Single-particle and collective degrees of freedom in Zr101 and Mo103,105

R. Orlandi, A. G. Smith, D. Patel, G. S. Simpson, R. M. Wall, J. F. Smith, O. J. Onakanmi, I. Ahmad, J. P. Greene, M. P. Carpenter, T. Lauritsen, C. J. Lister, R. V. F. Janssens, F. G. Kondev, D. Seweryniak, B. J. P. Gall, O. Dorveaux, and A. E. Stuchbery
Phys. Rev. C 73, 054310 – Published 16 May 2006

Abstract

The g factors of several low-lying excited states of the neutron-rich Zr101 and Mo103,105 nuclei have been measured for the first time. The isotopes were produced by the spontaneous fission of a Cf252 source, which was sandwiched between two magnetized iron foils and placed at the center of the Gammasphere spectrometer. The g factors of excited states of fission fragments were inferred from Larmor precessions deduced from the measurement of time-integrated perturbed angular correlation functions. The magnitude and sign of the quantity (gKgR)/Q0 were determined from the mixing ratios measured for the 3/2[411] and 5/2[532] rotational bands in Zr101 and Mo103,105. The combination of this quantity with the measured g factors permitted the separation of the particle-rotor parameters gK and gR for each band. The comparison of the extracted gK factors to Nilsson model predictions confirms current band assignments, and this agreement is consistent with an axially symmetric picture of these nuclei at low spins. The possible effect of triaxial deformation on the measured magnetic moments was investigated in the rigid triaxial rotor-plus-particle framework. The calculations suggest that triaxial deformation plays a stronger role in the Mo than in the Zr isotopes, but that triaxiality is likely to be dynamic. The extracted gR factors are consistently smaller than the Z/A limit, in agreement with observations in neighboring even-even nuclei.

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  • Received 26 September 2005

DOI:https://doi.org/10.1103/PhysRevC.73.054310

©2006 American Physical Society

Authors & Affiliations

R. Orlandi1,*, A. G. Smith1, D. Patel1, G. S. Simpson1,†, R. M. Wall1, J. F. Smith1, O. J. Onakanmi1, I. Ahmad2, J. P. Greene2, M. P. Carpenter2, T. Lauritsen2, C. J. Lister2, R. V. F. Janssens2, F. G. Kondev2,‡, D. Seweryniak2, B. J. P. Gall3, O. Dorveaux3, and A. E. Stuchbery4

  • 1University of Manchester, M13 9PL, Manchester, United Kingdom
  • 2Physics Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 3IPHC CNRS-IN2P3, ULP, F-67037 Strasbourg, France
  • 4Department of Nuclear Physics, RSPhysSE, Australian National University, Canberra, ACT 0200, Australia

  • *Present address: INFN - Laboratori Nazionali di Legnaro, Padova, Italy; electronic address: Riccardo.Orlandi@lnl.infn.it
  • Present address: LPSC, CNRS/IN2P3, Grenoble, France.
  • Present address: Nuclear Engineering Division, ANL, Argonne, IL 60439, USA.

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Vol. 73, Iss. 5 — May 2006

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