Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 485
... s - process in which the Fe nuclei which serve as the seed for the s - process were exposed to a superposition of exponentially decreasing neutron fluences . This phenomenological model was rather Y S successful in describing the ...
... s - process in which the Fe nuclei which serve as the seed for the s - process were exposed to a superposition of exponentially decreasing neutron fluences . This phenomenological model was rather Y S successful in describing the ...
Page 511
... s - process on curve in the framework of models which produce an exponential distribution of exposures by periodic time - dependent neutron irradiations . The optimum parameter space , defined by the best fit to the solar - system oN ...
... s - process on curve in the framework of models which produce an exponential distribution of exposures by periodic time - dependent neutron irradiations . The optimum parameter space , defined by the best fit to the solar - system oN ...
Page 518
... s - process path follows the valley of B- stability , as shown in Figure 1. The s - process path ends where a instability sets in at Bismuth . In contrast , for the classical r , or rapid , process , the neutron capture rate is much ...
... s - process path follows the valley of B- stability , as shown in Figure 1. The s - process path ends where a instability sets in at Bismuth . In contrast , for the classical r , or rapid , process , the neutron capture rate is much ...
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