Neutron-Nucleus Collisions: A Probe of Nuclear StructureRapaport |
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Page 139
... Isovector 0 0 ̄ ( 1/2 ′′ → 1 / 2 * ) transitions have been studied by the charge - exchange ( p , n ) reactions on 13,14C and 160 at Ep 35 MeV by means of the high - resolution neutron time - of - flight tech- nique . Angular ...
... Isovector 0 0 ̄ ( 1/2 ′′ → 1 / 2 * ) transitions have been studied by the charge - exchange ( p , n ) reactions on 13,14C and 160 at Ep 35 MeV by means of the high - resolution neutron time - of - flight tech- nique . Angular ...
Page 146
... isovector modes in nuclei reveal the role of isospin- as well as spin - isospin degrees of freedom in nuclear structure . Implications of the giant dipole- and isovector monopole oscillations for the equation of state of asymmetric ...
... isovector modes in nuclei reveal the role of isospin- as well as spin - isospin degrees of freedom in nuclear structure . Implications of the giant dipole- and isovector monopole oscillations for the equation of state of asymmetric ...
Page 529
... isovector potential U , is given by - U1 = · ( Up - U ) / 2 € n = ( 1 ) where the U's are the optical potentials for protons and neutrons and € = ( N - Z ) / A . The isovector potential U1 V1 + iW1 , and the OMP U = V + iW , both have ...
... isovector potential U , is given by - U1 = · ( Up - U ) / 2 € n = ( 1 ) where the U's are the optical potentials for protons and neutrons and € = ( N - Z ) / A . The isovector potential U1 V1 + iW1 , and the OMP U = V + iW , both have ...
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