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Erlangen 2001 – scientific programme

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HK: Physik der Hadronen und Kerne

HK 37: Kernphysik/Spektroskopie V - Isomere, g-Faktoren und Massen

HK 37.2: Talk

Wednesday, March 21, 2001, 17:00–17:15, D

A new g factor measurement of the 21+ state in 54Cr and its shell model interpretation including 50Cr and 52Cr + — •S. Wagner1, K.-H. Speidel1, O. Kenn1, R. Ernst1, S. Schielke1, J. Gerber2, N. Benczer-Koller3, G. Kumbartzki3, P. Maier-Komor4, F. Nowacki5, and Y.Y. Sharon31Institut für Strahlen- und Kernphysik, Univ. Bonn, D-53115 Bonn, Germany — 2Institut de Recherches Subatomiques, F-67037 Strasbourg, France — 3Dept. of Physics and Astronomy, Rutgers Univ., New Brunswick, NJ 08903, USA — 4Physik Department, TU München, D-85748 Garching, Germany — 5Laboratoire de Physique Théorique, F-67084 Strasbourg, France

Precise data from recent measurements of g factors for the 21+ and 41+ states of 50Cr and the 21+ state for 52Cr were well explained by large shell model calculations [1]. In particular, the puzzle of the g factor ratio of the 41+ to the 21+ state in 50Cr has been unravelled. These data were supplemented by a redetermination of the g factor of the 54Cr(21+) state. Like for the other Cr isotopes, the same technique of projectile Coulomb excitation in inverse kinematics was applied. 54Cr beams of 115 MeV were provided in its natural isotopic abundance by the ion source of the Cologne tandem accelerator. The g factor value obtained, g=0.832(56), and the B(E2) deduced from the lifetime are compared with shell model calculations within the same large configuration space as for the lighter isotopes.
[1] R. Ernst et al., Phys. Rev. Lett. 84 (2000) 416
+ supported by DFG and BMBF

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