Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 54
... deuteron beam to be " transferred " to the neutrons emitted into the cone near 0 ° . In our case at TUNL the deuteron beam typically is about 65 % polarized , so we can obtain an intense , clean beam of about 60 % polarization . Of ...
... deuteron beam to be " transferred " to the neutrons emitted into the cone near 0 ° . In our case at TUNL the deuteron beam typically is about 65 % polarized , so we can obtain an intense , clean beam of about 60 % polarization . Of ...
Page 280
... deuteron beam . Parameters for 25 MeV neutrons are 13 ) essentially those used by Mellema in his study of neutron scattering from As the deuteron energy increases , energy and angle straggling in the foil decrease , energy loss in the ...
... deuteron beam . Parameters for 25 MeV neutrons are 13 ) essentially those used by Mellema in his study of neutron scattering from As the deuteron energy increases , energy and angle straggling in the foil decrease , energy loss in the ...
Page 300
... deuteron 16.7 23.6 37.3 52.8 The B - fields are large enough that a superconducting solenoid will be necessary at the highest energies , particularly for deuterons . The field in a superconducting solenoid can be changed in times short ...
... deuteron 16.7 23.6 37.3 52.8 The B - fields are large enough that a superconducting solenoid will be necessary at the highest energies , particularly for deuterons . The field in a superconducting solenoid can be changed in times short ...
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