Abstract
Microscopic proton two-particle neutron two-hole shell-model calculations have been performed for the nucleus $_{52}^{132}\mathrm{Te}_{80}$. Evidence results for the existence of a weak-coupling pattern obtained by coupling nuclear low-lying levels in $_{52}^{134}\mathrm{Te}_{82}$ and $_{50}^{130}\mathrm{Sn}_{80}$. Electromagnetic properties for the most important low-lying levels in $_{52}^{132}\mathrm{Te}_{80}$ are also calculated and compared with existing experimental data. The limitations of proton two-particle- (neutron two-hole-) core coupling calculations are also exhibited when proton and/or neutron number only deviates from closed shell configurations by a small (\ifmmode\pm\else\textpm\fi{}2) number.NUCLEAR STRUCTURE $_{52}^{132}\mathrm{Te}_{80}$ shell-model 2p - 2h calculations, electromagnetic properties, ${T}_{\frac{1}{2}}$, comparison with 2p (2h)-core coupling macroscopic calculations.
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