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Brueckner-Hartree-Fock calculations for finite nuclei with renormalized realistic forces

机译:Brueckner-Hartree-Fock计算有限核,重整性现实力量

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One can adopt two-stepG-matrix approximations for the Brueckner-Hartree-Fock (BHF) calculations. The first G matrix is to soften the bare force, and the second one is to include the high-order correlations of the interaction in medium. The first G-matrix calculation for two-nucleon interaction should be done in the center-of-mass coordinate. As another alternative BHF approach, we have adopted the V_(low-k) technique to soften the interaction and used the G matrix to include high-order correlations. The V_(low-k) renormalization leads to high-momentum and low-momentum components of the interaction decoupled. With the V_(low-k) potential, we have performed the BHF calculations for finite nuclei. The G-matrix elements with exact Pauli exclusions are calculated in the self-consistent BHF basis. To see effects from further possible correlations beyond BHF, we have simultaneously performed renormalized BHF (RBHF) calculations with the same potential. In RBHF, the mean field derived from realistic forces is modified by introducing the particle-occupation depletion resulting from many-body correlations. The ground-state energies and radii of the closed-shell nuclei, ~4He, ~(16)O, and ~(40)Ca, have been investigated. The convergences of the BHF and RBHF calculations have been discussed and compared with other ab initio calculations with the same potential.
机译:可以采用Brueckner-Hartree-Fock(BHF)计算的二阶矩阵近似。第一G矩阵是为了软化裸力,第二个G矩阵是包括介质中相互作用的高阶相关性。对于两个核子相互作用的第一个G矩阵计算应在质量中心坐标中进行。作为另一种替代的BHF方法,我们采用了V_(低k)技术来软化交互并使用G矩阵来包括高阶相关性。 V_(低k)的重整化导致互动的较高动量和低动量分量分离。通过V_(低k)潜力,我们已经执行了有限核的BHF计算。具有精确保罗排除的G矩阵元素以自我支撑的BHF计算。要从BHF之外的进一步可能的相关性看,我们同时执行具有相同电位的重字化的BHF(RBHF)计算。在RBF中,通过引入由许多身体相关产生的粒子职业耗尽来修改来自现实力的平均场。已经研究了闭合壳核,〜4He,〜(16)O和〜(40)CA的地位能量和半径。已经讨论了BHF和RBHF计算的收敛,并与具有相同潜力的其他AB Initio计算进行了比较。

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  • 来源
    《Physical Review C》 |2017年第2017期|034321.1-034321.10|共10页
  • 作者单位

    School of Physics and State Key Laboratory of Nuclear Physics and Technology Peking University Beijing 100871 China;

    School of Physics and State Key Laboratory of Nuclear Physics and Technology Peking University Beijing 100871 China;

    School of Physics and State Key Laboratory of Nuclear Physics and Technology Peking University Beijing 100871 China;

    School of Physics and State Key Laboratory of Nuclear Physics and Technology Peking University Beijing 100871 China;

    School of Physics and State Key Laboratory of Nuclear Physics and Technology Peking University Beijing 100871 China;

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