7D-folding integral in a density-dependent microscopic optical model potential for nucleon-nucleus scattering
Journal Article
·
· Physical Review. C, Nuclear Physics
- Department of Physics-FCFM, University of Chile, Av. Blanco Encalada 2008, Santiago (Chile)
- CEA/DAM/DIF, F-91297 Arpajon (France)
Microscopic optical model potentials, based on density-dependent effective interactions, involve multidimensional integrals to account for the full Fermi motion of the target struck nucleon throughout the nucleus. If a spherical matter distribution is assumed, then each matrix element of the optical potential requires the evaluation of seven-dimensional integrals. In this work we provide a full account of these integrals, retaining the genuine off-shell structure of the nucleon-nucleon effective interaction. The evaluation is based on the asymptotic separation of the optical model potential for nucleon-nucleus scattering in momentum space, where the potential is split into a free t-matrix contribution and another which depends exclusively on the gradient of the density-dependent g matrix. The calculated potentials, based on the Paris nucleon-nucleon (NN) potential, are applied to proton elastic scattering from {sup 16}O and {sup 90}Zr at beam energies between 30 and 65 MeV. The results were compared with two approximations to the unabridged expression, revealing moderate differences among their scattering observables. When comparing with results based on the Argonne v{sub 18} NNpotential, these differences appear smaller than those attainable by the choice of the internucleon potential.
- OSTI ID:
- 21596757
- Journal Information:
- Physical Review. C, Nuclear Physics, Journal Name: Physical Review. C, Nuclear Physics Journal Issue: 3 Vol. 84; ISSN 0556-2813; ISSN PRVCAN
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
APPROXIMATIONS
ASYMPTOTIC SOLUTIONS
BARYONS
CALCULATION METHODS
DISTRIBUTION
ELASTIC SCATTERING
ELEMENTARY PARTICLES
ENERGY RANGE
EVEN-EVEN NUCLEI
FERMIONS
G MATRIX
HADRONS
INTERACTIONS
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
LIGHT NUCLEI
MATHEMATICAL MODELS
MATHEMATICAL SOLUTIONS
MATRICES
MEV RANGE
MEV RANGE 10-100
MILLISECONDS LIVING RADIOISOTOPES
NUCLEI
NUCLEON-NUCLEON POTENTIAL
NUCLEONS
OPTICAL MODELS
OXYGEN 16
OXYGEN ISOTOPES
POTENTIALS
PROTONS
RADIOISOTOPES
S MATRIX
SCATTERING
STABLE ISOTOPES
ZIRCONIUM 90
ZIRCONIUM ISOTOPES
APPROXIMATIONS
ASYMPTOTIC SOLUTIONS
BARYONS
CALCULATION METHODS
DISTRIBUTION
ELASTIC SCATTERING
ELEMENTARY PARTICLES
ENERGY RANGE
EVEN-EVEN NUCLEI
FERMIONS
G MATRIX
HADRONS
INTERACTIONS
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
LIGHT NUCLEI
MATHEMATICAL MODELS
MATHEMATICAL SOLUTIONS
MATRICES
MEV RANGE
MEV RANGE 10-100
MILLISECONDS LIVING RADIOISOTOPES
NUCLEI
NUCLEON-NUCLEON POTENTIAL
NUCLEONS
OPTICAL MODELS
OXYGEN 16
OXYGEN ISOTOPES
POTENTIALS
PROTONS
RADIOISOTOPES
S MATRIX
SCATTERING
STABLE ISOTOPES
ZIRCONIUM 90
ZIRCONIUM ISOTOPES