NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.J.Griffin Found 12 matches. 1995GR03 Nucl.Phys. A583, 257c (1995) The C(Q0( Question )) Scenario: Bound sharp positron decay, its resonant inverse, and sharp lines from [β+ + atom]
doi: 10.1016/0375-9474(94)00668-D
1992CI07 Fizika(Zagreb) B1, 51 (1992) N.Cindro, E.Betak, M.Korolija, J.J.Griffin A Microscopic Model for Calculating the Inital Number of Excitons in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 48Ti, 60Ni, 120,124Sn, 197Au, 27Al(16O, X), E=403 MeV; 48Ti, 60Ni, 120,124Sn, 197Au, 27Al(32S, X), E=504, 679 MeV; 48Ti, 60Ni, 120,124Sn, 197Au, 27Al(58Ni, X), E=876 MeV; calculated inital exciton number. Comparison with data.
1991CI05 Phys.Rev.Lett. 66, 868 (1991) N.Cindro, M.Korolija, E.Betak, J.J.Griffin Early Stages of Nucleus-Nucleus Collisions: A microscopic calculation of the initial number of degrees of freedom NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(16O, X), (32S, X), (58Ni, X), E=403-876 MeV; calculated preequilibrium nucleon emission initial degrees of freedom. Microscopic model.
doi: 10.1103/PhysRevLett.66.868
1990DW01 Phys.Scr. 42, 406 (1990) M.Dworzecka, M.Zielinska-Pfabe, J.J.Griffin Ambiguities in the Description of Nucleon Transfer in Deep Inelastic Scattering NUCLEAR REACTIONS 165Ho(56Fe, X), E=464 MeV; calculated fragment charge, mass distribution widths. Random walk.
doi: 10.1088/0031-8949/42/4/005
1987GR05 Z.Phys. A326, 51 (1987) J.J.Griffin, A.Lukasiak, M.Dworzecka Quantal Permeation Currents in Nuclear Heavy Ion Reactions NUCLEAR REACTIONS 238U(56Fe, X), E not given; calculated potential energy surface vs fragment mass, charge number. Quantal permeation currents.
1985GO12 Nucl.Phys. A440, 586 (1985) A.Gokmen, M.Dworzecka, J.J.Griffin Macroscopic Implications of Diverse Reaction Mechanisms in Ion-Ion Collisions NUCLEAR REACTIONS Ca(Cl, X), E=278 MeV; U, Fe(Fe, X), 238U, 165Ho(56Fe, X), E=464 MeV; calculated fragment mass, charge variances vs kinetic energy. Discrete random walk calculations.
doi: 10.1016/0375-9474(85)90247-7
1980CO15 Nucl.Phys. A348, 63 (1980) Mean Free Path of Nucleons in a Fermi Gas at Finite Temperature NUCLEAR REACTIONS 58Ni(n, n), (p, p), 40Ca, 208Pb(p, p), E not given; calculated nucleon free path. Nuclear Fermi gas, finite temperature.
doi: 10.1016/0375-9474(80)90545-X
1973GA03 Phys.Rev. C7, 590 (1973) Pauli Exclusion Effects in Reactions Involving Multinucleon Systems
doi: 10.1103/PhysRevC.7.590
1972GA16 Phys.Rev. C5, 1856 (1972) Pauli Breakup of Deuterons in O16 NUCLEAR REACTIONS 16O(d, pn), E=91, 125 MeV; calculated σ(Ep, θ(p), θ(n)); analyzed role of Pauli exclusion principle.
doi: 10.1103/PhysRevC.5.1856
1972LE09 Phys.Rev. C5, 1713 (1972) Even-Odd Effects in Precompound Emission NUCLEAR REACTIONS 116,117Sn(p, n), E=11, 12, 13, 14 MeV; analyzed even-odd effects in precompound particle emission.
doi: 10.1103/PhysRevC.5.1713
1966GR33 Phys.Rev.Lett. 17, 478 (1966) Statistical Model of Intermediate Structure NUCLEAR REACTIONS 117Sn(p, n), E=14 MeV; calculated yields; deduced a model is proposed for the formation and decay of the average compound-nuclear state in which a weak two-body residual interaction causes transitions among the eigenstates of an independent-particle Hamiltonian which lie in the region dE near the compound-nuclear excitation energy E. Comparison with available data.
doi: 10.1103/PhysRevLett.17.478
1965BR40 Phys.Rev. 139, B354 (1965) H.C.Britt, W.R.Gibbs, J.J.Griffin, R.H.Stokes (d, p-f) Angular-Correlation Study of Fission-Barrier Transition States: Energy Gap of a Highly Deformed Nucleus NUCLEAR REACTIONS, Fission 233U, 239Pu(d, pF), E=14.9 MeV; measured σ(Ep, θ(p), θ(fragment)). 234U, 240Pu deduced fission-barrier transition states.
doi: 10.1103/PhysRev.139.B354
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