2001
DOI: 10.1103/physrevc.64.014312
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Shell model study of neutron-rich nuclei near132Sn

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Cited by 49 publications
(58 citation statements)
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“…The values obtained are close to our microscopic results, but the fitted operator does not include the tensortype correction obtained microscopically. The calculations of Sarkar and Sarkar [3] are based on a fitted interaction for N = 82 plus a renormalized G matrix extrapolated from the region of 208 Pb for N > 82. Their wavefunctions for N = 82 should be comparable in accuracy to the present model.…”
Section: Examination Ofmentioning
confidence: 99%
See 1 more Smart Citation
“…The values obtained are close to our microscopic results, but the fitted operator does not include the tensortype correction obtained microscopically. The calculations of Sarkar and Sarkar [3] are based on a fitted interaction for N = 82 plus a renormalized G matrix extrapolated from the region of 208 Pb for N > 82. Their wavefunctions for N = 82 should be comparable in accuracy to the present model.…”
Section: Examination Ofmentioning
confidence: 99%
“…[1] for details) provided reasonable agreement with energy spectra and B(E2) in N = 80 and N = 82 Sn and Te isotones but failed to explain the B(E2) value in 136 Te. Magnetic moments were calculated for 134 Te, 136,137 Xe, and 137 Cs by Sarkar and Sarkar [3] with the KH5082 and CW5082 interactions fitted for 208 Pb and scaled to the 132 Sn region, and with empirical effective single-particle g factors. Shell Sn.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, the nuclides 135 I, 135 Te, 135 Sb, and 135 Sn remain an excellent testing ground for descriptions of nuclei with only three nucleons present beyond the 132 Sn double shell closure. Relatively detailed data have been available for some time for 135 I and 135 Te [5,6].…”
Section: Introductionmentioning
confidence: 99%
“…In this regard, it is of key importance the fact that, given the correspondence between the SP levels, the matrix elements of the effective interactions in 132 Sn and 208 Pb regions are expected to be proportional to one another. This has stimulated several shellmodel calculations on nuclei around 132 Sn [12,13,14] with two-body effective interactions originating from the modified version [15] of the Kuo-Herling interaction [16], originally designed for the Pb region. However, these attempts have not been successful, as discussed for instance in [14], where the conclusion was drawn that a consistent Hamiltonian for the three nuclei beyond the N = 82 shell closure, 134 Sb, 135 Sb, and 134 Sn, had yet to be found.…”
mentioning
confidence: 99%