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Reduction of spectroscopic overlap across the shell in neutron-rich nuclei
T. Redpath, P. Guèye, T. Baumann, B. A. Brown, A. Cunningham, P. A. DeYoung, N. Frank, C. R. Hoffman, A. N. Kuchera, B. Monteagudo Godoy, C. Persch, A. Revel, W. F. Rogers, M. Thoennessen, J. A. Tostevin, and D. Votaw
Phys. Rev. C 109, 054325 – Published 24 May 2024
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Abstract
Background: The recent discovery and spectroscopic measurements of and suggests the disappearance of the shell structure in these neutron-rich oxygen isotopes.
Purpose: We measured one- and two-proton removal cross sectionsfrom and , respectively, extracting spectroscopic factors and comparing them to shell model overlap functions coupled with eikonal reaction model calculations.
Method: The invariant mass technique was used to reconstruct the two-body () and three-body () decay energies from knockout reactions of (106.2 MeV/u) and (112.8 MeV/u) beams impinging on a target.
Results: The one-proton removal from strongly populated the ground state of and the extracted cross sectionof mb agrees with eikonal model calculations that are normalized by the shell model spectroscopic factors and account for the systematic reduction factor observed for single nucleon removal reactions within the models used. For the two-proton removal reaction from an upper limit of 0.08 mb was extracted for populating states in decaying though the ground state of .
Conclusions: The measured upper limit for the population of the ground state of in the two-proton removal reaction from indicates a significant difference in the underlying nuclear structure of and .
- Received 9 March 2024
- Accepted 25 April 2024
DOI:https://doi.org/10.1103/PhysRevC.109.054325
Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.
Published by the American Physical Society
Physics Subject Headings (PhySH)
- Research Areas
Direct reactionsEnergy levelsShell model
- Properties
20 ≤ A ≤ 38
- Techniques
Radioactive beams
Nuclear Physics
Authors & Affiliations
T. Redpath1,2,*, P. Guèye1,3,†, T. Baumann1, B. A. Brown1, A. Cunningham2,‡, P. A. DeYoung4, N. Frank5, C. R. Hoffman6, A. N. Kuchera7, B. Monteagudo Godoy4, C. Persch4,§, A. Revel1,3, W. F. Rogers8, M. Thoennessen1,3, J. A. Tostevin9, and D. Votaw1,3,∥
- 1Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA
- 2Department of Chemistry, Virginia State University, Petersburg, Virginia 23806, USA
- 3Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
- 4Department of Physics, Hope College, Holland, Michigan 49422-9000, USA
- 5Department of Physics, Engineering, and Astronomy, Augustana College, Rock Island, Illinois 61201, USA
- 6Physics Division, Argonne National Laboratory, Lemont, Illinois 60439, USA
- 7Department of Physics, Davidson College, Davidson, North Carolina 28035, USA
- 8Department of Physics, Indiana Wesleyan University, Marion, Indiana 46953, USA
- 9Department of Physics, University of Surrey, Guildford GU2 7XH, United Kingdom
- *tredpath@vsu.edu
- †gueye@frib.msu.edu
- ‡Present address: Morehouse School of Medicine, Atlanta, GA 30310, USA.
- §Present address: Department of Atmospheric and Oceanic Sciences, University of Colorado, Boulder, CO 80309, USA.
- ∥Present address: U.S. Department of Defense, Washington, DC 20301, USA.
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Figure 2
Reconstructed two-body (top) and three-body (bottom) decay energy spectra from (red, scaled by 0.1) and (blue) beams. The three-body data were filtered using the conditions described in the text.
Figure 3
Level scheme of the neutron-unbound oxygen isotopes populated in the present reactions. Experimentally known states for are shown in black. The energies and spin and parity assignments for were taken from Ref.[27] while the energy and tentative spin and parity assignments for are from Ref.[3]. States in and predicted by shell model calculations are shown in red. Decay paths included in the simulations are indicated by solid blue arrows. The dashed blue arrows show possible decays of states populated in (see Sec.4 for details.)
Figure 4
Top panel: reconstructed two-body decay energy () from (a)and (b)incident beams on the segmented beryllium target. Bottom panel: reconstructed three-body decay energy () from (c)and (d)incident beams on a beryllium target. The results of the simulations are shown in black solid lines which are the sums of the individual decay contributions indicated as solid colored lines in the panels and discussed in the text.