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Phys. Rev. Lett. 101, 142504 (2008) [4 pages]

Intruder Configurations in the A=33 Isobars: 33Mg and 33Al

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Vandana Tripathi1, S. L. Tabor1, P. F. Mantica2,3, Y. Utsuno4, P. Bender1, J. Cook2, C. R. Hoffman1, Sangjin Lee1, T. Otsuka5,6, J. Pereira2, M. Perry1, K. Pepper1, J. S. Pinter3, J. Stoker3, A. Volya1, and D. Weisshaar2
1Department of Physics, Florida State University, Tallahassee, Florida 32306, USA
2National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
3Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
4Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan
5Department of Physics and Center for Nuclear Study, University of Tokyo, Hongo, Tokyo 113-0033, Japan
6RIKEN, Hirosawa, Wako-shi, Saitama 351-0198, Japan

Received 2 July 2008; published 2 October 2008

The β decay of 33Mg (N=21) presented in this Letter reveals intruder configurations in both the parent and the daughter nucleus. The lowest excited states in the N=20 daughter nucleus, 33Al, are found to have nearly 2p-2h intruder configuration, thus extending the “island of inversion” beyond Mg. The allowed direct β-decay branch to the 5/2+ ground state of the daughter nucleus 33Al implies positive parity for the ground state of the parent 33Mg, contrary to an earlier suggestion of negative parity from a g-factor measurement. An admixture of 1p-1h and 3p-3h configurations is proposed for the ground state of 33Mg to explain all of the experimental observables.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.101.142504
DOI:
10.1103/PhysRevLett.101.142504
PACS:
23.20.Lv, 21.60.Cs, 23.40.−s, 27.30.+t

See Also

Comment: D. T. Yordanov, K. Blaum, M. De Rydt, M. Kowalska, R. Neugart, G. Neyens, and I. Hamamoto, Comment on “Intruder Configurations in the A=33 Isobars: 33Mg and 33Al, Phys. Rev. Lett. 104, 129201 (2010).