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Ray Lemar                                                                                                B�a�=���=��xKx<8�@�"��1���NVerdana1���NVerdana1���NVerdana1���NVerdana1���NVerdana1���NVerdana"$"#,##0_);\("$"#,##0\)!"$"#,##0_);[Red]\("$"#,##0\)""$"#,##0.00_);\("$"#,##0.00\)'""$"#,##0.00_);[Red]\("$"#,##0.00\)7*2_("$"* #,##0_);_("$"* \(#,##0\);_("$"* "-"_);_(@_).))_(* #,##0_);_(* \(#,##0\);_(* "-"_);_(@_)?,:_("$"* #,##0.00_);_("$"* \(#,##0.00\);_("$"* "-"??_);_(@_)6+1_(* #,##0.00_);_(* \(#,##0.00\);_(* "-"??_);_(@_)�"�"#,##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_-;_-* "-"??_-;_-@_-��� � ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� ��� �� � � ���� �� ���� �� ���� �� ���� �� �	�� �� � � � � ��������������������8�������������d��q:F���������c���-2���N�Wg���F�SW���c���-2���N�Wg���F�SW����������������̙��̙3f�3���������fff����3f3�f333�3�3f33�333\���`��YAPS SCCM 1981to2007.txt���d��   f�!PIsentropic compression experiments for mesoscale studies of energetic composites	1307-1310eBaer, M.R., Hobbs, M.L., Hall, C.A., Hooks, D.E., Gustavsen, R.L., Dattelbaum, D. and Sheffield, S.A.BIsentropic compression studies of energetic composite constituents	1165-1168(Bahl, K.L., Lee, R.S. and Weingart, R.C.OVelocity of spherically-diverging detonation waves in RX-26-AF, LX-17 and LX-10559-562Bai, C. and Ding, J.aA numerical study of hot spot formation and ignition of composite propellants under shock loading291-294Bai, C., Huang, F. and Ding, J.4Behavior of ammonium perchlorate under shock loading+Baker, E.L., Schimel, B. and Grantham, W.J.NNumerical optimization of ignition and growth reactive flow modeling for PAX2A�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. and Fortov, V.E.ZConductivity of C60 fullerene crystals under multi-step dynamic compression up to 300 kbar189-191?Averin, A.B., Dremov, V.V., Samarin, S.I. and Sapozhnikov, A.T.-Equation of state and phase diagram of carbon65-68wAverin, A.N., Alekseev, A.V., Batalov, S.V., Loboiko, B.G., Litvinov, B.V., Sumin, V.D., Filin, V.P. and Yagnakov, A.N.kInvestigation into low-temperatures influence on high explosive compounds sensitivity to shock-wave impacts847-849Averin, A.N., Batalov, S.V., Belenovsky, Y.A., Kostitsyn, O.V., Loboiko, B.C., Pestrechikhin, V.A., Sumin, V.D. and Filin, V.P.=Studying properties of explosives exposed to organic solvents917-920QAverkov, O.N., Gryadobitov, S.P., Kozlov, E.A., Lupilin, G.A. and Matushkin, N.D.~A solid state calorimeter for measuring the internal energy increment of metal samples, capable of surviving explosive loading859-862�Avrillaud, G., Asay, J.R., Bavay, M., Delchambre, M., Guerre, J., Bayol, F., Cubaynes, F., Kovalchuk, B.M., Mervini, J.A., Spielman, R.B., Hall, C.A., Hickman, R.J., Ao, T., Willis, M.D., Gupta, Y.M. and Bakeman, C.J.fVELOCE: A compact pulse for dynamic material characterization and hypervelocity impact of flyer plates	1161-1164Backofen, J.E. and Weickert, C.DInitial free-surface velocities imparted by grazing detonation waves919-922!Backofen, J.E. and 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 stages954-957DObtaining the Gurney energy constant for a two-step propulsion model958-961Backofen, J.E.vAdditional information showing that a cylinder's material and geometry affect measuring an explosive's Gurney velocity445-448JOn the spall strengths and Hugoniot elastic limits of some strong ceramics473-476'Aslam, T.D., Bdzil, J.B. and Hill, L.G.0Analysis of the LANL detonation-confinement testAslam, T.D.)Direct numerical simulation of detonation931-9351Detonation shock dynamics calibration of PBX 9501813-816#Asokamani, R. and Amirthakumari, M.[Metallisation and superconductivity in some of the ionic and covalent solids under pressure665-668,Assink, R.A., Boslough, M.B. and Cygan, R.T.LCharacterization of amorphous material in shocked quartz by NMR spectroscopy383-386/Atisivan, R., Bandyopadhyay, A. and Gupta, Y.M.1Dynamic tensile response of alumina-Al composites697-7000Atou, T., Kikuchi, M., Fukuoka, K. and Syona, Y.�Shock induced phase transition of scandium sesquioxide: Geometric factor governing high pressure transitions on rare earth sesquioxides331-334SAtou, T., Kawai, N., Nakamura, K.G., Kondo, K., Ito, S., Yubuta, K. and Kikuchi, M.YTEM observations of disproportionation of mullite and sillimanite under shock compressionJAtroshenko, S.A., Zhigachieva, N.I., Meshcheryakov, Y.I. and Tomilin, M.G.BThe method of visualisation of dynamic deformation modes in metals611-613Attia, A.V.CNumerical simulation of shock response of fluid-filled porous rocks637-640&Attia, A.V., Moran, B. and Glenn, L.A.;Comparative yield estimation via shock hydrodynamic methods281-2847Atwood, A.I., Curran, P.O., Price, C.F. and Wiknich, J.>Quasi-static compaction studies of a porous pyrotechnic powder745-748(Auroux, E., Boustie, M. and Romain, J.P.mImprovement of the laser spallation technique using an amplifying layer: Experimental and numerical technique	1211-1214*High pressure strength of shocked aluminum145-149.Asay, J.R., Trucano, T.G. and Chhabildas, L.C.CTime-resolved measurements of shock-induced vapor-pressure profiles159-162Asay, J.R. and Trucano, T.G.KExperimental measurements of shock-induced vaporization in cadmium and lead143-1469Asay, B.W., Ramsay, J.B., Anderson, M.U. and Graham, R.A.3Shock compression of Dupont Detasheet at low stress679-6826Asay, B.W., Laabs, G.W., Peterson, P.D. and Funk, D.J.OMeasurement of strain and temperature fields during dynamic shear of explosivesDAsay, B.W., Henson, B.F., Dickson, P.M., Fugard, C.S. and Funk, D.J.`Direct measurement of strain field evolution during dynamic deformation of an energetic material567-570
Asay, J.R.7Isentropic compression experiments on the Z accelerator261-266�Asay, J.R., Hall, C.A., Holland, K.G., Bernard, M.A., Stygar, W.A., Spielman, R.B., Rosenthal, S.E., McDaniel, D.H. and Hayes, D.B.5Isentropic compression of iron with the Z accelerator	1151-1154'Shock wave paradigms and new challenges26-35@Asay, B., Dickson, P., Henson, B., Smilowitz, L. and Tellier, L.VEffect of temperature profile on reaction violence in heated and self-ignited PBX 9501	1065-1068WWave structure studies in condensed matter physics: Single crystals to magnetic effects5Asay, B.W., Son, S.F., Busse, J.R. and Oschwald, D.M.]Observations on the mechanism of reaction propagation in metastable intermolecular composites827-830AAsay, B.W., Tasker, D.G., King, J.C., Sanders, V.E. and Son, S.F.UElectrical conductivity measurements in reacting metastable intermolecular composites927-9306Ashuach, Y., Rosenberg, Z., Dekel, E. and Ginzburg, A.<More on the strength of materials under high shock pressures	1241-1244(Ashuach, Y., Rosenberg, Z. and Dekel, E.<Armstrong, R.W., Zerilli, F.J., Holt, W.H. and Mock�  Jr., W.]Dislocation mechanics based constitutive relations for plastic flow and strength of HY steels	1001-1004Armstrong, R.W. and Elban, W.L.2Dislocation characteristics in energetic materials723-726Armstrong, R.W. and Grise, W.R.-Hot spots from dislocation pile-up avalanches	1033-1036-Armstrong, R.W., Arnold, W. and Zerilli, F.J.-Dislocation mechanics under extreme pressures623-626	Arndt, J. Shock isotropization of minerals473-480Arnold, W. and Sachs, W.DMeasuring and simulation of steady shock wave profiles in Armco iron337-340$Arnold, W., Held, M. and Stilp, A.J.!Spallation behavior of Armco iron421-424
Arnold, W.BInfluence of twinning on the elasto-plastic behavior of armco iron539-542&High strain rate failure of Armco iron	1035-1038@Initiation threshold of an insensitive underwater high explosive911-914Controlled fragmentation527-5306Tungsten heavy alloys for multiple impact applications	1319-1322 Arrieta, H.V. and Espinosa, H.D.>High and low temperature dynamic testing of advanced materials	1075-1078XArrigoni, M., Boustie, M., He, H.L., Bolis, C., Berthe, L., Barradas, S. and Jeandin, M.RBenefits of the impedance mismatch technique for laser shock adhesion test (LASAT)	1369-1372>Asakawa, Y., Aizawa, T., Shono, Y., Fukuoka, K. and Kihara, J.KShock-induced reaction from mechanically alloyed precursor in 3Ni-Al system&Asano, T., Cosstick, K. and Furuta, H.]Experimental evidence for a two-step mechanism of diffusion-controlled unimolecular reactions	1325-1328+Asay, J.R., Chhabildas, L.C. and Wise, J.L.8Strain rate effects of beryllium under shock compression427-431<Asay, J.R., Chhabildas, L.C., Kerley, G.I. and Trucano, T.G.2Simulations of an underground explosion in granite	1279-1282Antoun, T<  .H. and Lomov, I.N.YSimulation of a spherical wave experiment in marble using a multidirectional damage model	1423-1426(Ao, T., Chiu, G., Forsman, A. and Ng, A.HOptical signatures of a shock wave emerging from a metallic free surface971-974Ao, T., Vollrath, I. and Ng, A.4Optical probing of the electron temperature gradient	1243-1246>Ao, T., Asay, J.R., Davis, J.-P., Knudson, M.D. and Hall, C.A.sHigh-pressure quasi-isentropic loading and unloading of interferometer windows on the Veloce pulsed power generator	1157-1160(Aoki, K., Yamawaki, H. and Sakashita, M.>Infrared study of phase transition in solid CO2 under pressure263-266�Aprelkov, O.N., Ignatova, O.N., Igonin, V.V., Lebedev, A.I., Nadezhin, S.S., Podurets, A.M., Raevsky, V.A., Solovyev, V.P., Salishchev, G.A., Zocher, M.A., Kaul, A.M., McNaney, J.M. and Remington, B.A.?Twinning and dynamic strength of copper during high-rate strain619-622pArad, B., Moshe, E., Eliezer, S., Dekel, E., Ludmirsky, A., Henis, Z., Goldberg, I.B., Eliaz, N. and Eliezer, D.cSpall strength measurements in aluminum, copper and metallic glass at strain rates of about 107 s-1459-462<Arad, B., Werdiger, M., Moshe, E., Henis, Z. and Eliezer, S.GVelocity interferometer data reduction beyond optical delay limitations	1139-1142Araki, M. and Leiber, C.O.[Linear relation between shock velocity and pressure in relation to the Gr"�neisen parameter547-550Arienti, M. and Shepherd, J.E.ISuperseismic loading and shock polars: An example of fluid-solid coupling251-254Arione, S.E. and Duvall, G.E.KTemperature dependence of the precursor amplitude in <111> lithium fluoride299-302Arione, S.E. and Bjorkman, M.D.;Scaling of hole diameter from perforating impacts of plates749-752kRe-examination of the requirements to detect the failure wave velocity in SiC using penetration experiments707-710BAnderson�  Jr., C.E., Nicholls, A.E., Chocron, S. and Ryckman, R.A.Taylor anvil impact	1367-1370ZAnderson�  Jr., C.E., Orphal, D.L., Behner, T., Hohler, V., Wickert, M. and Templeton, D.W.NFailure and penetration response of borosilicate glass during short-rod impact	1277-1280,Andreev, N.E., Fortov, V.E. and Kostin, V.V.1Shock wave generation by ultra-short laser pulses	1259-1260AAndrews, S., Glancy, B., Forbes, J., Collignon, S. and Hudson, L.SExperiments on the modification of the energy release rate in a non-ideal explosive799-802.Andrews, T.D., Radford, D.D. and Tsembelis, K.;The response of a heavy tungsten alloy during shock loading29-32*Andrews, T., Chapman, D.J. and Proud, W.G.)The response of concrete to shock-loading469-472&Andriot, P., Chapron, P. and Olive, F.KEjection of material from shocked surfaces of tin, tantalum and lead-alloys505-5093Andriot, P., Chapron, P., Lambert, V. and Olive, F.oInfluence of melting on shocked free surface behavior using Doppler laser interferometry and X-ray densitometry(Shock Waves in Condensed Matter  �� 1983277-281'Andriot, P., Lalle, P. and Dejean, J.P.QQuasi-elastic behavior of pure titanium and TA6V4 titanium alloy at high pressure	1009-1012	Ang, J.A."Hypervelocity impact jet formation	1019-1022Antoun, T. and Rajendran, A.M.6Constitutive modeling of concrete under impact loading497-500Antoun, T.H. and DeCarli, P.S.3Wave propagation in intact and jointed calcite rock831-8342Antoun, T., Seaman, L., Curran, D. and Glinsky, M.QDamage and failure mechanisms associated with photoablation of biological tissues9Antoun, T.N., Vorobiev, O.Y., Lomov, I.N. and Glenn, L.A._Effects of initial temperature on the shock and release behavior of filled and unfilled epoxies669-672@Shock compression and release properties of alumina-filled epoxy685-688>Anderson, M.U., Cox, D.E., Montgomery, S.T. and Setchell, R.E.]Compositional effects on the shock compression and release properties of alumina-filled epoxy789-792/Anderson, S.P., Palamidi, E. and Harrigan, J.J.;Intermediate and high strain rate testing of soft materials	1237-1240Anderson, W.W.#Jump conditions for nonsteady waves	1303-1306zInitial temperature effects on the shock compression and release properties of different alumina-filled epoxy compositions683-6866Anderson�  Jr., C.E., O'Donoghue, P.E. and Bodner, S.R.+Tensile failure in tungsten alloy fragments371-3745Anderson�  Jr., C.E., O'Donoghue, P.E. and Skerhut, D.4Anisotropic model development for shock applications.Shock Compression of Condensed Matter  �� 1989177-180$Anderson�  Jr., C.E. and Walker, J.D.=Long rod penetration and the calculation of target resistance967-970WAnderson�  Jr., C.E., Littlefield, D.L., Blaylock, N.W., Bless, S.J. and Subramanian, R.4The penetration performance of short L/D projectiles	1809-1812$Anderson�  Jr., C.E. and Walker, J.W.@An analytic expression for P/L for WA long rods into armor steel	1135-1138RAnderson�  Jr., C.E., Bless, S.J., Sharron, T.R., Satapathy, S. and Normandia, M.J.2Investigation of yawed impact into a finite target925-928=Anderson�  Jr., C.E., Popelar, C.H., Nagy, A. and Walker, J.D.9A novel method for determining dynamic fracture toughness505-508'Anderson�  Jr., C.E. and Dannemann, K.A.CDeformation and damage of two aluminum alloys from ballistic impact	1298-13015Anderson�  Jr., C.E., Orphal, D.L. and Templeton, D.W.`Aminov, Y.A., Gorshkov, M.M., Zaikin, V.Y., Kovalenko, G.V., Nikitenko, Y.R. and Rykovanov, G.N.LInvestigation of isentrope for detonation products of TATB-based composition875-877-Aminov, Y.A., Eskov, N.S. and Nikitenko, Y.R.6Modeling of double shock initiation of LX-17 explosive913-916@Anbukumaran, K., Venkateswaran, C., Jaya, N.V. and Natarajan, S.HPiston-cylinder apparatus for high pressure and high temperature studies	1585-1588cAnderson, C.E., Wilbeck, J.S., Hokanson, J.C., Asay, J.R., Grady, D.E., Graham, R.A. and Kipp, M.E.!Sandia shock compression database185-1902Anderson, M.U., Graham, R.A. and Wackerbarth, D.E._Prediction and data analysis of current pulses from impact loaded piezoelectric polymers (PVDF)805-808Anderson, 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 GPa875-878Anderson, O.L./Imperfections of the 1993 phase diagram of iron907-910-Anderson, M.U., Graham, R.A. and Holman, G.T.RTime-resolved shock compression of porous rutile: Wave dispersion in porous solids	1111-1114Anderson, M.U. and Graham, R.A.XThe new simultaneous PVDF/VISAR measurement technique: Applications to highly porous HMXAnderson, W.W. and Ahrens, T.J.6Shock wave equations of state of chondritic meteorites115-1183Anderson, M.U., Chhabildas, L.C. and Reinhart, W.D.bSimultaneous PVDF/VISAR measurement technique for isentropic loading with graded density impactors841-844dAnderson, W.W., Cverna, F., Hixson, R.S., Vorthman, J., Wilke, M.D., Gray�  III, G.T. and Brown, K.L.,Phase transition and spall behavior in b-tin,Anderson, M.U., Setchell, R.E. and Cox, D.E.9Shock and release behavior of filled and unfilled epoxies551-554BHeat conduction and wav<  e propagation in thermo-microelastic solids287-290Alcon, R.R. and Mulford, R.N.0Shock tracker configuration of in-material gauge	1057-1060@Alcon, R.R., Sheffield, S.A., Martinez, A.R. and Gustavsen, R.L.CMagnetic gauge instrumentation on the LANL gas-driven two-stage gun845-848HAlcon, R.R., Robbins, D.L., Sheffield, S.A., Stahl, D.B. and Fritz, J.N.LShock compression of silicon polymer foams with a range of initial densities!Alexander, D.J. and Robbins, D.L.ALaser-driven planar impact of miniature specimens of HY-100 steel630-633[Alexander, C.S., Vogler, T.J., Reinhart, W.D., Grady, D.E., Kipp, M.E. and Chhabildas, L.C.UInfluence of shock wave measurement technique on the determination of Hugoniot states	1229-12325Alexander, C.S., Chhabildas, L.C. and Templeton, D.W.-The Hugoniot elastic limit of soda-lime glass733-738KAllan, N.L., Braithwaite, M., Cooper, D.L., Mackrodt, W.C. and Wright, S.C.NThe calculated behaviour of pericalse (MgO) at high temperatures and pressures53-56NAllen, R.M., Kirkpatrick, D.J., Longbottom, A.W., Milne, A.M. and Bourne, N.K.?Experimental and numerical study of free-field blast mitigation823-8264Alme, M.L., Christiansen, E.L. and Cour-Palais, B.G.DHydrocode simulations of the multi-shock meteoroid and debris shield975-978>Altman, B.S., Nemat-Nasser, S., Vecchio, K.S. and Isaacs, J.B.JHomogeneous deformation of a particulate reinforced metal matrix composite.Shock Compression of Condensed Matter  �� 1991543-546Altshuler, L.V.(Shock waves and extreme states of matter4Viscosity of water and glycerin behind a shock front509-512
Ames, R.G.ILimitations of the Hopkinson pressure bar for high-frequency measurements	1233-1236XApplication of detonation shock dynamics to Youngs-type discontinuous interface geometry809-812Aidun, J.B. and Gupta, Y.M.;Analysis of Lagrangian particle velocity gauge measurementsAidun, J.B.>Shear wave measurements in shock-induced, high-pressure phases)High Pressure Science and Technology 19932S.C. Schmidt, J.W. Shaner, G.A. Samara and M. Ross387-390]Discussion of stress tensor nonuniqueness with application to nonuniform, particulate systems985-988OAizawa, T., Kashiwabara, Y., Asakawa, Y., Fukuoka, K., Shono, Y. and Kihara, J.RShock induced reactions of titanium aluminides from mechanically alloyed precursor705-708#Aizawa, T., Yen, B.K. and Syono, Y.IShock-induced reaction mechanism to synthesize refractory metal silicides651-654'Aizawa, T., Ichige, K.-I. and Syono, Y.ZShock induced reaction to refractory metal disilicides from mechanically alloyed precursor,Shock Compression of Condensed Matter - 1999-M.D. Furnish, L.C. Chhabildas and R.S. Hixson759-762Melville, New York+Akahama, Y., Kobayashi, M. and Kawamura, H.;Pressure-induced structural sequence in sulfur up to 90 GPa425-4288Akashi, T., Lotrich, V., Sawaoka, A. and Beauchamp, E.K. Dynamic compaction of SiC powder779-784(Akashi, T., Sawaoka, A. and Graham, R.A.>The effect of shock compression on graphite-like boron nitride821-825Akedo, J. and Lebedev, M.aSynthesis of functional ceramic layers using novel method based on impact of ultra-fine particles	1101-1104&Akella, J., Smith, G.S. and Weir, S.T.^Static ultra-high pressure study of lanathanide and actinide metals using a diamond-anvil cell187-190;Akhavan, J., Millett, J.C.F., Bourne, N.K. and Longjohn, R.KMorphological studies of an inert polymer binder subjected to shock loading435-438Al�  Assaad, A.fShock 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 and R.A. Graham631-633JAhrens, T.J., Kostka, D., Vreeland�  Jr., T., Schwarz, R.B. and Kasiraj, P.%Shock compaction of molybdenum powder$Shock Waves in Condensed Matter 1983&J.R. Asay, R.A. Graham and G.K. Straub443-446
North-HollandAhrens, T.J.=Application of shock wave data to Earth and planetary science571-588Ahrens, T.J. and Potter, D.K.wDynamic consolidation of initial diamond single crystal powders and diamond-graphite into fused polycrystalline diamond419-422*Ahrens, T.J., Bass, J.D. and Abelson, J.R.Shock temperatures in metals851-857Ahrens, T.J. and Rubin, A.M.COne- and three-dimensional impact induced tensional failure in rock579-582GApplication of shock compression science to Earth and Planetary physics*Ahrens, T.J., Holland, K.G. and Chen, G.Q.0Shock temperatures and the melting point of iron,Shock Compression of Condensed Matter - 1997+S.C. Schmidt, D.P. Dandekar and J.W. Forbes133-136#Ahrens, T.J., Xia, K. and Coker, D.LDepth of cracking beneath impact craters: New constraint for impact velocity,Shock Compression of Condensed Matter - 2001(M.D. Furnish, N.N. Thadhani and Y. Horie	1393-1396#Ahrens, T.J., Shen, A.H. and Ni, S.)Giant impact induced atmospheric blow-off,Shock Compression of Condensed Matter - 2003(M.D. Furnish, Y.M. Gupta and J.W. Forbes	1419-1422Melville NYAi, H.A. and Ahrens, T.J.LNumerical modeling of shock-induced damage for granite under dynamic loading,Shock Compression of Condensed Matter - 20053M.D. Furnish, M. Elert, T.P. Russell and C.T. White	1431-1434&Aida, T., Walter, J.W. and Bdzil, J.B.@Momentum transfer in the one-dimensional impact of spaced plates,Shock Compression of Condensed Matter - 19914S.C. Schmidt, R.D. Dick, J.W. Forbes and D.G. Tasker983-986	AmsterdamElsevierAbdulazeem, M.S.RCoupling between shock and reaction zone in one-dimensional dense fluid detonation*Shock Compression of Condensed Matter 1995S.C. Schmidt and W.C. Tao373-376Woodbury, New YorkAmerican Institute of Physics:Abe, A., Katayama, M., Murata, K., Kato, Y. and Tanaka, K.CNumerical study of underwater explosion and following bubble pulses,Shock Compression of Condensed Matter - 20078M. Elert, M.D. Furnish, R. Chau, N. Holmes and J. Nguyen	1355-1358Melville, NY2Abramian, A.K., Andreev, V.L. and Indeitchev, D.A.IThe size of dents in circular shells resulting from submerged shock waves285-288=Addiss, J., Cai, J., Walley, S., Proud, W. and Nesterenko, V.IHigh strain and strain-rate behaviour of PTFE/aluminium/tungsten mixtures773-776,Agnew, S.F., Swanson, B.I. and Eckhart, D.G.:Spectroscopic studies of carbon disulfide at high pressure(Shock Waves in Condensed Matter  �� 1985
Y.M. Gupta221-229New YorkPlenumAgnew, S.F. and Swanson, B.I.tModel for the density dependence of electronic absorption bands: Application to carbon disulfide and other molecules&Shock Waves in Condensed Matter - 1987S.C. Schmidt and N.C. Holmes485-488FAgnew, S.F., Pinnick, D.A., Pettit, D.R., Dick, J.J. and Swanson, B.I.JComparative static and dynamic measurements in dinitrogen tetroxide (N2O4),Shock Compression of Condensed Matter - 1989+S.C. Schmidt, J.N. Johnson and L.W. Davison867-870�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. and Stolper, E.M.lModeling anisotropic plasticity: 3D Eulerian hydrocode simulations of high strain rate deformation processes279-282gCoupled plasticity and damage modeling and their applications in a three-dimensional Eulerian hydrocode529-532]Burley, S.J., Bourne, N.K., Fung, V., Hollands, R., Millett, J.C.F., Milne, A.M. and Wood, A.9Advances in the understanding of the large-scale gap test944-947)Burns, T.J., Grady, D.E. and Costin, L.S.>Brown, W.T., Schmidt, M.F., Dzwilewski, P.T. and Samaras, T.M.IElectromagnetic radiation from the detonation of metal encased explosives	1037-1040HBrown, E.N., Gray�  III, G.T., Rae, P.J., Trujillo, C.P. and Bourne, N.K.iEffect of pul< se duration on polytetrafluoroethylene shocked above the crystalline phase II-III transition147-150/Brown, E.N., Trujillo, C.P. and Gray�  III, G.T.uInfluence of polyethylene molecular conformation on Taylor impact measurements: A comparison of HDPE, UHMWPE, and PEX691-694\Brown, J.l., Vogler, T.J., Grady, D.E., Reinhart, W.D., Chhabildas, L.C. and Thornhill, T.F.Dynamic compaction of sandBrowning, R.V.EMicrostructural model of mechanical initiation of energetic materials405-408 Browning, J.S. and Montoya, J.L.-Hypervelocity impact tests of optical sensors,Shock Compression of Condensed Matter - 1995	1113-1116 Browning, R.V. and Scammon, R.J.fMechanical strength model for plastic bonded granular materials at high strain rates and large strains277-280EMicrostructural model of ignition for time-varying loading conditions987-990>Browning, R.V., Peterson, P.D., Roemer, E.L. and Scammon, R.J.7Grit particle enhanced non-shock ignition of explosives921-924\Browning, R.V., Peterson, P.D., Roemer, E.L., Oldenborg, M.R., Thompson, D.G. and Deluca, R.EExperimental study of grit particle enhancement in non-shock ignition	1041-1044BBrusso, J.A., Mikkola, D.E., Bloom, G., Lee, R.S. and Vonholle, W.aUse of electric gun experiments to study the shock deformation behavior of 21-6-9 stainless steel375-378IBucholtz, S.M., Gehr, R.J., Rupp, T.D., Sheffield, S.A. and Robbins, D.L.1Temperature controller system for gas gun targets	1245-1248;Bucholtz, S.M., Gehr, R.J., Alcon, R.R. and Gustavsen, R.L.7Improved temperature control system for gas gun targets	1085-1088�Brichikov, S.A., Dremov, V.V., Kovalenko, G.V., Kozlov, E.A., Petrovtsev, A.V., Varfolomeev, D.A., Bragov, A.M., Lomunov, A.K., Dobromyslov, A.V., Taluts, N.I., Juanicotena, A., Gatulle, M. and Voltz, C.^Phase transitions, high-rate straining, and fracture of iron under spherical explosive loadingBriggs, M. and Ferm, E.N.pAxial VISAR velocity measurements of the non-planar acceleration of a plate from a penetrating shaped charge jet	1371-1374<Briggs, R.E., Drodge, D.R., Williamson, D.M. and Proud, W.G.2Two-step loading in a split Hopkinson pressure bar	1173-11761Britan, A., Elperin, T., Igra, O. and Jiang, J.P.>Head-on collision of a planar shock wave with a granular layerBrown, W.T.cNumerical modeling of oblique impact hypervelocity impact using two-dimensional plane strain models529-533Brown, J.M. and Shaner, J.W.NRarefaction velocities in shocked tantalum and the high pressure melting point91-94+Brown, J.M., Furnish, M.D. and Boness, D.A.'Sound velocities for San Carlos olivine119-122=Brown, J.A., Gaffney, E.S., Blaisdell, G.L. and Johnson, J.B.@Techniques for gas gun studies of shock wave attenuation in snow657-660?A computational study of shock propagation in Indiana limestone629-6325Brown, J.M., Slutsky, L.J., Abramson, E. and Zaug, J.dSound velocities, elastic constants, thermal diffusivity, and structural relaxation at high pressure35-38Brown, C.A. and Russell, T.P.;Time resolved emission studies of aluminum/water combustion909-912%Brown, J., Curtis, J.P. and Lee, P.R.^Ab initio determination of the V of D of an octol from the statistics of its crystal structure333-336:On the strength behaviour of Kel-F-800 and estane polymers653-656 Bourne, N.K. and Gray�  III, G.T.+On the failure of boron carbide under shock775-778Bourne, N.K. and Vecchio, K.S.'Dynamic loading of a designer composite689-692Bourne, N.K. and Cooper, G.A.,New insights into shock propagation in glass/Bourne, N.K., Rosenberg, Z. and Millett, J.C.F.3Propagation of waves through a float glass laminateBourne, N.K./Mesoscale modelling of the response of aluminasLBourne, N.K., Millett, J.C.F., Chen, M.W., Dandekar, D.P. and McCauley, J.W.2Failure above and below the elastic limit in AD995(Boustie, M., Cottet, F. and Romain, J.P._Spalling due to a strong shock wave decay process in solid targets irradiated by a pulsed laserJBoustie, M., Seymarc, C., Auroux, E., de�  Ress"�guier, T. and Romain, J.P.`Coating debonding induced by confined laser shock interpreted in terms of shock wave propagationyBoustie, M., Cuq-Lelandais, J.-P., Berthe, L., Bolis, C., Barradas, S., Arrigoni, M., de�  Ress"�guier, T. and Jeandin, M.XOptical measurements of shock-induced chemical reactions in mixed aluminum-nickel powder767-772<Boslough, M.B., Cygan, R.T., Venturini, E.L. and Morosin, B.HShock-chemistry in natural materials and evolution of planetary surfaces381-386Boslough, M.B.gThermochemical model for shock induced chemical reactions in porous thermite: The heat detonation modelNPostshock spectral radiance measurements in nickel and nickel/aluminum powders617-620{Boslough, M.B., Chhabildas, L.C., Reinhart, W.D., Hall, C.A., Miller, J.M., Hickman, R., Mullin, S.A. and Littlefield, D.L.KPVDF gauge characterization of hypervelocity-impact-generated debris clouds	1833-1836!Boslough, M.B. and Crawford, D.A.WImpact-generated atmospheric plumes: Observations of Jupiter and implications for Earth	1187-11900Botcher, T.R., Ladouceur, H.D. and Russell, T.P.5Pressure dependent laser induced decomposition of RDX989-992 Boteler, J.M. and Lindfors, A.J.5Shock loading studies of AP/Al/HTPB based propellants767-770
Boteler, J.M.5Compression-shear study of glass reinforced polyester537-540,Boteler, J.M., Rajandran, A.M. and Grove, D.0Shock wave profiles in polymer matrix composites563-566 Boteler, J.M. and Dandekar, D.P.,Dynamic response of 5083-H131 aluminum alloy481-484Bouchu, M. and Guillamot, J.-Y.;Application of PVF2 active gage as an initiation diagnostic553-558!Bourasseau, E. and Maillet, J.-B.OParameter optimization for charge equilibration method in molecular simulations565-568#Bourcier, R.J. and Chhabildas, L.C.)High velocity erosion of metal interfaces741-7449Bourne, N.K., Rosenberg, Z., Crouch, I.G. and Field, J.E.PMicrostructural variations in seven aluminas and their effect on impact response769-772Bourne, N.K. and Rosenberg, Z.�Disagreement between shock and static temperature data: Calculation of argon optical transmittance in laser-heated diamond anvil cells173-176*Bonora, N., Ruggiero, A. and Milella, P.P.&Fracture energy effect on spall signal439-442GBonora, N., Ruggiero, A., Flater, P.J., House, J.W. and DeAngelis, R.J.\On the role of material post-necking stress-strain curve in the simulaiton of dynamic impact701-704)Bonora, N., Esposito, L. and Ruggiero, A.XEmbedded cohesive elements (ECE) approach to the simulation of spall fracture experiment477-480CBoogerd, P., Verbeek, H.J., Stuivinga, M. and van�  der�  Steen, A.C.4Shock wave equation of state for metals and ceramics89-92'Bordzilovsky, S.A. and Karakhanov, S.M.?Electrical resistivity of PTFE layers under dynamic compression801-804:Bordzilovsky, S.A., Karakhanov, S.M. and Merzhievsky, L.A.MShock response of a unidirectional composite at various orientation of fibers545-548
Borg, J.P.YEstimating the break-up diameter of an impulsively driven initially smooth fluid cylinder715-718YBorg, J.P., Schwalbe, L., Cogar, J., Chapman, D.J., Tsembelis, K., Ward, A. and Lloyd, A.3Dynamic compaction modeling of porous silica powder37-40Borg, J.P. and Vogler, T.J.8Mesoscale calculations of shock loaded granular ceramics227-230LBorodina, T.I., Fortov, V.E., Milyavskiy, V.V., Zharkov, A.S. and Zhuk, A.Z.:Shock wave synthesis of carbyne from graphite: New results	1082-10853Borschevsky, A.O., Gorshkov, M.M. and Tarasov, A.M.AThe twofold quartzite shock adiabat under pressures of 55-150 GPa95-98Boslough, M.B. and Ahrens, T.J.<  OA method of determining points on the principal isentropes of molecular liquids236-2407Particle velocity experiments in anorthosite and gabbro+Boslough, M.B., Graham, R.A. and Webb, D.M.ABoettger, J.C., Honnell, K.G., Mori, Y., Niiya, N. and Mizuno, T.1Theoretical equation of state for beryllium oxide33-36Bogach, A.A.CAnalysis of temperature influence on the dynamic fracture of metalsRBokarev, V.P., Temnitsky, I.N., Bondarev, Y.M., Mardashev, Y.S. and Batsanov, S.S.UEffect of explosion on the catalytic properties of stochiometric inorganic substances827-829zBoley, M.S., Thomas, R.J., Chandrasekhar, M., Chandrasekhar, H.R., Ram-Mohan, L.R., Samarth, N., Luo, H. and 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 wells203-206MBoley, M.S., Chandrasekhar, M., Chandrasekhar, H.R., Wu, Y. and Boolchand, P.sHydrostatic pressure studies of the Raman-active phonon modes in the bulk high-temperature superconductor YBa2Cu4O8681-684XBolis, C., Berthe, L., Boustie, M., Arrigoni, M., He, H.L., Jeandin, M. and Barradas, S.tVISAR pull-back signals as a diagnostic for the laser adherence test applied to copper coating on aluminum substrate	1373-1376Bolme, C.A.ISingle shot dynamic ellipsometry measurements of laser-driven shock waves	1211-1216*Boness, D.A., Brown, J.M. and Shaner, J.W.#Rarefaction studies in shocked leadBoness, D.A. and Brown, J.M.KTime-resolved optical spectroscopy of shock-compressed fluid alkali halides863-866Boness, D. and Brown, J.M._Melting along the Hugoniots of KBr and CaBr: Optical pyrometry-rarefaction overtake experiments'Heat capacity of shocked alkali halides85-88Boness, D.A.eMetastability in shocked iron: Controversy with regard to sound velocity and temperature measurements77-805Boness, D.A., Brown, J.M., Morgan, M. and Madamba, J.KCharacterization of shock-loaded aluminum-infiltrated boron carbide cermets393-396PBlumenthal, W.R., Abeln, S.P., Cannon, D.D., Gray�  III, G.T. and Carpenter, R.W.PInfluence of strain rate and temperature on the mechanical behavior of beryllium411-414eBlumenthal, W.R., Gray�  III, G.T., Idar, D.J., Holmes, M.D., Scott, P.D., Cady, C.M. and Cannon, D.D.]Influence of temperature and strain rate on the mechanical behavior of PBX 9502 and Kel-F 800671-674IBlumenthal, W.R., Cady, C.M., Lopez, M.F., Gray�  III, G.T. and Idar, D.J.hInfluence of temperature and strain rate on the compressive behavior of PMMA amnd polycarbonate polymers-Blumenthal, W.R., Brown, D.W. and Tom"�, C.N.?Evolution of crystallographic texture and strength in beryllium525-528,Bock, W.J., Urbanczyk, W. and Wisniewski, R.VFiber-optic pressure sensor using an electronically scanned white-light interferometer	1687-1690�Bockowski, M., Grzegory, I., Wr"e"blewski, M., Witek, A., Jun, J., Krukowski, S., Porowski, S., Ayral-Marin, R.M. and Tedenac, J.C.KCombustion synthesis of AlN at high pressure of nitrogen and argon mixtures	1255-1258PBocquillon, C., Bogicevic, C., Clerc, F., L"�ger, J.M., Fabre, C. and Rassat, A.MSynthesis of diamond at high pressure and high temperature from C60 fullerene647-650 Bodner, S.R. and Rajendran, A.M.DOn the strain rate and temperature dependence of hardening of copper499-502Boehler, R.<The phase diagram of iron to 2 Mbar: New static measurements)High-precision grinding of diamond anvils	1619-1620iBoehly, T.R., Miller, J.E., Meyerhofer, D.D., Eggert, J.H., Celliers, P.M., Hicks, D.G. and Collins, G.W.^Measurements of the release of alpha quartz: A new standard for impedance-matching experiments19-22 Boettger, J.C. and Wallace, D.C.6A model for the shock-induced phase transition in iron129-132195-198Bless, S.J.*Hypervelocity impact response of Ti and Be548-552HImpact physics facilities at the University of Dayton Research Institute668-673Bless, S.J. and Paisley, D.L.'Dynamic tensile fracture of OFHC copper(Bless, S.J., Yaziv, D. and Rosenberg, Z.'Spall zones in polycrystalline ceramicsShock Waves in Condensed Matter419-424)Bless, S.J., Brar, N.S. and Rosenberg, Z.3Strength of soda lime glass under shock compression$Shock Waves in Condensed Matter 1987309-312;Failure of ceramic and glass rods under dynamic compressionBless, S.J. and Brar, N.S.HLoad/unload hysteresis in ceramics measured by a reverberation technique483-486%Impact induced fracture of glass bars	1813-1816*Penetration mechanics of non-circular rods	1119-1122Bless, S.J. and Satapathy, S./Penetration of thick targets by yawed long rods933-936Bless, S.J. and Cazamias, J.XUsing the penetration-velocity relationship to correct for variations in target hardness	1291-1293Bless, S.J. and Bourne, N.K.OThe effect of shock rise time on strength of alumina in 1D stress and 1D strain711-714Bless, S. and Chau, R."Tensile failure of tungsten alloysBloom, G.H.5Gr"�neisen parameter measurements for high explosives588-592JBloom, G., Chau, H., Glaser, R., Honodel, C., Lee, R.S. and Weingart, R.C.BImprovements in thin-pulse shock initiation threshold measurementsLBloom, G., Duncan, A., Honodel, C., Lee, R., von�  Holle, W. and Weingart, R.fChanges in the particle size distribution of LX-17 samples induced by 3.5 ti 11 GPa planar shock waves569-571$Bloomquist, D.D. and Sheffield, S.A.VShock-compression temperature rise determined from resistivity of embedded metal foils304-308$Blumenthal, W.R. and Gray�  III, G.T.	1323-1326qBesson, J.M., Pruzan, P., Klotz, S., Hamel, G., Silvi, B., Nelmes, R.J., Loveday, J.S., Wilson, R.M. and Hull, S.cInteratomic distance in D2O VIII under high pressure from neutron scattering measurements to 10 GPa0Bezruchko, G.S., Kanel, G.I. and Razorenov, S.V.CMeasurements of sound speed in zinc in the negative pressure region>Bezruchko, G.S., Razorenov, S.V., Kanel, G.I. and Fortov, V.E.?Influence of temperature upon the a to w transition in titanium192-195)Bhate, N., Clifton, R.J. and Phillips, R.eAtomistic simulations of the motion of an edge dislocation in aluminum using the embedded atom method339-3429Bickham, S.R., Lenosky, T., Collins, L.A. and Kress, J.D.(Simulations of shock-compressed hydrogen45-48Biele, J.K.3Sounding experiments of high pressure gas discharge891-894IReflectometric detection of shock wave propagation within a concrete wallBillingsley, J.P.KEnergetic materials shock sensitivity relevance to specific heat properties429-432&The Hugoniot elastic limit decay limit199-202`HMX and HNS shock sensitivity correlation with specific heat and reactive temperature magnitudes899-902The HEL upper limit735-738iFOX-7 specific heat prediction from a proposed nominal/generic specific heat for CHNO energetic compounds]PBX-9502 shock sensitivity correlation with specific heat and reactive temperature magnitudes895-898"Binggeli, N. and Chelikowsky, J.R.1is simulated 'amorphous' silica really amorphous?397-400Birnboim, A. and Rosenberg, Z.6The response of shocked quartz gauge to impact loading Bjorkman, M.D. and Shrader, J.E.VShock wave propagation in beryllium at small impact stresses and elevated temperatures432-436"Bjorkman, M.D. and Holsapple, K.A.NPlane hypervelocity impact and source similitude dependence on a T<  illotson EOS%Benson, D.J., Do, I. and 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. and Guyot, F.FExperimental study of highly compressed iron using laser driven shocks83-86(Berghout, H.L., Son, S.F. and Asay, B.W.8Measurement of convective burn rates in gaps of PBX 9501Bergmann, O.R.`Industrial uses of explosive pressure: From rock blasting to metal bonding and synthetic diamond429-433Bergstresser, T. and Becker, S.BTemperature measurement of isentropically accelerated flyer platesEBernecker, R.R., Clairmont�  Jr., A.R., Sandusky, H.W. and Smith, M.S.IParticipation of aluminum in two-dimensional shock initiation experiments573-576Bernecker, R.R.-Shock initiation of some aqueous HMX mixtures695-698,Hugoniots of some elastomeric binder systems137-140$Observations on the Hugoniot for HMX141-144!Bernecker, R.R. and Simpson, R.L.CFurther observations on HMX particle size and buildup to detonation719-722Bernhard, R.P. and H""rz, F.XFragmentation history of glass projectiles impacting aluminum targets at 0.5 to 1.5 km/s	1147-1150#Bernhard, R.P. and Christiansen, E.bAnalysis of microstructures and projectile residues in hypervelocity impacts on fused silica glass Berry, R.A. and Williamson, R.L.IA multiphase mixture for the shock induced consolidation of metal powders335-340$Bessette, G.C. and Littlefield, D.L.HAnalysis of transverse loading in long-rod penetrators by oblique plates937-940`Bessette, G.C., Lawrence, R.J., Chhabildas, L.C., Reinhart, W.D., Thornhill, T.F. and Saul, W.V.IMulti-dimensional hydrocode analyses of penetrating hypervelocity impactslShock metamorphism of hornblende and plagioclase in conditions of step-like compression of polymineral rocks	1359-1362 Bell, P.M., Xu, J. and Mao, H.K.zStatic 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. and Prut, E.V.JNew method of processing compositions based on high molecular polyethylene	1029-1030Benedict, U.=Updated diagrams of high-pressure phase relations in f-metals241-244)Benham, R.A., Weirick, L.J. and Lee, L.M.8Calibration of thin-foil manganin gauge in ALOX material	1061-1064;Benjamin, R.F., McQueen, R.G., Marsh, S.P. and Shaner, J.W.>Results on Richtmyer-Meshkov instabilities in condensed fluids259-260 Bennett, B.I. and Liberman, D.A.0Quantum mechanical effects on the shock Hugoniot49-526Bennett, L.S., Iyer, K.R., Sorrell, F.Y. and Horie, Y.5Shock induced exothermic reactions in powder mixtures605-608#Beno, T., Bless, S. and Nichols, S.9New phenomena observed in plate impacts onto alumina bars839-842Benson, D.A. and Baer, M.R.,Grain burning experiments with HMX explosiveBenson, D.J. and Nellis, W.J.=Numerical simulation of the shock compaction of copper powderBenson, A.K.wInversion of compressional elastic wave data as a fnction of off set to recover bulk modulus, shear modulus and density1Benson, D.J., Nesterenko, V.F. and Jonsdottir, F.9Micromechanics of shock deformation of granular materials603-606�Characterizing subsurface lithology with elastic parameter contrasts from the decomposition and inversion of the elastic wave equation	1283-1286Benson, A.K. and Wu, J.�Predicting elastic properties of porous fluid-filled rocks by inverting the BGG equation: Applications to seismic and borehole data	1291-1294%Bauer, F., Moulard, H. and Samara, G.@Advances in ferroelectric polymers for shock compression sensorsSAdvances in PVDF shock sensors: Applications to polar materials and high explosives	1023-1028NPVDF gauge piezoelectric response under two-stage light gas gun impact loading	1149-11524PVDF shock compression sensors in shock wave physics	1121-1124"Piezoelectric polymer shock gauges	1183-11868Baumung, K., Singer, J., Razorenov, S.V. and Utkin, A.V.bHydrodynamic proton beam-target interaction experiments using an improved line-imaging velocimeter	1015-10184Baumung, K., Kanel, G.I., M"�ller, G. and Singer, J._Measurement of the adhesive strength of 200 mm thick turbine blade coatings by a dynamic method	1207-1210Be'ery, I. and Rosenberg, Z.<New high pressure encapsulation material for manganin gauges	1081-1084EBeard, B.C., Sharma, J., Sandusky, H.W., Glancy, B.C. and Elban, W.L.LDislocation density variation in shocked single crystal ammonium perchlorate571-574(Bedrov, D., Smith, G.D. and Sewell, T.D.^Molecular dynamics simulations of HMX crystal polymorphs using a flexible molecule force field403-406.Beissel, S.R., Gerlach, C.A. and Johnson, G.R.[Three-dimensional impact simulations by conversion of finite elements to meshfree particles193-196	Belak, J.:Computer simulation of molecular response at a shock front	1063-1066VMolecular dynamics simulation of high strain rate void nucleation and growth in copper211-214Belgaumkar, B.M.IShock induced instability due to crack-like defects in a solid propellant598-602American Institute of Physcs2Belgelzimer, Y.E., Efros, B.M. and Shishkova, N.V.'Metal fracture at hydrostatic extrusion	1051-1054hBeljatinskaja, I.V., Milyavskiy, V.V., Sazonova, L.V., Borodina, T.I., Zhernokletov, D.M. and Zhuk, A.Z.2Shear stresses in polymers under shock compression577-580KBatkov, Y.V., Knyazev, V.N., Novikov, S.A., Raveski, V.A. and Fishman, N.D.3Shear strength of aluminum at shockless compression501-504Batsanov, S.S.#Perspectives on inorganic chemistry&Shock Waves in Condensed Matter - 19810Inorganic synthesis under shock-wave compression14-267Baudin, G., Le�  Gallic, C., Davoine, F. and Bouinot, P.bExperimental method to determine the detonation characteristics of a very non-ideal high explosive940-943	Bauer, F.HBehavior of ferroelectric ceramics and PVF2 polymers under shock loading251-267ISL shock wave facilities674-679pPiezoelectric and electric properties of PVF2 polymers under shock wave action: Application to shock transducers&Shock Waves in Condensed Matter - 1983225-228_Ferroelectric properties and shock response of a poled PVF2 polymer and of VF2/C2F3H copolymers483-496Bauer, F. and Moulard, H.PState-of-the-art in the research work of piezoelectric PVDF polymer shock gauges627-630Bauer, F. and Lichtenberger, A.AUse of PVDF shock gauges for stress measurements in Hopkinson bar631-634Bauer, F. and Graham, R.A.ABehaviour of VF2/VF3 piezoelectric copolymers under shock loading793-796OBauer, F., Graham, R.A., Anderson, M.U., Lefebvre, H., Lee, L.M. and Reed, R.P.SResponse of the piezoelectric polymer PVDF to shock compression greater than 10 GPa887-8904High pressure applications of ferroelectric polymers	1727-1730'Bauer, F., Moulard, H. and Graham, R.A.iPiezoelectric response of ferroelectric polymers under shock loading: Nanosecond piezoelectric PVDF gauge	1073-1076ZBauer, F., Isner-Brown, P., Moulard, H., Couturier, S., De�  Resseguier, T. and Boustie, M.XPiezoelectric P(VDF-TrFE) thick copolymers: Response in current mode under shock loading$The shock Hugoniot of an epoxy resin135-138?Barrett, J.J.C., Brenner, D.W., Robertson, D.H. and White, C.T.0Detonation of solid O3: Effects of void collapse191-194QBarrett, W.H., Greenwoll, J.I., Smith, C.W.,<   Johnson, D.E. and 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=Barrett, J.J.C., Robertson, D.H., Elert, M.L. and White, C.T.ADetonation Hugoniot for ozone from molecular dynamics simulations329-331!Bartkowski, T. and Dandekar, D.P.;Spall strengths of sintered and hot pressed silicon carbide535-538#Bartkowski, P.T. and Dandekar, D.P.5Recompression of PMMA following shock induced tension0Bartkowski, P.T., Dandekar, D.P. and Grove, D.J./Spallation of hot pressed boron carbide ceramic779-782=Barzhkin, V.V., Lyapin, A.G., Popova, S.B. and Voloshin, R.N.KAmorphization of high pressure phases: Application to silicon and germanium249-250Bashkirov, A.G. and Orlov, A.V.AShock wave structure for some non-analytical-in-velocity closures
Bass, R.C.IMeasurements and calculations of shock propagation in dry desert alluvium633-637:Bassett, W.A., Weathers, M.S., Wu, T.-C. and Holmquist, T.'Equation of state of SiC up to 68.4 GPa145-148 Bassett, W.A. and Weathers, M.S.TFullerence structures produced from melted diamond at high pressure by laser heatingHThermodynamic significance of a high-pressure/temperature bcc iron phase915-918Bastea, M. and Reisman, D.B.1Ramp compression experiments: A sensitivity study	1169-1172ZBatalov, S.V., Averin, A.N., Batalova, I.A., Loboiko, B.G., Litvinov, B.V. and Filin, V.P.5On the mechanism of diamond formation from explosives753-755-Batkov, Y.V., Novikov, S.A. and Fishman, N.D.VBardenhagen, S.G., Harstad, E.N., Maudlin, P.J., Gray�  III, G.T. and Foster�  Jr., J.C.2Viscoelastic models for explosive binder materials3Bardenhagen, S.G., Greening, D.R. and Roessig, K.M.TThe material point method and simulation of wave propagation in heterogeneoous media187-192>Bardenhagen, S.G., Brydon, A.D., Williams, T.O. and Collet, C.nCoupling grain scale and bulk mechanical response for PBXs using numerical simulations of real microstructures479-482Bardo, R.D. and Jones, W.H.FA theoretical calculation of the 0 K isotherm for shocked nitromethane621-624Bardo, R.D.;Rate-determining steps for ignition of shocked nitromethane843-856iCunningham, B., Vandersall, K.S., Niles, A.M., Greenwood, D.W., Garcia, F., Forbes, J.W. and Wilson, W.H.:Carbon resistor pressure gauge calibration at low stresses	1137-1140Curran, D.R.GStress and temperature-driven nucleation of microscopic voids in metals135-139Curran, D.R. and Seaman, L.UComputational models for nucleation, growth, and coalescence of adiabatic shear bands&Shock Waves in Condensed Matter - 1985315-320GApplication of micromechanical failure models to shock physics problems321-326GIncubation times and rate-dependent toughness for macrocrack initiation305-308LAppropriate material softening and failure models for numerical calculations395-398'Curran, D.R., Seaman, L. and Cooper, T.]A micromechanical model for granular material and application to penetration of ceramic armor5Computer models of dynamic fracture and fragmentation*Curran, D.R., Cooper, T. and Tokheim, R.E.1Model for hot spots in porous frictional materialYThe importance of material properties for cratering and penetration in geologic materials945-948*Curran, D.R., Seaman, L. and Tokheim, R.E..Fragmentation models based on void coalescence"Dynamic fracture and fragmentationLComparison of mesomechanical and continuum granular flow models for ceramics315-3181Cygan, R.T., Boslough, M.B. and Kirkpatrick, R.J.IExperimentally shocked quartz, NMR spectroscopy, and shock wave barometry<NMR spectroscopy of experimentally shocked silicate minerals633-636NNMR spectroscopic examination of shocked sandstone from Meteor Crater, Arizona9Czerski, H., Greenaway, M.W., Proud, W.G. and Field, J.E.7Monitoring phase change in HMX during dropweight impactCowperthwaite, M. and Vidal, P.?Shock-change equations for classical two-dimensional detonation255-258>One-dimensional flows with straight particle velocity contours245-248@A new approach to the Wood and Kirkwood axial detonation problem	1357-1360	Cox, G.A.9A multiphase equation of state and strength model for tin208-211+A multi-phase equation of state for bismuth151-154 Coyne�  Jr., P.J. and Elban, W.L.>A strain rate sensitivity prediction for porous bed compaction;Crawford, P., Rainey, K., Rightley, P. and Hammerberg, J.E.dA novel experimental technique for the study of high-speed friction under elastic loading conditionsCrawford, D.A.nUsing mesoscale modeling to investigate the role of material heterogeneity in geologic and planetary materials	1453-1457>Crepeau, J., Needham, C., Caipen, T., Grady, D. and Harper, F.RFirst principles calculations of the interaction of blast waves with aqueous foams*Crockett, S., Chisholm, E. and Wallace, D.bA 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. and Burakovsky, L.?Testing of a liquid equation of state model against copper data-Cross, D.L.A., Dandekar, D.P. and Proud, W.G.Spall behaviour of PMMA655-658uCross, D.L.A., Chapman, D.J., Tsembelis, K., Proud, W.G., Borg, J.P., Lloyd, A., Schwalbe, L., Cogar, J. and Ward, A.+Experimental Hugoniot data of porous silica0Crouzet, B., Partouche-Sebban, D. and Carion, N.0Temperature measurements in shocked nitromethane	1253-12564Crouzet, B., Soulard, L., Carion, N. and Manczur, P.hInteraction between a steady detonation wave in nitromethane and geometrical complex confinement defects817-820+Cui, X.L., Zhu, W.J., He, H.L. and Li, Y.J.9Cortecuisse, S., Cansell, F., Fabre, D. and Petitet, J.P.ARaman spectroscopy of nitromethane under pressure and temperature295-297.Cosculluela, A., Cagnoux, J. and Collombet, F.LTwo types of experiment for studying uniaxial dynamic compression of alumina951-954Cottet, F. and Romain, J.P./Twinning in iron by laser generated shock waves130-134'Cottet, F., Fabbro, R. and Romain, J.P.SExperiments and simulation of laser-driven shock wave evolution in aluminum targetsLCottet, F., Hallouin, M., Romain, J.P., Fabbro, R., Faral, B. and P"�pin, H.JGeneration of ultra-high pressure shocks in 0.26 mm wavelength experiments531-534Cottet, F. and Boustie, M._Spall measurements in metallic targets using shock waves induced by short duration laser pulses�Theoretical study of the coupling of electrons and lattice wave packets in superconducting metastable states formed at high shock pressures595-598HTheoretical prediction of novel molecular solids formed at high pressure209-216"Bardwell, S. and Parpart-Henke, U.8The use of strong shock waves for isentropic compression331-333Barker, L.M.1High-pressure quasi-isentropic impact experiments217-2246Barker, L.M., Trucano, T.G., Wise, J.L. and Asay, J.R.RExperimental technique for measuring the isentrope of hydrogen to several megabars455-459-Barker, L.M., Trucano, T.G. and Munford, J.W.6Metal surface gouging by hypervelocity sliding contact753-756<Barker, L.M., Chhabildas, L.C., Trucano, T.G. and Asay, J.R.%Gas-accelerated plate stability study989-991%The accuracy of VISAR instrumentation833-836EThe development of the VISAR and its use in shock compression scienceAMulti-beam VISARs for simultaneous velocity vs. time measurements999-10025Barlow, A.J., Winter, R.E., Carley, D. and Taylor, P.AHydrocode modelling and analysis of a dynamic friction experiment521-524,Barnes, N., Bourne, N.K. and Millett, J.C.F.409-412�Bakhralh, S.M., Volodina, N.A., Drennov, O.B., Goreva, T.A., Mikhailov, A.L., Nizovtsev, P.N., Spiridonov, V.F. and Shuvalova, E.V.�Numerical simulation and experimental study of co<  ating stabilizing effect on shear instability growth in oblique impact of metal slabs	1363-1366CBalagansky, I.A., Balagansky, A.I., Razorenov, S.V. and Utkin, A.V.0Evolution of shock waves in silicon carbide rods835-838
Ball, G.J.(Numerical simulation of dynamic friction	1503-1506@Ballard, P., Fournier, J., Fabbro, R., Frelat, J. and Castex, L.)Residual stresses induced by laser shocks341-344;Bandak, F.A., Armstrong, R.W., Douglas, A.S. and Tsai, D.H.2Nanodislocation structures for shock strengthening*Bandyopadhyay, A., Das, K. and Gupta, Y.M.GShock wave synthesis of titanium silicide. 2: Effect of ceramic fillers	1079-10818Bar-On, E., Rajendran, A.M., Bless, S.J. and Grove, D.J.3Modeling of dynamic fracture in a solid cone target939-942 Bar-on, E. and Yankelevsky, D.Z.]Using Maxwell-Boltzmann's statistics for microcracks distribution function in a failure model9Bar-on, E., Partom, Y., Rubin, M.B. and Yankelevsky, D.Z.&On the HEL and the 'ramping' above HEL739-742
Bar-on, E./More on the response of ceramics to shock waves223-226Barbee�  III, T.W.0Phonons and metastability in compressed nitrogen163-1666Barber, J.L., Kadau, K., Germann, T.C. and Alder, B.J.9Simulation of fluid instabilities using atomistic methods301-304Barbieri, F. and Patuelli, C.fRecovery of copper after shock-loading by means of Fourier analysis of x-ray diffraction line profiles453-456EBardenhagen, S.G., Harstad, E.N., Foster�  Jr., J.C. and Maudlin, P.J.5Viscoelastic models for polymeric composite materials327-330`Modeling a material's instantaneous velocity during acceleration driven by a detonation gas-push936-939,Badding, J.V., Nesting, D.C. and Baron, R.B.GIn situ study of the solubility of hydrogen in rhenium at high pressure	1317-1320"Baek, S.-H., Lee, E.S. and Kim, I.nMeasurement of shock propagation and metal plasma expansion in underwater wire explosion by utilizing CW laser	1077-1080
Baer, M.R.RA mixture model for shock compression of porous multi-component reactive materials	1247-1250'Baer, M.R., Hertel, E.S. and Bell, R.L.4Multidimensional DDT modeling of energetic materials433-436KComputational modeling of heterogeneous reactive materials at the mesoscale27-33Baer, M.R. and Trott, W.M.EMesoscale descriptions of shock-loaded heterogeneous porous materials713-7165Mesoscale studies of shock loaded tin sphere lattices517-520Baer, B.J. and Yoo, C.-S.lVibrational spectra of dense molecular fluids in a laser-heated DAC: Implications to shock-compressed fluids	1249-1252HBaer, M.R., Hall, C.A., Gustavsen, R.L., Hooks, D.E. and Sheffield, S.A.HThe UV/visible absorption spectra of shocked nitromethane-amine mixtures	1559-1562Cook, M.D. and Haskins, P.J./Short range interactions of detonation products271-274)Cook, M.D., Haskins, P.J. and James, H.R.iAn investigation of projectile and barrier geometry effects on impact initiation of a secondary explosive675-678Cook, W.H. and Rajendran, A.M.&Modeling impact damage in AD85 alumina)Damage evolution in viscoelastic polymersClements, B.E. and Mas, E.M.[Modeling high explosives with the method of cells and Mori-Tanaka effective medium theories427-430-Clements, B.E., Mas, E.M. and Gray�  III, G.T.<Investigation of the observed anisotropic fracture in steels+Clements, B.E., Mas, E.M. and Maudlin, P.J.cDevelopments toward a continuum-level non-spherical void growth model using a micro-mechanics basis*Low-pressure equation of state of polymers57-60EClements, B.E., Mas, E.M., Plohr, J.N., Ionita, A. and Addessio, F.L.<Dynamic response of PBX9501 through the b-d phase transition204-207
Clifton, R.J.-Re-examination of the precursor decay anomaly407-411)Plate impact facility at Brown University661-662@Pressure shear impact and the dynamic plastic response of metals105-1115Clifton, R.J., Raiser, G., Ortiz, M. and Espinosa, H.'A soft recovery experiment for ceramics437-440'Clifton, R.J., Mello, M. and Brar, N.S.3Effect of shear on failure waves in soda lime glassClifton, R.J. and Bhate, N.8Bridging length scales in dynamic plasticity simulations19-260Clifton, R.J., Jearanaisilawong, P. and Jiao, T.7Hgih strain rate response of an epoxy and a vinyl esterCochran, S.G. and Tarver, C.M.bModeling particle size and initial temperature events on shock initiation of TATB-based explosives593-596Coffey, C.S.6Compressive waves and shock waves in anharmonic solids)Coffey, C.S., Davis, J.J. and Woody, D.L.;Energy localization in rapidly deforming crystalline solids253-256CMicroscopic processes of plastic deformation during shock or impact	1181-1184GEnergy dissipation and the initiation of explosives during plastic flow807-810Coffey, C.S. and Sharma, J.7Crystal failure and crack formation during plastic flow:Cho, Y.S., Baek, S.H., Lee, J., Choi, K.Y. and Song, S.-Y.#Interaction of two bubbles in water!Choi, C.S., Lee, S.W. and Kim, K.GTemperature rise in hot spots in porous explosives due to finite strain@Christiansen, E.L., Crews, J.L., Kerr, J.H. and Chhabildas, L.C.MHypervelocity impact testing above 10 km/s of advanced orbital debris shieldsChronister, E.L. and Baer, B.J.QAn optical study of pentacene in p-terphenyl at high pressure and low temperature	1507-1510Chung, D.-T.7The effect of the specimen shape on dynamic flow stress(Church, P., Townsley, R. and Millett, J.@Consideration of stress gauges in the modelling of plate impacts	1083-1086;Church, P.D., Proud, W.G., Andrews, T.D. and Goldthorpe, B.LThe spall strength measurement and modelling of AQ80 iron and copper systems487-490;Church, P.D., Andrews, T., Bourne, N.K. and Millett, J.C.F.Spallation in the alloy Ti6Al4VDChurch, P.D., Grief, A., Tsembelis, K., Proud, W.G. and Murray, N.H.?Experiment and simulation of the lateral gauge in glass targetsECinnamon, J.D., Palazotto, A.N., Brar, N.S., Kennan, Z. and Bajaj, D.FJohnson-Cook strength model constants for Vascomax 300 and 1080 steels709-712Clarke, S.A., Bolme, C.A., Murphy, M.J., Landon, C.D., Mason, T.A., Adrian, R.J., Akinci, A.A., Martinez, M.E. and Thomas, K.A.<Using schlieren visualization to track detonator performance	1089-1092
Clayton, J.D.JPlasticity and spall in high density polycrystals: Modeling and simulation311-314Clegg, R.A. and Hayhurst, C.J.tNumerical modelling of the compressive and tensile response of brittle materials under high pressure dynamic loading)Clegg, R.A., Hayhurst, C.J. and Nahme, H.lValidation of an advanced material model for simulating the impact and shock response of composite materialsClements, B.E.#Launch capabilities to over 10 km/s	1025-1031?Chhabildas, L.C., Boslough, M.B., Reinhart, W.D. and Hall, C.A.BDebris cloud characterization at impact velocities of 5 to 11 km/s	1841-1844=Chhabildas, L.C., Kmetyk, L.N., Reinhart, W.D. and Hall, C.A.Launch capabilities to 16 km/s	1197-1200?Chhabildas, L.C., Furnish, M.D., Reinhart, W.D. and Grady, D.E.Impact of AD995 alumina rods2Chhabildas, L.C., Furnish, M.D. and Reinhart, W.D.<Shock induced melting in aluminum: Wave profile measurements97-100IChhabildas, L.C., Trott, W.M., Reinhart, W.D., Cogar, J.R. and Mann, G.A.<Incipient spall studies in tantalum: Microstructural effects+Chidester, S.K., Tarver, C.M. and Lee, C.G.2Impact initiation of new and aged solid explosives<Chidester, S.K., Tarver, C.M., DePiero, A.H. and Garza, R.G.]Single and multiple impact ignition of new and aged high explosives in the Steven impact test663-666AChidester, S.K., Vandersall, K.S., Switzer, L.L. and Tarver, C.M.ZLX-04 violence measurements: Steven tests impacted by projectiles shot from a howitzer gun	1049-1052hChidester, S.K., Thompson, D.G., Vandersall, K.S., Idar, D.J., Tarver, C.M., Garcia, F. and Urtiew, P.A.wShock initiation experiments on PBX 9501 explosive at pressures bel<  ow  GPa with associated ignition and growth modeling903-906.Chijioke, A.D., Nellis, W.J. and Silvera, I.F.EIsotherms reduced from isentropes and Hugoniots up to several 100 GPa49-53*Chisholm, E., Crockett, S. and Wallace, D._Variation of thermal and cold curve contributions to thermodynamic functions along the HugoniotChisholm, E. and Wallace, D.SEstimating the viscosity coefficient of liquid metals from vibration-transit theoryChitanvis, S.M.-Hotspot mechanisms in shock-melted explosivesHPreliminary results from an asymptotic analysis of the Forest Fire model511-514ACritical propagation velocities of a steady autonomous detonation511-513Ch"�ret, R.*The life and work of Pierre Henri HugoniotECherne, F.J., Baskes, M.I., Germann, T.C., Ravelo, R.J. and Kadau, K.RShock Hugoniot and melt curve for a modified embedded atom method model of gallium)Cherne, F.J., Kadau, K. and Germann, T.C.PA molecular dynamics study of solid gallium using a modified embedded atom model9Cherne, F.J., Rigg, P.A., Anderson, W.W. and Cooley, J.C.6Examination of the spallation behavior of cerium metal489-492TChesnut, G.N., Streetman, B.D., Schiferl, D., Anderson, W.W., Nicol, M. and Meng, Y.VStatic X-ray diffraction of cerium: The standard approach and the magic-angle approach,Chesnut, G.N., Anderson, W.W. and Casson, J.7Static X-ray diffracton study of cerium to 300 kilobars0Chesnut, G.N., Velisavljevic, N. and Sanchez, L.1Static high pressure X-ray diffraction of Ti6Al4V27-30+Chhabildas, L.C., Wise, J.L. and Asay, J.R.)Reshock and release behavior of beryllium422-426Chhabildas, L.C.9The Sandia shock thermodynamics applied research facility621-625 Chhabildas, L.C. and Grady, D.E.'Shock loading behaviour of fused quartz175-1792Shock loading and release behavior of x-cut quartz601-6058Chhabildas, L.C., Carr, M.J., Kunz, S.C. and Morosin, B.&Shock-recovery experiments on PZT 95/5785-790!Chhabildas, L.C. and Barker, L.M.0Dynamic quasi-isentropic compression of tungsten111-114#Pressure-shear loading of materials579-584<Chhabildas, L.C., Barker, L.M., Asay, J.R. and Trucano, T.G.=Spall strength measurements on shock-loaded refractory metals-Chhabildas, L.C., Hertel, E.S. and Hill, S.A.+Whipple bumper shield tests at over 10 km/s991-994VChhabildas, L.C., Barker, L.M., Asay, J.R., Trucano, T.G., Kerley, G.I. and Dunn, J.E..Chen, D., Feng, J., Wang, J.-G. and Liu, G.-L.(Terminal effects of high velocity impactChen, S.-H.&Component Hugoniot in mixture material69-72BChen, G., Stump, N.A., Haire, R.G., Burns, J.B. and Peterson, J.R.3A luminescence study of B-type Eu2O3 under pressure359-362?Chen, J.H., Iwasaki, H., Kikegawa, T., Yaoita, K. and Tsuji, K.=Crystal structure of the high pressure phase of bismuth BiIIIChen, A.L. and Yu, P.Y.NNear-IR absorption measurements of the transition metal iodides under pressure-Chen, H.C., Meyers, M.A. and Nesterenko, V.F.5Shear localization in granular and comminuted alumina607-610%Chen, G.Q., Ahrens, T.J. and Hide, R.9Theory of shock magnetization of asteroids Gaspra and Ida929-932,Chen, T., Thadhani, N.N. and Hampikian, J.M.;Shock compaction and strengthenning of nanocrystalline NiAl733-736(Chen, Q., Cao, L., Gong, Z. and Jing, F.GHugoniots and shock temperature of dense helium under shock compression@Chen, X.-F., Gong, Z., Fei, Y., Zhang, L., Deng, L. and Jing, F.pA new evidence of the stability of (Mg,Fe)SiO3 perovskite at lower mantle conditions: Shock recovery experiments-Chen, Q.F., Cai, L.C., Zhang, Y. and Gu, Y.J.eThe dissociation and thermodynamics of dense fluid oxygen by self-consistent fluid variational theory23-267Chen, Y., Hu, H., Tang, X., Li, Q., Feng, Q. and Hu, J.[Phase transition behavior and abnormal spall in FeMnNi alloy with low a-e transition stress2Cheng, J.-Y., Zhou, G.-Q., Tang, Z.P. and Li, X.Z.lA unified theory of collective dislocation motion including both thermal activation and viscous drag effectskCheret, R., Andriot, P., Chapron, P., Le�  Drean, C., Lezaud, J.M., Loichot, R., Martineau, J. and Olive, F.DShock wave experiments using explosives and light gas-gun facilities626-630
Cheret, R.,Chapman, D.J., Tsembelis, K. and Proud, W.G.-The behaviour of dry sand under shock loading	1445-14480Chapman, D.J., Braithwaite, C.H. and Proud, W.G.*Shock-loading of statically compacted soil&Chapron, P., Elias, P. and Laurent, B.hExperimental determination of the pressure inducing melting in release for shock-loaded metallic samples171-173Charest, J.A. and Lynch, C.S.8The response of PVF2 stress gauges to shock wave loading797-800,A simple approach to piezofilm stress gauges897-900Charest, J.A. and Lilly, M.D.6PFV2 stress gauges for non-planar wave applications. 1	1731-1734Charest, J.A. and Mace, J.L.0Outputs of shock-loaded small piezoceramic disks	1153-1156Chartagnac, P.F.DDetermination of mean and deviatoric stresses in shock loaded solids397-401Chartagnac, P.3A pragmatic approach to sequential dynamic loadings923-930RChartagnac, P., Decaso, P., Jimenez, B., Bouchu, M., Cavailler, C. and Delavel, J.8Dynamic behaviour of PVF2 gauges in the 0-600 kbar range893-8961Charters, A.C., Menna, T.L. and Piekutowski, A.J.QHigh velocity penetration of semi-infinite steel by continuous and segmented rods931-934QChau, H., Dittbenner, G., Mikkelsen, K., Weingart, R., Froeschner, K. and Lee, R.2Performance of a 100 kV, 78 kJ electric gun system691-695)Chauvin, C., Hereil, P.L. and Sinatti, F.VAnalysis of temperature measurement at lead/LiF interface under shock wave compression2Chemerys, V.T., Raychenko, A.I. and Karpinos, B.S.YImpact interaction of projectile with conducting wall at the presence of electric current	1314-1317Chen, D.[Numerical simulation and analysis of single/two-stage gas gun for shock compression studies649-651Chen, X.-R. and Chen, B.-Y.AA study of the mechanism of pressure-casting charge of explosives737-740;Modeling of non-eroding penetration using ALE3D and Zapotec	1281-1284 Celebonovic, V. and Schulz, H.J.IThe electrical conductivity of the organic conductors under high pressure	1449-1452TCerreta, E., Gray�  III, G.T., Henrie, B.L., Brown, D.W., Hixson, R.S. and Rigg, P.A.vThe influence of peak stress on the mechanical behavior and the substructural evolution in shock-prestrained zirconium541-544UCerreta, E., Gray�  III, G.T., Lawson, A.C., Morris, C.E., Hixson, R.S. and Rigg, P.A.eThe influence of interstitial oxygen on the alpha to omega phase transition in titanium and zirconiumKCerreta, E.K., Gray�  III, G.T., Trujillo, C.P., Brown, D.W. and Tom"�, C.N.SThe influence of peak shock stress on the quasistatic reload response of hcp metals635-638LChakravarty, A., Gifford, M.J., Greenaway, M.W., Proud, W.G. and Field, J.E.:Factors affecting shock sensitivity of energetic materials,Chakravarty, A., Proud, W.G. and Field, J.E.-Small scale gap testing of novel compositions935-938@Chambers, G., Sandusky, H., Zerilli, F., Rye, K. and Tussing, R.SPressure measurements on a deforming surface in response to an underwater explosion6Chambers, G.P., Lee, R.J., Oxby, T.J. and Perger, W.F.7Electromagnetic properties of pre-detonating explosives890-897%Chandra, U., Mudgal, P. and Kumar, M.sStudy of phase transformations on nanocrystalline (La,Sr)(Mn,Fe)O3 systems by high-pressure M""ssbauer spectroscopy200-203:Chang, S.N., Meyers, M.A., Thadhani, N.N. and Erlich, D.C.PMartensitic transformations induced by tensile stres<  s pulse in an Fe-Ni-Mn alloy@Chang, S.N., Chung, D.-T., Ravichandran, G. and Nemat-Nasser, S.DPlate impact experiments on Mg-PSZ and improved target configuration389-392Chang, S.N. and Choi, J.H.3High strain rate response of a tungsten heavy alloy415-418PMeasurement of ignition and reaction parameters in non-ideal energetic materials	1045-1048[Carter, J.A., Wang, Z., Lagutchev, A., Fang, Y., Seong, N.-H., Cahill, D.G. and Dlott, D.D.HUltrafast shock wave coherent dissociation and spectroscopy of materials	1221-1224-Carton, E.P., Stuivinga, M. and Verbeek, H.J./Crack prevention in shock compaction of powders549-552TShock compaction of combustion synthesized ceramics in the cylindrical configuration+Carton, E.P., Stuivinga, M. and Boluijt, A.!TiC by SHS and dynamic compaction	1127-1130Carton, E.P. and Stuivinga, M.3Scale-up method for the shock compaction of powders	1086-1089)Explosive forming of aerospace componentsCase, S. and Horie, Y.=Modelling the shock response of polycrystals at the mesoscale(Casey, W.H., Carr, M.J. and Graham, R.A.>Crystal defects and the dissolution kinetics of shocked rutileCatanach, R.A. and Hill, L.G.JDiameter effect curve and detonation front curvature measurements for ANFO906-909;Caulder, S.M., Buess, M.L., Garroway, A.N. and Miller, P.J.bNQR line broadening due to crystal lattice imperfections and its relationship to shock sensitivity929-934+Cazalis, B., Boissi"�re, C. and Sibille, G.EShocks induced by laser driven flyer plates. 2: Numerical simulationsFCazamias, J.U., Bless, S.J., Hari�  Manoj�  Simha, C. and Hartnett, T.M.8Dynamic failure of a transparent polycrystalline ceramic611-614Cazamias, J.U.OThe effects of shear banding in 6-4 titanium on round and square Taylor impacts587-590+Cazamias, J.U., Fiske, P.S. and Bless, S.J."The Hugoniot elastic limit of ALONNCazamias, J.U., Reinhart, W.D., Konrad, C.H., Chhabildas, L.C. and Bless, S.J.#Bar impact tests on alumina (AD995)787-790 Cazamias, J.U. and Schrand, S.R.(Cansell, F., Fabre, D. and Petitet, J.P.PRaman study of benzene phase transition under high pressure and high temperatureBCao, B.Y., Meyers, M.A., Nesterenko, V.F., Benson, D. and Xu, Y.B.RShear localization-martensitic transformation interactions in Fe-Cr-Ni monocrystaleCao, B.Y., Meyers, M.A., Lassila, D.H., Schneider, M.S., Xu, Y.B., Kalantar, D.H. and Remington, B.A.ODefect substructures in plate impacted and laser shocked monocrystalline copper	1145-1148NCapellos, C., Baker, E.L., Nicolich, S., Balas, W., Pincay, J. and Stiel, L.I.?Eigenvalue detonation of combined effects aluminized explosives357-360*Card"�o, P.A., Gois, J.C. and Campos, J.A.,Thermal decomposition of energetic materials853-856ACarney, J.R., Ladouceur, H.D., Russell, T.P. and Pangilinan, G.I.QA new method for determining material thermal properties at static high pressures	1143-1146;Carney, J.R., Miller, J.S., Gump, J.C. and Pangilinan, G.I.IAtmospheric effects on the combustion of detonating aluminized explosives948-9510Carney, J.R., Wilkinson, J. and Lightstone, J.M.HTime-resolved optical measurements of detonation and combustion products	1225-1228Carr, M.J. and Beauchamp, E.K.qTransmission electron microscopical characterization of hot pressed shocked and unshocked aluminum nitride powder4Carr, M.J., Hills, C.R., Graham, R.A. and Wise, J.L.{The effects of microstructure on the hardness and deformation mode of shock-loaded 6061 aluminum and JBK-75 stainless steel335-338OCarroll, D.E., Chhabildas, L.C., Reinhart, W.D., Winfree, N.A. and Kerley, G.I.DComputational characterization of three-stage gun flier plate launch307-310ICart, E.J., Lee, R.J., Gustavson, P.K., Coffey, C.S. and Sutherland, G.T.3The role of shear in shock initiation of explosivesECart, E.J., Granholm, R.H., Joshi, V.S., Sandusky, H.W. and Lee, R.J.;Williamsburg equation of state for detonation product fluid73-76bEntropy production in ZND detonation with realistic equations of state for explosives and products353-356QCady, C.M., Gray�  III, G.T., Liu, C., Trujillo, C.P., Jacquez, B.L. and Mukai, T.bCompressive properties of a closed-cell aluminum foam as a function of strain rate and temperature>Cagliostro, D.J., Warnes, R.H., Johnson, N.L. and Fujita, R.K.\Spall measurements in shock-loaded hemispherical shells from free-surface velocity histories367-370Cagnoux, J.=Shock-wave compression of a borosilicate glass up to 170 kbar392-396Cagnoux, J. and Longy, F.2Is the dynamic strength of alumina rate-dependent?293-296KSpherical waves in pure alumina: Effects of grain size on flow and fracture Cai, H., Tang, Z.P. and Yang, B.AInverse method and consistency examination for Lagrangian anlysis973-976Cai, J. and Nesterenko, V.F.XCollapse of hollow cylinders of PTFE and aluminum particles mixtures using Hopkinson barDCai, J., Jiang, F., Vecchio, K.S., Meyers, M.A. and Nesterenko, V.F.=Mechanical and microstructural properties of PTFE/Al/W systemCalef, D.F.ETheoretical approaches to chemical dynamics in high compressed fluids457-462+Callen, B.W., Lamb, F.K. and Sullivan, J.D.DInsensitive interval in the evolution of shock waves from explosionsICampbell, E.M., Holmes, N.C., Libby, S.B., Remington, B.A. and Teller, E.DHigh energy-density physics: From nuclear testing to the superlasers21-27.Campbell, E.M., Cauble, R. and Remington, B.A.=High energy density science on the National Ignition Facility.Campbell, J.C., Vignjevic, R. and Bourne, N.K.;A numerical investigation of sleeved Taylor anvil specimensCampillo, A.J. and Schoen, P.E.:Reflective probing of laser generated kbar shocks in water347-3503On a criterion for thermo-plastic shear instability372-37Burns, T.J.4Dynamic instability in adiabatic thermoplastic shear145-1465A mechanism for high strain rate shear band formation&Shock waves in Condensed Matter - 1989345-348Burns, M.J. and Taylor, P.GA study of SDT in an ammonium nitrate (NH4NO3) based granular explosive8Burnside, N.J., Son, S.F., Asay, B.W. and Skidmore, C.B.1Particle characterization of pressed granular HMXBurt, J.A. and Gupta, Y.M.KTime-resolved ruby luminescence measurements under shock compression at 77K695-697hBushman, A.V., Efremov, V.P., Fortov, V.E., Kanel, G.I., Lomonosov, I.V., Ternovoi, V.Y. and Utkin, A.V.;Equation of state of composites under high energy densities79-82 Butkovich, T.R. and Burton, D.E.;Underground explosive fracture and permeability enhancement,Butler, S., Millett, J.C.F. and Bourne, N.K.4Shock induced equation of state of polyvinylchlorideBuy, F. and Llorca, F.cShock wave effects in copper: Design of an experimental device for post recovery mechanical testing319-322@The expanding shell test: Numerical simulation of the experimentBuy, F. and Voltz, C.FShock loading influence on the mechanical behavior of high purity iron533-536!Buy, F., Voltz, C. and Llorca, F.qThermodynamically based equation of state for shock wave studies: Application to the design of experiments on tin41-447Buzaud, E., Hereil, P.L., Pontiroli, C. and Lambert, P.7Modeling the shock compression of concrete under 20 GPa!Byers�  Brown, W. and Horton, T.V.aAnalytical representation of high density fluid equations of state based on statistical mechanics$Byers�  Brown, W. and Braithwaite, M.�Analytical representation of the adiabatic equation for detonation products based on statistical mechanics and intermolecular forces325-328Budge, K.G.EALE shock calculations using a stabilized serendipity rezoning scheme[Budin, A., Bogomaz, A., Kolikov, V., Kuprin, A., Leontiev, V., Rutberg, P. and Shirokov, N.GInvestigation of heavy current dischar< ges with high initial gas density937-939MBuelow, S.J., Anderson, J.E., Aiken, A.C., Arrington�  Jr., C.A. and Jones, B.GMass spectral studies of shocked salts and nitrocellulose polymer films	1377-1380Bukiet, B. and Menikoff, R.2Sharp shock model for propagating detonation waves259-262
Bukiet, B.*Solving curved detonation Riemann problems321-324Bukowinski, M.S.T.:Accurate self-consistent-field isotherms for NaCl to 30GPa218-222Bundy, F.P.<A history of the science and technology of diamond synthesis495-498Buravova, S.0Surface erosion under impact action of particles	1007-1010Burchell, M.J. and Thomson, R.BIntact hypervelocity particle capture in aerogel in the laboratory	1155-1158CBurchell, M.J., Leliwa-Kopystynki, J., Vaughan, B. and Zarnecki, J.9Comparison of H2O and CO2 ices under hypervelocity impact949-952Burchell, M.J.4Microbial life and shock compression: Life or death?	1439-1444Burkett, M.W. and Rabern, D.A.UStress fields generated by kinetic energy projectile interaction with ceramic targets947-950;Burkett, M.W., Clancy, S.P., Maudlin, P.J. and Holian, K.S.LDynamic mechanical behavior characterization of epoxy-cast Al+Fe2O3 mixtures>Ferranti�  Jr., L., Jordan, J.L., Dick, R.D. and Thadhani, N.N.AShock Hugoniot behavior of particle reinforced polymer composites123-126$Ferranti�  Jr., L. and Thadhani, N.N.^Incremental stress-strain response of polymers using instrumented reverse Taylor anvil impactsQFerreira, A., Yu, L.H., Thadhani, N.N., Chang, S.N., Chang, S.S. and Meyers, M.A.XShock compaction, synthesis, and chemically assisted bonding of aluminides and silicides$Ferreira, A. and Costa�  Junior, A.M.AAnalytical model for compaction of powder by means of shock wavesFerrel, R. and Romero, V.3SPH simulation of high density hydrogen compressionUField, J.E., Tsembelis, K., Brar, N.S., Proud, W.G., Dandekar, D.P. and Rosenberg, Z.AIssues related to lateral stress measurements in alumina ceramics;Field, J.E., Braithwaite, C.H., Guest, A.R. and Proud, W.G.>Investigation into the spall strengths of geological materials?Fietz, W.H., Metzger, J., Weber, T., Grube, K. and Ludwig, H.A.7Fatyanov, O.V., Ogura, T., Nicol, M.F. and Kondo, K.-I.MPrecise time-resolved mid-infrared radiometry of shocked carbon tetrachloride/Fedorov, A.V., Menshikh, A.V. and Yagodin, N.B.?On detonation wave front structure of condensed high explosivesMFedorov, A.V., Zotov, E.V., Krasovsky, G.B., Menshikh, A.V. and Yagodin, N.B.ADetonation front in homogeneous and heterogeneous high explosives
Fedorov, A.V.kExperimental investigation of heterogeneous high explosive decomposition mechanism in detonation wave front910-913�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. and Khokhlov, A.A.CRecording 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. and 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. and Davydov, V.A.2Shock wave initiation of mixture liquid explosives960-963rFedorov, A.V., Mikhailov, A.L., Nazarov, D.V., Finyushin, S.A., Menshikh, A.V., Davydov, V.A. and Govorunova, T.A.NStudy of detonation wave structure in solid and liquid tetranitromethane (TNM)964-967)Fellows, J., Haskins, P.J. and Cook, M.D._A study of deflagration-to-detonation transition in a model A-B system using molecular dynamics391-394(Feng, K.K., Jones, D.E.G. and Chan, S.K.;Shock initiation of bubble sensitized commercial explosivesFeng, R. and Gupta, Y.M.VEffect of epoxy bond response on combined compression-shear wave propagation in solidsFeng, S.S. and Wang, H.F.XA simple method of determining the attenuation of the shock pressure in porous materials963-966"Feng, R., Gupta, Y.M. and Yuan, G.'Fanget, A., Hereil, P.L. and Martin, C.SInfluence of the polymorphic transition and damage in steel on 2D waves propagation235-238
Fanget, A.pStability analysis of numerical solutions of wave propagation when pseudoviscosity is replaced by real viscosity%Fanget, A., Trumel, H. and Dragon, A.}A coupled viscoelastic-viscoplastic finite strain model for the dynamic behaviour of particulate composites: Numerical issues179-182@Faral, B., Fabbro, R., Virmont, J., Cottet, F. and Romain, J.-P.oGeneration of ultrahigh pressures obtained in colliding foil experiments: Importance of two-dimensional effects761-7633Faral, B., Fabbro, R., Cottet, F. and Romain, J.-P.tX-UV and visible emission of very high shocks (100 Mbar) in gold obtained by impedance mismatch in laser experimentsrFaral, B., Koenig, M., Boudenne, J.M., Batani, D., Benuzzi, A., Bossi, S., Temporal, M., Atzeni, S. and L""wer, T.LEOS impedance matching experiments at high pressure with smoothed laser beam943-946FFarber, D.L., Esposito, A.P., Zaug, J.M., Raugh, J.E. and Aracne, C.M.CFirst results of reaction propagation rates in HMX at high pressure(Farnsworth�  Jr., A.V. and Lawrence, R.J.ZBrown, E.N., Rae, P.J., Trujillo, C.P., Dattelbaum, D.M., Gray�  III, G.T. and Bourne, N.K.OShock and recovery of PTFE above and below the phase II to phase III transition196-199LDetermination of dynamic mechanical properties from explosively driven rings389-393Brar, N.S. and Gupta, Y.M.@Piezoresistance response of different batches of ytterbium foils513-518+Phase transition in shocked ytterbium foils151-153)Brar, N.S., Bless, S.J. and Rosenberg, Z.>Factors affecting ballistic efficiency of alumina and sapphire955-957)Brar, N.S., Rosenberg, Z. and Bless, S.J.\Applying Steinberg ��s model to the Hugoniot elastic limit of porous boron carbide specimens467-470Brar, N.S. and Rosenberg, Z.JOn the possibility of fracto-emission in ceramics during shock compression	1759-1762Shock Hugoniot of 1215 steel101-1049Brar, N.S., Espinosa, H.D., Yuan, G. and Zavattieri, P.D.BExperimental study of interface defeat in confined ceramic targets'Brar, N.S., Hopkins, A. and Laber, M.W.)Laser shock peening of titanium 6-4 alloy
Brar, N.S.;Failure waves in glass and ceramics under shock compression601-606Brar, N.S. and Joshi, V.S.QDynamic characterization of compliant/brittle materials using split Hopkinson bar+Brar, N.S., Proud, W.G. and Rajendran, A.M.:Ceramic bar impact experiments for improved material model727-730Brar, N.S. and Rajendran, A.M..Confined alumina bar-on-bar impact experiments843-846(Brar, N.S., Joshi, V.S. and Harris, B.W.PConstitutive model constants for low carbon steels from tension and torsion data*Braue, W., Schneider, H. and Hornemann, U.eShock-wave induced formation of 'diaplectic' glasses of mullite 2Al2O3:1SiO2 composition: a TEM study725-728*Brenner, D.W., Elert, M.L. and White, C.T.UIncorporation of reactive dynamics in simulations of chemically-sustained shock waves
Brenner, D.W.;Molecular potentials for simulating shock-induced chemistry115-1217Damaging of materials by bi-dimensional dynamic effects	1321-1326Bouton, E. and Vidal, P.@Estimate of shock Hugoniot adiabat of liquids from hydrodynamics352-3565Bouyer, V., Baudin, G., Le�  Gallic, C. and Herv"�, P.OEmission spectroscopy applied to shock to detonation transition in nitromethane	1223-1226<  &Bouyer, V., H"�bert, P. and Doucet, M._Study of the laser-induced decomposition of HNO3/2-nitropropane mixture at static high pressure	1217-1220Bovenkerk, H.P.:The commercialization of high pressure synthesized diamond'Boyle, V.M., Frey, R.B. and Bines, A.L.1Parallel/oblique impact on thin explosive samples819-8220Bragov, A.M., Lomunov, A.K. and Sergeichev, I.V./High-speed behavior of some shape memory alloysABragov, A.M., Lomunov, A.K., Sergeichev, I.V. and Gray�  III, G.T.;Dynamic behaviour of birch and sequoia at high strain rates	1511-1514+Braithwaite, M., Sims, C.E. and Allan, N.L.UThermodynamic representations for solid/melt systems at high pressure and temperature185-188.Braithwaite, C.H., Proud, W.G. and Field, J.E.JThe shock Hugoniot properties of quartz feldspathic gneiss and amphibolite	1435-1438;Braithwaite, C.H., Proud, W.G., Field, J.E. and Guest, A.R.:The shear strength and HEL of various geological materials8Brannon, P.J., Morris, R.W., Konrad, C.H. and Asay, J.R.FShock-induced luminescence from X-cut quartz and Z-cut lithium niobate303-306"Brannon, R.M. and Chhabildas, L.C."Shock-induced vaporization of zinc201-206
Brannon, R.M.-A consistent kinetics probability (CKP) model?Brannon, R.M., Montgomery, S.T., Aidun, J.B. and Robinson, A.C.<Macro- and meso-scale modeling of PZT ferroelectric ceramics197-200=Bransky, I., Hayek, M., Halevy, D., Miller, S. and Kivity, Y.'The dynamic response of soda-lime glass567-572QFractoemission and its effect upon noise in gauges placed near ceramic interfaces	1053-1056+Bourne, N.K., Rosenberg, Z. and Field, J.E.?Surface fracture zones in shock-loaded polycrystalline ceramics493-496ISimultaneous manganin gauge and VISAR measurements of shock wave profiles849-852Bourne, N.K. and Townsend, D.-Variations in the conductivity of shocked KCl109-1121Bourne, N.K., Gray�  III, G.T. and Millett, J.C.F.+On the failure of shocked titanium diboride589-5929Bourne, N.K., Millett, J.C.F., Barnes, N. and Belcher, I.JThe deviatoric response of an epoxy resin to one-dimensional shock loading649-652;Bourne, N.K., Millett, J.C.F., Gray�  III, G.T. and Mort, P.�X-ray diffraction studies of the structures of dynamically compressed beryllium, aluminum, lithium fluoride, potassium chloride, and silicon dioxideEk, D.R. and Asay, J.R.NThe stress and strain-rate dependence of spall strength in two aluminum alloys413-418*Elert, M.L., Brenner, D.W. and White, C.T.ASome one-dimensional molecular dynamics simulations of detonation275-278=Elert, M.L., Robertson, D.H., Barrett, J.J.C. and White, C.T.XMolecular dynamics study of reaction zone properties in chemically sustained shock waves183-186=Elert, M.L., Barrett, J.J.C., Robertson, D.H. and White, C.T.gMolecular dynamics investigation of the effects of variation in energy release on detonation initiation*Elert, M.L., Swanson, D.R. and White, C.T.EMolecular dynamics simulation of shock-induced chemistry in acetylene283-286&Elert, M.L., Zybin, S. and White, C.T.IMolecular dynamics modeling of impact-induced shock waves in hydrocarbons	1406-1409(Elert, M.L., Zybin, S.V. and White, C.T.AMolecular dynamics study of shock-induced chemistry in anthracene323-326Elias, P. and Chapron, P.UExperimental techniques for measuring mass ejection from shock-loaded metallic sample645-650%Elias, P., Chapron, P. and Mondot, M.VExperimental study of the slowing down of shock-induced matter ejection into argon gasKElliott, B.C.F., Wiegand, J., Siviour, C.R., Sarsfield, H. and Petrinic, N.bAn integrated experimental-numerical method for characterisation of materials at high strain rates645-648Eloy, J.-F. and Delpuech, A.kExperimental study of photon-phonon interactions in an explosive by laser probe mass spectrometry (LPMS-25)Emery, M.H. and Gardner, J.H.ILaser driven shock instabilities in multimaterial, layered, solid targetsMThermal behavior of Fe2O3/Al thermite mixtures in air and vacuum environments956-959%Durand, M., Lalle, P. and Andriot, P."Eight beam Perot-Fabry velocimeter	1751-1754Duvall, G.E.3Shock wave research: Yesterday, today, and tomorrow=Duvall, G.E., Granholm, R.H., Bellamy, P.M. and Hegland, J.E.OEffects of temperature on the UV-visible spectrum of dynamically compressed CS2213-219Three blind men and an elephantEakins, D.E. and Thadhani, N.N.BInvestigation of shock-induced reactions in a Ni+Al powder mixtureGMechanistic aspects of shock-induced reactions in Ni+Al powder mixtures	1025-1028-Eatwell, M., Millett, J.C.F. and Bourne, N.K.aLateral stress measurements in a shock loaded silicon carbide: Shear strength and delayed failure:Eatwell, M., Millett, J.C.F., Bourne, N.K. and Meziere, Y.BThe behaviour of a glass-fibre epoxy composite during plate impact7Eden, G., Carden, M.H., Collyer, A.M. and Smith, C.P.M.9Shock wave propagation in a 3-D quartz phenolic composite217-220/Edwards, M.R., Bourne, N.K. and Millett, J.C.F.NThe effect of orientation on the spall strength of the aluminium alloy 7010-T6523-526/Edwards, M.R., Millett, J.C.F. and Bourne, N.K.vQuasistatic and shock induced mechanical response of an aluminium-zinc-magnesium alloy as a function of heat treatment557-560,Efros, B., Shishkova, N. and Beigelzimer, Y.TStructural and phase transitions in metastable systems at deformation under pressure7Eggert, J.H., Hemley, R.J., Mao, H.K. and Feldman, J.L.HRotation-vibration and intermolecular dynamics of hydrogen and deuterium�Eggert, J., Bastea, M., Reisman, D.B., Rothman, S., Davis, J.-P., Knudson, M.D., Hayes, D.B., Gray�  III, G.T., Erskine, D. and Collins, G.W.>Ramp wave stress-density measurements of tantalum and tungsten	1177-1180	1436-14398Du, J., Liu, G., Liu, Y., Wang, H., Zhang, F. and He, H.BCurrent output from sandwich-structured ferroelectric power supply167-170
Duba, A.G.Iron: What is melt?923-926\Dudin, S.V., Fortov, V.E., Gryaznov, V.K., Mintsev, V.B., Shilkin, N.S. and Ushnurtsev, A.E.VInvestigation of shock compressed plasma parameters by interaction with magnetic fieldDuffy, T.S. and Ahrens, T.J.2Hugoniot sound velocities and finite strain theoryHFree surface velocity profiles in molybdenum shock compressed at 1400��C	1079-1082@Shock compression and release of polycrystalline magnesium oxide	1107-1110Duffy, T.S.CStrength of materals under static loading in the diamond anvil cell639-644IDunbar, E., Graham, R.A., Holman, G.T., Anderson, M.U. and Thadhani, N.N.JTime-resolved pressure measurements in chemically reacting powder mixturesDunn, J.E. and Grady, D.E.5Strain rate dependence in steady, plastic shock waves359-364
Dunn, J.E.>The evolution of plastic strain in steady, plastic shock wavesDunn, J.E. and Fosdick, R.bA dissipation principle and its consequences for structured shock waves in thermoelastic materials215-2185Implications and origins of shock structure in solids21-32JDunn, J., Price, D.F., Moon, S.J., Cauble, R.C., Springer, P.T. and Ng, A.<1-10 Mbar laser-driven shocks using the JANUS laser facilityDuprey, K.E. and Clifton, R.J.>Dynamic constitutive response of tantalum at high strain rates475-478.Pressure-shear response of thin tantalum foils&Dur"�es, L., Campos, J. and Gois, J.C.?New equation of state for the detonation products of explosives385-388(Dur"�es, L., Campos, J. and Portugal, A.4Reaction path of energetic materials using Thor codeADur"�es, L., Santos, R., Correia, A., Campos, J. and Portugal, A.SInfluence of tempe<  rature on the electrical conductivity of glass under shock effectCDremov, V.V., Kutepov, A.L., Petrovtsev, A.V. and Sapozhnikov, A.T.+Equation of state and phase diagram of iron87-902Dremov, V.V., Sapozhnikov, A.T. and Smirnova, M.A.bWide range equation of state of water taking into account evaporation, dissociation and ionization0Dremov, V.V., Sapozhnikov, P.A. and Bringa, E.M.hMolecular dynamics simulation of interaction between shock wave and high-symmetry intergranular boundary;Dremov, V.V., Karavaev, A.V., Kutepov, A.L. and Soulard, L.cMolecular dynamics simulation of thermodynamic and mechanical properties of beryllium and magnesium!Drennov, O.B. and Mikhailov, A.L._About formation of contact boundary between two metals in unsteady conditions of oblique impactBDrennov, O.B., Mikhaylov, A.L., Nizovtsev, P.N. and Raevskii, V.A.rGrowth of perturbations on metals interfaces at oblique collision with supersonic velocity of contact point motion@Drennov, O.B., Davydov, A.I., Mikhaylov, A.L. and Raevskii, V.A.jShear 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. and Dreger, Z.A..Recent high pressure photoluminescence studies	1491-1494<Drodge, D.R., Addiss, J.W., Williamson, D.M. and Proud, W.G.'Hopkinson bar studies of a PBX simulant513-516Drumheller, D.S.JA theory for the shock-loading response of an alumina-filled epoxy mixture527-528 Drumheller, D.S. and Grady, D.E.9The dynamic response of porous calcium carbonate minerals309-3130The role of distention in reacting porous solids-Drummond, N.D., Swift, D.C. and Ackland, G.J.#Ab initio model of porous periclaseVPost-shock chemical and ESR analysis of acrylamide and selected anthracene derivatives423-4253Dodson, B.W., Venturini, E.L. and Rogers�  Jr., J.W.GSubthreshold generation of free radicals in shock-loaded organic solids897-901 Dodson, B.W. and Bosclough, M.S./Techniques for recovery of shock-loaded samples767-769jDoherty, R.M., Forbes, J.W., Lawrence, G.W., Deiter, J.S., Baker, R.N., Ashwell, K.D. and Sutherland, G.T.CDetonation velocity of melt-cast ADN and ADN/nano-diamond cylindersDolan, D.H. and Gupta, Y.M.FTime-dependent freezing of water under multiple shock wave compression167-171&Dolgoborodov, A.Y. and Marshakov, V.N.LInvestigation of shock wave impulse influence on solid propellant combustion868-871ADonahue, L., Ripley, R.C., Horie, Y., Jenkins, C.M. and Zhang, F.2Cylindrical explosive dispersal of metal particles365-3685Dong, Q.-D., Zhang, J.-C., Liu, G.Z. and Jiang, H.-Z.3Fusion produced by implosion of spherical explosiveDoukas, A.G.?Pressure waves in medicine: From tissue injury to drug delivery	1431-1435Drake, R.P. and Reighard, A.B.BContext and theory for planar radiative shock experiments in xenon	1417-14208Dreger, Z.A., Gruzdkov, Y.A., Gupta, Y.M. and Dick, J.J.CTime-resolved emission spectroscopy in shocked PETN single crystalsDreger, Z.A.gOptical response of molecular crystals to non-hydrostatic compression in diamond anvil cell experiments	1233-1238Dreger, Z.A. and Gupta, Y.M.BRaman spectroscopy of RDX single crystals under static compression	1239-1242Dremin, A.N. and Babare, L.V..The shock wave chemistry of organic substances27-41Dremin, A.N. and Molodets, A.M.'Metal spall and fracture micromechanism415-420,Dremin, A.N., Orlov, A.V. and Molodets, A.M.1Elastic precursor decay in HMX explosive crystalsBDickson, P.M., Asay, B.W., Henson, B.F., Fugard, C.S. and Wong, J.YMeasurement of phase change and thermal decomposition kinetics during cookoff of PBX 9501837-840IDickson, P.M., Parker, G.R., Smilowitz, L.B., Zucker, J.M. and Asay, B.W.6Frictional heating and ignition of energetic materials;Dienes, J.K., Middleditch, J., Zuo, Q.H. and Kershner, J.D.3On the role of crack orientation in brittle failure447-4503Dietenberger, M.A., Rajendran, A.M. and Grove, D.J.NA use of microphysical fracture model to describe ceramic material upon impact457-4602Dietenberger, M.A., Antoun, T. and Rajendran, A.M.eSimulation of uniaxial stress-strain curves for arbitrary strain rates and confining stress histories265-268Ding, J.,A description of shock wave in the year 1637Ding, J.-L. and Hayes, D.-Phase transformation rate in shock-loaded KClDionne, J.P. and Lee, J.H.S.=Modeling the detonation structure of heterogeneous explosives317-3206Divakov, A.K., Khantuleva, T.A. and Mescheryakov, Y.I.QKinetics of mesostructure and reloading behavior of dynamically compressed solids553-556Dlott, D.D.9Ultrafast vibrational energy transfer in molecular solids709-7182Dobler, E.A., Gryadunov, A.N. and Shteinberg, A.S.BOn the possible gas detonation explosion of BaO2/Zr powder mixtureDodson, B.W. and Graham, R.A.Shock-induced organic chemistry42-51Dodson, B.W.RAn exploratory study of reactivity in organic compounds subjected to shock loading62-66 Dodson, B.W. and Venturini, E.L.(Shock-induced defects in cadmium sulfide335-339Dodson, B.W. and Taylor, P.A.6Monte Carlo simulation of shock-induced lattice damage395-396@Dodson, B.W., Arnold�  Jr., C., Venturini, E.L. and Lenahan, P.M.vUse of explosive energy for the production of multilayered composites from high Tc superconductive ceramics and metalsDesgreniers, S. and Legault, R.4High density crystalline structures of copper oxides	Dey, T.N.>Effective stress model for partially and fully saturated rocksDey, T.N. and Johnson, J.N.0Shear band formation in plastic bonded explosive
Dick, J.J.>Plane shock intiation on gamma-irradiated PETN single crystals@Pop plot and Arrhenius parameters for <110> PETN single crystals903-907'Stress-strain histories in shocked PMMA*Dick, J.J., Pettit, D.R. and Spencer, W.J.?Crystal orientation effects in PETN explosive with 4 GPa shocks713-715%Dick, J.J., Garcia, E. and Shaw, D.C.EShock initiation of PETN crystals: Steric effects due to plastic flow349-3527Dick, R.D., Williams, J.D., Young, C. and Lottero, R.E.*Blast pressure measurement from explosives*Dick, R.D., Fourney, W.L. and Weaver, T.A.PEffects of open joints and weak layers on wave propagation in geologic materials.Dick, J.J., Whitehead, M.C. and Martinez, A.R.\Crystal orientation dependence of elastic precursor strength in pentaerythritol tetranitrate,Dick, R.D., Fourney, W.L. and Williams, J.D.0Response of NTS tuff to high strain rate loading153-156:Orientation-dependent shock response of explosive crystals815-818.Dick, R.D., Armstrong, R.W. and Williams, J.D.3Split Hopkinson pressure bar tests on pure tantalum471-474 Dick, J.J. and 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. and Fourney, W.L.>High strain rate loading of polymeric foams and solid plasticsjStress-strain response of PBX 9501 below 1 GPa from embedded magnetic gauge data using Lagrangian analysisDick, J.J. and Martinez, A.R.HEvidence for kinetic effects on shock wave propagation in tectosilicates	1381-13844DeCarli, P.S., Weaver, C.A., Xie, Z. and Sharp, T.G.ZMeteorite studies illuminate phase transition behavior of minerals under shock compression	1427-14306DeCarli, P.S., El�  Goresy, A., Xie, Z. and Sharp, T.G.*Ejection mechanisms for Martian meteoritesDehn, J.)Modeling armor that uses interface defeatEDein, J., Tokheim, R., Curran, D., Chau, H., Weingart, R. and Lee, R.2Aluminum damage simulation in high-velocity impact171-174Dekel, E. and Rosenberg, Z.<More on the transition from rigid to eroding-rod penetr< ation	1327-1330Delpuech, A. and Menil, A.<Raman scattering temperature measurement behind a shock wave)Delpuech, A., Mentil, A. and Pouligny, B.YRaman scattering temperature measurement behind a shock wave: A study of solid explosives877-882Demmie, P.N.GModeling and simulation of explosively driven electromechanical devices'Demol, G., Goutelle, J.C. and Mazel, P.fCHARME: A reactive model for pressed explosivves using pore and grain size distributions as parametersDemol, G. and Sandusky, H.W.HPhysical and chemical microstructural damage in pressed CL-20 explosives+Demske, D.L., Forbes, J.W. and Tasker, D.G.mHigh current electrical resistance of PBX-9404 and dielectric breakdown measurements of naval high explosives?Demske, D., Brazell, N., Farley, W.E., Pogue, E. and Warnes, R.CIntense electron beam detonation of insensitive energetic materials(Denoual, C., Cottenot, C.E. and Hild, F.=Analysis of the degradation mechanisms in an impacted ceramicDenoual, C. and Diani, J.M.1Cavitation in compressible viscoplastic materials0Derbenev, I.V., Dremov, V.V. and Nikitenko, Y.R.AMolecular dynamics simulation of hot spots in energetic materials569-572Deribas, A.JEffect of metal particle size on blast performance of RDX-based explosives950-953Davis, J.-P. and Hayes, D.B.CIsentropic compression experiments on dynamic solidification in tin4Measurement of the dynamic b-g phase boundary in tin(Davison, L., Webb, D.M. and Graham, R.A.<Analysis of capsules for recovery of shock compressed matter67-71Davison, L./Numerical modeling of dynamic material response181-186Davison, D.USensing the threshold for initiation of high explosives in hydrodynamics calculations<Traditional analysis of nonlinear wave propagation in solids20-25.de�  Resseguier, T., Cottet, F. and Migault, A.>A 1D model for glass dynamic behaviour under explosive loading	1071-10746de�  Ress"�guier, T., Berterretche, P. and Hallouin, M.EEvidence of anisotropic wave propagation in laser shock-loaded quartz$de�  Ress"�guier, T. and Hallouin, M.BPhase transformation and spall fracture in laser shock-loaded ironHde�  Ress"�guier, T., Signor, L., Dragon, A., Severin, P. and Boustie, M.WTransition from solid to liquid spall in tin under laser shocks of increasing intensityDear, J.P. and Field, J.E.XAn investigation of the shock structures and conditions for jetting during liquid impact667-6723Deas, D., Millett, J.C.F., Bourne, N.K. and Kos, K.2The shock Hugoniot of two alumina-epoxy composites693-696*Deas, D., Millett, J.C.F. and Bourne, N.K.AThe shock induced equation of state of two ferroelectric ceramics851-854)Deb, S.K., Meenakshi, S. and Godwal, B.K.0High pressure Raman studies on p-dichlorobenzene	1531-1534
DeCarli, P.S.1Were carbonados synthesized by an ancient impact?757-7605More on the possibility of impact origin of carbonadoCDeCarli, P.S., Bowden, E., Sharp, T.G., Jones, A.P. and Price, G.D.;Daswani, J.M., Gupta, S.C., Sikka, S.K. and Chidambaram, R.KTheoretical analysis of the isostructural transition in zirconium at 53 GPayDattelbaum, D.M., Robbins, D.L., Sheffield, S.A., Orler, E.B., Gustavsen, R.L., Alcon, R.R., Lloyd, J.M. and Chavez, P.J.MQuasistatic and shock compressive response of fluorinated polymers: Kel-F 800HDattelbaum, D.M., Stevens, L.L., Orler, E.B., Ahart, M. and Hemley, R.J.ZBrillouin scattering determination of the acoustic properties of polymers at high pressure39-42Davidson, R.F. and Walsh, M.L.1Constitutive modeling for hypervelocity cratering	1159-1162;Davies, F.W., Smith, E.A., Martinez, A.A. and Gaffney, E.S. Wave propagation in jointed rock7Davies, F.W., Reeder, D.L., Johnson, D.E. and Lee, L.M.bThe derivation of material properties from measurements of radiation induced stress-time histories	1273-1276'Davis, J.F., Furlong, J.R. and Alme, M.ECeramics behavior at stress levels characteristic of ballistic impactDavis, J.J.]The effect of an electric field on the high strain rate properties of polymethyl methacrylate	1131-1134Davis, L.L. and Brower, K.R.=A study of organic reactions driven by shock waves in liquidsDavis, J.J. and Lindfors, A.J.PInert Hugoniot for a porous titanium-Teflon mixture: Experiment and calculations)Shock initiation chemistry of nitroarenes699-702)Davis, J.J., Woody, D.L. and Miller, P.J.9Shock and impact initiation of a porous incendiary device,Davis, L.L., Sheffield, S.A. and Engelke, R.*Detonation properties of bromonitromethane785-788Davis, L.L. and Hill, L.G.ANFO cylinder tests165-168RDavis, J.-P., Hayes, D.B., Asay, J.R., Watts, P.W., Flores, P.A. and Reisman, D.B.WInvestigation of liquid-solid phase transition using isentropic compression experiments221-224Davis, J.J. and Miller, P.J.Shock response of Ti-6Al-4VDandekar, D.P. and Grady, D.E.@Shock equation of state and dynamic strength of tungsten carbide783-786FA re-examination of two-step lateral stress history in silicon carbide731-734Dandekar, D.P. and Prakash, V.8Effect of shock induced shear on spall strength of SiC-N/Dandekar, D.P., Vaughan, B.A.M. and Proud, W.G.%Shear strength of aluminum oxynitride Dandrea, R.G. and Ashcroft, N.W.5Theory of the high temperature shocked metallic state57-69IDaniels, W.B., Lipp, M., Strachan, D., Yoo, C., Zhang, H.M. and Yu, Z.-H.PNonlinear optics probes of ultraviolet energy levels of solids at high pressures	1499-1502
Daniels, W.B.@Use- and diamond-friendly method of rounding diamond anvil edges	1617-1618/Danker, G.R., Newlander, C.D. and Colella, N.J.JAnalytical modeling of dynamic tensile behavior in loaded Vamac elastomers213-2165Dannemann, K.A., Lankford�  Jr., J. and Nicholls, A.E.bThe mechanism of strain rate strengthening during dynamic compression of closed-cell aluminum foamRDannemann, K.A., Lankford�  Jr., J., Nicholls, A.E., Vaidyanathan, R. and Green, C.RDynamic compression of aluminum foam processes by a freeform fabrication techniqueQDanson, C., Bann, R., Hardie, D., Pepler, D., Ross, I., Sails, S. and Woolsey, N.7Uniform focal profiles suitable for laser driven shocks&Daraio, C., Nesterenko, V. and Jin, S.0Strongly nonlinear waves in 3D phononic crystals7Daraio, C., Nesterenko, V.F., Herbold, E.B. and Jin, S.;Strongly nonlinear waves in polymer based phononic crystalsDaraio, C. and Nesterenko, V.F.ZPropagation of highly nonlinear signals in a two dimensional network of granular materials*Das, K., Bandyopadhyay, A. and Gupta, Y.M.jShock wave synthesis of titanium silicide. 1: Effects of impact velocity, milling time and compact density	1094-1097HLinks between the morphology of RDX crystals and their shock sensitivityd'Almeida, T. and Gupta, Y.M.9X-ray diffraction measurements in KCl shocked along [100]113-116$Dai, C., Eakins, D. and Thadhani, N.[On the applicability of analytical models to predict Hugoniot of nano-sized powder compacts
Dallman, J.C.(Absorption spectra of shocked liquid CS2231-235*Dally, J.W., Dick, R.D. and Williams, J.D. Dynamic loading with a short bar755-758�Dalton, D.A., Brewer, J., Bernstein, A.C., Grigsby, W., Milathianaki, D., Jackson, E., Adams, R., Rambo, P., Schwarz, J., Edens, A., Geissel, M., Smith, I., Taleff, E. and Ditmire, T.HLaser-induced spall of aluminum and aluminum alloys at high strain ratesDamamme, G.-The divergent quasistationary detonation waveUA new method to simulate shocks, detonations and transitions from shock to detonation575-577GDan, K., Tamura, H., Sawaoka, A.B., Mori, T., Hwang, M.D. and Horie, Y.ZMicrostructures of single-crystal copper rods shock-treated by a rod-in-cylinder technique Dandekar, D.P. and Lamothe, R.M.<  ?Shock, re-shock, and release behavior of a phenolic resin FF-17125-128 Dandekar, D.P. and Lopatin, C.M.0Shock response of SiC/2014-T4 aluminum composite365-369)Dandekar, D.P., Gaeta, P.J. and Horie, Y.?Double shock and release experiments in PMMA and Z-cut sapphireDandekar, D.P. and Hankin, M.EDeformation of a polyvinyl based elastomer subjected to shock loadingDandekar, D.P.;Effect of shock re-shock on spallation of titanium diboride-Response of ceramics under shock wave loading729-732!Dandekar, D.P. and Bartkowski, P.Shock response of AD995 aluminadExperimental technique to measure tensile impedance of a material under plane shock wave propagation7Shock, release, and tension response of soda lime glass!Dandekar, D.P. and Spletzer, S.V.^Effect of nano-void on the phase transformation of single crystal iron under shock compression155-158)Shock recovery experiments: An assessment407-414.Gray�  III, G.T., Hixson, R.S. and Morris, C.E.'Bauschinger effect during shock loadingSInfluence of peak pressure and temperature on the shock-loading reponse of tantalum	1103-1106,Shock loading response of advanced materialsBTemperature and deformation microstructure in the shock transition363-367IHigh pressure release wave measurements and phase transformation in CaCO3589-593<A strain-rate dependent spall mechanism transition in metalsGrady, D.E. and Furnish, M.D.NHugoniot and release properties of a water-saturated high silica content grout/Shock wave properties of high-strength ceramics455-458BImpact strength and indentation hardness of high-strength ceramics'Shock-wave properties of brittle solids	Grady, D.TDifferential Hugoniot and experimental estimate of the Gr"�neisen parameter for SiO2gShock profile studies on selected silicon carbide ceramics with application to dynamic yield mechanisms;Spall properties of Solenhofen limestone and Dresser basaltLFragmentation of expanding cylinders and the statistical theory of N.F. MottSAnalytic solutions and constitutive relations for shock propagation in porous media1The statistical fragmentation theory of N.F. Mott455-460.Solutions of spall and fragmentation of solidsThe shock wave profile+Graf, M.J., Greeff, C.W. and Boettger, J.C.GHigh-pressure Debye-Waller and Gr"�neisen parameters of gold and copperGraham, R.A.%The electrical-to-chemical connection52-56Graham, R.A. and Webb, D.M.LFixtures for controlled explosive loading and preservation of powder samplesdGraham, R.A., Morosin, B., Horie, Y., Venturini, E.L., Boslough, M., Carr, M.J. and Williamson, D.L.4Chemical synthesis under high pressure shock loading693-711Graham, R.A. and Carr, M.J.FAnalytical electron microscopy study of shock synthesised zinc ferrite803-808KShock-induced temperature distributions in powder compact recovery fixtures831-836EShock compression of solids as a physical-chemical-mechanical process(Graham, R.A., Morosin, B. and Bush, D.M.CSteady-state model of heterogeneous detonation with inert particles423-426Gonor, A.L. and Hooton, L.E.rShock wave diffraction over an inclusion in condensed matter and hot spot generation at the particle surface in HE955-958Gonor, A. and 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	1379-13826Gonthier, K.A., Menikoff, R., Son, S.F. and Asay, B.W.NModeling energy dissipation induced by quasi-static compaction of granular HMX289-292Gonthier, K.A. and Son, S.F.?Modeling compaction induced energy localization in granular HMXGoto, T. and Syono, Y.%Shock-induced phase transition in GaP320-324 Gourdin, W.H. and Weinland, S.L.1Hugoniot measurements on unsintered metal powders99-104
Gourdin, W.H.TPrediction of microstructural modification in dynamically consolidated metal powders;Dynamic compaction of a monosized spherical tungsten powder725-730YMetallurgical effects on the constitutive and fragmentation behavior of OFHC copper rings351-354.Gourdin, W.H., Weinland, S.L. and Boling, R.M.LElectromagnetic ring expansion as a high-rate test: Experimental developmentGourdin, W.H. and Lassila, D.H.WDeformation behavior of pre-shocked copper as a function of strain rate and temperatureGMultiple mechanisms in the thermally activated plastic flow of tantalum9Goveas, S.G., Millett, J.C.F., Bourne, N.K. and Knapp, I.TOne-dimensional shock and detonation characterization of ultrafine hexanitrostilbene.Goveas, S.G., Bourne, N.K. and Millett, J.C.F.EThe strength of polyethylene and polyoxymethylene under shock loadingGrady, D.E.1Fragment size prediction in dynamic fragmentation456-459MNonhydrostatic effects in stress-wave induced phase transformation of calciteAThree-dimensional displacement measurements ahead of a projectile	1095-1098;Goldrein, H.T., Grantham, S.G., Proud, W.G. and Field, J.E./Counihan, P.J., Crawford, A. and Thadhani, N.N._Nanostructure formation by dynamic densification and recrystallization of amorphous Ti-Si alloy'Cour-Palais, B.G. and Piekutowski, A.J.+The multi-shock hypervelocity impact shield979-982Cour-Palais, B.G.ASpacecraft outer thermal blankets as hypervelocity impact bumpers	1175-1178*Courchinoux, R., Chapron, P. and Elias, P.`Particle velocity profiles measured by LDI through a LiF window in loading-unloading experiments771-774Courchinoux, R. and Lalle, P.&Unreacted Hugoniot of ammonium nitrate	1397-1400@Dynamic properties of water: Sound velocity and refractive index61-64OCouturier, S., Boustie, M., de�  R"�ss"�guier, T., Hallouin, M. and Romain, J.P.gLaser driven shock pressure measurements by VF2/VF3 and PVDF gages for pulses of 2.5ns up to 1012 w/cm2	1097-1100!Cowperthwaite, M. and Gupta, Y.M.9Investigation of shear induced reaction in composition B3863-869Cowperthwaite, M.=An analytic analysis for the tension-recompression experiment585-588jAn investigation of the response of secondary explosives to conical-tipped projectiles and oblique impacts	1421-14247Projectile impact initiation of a homogeneous explosivedThe development of a new Arrhenius-basd burn model for both homogeneous and heterogeneous explosivesQCook, M.D., Haskins, P.J., Briggs, R.I., Cheese, P., Stennett, C. and Fellows, J.LHigh speed observation of fragment impact initiation of nitromethane chargesSCook, M.D., Haskins, P.J., Briggs, R.I., Stennett, C., Fellows, J. and Cheese, P.J.@Fragment impact characterization of melt-cast and PBX explosives	1047-1050RCook, M.D., Stennett, C., Haskins, P.J., Briggs, R.I., Wood, A.D. and Cheese, P.J.QThe role of binders in controlling the cook-off violence of HMX/HTPB compositions952-955*Cooper, T., Rosenberg, G. and Curran, D.R.dUtilization of shock wave concepts to improve ballistics modeling for armor penetration by long rodsVCooper, G.A., Longbottom, A.W., Bourne, N.K., Milne, A.M., Murray, I. and Hollands, R.APlate impact study of the shock to detonation transition in a PBX>Cooper, G.A., Millett, J.C.F., Bourne, N.K. and Dandekar, D.P.)Delayed failure in a shock loaded alumina847-850Corey, E.M. and Young, D.A..A new prototype equation of state data library43-46CCorley, J., Riedel, W., Hiermaier, S., Weidemaier, P. and 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. and Mydosh, J.A.RHigh pressure studies on the ferromagnetic dense Kondo systems CeRh3B2 and UCu2Ge2	1457-1460bCornish, R., Porter, D., Church, P., Gould, P., Andrews, T., Proud, B., Drodge, D. and Siviour, C.WComparison of Porter< -Gould constitutive model with compression test data for HTPB/sugar777-780GCogar, J.R., Robinson, N., Tsembelis, K., Proud, W.G. and Cross, D.L.A.1Shock Hugoniot data for low density silica powder	1090-1093Cohen, R.E. and Gong, Z.,Melting and melt structure at high pressures379-3827Cohen, R.E., Stixrude, L. and Papaconstantopoulos, D.A.tAn 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. and Ng, A.,Equation of state measurements of D2 on NOVA55-60&Collins, A., Chapman, D. and Proud, W.Front face spall of concreteColvin, J.D. and Kalantar, D.H.ZScaling of pressure with intensity in laser-driven shocks and effects of hot X-ray preheat	1413-1416Colvin, J.D.BModeling dynamic ductility: An equation of state for porous metals31-34�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. and Asay, J.R.?Use of Z-pinch sources for high pressure shock wave experiments997-10006Conroy, M., Oleynik, I.I., Zybin, S.V. and White, C.T.KAnisotropic constitutive relationships in energetic materials: PETN and HMX361-364"Constantinou, C.P. and Gupta, Y.M.NMicrowave interferometric hot spot density measurements in energetic materialsGlenn, L.A.;Shock attenuation in an inertial confinement fusion reactor510-514*Glenn, H.D., Rambo, J.T. and Terhune, R.W. Calculational study of Baneberry.Seismic verification of underground explosions613-620.Glenn, H.D., Stubbs, T.F. and Kalinowski, J.A.6Ground motion measurements for the QUESO nuclear event3Performance analysis of the two-stage light gas gun.Glenn, L.A., Latter, A.L. and Martinelli, E.A.Multistage gasdynamic launchers977-984&Partially decoupled explosion cavitiesaThe influence of rock material models on seismic discrimination of underground nuclear explosions343-3463Optimization studies of a three-stage light gas gunDOn improving the penetration of commercial shaped charge perforators>Glushak, B.L., Novikov, S.A., Sinitsyna, L.M. and Yukina, N.A.GPeculiarities of metal balls deformation by quasi-spherical shock waves513-515}Glushak, B.L., Ignatova, O.N., Nadezhin, S.S., Nizovtsev, P.N., Podurets, A.M., Raevsky, V.A., Zocher, M.A. and Preston, D.L._A phenomenological viscoplastic constitutive model for M1 copper acounting for grain morphology�Using laser induced shock waves to investigate the nanoparticle transition from bulk behavior to discrete atom/finite size behaviorIGerward, L., Olsen, J.S., Benedict, U., Dancausse, J.-P. and Heathman, S.WHigh-pressure X-ray diffraction studies of ThS2, US2, and other AnX2 and AnXY compounds Getting, I.C. and Spetzler, H.A.<Gas-charged piston-cylinder apparatus for pressures to 4 GPa	1581-1584Ghose, J. and Roy, A.Optical studies on Rh2O3,Gifford, M.J., Luebcke, P.E. and Field, J.E.ZA mechanism for the deflagration-to-detonation transition in ultrafine granular explosives*Gifford, M.J., Proud, W.G. and Field, J.E.>Observations on type II deflagration-to-detonation transitions878-881Giles, A.R. and Maw, J.R.LModelling the temperature and strain rate dependence of spallation in metals243-246Gilev, S.D. and Trubachev, A.M.UShock-induced conduction waves in solids and their applications in high power systemsLA study of semiconductor-metal transition in shocked monocrystalline siliconGilman, J.J.'Dynamics at detonation fronts in solidsThe plastic wave myth387-389 Gilman, J.J. and Armstrong, R.W.'Shear-induced polymerization of benzene!Strain induced chemical reactions	1349-1352*Topology of phase changes via bond-bending215-219DDeformation potentials and plasmon energies: Measures of sensitivity313-3160Plasmon diagnosis of shock and detonation frontsMechanical states of solids36-41+Cohesion in ball lightning and Cook plasmas	1257-1260-Bond modulus and stability of covalent solids855-8571Gilmore, M.R., Foster�  Jr., J.C. and Wilson, L.L.7Dynamic fracture studies using sleeved Taylor specimens519-522>Gilmore, M.R., Foster�  Jr., J.C., Wilson, L.L. and Jones, S.E.The generalized Taylor test	1331-1334HHugoniot measurements in vanadium using the LLNL two-stage light-gas gun89-90 Gathers, G.R. and Mitchell, A.C.SHugoniot measurements in aluminum to 420 GPa using the LLNL two-stage light-gas gun151-155NGathers, G.R., Osher, J.E., Chau, H.H., Weingart, R.C., Lee, C.G. and Diaz, E.9Release isentrope measurements with the LLNL electric gun175-1789Gathers, G.R., Chau, H.H., Osher, J.E. and Weingart, R.C.9Hugoniot measurements with the LLNL electric gun facilityHHugoniot measurements on a slurry of finely divided tungsten and plastic83-85MGautier, L., Belmas, R., Bry, A., Poullain, D., Picart, D. and Le�  Gallic, C.=Influence of thermal cycles on a TATB composition sensitivity4Gefken, P., Curran, D., Nesterenko, V.F. and Cai, J.�The explosive spherical cavity expansion for characterization of SiC-N ceramic dynamic behavior and post shock damage using RUS methodVGehr, R.J., Bucholtz, S.M., Rupp, T.D., Robbins, D.L., Stahl, D.B. and Sheffield, S.A.QLine ORVIS particle velocity measurements on the laser-driven miniflyer apparatus	1163-1166Gerin-Roze, J. Unusual self-similar compression	1515-15184Self-similar compression flows in spherical geometry(Germain-Lacour, M. and de�  Gliniasty, M.Ramp-wave generators studies481-485>German, V.N., Mikhailov, A.L., Osipov, R.S. and Tsyganov, V.A.9Structural transitions in solids under shock-wave loading247-250-Germann, T.C., Holian, B.L. and Lomdahl, P.S.EPlastic deformation in shock waves via molecular dynamics simulations
Germann, T.C.mLarge-scale molecular dynamics simulations of shock-induced plasticity, phase transformations, and detonation0Germann, T.C., Hammerberg, J.E. and Holian, B.L.HLarge-scale molecular dynamics simulations of ejecta formation in copperGerstman, B.S.�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. and Tierney�  IV, T./Shock response of iron on nanosecond timescales	1385-13883Gang, Y., Sun, C.-W., Ghang-Quan, Z. and Tang, Z.P.IMeasurements of laser induced stress waves by eddy-current velocity gauge925-927$Gao, J.-X., Bai, R.-S. and Cheng, C.1Measurement of temperature in shock-loaded solids639-642Gao, X.-Z. and Ding, J.WShock Hugoniot of porous materials in the completely and incompletely compacted regions1Gao, J.-X., Deng, R.-G., Xu, X.-H. and Rao, X.-L.7Effect of shock wave activation on nitriding of Sm2Fe17Garcia, B.O. and Chavez, D.J.%Shock compression of liquid hydrazineZGarcia, F., Forbes, J.W., Tarver, C.M., Urtiew, P.A., Greenwood, D.W. and Vandersall, K.S.XPressure wave measurements from thermal cook-off of an HMX-based high explosive PBX 9501882-885JGarcia, F., Vandersall, K.S., Forbes, J.W., Tarver, C.M. and Greenwood, D.`Pressure wave measurements resulting from thermal cook-off of the HMX based high explosive LX-04tThermal cook-off experiments of the HMX-based high explosive LX-04 to characterize violence with varying confinement;Garcia, F., Vandersall, K.S., Tarver, C.M. and Urtiew, P.A.tShock initiation experiments on the LLM-105 explosive RX-55-AA at 25��C and 150��C with ignition and growth modelingeGarmasheva, N.V., Filin, V.P., Loboiko, B.G., Averin, A.N., Mathieu, D., Simonetti, P. and Belmas, R.=Modeling and prediction of sensitivity in energetic materials439-441<  2Garrett, G.R., Chhabildas, L.C. and Reinhart, W.D.Shock compression of liquids81-842Garrett�  Jr., R.K., Rajendran, A.M. and Last, H.R.1Modeling spall in HY100, HY130, and AF1410 steels.Gathers, G.R., Mitchell, A.C. and Holmes, N.C.DFurnish, M.D., Chhabildas, L.C., Setchell, R.E. and Montgomery, S.T.DDynamic electromechanical characterization of axially poled PZT 95/5^Furnish, M.D., Robbins, J., Trott, W.M., Chhabildas, L.C., Lawrence, R.J. and Montgomery, S.T.>Multi-dimensional validation impact tests on PZT 95/5 and ALOX205-208QFurnish, M.D., Trott, W.M., Mason, J., Podsednik, J., Reinhart, W.D. and Hall, C.LAssessing mesoscale material response via high-resolution line-imaging VISARMFurnish, M.D., Reinhart, W.D., Trott, W.M., Chhabildas, L.C. and Vogler, T.J.\Variability in dynamic properties of tantalum: Spall, Hugoniot elastic limit and attenuation^Furnish, M.D., Vogler, T.J., Alexander, C.S., Reinhart, W.D., Trott, W.M. and Chhabildas, L.C.8Statistics of the Hugoniot elastic limit from line VISARGaeta, P.J. and Dandekar, D.P.&Shock response of Kennertium grade W-2269-272Gaffney, E.S. and Brown, J.A.EComparative response of alluvium to Hopkinson bar and gas gun loading621-626
Gaffney, E.S.BGeneration of 2 MHz plane-strain sine waves by 3D quartz compositeBGahagan, K.T., Reho, J.H., Moore, D.S., Funk, D.J. and Rabie, R.L.`Ultrafast time-resolved 2D spatial interferometry for shock wave characterization in metal films	1351-1354Gailly, B. and Petit, J.7Influence of the microstructure on armor steel spalling/Galbraith, S.D., Rosenberg, Z. and Bourne, N.K.RThe determination of the reverse phase transition b2-b1 stress in shock loaded KCl219-222HGallagher, K.G., Bass, J.D., Ahrens, T.J., Fitzner, M. and Abelson, J.R.tShock temperature of stainless steel and a high pressure-high temperature constraint on thermal diffusivity of Al2O3*Gallagher, K.G., Yang, W. and Ahrens, T.J./Free-surface light emission from shocked Teflon	1551-1554TGamache, R.M., Drotar, J.T., Lee, R.J., Callahan, J.H., Evans, T.W. and Turner, N.H.=Stability field of the orthorhombic perovskite type of MgSiO3791-7946Funk, D.J., Laabs, G.W., Peterson, P.D. and 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. and Yuan, V.W.GDynamic measurement of temperature using neutron resonance spectroscopyQFunk, D.J., Moore, D.S., Reho, J.H., Gahagan, K.T., McGrane, S.D. and Rabie, R.L.WUltrafast measurement of the optical properties of shocked nickel and laser heated gold	1227-1230xFunk, D.J., Meserole, C.A., Hof, D.E., Fisher, G.L., Roberts, J., Taylor, A.J., Lee, H.J., Workman, J. and McCulloch, Q.EAn ultrafast X-ray diffraction apparatus for the study of shock waves*Furnish, M.D., Grady, D.E. and Brown, J.M.FAnalysis of shock wave structure in single-crystal olivine using VISAR595-599
Furnish, M.D.@Dynamic compression and release experiments on Indiana limestone625-628DFurnish, M.D., Chhabildas, L.C., Steinberg, D.J. and Gray�  III, G.T.*Dynamic behavior of fully dense molybdenum-Furnish, M.D., Gray�  III, G.T. and Remo, J.L.<Dynamical behavior of octahedrite from the Henbury meteorite3Furnish, M.D., Chhabildas, L.C. and Steinberg, D.J.Dynamical behavior of tantalum	1099-1102Furnish, M.D. and Ito, E.;Experimental measurements of shock properties of stishovite93-96BFurnish, M.D., Lassila, D.H., Chhabildas, L.C. and Steinberg, D.J.WDynamic material properties of refractory metals: Tantalum and tantalum/tungsten alloys"Furnish, M.D. and Chhabildas, L.C.2Alumina strength degradation in the elastic regimezA reaction zone enthalpy balance model to simulate shock-to-detonation transition and unsteady detonation wave propagation%Frost, D.L., Aslam, T. and Hill, L.G.zApplication of detonation shock dynamics to the propagation of a detonation in nitromethane in a packed inert particle bedsFrost, D.L., Zhang, F., McCahan, S., Murray, S.B., Higgins, A.J., Slanik, M., Casas-Cordero, M. and Ornthanalai, C.FNear-field impulse effects from detonation of heterogeneous explosives946-949NFrost, D.L., Goroshin, S., Janidlo, S., Pryszlak, J., Levine, J. and Zhang, F.GFragmentation of reactive metallic particles during impact with a plate451-454?Frost, D.L., Goroshin, S., Levine, J., Ripley, R. and Zhang, F.WCritical conditions for ignition of aluminum particles in cylindrical explosive charges972-9753Frost, D.L., Cairns, M., Goroshin, S. and Zhang, F.MReaction of titanium and zirconium particles in cylindrical explosive charges781-784+Frutschy, K.J., Clifton, R.J. and Mello, M.OHigh-temperature pressure-shear plate impact studies on OFHC copper and pure WC463-466"Fu, R., Lindfors, A. and Davis, J.Scaling for internal blast	1440-1443-Fuchs, B.E., Droughton, J. and Persson, P.-A.-Modifications to Oh-Persson equation of state7Fugelso, E., Jacobson, J.D., Karpp, R.R. and Jensen, R.9Radiographic study of impact in polymer-bonded explosives607-611/Fujishiro, I., Nakamura, Y. and Yamanokuchi, H.qEvaluation of temperature dependence on ruby fluorescence at high pressure by viscosity measurement of lubricants	1059-1062Fuka, M.Z. and Prentice, J.K.8Interactive mesh generation in solid dynamics hydrocodes297-300'Fukunaga, O., Iizuka, M. and Sugano, T.NFormation pressure temperature region of diamond using alloy solvent catalysts1Funamori, N., Yagi, T., Uchida, T. and Utsumi, W.eInvestigation of thin laser-driven flyer plates using streak imaging and stop motion microphotography	1209-1212
Frankel, M.J.<Pressure dependent vibronic relaxation in shocked explosives593-597)Franken, J., Hambir, S.A. and Dlott, D.D.BPicosecond vibrational spectroscopy of shocked energetic materials@Fredenburg, D.A., Vogler, T.J., Saldana, C.J. and Thadhani, N.N.LShock consolidation of nanocrystalline aluminum for bulk component formation*Freim, J., McKittrick, J. and Nellis, W.J.-Shock compaction of alumina/zirconia ceramics	1263-1266Fried, L.E. and Tarver, C.?Molecular dynamics simulation of shocks in porous TATB crystalsFried, L.E. and Howard, W.M.3The equation of state of HF under shock compression'Fried, L.E., Reed, E.J. and Manaa, M.R.:Simulations of fluid nitromethane under extreme conditions5Fried, L.E., Goldman, N., Kuo, I.F.W. and Mundy, C.J.0Chemistry of H2O and HF under extreme conditions18-25Fritz, J.N. and McQueen, R.G.Reflected shocks in SiO29Fritz, J.N., Morris, C.E., Hixson, R.S. and McQueen, R.G.CLiquid sound speeds at pressure from the optical analyzer technique149-152Fritz, J.N.BOvertaking wave interaction, reflected shock or reflected release?Fritz, J.N. and Kennedy, J.E.>Air cushion effect in the short-pulse initiation of explosives2The isotope effect on the Hugoniot of polyethylene?Waves at high pressure and explosive products equation of state239-244fFroeschner, K.E., Chau, H., Dittbenner, G., Lee, R.S., Mikkelson, K., Steinberg, D. and Weingart, R.C.0Shock Hugoniot experiments using an electric gun174-178:Froeschner, K.E., Lee, R.S., Chau, H.H. and Weingart, R.C.-Shock Hugoniot measurements on Ta to 0.78 TPa
Froger, A.DOn the Taylor test: A continuum analysis of plastic wave propagationAFoster�  Jr., J.C., Christopher, F.R., Wilson, L.L. and Osborn, J.DMechanical ignition of combustion in condensed phase high explosives-Foster�  Jr., J.C., Glenn, J.G. and Gunger, M.yMeso-scale origins of the low-pressure equation of state and high rate mechani<  cal properties of plastic bonded explosivesJFoster�  Jr., J.C., Jones, S.E., Toness, O., DeAngelis, R.J. and Rule, W.K.JAn analytical estimate for mass loss from a high velocity rigid penetrator	1125-1128/Foster�  Jr., J.C., Gilmore, M. and 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/Foster�  Jr., J.C., Stewart, D.S. and Thomas, K.?Multi-scale statistical design of high energy density materials369-372.Fourney, W.L., Barker, D.B. and Holloway, D.C.0Mechanisms of fragmentation in brittle materials153-158(Fourney, W.L., Wang, X.J. and Dick, R.D.)Crush zone size dependence on charge size597-600:Fowler, C.M., Peterson, D.R., Hawke, R.S. and Brooks, A.L.%Rail gun development for EOS research686-690Fowler, C.M.Magnetic flux compression53-64Fowles, G.R.Shock wave stability520-524(Frachet, V., Elias, P. and Martineau, J.bMatter ejection from shocked materials: A physical model to understand the effects of free surfaceFrachet, V. and Mercier, P.GShaped charge virtual priming centers determination by image processing	1865-1858Frank, A.M. and Gathers, G.R./Shock pressure determination in detonator wiresFrank, A.M.Mechanisms of EBW HE initiationFrank, A.M. and Chau, H.H.Six-mm, plave wave shock driver	1651-1654Frank, A.M. and Trott, W.M.6Impulse time integral function and Lagrangian analysis189-192CLagrangian analysis, data covariance, and the impulse time integral317-324OIsentrope energy, Hugoniot temperature, and the Mie-Gruneisen equation of state)Forrestal, M.J., Luk, V.K. and Brar, N.S.BPerforation of aluminum armor plates with conical-nose projectiles951-953{Fortov, V.E., Bushman, A.V., Filimonov, A.S., Kvitov, S.V., Kulish, M.I., Lebedev, M.E., Polischuk, A.Y. and Ternovoi, V.Y.AOptical properties of dense plasma in shock and rarefaction wavessFortov, V.E., Efremov, V.P., Kanel, G.I., Morosov, P.V., Demidov, B.A., Lomonosov, I.V., Ni, A.L. and Vorobev, O.Y.iTheoretical and experimental investigation of shock waves generated by high energy charged particle beams,Fortov, V.E., Kostin, V.V. and Vorobev, O.Y.PGeneration of extreme states in condensed matter with high energy particle beams	1883-1886TFortov, V.E., Lebedev, M., Dyabilin, K., Vorobev, O., Smirnov, V. and Grabovskij, E.AGeneration of shock waves by soft X-radiation from Z-pinch plasmamFortov, V.E., Ternovoi, V.Y., Kvitov, S.V., Mintsev, V.B., Nikolaev, D.N., Pyalling, A.A. and Filimonov, A.S.�Thermodynamic properties and electrical conductivity of hydrogen at multiple shock compression up to 150 GPa pressure ionizationoFortov, V.E., Yakushev, V.V., Kagan, K.L., Lomonosov, I.V., Postnov, V.I., Yakusheva, T.I. and Kuryanchik, A.N.BAbnormal electric conductivity of lithium at high dynamic pressure237-240�Fortov, V.E., Gryaznov, V.K., Ilkaev, R.I., Mikhaylov, A.I., Mintsev, V.B., Mochalov, M.A., Pyalling, A.A., Ternovoi, V.Y. and Zhernokletov, M.V.MPressure ionization of condensed matter under intense shock waves at megabars135-140Fortov, V.E./Intense shock waves and nonideal plasma physics0Foster�  Jr., J.C., Maudlin, P.J. and Jones, S.E.:Laboratory experiments on explosions in geologic materialsFogel, M.B.2Yield strength modeling of shock damaged materials^Fogelson, D.J., Lee, L.M., Gilbert, D.W., Conley, W.R., Graham, R.A., Reed, R.P. and Bauer, F.RFabrication of standardized piezoelectric polymer shock gauges by the Bauer method615-618Foiles, S.M.^DFT calculations of structural and thermodynamic properties of molten Sn: Zero-pressure isobar$Follansbee, P.S. and Gray�  III, G.T.6Threshold stress measurements in shock-deformed copper371-376Follansbee, P.S.mHigh strain rate deformation mechanisms in copper and implications for behavior during shock wave deformation249-254)The HEL and rate-dependent yield behavior.Shear stress prediction in shock loaded copper!Foltz, M.F. and Maienschein, J.L.TPhase transitions in ammonium perchlorate to 26 GPa and 700K in a diamond anvil cell239-242Forbes, J.W. and Elban, W.L.�Comparison of axial longitudinal velocity measurements determined ultrasonically and by a weak shock velocity technique on an aluminized melt cast explosive583-587>Forbes, J.W., Tasker, D.G., Granholm, R.H. and Gustavson, P.K.DDirect observation of shocked explosive crystals immersed in liquids)Forbes, J.W., Lemar, E.R. and Baker, R.N.%Detonation wave curvature of PBXN-111	1389-1392Forbes, J.W. and Lemar, E.R.@Detonation wave velocity and curvature of brass encased PBXN-111;Forbes, J.W., Glancy, B.C., Liddiard, T.P. and Wilson, W.H.^Aquarium test evaluation of a pyrotechnic's ability to perform work in microsecond time framesForbes, J.W.MThe history of the APS Topical Group on Shock Compression of Condensed MattereForbes, J.W., Souers, P.C., Urtiew, P.A., Vandersall, K.S., Garcia, F., Greenwood, D.W. and Green, L.;Pressure wave measurements in cylinders of detonating LX-17902-905Forest, C.A.�Dependence of the intrinsic dTc/dp of YBa2Cu3Ox on the oxygen content and the additive Tc increase by pressure-induced oxygen ordering703-706~Filin, V.P., Loboyko, B.G., Averin, A.N., Litvinov, B.V., Korotkikh, I.G., Alekseev, A.V., Belenovsky, Y.A. and Taibinov, N.P.~On the mechanism of influence of explosive compounds: Destruction process on sensitivity of these compounds to mechanic impactGFilinov, V.S., Levashov, P.R., Bonitz, M., Fortov, V.E. and Ebeling, W.7On phase transition in strongly coupled hydrogen plasmaGFischer, R.P., Grun, J., Mignogna, R., Donnelly, D.W. and Covington, B.RAthermal annealing of semiconductors using shock waves generated by a laser-plasmaMFiske, P.S., Nellis, W.J., Lorenzana, H., Lipp, M., Kikuchi, M. and Syono, Y.mGeneration of pseudotachylites in shock experiments: Implications for impact cratering products and processes	1163-1165<Flater, P.J., House, J.W., De�  Angelis, R.J. and Nixon, M.E.ZDamage characterization in copper deformed under hydrostatic stress: Experimental analysis:Flater, P.J., House, J.W., O'Brien, J.M. and Hosford, W.F.SHigh strain-rate properties of tantalum processed by equal channel angular pressing
Fleming, K.J.[Analysis of a high intensity X-ray source using a specialized Doppler interferometer system6Flinn, J.E., Korth, G.E., Wright, R.N. and Green, R.C.)Dynamic consolidation of aluminum powders713-718(Flinn, J.E., Korth, G.E. and Doyle, T.E.MParticle interaction and bonding for dynamically consolidated Fe-40Ni powdersFlock, R.A. and Fowles, G.R./Explosive phase transition in superheated Freon273-276Flock, R.A.?Measurement of 'thin film' Gr"�neisen using x-cut quartz gauges763-766Flock, R.A. and Liu, D.T.>Numerical analysis of 'thin film' Gr"�neisen test measurements,Florence, A.L., Cizek, J.C. and Keller, C.E.ODynamic strength and inelastic deformation of ceramics under shock wave loading483-488iFerm, E.N., Morris, C.L., Quintana, J.P., Pazuchanic, P., Stacy, H., Zumbro, J.D., Hogan, G. and King, N.YProton radiography examination of unburned regions in PBX 9502 corner turning experiments966-969�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. and Thompson, R.T.AProton radiography experiments on shocked high explosive productsFerm, E.N. and Mariam, F.yProton radiography observations of the failure of a detonation wave to propagate to the end of a conical < explosive charge968-9711Ferranti�  Jr., L., Thadhani, N.N. and House, J.W.OHerrmann, B., Venkert, A., Kimmel, G., Landau, A., Shvarts, D. and Zaretsky, E.SFormation and morphology of twinning in titanium under high strain rate deformationDHerrmann, B., Landau, A., Shvarts, D., Favorsky, V. and Zaretsky, E.TModeling of uranium alloy response in plane impact and reverse ballistic experiments	1306-1309EHerrmann, B., Venkert, A., Favorsky, V., Shvarts, D. and Zaretsky, E.?U-0.75Ti and Ti6Al4V in planar and ballistic impact experiments8Herrmann, B., Favorsky, V., Zaretsky, E. and Shvarts, D.jCritical plastic strain as a criterion for failure in ballistic impact experiments of U/Ti and Ti64 alloys-Hertel, E.S., Chhabildas, L.C. and Hill, S.A.!Whipple bumper shield simulations&Hertel�  Jr., E.S. and Chhabildas, L.C.^Projectile shape influence on ballistic limit curves as determined by computational simulation	1179-1182)Heuz"�, O., Goutelle, J.C. and Baudin, G.YA new temperature-dependent equation of state for inert, reactive and composite materials
Heuz"�, O.BA complete equation of state for detonation products in hydrocodes450-453EHeuz"�, O., Martinez, E., Szarzynski, S., Mulford, R. and Swift, D.C.=Reactive flow in nitromethane using the CW2 equation of stateVBuilding of equations of state with numerous phase transitions: Application to bismuth212-215'Heuz"�, O., Jaouen, S. and Jourdren, H.1Henninger, R.J., Maudlin, P.J. and Rightley, M.L.GAccuracy of differential sensitivity for one-dimensional shock problems!Henninger, R.J. and Maudlin, P.J.8Code differentiation for hydrodynamic model optimizationHenninger, R.J..Sensitivities for Taylor test model parameters+Henrie, B.L., Mason, T.A. and Bingert, J.F.`Investigating incipiently spalled tantalum through multiple section planes and serial sectioning4Hensel, F., Hohl, G.F., Pilgrim, W.C. and Winter, R.SMetal-nonmetal transition and the dynamic structure factor of expanded fluid metalsDHenson, B.F., Funk, D.J., Dickson, P.M., Fugard, C.S. and Asay, B.W.KSurface temperature measurements of heterogeneous explosives by IR emission;Henson, B.F., Asay, B.W., Smilowitz, L.B. and Dickson, P.M.>Ignition chemistry in HMX from thermal explosion to detonationWHenson, B.F., Smilowitz, L., Asay, B.W., Romero, J.J., Oschwald, D.M. and Dickson, P.M.KMeasurement of the specific area of HMX and PBX 9501 by physical adsorptionEHenson, B.G., Smilowitz, L., Romero, J., Asay, B.W. and Dickson, P.M.YMeasurement of temperature and ignition time during fast compression and flow in PBX 9501�Henson, B.F., Smilowitz, L., Romero, J.J., Sandstrom, M.M., Asay, B.W., Schwartz, C., Saunders, A., Merrill, F., Morris, C., Murray, M.M., McNeil, W.V., Marr-Lyon, M. and Rightley, P.M.0Burn propagation in a PBX 9501 thermal explosion825-828.Herbold, E.B., Nesterenko, V.F. and Daraio, C.�Influence of controlled viscous dissipation on the propagation of strongly nonlinear waves in stainless steel based phononic crystals	1523-1526"Herbold, E.B. and Nesterenko, V.F.<Solitary and shock waves in strongly nonlinear metamaterials231-2349Herbold, E.B., Cai, J., Benson, D.J. and Nesterenko, V.F.]Simulation of particle size effect on dynamic properties and fracture of PTFE-W-Al composites3He, H.-L., Jin, X.-G., Jing, F.-Q. and Ahrens, T.J.?Characteristic of dynamic tensile fracture in augite-peridotite)He, H.-L., Shi, S.-C., Tan, H. and Xu, K./Shock compression of ZnO+a-Fe2O3 powder mixture721-723$He, H., kobayashi, T. and Sekine, T.BTime-resolved measurement of the launch of laser-driven foil plate	1339-1342dHe, H.L., Boustie, M., Arrigoni, M., de�  Ress"�guier, T., Auroux, E., Deleignies, M. and Gatulle, M.IHugoniot measurement of water from the impact of laser driven mini-flyers7He, H.L., Wang, Y.G., Li, X.M., Qi, M.L. and Jing, F.Q.PTwo critical damage parameters for the dynamic tensile fracture of ductile metal:Hearne, G.R., Sterer, E., Pasternak, M.P. and Taylor, R.D.mPressure dependence of the electronic and magnetic properties of the layered antiferromagnetic insulator FeI2	1461-1464'Hebert, D., Bertron, I. and Garnier, H.CNumerical and analytical analysis of thin laser-driven flyer plates821-824Farnsworth�  Jr., A.V.!Laser acceleration of thin flyers5Farnsworth�  Jr., A.V., Trott, W.M. and Setchell, R.E.2A computational study of laser driven flyer plates\Farrell, J.P., Batchelor, K., Dudnikov, V., Srinivasan-Rao, T., Smedley, J. and McDonald, J.eLaser triggered synchronizable X-ray system for real time study of shock waves in condensed materials	1185-1187Fast, L. and S""derlind, P.8Crystal structure of actinide metals at high compression7Fatyanov, O.V., Nicol, M.F., Ogura, T. and Kondo, K.-I.Equation of state for CCl4117-120#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. and Yang, S.-Y.<Stress-wave induced martensitic phase transformation in NiTi267-270Espinosa, H.D.<High strain rate modeling of ceramics and ceramic composites721-724$Espinosa, H.D., Mello, M. and Xu, Y.ZA desensitized displacement interferometer applied to fast moving particles in a continuum	1011-1014:Espinosa, H.D., Yuan, G., Dwivedi, S. and Zavattieri, P.D.MNumerical study of penetration in ceramic targets with a multiple-plane model901-904#Espinosa, H.D. and Zavattieri, P.D.LModeling of ceramic microstructures: Dynamic damage initiation and evolution333-3381Etters, R.D., Kobashi, K. and Chandrasekharan, V.kPrediction of pressure induced structural phase transitions and internal mode frequency changes in solid N2Etters, R.D. and Kuchta, B.fNew methods for calculating phase transitions in simple molecular crystals: Application to N2O and CO2)Evans, A.M., Graham, P. and Rothman, S.D.YRecent results from materials properties experiments using the AWE high power laser HELEN(Evans, D.J., Milne, A.M. and Softley, I.9The burning rate of aluminium particles in cylinder testsEwart, L. and Dandekar, D.P.`Relationship between the shock response and microstructural features of titanium diboride (TiB2)	1201-1204Fahrenthold, E.P.?Shock physics simulation using a hybrid particle-element method*Fahrenthold, E., Rabb, R. and Bohannan, A.<Numerical simulation of impact effects on multilayer fabrics	1285-1288*Fanget, A., Hereil, P.L. and Sibeaud, J.M.VThe influence of shock induced polymorphic transition in steel on 2D waves propagation	1087-1090%Endo, S., Takenaka, I. and Arashi, H.(A new phase transition in TiO2 at 80 GPaEpstein, J.S. and Deason, V.A.NDynamic moir"� interferometry: A review of research in weak shock environmentsEremets, M.i. and Utjuzh, A.N.JOptical nonmagnetic low-temperature hydrostatic pressure cells up to 3 GPa	1597-1600<Erickson, L.M., Palmer, H.G., Parker, N.L. and Vantine, H.C.dFree-surface velocity measurements of plates driven by reacting and detonating RX-03-BB and PBX-9404553-557Erickson, L.=Lawrence Livermore National Laboratory single-stage 101mm gun*Erlich, D.C., Shockey, D.A. and Seaman, L.>Symmetric rod impact technique for dynamic yield determination402-406Erlich, D.C. and Shockey, D.A.ODynamic flow curve of 4340 steel as determined by the symmetric rod impact testErlich, D.C. and Gran, J.K.JEffect of static transverse prestress on dynamic tensile failure in metals355-358Erlich, D.C. and Schmidt, C.G.<  (Rod impact experiments on thin specimensErlich, D.C. and Seaman, L.3Biaxial strain deformation and fracture of polymers*Shock Compression of Condensed Matter-1991Erlich, D.C. and Curran, D.R.yAn experimental technique for studying shock propagation in large-scale samples of snow and other highly porous materials'Erskine, D.J., Green, L. and Tarver, C.6VISAR wave profile measurements in supra-compressed HE717-720
Erskine, D.J.JCalculation of the refractive index change in dissociating shocked benzene883-886Erskine, D.J. and Nellis, W.J.CShock-induced martensitic transformation of highly ordered graphite185-186Erskine, D.5Opacity measurements in shock-generated argon plasmas"High pressure Hugoniot of sapphireKIncrease of the dynamic range of catchup experiments by high-pass filtering959-962Erskine, D.J. and Holmes, N.C.?Egorov, L.A., Barenboim, A.I., Mokhova, V.V. and Samoilov, A.I.9Railgun development for EOS applications: A status report643-648�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. and Wark, J.S.PIsentropic compression data on LX-04 explosive at 150��C using the Z accelerator	1315-1318aHarrach, R.J., Lee, Y.T., Trainor, R.J., Holmes, N.C., Rosen, M.D., Banner, D.L. and Olness, R.J.jContrasts in one- and two-dimensional hydrocode calculations of laser-generated shockwaves in disk targets164-168*Harrach, R.J., Sz""ke, A. and Howard, W.M.)Inertial effects in laser-driven ablation335-337
Harrach, D.J._High pressure, energy and impulse loading of the wall in a 1 GJ laboratory microfusion facilitypHarrigan, J.J., Hung, Y.-C., Tan, P.J., Bourne, N.K., Withers, P.J., Reid, S.R., Millett, J.C.F. and Milne, A.M.-High-rate compaction of aluminium alloy foams	1519-15220Harrigan, J.J., Millett, j.C.F. and Bourne, N.K.IStrength of the aluminium alloy 6082-T6 under high strain-rate conditionsHarris, P. and Presles, H.N.JReflection of a laser-generated optical signal from a shock front in water:Harris, E.J., Salisbury, D.A., Taylor, P. and Winter, R.E.CCharacterization of the SATURN air lens and its use in foam studies)Harris, E.J., Taylor, P. and Winter, R.E.AThe response of polyurethane foam to explosively generated shocks659-662Harris, E.J. and Winter, R.E.GCalculating the resistance of lateral manganin gauges in a steel matrix=Hydrocode analysis of lateral stress gauges in shock tantalum661-664+Harry, H.H., Uher, K.J. and Hagelberg, S.I.?The poly-rho test as a tool for screening explosive performance977-980/Harstad, E.N., Maudlin, P.J. and McKirgan, J.B.-Anisotropic failure modeling for HY-100 steel+Harstad, E.N., Addessio, F.L. and Zuo, Q.H.0A strength model for materials with phase change216-219SHartman, J.K., Wise, J.L., Graham, R.A., Johnson, R.O., Clark, G.E. and Burns, T.J.=Microwave dielectric constant of shock-loaded lithium niobateHarvey, W.B. and McQueen, R.G.XLagrangian analysis of velocity gauge data to determine reaction rate histories in EDC37The CREST reactive burn model)Hanfland, M., Hemley, R.J. and Mao, H.-K.WSynchrotron infrared measurements of pressure-induced transformations in solid hydrogen873-876Hanson, D.L. and Matzen, M.K..Study of ion-beam driven shock waves in metals;Hanson, D.L., Struve, K.W., Spielman, R.B. and Seaman, J.F.pApplication 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. and Rothman, S.D.+Progress on deuterium EOS measurements on ZcHanson, D.L., Johnston, R.R., Knudson, M.D., Asay, J.R., Hall, C.A., Bailey, J.E. and Hickman, R.J.TAdvanced cryogenic system capabilities for precision shock physics measurements on Z	1141-11444Harada, T., Kanomata, T., Yoshida, H. and Kaneko, T.=Pressure effect on transport properties of M3-xCoxGaC (x<0.3)	1441-1444Hardy, R.J. and Karo, A.M.7Stress and energy flux in the vicinity of a shock front161-164'Hardy, R.J., Root, S. and Swanson, D.R./Continuum properties from molecular simulations363-366HTwo dimensional continuum properties from molecular dynamics simulations'Hare, D.E., Webb, D.J. and Holmes, N.C._Imaging shocked sapphire at 200-460 kbar: The effect of crystal orientation on optical emission3Hare, D.E., Webb, D.J., Lee, S.-H. and Holmes, N.C.:Optical extinction of sapphire shock-loaded to 250-260 GPa	1231-1234kHare, D.E., Reisman, D.B., Garcia, F., Green, L.G., Forbes, J.W., Furnish, M.D., Hall, C. and Hickman, R.J.,The isentrope of unreacted LX-04 to 170 kbarQHare, D.E., Vandersall, K.S., Garcia, F., Davis, J.-P., Hall, C. and Forbes, J.W.;The Riemann problem for a model nonlinear elastic continuum169-1721Hammerberg, J.E., Preston, D.L. and Wallace, D.C.2A new model of rate dependent elastic-plastic flow-Hammerberg, J.E., Holian, B.L. and Zhou, S.J.0Studies of sliding friction in compressed copperHammerberg, J.E. and Pepin, J.2An analytic solution to a driven interface problemyHammerberg, J.E., Kyrala, G.A., Oro, D.M., Fulton, R.D., Anderson, W.E., Obst, A.W., Oona, H., Stokes, J. and Wilke, M.D.+A Pegasus dynamic liner friction experiment0Hammerberg, J.E., Germann, T.C. and Holian, B.L.Shock waves in dusty plasmasIHammerberg, J.E., Ravelo, R., Germann, T.C., Kress, J.D. and Holian, B.L./Sliding friction at compressed Ta/Al interfaces.Hammerberg, J.E., Ravelo, B. and Germann, T.C.2High density sliding of Ta/Al and Al/Al interfaces<Hammerberg, J.E., Ravelo, R., Germann, T.C. and Holian, B.L.9Frictional interactions at compressed aluminum interfaces<Hammetter, W.P., Hellman, J.R., Graham, R.A. and Morosin, B.WEnergy release and transformation of shock-modified zirconia upon annealing to 1550 ��C8Hammetter, W.F., Graham, R.A., Morosin, B. and Horie, Y.eEffects of shock modification on the self-propagating high temperature synthesis of nickel aluminides431-434CHammond, R.I., Church, P.D., Grief, A., Proud, W.G. and Field, J.E.WDependence of measured lateral stress on thickness of protective 'padding' around gauge,Hammond, R.I., Winter, R.E. and Harris, E.J.?Measurement of strength of EN3B mild steel using lateral gaugesKHan, C.-S., Liu, G.-Z., Dong, Y.-B., Feng, J.-P., Wang, D.-S. and Hu, H.-B.PExpansion movement and fracture of a cylindrical shell due to internal explosion%Hanagud, S., Lu, X. and Zaharieva, R.VEquation of state & failure criteria of dual functional structural energetic materials
Handley, C.A.	1163-1168yHall, C.A., Baer, M.R., Gustavsen, R.L., Hooks, D.E., Orler, E.B., Dattelbaum, D.M., Sheffield, S.A. and Sutherland, G.T.HA study of polymer materials subjected to isentropic compression loading	1311-1314$Hamashima, H., Kato, Y. and Itoh, S.7Determination of JWL parameters for non-ideal explosive/Hamashima, H., Osada, A., Itoh, S. and Kato, Y.tLow velocity detonation of nitromethane affected by precursor shock waves propagating in various container materialsHamate, Y. and Horie, Y.KA statistical approach on mechanistic modeling of high-explosive detonation=Development of a mechanistic burn modeling of high explosives
Hamate, Y.\A computational study of microstructure effects on shock ignition sensitivity of pressed HMX_Hamaya, N., Sakamoto, Y., Fujihisa, H., Fujii, Y., Takemura, K., Kikegawa, T. and Shimomura, O.8Rietveld analysis of high pressure phase of praseodymium5Hambir, S.A., Franken, J., Hill, J.R. and Dlott, D.D.UUltrafast vibrational spectroscopy of shocks in molecular materials: The first 100 ps%Hambir, S.A., Kim, H. and Dlott, D<  .D.7Ultrafast dynamics of nanoshocks in molecular materials945-950/Hamilton, D.C., Mitchell, A.C. and Nellis, W.J.HElectrical conductivity measurements in shock compressed liquid nitrogenHamilton, D.C. and Ree, F.H.gChemical equilibrium calculations for the high pressure and temperature dissociation of liquid nitrogenSHamilton, D.C., Nellis, W.J., Holmes, N.C., Radousky, H.B., Ree, F.H. and Nicol, M.`Electrical conductivity and equation of state measurements on planetary fluids at high pressures99-101�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. and Perry, T.S.6Shock physics with the NOVA laser for ICF applications	1281-1285Hammerberg, J.E.tShock initiation of 'virgin' and 'recycled' PBX 9502 measured with embedded electromagnetic particle velocity gaugestGustavsen, R.L., Dattelbaum, D.M., Orler, E.B., Hooks, D.E., Alcon, R.R., Sheffield, S.A., Hall, C.E. and Baer, M.R.ZIsentropic compression of nitroplasticized estane to about 35 kbar on the Sandia Z-MachineBExtended run distance measurements of shock initiation in PBX 9502.Gustavson, P.K., Tasker, D.G. and Forbes, J.W.9Underwater shock wave measurements using PVDF transducers905-908Gutkin, M.Y. and Ovidko, I.A.<Rotational effect and amorphization in shock loaded crystals401-404@Gyanchandani, J.S., Gupta, S.C., Sikka, S.K. and Chidambaram, R..On the valence transition in shocked ytterbium6On the shock discontinuities in titanium and zirconium131-134FHaberman, K.S., Bennett, J.G., Asay, B.W., Henson, B.F. and Funk, D.J.aModeling, simulation and experimental verification of constitutive models for energetic materialsHablot, O. and Soulard, L.#Shock decomposition of nitromethane857-860hHackenberg, R., Swift, D., Bourne, N., Gray�  III, G.T., Paisley, D., Thoma, D., Cooley, J. and Hauer, A.,Dynamic properties of nickel-titanium alloysTHagelberg, C.R., Swift, R.P., Carney, T.C., Greening, D., Hiltl, M. and Nellis, W.J.0Modeling shock recovery experiments of sandstone	1275-1278/Hall, C.A., Chhabildas, L.C. and Reinhart, W.D.fShock Hugoniot and release states in concrete mixtures with different aggregate sizes form 3 to 23 GPauHall, C.A., Asay, J.R., Trott, W.M., Knudson, M., Fleming, K.J., Bernard, M.A., Clark, B.F., Hauer, A. and Kyrala, G.:Aluminum Hugoniot measurements on the Sandia Z accelerator	1171-1174[Hall, C.A., Asay, J.R., Knudson, M.D., Hayes, D.B., Lemke, R.L., Davis, J.P. and Deeney, C.]Recent advances in quasi-isentropic compression experiments (ICE) on the Sandia Z accelerator�Progress in understanding shock deformation in condensed materials at the atomic/molecular level: Recent experimental developments15-26Gupta, S.C.NBand structure calculations to predict phase transformations at high pressures157-163rGupta, S.C., Agarwal, R.G., Gyanchandani, J.S., Roy, S., Suresh, N., Sikka, S.K., Kakodkar, A. and Chidambaram, R.-A single stage gas gun for shock wave studies'Gupta, S.C., Suresh, N. and Sikka, S.K.1On 5f band occupation in shock compressed thorium\Shock wave experiments at different length scales: Recent achievements and future challenges&Gupta, S.C., Ahrens, T.J. and Yang, W.9Shock induced vaporization of anhydrite CaSO4 and calcite	1259-1262(Gupta, S.C., Love, S.G. and Ahrens, T.J.JShock temperatures in calcite: Implication for shock induced decomposition_The coupling between shock waves and condensed matter: Continuum mechanics to quantum mechanics#Gustavsen, R.L. and Sheffield, S.A.4Unreacted Hugoniots for porous and liquid explosives0Gustavsen, R.L., Sheffield, S.A. and Alcon, R.R.PResponse 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 densities0Detonation wave profiles in HMX based explosivesgGustavsen, R.L., Sheffield, S.A., Alcon, R.R., Hill, L.G., Winter, R.E., Salisbury, D.A. and Taylor, P.TInitiation of EDC-37 measured with embedded electromagnetic particle velocity gauges[Gustavsen, R.L., Sheffield, S.A., Alcon, R.R., Winter, R.E., Taylor, P. and Salisbury, D.A.9Double shock initiation of the HMX based explosive EDC-37XGustavsen, R.L., Sheffield, S.A., Alcon, R.R., Forbes, J.W., Tarver, C.M. and Garcia, F.|Embedded electromagnetic gauge measurements and modeling of shock initiation in the TATB based explosives LX-17 and PBX 9502(Guirguis, R., McKeown, R. and Kelley, J.KA closed water-filled cylinder test for characterizing non-ideal explosives871-874!Ignition due to macroscopic shear"Guirguis, R.H. and Landsberg, A.M.Convective detonations926-929Guirguis, R.H. and Kelley, J.M.5Role of radiation in surface burning of melt cast TNTGuirguis, R.H. and Joshi, V.S.>An ignition model for liquid-solid powder hypergolic reactionsGuirguis, R. and Pangilinan, G.\Effect of phase transitions of inert additives on detonation properties of porous explosives6Gump, J.C., Wong, C.P., Zerilli, F.J. and Peiris, S.M.6High-pressure structural study of epsilon HNIW (CL-20)%Gump, J., Parker, L. and Peiris, S.M.SHMX (beta phase): Laser-ignited reaction kinetics and isothermal equations of state967-972Gump, J.C. and Peiris, S.M.AComparison of reaction kinetics of I-RDX and RDX at high pressure	1069-1072)Gump, J.C., Stoltz, C.A. and Peiris, S.M.QPhase stability of epsilon and gamma HNW (CL-20) at high-pressure and temperature127-132'Gupta, Y.M., Murri, W.J. and Henley, D.FLarge amplitude compression and shear wave propagation in an elastomerGupta, Y.M. and Murri, W.J.3Piezoelectric shear stress gage for dynamic loadingGupta, Y.M.0Analysis and modeling of piezoresistive responseGupta, S.C. and Gupta, Y.M.RResponse of ytterbium foils oriented parallel and perpendicular to the shock front237-238BPiezoelectric response of manganin foils: Experiments and analysis509-511DPiezoresistance response of manganin foils: Experiments and analysis&Shock waves in condensed matter - 1985Y. Gupta)Gupta, S.C., Gupta, Y.M. and Williams, M.APiezoresistance response of ytterbium foils in shocked liquid CS2601-603�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. and Gardes, D.>About masurements of stopping power behind intense shock waves879-882Grzegory, I.CCrystal growth of III-N semiconductors under high nitrogen pressure561-564TGrzegory, I., Krukowski, S., Jun, J., Bockowski, M., Wroblewski, M. and Porowski, S.8Stability of indium nitride at N2 pressure up to 20 kbarGu, G. and Vohra, Y.K.4Mo-Re and Ti-V alloys at extreme static compressionsGu, Z. and Jin, X.;Temperature dependence on shock response of stainless steel0Gu, Y.-B., Nesterenko, V.F. and Indrakanti, S.S.VBallistic testing and high-strain-rate properties of hot isostatically pressed Ti6Al4V	1294-1297'Gu, Y.-B., Nesterenko, V.F. and Cai, J.UShear localization and patterning of shear bands in PTFE and its mixtures with metalsVGudarenko, L.F., Gushchina, O.N., Zhernokletov, M.V., Medvedev, A.B. and Simakov, G.V.UShock compression and isentropic expansion of tungsten, nickel and tin porous samples"Gudarenko, L.F. and Kudelkin, V.G.cConstruction of wide-range equations of state through 'merging' local equations using mixture model127-130Gu"�ry, J.F.RDamage models with intermediate configuration large strain formulation and resultsGu"�ry, J.-F. and Seaman, L.9Simulations of microfractures in solid rocket propellants;Guest, A.R., Braithwaite, C.H., Proud, W.G. and Field, J.E.[The shock Hugoniot properties of geological materials and relationship<  to static propertiesGuirguis, R.H. and Oran, E.S.INumerical studies of laser-induced shock structure in condensed materials351-352Guirguis, R.*Munroe/channel effect and weak detonationsGuirguis, R.H.1-D detonability377-380&Energy release in non-ideal explosives381-384XDevelopment of third harmonic generation as a short pulse probe of shock heated material1Grinfeld, M.A., Schoenfeld, S.E. and Wright, T.W.IFailure fronts in brittle materials and their morphological instabilities858-861$Grote, D.L., Park, S.W. and Zhou, M.HAn experimental characterization of the dynamic impact failure of mortar	1271-1274Grove, D.J. and Rajendran, A.M.6Simulation of flyer plate-rod target impact experiment4Grove, D.J., Rajrendran, A.M. and Dietenberger, M.A.8Numerical simulation of a double flyer impact experimentGrove, J.W.3Irregular shock refractions at a material interface7Grove, D.J., Rajendran, A.M., Bar-On, E. and Brar, N.S.!Damage evolution in a ceramic rodcModeling of Kipp-Grady plate impact experiments on ceramics using the Rajendran-Grove ceramic model Grove, D.J. and Rajrendran, A.M.TEffects of pulverized material strength on penetration resistance of ceramic targetsOA comparison between scalar and multi-plane microcracking ceramic damage modelsHModeling of microcrack density based on damage evolution in ceramic rodsGrover, R.W.*Why linear Birch and Us-up expansions work139-142"Grover, R., Ree, F. and Holmes, N.1Equation-of-state from SiO2-aerogel Hugoniot data~Grun, J., Manka, C.K., Hoffman, C.A., Meyer, J.R., Glembocki, O.J., Qadri, S.B., Skelton, E.F., Donnelly, D. and Covington, B.9Athermal annealing of neutron-transmutation-doped silicon981-984!Grunschel, S.E. and Clifton, R.J.@Pressure-shear plate impact of aluminum at elevated temperaturesGruzdkov, Y.A. and Gupta, Y.M.DMechanism of chemical decomposition in a shocked condensed explosive813-818*Gruzdkov, Y.A., Gupta, Y.M. and Dick, J.J.ETime-resolved absorption spectroscopy in shocked PETN single crystals.High accuracy equations of state for standards89-94Greeff, C.W. and Liz"�rraga, R.<Liquid metal free energies from ab initio potential surfaces5Green, L.G., Lee, E.L., Breithaupt, D. and Walton, J.1The equation of state of PETN detonation products507-510IGreenaway, M.W., Gifford, M.J., Proud, W.G., Field, J.E. and Goveas, S.G.VAn investigation into the initiation of hexanitrostilbene by laser-driven flyer platesGreenaway, M.W. and Field, J.E..The development of a laser-driven flyer system,Greenaway, M.W., Laity, P.R. and Pelikan, V.JX-ray microtomography of sugar and HMX granular beds undergoing compactionGreene, R.G. and Ruoff, A.L.:Optical effects of fine ceramic powder in solidified gases%Greene, R.G., Luo, H. and Ruoff, A.L..High pressure Raman and EDXD study of diaspore	1535-1538/Greenfield, S.R., Swift, D.C. and Koskelo, A.C.7Transient interferometric studies of shocked bicrystals	1269-1272WGreenfield, S.R., Luo, S.N., Paisley, D.L., Loomis, E.N., Swift, D.C. and Koskelo, A.C.FTransient imaging displacement interferometry applied to shock loading	1093-1096Greening, D.R. and Koskelo, A.0Calculation of grain boundary shock interactions]Greenwood, D., Forbes, J., Garcia, F., Vandersall, K., Urtiew, P., Green, L. and Erickson, L.@Improvements in the signal fidelity of the manganin stress gauge	1157-11597Grignon, F., Benson, D., Vecchio, K.S. and Meyers, M.A.QExplosive welding of aluminum to aluminum: Analysis, computations and experiments	1098-1101gGrigsby, W., Bowes, B.T., Dalton, D.A., Bless, S., Downer, M.C., Taleff, E., Colvin, J. and Ditmire, T.GDiagnosis of Mbar laser produced shocks in tin using short pulse probes	1337-1340`Grigsby, W., Cho, B.I., Bernstein, A.C., Quevedo, H.J., Colvin, J., Downer, M.C. and Ditmire, T./Gray�  III, G.T., Hixson, R.S. and Johnson, J.N.mDynamic deformation and fracture response of a 6061-T6 Al  �� 50 vol. % Al2O3 continuous reinforced composite<Gray�  III, G.T., Blumenthal, W.R., Idar, D.J. and Cady, C.M.PInfluence of temperature on the high strain-rate mechanical behavior of PBX 9501583-586NGray�  III, G.T., Bourne, N.K., Zocher, M.A., Maudlin, P.J. and Millett, J.C.F.\Influence of crystallographic anisotropy on the Hopkinson fracture 'spallation' of zirconiumMGray�  III, G.T., Bourne, N.K., Millett, J.C.F., Lopez, M.F. and Vecchio, K.S.QInfluence of microstructural anisotropy on the spallation of 1080 eutectoid steel>Gray�  III, G.T., Bourne, N.K., Millett, J.C.F. and Lopez, M.F.�Influence of shock-wave profile shape ('Taylor-wave' versus square-topped) on the shock-hardening and spallation response of 316L stainless steel461-464�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. and Lopez, M.F.~Influence of shock prestraining and grain size on the dynamic-tensile-extrusion response of copper: Experiments and simulationgGray�  III, G.T., Cerreta, E., Hixson, R.S., Koller, D.D., Dougherty, L., Trujillo, C.P. and Lopez, M.F.gInfluence of microstructure on the Bauschinger effect and the shock hardening in 1080 high-carbon steelGrebenkin, K.F.!Semiconductor model of detonation982-985BGrebyonkin, K.F., Zherebtsov, A.I., Popova, V.V. and Taranik, M.V.3P,V,E,T equation of state for TATB-based explosives,Greeff, G.W., Trinkle, D.R. and Albers, R.C.BAlpha-omega transition in titanium: Equation of state and kineticsIGreeff, C.W., Rigg, P.A., Knudson, M.D., Hixson, R.S. and Gray�  III, G.T.<Modeling dynamic phase transitions in titanium and zirconium209-212:Greeff, C.W., Graf, M.J., Boettger, J.C. and Johnson, J.D._Shock-induced melting of a KCl:LiCl eutectic powder as determined from electrochemical response%Graham, R.A., Lee, L.M. and Bauer, F.MResponse of Bauer piezoelectric polymer stress gauges (PVDF) to shock loading:Graham, R.A., Anderson, M.U., Bauer, F. and Setchell, R.E.vPiezoelectric polarization of the ferroelectric polymer PVDF from 10 MPa to 10 GPa: Studies of loading path dependenceBridgman's concernWBallography: A billion nanosecond history of the Bee Bluff impact crater of south Texas	1462-14678Graham, R.A., Martin, M., Thadhani, N.N. and Morosin, B.JQuartz and hydrous iron oxides from the Bee Bluff structure of south Texas	1468-1471)Gran, J.K., Holmes, B.S. and Curran, D.R.@Measurement of explosive blast loads with flatpack stress gauges!Granholm, R.H. and Sandusky, H.W.4Small-scale shock reactivity and internal blast test.Granholm, R.H., Sandusky, H.W. and Felts, J.E. Factors affecting internal blastGrantham, S.G. and Proud, W.G.'Digital speckle X-ray flash photography803-806+Grantham, S.G., Proud, W.G. and Field, J.E.8Internal displacements in cement during ballistic impact	1335-1338CGrantham, S.G., Braithwaite, C.H., Proud, W.G. and Williamson, D.M.<Displacement maps in Taylor impact using speckle radiography	1333-1336Gratz, A.J. and Nellis, W.J.!Microstructures of shocked quartz203-205$Gray�  III, G.T. and Follansbee, P.S.sInfluence of peak pressure on the substructure evolution and mechanical properties of shock-loaded 6061-T6 aluminumGray�  II<  I, G.T.VKanel, G.I., Bogach, A.A., Razorenov, S.V., Savinykh, A.S., Chen, Z. and Rajendran, A.;A study of the failure wave phenomenon in brittle materialsKanel, G.I.)Failure waves in shock-compressed glasses870-875HKanel, G.I., Razorenov, S.V., Savinykh, A.S., Rajendran, A. and Chen, Z.PA study of failure wave phenomenon on glasses at peak stresses exceeding the HEL876-879OKanel, G.I., Savinykh, A.s., Garkushin, G.V., Razorenov, S.V. and Rajendran, A.vCharacterization of trace nickel in synthetic diamond and its relationship to the abundance of substitutional nitrogen9Kaiser, M.A., Wilson, L.T., Wicks, A.L. and Swantek, S.D.-Experimental techniques for the Hopkinson bargKalantar, D.H., Remington, B.A., Colvin, J.D., Gold, D.M., Mikaelian, K.O., Weber, S.V. and Wiley, L.G.)Shock compressed solids on the NOVA laser	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. and Wark, J.S.BLaser 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. and Wark, J.S.GDirect observation of the a-e transition in shocked single crystal iron240-243.Kalpana, G., Palanivel, B. and Rajagopalan, M.DBand structure and superconductivity of bcc tellurium under pressure673-676Kamegai, M.GNumerical analysis of Hopkinson bar experiments on dislocation dynamics-Kamegai, M., Klein, L.S. and Rosenkilde, C.E._Computer simulation of the effect of free surface reflection on shock wave propagation in water*Kamegai, M., Walton, O.R. and Taylor, A.G.NMicro-scale simulation of dynamic compaction of oxide and metal powder mixture
Kamm, J.R.NA simple hydrodynamic model for jetting from tubular hypervelocity penetrators	1825-1828Kandasamy, R. and Brar, N.S.LFlow stress and material model study at high strain rate and low temperature	1031-1034Kane, J.O. and Smith, R.F.OModeling non-equilibrium phase transitions in isentropically compressed bismuth244-2475Kaneko, T., Kanomata, T., Kawashima, T. and Yasui, H.JPressure effect on the Curie temperature and exchange striction of YMn2Ge2	1473-1476`Preparation and shock reactivity analysis of novel perfluoroalkyl-coated aluminum nanocomposites	1527-1530<Jouet, R.J., Carney, J.R., Lightstone, J.M. and Warren, A.D.NLaser ablation analysis of novel perfluoroalkyl-coated aluminum nanocomposites"Juanicotena, A. and Szarzynski, S.EInvestigation of dynamic friction induced by shock loading conditions!Jung, J., Jhung, K.S. and Kim, I.NHelmholtz free energy equation of state applied to carbon at megabar pressuressJuodkazis, S., Misawa, H., Gamaly, E.G., Luther-Davies, B., Rode, A.V., Hallo, L., Nicolai, P. and Tikhonchuk, V.T.uMulti-megabar pressure and super-dense materials created by laser-induced micro-explosion inside of transparent solid-Justus, B.L., Huston, A.L. and Campillo, A.J.DTemperature measurements of shocked water using a fluorescence probe.Justus, B.L., Merritt, C.D. and Campillo, A.J.MEfficient photogeneration of triplets in shock compressed 2,4-dinitrostilbeneLJyoti, G., Joshi, K.D., Gupta, S.C., Sikka, S.K., Dey, G.K. and Banerjee, S.IThe orientation relations between the a and w phases of shocked zirconiumIJyoti, G., Gupta, S.C., Ahrens, T.J., Kossakovski, D. and Beauchamp, J.L.5Mass spectrometer calibration of cosmic dust analyzer8Kadau, K., Germann, T.C., Lomdahl, P.S. and Holian, B.L.dShock-induced structural phase transformations studied by large-scale molecular-dynamics simulationsFKadau, K., Germann, T.C., Lomdahl, P.S., Holian, B.L. and Cherne, F.J.8Atomistic simulations of shock-induced phase transitions229-2345Atomistic simulation of shock-induced melting in iron236-239dKadau, K., Germann, T.C., Lomdahl, P.S., Albers, R.C., Wark, J.S., Higginbotham, A. and Holian, B.L.TAtomistic simulations of shock-induced phase transformations in polycrystalline ironoThe study of internal deformation fields in granular materials using 3D digital speckle X-ray flash photography(Golkov, R., Kleiman, D. and Zaretsky, E.MImpact response of single crystal potassium chloride at elevated temperatures9Goncharov, A.F., Struzhkin, V.V., Ruf, T. and Syassen, K.PEffect of pressure on coupled phonon and crystal-field excitations in NdBa2Cu3O70Goncharov, A.F., Struzhkin, V.V. and Syassen, K.�Superconductivity-induced phonon self-energy effects and electronic Raman scattering in YBa2Cu3O7-x single crystals under pressureGong, Z., Tan, H. and Jing, F.MShock wave equation of state and shock induced phase transition of HalloysiteGong, Z., Li, X. and Jing, F.SThe possible composition and thermal structure of the Earth's lower mantle and core	1401-1405)Gong, Z., Dai, F., Zhang, L. and Jing, F.KAn empirical material constant and equation of state on the solids Hugoniot2Gong, Z., Dai, F., Fei, Y., Zhang, L. and Jing, F.zEquation of state, phase stability of (Mg0.92Fe0.08)SiO3 perovskite from shock wave study and its geophysical implications	1444-14472Gong, Z., Yu, H., Deng, L., Zhang, L. and Yang, J.FVariations of thermal pressure for solids along the principal Hugoniot0Gong, Z., He, L., Fei, Y., Yang, J. and Jing, F.nSound velocity of (Mg0.92,Fe0.08)SiO3 perovskite up to 140 GPa shock pressure and its geophysical implications	1458-1461+Gong, S.W., Cheng, M., Liu, Z.J. and Lu, C.=Dynamic response of submerged solids to extreme fluid loading	1383-1386Gonor, A.L.gHigh-pressure vaporization and boiling of condensed material: A generalized Clausius-Clapeyron equation63-66%Gonor, A., Hooton, I. and Narayan, S.@Gobin, C., Lucas, H., Marteau, P., Hebert, P. and Petitet, J.-P.sHigh pressure spectroscopic study of the action of N-ethylamines and water on the 2-nitropropane/nitric acid system	1265-1268PGoel, B., Baumann, K., H""bel, W., Vorobiev, O.Y., Shutov, A.V. and Fortov, V.E.<Numerical analysis of foil acceleration experiments at KALIFFGogulya, M.F., Dolgoborodov, A.Y., Brazhnikov, M.A. and Dushenok, S.A.*Shock wave initiation of liquid explosivesTGogulya, M.F., Dolgoborodov, A.Y., Brazhnikov, M.A., Makhov, M.N. and Arkhipov, V.I.7Aluminised explosive compositions based on NQ and BTNEN962-965"Gogulya, M.F. and Brazhnikov, M.A.aSome aspects of shock-induced radiation of transparent media and its transformation with pressure	1329-1332%Gois, J.C., Campos, J. and Mendes, R.?Extinction and initiation of detonation of NM-PMMA-GMB mixtures2Gois, J.C., Campos, J., Plaksin, I. and Mendes, R.FFailure and re-initiation detonation phenomena in NM/PMMA-GMB mixtures$Gois, J., Campos, J. and Plaksin, I.^Effect of glass microballoons on failure and reaction regime of nitromethane/PMMA-GMB mixtures898-901wGold, D.M., Celliers, P.M., Collins, G.W., DaSilva, L.B., Cauble, R.C., Kalantar, D.H., Weber, S.V. and Remington, B.A.POptical interferometry diagnostics in laser-driven equation of state experimentsGGolden, J., Williams, F., Morosin, B., Venturini, E.L. and Graham, R.A..Catalytic activity of shock-loaded TiO2 powder72-76KGoldenberg, A., Britan, A., Ben-Dor, G., Igra, O., Hariton, I. and Glam, B.RDynamics of the load-transfer in a single straight chain of disks: FEM simulations201-204NGoldman, N., Fried, L.E., Mundy, C.J., Kuo, I.F.W., Curioni, A. and Reed, E.J.^Ab initio molecular dynamics simulations of water under static and shock compressed conditions.Goldrein, H.T., Synnergren, P. and Proud, W.G.,Ginzburg, A., Rosenberg, Z. and Birnboim, A.NThe measurement of very short stress signals with piezoresistive stress gaugesGinzburg, A. and Rosenberg, Z.VUsing reverberation te<  chniques to study the properties of shock loaded soda-lime glass529-531 Glaesemann, K.R. and Fried, L.E.2Recent advances in modeling Hugoniots with Cheetah515-518>Glam, B., Britan, A., Ben-Dor, G., Igra, O. and Goldenberg, A.0Dynamics of the contact stress in granular media	1261-1264,Glancy, B.C., Krall, A.D. and Sandusky, H.W.9Microwave interferometric applications in SDT/DDT studies,Glancy, B.C., Sandusky, H.W. and Krail, A.D.,Johnson, J.B., Brown, J.A. and Gaffney, E.S.cInterpretation of the stress histories from shock impact tests on snow using embedded stress gaugesJohnson, K.A. and Medina, W.J.NShock compaction of high-temperature superconducting YBa2Cu3O7 ceramic powders
Johnson, J.D.Carbon in detonations697-704WJohnson, J.B., Brown, J.A., Gaffney, E.S., Blaisdell, G.L., Sturm, M. and Barrett, S.A.Shock wave studies of snow107-110Johnson, J.D. and Shaw, M.S./The influence of a slow rate on detonation flowJohnson, J.N. and Tonks, D.L.HDynamic plasticity in transition from thermal activation to viscous drag371-378!Johnson, G.R. and Holmquist, T.J.BAn improved computational constitutive model for brittle materials<Johnson, J.N., Hixson, R.S., Tonks, D.L. and Gray�  III, G.T.6Shock compression and quasielastic release in tantalum?Micromechanical strength effects in shock compression of solids6Johnson, D.E., Lee, L.M., Hedemann, M.A. and Bauer, F.FPVDF measurement of soft X-ray induced shock and filter debris impulsenModeling of the slip-twinning transition in nanocrystalline nickel and nickel-tungsten under shock compression
Jayaraman, A.4Recent developments in static high pressure research13-36Jeanloz, R. and Grover, R.,Birch-Murnaghan and Us-up equations of stateeJensen, B.J., Rigg, P.A., Knudson, M.D., Hixson, R.S., Gray�  III, G.T., Sencer, B.H. and Cherne, F.J.+Dynamic compression of iron single crystals232-235Jett"�, F.X. and Higgins, A.J.WCritical diameter prediction for steady detonation in gasless metal-sulfur compositions,Jett"�, F.X., Goroshin, S. and Higgins, A.J.?Shock reactivity of non-porous mixtures of manganese and sulfurXTime-resolved temperature measurements of shock initiation in a manganese-sulfur mixtureJevais, J.R. and Zerah, G.KA new fluid integral equation application to the equation of state of xenon119-1243Jhung, K.S., Kim, I.H., Oh, K.-H. and Jhung, K.H.C.7Universal description of energetics of condensed matter329-332'Jiang, J., Goroshin, S. and Lee, J.H.S.4Shock wave induced chemical reaction in Mn+S mixture+Jiao, T., Clifton, R.J. and Grunschel, S.E.)High strain rate response of an elastomerNPressure sensitivity and tensile strength of an elastomer at high strain ratesJin, G.&Shock Hugoniot measurement on tungstenDJin, X., Zhang, H., Che, R., Zhou, L., Zhao, Q., Liu, J. and Xiu, L.IIsothermal equations of state for nanometer and micrometer nickel powders99-102OJin, Z.Q., Chen, K.H., Li, J., Zeng, H., Liu, P., Wang, Z.L. and Thadhani, N.N.CShock compaction of exchange-coupled nanocomposite magnetic powders	1102-1105IJin, Z.Q., Li, J., Thadhani, N.N., Wang, Z.L., Vedantam, T. and Liu, J.P.^Shock compression of FePt and FePt/Fe3Pt nanoparticles: Exchange-coupled nanocomposite magnetsJing, F.-Q.$Shock wave physics research in China33-44gThe irregular reflection from the symmetrical collision of two plane detonation waves in high explosive2Itskevich, E.S., Voronovsky, A.N. and Dizhur, E.M.^Investigations of quasi-particle spectra using electron-topological transitions under pressuremIvanov, D.S., Zhigilei, L.V., Bringa, E.M., De�  Koning, M., Remington, B.A., Caturia, M.J. and Pollaine, S.M.jMolecular dynamics simulations of shocks including electronic heat conduction and electron-phonon coupling6Iyer, K.R., Bennett, L.S., Sorrell, F.Y. and Horie, Y.1Solid state chemical reactions at the shock frontIyer, K. and Dandekar, D.HComputational design study for recovery of shock damaged silicon carbide866-869Jackson, I.GViscoelastic relaxation in iron and the shear modulus of the Inner CoreJackson, S.I. and Hill, L.G.JPredicting runaway reaction in a solid explosive containing a single crackNJacobsen, M.K., Kumar, R.S., Cornelius, A.L., Sinogeiken, S.V. and Nicol, M.F.?High pressure X-ray diffraction studies of Bi2-xSbxTe3(x=0,1,2))James, H.R., Cook, M.D. and Haskins, P.J.UThe effect of impact angle on the initiation threshold of bare and covered explosives+James, H.R., McElrue, D.H. and Winter, R.E.Recovery of uranium fragments	1302-1305James, H.R.MThe role of tip geometry in the initiation of explosives by shaped charge jet993-997EEstimaton of two-dimensional initiation thresholds from pop plot datagThe puzzle of explosive response to shock: Complexity to simplicity by changing the observational scale931-936;Shock initiation thresholds for insensitive high explosiveseJarmakani, H., McNaney, J.M., Schneider, M.S., Orlikowski, D., Nguyen, J.H., Kad, B. and Meyers, M.A.PDynamic response of copper subjected to quasi-isentropic, gas-gun driven loading6Jarmakani, H., Wang, Y.M., Bringa, E. and Meyers, M.A. Hwang, M., Horie, Y. and You, S.PModeling of shock-induced chemical reactions in powder mixtures 1: The VIR model;Hwang, L.W., Schroeder, J., Silvestri, M.R. and Zhao, X.-S.LOptical effects in II-VI semiconductor nanocrystal colloids at high pressureHyndman, D.A. and Gaffney, E.S.7Calibration of PVDF transducers at stresses below 1 MPa809-8116Idar, D.J., Peterson, P.D., Scott, P.D. and Funk, D.J.KLow strain rate compression measurements of PBXN-9, PBX 9501, and mock 9501IIdar, D.J., Straight, J.W., Osborn, M.A., Coulter, W.L. and 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. and Jacquez, B.L.lInfluence of polymer molecular weight, temperature, and strain rate on the mechanical properties of PBX 9501MIkazaki, F., Kamiya, K., Uchida, K., Kawamura, M., Gotoh, A. and Fujiwara, S.@Shock modified silicon nitride and its sintering characteristicsIlkaev, 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. and Yaroshenko, V.V.UQuasi-isentropic compressibility of gaseous deuterium in pressure range up to 300 GPa(Ionita, A., Mas, E.M. and Clements, B.E.ATwo-scale FEM in the dynamic response of a heterogeneous material7A two-scale FEM formulation for heterogeneous materials{Iqbal, Z., Thadhani, N.N., Chawla, N., Rao, K.V., Skumryev, S., Ramakrishna, B.L., Sharma, R., Eckhardt, H. and Owens, F.J.BShock synthesis and processing of high temperature superconductors575-5781Itoh, S., Natamitsu, Y., Liu, Z.Y. and Fujita, M.;On von Neumann reflection of shock wave in condensed matter=Itoh, S., Liu, Z., Nakamura, Y., Nagano, S. and Nadamitsu, Y.&A study of electromagnetic stress gage233-2362Huang, S., Ding, F., Jing, F., Dong, Y. and Li, Z.:Dynamic quasi-isentropic compression of oxygen free copperHuang, F., Bai, C. and Ding, J.@Mechanical response of a composite propellant to dynamic loading491-4941Huang, S., Jin, X., Li, Z., Wang, X. and Guan, K.GExperimental measurements of 2169 stainless steel under dynamic loadingHuang, Y.K.:Notes on two general models for the inquiry of shock waves$Huang, X.S., Ono, M. and Mashimo, T.jPreparation of metastable alloy bulk material in Fe-Cu system by me< chanical alloying and shock compression'Huang, X., Kuramoto, K. and Mashimo, T.aNonequilibrium bulk material in W-Ag system prepared by mechanical alloying and shock compressionHuang, H. and Asay, J.R.ACompressive strength of shocked aluminum for stresses of 4-22 GPa9Huang, W., Patterson, J.E., Lagutchev, A. and Dlott, D.D.BShock compression spectroscopy with high time and space resolution	1265-1270Huang, F. and Zhang, L._DOP test evaluation of the ballistic performance of armor ceramics against long rod penetrationHudson�  III, L.C.aComputational studies of sympathetic detonation between two axially adjacent, cased charges of H6+Huffman, A.R., Brown, J.M. and Carter, N.L.ITemperature 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. and Guyot, F.KExperimental study of laser shock-released states of iron into a LiF window-Huston, A.L., Justus, B.L. and 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 viscosity243-248Hutchens, G.J./Approximate blast theory: Application to solids442-445bCalculation of chemical detonation waves with hydrodynamics and a thermochemical equation of state Howard, W.M. and Molitoris, J.D.-Modeling propagation of shock waves in metalsHowe, P.M. and Benson, D.J.7Progress in the development of a shock initiation modelCHoy, D.E.P., Akaishi, M., Park, J.K., Horie, Y. and Whitfield, J.K.,Shock compression of aluminum nitride powderHrbek, G.M.�Invariant functional forms for the second, third, and fourth order Birch-Murnaghan equation of state for materials subjected to hydrodynamic shocksPhysical 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. and Brar, N.S.EHigh strain rate behavior of coextruded polycarbonate/PMMA compositesHsiung, L.L.NOn the micromechanisms of shock-induced martensitic transformation in tantalum228-231,Hu, J., Mao, H.-K., Shu, J. and Hemley, R.J.VHigh-pressure energy dispersive X-ray diffraction technique with synchrotron radiation441-444=Hu, B.-Y., Dong, Q.-D., Han, C.-S., Wang, D.-S. and Hu, H.-B.GMicroanalysis of adiabatic shear fracture in explosive-filled cylinders	1229-1132"Hu, J.-B., Tan, H. and Jing, F.-Q.+Shock-induced phase transition of bromoform.Hu, H., Tang, T., Hu, B., Wang, D. and Han, C.`Longitudinal propagation of fracture surface in cylindrical metal shells under explosive loadingHuan, S. and Ding, J.0Probe for two-dimensional flow field measurement593-595Huan, S., Yang, W. and Ding, J.KExperimental calibration for the dynamic tensile coefficient of metal foils Huan, S., Lu, F.-Y. and Ding, J.GAttenuation of two-dimensional axisymmetric shock waves in porous Al2O3261-264Huang, Z.-P. and Zhang, H.-P.?Hugoniot and shear strength of titanium-6-4 under shock loading	Horie, Y.)Glass transition in shock loaded ceramics315-319ASome thermodynamical influences of defects in shock-loaded solids369-373BHorie, Y., Hoy, D.E.P., Simonsen, I., Graham, R.A. and Morosin, B.+Shock-wave synthesis of titanium aluminides749-754Horie, Y. and Kipp, M.E.[Modeling of chemical reactions in the mixture of Al-Ni powders under shock-wave compression8Shock compaction of ceramic powders in reactive mixtures479-485MComputational modeling of shock-induced chemical reactions in powder mixturesGHorie, Y., Tang, Z.P., Anderson, M.U., Graham, R.A. and Sheffield, S.A.QDiscrete meso-element dynamic analysis of stress profiles in HMX explosive powderHorie, Y. and Yano, K.JNonequilibrium fluctuations in shock compression of polycrystalline a-iron/Horie, Y., Hamate, Y., Greening, D. and Dey, T.nReactive burn modeling of solid explosives with a statistical treatment of hot spots in two spatial dimensions(Horioka, K., Aizawa, T. and Tsuchida, M.VIon-beam driven shock device using accelerated high density plasmoid by phased Z-pinch993-996Horn, P. and Gupta, Y.M.[Wavelength shift of the ruby luminescence R-lines due to shock compression along the c-axis	H""rz, F.SMorphology and chemistry of projectile residue in small experimental impact cratersHostler, S.R. and Brennen, C.E.IMeasurements and simulation of wave propagation in agitated granular bedsHouser, B. and Ingalls, R.;Pressure-induced transition in Rb.31WO3 as measured by XAFS*Howard, W.M., Souers, P.C. and Fried, L.E.AKinetic calculations of explosives with slow-burning constituents*Howard, W.M., Fried, L.E. and Souers, P.C.+Modeling of non-ideal aluminized explosives9Howard, W.M., Fried, L.E., Souers, P.C. and Vitello, P.A.@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. and Stacy, H.L._A survey of high explosive-induced damage and spall in selected metals using proton radiography477-482$Holtz, M., Sauncy, T. and Zallen, R.6Pressure-Raman studies of implantation disordered GaAs*Holtz, M., Solin, S.A. and Pinnavaia, T.J.<Pressure-Raman studies of layered alumino-silicate compounds	1539-1542aHomae, T., Okamoto, A., Nakamura, K.G., Kondo, K.-I., Yoshida, M., Hirabayashi, K. and Niwase, K.�Cooling rate threshold in transformation of C60 fullerene to amorphous diamond and highly disordered carbon in SCARQ experiments:Homae, T., Wakabayashi, K., Matsumura, T. and Nakayama, Y.7Reduction of explosion damage using sand or water layer	1289-1292aHongo, T., Kawai, N., Nakamura, K.G., Atou, T., Yubuta, K., Kusaba, K., Kikuchi, M. and Kondo, K.:Phase transition of MnF2 by shock compression up to 33 GPa224-227mHonnell, K.G., Velisavljevic, N., Adams, C.D., Rigg, P.A., Chesnut, G.N., Alkin�  Jr., R.M. and Boettger, J.C.!Equation of state for Ti-beta-21S55-58*Hooks, D.E., Dick, J.J. and Martinez, A.R..Shock experiments on explosive single crystals'Hooks, D.E., Ramos, K.J. and Bahr, D.F.JThe effect of cracks and voids on the dynamic yield of RDX single crystals789-794(Hooper, J., Romero, N.A. and Zerilli, F.KPredicting noncovalent interactions with nonlocal density functional theoryHoover, W.G. and Moran, B..Dynamic and stress intensity in elastic stripsCHoover, W.G., Moran, B., Holian, B.L., Posch, H.A. and Bestiale, S./Computer simulation of nonequilibrium processesHopkins, A. and Brar, N.S.#Raman spectroscopy of shocked water307-308Holmes, B.S.*Measuring pressure from short laser pulses;Holmes, N.C., Nellis, W.J., Graham, W.B. and Walrafen, G.E.191-200Holmes, B.S. and Aidun, J.B.4Piezoresistant response of vapor-deposited ytterbium519-524Holmes, N.C. and See, E.F.8Shock compression of low-density microcellular materials&Shock compression of low-density foams'Holmes, N.C., Nellis, W.J. and Ross, M.,Sound velocities in shocked liquid deuteriumUHolt, W.H., Mock, W., Soper, W.G., Coffey, C.S., Ramachandran, V. and Armstrong, R.W.BShear banding in titanium via reverse-ballistic impact experiments(Shock Waves in Condensed Matter  �� 1989IHolt, W.H., Mock�  Jr., W., Clark, J.B., Zerilli, F.J. and Armstrong, R.W.qGas-gun reverse ballistic impact deformation and fracture of armco iron Taylor specimens of differing grain sizes	1193-1196HHolt, W.H., Mock�  Jr., W., Anderson, M.U., Holman, G.T. and Graham, R.A.<  �Effect of particle morphology on input and propagated stress wave profiles for two highly porous polytetrafluoroethylene powders7Holt, W.H., Wilson, L.T., Mock�  Jr., W. and Simpson, B.7Dynamic properties of a shock loaded tungsten composite9Holt, W.H., Mock�  Jr., W., Santiago, F. and Gamache, R.M.FExperiment to capture gaseous products from shock-decomposed materials	1196-1199-Holt, W.H., Mock�  Jr., W. and Armstrong, R.W.KCrystal 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. and Thomas, K.A.=Development of a non-radiographic spall and damage diagnostic<Hixson, R.S., Johnson, J.N., Gray�  III, G.T. and Price, J.D.GEffects of interfacial bonding on spallation in metal-matrix composites555-558YHixson, R.S., Vorthman, J.E., Gustvsen, R.L., Zurek, A.K., Thissell, W.R. and Tonks, D.L.ESpall wave-profile and shock-recovery experiments on depleted uraniumIHixson, R.S., Vorthman, J.E., Zurek, A.K., Anderson, W.W. and Tonks, D.L.!Spall response of U-Nb (6%) alloyMHixson, R.S., Gray�  III, G.T., Rigg, P.A., Addessio, L.B. and Yablinsky, C.A.4Dynamic damage investigations using triangular waves;Hixson, R.S., Koller, D.D., Gray�  III, G.T. and Hayes, D.B.#Dynamic properties of a Pb-Sb alloy51-54Hoffman, N.M. and Swift, D.C.`Predictions of the microstructural contribution to instability seeding in beryllium ICF capsules?Hokamoto, K., Fujita, M., Tanaka, S.-I., Ayabe, M. and Itoh, S.bPossibility of making polycrystalline diamond using high-temperature shock consolidation techniqueHolian, B.L.5Modeling shockwave deformation via molecular dynamicsHolian, K.S..Hydrocode simulations of hypervelocity impactsNShockwave-induced plasticity via large-scale nonequilibrium molecular dynamics173-177KHolian, B.L., Germann, T.C., Lomdahl, P.S., Hammerberg, J.E. and Ravelo, R.=Shock waves and their aftermath: A view from the atomic scale35-41AHolland, K.G., Chhabildas, L.C., Reinhart, W.D. and Furnish, M.D.+Experiments on CERCOM SiC rods under impact2Holman�  Jr., G.T., Graham, R.A. and Anderson, M.U.4Shock response of porous 2Al + Fe2O3 powder mixturesJHolmes, N.C., Trainor, R.J., Anderson, R.A., Veeser, L.R. and Reeves, G.A.7Impedance-match experiments using high intensity lasers160-163Holmes, N.C.FHigh energy laser facilities at Lawrence Livermore National Laboratory648-651KHolmes, N.C., Mitchell, A.C., Nellis, W.J., Graham, W.B. and Walrafen, G.E.PShock recovery experiments on sandstone under dry and water-saturated conditions	1251-1254Hirai, H. and Kondo, K.-I.MAmorphous diamond from C60 fullerene by shock compression and rapid quenchingHirai, H. and Kondo, K.|A wide variety of carbon behavior: Amorphous diamond fabricated from C60 fullerence by shock compression and rapid quenching675-680MHiroe, T., Matsuo, H., Fujiwara, K., Tanoue, T., Yoshide, M. and Fujiwara, S.LA production of cylindrical imploding shocks in solid by exploding wire rows	1667-1670UHiroe, T., Matsuo, H., Fujiwara, K., Sakai, S., Abe, T., Yoshida, M. and Fujiwara, S.JGeneration of cylindrical imploding shocks in solid using a high explosive0Hiroe, T., Fujiwara, K., Abe, T. and Yoshida, M.LRapid expansion and fracture of metallic cylinders driven by explosive loads465-4682Hiroe, T., Fujiwara, K., Hata, H. and Tsutsumi, D.sSpall fracture of metallic circular plates, vessel endplates and conical frustrums driven by direct explosive loads%Hironaka, Y., Nicol, M. and Kondo, K.*Shock induced polarization in some liquids_Hironaka, Y., Saito, F., Yazaki, A., Fujimoto, Y., Nakamura, K.G., Kondo, K.-I. and Yoshida, M.KPump-probe X-ray diffraction for condensed matter in picosecond time domainDHironaka, Y., Saito, F., Yazaki, A., Nakamura, K.G. and Kondo, K.-I.HPicosecond time-resolved X-ray diffraction: Estimation of local pressure/Hirosaki, Y., Murata, K., Kato, Y. and Itoh, S.EEffect of void size on the detonation pressure of emulsion explosives930-933:Hixson, R.S., Bellamy, P.M., Duvall, G.E. and Wilson, C.R.8Effect of shock waves on the absorption spectrum of ruby282-286Hixson, R.S. and Fritz, J.N.Shock compression of iron69-70+Hixson, R.S., McQueen, R.G. and Fritz, J.N.IThe shock Hugoniot of 316 stainless steel and sound velocity measurements105-108@Wave propagation in materials with non-convex equations of state47-50,Hicks, D.L., Norwood, F.R. and Trucano, T.G..TOODY-WONDY calculations of penetration events544-547~Higginbotham, A., Albers, R.C., Germann, T.C., Holian, B.L., Kadau, K., Lomdahl, P.S., Murphy, W.J., Nagler, B. and Wark, J.S.-Simulating EXAFS patterns of shocked crystalsGHiggins, A.J., Jett"�, F.X., Yoshinaka, A.C., Lee, J.H.S. and Zhang, F.5Detonation initiation in preshocked liquid explosives	1023-1026Hild, F. and Denoual, C.EA probabilistic model for the dynamic fragmentation of brittle solidsHilfi, H. and Brar, N.S.aEvaluation of Johnson-Cook model constants for aluminum based particulate metal matrix compositesBHill, L.G., Seitz, W.L., Kramer, J.F., Murk, D.M. and Medina, R.S.CWedge test data for three new explosives: LAX112, 2,4-DNI, and TNAZ5Hill, L.G., Seitz, W.L., Forest, C.A. and Harry, H.H.DHigh explosive corner turning performance and the LANL mushroom test751-754AHill, L.G., Bdzil, J.B., Davis, W.C., Engelke, R. and Frost, D.L.gFront curvature analysis and detonation shock dynamics calibration for pure and sensitized nitromethane
Hill, L.G.%Development of the LANL sandwich testHill, L.G. and Aslam, T.D.OThe LANL detonation-confinement test: Prototyope development and sample resultsIBurning crack networks and combustion bootstrapping in cookoff explosionsaCritical temperature correlation for a near-unity aspect ratio charge of arbitrary size and shape829-832Hiltl, M. and Nahme, H.]Macro- and micromechanical response of a shock-loaded glass-ceramic at different temperaturesHiltl, M. and Hornemann, U.rStructural deformations on fluorophlogopite crystals of a pre-heated and experimentally shocked mica glass-ceramicFHiltl, M., Swift, R.P., Hagelberg, C.R., Carney, T.C. and Nellis, W.J.Hereil, P.L. and Doubax, F.?Shock induced polymorphic phase transition in a low-alloy steel,Hereil, P.L., Lassalle, F. and Avrillaud, G.UGEPI: An ICE generator for dynamic material characterisation and hypervelocity impactH"�reil, P.-L. and Mabire, C.6Temperature measurement of TiN under shock compression	1235-1238Herrmann, W.1On constitutive modelling for the shock physicist346-3596Elastic-plastic constitutive equations at large strain855-858DLee, J.S., Hokamoto, K., Raghukandan, K., Yamashita, K. and Itoh, S.XDevelopment of an underwater dynamic compaction technique for making Al-based composites	1106-1109Lee, R.J. and Gustavson, P.K.uElectrical 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. and Lawrence, G.W.Reactive materials studies169-1744Lee, P.R., Curtis, J.P., Mills, J.T. and Lynch, N.J.OOn the detonation of an explosive by the shock resulting from projectile impactGLee, G., Mock, W., Fedderly, J., Drotar, J., Balizer, E. and Conner, M.TThe effect of mech<  anical deformation on the glass transition temperature of polyurea5Lee, R.J., Forbes, J.W., Palermo, E. and Wilson, W.H.BEffect of electric fields on sensitivity of an HMX based explosiveLee, K.-Y. and Moore, D.S.JPressing induced polymorphic phase transition in submicron-sized gamma-HMXLee, J.J. and Zhang, F.RShock-induced reactions in cylindrical charges of titanium-silicon powder mixturesELee, M.P., Wang, G.M., Sung, P.H., Chang, W.L., Lee, Y.L. and Lin, K.=The attenuation of shock waves in PU foam and its application687-692ALee, R.J., Tasker, D.G., Forbes, J.W., Beard, B.C. and Sharma, J.CShock ignition of an explosive due to electrostatic discharge (ESD)2Lee, L.M., Hyndman, D.A., Reed, R.P. and Bauer, F.'PVDF applications in shock measurementsLee, R.J. and Tasker, D.G.TFactors affecting the sensitivity of energetic materials to electrostatic initiation(Lee, W.M., Demske, D.L. and Miller, P.J.oOptically measured temperature profile of a condensed aluminum-water medium undergoing a fast chemical reactionCLee, L.M., Johnson, D.E., Bauer, F., Reed, R.P. and Greenwoll, J.I.MPiezoelectric polymer PVDF application under soft x-ray induced shock loading%Lee, I.-Y.S., Wen, X. and Dlott, D.D.^Ultrafast spectroscopy of temperature and pressure jump and shock waves in molecular materials	1543-1546MLee, I.-Y.S., Hare, D.E., Hill, J.R., Franken, J., Suzuki, H. and Dlott, D.D..Ultrafast spectroscopy of the first nanosecondLee, W.H. and Clancy, S.P.EA strong shock tube problem calculated by different numerical schemesLee, R.J. and Forbes, J.W.LPVDF transducer response from an electrical discharge in an aluminized solid9Lee, J., Kuk, J.H., Song, S.-Y., Cjoi, K.Y. and Lee, J.W.6Detonation in an aluminized explosive and its modelingLee, M. and Bless, S.J.QA discrete impact model for effect of yaw angle on penetration by rod projectilesYLee, J.H.S., Goroshin, S., Yoshinaka, A., Romano, M., Jiang, J., Hooton, I. and Zhang, F.:Attempts to initiate detonations in metal-sulphur mixtures2Lee, J.J., Jiang, J., Choong, K.H. and Lee, J.H.S.eEffect of diethylenetriamine and triethylamine sensitization on the critical diameter of nitromethane0Lee, J., Kuk, J.-H., Kim, C.-H. and Hwang, E.-H.*Lawrence, R.J., Grady, D.E. and Hall, C.A.LThe response of ceramic powders to high-level quasi-isentropic dynamic loads	1213-1216DLawrence, R.J., Reinhart, W.D., Chhabildas, L.C. and Thornhill, T.F.0Hypervelocity impact flash at 6, 11, and 25 km/s&Leal, B., Presles, H.N. and Baudin, G..Shock initiation of detonation in nitromethane687-690-Lebedev, T.S., Korchin, V.A. and Burtny, P.A.FPetrovelocity PT-modeling and elastic inhomogeneity of the lithosphere
Lebedev, T.S.QProblem of geophysical application of the results of experimental PT-petrophysicsLebedev, T.S. and Savenko, B.Y.9Features of PT-changes of remanent magnetization of rocks811-814-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. and Fadeev, L.A.\Perturbaton method for study of shear strength of materials at pressures up to about 300 GPa*Lecume, S., Spyckerelle, C. and Sommer, F.IStructure of pristine crystal defects revealed by AFM and microtomography,Lee, L.M., Fogelson, D.J. and Williams, W.D.'Dynamic stress transducer qualificationLee, L.M. and Forrestal, M.J.ZMie-Gr"�neisen EOS based on second order Birch-Murnaghan isotherm and Steinberg parametersHeld, M.:Critical area for the initiation of high explosive charges555-557Fragment generators>Profile of detonation front by longitudinal gaps in HE charges667-670ZAnalytical initiation criteria of high explosives at different projectile or jet densities7Hellman, J.R., Kuroda, K., Heuer, A.H. and Graham, R.A.CMicrostructural characterization of shock-modified zirconia powdersHemley, R.J. and Mao, H.K.,Static compression to multimegabar pressures27-38Hemley, R.J. and Mao, H.-K.,New findings in static high-pressure science17-26MHemsing, W.F., Mathews, A.R., Warnes, R.H., George, M.J. and Whittemore, G.R."VISAR: Line imaging interferometer0Henninger, R.J., Maudlin, P.J. and Harstad, E.N.8Differential sensitivity theory applied to the MESA code	1781-1784VDifferential sensitivity theory applied to the MESA2D code for multi-material problemsQShock induced a-e phase change in iron: Analysis of MD simulations and experiment220-223�Hawreliak, J., Butterfield, M., Davies, H., El-Dasher, B., Higginbotham, A., Kalantar, D., Kimminau, G., McNaney, J., Milathianaki, D., Murphy, W., Nagler, B., Park, N., Remington, B., Thorton, L., Whitcher, T., Wark, J. and Lorenzana, H.YIn situ probing of lattice response in shock compressed materials using X-ray diffraction	1327-13321Hayek, M., Hasson, A., Bransky, I. and Halevy, D.bDerivation of the dynamics of an explosively driven ring from magnetically induced electric signalHayek, M. and Luttwak, G. Mach stem formation in plexiglasHayes, D.B. and Grady, D.E.>A thermal-viscous model for heterogeneous yielding in aluminum412-416*Hayes, D.B., Kipp, M.E. and Nunziato, J.W.IApplication of mixture theory to shock initiation of porous HNS explosive)Hayes, D., Hixson, R.S. and McQueen, R.G.�High pressure elastic properties, solid-liquid phase boundary and liquid equation of state from release wave measurements in shock-loaded copperHayes, D. and Hall, C.XCorrecting free surface effects by integrating the equations of motion backward in spaceZHayes, D.B., Gray�  III, G.T., hixson, R.S., Zurek, A.K., Vorthman, J.E. and Anderson, W.W.?Precursor suppression by shear stress relaxation in U-Nb(6-wt%)9Hayes, D.B., Gray�  III, G.T., Hall, C.A. and Hixson, R.S.8Elastic-plastic behavior of U6Nb under ramp wave loadingHayes, D.B.+Analyzing ramp compression wave experiments	1181-11853Hayun, S., Frage, N., Dariel, M.P. and Zaretsky, E.=Dynamic mechanical behavior of boron carbide based composites747-7502He, H.-L., Jin, X.-G., Chen, P.-X. and Wang, W.-K.=Shock induced crystallization of metallic glass Fe40Ni40P12B8625-627He, Y.-H. and Ding, J.9The shape of detonation front and the detonation velocity	1365-1368'Perturbations in high-velocity gas flowHaskins, P.J. and Cook, M.D..Short range interactions in diatomic molecules113-118IMany-body contributions to the short range potentials for helium and neonFThe origin and computation of many-body forces in the repulsive region67-708Monte Carlo simulation of 3-body effects in dense heliumLMolecular dynamics studies of shock initiation in a model energetic material	1341-1344QMolecular 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. and Briggs, R.I.OThe effect of additives on the detonation characteristics of a liquid explosive890-8934Haskins, P.J., Cook, M.D., Flower, H. and Wood, A.D.*Ab initio prediction of impact sensitivity4Detonation failure in ideal and non-ideal explosives
Hatano, T.QTemperature dependence of shock-induced plasticity: A molecular dynamics approachHatt, D.J. and Waschl, J.A.$A study of laser-driven flyer platesCHatton, P.D., Crain, J., Ackland, G.J., Clark, S.J. and Piltz, R.O.3Metastable structures of tetrahedral semiconductors5Hatton, P.D., Crain, J., Kawamura, H. and Akahama, Y.OComparative studies of rotating anode and synchrotron-based image plate systems	1699-1702XHawke, R.S., Brooks, A.L., Mitchell, A.C., Fowler, C.M., Peterson, D.R. and Shaner, J.W.'Railguns for e< quation-of-state research179-183Hawke, R.S.@Theory of spectroscopy of point defects in solids: Cr impuritues2Kupershtokh, A.L., Ershov, A.P. and Medvedev, D.A.2Coagulation of carbon clusters in detonation front:Kuroyama, Y., Itoh, K., Liu, Z.Y., Fujita, M. and Itoh, S.9A new apparatus for direct transformation from hBN to cBN615-617$Kusaba, K., Syono, Y. and Matsui, Y.bMolecular dynamics calculation of rutile-fluorite phase transition induced by uniaxial compressionKusaba, K. and Weidner, D.J.*Structure of high pressure phase I in ZnTe)Kuscher, G.F., Hohler, V. and Stilp, A.J.6Non-linear propagation of elasto-plastic waves in rods377-382Kusubov, A.S. and Swift, R.P.0Fracture initiation using tailored-pulse loading470-474Kutepov, A. and Kutepova, S.6The ab initio study of structural stability of uraniumKuznetsov, N.M.Stability of shock waves229-232!Kuznetsov, N.M. and Oleinik, I.I.UNumerical simulation of relaxation phenomena in xenon compressed by strong shock wave!Kwiatkowski, C.S. and Gupta, Y.M.POptical measurements to probe inelastic deformation in shocked brittle materials641-6446L'Eplattenier, P., Avrillaud, G. and Vanpoperynghe, J.^0D modelisation of the magnetic flux compression scheme for isentropic compression experiments	1188-1191)Labaste, J.L., Doucet, M. and Joubert, P.;Shocks induced by laser driven flyer plates. 1: Experiments	1213-1215*Labaste, J.-L., Brisset, D. and Doucet, M.NDensity-functional molecular dynamics simulations of shocked molecular liquids8Kress, J.D., Mazevet, S., Collins, L.A. and Blottiau, P.CQuantum molecular dynamics simulations of shocked molecular liquids Kroupa, J.L. and Rajendran, A.M.cThe use of Grady-Kipp type fragmentation model to describe the impact behavior of ceramic materialsIKr"�ger, L., Kanel, G.I., Razorenov, S.V., Meyer, L. and Bezrouchko, G.S.dYield and strength properties of the Ti-6-22-22S alloy over a wide strain rate and temperature range4Kubota, S., Nagayama, K., Shimada, H. and Matsui, K.:Numerical simulation of laser initiation of thin explosive468-471:Pressure calculation of reacting explosive by mixture ruleTKubota, S., Ogata, Y., Wada, Y., Katoh, K., Saburi, T., Yoshida, M. and Nagayama, K.3Observation of shock initiation process in gap test<Kubota, S., Ogata, Y., Wada, Y., Saburi, T. and Nagayama, K.AObservations of shock-induced partial reactions in high explosiveGKudoh, Y., Nagase, T., Ohta, S., Sasaki, S., Kanzaki, M. and Tanaka, M.JCrystal structure and compressibility of superhydrous phase B, Mg2Si6H8O36Kudoh, Y. and Kanzaki, M.IOn 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. and Cho, Y.S.INumerical modeling of an underwater explosion for an aluminized explosiveKuklja, M.M. and Kunz, A.B.1Modeling of shock compression of RDX with defectsKuklja, M.M.KHow point and line defects affect detonation properties of energetic solids454-459.Kuklja, M.M., Rashkeev, S.N. and Zerilli, F.J.UAb initio calculations of the electronic structure of 1,1-diamino-2,2-dinitroethyleneYThe atomic and electronic structure of defects in 1,1-diamino-2,2-dinitroethylene (FOX-7)>Kuksin, A.Y., Norman, G.E., Stegailov, V.V. and Yanilkin, A.V.8High explosive detonations in varying oxygen atmospheres563-567)Kowalski, E., Tauscher, B. and Ludwig, H.1Autoxiation of linolenic acid under high pressure*Kowalski, P.M., Mazevet, S. and Saumon, D.?The free-free opacity in warm, dense, and weakly ionized heliumKozhevnikov, V.F.JAn acoustical study of prewetting phenomena in a compressed metallic vaporKozhushko, A. and Maiboroda, V./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 transitions169-171@Kozlov, E.A., Buslova, E.S., Boboedova, V.A. and Gorbachev, D.M.fMacrokinetics 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. and Sapozhnikova, G.N.�The acquisition and investigation of submicrocrystal structure materials in experiments on loading of metal spheres by spherically converging shock waves535-537Kozlov, E.A. and Zhukov, A.V.+Phase transitions in spherical stress waves.Kozlov, E.A., Feldman, V.I. and Sazonova, L.V.�Crystallochemical structure of rock-forming minerals and peculiarities, sequence and completeness of physicochemical transformations in weak and strong shock waves4Kraichikov, S.S., Dremov, V.V. and Sapozhnikov, P.A.JMolecular dynamics investigation into influence of nano-particles in spall399-402#Kraidenov, V.F. and Itskevich, E.S.5The thermopower of HTC superconductors under pressureIKress, J.D., Bickham, S.R., Collins, L.A., Holian, B.L. and Goedecker, S.?Tight-binding molecular dynamics of shock waves in hydrocarbons*Kress, J.D., Mazevet, S. and Collins, L.A.RWindow problem and complementary method for shock-temperature measurements of iron	1555-1558UKondo, K., Hironaka, Y., Ito, H., Sugiura, H., Ozaki, S., Takeba, A. and Katayama, M.@A trial of the three-stage light gas gun with a preheating stageBKondo, K., Fatyanov, O.V., Hironaka, Y., Moritoh, T. and Ozaki, S.DPerformance of the three-stage light gas gun with a preheating stagetKonrad, C.H., Chhabildas, L.C., Boslough, M.B., Piekutowski, A.J., Poorman, K.L., Mullin, S.A. and Littlefield, D.L.8Dependence 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. and Peery, J.S.8Experimental bench mark data for ALEGRA code validations-Koritskaya, S.V., Trunin, I.R. and Arnold, W.QCalculated experimental investigation of the Armco iron deformation in shock wave Korth, G.E. and Williamson, R.L.3Impact shock generator from explosive-driven plates-Korth, G.E., Williamson, R.L. and Rabin, B.H.EMetal matrix composites from dynamic consolidation of powder mixtures3Kos, K., Millett, J.C.F., Bourne, N.K. and Deas, D.ILateral stress measurements and shear strength of an alumina-filled epoxy7Koskelo, A., Greenfield, S., Greening, D. and Smith, D.(New windows into shocks at the mesoscale�Koskelo, A.C., Greenfield, S.R., Paisley, D.L., McClellan, K.J., Byler, D.D., Dickerson, R.M., Luo, S.N., Swift, D.C., Tonks, D.L. and Peralta, P.D.=Dynamics of the onset of damage in metals under shock loading%Kotelnikov, A.D. and Montgomery, D.C.>Numerical study of shock propagation in inhomogeneous materialWKotulski, J.D., Anderson, M.U., Brock, B.C., Gomez, J., Graham, R.A. and Vittitoe, C.N.BDetermination of equivalent circuit for PVDF shock-pressure gauges	1739-17429Kovar, F.R., Trigger, K.R., Guymon, L.G. and Harvey, J.R.Kobayashi, T. and Sekine, T.HSpectroscopic studies of some aromatic compounds under shock compression$Kobayashi, T., Sekine, T. and He, H.>Vibrational spectra of nitro compounds under shock compression&Kober, E.M., Bdzil, J.B. and Son, S.F.FModeling 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. and Hall, T.2Radiative shock experiments using high power laserhKoenig, M., Benuzzi-Mounaix, A., Ozaki, N., Ravasio, A., Vinci, T., Lepape, S., Tanaka, K. and Riley, D.6High energy density physics on LULI2000 laser facilityKKolesnikov, S.A., Utkin, A.V., Ananin, A.V., Pershin, S.V. and Fortov, V.E.<  MReaction zone of steady-state detonation waves in dinitrodiazapentane and RDXVKoller, D.D., Rigg, P.A., Gray�  III, G.T., Jensen, B.J., Hayes, D.B. and Maestas, J.D.'Low pressure Hugoniot for U-Nb (6 wt.%)yKoller, D.D., Hixson, R.S., Gray�  III, G.T., Rigg, P.A., Addessio, L.B., Cerreta, E.K., Maestas, J.D. and Yablinsky, C.A.6Explosively driven shock induced damage in OFHC copper599-602.Koller, D.D., Gray�  III, G.T. and Hixson, R.S.<Shockwave profile and Bauschinger effect in depleted uraniumKondaurov, V.I. and Lomov, I.N.TApplication of the Godunov-type methods for solution of the condensed matter problem'Kondo, K., Ahrens, T.J. and Sawaoka, A.KElectrical and optical measurements on fused quartz under shock compression299-303-Kondo, K., Sawaoka, A., Sato, K. and Ando, M.8Shock compression and phase transformation of AlN and BP325-329	Kondo, K.0Phase transformation of AlN by shock compression4Shock compaction method for nanocrystalline ceramics609-612(Shock compression of carbons and diamondKondo, K.-I.8Shock to detonation transition in homogeneous explosivesKlimenko, V.Y.,Multiprocess model of detonation (Version 3)PTwo mechanisms of explosive initiation by the impact of a cylindrical projectile9Homogeneous mechanisms for detonation of heterogeneous HE-Kline, K., Horie, Y., Dick, J.J. and Wang, W.'Impact response of PBX 9501 below 2 GPa=Kline, K.L., Armstrong, R.W., Kramer, M.P. and Richards, D.W.GComparative model X-ray diffraction characteristics of RDX and aluminumZKlotz, S., Besson, J.M., Hamel, G., Nelmes, R.J., Loveday, J.S., Wilson, R.M. and Hull, S.XCrystal structure studies to 10 GPa with the Paris-Edinburgh cell: High pressure aspects	1577-1580:Klug, D.D., Svensson, E.C., Montfrooij, W. and Sears, V.F.1Low-frequency modes in high-density amorphous iceAKmetyk, L.N., Chhabildas, L.C., Boslough, M.B. and Lawrence, R.J.@Effect of phase change in a debris cloud on a backwall structure	1829-1832MKnapp, I., Millett, J.C.F., Gray�  III, G.T., Bourne, N.K. and Meziere, Y.J.E.6The shock Hugoniot of the intermetallic compound Ni3Al)Knudson, M.D., Gupta, Y.M. and Kunz, A.B.^Transformation mechanism and kinetics for the pressure-induced phase transition in shocked CdS255-260Knudson, M.D. and Gupta, Y.M.LUse of stimulated emission to measure R-line shifts in shocked ruby crystalsPKnudson, M.D., Hanson, D.L., Bailey, J.E., Hall, C.A., Deeney, C. and Asay, J.R.=Equation of state measurements in liquid deuterium to 100 GPa81-86`Kobayashi, T., Shoji, M., Deol, R.S., Buchan, N., Heuberger, W., Jakubowicz, A. and Roentgen, P.uPressure dependence of photoluminescence in GaInP grown on misoriented (100) GaAs by metalorganic vapor phase epitaxy	1495-1498EKobayashi, T., Sekine, T., Fatyanov, O.V., Takazawa, E. and Zhu, Q.Y.FShock temperatures of soda-lime glass measured by an optical pyrometer	1454-1457+Kinoshita, T., Kawamura, K. and Mashimo, T.GMD simulation of dislocation behavior in KCl under uniaxial compressionKipp, M.E. and Davison, L.7Analyses of ductile flow and fracture in two dimensionsKipp, M.E. and Grady, D.E.7Flaw nucleation and energetics of dynamic fragmentation?An application of geometric statistics to dynamic fragmentation435-439+Kipp, M.E., Setchell, R.E. and Taylor, P.A.5Homogeneous reactive kinetics applied to granular HNS7Shock compression and release in high-strength ceramics1Elastic wave dispersion in high-strength ceramics
Kipp, M.E.)Target response to debris cloud incidence	1849-1852/Kipp, M.E., Chhabildas, L.C. and Reinhart, W.D.5Elastic shock response and spall strength of concrete;Kipp, M.E., Chhabildas, L.C., Reinhart, W.D. and Wong, M.K.4Polyurethane foam impact experiments and simulationsKirby, I.J. and Chan, S.K.\Analysis of VOD-diameter data using an analytical two-dimensional non-ideal detonation model=Kirkpatrick, S.W., Curran, D.R., Erlich, D.C. and Klopp, R.W.XThree-dimensional analyses of plate impact experiments with circular and star geometries9Kirkpatrick, D., Argyle, A., Harrison, K. and Leggett, J.bA comparison of the blast & fragment mitigation performance of several structurally weak materialsHKishimura, H., Kawano, H., Hironaka, Y., Nakamura, K.G. and Kondo, K.-I.~Transient lattice response to the interaction between pulse-laser and semiconductors probed by time-resolved X-ray diffractionKiyanda, C.B. and Short, M.KModelling of detonation in PBX 9502 using a stiffened gas EOS mixture model!Klee, C., Kroh, M. and Ludwig, D.AExperiments on the attenuation of shock waves in condensed matter486-4903Klein, B., Frage, N., Zaretsky, E. and Dariel, M.P.DDynamic response of titanium carbide-steel, ceramic-metal compositesKlevert, P.cEvaluation 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 materialsKim, K. and Oh, S.I.HDynamic compaction of elastic-visco-plastic poeous materials under shock376-380UKim, K.Y., Palmour�  III, H., Batchelor, A.D., Kanda, H., Akaishi, M. and Fukunaga, O.OEffects of dynamic vs. static compaction on the sinterability of alumina powderKim, K.;Particle size dependent reaction rate in shocked explosivesKim, H. and Dlott, D.D.9Blast and shock wave dynamics in complex molecular solids<Kim, I.H., Jhung, K.S., Oh, K.-H., Hahn, K.B. and Hong, S.H."Shock induced chemistry of dry air9Shock compression of proteins: The energy landscape model	1448-1453KKim, V.V., Fortov, V.E., Lomonosov, I.V., Matveichev, A.V. and Ostrik, A.V.63D computer modeling of high-velocity impact phenomena Kim, Y.K., Wada, H. and Itoh, S.AShock compaction of MnAs1-xSbx powder using underwater shock wave:Kimmel, A.V., Sushko, P.V., Shluger, A.L. and Kuklja, M.M.[An effect of charged and excited states on decomposition of 1,1-diamino-2,2-dinitroethylene�Kimminau, G., Nagler, B., Higginbotham, A., Murphy, W., Wark, J., Park, N., Hawreliak, J., Kalantar, D., Lorenzana, H. and Remington, B.TSimulating picosecond X-ray diffraction from crystals using FFT methods on MD outputKing, T.R. and Shively, J.H.Nonlinear Hugoniots,King�  Jr., H.E., Cook, R.L. and Herbst, C.A.ADensity scaling of viscosity measured via diamond cell viscometry	1055-10587Kingma, K.J., Hemley, R.J., Veblen, D.R. and Mao, H.-K.GHigh-pressure crystalline transformations and amorphization in a-quartz.Kingsbury, S.J., Tsembelis, K. and Proud, W.G.<The dynamic properties of the Atlanta Stone Mountain graniteDMeasurement of particle velocity using a mutual inductance techniqueKerrisk, J.F. and Meier, J.K.:Comparisons between fast shock tube calculations and testsMKesler, G., Karow, H.U., Baumung, K., Fortov, V.E., Kanel, G.I. and Licht, V.2High-power light ion beams and intense shock waves	1887-1890Khantouleva, T.A.;Non-local theory of high-rate processes in structured mediaRNonlocal theory of macro-meso-level energy exchange in the shock compressed matterKhantuleva, T.A.OShock waves propagation in scope of the nonlocal theory of dynamical plasticity*Khasainov, B., Victorov, S. and Heuz"�, O.\A comparison of two approaches for fast and accurate hydrodynamic simulations of detonations;Khasainov, B.A., Kuhl, A.L., Victorov, S.B. and Neuwald, P.:Model of non-premixed combustion of aluminium-air mixtures449-4523Khishchenko, K.V., Lomonosov, I.V. and Fortov, V.E.SEquations of state for organic compounds over wide range of densities and pr<  essures3Khishchenko, K.V., Fortov, V.E. and Lomonosov, I.V.GHigh temperature, high pressure equation of state for polymer materialsUEquations of state and physical-chemical transformations of shocked organic compoundshKhishchenko, K.V., Fortov, V.E., Lomonosov, I.V., Pavlovskii, M.N., Simakov, G.V. and Zhernokletov, M.V.RShock compression, adiabatic expansion and multi-phase equation of state of carbon Kiiski, A.A. and Ruuskanen, P.R.@Wear resistance coatings of steel made with shock wave technique	1659-1662/Kiiski, A.A., Deribas, A.A. and Shtertser, A.A.EStudy on explosive compaction of fine copper, iron and nickel powders?Kikuchi, M., Syono, Y., Shimoda, N., Fukuoka, K. and Hiraga, K.DRedox reaction on oxide-metal interface boundary under shock loading?Kikuchi, M., Kawamata, S., Okuda, K., Fukuoka, K. and Syono, Y.6Keck, J.D., Hamkey, D.L., Graham, R.A. and Morosin, B.cShock-induced chemical and structural modification of zirconia, lead oxide and their mixed products82-86Keller, C.E.5Utility of shock models for underground nuclear tests485-487Keller, A.R. and Zhou, M.XExperimental characterization of the dynamic failure resistance of TiB2/Al2O3 composites795-798,Kelley, J.M., Joshi, V.S. and Guirguis, R.H.3Mechanical behavior of explosives at high pressures864-867QKennedy, J.E., Lee, K.-Y., Son, S.F., Martin, E.S., Asay, B.W. and Skidmore, C.B.<Second-harmonic generation and the shock sensitivity of TATBAKennedy, G., Ferranti, L., Russell, R., Zhou, M. and Thadhani, N.sInfluence of microstructural bias on the Hugoniot elastic limit and spall strength of two-phase TiB2+Al2O3 ceramics,Kennedy, G., Ferranti, L. and Thadhani, N.N.zEffect of processing induced microstructural bias of phase distribution on spall strength of two-phase TiB2-Al2O3 ceramicsnKennedy, J., Plaksin, I., Thomas, K., Martin, E., Lee, K.-Y., Akinci, A., Asay, B., Campos, J. and Direito, J.1Instrumented Floret tests of detonation spreading	1500-15033Kennedy, G.B., Kim, Y.K., Hokamoto, K. and Itoh, S.OStudy of underwater shock compaction device for compaction of titanium diborideKerley, G.I.)Theoretical equations of state for metals208-212!Kerley, G.I. and Switendick, A.C.?Theory of molecular dissociation in shocked nitrogen and oxygen95-100Kerley, G.I. and Wise, J.L.-Shock-induced vaporization of porous aluminum#Theory of calcite equation of state613-616+A new multiphase equation of state for iron.Kerr, J.H., Christiansen, E.L. and Crews, J.L.4Hydrocode modeling of advanced debris shield designs	1167-1170(Kerr, S., Kirkpatrick, D. and Garden, S.<Phenomenological description of the failure waves in glasses?Kaneshige, M.J., Renlund, A.M., Schmitt, R.G. and Erikson, W.W.LDevelopment of scalable cook-off models using real-time in situ measurements Kani, K., Yamada, T. and Abe, M.DHugoniot and electric resistivity measurements on amorphous selenium7Kanomata, T., Kawashima, T., Yoshide, H. and Kaneko, T.EPressure effect on the Curie temperatures of MnRuAs, MnPdAs and MnRhP	1469-14726Kanzleiter, R., Atchison, W., Bowers, R. and Guzik, J.RSimulated, theoretical and experimental shock trajectories in cylindrical geometry'Karakhanov, S.M. and Bordzilovsky, S.A.%The reshock and release waves in PTFEKarger, N. and L"�demann, H.-D.ESelf diffusion in liquid hydrogen fluoride at pressures up to 600 MPa	1321-1324:Karo, A.M., Walker, F.E., Cunningham, W.G. and Hardy, J.R.wTheoretical studies of shock dynamics in two-dimensional structures V. Microscopic constraints on shock-induced signals92-96.Kaschner, G.C., Gray�  III, G.T. and Chen, S.R.OThe influence of texture and impurities on the mechanical behavior of zirconium>Kasiraj, P., Vreeland�  Jr., T., Schwarz, R.B. and Ahrens, T.J.:Mechanical properties of a shock consolidated steel powderBKatayama, Y., Koyama, N., Tsuji, K., Oyanagi, H. and Shimomura, O.5EXAFS study of isolated selenium chain under pressure&Katayama, Y., Koyama, N. and Tsuji, K.=Optical absorption of isolated selenium chains under pressureKaul, A.M. and Rodriguez, G.CExperimental series on behavior of post-damage recollected materialVKawai, N., Atou, T., Ito, S., Yubuta, K., Kikuchi, M., Nakamura, K.G. and Kondo, K.-I.KThe amorphization and disproportionation of mullite under shock compression248-251VKawai, N., Inoue, K., Misawa, S., Riedel, W., Tanaka, K., Hayashi, S. and Kondo, K.-I.3The dynamic behavior of mortar under impact-loading-Kanel, G.I., Rasorenov, S.V. and Fortov, V.E.BThe failure waves and spallations in homogeneous brittle materialsQKanel, G.I., Razorenov, S.V., Utkin, A.V., Baumung, K., Karow, H.U. and Licht, V.0Spallations near the ultimate strength of solids	1043-1046-Kanel, G.I., Utkin, A.V. and Tolstikova, Z.G.<Response of the high-filled elastomers to shock-wave loading	1123-1126Kanel, G.I. and Utkin, A.V.QEstimation of the spall fracture kinetics from the free-surface velocity profiles9Kanel, G.I., Razorenov, S.V., Utkin, A.V. and Grady, D.E.5The spall strength of metals at elevated temperatures503-506OKanel, G.I., Baumung, K., Rush, D., Singer, J., Razorenov, S.V. and Utkin, A.V.-Melting of shock compressed metals in releasebKanel, G.I., Razorenov, S.V., Utkin, A.V., Dudin, S.N., Mintsev, V.B., Bless, S. and Simha, C.H.M.RInvestigation 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. and Chhabildas, L.C._Thin foil acceleration method for measuring the unloading isentropes of shock-compressed matter7Kanel, G.I., Razorenov, S.V., Baumung, K. and 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 tensionLMeziere, Y.J.E., Millett, J.C.F., Bourne, N.K., Wallwork, A. and Workman, A.XLongitudinal and lateral stress measurements in NiTi under one-dimensional shock loading1Meziere, Y.J.E., Millett, J.C.F. and Bourne, N.K.VThe effect of fibre orientation on the shock response of a glass fibre epoxy composite Mikhailov, A.I. and Osipov, R.S.=Interface instabilities between shock-compressed metal layersNEquation of state and Hugoniot locus for porous materials: P-a model revisited Compaction waves in granular HMX(Compaction wave profiles in granular HMX"Pore collapse and hot spots in HMX#Detonation wave profile in PBX 9501986-9890Micro-gap experiments and insensitive explosives8Menoni, C.S., Patel, D., Hafich, M.J. and Robinson, G.Y.FBand offsets in InGaP/InAlP multiple quantum wells using high pressure<Merritt, C.D., Huston, A.L., Justus, B.L. and Campillo, A.J.3Ultrafast shock induced uniaxial strain in a liquid%Merzhievsky, L.A. and Tyagelsky, A.V..Modelling of shock compression of porous mediaMescheryakov, Y.I.RMesoscopical effects and particle velocity distribution in shock compressed solids	1065-10709Macro-meso energy exchange in dynamically deformed steels$Mescheryakov, Y.I. and Divakov, A.K.DShock-induced mesoscopic processes and dynamic strength of materialsQMescheryakov, Y.I., Zhigacheva, N.I., Petrov, Y.A., Divakov, A.K. and Cline, C.F.bComparative analysis of uniaxial strain shock tests and Taylor tests for armor and maraging steels+Meserole, C.A., Fisher, G.L. and Funk, D.J.dSynthesis of ideal iron film samples for shock physics experiments using ultrafast X-ray diffraction7Meshcheryakov, Y.I., Atroshenko, S.A. and Divakov, A.K.iRole of shock-induced particle distribution in processes of dynamic localization during backside spallingJMeshcheryakov, Y., Atroshenko, S.A., Vasilkov, V.B. and Chernyshenko, A.I.[Criteria of transition from translational to rotational motion of media under shock loading407-410Meshcheryakov, Y.I.BKinetics of microstructure and strain rate dependence of mate<  rials623-625EMeshcheryakov, Y.I., Divakov, A.K., Zhigacheva, N.I. and Petrov, Y.A._Shock-induced a-w phase transition and mechanisms of spallation in shock loaded titanium alloys|Crystal-structure studies of II-VI semiconductors using angle-dispersive diffraction techniques with an image-plate detectorMcQueen, R.G. and Fritz, J.N.�Some techniques and results from high-pressure shock-wave experiments utilizing the radiation from shocked transparent materials193-207+McQueen, R.G., Fritz, J.N. and Morris, C.E.:The velocity of sound behind strong shock waves in 2024 AlMcQueen, R.G. and Marsh, S.P.4High explosive systems for equation-of-state studiesMcQueen, R.G. and Isaak, D.G.>Bromoform (CHBr3)  �� A very high-pressure shock-wave analyzer
McQueen, R.G.2The velocity of sound behind strong shocks in SiO2%Mears, A., Baily, F. and Strohmer, R.GThe dynamic response of piezoelectric probes to low density foam impact:Meenakshi, S., Godwal, B.K., Rao, R.S. and Vijayakumar, V.1On tetragonal distortion in indium under pressure	Mehta, S.?Theoretical melt curves of aluminium, copper, tantalum and lead258-261Meier, J.K. and Kerrisk, J.F.,An introduction to the fast shock tube (FST)Meir, G. and Clifton, R.J.9Dislocation mobility in high purity LiF from 100K to 300K303-307?Meisel, L.V., Scanlon, R.D., Johnson, M.A. and Lanzerotti, Y.D.hSelf-affine analysis on curved reference surfaces: Self-affine fractal characterization of a TNT surface*Mello, M.C., Prakash, V. and Clifton, R.J.EMulti-point interferometer for monitoring two-dimensional wave motion&Mendes, R., Plaksin, I. and Campos, J.'Single and two initiation points of PBX3Mendes, R., Plaksin, I., Campos, J. and Ribeiro, J.$Double slapper initiation of the PBXMenikoff, R. and Lackner, K.S.@Generating strong shock waves with a supersonic peristaltic pumpMenikoff, R..Numerical anomalies mimicking physical effects253-258Menikoff, R. and Kober, E.>Discrete layer verification of the LiF window spall diagnostic?McCluskey, M.D., Riley, B.D., Perenchio, A.M. and Knoblauch, M.2Confocal microscopy of water under static pressure	1109-1112&McDaniel, O., Moore, C. and Tindol, S.Laser ordnance initiation.McDonald, R., Tanner, W.G. and Alexander, W.M.oA study using molecular dynamics of the shock waves produced in an aluminum thin film via hypervelocity impactsXKagi, H., Wakatsuki, M., Hayakawa, S., Nakamura, F., Gohshi, Y., Kanda, H. and isoya, J.\Hugoniot measurements of high pressure phase stability of titanium-silicon carbide (Ti3SiC2)eJordan, J.L., Dick, R.D., Ferranti, L., Thadhani, N.N., Austin, R.A., McDowell, D.L. and Benson, D.J.YEquation of state of aluminum-iron oxide (Fe2O3)-epoxy composite: Modeling and experiment157-1606Jordan, J.L., Dorgan, R.J., Nixon, M.E. and Dick, R.D.UInitiation of polymer bonded explosive (PBXN-110) by combined shock and shear loading941-9446Joshi, V.S., Grebe, H.A., Thadhani, N.N. and Iqbal, Z.CEffect of packing density on shock consolidation of diamond powders	1251-1253,Joshi, V.S., Thadhani, N.N. and Graham, R.A.gMechanistic 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. and Holman�  Jr., G.T.8Shock compression of quartz and aluminum powder mixturesSJoshi, K.D., Suresh, N., Jyoti, G., Kulshreshtha, S.K., Gupta, S.C. and 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. and Brower, K.LShock-induced grain burning in mixtures of ammonium perchlorate and aluminum*Joshi, V.S., Banks, M.L. and Krebsbach, K.=Explosive bonding of plates with diffusion barrier interfacesJoshi, V.S. and Lee, R.J.qResolving mechanical response of plastic bonded explosives at high strain rate using split Hopkinson pressure barJoshi, V.S. and Imam, M.A.8Dynamic characterization of shape memory titanium alloys581-584Joshi, V.S. and Carney, T.C.JModeling of bullet penetration in explosively welded composite armor plateJoshi, V.S.dRecent developments in shear ignition of explosives using hybrid drop weight-Hopkinson bar apparatus<Jouet, R.J., Granholm, R.H., Sandusky, H.W. and Warren, A.D.	1911-19148Johnson, J.N., Hixson, R.S., Tonks, D.L. and Zurek, A.K.0Rate-dependent spallation properties of tantalum.Johnson, D.E., Davies, F.W. and Hedemann, M.A.[Characterization and reduction of prompt electrical noise on the Saturn PRS X-ray simulator&The features of the principal HugoniotJohnson, J.N. and Dick, J.J.Spallation studies in estane=Johnson, G.R., Stryk, R.A., Beissel, S.R. and Holmquist, T.J.lConversion of finite elements into meshless particles for penetration computations involving ceramic targets	1287-1290)Johnson, J.N., Dolan, D.H. and Howe, P.M.<EOS of mixtures: Phase transformation and explosive reaction}Determination of simple constitutive models for borosilicate glass using penetration-velocity data from ballistic experiments	1293-12969Johnson, D., Chapman, D.J., Tsembelis, K. and Proud, W.G..The response of dry limestone to shock-loading	1387-1390	Jonas, J.3High pressure NMR studies of proteins and membranesJones, H.D.GTheoretical equation of state for liquid nitromethane at high pressures103-106Jones, H.D. and Zerilli, F.J.!Analytic equation of state for H6Jones, S.D. and Gupta, Y.M.AImpact surface VISAR measurements in CdS shocked along the c-axisVJones, H.D., Zerilli, F.J., Holt, W.H., Mock�  Jr., W., Miller, P.J. and Lindfors, A.J.%Equation of state for porous mixtures9Theoretical equation of state for water at high pressures;Equation of state for liquid nitromethane at high pressuresJordan, J.L. and Thadhani, N.N.PShock compaction and synthesis of the titanium-silicon ternary carbide (Ti3SiC2)OEffect 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. and Barsoum, M.W.(John, R., Antoun, T. and Rajendran, A.M.>Effect of strain rate and size on tensile strength of concrete0John�  Jr., H.J., Hudson�  III, F.E. and Robbs, R.8High strain rate testing of AP/Al/HTPB solid propellantsJohn�  Jr., H.J. and Alamo, M.F./High strain rate testing of HMX-based explosive
Johnson, J.N.!Spallation by ductile void growth438-441/Calculated shock pressures in the aquarium test568-572*Johnson, J.D., Shaw, M.S. and Holian, B.L.Dense molecular thermodynamics)Johnson, M.L., Nicol, M. and Holmes, N.C.8Molecular emission spectra from shock-decomposed benzene@Johnson, K.A., Staudhammer, K.P., Elliott, N.E. and Medina, W.J.ZStrain and ambient temperature microstructural effects in shock loaded 304 stainless steel'Hot-spot reaction in unsustained shocksKMathews, A.R., Boat, R.M., Hemsing, W.F., Warnes, R.H. and Whittemore, G.R.%Full field Fabry-Perot interferometer)Mathieu, D., Simonetti, P. and Martin, P.LA model to study the electronic response to an impact in energetic materials)Mathieu, D., Martin, P. and Simonetti, P.RNonadiabatic simulation of valence electrons in solids under sustained shock waves,Matsuda, A., Nakamura, K.G. and Kondo, K.-I.\Time-resolved Raman spectroscopy of benzene derivatives under laser-driven shock compression
Matsui, M.Marston, P.L. and Pullen, G.L.<Cavitation in water induced by the reflection of shock waves515-519Marston, P.L. and Unger, B.T.9Rapid cavitation induced by the reflection of shock waves401-405
Marston, P.L.ZWavefront geometries giving transverse cusp and hyperbolic umbilic foci in acoustic shocks*Martin, M., Hanagud, S. and Thadhani, N.N.JDynamic mechanical behavior of nickel-aluminum re< inforced epoxy compositesIMartin, E.S., Thomas, K.A., Clarke, S.A., Kennedy, J.E. and Stewart, D.S.BMeasurements of the DDT process in exploding bridgewire detonators*Martin, M., Kecskes, L. and Thadhani, N.N.eDynamic compression of a zirconium-based bulk metallic glass confined by a 316 stainless steel sleeveMMartinez, A.R., Sheffield, S.A., Whitehead, M.C., Olivas, H.D. and Dick, J.J.!New LANL gas driven two-stage gun	1643-1646Martinez, E. and Servas, J.M.?Sound velocity Doppler laser interferometry measurements on TiN	1200-1203*Martinez, A.R., Hooks, D.E. and Dick, J.J.ALongitudinal and lateral ytterbium gauge measurements in PBX 9501792-795!Martynov, A.I. and Batsanov, S.S.5The calculation of dimensions of the steady Mach wave677-680KMas, E.M., Clements, B.E., Blumenthal, W.R., Cady, C.M. and Gray�  III, G.T.tApplying micromechanics to finite element simulations of split Hopkinson pressure bar experiments in high explosivesTMas, E.M., Clements, B.E., Blumenthal, W.R., Cady, C.M., Gray�  III, G.T. and Liu, C.$A viscoelastic model for PBX binders*Mas, E.M., Clements, B.E. and George, D.C.(Direct numerical simulations of PBX 95016Mas, E.M., Clements, B.E., Ionita, A. and Peterson, P.ZFinite element method calculations on statistically consistent microstructures of PBX 9501Mashimo, T.UMeasurements of the combined compression-shear shock waves of over 20 GPa in sapphire\Effects of a dynamic confinement on the penetration resistance of ceramics against long rodsMalkov, I.Y. and Titiov, V.M.5Structure and properties of detonation soot particles-Mandell, D.A., Holian, K.S. and Henninger, R.@MESA: A 3-D Eulerian hydrocode for penetration mechanics studiesMandell, D.A. and Wingate, C.A.JNumerical simulations of glass impacts using smooth particle hydrodynamicsDMang, J.T., Skidmore, C.B., Howe, P.M., Hjelm, R.P. and Rieker, T.P.LStructural characterization of energetic materials by small angle scatteringCMang, J.T., Skidmore, C.B., Son, S.F., Hjelm, R.P. and Rieker, T.P.`An optical microscopy and small-angle scattering study of porosity in thermally treated PBX 9501Mang, J.T. and 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\Mangeant, C., Lassalle, F., L'Eplattenier, P., H"�reil, P.-L., Bergues, D. and Avrillaud, G.LSYRINX project: HPP generators devoted to isentropic compression experiments&Mao, H.-K., Hemley, R.J. and Mao, A.L.0Recent design of ultrahigh-pressure diamond cell	1613-1616Margolin, L.G.ACalculations of cratering experiments with the bedded crack model465-469-Margolin, L.G., Smith, B.W. and DeVault, G.P./A micromechanical model of porous-brittle solid329-333)Mark, D.B., Petel, O.E. and Higgins, A.J.?Detonation failure thickness measurement in an annular geometry*Marlin, P., Penazzi, L. and Bensoussan, P.HLaser-induced shock waves in aluminum with PVDF and quartz stress gauges(Marom, H., Sherman, D. and Rosenberg, Z.8On the inelastic response of alumina under shock loading(Marsh, S.P., McQueen, R.G. and Tan, T.H.Acceleration of metal plates985-987Marsh, S.P. and Tan, T.-H. Hypervelocity plate acceleration	1033-10392Virtual memory techniques in Eulerian calculationsbComparing Lagrangian Godunov and pseudo-viscosity schemes for multi-dimensional impact simulations5Interface tracking in Eulerian and MMALE calculationsLuttwak, G. and Falcovitz, J.;Staggered mesh Godunov schemes for Lagrangian hydrodynamics9Lutz, S.S., Turley, W.D., Rightley, P.M. and Primas, L.E.#Gated IR images of shocked surfacesLynch, C.S. and Charest, J.A.9Practical considerations on the piezofilm gauge techniqueLyzenga, G.A. and Ahrens, T.J.&One-dimensional isentropic compression
Lyzenga, G.A.?Optical pyrometry at high shock pressure and its interpretation268-276Mabire, C. and H"�reil, P.L.7Shock induced polymorphic transition and melting of tin1Shock induced melting of lead: Experimental studyMader, C.L. and Gittings, M.!Numerical modeling of Munroe jets>Maienschein, J.L., Urtiew, P.A., Garcia, F. and Chandler, J.B.4Effect of microvoids on the shock initiation of PETN<Mailhot, C., Yang, L.H., McMahan, A.K. and Barbee�  III, T.W.Polymeric nitrogenMaillet, J.-B. and Bernard, S.-Uniaxial Hugoniostat: Method and applicationsMaillet, J.-B.MD simulations of hot spots379-384HMaillet, J.-B., Crouzet, B., Matignon, C., Mondelain, L. and Soulard, L.#Multiscale simulation of detonationMain, J.A. and Gazonas, G.A.<Impulsive loading of cellular media in sandwich constructionMajewski, P.0Effects of thin glue bonds on shock waves in LiF500-504(Majewski, P., Gupta, Y.M. and Seaman, L.<Tension-recompression response of shock loaded polycarbonate407-413Makhov, M.N.@Explosion heat and metal acceleration ability of high explosivesMaksimov, I.L.LThermomagnetic shock wave and magnetic flux penetration into superconductors.Malaise, F., Tranchet, J.-Y. and Collombet, F.EDetonation propagation in 180�� ribs of an insensitive high explosivePLubyatinsky, S.N., Loboiko, B.G., Filin, V.P., Kostitsin, O.V. and Smirnov, E.B.(Steady 2D detonations and the DSD theoryLucht, R.A. and Charest, J.A.FCalibration and use of a rugged new piezoresistive pressure transducer Lugovoy, P.Z. and Gouliaev, V.I.APropagation of shock wave fronts in anisotropic layered materialsLundblad, E.G.4High pressure synthesis of diamond in Sweden in 1953Luo, H. and Ruoff, A.L.,X-ray diffraction study of sulfur to 212 GPa43-48%Luo, H., Greene, R.G. and Ruoff, A.L.BX-ray diffraction and Raman scattering studies of C6H5Cl to 60 GPaEOn the ultimate yield strength of diamond: Finite elasticity approach0High-pressure Raman scattering studies of sulfurMLuo, S.-N., Swift, D.C., Tierney, T., Xia, K., Tschauner, O. and Asimow, P.D.iTime-resolved X-ray diffraction investigation of superheating-melting of crystals under ultrafast heating(Luo, S.-N., Ahrens, T.J. and Swift, D.C.$Melting at the limit of superheating172-175
Luo, S.-N.BLimit of superheating and supercooling in solid-liquid transitions252-257Luther, G.G. and Vesser, L.RA microwave interferometer to measure particle and shock velocities simultaneouslyLuther, G.G. and Warthen, B.J.6Microwave interferometry to elucidate shock properties	1755-1758Luttwak, G.-Numerical simulation of water jet penetration%Luttwak, G., Florie, K. and Venis, A.(Numerical simulation of soft body impactSecond order discrete rezoning	1777-1780)Luttwak, G., Rosenberg, Z. and Kivity, Y.&Long rod penetration in oblique impactLuttwak, G. and Mayseless, M.dThree dimensional numerical simulations of the effect of cyclic perturbations on liner accelerations,Luttwak, G., Cowler, M.S. and Birnbaum, N.K.CEffects of processing techniques on the shock response of beryllium)Lopatin, C.M., Bless, S.J. and Brar, N.S.-Dynamic unloading behavior of soda lime glass*Lopatin, C., Wittman, C. and Holmquist, T.7Dynamic compressive properties of an explosive simulant495-496Lorenz, B. and Orgzall, I.>Optical absorption studies of sulfur at pressures up to 20 GPaLouro, L.H.L. and Meyers, M.A.;Stress-wave induced fragmentation in alumina-based ceramics*Shock Compression of Condensed Matter 1989,Louzada, K.L., Stewart, S.T. and Weiss, B.P.lShock demagnetization of pyrrhotite (Fe1-xS, x ��0.13) and implications for the Martian crust and meteorites	1476-1479ZLoveday, J.S., Wilson, R.M., Nelmes, R.J., Besson, J.M., Klotz, S., Hamel, G. and Hull, S.<  SCrystal structure studies with the Paris-Edinburgh cell: Neutron scattering aspects413-416Lowe, C.A. and Greenaway, M.W.'The dynamic compaction of microfine HMXL""wer, T. and Sigel, R.JUniform shock waves driven by thermal radiation from laser-heated cavitiesLu, F., Huan, S. and Ding, J._Viscoplasticity and porosity effects on the shock propagation in PMMA and porous aluminum oxide	1013-1016Lu, X. and Hanagud, S.V.TStructural phase transitions and equation of state of aluminum from first principlesLu, X. and Hanagud, S.sHigh pressure & high temperature equation of state and magnetic phase transitions of hematite from first principles Lu, X., Hamate, Y. and Horie, Y.5Physics-based reactive burn model: Grain size effects#Lubyatinsky, S.N. and Loboiko, B.G.>Reaction zone measurements in detonating aluminized explosivesEDensity effect on detonation reaction zone length in solid explosives743-746�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. and Filin, V.P./Lomonosov, I.V., Bushman, A.V. and Fortov, V.E.6Equations of state for metals at high energy densities2Wide-range multi-phase equation of state of metals121-124@Lomonosov, I.V., Bushman, A.V., Fortov, V.E. and Khishenko, K.V.2Caloric equations of state of structural materials Lomonosov, I.V. and 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?CLomonosov, I.V., Fortov, V.E., Khishchenko, K.V. and Levashov, P.R.Shock wave stability in metalsZPhase diagrams and thermodynamic properties of metals at high pressures, high temperatures;Theoretical investigation of shock wave stability in metalsKLomonosov, I.V., Fortov, V.E., Kim, V.V., Matveichev, A.V. and Ostrik, A.V.JInfluence of equation of state on results of hypervelocity impact modelingLomonosov, L.V.+Multi-phase equations of state for aluminumLomov, I.N. and Kondaurov, V.I.RFracture of brittle material with initial porosity under high energy density flows)Lomov, I.N., Antoun, T.H. and Glenn, L.A.IExplosion in the granite field: Hardening and softening behavior in rocks6Lomov, I.N., Antoun, T.H., Wagoner, J. and Rambo, J.T.;Three-dimensional simulation of the Baneberry nuclear event	1462-1465Lomov, I. and Liu, B.wApproximation of multifluid mixture response for simulation of sharp and diffuse material interfaces on a Eulerian grid1Lomov, I., Liu, B., Georgevich, V. and Antoun, T.RNumerical simulation of interaction of hypervelocity particle stream with a target#Long, K.S., Young, D. and Lee, F.H.-A new full-range equation of state for copper213-217Longy, F. and Cagnoux, J.-Plate impact recovery experiments of ceramicsMLoomis, E., Luo, S.N., Greenfield, S., Paisley, D., Swift, D. and Johnson, R.hDiscrete meso-element simulation of the failure behavior of short-fiber composites under dynamic loading1Penetration depth time history measurement method	1039-1042Liu, C.'Fracture of the PBX 9501 high explosive786-791$Liu, B.T., Lomov, I. and Glenn, L.A.ONumerical modeling of mixing and venting from explosions in undergound chambers	1472-14754Liu, B.T., Lomov, I.N., Blank, J.G. and Antoun, T.H.ASimulation of comet impact and survivability of organic compounds	1391-1394+Llorca, F., Juanicotena, A. and Dambrun, C.�Modeling of the high strain and high strain rate behavior of tantalum: Application to the dynamic expansion of a spherical shellLlorca, F. and Buy, F.eThe contribution of the expanding shell test to the modeling of elastoplasticity at high strain rates!Llorca, F., Buy, F. and Farre, J.5Experimental analysis of shock wave effects in copper638-641Llorca, F. and Roy, G.9Metallurgical investigation of dynamic damage in tantalum%Lloyd, A., Borg, J.P. and Downs, T.J.+Liquid breakup under one-dimensional strain634-637,Lloyd, C.E., Greenaway, M.W. and Proud, W.G.?Study of sensitivity and repeatability of piezoelectric sensors	1195-1198Lloyd, C.E. and Proud, W.G.NMeasuring density of high-velocity metallic sprays using piezoelectric sensorsZLoboyko, B.G., Alekseev, A.V., Litvinov, B.V., Sumin, V.D., Taybinov, N.P. and Filin, V.P.FInvestigation of explosives mechanic impact sensitivity on the samples_Loiseau, J., Szirti, D., Batchelor, P., Higgins, A.J., Tanguay, V., Yoshinaka, A. and Zhang, F.PPhase velocity generator for a two-stage implosion driven hypervelocity launcher	1297-1300FLojkowski, W., Porowski, S., Rebkin, E.I., Straumal, B.B. and Gust, W.`Pressure effect on grain boundary dewetting and premelting transition in a Fe-6 at.%Si bicrystal	1205-1208CA study of zoning requirements for 2-D and 3-D long-rod penetration'Littlefield, D.L. and Cour-Palais, B.G.TScaling relationships for evaluation of performance of advanced space debris shieldsLittlefield, D.L.COptimization of the performance of segmented-telescopic penetratorsJAn algorithm for modeling contact in three-dimensional Eulerian hydrocodes!Littlefield, D.L. and Baker, E.L.NImplementation 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. and 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 samples981-983=Liu, W.-N., Liu, H.-J., Feng, Y.-C., Sun, S.-L. and Su, W.-H.ePressure-induced grain fining and noncrystallization of crystal structure in Eu2+ activated Sr-borate.Liu, H., Liu, W., Guan, Z., Sun, S. and Su, W.LCrystallization of amorphous SrB4O7 under high pressure and high temperatureLiu, J. and Vohtra, Y.K.PCalibration and fluorescence intensities of Sm:doped YAG to ultra high pressures	1681-1684VLiu, F.-S., Chen, X.-M., Chen, P.-S., Chen, J.-X., Tan, H., Gou, Q.-Q. and Jing, F.-Q.9Equation of state and conductivity of shocked heavy waterLiu, L.-Q. and Katsabanis, P.D.BA constitutive model for predicting rock fragmentation by blastingLiu, C. and Ahrens, T.J.-Stress wave attenuation in shock damaged rockLiu, C.L. and Ahrens, T.J.2Wave generations from confined explosions in rocks Liu, Z., Nagano, S. and Itoh, S.2Overdriven detonation phenomenon in high explosive$Liu, C., Ahrens, T.J. and Brar, N.S.'Vitreous Ge02 response to shock loadingLiu, W., Tang, Z.P. and Liu, Y.%Li, X.-Z., Tang, Z.P. and Zhou, G.-Q.FMechanism of the shock-induced phase transition in CdS single crystalsLi, X.-J. and Zhang, K.>Explosive welding of multilayer amorphous ribbons into a plate>Li, D.J., Feng, J., Ding, B.Z., Yao, B., Hu, Z.Q. and Su, W.H.]The high pressure amorphization and the computer simulation of the pressure-quenching process=Li, D.J., Guo, M., Hu, Z.Q., Ding, B.Z., Yao, B. and Su, W.H.8Pressure-induced amorphization mechanism of Cd-Sb system9Li, M.M., Strachan, D.J., Tamargo, M. and Weinstein, B.A.<Pressure-induced instability of deep acceptor states in ZnSe#Li, H., Su, W., Li, L. and Wang, Y.ZStudy on the synthesis process of CeTbO3 compound under high pressure and high temperature2Li, X.-Z., Tang, Z.-P., Zhou, G.-Q. and Lin, S.-B.3Thermal effects in laser induced strong shock waves	1907-1910Liang, Y.-M. and Zhao, H.-Y.ATwo methods for measuring shock relations with improved EMV gauge%Liang, D., Chou, P.C. and Hashemi, J.3Shock and shear effects in explosives due to impact;Libersky, L.D., Randles, P.W., Bourne, N. and Vignjevic, R.[Simulation of void collapse in ammonium nitrate using a meshfree Lagrangian particle method Libersky, L.D. and Randles, P.W..Shocks and discontinuities in particle methodsLiddiard, T.P. and Forbes, J.W.GShock waves in fresh water generated by detonation of pentolite spheres578-582?Lightstone, J.M., Carney, J.R., Boswell, C.J. and Wilkinson, J.XTime-resolved spectroscopic measurements of aluminum oxidation<   in a laser ablation event0Lindfors, A.J., Finnegan, S.A. and Boteler, J.M.JA study of shock-induced reactivity in a porous pyrotechnic powder mixture7Littlefield, D.L., Anderson�  Jr., C.E. and Skaggs, S.R.2Analysis of penetration of steel and Al2O3 targets	1793-1796)Littlefield, D.L. and Anderson�  Jr., C.E.FLemke, R.W., Knudson, M.D., Davis, J.-P., Bliss, D.E. and Harjes, J.C.sSelf-consistent 2D magneto-hydrodynamic simulations of magnetically driven flyer plate experiments on the Z-machine	1175-1180'Le"e"n, G.C., Romo, S.R. and Tchijov, V.4A kinetic model of multiple phase transitions in ice(Lettieri, T., Kelley, J. and Ehrlich, C.OInvestigation of annular forces using an oscillating, gas-operated piston gauge	1605-1608'Leung, K.P., Yao, S.S. and Alfano, R.R.OPicosecond laser induced shock wave pressure measurements in Al, C-Si, and GaAs343-345PLevashov, P.R., Fortov, V.E., Khishchenko, K.V., Lomov, I.N. and Lomonosov, I.V.Shock wave data baseCLevashov, P.R., Fortov, V.E., Khishchenko, K.V. and Lomonosov, I.V.#Equation of state for liquid metals\Analysis of isobaric expansion data based on soft-sphere equation of state for liquid metals71-74:Levashov, P.R., Filinov, V.S., Fortov, V.E. and Bonitz, M.HThermodynamic properties of nonideal strongly degenerate hydrogen plasmauAuthors' reply to R. Pollock's comments on 'Thermodynamic properties of nonideal strongly degenerate hydrogen plasma'125-126CLevashov, P.R., Khishchenko, K.V., Lomonosov, I.V. and Fortov, V.E.PDatabase on shock-wave experiments and equations of state available via internet$Levashov, P.R. and Khishchenko, K.V.GTabular multiphase equations of state for metals and their applications59-62%Levy, A., Barak, G. and Ashkenazi, J.cThermodynamics of 3d metals  �� Band structure effects and their disappearance at high temperaturesLi, C.H. and Clifton, R.J.EDynamic stress-strain curves at plastic shear strain rates of 105 s-1360-366Li, W.GSimplified equation of state P=P(r,E) and P=P(r,T) for condensed matter167-173Li, H. and Wang, Z.CFree Lagrange method for two dimensional hydro-elastic-plastic flow7L"�ger, J.M., Haines, J., Atouf, A. and Tomaszewski, P.iPhase transitions in several metal dioxides as studied by angle dispersive X-ray diffraction up to 50 GPaLegrand, M.FInterface instabilities occurring during an explosive driven implosion(Legrand, B., Blanco, E. and Martinez, E.fValidation of a multitechnical device aimed to reach the temperature of a material under shock loading	1191-1194Leiper, G.A. and Kirby, I.J.�A method of parameterising hydrocode kinetic models for non-ideal explosives based on the variation of detonation velocity with charge diameter917-922Leiper, G.A. and Hackett, A.4Radial motion in unconfined axisymmetric detonations2Leitsin, V.N., Skripnyak, V.A. and Dmitrieva, M.A.jThree-scale model for numerical simulation of mechano-chemical processes in shock-compressed powder bodies6Lemar, E.R., Forbes, J.W., Erkman, J.O. and Watt, J.W.,NSWC/WO light gas gun and explosive facility663-667(Lemar, E.R., Forbes, J.W. and Watt, J.W.RUnreacted Hugoniot and shock initiation studies of composition B-3 and PBXW-109(I)539-5415Lemar, E.R., Forbes, J.W., Tasker, D.F. and Bur, A.J.DPolyvinylidene fluoride transducer for dynamic pressure measurements503-508Lemar, E.R. and Forbes, J.W.5Detonation wave curvature of cast Comp B and PBXN-111.Lemar, E.R., Forbes, J.W. and Sutherland, G.T.<Detonation wave velocity and curvature of IRX-4 and PBXN-110/Lemar, E.R., Forbes, J.W. and Cowperthwaite, M.lOblique shock wave calculations for detonation waves in brass confined and bare PBXN-111 cylindrical charges/Lemberg, V.F., Psakhie, S.G. and Zolnikov, K.P.BThermodynamic properties of simple metals under shock wave loading75-78Lemberg, V.F. and Psakhie, S.G.[The search for the conditions necessary to initiate chemical reaction by particle collision=Enhancement of detonation properties by electric energy input865-868-Lee, L.M., Montgomery, S.T. and Jilbert, P.H.,Multi-element quartz shock gauge developmentLee, R.J. and Joshi, V.S.iUse of high-speed photography to augment split Hopkinson pressure bar measurements of energetic materials860-863�Lee, K.K.M., Benedetti, L.R., Mackinnon, A., Hicks, D., Moon, S.J., Loubeyre, P., Occelli, F., Dewaele, A., Collins, G.W. and Jeanloz, R.sTaking thin diamonds to their limit: Coupling static-compression and laser-shock techniques to generate dense waterALee, K.-Y., Kennedy, J.E., Asay, B.W., Son, S.F. and Martin, E.S.cPreparation and characterization of fine-particle NTO and its formulation with aluminum nanopowders7Oleynik, I.I., Zybin, S.V., Elert, M.L. and White, C.T.GNanoscale molecular dynamics simulation of shock compression of silicon2Shear stresses in shock-compressed covalent solidsfOleynik, I.I., Conroy, M., Zybin, S.V., Zhang, L., van�  Duin, A.C., Goddard�  III, W.A. and White, C.T.tEnergetic materials at high compression: First-principles density functional theory and reactive force field studies)Oleynik, I.I., Conroy, M. and White, C.T.SAnisotropic constitutive relationships in energetic materials: Nitromethane and RDXOlson, M.A. and Kimsey, K.D.ICalculation of elastic-plastic wave propagation on the Connection Machine=Orlikowski, D., Correa, A.A., Schwegler, E. and Klepeis, J.E.@A Steinberg-Guinan model for high-pressure carbon: Diamond phaseXOrlikowski, D., Nguyen, J.H., Patterson, J.R., Minich, R., Martin, L.P. and Holmes, N.C.YNew experimental capabilities and theoretical insights of high pressure compression waves	1186-1191.Orphal, D.L., Kozhushko, A.A. and Sinani, A.B.^Possible detection of failure wave velocity in SiC using hypervelocity penetration experiments2Orphal, D.L., Walker, J.D. and Anderson�  Jr., C.E.4Ballistic response of fabrics: Model and experiments$Orphal, D.L. and Anderson�  Jr., C.E.HCrater diameter for L/D=1 like-material impacts on semi-infinite targets	1347-1350MOrphal, D.L., Behner, T., Hohler, V., Anderson�  Jr., C.E. and Templeton, D.W.JNumerical simulation of a sample recovery fixture for high velocity impact837-842Novikov, S.A. and Pushkov, V.A.UStudy of steel crack resistance under dynamic loading and temperature range 20-300��C@Novikov, S.A., Pushkov, V.A., Sinitsyn, V.A. and Gray�  III, G.T.UCrack resistance of aluminium composite under shock loading at different temperatures455-457Nunziato, J.W.8Initiation and growth-to-detonation in reactive mixtures581-588Nutt, G.L. and Hallquist, J.O.$Calibration of piezoresistive gaugesNutt, G.L. and Erickson, L.M.+Reactive flow Lagrange analysis in RX-26-AFFO'Donoghue, P.E., Anderson�  Jr., C.E., Renick, J.D. and O'Kelley, D.K.SFlyer plate impact of dry soils: A comparison of analytic and numerical predictionsGO'Donoghue, P.E., Friesenhahn, G.J., Anderson�  Jr., C.E. and Parr, C.H.JAnisotropic 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. and Wilke, M.D.8Ellipsometry in the study of dynamic material propertiesOgilvie, K. and Duvall, G.E.6Time resolved spectroscopy of shock compressed liquids292-295"Ogorodnikov, V.A<  . and Ivanov, A.G.5On the nature of scale effect in high-rate fracturing8Ogura, T., Nakamura, K.G., Takenaka, H. and Kondo, K.-I.DShock temperature of NaCl measured with wide-band optical radiometry	1215-1218Oh, K.-H. and Persson, P.-A.:Full range Hugoniot equation of state for porous materials	Oh, K.-H.IGraphical construction of P-Up porous Hugoniots from solid Hugoniot curveQComparison of high energy shock states for reactant material and product material4Oh, K.-H., Jhung, K.S., Kim, I.H. and Persson, P.-A.YTwo-variable feature of Gr"�neisen function observed in experimental porous Hugoniot data^Coupled thermal/chemical/mechanical modeling of insensitive explosives in thermal environments1Nonequilibrium detonation of composite explosives2Nichols�  III, A.L., Tarver, C.M. and McGuire, E.M.2ALE3D statistical hot spot model results for LX-173Statistical hot spot model for explosive detonation465-470Nicholson, D.W.2Shock induced temperature rise in a titanium plate)Nicol, M., Johnson, S.W. and Holmes, N.C.MShock-chemistry of benzene studied by spectra from and behind the shock front471-476#Nikkel�  Jr., D.J. and Lassila, D.H.TThe effect of the constitutive response on the predicted temperatures in copper jets	1857-1860QNikolaev, D.N., Filimonov, A.S., Fortov, V.E., Lomonosov, I.V. and Ternovoi, V.Y.3Mechanical properties of preshocked sapphire driverNNikolaev, D.N., Fortov, V.E., Filimonov, A.S., Kvitov, S.V. and Ternovoi, V.Y.@SiO2-aerogel plasma properties in the energy range up to 65 kJ/g1Nikolaev, D.N., Ternovoi, V.Y. and Pyalling, A.A.KNickel critical point parameters from shock experiments with porous samplesBNikolaev, D.N., Emelyanov, A.A., Pyalling, A.A. and Ternovoi, V.Y.fStudy of near-critical point thermodynamics of molybdenum by isentropic expansion and isobaric heating?Experimental determination of applied forces during penetration7Lee, Y.K., Williams, F.L., Graham, R.A. and Morosin, B.7Specific surface measurements of shock modified powders%Lee, C.K.B., Baker, J. and Peyton, S.VThe effect of equilibrium modeling of saturated quartz in energy coupling calculations7Lee, E.L., van�  Thiel, M., Green, L.G. and Mitchell, A.EDetonation product EOS: The region above the Chapman-Jouguet pressure5Lee, L.M., Williams, W.D., Graham, R.A. and Bauer, F.LStudies of the Bauer piezoelectric polymer gauge (PVF2) under impact loading497-502WCrystal growth of energetic materials during high acceleration using an ultracentrifuge489-491-Lanzerotti, M.Y.D., Autera, J. and Sharma, J./Crystal growth of TNAZ during high accelerationLanzerotti, Y. and Sharma, J.[Mechanical properties of energetic materials during high acceleration in an ultracentrifuge595-597CMechanical behavior of energetic materials during high acceleration853-8558Lanzerotti, Y., Capellos, C., Travers, B. and Sharma, J.CMechanical behavior of TNAZ/CAB explosives during high acceleration783-785+Lanzerotti, Y., Sharma, J. and Capellos, C.FMechanical behavior of TNAZ/Hytemp explosives during high acceleration8Lappo, K.N., Todd, S.N., Anderson, M.U. and Vogler, T.J.QNon-shock initiation of the plastic bonded explosive PBXN-5: Experimental results2Last, H.R., Garrett�  Jr., R.K. and Rajendran, A.M.LA comparative study of high strain rate behavior of three martensitic steelsLaverty, R. and Gazonas, G.JTransient stress optimization of elastic and viscoelastic composite stripsLawrence, W.8Measurement problems in high velocity impact experiments534-5386Measurements of penetration using instrumented targetsLawrence, R.J.-Stand-off shields for hypervelocity particles>The equivalence of simple models for radiation-induced impulseLawrence, W. and Franz, R.E.8Designing a cutting charge to cut the shaped charge jets:Analytic models for hypervelocity particle shield analysis	1837-18408Lawrence, R.J., Asay, J.R., Trucano, T.G. and Hall, C.A.-Analysis of radiation-driven explosive flyersNAnalysis of the interaction of short-pulse high-fluence radiation with targets	1185-1188lLawrence, R.J., Mehlhorn, T.A., Haill, T.A., Budge, K.G., Trucano, T.G., Cochrane, K.R. and MacFarlane, J.J.>Analysis of radiation-driven jetting experiments on NOVA and ZPInvestigation of driving plasma materials for laser acceleration of flyer plates	1189-1192)Laber, M.W., Brar, N.S. and Rosenberg, Z.!Shock response of 5083-0 aluminumLadd, A.J.C.?Molecular dynamics studies of plastic flow at high strain rates267-2807Laine, L., Ranestad, "�., Sandvik, A. and Snekkevik, A.2Numerical simulation of anti-tank mine detonations8Laity, P.R., Siviour, C.R., Church, P.D. and Proud, W.G.;High strain rate characterisation of a polymer bonded sugar	Lalle, P.KUse of glass as window in interferometric measurements of particle velocity751-7581Us-Up relation from isothermal equations of stateLalle, P. and Courchinoux, R.Melting on the Hugoniot207-210Lambourn, B.D.LAn interpretation of particle velocity histories during growth to detonation*An improved EOS for non-reacted explosives>Lambourn, B.D., Whitworth, N.J., Handley, C.A. and James, H.R.,A finite strain, non-reacted EOS for PBX9502;Lambrakos, S.G., Oran, E.S., Boris, J.P. and Guirguis, R.H.MMolecular dynamics simulation of shock-induced detonation in energetic solids@Landerville, A., Oleynik, I.I., Kozhushner, M.A. and White, C.T.[First-principles reactive molecular dynamics of chemistry in detonating energetic materials3Landwehr, A., B""ttner, M., Hahn, W. and Winter, R..The effect of high pressure on model membranesLane, J.M.D. and Marder, M.0Numerical method for shock front Hugoniot states,Lange, M.A., Ahrens, T.J. and Boslough, M.B.&Cratering and spall fracture in Gabbro Lanzerotti, M.Y.D. and Pinto, J.AChemical reaction of energetic materials during high acceleration909-916-Lanzerotti, M.Y.D., Pinto, J.J. and Wolfe, A.'Fracture surface topography of cast TNT8Lanzerotti, M.Y.D., Autera, J., Pinto, J. and Sharma, J.[Modeling of aluminum crystal fracture under high-rate strain based on atomistic simulations5Kumaran, S.U., Lim, C.T., Ong, K.C.G. and Tan, G.E.B.VEffects of different nose-shaped projectiles on the high speed perforation of concrete*Kunishige, H., Horie, Y. and Sawaoka, A.B.aNumerical and experimental studies of chemically reacting powder mixtures under shock compression
Kunz, A.B.Nakamura, A. and Mashimo, T.%Shock-induced phase transition of AlN,Nakamura, Y., Fujishiro, I. and Kawakami, H.dEstimation of refractive index and density of lubricants under high pressure by Brillouin scattering0Nakamura, K.G., Wakabayashi, K. and 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. and Kondo, K.vLiquid-solid phase transition of benzene under shock compression studied by time-resolved nonlinear Raman spectroscopy(Nakano, S., Fujioka, H. and Fukunaga, O..High pressure synthesis of cubic boron nitride!Namjoshi, S.A. and Thadhani, N.N.FReaction synthesis of shock densified titanium-silicon powder mixturesNamkung, J. and Coffey, C.S.APlastic deformation rate and initiation of crystalline explosives%Narayanan, V., Lu, X. and Hanagud, S.BShock-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. and Filinov, E.V.]Characterization of optically transparent window materials for isentropic compression studies3Negreskul, S.I., Psakhie, S.G. and Korostelev, S.Y.PThe simulation of explosive compact<  ion of powders by the element dynamics method4Nellis, W.J., Ross, M., van�  Thiel, M. and Brown, N.6The shock compression of liquid H2 to 10 GPa (100kbar)223-225Nellis, W.J.1Shocked fluids at high densities and temperatures31-40Nagayama, K.eUniversal description of solids at high pressures and temperatures based on the Gr"�neisen assumptioniStatistical 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 theoriesNagayama, K. and Mori, Y.:Anomaly in the temperature calculation of shocked polymers4Nagayama, K., Mori, Y., Shimada, K. and Nakahara, M.6Water shock Hugoniot measurement up to less than 1 GPa'Nagayama, K., Inou, K. and Nakahara, M.1Initiation of PETN powder by pulse laser ablation995-9988Nagayama, K., Ebisuzaki, H., Kubota, S. and Nakahara, M.&Pulse laser ignition of preheated PETN	1005-10083Nagayama, K., Mori, Y., Motegi, Y. and Nakahara, M.AShock Hugoniot compression data for several bio-related materials	1547-1550IGr"�neisen equation of state for condensed media and shock thermodynamics83-88�Nagler, B., Higginbotham, A., Kimminau, G., Murphy, W., Whitcher, T., Wark, J., Hawreliak, J., Kalantar, D., Lee, R., Lorenzana, H., Remington, B., Larsson, J., Park, N. and Sokolowski-Tinten, K.UProspects for using X-ray free-electron lasers to investigate shock-compressed matter#Nahme, H., Hohler, V. and Stilp, A.DElastic plastic behavior of shock-loaded Fe-SiO2 composite materialsPDetermination of the dynamic material properties of shock loaded silicon-nitride765-768#Nahme, H., Hiltl, M. and Arnold, W.hDynamic properties and microstructural response to shock loading of Armco iron at different temperatures$Nahme, H., Stilp, A.J. and Weber, K.GShock wave reflection behavior in double-layer meteoroid bumper systemsNahme, H. and Lach, E.nDetermination of the mechanical behavior of nitrogen alloyed steel (P900) at strain rates 10-3<de/dt<2*106 s-1	Nahme, H.IImproved EOS for describing high-temperature off-Hugoniot states in epoxyGMullin, S.A., Littlefield, D.L., Chhabildas, L.C. and Piekutowski, A.J.eComputational simulations of experimental impact data obtained at 7 to 11 km/s with aluminum and zinc	1817-18201Murata, K., Takahashi, K., Kato, Y. and Murai, K.SDevelopment of pressure gauge using PVDF copolymer for underwater shock measurementSMurphy, M.J., Simpson, R.L., Urtiew, P.A., Souers, P.C., Garcia, F. and Garza, R.G.XReactive flow model development for PBXW-126 using modern nonlinear optimization methods417-4207Murphy, W.J., Higginbotham, A., Wark, J.S. and Park, N.STemperature measurements of shocked crystals by use of nanosecond X-ray diffraction
Murr, L.E.uExamination of microstructural development by shock waves in condensed matter: Theoretical and practical consequences?Murr, L.E., Pradhan-Advani, M., Niou, C.S. and Schoenlein, L.H.zCorrelating critical process parameters and microstructures in explosively fabricated ceramic/metal matrix superconductors,Murray, N.H., Bourne, N.K. and Rosenberg, Z.#Precursor decay in several aluminas9Murray, N.H., Bourne, N.K., Field, J.E. and Rosenberg, Z.'Symmetrical Taylor impact of glass bars<Murray, N.H., Millett, J.C.F., Proud, W.G. and Rosenberg, Z.BIssues surrounding lateral stress measurements in alumina ceramics(Murri, W.J., Curran, D.R. and Seaman, L.)Fracture model for high energy propellant460-464Murri, W.J.@Shock wave facilities at Poulter Laboratory of SRI International652-6563Myers, S.A., Koch, C.C., Horie, Y. and Graham, R.A.5TEM of nickel aluminides produced by shock compaction755-759�Nagao, H., Nakamura, K.G., Kondo, K., Ozaki, N., Ono, T., Takamatsu, K., Tanaka, K.A., Nagai, K., Nakai, M., Wakabayashi, K., Okada, K. and Yoshida, M.@Equation of state of diamond under shock compression up to 2 TPa5Using the Hugoniot to approximate the release adiabat157-162BA method to estimate the yield of an underground nuclear explosion6Moss, W.C., Mitchell, A.C., Heinle, R. and Fritz, J.N.jParticle velocity measurements near underground nuclear explosions using axially symmetric magnetic gauges5Moss, W.C., Clarke, D.B., White, J.W. and Young, D.A.=Sonoluminescence, shock waves, and micro-thermonuclear fusion453-458Moulard, H. and Bauer, F.,Lagrangian analysis of the PVDF shock sensor)Mowrey, R.C., Elert, M.L. and White, C.T.:Quantum dynamics of energy transfer under shock conditions+Mukerji, R.J., Myers, S.A. and Whiteman, G.bA study of the effect of potting voids on the fragmentation of an explosively driven Nitinol shell3Mukundan, T., Constantinou, C.P. and Chaudhri, M.M.oMass spectrometric and spectroscopic investigations of the chemical sensitization of nitrocompounds by an amine.Mulder, A., Michels, J.P.J. and Schouten, J.A.IMonte Carlo calculations on the orientational behaviour of solid nitrogen*Mulford, R.N., Dick, J.J. and Pettit, D.R.JShock initiation of PETN crystals: Optical absorption and emission studies.Mulford, R.N., Sheffield, S.A. and Alcon, R.R.*Preshock desensitization of PBX explosives	1405-1408Mulford, R.N. and Alcon, R.R.5Shock initiation of PBX-9502 at elevated temperaturesMulford, R.N. and Romero, J.A.HSensitivity of the TATB-based explosive PBX-9502 after thermal expansionMulford, R.N. and Swift, D.C.>Reactive flow models for the desensitization of high explosive?Mesoscale modelling of shock initiation in HMX-based explosivesMulford, R. and Swift, D.OReactive flow in nitromethane using a quasiharmonic unreacted equation of state/Modelling temperatures of reacting nitromethane]Mulford, R.N., Swift, D.C., Lanier, N.E., Workman, J., Holmes, R.L., Graham, P. and Moore, A.GMonoclinic to tetragonal conversion of zirconia under shock compression-Morosin, B., Venturini, E.L. and Graham, R.A.;X-ray diffraction studies of shock-synthesised zinc ferrite797-801KMorosin, B., Graham, R.A., Venturini, E.L., Carr, M.J. and Williamson, D.L.3Shock-induced chemical synthesis of barium ferritesLMorosin, B., Graham, R.A., Venturini, E.L., Ginley, D.S. and Hammetter, W.F.`Shock-induced chemical synthesis of phases similar to the high temperature superconductor oxides+Morosin, B., Graham, R.A. and Pollack, S.S.:X-ray diffraction line broadening in shock modified PyriteWMorosin, B., Venturini, E.L., Holman, G.T., Newcomer, P.N., Dunn, R.G. and Graham, R.A.Shock-induced defects in HgO*Morris, C.E., Fritz, J.N. and Holian, B.L.7Quasi-elastic high-pressure waves in 2024 Al and copper382-386Morris, C.E.Shock Wave Physics Group (M-6)616-620+Morris, C.E., McQueen, R.G. and Marsh, S.P.3Mach disc formation in cylindrical recovery systems.Morris, C.E., Winkler, M.A. and Mitchell, A.C.@Ti-6%Al-4%V alloy wave profile measurements in the shadow regionMMorris, C.E., Loughran, E.D., Mortensen, G.F., Gray�  III, G.T. and Shaw, M.S.*Shock induced dissociation of polyethylene7Morris, J.P., Glenn, L.A., Antoun, T.H. and Lomov, I.N.uNumerical investigation into the performance of a rarefaction shock wave cutter for offshore oil-gas platform removal7Morris, J.P., Glenn, L.A., Heuze, F.E. and Bonner, M.P.dSimulations of underground structures subjected to dynamic loading using the distinct element method	1470-14730Moss, G.L., Netherwood�  Jr., P.H. and Seaman, L.QNucleation threshold s< tresses for the dynamic fracture of a low-alloy Ni-Cr steel446-450Moss, W.C. and Glenn, L.A.CA Bauschinger effect model suitable for use in large computer codes
Moss, W.C.5Morgado, J., Dur"�es, L., Campos, J. and Portugal, A.*Iron oxide/aluminum fast thermite reactionMori, Y. and Nagayama, K.�Sensitive detection of shock front and free surface velocity history for polymeric materials by new inclined-prism method in 1 GPa pressure regionXMeasurement of the slope of shock velocity-particle velocity Hugoniot curve for polymersNAnomalous 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 gaugekNonlinearity of polyethylene Hugoniot up to 1 GPa and its interpretation by Gr"�neisen parameter estimation1Mori, A., Tamaru, K., Hokamoto, K. and Fujita, M.AUnderwater explosive welding: Discussion based on weldable window	M"�ri, N.6Electrical and magnetic properties of Ce monopnictides	1477-1480Moriarty, J.A.THigh-pressure ion-thermal properties of metals from ab initio interatomic potentials101-106bFirst-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. and Yang, L.H.7Quantum-based atomistic simulation of transition metals403-4087Moritoh, T., Kawai, N., Nakamura, K.G. and Kondo, K.-I.NProjectile acceleration aiming at velocities above 9 km/s by a compact gas gun	1204-1207Morosin, B. and Graham, R.A.!Shock-induced inorganic chemistryqCrystallographic properties of lithium niobate shock-loaded from 3.7 to 20 GPa and preserved for post-shock study330-334HX-ray diffraction line broadening studies on shock-loaded TiO2 and Al2O3355-362+Morosin, B., Graham, R.A. and Hellman, J.R.nAnalysis of transitions between ferroelectric and antiferroelectric states under conditions of uniaxial strain179-1841Montgomery, S.T., Graham, R.A. and Anderson, M.U.UReturn to the shorted and shunted quartz gauge problem: Analysis with the SUBWAY codeLMontgomery, S.T., Brannon, R.M., Robbins, J., Setchell, R.E. and Zeuch, D.H.|Simulation of the effects of shock stress and electrical field strength on shock-induced depoling of normally poled PZT 95/5GMoore, D.S., Schmidt, S.C., Shaner, J.W., Shampine, D.L. and Holt, W.T.\Coherent anti-Stokes Raman scattering in benzene and nitromethane shock-compressed to 11 GPa207-211Moore, D.S. and Schmidt, S.C.AExperimental molecular spectroscopy in shock-compressed materials35-42Moore, L.M. and Graham, R.A.iResponse of standardized PVDF piezoelectric polymer gauges to direct shock pressures between 8 and 32 GPa8Moore, D.S., Schmidt, S.C., Shaw, M.S. and Johnson, J.D.6Vibrational 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. and Nicholson, J.W.VTime- 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. and Rabie, R.L.DSub-picosecond laser-driven shocks in metals and energetic materials	1333-1338)Moore, D.S., McGrane, S.D. and Funk, D.J.QUltrafast spectroscopic investigation of shock compressed energetic polymer films!Moran, B. and Goldwire�  Jr., H.C.VEffect of source modelling on the inferred yield from an underground nuclear explosion645-647	Moran, B.Verification test problems	1399-1402Morano, E.O. and Shepherd, J.E.=Effect of reaction rate periodicity on detonation propagation446-449lMitchell, A.C., Nellis, W.J., Holmes, N.C., Erskine, D.J., McCandless, P.C., Ravizza, D.L. and Cassidy, L.D.JEquation of state data of shock compressed liquid CO2 and synthetic UranusEMochalov, M.A., Glukhodedov, V.D., Kirshanov, S.I. and Lebedeva, T.S.iElectric conductivity of liquid argon, krypton and xenon under shock compression up to pressure of 90 GPa*Mock�  Jr., W., Holt, W.H. and Kerley, G.I.!Shock and recovery of PTFE powderMock�  Jr., W. and Holt, W.H.>Impact initiation of rods of pressed PTFE and aluminum powdersMock�  Jr., W. and Drotar, J.T.[Effect of aluminum particle size on the impact initiation of pressed PTFE/Al composite rods6Molinar, G.F., Ehrlich, C., Houck, J. and Cresto, P.C.EElastic distortions of a multi-mode piston-cylinder unit up to 28 MPa	1589-1592+Molinari, V.G., Mostacci, D. and Sumini, M.\Particle density and temperature distribution in the early stage of laser-plasma interactionMolinari, V.G. and Teodori, F.=Energy propagation from a spherically symmetric particle flowMolinari, V. and Teodori, F.pAnalysis of the slowing of a high energy proton shot through a target in the frame of the Fokker-Planck equation*Molinari, V., Mostacci, D. and Teodori, F.�Analysis of the slowing down of high energy proton shots through matter via a Monte Carlo simulation of the Fokker Planck equation	1466-14690Molodets, A.M., Molodets, M.A. and Nabatov, S.S.,Free energy and shock compression of diamond.Monat, J.E., Carney, J.R. and Pangilinan, G.I.ANovel optical fiber-based gauge for measuring transient pressures=Monat, J.E., Carney, J.R., Whitley, V.H. and Pangilinan, G.I.gTemporal profiles of explosively-generated pressures in solids measured by an optical fiber-based gauge	1199-1202:Monat, J.E., Tersine, E.G., Morgan, B.A. and Ostrowski, P.!Ignition of TNT using a CO2 laserMontgomery, S.T.bMing, L.C., Manghnani, M.H., Balogh, J., Qadri, S.B., Skelton, E.F., Webb, A.W. and Jamieson, J.C.AStatic P-T-V measurements on MgO: Comparison with shock wave dataMinich, R.W.>Optimal velocity amplification in a system of colliding plates5Minich, R.W., Kumar, M., Schwarz, A. and Cazamias, J.,Scaling, microstructure and dynamic fractureMinnaar, K. and Zhou, M.1Characterization of impact in composite laminates	1208-1211Minomura, S.WHigh pressure studies of lattice and electronic structures of Si/Si1-xGex superlattices>Mintmire, J.W., Robertson, D.H., Brenner, D.W. and White, C.T.dMolecular dynamics simulations of pressure wave effects at voids in a model condensed-phase materialKMintmire, J.W., Robertson, D.H., Elert, M.L., Brenner, D.W. and White, C.T.?Molecular dynamics of void collapse mechanisms in shocked media969-972aMintsev, V.B., Ternovoi, V.Y., Gryaznov, V.K., Pyalling, A.A., Fortov, V.E. and Iosilevskii, I.L.1Electrical conductivity of shock compressed xenonMishin, G. and Yushchenkova, N.+Nonlinear processes in shock waves in gases741-743QMishra, A., Martin, M., Gregori, F., Asaro, R.J., Meyers, M.A. and Thadhani, N.N.0Reverse Taylor tests on ultrafine grained copperMissionnier, M. and Heuz"�, O.NModeling of shock waves with multiple phase transitions in condensed materials262-265,Mitchell, A.C., Nellis, W.J. and Monahan, B.2Enhanced performance of a two-stage, light gas-gun184-187.Mitchell, A.C., Nellis, W.J. and Trainor, R.J.BThe Lawrence Livermore National Laboratory two-stage light gas-gun613-615�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. and Olness, R.J.`Shock impedance match experiments in aluminum and molybdenum between 0.1  �� 2.5 TPa (1-2< 5 Mbar)<Measurements of strain in a shock loaded, high-density glass<Millett, J.C.F., Tsembelis, K., Bourne, N.K. and Field, J.E.'The shock Hugoniot of two igneous rocks=Millett, J.C.F., Bourne, N.K., Gray�  III, G.T. and Cooper, G.(On the shock response of polychloroprene Millett, J.C.F. and 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. and Stevens, G.S.5On the shock response of the shape memory alloy, NiTi>Millett, J.C.F., Jones, i.P., Bourne, N.K. and Gray�  III, G.T.LThe effect of microstructure on the shock behaviour of g-titanium aluminides1Millett, J.C.F., Gray�  III, G.T. and Bourne, N.K.ALongitudinal and lateral stress measurements in shock loaded PEEKALateral stress measurements in pure tungsten during shock loading>Millett, J.C.F., Bourne, N.K., Brown, E.N. and Gray�  III, G.T.TShear strength and its variation according to structure in shock loaded polyethyleneKMilman, V.Y., Nemoshkalenko, V.V., Zhalko-Titarenko, A.V. and Antonov, V.N.6Equation of state of transition fcc metals up to 1 TPaLMilman, Y.V., Gooch, W., Timofeeva, I.I., Chugunova, S.I. and Gridneva, I.V.IPressure induced phase transition in ceramic materials during indentationMilne, A.M. and Bourne, N.K.CExperimental and numerical study of temperatures in cavity collapse914-917-Milne, A.M., Bourne, N.K. and Millett, J.C.F.=On the unreacted Hugoniots of three plastic bonded explosivesZMilyavskiy, V.V., Utkin, A.V., Zaretsky, E.B., Zhuk, A.Z., Yakushev, V.V. and Fortov, V.E.Hugoniot of C60 fulleritetMilyavskiy, V.V., Khishchenko, K.V., Utkin, A.V., Valiano, G.E., Yakushev, V.V., Zhernokletov, M.V. and Fortov, V.E.8Shock compression and equation of state of C60 fulleriteMikkola, D.E. and Wright, R.N.&Metallurgical effects of shock loading98-117^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 state642-645Militzer, B. and Hubbard, W.B.aImplications of shock wave experiments with precompressed materials for giant planetary interiors	1395-1398YMiljkovic, K., Taylor, E.A., Tsembelis, K., Proud, W.G., Cockell, C.S. and Zarnecki, J.C.\Impact pressures generated by spherical particle hypervelocity impact on Yorkshire sandstoneMiller, M.D.GWave propagation and long-time behavior on the driven Sine-Gordon chain281-286Miller, S.A.IPiezoresistant response of rolled ytterbium foils to double-shock loadingMiller, A.R.1Explosive synthesis of a Y-Ba-Cu-O superconductorMiller, P.J. and Guirguis, R.H.]Effects of late chemical reactions on the energy partition in non-ideal underwater explosions!Miller, P.J. and Sutherland, G.T."Reaction rate modeling of PBXN-110Miller, P.J. and Lindfors, A.J.VShock loading and reactive flow modeling studies of void induced AP/Al/HTPB propellant!Miller, J.S. and Pangilinan, G.I.=Measurements of aluminum combustion in energetic formulations=Miller, J.E., Boehly, T.R., Meyerhofer, D.D. and Eggert, J.H./Equation-of-state measurements in Ta2O5 aerogel/Millett, J.C.F., Bourne, N.K. and Rosenberg, Z.WShear stress measurements in copper, iron and mild steel under shock loading conditionsKAn investigation of the a-e phase transition in shock loaded EN3 mild steel@Millett, J.C.F., Galbraith, S.D., Rosenberg, Z. and Bourne, N.K.bDirect measurements of strain in the B1/B2 phase transformation in shock loaded potassium chlorideMeuken, D. and Carton, E.P.Explosive welding and cladding	1110-1113zMeyer�  Jr., H.W., Abeln, T., Bingert, S., Bruchey, W.J., Brannon, R.M., Chhabildas, L.C., Dienes, J.K. and Middleditch, J.0Crack behavior of ballistically impacted ceramic%Meyer�  Jr., H.W. and Schoenfeld, S.E.6Effects of damage criteria on the onset of penetration	1343-1346<Meyers, M.A., Thadhani, N.H., Erlich, D.C. and DeCarli, P.S.:Martensitic transformation induced by tensile stress waves(Meyers, M.A., Wang, S.L. and Gupta, B.B.?Mechanical and thermal response of sohck-consolidated Mar-M 200Meyers, M.A. and Kuriyama, S.2Modeling of instability at the tip of a shear band321-328)Meyers, M.A., Yu, L.-H. and Vecchio, K.S.Shock synthesis of silicides*Meyers, M.A., Benson, D.J. and Shang, S.S.9Energy expenditure and limitations in shock consolidation*Meyers, M.A., Xue, Q. and Nesterenko, V.F.4Evolution in the patterning of adiabatic shear bandsCMeyers, M.A., Perez-Prado, M.T., Xue, Q., Xu, Y. and McNelley, T.R.LMicrostructural 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. and Ravichandran, G.PPlastic deformation in laser-induced shock compression of monocrystalline copperIMeziere, Y., Akhavan, J., Stevens, G.S., Millett, J.C.F. and Bourne, N.K.6The shock Hugoniot of hydroxy-terminated polybutadiene;Ribeiro, J.B., Mendes, R.L., Plaksin, L.Y. and Campos, J.A.NFeatures of the shock and detonation waves in cylindrical explosive compactionRice, B.M. and Trevino, S.F.@Monte Carlo calculations of the properties of solid nitromethaneRichmond, C.T.?Gap test modeling to predict wedge tests initiation of PBXN-1036Modeling the asymmetric burning of ultrafine particles8Modeling the asymmetric burning of agglomerate particles(Dynamic properties of tributyl phosphate@Reinhart, W.D., Chhabildas, L.C., Trott, W.M. and Dandekar, D.P.BInvestigating multi-dimensional effects in single-crystal sapphire#Reinhart, W.D. and Chhabildas, L.C.7Dynamic strength of AD995 alumina at Mbar stress levels759-764<Response to unloading and reloading of shock compressed PMMA1Reinhart, W.D., Vogler, T.J. and Chhabildas, L.C.LStrength measurements on dry Indiana limestone using ramp loading techniques	1409-1412!Reinovsky, R.E. and Trainor, R.J.NHydrodynamic and material properties experiments using pulsed power techniques{Reinovsky, R.E., Anderson, W.E., Atchison, W.L., Faehl, R.J., Keinigs, R.K., Lindemuth, I.R., Thompson, M.C. and Taylor, A.]Shock-wave and material properties experiments using the Los Alamos Atlas pulsed power systemyReisman, D.B., Forbes, J.W., Tarver, C.M., Garcia, F., Cauble, R.C., Hall, C.A., Asay, J.R., Struve, K. and Furnish, M.D.4Isentropic compression of LX-04 on the Z acceleratoryRemington, B.A., Hawreliak, J., Lorenz, K.T., Lorenzana, H.E., McNaney, J.M., Pollaine, S.M., Swift, D.C. and Yaakobi, B.+Materials response under extreme conditions765-770%Remiot, C., Chapron, P. and Demay, B.WA flash X-ray radiography diagnostic for studying surface phenomena under shock loading	1763-1766(Remiot, C., Mexmain, J.M. and Bonnet, L.HPrecise method to determine points on isentropic release curve on copperRemo, J.L. and Furnish, M.D.2High intensity X-ray coupling to meteorite targets	1410-1413Renero, C. and Prieto, F.E.;Reduced variables and universality in high pressure physics#Shock Hugoniot for porous materials.Renlund, A.M., Sheffield, S.A. and Trott, W.M.UTime-resolved infrared spectral photography studies of shock-induced chemistry in CS2237-242Renlund, A.M. and Trott, W.M.HModeling high pressure and high temperature phase changes in bulk carbonNReed, R.P., Graham, R.A., Moore, L.M., Lee, L.M., Fogelson, D.J. and Bauer, F.*The Sandia standard for PVDF shock sensorsReed, R.P. and Greenwoll, J.I.UCharacteristics and pulsed radiation response of non-ideal quartz shock stress gauges<  	1711-1714QReed, R.P., Greenwoll, J.I., Bauer, F., Lee, L.M., Davies, F.W. and Johnson, D.J.>Pulsed radiation response of stressed PVDF shock stress gauges	1743-1746.Reed, E.J., Joannopoulos, J.D. and Fried, L.E.iHugoniot constraint molecular dynamics study of a transformation to a metastable phase in shocked silicon;Reed, E.J., Manaa, M.R., Joannopoulos, J.D. and Fried, L.E.RElectronic excitations, vibrational spectra, and chemistry in nitromethane and HMX385-390;Reed, E.J., Fried, L.E., Manaa, M.R. and Joannopoulos, J.D.OA method for tractable dynamical studies of single and double shock compression/Reed, E.J., Soljacic, M. and Joannopoulos, J.D.-The color of shock waves in photonic crystals	1307-13128Reed, E.J., Soljacic, M., Gee, R. and Joannopoulos, J.D.QPrediction of coherent optical radiation from shock waves in polarizable crystals	1345-1348KReed, E.J., Manaa, M.R., Fried, L.E., Glaesemann, K. and Joannopoulos, J.D.:A transient semi-metallic layer in detonating nitromethane9Reed, E.J., Armstrong, M.R., Kim, K.-Y. and Glownia, J.H.bCoherent THz frequency radiation from shock waves: A new ultrafast strain wave detection mechanismAReho, J.H., Moore, D.S., Funk, D.J., Fisher, G.L. and Rabie, R.L.iUltrafast spectroscopic investigation of shock compressed glycidyl azide polymer and nitrocellulose films	1219-12221Reinhart, W.D., Chhabildas, L.C. and Wilson, L.T.MDynamic yield strength and spall strength determination for AerMet 100 steels?Reinhart, W.D., Chhabildas, L.C., Winfree, N.A. and Grady, D.E.�Hugoniot elastic limit and spall strength of aluminum and copper single crystals over a wide range of strain rates and temperatures=Razorenov, S.V., Savinykh, A.S., Kanel, G.I. and Shakun, S.N.YSub-microsecond yield and tensile strengths of metals and alloys at elevated temperatures=Razorenov, S.V., Kanel, G.I., Savinykh, A.S. and Fortov, V.E.	1769-1772YMcDonald, S.A., Bourne, N.K., Withers, P.J., Millett, J.C.F., Bennett, K. and Milne, A.M.UThe shock response, simulation and microstructural determination of an inert simulant_McDonald, S.A., Bourne, N.K., Gray�  III, G.T., Cerretta, E.K., Millett, J.C.F. and Whiteman, G.*Shock loading and Taylor impact of Ti6Al4V/McGlaun, J.M., Zeigler, F.J. and Thompson, S.L.PCTH: A three-dimensional, large deformation deformation, shock wave physics code)McGrane, S.D., Moore, D.S. and Funk, D.J.`Measurement of shocked thin polymer film Hugoniot properties with ultrafast dynamic ellipsometry	1181-1186#McGregor, N.M. and Sutherland, G.T.<Plate impact experiments on a porous Teflon-aluminum mixture!McGregor, N.M. and Lindfors, A.J.gShock reactivity study on standard and reduced sensitivity RDX of different particle size distributionsGMcLaughlin, K., Oleynik, I.I., Zybin, S.V., Elert, M.L. and White, C.T.WMolecular dynamics simulations of an anomalous response of diamond to shock compression
McMahan, A.K.1The a-b transition on T=0 high pressure beryllium340-344McMahan, A.K. and Skriver, H.L.BPositron annihilation and pressure-induced electron s-d transition107-1129McMahon, M.I., Nelmes, R.J., Wright, N.G. and Allan, D.R.�Crystal-structure studies of III-V and group IV semiconductors using angle-dispersive diffraction techniques with an image-plate detector@Molecular dynamics study of iron at Earth's inner core conditionMattsson, A.E.*Equation of state for a high-density glass,Maw, J.R., Whitworth, N.J. and Holland, R.B.>Multiple shock compression of polyurethane and syntactic foamsMaw, J.R. and Giles, A.R.:Numerical modelling of spallation in 2D hydrodynamic codes295-298Maw, J.R. and Whitworth, N.J.RShock compression and the equation of state of fully dense and porous polyurethane	Maw, J.R.2Lagrangian analysis of EDC37 shock initiation data	1027-1030IA characteristics code for analysis of isentropic compression experiments3Analytical equations of state for use in hydrocodesOMayer, F.J., Maynard, R.L., Musinski, D.L., Schmerberg, N.W. and Benjamin, R.J.XRecent developments in microshell-tipped optical fibers as high pressure shock detectors547-551(Mayseless, M., Harvey, W.B. and Hetz, A.PA computational study of non-porous and porous liners in explosively-formed jets-Mayseless, M., Luttwak, G. and Birnbaum, N.K..Numerical simulations of rod-plate interaction	1133-1136SMazavet, S., Kress, J.D., Collins, L.A., Wood, W.W., Johnson, J.D. and Blottiau, P.IDensity functional calculation of the Hugoniot of shocked liquid nitrogenDMazevet, S., Kress, J.D., Magee, N.H., Keady, J.J. and Collins, L.A.CQuantum molecular dynamics calculations of Rosseland mean opacities293-297#Mazor, A., Partom, Y. and Barak, G.DEquation of state of gold in the high-temperature low-density regimeMcCammon, C.VHigh pressure in situ investigation of cubanite (CuFe2S3): Structural phase transition=McClellan, K.J., Swift, D.C., Paisley, D.L. and Koskelo, A.C.+Dynamic properties of nickel-aluminum alloyuMcCluskey, C.W., Wilke, M.D., Anderson, W.W., Byers, M.E., Holtkamp, D.B., Rigg, P.A., Furnish, M.D. and Romero, V.T..Shock yielding properties of brittle materials>Mashimo, T., Kodama, M., Kusaba, K., Fukuoka, K. and Syono, Y.WHugoniot measurement study of the partially stabilised and stabilised zirconia ceramics9Shock compression of ceramic materials: Yielding propertyMashimo, T. and Uchino, M.+Shock compression behavior of boron carbide531-533(Mashimo, T., Nakamura, M. and Uchino, M.FMeasurement of shock-wave structure of LiF single crystal by the VISAR@Mashimo, T., Tsumoto, K., Noguchi, Y., Fukuoka, K. and Syono, Y.WHugoniot measurement of alumina single crystal in the pressure range up to over 100 GPa101-103.Shock compression properties of hard materials175-180*Mason, T.A., Henrie, B.L. and Thomas, K.A.5Damage progression in explosively loaded polycrystals/Matheson, E.R., Drumheller, D.S. and Baer, M.R.`A coupled damage and reaction model for simulating energetic material response to impact hazardsJAn internal damage model for viscoelastic-viscoplastic energetic materials"Matheson, E.R. and Rosenberg, J.T.SA mechanistic study of delayed detonation in impact damaged solid rocket propellant464-467Matheson, E.R. and Nguyen, D.Q.UA rate-dependent viscoelastic damage model for simulation of solid propellant impactsHA viscoelastic fracture model for simulation of solid propellant impacts644-647ERagan, C.E., Diven, B.C., Rich, M., Teasdale, W.A. and Robinson, E.E.&Precise ultrahigh-pressure experiments:Raghupathy, R., Gazonas, G.A., Molinari, J.F. and Zhou, F.[Numerical convergence of the cohesive element approach in dynamic fragmentation simulations654-657Raiser, G. and Clifton, R.J.AFailure waves in uniaxial compression of an aluminosilicate glassRajendran, A.M. and Bless, S.J.VUse of the Bodner-Partom model viscoplastic constitutive model to describe HY100 steel383-388,Rajendran, A.M., Grove, D.J. and Bless, S.J.0A new yield function based dynamic failure model3Rajendran, A.M., Dietenberger, M.A. and Grove, D.J.9Results from the recently developed dynamic failure model+Rajendran, A.M., Brar, N.S. and Khobaib, M.CEffects of dynamic pre-strain on the subsequent tensile flow stress+Rajendran, A.M., Grove, D.J. and Bar-On, E.?Transformation of CS2 to a polymer at 10 GPa: An infrared study2Psakhie, S.G., Korostelev, S.Y. and Vorobyov, V.I.\Formation of nanocrystalline structure by shock wave propagation through amorphous materials157-1592Pyalling, A.A., Ternovoi, V.Y. and Filimonov, A.S.uTemperature measurements of single and double shock compressed liquid nitrogen in overtaking shock wave configuration3Qadri, S.B., Skelton, E.F., Webb, A.W. and Hu, J.Z.%Pressure induced polymorphism of ZnTeBQadri, S.B., Skelton, E.F., Webb, A.W., Hu, J.Z. and Furdyna, J.K./Pressure induced phase transition of Zn1-xCoxSeQi, M., He, H. and Yan, S.XA study of the critical fracture behavior of high < purity aluminum in the dynamic loading>Quenneville, J., Germann, T.C., Thompson, A.P. and Kober, E.M.?Molecular dynamics studies of thermal induced chemistry in TATB&Quidot, M., Racimor, P. and Chabin, P./Constitutive models for PBX at high strain rate,Rabie, R.L., Vorthman, J.E. and Dienes, J.K.BThree-dimensional computer modeling of a shock recovery experimentRabie, R. and Dick, J.J.FEquation of state and crushing dynamics of low-density silica aerogels4Radchenko, A.V., Kobenko, S.V. and Krivosheina, M.N.gEffect of oriented elastic and strength characteristics on the impact fracture of anisotropic materials*Radford, D.D., Proud, W.G. and Field, J.E.MThe deviatoric response of three dense glasses under shock loading conditions-Radford, D.D., Willmott, G.R. and Field, J.E.AThe effect of structure on failure front velocities in glass rods,Radford, D.D., Tsembelis, K. and Proud, W.G.&The dynamic behavior of a filled glass884-8879Radousky, H.B., Mitchell, A.C., Nellis, W.J. and Ross, M.)Shock temperature measurements in ammonia467-472Radousky, H.B.%Shock-induced cooling in dense fluids7Rae, P.J., Goldrein, H.T., Palmer, S.J.P. and Proud, W.Prentice, H.J. and Proud, W.G.mThree-dimensional dynamic deformation measurements using stereoscopic imaging and digital speckle photography,Preston, D.L., Tonks, D.L. and Wallace, D.C.CThe rate dependence of the saturation flow stress of Cu and 1100 AlfPrice, R.H., Rosen, M.D., Banner, D.L., Holmes, N.C., Kobierecki, M., Zickuhr, J.R. and Ahlstrom, H.G.LTime and space resolved measurements of the dynamics of laser fusion targets155-163*Prieto, F.E., Loske, A.M. and Yarger, F.L.QStudy of pressure transducers and electrodes for underwater shock wave generators	1723-1726Pritchard, D.S.PFurther investigation of stresses and strains in targets impacted by penetrators&Shock waves in condensed matter - 1983GFuzzy logic applied to shaped charge jet penetration of glass composite)Proud, W.G., Bourne, N.K. and Field, J.E.4Shock-induced luminescence in polymethylmethacrylateProud, W.G. and Field, J.E.+Shock-induced reaction in hydrogen peroxideProud, W.G.;The measurement of hot-spots in granulated ammonium nitrate(Proud, W.G., Kirby, I.J. and Field, J.E.AThe nature, number and evolution of hot-spots in ammonium nitrate	1017-1020'Proud, W.G., Wang, J. and Cross, D.L.A.DThe effect of sample roughness and planarity on gauge response times	1203-1206�Proud, W.G., Chapman, D.J., Williamson, D.M., Tsembelis, K., Addiss, J., Bragov, A., Lomunov, A., Cullis, I.G., Church, P.D., Gould, P., Porter, D., Cogar, J.R. and Borg, J.;The dynamic compaction of sand and related porous materials	1403-1408Pr"�mmer, R.4Explosive welding of tin, uranium and thorium copper467-469'Pruzan, P., Chervin, J.C. and Canny, B.jDetermination of the ice VII-VIII transition line at high pressure and low temperature by Raman scattering8Pruzan, P., Chervin, J.C., Canny, B. and Kuyumchev, A.A.SPorowski, S., Jun, J., Krukowski, S., Bockowski, M., Tedenac, J.C. and Record, M.C.MHigh pressure differential thermal analysis (DTA) and crystal growth of a-HgSPPorowski, S., Lojkowski, W., Molodov, D.A., Shvindlerman, L.S. and Gottstein, G.KEffect 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. and Yakushev, V.V.UThe opportunity of the use of sapphire at multiple shock-wave compression of hydrogen?Postnov, V.I., Fortov, V.E., Yakushev, V.V. and Yakusheva, T.I.jElectrical conductivity investigation of graphite-diamond transition under multiple shock-wave compressionDPovarnitsyn, M.E., Itina, T.E., Khishchenko, K.V. and Levashov, P.R.MPhase transitions and metastable states in ultrashort laser-metal interactionPrakash, A.\Time evolution of pressure fields generated in impact of cylindrical projectiles with plates	1805-18080Prakash, A., McCormick, A.V. and Zachariah, M.R.0Thermo-kinetic study of sore-shell nanothermites	1006-1009PPravica, M., Quine, Z., Romano, E., Bajar, S., Yulga, B., Yang, W. and Hooks, D.0Anisotropic decomposition of energetic materials	1117-11208Predebon, W.W., O'Donoghue, P.E. and Anderson�  Jr., C.E.KGap closure and opening between preformed fragments during explosive launch4Predebon, W.W., Anderson�  Jr., C.E. and Walker, J.D.<Inclusion of equivalent plastic strain in Eulerian wavecodesPrentice, J.K.KMethodology and applications of the HULL hydrocode Eulerian/Lagrangian linkPrentice, J.K. and Kipp, M.E.DModeling of rate dependent brittle fracture in an Eulerian hydrocode+Prentice, J.K., Fikani, M.K. and Fuka, M.Z.2TOLTEC: A multidimensional solid dynamics wavecode;Prentice, H.J., Grantham, S.G., Proud, W.G. and Field, J.E.LThree-dimensional penetration measurements using digital speckle photography3Detonation meso-scale tests for energetic materials922-925fPlaksin, I., Campos, J., Direito, J., Mendes, R., Sim"�es, P., Portugal, A., Ribeiro, J. and G"e"is, J.PCoarse explosive particles of PBX as a dominant factor of detonation instabilityYPlaksin, I., Campos, J., Mendes, R., Ribeiro, J., Direito, J., Braga, D. and Coffey, C.S.1Effect of shear stress in shock initiation of PBX[Plaksin, I., Direito, J., Coffey, C.S., Campos, J., Ribeiro, J., Mendes, R. and Kennedy, J.VMesoscale probing of CRZ structure in PBX: DW oscillations from ignition up to failure	1002-1005KPlaksin, I., Coffey, C.S., Campos, J., Mendes, R., Ribeiro, J. and Gois, J.jShear induced reaction localization and mechanisms of energy dissipation in PBXs subjected to strong shock	1427-1432.Plohr, J.N., Clements, B.E. and Addessio, F.L.GDynamically driven phase transformations in damaged composite materials266-269Plohr, B.J. and Plohr, J.Y.N.DSimplified shock conditions for large-strain thermo-visco-plasticityPodlesak, M.TInvestigation of electrical shock conductivity in a polymer shock compression switch0Podurets, A.M., Barenboim, A.I. and Trunin, R.F.QX-ray flash diffraction study of shock phase transitions in zirconium and bismuth231-233"Poirier, J.-P. and Shankland, T.J.1Dislocation theory of melting for iron, revisited!Polishchuk, A.Y. and Fortov, V.E.sNew theoretical approach in calculation of laser beam and particle beam ranges in shock-compressed condensed matter781-783Polishchuk, A.Y.NKinetic and optical properties of condensed matter in ultra strong laser field	1895-1987Pollock, R.VComments on 'Thermodynamic properties of nonideal strongly degenerate hydrogen plasma'123-1244Poole, C.P., Farach, H.A., Owens, F.J. and Pinto, J.5Compression induced aligned radicals in nitroanilines647-649IPhillips, D.S., Schwarz, R.B., Skidmore, C.B., Hiskey, M.A. and Son, S.F.*Some observations on the structure of TATBPickup, I.M. and Barker, A.K."Damage kinetics in silicon carbide7Deviatoric strength of silicon carbide subject to shockPickup, I.M. and Bourne, N.K.,The failure of aluminium nitride under shock.Pickup, I.M., Millett, J.C.F. and Bourne, N.K.LThe shock behaviour of a SiO2-Li2O transparent glass-ceramic armour materialPiekutowski, A.J.%Distribution of mass in debris clouds953-9562Pinheiro, L.M.V., Calado, A.R.T. and Viana, C.A.N.GPressure effects on Menschutkin reactions in butan-1-ol and pentan-1-olPistinner, S.L.bHigh pressure electronic conductions from a phenomenological equation of state: Application to tin9Pistinner, S.L., Pecker, S., Werdiger, M. and Eliezer, S.aOn the maximal deviation from the mirror image approximation due to solid liquid phase transitionoPiza"�a, C., Murr, L.E., Anchondo, I.A., Pi"�a, C.Y., Baquera, M.T., Tamoria, T.L., Chen, H.C. and Cytron, S.J.< �DRX-induced solid-state flow and projectile-target mixing during [001] single-crystal tungsten rod penetration into steel targetspPlaksin, I.Y., Shutov, V.I., Gerasimov, V.M., Gerasimenko, V.F., Morozov, V.G., Karpenko, I.I. and 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. and Gois, J.C.2Interaction of double corner turning effect in PBX=Plaksin, I., Campos, J., Mendes, R., Ribeiro, J. and Gois, J.EMechanism of detonation wave propagation in PBX with energetic binder3Plaksin, I., Campos, J., Ribeiro, J. and Mendes, R.(Detonation phenomena of PBX microsamples918-921fPlaksin, I., Campos, J., Ribeiro, J., Mendes, R., G"e"is, J., Portugal, A., Sim"�es, P. and Pedroso, L._High-speed photography of detonation propagation in dynamically precompressed liquid explosivesJPeterson, P.D., Mang, J.T., Fletcher, M.A., Olinger, B.W. and Roemer, E.L.BInfluence of pressing parameters on the microstructure of PBX 9501796-799>Peterson, P.D., Avilucea, G.R., Bishop, R.L. and Sanchez, J.A.ZIndividual contributions of friction and impact on non-shock initiation of high explosivesIPeterson, P.D., Lee, K.-Y., Moore, D.S., Scharff, R.J. and Avilucea, G.R.bThe evolution of sensitivity in HMX-based explosives during the reversion from delta to beta phasePetit, J. and Hereil, P.L.0Characterization of recovered shocked Armco iron0Petit, J., Kazeev, M., Levit, P. and Tolstov, Y.SElectromagnetic cylindrical compression test under large strain at high strain rate,Petrovic, J.J., Olinger, B.W. and Roof, R.B.=Behavior of Si3N4 powder subjected to explosive shock loading Petrovsky, V.P. and Ostrik, A.V.hExperimental methods of investigating composite structures strength against unstationary loading effects5Petrovtsev, A.V., Bychenkov, V.A. and Kovalenko, G.V.sNumerical simulation of elastic-viscous-plastic properties: Polymorphous transformations and spall fracture in iron591-5942Petrovtsev, A.V., Zhugin, Y.N. and Kovalenko, G.V.FModeling polymorphic transformations of quartzite in dynamic processes^Petrovtsev, A.V., Dremov, V.V., Vildanov, V.G., Gorshkov, M.M., Zahikin, V.T. and Zhugin, Y.N.-Equation of state and phase diagram of quartz2Peyronneau, J., Poirier, J.-P. and Shankland, T.J.`Electrical conductivity of perovskite-magnesiow"�stite as a function of pressure and temperature	1465-1468Phillips, L. and Oran, E.S.FMolecular dynamics simulations of shocks in imperfect crystal latticesPhillips, L.@Shock compression of a 2D model of DT embedded in a plastic foam+A theoretical equation of state for uraniumBPeralta, P., Swift, D., Loomis, E., Lim, C.-H. and McClellan, K.J.ICharacterization of laser-driven shocked NiAl monocrystals and bicrystals601-604 Pereira, C.M. and Chaudhri, M.M.NOptical and Raman studies of explosives under varying pressure and temperature5Perevalova, V.P., Kaminskii, P.P. and Kuznetsov, V.M.GEquation of state (EOS) and bulk modulus under pressure of noble metalsPerez, M. and Costeraste, J.@Infrared method for postshock temperature measurements of solids	Perez, M.TThe 'MIVAR': A ramp-wave generator material fabricated by the plasma spray techniqueYResidual temperature measurements of shocked copper and iron plates by infrared pyrometry1Perger, W.F., Zhao, J., Blanco, M. and Pandey, R.`First-principles intermolecular binding energies in molecular crystals with optimized basis sets3Perger, W.F., Zhao, J., Winey, J.M. and Gupta, Y.M.xFirst-principles studies of PETN single crystal unit cell volumes and vibrational frequencies under hydrostatic pressurePerry, F.C.EInvestigations of hydrodynamic stability using electron and ion beams639-643EDynamic heterogeneous response of aluminum and copper to stress wavesPerry, F.C. and Noack, D.D.EHeterogeneous response of aluminum and lithium niobate to shock waves655-660*Persson, P.A., Ward, R. and Thadhani, N.N.FShock induced reaction synthesis (SRS) assisted compaction of ceramicsFPetel, O.E., Tanguay, V., Higgins, A.J., Yoshinaka, A.C. and Zhang, F.<Detonation propagation in shock-compressed liquid explosivesPetel, O.E. and Higgins, A.J.EComparison of failure thickness and critical diameter of nitromethane994-9979Petel, O.E., Higgins, A.J., Yoshinaka, A.C. and Zhang, F.LEffect of shock precompression on the critical diameter of liquid explosives998-1001Partouche-Sebban, D.RHigh-speed multi-wavelength pyrometry and emissivity measurement of shocked metals	1293-1298
Passman, S.L.%Models for penetration of thin platesEPasternak, M.P., Hearne, G., Sterer, E., Taylor, R.D. and Jeanloz, R._High pressure metallization of Mott insulators: Magnetic, structural, and electronic properties
Pastine, D.J.+Radio emissions from unequilibrated sources861-864KPatel, D., Temkin, H., Menoni, C.S., Logan, R.A., Coblentz, D. and Tome, C.dEnhanced characteristics of InGaAsP buried quaternary lasers with pressure in the diamond anvil cellPatel, M.V. and Streitz, F.H.ESimulations of rapid pressure-induced solidification in molten metals298-301*Patterson, J., Lagutchev, A. and Dlott, D.;Shock compression of molecules with 1.5 Angstrom resolution-Patterson, J.E., Dreger, Z.A. and Gupta, Y.M.GRaman spectroscopy of RDX crystals shocked along different orientations(Paul, W., Burnett, J.H. and Cheong, H.M.0Role of high pressures in semiconductor researchGPauler, D.K., Kress, J.D., Lightfoot, J.M., Woods, L. and Russell, B.G.FDecomposition of nitroplasticizer in plastic bonded explosive PBX 9501SPavlovskii, A.I., Tatsenko, O.M., Platonov, V.V., Volkov, A.A. and Markevtsev, I.M.HInvestigation of ruby luminescence R-line by isentropic megabar pressure0Peiris, S.M., Pangilinan, G.I. and Russell, T.P.?The laser-induced decomposition of TATB at static high pressureEStructural changes in ammonium perchlorate under compression to 5 GPa?Peiris, S.M., Pangilinan, G.I., Zerilli, F.J. and Russell, T.P.\Structural studies and EOS of diaminodinitroethylene (DADNE, FOX-7) under static compression.Pelak, R.A., Rightley, P. and Hammerberg, J.E.)Friction in high-speed impact experiments2Erratum: Friction in high-speed impact experiments
P"�nicaud, M./Parker, L.J., Ladouceur, H.D. and Russell, T.P.PTeflon and Teflon/Al (nanocrystalline) decomposition chemistry at high pressuresIParker, G.R., Asay, B.W., Dickson, P.M., Henson, B.F. and Smilowitz, L.B.8Effect of thermal damage on the permeability of PBX 9501VParker, G.R., Dickson, P.M., Asay, B.W., Smilowitz, L.B., Henson, B.F. and Perry, W.L.TUnderstanding the mechanisms leading to gas permeation in thermally damaged PBX 9501?Parker, G.R., Asay, B.W., Dickson, P.M., Rae, P. and Ionita, A.xNon-random crack opening in partially confined, thermally damaged PBX 9501 and observations on its effects on combustion9Parker, A., Claridge, R.P., Proud, W.G. and Johnson, N.A.bCharacterisation and modification of thermally stable high explosives for laser flyer applications'Partom, Y., Yaziv, D. and Rosenberg, Z.7Shock release of 2024-T351 aluminum in the 10 GPa range387-391Partom, Y. and Rosenberg, Z.#More on the precursor decay anomaly
Partom, Y.;Modeling the crossover in reaction rate for micronized TATB@Understanding the Swegle-Grady (strain rate goes as s4) relation317-319Partom, Y. and Yaziv, D.HPenetration of L/D=10 and 20 tungsten alloy projectiles into RHA targets	1801-1804.Accounting for the penetration entrance effect<Calibration of DSD parameters for LX-07 from rate-stick data+Failure diameter of confined explosive rods0Partom, Y., Anderson�  Jr., C.E. and Orphal, D.L.GFurther investigation of the target resistance penetration parameter Rt	1129-1132<  FHydro-reactive computations with a temperature dependent reaction rate460-463!Long-rod moving-plate interactionMore on D(k) for PBX-9502/Reactive flow calculations near a free boundaryXPartouche-Sebban, D., P"�lissier, J.-L., Anderson, W.W., Hixson, R.S. and Holtkamp, D.B.GCharacterization of sapphire for optical pyrometry in shock experiments*Paisley, D.L., Warnes, R.H. and Kopp, R.A.zLaser-driven flat plate impacts to 100 GPa with sub-nanosecond pulse duration and resolution for material property studiesFPaisley, D.L., Swift, D.C., Johnson, R.P., Kopp, R.A. and Kyrala, G.A.^Laser-launched flyer plates and direct laser shocks for dynamic material property measurementsvPaisley, D.L., Luo, S.N., Swift, D.C., Greenfield, S., Loomis, E., Johnson, R., Peralta, P., Koskelo, A. and Tonks, D.@Experimental method for laser-driven flyer plates for 1-D shocks&Pak, H.-R., Horie, Y. and Graham, R.A.OSynthesis of nickel-aluminum alloys by shock compression of composite particles761-766.Palanivel, B., Kalpana, G. and Rajagopalan, M.-Physical properties of thorium under pressure0Palmer, S.J.P., Williamson, D.M. and Proud, W.G.4Adhesion studies between HMX and EDC37 binder system;Palmer, S.J.P., Williamson, D.M., Proud, W.G. and Bauer, C.0Thermal properties of a UK PBX and binder systemoPalmour�  III, H., Kim, K.Y., Batchelor, A.D., Hare, T.M., Goudey, G.T., More, K.L., Linse, V.D. and Adair, J.H.PInfluence of dynamic pressure on sinterability of shock-consolidated TiC powders"Pangilinan, G.I. and Russell, T.P.bReal-time changes induced by pulsed laser heating in ammonium perchlorate at static high pressures4Panov, V., Vignjevic, R., Bourne, N. and Millett, J.9Material failure modelling in metals at high strain rates646-649Pappu, S. and Murr, L.E.EMicrostructural and computer simulation studies on some EFP materials;Paris, V.E., Zaretsky, E.B., Kanel, G.I. and Savinykh, A.S.TDiagnostics of ductility, failure and compaction of ceramics under shock compressionParis, V.E. and Zaretsky, E.B.QStudy of compressive failure of alumina in impact experiments with divergent flow880-883+Parkash, V., Freund, L.B. and Clifton, R.J.%Plane strain fracture in plate impact9Failure wave in DEDF and sodalime glass during rod impactZOrphal, D.L., Anderson�  Jr., C.E., Behner, T., Hohler, V., Wickert, M. and Templeton, D.W.8Failure kinetics in borosilicate glass during rod impactSOsher, J.E., Chau, H.H., Gathers, G.R., Lee, R.S., Pomykal, G.W. and Weingart, R.C.pShock-wave studies using plastic flyers driven by an electric gun for hypervelocity impact on selected materials9Osher, J.E., Chau, H.H., Gathers, G.R. and Weingart, R.C.QCharacteristics of flyer impact for one-dimensional shock-wave study applications"�stmark, H.WShock induced sub-detonation chemical reactions in 1,3,5-triamino-2,4,6-trinitrobenzeneOvidko, I.A.ROn dislocation ensemble evolution in fcc metals under high strain rate deformation461-4638On new mechanism for plastic flow in shock loaded solidsOwens, F.J.kElectron paramagnetic resonance study of shock-induced reactions of some small molecules in the solid stateOwens, F.J. and Politzer, P.mMolecular orbital calculation of indices of impact and shock induced reactivity in trinitroaromatic molecules857-861FEffect of shock and hydrostatic pressure on H bonding in water and iceOwens, F.J. and Iqbal, Z.rMicrowave absorption measurement of flux trapping in shocked processed high temperature superconductor YBa2Cu3O7-y599-601)Owens, F.J., Iqbal, Z. and Thadhani, N.N.]Magnetic field dependent microwave absorption in the shocked 85K superconductor Bi-Sr-Ca-Cu-O=Oxby, T., Perger, W.F., Zhao, J., Winey, J.M. and Gupta, Y.M.CCalculating elastic constants of molecular crystals using CRYSTAL98:Pahl, R.J., Trott, W.M., Snedigar, S. and Caste"�eda, J.N.aEvaluation of aluminum participation in the development of reactive waves in shokc compressed HMX990-993
Paisley, D.L.PLaser-driven miniature flyer plates for shock initiation of secondary explosives0Oh, K.-H., Yang, Y.-J., Kim, H.-J. and Kim, H.W.0A simple model for multiple shock Hugoniot state$Oh, K.-H., Kim, H.-J. and Lee, H.-W.5Behavior of Gr"�neisen g in the multiple shock regionHOhno, I., Hanayama, Y., Kimura, M., Suzuki, I., Oda, H. and Kumazawa, M.LPressure derivatives of elastic constants of iron by cavity resonance method@Oinuma, S., Tanaka, K., Iida, M., Nakayama, Y. and Matsunaga, T.+Diamonds recovered from detonation productsVIn situ magnetic gauging technique used at LANL: Method and shock information obtained	1043-1048TSheffield, S.A., Davis, L.L., Baer, M.R., Engelke, R., Alcon, R.R. and Renlund, A.M.:Hugoniot and shock initiation studies of isopropyl nitrateLSheffield, S.A., Gustavsen, R.L., Alcon, R.R., Robbins, D.L. and Stahl, D.B.@High pressure Hugoniot and reaction rate measurements in PBX9501^Sheffield, S.A., Dattelbaum, D.M., Alcon, R.R., Robbins, D.L., Stahl, D.B. and Gustavsen, R.L.DShock-induced chemical reaction in organic and silicon based liquidsShen, X.A. and Gupta, Y.M.PTime-resolved luminescence measurements in ruby shocked along the crystal A-axis893-895
Sherman, D.M.IElectronic structure, entropy and the high-pressure stability of bcc ironAShibue, T., Nakayama, E., Natsumura, T., Tanaka, T. and Asano, T.0Numerical simulation of impact penetration tests	1789-1792[Shigemori, K., Ichinose, D., Irifune, T., Otani, K., Shiota, T., Sakaiya, T. and Azechi, H.^Measurements of sound velocity of laser-irradiated iron foils relevant to Earth Core condition	1480-1483
Shimamura, S.HA computer model for the evolution of impact damage in brittle materialsShimizu, H. and Sasaki, S.New method of high-pressure Brillouin studies for elastic properties of molecular single crystals grown in a diamond-anvil cellAShishkova, N.V., Malyshev, E.N., Shepel, V.M. and Mikheenko, P.N.]Influence of pressure and temperature of deformation on phase composition of yttrium ceramicsNShkuratov, S.I., Talantsev, E.F., Baird, J., Altgilbers, L.L. and Stults, A.H.xTransverse explosive shock-wave compression of Nd2Fe14B high-energy hard ferromagnets: Induced magnetic phase transition282-285tDirect Monte Carlo simulation of chemical equilibrium composition of molecular fluid mixtures under shock conditions>Chemical equilibrium in high pressure molecular fluid mixturesPAn 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 clustersTA hybrid Monte Carlo method for equilibrium equation of state of detonation products:Direct simulation of detonation products equation of stateShaw, M.S. and Tymczak, C.J.~Theoretical N2 Hugoniot using MondoSCF density functional quantum energies and a very efficient Monte Carlo reweighting scheme�Monte Carlo simulations of the effect of cross-potential variations on the equation of state of N2CO2 mixtures and of detonation products$Sheffield, S.A. and Bloomquist, D.D.1Low pressure Hugoniot cusp in polymeric materials57-61Sheffield, S.A. and Fisk, G.A.DParticle velocity measurements in laser irradiated foils using ORVIS7Sheffield, S.A., Rogers�  Jr., J.W. and Caste"�eda, J.N.MVelocity measurements of laser-driven flyers backed by high impedance windows541-546Sheffield, S.A. and Dugan, D.W.4Description of a new 63-mm diameter gas gun facility565-570Sheffield, S.A.-Onset of shock-induced reaction in liquid CS2Sheffield, S.A. and Alcon, R.R.)Shock indu<  ced reaction in several liquids,In-situ magnetic gauge measurements in Kel-FNSheffield, S.A., Gustavsen, R.L., Alcon, R.R., Graham, R.A. and Anderson, M.U.<Particle velocity and stress measurements in low density HMX0Sheffield, S.A., Gustavsen, R.L. and Alcon, R.R.FObservations of shock-induced reaction in liquid bromoform up to 11GPa6Hugoniot and initiation measurements on TNAZ explosive9Porous HMX initiation studies: Sugar as an inert simulantElastic properties of HMXSewell, T.D. and Menikoff, R.DComplete equation of state for b-HMX and implications for initiation7Shahinpoor, M., Asay, J.R., Dixon, W.R. and Hawke, R.S.5Effects of barrel joints on hypervelocity projectilesGShaner, J.W., Hixson, R.S., Winkler, M.A., Boness, D.A. and Brown, J.M.Birch's law for fluid metalsShaner, J.W.;Role of d-electrons in phase transitions and thermodynamicsbSharma, J., Hoffsommer, J.C., Glover, D.J., Coffey, C.S., Santiago, F., Stolovy, A. and Yasuda, S.pComparative study of molecular fragmentation in sub-initiated TATB caused by impact, UV, heat and electron beams9Sharma, J., Forbes, J.W., Coffey, C.S. and Liddiard, T.P.FThe nature of reaction sites and sensitization centers in TATB and TNTtNiles, A.M., Garcia, F., Greenwood, D.W., Forbes, J.W., Tarver, C.M., Chidester, S.K., Garza, R.G. and Switzer, L.L.[Measurement of low level explosive reaction in gauged multi-dimensional Steven impact tests886-889ENiska, H.M., Charron, A.E., Schulz, T.J., Perger, W.F. and Kunz, A.B.=Dynamic simulation of a crystal lattice under impulse loading>Norman, G.E., Kuksin, A.Y., Stegailov, V.V. and Yanilkin, A.v.pAtomistic simulation of plasticity and fracture of crystalline and polycrystalline metals under high strain rate329-334+Norwood, F.R., Graham, R.A. and Sawaoka, A.4Instability of plastic flow at dynamic pore collapse=Nesterenko, V.F., Meyers, M.A., Chen, H.C. and LaSalvia, J.C.=Chemical reactions in controlled high-strain-rate shear bandsNControlled high rate strain shear bands in inert and reactant porous materials609-614=Solitons, shock waves in strongly nonlinear particulate media9Nesterenko, V.F., Indrakanti, S.S., Brar, S. and Gu, Y.B.GLong rod penetration test of hot isostatically pressed Ti-based targets6Nesterenko, V., Maple, M.B., Taylor, B.J. and Gu, Y.B.[Modification of magnesium diboride properties using shock loading and hot isotatic pressing	1114-1117MNeumeier, J.J., Nellis, W.J., Maple, M.B., Torikachvili, M.S. and Sales, B.C.GSuperconductivity of A15-phase Nb3Si synthesized by Mbar shock pressureNeuwald, P.6Explosively driven combustion of shock-dispersed fuels976-981,Newlander, C.D., Stone, S.F. and Burns, J.B.QMeasurement and analysis of pulsed laser generated stress waves in epoxy and PMMA<Newlander, C.D., Cherest, J.A., Lilly, M.C. and Eisler, R.D.Wave propagation in polymers. 22Ng, A., Pareniuk, D., Celliers, P. and DaSilva, L.3Reflectivity measurements on shock-unloading solidsNg, A.8Recent experiments in laser-driven shock waves in solidsjNg, A., da�  Silva, L., Godwal, B.K., Chiu, G., Cottet, F., Richardson, M.C., Jaanimagi, P.A. and Lee, Y.T.EK-shell photoabsorption edge spectroscopy in shock compressed plasmasShock waves and plasma physics53-58Nguyen, J.H. and Holmes, N.C./Iron sound velocities in shock wave experiments/Shock induced birefringence in lithium fluorideLNguyen, J.H., Orlikowski, D., Streitz, F.H., Holmes, N.C. and Moriarty, J.A.TSpecifically prescribed dynamic thermodynamic paths and resolidification experiments	1225-1230Nichols�  III, A.L.WNellis, W.J., Moss, W.C., Radousky, H.B., Mitchell, A.C., Maple, M.B. and McElfresh, M.>Properties of niobium recovered from megabar dynamic pressures719-724Nitrogen at high pressure43-49+Nellis, W.J., Gourdin, W.H. and Maple, M.B..Shock-induced melting and rapid solidificationaNellis, W.J., Koch, R., Davidson, H., Hunter, J.W., Brocius, W.F., Marshall, A. and Geballe, T.H.=Micron thin niobium films recovered from Mbar shock pressuresLNellis, W.J., Mitchell, A.C., Erskine, D.J., McCandless, P.C. and Weir, S.T.JEnergy gap of molecular hydrogen from electrical conductivity measurements111-112\Fluids at high shock pressures and temperatures and some thoughts about future possibilitiesTNellis, W.J., Weir, S.T., Hinsey, N.A., Balachandran, U., Kramer, M.J. and Raman, R..Disks of YBa2Cu3O7 shocked to 10 GPa pressuresNellis, W.J. and Mitchell, A.C.6Molecular and planetary fluids at high shock pressures13-19HSensitivity and accuracy of Hugoniot measurements at ultrahigh pressuresNellis, W.J. and Dlott, D.3Future directions in dynamic high pressure researchNellis, W.J. and Petach, T.,Systematics of compression of hard materialsNelmes, R.J. and McMahon, M.I.9Powder diffraction studies of structures at high pressure8Nemat-Nasser, S., Sano, Y., Chang, S.N. and Meyers, M.A.TIncubation time and growth pattern of martensite under a short duration stress pulse181-184Nemes, J.A. and Eftis, J.LUse of viscoplastic constitutive theory for simulating spallation thresholdsbNemtchinov, I.V., Shulov, V.V., Artemieva, N.A., Ivanov, B.A., Kosarev, I.B. and Trubetskaya, I.A.0Light flashes caused by impacts against the Moon957-960Nesterenko, V.F.`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. and Ershov, I.V.?Spall plane formation near spall threshold for different metals
Naimark, O.B.bMesodefects collective properties and self-similar regularity of shocked condensed matter behavior2Naimark, O., Plekhov, O., Proud, W. and Uvarov, S.ODamage-failure transition: Dynamic crack branching, fragmentation, failure waveLSekine, T., Hirata, N., Yamaguchi, A., Kobayashi, T., He, H. and Tang, Z.-P.RShock flattening of spheres in porous media: Implications for flattened chondrules+Sekine, T., Kobayashi, T. and Hintzen, H.T..Shock compression of magnesium silicon nitride@Selezenev, A.A., Berezhko, P.G., Ganchuk, N.S. and Kreknin, D.A.MMolecular 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. and Voronin, B.L.AMolecular dynamics simulation of shock wave compression of metals374-377!Schonberg, W.P. and Ebrahim, A.R.YA shock physics based model of a oblique impact of a thin plate by a spherical projectileSchott, G.L.EMeasured Hugoniot states of a two-element fluid, O2 + N2 near 2 Mg/m3%Schouten, J.A. and Scheerboom, M.I.M.YInfluence of a rare gas on the vibrational spectrum of a diatomic system at high pressure	1487-14906Schuster, S.H., England, R., Koik, V. and Wagner, M.H.z1- and 2-dimensional calculations of the effect of high pressure EOS models on the energy partitioning in cratering events<Schwartz, A.J., Cazamias, J.U., Fiske, P.S. and Minich, R.W.;Grain size and pressure effects on spall strength in copper�Schwartz, C.L., Hogan, G.E., Kwiatkowski, K., Rigg, P.A., Rightley, P.M., Mariam, F.G., Marr-Lyon, M., Merrill, F.E., Morris, C.L., Saunders, A. and Tupa, D.<New capabilities of 800 MeV proton radiography at Los Alamos	1136-1138>Schwarz, R.B., Kasiraj, P., Vreeland�  Jr., T. and Ahrens, T.J.DThe effect of shock duration on the dynamic consolidation of powdersSchwarz, O.J. and Horie, Y.IStress fluctuation and order generation in shearing of granular materials
Seaman, L.@Development of computational models for microstructural features118-129Seaman, L. and Keough, D.D.;Lagrangian analysis with an emphasis on unloading phenomena3Determining a soil model from wave propagation data627-632]Seaman, C.L., Early, E.A., Maple, M.B., Nellis, W.J., Holt, J.B., Kamegai, M. and Smith, G.S.WSuperconducting and microstructural properties of shock compacted high Tc oxide powders.Seaman, L., Boustie, < M. and de�  Resseguier, T.HUse of the Steinberg and Carroll-Holt model concepts in ductile fractureSeaman, L. and Curran, D.R..Inertia and temperature effects in void growthSecco, R.A.9High pressure measurements of viscosities of Fe-S liquidsQUniversal relations for acceleration wave speeds in nonlinear viscoelastic solidswApproximate universal relations between shock and acceleration wave speeds for oblique plate impact of inelastic solidsSchiferl, S.K.HTwinning, texture and constitutive relations for explosively formed jets0Schiferl, S.K., Davidson, R.F. and Maudlin, P.J.1Effects 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. and Fischer, J.E.+Role of pressure in the study of fullerenes,Schloessin, H.H., Secco, R.A. and Spal, R.D.MOn pressure figures in single crystals, mechanical strength and high stresses8Schmalz, R.F., Fedosejevs, R., Sigel, R. and Teng, Y.-L.&Laser-driven shock waves in plexiglass535-539
Schmidt, R.M.Boeing shock physics laboratory634-638+Schmidt, S.C., Moore, D.S. and Shaner, J.W.2Raman spectroscopies in shock-compressed materials293-3028Schmidt, S.C., Moore, D.S., Shaw, M.S. and Johnson, J.D.<Vibrational spectroscopy of shock compressed fluid N2 and O2ICoherent anti-Stokes Raman spectroscopy of shock-compressed liquid oxygenSchmitt, D.R. and Ahrens, T.J.+Emission spectra of shock compressed solids*Schmitt, D., Svendsen, B. and Ahrens, T.J.%Shock induced radiation from minerals261-2658Schmitt, M.J., Kopp, R.A., Moore, D.S. and McGrane, S.D.EAnalysis of laser-driven shocks in confined and unconfined geometries
Schmitt, R.G.0Toward a new paradigm for reactive flow modelingSchneider, H. and Jung, I.EStructural deformation of experimentally shock-loaded periclase (MgO)140-144YSchneider, M.S., Gregori, F., Kad, B.K., Kalantar, D.H., Remington, B.A. and Meyers, M.A.DLaser-induced shock compression of copper and copper aluminum alloysLShock compression of deuterium at Mbar pressures and the interior of Jupiter
Saumon, D.'A new tabular EOS for hydrogen isotopesSavic, P. and Celebonovic, V.0Dense matter theory: A simple classical approach>Savinykh, A.S., Kanel, G.I., Razorenov, S.V. and Rajendran, A.HCompressive fracture of brittle materials under divergent impact loading888-891<A study of pre-stress effect on the failure waves in glassesASaw, C.K., Zaug, J.M., Farber, D.L., Weeks, B.L. and Aracne, C.M.eUsing simultaneous time-resolved SHG and XRD diagnostics to examine phase transitions of HMX and TATB856-859Saw, C.K. and Tarver, C.M.:Binder/HMX interaction in PBX9501 at elevated temperaturesSawaoka, A. and Kondo, K.4Shock wave facility at Tokyo Institute of Technology696-700
Sawaoka, A.B.7The role of shock wave compression in materials science51-56Sawaoka, A.B. and Akashi, T.?A new concept of dynamic sintering utilizing post shock heating6Sawaoka, A.B., Kunishige, H., Tamura, H. and Horie, Y.OHeterogeneous shock compression mechanism of diamond powders in a metal capsule<Sawaoka, A.B., Dan, K., Tamura, H., Horie, Y. and Yamada, K.oLocal rapid quenching in a powder mixture and its utilization to synthesize novel compounds in the B-C-N system*Sawas, O., Brar, N.S. and Ramamurthy, A.C.QHigh strain rate characterization of plastics using polymeric split Hopkinson bar(Sawas, O., Brar, N.S. and Brockman, R.A.GHigh 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 impactHUniversal relations for pressure-shear waves in nonlinear elastic solidsScheidler, M. and Gazonas, G.UAnalytical and computational study of one-dimensional impact of graded elastic solids.Sandstrom, F.W., Persson, P.A. and Olinger, B.ZIsothermal and shock compression of high density ammonium nitrate and ammonium perchlorate=Sandstrom, F.W., Abernathy, R.L., Leone, M.G. and Banks, M.L.ODiameter effect and detonation front curvature of ideal and nonideal explosives.Sandusky, H.W., Elban, W.L. and Liddiard, T.P.Compaction of porous beds%Shock Waves in Condense Matter - 1983"Sandusky, H.W. and Bernecker, R.R.=Shock reactivity experiments on a porous composite propellantCGun-launched impact initiation of the composite propellant PBXN-103!Sandusky, H.W. and Chambers, G.P.6Shock reactivity of the liquid propellant Otto Fuel II'Instrumentation of slow cook-off events2Sandusky, H.W., Granholm, R.H. and Yakaboski, O.N.2Deformation around cavities from compressive loads!Sandusky, H.W. and Granholm, R.H.4Prompt reaction of aluminum in detonating explosives(Violent reactions from non-shock stimuli991-996Sano, Y. and Sano, T.KThermal properties of close-packed iron determined using Hugoniot functions2Precursor decay in single crystal lithium fluoride/Unsteady state Rankine-Hugoniot jump conditions2Jump across an outgoing spherical shock wave frontLEvaluation of the precursor decay anomaly in single crystal lithium fluoride.Dynamic yielding behind near-steady precursorsOSapozhnikov, F.A., Dremov, V.V., Derbenev, I.V., Karavaev, A.V. and Soulard, L.4Molecular dynamics simulation of TATB-like explosiveSarracino, R.S. and Guest, A.>Measured and predicted strains in the near zone of a blastholeSasaki, S. and Shimizu, H.5High-pressure Brillouin study of liquid and solid N2OQSatapathy, S., Cazamias, J., Bless, S., Monfredo�  Gee, R., Meyer, L. and Brar, N.1Dynamic strength of tungsten-nickel-cobalt alloysSaumon, D. and Guillot, T.-Rycerz, Z.A., Jacobs, P.W.M. and Hooton, I.E.&Molecular dynamics study of detonationGSaburi, T., Kubota, S., Ogata, Y., Wada, Y., Itou, A. and Nakanishi, T.CStudy of the projectile impact on aluminum targets divided by water1Salansky, N., Mar, H., Hawken, D. and Kleiman, Y.<Basic features of dynamic phase transition in finite samples:Salisbury, D.A., Winter, R.E., Taylor, P. and Harris, E.J.*The response of foams to shock compression-Salisbury, D.A., Giles, A.R. and Winter, R.E..Transmission of shocks along thin-walled tubes Salisbury, D.A. and Markland, L.HAssessment and application of a PVDF gauge strain compensation technique(Salisbury, D., Winter, R. and Biddle, L.rA study on the effect of electrical energy imput on detonation failure in wedges of the TATB-based explosive EDC35	1010-1013Saltz, D. and G"�len, S.C.0A study of the liquefaction shock wave structure)Salyer, T.R., Khalsa, N.S. and Hill, L.G.6An automated test bed for VISAR probe characterizationSalyer, T.R. and Hill, L.G.5The incidental effects of gaps in detonating PBX 9501Samara, G.A. and Bauer, F.7Hydrostatic pressure studies of PVDF and its copolymersSamara, G.A.XThe effects of pressure on the b molecular relaxation process in polyvinylidene fluoride:Samara, G.A., Hansen, L.V., Morosin, B. and Schirber, J.E.\Effects of pressure on the orientational ordering and phase transitions in solid C60 and C70LFrom ferroelectric to quantum paraelectric KTa1-xNbxO3 (KTN): A model system176-179)Samsonov, D., Zhdanov, S. and Morfill, G.3Shock waves and solitons in complex (dusty) plasmas	Sanai, M.ATwo examples of industrial applications of shock physics research463-467QSander, R., Blais, N., Engelke, R., Dattelbaum, D., Sheffield, S. and McInroy, R./Shock-induced chemistry in polydimethylsiloxaneRubin, M.B.+Analysis of weak shocks in 6061-T6 aluminum&Rubin, M.B., Elata, D. and Attia, A.V._Modeling added compressibility of porosity and the thermomechanical response of wet porous rockLRudakov, F.M., Hastings, J.B., Dowell, D.H., Schmerge, J.F. and .Weber, P.M.HMegavolt electron beams for ultrafast time-resolved electron diffraction	1287-1292Ruggiero, A. and Bonora, N.<  KDuctile damage prediction in Taylor impact cylinder test using CDM approachZOn the presence of the elastic precursor in re-shock experiment: An unorthodox explanationnRuggiero, A., Bonora, N., Torrice, G., Di�  Sciuva, M., Degiovanni, M., Mattone, M., Gherlone, M. and Frola, C.aNickel based superalloy containment case design: Constitutive modeling and computational analysisRumchik, C.G. and Jordan, J.L.dEffect of aluminum particle size on the high strain rate properties of pressed aluminized explosivesRuoff, A.L.+High pressure as a probe of the solid state13-34'Implications of experiments on hydrogenRuoff, A.L. and Ghandehari, K.;Thermodynamic limits of the index of refraction of hydrogen3Refractive index of diamond anvils at high pressure1Ruoff, A.L., Luo, H., Xia, H. and Vanderborgh, C.)5 mm X-ray appertures and their metrology	1633-1636FRupp, T.D., Gehr, R.J., Stahl, D.B., Sheffield, S.A. and Robbins, D.L.@Temperature controlled vessel for equation of state measurementsVRupp, T.D., Gehr, R.J., Bucholtz, S.M., Robbins, D.L., Stahl, D.B. and Sheffield, S.A.TStereo camera system for calibration and analysis of small laser-driven flyer plates%Russell, R., Bless, S.J. and Beno, T.-Impact induced failure zones in Homalite bars(Rutkevich, I., Zaretsky, E. and Mond, M.$Stability of strong shocks in metals,Ruuskanen, P.R., Kiiski, A.A. and Heczko, O.;Microstructure of dynamically compacted amorphous materialsoA review of some recent theoretical calculations of phase transitions and comparisons with experimental results,Ross, M., Mao, H.K., Bell, P.M. and Xu, J.A.NThe equation of state of dense argon: A comparison of shock and static studies;The dissociation of dense liquid nitrogen and shock coolingRoth, J.vCorrelation of impulsive strain effects in rocks with detonation parameters of the strain-generating explosive charges475-479EFurther considerations of the adiabatic exponent in steady detonation%Do JCZ and BKW EoS need modification?hLarge-scale molecular dynamics simulations of shock wave in Laves crystals and icosahedral quasicrystals378-381FConstant volume specific heat capacity of the CJ state of nitromethane.Shock waves and solitary waves in bcc crystals302-305?The relation between solitons and interactions in bcc materials,Rothman, S.R., Evans, A.M. and Freeman, N.J.9Copper shock Hugoniot experiments using high power lasersRothman, S.D. and Evans, A.M.7High 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. and Hall, C.ZMeasurements of the equation of state of lead under varying conditions by multiple methodsARothman, S.D., Parker, K.W., Davis, J.-P., Palmer, J. and Maw, J.CIsentropic compression of lead and lead alloy using the 'Z' machineRottenkolber, E. and Arnold, W.7An analytic model of close-range blast fragment loading	1403-1406
Rottler, J.S.ZMultigroup radiation transport in one-dimensional Lagrangian radiation-hydrodynamics codesMRadiation diffusion in the three-dimensional radiation-hydrodynamics code CTHiRoutley, N.R., Price, E., Keightley, P.T., Millett, J.C.F., Bourne, N.K., Brown, E.N. and Gray�  III, G.T.JAn investigation of surface velocimetry of shocked polyethylene using HetVLTwo dimensional compression shock waves generated by plate impact techniques2The response of ceramic materials to shock loading439-446^Shear strength of titanium diboride under shock loading measured by transverse manganin gaugesRosenberg, Z. and Brar, N.S.+Hysteresis of lateral piezoresistive gauges	1707-1710jOn the correlation between dynamic compressive strengths of strong ceramics and their indentation hardnessRosenberg, Z. and Ginzburg, A.OOn the source for failure of commercial manganin gauges at high shock pressures?Rosenberg, Z., Dekel, E., Hohler, V., Stilp, A.J. and Weber, K.bPenetration of tungsten alloy rods into composite ceramic targets: Experiments and 2-D simulations@Review on lateral stress measurements with piezoresistive gauges	1033-1037@Rosenberg, Z., Bourne, N.K., Gray�  III, G.T. and Millett, J.C.F.@On the measurement of shear-strength in quasi-isentropic loadingRosenberg, Z. and Dekel, E.-On the entrance phase in long rod penetration	1310-1313)Rosenberg, Z., Ginzburg, A. and Dekel, E.EMore on the use of commercial carbon resistors as low pressure gauges/Rosenberg, Z., Bourne, N.K. and Millett, J.C.F._Calibration of commercial gauges of varying geometry to measure the lateral component of stress6Rosenberg, Z., Ashuach, Y., Bourne, N.K. and Dekel, E.OOn the shock response of soda lime glass: The failure of embedded stress gauges�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. and Wark, J.S.fX-ray diffraction from shocked crystals: Experiments and predictions of molecular dynamics simulationsRoss, M. and Nellis, W.J.OEquation of state experiments and theory relevant to modeling the major planets226-230Ross, M.dMicrostructural-hardness correlations in shock-loaded and quasi-statically deformed 6061-T6 aluminum
North HollandARomain, J.P., Hallouin, M., Gerland, M., Cottet, F. and Marty, L.Fa to e phase transition in iron induced by laser generated shock wavesRomain, J.P. and Zagouri, D.ULaser shock studies using an electromagnetic gauge for particle velocity measurements4Romain, J.P., Bauer, F., Zagouri, D. and Boustie, M.?Measurements of laser induced shock pressures using PVDF gauges	1915-1918Romero, V. and Williams, P.E.%Blast waves from non-ideal explosivesxRosen, M.D., Phillion, D.W., Price, R.H., Campbell, E.M., Obenschain, S.P., Whitlock, R.R., McLean, E.A. and Ripin, B.H.iCreation of ultra high pressure shocks by the collision of laser accelerated disks: Experiment and theory*Rosenberg, G., Yaziv, D. and Mayseless, M.LElectromagnetic gauge for measuring the radial particle velocity in 2-D flow495-499
Rosenberg, G.>RAFAEL Terminal Ballistics Laboratory: Facility and capability706-710.Rosenberg, Z., Mayseless, M. and Rosenberg, G.NMeasurement of the radial displacement in 2D flow by embedded constantan wiresRosenberg, Z. and Partom, Y.jDirect measurement of temperature in shock-loaded polymethylmethacrylate with very thin copper thermistors`On the lateral stress measurement in shock loaded targets with transverse piezoresistance gauges525-530
Rosenberg, Z.fDetermination of dynamic yield strengths with manganin gauges embedded in impulsively-loaded long rods=Rosenberg, G., Lopatin, C.M., Rajendran, A.M. and Bless, S.J.;Electrically driven expanding ring generator set up at UDRI)Rosenberg, Z., Brar, N.S. and Bless, S.J.UDetermination of the strength of shock loaded ceramics using double impact techniquesRosenberg, G. and Curran, D.R.|Multiphase equation of state and strength properties of beryllium from ab initio and quantum molecular dynamics calculations;Robertson, D.H., Brenner, D.W., Elert, M.L. and White, C.T.NSimulations of chemically-sustained shock fronts in a model energetic materialRobertson, D.H.1Molecular dynamics simulations of shock processes.Robertson, D.H., Brenner, D.W. and White, C.T.sEffects of crystal orientation on the properties of a chemically sustained shock wave in a model energetic material=Robertson, D.H., Barrett, J.J.C., Elert, M.L. and White, C.T.HSelf-similar behavior from molecular dynamics simulations of detonationsRobinson, A.C.=An analytical model fo<  r Rayleigh-Taylor instability in solidsGRobinson, A.C., Vaughan, C.T., Fang, H.E., Diegert, C.F. and Cho, K.-S.HHydrocode development on the NCUBE and the Connection Machine HypercubesRobinson, C.M.1Modelling of laser spall experiments in aluminium9A multi-phase equation of state for solid and liquid leadIMaterial properties on a phase boundary of a multiphase equation of state274-277-Rodriguez, G., Roberts, J.P. and Taylor, A.J.iElectromagnetically-driven cylindrical 2D shockwave profile measurements in water with laser shadowgraphy9Rodriguez, G., Clarke, S.A., Taylor, A.J. and Forsman, A.qDiagnosis of ultrafast laser-heated metal surfaces and plasma expansion with absolute displacement interferometry	1401-1404#Roessig, K.M. and Foster�  Jr., J.C.PExperimental simulations of dynamic stress bridging in plastic bonded explosives
Roessig, K.M.0Mesoscale mechanics of plastic bonded explosives973-978.Roessig, K.M., Gonthier, K.A. and Klomfass, A.>Modeling of low pressure compaction and mesoscale localization800-803>Rohde, R.W., Wise, J.L., Byrne, J.G. and Panchanadeeswaran, S.#Riedel, W., Nahme, H. and Thoma, K.bEquation of state properties of modern composite materials: Modeling shock, release and spallationRigg, P.A. and Gupta, Y.M.wX-ray diffraction measurements to determine longitudinal and transverse lattice deformation in shocked lithium fluoride	1051-1056GRigg, P.A., Anderson, W.W., Olson, R.T., Buttler, W.T. and Hixson, R.S.HInvestigation of ejecta production in tin using plate impact experimentsVRigg, P.A., Schwartz, C.L., Hixson, R.S., Saunders, A., Merrill, F.E. and Morris, C.L.KDirect shock-density measurements using plate impact and proton radiography	1125-1130Rightley, M.lCalibration and validation of high explosives equations of state with an experimental cylinder test database#Rimer, N., Cherry, J.T. and Lie, K.HSimulation of particle velocity records from small scale explosive tests*Riou, C., Cottentot, C.E. and Boussuge, M.6New experimental approach of impact on silicon carbide'Ripley, R.C., Zhang, F. and Lien, F.-S.FShock interaction of metal particles in condensed explosive detonationMAcceleration and heating of metal particles in condensed explosive detonationTRobbins, D.L., Gehr, R.J., Harper, R.W., Rupp, T.D., Sheffield, S.A. and 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. and Stahl, D.B.5Dynamic properties of shock loaded thin uranium foils.Robbins, D.L., Sheffield, S.A. and Alcon, R.R.9Magnetic particle velocity measurements of shocked TeflonRobbins, J. and Voth, T.E.wAn extended finite element method formulation for modeling the response of polycrystalline materials to dynamic loading7Roberson, S., Davis, R.F., Joshi, V.S. and Fienello, D.-Shock compaction of molybdenum nitride powder643-646'Robert, G., Sollier, A. and Legrand, P.:Spectroscopic studies of shocked and detonating explosives547-552PRaman spectroscopic studies of shock-compressed nitromethane and nitromethane-d3
Renlund, A.M.KReactive wave growth in shock-compressed thermally degraded high explosives$Resnyansky, A.D. and Gray�  III, G.T.RNumerical simulations of the influence of loading pulse shape on SHPB measurements2Resnyansky, A.D., Bourne, N.K. and Millett, J.C.F.BExperiment and theory for the characterization of porous materials!Resnyansky, A.D. and Bourne, N.K.bFactors influencing the shape of the fracture wave induced by the rod impact of a brittle material*Shock compression of dry and hydrated sand	1474-1477Resnyansky, A.D.>Constitutive modelling of shock compression of a porous copper4Kinetic behaviour of failure waves in a filled glass"Resnyansky, A.D. and Weckert, S.A.jExpeirmental and theoretical assessment of a device used for evaluation of blast and fragmentation effects	1067-1070>Ribeiro, J., Plaksin, I., Campos, J., Mendes, R. and G"e"is, J.XProcess of shock attenuation inside a hollow glass microsphere/polymeric composite media3Ribeiro, J., Campos, J., Plaksin, I. and Mendes, R.7Shock wave propagation process in epoxy syntactic foams>Ribeiro, J., G"e"is, J., Campos, J., Plaksin, I. and Mendes, R.jInvestigation of collapse and jet formation of hollow glass micro spheres in inert and energetic materials	1021-1024NCharacteristics of shock-compressed configuration of Ti and Si powder mixturesHThadhani, N.N., Subramanian, V., Russell, R., Savage, D. and Gupta, Y.M.XThe effect of pulse duration on shock-induced chemical reaction in Ti-Si powder mixtures^Thadhani, N.N., Vandersall, K.S., Russell, R.T., Graham, R.A., Holman, G.T. and Anderson, M.U.SShock compression of Al+Fe2O3 powder mixtures of different volumetric distributions-Thakur, A.M., Thadani, N.N. and Schwarz, R.B.JMartensitic transformation in NiTi alloys induced by tensile stress pulsesTham, R.H. and Stilp, A.J.DDynamic strength calculations of W-alloys based on grain deformation,Thissell, W.R., Zurek, A.K. and Addessio, F.bMechanical properties and failure mechanisms of carbon fiber reinforced epoxy laminated composites9Thissell, W.R., Zurek, A.K., Tonks, D.L. and Hixson, R.S.ETasker, D.G., Dick, R.D., Wilson, W.H., Lee, R.J. and Gustavson, P.K.NResponse of wet, saturated, and dry riverbed sands to high strain rate loading)Tasker, D.G., Dick, R.D. and Wilson, W.H.MMechanical properties of explosives under high deformation loading conditions[Tasker, D.G., Goforth, J.H., Oona, H., Fowler, C.M., King, J.C., Herrera, D. and Torres, D.VAdvances 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. and Tabaka, L.5Results from isentropic compression experiments (ICE)(Tasker, D.G., Goforth, J.H. and Oona, H.?Isentropic compression studies with high explosive pulsed powerTaylor, J.W.Thunder in the mountainsTaylor, P.A.PThe effects of grain size on the shock sensitivity of porous granular explosivesTaylor, P.A. and Dodson, B.W.3Simulation of lattice damage due to dynamic loading287-292*Taylor, P.A., Boslough, M.B. and Horie, Y.>Modeling of shock-induced chemistry in nickel-aluminum systems.Shock-induced atomic-scale structure in metalsdTaylor, P.E., Gilbert, P.H., Kernthaler, C., Lee, L.M., Smith, E.A., Reeder, S.T. and Anderson, M.U.&Quartz gauge response in ion radiationJTaylor, P., Salisbury, D.A., Markland, L.S., Winter, R.E. and Andrew, M.I.7Reaction of shocked but undetonated HMX-based explosive*Taylor, P., Cook, I.T. and Salisbury, D.A.UDevelopment of an explosively driven sustained shock generator for shock wave studiesGTaylor, E.A., Tsembelis, K., Chapman, D., Proud, W.G. and Cockell, C.S.:Hugoniot properties of dry Yorkshire sandstone up to 8 GPa	1488-1491=Ternovoi, V.Y., Fortov, V.E., Kvitov, S.V. and Nikolaev, D.N.4Experimental study of lead critical point parametersTappan, A.S.DMicronenergetics: Combustion and detonation at sub-millimeter scales997-1002-Tarver, C.M., Erickson, L.M. and Parker, N.L.oShock initiation, detonation wave propagation and metal acceleration measurements and calculations for RX-26-AFTarver, C.M. and Maiden, D.E.fExperimental measurements and numerical simulations of metal spallation by detonating solid explosivesTarver, C.M.5The structure of detonation waves in solid explosives311-315,Tarver, C.M., Simpson, R.L. and Urtiew, P.A.1Shock initiation on an e-Cl-20-estane formulationBChemical reaction and equilibration mechanisms in detonation waves^Next generation experiments and models for shock initiation and detonation of solid explosives873-8777Tarver, C.M., Forbes, J.W., Urtiew, P.A. and Garcia, F.%Shock sensitivity of LX-04 at 150 ��<  C.What is a shock wave to an explosive molecule?42-497Tarver, C.M., Forbes, J.W., Garcia, F. and Urtiew, P.A.SManganin gauge and reactive flow modeling study of the shock initiation of PBX 95011On the existence of pathological detonation waves1Detonation reaction zones in condensed explosives	1026-1029 Tarver, C.M. and Chidester, S.K.>Ignition and growth modeling of detonating TATB cones and arcs(Tashiro, S., Mashimo, T. and Nishida, M.EConsolidation of tantalum nitride system powders by shock compression	1295-1298Tasker, D.G. and Lee, R.J.MHigh current electrical conduction of pressed condensed detonating explosives923-928ALarge tensions and strength of iron in different structure states650-653PRazorenov, S.V., Kanel, G.I., Herrmann, B., Zaretsky, E.B. and Ivanchihina, G.E.MInfluence of nano-size inclusions on spall fracture of copper single crystalsReaugh, J.E.;Computer simulation and analysis of the expanding ring test395-399>Computer simulations of the explosive consolidation of powders>The influence of target strength model on computed perforation	1797-1800CComputer simulations to study the high-pressure deflagration of HMX5Redmer, R., Juranek, H., Nettelmann, N. and Holst, B.+Warm dense hydrogen in the chemical pictureYRedmer, R., Holst, B., Kietzmann, A., Nettelmann, N., Desjarlais, M.F. and Mattsson, T.R.8Nonmetal-to-metal transition in warm hydrogen and helium:Ree, F.H., Nellis, W.J., van�  Thiel, M. and Mitchell, A.C.SExperimental and theoretical studies on shock compression of liquid carbon monoxideIRee, F.H., Nellis, W.J., Trainor, R.J., Mitchell, A.C. and Boslough, M.B.OTheoretical and experimental studies of shock-compressed benzene and polybutene	Ree, F.H.>Phase changes and chemistry at high pressures and temperaturesRee, F.H. and Calef, D.F.0Theoretical Hugoniot of liquid hydrogen fluorideRee, F.H. and van�  Thiel, M.REffective like- and unlike-pair interactions at high pressure and high temperature-One- and multi-component theories of mixturesRee, F.H. and Choi, Y.CStability of the face-centered-cubic phase of heavy rare gas solidsRee, F.H. and Glosli, J.N.1Response of thin sheet due to debris cloud impactRajendran, A.M.,Modeling the shock response of AD995 aluminaRajendran, A.M. and Grove, D.J.EDetermination of Rajendran-Grove ceramic constitutive model constantsRajendran, A.M. and Walsh, K.P.iModeling of in-situ ballistic measurements using the Rajendran-Grove and Johnson-Holmquist ceramic models,Ramamurthy, A.C., Bless, S.J. and Brar, N.S.3Stresses in painted steel coupons from stone impact	1091-1094?Randles, P.W., Libersky, L.D., Carney, T.C. and Sandstrom, F.W.0SPH simulation of fragmentation in the MK82 bombRanga�  Rao, M.P.Spherical shocks in solids681-685Ranga�  Rao, M.P. and Ramu, A.(Study of shock propagation due to impact'Rao, R.S., Godwal, B.K. and Sikka, S.K.1On the primitive hexagonal and w phases of carbonRasky, D.J. and McHenry, M.R.?Construction of porous Hugoniots from solid material properties7Ravelo, R., Holian, B.L., Germann, T.C. and Lomdahl, P.=Directional dependence in shock-induced melting of fcc metals270-2732Ravichandran, G., Chang, S.N. and Nemat-Nasser, S.:Elasto-plastic behavior of a partially stabilized zirconia=Ravichandran, G., Rosakis, A.J., Hodowany, J. and Rosakis, P.OOn the conversion of plastic work into heat during high strain rate deformation557-562Ravindran, P. and Asokamani, R.WElectronic structure and pressure induced superconductivity in Ge, Sn and Pb telluridesVRazorenov, S.V., Bogatch, A.A., Kanel, G.I., Utkin, A.V., Fortov, V.E. and Grady, D.E.MElastic-plastic deformation and spall fracture of metals at high temperaturesTRazorenov, S.V., Kanel, G.I., Utkin, A.V., Bogach, A.A., Burkins, M. and Gooch, W.A.aDynamic strength and edge effects at spall fracture for titanium alloys of varying oxygen content9Razorenov, S.V., Kanel, G.I., Baumung, K. and Bluhm, H.J.)Moir"� interferometry studies of PBX 9501=Rae, P.J., Gray�  III, G.T., Dattelbaum, D.M. and Bourne, N.K.+The Taylor impact response of PTFE (Teflon)Rae, P.J. and Brown, E.N.3The Taylor impact and large strain response of PEEK	1399-13026Rae, P.J., Dickson, P.M., Parker, G.R. and Novak, A.M.MHydrocode modeling and an experimental study of explosively driven water jets{Raevsky, V.A., Aprelkov, O.N., Igonin, V.V., Ignatova, O.N., Knyazev, V.N., Lebedev, A.I., Sinitsyna, S.N. and Yukina, N.A.IHeterogeneous deformation of copper in shock waves a subgrain scale level761-764Raftenberg, M.N.CTensile damage effects in steel plate perforation by a tungsten rodEApplication of a brittle damage model to normal plate-on-plate impact862-865ERagan, C.E., Diven, B.C., Rich, M., Robinson, E.E. and Teasdale, W.A.2Shock compression measurements at pressures >1 TPa169-173Ragan, C.E.$Nuclear-explosive-driven experiments<Syono, Y., Noguchi, Y., Fukuoka, K., Kusuba, K. and Atou, T.OShock induced phase transition of MnO and several other transition metal oxides+Szarzynski, S., Martinez, E. and Heuz"�, O.YExperimental study of the detonation initiation of pure nitromethane by a reflected shock899-901PSzirti, D., Loiseau, J., Batchelor, P., Higgins, A.J., Tanguay, V. and Zhang, F.EDevelopment of a single-stage implosion-driven hypervelocity launcherTagi, Y.|Recent advances in high pressure and high temperature in situ X-ray studies using sintered diamond and synchrotron radiation	1621-1624ATakarabe, K., Takumi, M., Minomura, S., Nakagawa, T. and Ohta, K.:Resonant tunneling in triple barriers diode under pressureKTakarabe, K., Hitomi, S., Mori, Y., Minomura, S., Niwa, E. and Masumoto, K.0Pressure effects on optical properties of AgGaS2OTakarabe, K., Shirase, N., Minomura, S., Kato, H., Watanabe, Y. and Matsuda, K.5Electron emission spectra of DX center under pressureOTakashima, K., Tonda, H., Nishida, M., Hagino, S., Suzuki, M. and Takeshita, T.BPreparation of oxide superconducting coils by explosive compaction4Takayama, K., Saito, K., Obara, T. and Kameshima, N.SHigh pressure generation by underwater shock wave focusing in an ellipsoidal cavityTakemura, K./High-pressure X-ray diffraction study of barium4Takizawa, H., Yamazaki, K., Endo, T. and Shimada, M.WHigh-pressure synthesis and magnetic properties of T1-xT'xGe4(T,T':3d transition metal)7Tamura, H., Ueda, K., Sawaoka, A.B. and Igenbergs, E.B.2Microprojectile acceleration by plasma acceleratorTamura, S. and Horie, Y.FEquations of state for the alkali metals, with generalizations to NaCl
Swenson, C.A.1Shock wave overtake measurements on cesium iodide135-144Swift, R.P.CShock attenuation in saturated rock using an effective stress modelSwift, D.C.Shear banding in Ti-6Al-VSwift, R.P. and Snell, C.M.CSource conditions for exploding wire stress wave impact experiments	1671-1674.Ab fere initio equations of state for aluminum,Ab fere initio equations of state for solids4Ab initio polymorphic equations of state for siliconSwift, D.C. and Braithwaite, M.<Temperature-dependent reactive flow for non-ideal explosives6Swift, D.C., Paisley, D.L., Kyrala, G.A. and Hauer, A.GSimultaneous VISAR and TXD measurements on shocks in beryllium crystals&Swift, D., Paisley, D. and Knudson, M.FEquation of state measurements for beryllium in the ICF capsule regimeSwift, D.C. and Ruiz, C.R.<Laser-induced Mach waves for ultra high pressure experimentsRSwitzer, L.L., Vandersall, K.S., Chidester, S.K., Greenwood, D.W. and Tarver, C.M.]Threshold studies of heated HMX-based energetic material targets using the Steven impact testSyed, I.H. and Brar, N.S.?Strain rate sensitivity of graphite/polymer laminate compositesdHigh strain rate compression and tens< ion characterization of high strength (automotive) sheet steelsJSyono, Y., Goto, T., Wang, W.K., Iwasaki, H., Ohshima, S. and Wakiyama, T.+Shock synthesis experiments of Nb-Si system87-91Syono, Y. and Goto, T.HShock wave facilities for high pressure experiments at Tohoku University701-705	Syono, Y.QShock-induced phase transitions in solids: Their understanding at atomistic levelcSyono, Y., Nagoshi, M., Kikuchi, M., Tokiwa, A., Aoyagi, E., Suzuki, T., Kusaba, K. and Fukuoka, K.=Shock loading effects on high Tc superconductor Bi-Sr-Ca-Cu-O?Sutherland, G.T., Gustavson, P.K., Lemar, E.R. and O'Connor, J.(Shock response of the explosive PBXN-103Sutherland, G.T. and Burns, J.:Explosive response model evaluation using the explosive H62Stress growth measurements for the explosive IRX-4CShock response of a mock explosive containing sugar and HTPB binder808-811.Sutherland, G.T., Lemar, E.R. and Marcus, M.H.�Analysis of wave curvature experiments for monomodal explosives with different crystal quality and particle size characteristicsvSuzuki, I., Kumazawa, M., Inouye, Y., Ohno, I., Oda, H., Sasaki, K., Sugawara, T., Syono, Y., Kumagai, H. and Suda, N.vElasticity measurements on the material analogous to iron in the inner core of the Earth by FT-ultrasonic spectroscopySvendsen, B. and Ahrens, T.J.*Thermal history of shock compressed solids0Swallowe, G.M., Field, J.E. and Hutchinson, C.D.IImpact experiments on thin layers of polymers and intermediate explosives891-898,Swanson, R.W., Straub, G.K. and Holian, B.L.@Molecular dynamics study of sodium using a model pseudopotential241-245*Swanson, D.R., Elert, M.L. and White, C.T.:Detonation Hugoniots produced by piston-driven simulationsSwanson, D.R. and White, C.T.;Steady flow detonations from molecular dynamics simulations7Sweeney, M.A., Perry, F.C., Asay, J.R. and Widner, M.M.-Shock effects in particle beam fusion targets188-192Swegle, J.W. and Grady, D.E.AShock viscosity and the calculation of steady shock wave profiles353-357Swegle, J.W.:A numerical study of Rayleigh-Taylor instability in solidsJHeterogeneous deformation model for the high pressure strength of aluminumRIrreversible phase transitions and wave propagation in silicate geologic materials
Swegle, J.1Non-steady wave profiles and the fourth-power law249-252 Swenson, C.A. and Anderson, M.S.�Formation of six new orthorhombic approximants of decagonal quasicrystals in Al70Co15Ni10Tb5 alloy by quenching under high-static pressure'Su, D., Santare, M.H. and Gazonas, G.A.LNumerical modeling of wave propagation in anisotropically microcracked media"Subramanian, V. and Thadhani, N.N.MReaction behavior of shock compressed aluminum and iron-oxide powder mixturesSudenkov, Y.pInfluence of the structural levels on the elastic-plastic hardening of metals under submicrosecond shock loading627-629Suito, K. and Miyoshi, M._Measurement of ultrasonic wave velocities in silica glass at high temperature and high pressureISultanov, V.G., Kim, V.V., Lomonosov, I.V., Shutov, A.V. and Fortov, V.E..Numerical modelling of deep impact experiments.Sun, C., Zhao, F., Wen, S., Li, Q. and Liu, C.?High velocity flyers accelerated by multi-stage explosive slabsbSun, C., Wang, G., Liu, C., Zhao, J., Tan, F., Wang, G., Mo, J., Zhang, N., Jiang, J. and Chen, J.]Magnetically driven isentropic compression and flyer plate experiments using a capacitor bankSundaram, S. and Clifton, R.J.GFlow behavior of soda-lime glass at high pressures and high shear ratesSurh, M.P. and Runge, K.J.'Theoretical phase diagrams for solid H2Sutherland, G.T.GMultiple stress-time profiles in the Navy explosive PBXN-110 (PBXW-113)JSutherland, G.T., Forbes, J.W., Lemar, E.R., Ashwell, K.D. and Baker, R.N.JMultiple stress-time profiles in a RDX/AP/Al/HTPB plastic bonded explosivetSutherland, G.T., Lemar, E.R., Forbes, J.W., Anderson, E., Miller, P., Ashwell, K.D., Baker, R.N. and Liddiard, T.P.jShock wave and detonation wave response of selected HMX based research explosives with HTPB binder systemsLSutherland, G.T., Ashwell, K.D., O'Connor, J.H., Baker, R.N. and Lemar, E.R.3Shock response of several plastic bonded explosivesrStokes, J., Fulton, R.D., Morgan, D.V., Obst, A.W., Oro, D.M., Oona, H., Anderson, W., Chandler, E.A. and Egan, P.^Material failure and pattern growth in shock-driven aluminum cylinders at the Pegasus facilityStoltz, C.A. and Peiris, S.M.<T-jump/FTIR studies of poly-glycidyl nitrate (PGN) pyrolysisStout, R.B. and Anderson, G.A.(Dislocation kinetics behind shear shocksStout, R.B.BMicrocrack dependent discontinuity conditions across a shock front6Strachan, A., van�  Duin, A.C.T. and Goddard�  III, W.A.ZInitial chemical events in the energetic material RDX under shock loading: Role of defectsVStraight, J.W., Idar, D.J., Smith, L., Osborn, M.A., Viramontes, L.E. and Chavez, P.J.MMeasuring the energy release of low amplitude impact of high explosive events Strand, O.T. and Whitworth, T.L.NUsing the heterodyne method to measure velocities on shock physics experiments?Strassburger, E., Patel, P., McCauley, J.W. and Templeton, D.W.�High-speed photographic study of wave propagation and impact damage in fused silica and AlON using the edge-on impact (EOI) method892-895Straub, G.K.>The overlap of electron core states for very high compressions85-93+Straub, G.K., Wills, J.M. and Wallace, D.C.'Elastic moduli of copper under pressureNExtrapolation of the shear modulus to high compressions and negative pressures#Streletz, G.J. and MacFarland, L.H.=A new browser for the visualization of equation of state dataEStrutt, A.J., Vecchio, K.S., Yu, L.-H., Meyers, M.A. and Graham, R.A.Stuivinga, M. and Carton, E.P./Shock wave compacted, melt infiltrated ceramics-Stuivinga, M., Verbeek, H.J. and Carton, E.P.;Planar compaction of ceramic powders with mining explosives745-750DSu, W.-H., Yu, R.-C., Xu, D.-P., Li, X.-Z., Zhang, Z. and Kuo, K.-H._The role of high pressure experiment and theory in our understanding of gaseous and icy planetsStewart, S.T. and Ahrens, T.J.$Shock wave propagation in porous ice@A new H2O ice Hugoniot: Implications for planetary impact events	1478-1483-Stewart, S.T., Ahrens, T.J. and O'Keefe, J.D.8Impact-induced melting of near-surface water ice on Mars	1484-1487hStewart, D.S., Thomas, K.A., Clarke, S., Mallett, H., Martin, E., Martinez, M., Munger, A. and Saenz, J.HOn the initiation mechanism in exploding bridgewire and laser detonators7Stewart, D.S., Lambert, D.E., Yoo, S. and Wescott, B.L.LExperimental validation of detonation shock dynamics in condensed explosives	1018-1021eStewart, S.T., Kennedy, G.B., Senft, L.E., Furlanetto, M.R., Obst, A.W., Payton, J.R. and Seifter, A.GPost-shock temperature and free surface velocity measurements of basalt(Stewart, D.S., Yoo, S. and Lambert, D.E.4Critical ignition transients in condensed explosives(Stiel, L.I., Rotondi, P. and Baker, E.L.5Optimization of parameters for JCZ3 equation of stateStiel, L.I. and Baker, E.L.>Detonation energies of explosives by optimized JCZ3 proceduresSOptimized JCZ3 procedures for detonation properties at highly overdriven conditions)Stiel, L.I., Baker, E.L. and Capellos, C.KJAGUAR analyses of experimental detonation values for aluminized explosivesEStudy of detonation and cylinder velocities for aluminized explosives5Stiel, L.I., Baker, E.L., Capellos, C. and Poulos, W.JJAGUAR procedures for detonation behavior of silicon containing explosives`Stilp, A.J., Hohler, V., Schneider, E., Tham, R., H"�lsewig, M., Kuscher, G. and Junckermann, W.-Impact facilities at the Ernst-Mach Institute711-712Stixrude, L. and Cohen, R.E.BFirst principles investigation of bcc, fcc, and hcp phases of ironCFlyer velocity characteristics of the laser-driven miniflyer systemStapleton, B.S. and Gupta, Y.M.< FResponse of single crystal calcite shocked to 40 kbar along the c-axisStassis, C.iInelastic neutron scattering of g-iron and the determination of the elastic constants by lattice dynamics0Staudhammer, K.P., Johnson, K.A. and Olinger, B.L1.2 Mbar shock loaded 304 stainless steel: Residual structure and properties#Staudhammer, K.P. and Johnson, K.A.<Mach stem characterization in Mbar designs using RSR powders737-742Staudhammer, K.P.5Temperature effects in shock consolidation of powdersSteele, R.D. and Tan, T.-H.Fast shock tube assemblies>Stegailov, V.V., Kuksin, A.Y., Norman, G.E. and Yanilkin, A.V.^Atomistic study of nanoprecipitates influence on plasticity and fracture of crystalline metals$Steinberg, D.J. and Sharp�  Jr., R.W.kInterpretation of shock-wave data for beryllium and uranium with an elastic-viscoplastic constitutive model367-371Steinberg, D.J.1A rate dependent constitutive model for beryllium4Computer studies of the dynamic strength of ceramics2A rate-dependent constitutive model for molybdenum-Modeling release behavior in shocked tantalum2Stepanov, G.N., Gavriliuk, A.G. and Lyubutin, I.S.;Mossbauer study of HSTHF for Sn119 in NdFeO3 under pressure	1481-1484-Sterer, E., Pasternak, M.P. and .Taylor, R.D.8Pressure induced metallization of the Mott insulator VI2	1453-14568Stevens, G.D., Vesser, L.R., Rigg, P.A. and Hixson, R.S.0Suitability of magnesium oxide as a VISAR window	1353-1356}Stevens, G.D., Lutz, S.S., Marshall, B.R., Turley, W.D., Veeser, L.R., hixson, R.S., Jensen, B.J., Rigg, P.A. and Wilke, M.D.ZSurface specularity as an indicator of shock-induced solid-liquid phase transitions in tinStevenson, D.J.=Song, H., Bless, S.J., Brar, N.S., Simha, C.H. and Jang, S.D.+Shock properties of Al2O3 and ZrO2 ceramics+Song, S.G., Gray�  III, G.T. and Lopez, M.F.5Deformation response of zirconium after shock-loadingSorber, S.S. and Winter, R.E.CThe effect of precursor shocks on the growth to detonation of EDC37$Sorber, S., Taylor, P. and Burns, M.VAn experimental study of corner turning in a granular ammonium nitrate based explosive869-872JSorenson, D.S., Minich, R.W., Romero, J.L., Tunnell, T.W. and Malone, R.M.LEjecta particle size distributions for shock-loaded tin and aluminum targetsSorrell, F.Y. and Kuo, T.-M./Dynamic response of moist soil to shock loadingSouers, P.C. and Garza, R.*Size effect and detonation front curvatureSoulard, L. and Bauer, F.\Applications of standardized PVDF shock gauges for shock pressure measurements in explosivesSoulard, L.BShock polar calculation using Gauss' principle of least constraintNShock polar calculation of inert nitromethane by molecular dynamics simulationOMolecular dynamics and experimental study of shock polarization of nitromethaneSoulard, L. and Crouzet, B.?Molecular dynamics analysis of a liquid explosive reaction zonehSpaulding, D.K., Hicks, D.G., Smith, R.F., Eggert, J.H., McWilliams, R.S., Collins, G.W. and Jeanloz, R.LNew optical diagnostics for equation of state experiments on the Janus laser
Stacey, F.QThermodynamic relationships and the properties of iron at Earth's core conditionsCStacy, H.L., Steitz, W.L., Wackerle, J., Polcyn, M. and Esparza, E.0Contained high explosive firing facility (CHEFF)	1675-1678/Staehler, J.M., Predebon, W.W. and Pletka, B.J.=The response of a high purity alumina to plate impact testingTStahl, D.B., Gehr, R.J., Harper, R.W., Rupp, T.D., Sheffield, S.A. and Robbins, D.L.4Proton radiography of a thermal explosion in PBX9501Smith, R.W. and Srolovitz, D.J.RComputer simulation of impact induced fracture and fragmentation in brittle solids/Smugeresky, J.E., McCabe, T.J. and Graham, R.A.gEffect of powder particle size and shape on the microstructure of explosively compacted stainless steel#Soga, S., Kondo, K. and Sawaoka, A.2Shock compaction of TiN/TiC solid solution powdersSSokolov, S.N., Milyavskiy, V.V., Khishchenko, K.V., Borodina, T.I. and Fortov, V.E.DPhase transitions of C70 fullerite under step-like shock compression7Solie, D.J., Johnson, J.B., Dutta, P.K. and Kalafut, J.TEffects of temperature on an ISL-PVDF shock sensor between +20 deg. C and -40 deg. C891-892,Solie, D.J., Johnson, J.B. and Barrett, S.A.5The response of natural snow to explosive shock waves�Sollier, A., Auroux, E., Vauthier, J.-S., Boustie, M., He, H., de�  Ress"�guier, T., Berterretche, P., Desbiens, N., Bourasseau, E. and Maillet, J.-B.^A new experimental design for laser-driven shocks on precompressed and preheated water samples	1192-1195Solv"�, G. and Cagnoux, J.7The behavior of pyrex glass against a shaped-charge jetBSomayazulu, M.S., Ramachandran, H.S., Sharma, S.M. and Sikka, S.K.IPhase transition in potassium titanyl phosphate (KTP) under high pressure.Somayazulu, M.S., Sharma, S.M. and Sikka, S.K.LMolecular dynamical calculations of a-quartz: Implications for shock results%Son, S.F., Asay, B.W. and Bdzil, J.B.?Inert plug formation in the DDT of granular energetic materials	Son, S.F.The combustion of explosives	1059-1064Son, S.F. and Berghout, H.L.(Flame spread across surfaces of PBX 9501	1014-1017Song, I. and Thadhani, N.N.HEffects of shock processing parameters on synthesis of nickel aluminidesSong, S. and Gray�  III, G.T./Omega phase formation in shock-loaded zirconiumRSkidmore, C.B., Phillips, D.S., Asay, B.W., Idar, D.J., Howe, P.M. and Bolme, D.S.;Microstructural effects in PBX 9501 damaged by shear impact\Skokov, V.I., Ignatova, O.N., Malyshev, A.N., Podurets, A.M., Raevsky, V.A. and Zocher, M.A./Temporal softening and its effect upon strength2Skripnyak, V.A., Skripnyak, E.G. and Zhukova, Y.V.QComputer simulation of the propagation of short shock pulses in ceramic materials2Skripnyak, E.G., Skripnyak, V.A. and Nazarov, M.N.ZMechanical behaviour of nanostructured materials at high strain rates: Computer simulationRSkripnyak, V.A., Skripnyak, E.G., Garkushin, G.V., Kolobov, Y.R. and 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 K658-661Skryl, Y. and Kuklja, M.M.ANumerical simulation of the vacancy diffusion in shocked crystalsKNumerical simulation of diffusion of electrons and holes in shocked silicon'Skryl, Y., Belak, A.A. and Kuklja, M.M.INumerical simulation of shock induced polarization in binary electrolytesSlough, W.J. and Perger, W.F.dCalculation of RDX molecular crystal geometry and vibrational frequencies under hydrostatic pressureKSmilowitz, L.B., Henson, B.F., Asay, B.W., Dickson, P.M. and Robinson, J.M.0Kinetics of the b-d phase transition in PBX 9501cSmilowitz, L., Henson, B.F., Asay, B.W., Dickson, P.M., Oschwald, D.M., Romero, J.J. and Parker, G.:Morphology changes during thermal decomposition of PBX9501fSmilowitz, L., Henson, B.F., Sandstrom, M.M., Asay, B.W., Oschwald, D.M., Romero, J.J. and Novak, A.M.DFast internal temperature measurements in PBX9501 thermal explosions�Smilowitz, L., Henson, B.F., Romero, J.J., Sandstrom, M.M., Asay, B.W., Schwartz, C., Saunders, A., Merrill, F., Morris, C., Murray, M.M., McNeil, W.V., Marr-Lyon, M. and Rightley, P.M.#Silvestrov, V.V. and Gorshkov, N.N.IEffect of strain rate on the tensile strength of copper shaped charge jetqSimakov, V.G., Borisenok, V.A., Bragunets, V.A., Volgiin, V.A., Zhernokletov, M.V., Zocher, M.A. and Cherne, F.J.2Study of phase transitions in cerium by PVDF gaugeSimha, C.H.M. and Bless, S.J.CCarbon piezoresistive gauges in one-dimensional stress measurements	1037-1039*Simha, C.H.M., Bless, S.J. and Bedford, A.,Modelling precursor decay in AD-99.5 alumina/What is the peak stress in ceramic bar impacts?Simonenko, V.A.<  BShock compression of condensed matter up to gigabar pressure range41-47*Simonsen, I.K., Horie, Y. and Graham, R.A.$Shock synthesis of nickel aluminides743-748,Simpson, R.L., Urtiew, P.A. and Tarver, C.M.2Shock initiation of 1,3,3-trinitroazetidine (TNAZ)Singh, A.K.lThe effect of stress anisotropy on the lattice strains measured with an X-ray difraction opposed anvil setup	1629-1632eSinitsyna, L.M., Novikov, S.A., Gray�  III, G.T., Cerreta, E., Henrie, B., Lopez, M. and Yablinsky, C.JSubstructure evolution in energetic-driven spherically shock-loaded copper(Sitaud, B., P"�r"�, J. and Th"�venin, T.3Melting curve determination for cerium up to 30 GPa\Siviour, C.R., Williamson, D.M., Grantham, S.G., Palmer, S.J.P., Proud, W.G. and Field, J.E.(Split Hopkinson bar measurements of PBXs804-807Siviour, C.R. and Proud, W.G.=Measurements of strain propagation in Hopkinson bar specimens?Damage formation during high strain rate deformation of PBS9501�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. and Liebenberg, D.H..Effects of pressure on high Tc superconductors8Skidmore, C.B., Phillips, D.S., Son, S.F. and Asay, B.W.-Characterization of HMX particles in PBX 9501ZShkuratov, S.I., Talantsev, E.F., Baird, J., Temkin, H., Altgilbers, L.L. and Stults, A.H.�Longitudinal shock wave depolarization of Pb(Zr52Ti48)O3 polycrystalline ferroelectrics and their utilization in explosove pulsed powerrShon, J.W., Ree, F.H., Viecelli, J.A., van�  Thiel, M., Young, D.A., Schmidt, R.D., Hrubesh, L.H. and Vantine, H.C.BHugoniots of aerogels involving carbon and resorcinal formaldehyde>Shor, A., Zaretsky, E., Ohtera, K., Sasoh, A. and Takayama, K.6Dynamic mechanical properties of aluminum alloys GIGASTShotnikova, M.A., Strokina, T.I., Krylov, N.A., Mescheryakov, Y.I. and Divakov, A.K.9Formation of rotation in titanium alloys at shock loadingShpatakovskaya, G.V.NGeneralized statistical model: Scott correction at any temperature and density Shrader, J.E. and Bjorkman, M.D.EHigh temperature phase transformation on the titanium alloy Ti-6Al-4V310-314	Shuda, Z.6The surface impurity distribution on synthetic diamond<Shunin, V.M., Nabatov, S.S., Yakushev, V.V. and Volkov, A.P.SHigh-speed spherical solid registration by the use of piezoelectric composite filmsCSignor, L., de�  Ress"�guier, T., Roy, G., Dragon, A. and Llorca, F.sFragment-size prediction during dynamic fragmentation of shock-melted tin: Recovery experiments and modeling issuesSikka, S.K.BShock Hugoniot equation of state  �� electron band theory approach71-84-Sikka, S.K., Sharma, S.M. and Chidambaram, R.RSteric constraints: A powerful criterion to predict the onset of phase transitionsSikka, S.K. and Gupta, S.C.(Shock induced amorphization of materials145-150'Silvera, I.F., Chen, N. and Moshary, F.JOrientational order in the solid hydrogens: The boomerang phase line in HDISilvestri, M.R., Schroeder, J., Persans, P.D., Hwang, L.W. and Zhao, X.S.DOptical high pressure studies of ternary semiconducting nanocrystals,Sheffield, S.A., Davis, L.L. and Engelke, R.UDetonation properties of nitromethane, deuterated nitromethane, and bromonitromethane+Weir, S.T., Nellis, W.J. and Mitchell, A.C.@Electrical conductivity of hydrogen shocked to megabar pressures881-883
Weirick, L.J.GShock characterization of epoxy - 42 volume percent glass microballoonsWeirick, L.J. and Navarro, M.J.#Shock characterization of TOAD pinsUWerdiger, M., Eliezer, S., Moshe, e., Henis, Z., Dekel, E., Horovitz, Y. and Arad, B.8Al and Cu dynamic strength at a strain rate of 5.108 s-1
Wescott, B.L.?Generalized pseudo-reaction zone model for non-ideal explosivesWester, M. and Prentice, J.K.GThe development of a multiple mesh capability for an Eulerian hydrocodeMWhite, C.T., Barrett, J.J.C., Mintmire, J.W., Elert, M.L. and Robertson, D.H.TMolecular dynamics study of chemistry from strong shock waves interacting with voids(White, A., Zerilli, F.J. and Jones, H.D.?An ab initio method for estimating equation of state parameters;White, C.T., Robertson, D.H., Swanson, D.R. and Elert, M.L.@Critical widths in molecular dynamics simulations of detonationsWhite, S.J.\Direct comparison of a range of strain-rate dependent strength models on Taylor impact tests.Whiteman, G., Millett, J.C.F. and Bourne, N.K.[Longitudinal and lateral stress measurements in stainless steel 304L under 1D shock loading
Whitley, V.H.&Optical absorption measurements of RDX(Whitlock, R.R., Wark, J.S. and Kiehn, G.6Streaked X-ray diffraction from laser-shocked crystalsWhitlock, R.R. and Wark, J.S.HPlasticity in shocked single crystals viewed by pulsed x-ray diffractionWhitworth, N.J. and Maw, J.R.;Modelling shock desensitisation of heterogeneous explosivesAModelling 'hot-spot' initiation in heterogeneous solid explosivesWhitworth, N.J.�Wark, J., Higginbotham, A., Kimminau, G., Murphy, W., Nagler, B., Whitcher, T., Hawreliak, J., Kalantar, D., Butterfield, M., El-Dasher, B., McNaney, J., Milathianaki, D., Lorenzana, H., Remington, B., Davies, H., Thornton, L., Park, N. and Lukezic, S.XA geometry for sub-nanosecond X-ray diffraction from laser-shocked polycrystalline foilsWarnes, R.H. and Tonks, D.L.LMeasurement and analysis of 3 GPa shock wave profiles in annealed OFE copperGMeasurement and analysis of three 1.5 GPa shock-wave profiles in copper+Warnes, R.H., Paisley, D.L. and Tonks, D.L.7Hugoniot and spall data from the laser-driven miniflyer,Warren, A.D., Lawrence, G.W. and Jouet, R.J.RInvestigation of formulations containing perfluoro-coated oxide-free nano-aluminumWashabaugh, P.D. and Hill, L.G.wInvestigation of the sub-microsecond features of dynamic crack propagation in PMMA and the RDX-based explosive PBX 9205HWebb, A.W., Qadri, S.B., Skelton, E.F., Moulton, N.E. and Vanderah, T.A."Compressibility of Ti2Ba2CaCu2O8+d;Webb, A.W., Osofsky, M.S., Skelton, E.F. and Vanderah, T.A.`Pressure dependence of resistivity for normal-state '123'-superconducting copper oxide compoundsWeerasooriya, T.:Modeling flow behavior of 93W-5Ni-2Fe tungsten heavy alloy?Modeling flow behavior of 93W-5Ni-2Fe due to sudden rate changegModeling compressive flow behavior of a tungsten heavy alloy at different strain rates and temperatures Wei, D., Zhang, F. and Woo, T.K.PAb initio molecular dynamics simulations of molecular collisions of nitromethane3Weidner, D.J., Wang, Y., Meng, Y. and Vaughan, M.T.?Deviatoric stress measurements at high pressure and temperature\Weinstein, B.A., Ritter, T.M., Stair, K., Choi-Feng, C., Devane, G., Kim, H.M. and Wie, C.R.bStrain relaxation in highly mismatched heterostructures under high-pressure/temperature conditions[Improved analytical model for the piezoresistive response of lateral manganin stress gaugesWang, W. and Tang, Z.8A study on the propagation of macroscopic phase boundaryWang, W. and Tang, Z.P.5A one-dimensional phase transition constitutive model%Wang, Y., Ahuja, R. and Johansson, B.KCalculated Hugoniot curves of porous metals: Copper, nickel, and molybdenum*Wang, W., Tang, Z., Gong, P. and Horie, Y.'Discrete element method modeling of gas Wang, W., Tang, Z. and Horie, Y.QDiscrete element method simulation of nonlinear viscoelastic stress wave problems371-373+Wang, S., Yang, Y., Sun, Z. and Dlott, D.D.qShock-induced chemical reaction propagation in nanoenergetic materials observed with nanometer spatial resolution;Wang, G., Sun, C., Liu, C., Zhao, J., Tan, F. and Zhang, N.Sharma, S.M. and Gupta, Y.M.SRelating the ruby R-line spectra to deformation under shock amd h<  ydrostatic loading887-892
Sharma, J.MChemistry of energetic materials under shock caused by electronic excitations639-645Sharma, J. and Coffey, C.S.RNature of ignition sites and hot spots studied by using an atomic force microscopedSharma, J., Hoover, S.M., Coffey, C.S., Tompa, A.S., Sandusky, H.W., Armstrong, R.W. and Elban, W.L.AStructure of crystal defects in damaged RDX as revealed by an AFMMSharma, J., Coffey, C.S., Armstrong, R.W., Elban, W.L. and Lanzerotti, M.Y.D.pNanostructure of porosity (and entrapped solvent effects) in laboratory-grown crystals of RDX as revealed by AFMGSharma, J., Coffey, C.S., Armstrong, R.W., Elban, W.L. and Hoover, S.M.�Sub-molecular fracture steps in shock-shattered RDX crystals and follow-on nano-indentation evaluation of early state plasticityShaw, M.S. and Johnson, J.D.<A slow reaction rate in detonations due to carbon clustering
Shaw, M.S.QSelim, F.A., Wells, D.P., Harmon, J.F., Kwofie, J., Lancaster, G. and Jones, J.L.^Measurements of dynamic structural changes in laser-shocked materials by positron annihilationQSenf, H., Hornemann, U., Rothenh"�usler, H., Scharpf, F., Poth, A. and Pfrang, W.ZExperimental and numerical investigations concerning the dynamics of penetration processes539-543Seo, M.S. and Ryu, J.KExplosively driven ferroelectric generator for compact pulsed power systems	1313-1316Setchell, R.E.)Sandia 25 meter compressed helium/air gunSetchell, R.E. and Taylor, P.A.GDynamic and static compressibility of porous granular hexanitrostilbene871-876AVisible emission from granular explosives during shock initiation/Response of PVDF gauges to structured waveformsRSetchell, R.E., Chhabildas, L.C., Furnish, M.D., Montgomery, S.T. and Holman, G.T.PDynamic electromechanical characterization of the ferroelectric ceramic PZT 95/5DSetchell, R.E., Montgomery, S.T., Chhabildas, L.C. and Furnish, M.D.cThe effects of shock stress and field strength on shock-induced depoling of normally poled PZT 95/5MRecent progress in understanding the shock response of ferroelectric ceramics191-196=Setchell, R.E., Tuttle, B.A., Voigt, J.A. and Venturini, E.L.LEffects of initial porosity in the shock response of normally poled PZT 95/5,Setchell, R.E., Tuttle, B.A. and Voigt, J.A.9Microstructural effects on the shock repsonse of PZT 95/5180-183>Setchell, R.E., Montgomery, S.T., Cox, D.E. and Anderson, M.U.UDielectric properties of PZT 95/5 during shock compression under high electric fields278-281]Initial temperature effects on the dielectric properties of PZT 95/5 during shock compressionSewell, T.D.JMonte Carlo calculations of the physical properties of RDX, b-HMX and TATB6Sewell, T.D., Bedrov, D., Menikoff, R. and Smith, G.D.BLoad cycling and pressure efficiency in a large volume cubic press	1593-15968High pressure DSC signal amplification using thermopiles	1691-1694 Segletes, S.B. and Walters, W.P.$Comments on the Gr"�neisen parameterSegletes, S.B.*Vibrational stiffness of an atomic latticeXSeifter, A., Stewart, S.T., Furlanetto, M.R., Kennedy, G.B., Payton, J.R. and Obst, A.W./Post-shock temperature measurements of aluminumSeitz, W.L.'Short-duration shock initiation of TATB&Sekine, T., Akaishi, M. and Setaka, N.AShock-induced oxidation-reduction reaction in the system Fe-Fe2O3
Sekine, T.%Shock transformation in boron nitrideSekine, T. and Ahrens, T.J.)Equation of state of heated glassy carbonQSekine, T., Maruyama, Y., Nagata, M., Mizutani, N., Kitagawa, H. and Inoguchi, H.0Shock-induced phase transformation of fullerites8Sekine, T., Tashiro, S., Kobayashi, T. and Matsumura, T.;The NIRIM two-stage light gas gun: Performance test resultsSekine, T. and Kobayashi, T.[Shock-induced phase transition of 6H polytype SiC and an implication for post-diamond phasePShock-induced process during compression of graphite perpendicular to the c-axis6Shock-induced cubic silicon nitride and its properties	1113-11182Walker, J.D., Anderson�  Jr., C.E. and Lankford, J.MNumerical simulations of split Hopkinson pressure bar compression experiments$Walker, J.D. and Anderson�  Jr., C.E.CThe influence of projectile nose shape on the shock phase of impactGVildanov, V.G., Gorshkov, M.M., Slobodenjukov, V.M. and Rushkovan, E.H.JShock compression of low initial density quartz at pressures up to 100 GPaVisscher, P.B. and Holian, B.L.^Vibrational relaxation rates in molecular fluids via equilibrium simulation: Thermal softening5Vitello, P., Fried, L.E., Pudliner, B. and McAbee, T.FSparse partial equilibrium tables in chemically resolved reactive flowVitello, P. and Souers, P.C.-The piecewise linear reactive flow rate model6Vitello, P., Garza, R., Hernandez, A. and Souers, P.C.The energy diameter effect877-880�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. and Buttler, W.T.XA new spin on an old technology: Piezoelectric ejecta diagnostics for shock environmentsVogler, T.J. and Asay, J.R.MA distributional model for elastic-plastic behavior of shock-loaded materialsVogler, T.J. and Borg, J.P.XMesoscale and continuum calculations of wave profiles for shock-loaded granular ceramics6Vohra, Y.K., McCauley, T.S., Gu, G. and Vagarali, S.S.7Isotopically pure 12C diamond anvil at megabar pressureVoltz, C. and Roy, G.[Study of spalling for high purity iron below and aobe shock induced a to e phase transitionVoltz, C., Buy, F. and Roy, G.WIron damage and spalling behavior below and above shock induced a to e phase transition678-683von�  Holle, W.G.^Temperature measurements of shocked translucent materials by time-resolved infrared radiometry287-291]Shock wave diagnostics by time-resolved infrared radiometry and non-linear Raman spectroscopy283-291)Vong, T.S., Leyrat, J.P. and Pujols, H.C.EImpact effects of a two-parts high velocity jet on homogeneous target9Vorobiev, O.Y., Antoun, T.H., Lomov, I.N. and Glenn, L.A.:A strength and damage model for rock under dynamic loading0Spall strength of ceramic in a multilayer system8Vecchio, K.S., Andrade, U., Meyers, M.A. and Meyer, L.W.FMicrostructural evolution in high strain, high strain-rate deformation!Vecchio, K.S. and Gray�  III, G.T.DEffects of shock loading on a solid-solution strengthened superalloy
Vecchio, K.S.AElectron microscopy of shock synthesized silicides and aluminides0Vedantam, K., Bajaj, D., Brar, N.S. and Hill, S.7Johnson-Cook strength models for mild and DP 590 steels\Veeser, L.R., Gray�  III, G.T., Vorthman, J.E., Rodriguez, P.J., Hixson, R.S. and Hayes, D.B.,High pressure response of a high-purity ironJVenkateswaran, U.D., Mak, C.-L., Bak, J., Sooryakumar, R. and Jonker, B.T.CPressure-induced enhancement of exchange interactions in Zn1-xCoxSe>Venkateswaran, C., Jeyabalan, K., Jaya, N.V. and Natarajan, S.AHigh pressure studies of Y0.8Ba2.2Cu3O6+y and Y0.8Sr0.2Ba2Cu3O6+y685-686-Venturini, E.L., Morosin, B. and Graham, R.A.)Paramagnetic defects in shock-loaded TiO277-81IMagnetic properties of shock-synthesised and furnace-reacted zinc ferrite815-820-Venturini, E.L., Graham, R.A. and Morosin, B.BStatic magnetization and microwave loss in shock-modified ferrites;Venturini, E.L., Graham, R.A., Ginley, D.S. and Morosin, B.VEffects of shock modification on superconductivity in Tl2Ca2Ba2Cu3Oy and Bi2CaSr2Cu2Ox;Vidal, P., Cowperthwaite, M., Presles, H.-N. and Bouton, E.cA study of the curvature of a two-dimensional detonation wave at an explosive-confinement interfaceJVignjevic, R., Millett, J.C.F., Bourne, N.K., Meziere, Y. and Lukyanov, A.CThe behaviour of a carbon-fibre epoxy composite under shock loadingGVignjevic<  , R., Campbell, J.C., Bourne, N., Matic, O. and Djordjevic, N.,Modelling shock waves in composite materials9Vignkevic, R., Bourne, N.K., Hughes, K. and Stojkovic, M.)Simulation of a shock recovery experiment'van�  Thiel, M., Ree, F.H. and Sayer, J.eEquilibrium shock and release properties of post deformation mixtures of PBX-9404 LX-14, RDX, and TNT883-889(van�  Thiel, M., Ree, F.H. and Grover, R.1Three phase carbon EOS with electronic excitationvan�  Thiel, M.aThermodynamic properties and hydrodynamic response of high-density high-temperature CHNO mixtures79-86van�  Thiel, M. and Ree, F.H.JLindemann melting law for anisentropic crystals: Graphite to liquid carbon+Unlike pair interactions in N2-H2O mixtures#Vandersall, K.S. and Thadhani, N.N.7Shock compression synthesis of B1-type tantalum nitrideRDynamic densification of Mo-Si powder compacts for reactive solid state processingVShock compression of Mo-Si powder mixtures using recovery and instrumented experimentsIVandersall, K.S., Forbes, J.W., Tarver, C.M., Urtiew, P.A. and Garcia, F.FRe-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 gaugesjVandersall, K.S., Murty, S.S., Chidester, S.K., Forbes, J.W., Garcia, F., Greenwood, D.W. and Tarver, C.M.rInvestigation of Steven impact test using a transportation hook projectile with gauged experiments and 3D modeling;Vandersall, K.S., Tarver, C.M., Garcia, F. and Urtiew, P.A.\Shock initiation experiments on PBX9501 explosive at 150��C for ignition and growth modelingLVandersall, K.S., Tarver, C.M., Garcia, F., Urtiew, P.A. and Chidester, S.K.jShock initiation experiments on hte HMX based explosive LX-10 with associated ignition and growth modeling*Vantine, H.C., Chan, J. and Erickson, L.M.!Thin pulse initiation of PBX-9404558-562,Vassiliou, J.K., Otto, J.W. and Porter, R.F.+The equation of state of d-TaN0.8 to 72 GPa:Vaughan, B.A.M., Murray, N.H., Proud, W.G. and Field, J.E.=Utkin, A.V., Kolesnikov, S.A., Pershin, S.V. and Fortov, V.E.jReaction zone transformation for steady-state detonation of high explosives under initial density increase938-9419Utkin, A.V., Sosikov, V.A., Bogach, A.A. and Fortov, V.E.!Tension of liquids by shock waves+Utkin, A.V., Sosikov, V.A. and Fortov, V.E.6Tension of ethyl alcohol and hexadecane by shock waves896-8994Utsumi, W., Yamakata, M., Yagi, T. and Shimomura, O.�In situ X-ray diffraction study of the phase transition from graphite to hexagonal diamond under high pressures and high temperaturesVaidya, R.U. and Zurek, A.K.?Dynamic mechanical deformation of a SiCp/Al-Li (8090) composite9Vaidya, R.U., Song, S.G., Zurek, A.K. and 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 interfacesGParticle-velocity dependent rate constants from transition-state theoryValone, S.M. and Kapila, V.JNonequilibrium atomistic polymer simulations under shear and shock loading$Valyanskaya, T.V. and Stepanov, G.N.KSuperconductivity at 12 K in silicon under low temperature pressure release$Van�  Camp, P.E. and Van�  Doren, V.E.1Theoretical high pressure study of boronphosphidesvan�  der�  Heijden, A.E.D.M., Bouma, R.H.B., Carton, E.P., Pacheco, M.M., Meuken, B., Webb, R. and Zevenbergen, J.F.nProcessing, application and characterization of (ultra)fine and nanometric materials in energetic compositions	1121-1126ivan�  Duin, A.C.T., Zybin, S.V., Chenoweth, K., Zhang, L., Han, S.-P., Strachan, A. and Goddard�  III, W.A.dReactive force fields based on quantum mechanics for applications to materials at extreme conditions(van�  Hinsberg, M.G.E. and Schouten, J.A./The phase diagram of nitrogen clathrate hydrate=Urakawa, S., Ohno, H., Igawa, N., Kondo, T. and Shimomura, O.>Synchrotron radiation study on the phase relations of KAlSi3O8/Urlin, V.D., Mochalov, M.A. and Mikhailov, O.L.FQuasi-isentropic compression of liquid argon at pressure up to 500 GPa55-560Urlin, V.D., Mochalov, M.A. and Mikhailova, O.L.hQuasi-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. and Simpson, R.L.2Shock initiation of 2,4-dinitroimidazole (2,4-DNI)7Urtiew, P.A., Tarver, C.M., Forbes, J.W. and Garcia, F.3Shock sensitivity of LX-04 at elevated temperatures7Urtiew, P.A., Forbes, J.W., Tarver, C.M. and Garcia, F.2Calibration of manganin pressure gauges at 250 ��C7Urtiew, P.A., Forbes, J.W., Garcia, F. and Tarver, C.M.%Shock initiation of UF-TATB at 250��CxUrtiew, P.A., Forbes, J.W., Tarver, C.M., Vandersall, K.S., Garcia, F., Greenwood, D.W., Hsu, P.C. and Maienschein, J.L.NShock sensitivity of LX-04 containing delta-phase HMX at elevated temperaturesIUrtiew, P.A., Forbes, J.W., Tarver, C.M., Vandersall, K.S. and Garcia, F.#Dynamic loading of Teflon at 200��C$Usuba, S., Kondo, K. and Sawaoka, A.lStatus of electromagnetic mass-accelerator development and prospect of application to high-pressure researchKUtkin, A.V., Kanel, G.I., Baumung, K., Karow, H.U., Rusch, D. and Licht, V.5Ion beam diagnostics by methods of shock-wave physics	1891-1894(Utkin, A.V., Kanel, G.I. and Baumung, K.CExperimental observations of state of matter heated by the ion beamGUtkin, A.V., Kanel, G.I., Razorenov, S.V., Bogach, A.A. and Grady, D.E.PElastic moduli and dynamic yield strength of metals near the melting temperature:Utkin, A.V., Kanel, G.I., Bogach, A.A. and Razorenov, S.V.[Macrokinetics of the energy release in high explosives containing nano-size boron particles9The shock Hugoniot properties of cement paste up to 5 GPa*Tsembelis, K., Proud, W.G. and Field, J.E.OThe principal Hugoniot and dynamic strength of dolerite under shock compression<The dynamic strength of cement paste under shock compression	1414-1417<Tsembelis, K., Proud, W.G., Willmott, G.R. and Cross, D.L.A.EThe shock Hugoniot properties of cement paste and mortar up to 18 GPaTsembelis, K. and Proud, W.G.&The dynamic behavior of micro-concrete	1496-14994Tsembelis, K., Ramsden, B., Proud, W.G. and Borg, J._CAV_KO: A simple 1D Lagrangian hydrocide for MS Excel with automatic generation of x-t diagrams,Tsou, P., Griffiths, D.J. and Buettner, D.J.HStructural influence on hypervelocity intact capture in underdense media4Tsuji, K., Yamamoto, Y., Katayama, Y. and Koyama, N.CAmorphization from quenched high-pressure phase in III-IV compounds(Tsukahara, Y., Matsuo, A. and Tanaka, K.\Numerical simulation of high velocity impact phenomenon by the distinct element method (DEM)	1309-1312/Tsukinovsky, D., Zaretsky, E. and Rutkevich, I.APolyurethane in plane impact with velocities from 10 to 400 m/secTunison, K.S. and Gupta, Y.M.LElastic precursor decay in shocked pure LiF crystals: Role of surface damage+Tyler, C., Millett, J.C.F. and Bourne, N.K.7Spallation in Ti6Al4V: Stress measurements and recovery674-677-Tyler, C.E., Bourne, N.K. and Millett, J.C.F.LStrength of polyethylene, polypropylene and polystyrene behind a shock frontUchino, M. and Mashimo, T.%Hugoniot measurements of zinc sulfide975-976BUeno, M., Yoshida, M., Onodera, A., Shimomura, O. and Takemura, K.IEquation of state and pressure-induced phase transition of III-V nitrides'Ulivi, L., Barocchi, F. and Pratesi, G.CBrillouin scattering from fluid and solid hydrogen at high pressuresInvestigation of <  microscale shock phenomena using a line-imaging optically recording velocity interferometer system;Trott, W.M., Knudson, M.D., Chhabildas, L.C. and Asay, J.R.�Measurements of spatially resolved velocity variations in shock compressed heterogeneous materials using a line-imaging velocity interferometer993-9985Trott, W.M., Setchell, R.E. and Farnsworth�  Jr., A.V.wInvestigation of the effects of target material strength on the efficiency of acceleration of thick laser-driven flyers>Trott, W.M., Chhabildas, L.C., Baer, M.R. and Caste"�eda, J.N.iInvestigation of dispersive waves in low-density sugar and HMX using line-imaging velocity interferometrybDevelopment of laser-driven flyer techniques for equation of state studies of microscale materialsTrucano, T.G. and Grady, D.E.MIntermediate velocity penetration of steel spheres into deep aluminum targets8Trucano, T.G., Barker, L.M., Asay, J.R. and Kerley, G.I.ONumerical studies of the dynamic isentropic loading of solid molecular hydrogen461-465.Trucano, T.G., Asay, J.R. and Chhabildas, L.C.<Hydrocode benchmarking of 1-D shock vaporization experiments"Trucano, T.G. and Chhabildas, L.C.:Calculations supporting hypervelocity launcher development	1639-1642Trunin, R.F. and Simakov, G.V.<The peculiarities of porous metal compression in shock wavesTTrunin, R.F., Zhernokletov, M.V., Simakov, G.V., Gudarenko, L.F. and Gushchina, O.N.^Shock compression of highly porous samples of copper, iron, nickel and their equation of stateTsai, D.H. and Trevino, S.F.pModel simulation of chemical reaction in a diatomic crystal. 1: Energy exchange in rapid exothermic dissociationTse, J.S. and Klug, D.D.LMolecular dynamics studies of high pressure phase transitions and structures;Tsembelis, K., Millett, J.C.F., Proud, W.G. and Field, J.E.pTonks, D.L., Paisley, D.L., Peralta, P.D., Greenfield, S.R., Byler, D.D., Luo, S., Swift, D.C. and Koskelo, A.C.0Spallation damage in copper with columnar grainsJTowler, M.D., Hines, R.I., Allan, N.L., Braithwaite, M. and Mackrodt, W.C.OEquations of state for polar solids at high pressures and elevated temperaturesTownsend, D. and Bourne, N.K.0Measurements of the conductivity of shocked PMMA	1267-1270.Trainor, R.J., Holmes, N.C. and Anderson, R.A.6Ultrahigh pressure laser-driven shock wave experiments145-154=Traiviratana, S., Bringa, E.M., Benson, D.J. and Meyers, M.A.FVoid growth in single and bicrystalline metals: Atomistic calculations)Tran, P.X., Brenner, D.W. and White, C.T.BNonlinear dynamics of chains interacting with a steady shock frontTranchet, J.Y. and Cagnoux, J.dA model of plasticity with strain-hardening for shock-wave behavior of non porous and porous aluminaITrebinski, R., Wlodarczyk, E., Cudzilo, S., Paszula, J. and Trzcinski, W.3Investigations into the detonative synthesis of bBNTrevino, S.F. and Tsai, D.H.aModel simulation of chemical reaction in a diatomic crystal. 2: Kinetics of equilibrium chemistryyTringe, J.W., Molitoris, J.D., Garza, R.G., Andreski, H.G., Batteux, J.D., Lauderbach, L.M., Vincent, E.R. and Wong, B.M.6Detailed comparison of blast effects in air and vacuum	1305-1308Trott, W.M. and Meeks, K.D.DAcceleration of thin foil targets using fiber-coupled optical pulsesTrott, W.M.GStudies 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. and Ebersole, H.N./Hugoniot equation of state of liquid propellantVHigh-speed optical studies of the driving plasma in laser acceleration of flyer platesTrott, W.M. and Asay, J.R.6Aerogel algorithm for shrapnel penetration experiments5Tollier, L., Cottet, F., Boustie, M. and Ansart, J.P.WExperimental and numerical studies of Ti-6Al-4V spallation by laser and impact loadings)Tollier, L., Bartnicki, E. and Fabbro, R.QExperimental and numerical study of laser-driven spallation with VISAR diagnosticTomar, V. and Zhou, M.9Molecular dynamics simulation of shock induced detonation]Molecular dynamics modeling of shock wave propagation in fcc-Al, a-Fe2O3 and their interfacesBTong, X., Xu, D.-P., Su, W.-H., Xiao, L.-Z., Li, S.-T. and Han, L.mStudy on surface photovoltage spectra of CdS nanocrystalline materials synthesized under high static pressureTonks, D.L.HConstitutive relation for 6061T6 aluminum under shock loading conditions347-351WRelation between shock strength and strain-rate plasticity at maximum deviatoric stressElseiverTonks, D.L. and Johnson, J.N.AShock wave evolution of the mechanical threshold stress in copper8Reverse plasticity effects in free-surface wave profiles<Tonks, D.L., Hixson, R.S., Johnson, J.N. and Gray�  III, G.T.WDislocation drag contribution to high-rate plastic deformation in shock-loaded tantalum5Shock wave plasticity in molybdenum at 293K and 1673KcTonks, D.L., Hixson, R., Gustavsen, R.L., Vorthman, J.E., Kelly, A., Zurek, A.K. and Thissell, W.R.*Spallation studies on shock loaded uraniumBTonks, D.L., Vorthman, J.E., Hixson, R., Kelly, A. and Zurek, A.K.2Spallation studies on shock-loaded U-6 wt. pct. Nb+Tonks, D.L., Zurek, A.K. and Thissell, W.R.)Void coalescence model for ductile damage.Tonks, D.L., Thissell, W.R. and Schwartz, D.S.PModeling incipient copper damage data from the tensile Hopkinson bar and gas gunJTonks, D.L., Henrie, B.L., Trujillo, C.P., Holtkamp, D. and Thissell, W.R.:Roughness of ductile damage paths in shock loaded tantalum670-673OThornhill, T.F., Reinhart, W.D., Chhabildas, L.C., Grady, D.E. and Wilson, L.T./Cylinder fragmentation using gas gun techniquesBThornhill, T.F., Vogler, T.J., Reinhart, W.D. and Chhabildas, L.C.CPolycrystalline aluminum oxynitride Hugoniot and optical properties2Thornhill, T.F., Chhabildas, L.C. and Vogler, T.J.(Tube fragmentation of multiple materials666-669Thyer, A.M. and W, Byers�  B.HQuantitative computer analysis of low velocity detonation in AN and ANFO,Tierney, T.E., Swift, D.C. and Johnson, R.P.LNovel techniques for laser-irradiation driven, dynamic materials experimentsSTierney, T.E., Swift, D.C., Luo, S.-N., Niemczura, J., Gammel, J.T. and Peralta, P.aQuasi-isentropic and shock compression measurements of iron response by direct laser illumination	1425-1428/Timofeev, B.B., Egorov, B.V. and Zvorykin, L.O.FHydrodynamic theory of shock induced anomalous mass transfer in solids.Titov, V.M., Anisichkin, V.F. and Malkov, I.Y.8Diamond synthesis from dynamically loaded organic matter6Todd, S.N., Vogler, T.J., Caipen, T.L. and Grady, D.E.SNon-shock initiation model for plastic bonded explosive PBXN-5: Theoretical results)Togaya, M., Sugiyama, S. and Mizuhara, E.Melting line of graphiteTokheim, R.E. and Lutze, A.B.@Characterization of thermomechanical response of porous vanadium246-250
Tokheim, R.E.QAnalysis of electrical noise from shock loading a steel flatpack soil stress gage559-564-Tokheim, R.E., Erlich, D.C. and Kobayashi, T.3Characterization of spall in Kevlar/Epoxy composite<Interpretation of quartz-gage response in radiation problems	1715-1718 Tokheim, R.E. and Williams, G.C.UComputed and observed experimental double pulse phenomena in aluminum PRS experimentsATokheim, R.E., Erlich, D.C., Curran, D.R., Tobin, M. and Eder, D.mExperimental quantitative damage measurements and void growth model predictions in the spallation of tantalumrThissell, W.R., Zurek, A.K., Macdougall, D.A.S., Miller, D., Everett, R., Geltmacher, A., Brooks, R. and Tonks, D.NThe effect of material cleanliness in dynamic damage evolution in 10100 copper7Thissell, W.R., Tonks, D.L., Schwartz, D. and House, J.[Dynamic failure resistance of two tantalum materials with different melt practice sequencesThissell, 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. and Zurek, A.K.WMetallurgical characterization of Atlas cylindrically convergent spallation experiments"Thoma, K., Klee, C. and Ludwig, D.@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. and Gunshor, R.L.tRaman and photo-modulated reflectivity studies of ZnTe/InAs semiconductor heterostructure under hydrostatic pressureThomas, J.N.RInfluence of plasticity models upon the outcome of simulated hypervelocity impacts	1785-1788MThomas, K.A., Martin, E.S., Kennedy, J.E., Garcia, I.A. and Foster�  Jr., J.C.<Transient detonation processes in a plastic bonded explosive!Thompson, W.E. and Predebon, W.W.XAn investigation of incipient fracture in shock-loaded lamellar cobalt-aluminum eutectic451-455Thompson, D.G. and Wright, W.J.2Mechanical properties from PBX 9501 pressing studyvThompson, D.G., Gustavsen, R.L., Hooks, D.E., Peterson, P.D., DeLuca, R., Stahl, D.B., Hagelberg, S.I. and Alcon, R.R.KA study of the shock sensitivity of PBX 9501 damaged by compressive loadingaTernovoi, V.Y., Filimonov, A.S., Fortov, V.E., Lomosonov, O.V., Nikolaev, D.N. and Pyalling, A.A.AInvestigation of tin thermodynamics in near critical point region^Ternovoi, V.Y., Filimonov, A.S., Fortov, V.E., Kvitov, S.V., Nikolaev, D.N. and Pyalling, A.A.JLiquid-vapor phase boundaries determination by dynamic experimental methodOTernovoi, V.Y., Filimonov, A.S., Pyalling, A.A., Mintsev, V.B. and Fortov, V.E.DThermophysical properties of helium under multiple shock compression2Ternovoi, V.Y., Pyalling, A.A. and 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^Ternovoi, V.Y., Kvitov, S.V., Nikolaev, D.N., Pyalling, A.A., Filimonov, A.S. and Fortov, V.E.UExperimental study of transition of Jupiter and Saturn atmosphere to conducting state	1492-1495Thadhani, N.N.;Shock induced chemical synthesis of intermetallic compounds503-510+Thadhani, N.N., Dunbar, E. and Graham, R.A.*Zwitter, D.E., Kuklja, M.M. and Kunz, A.B.TA computation of the frequency dependent dielectric function for energetic materials8Zybin, S.V., Elert, M.L., Harrison, J.A. and White, C.T.PAtomistic modeling of orientation dependence of shock wave properties in diamond(Zybin, S.V., Elert, M.L. and White, C.T.BMolecular dynamics study of non-reacting shock waves in anthracene306-309;Zybin, S.V., Zhakhovskii, V.V., Elert, M.L. and White, C.T.QMolecular dynamics studies of orientation dependence of shock structure in solids310-315MZybin, S.V., Zhakhovskii, V.V., Bringa, E.M., Abarzhi, S.I. and Remington, B.ZMolecular dynamics simulations of the Richtmyer-Meshkov instability in shock loaded solids437-441Abbott, R.D. and Bjorkman, M.D.7
mExperimental study of spalling strength and the hydro-elastic-viscoplastic constitutive equations with damage)Zhou, M., Clifton, R.J. and Needleman, A.CThe role of material inhomogeneities in the localization of strains/Zhou, X.M., Hu, J.B., Jing, F.Q. and Wang, J.G.USound velocity measurement for 4.2Ni2.45Fe0.35Co0.05MnW alloy under shock compression109-113-Zhou, G., Yun, S.R., Huang, F.L. and Ding, J.�Theoretical research on mechanisms by which carbon in explosives is synthesized into ultrafine diamond in detonation processes: 'Gaslike-liquid-solid-graphitization' modelZhou, M. and Zhai, J.LModelling of micromechanical fracture using a cohesive finite element method623-6280Zhou, J.K., Hsiung, L.L., Chau, R. and Saw, C.K.:An X-ray study of shock-recovered tantalum single crystalsZhu, J.S. and Fan, Z.M.PEffects of lateral expansion and artificial viscosity on steady detonation waves)Zhuang, S., Liu, C., Wang, C. and Sun, C.IDynamic fracture of iron under shock loading induced by pulsed laser beam	1903-1906,Zhuang, S., Ravichandran, G. and Grady, D.E.HInfluence of interface scattering on shock waves in heterogeneous solidsZhugin, Y.N.XThe behaviour of a-quartz under high dynamic and static pressures: New results and viewsZou, G., Meng, J. and Cui, Q.HStudy of the Raman spectra of Bi2Ti4O11 at high temperature and pressureJZucker, J.M., Barra, A.J., Zerkle, D.K., Kaneshige, M.J. and Dickson, P.M.<Thermal decomposition models for high explosive compositions Zurek, A.K. and Follansbee, P.S.7Microstructural effects on spall fracture in 1008 steelZurek, A.K. and Hunter, D.A.=Dynamic testing and characterization of pre-fractured ceramicfZurek, A.K., Embury, J.D., Kelly, A., Thissell, W.R., Gustavsen, R.L., Vorthman, J.E. and Hixson, R.S.CMicrostructure of depleted uranium under uniaxial strain conditionsrMolecular dynamics simulations of shock-induced chemical, mechanical, and thermal processes in Ni/Al nanolaminatesZheng, L. and Luo, S.-N.MSimulated structure modifications on silica subjected to UV-laser irradiation$Zhernokletov, M.V. and Simakov, G.I.JStudies of shock-compressed graphite behavior in reshock and release wavesVZhernokletov, M.V., Trunin, R.F., Gudarenko, L.F., Trushchin, V.D. and Gushchina, O.N.HDatabase on material properties studied in experiments using shock wavesbZhernokletov, M.V., Lebedeva, T.S., Medvedev, A.B., Mochalov, M.A., Shuykin, A.N. and Fortov, V.E.JThermodynamic 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. and Fortov, V.E.|Experimental measurement of compressibility and temperature in shock-compressed liquid xenon in pressure range up to 350 GPaaZhernokletov, M.V., Kovalev, A.E., Komissarov, V.V., Novikov, M.G., Zocher, M.A. and Cherne, F.J.TMeasurement of sound velocities and shear strength of cerium under shock compressionyZhernokletov, D.M., Milyavskiy, V.V., Khishchenko, K.V., Charakhchyan, A.A., Borodina, T.L., Valyano, G.E. and Zhuk, A.Z.CShock-wave loading of graphite in steel targets with conic cavities3Zhiembetov, A.K., Mikhaylov, A.L. and Smirnov, G.S.=Experimental study of explosive fragmentation of metals meltsPFragmentation properties of cerium and copper M1 on dynamic volumetric expansion694-697fZhmodik, S.M., Verkhovtseva, N.V., Nesterenko, V.F., Chikov, B.M., Airijant, E. and Nemirovskaya, N.A.:Shock induced gold redistribution in quartz-pyrite mixture$Zhou, G.-Q., Tang, Z.P. and Yang, G.RNumerical study of laser-induced two-dimensional shock waves in metallic materials%Zhou, G.-Q., Tang, Z.P. and Li, X.-Z.3Predicting of fragment number and size distribution6Zhang, H., Patanella, A., Espinosa, H.D. and Pae, K.D.*Tasker, D.G., Granholm, R.H. and Lee, R.J.mThe fast measurement of electrical conductivity structure within the detonation zone of a condensed explosiveTasker, D.G. and Baker, R.N.sA new, unbiased method for analyzing streak data, the calibration of the NSWC expanded large scale gap test (ELSGT)|X-ray study of the transitions among the rutile, a-PbO2 and baddeleyite phases of TiO2 at high pressure and high temperature4Tang, W.-H., Zhang, R.-Q., Jing, F.-Q. and Hu, J.-B.KRestudy on the thermal relaxation at interfaces following shock compression Tang, P.K. and Scannapieco, A.J.Modeling cylinder test'Tang, Z.P., Horie, Y. and Psakhie, S.G.TDiscrete 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. and Fritz, J.N.0Modeling PBX 9501 overdriven release experiments!Tang, Z.P., Liu, W. and Horie, Y.BNumerical investigation of pore collapse under dynamic compression2Tang, Z.P., Liu, W., Wang, W., Chen, L. and Hu, X.J3D discrete meso-element method and its application to spherical collisionTang, Z.P. and Wang,<   W.W.HDiscrete element modeling for shock processes of heterogeneous materials679-684Tang, Z. and Xu, J.]A combined DEM/FEM multiscale method and structure failure simulation under laser irradiation0Tang, Z., Tang, X., Zhang, X., Hu, H. and Xu, W.^Abnormal spall behavior observed in pure iron and FeMnNi alloy undergoing a-e phase transition662-665.Tang, T., Hu, H., Li, Q., Sun, X. and Wang, D.[Studies on the fracture of HR-2 steel and LY12 aluminum cylinders under explosive implodingTanguay, V. and Higgins, A.J.pComparison of critical conditions for initiation of porous PETN by shock waves transmitted from solids and gases(Taniguchi, T., Kondo, K. and Sawaoka, A.1Shock wave profiles in powder compacts of a Al2O3773-778,Tao, W.C., Tarver, C.M. and Breithaupt, D.R.FFundamental chemical interactions in metal filled composite explosives'Tappan, B.C., Son, S.F. and Moore, D.S.YNano-aluminum reaction with nitrogen in the burn front of oxygen-free energetic materials	1022-1025EDiscrete meso-element simulation of chemical reactions in shear bandsCTan, T.H., Fritz, J.N., Marsh, S.P., McQueen, R.G. and Steele, R.D.CCharacterization of simple explosively driven particle acceleration665-667Tan, T.-H. and Marsh, S.P.<Plasma production from shock compression of condensed matter)Tanaka, K., Fujiwara, S. and Kusakabe, M.*2-D simulations of shock recovery fixtures,Calculations of liquid plane-wave generatorsOTanaka, K., Fujiwara, S., Sellam, M., Presles, H.N., Brochet, C. and Cheret, R.5Calculations of overdriven detonation in nitromethaneTanaka, K. and Ookouchi, T.6Impact of dryice projectiles on elastic plastic bodies9High-speed impact of dry-ice projectiles onto thin plates	1853-1856dTanaka, K., Noda, K., Hyodo, Y., Nakamura, H., Kosaka, K., Nakayama, T., Katayama, M. and Takeba, A.:XDT in HTPB propellant from steel flyer plate impact tests
Tanaka, K.@Shock compression of solid with voids by gridless Lagrangian SPH%Tanaka, S., Hokamoto, K. and Itoh, S.PAnalysis of particle penetration into aluminum plate using underwater shock waveSNumerical studies on the explosive welding by smoothed particle hydrodynamics (SPH)	1301-1304Tang, Z.P. and Gupta, Y.M.(Shock response of CdS/BAMO:THF composite305-307)Tang, Z.P., Bellamy, P.M. and Gupta, Y.M.JStress dependence of the current ramping observed in shorted quartz gauges609-6105Tang, P.K., Seitz, W.L., Stacy, H.L. and 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 stateDTang, Z.P., Li, X.Z., Zhou, G.Q., Lin, S.B., Li, D.H. and Wang, W.Q.kExperimental investigation of shear stress effects on shock-induced phase transition in InSb single crystalTang, J. and Endo, S.GSyono, Y., Taguchi, H., Fukai, Y., Atou, T., Kusaba, K. and Fukuoka, K.FShock compression of VH0.50, NbH0.75, and TaH0.50: A comparative study4Syono, Y., Hikosaka, H., Kikuchi, M. and Fukuoka, K.>Shock-synthesis of a metastable tetragonal phase of EuBa2Cu3Oy"Dynamic friction of nano-materials3Zhang, F., Thibault, P.A., Link, R. and Gonor, A.L.WMomentum transfer during shock interaction with metal particles in condensed explosives934-937fZhang, Y., Mashimo, T., Fukuoka, K., Kikuchi, M., Sekine, T., Kobayashi, T., Chau, R. and Nellis, W.J.PHugoniot measurement of GGG (Gd3Ga5O12) in the pressure range up to over 100 GPa127-128Zhang, D.Z.:Shock dispersion in composite material with polymer binderZhang, D. and Feng, R.CPolycrystal modeling to determine the strengths of shocked ceramicsNZhang, L., Zybin, S.V., van�  Duin, A.C.T., Dasgupta, S. and Goddard�  III, W.A._Shock induced decomposition and sensitivity of energetic materials by ReaxFF molecular dynamicsRThermal decomposition of energetic materials by ReaxFF reactive molecular dynamics<Zhang, F.-P., Du, J.-M., Zhang, Y., Liu, Y.-S. and He, H.-L.ODischarge of PZT95/5 ferroelectric ceramics under tilted shock wave compression213-215)Zhang, F., Anderson, J. and Yoshinaka, A.;Post-detonation energy release from TNT-aluminum explosives885-888)Zhang, W., Jiang, C., Ma, W. and Fang, B.YNumerical simulations of fragmentation onset velocity of projectile impact on thin bumper:Zhao, S.D., Ling, Z., Shen, L.T., Chen, S.X. and Bai, Y.L.3An experimental approach to evolution of spallation#Zhao, F., Sun, C.-W. and Wei, T.-Z.CA developed unified criterion for the initiation of bare explosives	1361-13641Zhao, J., Winey, J.M., Gupta, Y.M. and Perger, W.NElastic properties of molecular crystals using density functional calculations3Zhao, J., Winey, J.M., Gupta, Y.M. and Perger, W.F.:First-principles studies of RDX crystals under compression(Zhao, S., Germann, T.C. and Strachan, A.�Dislocation mechanics based constitutive equation incorporating dynamic recovery and applied to thermomechanical shear instabilityXApplication of Eyring's thermal activation theory to constitutive equations for polymersBThermal activation constitutive model for polymers applied to PTFEZerilli, F.J. and Kuklja, M.M.4Ab initio 0K isotherm for organic molecular crystals0Equation of state of FOX-7 from first principles(Ab initio equation of state for beta-HMX)Zerwekh, W.D., Marsh, S.P. and Tan, T.-H.!Phase detonated shock tube (PFST)	1877-1880?Zha, C.-S., Hemley, R.J., Mao, H.-K., Duffy, T.S. and Meade, C.0Brillouin scattering of silica glass to 57.5 GPa?Zhakhovskii, V.V., Zybin, S.V., Abarzhi, S.I. and Nishihara, K.\Atomistic dynamics of the Richtmyer-Meshkov instability in cylindrical and planar geometriesZhang, K., Xi, J. and Gao, J.;Research on wave formation in multilayer explosive claddingEZhang, Y., Morosin, B., Graham, R.A., Hubbard, C.R. and Stewart, J.M.wShock induced solid state reaction and phase transition: X-ray profile studies on shock modified Fe3O4 and ZrO2 powders4Zhang, B.P., Zheng, Y.L., Peng, Q.Y. and Xiong, Y.M.ODynamic behavior of tungsten sintered alloys at high strain rates up to 105 s-15Zhang, B.-P., Xiong, Y.-M., Yang, C. and Jiang, C.-L.YThe influence of tungsten-atom transition on the mechanical properties of tungsten alloys(Zhang, S., Vohra, Y.K. and Brister, K.E.LSynchrotron X-ray and laser induced fluorescence in diamond at high pressure3Zhang, R.-Q., Kang, Q., Tang, W.-H. and Jing, F.-Q.%Equation of state (EOS) for 93W alloy105-107!Zhang, Z., Huan, S. and Lu, F.-Y.WLagrangian analysis method of flow field in detonation reaction zone of high explosivesZhang, J.-H. and Ding, J.CQuasitemperature distribution in shocked energetic molecular solidsZhang, L. and Jin, X./Dynamic response of pure titanium up to 1000��CeZaug, J.M., Farber, D.L., Craig, I.M., Blosch, L.L., Shuh, D.K., Hansen, D.W. and Aracne-Ruddle, C.M.WQuasi-dynamic pressure and temperature initiated b <-> d solid phase transitions in HMX#Zavattieri, P.D. and Espinosa, H.D.<Ballistic penetration of multi-layered ceramic/steel targets>Zeigler, F.J., McGlaun, J.M., Thompson, S.L. and Trucano, T.G.JComputations of hypervelocity impact uding the CTH shock wave physics code%Zeinert, P., Bless, S.J. and Beno, T.IComminuted particles originating from catastrophic failure of a glass bar900-9023Zelepugin, S.A., Nikulichev, V.B. and Ivanova, O.V.]Numerical simulation of superfast shock-induced chemical reaction in titanium-silicon mixture"Zelepugin, S.A. and Dorokhov, N.S.PFailure of a long rod projectile obliquely interacting with a three-layer target	1407-1410�Zellner, M.B., Grover, M., Hammerberg, J.E., hixson, R.S., Iverson, A.J., Macrum, G.S., Morley, K.B., Obst, A.W., Olson, R.T., Payton, J.R., Rigg, P.A., Routley, N., Stevens, G.D., Turley, W.D., Veeser, L. and Buttler, W.T.FPressure effects on the ejection of material from shocked tin surfaces
Zerilli, F.J.,Shock induced molecular excitation in solids!Zerilli, F.J. and Armstrong, R.W.zDislocation mechanics based constitutive relations for materials dynamics modelling:<   Slip and deformation twinning in iron(Shock Waves in Condensed Matter  �� 1987_Dislocation mechanics based constitutive relations for dynamic straining to tensile instabilityLModeling shock waves with dislocation mechanics based constitutive relations257-260Zerilli, F.J. and Jones, H.D.3High pressure equation of state for HF, CF4, and F2<Constitutive relations for the plastic deformation of metals/Surface energy and the size of diamond crystals1Constitutive relations for titanium and Ti-6Al-4VOExperimental investigation of phase conversion of boron nitride under explosion%Yun, S.R., Huang, Z.P. and Shun, Y.F.QPressure measurement in a recovery tube for superhard BN synthesized by explosionBYunoshev, A.S., Silvestrov, V.V., Kalinin, A.A. and Palyanov, Y.N.@Shock-wave synthesis and HPHT sintering of cubic silicon nitride7Zahariev, F., Hu, A., Hooper, J., Woo, T. and Zhang, F.?Ab initio based simulations of high-pressure phases of nitrogenDZakaria, M., Wu, X., Loretto, M.H., Millett, J.C.F. and Bourne, N.K.EDefect analysis in Ti-based alloys deformed at different strain ratesAZakraysek, A.J., Sutherland, G.T., Sandusky, H.D. and Strange, D.\A new gun facility dedicated to preforming shock physics and terminal ballistics experiments
Zang, J.M.oSound speed and thermal property measurements of inert materials: Laser spectroscopy and the diamond anvil cell73-786Zang, J.M., Howard, W.M., Fried, L.E. and Hansen, D.W.<Detonation product EOS studies: Using ISLS to refine CheetahZaretsky, E.'Dislocation dynamics behind shock frontMMechanism and kinetics of phase transformation in KCl under shock compressionZaretsky, E. and Kaluzhny, M.EFracture threshold and shock induced strengthening of stainless steel\X-ray diffraction technique with VISAR support for study of shock-compressed single crystals8Zaretsky, E., Levi-Hevroni, D., Ofer, D. and Shvarts, D.9Lateral sample motion in the plate-rod impact experiments2X-ray diffraction on shock-strained single crystalGSpatial evolution of three-wave structure in shocked potassium chloride<Zaretsky, E.B., Kanel, G.I., Razorenov, S.V. and Baumung, K.IAnomalous high-temperature shock-induced strengthening of two superalloys*Zaretsky, E., Herrmann, B. and Shvarts, D.3Dynamic response of high temperature uranium phasesZaretsky, E.B.8Shock initiation and detonability of liquid nitromethane9Yoshinaka, A.C., Zhang, F., Petel, O.E. and Higgins, A.J.GInitiation of detonation in multiple shock-compressed liquid explosives'Yoshinaka, A., Zhang, F. and Wilson, W.DEffect of shock compression on aluminum particles in condensed media You, S., Horie, Y. and Hwang, M.[Modeling of shock-induced chemical reactions in powder mixtures 2: Continuum mixture theoryYoung, D.A. and Grover, R.MTheory of the iron equation of state and melting curve to very high pressuresETheory of the carbon phase diagram at high pressures and temperaturesYoung, D.A."The periodic law at high pressures45-52Young, R.D.,Generalized hydrodynamic penetration process	Young, C.?Electromagnetic gauge measurement of dynamic tensile fracturingYoung, R. and Silling, S.MExperimental technique to obtain material response at strain rates to 105 s-1	1647-1650,Young, R.D., Littlefield, D.L. and Horie, Y.&Investigation of anomalous penetration	1821-1824?Probing the shock induced reaction threshold of powder mixtures/Young, D.A., Barbee�  III, T.W. and Rogers, F.J.:New equation of state models for hydrodynamic applications-A new global hydrogen equation of state modelYoung, J.A. and Wirth, B.D.SThe interaction of dislocations and radiation-induced obstacles at high strain-rate6Yu, L.H., Nellis, W.J., Meyers, M.A. and Vecchio, K.S.$Shock synthesis of niobium silicides0Yuan, G., Zhou, G.-Q., Tang, Z.P. and Wang, L.L.DAn analytical model for laser-supported detonation waves on a target	1899-1902!Yun, S.-R., Hou, X.-F. and Lu, M.VExperimental determination of two-dimensional strain of liners under explosive loading625-638Yun, S., Hou, X. and Lu, M.2Yun, S.-R., Sun, Y.-F., Chang, J.-Y. and Wu, F.-Y.YSimulating the thermal response of high explosives on time scales of days to microseconds9Yoh, J.J., Lee, H.H., Choi, J.H., Lee, K.C. and Kim, K.H.JA study of phase explosion of metal using high power Nd:YAG laser ablation5Yokoo, M., Kawai, N., Nakamura, K.G. and Kondo, K.-I.:Hugoniot measurements of gold in pressure range to 580 GPa(Yoneda, A., Spetzler, H. and Getting, I.RImplication of the complete travel time equation of state for a new pressure scale	1609-1612(Yoo, C.S., Furrer, J.J. and Duvall, G.E.LAbsorption spectra and reactions of carbon disulfide under shock compression'Yoo, C.S., Gupta, Y.M. and Duvall, G.E.KElectronic and chemical changes of carbon disulfide under shock compression675-682	Yoo, C.S.bShock induced absorption changes of anthracene in comparison with changes at static high pressures#Yoo, C.S., Holmes, N.C. and See, E.lShock induced optical changes in Al2O3 at 200 GPa: Implications for shock temperature measurements in metals-Yoo, C.S., Holmes, N.C., Ross, M. and See, E.1Shock temperature measurements of iron to 350 GPaYoo, C.S. and Holmes, N.C. Shock initiation of nitromethane	1567-1570(Yoo, C.S., Holmes, N.C. and Souers, P.C.HTime-resolved temperatures of shocked and detonating energetic materialsYoo, Y.-H. and Kum, O.bNumerical simulation of long rod interaction with multi-layered ceramic materials at oblique angle*Yoshida, M., Fujiwara, S. and Kusakabe, M.WA new method for the evaluation of the Gruneisen parameter from Lagrangian gage records(Yoshida, M., Tanaka, K. and Fujiwara, S.YA computational study of a shock collision fixture for high-pressure recovery experimentsYoshida, M. and Thadhani, N.N.tStudy of shock induced solid state reactions by recovery experiments and measurements of Hugoniot and sound velocity585-592Yoshinaka, A. and Zhang, F.OCalculation of nonequilibrium velocities in powder mixtures under shock loadingYano, K. and Horie, Y.CParticle velocity dispersion in shock compression of solid mixturesCDiscrete-element modeling of shock-induced phase transition in iron$Yano, K., Horie, Y. and Greening, D.3Mechanistic model of hot-spot: A unifying frameworkaYao, B., Ding, B.Z., Li, D.J., Hu, Z.Q., Su, W.H., Geng, Y.Z., Hu, A.G., Lou, T.P. and Yang, J.H.6A discussion on a new phase in polycrystalline diamond'Yao, J., Gunger, M.E. and Matuska, D.A.2Simulation of shaped-charge with SPH rezone methodYao, J.0A fast three-dimensional lighting time algorithmYao, G.W. and Liu, Z.F._Experimental study on shear response of 92.93 wt% alumina under combined pressure-shear loading*Yarger, F.L., Prieto, F.E. and Loske, A.M..Underwater shock waves in medical applicationsSYazaki, A., Kishimura, H., Hironaka, Y., Saito, F., Nakamura, K.G. and Kondo, K.-I.\Transition from expansion to shock compression in laser irradiated silicon by multiple shots(Yaziv, D., Bless, S.J. and Rosenberg, Z.+Shock fracture and recompaction of ceramics425-4305Yaziv, D., Yeshurun, Y., Partom, Y. and Rosenberg, Z.9Shock structure and precursor delay in commercial alumina*Yaziv, D., Cox, P.A. and Riegel�  III, J.P.]Modified integral theory of impact to model long rod penetration at normal and oblique impact;Yelkin, V.M., Kozlov, E.A., Kakshina, E.V. and Moreva, Y.S.TTwo-phase (g,a) equation of state for cerium and features of its dynamic compressionTYenice, K.M., Lee, S.A., Venkateswaran, U.D., Williamson�  III, W. and Dubowski, J.J.QPhotoluminescence study of CdTe-Cd1-xMnxTe multiple quantum well at high pressure-Yeshurun, Y., Rosenberg, G. and Rosenberg, Z.KMeasurements of compressive and tensile waves in a shock loaded pyrex glass431-435Yoh, J.J. and McClelland, M.A.KYagi, T., Hishinuma, T<  ., Yamakata, M., Uchida, T., Utsumi, W. and Fukai, Y.SFormation and structure of iron hydride under the condition of the Earth's interior!Yagi, T., Kondo, T. and Syono, Y.pHigh pressure in situ X-ray diffraction study of MnO to 137 GPa and comparison with shock compression experiment*Yakovlev, I.V., Pai, V.V. and Kuzmin, G.E.[Approximate estimate of loading parameters in composites for the case of strong shock wavesYakushev, V.V.fElectrical effects in polarized polymer films under high velocity impact: Application to impact gauges	1069-1073"Yakushev, V.V. and Yakusheva, T.I.6Electrical conductivity of shock-compressed PVDF films,Yakushev, V.V., Utkin, A.V. and Zhukov, A.N.?Hugoniot and phase transition in silicon nitride porous samples0Yamakata, M., Yagi, T., Utsumi, W. and Fukai, Y.fElectrical conductivity and crystal structure of iron hydride under high pressure and high temperatureYamamoto, H. and Sawaoka, A.B.{Microstructure and superconducting critical temperature of dynamically consolidated YBa2Cu3O7-x without post heat treatment$Yang, G., Tang, Z.P. and Zhou, G.-Q.=Non-Fourier thermoelastic response of metal induced by lasers5Yang, W., Ahrens, T.J., Miller, G.H. and Petach, M.B.#Jet ejecta mass upon oblique impactYang, W.-B. and Ahrens, T.J..Oblique impact jetting of geological materials3Yang, W., Chen, G., Anderson, W.W. and Ahrens, T.J.4Shock compression and isentropic release of rhyolite	1115-1118/Yang, Y., Gould, R.D., Horie, Y. and Iyer, K.R.XNew evidence concerning the shock-induced chemical reaction mechanism in a Ni/Al mixture>Yanilkin, A.V., Kuksin, A.Y., Norman, G.E. and Stegailov, V.V.SAtomistic simulations of fracture in nanocrystalline copper under high strain rates"Yano, K., Horie, Y. and Tang, Z.P.+Wright, T.W., Ramesh, K.T. and Molinari, A.MStatus of statistical modeling for damage from nucleation and growth of voids690-693NWright, M., Williams, P., Richardson, J., Edmonds, E., Jones, A. and Drake, R.GUK marginal initiation characterisation test (MICT) for high explosives2Wu, Y.H., Onomichi, M., Sasaki, S. and Shimizu, H.NHigh-pressure Raman studies of liquids and solids of some fluorinated methanesWu, T.-C. and Bassett, W.A.\Measuring deviatoric stress in the diamond anvil cell using two X-ray diffraction geometries	1625-1628Wu, Q., Tan, H. and Jing, F.-Q.LA thermodynamic model for prediction of shock adiabatics of porous materials Xia, H., Xia, Q. and Ruoff, A.L.,Equation of state of BP to megabar pressures Xia, Q., Xia, H. and Ruoff, A.L.>New high pressure phases of the III-IV compounds AlN, GaN, InNXiao, D., Li, Y. and Hu, S./Study of small dimension specimens on SHPB test,Xu, K., Yu, D.-Y., Xu, Y.-X. and Zeng, X.-F.OEffect of charge diameter on detonation pressure measured by aquarium technique573-5779Xu, D.-P., Tong, X., Su, W.-H., Xiao, L.-Z. and Li, S.-T.iStructure and magnetic properties of CdS nanocrystalline materials synthesized under high static pressureXu, Y. and Espinosa, H.D.*Damage quantification in confined ceramicsXu, X. and Thadhani, N.N.iInvestigation of shock-induced chemical reactions in Ni-Ti powder mixtures using instrumented experiments*Xue, Q., Nesterenko, V.F. and Meyers, M.A.USelf-organization of adiabatic shear bands in titanium, Ti-6Al-4V and stainless steel'Xue, Q., Gray�  III, G.T. and Chen, S.R.MInfluence of shock prestraining on shear localization in 316L stainless steel*Xue, Q., Cerreta, E.K. and Gray�  III, G.T.�Influence of explosive-driven shock prestraining on the microstructural evolution and shear localization of 304 and 316L stainless steels,Wood, S.M., Gupta, Y.M. and Pangilinan, G.I.PTime-resolved Raman measurements in shocked Z-cut, a-quartz subjected to tension	1571-1574+Wood, B.P., Trainor, R.J. and Keinigs, R.K.AShock compression experimental capabilities of the ATLAS facility#Woody, D., Davis, J. and Coffey, S.YReal time imaging of shear bands induced by low velocity shocks during impact of crystalsWoody, D.L. and Davis, J.J.FThe effect of low velocity impact on various inert crystalline samples)Woody, D.L., Davis, J.J. and Deiter, J.S.8Plastic flow generated solid state metal/metal reactionsWRecovery studies of impact-induced metal/polymer reactions in titanium based composites667-669Woody, D. and Davis, J.J.^The effect of variation of aluminum particle size and polymer on the performance of explosives942-945)Woody, D.L., Dokhan, A. and Johnson, C.E.WPerformance comparisons of nanoaluminum, coated microaluminum and their bimodal mixture4Woolsey, N.C., Wark, J.S., Blyth, W.J. and Riley, D.'Sub-nanosecond powder x-ray diffractionWoolsey, N.C. and Wark, J.S.\Simulated X-ray streak camera data of in situ diffraction from laser-shocked single crystals	1919-19223Woolsey, N.C., Cauble, R., Lee, R.W. and Wark, J.S.TIn situ X-ray diffraction from uniform radiation driven shocks in crystalline solidsLWorkman, A., Meziere, Y.J.E., Millett, J.C.F., Bourne, N.K. and Wallwork, A.FShear stress in nickel and Ni-60Co under one-dimensional shock loading,Wright, N.G., McMahon, M.I. and Nelmes, R.J.JMicrostructural aspects of reconstructive phase transitions under pressure*Wright, S.I., Bingert, J.F. and Zernow, L.DMicrotextural characterization of copper shaped charge jet fragments9Wright, T.W., Schoenfeld, S.E., Ramesh, K.T. and Wu, X.Y.FProgress in computational models for damage from shear bands and voids$Wise, S., Bless, S.J. and Brar, N.S./Shock compression of chemically bonded ceramicsWise, J.L. and Grady, D.E.KDynamic, multiaxial impact response of confined and unconfined ceramic rodsRWise, J.L., Jones, S.C., Hall, C.A., Reinhart, W.D., Hickman, R.J. and Gluth, J.W.VEffects of annealing and preheating on the impact response of selected braze materials686-689AWise, J.L., Jones, S.C., Hall, C.A., Asay, J.R. and Sanchez, D.M.<Dynamic response of Kovar to shock and ramp-wave compression Wisniewski, R. and Molinar, G.F.@High pressure transducer with ceramic free rod as active element	1685-1686Witczak, Z.�The effect of hydrostatic pressurization on the microstructure and mechanical properties of the L12 Cu-modified titanium trialuminide,Witczak, Z., Jemielniak, R. and Szczepek, J.}The apparatus for mechanical testing of materials under high hydrostatic pressure with the in situ acoustic emission analyzer	1601-16044Wittman, C., Lopatin, C., Perron, P. and Swenson, J.2Strain rate dependency of copper recrystallizationKWixom, M.R., Fechner, W.B., Maynard, R.L., Schmerberg, N.W. and Mayer, F.J.&Shock processing in spherical geometryWixom, M.R.TShock recovery experiments on high nitrogen content, high molecular weight compoundsWixom, M.W.7An electroluminescent fiber optic shock pressure sensorWong, M.K.W. and Gupta, Y.M.MResponse of lateral piezoresistance gauges in fused silica shocked to 60 kbarTDynamic inclusion analyses of lateral piezoresistive gauges under shock wave loadingWong, P.T.T.CHigh pressure FT-IR spectroscopy for biomedical and cancer researchWong, M.K.W.:Experiments and analysis of lateral piezoresistance gauges	1735-1738Wong, C.P. and Gump, J.C.UVibrational spectroscopic studies of reduced-sensitivity RDX under static compressionJEOS data of Ti6Al4V to impact velocities of 10.4 km/s on a three-stage gunWinkler, W.D. and Stilp, A.J.NSpallation behavior of TiB2, SiC, and B4C under planar impact tensile stressesMPressure induced macro- and micromechanical phenomena in planar impacted TiB2Winkler, W.-D. and Nahme, H.GA simple recovery technique for shock wave studies of brittle materials	1663-1666,Winter, R.E., Markland, L.S. and Prior, S.D.1Modelling shock initiation of HMX-based explosiveSWinter, R.E., Taylor, P., Carley, D.J., Barlow, A.J., Pragnell, H. and Markland, L.jA flash X-ray technique to measure strain distribution at interfaces sliding at high pressure and velocityRWinter, R.E., Smeeton, V.S., De'Ath, J., T<  aylor, P., Markland, L. and Barlow, A.J.FMetallography of sub-surface flows generated by shock-induced frictionLWinter, R.E., Whiteman, G., Haining, G.S., Salisbury, D.A. and Tsembelis, K.6Measurement of equation of state of silicone elastomerWinter, R.E. and Harris, E.J.:Stress-induced resistivity of padded lateral stress gauges-Perturbations caused by lateral stress gaugesCWinter, R.E., Keightley, P.T., Kim, H.J., Rigney, D.A. and Emge, A.,Microstructures produced by dynamic friction+Wise, J.L., Chhabildas, L.C. and Asay, J.R.Shock compression of beryllium417-421
Wise, J.L.^Refractive index and equation of state of a shock-compressed aqueous solution of zinc chlorideWise, J.L. and Chhabildas, L.C.SLaser interferometer measurements of refractive index in shock compressed materials441-454Wise, J.L. and Mikkola, D.E.UHugoniot and wave-profile measurements on shock-loaded stainless steel (21Cr-6Ni-9Mn)Wise, J.L. and Kipp, M.E.>Time-resolved penetration response of ceramic and steel plates*Wise, J.L., Kerley, G.I. and Trucano, T.G.4Shock-vaporization studies on zinc and porous carbon0Williamson, D.M., Palmer, S.J.P. and Proud, W.G.*Fracture studies of PBX simulant materials<Williamson, D.M., Palmer, S.J.P., Proud, W.G. and Govier, R.SBrazilian disc testing of a UK PBX above and below the glass transition temperature+Willmott, G.R., Proud, W.G. and Field, J.E.Shock properties of kimberliteWills, J.M. and Eriksson, O.]Theoretical studies of the crystal structure of rare earths and actinides at zero temperature*Wilson, C.R., duvall, G.E. and Ogilvie, K.DThe resisitivity of liquid carbon disulfide during shock compression296-298Wilson, K.R.4Molecular dynamics of chemical reactions in solution27-34Wilson, W.H. and Holloway, D.C.DRelationship between wavefront curvature and surface tensile strainsWilson, W.H.RExperimental study of reaction and stress growth in projectile impacted explosives<Wilson, W.H., Forbes, J.W., Liddiard, T.P. and Doherty, R.M.2Sensitivity studies of a new energetic formulationMWilson, W.H., Forbes, J.W., Gustavson, P.K., Lemar, E.R. and Sutherland, G.T.9Detonation properties of the non-ideal explosive PBXW-123mWilson, J.N., Hashemi, J., James, D., G"�ven, N., Dallas, T., Kuhrts, K., Combs, B., Hale, M. and Willson, G.ZMetallurgical analysis and computer simulation of a solid steel sphere under shock loading(Winey, J.M., Gupta, Y.M. and Casey, K.G.@Shock-induced changes in the absorption spectrum of nitromethane	1563-1566GWiney, J.M., Dreger, Z.A., Gruzdkov, Y.A., Jensen, B.J. and Gupta, Y.M.OEquation of state and temperature measurements for shocked ammonium perchlorateWiney, J.M. and Gupta, Y.M..Anisotropic modeling for shock single crystals367-372Winfree, N.A. and Kerley, G.I..Equation of state model for tributyl phosphateOWinfree, N.A., Chhabildas, L.C., Reinhart, W.D., Carroll, D.E. and Kerley, G.I.XDevelopment of a simple model of 'hot-spot' initiation in heterogeneous solid explosives^Application of the CREST reactive burn model to two-dimensional PBX 9502 explosive experiments881-8849Wicks, A.L., Kaiser, M.A., Wilson, L.T. and Swantek, S.D.WExperimentally derived bar dispersion and transducer selection for split Hopkinson bars
Wiegand, D.A.DMechanical failure properties of composite plastic bonded explosivesPThe influence of confinement on the mechanical properties of energetic materialsWiegand, D. and Reddingius, B.XMechanical properties of plastic bonded composites as a function of hydrostatic pressure812-815
Wilkerson, S.mA numerical formulation using the boundary integral method for three-dimensional bubble dynamics calculations?Wilkinson, J., Lightstone, J.M., Boswell, C.J. and Carney, J.R.?Emission spectroscopy of aluminum in post-detonation combustion,Williams, W.D., Fogelson, D.J. and Lee, L.M.#Carbon piezoresistive stress gauges7Williams, F.L., Lee, Y.K., Morosin, B. and Graham, R.A.PCatalytic activity of shock modified ZnO for CO oxidation and methanol synthesis791-796Williams, Q. and Jeanloz, R.IAnalysis of CsI shock-wave data in terms of high-temperature dissociation73-75Williams, P.E.AThe influence of the reaction rate of explosives on blast effects Williamson, R.L. and Berry, R.A.VMicrolevel numerical modeling of the shock wave induced consolidation of metal powders341-346?Williamson, D.L., Morosin, B., Venturini, E.L. and Graham, R.A.1Mossbauer study of shock-synthesised zinc ferrite809-814!Williamson, R.L. and Wright, R.N.gA particle-level numerical simulation of the dynamic consolidation of a metal matrix composite materialAWilliamson, D., Palmer, S., Grantham, S., Proud, W. and Field, J. Mechanical properties of PBS9501816-819QWeir, S.T., Nellis, W.J., Kramer, M.J., Seaman, C.L., Early, E.A. and Maple, M.B.EShock induced defects and flux pinning in YBa2Cu3O7-d + Ag composites563-565ILarge area and short-pulse shock initiation of a TATB/HMX mixed explosiveCWark, J.S., Whitlock, R.R., Hauer, A., Swain, J.E. and Solone, P.J.9Short-pulse X-ray diffraction from laser-shocked crystals781-786<Wark, J.S., Whitlock, R.R., Kiehn, G., Smith, R. and Lin, Z.?Simulation of transient x-ray diffraction from shocked crystalsMWark, J.S., Woolsey, N.C., Riley, D., Blyth, W., Whitlock, R.R. and Keihn, G.vDirect measurements of compressive and tensile strain during shock breakout by use of sub-nanosecond x-ray diffractionFWark, 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. and Stolken, J.S.?Picosecond X-ray diffraction from laser-shocked copper and iron286-291)Multi-material velocities for mixed cells	1773-1776Walker, J.D.!Incoherence of shaped charge jets	1869-1872Walker, J.D. and Young, R.D.GDeformation mechanisms of powder particles during dynamic consolidationLAn analytic penetration model for a Drucker-Prager yield surface with cutoffWalker, J.D. and Thacker, B.H.%Yield surfaces for anisotropic plates5Walker, J.D., Dannemann, K.A. and Anderson�  Jr., C.E.8Anisotropic failure model development and implementationQNew directions and new challenges in analytical modeling of penetration mechanics	1273-1278
Wallace, D.C.37-49'Overdriven shocks in solids and liquidsLWallwork, A., Meziere, Y.J.E., Millett, J.C.F., Bourne, N.K. and Workman, A.6Spallation in NiTi under one-dimensional shock loading682-685Walsh, J.M.`On the problem of the oblique interaction of a detonation wave with an explosive-metal interface
Walters, C.T.2Laser generation of 100 kbar shock waves in solids
Walters, W.P.Shaped charges and shock waves	1053-1060Walters, W.P. and Summers, R.L._An analytical expression for the velocity difference between jet particles from a shaped charge	1861-1864Shaped charge jet particulation	1873-1876Wang, J. Asymmetric supersonic collisions661-666)Wang, S.L., Meyers, M.A. and Graham, R.A.;Shock consolidation of IN-100 nickel-base superalloy powder731-736"Wang, Z.-X., Li, H. and Zhu, J.-S.XNumerical simulation of one dimensional unsteady detonation by method of characteristicsWang, J.-H. and Zhang, J.-G.gMolecular dynamics simulation of ejection induced by reflection of shock wave at free surface of metals'Wang, J.-H., Duan, W.-S. and Pan, Y.-S.?Molecular dynamics investigation of shock wave in one dimension&Wang, W., Jin, X.-G. and Rosenberg, Z.)Vorobiev, O., Cowler, M. and Birnbaum, N.?A modular material modeling architecture for nonlinear dynamicsVorthman, J.E.JFacilities for the study of shock induced decomposition of high explosives680-684Vorthman, J. and Wackerle, J.7Multiple-wav<�e effects on explosives decomposition ratesHVorthman, J.E., Hixson, R.S., Anderson, W.W., Fritz, J.N. and Shaw, M.S.)Release isentropes in overdriven PBX 9502FVos, W.L., Finger, L.W., Hemley, R.J., Mao, H.-K. and Yoder�  Jr., H.S.)Phase behavior of H2-H2O at high pressure%Vrel, D., Huang, X.S. and Mashimo, T.7Shock compression recovery experiments on some dioxides8Vukuturi, S., Perger, W.F., Dreger, Z.A. and Gupta, Y.M.5First-principles vibrational study of pentaerythritolWackerle, J. and Anderson, A.D.JBurning topology in the shock-induced reaction of heterogeneous explosivesWackerle, J. and Stacy, H.L.*Refractive index of shocked alkali halidesGShock-induced heating, phase transitions, and opacity in alkali halides0Wakabayashi, K., Nakamura, K.G. and Kondo, K.-I.dShock-induced orientation of benzen molecules studied by nanosecond time-resolved Raman spectroscopyFWakabayashi, K., Matsumura, T., Nakayama, Y., Yamada, E. and Koshi, M.]Temporal change of Raman spectra of carbon tetrachloride under laser-driven shock compression@Wakatsuki, M., Takano, K.J., Kagi, H., Yuino, T. and Kumagai, S.RReal-time evaluation of pressure using the pressure effect on EMF of thermocouples	1695-1698Walker, F.E. and Karo, A.M.fComparison of detonation velocities and average vibrational motion of atom pairs in organic explosives��DYV	4#��/]�<S�K��W[b�q\�~��HH�sL�w���
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Anon7 - 2021