Abstract

In this work two new families of non-singular or regular black hole solutions are displayed. These black holes behave as de Sitter space near its center and have a well defined AdS asymptotic region for negative cosmological constant. These solutions are constructed on a general ground through the introduction of a finite density of mass/energy. This removes the usual singularity of a black hole and also introduces a new internal geometry. The thermodynamic properties of these solutions are discussed as well.

Highlights

  • One of the most relevant predictions of General Relativity was the existence of black holes and nowadays there is substantial evidence that this is a usual phenomenon in nature

  • For the physics of a black hole, this implies that the gravitational collapse stops before a singularity can be formed

  • In practice Planck stars can be studied as a geometry which far away from the core recovers a standard black hole solution, says Schwarzschild for instance, but whose center, contains a dense core, can still be treated as a manifold

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Summary

Introduction

One of the most relevant predictions of General Relativity was the existence of black holes and nowadays there is substantial evidence that this is a usual phenomenon in nature. The core of the geometry must approach, in a first approximation, a de Sitter space as such the geodesics diverge mimicking the repulsing force mentioned above This kind of solutions are called non-singular or regular black holes and in the context of this work can be considered synonyms to Planck star. It is direct to check that the equations of motion can be rewritten as This seems to indicate, as expected, that any Lovelock gravity should have for ground states constant curvature manifolds. It is direct to demonstrate that, in general, the κi can be complex numbers, even though ∀αp ∈ R This does restrict the possible constant curvature solutions, and so the potential ground states of the theory, and severely constraints the space of solutions with a well defined asymptotic region for arbitrary {αp}.

A well posed mass definition
First family of solutions: regular black holes in pure Lovelock theory
Global analysis
Internal geometry
The non spherical symmetric solutions
Horizons
Limits of this solution
The thermodynamics before the thermodynamics
Thermodynamics of asymptotically AdS solutions
Charges
Entropy
Temperature
Planck energy density
Structure of solutions
Heat capacity The heat capacity can be defined for Q constant as CQ dT
Conclusions and discussions

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