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arXiv 1509.07142hep-th
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Horndeski引力中的黑洞熵和粘性束缚

Black Hole Entropy and Viscosity Bound in Horndeski Gravity

Xing-Hui Feng, Hai-Shan Liu, H. Lü, C. N. Pope

摘要:

Horndeski引力是一种耦合到标量场的引力理论,其中作用量包含标量通过其一阶导数与爱因斯坦张量或类似的高阶导数张量的额外非最小二次耦合,这些张量来自高斯-邦纳或洛夫洛克项的变化。在本文中,我们研究静态黑洞解的热力学$n$维,在最简单的情况下,Horndeski耦合到爱因斯坦张量。我们应用Wald形式主义计算的黑洞的熵,并表明,有一个额外的贡献,以上来自标准Wald熵公式。额外的贡献可以归因于标量场行为中的不寻常特征。我们还表明,一个传统的正则化计算欧几里德行动导致的熵不同意与沃尔德结果的表达。这似乎可能是由于减法程序中的模糊性。我们还计算了在对偶CFT的粘度,并表明,粘度/熵比可以违反$η/S\ge 1/(4π)$约束的适当选择的参数。

英文摘要:

Horndeski gravities are theories of gravity coupled to a scalar field, in which the action contains an additional non-minimal quadratic coupling of the scalar, through its first derivative, to the Einstein tensor or the analogous higher-derivative tensors coming from the variation of Gauss-Bonnet or Lovelock terms. In this paper we study the thermodynamics of the static black hole solutions in $n$ dimensions, in the simplest case of a Horndeski coupling to the Einstein tensor. We apply the Wald formalism to calculate the entropy of the black holes, and show that there is an additional contribution over and above those that come from the standard Wald entropy formula. The extra contribution can be attributed to unusual features in the behaviour of the scalar field. We also show that a conventional regularisation to calculate the Euclidean action leads to an expression for the entropy that disagrees with the Wald results. This seems likely to be due to ambiguities in the subtraction procedure. We also calculate the viscosity in the dual CFT, and show that the viscosity/entropy ratio can violate the $η/S\ge 1/(4π)$ bound for appropriate choices of the parameters.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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