Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 304
... resonance at 0.956 MeV and no s - wave resonances were found . Although several other small resonances were observed , their spins and parities could not be determined . Divadeenam et al.2 calculated the energies and strengths of ...
... resonance at 0.956 MeV and no s - wave resonances were found . Although several other small resonances were observed , their spins and parities could not be determined . Divadeenam et al.2 calculated the energies and strengths of ...
Page 417
... resonance angle , which now becomes the important physical observable rather than the customary resonance angular momentum . At each angle the energy dependence is given by the same resonance formula dependent upon ER This energy ...
... resonance angle , which now becomes the important physical observable rather than the customary resonance angular momentum . At each angle the energy dependence is given by the same resonance formula dependent upon ER This energy ...
Page 437
... resonance region , these being used in eq . ( 15 ) for the calculation of even - 1 and odd - 1 transmission coefficients respectively . Transmission coefficients for electromagnetic radiation are based on the giant dipole resonance ...
... resonance region , these being used in eq . ( 15 ) for the calculation of even - 1 and odd - 1 transmission coefficients respectively . Transmission coefficients for electromagnetic radiation are based on the giant dipole resonance ...
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