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Exact Solutions of Einstein–Maxwell(-Dilaton) Equations with Discrete Translational Symmetry

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Einstein Equations: Local Energy, Self-Force, and Fields in General Relativity

Abstract

The aim of this work is to construct exact solutions of Einstein–Maxwell(-dilaton) equations possessing a discrete translational symmetry. We present two approaches to the problem. The first one is to solve Einstein–Maxwell equations in 4D, and the second one relies on dimensional reduction from 5D. We examine the geometry of the solutions, their horizons and singularities and compare them.

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Notes

  1. 1.

    The term extremal refers to the fact that the black hole horizons are degenerate, which in this case translates to their charges equal to their masses.

  2. 2.

    The number of spacelike dimensions is denoted as n.

  3. 3.

    Latin indices range over 1, …, n and label only spatial components, and Greek indices are 0, …, n.

  4. 4.

    The Laplacian for the spatial metric h is defined as \(\Delta _h f \equiv h^{ij} \nabla _{i} \nabla _{j} f = \frac {1}{\sqrt {\mathfrak {h}}} \left (\sqrt {\mathfrak {h}} h^{ij} f_{i}\right )_{,j}\).

  5. 5.

    Dirac comb is a periodic tempered distribution defined as

  6. 6.

    Modified Bessel function of the second kind Kν is defined as

    $$\displaystyle \begin{aligned} K_\nu \left(x\right) \equiv \int_{0}^{\infty} \exp \left(-x \text{cosh} t \right) \text{cosh}\left(\nu t\right) \mathrm{d}{t}, x > 0. \end{aligned}$$
  7. 7.

    From the Newton integral test, we get the following inequality for integrable, non-increasing and non-negative Cl:

    $$\displaystyle \begin{aligned} C_l \geq 0, \frac{\partial{C_l}}{\partial{l}} \leq 0 \, \forall l \geq 1, \sum_{l=1}^{\infty} C_l < \infty \Rightarrow \int_{1}^{\infty} C_l \mathrm{d}{l} \leq \sum_{l=1}^{\infty} C_l \leq C_1 + \int_{1}^{\infty} C_l \mathrm{d}{l}. \end{aligned}$$
  8. 8.

    For simple binary MP black holes in 5D, the horizon is not smooth. Thanks to the alignment of all black holes in the crystal, the horizons of individual black holes are smooth.

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Acknowledgements

J.R. was supported by grant GAUK 80918. M.Ž. acknowledges support by GACR 17-13525S.

Grants GAUK 80918, GACR 17-13525S.

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Correspondence to Jiří Ryzner .

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Ryzner, J., Žofka, M. (2022). Exact Solutions of Einstein–Maxwell(-Dilaton) Equations with Discrete Translational Symmetry. In: Cacciatori, S.L., Kamenshchik, A. (eds) Einstein Equations: Local Energy, Self-Force, and Fields in General Relativity. Tutorials, Schools, and Workshops in the Mathematical Sciences . Birkhäuser, Cham. https://doi.org/10.1007/978-3-031-21845-3_10

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