Abstract

In this paper, we study Einstein gravity either minimally or non-minimally coupled to a vector field which breaks the gauge symmetry explicitly in general dimensions. We first consider a minimal theory which is simply the Einstein-Proca theory extended with a quartic self-interaction term for the vector field. We obtain its general static maximally symmetric black hole solution and study the thermodynamics using Wald formalism. The aspects of the solution are much like a Reissner-Nordstrøm black hole in spite of that a global charge cannot be defined for the vector. For non-minimal theories, we obtain a lot of exact black hole solutions, depending on the parameters of the theories. In particular, many of the solutions are general static and have maximal symmetry. However, there are some subtleties and ambiguities in the derivation of the first laws because the existence of an algebraic degree of freedom of the vector in general invalids the Wald entropy formula. The thermodynamics of these solutions deserves further studies.

Highlights

  • We will adopt the Wald formalism to derive the first law of thermodynamics for all the solutions we obtain

  • We study generalized Einstein-Proca theories in general dimensions by introducing either a quartic selfinteraction term for the vector or non-minimally coupled terms between the curvature and the vector

  • We find that there are two distinct class solutions, both of which are general static and have maximal symmetry, depending on whether Ar vanishes

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Summary

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To govern the validity of Wald entropy formula, one should impose proper boundary conditions on the horizon for both At and Ar , which in general results to a degenerate solution characterized by only one parameter, in contrast to the general two-parameter family solutions. This does not make sense in the derivation of the first law. 4–6, we study non-minimally coupled vector-tensor theories and obtain a lot of exact black hole solutions depending on the parameters of the theories.

Structure of general static solutions
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Wald formalism and thermodynamics
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Minimal theory
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Non-minimal theory: case I
The solution and thermodynamics
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Euclidean action
Non-minimal theory: case II
Unconventional black hole
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Stealth black hole and beyond
Without Proca mass
With Proca mass
Derivation of the solutions
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Planar black holes
Spherical black holes
Conclusions
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Full Text
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