Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 359
... solid angle , completion date . QDDDDQ , 2 x 10 resolution , 12 msr solid angle , completed in 1983 . ( n , n ' ) ( n , charged particle ) ( n , Y ) ( p , n ) Other 1.3 m diameter graphite sphere neutron detector Special features of ...
... solid angle , completion date . QDDDDQ , 2 x 10 resolution , 12 msr solid angle , completed in 1983 . ( n , n ' ) ( n , charged particle ) ( n , Y ) ( p , n ) Other 1.3 m diameter graphite sphere neutron detector Special features of ...
Page 405
... solid angle of 1 sr is 109 n / sec . The peak width is then of the order of 0.2 MeV / mm target . In the production of " white beams " , thick beryllium or tantalum - targets are most suitable as production targets . The maximum flight ...
... solid angle of 1 sr is 109 n / sec . The peak width is then of the order of 0.2 MeV / mm target . In the production of " white beams " , thick beryllium or tantalum - targets are most suitable as production targets . The maximum flight ...
Page 405
... solid angle of 1 sr is 109 n / sec . The peak width is then of the order of 0.2 MeV / mm target . In the production of " white beams " , thick beryllium or tantalum - targets are most suitable as production targets . The maximum flight ...
... solid angle of 1 sr is 109 n / sec . The peak width is then of the order of 0.2 MeV / mm target . In the production of " white beams " , thick beryllium or tantalum - targets are most suitable as production targets . The maximum flight ...
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