Beyond-mean-field study of the hyperon impurity effect in hypernuclei with shape coexistence
arXiv:1703.01715 · doi:10.1103/PhysRevC.95.034309
Abstract
[Background] The hyperon impurity effect in nuclei has been extensively studied in different mean-field models. Recently, there is a controversy about whether the hyperon is more tightly bound in the normal deformed (ND) states than that in the superdeformed (SD) states.[Purpose] This article is aimed to provide a beyond-mean-field study of the low-lying states of hypernuclei with shape coexistence and to shed some light on the controversy.[Method] The models of relativistic mean-field and beyond based on a relativistic point-coupling energy functional are adopted to study the low-lying states of both Ar and Ar. The wavefunctions of low-lying states are constructed as a superposition of a set of relativistic mean-field states with different values of quadrupole deformation parameter. The projections onto both particle number and angular momentum are considered.[Results] The binding energies in both ND and SD states of Ar are studied in the case of the hyperon occupying , or state in the spherical limit, respectively. For comparison, four sets of nucleon-hyperon point-coupling interactions are used respectively. Moreover, the spectra of low-lying states in Ar and Ar are calculated based on the same nuclear energy density functional. The results indicate that the SD states exist in Ar for all the four effective interactions. Furthermore, the reduces the quadrupole collectivity of ND states to a greater extent than that of SD states. For Ar, the beyond-mean-field decreases the binding energy of the SD state by 0.17 MeV, but it almost has no effect on that of the ND state. [Conclusions] In Ar, the and binding energies of the SD states ...
11 pages, 15 figures, 4 tables, will be published in Phys. Rev. C
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