Single-particle and collective structures in Cr55 and V55

A. N. Deacon, D. Steppenbeck, S. Zhu, S. J. Freeman, R. V F Janssens, M. P. Carpenter, B. Fornal, M. Honma, B. P. Kay, F. G. Kondev, J. Kozemczak, A. Larabee, T. Lauritsen, C. J. Lister, A. P. Robinson, D. Seweryniak, J. F. Smith, Y. Sun, X. Wang, F. R. XuY. C. Yang

    Research output: Contribution to journalArticlepeer-review

    Abstract

    Excited states in V55 and Cr55 have been populated via pn and 2n evaporation channels, respectively, following the fusion of a Ca48 beam at 172 MeV with a Be9 target. Level schemes have been deduced for the two nuclides to excitation energies of 7467 (V55) and 12226 keV (Cr55), with spins of 27/2 + and 33/2+, respectively. Negative-parity states are compared with shell-model calculations using three different effective interactions in the full fp model space. Negative-parity levels of Cr55 are explained in terms of single-particle fp-shell configurations outside N=28 and N=32 cores. Positive-parity states in both isotopes show evidence for the involvement of neutron g9/2 configurations. In the case of Cr55, a quasirotational structure based on the 1/2+[440] Nilsson orbital is observed up to the terminating state. In V55, positive-parity states do not exhibit well-developed collective features, and the observation of octupole decays is an indication of their importance in transitions from neutron g 9/2 configurations to the fp shell. Experimental results are compared with the predictions of a traditional shell model, the projected shell model, and total-Routhian-surface calculations. © 2011 American Physical Society.
    Original languageEnglish
    Article number064305
    JournalPhysical Review C - Nuclear Physics
    Volume83
    Issue number6
    DOIs
    Publication statusPublished - 15 Jun 2011

    Fingerprint

    Dive into the research topics of 'Single-particle and collective structures in Cr55 and V55'. Together they form a unique fingerprint.

    Cite this