Physics Letters B (Aug 2016)

Shell evolution approaching the N=20 island of inversion: Structure of 26Na

  • G.L. Wilson,
  • W.N. Catford,
  • N.A. Orr,
  • C.Aa. Diget,
  • A. Matta,
  • G. Hackman,
  • S.J. Williams,
  • I.C. Celik,
  • N.L. Achouri,
  • H. Al Falou,
  • R. Ashley,
  • R.A.E. Austin,
  • G.C. Ball,
  • J.C. Blackmon,
  • A.J. Boston,
  • H.C. Boston,
  • S.M. Brown,
  • D.S. Cross,
  • M. Djongolov,
  • T.E. Drake,
  • U. Hager,
  • S.P. Fox,
  • B.R. Fulton,
  • N. Galinski,
  • A.B. Garnsworthy,
  • D. Jamieson,
  • R. Kanungo,
  • K.G. Leach,
  • J.N. Orce,
  • C.J. Pearson,
  • M. Porter-Peden,
  • F. Sarazin,
  • E.C. Simpson,
  • S. Sjue,
  • D. Smalley,
  • C. Sumithrarachchi,
  • S. Triambak,
  • C. Unsworth,
  • R. Wadsworth

DOI
https://doi.org/10.1016/j.physletb.2016.05.093
Journal volume & issue
Vol. 759, no. C
pp. 417 – 423

Abstract

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The levels in 26Na with single particle character have been observed for the first time using the d(25Na, pγ) reaction at 5 MeV/nucleon. The measured excitation energies and the deduced spectroscopic factors are in good overall agreement with (0+1)ħω shell model calculations performed in a complete spsdfp basis and incorporating a reduction in the N=20 gap. Notably, the 1p3/2 neutron configuration was found to play an enhanced role in the structure of the low-lying negative parity states in 26Na, compared to the isotone 28Al. Thus, the lowering of the 1p3/2 orbital relative to the 0f7/2 occurring in the neighbouring Z=10 and 12 nuclei – 25,27Ne and 27,29Mg – is seen also to occur at Z=11 and further strengthens the constraints on the modelling of the transition into the island of inversion.

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