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How different is the core of $^{25}$F from $^{24}$O$_{g.s.}$?

Authors :
Tang, T. L.
Uesaka, T.
Kawase, S.
Beaumel, D.
Dozono, M.
Fujii, T.
Fukuda, N.
Fukunaga, T.
Galindo-Uribarri, A.
Hwang, S. H.
Inabe, N.
Kameda, D.
Kawahara, T.
Kim, W.
Kisamori, K.
Kobayashi, M.
Kubo, T.
Kubota, Y.
Kusaka, K.
Lee, C. S.
Maeda, Y.
Matsubara, H.
Michimasa, S.
Miya, H.
Noro, T.
Obertelli, A.
Ogata, K.
Ota, S.
Padilla-Rodal, E.
Sakaguchi, S.
Sakai, H.
Sasano, M.
Shimoura, S.
Stepanyan, S. S.
Suzuki, H.
Takaki, M.
Takeda, H.
Tokieda, H.
Wakasa, T.
Wakui, T.
Yako, K.
Yanagisawa, Y.
Yasuda, J.
Yokoyama, R.
Yoshida, K.
Zenihiro, J.
Publication Year :
2018

Abstract

The neutron-shell structure of $^{25}$F was studied using quasi-free (p,2p) knockout reaction at 270A MeV in inverse kinematics. The sum of spectroscopic factors of $\pi$0d$_{5/2}$ orbital is found to be $1.0 \pm 0.3$. However, the spectroscopic factor for the ground-state to ground-state transition ($^{25}$F, $^{24}$O$_{g.s.}$) is only $0.36\pm 0.13$, and $^{24}$O excited states are produced from the 0d$_{5/2}$ proton knockout. The result shows that the $^{24}$O core of $^{25}$F nucleus significantly differs from a free $^{24}$O nucleus, and the core consists of 35% $^{24}$O$_{g.s}$. and 65% excited $^{24}$O.<br />Comment: 5 pages, 5 figures

Subjects

Subjects :
Nuclear Experiment
Nuclear Theory

Details

Database :
arXiv
Publication Type :
Report
Accession number :
edsarx.1810.10113
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevLett.124.212502