Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 143
... REACTION AT 65.5 MeV C.M. Castaneda , J.L. Romero , F.P. Brady J.R. Drummond , T.D. Ford , B. McEachern Department of Physics and Crocker Nuclear Laboratory University of California , Davis , CA 95616 ABSTRACT The charge exchange reaction ...
... REACTION AT 65.5 MeV C.M. Castaneda , J.L. Romero , F.P. Brady J.R. Drummond , T.D. Ford , B. McEachern Department of Physics and Crocker Nuclear Laboratory University of California , Davis , CA 95616 ABSTRACT The charge exchange reaction ...
Page 282
... reaction is essentially the same as with the T ( d , n ) reaction ( Fig . 7d ) . The counting rate is more than twice as high at 25 MeV with the T ( p , n ) source ( for the same gas pressure , flight path , etc. ) and remains ...
... reaction is essentially the same as with the T ( d , n ) reaction ( Fig . 7d ) . The counting rate is more than twice as high at 25 MeV with the T ( p , n ) source ( for the same gas pressure , flight path , etc. ) and remains ...
Page 427
... reaction mechanisms and complexity in statistical phenomena that is not encountered elsewhere . Section 2 of this paper reviews the basic problems of statistical reaction theory , specifically the difficulty of averaging over ...
... reaction mechanisms and complexity in statistical phenomena that is not encountered elsewhere . Section 2 of this paper reviews the basic problems of statistical reaction theory , specifically the difficulty of averaging over ...
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