Back to Search Start Over

Identification of the Lowest $T=2$, $J^{\pi=}0^+$ Isobaric Analog State in $^{52}$Co and Its Impact on the Understanding of $\beta$-Decay Properties of $^{52}$Ni

Authors :
Xu, X.
Zhang, P.
Shuai, P.
Chen, R. J.
Yan, X. L.
Zhang, Y. H.
Wang, M.
Litvinov, Yu. A.
Xu, H. S.
Bao, T.
Chen, X. C.
Chen, H.
Fu, C. Y.
Kubono, S.
Lam, Y. H.
Liu, D. W.
Mao, R. S.
Ma, X. W.
Sun, M. Z.
Tu, X. L.
Xing, Y. M.
Yang, J. C.
Yuan, Y. J.
Zeng, Q.
Zhou, X.
Zhou, X. H.
Zhan, W. L.
Litvinov, S.
Blaum, K.
Audi, G.
Uesaka, T.
Yamaguchi, Y.
Yamaguchi, T.
Ozawa, A.
Sun, B. H.
Sun, Y.
Dai, A. C.
Xu, F. R.
Source :
Phys. Rev. Lett. 117, 182503 (2016)
Publication Year :
2016

Abstract

Masses of $^{52g,52m}$Co were measured for the first time with an accuracy of $\sim 10$ keV, an unprecedented precision reached for short-lived nuclei in the isochronous mass spectrometry. Combining our results with the previous $\beta$-$\gamma$ measurements of $^{52}$Ni, the $T=2$, $J^{\pi}=0^+$ isobaric analog state (IAS) in $^{52}$Co was newly assigned, questioning the conventional identification of IASs from the $\beta$-delayed proton emissions. Using our energy of the IAS in $^{52}$Co, the masses of the $T=2$ multiplet fit well into the Isobaric Multiplet Mass Equation. We find that the IAS in $^{52}$Co decays predominantly via $\gamma$ transitions while the proton emission is negligibly small. According to our large-scale shell model calculations, this phenomenon has been interpreted to be due to very low isospin mixing in the IAS.<br />Comment: Accepted for publication in PRL. 5 pages, 2figures

Subjects

Subjects :
Nuclear Experiment

Details

Database :
arXiv
Journal :
Phys. Rev. Lett. 117, 182503 (2016)
Publication Type :
Report
Accession number :
edsarx.1610.09772
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevLett.117.182503