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Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. XVI. Inclusion of self-energy effects in pairing

机译:斯基尔梅 - Hartree-Fock-Bogoliubov质量配方的进一步探索。 XVI。 将自能效应纳入配对

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Extending our earlier work, a new family of three Hartree-Fock-Bogoliubov (HFB) mass models, labeled HFB-30, HFB-31, and HFB-32, is presented, along with their underlying interactions, BSk30, BSk31, and BSk32, respectively. The principle new feature is a purely phenomenological pairing term that depends on the density gradient. This enables us to have a bulk pairing term that is fitted to realistic nuclear-matter calculations in which for the first time the self-energy corrections are included, while the behavior of the nucleon effective masses in asymmetric homogeneous nuclear matter is significantly improved. Furthermore, in the particle-hole channel all the highly realistic constraints of our earlier work are retained. In particular, the unconventional Skyrme forces containing t(4) and t(5) terms are still constrained to fit realistic equations of state of neutron matter stiff enough to support the massive neutron stars PSR J1614-2230 and PSR J0348+0432. All unphysical long-wavelength spin and spin-isospin instabilities of nuclear matter, including the unphysical transition to a polarized state in neutron-star matter, are eliminated. Our three interactions are characterized by values of the symmetry coefficient J of 30, 31, and 32 MeV, respectively. The best fit to the database of 2353 nuclear masses is found for model HFB-31 (J = 31 MeV) with a model error of 0.561 MeV. This model also fits the charge-radius data with an root-mean-square error of 0.027 fm.
机译:延长我们的早期工作,提供了一个新的三个Hartree-Fock-Bogoliubov(HFB)质量模型,标记为HFB-30,HFB-31和HFB-32,以及其潜在的交互,BSK30,BSK31和BSK32 , 分别。该原理新特征是纯粹的现象学配对项,其取决于密度梯度。这使我们能够拥有散装配对项,该术语适合于现实的核问题计算,其中第一次包括自能校正,而不对称均匀核物质的核仁有效质量的行为得到显着改善。此外,在粒子孔通道中,保留了我们之前工作的所有高度现实的约束。特别地,含有T(4)和T(5)项的非传统kyrme力仍然受到限制,以适应中子物质刚性的现实方程,足以支撑大规模中子恒星PSRJ1614-2230和PSRJ0348 + 0432。消除了所有不受神经的长波长旋转和旋流型核物质的旋转型,包括在中子星物中的不透视到偏振状态的不椎间膜物质。我们的三个相互作用分别表征了30,31和32MeV的对称系数J的值。最适合于2353核群体的数据库,用于模型HFB-31(J = 31 MEV),模型误差为0.561 MEV。该模型也适用于电荷半径数据,具有0.027 fm的根均方误差。

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