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首页> 外文期刊>The Astrophysical journal >Post-Newtonian Treatment of Bar Mode Instability in Rigidly Rotating Equilibrium Configurations for Polytropic Stars
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Post-Newtonian Treatment of Bar Mode Instability in Rigidly Rotating Equilibrium Configurations for Polytropic Stars

机译:多变恒星刚性旋转平衡构型下棒模不稳定性的牛顿后处理

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In this paper we determine the onset point of secular instability for the nonaxisymmetric bar mode in rigidly rotating equilibrium configurations in the post-Newtonian approximation, in order to apply it to neutron stars. The treatment is based on a precedent Newtonian analytic energy variational method that we have extended to the post-Newtonian case. This method, based on Landau's theory of second-order phase transitions, provides the critical value of the ellipsoid polar eccentricity e at the onset of instability, i.e., at the bifurcation point from the axisymmetric Maclaurin to the triaxial Jacobi ellipsoids, and it is valid for any equation of state. The extension of this method to post-Newtonian fluid configurations has been accomplished by combining two earlier orthogonal works, specialized, respectively, to slow rotating configurations but with arbitrary density profile and to constant mass density but arbitrarily fast rotating ellipsoids. We also determine the explicit expressions for the density functionals that allow the generalization of the physical quantities involved in our treatment from the constant mass density to an arbitrary density profile form. We find that, considering homogeneous ellipsoids, the value of the critical eccentricity increases as the stars become more relativistic, in qualitative agreement with previous investigations but with a less marked amount of such an increase. Then we have studied the dependence of this critical value on the configuration equation of state. Considering polytropic matter distributions, we find that the increase in the eccentricity at the onset of instability with the star compactness is confirmed for softer equations of state (with respect to the incompressible case). The amount of this stabilizing effect is nearly independent of the polytropic index.
机译:在本文中,我们确定了牛顿后近似中刚性旋转平衡构型中非轴对称棒模式的长期不稳定性起点,以便将其应用于中子星。这种处理是基于先例的牛顿解析能量变分方法,该方法已经扩展到后牛顿的情况。该方法基于Landau的二阶相变理论,在不稳定性开始时(即从轴对称Maclaurin到三轴Jacobi椭球的分叉点)提供了椭球极性偏心率e的临界值,并且是有效的对于任何状态方程。该方法扩展到牛顿后流体形态,是通过结合两个较早的正交工作而完成的,分别是专门针对慢速旋转形态但具有任意密度分布图和恒定质量密度但任意快速旋转的椭球体。我们还确定了密度泛函的显式表达式,该泛函允许对从恒定质量密度到任意密度分布形式的治疗中涉及的物理量进行泛化。我们发现,考虑到均匀的椭球体,与恒星变得相对论时,临界偏心率的值会增加,这与以前的研究在质量上吻合,但这种增加的幅度较小。然后,我们研究了该临界值对状态组态方程的依赖性。考虑多方物质分布,我们发现对于较软的状态方程(相对于不可压缩的情况),在不稳定性开始时的偏心率随星形密实度的增加得到了确认。这种稳定作用的量几乎与多变指数无关。

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