论文标题

来自rényi统计的新兴阶段,热力学几何形状和带电的黑洞的关键性

Emergent Phase, Thermodynamic Geometry and Criticality of Charged Black Holes from Rényi Statistics

论文作者

Hirunsirisawat, Ekapong, Nakarachinda, Ratchaphat, Promsiri, Chatchai

论文摘要

最近,使用Rényi统计数据,可以从热力学的考虑考虑到渐近平坦的Reissner-Nordström黑洞(RN-AF)中发生新的新兴阶段。我们介绍了RN-AF在Gibbs-Boltzmann(GB)和替代性Rényi统计数据中的热力学和机械稳定性的分析,分别将$ Q $和静电电位$ ϕ $视为压力和体积。有趣的是,在Rényi热力学框架中,RN-AF的新兴阶段可以在热力学和机械上稳定。随着麦克斯韦相等的面积法在$ q-ϕ $平面中的构建,可以在某些电荷值中找到近超级黑洞相和新兴相之间的共存线,这可以作为液体和气相共存的蒸气压。在热力学几何形状的方面,黑洞微观结构之间的微观相互作用在Rényi描述中可能令人反感。这意味着可以通过远程相互作用系统的非xtentigentiatentival性质出现自我散发系统的微骨之间的新型相关性。最后,我们还研究了Rényi统计中RN-AF的关键现象与范德华(VDW)流体相比,发现两个系统相关物理量的关键指数都是相同的。这意味着两个系统都处于相变的相同通用类别中。

Recently, a novel emergent phase can occur from thermodynamic consideration of the asymptotically flat Reissner-Nordström black hole (RN-AF) using Rényi statistics. We present an analysis of the thermodynamical and mechanical stabilities of the RN-AF in both the Gibbs-Boltzmann (GB) and the alternative Rényi statistics when charge $q$ and electrostatic potential $ϕ$ are treated as pressure and volume, respectively. Interestingly, the emergent phase of the RN-AF can be both thermodynamically and mechanically stable in some range of parameters in the framework of Rényi thermodynamics. With the construction of the Maxwell equal area law in $q-ϕ$ plane, the coexistence line between the near-extremal black hole phase and the emergent phase can be found in some values of charge which can be associated as the vapor pressure at which the liquid and gas phases coexist. In the aspect of thermodynamic geometry, the microscopic interaction between the black hole microstructures can be repulsive in the Rényi description. This implies that a novel correlation between the microstates of a self-gravitating system could be emerged via the nonextensive nature of long-range interaction systems. Finally, we also investigate the critical phenomena of the RN-AF in Rényi statistics compared to that of the van der Waals (vdW) fluid and find that the critical exponents of the relevant physical quantities of both systems are identical. This implies that both systems are in the same universality class of the phase transition.

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