1994
DOI: 10.1103/physrevc.50.2841
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Large-space shell-model calculations for light nuclei

Abstract: An effective two-body interaction is constructed from a new Reidlike N N potential for a large no-core space consisting of six major shells and is used to generate the shell-model properties for light nuclei from A=2 to 6. For practical reasons, the model space is partially truncated for A=6. Binding energies and other physical observables are calculated and they compare favorably with experiment.

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Cited by 82 publications
(158 citation statements)
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“…Unlike in the original paper [13], we introduce a shift ∆, as the G-matrix cannot be evaluated for the energy ε α , using the reference matrix method (8). Note that (12) is the interaction used in the previous no-core shell-model studies [4][5][6]8] with ∆ treated as a free parameter. One can also use the alternative procedure, usually called the vertex-renormalization approach, which can be obtained from Eq.…”
Section: Shell Model Hamiltonian and Starting-energy Independent mentioning
confidence: 99%
See 3 more Smart Citations
“…Unlike in the original paper [13], we introduce a shift ∆, as the G-matrix cannot be evaluated for the energy ε α , using the reference matrix method (8). Note that (12) is the interaction used in the previous no-core shell-model studies [4][5][6]8] with ∆ treated as a free parameter. One can also use the alternative procedure, usually called the vertex-renormalization approach, which can be obtained from Eq.…”
Section: Shell Model Hamiltonian and Starting-energy Independent mentioning
confidence: 99%
“…Large-basis no-core shell-model calculations have recently been performed [1][2][3][4][5][6][7][8]. In these calculations all nucleons are active, which simplifies the effective interaction as no hole states are present.…”
Section: Introductionmentioning
confidence: 99%
See 2 more Smart Citations
“…Large-basis no-core shell-model calculations have recently been performed [1][2][3][4][5][6][7][8][9][10][11]. In these calculations all nucleons are active, which simplifies the effective interaction as no hole states are present.…”
Section: Introductionmentioning
confidence: 99%