Conformally-flat, non-singular static metric in infinite derivative gravity

Detalhes bibliográficos
Autor(a) principal: Buoninfante, Luca
Data de Publicação: 2018
Outros Autores: Koshelev, Alexey, Lambiase, Gaetano, Marto, João, Mazumdar, Anupam
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)
Texto Completo: http://hdl.handle.net/10400.6/6475
Resumo: In Einstein's theory of general relativity the vacuum solution yields a blackhole with a curvature singularity, where there exists a point-like source with a Dirac delta distribution which is introduced as a boundary condition in the static case. It has been known for a while that ghost-free infinite derivative theory of gravity can ameliorate such a singularity at least at the level of linear perturbation around the Minkowski background. In this paper, we will show that the Schwarzschild metric does not satisfy the boundary condition at the origin within in nite derivative theory of gravity, since a Dirac delta source is smeared out by non-local gravitational interaction. We will also show that the spacetime metric becomes conformally-flat and singularity-free within the non-local region, which can be also made devoid of an event horizon. Furthermore, the scale of non-locality ought to be as large as that of the Schwarzschild radius, in such a way that the gravitational potential in any metric has to be always bounded by one, implying that gravity remains weak from the infrared all the way up to the ultraviolet regime, in concurrence with the results obtained in [arXiv:1707.00273]. The singular Schwarzschild blackhole can now be potentially replaced by a non-singular compact object, whose core is governed by the mass and the e efective scale of non-locality.
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spelling Conformally-flat, non-singular static metric in infinite derivative gravityGeneral relativityInfinite derivative gravityIn Einstein's theory of general relativity the vacuum solution yields a blackhole with a curvature singularity, where there exists a point-like source with a Dirac delta distribution which is introduced as a boundary condition in the static case. It has been known for a while that ghost-free infinite derivative theory of gravity can ameliorate such a singularity at least at the level of linear perturbation around the Minkowski background. In this paper, we will show that the Schwarzschild metric does not satisfy the boundary condition at the origin within in nite derivative theory of gravity, since a Dirac delta source is smeared out by non-local gravitational interaction. We will also show that the spacetime metric becomes conformally-flat and singularity-free within the non-local region, which can be also made devoid of an event horizon. Furthermore, the scale of non-locality ought to be as large as that of the Schwarzschild radius, in such a way that the gravitational potential in any metric has to be always bounded by one, implying that gravity remains weak from the infrared all the way up to the ultraviolet regime, in concurrence with the results obtained in [arXiv:1707.00273]. The singular Schwarzschild blackhole can now be potentially replaced by a non-singular compact object, whose core is governed by the mass and the e efective scale of non-locality.uBibliorumBuoninfante, LucaKoshelev, AlexeyLambiase, GaetanoMarto, JoãoMazumdar, Anupam2018-11-23T15:20:40Z20182018-01-01T00:00:00Zinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleapplication/pdfhttp://hdl.handle.net/10400.6/6475eng10.1088/1475-7516/2018/06/014metadata only accessinfo:eu-repo/semantics/openAccessreponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãoinstacron:RCAAP2023-12-15T09:44:57Zoai:ubibliorum.ubi.pt:10400.6/6475Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireopendoar:71602024-03-20T00:47:11.556911Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) - Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãofalse
dc.title.none.fl_str_mv Conformally-flat, non-singular static metric in infinite derivative gravity
title Conformally-flat, non-singular static metric in infinite derivative gravity
spellingShingle Conformally-flat, non-singular static metric in infinite derivative gravity
Buoninfante, Luca
General relativity
Infinite derivative gravity
title_short Conformally-flat, non-singular static metric in infinite derivative gravity
title_full Conformally-flat, non-singular static metric in infinite derivative gravity
title_fullStr Conformally-flat, non-singular static metric in infinite derivative gravity
title_full_unstemmed Conformally-flat, non-singular static metric in infinite derivative gravity
title_sort Conformally-flat, non-singular static metric in infinite derivative gravity
author Buoninfante, Luca
author_facet Buoninfante, Luca
Koshelev, Alexey
Lambiase, Gaetano
Marto, João
Mazumdar, Anupam
author_role author
author2 Koshelev, Alexey
Lambiase, Gaetano
Marto, João
Mazumdar, Anupam
author2_role author
author
author
author
dc.contributor.none.fl_str_mv uBibliorum
dc.contributor.author.fl_str_mv Buoninfante, Luca
Koshelev, Alexey
Lambiase, Gaetano
Marto, João
Mazumdar, Anupam
dc.subject.por.fl_str_mv General relativity
Infinite derivative gravity
topic General relativity
Infinite derivative gravity
description In Einstein's theory of general relativity the vacuum solution yields a blackhole with a curvature singularity, where there exists a point-like source with a Dirac delta distribution which is introduced as a boundary condition in the static case. It has been known for a while that ghost-free infinite derivative theory of gravity can ameliorate such a singularity at least at the level of linear perturbation around the Minkowski background. In this paper, we will show that the Schwarzschild metric does not satisfy the boundary condition at the origin within in nite derivative theory of gravity, since a Dirac delta source is smeared out by non-local gravitational interaction. We will also show that the spacetime metric becomes conformally-flat and singularity-free within the non-local region, which can be also made devoid of an event horizon. Furthermore, the scale of non-locality ought to be as large as that of the Schwarzschild radius, in such a way that the gravitational potential in any metric has to be always bounded by one, implying that gravity remains weak from the infrared all the way up to the ultraviolet regime, in concurrence with the results obtained in [arXiv:1707.00273]. The singular Schwarzschild blackhole can now be potentially replaced by a non-singular compact object, whose core is governed by the mass and the e efective scale of non-locality.
publishDate 2018
dc.date.none.fl_str_mv 2018-11-23T15:20:40Z
2018
2018-01-01T00:00:00Z
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dc.relation.none.fl_str_mv 10.1088/1475-7516/2018/06/014
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