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Phys. Rev. Lett. 102, 092501 (2009) [4 pages]

Shell Erosion and Shape Coexistence in 1643S27

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L. Gaudefroy1,*, J. M. Daugas1, M. Hass2, S. Grévy3, Ch. Stodel3, J. C. Thomas3, L. Perrot4, M. Girod1, B. Rossé1, J. C. Angélique5, D. L. Balabanski6, E. Fiori7, C. Force3, G. Georgiev7, D. Kameda8, V. Kumar2, R. L. Lozeva7, I. Matea9, V. Méot1, P. Morel1, B. S. Nara Singh10, F. Nowacki11, and G. Simpson5
1CEA, DAM, DIF, F-91297 Arpajon, France
2The Weizmann Institute, 76100 Rehovot, Israel
3GANIL, CEA/DSM - CNRS/IN2P3, F-14076 Caen, France
4IPN, IN2P3-CNRS, F-91406 Orsay, France
5LPSC, F-38026 Grenoble, France
6Faculty of Physics, University of Sofia, BG-1164 Sofia, Bulgaria
7CSNSM, F-91404 Orsay, France
8RIKEN, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan
9CENBG, UMR 5797 CNRS/IN2P3, Université Bordeaux 1, F-33175 Gradignan, France
10Department of Physics, University of York, YO 10 5DD York, United Kingdom
11IPHC, IN2p3-CNRS, F-67037 Strasbourg, France

Received 30 October 2008; revised 17 December 2008; published 2 March 2009

See accompanying Physics Viewpoint

We report on the g-factor measurement of the first isomeric state in 1643S27 [Ex=320.5(5)  keV, T1/2=415(5)  ns, and g=0.317(4)]. The 7/2- spin-parity of the isomer and the intruder nature of the ground state of the nucleus are experimentally established for the first time, providing direct and unambiguous evidence of the collapse of the N=28 shell closure in neutron-rich nuclei. The shell model, beyond the mean-field and semiempirical calculations, provides a very consistent description of this nucleus showing that a well deformed prolate and quasispherical states coexist at low energy.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.102.092501
DOI:
10.1103/PhysRevLett.102.092501
PACS:
21.10.Ky, 21.60.Cs, 23.35.+g, 27.40.+z

*laurent.gaudefroy@cea.fr