Physics Letters B (Nov 2018)

Shape coexistence and mixing of low-lying 0+ states in 96Sr

  • S. Cruz,
  • P.C. Bender,
  • R. Krücken,
  • K. Wimmer,
  • F. Ames,
  • C. Andreoiu,
  • R.A.E. Austin,
  • C.S. Bancroft,
  • R. Braid,
  • T. Bruhn,
  • W.N. Catford,
  • A. Cheeseman,
  • A. Chester,
  • D.S. Cross,
  • C.Aa. Diget,
  • T. Drake,
  • A.B. Garnsworthy,
  • G. Hackman,
  • R. Kanungo,
  • A. Knapton,
  • W. Korten,
  • K. Kuhn,
  • J. Lassen,
  • R. Laxdal,
  • M. Marchetto,
  • A. Matta,
  • D. Miller,
  • M. Moukaddam,
  • N.A. Orr,
  • N. Sachmpazidi,
  • A. Sanetullaev,
  • C.E. Svensson,
  • N. Terpstra,
  • C. Unsworth,
  • P.J. Voss

Journal volume & issue
Vol. 786
pp. 94 – 99

Abstract

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The low energy excited 02,3+ states in 96Sr are amongst the most prominent examples of shape coexistence across the nuclear landscape. In this work, the neutron [2s1/2]2 content of the 01,2,3+ states in 96Sr was determined by means of the d(95Sr, p) transfer reaction at the TRIUMF-ISAC2 facility using the SHARC and TIGRESS arrays. Spectroscopic factors of 0.19(3) and 0.22(3) were extracted for the 96Sr ground and 1229 keV 0+ states, respectively, by fitting the experimental angular distributions to DWBA reaction model calculations. A detailed analysis of the γ-decay of the isomeric 03+ state was used to determine a spectroscopic factor of 0.33(13). The experimental results are compared to shell model calculations, which predict negligible spectroscopic strength for the excited 0+ states in 96Sr. The strengths of the excited 02,3+ states were also analyzed within a two-level mixing model and are consistent with a mixing strength of a2=0.40(14) and a difference in intrinsic deformations of |Δβ|=0.31(3). These results suggest coexistence of three different configurations in 96Sr and strong shape mixing of the two excited 0+ states. Keywords: Single-particle structure, Transfer reaction, Shape coexistence