Inverse-kinematics proton scattering from $^{42,44}$S, $^{41,43}$P and the collapse of the $N=28$ major shell closure
L. A. Riley, D. Bazin, J. Belarge, P. C. Bender, B. A. Brown, P. D., Cottle, B. Elman, A. Gade, S. D. Gregory, E. B. Haldeman, K. W. Kemper, B. R., Klybor, M. A. Liggett, S. Lipschutz, B. Longfellow, E. Lunderberg, T., Mijatovic, J. Pereira, L. M. Skiles, R. Titus, A. Volya

TL;DR
This study investigates the structure of neutron-rich isotopes $^{42,44}$S and $^{41,43}$P through inverse-kinematics proton scattering, revealing insights into shell evolution and favoring the SDPF-MU interaction model.
Contribution
It provides new experimental data on deformation lengths and neutron-to-proton matrix element ratios, and compares shell model interactions, highlighting the collapse of the $N=28$ shell closure.
Findings
Deformation lengths for $^{42,44}$S determined from proton scattering.
Neutron-to-proton matrix element ratios calculated for $^{42,44}$S.
Results favor the SDPF-MU shell model interaction.
Abstract
Excited states of the neutron-rich isotopes S and P have been studied via inverse-kinematics proton scattering from a liquid hydrogen target, using the GRETINA -ray tracking array to extract inelastic scattering cross sections. Deformation lengths of the excitations in S have been determined and, when combined with deformation lengths determined with electromagnetic probes, yield the ratio of neutron-to-proton matrix elements for the excitations in these nuclei. The present results for P are used to compare two shell model interactions, SDPF-U and SDPF-MU. As in a recent study of Si, the present results on P favor the SDPF-MU interaction.
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