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Neutron-unbound states in Ne 31

  • D. Chrisman
  • , A. N. Kuchera
  • , T. Baumann
  • , A. Blake
  • , B. A. Brown
  • , J. Brown
  • , C. Cochran
  • , P. A. Deyoung
  • , J. E. Finck
  • , N. Frank
  • , P. Guèye
  • , H. Karrick
  • , H. Liu
  • , J. McDonaugh
  • , T. Mix
  • , B. Monteagudo
  • , T. H. Redpath
  • , W. F. Rogers
  • , R. Seaton-Todd
  • , A. Spyrou
  • K. Stiefel, M. Thoennessen, J. A. Tostevin, D. Votaw

Research output: Contribution to journalArticlepeer-review

9 Scopus citations

Abstract

Background: The island of inversion near the N=20 shell gap is home to nuclei with reordered single-particle energy levels compared with the spherical shell model. Studies of Ne31 have revealed that its ground state has a halo component characterized by a valence neutron orbiting a deformed Ne30 core. This lightly bound nucleus with a separation energy of only Sn=170 keV is expected to have excited states that are neutron unbound. Purpose: The purpose of this experiment was to investigate the low-lying excited states in Ne31 that decay by the emission of a single neutron. Methods: An 89 MeV/nucleon Mg33 beam impinged on a segmented Be reaction target. Neutron-unbound states in Ne31 were populated via a two-proton knockout reaction. The Ne30 fragment and associated neutron from the decay of Ne31 were detected by the MoNA-LISA-Sweeper experimental setup at the National Superconducting Cyclotron Laboratory. Invariant-mass spectroscopy was used to reconstruct the two-body decay energy (Ne30+n). Results: The two-body decay energy spectrum exhibits two features: a low-lying peak at 0.30±0.17 MeV and a broad enhancement at 1.50±0.33 MeV, each fit with an energy-dependent asymmetric Breit-Wigner lineshape representing a resonance in the continuum. Accompanying shell-model calculations using the FSU interaction within NuShellX, combined with cross-section calculations using the eikonal reaction theory, indicate that these peaks in the decay energy spectrum are caused by multiple resonant states in Ne31. Conclusions: Excited states in Ne31 were observed for the first time. Transitions from calculated shell-model final states in Ne31 to bound states in Ne30 are in good agreement with the measured decay energy spectrum. Cross-section calculations for the two-proton knockout populating Ne31 states as well as spectroscopic factors pertaining to the decay of Ne31 into Ne30 are used to examine the results within the context of the shell-model expectations.

Original languageEnglish
Article number034313
JournalPhysical Review C
Volume104
Issue number3
DOIs
StatePublished - Sep 2021
Externally publishedYes

Funding

We would like to acknowledge the effort of the National Superconducting Cyclotron Laboratory operations staff for providing high-quality beams and device support for the Sweeper detectors. We would also like to acknowledge the MoNA collaboration for providing device support for MoNA-LISA and Sweeper detectors and contributions to the experiment execution. This work was supported by the National Science Foundation, USA under Grants No. PHY-1102511, No. PHY-1565546, No. PHY-1613188, No. PHY-1713522, No. PHY-1613429, No. PHY-1713956, No. PHY-1205357, No. PHY-2011398, and No. PHY-2012040. This work was also supported by the Department of Energy National Nuclear Security Administration, USA through the Nuclear Science and Security Consortium under Award No. DE-NA0003180 and/or DE-NA0000979. J.A.T. acknowledges support from the Science and Technology Facilities Council (UK) Grant No. ST/L005743/1.

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