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Beyond-mean-field study of the hyperon impurity effect in hypernuclei with shape coexistence

机译:超均外杂质效应与形状共存的高谐杂质效应的超越

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Background: The hyperon impurity effect in nuclei has been extensively studied in different mean-field models. Recently, there is a controversy about whether the Λ 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 _Λ~(37) Ar and ~(36)Ar. The wave functions 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 Λ binding energies in both ND and SD states of _Λ~(37) Ar are studied in the case of the Λ hyperon occupying the s,p, or d 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 ~(36)Ar and _Λ~(37)_sAr are calculated based on the same nuclear energy density functional. The results indicate that the SD states exist in _Λ~(37) Ar for all four effective interactions. Furthermore, the Λ_s reduces the quadrupole collectivity of ND states to a greater extent than that of SD states. For _Λ~(37) Ar, the beyond-mean field decreases the Λ_s binding energy of the SD state by 0.17 MeV, but it almost has no effect on that of the ND state. Conclusions: In _Λ_s~(37) Ar, the Λ_p and Λ_d binding energies of the SD states are always larger than those of the ND states. For Λ_s , the conclusion depends on the effective nucleon-hyperon interaction. Moreover, the beyond-mean-field model calculation indicates that the Λ_s hyperon is less bound in the SD state than that in the ND state.
机译:背景:在不同平均场模型中,核中的高速杂质效应已被广泛研究。最近,λ超谐在正常变形(ND)状态中是否更紧密地绑定存在争议,这些争议在于SuperDeformed(SD)状态。目的:本文旨在提供对具有形状共存的低洼地位的低位陈述和争夺争议。方法:采用相对论平均场和超越基于相对论的点耦合能功能的模型研究_λ〜(37)AR和〜(36)AR的低位状态。低洼状态的波函数被构造为具有不同Quadrupole变形参数的不同值的一组相对论平均场状态的叠加。考虑到粒子数和角动量的突起。结果:在λ超谐座位占据球形极限中的λ超谐振位的情况下,研究了ND和SD态中的λ结合能量和SD态的λ〜(37)AR的末端。为了进行比较,分别使用四组核子 - 超耦合相互作用。此外,基于相同的核能密度函数计算,在〜(36)AR和_λ〜(37)_SAR中的低洼状态的光谱。结果表明,SD状态存在于所有四个有效相互作用的_λ〜(37)AR中。此外,λ_S在更大程度上减少了ND状态的四极其集距性,而不是SD状态。对于_λ〜(37)AR,超越平均字段将SD状态的λ_S绑定能量降低0.17 meV,但它几乎没有对ND状态的影响。结论:在_λ_s〜(37)AR中,SD状态的λ_p和λ_d绑定能量总是大于ND状态的绑定能量。对于λ_s,结论取决于有效的核子超谐交互。此外,超越平均场模型计算指示λ_s超谐振度在SD状态下界定而不是ND状态。

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  • 来源
    《Physical Review C》 |2017年第2017期|034309.1-034309.10|共10页
  • 作者单位

    Department of Physics and Institute of Theoretical Physics and Astrophysics Xiamen University Xiamen 361005 China;

    School of Physical Science and Technology Southwest University Chongqing 400715 China;

    School of Physical Science and Technology Southwest University Chongqing 400715 China Department of Physics and Astronomy University of North Carolina Chapel Hill North Carolina 27516-3255 USA;

    Department of Physics East China Normal University Shanghai 200241 China;

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