NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.Schulz Found 45 matches. 1994DO13 Phys.Rev. C49, 3182 (1994) R.Donangelo, A.Romanelli, H.Schulz, A.C.Sicardi-Schifino Dynamical Effects in the Growth of Density Instabilities
doi: 10.1103/PhysRevC.49.3182
1994SE14 Phys.Lett. 338B, 111 (1994) A.D.Sedrakian, D.Blaschke, G.Ropke, H.Schulz Nuclear In-Medium Effects on the Thermal Conductivity and Viscosity of Neutron Star Matter NUCLEAR REACTIONS 1n(n, n), E not given; calculated σ vs E(rel) in nuclear medium; deduced neutron star matter viscosity, thermal conductivity in-medium effects dependence.
doi: 10.1016/0370-2693(94)91352-8
1993BA11 Phys.Rev. C47, R1838 (1993) W.Bauer, J.P.Bondorf, R.Donangelo, R.Elmer, B.Jakobsson, H.Schulz, F.Schussler, K.Sneppen Large Radial Flow in Nucleus-Nucleus Collisions NUCLEAR REACTIONS Ag, Br(94Kr, X), E=70-120 MeV/nucleon; measured fragment transverse kinetic energy vs fragment charge; deduced excited matter explosive breakup. Other reactions discussed.
doi: 10.1103/PhysRevC.47.R1838
1993BO22 Phys.Rev. C48, 459 (1993) J.P.Bondorf, C.H.Dasso, R.Donangelo, G.Pollarolo, H.Schulz, K.Sneppen Deep Inelastic Collision followed by Disassembly in the Reaction 136Xe + 209Bi at E(lab)/A = 28.2 MeV NUCLEAR REACTIONS 209Bi(136Xe, X), E=28.2 MeV/nucleon; calculated neutron, charged particle multiplicities. Highly dissipative process, independent colliding nuclei decay.
doi: 10.1103/PhysRevC.48.459
1993CA34 Phys.Lett. 318B, 415 (1993) L.F.Canto, R.Donangelo, A.Romanelli, H.Schulz A Coupled-Channels Study of 11Li Coulomb Dissociation NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; analyzed projectile breakup data; deduced continuum-continuum coupling role. Coupled-channels approach, semi-classical approximation, breakup into 9Li+2n.
doi: 10.1016/0370-2693(93)91533-S
1993IE01 Phys.Rev.Lett. 70, 730 (1993) K.Ieki, D.Sackett, A.Galonsky, C.A.Bertulani, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, H.Schulz, B.M.Sherrill, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Coulomb Dissociation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured nn-correlation following projectile dissociation; deduced dissociation mechanism.
doi: 10.1103/PhysRevLett.70.730
1993SA21 Phys.Rev. C48, 118 (1993) D.Sackett, K.Ieki, A.Galonsky, C.A.Bertulani, H.Esbensen, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, H.Schulz, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Electromagnetic Excitation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured 9Li(n)-, γ(9Li)-coin following 11Li Coulomb dissociation; deduced dissociation σ, photonuclear σ(E1), breakup mechanism.
doi: 10.1103/PhysRevC.48.118
1992BA26 Phys.Rev. C45, R2541 (1992) H.W.Barz, J.P.Bondorf, R.Donangelo, I.N.Mishustin, H.Schulz, K.Sneppen Fluctuations and Intermittency in Multifragmentation Processes NUCLEAR STRUCTURE Z=79; calculated multiplicity distribution, factorial moments vs resolution; deduced intermittency causes. Cold, Copenhagen statistical multi-fragmentation models.
doi: 10.1103/PhysRevC.45.R2541
1992BA32 Phys.Rev. C46, R42 (1992) H.W.Barz, J.P.Bondorf, C.H.Dasso, R.Donangelo, G.Pollarolo, H.Schulz, K.Sneppen Mechanism for Nuclear Disassembly of the Ar + Th and Pb + Au Systems at Intermediate Energies NUCLEAR REACTIONS 232Th(40Ar, xn), E=27-77 MeV/nucleon; 197Au(208Pb, xn), E=29 MeV/nucleon; analyzed neutron multiplicity data; deduced collision process binary character.
doi: 10.1103/PhysRevC.46.R42
1992BA51 Nucl.Phys. A548, 427 (1992) H.W.Barz, J.P.Bondorf, R.Donangelo, F.S.Hansen, B.Jakobsson, L.Karlsson, H.Nifenecker, R.Elmer, H.Schulz, F.Schussler, K.Sneppen, K.Soderstrom Analysis of Central Events in the Reaction of 16O and 36Ar with Emulsion at 210 and 65 MeV per Nucleon NUCLEAR REACTIONS Ag, Br(16O, X), E ≈ 210 MeV/nucleon; Ag, Br(36Ar, X), E ≈ 65 MeV/nucleon; measured fragment charge, emission angle; deduced fragmentation mechanism features. Additional momentum flow tensor analysis.
doi: 10.1016/0375-9474(92)90693-E
1992BA69 Nucl.Phys. A545, 213c (1992) H.W.Barz, J.P.Bondorf, A.S.Botwina, R.Donangelo, I.N.Mishustin, H.Schulz, K.Sneppen Gating in Fragmentation Processes ( Question ) NUCLEAR REACTIONS 232Th(40Ar, X), E=44, 77 MeV/nucleon; calculated neutron multiplicity distributions. Equilibrium approach to fragmentation, ergodicity assumption. NUCLEAR STRUCTURE A=272; Z=108; calculated fission fragment multiplicity distribution. Equilibrium approach to fragmentation, ergodicity assumption.
doi: 10.1016/0375-9474(92)90460-2
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
1992PH02 Phys.Lett. 291B, 7 (1992) L.Phair, M.A.Lisa, D.R.Bowman, C.K.Gelbke, W.G.Gong, Y.D.Kim, W.G.Lynch, G.F.Peaslee, H.Schulz, R.T.de Souza, M.B.Tsang, F.Zhu Fluctuations in Multifragment Decays NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; analyzed charged particle distributions; deduced inconsistency with intermittency signals assumption.
doi: 10.1016/0370-2693(92)90111-G
1991BA41 Nucl.Phys. A531, 453 (1991) H.W.Barz, J.P.Bondorf, R.Donangelo, R.Elmer, F.S.Hansen, B.Jakobsson, L.Karlsson, H.Nifenecker, H.Schulz, F.Schussler, K.Sneppen, K.Soderstrom Flow Effects in Intermediate-Energy Nuclear Collisions NUCLEAR REACTIONS Ag, Br(36Ar, X), E ≈ 50-80 MeV/nucleon; Ag, Br(16O, X), E ≈ 200-220 MeV/nucleon; analyzed fragment average kinetic energy vs charge; deduced reaction mechanism features, per nucleon flow energy. Statistical multi-fragmentation model.
doi: 10.1016/0375-9474(91)90621-C
1991BA47 Phys.Lett. 267B, 317 (1991) H.W.Barz, D.A.Cebra, H.Schulz, G.D.Westfall Event Shape Analysis of the Reaction 40Ar + 51V within a Prompt Multifragmentation Scenario NUCLEAR REACTIONS 51V(40Ar, X), E=35-85 MeV/nucleon; analyzed data; deduced multifragmentation mechanism. Statistical fragmentation followed by sequential decay.
doi: 10.1016/0370-2693(91)90938-M
1990BA26 Phys.Lett. 244B, 161 (1990) H.W.Barz, J.P.Bondorf, K.Sneppen, H.Schulz Velocity Correlations in the Multifragmentation Scenario NUCLEAR REACTIONS Ag(16O, X), E=84 MeV/nucleon; calculated fragment relative velocity distribution function; deduced correlation data need. Primordial hot fragment evaporation.
doi: 10.1016/0370-2693(90)90047-A
1990RO12 Fiz.Elem.Chastits At.Yadra 21, 364 (1990); Sov.J.Part.Nucl 21, 153 (1990) G.Ropke, H.Schulz, K.K.Gudima, V.D.Toneev Dynamical Approaches to Heavy-Ion Collisions at Intermediate Energies NUCLEAR REACTIONS 40Ca(40Ca, X), E=50-400 MeV/nucleon; calculated nucleon density evolution. Various dynamical methods.
1989BA09 Phys.Rev. C39, 1176 (1989) H.W.Barz, H.Schulz, J.P.Bondorf, R.Donangelo, K.Sneppen Multiplicity Distributions for the Reaction 40Ar on 27Al Calculated in the Statistical Multifragmentation Model NUCLEAR REACTIONS 27Al(40Ar, X), E=25, 65 MeV/nucleon; calculated intermediate mass fragment production σ vs multiplicity. Statistical multifragmentation model.
doi: 10.1103/PhysRevC.39.1176
1988BA28 Phys.Rev. C37, 2910 (1988) H.W.Barz, J.P.Bondorf, J.A.Lopez, H.Schulz Emission Temperature and Source Radii Inferred from Two-Particle Correlation Measurements in Nuclear Collisions NUCLEAR REACTIONS 197Au(40Ar, X), E=60 MeV/nucleon; calculated fragment yield vs mass distribution. Kr(p, 12C), E not given; calculated σ(E(12C)). Statistical multi-fragmentation model.
doi: 10.1103/PhysRevC.37.2910
1988BA53 Phys.Lett. 211B, 10 (1988) H.W.Barz, H.Schulz, J.P.Bondorf, J.Lopez, K.Sneppen On Isotopic Yield Ratios of Complex Fragments from Heavy Ion Induced Reactions NUCLEAR STRUCTURE 58,64Ni, 108Ag, 197Au; calculated complex fragment isotope yield ratio. Statistical model.
doi: 10.1016/0370-2693(88)90797-6
1988DO12 Z.Phys. A331, 107 (1988) B.S.Dolbilkin, R.L.Kondratiev, V.P.Lisin, Sh.Khan, Th.Kihm, K.T.Knopfle, H.J.Schulz, Chenlin Wen, J.Friedrich Direct Decay of the Giant Dipole Resonance in 58,60Ni and 64Zn from (e, e'c) Experiments NUCLEAR REACTIONS 58,60Ni, 64Zn(e, e'p), (e, e'α), E=137.2 MeV; measured e'(particle)-coin spectra. 59,57Co, 63Cu deduced level population strengths.
1987BA02 Nucl.Phys. A462, 742 (1987) H.W.Barz, J.P.Bondorf, H.Schulz Energy Spectra of Fragments Calculated with the Model of the Statistical Multifragmentation of Nuclei NUCLEAR REACTIONS Kr, Xe(p, X), E=80-350 GeV; calculated σ(fragment E) for X=12C, 16O. Statistical multi-fragmentation model.
doi: 10.1016/0375-9474(87)90574-4
1987BA03 Phys.Lett. 184B, 125 (1987) H.W.Barz, J.P.Bondorf, H.Schulz On the Limiting Excitation Energy of Nuclei NUCLEAR STRUCTURE A=100; calculated entropy, temperature, multiplicity. Multi-fragmentation model.
doi: 10.1016/0370-2693(87)90554-5
1987BA31 Phys.Lett. 191B, 232 (1987) H.W.Barz, J.P.Bondorf, R.Donangelo, H.Schulz, K.Sneppen Isotope Distribution in Nuclear Multifragmentation NUCLEAR REACTIONS Kr(p, X), E=3.7, 6.5, 8 MeV/nucleon; calculated isotope distribution for mass ≤ 35. Statistical multi-fragmentation model.
doi: 10.1016/0370-2693(87)90245-0
1987BA48 Phys.Lett. 194B, 459 (1987) H.W.Barz, J.Bondorf, R.Donangelo, J.A.Lopez, H.Schulz Ternary versus Binary Fragmentation Processes NUCLEAR REACTIONS 100Mo(100Mo, X), E=12, 14.7, 18.8 MeV/nucleon; calculated ternary to binary fragmentation process ratio. Statistical multifragmentation model.
doi: 10.1016/0370-2693(87)90216-4
1987BA73 Europhys.Lett. 4, 997 (1987) H.W.Barz, J.P.Bondorf, C.Guet, J.Lopez, H.Schulz Subthreshold Pion Production and Statistical Multifragmentation in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 40Ca(40Ar, π0), E=44 MeV/nucleon; calculated σ(E(π0)). Multifragmentation model.
doi: 10.1209/0295-5075/4/9/008
1987GU05 Yad.Fiz. 45, 80 (1987) K.K.Gudima, G.Ropke, V.D.Toneev, H.Schulz Entropy of a System Formed in Heavy Ion Collisions NUCLEAR REACTIONS Ar(Ar, X), Ca(Ca, X), 93Nb(93Nb, X), E=0.4-2 GeV/nucleon; calculated entropy evolution. Cascade model.
1986AN13 Phys.Lett. 174B, 18 (1986) L.N.Andronenko, A.A.Kotov, L.A.Vaishnene, W.Neubert, H.W.Barz, J.P.Bondorf, R.Donangelo, H.Schulz Mass Yield Distributions for 1 GeV Proton-Induced Nuclear Reactions on Ni and Ag NUCLEAR REACTIONS Ni, Ag(p, X), E=1 GeV; calculated inclusive fragment σ vs mass.
doi: 10.1016/0370-2693(86)91120-2
1986BA70 Nucl.Phys. A460, 714 (1986) H.W.Barz, J.P.Bondorf, H.Schulz, L.N.Andronenko, A.A.Kotov, L.A.Vaishnene, W.Neubert Onset of Multifragmentation Dominance at 1 GeV Proton-Induced Nuclear Reaction for Target Nuclei with A ≤ 160 RADIOACTIVITY 252Cf(SF); measured fission (fragment)(fragment)(θ); deduced longitudinal momentum transfer, multifragmentation dominance. NUCLEAR REACTIONS Ag, Sm, U(p, F), E=1 GeV; measured fission (fragment)(fragment)(θ); deduced longitudinal momentum transfer, multifragmentation dominance.
doi: 10.1016/0375-9474(86)90533-6
1985RO10 Phys.Rev. C31, 1556 (1985) G.Ropke, H.Schulz, L.N.Andronenko, A.A.Kotov, W.Neubert, E.N.Volnin Depletion of Light Cluster Production in 1 GeV Proton-Nucleus Collisions NUCLEAR REACTIONS Ag(p, X), E=1 GeV; measured inclusive fragment production σ vs mass.
doi: 10.1103/PhysRevC.31.1556
1984RO19 Nucl.Phys. A424, 594 (1984) Particle Clustering and Mott Transitions in Hot Nuclear Matter at Finite Temperature (III). Heavy Cluster Abundances and Coulomb Interaction NUCLEAR STRUCTURE A=1-16; calculated cluster abundance vs mass. Debye-Thomas-Fermi approach, Coulomb interaction.
doi: 10.1016/0375-9474(84)90011-3
1981MU17 Fiz.Elem.Chastits At.Yadra 12, 1001 (1981); Sov.J.Part.Nucl. 12, 403 (1981) Quasiclassical Theory of Rapid Rotation NUCLEAR STRUCTURE A=40-100; calculated density distribution, shape dependence on spin. Rotating nuclei, quasiclassical theory.
1978EF01 Nucl.Phys. A309, 344 (1978) On a Simple Energy-Dependent Boundary Condition Model and the Binding Energy of the Triton NUCLEAR STRUCTURE 3H; calculated binding energy. Energy-dependent boundary condition model.
doi: 10.1016/0375-9474(78)90486-4
1976PE13 Yad.Fiz. 24, 313 (1976); Sov.J.Nucl.Phys. 24, 163 (1977) Dynamical Effects in Interactions of Complex Nuclei NUCLEAR REACTIONS 208Pb, 146Nd, 152Sm(16O, X), 208Pb, 232Th(84Kr, X); calculated Coulomb barrier.
1974BA57 Phys.Scr. 10, 115 (1974) J.Bang, V.E.Bunakov, F.A.Gareev, R.M.Jamalejev, H.Schulz On the Possibilities in Calculations of Stripping Form Factors NUCLEAR REACTIONS 42Ca(p, d); calculated σ(Ed, θ), form factors.
doi: 10.1088/0031-8949/10/3/004
1974BA65 Yad.Fiz. 20, 346 (1974); Sov.J.Nucl.Phys. 20, 184 (1975) Calculation of Form Factors for Two-Nucleon Cluster Transfer NUCLEAR REACTIONS 12C(t, p); calculated σ(Ep, θ), form factors.
1974BA85 Fiz.Elem.Chastits At.Yadra 5, 263 (1974); Sov.J.Particles Nucl. 5, 103 (1974) J.Bang, V.E.Bunakov, F.A.Gareev, H.Schulz Configuration Mixing Effects in Single-Nucleon Transfer Reactions NUCLEAR REACTIONS 42Ca(p, d), E=26.5 MeV; calculated form factors. 176Yb(d, p), E=121 MeV; calculated σ(Ed, θ). 170Er(d, p); calculated σ.
1973GA12 Yad.Fiz. 17, 761 (1973); Sov.J.Nucl.Phys. 17, 397 (1974) F.A.Gareev, M.Baznat, H.J.Wiebicke, H.Schulz One-Nucleon Transfer Reactions to Quasi-Intersecting Levels 1/2+ [660] and 1/2+[400], 3/2+ [651] and 3/2+ [402] NUCLEAR REACTIONS 160Gd, 164Dy(d, t); measured nothing, calculated σ(θ). 159Gd, 163Dy levels deduced β.
1973GA24 Nucl.Phys. A215, 570 (1973) F.A.Gareev, R.M.Jamalejev, H.Schulz, J.Bang A Method for Calculation of Stripping Form Factors in CCBA NUCLEAR REACTIONS 52Cr(d, p), E=7.5 MeV; calculated σ(Ep, θ). 53Cr calculated levels, J, π, L.
doi: 10.1016/0375-9474(73)90489-2
1972BE19 JINR-E4-6353 (1972) Calculation of the Body-Form Factor for the 3He and 3H Nuclei by Means Of the Modified BKR Potential NUCLEAR STRUCTURE 3H, 3He; calculated charge form factors; analyzed singlet, triplet N-N interaction contributions.
1972GA06 Nucl.Phys. A182, 625 (1972) S.I.Gabrakov, A.A.Kuliev, N.I.Pyatov, D.I.Salamov, H.Schulz Collective 1+ States in Doubly Even Deformed Nuclei NUCLEAR STRUCTURE 168Er; calculated levels, B(M1). Tamm-dankoff, RPA.
doi: 10.1016/0375-9474(72)90541-6
1972KU15 Nucl.Phys. A189, 257 (1972) A.B.Kurepin, H.Schulz, H.J.Wiebicke Coupled-Channel Analysis of 12 MeV Proton Scattering on 148,154Sm NUCLEAR REACTIONS 148,154Sm(p, p), (p, p'), E=12 MeV; analyzed σ(θ). 148,154Sm deduced deformation parameters β2, β4. Coupled-channel formalism.
doi: 10.1016/0375-9474(72)90294-1
1972SC04 Nucl.Phys. A180, 625 (1972) H.Schulz, H.J.Wiebicke, F.A.Gareev Deuteron Stripping on Deformed Nuclei NUCLEAR REACTIONS 24Mg, 176Yb(d, p), E=13.5, 12 MeV; calculated σ(θ). Coupled-channel DWBA.
doi: 10.1016/0375-9474(72)90884-6
1970SC32 Nucl.Phys. A159, 324 (1970) H.Schulz, H.J.Wiebicke, R.Fulle, D.Netzband, K.Schlott A Generalized DWBA Model Applied to the 24Mg(d, p)25Mg Reaction at E = 13.5 MeV NUCLEAR REACTIONS 24Mg(d, p), E=13.5 MeV; calculated σ(θ). DWBA.
doi: 10.1016/0375-9474(70)90045-X
1967SC16 Nucl.Phys. A101, 577 (1967) H.Schulz, H.J.Wiebicke, R.Reif Single-Particle States in Non-Local Potentials and Direct Nuclear Reactions
doi: 10.1016/0375-9474(67)90653-7
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