NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 24, 2024.

Search: Author = D.H.Gross

Found 53 matches.

Back to query form



2006GR25      Eur.Phys.J. A 30, 293 (2006)

D.H.E.Gross

Nuclear multifragmentation, its relation to general physics

doi: 10.1140/epja/i2005-10317-6
Citations: PlumX Metrics


2003GR29      Phys.Lett. B 574, 186 (2003)

D.H.E.Gross

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
Citations: PlumX Metrics


2001GR04      Nucl.Phys. A681, 366c (2001)

D.H.E.Gross

Phase Transitions in ' Small ' Systems - A Challenge for Thermodynamics -

doi: 10.1016/S0375-9474(00)00540-6
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1998BO15      Phys.Rev. C58, R23 (1998)

A.S.Botvina, D.H.E.Gross

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
Citations: PlumX Metrics


1997BO30      Phys.Lett. 408B, 31 (1997)

A.S.Botvina, D.H.E.Gross

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
Citations: PlumX Metrics


1995BO13      Phys.Lett. 344B, 6 (1995)

A.S.Botvina, D.H.E.Gross

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
Citations: PlumX Metrics


1995BO24      Nucl.Phys. A592, 257 (1995)

A.S.Botvina, D.H.E.Gross

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994GR02      Nucl.Phys. A567, 317 (1994)

D.H.E.Gross, K.Sneppen

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
Citations: PlumX Metrics


1994GR17      Z.Phys. A349, 291 (1994)

D.H.E.Gross

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994SC11      Nucl.Phys. A573, 143 (1994)

O.Schapiro, D.H.E.Gross

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
Citations: PlumX Metrics


1994SC28      Nucl.Phys. A576, 428 (1994)

O.Schapiro, D.H.E.Gross

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
Citations: PlumX Metrics


1993GR04      Nucl.Phys. A553, 175c (1993)

D.H.E.Gross

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
Citations: PlumX Metrics


1993GR14      Phys.Lett. 318B, 405 (1993)

D.H.E.Gross, R.Heck

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
Citations: PlumX Metrics


1993LI05      Nucl.Phys. A554, 257 (1993)

B.-A.Li, D.H.E.Gross

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
Citations: PlumX Metrics


1993LI39      Phys.Lett. 318B, 39 (1993)

B.-A.Li, D.H.E.Gross

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1991JA01      Nucl.Phys. A524, 321 (1991)

H.R.Jaqaman, D.H.E.Gross

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1990LU03      Z.Phys. A336, 57 (1990)

L.Luo, D.H.E.Gross

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)

D.H.E.Gross, X.-Z.Zhang

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1988GR06      Phys.Lett. 203B, 26 (1988)

D.H.E.Gross

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
Citations: PlumX Metrics


1988GR19      Nucl.Phys. A488, 217c (1988)

D.H.E.Gross

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1983GR26      Phys.Lett. 130B, 131 (1983)

D.H.E.Gross, M.C.Nemes

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
Citations: PlumX Metrics


1983HA09      Z.Phys. A311, 131 (1983)

K.M.Hartmann, D.H.E.Gross

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
Citations: PlumX Metrics


1982GR04      Phys.Lett. 110B, 31 (1982)

D.H.E.Gross, L.Satpathy

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
Citations: PlumX Metrics


1981FR06      Z.Phys. A299, 369 (1981)

P.Frobrich, D.H.E.Gross

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
Citations: PlumX Metrics


1980BR29      Z.Phys. A298, 91 (1980)

U.Brosa, D.H.E.Gross

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
Citations: PlumX Metrics


1977GR07      Phys.Lett. 67B, 1 (1977)

D.H.E.Gross, J.Wilczynski

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1974GR05      Phys.Lett. 48B, 302 (1974)

D.H.E.Gross, H.Kalinowski

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
Citations: PlumX Metrics


1972GR49      Phys.Lett. 42B, 41 (1972)

D.H.E.Gross

The Statistical Model of Nuclei and its Relation to the Strutinsky Averaging Method

doi: 10.1016/0370-2693(72)90710-1
Citations: PlumX Metrics


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
Citations: PlumX Metrics


Back to query form