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Identification of Prompt Proton Emission in N=Z−1 Ga61: Isospin Symmetry at the Limit of Nuclear Binding

Y. Hrabar1,*, P. Golubev1, D. Rudolph1, L. G. Sarmiento1, C. Müller-Gatermann2, W. Reviol2, D. Seweryniak2, J. Wu2,†, H. M. Albers3 et al.

J. T. Anderson2, M. A. Bentley4, B. G. Carlsson1, M. P. Carpenter2, C. J. Chiara5, P. A. Copp2,‡, D. M. Cox1, J. Ekman6, C. Fahlander1, U. Forsberg1,§, T. Huang2,∥, A. Idini1, H. Jayatissa2,‡, T. Lauritsen2, X. Pereira-Lopez4,¶, S. Stolze2, S. Uthayakumaar4,**, and G. L. Wilson2,7,††

  • *Contact author: yuliia.hrabar@fysik.lu.se
  • †Present address: Brookhaven National Laboratory, Brookhaven, USA.
  • ‡Present address: Physics Division, Los Alamos National Laboratory, Los Alamos, USA.
  • §Present address: Cyclife Sweden AB, Nyköping, Sweden.
  • ∥Present address: Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Present address: Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon, Republic of Korea.
  • **Present address: Facility for Rare Isotope Beams, Michigan State University, East Lansing, USA.
  • ††Present address: United Kingdom Atomic Energy Authority, Abingdon, United Kingdom.

Phys. Rev. Lett. 135, 222503 – Published 25 November, 2025

DOI: https://doi.org/10.1103/kwm2-9bmd

Abstract

Excited states in the proton drip line nucleus Ga61 were populated via the fusion-evaporation reaction Mg24(Ca40,p2n)Ga61. The experimental setup at Argonne National Laboratory comprised a novel combination of the Gammasphere array with two CD-shaped double-sided Si-strip detectors inside the Microball CsI(Tl) charged-particle detection array, as well as the Neutron-Shell liquid scintillators and the Fragment Mass Analyzer. Owing to the setup’s unprecedented in-beam proton spectroscopy and tracking capabilities, a coincidence between a 957.6(5)-keV γ ray and a 1.876(24)-MeV proton line was observed, which identifies the quasibound proton πg9/2 single-particle state in Ga61 at Ex=2150(34)  keV. This probes isospin symmetry at the limit of nuclear binding by providing a unique challenge for the shell-model interpretation of mirror nuclei beyond doubly magic Ni56.

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