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B(E2;21+→01+)B(E2;2^{+}_{1}\rightarrow0^{+}_{1}) anomaly in 166^{166}Os

Published 9 Sep 2025 in nucl-th | (2509.07692v1)

Abstract: Recently, the very small B(E2;21<sup>+→01<sup>+)B(E2;2_{1}<sup>{+}\rightarrow0_{1}<sup>{+}) value was found in <sup>166<sup>{166}Os, which is 7(4) W.u. \textbf{and} much smaller than the values of adjacent nuclei <sup>168,170<sup>{168,170}Os, 74(13) W.u. and 97(9) W.u.. With the help of a new technique ``SU(3) analysis" and a new explanatory framework of the B(E2) anomaly, it was found that, the B(E2;21<sup>+→01<sup>+)B(E2;2_{1}<sup>{+}\rightarrow0_{1}<sup>{+}) anomaly really can exist. In this paper, we discuss the B(E2;21<sup>+→01<sup>+)B(E2;2_{1}<sup>{+}\rightarrow0_{1}<sup>{+}) anomaly in <sup>166<sup>{166}Os for the first time. Four results are used to fit the experimental data in <sup>166,168,170<sup>{166,168,170}Os successfully. This implies that the level-crossing or level-anticrossing explanation is more reasonable.

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