\begin{document}$ ^{132} $\end{document}Sn have attracted considerable interest in both nuclear physics and nuclear astrophysics. For the particle-hole nuclei in this region, the low-lying and high core excitations have been well described by shell model calculations using the extended pairing plus multipole-multipole force model. However, there is a significant difference between experiment and theory in the high-spin level 17\begin{document}$ ^+ $\end{document} of \begin{document}$ ^{132} $\end{document}Te. We intend to illustrate this difference through monopole interactions. For this purpose, the monopole corrections between \begin{document}$\pi(\nu)0g_{7/2},~ \nu 1d_{5/2}$\end{document} and \begin{document}$ \pi(\nu)0h_{11/2} $\end{document} are investigated in \begin{document}$ ^{132-134} $\end{document}Te, \begin{document}$ ^{131-133} $\end{document}Sb, and \begin{document}$ ^{130} $\end{document}Sn. Some theoretical levels are connected to the (17\begin{document}$ ^+ $\end{document}) state of \begin{document}$ ^{132} $\end{document}Te with the monopole correction (Mc) of \begin{document}$ Mc(\nu d_{5/2},\nu h_{11/2}) $\end{document} and the quadruple-quadruple force between the proton and neutron, i.e., levels 3\begin{document}$ ^- $\end{document}(8\begin{document}$ ^- $\end{document}) in \begin{document}$ ^{130} $\end{document}Sn, level 14\begin{document}$ ^- $\end{document} in \begin{document}$ ^{132} $\end{document}Te, and level 23/2\begin{document}$ ^- $\end{document} in \begin{document}$ ^{131} $\end{document}Sb. Their observations at lower energies can confirm the datum of level (17\begin{document}$ ^+ $\end{document}) in \begin{document}$ ^{132} $\end{document}Te with an illustration of monopole effects and quadruple-quadruple force."> Monopole effects and high-spin levels in neutron-rich <sup>132</sup>Te -
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