Kasner eons in Lovelock black holes

In the vicinity of spacelike singularities, general relativity predicts that the metric behaves, at each point, as a Kasner space which undergoes a series of “Kasner epochs” and “eras” characterized by certain transition rules. The period during which this process takes place defines a “Kasner eon,” which comes to an end when higher-curvature or quantum effects become relevant. When higher-curvature densities are included in the action, spacetime can undergo transitions into additional Kasner eons. During each eon, the metric behaves locally as a Kasner solution to the higher-curvature density controlling the dynamics. In this paper we identify the presence of Kasner eons in the interior of static and spherically symmetric Lovelock gravity black holes. We determine the conditions under which eons occur and study the Kasner metrics which characterize them, as well as the transitions between them. We show that the null energy condition implies a monotonicity property for the effective Kasner exponent at the end of the Einsteinian eon. We also characterize the Kasner solutions of more general higher-curvature theories of gravity. In particular, we observe that the Einstein gravity condition that the sum of the Kasner exponents adds up to 1, <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:msubsup><a:mo>∑</a:mo><a:mrow><a:mi>i</a:mi><a:mo>=</a:mo><a:mn>1</a:mn></a:mrow><a:mrow><a:mi>D</a:mi><a:mo>−</a:mo><a:mn>1</a:mn></a:mrow></a:msubsup><a:msub><a:mi>p</a:mi><a:mi>i</a:mi></a:msub><a:mo>=</a:mo><a:mn>1</a:mn></a:math>, admits a universal generalization in the form of a family of Kasner metrics satisfying <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msubsup><c:mo>∑</c:mo><c:mrow><c:mi>i</c:mi><c:mo>=</c:mo><c:mn>1</c:mn></c:mrow><c:mrow><c:mi>D</c:mi><c:mo>−</c:mo><c:mn>1</c:mn></c:mrow></c:msubsup><c:msub><c:mi>p</c:mi><c:mi>i</c:mi></c:msub><c:mo>=</c:mo><c:mn>2</c:mn><c:mi>n</c:mi><c:mo>−</c:mo><c:mn>1</c:mn></c:math> which exists for any order-<e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>n</e:mi></e:math> higher-curvature density and in general dimensions. Published by the American Physical Society 2024

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Journal
Physical review. D/Physical review. D.
Published
2024-12-06
DOI
https://doi.org/10.1103/physrevd.110.124015
Citations
5
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
3.30

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article

Kasner eons in Lovelock black holes

Pablo A. Cano, Pablo Bueno, Robie A. Hennigar, Ming-Da Li
5 citations
Physical review. D/Physical review. D.
Black Holes and Theoretical Physics
3.30
article

Kasner eons in Lovelock black holes

Pablo A. Cano, Pablo Bueno, Robie A. Hennigar, Ming-Da Li
article en
5 citations

Abstract

In the vicinity of spacelike singularities, general relativity predicts that the metric behaves, at each point, as a Kasner space which undergoes a series of “Kasner epochs” and “eras” characterized by certain transition rules. The period during which this process takes place defines a “Kasner eon,” which comes to an end when higher-curvature or quantum effects become relevant. When higher-curvature densities are included in the action, spacetime can undergo transitions into additional Kasner eons. During each eon, the metric behaves locally as a Kasner solution to the higher-curvature density controlling the dynamics. In this paper we identify the presence of Kasner eons in the interior of static and spherically symmetric Lovelock gravity black holes. We determine the conditions under which eons occur and study the Kasner metrics which characterize them, as well as the transitions between them. We show that the null energy condition implies a monotonicity property for the effective Kasner exponent at the end of the Einsteinian eon. We also characterize the Kasner solutions of more general higher-curvature theories of gravity. In particular, we observe that the Einstein gravity condition that the sum of the Kasner exponents adds up to 1, <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:msubsup><a:mo>∑</a:mo><a:mrow><a:mi>i</a:mi><a:mo>=</a:mo><a:mn>1</a:mn></a:mrow><a:mrow><a:mi>D</a:mi><a:mo>−</a:mo><a:mn>1</a:mn></a:mrow></a:msubsup><a:msub><a:mi>p</a:mi><a:mi>i</a:mi></a:msub><a:mo>=</a:mo><a:mn>1</a:mn></a:math>, admits a universal generalization in the form of a family of Kasner metrics satisfying <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msubsup><c:mo>∑</c:mo><c:mrow><c:mi>i</c:mi><c:mo>=</c:mo><c:mn>1</c:mn></c:mrow><c:mrow><c:mi>D</c:mi><c:mo>−</c:mo><c:mn>1</c:mn></c:mrow></c:msubsup><c:msub><c:mi>p</c:mi><c:mi>i</c:mi></c:msub><c:mo>=</c:mo><c:mn>2</c:mn><c:mi>n</c:mi><c:mo>−</c:mo><c:mn>1</c:mn></c:math> which exists for any order-<e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>n</e:mi></e:math> higher-curvature density and in general dimensions. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(12)
Universitat de Barcelona (ES)
“la Caixa” Foundation, Ministerio de Ciencia e Innovación, Horizon 2020 Framework Programme, European Regional Development Fund, Agencia Estatal de Investigación, H2020 Marie Skłodowska-Curie Actions
Openalex Percentile: Top 6%
Black Holes and Theoretical Physics
3.30
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