Chronology Protection of Rotating Black Holes in a Viable Lorentz-Violating Gravity

We study causal properties of the recently found rotating black-hole solution in the low-energy sector of Horava gravity as a viable Lorentz-violating (LV) gravity in four dimensions with the LV Maxwell field and a cosmological constant $Λ(>-3/a^2)$ for an arbitrary rotation parameter $a$. The region of non-trivial causality violation containing closed timelike curves is exactly the same as in the Kerr-Newman or the Kerr-Newman-(Anti-)de Sitter solution. Nevertheless, chronology is protected in the new rotating black hole because the causality violating region becomes physically inaccessible by exterior observers due to the new three-curvature singularity at its boundary that is topologically two-torus including the usual ring singularity at $(r,θ)=(0,π/2)$. As a consequence, the physically accessible region outside the torus singularity is causal everywhere.

Publication Details

Journal
ArXiv.org
Published
2025-09-24
Primary Topic
Energy Efficiency and Management
Type
article
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article

Chronology Protection of Rotating Black Holes in a Viable Lorentz-Violating Gravity

ArXiv.org
Energy Efficiency and Management
article

Chronology Protection of Rotating Black Holes in a Viable Lorentz-Violating Gravity

article en

Abstract

We study causal properties of the recently found rotating black-hole solution in the low-energy sector of Horava gravity as a viable Lorentz-violating (LV) gravity in four dimensions with the LV Maxwell field and a cosmological constant $Λ(>-3/a^2)$ for an arbitrary rotation parameter $a$. The region of non-trivial causality violation containing closed timelike curves is exactly the same as in the Kerr-Newman or the Kerr-Newman-(Anti-)de Sitter solution. Nevertheless, chronology is protected in the new rotating black hole because the causality violating region becomes physically inaccessible by exterior observers due to the new three-curvature singularity at its boundary that is topologically two-torus including the usual ring singularity at $(r,θ)=(0,π/2)$. As a consequence, the physically accessible region outside the torus singularity is causal everywhere.

ArXiv.org
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Energy Efficiency and Management
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Chronology Protection of Rotating Black Holes in a Viable Lorentz-Violating Gravity · ArXiv.org (2025) | TGRS Research Map | TGRS