Vandebrouck, M, Lepailleur, A, Sorlin, O, Aumann, T, Caesar, C, Holl, M, Panin, V, Wamers, F, Stroberg, SR, Holt, JD et al (show 100 more authors)
(2017)
Effective proton-neutron interaction near the drip line from unbound states in <SUP>25,26</SUP>F.
PHYSICAL REVIEW C, 96 (5).
054305-.
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Abstract
Background: Odd-odd nuclei, around doubly closed shells, have been extensively used to study proton-neutron interactions. However, the evolution of these interactions as a function of the binding energy, ultimately when nuclei become unbound, is poorly known. The $^{26}$F nucleus, composed of a deeply bound $\pi0d\_{5/2}$ proton and an unbound $\nu0d\_{3/2}$ neutron on top of an $^{24}$O core, is particularly adapted for this purpose. The coupling of this proton and neutron results in a $J^{\pi} = 1^{+}\_1 - 4^{+}\_1$ multiplet, whose energies must be determined to study the influence of the proximity of the continuum on the corresponding proton-neutron interaction. The $J^{\pi} = 1^{+}\_1, 2^{+}\_1,4^{+}\_1$ bound states have been determined, and only a clear identification of the $J^{\pi} =3^{+}\_1$ is missing.Purpose: We wish to complete the study of the $J^{\pi} = 1^{+}\_1 - 4^{+}\_1$ multiplet in $^{26}$F, by studying the energy and width of the $J^{\pi} =3^{+}\_1$ unbound state. The method was firstly validated by the study of unbound states in $^{25}$F, for which resonances were already observed in a previous experiment.Method: Radioactive beams of $^{26}$Ne and $^{27}$Ne, produced at about $440A$\,MeV by the FRagment Separator at the GSI facility, were used to populate unbound states in $^{25}$F and $^{26}$F via one-proton knockout reactions on a CH$\_2$ target, located at the object focal point of the R$^3$B/LAND setup. The detection of emitted $\gamma$-rays and neutrons, added to the reconstruction of the momentum vector of the $A-1$ nuclei, allowed the determination of the energy of three unbound states in $^{25}$F and two in $^{26}$F. Results: Based on its width and decay properties, the first unbound state in $^{25}$F is proposed to be a $J^{\pi} = 1/2^-$ arising from a $p\_{1/2}$ proton-hole state. In $^{26}$F, the first resonance at 323(33)~keV is proposed to be the $J^{\pi} =3^{+}\_1$ member of the $J^{\pi} = 1^{+}\_1 - 4^{+}\_1$ multiplet. Energies of observed states in $^{25,26}$F have been compared to calculations using the independent-particle shell model, a phenomenological shell-model, and the ab initio valence-space in-medium similarity renormalization group method.Conclusions: The deduced effective proton-neutron interaction is weakened by about 30-40\% in comparison to the models, pointing to the need of implementing the role of the continuum in theoretical descriptions, or to a wrong determination of the atomic mass of $^{26}$F.
Item Type: | Article |
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Additional Information: | 14 pages, 7 figures, 3 tables, submitted to PRC |
Uncontrolled Keywords: | nucl-ex, nucl-ex |
Depositing User: | Symplectic Admin |
Date Deposited: | 15 Mar 2018 11:28 |
Last Modified: | 18 Oct 2023 08:40 |
DOI: | 10.1103/PhysRevC.96.054305 |
Related URLs: | |
URI: | https://livrepository.liverpool.ac.uk/id/eprint/3019053 |
Available Versions of this Item
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Effective proton-neutron interaction near the drip line from unbound states in F-25,F-26. (deposited 14 Mar 2018 10:33)
- Effective proton-neutron interaction near the drip line from unbound states in <SUP>25,26</SUP>F. (deposited 15 Mar 2018 11:28) [Currently Displayed]