NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = D.H.Gross Found 53 matches. 2006GR25 Eur.Phys.J. A 30, 293 (2006) Nuclear multifragmentation, its relation to general physics
doi: 10.1140/epja/i2005-10317-6
2003GR29 Phys.Lett. B 574, 186 (2003) Remarkable long-range-systematic in the binding energies of α-nuclei. II NUCLEAR STRUCTURE A=4-100; analyzed two-nucleon and alpha-particle separation energies; deduced α-cluster structure features.
doi: 10.1016/j.physletb.2003.09.030
2001GR04 Nucl.Phys. A681, 366c (2001) Phase Transitions in ' Small ' Systems - A Challenge for Thermodynamics -
doi: 10.1016/S0375-9474(00)00540-6
2000OE06 Part. and Nucl., Lett. 99, 70 (2000) H.Oeschler, A.S.Botvina, D.H.E.Gross, S.P.Avdeyev, V.A.Karnaukhov, L.A.Petrov, V.K.Rodionov, O.V.Bochkarev, L.V.Chulkov, E.A.Kuzmin, A.Budzanowski, W.Karcz, M.Janicki, E.Norbeck Variation of the Coulomb Replusion in Multifragmentation NUCLEAR REACTIONS 197Au(p, X), E=8.1 GeV; measured intermediate mass fragments yields, charge and energy distributions; deduced contribution from Coulomb repulsion vs fragment multiplicity.
1999BO16 Phys.Rev. C59, 3444 (1999) A.S.Botvina, M.Bruno, M.D'Agostino, D.H.E.Gross Influence of Coulomb Interaction of Projectile- and Target-Like Sources on Statistical Multifragmentation NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; calculated fragment charge yields, velocity distributions; deduced Coulomb effects. Statistical multifragmentation.
doi: 10.1103/PhysRevC.59.3444
1999CH23 Eur.Phys.J. A 5, 251 (1999) A.Chbihi, O.Schapiro, S.Salou, D.H.E.Gross Experimental and Theoretical Search for a Phase Transition in Nuclear Fragmentation NUCLEAR REACTIONS 100Mo(28Si, X), E=701 MeV; analyzed particle spectra; calculated compound nucleus energy vs temperature; deduced phase transition features. Berlin microcanonical statistical multifragmentation model, caloric equation of state.
doi: 10.1007/s100500050283
1998BO15 Phys.Rev. C58, R23 (1998) Statistical Nature of Multifragmentation NUCLEAR REACTIONS 197Au(36Ar, X), E=110 MeV/nucleon; calculated charged fragments total transverse energy, multiplicity; deduced statistical characteristics of multifragmentation.
doi: 10.1103/PhysRevC.58.R23
1997BO30 Phys.Lett. 408B, 31 (1997) Charge Distributions in Multifragmentation Indicating the Nuclear Liquid-Gas Phase-Transition ( Question ) NUCLEAR REACTIONS 197Au(129Xe, X), E=60 MeV/nucleon; calculated intermediate mass fragment charge distribution; deduced data analysis filtering role, phase transition implications.
doi: 10.1016/S0370-2693(97)00821-6
1995BO13 Phys.Lett. 344B, 6 (1995) Sequential or Simultaneous Multifragmentation of Nuclei ( Question ) NUCLEAR STRUCTURE 197Au; calculated intermediate mass fragment multiplicity distribution. Simultaneous fragmentation model.
doi: 10.1016/0370-2693(94)01590-9
1995BO24 Nucl.Phys. A592, 257 (1995) The Effect of Large Angular Momenta on Multifragmentation of Hot Nuclei NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; calculated total(c.m.) kinetic energy vs projectile fragments relative Coulomb energy. Microcanonical thermodynamics.
doi: 10.1016/0375-9474(95)00299-G
1995KH04 Nucl.Phys. A583, 353c (1995) D.T.Khoa, A.Faessler, N.Ohtsuka, D.H.E.Gross Thermalization Effects in Heavy-Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=100, 400 MeV/nucleon; calculated average matter density, temperature, one-body entropy time evolution; deduced thermalization process related features. Quantum molecular dynamics approach.
doi: 10.1016/0375-9474(94)00686-H
1995LI09 Nucl.Phys. A583, 585c (1995) V.Lips, R.Barth, H.Oeschler, S.P.Avdeyev, V.A.Karnaukhov, W.D.Kuznetsov, L.A.Petrov, O.V.Bochkarev, L.V.Chulkov, E.A.Kuzmin, W.Karcz, W.Neubert, E.Norbeck, B.-A.Li, D.H.E.Gross Multifragmentation Induced by Relativistic α-Projectiles NUCLEAR REACTIONS 197Au(α, X), E=1-3.6 GeV/nucleon; measured intermediate mass fragment multiplicity, spectra; deduced breakup density, breakup mechanism.
doi: 10.1016/0375-9474(94)00731-2
1994GR02 Nucl.Phys. A567, 317 (1994) Statistical Multifragmentation: Comparison of two quite successful models NUCLEAR STRUCTURE 131Xe; calculated fragmentation excitation energy vs temperature. Statistical multi-fragmentation.
doi: 10.1016/0375-9474(94)90151-1
1994GR17 Z.Phys. A349, 291 (1994) Statistical Multifragmentation NUCLEAR STRUCTURE 197Au; calculated fragment vs excitation energy, relative decay yields following breakup. Statistical multi-fragmentation, microcanonical Metropolis Monte Carlo techniques.
doi: 10.1007/BF01288977
1994LI37 Phys.Lett. 335B, 1 (1994) B.-A.Li, D.H.E.Gross, V.Lips, H.Oeschler Freeze-Out Configuration in Multifragmentation NUCLEAR REACTIONS 197Au(α, X), E=1, 3-6 GeV/nucleon; calculated intermediate fragment vs correlation angle, charge, velocity vs multiplicity. Statistical model plus many-body Coulomb trajectory.
doi: 10.1016/0370-2693(94)91548-2
1994LI40 Phys.Lett. 338B, 141 (1994) V.Lips, R.Barth, H.Oeschler, S.P.Avdeyev, V.A.Karnaukhov, V.D.Kuznetsov, L.A.Petrov, O.V.Bochkarev, L.V.Chulkov, E.A.Kuzmin, W.Karcz, W.Neubert, E.Norbeck, D.H.E.Gross Evidence for Simultaneous Breakup in Reactions with Relativistic α-Projectiles NUCLEAR REACTIONS 197Au(α, X), E at 3.6 GeV/nucleon; measured (fragment)(fragment) relative angle distribution; deduced intermediate mass fragment emission time scale dependence, Coulomb trajectory calculations.
doi: 10.1016/0370-2693(94)91357-9
1994SC06 Nucl.Phys. A568, 333 (1994) O.Schapiro, A.R.DeAngelis, D.H.E.Gross IMF-IMF Correlations NUCLEAR STRUCTURE 197Au; calculated intermediate-mass fragment correlation function versus excitation. Coulomb effects.
doi: 10.1016/0375-9474(94)90206-2
1994SC11 Nucl.Phys. A573, 143 (1994) IMF-IMF Correlations: Information on space-time structure of the fragmenting source NUCLEAR REACTIONS Cu(129Xe, X), E=50 MeV/nucleon; low multiplicity event correlation function; deduced fragmenting source space time structure. Berlin multi-fragmentation model, intermediate mass fragment correlation.
doi: 10.1016/0375-9474(94)90018-3
1994SC28 Nucl.Phys. A576, 428 (1994) IMF-IMF Correlations 3-4-Fragment Correlations Reveal Details of the Breaking Process NUCLEAR STRUCTURE 197Au; calculated fragmentation characteristics, intermediate mass fragments. Berlin multi-fragmentation model.
doi: 10.1016/0375-9474(94)90252-6
1993GR04 Nucl.Phys. A553, 175c (1993) Multifragmentation NUCLEAR REACTIONS 96Mo(96Mo, X), E=55 MeV/nucleon; compiled, reviewed calculated one-particle density distribution vs time; deduced multifragmentation, mechanism. NUCLEAR STRUCTURE 197Au; compiled, reviewed fragmentation yield, fragment mass vs excitation calculations; deduced multifragmentation mechanism.
doi: 10.1016/0375-9474(93)90622-5
1993GR14 Phys.Lett. 318B, 405 (1993) What is Wrong with the Bethe-Formula for the Nuclear Level-Density ( Question ) Measurable Differences between Grandcanonical and the Microcanonical Treatments NUCLEAR STRUCTURE 131Xe; calculated multi-fragment relative yield vs excitation energy; deduced Bethe-formula level density features, model dependences. Grandcanonical, micro-canonical treatments.
doi: 10.1016/0370-2693(93)91531-Q
1993LI05 Nucl.Phys. A554, 257 (1993) Dynamical Instability and Nuclear Multifragmentation in BUU Model for Heavy-Ion Collisions NUCLEAR REACTIONS 96Mo(96Mo, X), E=55, 100 MeV/nucleon; calculated one-body density distribution scatter plots; deduced dynamical instabilities development features. Boltzmann-Uehling-Uhlenbeck transport model.
doi: 10.1016/0375-9474(93)90342-U
1993LI39 Phys.Lett. 318B, 39 (1993) Unusual Behaviour of Heavy Collision Residues ( Question ) NUCLEAR REACTIONS U(d, X), E at 3.65 GeV/nucleon; calculated fragment mass distribution vs U nucleus excitation; deduced evaporation residues role in structure. Statistical model.
doi: 10.1016/0370-2693(93)91780-Q
1992GR23 Ann.Phys.(Leipzig) 1, 467 (1992) D.H.E.Gross, B.-A.Li, A.R.DeAngelis Fragmentation, Dissipative Expansion, and Freeze-Out in Medium Energy Heavy-Ion Collisions NUCLEAR REACTIONS 96Mo(96Mo, X), E=55 MeV/nucleon; calculated one-particle density distribution; deduced different stages in nuclear fragmentation. Boltzmann-Uehling-Uhlenbeck transport equation with, without Coulomb interaction.
doi: 10.1002/andp.19925040609
1992HU06 Phys.Rev. C46, R1577 (1992) J.Hubele, P.Kreutz, V.Lindenstruth, J.C.Adloff, M.Begemann-Blaich, P.Bouissou, G.Imme, I.Iori, G.J.Kunde, S.Leray, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, J.Pochodzalla, G.Raciti, G.Rudolf, H.Sann, A.Schuttauf, W.Seidel, L.Stuttge, W.Trautmann, A.Tucholski, R.Heck, A.R.DeAngelis, D.H.E.Gross, H.R.Jaqaman, H.W.Barz, H.Schulz, W.A.Friedman, R.J.Charity Statistical Fragmentation of Au Projectiles at E/A = 600 MeV NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; measured intermediate mass fragments mean multiplicity.
doi: 10.1103/PhysRevC.46.R1577
1992JA07 Nucl.Phys. A541, 492 (1992) H.R.Jaqaman, A.R.DeAngelis, A.Ecker, D.H.E.Gross Charge-Conservation, Quantum Symmetry, and Metropolis Sampling in an Exactly Solvable Model of Nuclear Fragmentation NUCLEAR STRUCTURE Z=99; calculated unaveraged Campi plot for largest fragment vs model parameter. Exactly solvable fragmentation model, Monte Carlo method.
doi: 10.1016/0375-9474(92)90188-P
1991JA01 Nucl.Phys. A524, 321 (1991) Signals of the Liquid-Gas Phase Transition in the Fragmentation of Hot Nuclei: Finite-size scaling NUCLEAR STRUCTURE 131Xe, 165Ho, 197Au, 209Bi, 232Th, 252Es; calculated fragment size vs second moment; deduced phase transition features. Hot nuclei fragmentation, finite size scaling.
doi: 10.1016/0375-9474(91)90029-6
1991MO18 Nucl.Phys. A533, 333 (1991) K.Mohring, T.Srokowski, D.H.E.Gross Modelling Dissipative Break-Up of Heavy Ions NUCLEAR REACTIONS 197Au(20Ne, X), E=150-400 MeV; calculated σ(fragment θ) for X=9Be-19F, fusion σ(E); deduced reaction mechanism. Classical dynamical model.
doi: 10.1016/0375-9474(91)90494-Q
1990LU03 Z.Phys. A336, 57 (1990) Microscopic Calculation of the Surface Absorption in the Optical Potential NUCLEAR REACTIONS 40Ca(n, n), E not given; calculated imaginary potential. Microscopic model, 2p-1h, 1p-2h contributions.
1989GR10 Nucl.Phys. A495, 231c (1989) Thermodynamics of Nuclei and Nuclear Fragmentation NUCLEAR STRUCTURE 131Xe, 197Au; calculated excitation energy vs temperature. Equipartition model.
doi: 10.1016/0375-9474(89)90322-9
1989GR14 Phys.Lett. 224B, 29 (1989) D.H.E.Gross, G.Klotz-Engmann, H.Oeschler Relative Velocities between Fragments. A Key Quantity in Multifragmentation NUCLEAR REACTIONS 197Au(α, X), E=800 MeV/nucleon; measured two-fragment relative velocity distribution; deduced multi-fragmentation evidence.
doi: 10.1016/0370-2693(89)91044-7
1988GR01 Phys.Lett. 200B, 397 (1988) D.H.E.Gross, Y.-M.Zheng, H.Massmann New Kind of Phase Transition in Hot Nuclei NUCLEAR STRUCTURE 131Xe; calculated phase transitions. Monte Carlo simulations.
doi: 10.1016/0370-2693(88)90141-4
1988GR06 Phys.Lett. 203B, 26 (1988) Multifragmentation at Low Energies ( Question ) NUCLEAR REACTIONS 139La(12C, X), E=50 MeV/nucleon; calculated fragment relative yield following incomplete fusion. 146Nd deduced fragmentation features.
doi: 10.1016/0370-2693(88)91563-8
1988GR19 Nucl.Phys. A488, 217c (1988) Theoretical Approaches to Statistical Multifragmentation NUCLEAR REACTIONS Ag(32S, X), (16O, X), E not given; analyzed data; deduced 131Xe decay features. Statistical multifragmentation.
doi: 10.1016/0375-9474(88)90264-3
1988MO05 Phys.Lett. 203B, 210 (1988) K.Mohring, T.Srokowski, D.H.E.Gross, H.Homeyer A Dynamical Model for Projectile Break-Up and Incomplete Fusion NUCLEAR REACTIONS 197Au, 20Ne(20Ne, X), E ≈ 100-400 MeV; measured fusion σ(E), σ(θ(X), θα). Dynamical model. Projectile breakup.
doi: 10.1016/0370-2693(88)90540-0
1988ZH13 Chin.J.Nucl.Phys. 10, 300 (1988) Zheng Yuming, S.Xu, X.Zhang, D.H.E.Gross Microcanonical Simulation for the Decay of Very Hot Nuclei NUCLEAR STRUCTURE 238U; calculated fragment mass distribution, charge distribution and energy spectra. Hot nucleus fragmentation.
1987ZH02 Nucl.Phys. A461, 641 (1987) X.-Z.Zhang, D.H.E.Gross, S.-Y.Xu, Y.-M.Zheng On the Decay of Very Hot Nuclei. (I). Canonical Metropolis Sampling of Multifragmentation NUCLEAR REACTIONS 238U(p, X), E=1-400 GeV; calculated σ vs fragment mass, yields vs fragment energy. Canonical Metropolis sampling method.
doi: 10.1016/0375-9474(87)90414-3
1987ZH03 Nucl.Phys. A461, 668 (1987) X.-Z.Zhang, D.H.E.Gross, S.-Y.Xu, Y.-M.Zheng On the Decay of Very Hot Nuclei. (II). Microcanonical Metropolis Sampling of Multifragmentation NUCLEAR REACTIONS 238U(p, X), E=1-400 GeV; calculated σ vs fragment mass, yield vs temperature, charge fragment multiplicities. Microcanonical Metropolis sampling method.
doi: 10.1016/0375-9474(87)90415-5
1986AB09 Z.Phys. A325, 373 (1986) A.Y.Abul-Magd, D.H.E.Gross, Xu Shu-yan, Zheng Yu-ming Mass Yield in High-Energy Proton-Uranium Collisions from a Complete, Microcanonical Statistical Decay NUCLEAR REACTIONS 238U(p, X), E=3 GeV; calculated σ vs mass. Glauber approximation.
1986GR03 Phys.Rev.Lett. 56, 1544 (1986) D.H.E.Gross, Zhang Xiao-Ze, Xu Shu-yan Decay of very Hot Nuclei NUCLEAR STRUCTURE 235U; calculated average charged fragment, prompt, evaporated neutron numbers, heavy fragment multiplicity, temperature.
doi: 10.1103/PhysRevLett.56.1544
1985MO02 Nucl.Phys. A433, 671 (1985) E.Moeller, M.C.Nemes, D.H.E.Gross Monte Carlo Simulation of Carbon Fragmentation at High Energies NUCLEAR REACTIONS 12C(p, X), E=high; calculated target fragmentation; deduced dominant decay channels, Coulomb interaction role. Monte Carlo simulation.
doi: 10.1016/0375-9474(85)90024-7
1984RE09 Phys.Rev. C30, 878 (1984) P.-G.Reinhard, J.Friedrich, K.Goeke, F.Grummer, D.H.E.Gross Dynamics of the 16O + 16O → 32S Fusion Process NUCLEAR STRUCTURE 4He, 12C, 16O, 20Ne, 24Mg, 32S, 40Ca; calculated binding energy, diffraction, rms radii, surface width. 16O; calculated charge density. Quantized adiabatic TDHF. NUCLEAR REACTIONS, ICPND 16O(16O, X), E(cm)=2-50 MeV; calculated subbarrier, above barrier fusion σ(E), astrophysical S-factor vs E. 16O(e, e), E not given; calculated form factor. Quantized adiabatic TDHF.
doi: 10.1103/PhysRevC.30.878
1983GR26 Phys.Lett. 130B, 131 (1983) Remarkable Long-Range-Systematics in the Binding Energies of α-Nuclei NUCLEAR STRUCTURE A=4-72; calculated two-nucleon separation energy; deduced evidence for α-structure.
doi: 10.1016/0370-2693(83)91026-2
1983HA09 Z.Phys. A311, 131 (1983) Charge Transfer Prior to Fusion NUCLEAR REACTIONS 116Sn(35Cl, X), E=160-400 MeV; 208Pb(26Mg, X), E=150-250 MeV; measured σ(fusion) vs E.
doi: 10.1007/BF01411618
1982GR04 Phys.Lett. 110B, 31 (1982) Capture Cross Section in the Surface Friction Model NUCLEAR REACTIONS 208Pb(26Mg, X), (27Al, X), E(cm) ≈ 100-250 MeV; 208Pb(48Ca, X), (50Ti, X), (52Cr, X), (58Fe, X), E(cm) ≈ 200-350 MeV; calculated σ(capture) vs E. Surface friction model.
doi: 10.1016/0370-2693(82)90945-5
1981FR06 Z.Phys. A299, 369 (1981) No Need for a New Type of Strongly Damped Collision in the System 132Xe + 56Fe at Energies below 7.12 MeV/u NUCLEAR REACTIONS 56Fe(132Xe, X), E=550-1000 MeV; calculated σ(fusion, E), σ(inelastic). Friction model.
1981GR03 Z.Phys. A299, 63 (1981) D.H.E.Gross, R.C.Nayak, L.Satpathy A Classical Description of Deep Inelastic Collisions with Surface Friction and Deformation NUCLEAR REACTIONS 232Th(40Ar, X), E=379 MeV; 209Bi(136Xe, X), E=1130 MeV; calculated distance of closest approach, deflection function vs L, nuclear potential vs deformation, final energy vs θ. Friction model, deep inelastic, fusion reactions.
doi: 10.1007/BF01415743
1980BR29 Z.Phys. A298, 91 (1980) How and Why to Measure the Overlap of Nuclei in Heavy-Ion Collisions NUCLEAR REACTIONS 209Bi(56Fe, X), E=465 MeV; 197Au(132Xe, X), E=890 MeV; 110Pd(208Pb, X), E=1180 MeV; calculated neutron, proton break through, tunnelling distances, mean separation energies; deduced plausibility of hard friction model. Peripheral collisions, neutron-rich mass exchange.
doi: 10.1007/BF01554048
1977GR07 Phys.Lett. 67B, 1 (1977) Does Radial Friction Cause Emission of Fast α-Particles (Question) NUCLEAR REACTIONS 232Th(40Ar, X), E=379 MeV; analyzed fast α-emission.
doi: 10.1016/0370-2693(77)90788-2
1976DE26 Z.Phys. A277, 385 (1976) J.N.De, D.H.E.Gross, H.Kalinowski A Classical Description of Deep Inelastic Collisions NUCLEAR REACTIONS 232Th(40Ar, X), E=379 MeV; 40Ca(40Ca, X), E=278 MeV; 209Bi(84Kr, X), E=525, 600 MeV; 208Pb(40Ca, X), E=288 MeV; 186W(63Cu, X), E=395 MeV; 197Au(63Cu, X), E=443, 365 MeV; calculated σ for deep inelastic scattering.
doi: 10.1007/BF01545976
1974GR05 Phys.Lett. 48B, 302 (1974) On the Mechanism of Heavy Ion Collisions Leading to a Compound System and to Deep Inelastic Reactions NUCLEAR REACTIONS 27Al, 48Ti, 58Ni, 63Cu, 107Ag, 158Gd, 197Au(12C, X), 27Al, 59Co, 63Cu, 107Ag, 154Sm, 197Au(16O, X), 27Al, 63Cu, 107Ag, 209Bi(20Ne, X), 103Rh(14N, X), 77Se, 121Sb, 165Ho, 238U(40Ar, X), 159Tb(11B, X), 209Bi, 238U(84Kr, X); measured nothing, calculated σ, minimum L for compound formation.
doi: 10.1016/0370-2693(74)90595-4
1972GR49 Phys.Lett. 42B, 41 (1972) The Statistical Model of Nuclei and its Relation to the Strutinsky Averaging Method
doi: 10.1016/0370-2693(72)90710-1
1971WI15 Phys.Rev. C4, 1070 (1971) U.Wille, D.H.E.Gross, R.Lipperheide Calculation of the Separation-Energy Spectrum in the Reaction 12C(p, 2p) NUCLEAR REACTIONS 12C(p, 2p), E=460 MeV; calculated σ. N-N correlations, coupling to continuum channels.
doi: 10.1103/PhysRevC.4.1070
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