1997
DOI: 10.1006/ndsh.1997.0009
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Nuclear Data Sheets for A ;eq 124

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Cited by 69 publications
(51 citation statements)
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“…The 5 − states are µs isomers in 116 Sn [46] and 124 Sn [47] only, but these are ns isomers in the other even-A 118-122,128-130 Sn nuclei [48][49][50][51][52] because they can decay by E1 transitions to the 4 + states lying just below them. However, in the odd-A isotopes, the 19/2 + states are all isomeric in the µs range because each of them comes below the (4 + ⊗ νh 11/2 )17/2 − and 19/2 − states.…”
Section: Level Systematicsmentioning
confidence: 99%
“…The 5 − states are µs isomers in 116 Sn [46] and 124 Sn [47] only, but these are ns isomers in the other even-A 118-122,128-130 Sn nuclei [48][49][50][51][52] because they can decay by E1 transitions to the 4 + states lying just below them. However, in the odd-A isotopes, the 19/2 + states are all isomeric in the µs range because each of them comes below the (4 + ⊗ νh 11/2 )17/2 − and 19/2 − states.…”
Section: Level Systematicsmentioning
confidence: 99%
“…First, because it was not included in the finetuning, and in addition, the experimental data available is not very clear about the first excited 0 + state, which is very important for our analysis. In particular, although the recent double-beta decay experimental studies [28][29][30] assume that this state is at 1.156 MeV excitation energy, the latest Nuclear Data Sheets [71,72] Fig. 1).…”
Section: A Energy Levelsmentioning
confidence: 99%
“…This normalization factor was used for every other measured inelastic scattering cross section. The calculations for different 2 + excited states performed using the standard collective form factor and the adopted B(E2)↑ [22,23] were able to reproduce well the experimental data. For the 1 − pygmy states, a calculation including both the Coulomb and nuclear contributions and corresponding to a form factor of GDR type is shown in Fig.…”
Section: Resultsmentioning
confidence: 64%