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Magnetic moment and lifetime measurements of Coulomb-excited states in Cd 106

  • N. Benczer-Koller
  • , G. J. Kumbartzki
  • , K. H. Speidel
  • , D. A. Torres
  • , S. J.Q. Robinson
  • , Y. Y. Sharon
  • , J. M. Allmond
  • , P. Fallon
  • , I. Abramovic
  • , L. A. Bernstein
  • , J. E. Bevins
  • , H. L. Crawford
  • , Z. E. Guevara
  • , A. M. Hurst
  • , L. Kirsch
  • , T. A. Laplace
  • , A. Lo
  • , E. F. Matthews
  • , I. Mayers
  • , L. W. Phair
  • F. Ramirez, A. Wiens

Research output: Contribution to journalArticlepeer-review

10 Scopus citations

Abstract

Background: The Cd isotopes are well studied, but experimental data for the rare isotopes are sparse. At energies above the Coulomb barrier, higher states become accessible. Purpose: Remeasure and supplement existing lifetimes and magnetic moments of low-lying states in Cd106. Methods: In an inverse kinematics reaction, a Cd106 beam impinging on a C12 target was used to Coulomb excite the projectiles. The high recoil velocities provide a unique opportunity to measure g factors with the transient-field technique and to determine lifetimes from lineshapes by using the Doppler-shift-attenuation method. Large-scale shell-model calculations were carried out for Cd106. Results: The g factors of the 21+ and 41+ states in Cd106 were measured to be g(21+)=+0.398(22) and g(41+)=+0.23(5). A lineshape analysis yielded lifetimes in disagreement with published values. The new results are τ(Cd106;21+)=7.0(3)ps and τ(Cd106;41+)=2.5(2)ps. The mean life τ(Cd106;22+)=0.28(2)ps was determined from the fully-Doppler-shifted γ line. Mean lives of τ(Cd106;43+)=1.1(1)ps and τ(Cd106;31-)=0.16(1)ps were determined for the first time. Conclusions: The newly measured g(41+) of Cd106 is found to be only 59% of the g(21+). This difference cannot be explained by either shell-model or collective-model calculations.

Original languageEnglish
Article number034303
JournalPhysical Review C
Volume94
Issue number3
DOIs
StatePublished - Sep 6 2016

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