Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 282
... detectors . Annand et al . have shown that a 6.8 & detector can be built with timing properties only slightly inferior to the 2.9 & detector used at 26 MeV ( and assumed in the calculations of Table I ) . A 11.6 & detector was ...
... detectors . Annand et al . have shown that a 6.8 & detector can be built with timing properties only slightly inferior to the 2.9 & detector used at 26 MeV ( and assumed in the calculations of Table I ) . A 11.6 & detector was ...
Page 378
... detector . DETECTOR The detectors for ( n , n ) can be of the same kind currently being used for ( p , n ) at IUCF . These detectors , described elsewhere , 3,4 are meter long bars of plastic scintillator with photomultiplier tubes at ...
... detector . DETECTOR The detectors for ( n , n ) can be of the same kind currently being used for ( p , n ) at IUCF . These detectors , described elsewhere , 3,4 are meter long bars of plastic scintillator with photomultiplier tubes at ...
Page 384
... detectors and where total energy detectors are used worsen the resolution as well as produce backgrounds at lower energies . Local shielding of the detectors as well as the sources is the most economical way of reducing backgrounds in ...
... detectors and where total energy detectors are used worsen the resolution as well as produce backgrounds at lower energies . Local shielding of the detectors as well as the sources is the most economical way of reducing backgrounds in ...
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