Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 29
... channels . The most important rearrangement channels will be the ( p , d ) or ( n , d ) pickup channels with a deuteron propagating in the intermediate states . These channels are not mutually orthogonal with the in- elastic one ...
... channels . The most important rearrangement channels will be the ( p , d ) or ( n , d ) pickup channels with a deuteron propagating in the intermediate states . These channels are not mutually orthogonal with the in- elastic one ...
Page 430
... channels with transmission coefficients T = 0.75 the distribution of partial widths Nu Gue ) for any one channel can be described as a chi - squared distribution with v . The correlation coefficient for the partial width amplitudes for ...
... channels with transmission coefficients T = 0.75 the distribution of partial widths Nu Gue ) for any one channel can be described as a chi - squared distribution with v . The correlation coefficient for the partial width amplitudes for ...
Page 431
... channel and two - channel reduced R - matrix theory ( in which the eliminated channels each satisfy the condition that Tλ ( e ) / D << 1 ) with a uniform picket - fence set of levels that То T C = 2π ( < ♪ ( c ) > / D ) / | 1 + π < I ...
... channel and two - channel reduced R - matrix theory ( in which the eliminated channels each satisfy the condition that Tλ ( e ) / D << 1 ) with a uniform picket - fence set of levels that То T C = 2π ( < ♪ ( c ) > / D ) / | 1 + π < I ...
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