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Entropy of the Quantum Scalar Field in Static Black Holes

机译:静态黑洞中量子标量场的熵

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摘要

The quantum corrections to the entropy of static black holes are investigated by two methods: the brick wall method of 't Hooft and the Euclidean path integral approach of Gibbons and Hawking. Two general formulas for the entropy are obtained and some examples are considered. It is shown that if the contribution from the vacuum surrounding the system is ignored, then the two approaches give the same results. It is found that the entropy of the quantum scalar field in a general static black hole consists of two parts: a quadratically divergent term which takes a geometric character and a logarithmically divergent term which is not proportional to the horizon area. The logarithmically divergent term, in general, depends on the black hole characteristics (in particular, the whole entropy is determined only by this term for some extreme cases) and therefore cannot be neglected as a nonessential additive constant. The renormalization of the entropy is also discussed briefly.
机译:用两种方法研究了静态黑洞熵的量子校正:t Hooft的砖墙方法和Gibbons和Hawking的欧氏路径积分法。获得了两个熵的通用公式,并考虑了一些示例。结果表明,如果忽略了系统周围真空的贡献,那么两种方法将得出相同的结果。发现一般静态黑洞中量子标量场的熵由两部分组成:具有几何特征的二次发散项和与视界不成比例的对数发散项。通常,对数发散项取决于黑洞特性(特别是,在某些极端情况下,整个熵仅由该项确定),因此不能忽略其为非必要的加性常数。还简要讨论了熵的重新归一化。

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