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Phys. Rev. C 65, 047303 (2002) [4 pages]

Hypernucleus Λ40Ca and recent hyperon-nucleon potentials

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Yiharn Tzeng1, S. Y. Tsay Tzeng2, and T. T. S. Kuo1,3
1Institute of Physics, Academia Sinica, Taipei 11529, Taiwan, Republic of China
2Department of Photonics, National Taipei University of Technology, Taipei, Taiwan, Republic of China
3Department of Physics, State University of New York, Stony Brook, New York 11794

Received 12 December 2001; published 21 March 2002

The Nijmegen NSC89 and the most recent NSC97 hyperon-nucleon potentials are adopted to study the structures of hypernuclei. Investigations are concentrated on the hypernucleus Λ40Ca by using our two-frequency shell-model folded-diagram approach. We first calculate the YN G matrix with an exact Pauli exclusion operator. The nucleon frequency for the harmonic oscillator basis wave function is chosen from the empirical formula ħωN=45A-1/3-25A-2/3, while the hyperon one is obtained as the frequency when the lowest hyperon single-particle energy in the hypernucleus reaches a saturation minimum. The energy-independent effective interaction Veff is then obtained from the YN G matrix elements, using a -box folded-diagram framework. We will examine how our calculated spectra vary via these different versions of the realistic hyperon-nucleon potentials. Special attention is drawn on the contribution of the ΛN-ΣN coupling diagram. Although this diagram contributes significantly to Veff in most cases, it does not alter much to the final spectrum.

© 2002 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.65.047303
DOI:
10.1103/PhysRevC.65.047303
PACS:
21.80.+a, 21.60.Cs, 24.10.Cn, 27.20.+n