THE NUCLEAR MASS AT FINITE ANGULAR MOMENTA

Author:

RAGNARSSON INGEMAR1,KONDEV FILIP G.2,PAUL EDWARD S.3,RILEY MARK A.4,SIMPSON JOHN5

Affiliation:

1. Division of Mathematical Physics, Lund Institute of Technology, P.O. Box 118, SE-221 00 Lund, Sweden

2. Nuclear Engineering Division, Argonne National Laboratory, Argonne, Illinois 60439, USA

3. Oliver Lodge Laboratory, University of Liverpool, Liverpool L69 7ZE, United Kingdom

4. Department of Physics, Florida State University, Tallahassee, Florida 32306, USA

5. CCLRC, Daresbury Laboratory, Daresbury, Warrington, WA4 4AD, United Kingdom

Abstract

The definition of experimental shell energies for nuclear ground states is generalized to finite angular momenta corresponding to a systematic expansion of the (N,Z)-plane to an (N,Z,I) space. Special emphasis is put on high-spin states where it is expected that odd and even nuclei should have similar properties. Different coupling schemes are compared and energetically favoured conditions to build high-spin states are discussed.

Publisher

World Scientific Pub Co Pte Lt

Subject

General Physics and Astronomy,Nuclear and High Energy Physics

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