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Quantum Instability for Charged Particles on Charged Nariai Black Hole Manifold: Exact 4D Results for Black Hole Discharge Phenomenon

机译:带电Nariai黑洞流形上带电粒子的量子不稳定性:黑洞放电现象的精确4D结果

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Spontaneous loss of charge by a charged black hole is a relevant topic in the framework of quantum effects in the field of a black hole. It belongs to the framework of phenomena which are due to vacuum instability in presence of an external field, with consequent pair creation. Quantum-electrodynamics effects in presence of an external electric field have been in particular a key-topic which has been extensively discussed. In black hole manifolds, discharge process has been considered at first in the case of Reissner-Nordstr?m black holes. Still, analytical results are limited to the semiclassical approximation (WKB). We first review some aspects of the theory of pair creation in presence of an external electrostatic field, as discussed in the seminal paper by J.Schwinger, and its relation with the so-called Klein paradox. Furthermore, we recall some basic aspects of pair creation in charged black hole backgrounds, with particular reference to the Damour-Deruelle-Ruffini method. Then we provide an example of exact calculations for the quantum instability which is at the root of the spontaneous discharge process for 4D charged black holes, by exploiting the property of the charged Nariai black hole background to allow to bring back the problem to a Kaluza-Klein reduction. Both the zeta-function approach and the transmission coefficient approach are taken into account in order to calculate the imaginary part of the effective action, which signals the presence of an instability phenomenon for the quantum vacuum. A comparison between the two methods is also provided, as well as a comparison with WKB results. Finally, we also take into account how thermal effects, which are associated with the presence of a non-zero black hole temperature, affect the discharge process.
机译:带电黑洞的自发电荷损失是黑洞领域量子效应框架中的一个相关主题。它属于现象的框架,这些现象是由于在外部场的存在下真空不稳定性造成的,因此产生了配对。特别是在存在外部电场的情况下的量子电动力学效应已经成为广泛讨论的关键话题。在黑孔歧管中,首先考虑使用Reissner-Nordstr?m黑孔的放电过程。尽管如此,分析结果仍限于半经典近似(WKB)。我们首先回顾一下在J.Schwinger的开创性论文中讨论的在外部静电场存在下的线对创建理论的某些方面,以及它与所谓的Klein悖论的关系。此外,我们还回顾了带电黑洞背景下线对创建的一些基本方面,特别是参考了Damour-Deruelle-Ruffini方法。然后,我们通过利用带电Nariai黑洞背景的性质将问题带回到Kaluza-中,提供了一个精确计算示例的量子不稳定性,它是4D带电黑洞自发放电过程的根本。减少克莱因。为了计算有效作用的虚部,必须同时考虑zeta函数法和透射系数法,这表明存在量子真空不稳定性现象。还提供了两种方法之间的比较,以及与WKB结果的比较。最后,我们还考虑了与非零黑洞温度相关的热效应如何影响放电过程。

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