How different is the core of $^{25}$F from $^{24}$O$_{g.s.}$?
T. L. Tang, T. Uesaka, S. Kawase, D. Beaumel, M. Dozono, T. Fujii, N., Fukuda, T. Fukunaga, A. Galindo-Uribarri, S. H. Hwang, N. Inabe, D. Kameda,, T. Kawahara, W. Kim, K. Kisamori, M. Kobayashi, T. Kubo, Y. Kubota, K., Kusaka, C. S. Lee, Y. Maeda, H. Matsubara, S. Michimasa

TL;DR
This study investigates the neutron-shell structure of $^{25}$F using knockout reactions, revealing that its core significantly differs from a free $^{24}$O nucleus and contains a mixture of ground and excited states.
Contribution
It provides new experimental data on the spectroscopic factors and core composition of $^{25}$F, highlighting the difference from a free $^{24}$O core.
Findings
The spectroscopic factor for the $^{25}$F to $^{24}$O ground-state transition is 0.36.
The $^{24}$O core in $^{25}$F is approximately 35% in the ground state and 65% in excited states.
The sum of spectroscopic factors for the $ u$0d$_{5/2}$ orbital is 1.0 ± 0.3.
Abstract
The neutron-shell structure of F was studied using quasi-free (p,2p) knockout reaction at 270A MeV in inverse kinematics. The sum of spectroscopic factors of 0d orbital is found to be . However, the spectroscopic factor for the ground-state to ground-state transition (F, O) is only , and O excited states are produced from the 0d proton knockout. The result shows that the O core of F nucleus significantly differs from a free O nucleus, and the core consists of 35% O. and 65% excited O.
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