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arXiv 1105.0201math.DGgr-qcmath-phmath.MP
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关于奇异半黎曼流形

On Singular Semi-Riemannian Manifolds

Ovidiu Cristinel Stoica

摘要:

在黎曼流形或半黎曼流形上,度量决定了像列维-奇维塔联络和黎曼曲率这样的不变量。如果度量退化(如奇异半黎曼几何),这些构造不再有效,因为它们是基于度量的逆,以及相关的运算,如共变指标之间的收缩。在这篇文章中,我们发展了奇异半黎曼流形的几何。首先,我们引入了一个不变的和规范的收缩之间的共变指标,适用于退化度量。这种收缩适用于一种特殊类型的张量场,它在收缩指数中是根零化子。然后,我们利用这种压缩和Koszul形式定义共变张量场的根零化子指标的共变导数,一类奇异半黎曼流形命名为根平稳。利用这一共变导数构造了黎曼曲率,并证明了在一类奇异半黎曼流形上,称为半正则流形,黎曼曲率是光滑的。我们应用这些结果来构建一个版本的爱因斯坦张量的密度的重量2保持光滑,即使在存在半正则奇点。因此,我们可以写出爱因斯坦方程的一个致密化版本,它是光滑的,并且如果度规是非简并的,它等价于标准爱因斯坦方程。

英文摘要:

On a Riemannian or a semi-Riemannian manifold, the metric determines invariants like the Levi-Civita connection and the Riemann curvature. If the metric becomes degenerate (as in singular semi-Riemannian geometry), these constructions no longer work, because they are based on the inverse of the metric, and on related operations like the contraction between covariant indices. In this article we develop the geometry of singular semi-Riemannian manifolds. First, we introduce an invariant and canonical contraction between covariant indices, applicable even for degenerate metrics. This contraction applies to a special type of tensor fields, which are radical-annihilator in the contracted indices. Then, we use this contraction and the Koszul form to define the covariant derivative for radical-annihilator indices of covariant tensor fields, on a class of singular semi-Riemannian manifolds named radical-stationary. We use this covariant derivative to construct the Riemann curvature, and show that on a class of singular semi-Riemannian manifolds, named semi-regular, the Riemann curvature is smooth. We apply these results to construct a version of Einstein's tensor whose density of weight 2 remains smooth even in the presence of semi-regular singularities. We can thus write a densitized version of Einstein's equation, which is smooth, and which is equivalent to the standard Einstein equation if the metric is non-degenerate.

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