Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Results 1-3 of 88
Page 39
... proton optical potential , accounting for the difference in ki- netic energy of neutrons and protons in the region of the nucleus . This correction is necessary because the nuclear part of the opti- cal potential is energy dependent and ...
... proton optical potential , accounting for the difference in ki- netic energy of neutrons and protons in the region of the nucleus . This correction is necessary because the nuclear part of the opti- cal potential is energy dependent and ...
Page 102
... neutron and proton scattering are compared with data36,37 in Figs . 18 and 19. The proton transition density was a Tassie - model form , normalized to the B ( E2 ) determined from Coulomb excitation38 . The solid curves show the ...
... neutron and proton scattering are compared with data36,37 in Figs . 18 and 19. The proton transition density was a Tassie - model form , normalized to the B ( E2 ) determined from Coulomb excitation38 . The solid curves show the ...
Page 195
... neutron component . The gross relationships between the proton and neutron components are characterized by collective motion in which the protons and neutrons move with equal amplitude in phase ( the isoscalar mode ) and out of phase ...
... neutron component . The gross relationships between the proton and neutron components are characterized by collective motion in which the protons and neutrons move with equal amplitude in phase ( the isoscalar mode ) and out of phase ...
Contents
Implication of microscopic reaction analyses below | 14 |
Test of effective interactions for nucleon scattering | 90 |
SESSION | 301 |
Copyright | |
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1985 American Institute analysis angular distributions average calculations central potential channels charged particle conference topics Copyright 1985 American coupling cyclotron deformation detectors Deuterons effective interaction elastic and inelastic energy dependence energy range energy resolution experimental Fermi gas fission flight path imaginary potential inelastic scattering Institute of Physics intermediate isospin isovector Laboratory Lett level density low energy magnet matrix elements mb/sr measurements microscopic neutron and proton neutron beam neutron energy Neutron Facilities neutron scattering neutron source Nucl nuclear structure nuclei nucleon obtained Ohio University optical model optical potential parameters parity peak phenomenological Phys pions Polarized intensity probe proton proton and neutron pulse R-matrix ratio reaction related to conference resonance s-process s-wave sensitivity shell shell model shown in Fig solid angle Spectrometers spin strength studies swinger tion total cross section transition densities values volume integrals wave functions width