NUCLEAR PHYSICS |
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Giant Monopole Resonance and Nuclear Incompressibility of Hypernuclei |
Hong Lv1, Shi-Sheng Zhang2, Zhen-Hua Zhang1, Yu-Qian Wu1, Jiang Liu1, Li-Gang Cao1** |
1School of Mathematics and Physics, North China Electric Power University, Beijing 102206 2School of Physics and Nuclear Energy Engineering, Beihang University, Beijing 100191
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Cite this article: |
Hong Lv, Shi-Sheng Zhang, Zhen-Hua Zhang et al 2018 Chin. Phys. Lett. 35 062102 |
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Abstract The isoscalar giant monopole resonances (ISGMRs) of hypernuclei $^{42}_{{\Lambda}{\Lambda}}$Ca, $^{122}_{{\Lambda}{\Lambda}}$Sn, and $^{210}_{{\Lambda}{\Lambda}}$Pb are investigated using a fully self-consistent Skyrme–Hartree–Fock plus random phase approximation method. The Skyrme-type forces, SGII, No.5 and S${\Lambda}{\Lambda}$1, are adopted to describe the nucleon–nucleon, ${\Lambda}$ hyperon–nucleon and ${\Lambda}$ hyperon–${\Lambda}$ hyperon (${\Lambda} {\Lambda}$) interactions, respectively. For a given hyperon fraction, we find that effects of ${\Lambda} {\Lambda}$ interaction on the properties of infinite symmetric nuclear matter and finite hypernuclei are very small. The ISGMR strengths are shifted to the high energy region when two ${\Lambda}$ are added into normal nuclei. The changes are from two parts, one is due to the mean field calculations, and the other is from the residual interaction associated with ${\Lambda}$ hyperons. The constrained energies are increased by about 0.5–0.7 MeV, which consequently enhances the effective incompressibility modulus of hypernuclei.
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Received: 12 February 2018
Published: 19 May 2018
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PACS: |
21.60.Jz
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(Nuclear Density Functional Theory and extensions (includes Hartree-Fock and random-phase approximations))
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21.80.+a
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(Hypernuclei)
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24.30.Cz
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(Giant resonances)
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21.30.-x
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(Nuclear forces)
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Fund: Supported by the National Natural Science Foundation of China under Grant Nos 11575060, 11775014, 11505058 and 11435014. |
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