1977
DOI: 10.1016/0375-9474(77)90429-8
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Alpha and 8Be cluster amplitudes and core excitations in s-d shell nuclei

Abstract: SU(3) and SU(4) recoupling are used to develop technique°for the calculation of norm and overlap matrix element°for properly antisymmetrized cluster wave function°. These techniques are illustrated in detail by the calculation of a and°13e cluster amplitude°for°fate°of a fewẽ xcitation in s-d shell nuclei. These extend earlier SU(3) strong coupling results for states of highest intrinsic deformation to all values of (~~making it possible to wlailate a-amplitudes for SU(3) weal: and intermediate coupling wave f… Show more

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Cited by 30 publications
(4 citation statements)
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“…This requires calculations of Hamiltonian ( Ô = A ĤA) and norm ( Ô = AA) kernels, which involve computations of overlaps of the type Ψ | Ô |Ψ (A properly takes into account antisymmetrization). In the SU(3)-based RGM framework of Hecht [207], the "localized" part of the kernels is reduced to calculating norm and Hamiltonian overlaps between the SU(3)-scheme RGM basis, which, e.g., for two fragments of mass number f and A − f can be written as,…”
Section: Resonating-group Methods (Rgm) In the Su(3) And Symplectic S...mentioning
confidence: 99%
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“…This requires calculations of Hamiltonian ( Ô = A ĤA) and norm ( Ô = AA) kernels, which involve computations of overlaps of the type Ψ | Ô |Ψ (A properly takes into account antisymmetrization). In the SU(3)-based RGM framework of Hecht [207], the "localized" part of the kernels is reduced to calculating norm and Hamiltonian overlaps between the SU(3)-scheme RGM basis, which, e.g., for two fragments of mass number f and A − f can be written as,…”
Section: Resonating-group Methods (Rgm) In the Su(3) And Symplectic S...mentioning
confidence: 99%
“…As emphasized and shown in Refs. [207,208], the main advantage arises from the fact that the norm overlaps (both direct and exchange terms) are diagonal in this basis and that one can avoid the complications of embedding the angular momentum. Another important feature is that once the overlaps are calculated in labframe coordinates, the translationally-invariant overlaps can be straightforwardly calculated using an U(A)× U(3) approach, which is especially suitable for the SU(3)-coupled wave functions [207].…”
Section: Resonating-group Methods (Rgm) In the Su(3) And Symplectic S...mentioning
confidence: 99%
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“…All of these features make this method particularly suitable for unified descriptions of nuclear structure and reaction observables. Following the success of the Elliott model [32,33], showing that a leading (most deformed) SU(3) shell-model configuration describes reasonably well the ground-state rotational band in intermediate-mass nuclei, the RGM has been extensively used with an SU(3) basis and its nocore shell-model extension, the symplectic Sp(3, R) basis [34][35][36]. Applications of the model with Gaussian interactions have successfully calculated α and 8 Be cluster amplitudes, spectroscopic amplitudes for heavy-fragment clusters, and sub-Coulomb 12 C+ 12 C resonances [37][38][39].…”
mentioning
confidence: 99%