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arXiv 0811.0578gr-qc
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两种非共动刚性流体的径向运动和球对称

Two non-comoving stiff fluids in radial motion and spherical symmetry

Valentin Kostov

摘要:

本文讨论了两种刚性流体(能量密度=压力)在球对称条件下作径向运动的问题。度量测量被选择为球对称的,共形静态的乘法分离的变量。第一流体通过无质量标量场进行数学描述。坐标系被选择为与第二流体一起运动,变量分离要求第二流体也是刚性的。流体只在重力作用下相互作用,它们的能量动量张量分别守恒。将爱因斯坦方程化为一个二阶非线性常微分方程,并由此导出一个Abel常微分方程。使用多项式分析法找到了一些特殊的精确解。解中的两个非共动引力源既可以解释为标量场,也可以解释为刚性流体。一个完整的分析进行的参数范围内的硬流体的解释是物理上可接受的。推导出解的共形向量的一般公式。通过使第二流体为零,产生了几个单标量场解,其中一些似乎是新的。本文所考虑的所有解在原点都有类时奇点(除了平凡的FRW解),并且不是渐近平坦的(除了k=0的静态解)。

英文摘要:

The problem of two stiff fluids (energy density = pressure) moving radially in spherical symmetry is treated. The metric ansatz is chosen spherically symmetric, conformally static with a multiplicative separation of variables. The first fluid is described mathematically via a massless scalar field. The coordinate system is chosen comoving with the second fluid which the separation of variables requires to be stiff too. The fluids are interacting only gravitationally and their energy momentum tensors are separately conserved. The Einstein equations are reduced to a single nonlinear ODE of second order which is shown to lead to an Abel ODE. A few particular exact solutions were found using a polynomial ansatz. The two non-comoving gravitational sources in the solutions can be interpreted either as scalar fields or stiff fluids. A complete analysis is performed on the range of parameters for which the stiff fluid interpretation is physically acceptable. General formulas are derived for the conformal vectors of the solutions. By making the second fluid vanish, a few single scalar field solutions are generated some of which appear to be new. All solutions considered in this paper have a time-like singularity at the origin (except the trivial FRW one) and are not asymptotically flat (except the static one with k=0).

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