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Nuclear structure investigation of the near-spherical nucleus 93Zr

  • S. X. Guan
  • , C. B. Li*
  • , Y. Zheng
  • , T. X. Li
  • , X. G. Wu
  • , Y. Q. Li
  • , R. Hong
  • , H. Y. Wu
  • , M. Zheng
  • , Z. H. Zhao
  • , Z. Y. He
  • , J. Z. Li
  • , J. Shi
  • , J. N. Zou
  • , L. W. Yang
  • , Y. D. Fang
  • , J. H. Xu
  • , J. H. Li
  • , Z. H. Jia
  • , C. X. Jia
  • W. Q. Zhang, J. L. Wang, C. Y. Guo, Z. X. Zhou, L. Ni, G. S. Li, X. H. Zhou, B. Guo, S. Y. Wang, M. L. Liu, Y. H. Zhang, C. Y. He, F. L. Liu, S. Wang, D. P. Sun, L. H. Zhu
*Corresponding author for this work
  • China National Nuclear Corporation
  • Xihua University
  • Peking University
  • Jilin University
  • Henan University of Technology
  • CAS - Institute of Modern Physics
  • Shandong University

Research output: Contribution to journalArticlepeer-review

Abstract

The excited states of 93Zr have been investigated using the heavy-ion fusion-evaporation reaction 82Se(18O, α3n) 93Zr at the beam energies of 82 and 88 MeV. Particle-γ -γ and γ -γ coincidence measurements using CsI and HPGe arrays are employed to gain selectivity to Zr isotopic products. The level scheme of 93Zr was extended up to E ≈ 12.5 Mev and Iπ = (47/2−) with twenty-six new γ -ray transitions. The observation of γ rays with ≈2 Mev and the associated fragmentation of the γ -ray flux into many competing pathways provide a clear experimental signature for the breaking core. Level structures in 93Zr were interpreted in the framework of the spherical shell model in a model space including the proton orbitals (1 f5/2, 2p3/2, 2p1/2, 1g9/2) and neutron orbits (1g9/2, 1g7/2, 2d5/2, 1h11/2). A possible reduction of the Z = 38 subshell spacing gap in 93Zr is discussed.

Original languageEnglish
JournalPhysical Review C
Volume112
Issue number1
DOIs
StatePublished - 2 Jul 2025

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