Realistic single-particle K-matrix for deformed and fissioning nuclei
Journal Article
·
· Nuclear Physics. A
A low-order approximation to the Brueckner-- Goldman densitydependent single-particle reaction matrix is used. The effective single-particle Hamiltonian is nonlocal and depends on a smeared density. The isospin depcndence, spin- orbit, center-of-mass, and Coulomb corrections are performed in a realistic manner. A large orthogonal (spherical/deformed) oscillator basis or a nonorthogonal basis consisting of two overlapping harmonic oscillators is used to diagonalize the Hamiltonian in an iterative self-consistent scheme. The nonlocality, the density-dependent terms, and the Coulomb terms are expanded in Gaussian forms by using a linearized high-speed technique. Results for the total BE, s.p. energies. quadrupole moments, radii, and proton and neutron density distributions of light nuclei are found to be in good agreement with experiment. Fission effects in the reactions /sup 8/Be yields alpha + alpha and /sup 32/ S yields /sup 16/0 + /sup 16/O are studied. (auth)
- Research Organization:
- Duke Univ., Durham, NC
- Sponsoring Organization:
- USDOE
- NSA Number:
- NSA-29-006622
- OSTI ID:
- 4379053
- Journal Information:
- Nuclear Physics. A, Journal Name: Nuclear Physics. A Journal Issue: 1 Vol. 215; ISSN 0375-9474
- Publisher:
- Elsevier
- Country of Publication:
- Country unknown/Code not available
- Language:
- English
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PROPERTIES OF FINITE NUCLEI
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Sat Dec 31 23:00:00 EST 1960
· Physical Review (U.S.) Superseded in part by Phys. Rev. A, Phys. Rev. B: Solid State, Phys. Rev. C, and Phys. Rev. D
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OSTI ID:4120856
PROPERTIES OF FINITE NUCLEI
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Mon Jan 14 23:00:00 EST 1963
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Structure of the giant multipole resonances in /sup 20/Ne and /sup 28/Si
Journal Article
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Tue Sep 01 00:00:00 EDT 1981
· Phys. Rev. C; (United States)
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Related Subjects
*BERYLLIUM 8-- QUADRUPOLE MOMENTS
*CALCIUM 40-- QUADRUPOLE MOMENTS
*CALCIUM 48-- QUADRUPOLE MOMENTS
*CARBON 12-- QUADRUPOLE MOMENTS
*HELIUM 4-- QUADRUPOLE MOMENTS
*NEON 20-- QUADRUPOLE MOMENTS
*OXYGEN 16-- QUADRUPOLE MOMENTS
*SILICON 28-- QUADRUPOLE MOMENTS
*SULFUR 32-- QUADRUPOLE MOMENTS
COULOMB CORRECTION
DEFORMED NUCLEI
DISTRIBUTION
ENERGY LEVELS
FISSION
GAUSS FUNCTION
HAMILTONIANS
HARMONIC OSCILLATOR MODELS
ISOSPIN
K MATRIX
L-S COUPLING
N68212 --Physics (Nuclear
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A <= 5--Mass
Abundance & Binding Energy
N68312 --Physics (Nuclear
Theoretical)--Nuclear Properties & Reactions
6 <= A <= 19--Mass
Abundance & Binding Energy
N68412 --Physics (Nuclear
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20 <= A <= 38--Mass
Abundance & Binding Energy
N68512 --Physics (Nuclear
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39 <= A <= 58--Mass
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N69230* --Physics (Nuclear)--Nuclear Theory--Nuclear Reactions & Scattering
NEUTRONS
NUCLEAR REACTIONS
PROTONS
SINGLE-PARTICLE MODEL
*CALCIUM 40-- QUADRUPOLE MOMENTS
*CALCIUM 48-- QUADRUPOLE MOMENTS
*CARBON 12-- QUADRUPOLE MOMENTS
*HELIUM 4-- QUADRUPOLE MOMENTS
*NEON 20-- QUADRUPOLE MOMENTS
*OXYGEN 16-- QUADRUPOLE MOMENTS
*SILICON 28-- QUADRUPOLE MOMENTS
*SULFUR 32-- QUADRUPOLE MOMENTS
COULOMB CORRECTION
DEFORMED NUCLEI
DISTRIBUTION
ENERGY LEVELS
FISSION
GAUSS FUNCTION
HAMILTONIANS
HARMONIC OSCILLATOR MODELS
ISOSPIN
K MATRIX
L-S COUPLING
N68212 --Physics (Nuclear
Theoretical)--Nuclear Properties & Reactions
A <= 5--Mass
Abundance & Binding Energy
N68312 --Physics (Nuclear
Theoretical)--Nuclear Properties & Reactions
6 <= A <= 19--Mass
Abundance & Binding Energy
N68412 --Physics (Nuclear
Theoretical)--Nuclear Properties & Reactions
20 <= A <= 38--Mass
Abundance & Binding Energy
N68512 --Physics (Nuclear
Theoretical)--Nuclear Properties & Reactions
39 <= A <= 58--Mass
Abundance & Binding Energy
N69230* --Physics (Nuclear)--Nuclear Theory--Nuclear Reactions & Scattering
NEUTRONS
NUCLEAR REACTIONS
PROTONS
SINGLE-PARTICLE MODEL