New interpretation of the original charged BTZ black hole spacetime

IF 3.6 3区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS
Tomáš Hale, Brayden R Hull, David Kubizňák, Robert B Mann and Jana Menšíková
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引用次数: 0

Abstract

In their seminal 1992 paper, Bañados, Teitelboim and Zanelli (BTZ) proposed a simple charged generalization of what is now known as the spinning BTZ black hole, the proposal being that a rotating metric can be supported by a ‘static vector’ potential. While with such an ansatz the Einstein equations are satisfied, and the corresponding energy-momentum tensor is divergence-less, the Maxwell equations do not (due to the special degenerate form of the corresponding field strength) hold. More recently, Deshpande and Lunin have proposed a generalized ‘Einstein–Maxwell’ system that yields analytic rotating black holes in all odd dimensions. In this paper, we show that the original charged BTZ solution can be re-interpreted as a solution of the Deshpande–Lunin theory. Moreover, as we shall explicitly illustrate on an example of regularized conformal electrodynamics, a similar construction also works for any non-linear electrodynamics in 3-dimensions. At the same time, all these spacetimes represent self-gravitating solutions of (non-linear electrodynamics generalized) force-free electrodynamics.
对原带电BTZ黑洞时空的新解释
在他们1992年的开创性论文Bañados中,Teitelboim和Zanelli (BTZ)提出了一个简单的带电概化,现在被称为旋转BTZ黑洞,该提议是旋转度规可以由“静态矢量”势支持。在这样的反态下,爱因斯坦方程是满足的,相应的能量动量张量是无散度的,而麦克斯韦方程则不成立(由于相应场强的特殊简并形式)。最近,Deshpande和Lunin提出了一个广义的“爱因斯坦-麦克斯韦”系统,该系统可以在所有奇维空间产生解析旋转黑洞。在本文中,我们证明了原来的带电BTZ解可以被重新解释为Deshpande-Lunin理论的解。此外,正如我们将在正则共形电动力学的例子中明确说明的那样,类似的结构也适用于任何三维的非线性电动力学。同时,所有这些时空都表示(非线性电动力学广义)无力电动力学的自引力解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Classical and Quantum Gravity
Classical and Quantum Gravity 物理-天文与天体物理
CiteScore
7.00
自引率
8.60%
发文量
301
审稿时长
2-4 weeks
期刊介绍: Classical and Quantum Gravity is an established journal for physicists, mathematicians and cosmologists in the fields of gravitation and the theory of spacetime. The journal is now the acknowledged world leader in classical relativity and all areas of quantum gravity.
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