论文标题

核面食在完全三维几何形状中的弹性特性

Elastic properties of nuclear pasta in a fully three-dimensional geometry

论文作者

Xia, Cheng-Jun, Maruyama, Toshiki, Yasutake, Nobutoshi, Tatsumi, Toshitaka, Zhang, Ying-Xun

论文摘要

对中子恒星物质的弹性特性的现实估计是在相对论均值模型的框架中具有较大的应变($ \ varepsilon \ sillesim 0.5 $),具有Thomas-Fermi近似值,其中各种晶体构型在具有全面的三维对称性中被认为是各种晶体构型。我们的计算证实了假设库仑晶体在中子滴水密度上方的液滴相位的有效性,尽管发现弹性常数在达到峰后正在减小,但在中子滴水密度高于中子滴水密度上方。同样,在不可压缩的液体滴度模型中得出的分析公式对小杆相的杆相的描述很好地描述了,从而高估了弹性常数在较大的密度下。对于平板,由于其厚度变化的疏忽,液体抽吸模型的分析公式定性地一致,但与我们的数值估计不一致。通过拟合数值结果,这些分析公式通过引入衰减因子得到改善。检查了核对称能的影响,采用两个参数集,对应于对称能量$ L = 41.34 $和89.39 MEV的斜率。即使是由多晶的各向异性引起的不确定性,以$ L = 41.34 $和89.39 MeV获得的中子恒星物质的弹性特性也有明显不同,从而导致各种中子星活动的可检测差异。

Realistic estimations on the elastic properties of neutron star matter are carried out with a large strain ($\varepsilon \lesssim 0.5$) in the framework of relativistic-mean-field model with Thomas-Fermi approximation, where various crystalline configurations are considered in a fully three-dimensional geometry with reflection symmetry. Our calculation confirms the validity of assuming Coulomb crystals for the droplet phase above neutron drip density, which nonetheless does not work at large densities since the elastic constants are found to be decreasing after reaching their peaks. Similarly, the analytic formulae derived in the incompressible liquid-drop model give excellent description for the rod phase at small densities, which overestimates the elastic constants at larger densities. For slabs, due to the negligence on the variations of their thicknesses, the analytic formulae from liquid-drop model agree qualitatively but not quantitatively with our numerical estimations. By fitting to the numerical results, these analytic formulae are improved by introducing dampening factors. The impacts of nuclear symmetry energy are examined adopting two parameter sets, corresponding to the slope of symmetry energy $L = 41.34$ and 89.39 MeV. Even with the uncertainties caused by the anisotropy in polycrystallines, the elastic properties of neutron star matter obtained with $L = 41.34$ and 89.39 MeV are distinctively different, results in detectable differences in various neutron star activities.

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