslam T.D.,  Bdzil J.B., Hill L.G. 2 Analysis of the LANL detonation-confinement test Aslam T.D. + Direct numerical simulation of detonation 	 931-935 Asokamani R., Amirthakumari M. ] Metallisation and superconductivity in some of the ionic and covalent solids under pressure 	 665-668 (Assink R.A.,  Boslough M.B., Cygan R.T. N Characterization of amorphous material in shocked quartz by NMR spectroscopy 	 383-386 +Atisivan R.,  Bandyopadhyay A., Gupta Y.M. 3 Dynamic tensile response of alumina-Al composites 	 697-700 Armstrong R.W., Grise W.R. / Hot spots from dislocation pile-up avalanches  1033-1036 	Arndt J. " Shock isotropization of minerals 	 473-480 Arnold W., Sachs W. F Measuring and simulation of steady shock wave profiles in Armco iron 	 337-340  Arnold W.,  Held M., Stilp A.J. # Spallation behavior of Armco iron 	 421-424 
Arnold W. D Influence of twinning on the elasto-plastic behavior of armco iron 	 539-542 ( High strain rate failure of Armco iron  1035-1038 B Initiation threshold of an insensitive underwater high explosive 	 911-914  Controlled fragmentation 	 527-530 8 Tungsten heavy alloys for multiple impact applications  1319-1322 Arrieta H.V., Espinosa H.D. @ High and low temperature dynamic testing of advanced materials  1075-1078 TArrigoni M.,  Boustie M.,  He H.L.,  Bolis C.,  Berthe L.,  Barradas S., Jeandin M. T Benefits of the impedance mismatch technique for laser shock adhesion test (LASAT)  1369-1372 :Asakawa Y.,  Aizawa T.,  Shono Y.,  Fukuoka K., Kihara J. M Shock-induced reaction from mechanically alloyed precursor in 3Ni-Al system "Asano T.,  Cosstick K., Furuta H. _ Experimental evidence for a two-step mechanism of diffusion-controlled unimolecular reactions  1325-1328 'Asay J.R.,  Chhabildas L.C., Wise J.L. : Strain rate effects of beryllium under shock compression 	 427-431 8Asay J.R.,  Chhabildas L.C.,  Kerley G.I., Trucano T.G. , High pressure strength of shocked aluminum 	 145-149 *Asay J.R.,  Trucano T.G., Chhabildas L.C. E Time-resolved measurements of shock-induced vapor-pressure profiles 	 159-162 Asay J.R., Trucano T.G. M Experimental measurements of shock-induced vaporization in cadmium and lead 	 143-146 5Asay B.W.,  Ramsay J.B.,  Anderson M.U., Graham R.A. 5 Shock compression of Dupont Detasheet at low stress 	 679-682 5 Wave propagation in intact and jointed calcite rock 	 831-834 .Antoun T.,  Seaman L.,  Curran D., Glinsky M. S Damage and failure mechanisms associated with photoablation of biological tissues  1277-1280 5Antoun T.N.,  Vorobiev O.Y.,  Lomov I.N., Glenn L.A. 4 Simulations of an underground explosion in granite  1279-1282 Antoun T.H., Lomov I.N. [ Simulation of a spherical wave experiment in marble using a multidirectional damage model  1423-1426 $Ao T.,  Chiu G.,  Forsman A., Ng A. J Optical signatures of a shock wave emerging from a metallic free surface 	 971-974 Ao T.,  Vollrath I., Ng A. 6 Optical probing of the electron temperature gradient  1243-1246 $Aoki K.,  Yamawaki H., Sakashita M. @ Infrared study of phase transition in solid CO2 under pressure 	 263-266 lArad B.,  Moshe E.,  Eliezer S.,  Dekel E.,  Ludmirsky A.,  Henis Z.,  Goldberg I.B.,  Eliaz N., Eliezer D. e Spall strength measurements in aluminum, copper and metallic glass at strain rates of about 107 s-1 	 459-462 8Arad B.,  Werdiger M.,  Moshe E.,  Henis Z., Eliezer S. I Velocity interferometer data reduction beyond optical delay limitations  1139-1142 Araki M., Leiber C.O. \ Linear relation between shock velocity and pressure in relation to the Gr�neisen parameter 	 547-550 Arienti M., Shepherd J.E. K Superseismic loading and shock polars: An example of fluid-solid coupling 	 251-254 Arione S.E., Duvall G.E. M Temperature dependence of the precursor amplitude in <111> lithium fluoride 	 299-302 Arione S.E., Bjorkman M.D. = Scaling of hole diameter from perforating impacts of plates 	 749-752 7Armstrong R.W.,  Zerilli F.J.,  Holt W.H., Mock�Jr. W. _ Dislocation mechanics based constitutive relations for plastic flow and strength of HY steels  1001-1004 Armstrong R.W., Elban W.L. 4 Dislocation characteristics in energetic materials 	 723-726 6 The penetration performance of short L/D projectiles  1809-1812 Anderson�Jr. C.E., Walker J.W. B An analytic expression for P/L for WA long rods into armor steel  1135-1138 MAnderson�Jr. C.E.,  Bless S.J.,  Sharron T.R.,  Satapathy S., Normandia M.J. 4 Investigation of yawed impact into a finite target 	 925-928 8Anderson�Jr. C.E.,  Popelar C.H.,  Nagy A., Walker J.D. ; A novel method for determining dynamic fracture toughness 	 505-508 "Anderson�Jr. C.E., Dannemann K.A. E Deformation and damage of two aluminum alloys from ballistic impact  1298-1301 0Anderson�Jr. C.E.,  Orphal D.L., Templeton D.W. m Re-examination of the requirements to de<  tect the failure wave velocity in SiC using penetration experiments 	 707-710 =Anderson�Jr. C.E.,  Nicholls A.E.,  Chocron S., Ryckman R.A.  Taylor anvil impact  1367-1370 (Andreev N.E.,  Fortov V.E., Kostin V.V. 3 Shock wave generation by ultra-short laser pulses  1259-1260 =Andrews S.,  Glancy B.,  Forbes J.,  Collignon S., Hudson L. U Experiments on the modification of the energy release rate in a non-ideal explosive 	 799-802 *Andrews T.D.,  Radford D.D., Tsembelis K. = The response of a heavy tungsten alloy during shock loading  29-32 "Andriot P.,  Chapron P., Olive F. M Ejection of material from shocked surfaces of tin, tantalum and lead-alloys 	 505-509 /Andriot P.,  Chapron P.,  Lambert V., Olive F. q Influence of melting on shocked free surface behavior using Doppler laser interferometry and X-ray densitometry ( Shock Waves in Condensed Matter   1983 	 277-281 #Andriot P.,  Lalle P., Dejean J.P. S Quasi-elastic behavior of pure titanium and TA6V4 titanium alloy at high pressure  1009-1012 	Ang J.A. $ Hypervelocity impact jet formation  1019-1022 Antoun T., Rajendran A.M. 8 Constitutive modeling of concrete under impact loading 	 497-500 Antoun T.H., DeCarli P.S. Anderson O.L. 1 Imperfections of the 1993 phase diagram of iron 	 907-910 )Anderson M.U.,  Graham R.A., Holman G.T. T Time-resolved shock compression of porous rutile: Wave dispersion in porous solids  1111-1114 Anderson M.U., Graham R.A. Z The new simultaneous PVDF/VISAR measurement technique: Applications to highly porous HMX Anderson W.W., Ahrens T.J. 8 Shock wave equations of state of chondritic meteorites 	 115-118 /Anderson M.U.,  Chhabildas L.C., Reinhart W.D. d Simultaneous PVDF/VISAR measurement technique for isentropic loading with graded density impactors 	 841-844 _Anderson W.W.,  Cverna F.,  Hixson R.S.,  Vorthman J.,  Wilke M.D.,  Gray�III G.T., Brown K.L. . Phase transition and spall behavior in b-tin (Anderson M.U.,  Setchell R.E., Cox D.E. ; Shock and release behavior of filled and unfilled epoxies 	 551-554 a Effects of initial temperature on the shock and release behavior of filled and unfilled epoxies 	 669-672 B Shock compression and release properties of alumina-filled epoxy 	 685-688 :Anderson M.U.,  Cox D.E.,  Montgomery S.T., Setchell R.E. _ Compositional effects on the shock compression and release properties of alumina-filled epoxy 	 789-792 +Anderson S.P.,  Palamidi E., Harrigan J.J. = Intermediate and high strain rate testing of soft materials  1237-1240 Anderson W.W. % Jump conditions for nonsteady waves  1303-1306 1Anderson�Jr. C.E.,  O'Donoghue P.E., Bodner S.R. - Tensile failure in tungsten alloy fragments 	 371-374 0Anderson�Jr. C.E.,  O'Donoghue P.E., Skerhut D. 6 Anisotropic model development for shock applications . Shock Compression of Condensed Matter   1989 	 177-180 Anderson�Jr. C.E., Walker J.D. ? Long rod penetration and the calculation of target resistance 	 967-970 RAnderson�Jr. C.E.,  Littlefield D.L.,  Blaylock N.W.,  Bless S.J., Subramanian R. W Influence of shock wave measurement technique on the determination of Hugoniot states  1229-1232 GAllan N.L.,  Braithwaite M.,  Cooper D.L.,  Mackrodt W.C., Wright S.C. P The calculated behaviour of pericalse (MgO) at high temperatures and pressures  53-56 JAllen R.M.,  Kirkpatrick D.J.,  Longbottom A.W.,  Milne A.M., Bourne N.K. A Experimental and numerical study of free-field blast mitigation 	 823-826 0Alme M.L.,  Christiansen E.L., Cour-Palais B.G. F Hydrocode simulations of the multi-shock meteoroid and debris shield 	 975-978 :Altman B.S.,  Nemat-Nasser S.,  Vecchio K.S., Isaacs J.B. L Homogeneous deformation of a particulate reinforced metal matrix composite . Shock Compression of Condensed Matter   1991 	 543-546 Altshuler L.V. * Shock waves and extreme states of matter  3-14 6 Viscosity of water and glycerin behind a shock front 	 509-512 
Ames R.G. K Limitations of the Hopkinson pressure bar for high-frequency measurements  1233-1236 \Aminov Y.A.,  Gorshkov M.M.,  Zaikin V.Y.,  Kovalenko G.V.,  Nikitenko Y.R., Rykovanov G.N. N Investigation of isentrope for detonation products of TATB-based composition 	 875-877 )Aminov Y.A.,  Eskov N.S., Nikitenko Y.R. 8 Modeling of double shock initiation of LX-17 explosive 	 913-916 <Anbukumaran K.,  Venkateswaran C.,  Jaya N.V., Natarajan S. J Piston-cylinder apparatus for high pressure and high temperature studies  1585-1588 _Anderson C.E.,  Wilbeck J.S.,  Hokanson J.C.,  Asay J.R.,  Grady D.E.,  Graham R.A., Kipp M.E. # Sandia shock compression database 	 185-190 .Anderson M.U.,  Graham R.A., Wackerbarth D.E. a Prediction and data analysis of current pulses from impact loaded piezoelectric polymers (PVDF) 	 805-808 Anderson M.U. � Response of the polymers Kel-F, polysulfone, high density polyethylene and PMMA to shock loading and release from 0.3 to 2.4 GPa 	 875-878 	 705-708 Aizawa T.,  Yen B.K., Syono Y. K Shock-induced reaction mechanism to synthesize refractory metal silicides 	 651-654 #Aizawa T.,  Ichige K.-I., Syono Y. \ Shock induced reaction to refractory metal disilicides from mechanically alloyed precursor . Shock Compression of Condensed Matter - 1999 , M.D. Furnish, L.C. Chhabildas, R.S. Hixson 	 759-762  Melville, New York 'Akahama Y.,  Kobayashi M., Kawamura H. = Pressure-induced structural sequence in sulfur up to 90 GPa 	 425-428 4Akashi T.,  Lotrich V.,  Sawaoka A., Beauchamp E.K. " Dynamic compaction of SiC powder 	 779-784 $Akashi T.,  Sawaoka A., Graham R.A. @ The effect of shock compression on graphite-like boron nitride 	 821-825 Akedo J., Lebedev M. c Synthesis of functional ceramic layers using novel method based on impact of ultra-fine particles  1101-1104 "Akella J.,  Smith G.S., Weir S.T. ` Static ultra-high pressure study of lanathanide and actinide metals using a diamond-anvil cell 	 187-190 7Akhavan J.,  Millett J.C.F.,  Bourne N.K., Longjohn R. M Morphological studies of an inert polymer binder subjected to shock loading 	 435-438 
Al�Assaad A. D Heat conduction and wave propagation in thermo-microelastic solids 	 287-290 Alcon R.R., Mulford R.N. 2 Shock tracker configuration of in-material gauge  1057-1060 <Alcon R.R.,  Sheffield S.A.,  Martinez A.R., Gustavsen R.L. E Magnetic gauge instrumentation on the LANL gas-driven two-stage gun 	 845-848 DAlcon R.R.,  Robbins D.L.,  Sheffield S.A.,  Stahl D.B., Fritz J.N. N Shock compression of silicon polymer foams with a range of initial densities Alexander D.J., Robbins D.L. C Laser-driven planar impact of miniature specimens of HY-100 steel 	 630-633 WAlexander C.S.,  Vogler T.J.,  Reinhart W.D.,  Grady D.E.,  Kipp M.E., Chhabildas L.C. ? Application of shock wave data to Earth and planetary science 	 571-588 Ahrens T.J., Potter D.K. y Dynamic consolidation of initial diamond single crystal powders and diamond-graphite into fused polycrystalline diamond 	 419-422 &Ahrens T.J.,  Bass J.D., Abelson J.R.  Shock temperatures in metals 	 851-857 Ahrens T.J., Rubin A.M. E One- and three-dimensional impact induced tensional failure in rock 	 579-582 I Application of shock compression science to Earth and Planetary physics  3-8 &Ahrens T.J.,  Holland K.G., Chen G.Q. 2 Shock temperatures and the melting point of iron . Shock Compression of Condensed Matter - 1997 * S.C. Schmidt, D.P. Dandekar, J.W. Forbes 	 133-136 Ahrens T.J.,  Xia K., Coker D. N Depth of cracking beneath impact craters: New constraint for impact velocity . Shock Compression of Condensed Matter - 2001 ' M.D. Furnish, N.N. Thadhani, Y. Horie  1393-1396  Melville, NY Ahrens T.J.,  Shen A.H., Ni S. + Giant impact induced atmospheric blow-off . Shock Compression of Condensed Matter - 2003 ' M.D. Furni<�
sh, Y.M. Gupta, J.W. Forbes  1419-1422 
 Melville NY Ai H.A., Ahrens T.J. N Numerical modeling of shock-induced damage for granite under dynamic loading . Shock Compression of Condensed Matter - 2005 2 M.D. Furnish, M. Elert, T.P. Russell, C.T. White  1431-1434 Aidun J.B., Gupta Y.M. = Analysis of Lagrangian particle velocity gauge measurements Aidun J.B. @ Shear wave measurements in shock-induced, high-pressure phases + High Pressure Science and Technology 1993 1 S.C. Schmidt, J.W. Shaner, G.A. Samara, M. Ross 	 387-390 _ Discussion of stress tensor nonuniqueness with application to nonuniform, particulate systems 	 985-988 KAizawa T.,  Kashiwabara Y.,  Asakawa Y.,  Fukuoka K.,  Shono Y., Kihara J. T Shock induced reactions of titanium aluminides from mechanically alloyed precursor Abbott R.D., Bjorkman M.D. B Momentum transfer in the one-dimensional impact of spaced plates . Shock Compression of Condensed Matter - 1991 3 S.C. Schmidt, R.D. Dick, J.W. Forbes, D.G. Tasker 	 983-986  Amsterdam 	 ElsevierAbdulazeem M.S. T Coupling between shock and reaction zone in one-dimensional dense fluid detonation , Shock Compression of Condensed Matter 1995  S.C. Schmidt, W.C. Tao 	 373-376  Woodbury, New York  American Institute of Physics.Abramian A.K.,  Andreev V.L., Indeitchev D.A. K The size of dents in circular shells resulting from submerged shock waves 	 285-288 (Agnew S.F.,  Swanson B.I., Eckhart D.G. < Spectroscopic studies of carbon disulfide at high pressure ( Shock Waves in Condensed Matter   1985  Y.M. Gupta 	 221-229 
 New York  PlenumAgnew S.F., Swanson B.I. v Model for the density dependence of electronic absorption bands: Application to carbon disulfide and other molecules ( Shock Waves in Condensed Matter - 1987  S.C. Schmidt, N.C. Holmes 	 485-488 BAgnew S.F.,  Pinnick D.A.,  Pettit D.R.,  Dick J.J., Swanson B.I. L Comparative static and dynamic measurements in dinitrogen tetroxide (N2O4) . Shock Compression of Condensed Matter - 1989 * S.C. Schmidt, J.N. Johnson, L.W. Davison 	 867-870 �Ahrens T.J.,  Boslough M.B.,  Ginn W.G.,  Vassiliou M.S.,  Lange M.A.,  Watt J.P.,  Kondo K.-I.,  Svendsen R.F.,  Rigden S.M., Stolper E.M. h Shock wave apparatus for studying minerals at high pressure and impact phenomena on planetary surfaces ( Shock Waves in Condensed Matter   1981 % W.J. Nellis, L. Seaman, R.A. Graham 	 631-633 EAhrens T.J.,  Kostka D.,  Vreeland�Jr. T.,  Schwarz R.B., Kasiraj P. ' Shock compaction of molybdenum powder & Shock Waves in Condensed Matter 1983 % J.R. Asay, R.A. Graham, G.K. Straub 	 443-446  North-HollandAhrens T.J. ��?h��i
M:#���1��=c~lK����Y0��f���ls�
��J����L�`v\>�R��X�H��1�!����c������$�����C
`��_�Y�W�'i���3"
eA����P�	��k_����l���x�8����������V�0�F� ��������g��m���M<����r����&L�4���A>\O����\���-k/���y������o����U��M|�6M��<
��������r��	U��	[
�A!�M�0�Mc>����K�M�W����e��Cs)
��:� ����Y������A����D�����.��M�e��������R���%="oM�-����9�R=GK���S�	��x`b���kt���w�
��*���޴�XC
��RتX;>����Mt������7������k��
��F-����O$m��s/m���<���H
vSL��
_����j�Mbv ��*��Mu�
��%����X������
��P����>s������I�����Jxeo	w���*$��5����@�5K��V�	���`�������`����M'���������I��bLRW �1�M&����pP��8�Hp������)� D!������~��	

�8�����������H ����`HpMI�I��M&�RW bLM&�������p���������p��<��sh, Y.M. Gupta, J.W. Forbes  1419-1422 
 Melville NY Ai H.A., Ahrens T.J. N Numerical modeling of shock-induced damage for granite under dynamic loading . Shock Compression of Condensed Matter - 2005 2 M.D. Furnish, M. Elert, T.P. Russell, C.T. White  1431-1434 Aidun J.B., Gupta Y.M. = Analysis of Lagrangian particle velocity gauge measurements Aidun J.B. @ Shear wave measurements in shock-induced, high-pressure phases + High Pressure Science and Technology 1993 1 S.C. Schmidt, J.W
	�%��M
�a�r~�F��ֵ��f�.����	�N+<�L�]nn6��Ơ��V������v>'�7�H^Y&j�z��~�F������f�.	�	�"	�3	ND	U	�e	�v	n�	6�	��	ƹ	��	V�	�	�	�
v
>/
@
�P
�a
^r
&�
�
��
~�
F�
�
��
��
f	.�*�;�LN]n�~��n�6�������V���&v7>HY�i�z^�&����~�F���
�
f"
.3
�C
�T
�[

d����MbP?_*+��%�����"�?�?U
}��}�}$�}I)}�)}�
}m}�M
�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
 �@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
 �@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
��@�
�
�
�
�
��
��
~
�@�
�
�
�
�
��
	�

~
�@�
��
��
��
��
��
��
	�~
	�@�
	��
	��
	��
	��
	��
	��

�~

�@�

��

��

��

��

��

��
�~
 �@�
��
��
��
��
��
��

~
0�@�
��
��
��
��
��
��

�~

8�@�

��

��

��

��

��

��
�~
H�@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
 �@�
��
��
�~
�@�
��
��
�~
(�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
��
��
��
�~
@�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
H�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 �~
 P�@�
 ��
 ��
 ��
 ��
 ��
 ��
!�~
!H�@�
!��
!��
!��
!��
!��
!��
"�~
"X�@�
"[�
"��
"��
"\�
"��
"��
#]~
# �@�
#^�
#��
#��
#_�
#��
#��
$`~
$P�@�
$a�
$��
$��
$b�
$��
$��
%c~
% �@�
%d�
%��
%��
%e�
%��
%��
&f~
& �@�
&g�
&h�
&��
&i�
&��
&��
'j~
' �@�
'k�
'��
'��
'l�
'��
'��
(j~
( �@�
(m�
(��
(��
(n�
(��
(��
)o~
)X�@�
)p�
)��
)��
)q�
)��
)��
*r~
*H�@�
*s�
*��
*��
*t�
*��
*��
+u~
+P�@�
+v�
+��
+��
+w�
+��
+��
,x~
,(�@�
,y�
,��
,��
,z�
,��
,��
-{~
-�@�
-|�
-��
-��
-}�
-��
-��
.~~
.�@�
.�
.��
.��
.��
.��
.��
/�~
/ �@�
/��
/��
/��
/��
/��
/��
00~
0(�@�
01�
0��
0��
02�
0��
0��
13~
1(�@�
14�
1��
1��
15�
1��
1��
26~
20�@�
27�
2��
2��
2��
2��
2��
38~
38�@�
39�
3��
3��
3:�
3��
3��
4;~
48�@�
4<�
4��
4��
4=�
4��
4��
5>~
5@�@�
5?�
5��
5��
5�
5��
5��
6@~
6@�@�
6A�
6��
6��
6B�
6��
6��
7@~
7H�@�
7C�
7��
7��
7D�
7��
7������������������������������������������������������������������������������������������������������������������������������������
8@~
8P�@�
8E�
8��
8��
8F�
8��
8��
9G~
9X�@�
9H�
9��
9��
9I�
9��
9��
:J~
:X�@�
:K�
:��
:��
:L�
:��
:��
;M~
;X�@�
;N�
;��
;��
;O�
;��
;��
<P~
<�@�
<Q�
<��
<��
<R�
<��
<��
=S~
=�@�
=T�
=U�
=��
=V�
=��
=��
>W~
> �@�
>X�
>��
>��
>Y�
>��
>��
?Z~
?(�@�
?�
?��
?��
?�
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@~
@0�@�
@�
@��
@��
@�
@��
@��
A~
A8�@�
A�
A��
A��
A	�
A��
A��
B
~
B@�@�
B�
B��
B��
B�
B��
B��
C
~
CH�@�
C�
C��
C��
C�
C��
C��
D~
DP�@�
D�
D��
D��
D�
D��
D��
E~
EX�@�
E�
E��
E��
E�
E��
E��
F~
F0�@�
F�
F��
F��
F�
F��
F��
G~
G0�@�
G�
G��
G��
G�
G��
G��
H~
HX�@�
H�
H��
H��
H�
H��
H��
I~
I��@�
I �
I�
I�
I!�
I��
I��
J"~
J�@�
J#�
J$�
J�
J%�
J��
J	�
K&~
K(�@�
K'�
K��
K��
K(�
K��
K��
L)~
L �@�
L*�
L��
L��
L+�
L��
L��
M,~
M �@�
M-�
M��
M��
M.�
M��
M��
N/~
N(�@�
N��
N��
N��
N��
N��
N��
O�~
O0�@�
O��
O��
O��
O��
O��
O��
P�~
P@�@�
P��
P��
P��
P��
P��
P��
Q�~
QP�@�
Q��
Q��
Q��
Q��
Q��
Q��
R�~
R@�@�
R��
R��
R��
R��
R��
R��
S�~
SH�@�
S��
S��
S��
S��
S��
S��
T�~
T(�@�
T��
T��
T��
T��
T��
T��
U�~
U8�@�
U��
U��
U��
U��
U��
U��
V�~
VP�@�
V��
V��
V��
V��
V��
V��
W�~
W �@�
W��
W��
W��
W��
W��
W��
X�~
XH�@�
X��
X��
X��
X��
X��
X��
Y�~
Y�@�
Y��
Y��
Y��
Y��
Y��
Y��
Z�~
Z�@�
Z��
Z��
Z��
Z��
Z��
Z��
[�~
[(�@�
[��
[��
[��
[��
[��
[��
\�~
\@�@�
\�
\��
\��
\�
\��
\��
]�~
]X�@�
]��
]��
]��
]��
]��
]��
^�~
^�@�
^��
^$�
^�
^��
^��
^	�
_�~
_�@�
_��
_��
_��
_��
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`�~
`�@�
`��
`��
`��
`��
`��
`��
a�~
a �@�
a��
a��
a��
a��
a��
a��
b�~
b(�@�
b��
b��
b��
b��
b��
b��
c�~
c@�@�
c��
c��
c��
c��
c��
c��
d�~
dH�@�
d��
d��
d��
d��
d��
d��
e�~
eP�@�
e��
e��
e��
e��
e��
e��
f�~
f@�@�
f��
f��
f��
f��
f��
f��
g�~
gP�@�
g��
g��
g��
g��
g��
g��
h�~
h0�@�
h��
h��
h��
hF�
h��
h��
i�~
i(�@�
i��
i��
i��
i��
i��
i��
j�~
j��@�
j��
j�
j�
j��
j��
j��
k�~
k�@�
k��
k��
k��
k��
k��
k��
l�~
l�@�
l��
l��
l��
l��
l��
l��
m�~
m�@�
m��
mU�
m��
m��
m��
m��
n�~
n �@�
n��
n��
n��
n��
n��
n��
o|~
o0�@�
o}�
o��
o��
o	�
o��
o��
p~~
p8�@�
p�
p��
p��
p��
p��
p��
q�~
q@�@�
q��
q��
q��
q��
q��
q��
r�~
r@�@�
r��
r��
r��
r��
r��
r��
s�~
sH�@�
s��
s��
s��
s��
s��
s��
t�~
tH�@�
t��
t��
t��
t��
t��
t��
u�~
uP�@�
u��
u��
u��
u��
u��
u��
v�~
vP�@�
v��
v��
v��
v��
v��
v��
w�~
wX�@�
w��
w��
w��
w��
w��
w��
x�~
xX�@�
x��
x��
x��
x��
x��
x��
y�~
yP�@�
y��
y��
y��
y��
y��
y��
z�~
zX�@�
z��
z��
z��
z��
z��
z��
{�~
{(�@�
{��
{��
{��
{��
{��
{��
|�~
|(�@�
|��
|��
|��
|��
|��
|��
}�~
}H�@�
}��
}��
}��
}��
}��
}��
~Z~
~(�@�
~[�
~��
~��
~\�
~��
~��
]~
0�@�
^�
��
��
_�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�`~
��@�
�a�
���
���
�b�
���
���
�c~
� �@�
�d�
���
���
�e�
���
���
�f~
�0�@�
�g�
���
���
�h�
���
���
�i~
�@�@�
�j�
���
���
�k�
���
���
�l~
�X�@�
�m�
���
���
�n�
���
���
�o~
�0�@�
�p�
���
���
�q�
���
���
�r~
�0�@�
�s�
���
���
�t�
���
���
�u~
�P�@�
�v�
���
���
�w�
���
���
�x~
� �@�
�y�
���
���
�z�
���
���
�{~
�@�@�
�0�
���
���
�1�
���
���
�2~
�H�@�
�3�
���
���
�4�
���
���
�2~
�H�@�
�5�
���
���
�6�
���
���
�7~
�X�@�
�8�
���
���
�9�
���
���
�7~
�X�@�
�:�
���
���
�;�
���
���
�<~
�(�@�
�=�
���
���
�>�
���
���
�?~
�(�@�
�@�
���
���
�A�
���
���
�B~
�0�@�
�C�
���
���
�D�
���
���
�?~
�@�@�
�E�
���
���
�F�
���
���
�G~
�H�@�
�H�
���
���
�I�
���
���
�G~
�P�@�
�J�
���
���
�K�
���
���
�L~
�P�@�
�M�
���
���
�N�
���
���
�O~
�X�@�
�P�
���
���
�Q�
���
���
�R~
��@�
�S�
�$�
��
�T�
���
�	�
�U~
��@�
�V�
���
���
�W�
���
���
�X~
� �@�
�Y�
���
���
���
���
���
�~
�0�@�
��
���
���
�	�
���
���
�
~
�X�@�
��
���
���
��
���
���
�
~
�X�@�
��
���
���
��
���
���
�~
�X�@�
��
���
���
��
���
���
�~
��@�
��
���
���
��
���
���
�~
� �@�
��
���
���
�T�
���
���
�~
�P�@�
��
���
���
��
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�~
� �@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
� �
���
���
�!~
�H�@�
�"�
���
���
�#�
���
���
�$~
�(�@�
�%�
���
���
�&�
���
���
�'~
��@�
�(�
���
���
�)�
���
���
�*~
�0�@�
�+�
���
���
�,�
���
���
�-~
�8�@�
�.�
���
���
�e�
���
���
�/~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
��
���
���
�~
�H�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
��
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
���@�
���
���
��
���
���
���
��~
���@�
���
���
��
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
��
���
���
�	�
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
�I�
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
�Z�
���
���
�[�
���
���
�\~
�0�@�
�]�
���
���
�^�
���
���
�_~
�@�@�
�`�
���
���
�a�
���
���
�b~
� �@�
�c�
���
���
�d�
���
���
�e~
�H�@�
�f�
���
���
�g�
���
���
�h~
�P�@�
�i�
���
���
�j�
���
���
�k~
�(�@�
�l�
���
���
�m�
���
���
�k~
�8�@�
�n�
���
���
�o�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�p~
���@�
�q�
���
��
�r�
���
�s�
�t~
�(�@�
�u�
���
���
�v�
���
���
�w~
��@�
�x�
���
���
�y�
���
���
�z~
�(�@�
�{�
���
���
�|�
���
���
�}~
�(�@�
�~�
���
���
��
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
�3�
���
�	�
�4~
� �@�
�5�
���
���
�6�
���
���
�7~
� �@�
�8�
���
���
�9�
���
���
�:~
�X�@�
�;�
���
���
�<�
���
���
�=~
��@�
�>�
�$�
��
�d�
���
�	�
�?~
�(�@�
�@�
���
���
���
���
���
�A~
�0�@�
�B�
���
���
���
���
���
�C~
�0�@�
�D�
���
���
�E�
���
���
�A~
�@�@�
�F�
���
���
�G�
���
���
�H~
�@�@�
�I�
���
���
�J�
���
���
�K~
�H�@�
�L�
���
���
�M�
���
���
�N~
�H�@�
�O�
���
���
�P�
���
���
�Q~
�@�@�
�R�
���
���
�=�
���
���
�S~
��@�
�T�
�$�
��
�U�
���
�	�
�V~
�H�@�
�W�
���
���
�X�
���
���
�Y~
��@�
�	�
���
���
�
�
���
���
�~
� �@�
��
���
���
�
�
���
���
�~
�0�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
��
���
���
�~
�8�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
���
���
���
�~
��@�
��
���
���
��
���
���
�~
�8�@�
��
���
���
��
���
���
� ~
�P�@�
�!�
���
���
�"�
���
���
�#~
�(�@�
�$�
���
���
�	�
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
%~
P�@�
&�
��
��
�
��
��
'~
X�@�
(�
��
��
)�
��
��
*~
H�@�
+�
��
��
,�
��
��
-~
@�@�
.�
��
��
/�
��
��
0~
8�@�
1�
��
��
2�
��
��
0~
@�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
��
��
��
�~
@�@�
��
��
��
��
��
��
	�~
	H�@�
	��
	��
	��
	��
	��
	��

�~

(�@�

��

��

��

��

��

��
�~
�@�
��
��
��
��
��
��
�~
��@�
��
�
�
��
��
��

�~

�@�

��

��

�

��

��

	�
�~
��@�
��
�
�
��
��
��
�~
��@�
��
�
�
��
��
��
�~
�@�
��
��
�
&�
��
	�
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
�
��
��
�~
 �@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
0�@�
�
��
��
�
��
��
~
8�@�
�
��
��
�
��
��
~
H�@�
�
��
��
�
��
��
~
P�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
E�
��
��
�~
��@�
��
�
�
��
��
��
�~
�@�
��
$�
�
��
��
	�
�~
�@�
��
��
��
��
��
��
�~
��@�
��
�
�
��
��
��
�~
�@�
��
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 �~
 8�@�
 ��
 ��
 ��
 ��
 ��
 ��
!�~
!@�@�
!��
!��
!��
!��
!��
!��
"�~
"H�@�
"��
"��
"��
"��
"��
"��
#�~
#P�@�
#��
#��
#��
#��
#��
#��
$�~
$(�@�
$��
$��
$��
$��
$��
$��
%�~
%(�@�
%��
%��
%��
%��
%��
%��
&�~
&(�@�
&��
&��
&��
&��
&��
&��
'�~
'0�@�
'��
'��
'��
'��
'��
'��
(�~
((�@�
(��
(��
(��
(1�
(��
(��
)�~
)(�@�
)��
)��
)��
)��
)��
)��
*�~
*8�@�
*��
*��
*��
*��
*��
*��
+�~
+X�@�
+��
+��
+��
+��
+��
+��
,�~
,8�@�
,��
,��
,��
,��
,��
,��
-�~
-�@�
-��
-��
-��
-��
-��
-��
.�~
.(�@�
.��
.��
.��
.��
.��
.��
/�~
/(�@�
/��
/��
/��
/��
/��
/��
0�~
0P�@�
0��
0��
0��
0��
0��
0��
1�~
1�@�
1��
1��
1��
1:�
1��
1��
2�~
2�@�
2��
2��
2��
2��
2��
2��
3�~
3 �@�
3e�
3��
3��
3��
3��
3��
4�~
40�@�
4f�
4��
4��
4g�
4��
4��
5h~
5@�@�
5i�
5��
5��
5j�
5��
5��
6k~
6@�@�
6l�
6��
6��
6m�
6��
6��
7n~
7P�@�
7o�
7��
7��
7p�
7��
7��
8q~
8X�@�
8r�
8��
8��
8s�
8��
8��
9t~
90�@�
9u�
9��
9��
9v�
9��
9��
:w~
:�@�
:x�
:��
:��
:y�
:��
:��
;z~
;8�@�
;{�
;��
;��
;|�
;��
;��
<}~
<P�@�
<~�
<��
<��
<�
<��
<��
=�~
=X�@�
=��
=��
=��
=��
=��
=��
>�~
>P�@�
>��
>��
>��
>��
>��
>��
?�~
?8�@�
?��
?��
?��
?��
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@�~
@��@�
@��
@�
@�
@��
@��
@��
A�~
A�@�
A��
A�
A�
A��
A��
A	�
B�~
B�@�
B8�
B��
B��
B9�
B��
B��
C:~
C�@�
C;�
C��
C��
C<�
C��
C��
D=~
D�@�
D>�
D��
D��
D��
D��
D��
E=~
E �@�
E?�
E��
E��
E@�
E��
E��
FA~
F(�@�
FB�
F��
F��
FC�
F��
F��
GD~
G0�@�
GE�
G��
G��
GF�
G��
G��
HG~
H8�@�
HH�
H��
H��
HI�
H��
H��
IJ~
I0�@�
IK�
I��
I��
IL�
I��
I��
JM~
J8�@�
JN�
J��
J��
JO�
J��
J��
KP~
K@�@�
KQ�
K��
K��
KR�
K��
K��
LS~
L�@�
LT�
L��
L��
LU�
L��
L��
MV~
MX�@�
MW�
M��
M��
MX�
M��
M��
NY~
N�@�
NZ�
N��
N��
N[�
N��
N��
O\~
O(�@�
O]�
O��
O��
O^�
O��
O��
P_~
P0�@�
P`�
P��
P��
Pa�
P��
P��
Q_~
Q0�@�
Qb�
Q��
Q��
Qc�
Q��
Q��
Rd~
R8�@�
R�
R��
R��
R
�
R��
R��
S_~
S8�@�
S�
S��
S��
S�
S��
S��
T~
T@�@�
T�
T��
T��
T�
T��
T��
U~
U@�@�
U�
U��
U��
U�
U��
U��
V~
VH�@�
V�
V��
V��
V�
V��
V��
W~
WH�@�
W�
W��
W��
W�
W��
W��
X~
XH�@�
X�
X��
X��
X�
X��
X��
Y~
YP�@�
Y �
Y��
Y��
Y!�
Y��
Y��
Z"~
ZP�@�
Z#�
Z��
Z��
Z�
Z��
Z��
[$~
[P�@�
[%�
[��
[��
[�
[��
[��
\&~
\X�@�
\'�
\��
\��
\��
\��
\��
](~
] �@�
])�
]��
]��
]��
]��
]��
^*~
^8�@�
^+�
^��
^��
^��
^��
^��
_,~
_H�@�
_-�
_��
_��
_.�
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`/~
`(�@�
`0�
`��
`��
`��
`��
`��
a1~
a0�@�
a2�
a��
a��
a3�
a��
a��
b4~
bX�@�
b5�
b��
b��
b��
b��
b��
c6~
cX�@�
c7�
c��
c��
c��
c��
c��
d�~
dH�@�
d��
d��
d��
d��
d��
d��
e�~
eX�@�
e��
e��
e��
e��
e��
e��
f�~
f�@�
f��
f$�
f�
f��
f��
f	�
g�~
g0�@�
g��
g��
g��
g��
g��
g��
h�~
h@�@�
h��
h��
h��
h��
h��
h��
i�~
iH�@�
i��
i��
i��
i��
i��
i��
j�~
j�@�
j��
j��
j��
j��
j��
j��
k�~
k�@�
k��
k��
k��
k��
k��
k��
l�~
l�@�
l��
l��
l��
l��
l��
l��
m�~
m�@�
m��
mU�
m��
m��
m��
m��
n�~
n �@�
n��
n��
n��
n��
n��
n��
o�~
o(�@�
o��
o��
o��
o��
o��
o��
p�~
p0�@�
p�
p��
p��
p�
p��
p��
q~
q8�@�
q�
q��
q��
q.�
q��
q��
r~
r@�@�
r�
r��
r��
r��
r��
r��
s~
s@�@�
s�
s��
s��
s�
s��
s��
t	~
tH�@�
t
�
t��
t��
t"�
t��
t��
u~
uP�@�
u��
u��
u��
u��
u��
u��
v�~
vX�@�
v��
v��
v��
v��
v��
v��
w�~
w0�@�
w��
w��
w��
w��
w��
w��
x�~
x�@�
x��
x��
x��
x��
x��
x��
y�~
y �@�
y��
y��
y��
y��
y��
y��
z�~
zX�@�
z��
z��
z��
z��
z��
z��
{�~
{0�@�
{��
{��
{��
{��
{��
{��
|�~
|��@�
|��
|�
|�
|��
|��
|��
}�~
}�@�
}��
}$�
}�
}��
}��
}	�
~�~
~�@�
~��
~��
~��
~��
~��
~��
�~
�@�
��
��
��
��
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
�Y�
���
���
�Z~
���@�
�[�
��
��
�\�
���
���
�]~
�(�@�
�^�
���
���
�_�
���
���
�`~
� �@�
�a�
���
���
�b�
���
���
�c~
�0�@�
�d�
���
���
�e�
���
���
�f~
�8�@�
�g�
���
���
�h�
���
���
�i~
�X�@�
�j�
���
���
�k�
���
���
�l~
� �@�
�m�
���
���
�n�
���
���
�o~
�H�@�
�p�
���
���
�q�
���
���
�o~
�P�@�
�r�
���
���
�s�
���
���
�t~
�X�@�
�u�
���
���
�v�
���
���
�w~
���@�
�x�
���
��
�y�
���
���
�z~
��@�
�{�
�$�
��
�|�
���
�	�
�z~
��@�
�}�
�~�
���
��
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�8�@�
���
���
���
�d�
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
�2~
��@�
�3�
�$�
��
�.�
���
�	�
�4~
�H�@�
�5�
���
���
�6�
���
���
�4~
�H�@�
�7�
���
���
�,�
���
���
�8~
�P�@�
�9�
���
���
�:�
���
���
�;~
�X�@�
�<�
���
���
�=�
���
���
�>~
�X�@�
�?�
���
���
���
���
���
�@~
��@�
�A�
���
���
�j�
���
���
�B~
� �@�
�C�
���
���
�D�
���
���
�B~
�(�@�
�E�
���
���
�F�
���
���
�B~
�0�@�
�G�
���
���
�H�
���
���
�I~
�H�@�
�J�
���
���
���
���
���
�K~
��@�
�L�
���
���
�M�
���
���
�N~
���@�
�O�
���
��
�P�
���
���
�Q~
��@�
�R�
���
���
�S�
���
���
�N~
��@�
�T�
���
���
�9�
���
���
�U~
�(�@�
�V�
���
���
�W�
���
���
�X~
�X�@�
��
���
���
���
���
���
�~
��@�
��
���
���
��
���
���
�~
��@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
��
���
���
�~
�8�@�
��
���
���
��
���
���
�~
��@�
��
�$�
��
��
���
�	�
�~
�(�@�
��
���
���
���
���
���
�~
�P�@�
� �
���
���
�O�
���
���
�!~
�X�@�
�"�
���
���
�#�
���
���
�$~
�@�@�
�%�
���
���
�&�
���
���
�'~
�P�@�
�(�
���
���
�)�
���
���
�*~
�X�@�
�+�
���
���
�,�
���
���
�-~
��@�
�.�
�$�
��
�g�
���
�	�D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�/~
��@�
�0�
���
���
�1�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�	�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�[�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
�N�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
�\�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
��
���
���
�~
�@�@�
��
���
���
��
���
���
�~
�H�@�
�	�
���
���
�
�
���
���
�~
�H�@�
��
���
���
�L�
���
���
�
~
�H�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�b�
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�^�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
��~
�0�@�
�h�
���
���
�i�
���
���
�j~
�0�@�
�k�
���
���
�l�
���
���
�m~
�@�@�
�n�
���
���
�o�
���
���
�p~
�P�@�
�q�
���
���
���
���
���
�r~
�X�@�
�s�
���
���
���
���
���
�t~
�(�@�
�u�
���
���
���
���
���
�v~
���@�
�w�
��
��
�x�
���
���
�y~
��@�
�z�
���
���
�{�
���
���
�|~
��@�
�}�
�U�
���
�~�
���
���
�~
�P�@�
���
���
���
�e�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
�/�
���
���
��~
���@�
���
��
��
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
��
���
���
�	�D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
�@�
=�
��
��
>�
��
��
?~
�@�
@�
��
��
A�
��
��
B~
�@�
C�
��
��
D�
��
��
�~
�@�
E�
��
��
F�
��
��
G~
�@�
H�
��
��
��
��
��
I~
 �@�
J�
��
��
K�
��
��
L~
 �@�
M�
��
��
N�
��
��
O~
(�@�
P�
��
��
Q�
��
��
R~
0�@�
S�
��
��
T�
��
��
	U~
	8�@�
	V�
	��
	��
	�
	��
	��

W~

@�@�

X�

��

��

Y�

��

��
Z~
H�@�
[�
��
��
��
��
��
\~
8�@�
]�
��
��
�
��
��

^~

@�@�

_�

��

��

`�

��

��
a~
X�@�
b�
��
��
c�
��
��
d~
X�@�
e�
��
��
f�
��
��
g~
P�@�
�
��
��
=�
��
��
~
X�@�
�
��
��
_�
��
��
~
P�@�
�
��
��
6�
��
��
~
X�@�
�
��
��
�
��
��
~
@�@�
 �
��
��
#�
��
��
!~
�@�
"�
��
��
��
��
��
#~
0�@�
$�
��
��
[�
��
��
%~
(�@�
&�
��
��
'�
��
��
(~
0�@�
)�
��
��
��
��
��
*~
@�@�
+�
��
��
,�
��
��
-~
H�@�
.�
��
��
/�
��
��
0~
H�@�
1�
��
��
�
��
��
2~
P�@�
3�
��
��
�
��
��
4~
X�@�
5�
��
��
6�
��
��
7~
X�@�
8�
��
��
9�
��
��
:~
@�@�
;�
��
��
Y�
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&	

 !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIK����LMNOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~����'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 <~
 H�@�
 ��
 ��
 ��
 F�
 ��
 ��
!�~
!@�@�
!��
!��
!��
!��
!��
!��
"�~
"H�@�
"��
"��
"��
"��
"��
"��
#�~
#H�@�
#��
#��
#��
#��
#��
#��
$�~
$P�@�
$��
$��
$��
$�
$��
$��
%�~
%X�@�
%��
%��
%��
%��
%��
%��
&�~
&X�@�
&��
&��
&��
&��
&��
&��
'�~
'��@�
'��
'�
'�
'��
'��
'��
(�~
(��@�
(��
(�
(�
(��
(��
(��
)�~
)�@�
)��
)��
)�
)�
)��
)	�
*~
*�@�
*�
*��
*��
*�
*��
*��
+~
+8�@�
+�
+��
+��
+�
+��
+��
,~
,@�@�
,�
,��
,��
,�
,��
,��
-	~
-X�@�
-
�
-��
-��
-��
-��
-��
.~
.�@�
.�
.$�
.�
.
�
.��
.	�
/~
/�@�
/�
/$�
/�
/��
/��
/	�
0~
0 �@�
0�
0��
0��
0�
0��
0��
1~
1(�@�
1�
1��
1��
1�
1��
1��
2~
20�@�
2�
2��
2��
2�
2��
2��
3~
3H�@�
3��
3��
3��
3R�
3��
3��
4�~
4P�@�
4��
4��
4��
4��
4��
4��
5�~
5(�@�
5��
5��
5��
5��
5��
5��
6�~
6(�@�
6��
6��
6��
62�
6��
6��
7�~
78�@�
7��
7��
7��
7��
7��
7��
8�~
8X�@�
8��
8��
8��
8��
8��
8��
9�~
98�@�
9��
9��
9��
9��
9��
9��
:�~
:(�@�
:��
:��
:��
:��
:��
:��
;�~
;�@�
;��
;��
;��
;��
;��
;��
<�~
< �@�
<��
<��
<��
<��
<��
<��
=�~
=(�@�
=��
=��
=��
=��
=��
=��
>�~
>(�@�
>��
>��
>��
>��
>��
>��
?�~
?0�@�
?��
?��
?��
?b�
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@�~
@8�@�
@��
@��
@��
@��
@��
@��
A�~
A@�@�
A��
A��
A��
A��
A��
A��
B�~
BH�@�
B��
B��
B��
B��
B��
B��
C�~
CX�@�
C��
C��
C��
C��
C��
C��
D�~
D�@�
D��
DU�
D��
D��
D��
D��
E�~
EP�@�
E��
E��
E��
E�
E��
E��
F�~
FX�@�
F��
F��
F��
F��
F��
F��
G�~
G8�@�
G��
G��
G��
G��
G��
G��
H�~
HH�@�
H��
H��
H��
H��
H��
H��
I�~
I(�@�
I��
I��
I��
I��
I��
I��
J�~
J(�@�
J��
J��
J��
J��
J��
J��
K�~
K �@�
K��
K��
K��
K��
K��
K��
L�~
L��@�
L��
L�
L�
L��
L��
L��
M�~
M�@�
M��
M$�
M�
M,�
M��
M	�
N�~
N�@�
Nz�
N��
N��
N{�
N��
N��
O|~
O�@�
O}�
O��
O��
O��
O��
O��
P~~
P8�@�
P�
P��
P��
P��
P��
P��
Q�~
Q �@�
Q��
Q��
Q��
Q��
Q��
Q��
R�~
R0�@�
R��
R��
R��
R��
R��
R��
S�~
S �@�
S��
S��
S��
S��
S��
S��
T�~
T(�@�
T��
T��
T��
T��
T��
T��
U�~
U0�@�
U��
U��
U��
U��
U��
U��
V�~
V0�@�
V��
V��
V��
V��
V��
V��
W�~
W�@�
W��
W��
W��
W��
W��
W��
X�~
X�@�
X��
X��
X��
X��
X��
X��
Y�~
Y�@�
Y��
Y��
Y��
Y��
Y��
Y��
Z�~
Z �@�
Z��
Z��
Z��
Z��
Z��
Z��
[�~
[(�@�
[��
[��
[��
[��
[��
[��
\�~
\X�@�
\��
\��
\��
\��
\��
\��
]�~
]�@�
]��
]��
]�
]��
]��
]	�
^�~
^P�@�
^��
^��
^��
^|�
^��
^��
_�~
_X�@�
_U�
_��
_��
_V�
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`W~
`@�@�
`X�
`��
`��
`��
`��
`��
aY~
aP�@�
aZ�
a��
a��
a/�
a��
a��
b[~
bX�@�
b\�
b��
b��
bq�
b��
b��
c]~
cP�@�
c^�
c��
c��
c_�
c��
c��
d`~
dX�@�
da�
d��
d��
d��
d��
d��
eb~
eP�@�
ec�
e��
e��
ed�
e��
e��
fe~
fH�@�
ff�
f��
f��
fg�
f��
f��
gh~
g��@�
gi�
g�
g�
gj�
g��
g��
hk~
h�@�
hl�
hm�
h��
hn�
h��
h��
ih~
i�@�
io�
i��
i��
ip�
i��
i��
jh~
j�@�
jq�
j��
j��
jr�
j��
j��
kk~
k �@�
ks�
k��
k��
kt�
k��
k��
lu~
l �@�
lv�
l��
l��
lB�
l��
l��
mh~
m(�@�
mw�
m��
m��
m��
m��
m��
nx~
n0�@�
ny�
n��
n��
n��
n��
n��
oh~
o8�@�
o)�
o��
o��
o*�
o��
o��
p+~
p@�@�
p,�
p��
p��
pr�
p��
p��
qh~
qP�@�
q-�
q��
q��
q.�
q��
q��
rh~
rX�@�
r/�
r��
r��
r0�
r��
r��
s1~
s�@�
s2�
s��
s��
s�
s��
s��
t1~
t �@�
t3�
t��
t��
t4�
t��
t��
u1~
u(�@�
u5�
u��
u��
u�
u��
u��
v6~
vP�@�
v7�
v��
v��
v��
v��
v��
w6~
wX�@�
w8�
w��
w��
wc�
w��
w��
x9~
x@�@�
x:�
x��
x��
x;�
x��
x��
y<~
y�@�
y=�
y��
y��
y>�
y��
y��
z?~
z�@�
z@�
z��
z��
zA�
z��
z��
{B~
{��@�
{C�
{��
{�
{E�
{��
{s�
|B~
|�@�
|D�
|$�
|�
|E�
|��
|	�
}F~
}(�@�
}G�
}��
}��
}H�
}��
}��
~I~
~�@�
~J�
~��
~�
~K�
~��
~	�
L~
�@�
M�
��
��
N�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�O~
��@�
�P�
���
���
�e�
���
���
�Q~
��@�
�R�
�U�
���
�Y�
���
���
�S~
� �@�
�T�
���
���
�/�
���
���
�S~
�(�@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
�o�
���
���
�S~
�0�@�
��
���
���
�n�
���
���
�S~
�8�@�
��
���
���
���
���
���
�	~
�@�@�
�
�
���
���
���
���
���
�~
�H�@�
��
���
���
�
�
���
���
�S~
�P�@�
��
���
���
��
���
���
�~
�X�@�
��
���
���
�i�
���
���
�~
��@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
��
���
���
�~
��@�
��
�U�
���
��
���
���
�~
�H�@�
��
���
���
��
���
���
� ~
�P�@�
�!�
���
���
���
���
���
�"~
� �@�
�#�
���
���
�I�
���
���
�$~
�P�@�
�%�
���
���
���
���
���
�&~
�X�@�
�'�
���
���
�'�
���
���
�(~
�P�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
��
���
���
��~
�8�@�
���
���
���
�`�
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�H�@�
��
���
���
��
���
���
�~
�P�@�
���
���
���
�&�
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
��
���
���
�	�
��~
� �@�
���
���
���
�H�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
��
���
���
��~
��@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
���
��
���
���
�	�
��~
�P�@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�9�
���
���
��~
�8�@�
���
���
���
�H�
���
���
��~
�@�@�
���
���
���
��
���
���
��~
��@�
���
�$�
��
�B�
���
�	�
��~
��@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�_�
���
���
��~
�X�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�D�
���
���
��~
��@�
���
���
���
�@�
���
���
��~
�8�@�
���
���
���
���
���
���
��~
���@�
���
��
�~
� �@�
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
�_�
���
���
�`�
���
���
�a~
� �@�
�b�
���
���
���
���
���
�c~
�(�@�
�d�
���
���
�b�
���
���
�e~
�(�@�
�f�
���
���
���
���
���
�g~
�0�@�
�h�
���
���
�i�
���
���
��~
�0�@�
�j�
���
���
�k�
���
���
�l~
�8�@�
�m�
���
���
�n�
���
���
�o~
�8�@�
�p�
���
���
���
���
���
�q~
�@�@�
�r�
���
���
���
���
���
��~
�@�@�
�s�
���
���
�t�
���
���
�u~
�H�@�
�v�
���
���
�w�
���
���
�x~
�@�@�
�y�
���
���
�z�
���
���
�{~
�X�@�
�|�
���
���
���
���
���
�}~
�P�@�
�~�
���
���
��
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�.�
���
���
�/~
��@�
�0�
���
���
���
���
���
�1~
�@�@�
�2�
���
���
�4�
���
���
�3~
�8�@�
�4�
���
���
�5�
���
���
�6~
�P�@�
�7�
���
���
�8�
���
���
�9~
� �@�
�:�
���
���
�;�
���
���
�<~
�8�@�
�=�
���
���
�>�
���
���
�?~
���@�
�@�
���
��
�A�
���
���
�B~
���@�
�C�
���
��
�D�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�E~
���@�
�F�
��
��
�G�
���
���
�H~
��@�
�I�
�$�
��
�J�
���
�	�
�K~
��@�
�L�
�$�
��
�M�
���
�	�
�N~
��@�
�O�
���
���
�P�
���
���
�Q~
��@�
�R�
�U�
���
�S�
���
���
�T~
�@�@�
�U�
���
���
���
���
���
�V~
�P�@�
�W�
���
���
�X�
���
���
�Y~
�H�@�
�Z�
���
���
�[�
���
���
�\~
��@�
�]�
���
���
���
���
���
�^~
�P�@�
�	�
���
���
�
�
���
���
�~
�X�@�
��
���
���
�
�
���
���
�~
�@�@�
��
���
���
��
���
���
�~
���@�
��
���
��
��
���
���
�~
��@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
���
���
���
�~
�H�@�
��
���
���
��
���
���
�~
�P�@�
��
���
���
�6�
���
���
�~
�X�@�
��
���
���
���
���
���
�~
�@�@�
� �
���
���
�L�
���
���
�!~
�H�@�
�"�
���
���
���
���
���
�#~
�P�@�
�$�
���
���
��
���
���
�~
�X�@�
�%�
���
���
�&�
���
���
�'~
�(�@�
�(�
���
���
�)�
���
���
�*~
���@�
�+�
��
��
�,�
���
���
�-~
��@�
���
���
���
���
���
���
�*~
�@�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
(�@�
��
��
��
O�
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
o�
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
U�
��
��
��
��
�~
H�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
��
��
��
�~
@�@�
��
��
��
�
��
��
~
0�@�
�
��
��
�
��
��
	~
	8�@�
	�
	��
	��
	�
	��
	��

~

X�@�

�

��

��

�

��

��
~
(�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��

�~

�@�

��

��

��

��

��

��
�~
�@�
��
U�
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
y�
��
��
�~
�@�
��
U�
��
��
��
��
�~
H�@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
d�
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
S�
��
��
�~
@�@�
��
��
��
��
��
��
�~
H�@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 �~
 �@�
 ��
 ��
 ��
 
�
 ��
 ��
!�~
!�@�
!��
!��
!��
!��
!��
!��
"�~
" �@�
"��
"��
"��
"��
"��
"��
#�~
#(�@�
#��
#��
#��
#R�
#��
#��
$�~
$�@�
$��
$��
$��
$�
$��
$��
%�~
%(�@�
%��
%��
%��
%��
%��
%��
&�~
&��@�
&��
&�
&�
&��
&��
&��
'�~
'��@�
'��
'�
'~
'h�@�
'��
'��
(�~
(��@�
(��
(�
(�
(��
(��
(��
)�~
)�@�
)��
)��
)�
)��
)��
)	�
*b~
*�@�
*c�
*��
*��
*d�
*��
*��
+e~
+�@�
+f�
+U�
+��
+n�
+��
+��
,g~
, �@�
,h�
,i�
,��
,��
,��
,��
-j~
-(�@�
-k�
-��
-��
-�
-��
-��
.l~
.�@�
.m�
.��
.��
.n�
.��
.��
/o~
/�@�
/p�
/��
/��
/q�
/��
/��
0r~
0 �@�
0s�
0��
0��
0t�
0��
0��
1u~
1(�@�
1v�
1��
1��
1K�
1��
1��
2u~
2(�@�
2w�
2��
2��
2�
2��
2��
3o~
30�@�
3x�
3��
3��
3y�
3��
3��
4z~
40�@�
4{�
4��
4��
4|�
4��
4��
5o~
50�@�
5}�
5��
5��
5~�
5��
5��
6o~
60�@�
6�
6��
6��
6��
6��
6��
7�~
7@�@�
7��
7��
7��
7��
7��
7��
8�~
8(�@�
8��
8��
8��
8��
8��
8��
9�~
90�@�
9��
9��
9��
9��
9��
9��
:�~
:8�@�
:��
:��
:��
:��
:��
:��
;�~
;@�@�
;��
;��
;��
;��
;��
;��
<�~
<�@�
<B�
<��
<�
</�
<��
<	�
=C~
=(�@�
=D�
=��
=��
=��
=��
=��
>E~
>@�@�
>F�
>��
>��
>e�
>��
>��
?G~
?H�@�
?H�
?��
?��
?��
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@I~
@(�@�
@J�
@��
@��
@K�
@��
@��
AL~
AX�@�
AM�
A��
A��
A��
A��
A��
BN~
B(�@�
BO�
B��
B��
BP�
B��
B��
CQ~
C0�@�
CR�
C��
C��
CS�
C��
C��
DT~
D0�@�
DU�
D��
D��
D��
D��
D��
EV~
E8�@�
EW�
E��
E��
EX�
E��
E��
FY~
F�@�
FZ�
F��
F��
F[�
F��
F��
G\~
G�@�
G]�
G��
G��
Gz�
G��
G��
H^~
H0�@�
H_�
H��
H��
H`�
H��
H��
Ia~
IH�@�
I!�
I��
I��
I^�
I��
I��
J"~
J �@�
J#�
J��
J��
J$�
J��
J��
K%~
K0�@�
K&�
K��
K��
KH�
K��
K��
L'~
LH�@�
L(�
L��
L��
L)�
L��
L��
M*~
MH�@�
M+�
M��
M��
M,�
M��
M��
N-~
N0�@�
N.�
N��
N��
N��
N��
N��
O/~
O@�@�
O0�
O��
O��
O1�
O��
O��
P2~
P@�@�
P3�
P��
P��
Py�
P��
P��
Q4~
Q8�@�
Q5�
Q��
Q��
Q��
Q��
Q��
R6~
R@�@�
R7�
R��
R��
Ry�
R��
R��
S8~
SH�@�
S9�
S��
S��
S:�
S��
S��
T;~
TX�@�
T<�
T��
T��
TI�
T��
T��
U=~
UX�@�
U>�
U��
U��
Un�
U��
U��
V?~
VX�@�
V@�
V��
V��
VA�
V��
V��
W~
WX�@�
W�
W��
W��
W�
W��
W��
X~
XH�@�
X�
X��
X��
X�
X��
X��
Y~
Y �@�
Y�
Y��
Y��
Y	�
Y��
Y��
Z
~
Z(�@�
Z�
Z��
Z��
Z��
Z��
Z��
[~
[0�@�
[
�
[��
[��
[�
[��
[��
\~
\8�@�
\�
\��
\��
\�
\��
\��
]~
]H�@�
]�
]��
]��
]�
]��
]��
^~
^P�@�
^�
^��
^��
^<�
^��
^��
_~
_X�@�
_�
_��
_��
_�
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`~
`X�@�
`�
`��
`��
`��
`��
`��
a~
a�@�
a�
a��
a��
a_�
a��
a��
b~
b0�@�
b�
b��
b��
b��
b��
b��
c ~
c8�@�
c��
c��
c��
c��
c��
c��
d�~
dP�@�
d��
d��
d��
d��
d��
d��
e�~
e(�@�
e��
e��
e��
e��
e��
e��
f�~
f0�@�
f��
f��
f��
f��
f��
f��
g�~
gP�@�
g��
g��
g��
g_�
g��
g��
h�~
hP�@�
h��
h��
h��
h��
h��
h��
i�~
i0�@�
i��
i��
i��
i��
i��
i��
j�~
jX�@�
j��
j��
j��
j��
j��
j��
k�~
k0�@�
k��
k��
k��
k+�
k��
k��
l�~
l�@�
l��
l��
l��
l��
l��
l��
m�~
m�@�
m��
m��
m��
m��
m��
m��
n�~
n�@�
n��
n$�
n�
n��
n��
n	�
o�~
o�@�
o��
o��
o��
o��
o��
o��
p�~
p �@�
p�
p��
p��
pg�
p��
p��
q�~
q�@�
q��
q$�
q�
q�
q��
q	�
r�~
r�@�
r��
r$�
r�
r��
r��
r	�
s�~
s�@�
s��
s��
s��
s��
s��
s��
t�~
tP�@�
t��
t��
t��
t��
t��
t��
u�~
u�@�
u��
u��
u��
u��
u��
u��
v�~
v�@�
v��
v��
v��
v��
v��
v��
w�~
w�@�
w��
w��
w��
w`�
w��
w��
x�~
x �@�
x��
x��
x��
x��
x��
x��
y�~
y0�@�
y��
y��
y��
y��
y��
y��
z�~
z��@�
z��
z�
z�
z��
z��
z��
{�~
{�@�
{��
{��
{��
{6�
{��
{��
|�~
|(�@�
|��
|��
|��
|��
|��
|��
}�~
}0�@�
}��
}��
}��
}��
}��
}��
~�~
~8�@�
~��
~��
~��
~��
~��
~��
�~
H�@�
��
��
��
~�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�H�@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
� �@�
���
���
���
�h�
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�6�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
�W�
���
���
�m~
�8�@�
�n�
���
���
���
���
���
�o~
�@�@�
�p�
���
���
���
���
���
�q~
�@�@�
�r�
���
���
�s�
���
���
�t~
�H�@�
�u�
���
���
�v�
���
���
�w~
��@�
�x�
���
��
�y�
���
�	�
�z~
�0�@�
�{�
���
���
�|�
���
���
�}~
���@�
�~�
��
��
��
���
���
��~
��@�
���
�U�
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
���
�S�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�t�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
�8�@�
���
���
���
�3�
���
���
��~
�(�@�
�G�
���
���
�H�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�I~
�0�@�
�J�
���
���
�X�
���
���
�K~
�@�@�
�L�
���
���
���
���
���
�M~
�P�@�
�N�
���
���
�,�
���
���
�O~
�X�@�
�P�
���
���
�Q�
���
���
�R~
��@�
�S�
�$�
��
�F�
���
�	�
�T~
�(�@�
�U�
���
���
�V�
���
���
�W~
�0�@�
�X�
���
���
���
���
���
�Y~
�8�@�
�Z�
���
���
���
���
���
�W~
�@�@�
�[�
���
���
���
���
���
�W~
�@�@�
�\�
���
���
�]�
���
���
�^~
���@�
�_�
��
��
�`�
���
���
�a~
��@�
�b�
�$�
��
�g�
���
�	�
�c~
�P�@�
�d�
���
���
�`�
���
���
�e~
�@�@�
�f�
���
���
�$�
���
���
�g~
�H�@�
�h�
���
���
�i�
���
���
�j~
�P�@�
�k�
���
���
�l�
���
���
�&~
�X�@�
�'�
���
���
�(�
���
���
�)~
�8�@�
�*�
���
���
�+�
���
���
�,~
�P�@�
�-�
���
���
�.�
���
���
�/~
�8�@�
�0�
���
���
���
���
���
�1~
���@�
�2�
��
��
�3�
���
���
�4~
�(�@�
�5�
���
���
�6�
���
���
�7~
� �@�
�8�
���
���
�9�
���
���
�:~
�(�@�
�;�
���
���
�{�
���
���
�<~
�(�@�
�=�
���
���
�>�
���
���
�?~
�0�@�
�@�
���
���
���
���
���
�A~
�8�@�
�B�
���
���
���
���
���
�C~
�H�@�
�D�
���
���
�E�
���
���
�F~
�P�@�
���
���
���
�e�
���
���
�~
��@�
��
���
���
��
���
���
�~
��@�
��
���
���
��
���
���
�~
� �@�
��
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�~
�(�@�
�	�
���
���
�3�
���
���
�
~
�(�@�
��
���
���
��
���
���
�
~
�0�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
���
���
���
�~
�8�@�
��
���
���
���
���
���
�~
�@�@�
��
���
���
�e�
���
���
�~
�H�@�
��
���
���
��
���
���
�~
�P�@�
��
���
���
���
���
���
�~
�X�@�
��
���
���
���
���
���
�~
��@�
��
���
���
��
���
���
� ~
��@�
�!�
���
���
�"�
���
���
�#~
��@�
�$�
���
���
�F�
���
���
�%~
�H�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
�>�
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
��~
�0�@�
���
���
���
��
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�n�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
�;�
���
���
��~
� �@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�9�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�)�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
��
���
���
��~
�8�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�H�@�
�]�
���
���
�^�
���
���
�_~
�P�@�
�`�
���
���
�a�
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
b~
�@�
c�
��
��
=�
��
��
d~
8�@�
e�
��
��
f�
��
��
g~
X�@�
h�
��
��
i�
��
��
j~
P�@�
k�
��
��
l�
��
��
m~
�@�
n�
��
��
��
��
��
o~
 �����������������������������������������������������������������������������������������������������������������������������������@�
p�
��
��
`�
��
��
q~
��@�
r�
�
�
s�
��
��
t~
�@�
u�
$�
�
n�
��
	�
q~
�@�
v�
��
��
w�
��
��
	x~
	�@�
	y�
	��
	��
	z�
	��
	��

q~

�@�

{�

��

��

�

��

��
|~
�@�
}�
��
��
~�
��
��
q~
 �@�
�
��
��
��
��
��

q~

0�@�

��

��

��

��

��

��
q~
8�@�
��
��
��
�
��
��
q~
@�@�
��
��
��
g�
��
��
�~
@�@�
��
��
��
��
��
��
�~
P�@�
;�
��
��
<�
��
��
=~
0�@�
>�
��
��
A�
��
��
?~
@�@�
@�
��
��
A�
��
��
B~
H�@�
C�
��
��
D�
��
��
E~
X�@�
F�
��
��
G�
��
��
H~
0�@�
I�
��
��
��
��
��
J~
8�@�
K�
��
��
	�
��
��
L~
H�@�
M�
��
��
N�
��
��
O~
@�@�
P�
��
��
b�
��
��
Q~
��@�
R�
��
�
S�
��
��
T~
P�@�
U�
��
��
V�
��
��
W~
@�@�
X�
��
��
Y�
��
��
Z~
H�@�
[�
��
��
��
��
��
\~
P�@�
�
��
��
��
��
��
~
(�@�
�
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 ~
 (�@�
 �
 ��
 ��
 �
 ��
 ��
!~
!8�@�
!�
!��
!��
! �
!��
!��
"!~
"H�@�
""�
"��
"��
"#�
"��
"��
#$~
#P�@�
#%�
#��
#��
#��
#��
#��
$&~
$P�@�
$'�
$��
$��
$(�
$��
$��
%)~
%X�@�
%*�
%��
%��
%g�
%��
%��
&+~
&X�@�
&,�
&��
&��
&-�
&��
&��
'.~
'H�@�
'/�
'��
'��
'0�
'��
'��
(1~
(H�@�
(2�
(��
(��
(3�
(��
(��
)4~
)P�@�
)5�
)��
)��
)6�
)��
)��
*7~
*X�@�
*8�
*��
*��
*9�
*��
*��
+:~
+8�@�
+��
+��
+��
+��
+��
+��
,�~
,@�@�
,��
,��
,��
,��
,��
,��
-�~
-��@�
-��
-�
-�
-��
-��
-��
.�~
.�@�
.��
.$�
.�
.��
.��
.	�
/�~
/�@�
/��
/$�
/�
/��
/��
/	�
0�~
0�@�
0��
0��
0��
0��
0��
0��
1�~
1�@�
1��
1��
1��
1��
1��
1��
2~
2�@�
2�
2��
2��
2��
2��
2��
3~
3 �@�
3�
3��
3��
3��
3��
3��
4~
40�@�
4�
4��
4��
4^�
4��
4��
5~
5X�@�
5�
5��
5��
5��
5��
5��
6~
6��@�
6�
6�
6�
6	�
6��
6��
7~
7�@�
7
�
7��
7�
7;�
7��
7	�
8~
8�@�
8�
8$�
8�
8�
8��
8	�
9~
9�@�
9
�
9��
9��
9�
9��
9��
:~
:�@�
:�
:��
:��
:,�
:��
:��
;~
;�@�
;�
;��
;��
;��
;��
;��
<~
< �@�
<�
<��
<��
<�
<��
<��
=~
=(�@�
=�
=��
=��
=[�
=��
=��
>~
>0�@�
>�
>��
>��
>�
>��
>��
?~
?8�@�
?�
?��
?��
?��
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@~
@@�@�
@��
@��
@��
@��
@��
@��
A~
A@�@�
A��
A��
A��
A��
A��
A��
B~
BH�@�
B��
B��
B��
B�
B��
B��
C~
CP�@�
C��
C��
C��
C�
C��
C��
D~
DP�@�
D��
D��
D��
D��
D��
D��
E~
EX�@�
E��
E��
E��
E��
E��
E��
F�~
FP�@�
F��
F��
F��
Fq�
F��
F��
G�~
G��@�
G��
G��
G�
G��
G��
G��
H�~
H�@�
H��
H$�
H�
Ho�
H��
H	�
I�~
I�@�
I��
I��
I��
I��
I��
I��
J�~
J�@�
J��
J��
J��
J��
J��
J��
K�~
K�@�
K��
K��
K��
K��
K��
K��
L�~
L�@�
L��
L��
L��
L��
L��
L��
M�~
M�@�
M��
M��
M��
MX�
M��
M��
N�~
N�@�
N��
N��
N��
N��
N��
N��
O�~
O �@�
O��
O��
O��
Oq�
O��
O��
P�~
P(�@�
P��
P��
P��
P��
P��
P��
Q�~
QX�@�
Q��
Q��
Q��
Q��
Q��
Q��
R�~
RX�@�
R��
R��
R��
R��
R��
R��
S�~
S �@�
S��
S��
S��
Sw�
S��
S��
T�~
TX�@�
T��
T��
T��
T��
T��
T��
U�~
UH�@�
U��
U��
U��
U��
U��
U��
V�~
VP�@�
V��
V��
V��
V��
V��
V��
W�~
WX�@�
W��
W��
W��
W��
W��
W��
X�~
X �@�
X��
X��
X��
X��
X��
X��
Y�~
Y�@�
Y��
Y��
Y��
Y,�
Y��
Y��
Z�~
Z�@�
Z��
ZU�
Z��
Z��
Z��
Z��
[�~
[ �@�
[��
[��
[��
[��
[��
[��
\�~
\(�@�
\��
\��
\��
\��
\��
\��
]�~
](�@�
]��
]��
]��
]��
]��
]��
^�~
^0�@�
^��
^��
^��
^��
^��
^��
_�~
_8�@�
_��
_��
_��
_��
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`�~
`@�@�
`��
`��
`��
`n�
`��
`��
a�~
aH�@�
a��
a��
a��
a��
a��
a��
b�~
bP�@�
b��
b��
b��
b~�
b��
b��
c~
cX�@�
c��
c��
c��
c��
c��
c��
d�~
dX�@�
d��
d��
d��
d��
d��
d��
e�~
eP�@�
e��
e��
e��
e�
e��
e��
f�~
fH�@�
f��
f��
f��
f��
f��
f��
g�~
gP�@�
g��
g��
g��
g��
g��
g��
h�~
hX�@�
h��
h��
h��
h��
h��
h��
i�~
i�@�
i��
i��
i��
i��
i��
i��
j�~
jH�@�
j��
j��
j��
j��
j��
j��
k�~
kP�@�
k��
k��
k��
k��
k��
k��
l�~
lX�@�
l��
l��
l��
l��
l��
l��
m�~
m(�@�
m��
m��
m��
m��
m��
m��
n�~
n(�@�
n��
n��
n��
n��
n��
n��
o�~
oP�@�
o��
o��
o��
o��
o��
o��
p�~
pP�@�
p��
p��
p��
p�
p��
p��
q�~
qH�@�
q��
q��
q��
q��
q��
q��
rW~
rP�@�
rX�
r��
r��
rY�
r��
r��
sZ~
sX�@�
s[�
s��
s��
s\�
s��
s��
t]~
tX�@�
t^�
t��
t��
t_�
t��
t��
u`~
u@�@�
ua�
u��
u��
ub�
u��
u��
vc~
v�@�
vd�
v��
v��
v��
v��
v��
we~
w�@�
wf�
w��
w��
wg�
w��
w��
xh~
x �@�
xi�
x��
x��
x�
x��
x��
yj~
y �@�
yk�
y��
y��
y��
y��
y��
zc~
z(�@�
zl�
z��
z��
z��
z��
z��
{m~
{0�@�
{n�
{��
{��
{)�
{��
{��
|c~
|8�@�
|o�
|��
|��
|��
|��
|��
}c~
}@�@�
}p�
}��
}��
}��
}��
}��
~q~
~�@�
~r�
~��
~��
~s�
~��
~��
t~
 �@�
u�
��
��
��
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�v~
�8�@�
�w�
���
���
�x�
���
���
�y~
�8�@�
�z�
���
���
�{�
���
���
�|~
�@�@�
�}�
���
���
�l�
���
���
�-~
�8�@�
�.�
���
���
�/�
���
���
�0~
�(�@�
�1�
���
���
�2�
���
���
�3~
�(�@�
�4�
���
���
�X�
���
���
�5~
�(�@�
�6�
���
���
�7�
���
���
�8~
�8�@�
�9�
���
���
���
���
���
�:~
�H�@�
�;�
���
���
�<�
���
���
�=~
�P�@�
�>�
���
���
��
���
���
�?~
�@�@�
�@�
���
���
�j�
���
���
�A~
�H�@�
�B�
���
���
�C�
���
���
�D~
�(�@�
�E�
���
���
�F�
���
���
�G~
�0�@�
�H�
���
���
���
���
���
�I~
��@�
�J�
�$�
��
�K�
���
�	�
�L~
� �@�
�M�
���
���
��
���
���
�N~
�0�@�
�O�
���
���
�P�
���
���
�N~
�0�@�
�Q�
���
���
�R�
���
���
�S~
�8�@�
�T�
���
���
�U�
���
���
�N~
�@�@�
�V�
���
���
���
���
���
�~
�H�@�
��
���
���
��
���
���
�~
�P�@�
��
���
���
�y�
���
���
�~
�X�@�
�	�
���
���
�^�
���
���
�
~
�P�@�
��
���
���
��
���
���
�~
�P�@�
�
�
���
���
��
���
���
�~
�X�@�
��
���
���
��
���
���
�~
���@�
��
��
�~
�P{@�
���
���
�~
���@�
��
��
�~
�h�@�
���
���
�~
���@�
��
��
�~
�p�@�
���
���
�~
��@�
��
�$�
��
��
���
�	�
�~
��@�
��
���
���
��
���
���
�~
��@�
��
��
��
��
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
� ~
��@�
�!�
���
���
�"�
���
���
�~
� �@�
�#�
���
���
�$�
���
���
�%~
� �@�
�&�
���
���
�'�
���
���
�(~
� �@�
�)�
���
���
�<�
���
���
�*~
�(�@�
�+�
���
���
���
���
���
�~
�@�@�
�,�
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�H�
���
���
�~
�H�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
�#�
���
���
��~
�@�@�
���
���
���
�/�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�+�
���
���
��~
�P�@�
���
���
���
�W�
���
���
��~
�X�@�
���
���
���
�V�
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
�~
��@�
��
���
���
���
���
���
�~
��@�
���
�U�
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�2�
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�\�
���
���
��~
�P�@�
���
���
���
�1�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
�b�
���
���
��~
�@�@�
���
���
���
���
���
���
��~
��@�
���
���
���
�7�
���
���
��~
��@�
���
���
���
�g�
���
���
��~
��@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
��
���
���
��~
�@�@�
���
���
���
��
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�X�
���
���
��~
�X�@�
���
���
���
��
���
���
��~
��@�
���
�$�
��
��
���
�	�
��~
��@�
���
���
���
���
���
���
�~
�P�@�
���
���
���
�s�
���
���
��~
�X�@�
���
���
���
�l�
���
���
��~
� �@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�b�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�H�@�
�Z�
���
���
�[�
���
���
�\~
�P�@�
�]�
���
���
���
���
���
�^~
�X�@�
�_�
���
���
�`�
���
���
�a~
���@�
�b�
��
��
�c�
���
���
�d~
��@�
�e�
�$�
��
�f�
���
�	�
�g~
��@�
�h�
�U�
���
���
���
���
�i~
�X�@�
�j�
���
���
�k�
���
���
�l~
���@�
�m�
��
�~
�Ps@�
���
���
�n~
�H�@�
�o�
���
���
���
���
���
�p~
�P�@�
�q�
���
���
�r�
���
���
�s~
�X�@�
�t�
���
���
�F�
���
���
�u~
�P�@�
�v�
���
���
�w�
���
���
�x~
�P�@�
�y�
���
���
���
���
���
�z~
�X�@�
�{�
���
���
�|�
���
���
�}~
���@�
�~�
��
��
�%�
���
���
�5~
��@�
�6�
�U�
���
���
���
���
�7~
��@�
�8�
���
���
�9�
���
���
�7~
��@�
�:�
���
���
�q�
���
���
�7~
��@�
�;�
�U�
���
�<�
���
���
�7~
� �@�
�=�
���
���
��
���
���
�7~
�(�@�
�>�
���
���
�?�
���
���
�7~
�0�@�
�@�
���
���
���
���
���
�7~
�8�@�
�A�
���
���
�r�
���
���
�B~
�H�@�
�C�
���
���
�D�
���
���
�E~
�X�@�
�F�
���
���
���
���
���
�G~
�P�@�
�H�
���
���
���
���
���
�I~
�0�@�
�J�
���
���
�K�
���
���
�L~
�(�@�
�M�
���
���
���
���
���
�N~
�(�@�
�O�
���
���
�P�
���
���
�Q~
���@�
�R�
��
��
�S�
���
���
�T~
��@�
�U�
���
���
�V�
���
���
�W~
�X�@�
�X�
���
���
�Y�
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
~
�@�
�
��
��
|�
��
��
~
�@�
�
��
��
��
��
��
~
��@�
�
�
�
�
��
��
~
�@�
�
$�
�
�
��
	�
~
@�@�
�
��
��
�
��
��
~
H�@�
�
��
��
�
��
��
~
P�@�
�
��
��

�
��
��
 ~
X�@�
!�
��
��
�
��
��
"~
 �@�
#�
��
��
$�
��
��
	%~
	(�@�
	&�
	��
	��
	'�
	��
	��

(~

0�@�

)�

��

��


�

��

��
*~
0�@�
+�
��
��
,�
��
��
-~
H�@�
.�
��
��
/�
��
��

0~

P�@�

1�

��

��

��

��

��
2~
(�@�
3�
��
��
4�
��
��
�~
X�@�
��
��
��
��
��
��
�~
�@�
��
$�
�
��
��
	�
�~
�@�
��
��
��
��
��
��
�~
 �@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
�@�
��
$�
�
��
��
	�
�~
 �@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
 �@�
��
��
��
L�
��
��
�~
(�@�
��
��
��
�
��
��
�~
0�@�
�
��
��
��
��
��
~
8�@�
�
��
��
��
��
��
~
@�@�
�
��
��
��
��
��
~
H�@�
�
��
��
��
��
��
~
X�@�
	�
��
��
��
��
��

~
(�@�
�
��
��
��
��
��
~
8�@�

�
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 ~
 H�@�
 �
 ��
 ��
 �
 ��
 ��
!�~
!P�@�
!��
!��
!��
!x�
!��
!��
"�~
"X�@�
"��
"��
"��
"��
"��
"��
#�~
#X�@�
#��
#��
#��
#��
#��
#��
$�~
$ �@�
$��
$��
$��
$V�
$��
$��
%�~
%P�@�
%��
%��
%��
%��
%��
%��
&�~
&H�@�
&��
&��
&��
&��
&��
&��
'�~
'��@�
'��
'�
'�
'��
'��
'��
(�~
( �@�
(��
(��
(��
(��
(��
(��
)�~
)H�@�
)��
)��
)��
)��
)��
)��
*�~
*H�@�
*��
*��
*��
*��
*��
*��
+�~
+P�@�
+��
+��
+��
+��
+��
+��
,�~
,X�@�
,��
,��
,��
,o�
,��
,��
-�~
- �@�
-��
-��
-��
-��
-��
-��
.�~
.0�@�
.��
.��
.��
.��
.��
.��
/�~
/H�@�
/��
/��
/��
/��
/��
/��
0�~
0H�@�
0��
0��
0��
0��
0��
0��
1�~
1P�@�
1��
1��
1��
1,�
1��
1��
2�~
2X�@�
2��
2��
2��
2��
2��
2��
3�~
3��@�
3��
3�
3�
3��
3��
3��
4�~
4H�@�
4��
4��
4��
4��
4��
4��
5�~
58�@�
5��
5��
5��
5��
5��
5��
6�~
60�@�
6��
6��
6��
6T�
6��
6��
7�~
70�@�
7��
7��
7��
7��
7��
7��
8�~
88�@�
8��
8��
8��
8��
8��
8��
9�~
9@�@�
9��
9��
9��
9��
9��
9��
:�~
:H�@�
:��
:��
:��
:V�
:��
:��
;�~
;P�@�
;��
;��
;��
;��
;��
;��
<�~
<X�@�
<��
<��
<��
<{�
<��
<��
=�~
=0�@�
=��
=��
=��
=��
=��
=��
>�~
>8�@�
>��
>��
>��
>��
>��
>��
?�~
?@�@�
?��
?��
?��
?��
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@�~
@(�@�
@��
@��
@��
@r�
@��
@��
A�~
A8�@�
A��
A��
A��
A��
A��
A��
B�~
B(�@�
B��
B��
B��
B��
B��
B��
C�~
C0�@�
C��
C��
C��
Cw�
C��
C��
D�~
DP�@�
D��
D��
D��
D��
D��
D��
E�~
E8�@�
E��
E��
E��
E��
E��
E��
F�~
F@�@�
F��
F��
F��
F��
F��
F��
G�~
GH�@�
G��
G��
G��
G�
G��
G��
H�~
HH�@�
H��
H��
H��
H��
H��
H��
I�~
I��@�
I��
I�
I�
I��
I��
I��
J�~
J �@�
J��
J��
J��
J��
J��
J��
K�~
K(�@�
K��
K��
K��
K��
K��
K��
L�~
L0�@�
L��
L��
L��
L��
L��
L��
M�~
M8�@�
MW�
M��
M��
M��
M��
M��
NX~
N@�@�
NY�
N��
N��
N��
N��
N��
OZ~
OP�@�
O[�
O��
O��
O\�
O��
O��
P]~
PP�@�
P^�
P��
P��
P/�
P��
P��
Q_~
Q@�@�
Q`�
Q��
Q��
QL�
Q��
Q��
Ra~
R�@�
Rb�
R��
R��
R}�
R��
R��
Sc~
S�@�
Sd�
S��
S��
S��
S��
S��
Ta~
T8�@�
Te�
T��
T��
Tf�
T��
T��
Ug~
U@�@�
Uh�
U��
U��
Ui�
U��
U��
Vj~
V@�@�
Vk�
V��
V��
V��
V��
V��
Wl~
W(�@�
Wm�
W��
W��
W�
W��
W��
Xn~
X��@�
Xo�
X�
X�
Xp�
X��
X��
Yq~
Y��@�
Yr�
Y�
Y�
Ys�
Y��
Y��
Zt~
Z�@�
Zu�
Z$�
Z�
Zv�
Z��
Z	�
[w~
[�@�
[x�
[$�
[�
[,�
[��
[	�
\y~
\�@�
\u�
\��
\��
\z�
\��
\��
]{~
]�@�
]|�
]��
]��
]}�
]��
]��
^~~
^ �@�
^�
^��
^��
^��
^��
^��
_q~
_(�@�
_��
_��
_��
_i�
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`<~
`8�@�
`=�
`��
`��
`��
`��
`��
a>~
a�@�
a?�
a@�
a��
a��
a��
a��
bA~
b(�@�
bB�
b��
b��
bC�
b��
b��
cD~
c0�@�
cE�
c��
c��
c
�
c��
c��
dF~
d@�@�
dG�
d��
d��
d��
d��
d��
eH~
eH�@�
eI�
e��
e��
eJ�
e��
e��
fK~
fX�@�
fL�
f��
f��
f�
f��
f��
gM~
gP�@�
gN�
g��
g��
g7�
g��
g��
hO~
hP�@�
hP�
h��
h��
hQ�
h��
h��
iR~
i(�@�
iS�
i��
i��
i@�
i��
i��
jT~
j(�@�
jU�
j��
j��
jV�
j��
j��
k~
kH�@�
k�
k��
k��
k��
k��
k��
l~
lX�@�
l�
l��
l��
l�
l��
l��
m~
mP�@�
m�
m��
m��
m��
m��
m��
n~
n��@�
n �
n��
n~
n~@�
n��
n��
o!~
o�@�
o"�
o��
o��
o�
o��
o��
p#~
p@�@�
p$�
p��
p��
p3�
p��
p��
q%~
q��@�
q&�
q�
q�
q'�
q��
q��
r%~
r�@�
r(�
r$�
r�
r)�
r��
r	�
s*~
s�@�
s+�
s��
s��
s,�
s��
s��
t-~
t�@�
t.�
t��
t��
t��
t��
t��
u%~
u�@�
u/�
u��
u��
u0�
u��
u��
v%~
v(�@�
v1�
v��
v��
v��
v��
v��
w2~
w0�@�
w3�
w��
w��
w�
w��
w��
x4~
xH�@�
x5�
x��
x��
x8�
x��
x��
y6~
yP�@�
y7�
y��
y��
yI�
y��
y��
z8~
z8�@�
z9�
z��
z��
z:�
z��
z��
{;~
{�@�
{��
{��
{��
{	�
{��
{��
|�~
|�@�
|��
|$�
|�
|��
|��
|	�
}�~
}P�@�
}��
}��
}��
}��
}��
}��
~�~
~(�@�
~��
~��
~��
~�
~��
~��
�~
8�@�
��
��
��
`�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�@�@�
��
���
���
���
���
���
�~
�H�@�
��
���
���
���
���
���
�~
�X�@�
��
���
���
�6�
���
���
�~
�P�@�
��
���
���
���
���
���
�~
��@�
��
�$�
��
�l�
���
�	�
�	~
�@�@�
�
�
���
���
���
���
���
�	~
�H�@�
��
���
���
�:�
���
���
�	~
�H�@�
��
���
���
�s�
���
���
�
~
�@�@�
��
���
���
���
���
���
�~
�X�@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
��
���
���
��~
�0�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�,�
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
��
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�g�
���
���
��~
��@�
���
���
���
��
���
���
��~
�P�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�|�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
�
�
���
���
��~
�@�@�
���
���
���
�_�
���
���
��~
�H�@�
���
���
���
�$�
���
���
��~
��@�
���
���
���
�{�
���
���
��~
�P�@�
���
���
���
�F�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�
�
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�\�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
��~
�@�@�
���
���
���
�2�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
�b~
��@�
�c�
���
���
�d�
���
���
�e~
� �@�
�f�
���
���
�g�
���
���
�h~
�8�@�
�i�
���
���
�_�
���
���
�j~
�X�@�
�k�
���
���
���
���
���
�l~
��@�
�m�
���
���
�&�
���
���
�n~
�8�@�
�o�
���
���
�p�
���
���
�q~
�P�@�
�r�
���
���
�s�
���
���
�t~
�X�@�
�u�
���
���
�F�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�v~
��@�
�w�
�U�
���
�x�
���
���
�y~
� �@�
�z�
���
���
���
���
���
�{~
�8�@�
�|�
���
���
�E�
���
���
�}~
�@�@�
�~�
���
���
���
���
���
�~
���@�
���
��
��
���
���
���
�~
���@�
���
��
��
���
���
���
��~
��@�
���
���
��
���
���
�	�
��~
��@�
���
���
���
�V�
���
���
��~
��@�
���
���
���
��
���
���
�~
��@�
���
���
���
���
���
���
��~
��@�
�8�
�U�
���
�1�
���
���
�9~
��@�
�:�
���
���
�i�
���
���
�;~
��@�
�<�
���
���
�=�
���
���
�>~
� �@�
�?�
���
���
�@�
���
���
�A~
� �@�
�B�
���
���
���
���
���
�C~
� �@�
�D�
���
���
�E�
���
���
�F~
�(�@�
�G�
���
���
�x�
���
���
�H~
�(�@�
�I�
���
���
�Y�
���
���
�~
�(�@�
�J�
���
���
�#�
���
���
�K~
�(�@�
�L�
���
���
�M�
���
���
�N~
�0�@�
�O�
���
���
���
���
���
�P~
�0�@�
�Q�
���
���
���
���
���
�;~
�8�@�
�R�
���
���
���
���
���
�S~
�@�@�
�T�
���
���
�i�
���
���
�U~
�H�@�
�V�
���
���
�W�
���
���
�X~
�P�@�
�Y�
���
���
��
���
���
�Z~
�(�@�
�[�
���
���
���
���
���
�\~
��@�
�]�
���
���
�^�
���
���
�_~
�8�@�
�`�
���
���
�q�
���
���
�a~
�@�@�
��
���
���
���
���
���
�~
�@�@�
��
���
���
��
���
���
�\~
�H�@�
��
���
���
�^�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�\~
�P�@�
��
���
���
�V�
���
���
�~
�@�@�
� �
���
���
�A�
���
���
�~
�H�@�
�!�
���
���
���
���
���
�"~
�P�@�
�#�
���
���
�j�
���
���
�$~
�X�@�
�%�
���
���
�&�
���
���
�'~
�(�@�
�(�
���
���
�)�
���
���
�*~
�(�@�
�+�
���
���
�,�
���
���
�-~
�0�@�
�.�
���
���
�!�
���
���
�/~
�8�@�
�0�
���
���
�&�
���
���
�1~
�8�@�
�2�
���
���
��
���
���
�3~
�@�@�
�4�
���
���
�\�
���
���
�5~
�H�@�
�6�
���
���
�s�
���
���
�7~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���	

 !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKM����NOPQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~�
�~
�X�@�
��
���
���
���
���
���
�~
�X�@�
��
���
���
�p�
���
���
�~
��@�
��
���
���
���
���
���
�~
��@�
��
���
���
�U�
���
���
�~
�0�@�
�	�
���
���
�
�
���
���
�~
�@�@�
��
���
���
�Y�
���
���
�
~
�H�@�
��
���
���
���
���
���
�~
�P�@�
��
���
���
��
���
���
�
~
�X�@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
���
���
���
�~
�@�@�
��
���
���
���
���
���
�~
�@�@�
��
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
���@�
���
��
�~
��w@�
���
���
��~
��@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
 �@�
��
��
��
l�
��
��
�~
(�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
/�
��
��
	�~
	0�@�
	��
	��
	��
	��
	��
	��

�~

8�@�

��

��

��

��

��

��
�~
8�@�
��
��
��
��
��
��
�~
@�@�
��
��
��
��
��
��

�~

H�@�

��

��

��

E�

��

��
�~
P�@�
��
��
��
#�
��
��
�~
X�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
P�@�
��
��
��
��
��
��
�~
�@�
��
��
��
Q�
��
��
�~
(�@�
��
��
��
��
��
��
�~
H�@�
��
��
��
��
��
��
�~
@�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
��@�
��
�
�
��
��
��
�~
8�@�
��
��
��
��
��
��
�~
�@�
��
$�
�
p�
��
	�
�~
(�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
��@�
��
��
�
��
��
��
�~
�@�
��
$�
�
��
��
	�
�~
H�@�
��
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 �~
 H�@�
 ��
 ��
 ��
 ��
 ��
 ��
!�~
!@�@�
!��
!��
!��
!��
!��
!��
"�~
"H�@�
"��
"��
"��
"A�
"��
"��
#�~
#P�@�
#j�
#��
#��
#��
#��
#��
$k~
$P�@�
$l�
$��
$��
$m�
$��
$��
%n~
%��@�
%o�
%�
%�
%p�
%��
%��
&q~
&�@�
&r�
&��
&��
&s�
&��
&��
't~
'�@�
'u�
'��
'��
'��
'��
'��
(n~
(�@�
(v�
(��
(��
(w�
(��
(��
)n~
)(�@�
)x�
)��
)��
)A�
)��
)��
*y~
*0�@�
*z�
*��
*��
*{�
*��
*��
+|~
+P�@�
+}�
+��
+��
+{�
+��
+��
,~~
, �@�
,�
,��
,��
,c�
,��
,��
-�~
-(�@�
-��
-��
-��
-��
-��
-��
.�~
.@�@�
.��
.��
.��
.R�
.��
.��
/�~
/H�@�
/��
/��
/��
/��
/��
/��
0�~
0P�@�
0��
0��
0��
0S�
0��
0��
1�~
1X�@�
1��
1��
1��
1��
1��
1��
2�~
2X�@�
2��
2��
2��
2��
2��
2��
3�~
30�@�
3��
3��
3��
3K�
3��
3��
4�~
48�@�
4��
4��
4��
4^�
4��
4��
5�~
5@�@�
5F�
5��
5��
5i�
5��
5��
6G~
6H�@�
6H�
6��
6��
6��
6��
6��
7I~
7(�@�
7J�
7��
7��
7K�
7��
7��
8L~
80�@�
8M�
8��
8��
8��
8��
8��
9N~
9�@�
9O�
9��
9��
9�
9��
9��
:P~
:0�@�
:Q�
:��
:��
:[�
:��
:��
;R~
;�@�
;S�
;$�
;�
;�
;��
;	�
<T~
<��@�
<U�
<�
<�
<V�
<��
<��
=W~
=�@�
=X�
=$�
=�
=�
=��
=	�
>Y~
>�@�
>Z�
>��
>��
>{�
>��
>��
?[~
?�@�
?\�
?��
?��
?`�
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@]~
@ �@�
@^�
@��
@��
@��
@��
@��
A[~
AP�@�
A_�
A��
A��
A`�
A��
A��
Ba~
BX�@�
Bb�
B��
B��
B,�
B��
B��
Cc~
C0�@�
Cd�
C��
C��
Ce�
C��
C��
Df~
D(�@�
Dg�
D��
D��
Dh�
D��
D��
Ei~
E(�@�
E�
E��
E��
E�
E��
E��
F ~
FP�@�
F!�
F��
F��
F"�
F��
F��
G#~
GX�@�
G$�
G��
G��
Gt�
G��
G��
H%~
H��@�
H&�
H�
H�
H��
H��
H��
I'~
I�@�
I(�
I��
I�
I��
I��
I	�
J'~
J�@�
J)�
J��
J��
J*�
J��
J��
K+~
K�@�
K,�
K��
K��
K��
K��
K��
L'~
L�@�
L-�
L��
L��
LP�
L��
L��
M'~
M �@�
M.�
M��
M��
M��
M��
M��
N/~
N(�@�
N0�
N��
N��
N1�
N��
N��
O2~
O8�@�
O3�
O��
O��
O��
O��
O��
P4~
P@�@�
P5�
P��
P��
P��
P��
P��
Q6~
QX�@�
Q7�
Q��
Q��
Q)�
Q��
Q��
R8~
R �@�
R9�
R��
R��
R��
R��
R:�
S;~
SP�@�
S<�
S��
S��
S��
S��
S��
T=~
T��@�
T>�
T�
T�
T?�
T��
T��
U@~
UH�@�
UA�
U��
U��
U�
U��
U��
VB~
V8�@�
VC�
V��
V��
V��
V��
V��
WD~
W0�@�
WE�
W��
W��
W��
W��
W��
XD~
X8�@�
X��
X��
X��
XR�
X��
X��
YD~
YP�@�
Y��
Y��
Y��
Yd�
Y��
Y��
Z�~
ZH�@�
Z�
Z��
Z��
Z��
Z��
Z��
[~
[P�@�
[�
[��
[��
[��
[��
[��
\~
\(�@�
\�
\��
\��
\�
\��
\��
]~
](�@�
]�
]��
]��
]��
]��
]��
^~
^(�@�
^	�
^��
^��
^
�
^��
^��
_~
_X�@�
_�
_��
_��
_[�
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`
~
`@�@�
`�
`��
`��
`�
`��
`��
a~
a@�@�
a�
a��
a��
a�
a��
a��
b~
bP�@�
b�
b��
b��
b�
b��
b��
c~
c(�@�
c�
c��
c��
c�
c��
c��
d~
d8�@�
d�
d��
d��
d��
d��
d��
e~
e@�@�
e�
e��
e��
e��
e��
e��
f~
fH�@�
f�
f��
f��
f��
f��
f��
g�~
g0�@�
g��
g��
g��
g�
g��
g��
h�~
hH�@�
h��
h��
h��
h�
h��
h��
i�~
iX�@�
i��
i��
i��
i��
i��
i��
j�~
jP�@�
j��
j��
j��
j��
j��
j��
k�~
kX�@�
k��
k��
k��
kF�
k��
k��
l�~
lX�@�
l��
l��
l��
l��
l��
l��
m�~
m0�@�
m��
m��
m��
m��
m��
m��
n�~
n��@�
n��
n�
n�
n��
n��
n��
o�~
o��@�
o��
o�
o�
o��
o��
o��
p�~
p �@�
p��
p��
p��
p�
p��
p��
q�~
q �@�
q��
q��
q��
q��
q��
q��
r�~
r(�@�
r��
r��
r��
r^�
r��
r��
s�~
s(�@�
s��
s��
s��
s��
s��
s��
t�~
t0�@�
t��
t��
t��
tC�
t��
t��
u�~
u@�@�
u��
u��
u��
u{�
u��
u��
v�~
v(�@�
v��
v��
v��
v��
v��
v��
w�~
w@�@�
w��
w��
w��
w��
w��
w��
x�~
x@�@�
x��
x��
x��
x��
x��
x��
y�~
y�@�
y��
y��
y��
yD�
y��
y��
z�~
z�@�
z��
z��
z��
z��
z��
z��
{�~
{X�@�
{��
{��
{��
{��
{��
{��
|�~
|P�@�
|��
|��
|��
|��
|��
|��
}�~
}8�@�
}��
}��
}��
}��
}��
}��
~�~
~(�@�
~��
~��
~��
~��
~��
~��
�~
��@�
��
�
�
��
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�(�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�W�
���
���
��~
� �@�
���
���
���
�y�
���
���
��~
� �@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�m�
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�w�
���
���
��~
�P�@�
���
���
���
�-�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�R�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
�x~
�X�@�
�y�
���
���
�z�
���
���
�{~
�(�@�
�|�
���
���
�\�
���
���
�}~
�(�@�
�~�
���
���
���
���
���
�}~
�(�@�
��
���
���
��
���
���
��~
�8�@�
���
���
���
��
���
���
��~
�@�@�
���
���
���
��
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�q�
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
�U�
���
��
���
���
��~
�(�@�
���
���
���
�8�
���
���
��~
��@�
���
���
���
���
���
���
��~
���@�
�K�
��
��
�L�
���
���
�M~
�H�@�
�N�
���
���
���
���
���
�O~
� �@�
�P�
���
���
�Q�
���
���
�R~
� �@�
�S�
���
���
���
���
���
�T~
�@�@�
�U�
���
���
�V�
���
���
�W~
�H�@�
�X�
���
���
�Y�
���
���
�Z~
�0�@�
�[�
���
���
�\�
���
���
�]~
�@�@�
�^�
���
���
�_�
���
���
�`~
�8�@�
�a�
���
���
�l�
���
���
�b~
��@�
�c�
���
���
�d�
���
���
�e~
�H�@�
�f�
���
���
���
���
���
�g~
�X�@�
�h�
���
���
���
���
���
�i~
� �@�
�j�
���
���
�k�
���
���
�i~
�(�@�
�l�
���
���
��
���
���
�m~
�0�@�
�n�
���
���
�o�
���
���
�p~
�P�@�
�q�
���
���
�M�
���
���
�p~
�X�@�
�r�
���
���
���
���
���
�s~
��@�
�t�
���
���
���
���
���
�u~
�(�@�
�v�
���
���
���
���
���
�w~
�X�@�
�!�
���
���
�\�
���
���
�"~
��@�
�#�
�$�
��
���
���
�	�
�$~
��@�
�%�
���
���
�&�
���
���
�'~
� �@�
�(�
���
���
���
���
���
�)~
�(�@�
�*�
���
���
�+�
���
���
�,~
�0�@�
�-�
���
���
���
���
���
�.~
�8�@�
�/�
���
���
�0�
���
���
�.~
�H�@�
�1�
���
���
�2�
���
���
�3~
�P�@�
�4�
���
���
�5�
���
���
�6~
�X�@�
�7�
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�8~
�0�@�
�9�
���
���
���
���
���
�:~
�X�@�
�;�
���
���
���
���
���
�<~
���@�
�=�
��
��
�>�
���
���
�<~
��@�
�?�
���
���
�h�
���
���
�@~
��@�
�A�
���
���
�y�
���
���
�@~
� �@�
�B�
���
���
���
���
���
�C~
� �@�
�D�
���
���
���
���
���
�@~
�(�@�
�E�
���
���
�F�
���
���
�G~
�@�@�
�H�
���
���
���
���
���
�@~
�@�@�
�I�
���
���
�J�
���
���
�~
�H�@�
��
���
���
�W�
���
���
�~
�P�@�
��
���
���
��
���
���
�~
�X�@�
��
���
���
���
���
���
�~
�8�@�
�	�
���
���
�
�
���
���
�~
�(�@�
��
���
���
�
�
���
���
�
~
�(�@�
��
���
���
���
���
���
�~
�(�@�
��
���
���
��
���
���
�~
�X�@�
��
���
���
�h�
���
���
�~
�P�@�
��
���
���
���
���
���
�~
��@�
��
�$�
��
�Q�
���
�	�
�~
��@�
��
�$�
��
��
���
�	�
�~
��@�
��
�$�
��
���
���
�	�
�~
��@�
��
�$�
��
�
�
���
�	�
�~
��@�
��
���
��
�@�
���
�	�
� ~
��@�
��
�
���
���
��
�
���
���
��
~
��@�
��
�
���
���
��
�
���
���
��
~
��@�
��
�
���
���
��
���
���
��
~
��@�
��
�
���
���
�$�
���
���
��
~
� �@�
��
�
���
���
�
�
���
���
��
~
� �@�
��
�
���
���
�[�
���
���
��
~
� �@�
��
�
���
���
�/�
���
���
��
~
�(�@�
��
�
���
���
��
�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��
~
�0�@�
��
�
���
���
���
���
���
��
~
�0�@�
��
�
���
���
�:�
���
���
��
~
�0�@�
��
�
���
���
��
�
���
���
��
~
�8�@�
��
�
���
���
��
�
���
���
��
~
�8�@�
��
�
���
���
�l�
���
���
��
~
�@�@�
��
�
���
���
��
���
���
��
~
�@�@�
��
�
���
���
���
���
���
�~
�@�@�
��
�
���
���
��
�
���
���
��
~
�@�@�
��
�
���
���
�^�
���
���
��
~
�H�@�
��
�
���
���
��
�
���
���
��
~
�H�@�
��
�
���
���
��
���
���
��
~
�P�@�
��
�
���
���
��
�
���
���
��
~
�P�@�
��
�
���
���
��
�
���
���
��
~
�P�@�
��
�
���
���
���
���
���
��
~
�X�@�
��
�
���
���
��
�
���
���
��
~
�X�@�
��
�
���
���
���
���
���
��
~
�(�@�
��
�
���
���
���
���
���
��
~
� �@�
��
�
���
���
���
���
���
��
~
�X�@�
��
�
���
���
��
�
���
���
��
~
��@�
��
�
���
���
��
�
���
���
��
~
��@�
��
�
���
���
���
���
���
��
~
�H�@�
��
�
���
���
��
�
���
���
��
~
���@�
��
�
��
��
��
�
���
���
��
~
��@�
��
�
�$�
��
��
�
���
�	�
��
~
��@�
��
�
���
���
��
�
���
���
��
~
�(�@�
��
�
���
���
���
���
���
��
~
�0�@�
��
�
���
���
�>�
���
���
��
~
�8�@�
��
�
���
���
��
���
���
��
~
��@�
��
�
�U�
���
��
�
���
���
��
~
� �@�
��
�
���
���
���
���
���
��
~
�P�@�
��
�
���
���
��
�
���
���
��
~
�H�@�
��
�
���
���
��
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�
~
(�@�
�
�
��
��
�
�
��
��
�
~
�@�
y
�
$�
�
z
�
��
	�
{
~
8�@�
|
�
��
��
e�
��
��
}
~
@�@�
~
�
��
��
v�
��
��
}
~
H�@�

�
��
��
�
�
��
��
�
~
H�@�
�
�
��
��
��
��
��
�
~
H�@�
�
�
��
��
�
�
��
��
�
~
P�@�
�
�
��
��
�
��
��
�
~
�@�
�
�
��
��
��
��
��
	�
~
	��@�
	�
�
	�
	�
	�
�
	��
	��

�
~

�@�

�
�

��

��

�
�

��

��
�
~
�@�
�
�
��
��
��
��
��
�
~
 �@�
�
�
��
��
��
��
��

�
~

 �@�

�
�

��

��

��

��

��
�
~
(�@�
�
�
��
��
0�
��
��
�
~
(�@�
�
�
��
��
��
��
��
�
~
(�@�
�
�
��
��
|�
��
��
�
~
(�@�
X
�
��
��
W�
��
��
Y
~
(�@�
Z
�
��
��
[
�
��
��
\
~
�@�
]
�
$�
�
��
��
	�
^
~
 �@�
_
�
��
��
�
��
��
`
~
P�@�
a
�
��
��
R�
��
��
b
~
X�@�
c
�
��
��
�
�
��
��
d
~
��@�
e
�
�
�
f
�
��
��
g
~
0�@�
h
�
��
��
��
��
��
i
~
(�@�
j
�
��
��
k
�
��
��
l
~
0�@�
m
�
��
��
��
��
��
n
~
0�@�
o
�
��
��
��
��
��
p
~
8�@�
q
�
��
��
��
��
��
p
~
@�@�
r
�
��
��
d�
��
��
s
~
P�@�
t
�
��
��
��
��
��
u
~
0�@�
v
�
��
��
w
�
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 x
~
 (�@�
 /
�
 ��
 ��
 �
 ��
 ��
!0
~
!(�@�
!1
�
!��
!��
!��
!��
!��
"2
~
"(�@�
"3
�
"��
"��
"4
�
"��
"��
#5
~
#0�@�
#6
�
#��
#��
#��
#��
#��
$7
~
$0�@�
$8
�
$��
$��
$,�
$��
$��
%9
~
%0�@�
%:
�
%��
%��
%�
%��
%��
&;
~
&8�@�
&<
�
&��
&��
&z�
&��
&��
'=
~
'@�@�
'>
�
'��
'��
'
�
'��
'��
(?
~
(@�@�
(@
�
(��
(��
(��
(��
(��
)A
~
)@�@�
)B
�
)��
)��
)D�
)��
)��
*9
~
*@�@�
*C
�
*��
*��
*D
�
*��
*��
+E
~
+P�@�
+F
�
+��
+��
+G
�
+��
+��
,H
~
,X�@�
,I
�
,��
,��
,J
�
,��
,��
-K
~
-@�@�
-L
�
-��
-��
-�
-��
-��
.M
~
.H�@�
.N
�
.��
.��
.��
.��
.��
/O
~
/H�@�
/P
�
/��
/��
/Q
�
/��
/��
0R
~
0P�@�
0S
�
0��
0��
0�
0��
0��
1T
~
1X�@�
1U
�
1��
1��
1V
�
1��
1��
2W
~
2X�@�
2
�
2��
2��
2

�
2��
2��
3
~
30�@�
3
�
3��
3��
3<�
3��
3��
4
~
4(�@�
4
�
4��
4��
4
�
4��
4��
5
~
5(�@�
5
�
5��
5��
51�
5��
5��
6
~
6(�@�
6
�
6��
6��
6
�
6��
6��
7
~
7(�@�
7
�
7��
7��
7��
7��
7��
8
~
80�@�
8
�
8��
8��
8
�
8��
8��
9
~
9@�@�
9
�
9��
9��
9g�
9��
9��
:
~
:H�@�
:
�
:��
:��
:D�
:��
:��
;
~
;P�@�
;
�
;��
;��
;��
;��
;��
< 
~
<X�@�
<!
�
<��
<��
<^�
<��
<��
="
~
=8�@�
=#
�
=��
=��
=��
=��
=��
>$
~
>H�@�
>%
�
>��
>��
>��
>��
>��
?&
~
?P�@�
?'
�
?��
?��
?(
�
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@)
~
@X�@�
@*
�
@��
@��
@1�
@��
@��
A+
~
A��@�
A,
�
A�
A�
A-
�
A��
A��
B.
~
B�@�
B��
B��
B��
B�
B��
B��
C�~
C�@�
C��
C��
C��
C4�
C��
C��
D�~
D �@�
D��
D��
D��
D��
D��
D��
E�~
E(�@�
E��
E��
E��
E��
E��
E��
F�~
F�@�
F��
F��
F��
F��
F��
F��
G�~
GX�@�
G��
G��
G��
G��
G��
G��
H�~
H(�@�
H��
H��
H��
H��
H��
H��
I�~
IX�@�
I��
I��
I��
Ii�
I��
I��
J�~
J0�@�
J��
J��
J��
Jl�
J��
J��
K�~
K(�@�
K��
K��
K��
K��
K��
K��
L
~
LX�@�
L
�
L��
L��
L@�
L��
L��
M
~
MX�@�
M
�
M��
M��
Mi�
M��
M��
N
~
N0�@�
N
�
N��
N��
N��
N��
N��
O
~
O8�@�
O
�
O��
O��
O
�
O��
O��
P
~
PP�@�
P	
�
P��
P��
Pz�
P��
P��
Q

~
QX�@�
Q
�
Q��
Q��
Q��
Q��
Q��
R�~
R0�@�
R��
R��
R��
R��
R��
R��
S�~
S@�@�
S��
S��
S��
SW�
S��
S��
T�~
T(�@�
T��
T��
T��
T��
T��
T��
U�~
U(�@�
U��
U��
U��
U��
U��
U��
V�~
V(�@�
V��
V��
V��
VW�
V��
V��
W�~
W(�@�
W��
W��
W��
W�
W��
W��
X�~
X(�@�
X��
X��
X��
X��
X��
X��
Y�~
YP�@�
Y��
Y��
Y��
Y��
Y��
Y��
Z�~
ZP�@�
Z��
Z��
Z��
Z��
Z��
Z��
[�~
[X�@�
[��
[��
[��
[��
[��
[��
\�~
\ �@�
\��
\��
\��
\�
\��
\��
]�~
](�@�
]��
]��
]��
]��
]��
]��
^�~
^�@�
^��
^$�
^�
^�
^��
^	�
_�~
_ �@�
_��
_��
_��
_��
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`�~
`(�@�
`��
`��
`��
`��
`��
`��
a�~
a0�@�
a��
a��
a��
a��
a��
a��
b�~
b8�@�
b��
b��
b��
bY�
b��
b��
c�~
c@�@�
c��
c��
c��
c��
c��
c��
d�~
dH�@�
d��
d��
d��
d��
d��
d��
e�~
eH�@�
e��
e��
e��
e��
e��
e��
f�~
fX�@�
f��
f��
f��
f,�
f��
f��
g�~
gH�@�
g��
g��
g��
g��
g��
g��
h�~
h �@�
h��
h��
h��
h��
h��
h��
i�~
i��@�
i��
i�
i�
i>�
i��
i��
j�~
j��@�
j��
j�
j�
j��
j��
j��
k�~
k@�@�
k��
k��
k��
k�
k��
k��
l�~
lH�@�
l��
l��
l��
lQ�
l��
l��
m�~
m8�@�
m��
m��
m��
m��
m��
m��
n�~
n(�@�
n��
n��
n��
n��
n��
n��
o�~
oH�@�
o��
o��
o��
oM�
o��
o��
p�~
pP�@�
p��
p��
p��
p��
p��
p��
q�~
qP�@�
q��
q��
q��
q�
q��
q��
r�~
rX�@�
r��
r��
r��
rV�
r��
r��
s�~
s��@�
s��
s�
s�
s��
s��
s��
t�~
t�@�
t��
t��
t��
t��
t��
t��
u�~
uP�@�
u��
u��
u��
u��
u��
u��
v�~
v�@�
v��
v��
v��
v �
v��
v��
w�~
w@�@�
w��
w��
w��
w��
w��
w��
x�~
x0�@�
x��
x��
x��
x
�
x��
x��
y�~
y �@�
y��
y��
y��
y��
y��
y��
z�~
z0�@�
z��
z��
z��
zR�
z��
z��
{�~
{@�@�
{i�
{��
{��
{��
{��
{��
|j~
|H�@�
|k�
|��
|��
|��
|��
|��
}l~
}X�@�
}m�
}��
}��
}b�
}��
}��
~n~
~H�@�
~o�
~��
~��
~p�
~��
~��
q~
(�@�
r�
��
��
s�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�t~
���@�
�u�
��
��
�v�
���
���
�w~
��@�
�x�
���
���
�y�
���
���
�z~
��@�
�{�
���
���
�z�
���
���
�|~
�@�@�
�}�
���
���
�|�
���
���
�~~
��@�
��
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
�w�
���
���
��~
�X�@�
���
���
���
��
�
���
���
��~
�(�@�
�C�
���
���
�D�
���
���
�E~
�H�@�
�F�
���
���
�G�
���
���
�H~
�P�@�
�I�
���
���
�J�
���
���
�K~
��@�
�L�
���
���
�M�
���
���
�N~
�H�@�
�O�
���
���
���
���
���
�P~
�H�@�
�Q�
���
���
�R�
���
���
�S~
�P�@�
�T�
���
���
���
���
���
�U~
�X�@�
�V�
���
���
�/�
���
���
�W~
��@�
�X�
���
���
���
���
���
�W~
��@�
�Y�
���
���
���
���
���
�Z~
��@�
�[�
���
���
�\�
���
���
�W~
�(�@�
�\�
���
���
���
���
���
�]~
�0�@�
�^�
���
���
�_�
���
���
�`~
�8�@�
�a�
���
���
���
���
���
�b~
�@�@�
�c�
���
���
�d�
���
���
�e~
�X�@�
�f�
���
���
�Q
�
���
���
�g~
�@�@�
�h�
���
���
���
���
���
�g~
�@�@�
��
���
���
�	�
���
���
�~
�H�@�
� �
���
���
�!�
���
���
�"~
�X�@�
�#�
���
���
�w�
���
���
�$~
� �@�
�%�
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�&~
�8�@�
�'�
���
���
���
���
���
�(~
�@�@�
�)�
���
���
�	�
���
���
�*~
�P�@�
�+�
���
���
���
���
���
�,~
�(�@�
�-�
���
���
���
���
���
�.~
�P�@�
�/�
���
���
�
�
���
���
�0~
�0�@�
�1�
���
���
���
���
���
�2~
�0�@�
�3�
���
���
�4�
���
���
�5~
�8�@�
�6�
���
���
�D�
���
���
�7~
�H�@�
�8�
���
���
�9�
���
���
�7~
�P�@�
�:�
���
���
��
���
���
�;~
��@�
�<�
���
���
�=�
���
���
�>~
�@�@�
�?�
���
���
�M�
���
���
�@~
�@�@�
�A�
���
���
�B�
���
���
��~
�H�@�
���
���
���
�p�
���
���
��~
�P�@�
���
���
���
��
���
���
�~
� �@�
��
���
���
��
�
���
���
�~
�(�@�
��
���
���
�d�
���
���
�~
�P�@�
��
���
���
�
�
���
���
�~
�P�@�
��
���
���
���
���
���
�	~
��@�
�
�
���
���
���
���
���
�~
�(�@�
��
���
���
�
�
���
���
�~
�X�@�
��
���
���
�$�
���
���
�~
��@�
��
���
���
�n�
���
���
�~
�P�@�
��
���
���
��
���
���
�~
�P�@�
��
���
���
���
���
���
�~
���@�
��
��
��
��
���
���
�~
��@�
��
���
���
��
���
���
�~
�(�@�
���
���
���
���
���
���
�~
�(�@�
���
���
���
�4�
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
���
���
�@�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
�U�
���
�K�
���
���
��~
� �@�
���
���
���
��
�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
��
���
���
��~
�@�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
��
���
���
��~
��@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�/�
���
���
��~
�P�@�
���
���
���
�|�
���
���
��~
�P�@�
���
���
���
�F�
�������������������������������������������������������������������������������������������������������������������������������������
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�p�
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
�$�
��
���
���
�	�
��~
��@�
���
�$�
��
��
���
�	�
��~
��@�
���
�m�
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�d�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�p�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
�$�
��
���
���
�	�
��~
�H�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
�l�
���
���
�9�
���
���
�m~
��@�
�n�
���
���
�E�
���
���
�o~
�(�@�
�p�
���
���
���
���
���
�q~
�0�@�
�r�
���
���
���
���
���
�s~
�8�@�
�t�
���
���
���
���
���
�u~
�P�@�
�v�
���
���
���
���
���
�w~
�0�@�
�x�
���
���
�i�
���
���
�w~
�8�@�
�y�
���
���
��
���
���
�z~
�@�@�
�{�
���
���
�q�
���
���
�w~
�@�@�
�|�
���
���
�i�
���
���
�}~
�@�@�
�~�
���
���
�A�
���
���
�~
�H�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
��
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�V
�
���
���
��~
�P�@�
���
���
���
�`�
���
���
��~
�X�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
�@�
��
U�
��
�
�
��
��
G~
@�@�
H�
��
��
��
��
��
I~
H�@�
J�
��
��
K�
��
��
L~
X�@�
M�
��
��
��
��
��
N~
P�@�
O�
��
��
��
��
��
P~
�@�
Q�
$�
�
��
��
	�
R~
0�@�
S�
��
��

�
��
��
T~
X�@�
U�
��
��
��
��
��
V~
H�@�
W�
��
��
X�
��
��
	Y~
	(�@�
	Z�
	��
	��
	��
	��
	��

[~

 �@�

\�

��

��

��

��

��
]~
(�@�
^�
��
��
_�
��
��
`~
@�@�
a�
��
��
��
��
��

b~

�@�

c�

��

��

d�

��

��
e~
X�@�
f�
��
��
��
��
��
g~
X�@�
h�
��
��
i�
��
��
j~
��@�
k�
�
�
'�
��
��
(~
��@�
)�
�
�
*�
��
��
+~
�@�
,�
$�
�
��
��
	�
-~
�@�
.�
U�
�~
�W@�
��
��
/~
@�@�
0�
��
��
��
��
��
1~
8�@�
2�
��
��
��
��
��
3~
X�@�
4�
��
��
��
��
��
5~
(�@�
6�
��
��
7�
��
��
8~
0�@�
9�
��
��
��
��
��
:~
@�@�
;�
��
��
,�
��
��
<~
H�@�
=�
��
��
��
��
��
>~
P�@�
?�
��
��
@�
��
��
A~
8�@�
B�
��
��
��
��
��
C~
P�@�
D�
��
��
E�
��
��
F~
X�@�
�
��
��
�
��
��
~
�@�
�
��
��
�
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 	~
 0�@�
 
�
 ��
 ��
 �
 ��
 ��
!~
!H�@�
!
�
!��
!��
!V�
!��
!��
"~
"�@�
"�
"��
"��
"�
"��
"��
#~
#�@�
#�
#��
#��
#�
#��
#��
$~
$�@�
$�
$��
$��
$��
$��
$��
%~
% �@�
%�
%��
%��
%n�
%��
%��
&~
&@�@�
&�
&��
&��
&�
&��
&��
'~
'H�@�
'�
'��
'��
'�
'��
'��
(~
(P�@�
(�
(��
(��
( �
(��
(��
)!~
)�@�
)"�
)��
)��
)#�
)��
)��
*$~
*H�@�
*%�
*��
*��
*&�
*��
*��
+�
~
+P�@�
+�
�
+��
+��
+U�
+��
+��
,�
~
,8�@�
,�
�
,��
,��
,��
,��
,��
-�
~
-@�@�
-�
�
-��
-��
-��
-��
-��
.�
~
.@�@�
.�
�
.��
.��
.V�
.��
.��
/�
~
/H�@�
/�
�
/��
/��
/��
/��
/��
0�
~
0P�@�
0�
�
0��
0��
0^�
0��
0��
1�
~
1X�@�
1�
�
1��
1��
1�
�
1��
1��
2�
~
2(�@�
2�
�
2��
2��
2�
�
2��
2��
3�
~
3�@�
3�
�
3��
3��
3�
�
3��
3��
4�
~
4�@�
4�
�
4��
4��
4��
4��
4��
5�
~
5(�@�
5�
�
5��
5��
5��
5��
5��
6�
~
6X�@�
6�
�
6��
6��
6�
�
6��
6��
7�
~
7H�@�
7�
�
7��
7��
7�
�
7��
7��
8�
~
8��@�
8�
�
8��
8�
8�
�
8��
8��
9�
~
9��@�
9�
�
9�
9�
9�
9��
9��
:�
~
:�@�
:�
:$�
:�
:�
:��
:	�
;~
;�@�
;�
�
;$�
;�
;��
;��
;	�
<�
~
<�@�
<�
�
<��
<��
<�
�
<��
<��
=�
~
=�@�
=�
�
=��
=��
=��
=��
=��
>�
~
>�@�
>�
�
>��
>��
>p�
>��
>��
?�
~
? �@�
?�
�
?��
?��
?w�
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@�
~
@0�@�
@�
�
@��
@��
@o�
@��
@��
A�
~
A��@�
A�
�
A�
A�
A�
�
A��
A��
B�
~
B��@�
B�
�
B�
B�
B�
�
B��
B��
C�
~
C�@�
C�
�
C$�
C�
Co�
C��
C	�
D�
~
D�@�
D�
�
D��
D��
D.�
D��
D��
E�
~
E�@�
E�
�
E��
E��
E
�
E��
E��
F�
~
FH�@�
F�
�
F��
F��
F��
F��
F��
G�
~
GP�@�
G�
�
G��
G��
G�
�
G��
G��
H�
~
H��@�
H�
�
H�
H�
H�
�
H��
H��
I�
~
I�@�
I�
�
I��
I�
I��
I��
I	�
J�
~
J�@�
J�
�
J��
J��
J�
�
J��
J��
K�
~
K�@�
K�
�
K��
K��
K��
K��
K��
L�
~
L �@�
L�
�
L��
L��
L��
L��
L��
M�
~
M0�@�
M�
�
M��
M��
M�
�
M��
M��
N�
~
N0�@�
N�
�
N��
N��
N��
N��
N��
O�
~
OX�@�
O�
�
O��
O��
O	�
O��
O��
P�
~
P �@�
P�
�
P��
P��
Pr�
P��
P��
Q�
~
Q(�@�
Q�
�
Q��
Q��
Q��
Q��
Q��
R�
~
R �@�
R�
�
R��
R��
R��
R��
R��
S�
~
S(�@�
S�
�
S��
S��
S�
�
S��
S��
T�
~
T0�@�
T�
�
T��
T��
T�
�
T��
T��
U�
~
U8�@�
U�
�
U��
U��
U�
U��
U��
V�
~
V@�@�
V�
�
V��
V��
V�
�
V��
V��
W�
~
WH�@�
W�
�
W��
W��
W��
W��
W��
X�
~
XP�@�
X�
�
X��
X��
X��
X��
X��
Y�
~
YX�@�
Y�
�
Y��
Y��
Y~�
Y��
Y��
Z�
~
Z(�@�
Z�
�
Z��
Z��
Z�
�
Z��
Z��
[�
~
[0�@�
[�
�
[��
[��
[�
�
[��
[��
\{
~
\0�@�
\|
�
\��
\��
\}
�
\��
\��
]~
~
]�@�
]
�
]��
]��
]n�
]��
]��
^�
~
^�@�
^�
�
^��
^��
^
�
^��
^��
_�
~
_0�@�
_�
�
_��
_��
_��
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`�
~
`8�@�
`�
�
`��
`��
`:�
`��
`��
a�
~
a@�@�
a�
�
a��
a��
a��
a��
a��
b�
~
b��@�
b�
�
b��
b�
b�
�
b��
b��
c�
~
c��@�
c�
�
c�
c�
c�
�
c��
c��
d�
~
d�@�
d�
�
d��
d��
d�
�
d��
d��
e�
~
eX�@�
e�
�
e��
e��
eD�
e��
e��
f�
~
f(�@�
f�
�
f��
f��
f6�
f��
f��
g�
~
g0�@�
g�
�
g��
g��
g��
g��
g��
h�
~
h0�@�
h�
�
h��
h��
h�
h��
h��
i�
~
i8�@�
i�
�
i��
i��
i@�
i��
i��
j�
~
j@�@�
j�
�
j��
j��
jq�
j��
j��
k�
~
kH�@�
kW
�
k��
k��
kX
�
k��
k��
lY
~
lP�@�
lZ
�
l��
l��
l[
�
l��
l��
m\
~
mX�@�
m]
�
m��
m��
m^
�
m��
m��
n_
~
n �@�
n`
�
n��
n��
n��
n��
n��
o_
~
o(�@�
oa
�
o��
o��
ob
�
o��
o��
pc
~
p0�@�
pd
�
p��
p��
p��
p��
p��
qe
~
q8�@�
qf
�
q��
q��
qg
�
q��
q��
rh
~
r@�@�
ri
�
r��
r��
r��
r��
r��
sj
~
s@�@�
sk
�
s��
s��
sK�
s��
s��
tl
~
tP�@�
tm
�
t��
t��
t��
t��
t��
un
~
u(�@�
uo
�
u��
u��
u��
u��
u��
vp
~
v(�@�
vq
�
v��
v��
vk�
v��
v��
wr
~
wH�@�
ws
�
w��
w��
w��
w��
w��
xt
~
xX�@�
xu
�
x��
x��
x?�
x��
x��
yv
~
y(�@�
yw
�
y��
y��
y��
y��
y��
zx
~
z8�@�
zy
�
z��
z��
zr�
z��
z��
{z
~
{H�@�
{4
�
{��
{��
{�
{��
{��
|5
~
|X�@�
|6
�
|��
|��
|��
|��
|��
}7
~
}P�@�
}8
�
}��
}��
}K�
}��
}��
~9
~
~�@�
~:
�
~��
~��
~��
~��
~��
;
~
��@�
<
�
�
�
=
�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�>
~
��@�
�?
�
�$�
��
�@
�
���
�	�
�A
~
��@�
�B
�
���
���
�C
�
���
���
�>
~
��@�
�D
�
���
���
�E
�
���
���
�F
~
��@�
�G
�
���
���
���
���
���
�H
~
��@�
�I
�
���
���
�i�
���
���
�J
~
� �@�
�K
�
���
���
�L
�
���
���
�>
~
�(�@�
�M
�
���
���
���
���
���
�N
~
�(�@�
�O
�
���
���
�
�
���
���
�P
~
�8�@�
�Q
�
���
���
�R
�
���
���
�>
~
�X�@�
�S
�
���
���
�:�
���
���
�T
~
�(�@�
�U
�
���
���
���
���
���
�V
~
� �@�
�
�
���
���
�
�
���
���
�
~
��@�
�
�
���
���
��
�
���
���
�
~
�8�@�
�
�
���
���
�
�
���
���
�
~
��@�
�
�
���
���
�U�
���
���
�
~
�(�@�
�
�
���
���
�p�
���
���
�
~
�0�@�
�
�
���
���
�I�
���
���
�
~
�8�@�
�
�
���
���
�
�
���
���
�
~
�@�@�
� 
�
���
���
�V�
���
���
�!
~
�@�@�
�"
�
���
���
���
���
���
�#
~
�P�@�
�$
�
���
���
�%
�
���
���
�&
~
��@�
�'
�
���
���
��
���
���
�(
~
�X�@�
�)
�
���
���
�*
�
���
���
�+
~
��@�
�,
�
�U�
���
���
���
���
�-
~
�@�@�
�.
�
���
���
���
���
���
�/
~
��@�
�0
�
���
���
��
���
���
�1
~
��@�
�2
�
���
���
�9�
���
���
�3
~
��@�
��	�
���
���
���
���
���
�1
~
�H�@�
��	�
���
���
��	�
���
���
��	~
�@�@�
��	�
���
���
���
���
���
��	~
�H�@�
��	�
���
���
���
���
���
��	~
�P�@�
��	�
���
���
��	�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��	~
�0�@�
��	�
���
���
�9�
���
���
��	~
�8�@�
��	�
���
���
��
���
���
��	~
�P�@�
��	�
���
���
���
���
���
��	~
�X�@�
��	�
���
���
��	�
���
���
��	~
��@�
��	�
���
��
��
���
�	�
��	~
��@�
�
�
���
���
�
�
���
���
�
~
�(�@�
�
�
���
���
�
�
���
���
�
~
�8�@�
�
�
���
���
�n�
���
���
�
~
�@�@�
�
�
���
���
�
�
���
���
�	
~
�H�@�
�

�
���
���
�
�
���
���
�
~
�P�@�
�
�
���
���
�[�
���
���
�
~
�H�@�
�
�
���
���
�
�
���
���
��	~
�@�@�
��	�
���
���
���
���
���
��	~
��@�
��	�
���
���
��	�
���
���
��	~
�0�@�
��	�
���
���
�{�
���
���
��	~
�8�@�
��	�
���
���
��	�
���
���
��	~
��@�
��	�
�$�
��
��	�
���
�	�
��	~
���@�
��	�
��
��
���
���
���
��	~
��@�
��	�
�$�
��
�9�
���
�	�
��	~
��@�
��	�
���
���
���
���
���
��	~
��@�
��	�
�U�
���
�
�
���
���
��	~
�H�@�
��	�
���
���
�A�
���
���
��	~
���@�
��	�
��
��
��	�
���
���
��	~
�0�@�
��	�
���
���
���
���
���
��	~
�H�@�
��	�
���
���
��	�
���
���
��	~
��@�
��	�
�U�
���
���
���
���
��	~
��@�
��	�
�U�
���
��
���
���
��	~
��@�
��	�
���
���
�4�
���
���
��	~
� �@�
��	�
���
���
�^�
���
���
��	~
�(�@�
��	�
���
���
�g�
���
���
��	~
�0�@�
��	�
���
���
���
���
���
��	~
�(�@�
��	�
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��	~
��@�
��	�
���
���
���
���
���
��	~
�X�@�
��	�
���
���
���
���
���
��	~
�X�@�
��	�
���
���
�}
�
���
���
��	~
�X�@�
��	�
���
���
�
�
���
���
��	~
� �@�
��	�
���
���
�r�
���
���
��	~
�@�@�
��	�
���
���
���
���
���
��	~
�H�@�
��	�
���
���
���
���
���
��	~
�P�@�
��	�
���
���
��	�
���
���
��	~
�X�@�
��	�
���
���
��	�
���
���
��	~
��@�
��	�
���
���
���
���
���
��	~
��@�
��	�
���
���
��
���
���
��	~
�0�@�
��	�
���
���
�U�
���
���
��	~
��@�
��	�
���
���
��	�
���
���
��	~
� �@�
��	�
���
���
�R�
���
���
��	~
��@�
��	�
�$�
��
���
���
�	�
��	~
��@�
��	�
���
���
��	�
���
���
��	~
��@�
��	�
���
���
���
���
���
��	~
��@�
��	�
���
���
��	�
���
���
��	~
� �@�
��	�
���
���
���
���
���
��	~
�P�@�
��	�
���
���
���
���
���
��	~
�X�@�
��	�
���
���
��	�
���
���
��	~
��@�
��	�
���
���
�o�
���
���
��	~
� �@�
��	�
���
���
��	�
���
���
��	~
�H�@�
��	�
���
���
���
���
���
��	~
��@�
��	�
���
���
��	�
���
���
��	~
�(�@�
��	�
���
���
�X�
���
���
��	~
�X�@�
�b	�
���
���
�w�
���
���
�c	~
��@�
�d	�
�$�
��
���
���
�	�
�e	~
�8�@�
�f	�
���
���
���
���
���
�g	~
�X�@�
�h	�
���
���
�i	�
���
���
�j	~
�@�@�
�k	�
���
���
���
���
���
�l	~
�P�@�
�m	�
���
���
�n	�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�o	~
�X�@�
�p	�
���
���
�q	�
���
���
�r	~
� �@�
�s	�
���
���
�i�
���
���
�t	~
�@�@�
�u	�
���
���
�g
�
���
���
�v	~
�P�@�
�w	�
���
���
�(�
���
���
�x	~
�X�@�
�y	�
���
���
���
���
���
�z	~
���@�
�{	�
��
��
�|	�
���
���
�}	~
��@�
�~	�
���
��
��
���
�	�
�	~
��@�
��	�
���
���
���
���
���
�	~
��@�
��	�
���
���
��	�
���
���
��	~
�(�@�
��	�
���
���
��	�
���
���
�	~
�0�@�
��	�
���
���
���
���
���
�	~
�8�@�
�<	�
���
���
���
���
���
�	~
�@�@�
�=	�
���
���
�>	�
���
���
�?	~
�@�@�
�@	�
���
���
�A	�
���
���
�	~
�H�@�
�B	�
���
���
�C	�
���
���
�	~
�H�@�
�D	�
���
���
�G�
���
���
�	~
�P�@�
�E	�
���
���
�/�
���
���
�F	~
�P�@�
�G	�
���
���
�H	�
���
���
�I	~
�P�@�
�J	�
���
���
�K	�
���
���
�L	~
��@�
�M	�
���
���
�o�
���
���
�N	~
�(�@�
�O	�
���
���
�1�
���
���
�P	~
�@�@�
�Q	�
���
���
�R	�
���
���
�S	~
�(�@�
�T	�
���
���
���
���
���
�U	~
�P�@�
�V	�
���
���
�W	�
���
���
�X	~
�P�@�
�Y	�
���
���
�,�
���
���
�Z	~
�(�@�
�[	�
���
���
�|�
���
���
�\	~
�X�@�
�]	�
���
���
���
���
���
�^	~
�0�@�
�_	�
���
���
���
���
���
�`	~
�@�@�
�a	�
���
���
��
���
���
�`	~
�@�@�
�	�
���
���
�6�
���
���
�	~
�H�@�
�	�
���
���
�
�
���
���
�	~
�@�@�
�	�
���
���
�K�
���
���D�lppppppppppppppppppppppppppppppp		�F	,	�D�	,L�		���	؏	��F		�
	�8�		
		؏L�	���D	�]4�	@	,		�			r		�L�	PI	��	@0�	��	,�	h�*C�
		~
	H�@�
		�
	��
	�~
	�@�
	��
	��
	 	~
	�@�
	!	�
	$�
	�
	��
	��
		�
	"	~
	P�@�
	#	�
	��
	��
	$	�
	��
	��
	%	~
	�@�
	&	�
	��
	��
	��
	��
	��
	'	~
	 �@�
	(	�
	��
	��
	q�
	��
	��
	)	~
	�@�
	*	�
	��
	��
	��
	��
	��
	+	~
	�@�
	,	�
	��
	��
	��
	��
	��
	+	~
	 �@�
	-	�
	��
	��
	��
	��
	��
	.	~
	P�@�
	/	�
	��
	��
	��
	��
	��
		0	~
		X�@�
		1	�
		��
		��
		B�
		��
		��

	2	~

	��@�

	3	�

	�

	�

	4	�

	��

	��
	2	~
	�@�
	5	�
	$�
	�
	��
	��
		�
	6	~
	�@�
	7	�
	��
	��
	8	�
	��
	��

	9	~

	�@�

	:	�

	��

	��

	��

	��

	��
	;	~
	P�@�
	��
	��
	��
	q�
	��
	��
	�~
	X�@�
	��
	��
	��
	��
	��
	��
	�~
	X�@�
	��
	��
	��
	��
	��
	��
	�~
	P�@�
	��
	��
	��
	��
	��
	��
	�~
	�@�
		�
	��
	��
	��
	��
	��
		~
	8�@�
		�
	��
	��
	��
	��
	��
		~
	�@�
		�
	$�
	�
	+�
	��
		�
		~
	0�@�
		�
	��
	��
	��
	��
	��
		~
	H�@�
		�
	��
	��
			�
	��
	��
	
	~
	P�@�
		�
	��
	��
	��
	��
	��
		~
	X�@�
	
	�
	��
	��
	��
	��
	��
		~
	(�@�
		�
	��
	��
		�
	��
	��
		~
	 �@�
		�
	��
	��
	��
	��
	��
		~
	0�@�
		�
	��
	��
	��
	��
	��
		~
	@�@�
		�
	��
	��
	�
	��
	��
		~
	8�@�
		�
	��
	��
		�
	��
	��
		~
	@�@�
	��
	��
	��
	
�
	��
	��
	�~
	H�@�
	��
	��
	��
	��
	��
	��D�lppppppppppppppppppppppppppppppp 	!	�F"	,#	�D�$	,L�%	&	���'	؏(	��F)	�*	�8�+	,	-	.	؏L�/	���D0	�]4�1	@2	,3	4	�5	6	7	r8	9	�L�:	PI;	��<	@0�=	��>	,�?	h�*C�
 	�~
 	P�@�
 	��
 	��
 	��
 	��
 	��
 	��
!	�~
!	8�@�
!	��
!	��
!	��
!	��
!	��
!	��
"	�~
"	(�@�
"	��
"	��
"	��
"	G�
"	��
"	��
#	�~
#	X�@�
#	��
#	��
#	��
#	��
#	��
#	��
$	�~
$	0�@�
$	��
$	��
$	��
$	��
$	��
$	��
%	�~
%	8�@�
%	��
%	��
%	��
%	A�
%	��
%	��
&	�~
&	@�@�
&	��
&	��
&	��
&	w�
&	��
&	��
'	�~
'	H�@�
'	��
'	��
'	��
'	��
'	��
'	��
(	�~
(	H�@�
(	��
(	��
(	��
(	��
(	��
(	��
)	�~
)	P�@�
)	��
)	��
)	��
)	��
)	��
)	��
*	�~
*	P�@�
*	��
*	��
*	��
*	��
*	��
*	��
+	�~
+	X�@�
+	��
+	��
+	��
+	��
+	��
+	��
,	�~
,	X�@�
,	��
,	��
,	��
,	��
,	��
,	��
-	�~
-	X�@�
-	��
-	��
-	��
-	��
-	��
-	��
.	�~
.	 �@�
.	��
.	��
.	��
.	��
.	��
.	��
/	�~
/	0�@�
/	��
/	��
/	��
/	��
/	��
/	��
0	�~
0	(�@�
0	��
0	��
0	��
0	��
0	��
0	��
1	�~
1	 �@�
1	��
1	��
1	��
1	��
1	��
1	��
2	�~
2	(�@�
2	��
2	��
2	��
2	��
2	��
2	��
3	�~
3	H�@�
3	��
3	��
3	��
3	��
3	��
3	��
4	�~
4	 �@�
4	��
4	��
4	��
4	��
4	��
4	��
5	�~
5	(�@�
5	��
5	��
5	��
5	��
5	��
5	��
6	�~
6	(�@�
6	��
6	��
6	��
6	�
6	��
6	��
7	�~
7	8�@�
7	��
7	��
7	��
7	^�
7	��
7	��
8	�~
8	H�@�
8	��
8	��
8	��
8	��
8	��
8	��
9	�~
9	(�@�
9	��
9	��
9	��
9	��
9	��
9	��
:	�~
:	X�@�
:	��
:	��
:	��
:	��
:	��
:	��
;	�~
;	�@�
;	��
;	��
;	��
;	�
;	��
;	��
<	�~
<	�@�
<	��
<	U�
<	��
<	��
<	��
<	��
=	�~
=	�@�
=	��
=	��
=	��
=	��
=	��
=	��
>	�~
>	�@�
>	��
>	��
>	��
>	��
>	��
>	��
?	�~
?	 �@�
?	��
?	��
?	��
?	S�
?	��
?	��D�lppppppppppppppppppppppppppppppp@	A	�FB	,C	�D�D	,L�E	F	���G	؏H	��FI	�J	�8�K	L	M	N	؏L�O	���DP	�]4�Q	@R	,S	T	�U	V	W	rX	Y	�L�Z	PI[	��\	@0�]	��^	,�_	h�*C�
@	�~
@	P�@�
@	��
@	��
@	��
@	O�
@	��
@	��
A	�~
A	X�@�
A	��
A	��
A	��
A	��
A	��
A	��
B	�~
B	 �@�
B	��
B	��
B	��
B	3�
B	��
B	��
C	�~
C	��@�
C	��
C	�
C	�
C	��
C	��
C	��
D	�~
D	(�@�
D	��
D	��
D	��
D	��
D	��
D	��
E	�~
E	�@�
E	��
E	��
E	~
E	�p@�
E	��
E		�
F	�~
F	8�@�
F	��
F	��
F	��
F	e�
F	��
F	��
G	�~
G	8�@�
G	��
G	��
G	��
G	y�
G	��
G	��
H	�~
H	@�@�
H	��
H	��
H	��
H	�
H	��
H	��
I	�~
I	H�@�
I	l�
I	��
I	��
I	��
I	��
I	��
J	m~
J	P�@�
J	n�
J	��
J	��
J	o�
J	��
J	��
K	p~
K	X�@�
K	q�
K	��
K	��
K	r�
K	��
K	��
L	s~
L	�@�
L	t�
L	$�
L	�
L	u�
L	��
L		�
M	v~
M	(�@�
M	w�
M	��
M	��
M	��
M	��
M	��
N	x~
N	(�@�
N	y�
N	��
N	��
N	q�
N	��
N	��
O	z~
O	�@�
O	{�
O	U�
O	��
O	|�
O	��
O	��
P	}~
P	H�@�
P	~�
P	��
P	��
P	��
P	��
P	��
Q	~
Q	(�@�
Q	��
Q	��
Q	��
Q	6�
Q	��
Q	��
R	�~
R	(�@�
R	��
R	��
R	��
R	�
R	��
R	��
S	�~
S	@�@�
S	��
S	��
S	��
S	
�
S	��
S	��
T	�~
T	�@�
T	��
T	$�
T	�
T	��
T	��
T		�
U	�~
U	 �@�
U	��
U	��
U	��
U	�
U	��
U	��
V	�~
V	H�@�
V	��
V	��
V	��
V	i�
V	��
V	��
W	�~
W	H�@�
W	��
W	��
W	��
W	�
W	��
W	��
X	�~
X	P�@�
X	��
X	��
X	��
X	A�
X	��
X	��
Y	�~
Y	X�@�
Y	A�
Y	��
Y	��
Y	B�
Y	��
Y	��
Z	C~
Z	�@�
Z	D�
Z	��
Z	��
Z	E�
Z	��
Z	��
[	F~
[	�@�
[	G�
[	��
[	��
[	��
[	��
[	��
\	H~
\	H�@�
\	I�
\	��
\	��
\	�	�
\	��
\	��
]	J~
]	P�@�
]	K�
]	��
]	��
]	��
]	��
]	��
^	L~
^	X�@�
^	M�
^	��
^	��
^	N�
^	��
^	��
_	O~
_	X�@�
_	P�
_	��
_	��
_	Q�
_	��
_	��D�lppppppppppppppppppppppppppppppp`	a	�Fb	,c	�D�d	,L�e	f	���g	؏h	��Fi	�j	�8�k	l	m	n	؏L�o	���Dp	�]4�q	@r	,s	t	�u	v	w	rx	y	�L�z	PI{	��|	@0�}	��~	,�	h�*C�
`	R~
`	8�@�
`	S�
`	��
`	��
`	��
`	��
`	��
a	R~
a	X�@�
a	T�
a	��
a	��
a	U�
a	��
a	��
b	V~
b	��@�
b	W�
b	�
b	�
b	X�
b	��
b	��
c	Y~
c	��@�
c	Z�
c	�
c	�
c	[�
c	��
c	��
d	\~
d	�@�
d	]�
d	$�
d	�
d	j�
d	��
d		�
e	^~
e	X�@�
e	_�
e	��
e	��
e	`�
e	��
e	��
f	a~
f	(�@�
f	b�
f	��
f	��
f	D
�
f	��
f	��
g	c~
g	�@�
g	d�
g	��
g	��
g	e�
g	��
g	��
h	f~
h	�@�
h	g�
h	��
h	��
h	��
h	��
h	��
i	h~
i	�@�
i	i�
i	��
i	��
i	��
i	��
i	��
j	j~
j	�@�
j	k�
j	��
j	��
j	�
j	��
j	��
k	~
k	 �@�
k	�
k	��
k	��
k	X
�
k	��
k	��
l	~
l	(�@�
l	�
l	��
l	��
l	��
l	��
l	��
m	 ~
m	0�@�
m	!�
m	��
m	��
m	��
m	��
m	��
n	"~
n	8�@�
n	#�
n	��
n	��
n	w�
n	��
n	��
o	$~
o	(�@�
o	%�
o	��
o	��
o	&�
o	��
o	��
p	'~
p	0�@�
p	(�
p	��
p	��
p	\�
p	��
p	��
q	)~
q	�@�
q	*�
q	��
q	��
q	+�
q	��
q	��
r	,~
r	�@�
r	-�
r	��
r	��
r	��
r	��
r	��
s	.~
s	(�@�
s	/�
s	��
s	��
s	 �
s	��
s	��
t	0~
t	�@�
t	1�
t	U�
t	��
t	�
t	��
t	��
u	2~
u	X�@�
u	3�
u	��
u	��
u	4�
u	��
u	��
v	5~
v	�@�
v	6�
v	��
v	��
v	R�
v	��
v	��
w	7~
w	H�@�
w	8�
w	��
w	��
w	9�
w	��
w	��
x	:~
x	(�@�
x	;�
x	��
x	��
x	D�
x	��
x	��
y	<~
y	8�@�
y	=�
y	��
y	��
y	�
y	��
y	��
z	>~
z	@�@�
z	?�
z	��
z	��
z	��
z	��
z	��
{	@~
{	H�@�
{	��
{	��
{	��
{	��
{	��
{	��
|	�~
|	P�@�
|	��
|	��
|	��
|	��
|	��
|	��
}	�~
}	X�@�
}	��
}	��
}	��
}	��
}	��
}	��
~	�~
~	�@�
~	�
~	��
~	��
~	�
~	��
~	��
	�~
	�@�
	�
	��
	��
	�
	��
	��D�lppppppppppppppppppppppppppppppp�	�	�F�	,�	�D��	,L��	�	����	؏�	��F�	��	�8��	�	�	�	؏L��	���D�	�]4��	@�	,�	�	��	�	�	r�	�	�L��	PI�	���	@0��	���	,��	h�*C�
�	�~
�	(�@�
�	�
�	��
�	��
�	�
�	��
�	��
�	�~
�	P�@�
�	�
�	��
�	��
�	�
�	��
�	��
�	~
�	X�@�
�	�
�	��
�	��
�	C�
�	��
�	��
�	~
�	��@�
�		�
�	�
�	~
�	@X@�
�	��
�	��
�	
~
�	�@�
�	�
�	$�
�	�
�	=�
�	��
�		�
�	~
�	�@�
�	
�
�	��
�	��
�	y�
�	��
�	��
�	~
�	�@�
�	�
�	U�
�	��
�	�
�	��
�	��
�	~
�	 �@�
�	�
�	��
�	��
�	��
�	��
�	��
�	~
�	(�@�
�	�
�	��
�	��
�	j�
�	��
�	��
�	~
�	(�@�
�	�
�	��
�	��
�	Q�
�	��
�	��
�	~
�	@�@�
�	�
�	��
�	��
�	��
�	��
�	��
�	~
�	�@�
�	�
�	��
�	��
�	�	�
�	��
�	��
�	~
�	(�@�
�	�
�	��
�	��
�	�
�	��
�	��
�	�~
�	(�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	n�
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	>�
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	�
�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	�
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	(�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	0�@�
�	��
�	��
�	��
�	6�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��D�lppppppppppppppppppppppppppppppp�	�	�F�	,�	�D��	,L��	�	����	؏�	��F�	��	�8��	�	�	�	؏L��	���D�	�]4��	@�	,�	�	��	�	�	r�	�	�L��	PI�	���	@0��	���	,��	h�*C�
�	�~
�	(�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	0�@�
�	��
�	��
�	��
�	;�
�	��
�	��
�	�~
�	�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	0�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	0�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	n�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	
�
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	T�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	 �@�
�	��
�	��
�	��
�	s�
�	��
�	��
�	�~
�	8�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	_�
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	s�
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	G�
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	�@�
�	��
�	$�
�	�
�	K�
�	��
�		�
�	�~
�	0�@�
�	��
�	��
�	��
�	Y�
�	��
�	��
�	�~
�	X�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	@�@�
�	��
�	��
�	��
�	�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	o~
�	8�@�
�	p�
�	��
�	��
�	q�
�	��
�	��
�	r~
�	 �@�
�	s�
�	��
�	��
�	��
�	��
�	��
�	t~
�	(�@�
�	u�
�	��
�	��
�	��
�	��
�	��
�	v~
�	(�@�
�	w�
�	��
�	��
�	��
�	��
�	��
�	x~
�	8�@�
�	y�
�	��
�	��
�	9�
�	��
�	��D�lppppppppppppppppppppppppppppppp�	�	�F�	,�	�D��	,L��	�	����	؏�	��F�	��	�	

 !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMO����PQRSTUVWXYZ[\]^_`abcdefghijklmnopqrstuvwxyz{|}~�8��	�	�	�	؏L��	���D�	�]4��	@�	,�	�	��	�	�	r�	�	�L��	PI�	���	@0��	���	,��	h�*C�
�	z~
�	�@�
�	{�
�	��
�	��
�	��
�	��
�	��
�	|~
�	 �@�
�	}�
�	��
�	��
�	��
�	��
�	��
�	~~
�	H�@�
�	�
�	��
�	��
�	��
�	��
�	��
�	~~
�	P�@�
�	��
�	��
�	��
�	@�
�	��
�	��
�	~~
�	X�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	>	�
�	��
�	��
�	�~
�	H�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	P�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	�@�
�	��
�	�
�	�
�	��
�	��
�	��
�	M~
�	�@�
�	N�
�	��
�	��
�	��
�	��
�	��
�	O~
�	 �@�
�	P�
�	��
�	��
�	y�
�	��
�	��
�	Q~
�	(�@�
�	R�
�	��
�	��
�	S�
�	��
�	��
�	T~
�	8�@�
�	U�
�	��
�	��
�	��
�	��
�	��
�	V~
�	�@�
�	W�
�	$�
�	�
�	��
�	��
�		�
�	X~
�	��@�
�	Y�
�	�
�	�
�	Z�
�	��
�	��
�	[~
�	��@�
�	\�
�	�
�	�
�	]�
�	��
�	��
�	^~
�	�@�
�	_�
�	$�
�	�
�	��
�	��
�		�
�	`~
�	�@�
�	a�
�	$�
�	�
�	��
�	��
�		�
�	`~
�	�@�
�	b�
�	��
�	��
�	c�
�	��
�	��
�	d~
�	�@�
�	e�
�	��
�	��
�	�
�	��
�	��
�	f~
�	�@�
�	g�
�	��
�	��
�	M�
�	��
�	��
�	h~
�	�@�
�	i�
�	��
�	��
�	�
�	��
�	��
�	j~
�	�@�
�	k�
�	��
�	��
�	n	�
�	��
�	��
�	d~
�	 �@�
�	l�
�	��
�	��
�	m�
�	��
�	��
�	h~
�	 �@�
�	n�
�	��
�	��
�	n�
�	��
�	��
�	-~
�	(�@�
�	.�
�	��
�	��
�	/�
�	��
�	��
�	d~
�	0�@�
�	0�
�	��
�	��
�	i�
�	��
�	��
�	1~
�	0�@�
�	2�
�	��
�	��
�	c�
�	��
�	��
�	3~
�	8�@�
�	4�
�	��
�	��
�	w�
�	��
�	��
�	d~
�	@�@�
�	5�
�	��
�	��
�	6�
�	��
�	��D�lppppppppppppppppppppppppppppppp�	�	�F�	,�	�D��	,L��	�	����	؏�	��F�	��	�8��	�	�	�	؏L��	���D�	�]4��	@�	,�	�	��	�	�	r�	�	�L��	PI�	���	@0��	���	,��	h�*C�
�	7~
�	H�@�
�	8�
�	��
�	��
�	��
�	��
�	��
�	9~
�	H�@�
�	:�
�	��
�	��
�	;�
�	��
�	��
�	<~
�	P�@�
�	=�
�	��
�	��
�	A	�
�	��
�	��
�	>~
�	X�@�
�	?�
�	��
�	��
�	a�
�	��
�	��
�	@~
�	P�@�
�	A�
�	��
�	��
�	

�
�	��
�	��
�	B~
�	��@�
�	C�
�	�
�	�
�	D�
�	��
�	��
�	E~
�	�@�
�	F�
�	��
�	�
�	�
�	��
�		�
�	G~
�	�@�
�	H�
�	��
�	��
�	��
�	��
�	��
�	E~
�	�@�
�	I�
�	��
�	��
�	��
�	��
�	��
�	J~
�	��@�
�	K�
�	��
�	�
�	L�
�	��
�	��
�	J~
�	0�@�
�		�
�	��
�	��
�	g�
�	��
�	��
�	J~
�	@�@�
�	
�
�	��
�	��
�	��
�	��
�	��
�	J~
�	H�@�
�	�
�	��
�	��
�	�
�	��
�	��
�	J~
�	P�@�
�	
�
�	��
�	��
�	i�
�	��
�	��
�	J~
�	P�@�
�	�
�	��
�	��
�	�
�	��
�	��
�	~
�	0�@�
�	�
�	��
�	��
�	j�
�	��
�	��
�	~
�	8�@�
�	�
�	��
�	��
�	��
�	��
�	��
�	~
�	H�@�
�	�
�	��
�	��
�	��
�	��
�	��
�	~
�	P�@�
�	�
�	��
�	��
�	��
�	��
�	��
�	~
�	X�@�
�	�
�	��
�	��
�	�
�	��
�	��
�	~
�	�@�
�	�
�	��
�	��
�	
�
�	��
�	��
�	~
�	�@�
�	�
�	U�
�	��
�	j�
�	��
�	��
�	~
�	�@�
�	�
�	��
�	��
�	��
�	��
�	��
�	 ~
�	0�@�
�	!�
�	��
�	��
�	�
�	��
�	��
�	"~
�	X�@�
�	#�
�	��
�	��
�	$�
�	��
�	��
�	%~
�	P�@�
�	&�
�	��
�	��
�	)�
�	��
�	��
�	%~
�	X�@�
�	'�
�	��
�	��
�	�
�	��
�	��
�	(~
�	(�@�
�	)�
�	��
�	��
�	*�
�	��
�	��
�	(~
�	(�@�
�	+�
�	��
�	��
�	�
�	��
�	��
�	,~
�	(�@�
�	��
�	��
�	��
�	�
�
�	��
�	��
�	,~
�	(�@�
�	��
�	��
�	��
�	��
�	��
�	��
�	�~
�	(�@�
�	��
�	��
�	��
�	��
�	��
�	��D�lppppppppppppppppppppppppppppppp

�F
,
�D�
,L�

���
؏
��F	
�

�8�



؏L�
���D
�]4�
@
,

�


r

�L�
PI
��
@0�
��
,�
h�*C�

�~

H�@�

��

��

��

#�

��

��

�~

P�@�

��

��

��

�
�

��

��

�~

H�@�

��

��

��

�

��

��

�~

8�@�

��

��

��

o�

��

��

�~

(�@�

��

��

��

_�

��

��

�~

P�@�

��

��

��

��

��

��

�~

��@�

��

�

~

�u@�

��

��

�~

@�@�

��

��

��

��

��

��

�~

H�@�

��

��

��

��

��

��
	
�~
	
P�@�
	
��
	
��
	
��
	
B�
	
��
	
��


�~


X�@�


��


��


��


��


��


��

~

0�@�

�

��

��

o�

��

��

~

X�@�

�

��

��

��

��

��

~

�@�

�

��

��

�

��

��

~

�@�

�

��

��

	�

��

��

~

(�@�

��

��

��

q�

��

��

~

P�@�

��

��

��

��

��

��

�~

P�@�

��

��

��

D�

��

��

�~

0�@�

��

��

��

��

��

��

�~

X�@�

��

��

��

 �

��

��

�~

(�@�

��

��

��

��

��

��

�~

@�@�

��

��

��

�	�

��

��

�~

�@�

��

��

�

��

��

	�

�~

0�@�

��

��

��

�

��

��

�~

0�@�

��

��

��

z�

��

��

�~

8�@�

��

��

��


�

��

��

�~

H�@�

��

��

��

��

��

��

�~

P�@�

��

��

��

�

��

��

�~

X�@�

��

��

��

��

��

��

�~

X�@�

��

��

��

�

��

��

�~

0�@�

��

��

��

1�

��

��

�~

(�@�

��

��

��

��

��

��D�lppppppppppppppppppppppppppppppp 
!
�F"
,#
�D�$
,L�%
&
���'
؏(
��F)
�*
�8�+
,
-
.
؏L�/
���D0
�]4�1
@2
,3
4
�5
6
7
r8
9
�L�:
PI;
��<
@0�=
��>
,�?
h�*C�
 
�~
 
@�@�
 
��
 
��
 
��
 
+�
 
��
 
��
!
�~
!
P�@�
!
��
!
��
!
��
!
:�
!
��
!
��
"
�~
"
(�@�
"
��
"
��
"
��
"
_�
"
��
"
��
#
�~
#
X�@�
#
��
#
��
#
��
#
��
#
��
#
��
$
�~
$
H�@�
$
��
$
��
$
��
$
��
$
��
$
��
%
�~
%
P�@�
%
��
%
��
%
��
%
��
%
��
%
��
&
�~
&
��@�
&
��
&
�
&
�
&
��
&
��
&
��
'
�~
'
�@�
'
��
'
��
'
��
'
��
'
��
'
��
(
�~
(
�@�
(
��
(
��
(
��
(
M�
(
��
(
��
)
�~
)
 �@�
)
��
)
��
)
��
)
��
)
��
)
��
*
�~
*
(�@�
*
��
*
��
*
��
*
��
*
��
*
��
+
�~
+
0�@�
+
��
+
��
+
��
+
��
+
��
+
��
,
�~
,
8�@�
,
��
,
��
,
��
,
�
�
,
��
,
��
-
�~
-
0�@�
-
��
-
��
-
��
-
��
-
��
-
��
.
�~
.
8�@�
.
��
.
��
.
��
.
��
.
��
.
��
/
�~
/
@�@�
/
��
/
��
/
��
/

�
/
��
/
��
0
�~
0
H�@�
0
��
0
��
0
��
0
!�
0
��
0
��
1
�~
1
P�@�
1
��
1
��
1
��
1
��
1
��
1
��
2
�~
2
X�@�
2
��
2
��
2
��
2
��
2
��
2
��
3
�~
3
�@�
3
u�
3
��
3
��
3
H�
3
��
3
��
4
v~
4
 �@�
4
w�
4
��
4
��
4
��
4
��
4
��
5
x~
5
(�@�
5
y�
5
��
5
��
5
��
5
��
5
��
6
z~
6
(�@�
6
{�
6
��
6
��
6
9�
6
��
6
��
7
|~
7
�@�
7
}�
7
��
7
��
7
~�
7
��
7
��
8
~
8
��@�
8
��
8
�
8
�
8
��
8
��
8
��
9
�~
9
�@�
9
��
9
$�
9
�
9
��
9
��
9
	�
:
�~
:
�@�
:
��
:
��
:
��
:
��
:
��
:
��
;
�~
;
�@�
;
��
;
��
;
��
;
/�
;
��
;
��
<
�~
<
�@�
<
��
<
$�
<
�
<
��
<
��
<
	�
=
�~
=
�@�
=
��
=
��
=
��
=
��
=
��
=
��
>
�~
>
P�@�
>
��
>
��
>
��
>
��
>
��
>
��
?
�~
?
X�@�
?
��
?
��
?
��
?
��
?
��
?
��D�lppppppppppppppppppppppppppppppp@
A
�FB
,C
�D�D
,L�E
F
���G
؏H
��FI
�J
�8�K
L
M
N
؏L�O
���DP
�]4�Q
@R
,S
T
�U
V
W
rX
Y
�L�Z
PI[
��\
@0�]
��^
,�_
h�*C�
@
�~
@
��@�
@
��
@
�
@
�
@
��
@
��
@
��
A
�~
A
P�@�
A
��
A
��
A
��
A
9�
A
��
A
��
B
�~
B
@�@�
B
��
B
��
B
��
B
��
B
��
B
��
C
�~
C
�@�
C
��
C
��
C
�
C
6�
C
��
C
	�
D
�~
D
(�@�
D
N�
D
��
D
��
D
O�
D
��
D
��
E
P~
E
�@�
E
Q�
E
$�
E
�
E
	�
E
��
E
	�
F
R~
F
H�@�
F
S�
F
��
F
��
F
��
F
��
F
��
G
T~
G
�@�
G
U�
G
$�
G
�
G
��
G
��
G
	�
H
V~
H
8�@�
H
W�
H
��
H
��
H
��
H
��
H
��
I
X~
I
��@�
I
Y�
I
�
I
�
I
Z�
I
��
I
��
J
[~
J
�@�
J
\�
J
��
J
�
J
1�
J
��
J
	�
K
X~
K
�@�
K
]�
K
��
K
��
K
^�
K
��
K
��
L
_~
L
�@�
L
`�
L
��
L
��
L
d�
L
��
L
��
M
a~
M
8�@�
M
b�
M
��
M
��
M
��
M
��
M
��
N
c~
N
H�@�
N
d�
N
��
N
��
N
i�
N
��
N
��
O
e~
O
(�@�
O
f�
O
��
O
��
O
n�
O
��
O
��
P
e~
P
(�@�
P
g�
P
��
P
��
P
h�
P
��
P
��
Q
e~
Q
(�@�
Q
i�
Q
��
Q
��
Q
j�
Q
��
Q
��
R
k~
R
8�@�
R
l�
R
��
R
��
R
�
R
��
R
��
S
m~
S
@�@�
S
n�
S
��
S
��
S
��
S
��
S
��
T
o~
T
X�@�
T
p�
T
��
T
��
T
s�
T
��
T
��
U
q~
U
�@�
U
r�
U
$�
U
�
U
{�
U
��
U
	�
V
s~
V
�@�
V
t�
V
��
V
��
V
��
V
��
V
��
W
+~
W
�@�
W
,�
W
��
W
��
W
�
W
��
W
��
X
-~
X
 �@�
X
.�
X
��
X
��
X
��
X
��
X
��
Y
/~
Y
(�@�
Y
0�
Y
��
Y
��
Y
_�
Y
��
Y
��
Z
1~
Z
0�@�
Z
2�
Z
��
Z
��
Z
K�
Z
��
Z
��
[
3~
[
8�@�
[
4�
[
��
[
��
[
�
[
��
[
��
\
3~
\
@�@�
\
5�
\
��
\
��
\
��
\
��
\
��
]
+~
]
H�@�
]
6�
]
��
]
��
]
7�
]
��
]
��
^
8~
^
H�@�
^
9�
^
��
^
��
^
��
^
��
^
��
_
:~
_
0�@�
_
;�
_
��
_
��
_
��
_
��
_
��D�lppppppppppppppppppppppppppppppp`
a
�Fb
,c
�D�d
,L�e
f
���g
؏h
��Fi
�j
�8�k
l
m
n
؏L�o
���Dp
�]4�q
@r
,s
t
�u
v
w
rx
y
�L�z
PI{
��|
@0�}
��~
,�
h�*C�
`
<~
`
H�@�
`
=�
`
��
`
��
`
>�
`
��
`
��
a
?~
a
P�@�
a
@�
a
��
a
��
a
�
a
��
a
��
b
A~
b
��@�
b
B�
b
�
b
�
b
C�
b
��
b
��
c
D~
c
P�@�
c
E�
c
��
c
��
c
F�
c
��
c
��
d
G~
d
��@�
d
H�
d
�
d
�
d
��
d
��
d
��
e
I~
e
�@�
e
J�
e
��
e
��
e
K�
e
��
e
��
f
G~
f
�@�
f
L�
f
��
f
��
f
8�
f
��
f
��
g
G~
g
�@�
g
M�
g
��
g
��
g
��
g
��
g
��
h
~
h
8�@�
h
	�
h
��
h
��
h

�
h
��
h
��
i
~
i
@�@�
i
�
i
��
i
��
i
��
i
��
i
��
j
G~
j
H�@�
j

�
j
��
j
��
j
�
j
��
j
��
k
~
k
H�@�
k
�
k
��
k
��
k
��
k
��
k
��
l
~
l
P�@�
l
�
l
��
l
��
l
�
l
��
l
��
m
~
m
X�@�
m
�
m
��
m
��
m
�
m
��
m
��
n
~
n
8�@�
n
�
n
��
n
��
n
�
n
��
n
��
o
~
o
H�@�
o
�
o
��
o
��
o
��
o
��
o
��
p
~
p
P�@�
p
�
p
��
p
��
p
&�
p
��
p
��
q
~
q
�@�
q
�
q
��
q
��
q
��
q
��
q
��
r
~
r
�@�
r
 �
r
��
r
��
r
�
r
��
r
��
s
!~
s
�@�
s
"�
s
U�
s
��
s

�
s
��
s
��
t
#~
t
�@�
t
$�
t
$�
t
�
t
i�
t
��
t
	�
u
%~
u
�@�
u
&�
u
��
u
��
u
X�
u
��
u
��
v
'~
v
�@�
v
(�
v
��
v
��
v
)�
v
��
v
��
w
*~
w
 �@�
w
��
w
��
w
��
w
��
w
��
w
��
x
�~
x
0�@�
x
��
x
��
x
��
x
�
x
��
x
��
y
�~
y
8�@�
y
��
y
��
y
��
y
R�
y
��
y
��
z
�~
z
@�@�
z
��
z
��
z
��
z
�
z
��
z
��
{
�~
{
H�@�
{
��
{
��
{
��
{
z�
{
��
{
��
|
�~
|
�@�
|
��
|
��
|
��
|
��
|
��
|
��
}
�~
}
 �@�
}
��
}
��
}
��
}
��
}
��
}
��
~
�~
~
(�@�
~
��
~
��
~
��
~
q�
~
��
~
��

�~

8�@�

��

��

��

��

��

��D�lppppppppppppppppppppppppppppppp�
�
�F�
,�
�D��
,L��
�
����
؏�
��F�
��
�8��
�
�
�
؏L��
���D�
�]4��
@�
,�
�
��
�
�
r�
�
�L��
PI�
���
@0��
���
,��
h�*C�
�
�~
�
@�@�
�
��
�
��
�
��
�
S�
�
��
�
��
�
�~
�
H�@�
�
��
�
��
�
��
�
&�
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
	�
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
X�
�
��
�
��
�
�~
�
��@�
�
�
�
�
�
�
�
�
�
��
�
��
�
~
�
�@�
�
�
�
$�
�
�
�
��
�
��
�
	�
�
~
�
�@�
�
�
�
��
�
��
�
�
�
��
�
��
�
~
�
�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
+�
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
t�
�
��
�
��
�
�~
�
 �@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
0�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
0�@�
�
��
�
��
�
��
�
/�
�
��
�
��
�
�~
�
8�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
@�@�
�
��
�
��
�
��
�
I�
�
��
�
��
�
�~
�
@�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
H�@�
�
��
�
��
�
��
�
v�
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
�
�
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
X�
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
v�
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
,�
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
X�
�
��
�
��
�
�~
�
@�@�
�
��
�
��
�
��
�
�
�
��
�
��
�
�~
�
@�@�
�
��
�
��
�
��
�
.�
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
��
�
��
�
��D�lppppppppppppppppppppppppppppppp�
�
�F�
,�
�D��
,L��
�
����
؏�
��F�
��
�8��
�
�
�
؏L��
���D�
�]4��
@�
,�
�
��
�
�
r�
�
�L��
PI�
���
@0��
���
,��
h�*C�
�
�~
�
(�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
��@�
�
��
�
�
�
�
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
0�@�
�
��
�
��
�
��
�
z�
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
�
�
��
�
��
�
�~
�
8�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
=�
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
9�
�
��
�
��
�
�~
�
0�@�
�
��
�
��
�
��
�
q�
�
��
�
��
�
�~
�
0�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
8�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
@�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
 �@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
0�@�
�
��
�
��
�
��
�
q�
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
(�@�
�
��
�
��
�
��
�
M�
�
��
�
��
�
�~
�
8�@�
�
e�
�
��
�
��
�
��
�
��
�
��
�
f~
�
@�@�
�
g�
�
��
�
��
�
r�
�
��
�
��
�
h~
�
H�@�
�
i�
�
��
�
��
�
��
�
��
�
��
�
j~
�
X�@�
�
k�
�
��
�
��
�
��
�
��
�
��
�
l~
�
X�@�
�
m�
�
��
�
��
�
n�
�
��
�
��
�
o~
�
H�@�
�
p�
�
��
�
��
�
��
�
��
�
��
�
o~
�
P�@�
�
q�
�
��
�
��
�
��
�
��
�
��
�
r~
�
X�@�
�
s�
�
��
�
��
�
d�
�
��
�
��
�
t~
�
H�@�
�
u�
�
��
�
��
�
��
�
��
�
��
�
v~
�
P�@�
�
w�
�
��
�
��
�
��
�
��
�
��D�lppppppppppppppppppppppppppppppp�
�
�F�
,�
�D��
,L��
�
����
؏�
��F�
��
�8��
�
�
�
؏L��
���D�
�]4��
@�
,�
�
��
�
�
r�
�
�L��
PI�
���
@0��
���
,��
h�*C�
�
x~
�
X�@�
�
y�
�
��
�
��
�
k�
�
��
�
��
�
z~
�
0�@�
�
{�
�
��
�
��
�
��
�
��
�
��
�
|~
�
�@�
�
}�
�
��
�
��
�
��
�
��
�
��
�
~~
�
�@�
�
�
�
$�
�
�
�
��
�
��
�
	�
�
�~
�
 �@�
�
>�
�
��
�
��
�
?�
�
��
�
��
�
@~
�
(�@�
�
A�
�
��
�
��
�
��
�
��
�
��
�
B~
�
�@�
�
C�
�
��
�
��
�
Y�
�
��
�
��
�
D~
�
(�@�
�
E�
�
��
�
��
�
��
�
��
�
��
�
F~
�
(�@�
�
G�
�
��
�
��
�
k�
�
��
�
��
�
H~
�
0�@�
�
I�
�
��
�
��
�
�
�
��
�
��
�
J~
�
H�@�
�
K�
�
��
�
��
�
L�
�
��
�
��
�
M~
�
X�@�
�
N�
�
��
�
��
�
O�
�
��
�
��
�
P~
�
�@�
�
Q�
�
��
�
��
�
��
�
��
�
��
�
R~
�
(�@�
�
S�
�
��
�
��
�
��
�
��
�
��
�
T~
�
(�@�
�
U�
�
��
�
��
�
��
�
��
�
��
�
V~
�
0�@�
�
W�
�
��
�
��
�
��
�
��
�
��
�
X~
�
X�@�
�
Y�
�
��
�
��
�
��
�
��
�
��
�
Z~
�
H�@�
�
[�
�
��
�
��
�
{�
�
��
�
��
�
\~
�
 �@�
�
]�
�
��
�
��
�
�
�
��
�
��
�
^~
�
8�@�
�
_�
�
��
�
��
�
D�
�
��
�
��
�
`~
�
�@�
�
a�
�
��
�
��
�
w�
�
��
�
��
�
b~
�
@�@�
�
c�
�
��
�
��
�
��
�
��
�
��
�
b~
�
H�@�
�
d�
�
��
�
��
�
m�
�
��
�
��
�
b~
�
H�@�
�
�
�
��
�
��
�
�
�
��
�
��
�
~
�
X�@�
�
�
�
��
�
��
�
��
�
��
�
��
�
~
�
(�@�
�
�
�
��
�
��
�
��
�
��
�
��
�
~
�
(�@�
�
�
�
��
�
��
�
�
�
��
�
��
�
~
�
(�@�
�
 �
�
��
�
��
�
h�
�
��
�
��
�
!~
�
@�@�
�
"�
�
��
�
��
�
P�
�
��
�
��
�
#~
�
 �@�
�
$�
�
��
�
��
�
��
�
��
�
��
�
%~
�
(�@�
�
&�
�
��
�
��
�
6�
�
��
�
��
�
'~
�
�@�
�
(�
�
$�
�
�
�
��
�
��
�
	�D�lppppppppppppppppppppppppppppppp�
�
�F�
,�
�D��
,L��
�
����
؏�
��F�
��
�8��
�
�
�
؏L��
���D�
�]4��
@�
,�
�
��
�
�
r�
�
�L��
PI�
���
@0��
���
,��
h�*C�
�
)~
�
�@�
�
*�
�
��
�
��
�
+�
�
��
�
��
�
,~
�
�@�
�
-�
�
��
�
��
�
^�
�
��
�
��
�
.~
�
�@�
�
/�
�
��
�
��
�
R�
�
��
�
��
�
0~
�
��@�
�
1�
�
�
�
�
�
2�
�
��
�
��
�
3~
�
�@�
�
4�
�
��
�
��
�
��
�
��
�
��
�
3~
�
 �@�
�
5�
�
��
�
��
�
�
�
��
�
��
�
3~
�
(�@�
�
6�
�
��
�
��
�
:�
�
��
�
��
�
3~
�
0�@�
�
7�
�
��
�
��
�
9�
�
��
�
��
�
8~
�
(�@�
�
9�
�
��
�
��
�
:�
�
��
�
��
�
;~
�
(�@�
�
<�
�
��
�
��
�
=�
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�

�
�
��
�
��
�
�~
�
@�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
�
�
��
�
��
�
~
�
X�@�
�
�
�
��
�
��
�
n�
�
��
�
��
�
~
�
X�@�
�
�
�
��
�
��
�
�
�
��
�
��
�
~
�
X�@�
�
�
�
��
�
��
�
�
�
��
�
��
�
~
�
0�@�
�
	�
�
��
�
��
�
��
�
��
�
��
�

~
�
8�@�
�
�
�
��
�
��
�
��
�
��
�
��
�

~
�
@�@�
�
�
�
��
�
��
�
o�
�
��
�
��
�

~
�
P�@�
�
�
�
��
�
��
�
2�
�
��
�
��
�

~
�
X�@�
�
�
�
��
�
��
�
��
�
��
�
��
�
~
�
��@�
�
�
�
�
�
�
�
�
�
��
�
��
�
~
�
(�@�
�
�
�
��
�
��
�
��
�
��
�
��
�
~
�
@�@�
�
�
�
��
�
��
�

�
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
�
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
�
�
�
��
�
��
�
�~
�
P�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
X�@�
�
��
�
��
�
��
�
��
�
��
�
��
�
�~
�
�@�
�
��
�
��
�
��
�
��
�
��
�
��D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
�@�
��
��
��
o�
��
��
�~
 �@�
��
��
��
�
��
��
�~
@�@�
��
��
��
V�
��
��
�~
(�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
��
��
��
�~
@�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
	�~
	H�@�
	��
	��
	��
	��
	��
	��

�~

(�@�

��

��

��

�

��

��
�~
8�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
K�
��
��

�~

(�@�

��

��

��

&�

��

��
�~
�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
0�@�
��
��
��
��
��
��
�~
8�@�
��
��
��
n	�
��
��
�~
@�@�
��
��
��
��
��
��
�~
H�@�
��
��
��
h�
��
��
�~
P�@�
��
��
��
��
��
��
�~
(�@�
��
��
��
��
��
��
�~
�@�
��
��
��
3�
��
��
�~
�@�
��
��
��
��
��
��
�~
��@�
��
�
�
��
��
��
�~
@�@�
��
��
��
�
��
��
�~
H�@�
��
��
��
t�
��
��
�~
��@�
��
�
�
��
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
��
��
��
�~
�@�
��
��
��
�
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 �~
 �@�
 ��
 U�
 ��
 ��
 ��
 ��
!�~
! �@�
!��
!��
!��
!��
!��
!��
"�~
"�@�
"��
"$�
"�
"_�
"��
"	�
#�~
#�@�
#��
#��
#��
#��
#��
#��
$�~
$�@�
$��
$��
$��
$V�
$��
$��
%�~
%(�@�
%��
%��
%��
%[
�
%��
%��
&�~
&(�@�
&��
&��
&��
&��
&��
&��
'�~
'0�@�
'��
'��
'��
'F�
'��
'��
(�~
(8�@�
(��
(��
(��
(��
(��
(��
)�~
)@�@�
)��
)��
)��
)K�
)��
)��
*�~
*@�@�
*��
*��
*��
*o�
*��
*��
+�~
+H�@�
+��
+��
+��
+��
+��
+��
,�~
,P�@�
,��
,��
,��
,��
,��
,��
-�~
-X�@�
-��
-��
-��
-��
-��
-��
.�~
.P�@�
.��
.��
.��
.��
.��
.��
/c~
/H�@�
/d�
/��
/��
/��
/��
/��
0c~
0P�@�
0e�
0��
0��
0w�
0��
0��
1f~
1��@�
1g�
1��
1�
1h�
1��
1��
2i~
2��@�
2j�
2�
2�
2k�
2��
2��
3l~
3�@�
3m�
3��
3��
3�
3��
3��
4n~
4�@�
4o�
4��
4��
4��
4��
4��
5p~
5(�@�
5q�
5��
5��
5R	�
5��
5��
6r~
60�@�
6s�
6��
6��
6��
6��
6��
7t~
78�@�
7u�
7��
7��
7v�
7��
7��
8w~
8P�@�
8x�
8��
8��
8y�
8��
8��
9z~
9(�@�
9{�
9��
9��
9|�
9��
9��
:}~
:(�@�
:~�
:��
:��
:��
:��
:��
;~
;(�@�
;��
;��
;��
;$	�
;��
;��
<�~
<(�@�
<��
<��
<��
<�
<��
<��
=�~
=�@�
=��
=��
=��
=		�
=��
=��
><~
>�@�
>=�
>��
>��
>�
>��
>��
?>~
?(�@�
??�
?��
?��
?}
�
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@@~
@(�@�
@A�
@��
@��
@��
@��
@��
AB~
A�@�
AC�
A��
A��
A:�
A��
A��
BD~
B8�@�
BE�
B��
B��
BP�
B��
B��
CF~
C�@�
CG�
C��
C��
CH�
C��
C��
DI~
D0�@�
DJ�
D��
D��
DI�
D��
D��
EK~
E�@�
EL�
E$�
E�
E��
E��
E	�
FK~
F�@�
FM�
F��
F��
F�
F��
F��
GN~
G�@�
GO�
G��
G��
Gi�
G��
G��
HP~
H �@�
HQ�
H��
H��
H�
H��
H��
IP~
I(�@�
IR�
I��
I��
IS�
I��
I��
JT~
J@�@�
JU�
J��
J��
J��
J��
J��
KV~
KX�@�
KW�
K��
K��
KX�
K��
K��
LY~
L�@�
LZ�
L��
L��
L[�
L��
L��
M\~
M�@�
M]�
M��
M��
M^�
M��
M��
N_~
N�@�
N`�
N��
N��
Nq�
N��
N��
Oa~
O �@�
Ob�
O��
O��
O��
O��
O��
P~
P(�@�
P�
P��
P��
P,�
P��
P��
Q~
Q(�@�
Q�
Q��
Q��
QM�
Q��
Q��
R~
R0�@�
R�
R��
R��
Rq�
R��
R��
S~
S0�@�
S �
S��
S��
S��
S��
S��
T!~
T0�@�
T"�
T��
T��
T��
T��
T��
U~
U0�@�
U#�
U��
U��
Uw�
U��
U��
V$~
V8�@�
V%�
V��
V��
Vg�
V��
V��
W&~
W@�@�
W'�
W��
W��
W��
W��
W��
X(~
X@�@�
X)�
X��
X��
X��
X��
X��
Y*~
YH�@�
Y+�
Y��
Y��
Y,�
Y��
Y��
Z-~
ZX�@�
Z.�
Z��
Z��
Z��
Z��
Z��
[/~
[X�@�
[0�
[��
[��
[1�
[��
[��
\2~
\P�@�
\3�
\��
\��
\c�
\��
\��
]4~
]�@�
]5�
]��
]��
]6�
]��
]��
^7~
^ �@�
^8�
^��
^��
^_�
^��
^��
_9~
_X�@�
_:�
_��
_��
_;�
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`�~
`�@�
`��
`$�
`�
`��
`��
`	�
a�~
a�@�
a��
a��
a��
a��
a��
a��
b�~
b �@�
b��
b��
b��
b��
b��
b��
c�~
c0�@�
c��
c��
c��
c2�
c��
c��
d�~
d8�@�
d��
d��
d��
d��
d��
d��
e�~
e@�@�
e�
e��
e��
e�
e��
e��
f~
f@�@�
f�
f��
f��
f2�
f��
f��
g�~
gH�@�
g�
g��
g��
g�
g��
g��
h~
hH�@�
h�
h��
h��
h��
h��
h��
i�~
iP�@�
i�
i��
i��
i��
i��
i��
j�~
jX�@�
j	�
j��
j��
j
�
j��
j��
k~
k(�@�
k�
k��
k��
k
�
k��
k��
l~
l�@�
l�
l��
l��
l�
l��
l��
m~
m�@�
m�
m��
m��
m2�
m��
m��
n~
n�@�
n�
n��
n��
n��
n��
n��
o~
o0�@�
o�
o��
o��
o��
o��
o��
p~
p8�@�
p�
p��
p��
p		�
p��
p��
q�~
qP�@�
q��
q��
q��
q��
q��
q��
r�~
rX�@�
r��
r��
r��
r"�
r��
r��
s�~
s�@�
s��
s��
s�
s��
s��
s	�
t�~
t�@�
t��
t$�
t�
t|�
t��
t	�
u�~
u�@�
u��
u��
u��
u��
u��
u��
v�~
v�@�
v��
v��
v��
vt�
v��
v��
w�~
w�@�
w��
wU�
w��
w��
w��
w��
x�~
x0�@�
x��
x��
x��
x��
x��
x��
y�~
yH�@�
y��
y��
y��
y=�
y��
y��
z�~
zP�@�
z��
z��
z��
zr�
z��
z��
{�~
{X�@�
{��
{��
{��
{��
{��
{��
|�~
|0�@�
|��
|��
|��
|��
|��
|��
}�~
}8�@�
}��
}��
}��
}�
}��
}��
~�~
~@�@�
~��
~��
~��
~��
~��
~��
�~
H�@�
��
��
��
@�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�Q�
���
���
��~
�0�@�
���
���
���
�6�
���
���
��~
�8�@�
���
���
���
�8�
���
���
��~
��@�
���
�U�
���
�s�
���
���
��~
��@�
���
���
��
� �
���
�	�
��~
�0�@�
���
���
���
�B�
���
���
��~
�@�@�
���
���
���
�l�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�_�
���
���
��~
�P�@�
���
���
���
���
���
���
��~
��@�
���
�$�
��
�R�
���
�	�
��~
�(�@�
���
���
���
�w�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�i�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
�z�
���
���
�{�
���
���
�|~
� �@�
�}�
���
���
���
���
���
�~~
��@�
��
���
���
�r�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
�7�
���
���
��~
�(�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�0�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
�<�
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
�����������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������
��~
�(�@�
���
���
���
�b�
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
�W�
���
���
���
���
���
��~
� �@�
�X�
���
���
��
���
���
�Y~
�(�@�
�Z�
���
���
���
���
���
��~
�0�@�
�[�
���
���
���
���
���
�\~
�8�@�
�]�
���
���
���
���
���
�^~
�@�@�
�_�
���
���
�g�
���
���
�`~
�H�@�
�a�
���
���
��
���
���
�b~
�P�@�
�c�
���
���
���
���
���
�d~
�X�@�
�e�
���
���
�f�
���
���
�g~
�(�@�
�h�
���
���
���
���
���
�i~
�H�@�
�j�
���
���
�k�
���
���
�l~
���@�
�m�
��
��
�n�
���
���
�o~
� �@�
�p�
���
���
�C�
���
���
�q~
�(�@�
�r�
���
���
�o�
���
���
�s~
�(�@�
�t�
���
���
�G�
���
���
�u~
��@�
�v�
�$�
��
�4�
���
�	�
�w~
��@�
�x�
���
���
���
���
���
�y~
� �@�
�8�
���
���
�>	�
���
���
�y~
�(�@�
�9�
���
���
�:�
���
���
�;~
�0�@�
�<�
���
���
�V�
���
���
�y~
�0�@�
�=�
���
���
���
���
���
�>~
�8�@�
�?�
���
���
�z�
���
���
�@~
�@�@�
�A�
���
���
�B�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�C~
�@�@�
�D�
���
���
�r�
���
���
�E~
�H�@�
�F�
���
���
���
���
���
�C~
�H�@�
�G�
���
���
��	�
���
���
�H~
��@�
�I�
�$�
��
���
���
�	�
�J~
��@�
�K�
���
���
�L�
���
���
�M~
��@�
�N�
���
���
�&�
���
���
�O~
�(�@�
�P�
���
���
�Q�
���
���
�R~
�0�@�
�S�
���
���
�1�
���
���
�T~
�8�@�
�U�
���
���
�P�
���
���
�V~
��@�
��
�$�
��
���
���
�	�
�~
�(�@�
��
���
���
���
���
���
�~
�@�@�
��
���
���
�k�
���
���
�~
�H�@�
��
���
���
���
���
���
�~
�H�@�
��
���
���
��
���
���
�~
�P�@�
��
���
���
���
���
���
�~
�X�@�
��
���
���
��
���
���
� ~
� �@�
�!�
���
���
�6�
���
���
�"~
�(�@�
�#�
���
���
�9�
���
���
�$~
�8�@�
�%�
���
���
���
���
���
�&~
��@�
�'�
���
���
���
���
���
�(~
�X�@�
�)�
���
���
�*�
���
���
�+~
�0�@�
�,�
���
���
�-�
���
���
�.~
�(�@�
�/�
���
���
���
���
���
�0~
�(�@�
�1�
���
���
�2�
���
���
�3~
�(�@�
�4�
���
���
���
���
���
�5~
�0�@�
�6�
���
���
�7�
���
���
��~
�8�@�
���
���
���
�K�
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�+�
���
���
��~
�H�@�
���
���
���
�D
�
���
���
��~
�P�@�
���
���
���
�c�
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
�$�
��
���
���
�	�
�~
�(�@�
��
���
���
��
���
���
�~
�0�@�
��
���
���
���
���
���
�~
�8�@�
��
���
���
��
���
���
�~
�@�@�
��
���
���
�2�
���
���
�	~
�H�@�
�
�
���
���
��
���
���
�~
�P�@�
�
�
���
���
�b
�
���
���
�~
�X�@�
��
���
���
��
���
���
�~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
�q�
���
���
��~
�H�@�
���
���
���
�4�
���
���
��~
�P�@�
���
���
���
�}
�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
�
�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
�s�
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�i�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
���
���
���
��~
���@�
���
��
��
���
���
���D�lppppppppppppppppppppppppppppppp�F,�D�,L����؏��F	�
�8�
؏L����D�]4�@,�r�L�PI��@0���,�h�*C�
�~
(�@�
��
��
��
~�
��
��
�~
H�@�
��
��
��
n	�
��
��
�~
 �@�
��
��
��
��
��
��
�~
(�@�
��
��
��
�
��
��
�~
(�@�
��
��
��
K�
��
��
�~
X�@�
��
��
��
�
��
��
�~
@�@�
��
��
��
F�
��
��
�~
(�@�
��
��
��

�
��
��
�~
(�@�
��
��
��
��
��
��
	�~
	��@�
	��
	��
	�
	��
	��
	��

�~

�@�

��

��

��

��

��

��
�~
�@�
��
��
��
l�
��
��
�~
�@�
��
��
��
��
��
��

�~

(�@�

��

��

��

��

��

��
�~
X�@�
��
��
��
�	�
��
��
�~
0�@�
��
��
��

�
��
��
�~
�@�
��
��
��
_�
��
��
�~
P�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
��
��
��
�~
X�@�
��
��
��
.�
��
��
�~
P�@�
��
��
��
@�
��
��
�~
(�@�
��
��
��
i�
��
��
�~
P�@�
��
��
��
�
��
��
n~
X�@�
o�
��
��
p�
��
��
q~
��@�
r�
�
�
s�
��
��
q~
�@�
t�
$�
�
u�
��
	�
v~
0�@�
w�
��
��
\�
��
��
x~
@�@�
y�
��
��
5�
��
��
z~
P�@�
{�
��
��
��
��
��
|~
��@�
}�
�
�
~�
��
��
~
�@�
��
$�
�
w�
��
	�
�~
@�@�
��
��
��
��
��
��D�lppppppppppppppppppppppppppppppp !�F",#�D�$,L�%&���'؏(��F)�*�8�+,-.؏L�/���D0�]4�1@2,34�567r89�L�:PI;��<@0�=��>,�?h�*C�
 �~
 (�@�
 ��
 ��
 ��
 ��
 ��
 ��
!�~
!8�@�
!��
!��
!��
!��
!��
!��
"�~
"P�@�
"��
"��
"��
"��
"��
"��
#�~
#�@�
#��
#$�
#�
#$	�
#��
#	�
$�~
$�@�
$��
$��
$��
$��
$��
$��
%�~
%�@�
%��
%U�
%��
%v�
%��
%��
&�~
&H�@�
&��
&��
&��
&H�
&��
&��
'�~
'(�@�
'��
'��
'��
'��
'��
'��
(�~
(�@�
(@�
(��
(��
(i�
(��
(��
)A~
)�@�
)B�
)U�
)��
)��
)��
)��
*C~
* �@�
*D�
*��
*��
*`�
*��
*��
+C~
+(�@�
+E�
+��
+��
+F�
+��
+��
,G~
,(�@�
,H�
,��
,��
,I�
,��
,��
-J~
-0�@�
-K�
-��
-��
-D�
-��
-��
.C~
.8�@�
.L�
.��
.��
.��
.��
.��
/M~
/@�@�
/N�
/��
/��
/��
/��
/��
0O~
0H�@�
0P�
0��
0��
0��
0��
0��
1G~
1H�@�
1Q�
1��
1��
1R�
1��
1��
2S~
2�@�
2"�
2��
2��
2T�
2��
2��
3S~
3 �@�
3U�
3��
3��
3��
3��
3��
4V~
4X�@�
4W�
4��
4��
4X�
4��
4��
5Y~
5�@�
5Z�
5��
5��
5��
5��
5��
6[~
6 �@�
6\�
6��
6��
6��
6��
6��
7]~
7 �@�
7^�
7��
7��
7_�
7��
7��
8`~
8(�@�
8a�
8��
8��
8b�
8��
8��
9`~
9(�@�
9c�
9��
9��
9d�
9��
9��
:e~
:�@�
:f�
:��
:��
:g�
:��
:��
;h~
;�@�
;i�
;��
;��
;j�
;��
;��
<k~
<�@�
<l�
<��
<��
<^�
<��
<��
=m~
= �@�
="�
=��
=��
=v�
=��
=��
>#~
>(�@�
>$�
>��
>��
>%�
>��
>��
?&~
?0�@�
?'�
?��
?��
?��
?��
?��D�lppppppppppppppppppppppppppppppp@A�FB,C�D�D,L�EF���G؏H��FI�J�8�KLMN؏L�O���DP�]4�Q@R,ST�UVWrXY�L�ZPI[��\@0�]��^,�_h�*C�
@(~
@@�@�
@)�
@��
@��
@��
@��
@��
A*~
A@�@�
A+�
A��
A��
A�
A��
A��
B,~
BH�@�
B-�
B��
B��
B<�
B��
B��
C.~
CH�@�
C/�
C��
C��
C��
C��
C��
D0~
DH�@�
D1�
D��
D��
D2�
D��
D��
E3~
EP�@�
E4�
E��
E��
E��
E��
E��
F5~
F�@�
F6�
F��
F��
F7�
F��
F��
G8~
G�@�
G9�
G��
G��
G��
G��
G��
H:~
H �@�
H;�
H��
H��
H��
H��
H��
I<~
IX�@�
I=�
I��
I��
I>�
I��
I��
J?~
J�@�
J�
J��
J��
Jg�
J��
J��
K?~
K(�@�
K�
K��
K��
K��
K��
K��
L~
L0�@�
L�
L��
L��
L_�
L��
L��
M~
M(�@�
M�
M��
M��
M	�
M��
M��
N~
N(�@�
N	�
N��
N��
N�
N��
N��
O
~
O(�@�
O�
O��
O��
O��
O��
O��
P
~
P0�@�
P�
P��
P��
P6�
P��
P��
Q
~
Q8�@�
Q
�
Q��
Q��
QS�
Q��
Q��
R~
RH�@�
R�
R��
R��
R��
R��
R��
S~
S(�@�
S�
S��
S��
S�
S��
S��
T~
T(�@�
T�
T��
T��
T��
T��
T��
U~
U�@�
U�
U��
U��
U�
U��
U��
V~
V(�@�
V�
V��
V��
V�
V��
V��
W~
W �@�
W�
W��
W��
Wp�
W��
W��
X~
X0�@�
X�
X��
X��
X��
X��
X��
Y~
YH�@�
Y�
Y��
Y��
Y��
Y��
Y��
Z ~
Z�@�
Z!�
ZU�
Z��
Zm�
Z��
Z��
[�~
[0�@�
[��
[��
[��
[��
[��
[��
\�~
\@�@�
\��
\��
\��
\��
\��
\��
]�~
]@�@�
]��
]��
]��
]P�
]��
]��
^�~
^P�@�
^��
^��
^��
^��
^��
^��
_�~
_X�@�
_��
_��
_��
_��
_��
_��D�lppppppppppppppppppppppppppppppp`a�Fb,c�D�d,L�ef���g؏h��Fi�j�8�klmn؏L�o���Dp�]4�q@r,st�uvwrxy�L�zPI{��|@0�}��~,�h�*C�
`�~
`�@�
`��
`��
`��
`��
`��
`��
a�~
a �@�
a��
a��
a��
a��
a��
a��
b�~
b0�@�
b��
b��
b��
b��
b��
b��
c�~
c@�@�
c��
c��
c��
c��
c��
c��
d�~
dH�@�
d��
d��
d��
dK�
d��
d��
e�~
e@�@�
e��
e��
e��
e�
e��
e��
f�~
f8�@�
f��
f��
f��
f��
f��
f��
g�~
g@�@�
g��
g��
g��
g��
g��
g��
h�~
hP�@�
h��
h��
h��
h��
h��
h��
i�~
i�@�
i��
i��
i��
i��
i��
i��
j�~
j�@�
j��
j��
j�
j
�
j��
j	�
k�~
k�@�
k��
k��
k��
k�
k��
k��
l~
l�@�
l��
l��
l��
l��
l��
l��
m�~
m0�@�
m��
m��
m��
m\�
m��
m��
n�~
n�@�
n��
n��
n��
n��
n��
n��
o�~
o�@�
o��
o��
o��
o��
o��
o��
p�~
p�@�
p��
p��
p��
p/�
p��
p��
q�~
qP�@�
q��
q��
q��
q��
q��
q��
r�~
rX�@�
r��
r��
r��
r>	�
r��
r��
s�~
sP�@�
s��
s��
s��
s��
s��
s��
t�~
t(�@�
t��
t��
t��
t��
t��
t��
u�~
u��@�
u��
u�
u�
u��
u��
u��
v�~
v�@�
v��
v��
v��
v��
v��
v��
w�~
w�@�
w��
wU�
w��
wQ�
w��
w��
x�~
x �@�
x��
x��
x��
x��
x��
x��
y�~
y(�@�
y��
y��
y��
y��
y��
y��
z�~
z0�@�
z��
z��
z��
z��
z��
z��
{�~
{@�@�
{��
{��
{��
{��
{��
{��
|�~
|(�@�
|��
|��
|��
|��
|��
|��
}�~
}@�@�
}��
}��
}��
}��
}��
}��
~�~
~X�@�
~��
~��
~��
~��
~��
~��
�~
@�@�
��
��
��
&�
��
��D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
�H�@�
���
���
���
��
�
���
���
��~
� �@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�q�
���
���
��~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
��
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
��	�
���
���
��~
���@�
���
��
��
���
���
���
��~
��@�
���
�$�
��
�5�
���
�	�
��~
��@�
���
���
���
���
���
���
��~
��@�
�p�
���
���
���
���
���
�q~
��@�
�r�
���
���
�`�
���
���
�s~
� �@�
�t�
���
���
���
���
���
�u~
� �@�
�v�
���
���
�+�
���
���
�w~
�(�@�
�x�
���
���
���
���
���
�y~
�X�@�
�z�
���
���
�{�
���
���
�|~
�(�@�
�}�
���
���
�~�
���
���
�~
�(�@�
���
���
���
�T�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�{�
���
���
��~
��@�
���
���
���
�g�
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
�>	�
���
���
��~
� �@�
���
���
���
�U�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�X�@�
�N�
���
���
���
���
���
�O~
�(�@�
�P�
���
���
�Q�
���
���
�R~
�@�@�
�S�
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�T~
� �@�
�U�
���
���
��
���
���
�V~
�(�@�
�W�
���
���
�^
�
���
���
�X~
�0�@�
�Y�
���
���
�n�
���
���
�X~
�8�@�
�Z�
���
���
�[�
���
���
�\~
�H�@�
�]�
���
���
�^�
���
���
�_~
�P�@�
�`�
���
���
���
���
���
�a~
� �@�
�b�
���
���
�w�
���
���
�c~
�(�@�
�d�
���
���
�e�
���
���
�f~
�0�@�
�g�
���
���
���
���
���
�h~
�X�@�
�i�
���
���
���
���
���
�j~
�(�@�
�k�
���
���
���
���
���
�l~
�0�@�
�m�
���
���
�L�
���
���
�n~
�P�@�
�o�
���
���
���
���
���
�-~
�X�@�
�.�
���
���
�/�
���
���
�0~
�X�@�
�1�
���
���
��
���
���
�2~
�(�@�
�3�
���
���
���
���
���
�4~
�(�@�
�5�
���
���
�6�
���
���
�7~
�0�@�
�8�
���
���
���
���
���
�9~
�(�@�
�:�
���
���
�Y�
���
���
�;~
�(�@�
�<�
���
���
���
���
���
�=~
���@�
�>�
��
��
�?�
���
���
�@~
�(�@�
�A�
���
���
�k�
���
���
�B~
�8�@�
�C�
���
���
���
���
���
�D~
�H�@�
�E�
���
���
���
���
���
�F~
�@�@�
�G�
���
���
���
���
���
�H~
�P�@�
�I�
���
���
�4�
���
���
�J~
�X�@�
�K�
���
���
�
�
���
���
�L~
�(�@�
�M�
���
���
�`�
���
���
�~
�8�@�
��
���
���
���
���
���
�
~
�0�@�
��
���
���
�M�
���
���
�~
�0�@�
��
���
���
��
���
���
�~
�8�@�
��
���
���
���
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
�~
�(�@�
��
���
���
���
���
���
�~
��@�
��
���
���
�T�
���
���
�~
��@�
��
�U�
���
�V�
���
���
�~
� �@�
��
���
���
���
���
���
�~
�(�@�
��
���
���
��
���
���
�~
�(�@�
��
���
���
� �
���
���
�!~
�8�@�
�"�
���
���
���
���
���
�#~
�0�@�
�$�
���
���
�R�
���
���
�%~
�8�@�
�&�
���
���
���
���
���
�%~
�@�@�
�'�
���
���
���
���
���
�(~
�H�@�
�)�
���
���
���
���
���
�*~
�(�@�
�+�
���
���
���
���
���
�,~
�H�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�&�
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
�9�
���
���
��~
� �@�
���
���
���
��
���
���
��~
�X�@�
���
���
���
�j�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
���
���
���
��~
�(�@�
��
���
���
��
���
���
�~
��@�
��
���
���
���
���
���
�~
��@�
��
���
���
��
���
���
�~
� �@�
��
���
���
���
���
���
�	~
� �@�
�
�
���
���
�o�
���
���
��~
�(�@�
���
���
���
�y�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
�w�
���
���
��~
�P�@�
���
���
���
��
���
���D�lppppppppppppppppppppppppppppppp���F�,��D��,L�������؏���F����8�����؏L�����D��]4��@�,������r���L��PI����@0�����,��h�*C�
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
� �@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
��
���
���
��~
�X�@�
���
���
���
���
���
���
��~
� �@�
���
���
���
�$	�
���
���
��~
��@�
���
�$�
��
�q�
���
�	�
��~
��@�
���
���
���
���
���
���
��~
��@�
���
�U�
���
���
���
���
��~
��@�
���
���
���
�1�
���
���
��~
� �@�
���
���
���
�w�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�(�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�@�@�
���
���
���
�_�
���
���
��~
�P�@�
���
���
���
�b�
���
���
��~
�(�@�
���
���
���
�J�
���
���
��~
�(�@�
���
���
���
���
���
���
��~
��@�
���
���
���
���
���
���
��~
��@�
���
���
���
�>�
���
���
��~
��@�
���
���
���
�i�
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�X�@�
���
���
���
�p�
���
���
��~
�X�@�
���
���
���
���
���
���
��~
�P�@�
���
���
���
�V�
���
���
��~
�@�@�
���
���
���
�&�
���
���
��~
�8�@�
���
���
���
���
���
���
��~
�H�@�
���
���
���
�V�
���
���
��~
�(�@�
���
���
���
��
���
���
��~
�0�@�
���
���
���
���
���
���
��~
�0�@�
���
���
���
���
���
���D�lppppppppppppppppppppppppppppppp

�F
,
�D�
,L�

���
؏
��F	
�

�8�




؏L�
���D
�]4�
@
,

�


r

�L�
PI
��
@0�
��
,�
h�*C�

�~

8�@�

|�

��

��

q�

��

��

}~

@�@�

~�

��

��


�

��

��

�~

@�@�

�

��

��

��

��

��

�~

H�@�

��

��

��

��

��

��

�~

P�@�

��

��

��

��

��

��

�~

X�@�

��

��

��

�	�

��

��

�~

@�@�

��

��

��


�

��

��

�~

@�@�

��

��

��

X�

��

��

�~

�@�

��

��

��

��

��

��
	
�~
	
X�@�
	
��
	
��
	
��
	
��
	
��
	
��


�~


X�@�


��


��


��


�


��


��

�~

X�@�

��

��

��

��

��

��

�~

�@�

��

$�

�

�

��

	�


�~


�@�


��


��


��


��


��


��

�~

�@�

��

��

��

��

��

��

�~

 �@�

��

��

��

��

��

��

�~

(�@�

[�

��

��

;�

��

��

�~

(�@�

\�

��

��

I�

��

��

�~

0�@�

]�

��

��

&�

��

��

�~

0�@�

^�

��

��

0�

��

��

�~

8�@�

_�

��

��

��

��

��

�~

@�@�

`�

��

��

{�

��

��

�~

H�@�

a�

��

��

��

��

��

b~

P�@�

c�

��

��

��

��

��

b~

X�@�

d�

��

��

��

��

��

e~

(�@�

f�

��

��

g�

��

��

h~

(�@�

i�

��

��

�

��

��

j~

X�@�

k�

��

��

D�

��

��

l~

�@�

m�

��

��

��

��

��

n~

�@�

o�

��

��

��

��

��

p~

 �@�

q�

��

��

��

��

��

r~

 �@�

s�

��

��

^�

��

��D�lppppppppppppppppppppppppppppppp 
!
�F"
,#
�D�$
,L�%
&
���'
؏(
��F)
�*
�8�+
,
-
.
؏L�/
���D0
�]4�1
@2
,3
4
�5
6
7
r8
9
�L�:
PI;
��<
@0�=
��>
,�?
h�*C�
 
t~
 
(�@�
 
u�
 
��
 
��
 
��
 
��
 
��
!
v~
!
0�@�
!
w�
!
��
!
��
!
x�
!
��
!
��
"
y~
"
0�@�
"
z�
"
��
"
��
"
��
"
��
"
��
#
{~
#
0�@�
#
9�
#
��
#
��
#
�
�
#
��
#
��
$
:~
$
8�@�
$
;�
$
��
$
��
$

�
$
��
$
��
%
<~
%
@�@�
%
=�
%
��
%
��
%
H�
%
��
%
��
&
>~
&
H�@�
&
?�
&
��
&
��
&
@�
&
��
&
��
'
A~
'
P�@�
'
B�
'
��
'
��
'
C�
'
��
'
��
(
D~
(
P�@�
(
E�
(
��
(
��
(
��
(
��
(
��
)
F~
)
X�@�
)
G�
)
��
)
��
)
P�
)
��
)
��
*
H~
*
X�@�
*
I�
*
��
*
��
*
��
*
��
*
��
+
H~
+
X�@�
+
J�
+
��
+
��
+
�
+
��
+
��
,
K~
,
 �@�
,
L�
,
��
,
��
,
��
,
��
,
��
-
M~
-
(�@�
-
N�
-
��
-
��
-
O�
-
��
-
��
.
P~
.
P�@�
.
Q�
.
��
.
��
.
��
.
��
.
��
/
R~
/
X�@�
/
S�
/
��
/
��
/
��
/
��
/
��
0
T~
0
X�@�
0
U�
0
��
0
��
0

�
0
��
0
��
1
V~
1
X�@�
1
W�
1
��
1
��
1
��
1
��
1
��
2
X~
2
0�@�
2
Y�
2
��
2
��
2
��
2
��
2
��
3
Z~
3
8�@�
3
�
3
��
3
��
3

�
3
��
3
��
4
~
4
H�@�
4
�
4
��
4
��
4
��
4
��
4
��
5
~
5
P�@�
5
 �
5
��
5
��
5
��
5
��
5
��
6
!~
6
H�@�
6
"�
6
��
6
��
6
��
6
��
6
��
7
!~
7
X�@�
7
#�
7
��
7
��
7
$�
7
��
7
��
8
%~
8
P�@�
8
&�
8
��
8
��
8
�
8
��
8
��
9
'~
9
�@�
9
(�
9
U�
9
��
9
�
9
��
9
��
:
)~
:
 �@�
:
*�
:
��
:
��
:
��
:
��
:
��
;
+~
;
(�@�
;
,�
;
��
;
��
;
J�
;
��
;
��
<
-~
<
0�@�
<
.�
<
��
<
��
<
/�
<
��
<
��
=
0~
=
0�@�
=
1�
=
��
=
��
=
��
=
��
=
��
>
2~
>
@�@�
>
3�
>
��
>
��
>
4�
>
��
>
��
?
5~
?
�@�
?
6�
?
��
?
��
?
��
?
��
?
��D�lppppppppppppppppppppppppppppppp@
A
�FB
,C
�D�D
,L�E
F
���G
؏H
��FI
�J
�8�K
L
�
@
7~
@
(�@�
@
8�
@
��
@
��
@
�
@
��
@
��
A
~
A
H�@�
A
�
A
��
A
��
A
6�
A
��
A
��
B
~
B
0�@�
B
�
B
��
B
��
B
Y�
B
��
B
��
C
~
C
(�@�
C
�
C
��
C
��
C
��
C
��
C
��
D
~
D
X�@�
D
�
D
��
D
��
D
T�
D
��
D
��
E
	~
E
�@�
E

�
E
��
E
��
E
D�
E
��
E
��
F
~
F
(�@�
F
�
F
��
F
��
F
Q�
F
��
F
��
G

~
G
8�@�
G
�
G
��
G
��
G
3�
G
��
G
��
H
~
H
@�@�
H
�
H
��
H
��
H
��
H
��
H
��
I
~
I
H�@�
I
�
I
��
I
��
I
d�
I
��
I
��
J
~
J
P�@�
J
�
J
��
J
��
J
�
J
��
J
��
K
~
K
P�@�
K
�
K
��
K
��
K
�
K
��
K
��
L
~
L
X�@�
L
�
L
��
L
��
L
�
L
��
L
����pppppppppppp>�@�?
��������
������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������������
��Oh��+'��0�8@Xp��'Stephen WalleyxStephen WalleyxMicrosoft Excel@�ԑ	����
��՜.��+,��0�	PXx����
��'University of Cambridge$
APS SCCM 1981to2005.txtWorksheets������ �FMicrosoft Excel Worksheet����8FIBExcel.Sheet.8CompObj������������	X������������������������������������

Anon7 - 2021