Abstract
The nonlocalized aspect of clustering, which is a new concept for self-conjugate nuclei, is extended for the investigation of the nucleus . A modified version of the Tohsaki-Horiuchi-Schuck-Röpke (THSR) wave function is introduced with a new phase factor. It is found that the constructed negative-parity THSR wave function is very suitable for describing the cluster states of . Namely, the nonlocalized clustering is shown to prevail in . The calculated binding energy and radius of are consistent with calculations in other models and with experimental values. The squared overlaps between the single THSR wave function and the Brink + generator coordinate method wave function for the rotational band of are found to be near 96%. Furthermore, by showing the density distribution of the ground state of , the -orbit structure is naturally reproduced by using this THSR wave function.
- Received 11 August 2014
- Revised 2 November 2014
DOI:https://doi.org/10.1103/PhysRevC.91.014313
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