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arXiv 2304.01807hep-thcond-mat.quant-gascond-mat.str-el
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在不违反KSS粘性界限的情况下破坏旋转对称性

Breaking rotations without violating the KSS viscosity bound

Matteo Baggioli, Sera Cremonini, Laura Early, Li Li, Hao-Tian Sun

AI总结:

本文在全息p波超流模型中研究旋转对称性破缺对剪切粘性与熵密度比的影响,推导出适用于显式破缺的视界公式,并证明即使旋转对称性被破坏,$η/s$在零温极限下仍不低于KSS界限$1/4π$。

摘要:

我们重新审视了全息p波超流模型中剪切粘性与熵密度之比的计算,重点关注旋转对称性破缺的作用。我们研究了显式对称性破缺与自发对称性破缺之间的相互作用,并推导出一个简单的视界公式来计算$η/s$,该公式在存在显式旋转破缺的情况下同样适用,并与数值数据完全一致。我们观察到,显式破坏旋转不变性的源会抑制破缺相中$η/s$的值,与自发对称性破缺的效应相互竞争。然而,在零温度极限下,$η/s$始终趋于一个常数值,且该值从不小于Kovtun-Son-Starinets(KSS)界限$1/4π$。这一行为似乎与先前的全息各向异性模型形成对比,后者发现$η/s$在低温下以幂律形式趋于零。我们证明这一差异源于极值极限下近视界几何的性质。因此,我们的构造表明,旋转对称性的破缺本身并不必然意味着违反KSS界限。

英文摘要:

We revisit the computation of the shear viscosity to entropy ratio in a holographic p-wave superfluid model, focusing on the role of rotational symmetry breaking. We study the interplay between explicit and spontaneous symmetry breaking and derive a simple horizon formula for $η/s$, which is valid also in the presence of explicit breaking of rotations and is in perfect agreement with the numerical data. We observe that a source which explicitly breaks rotational invariance suppresses the value of $η/s$ in the broken phase, competing against the effects of spontaneous symmetry breaking. However, $η/s$ always reaches a constant value in the limit of zero temperature, which is never smaller than the Kovtun-Son-Starinets (KSS) bound, $1/4π$. This behavior appears to be in contrast with previous holographic anisotropic models which found a power-law vanishing of $η/s$ at small temperature. This difference is shown to arise from the properties of the near-horizon geometry in the extremal limit. Thus, our construction shows that the breaking of rotations itself does not necessarily imply a violation of the KSS bound.

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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