EPJ Web of Conferences (Jan 2017)

Isomer-delayed gamma-ray spectroscopy of neutron-rich 166Tb

  • Gurgi L.A.,
  • Regan P.H.,
  • Söderström P.-A.,
  • Watanabe H.,
  • Walker P.M.,
  • Podolyák Zs.,
  • Nishimura S.,
  • Berry T.A.,
  • Doornenbal P.,
  • Lorusso G.,
  • Isobe T.,
  • Baba H.,
  • Xu Z.Y.,
  • Sakurai H.,
  • Sumikama T.,
  • Catford W.N.,
  • Bruce A.M.,
  • Browne F.,
  • Lane G.J.,
  • Kondev F.G.,
  • Odahara A.,
  • Wu J.,
  • Liu H.L.,
  • Xu F.R.,
  • Korkulu Z.,
  • Lee P.,
  • Liu J.J.,
  • Phong V.H.,
  • Yagi A.,
  • Zhang G.X.,
  • Alharbi T.,
  • Carroll R.J.,
  • Chae K.Y.,
  • Dombradi Zs.,
  • Estrade A.,
  • Fukuda N.,
  • Griffin C.,
  • Ideguchi E.,
  • Inabe N.,
  • Kanaoka H.,
  • Kojouharov I.,
  • Kubo T.,
  • Kubono S.,
  • Kurz N.,
  • Kuti I.,
  • Lalkovski S.,
  • Lee E.J.,
  • Lee C.S.,
  • Lotay G.,
  • Moon C.B.,
  • Nishizuka I.,
  • Nita C.R.,
  • Patel Z.,
  • Roberts O.J.,
  • Schaffner H.,
  • Shand C.M.,
  • Suzuki H.,
  • Takeda H.,
  • Terashima S.,
  • Vajta Zs.,
  • Kanaya S.,
  • Valiente-Dobòn J.J.

DOI
https://doi.org/10.1051/epjconf/201714610009
Journal volume & issue
Vol. 146
p. 10009

Abstract

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This short paper presents the identification of a metastable, isomeric-state decay in the neutron-rich odd-odd, prolate-deformed nucleus 166Tb. The nucleus of interest was formed using the in-flight fission of a 345 MeV per nucleon 238U primary beam at the RIBF facility, RIKEN, Japan. Gamma-ray transitions decaying from the observed isomeric states in 166Tb were identified using the EURICA gamma-ray spectrometer, positioned at the final focus of the BigRIPS fragments separator. The current work identifies a single discrete gamma-ray transition of energy 119 keV which de-excites an isomeric state in 166Tb with a measured half-life of 3.5(4) μs. The multipolarity assignment for this transition is an electric dipole and is made on the basis internal conversion and decay lifetime arguments. Possible two quasi-particle Nilsson configurations for the initial and final states which are linked by this transition in 166Tb are made on the basis of comparison with Blocked BCS Nilsson calculations, with the predicted ground state configuration for this nucleus arising from the coupling of the v(1-/2)[521] and π(3+/2) Nilsson orbitals.