Towards the intermolecular force in charged AdS black hole

Van Quyet Hoang, Huu Phat Tran, Tuan Anh Nguyen
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Abstract

In this paper we attempt to find the intermolecular force of charged AdS black holes (BH). We first write the equation of state of BH in the form of the van der Waals (vdW) equation and show that this equation describes accurately the BH phase transition. Based on the Lennard- Jones (LJ) potential we establish the modified LJ force which is compatible with this vdW equation. Of particular interest, in the first time we find that this force can be always written as the sum of the topological force, created by the topological charge, and the electrostatic force, created by charged conducting micro-sphere with definite radius. Then the phase transition of BH is totally controlled by these forces. In the process of phase transition from small to large BHs the sum of these forces changes from repulsive to attractive forces and this behavior is supported by the scalar curvature of the thermodynamic geometry. Combining these properties, we arrive at the physical picture of the BH molecules: they behave like charged conducting micro-spheres which bear topological charge. It necessarily to remark that although our intermolecular force is better than the one obtained recently in [29], it remains an approximate force.
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迈向带电 AdS 黑洞中的分子间力
本文试图找出带电 AdS 黑洞(BH)的分子间作用力。我们首先以范德华(vdW)方程的形式写出了黑洞的状态方程,并证明该方程准确地描述了黑洞的相变。基于伦纳德-琼斯(LJ)势,我们建立了与 vdW 方程兼容的修正 LJ 力。特别有趣的是,我们首次发现这种力总是可以写成拓扑电荷产生的拓扑力与带电导电微球产生的静电力之和。因此,BH 的相变完全由这些力控制。在从小球到大球的相变过程中,这些力的总和会从排斥力变为吸引力,这种行为得到热力学几何标量曲率的支持。结合这些特性,我们得出了 BH 分子的物理图景:它们就像带电的导电微球,带有拓扑电荷。必须指出的是,尽管我们的分子间作用力比最近在文献[29]中得到的要好,但它仍然是一种近似的作用力。
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