Naked singularities, topological defects and brane couplings

A conical defect in 2 + 1 anti-de Sitter space is a BTZ solution with a negative mass parameter. This is a naked singularity, but a rather harmless one: it is a point particle. Naturally, the energy density and the spacetime curvature have a δ-like singularity at the conical defect, but that does no...

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Publicado: 2011
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Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_02182718_v20_n5_p839_Edelstein
http://hdl.handle.net/20.500.12110/paper_02182718_v20_n5_p839_Edelstein
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spelling paper:paper_02182718_v20_n5_p839_Edelstein2025-07-30T17:59:51Z Naked singularities, topological defects and brane couplings brane couplings Naked singularities topological defects A conical defect in 2 + 1 anti-de Sitter space is a BTZ solution with a negative mass parameter. This is a naked singularity, but a rather harmless one: it is a point particle. Naturally, the energy density and the spacetime curvature have a δ-like singularity at the conical defect, but that does not give rise to any unphysical situations. Since the conical solution implies the presence of a source, applying reverse enginnering, one can identify the coupling term that is required in the action to account for that source. In that way, a relation is established between the identification operation that gives rise to the topological defect and the interaction term in the action that produces it. This idea has a natural extension to higher dimensions, where instead of a point particle (zero-brane) one finds membranes of even spatial dimensions (p-branes, with p = 2n). The generalization to other abelian and nonabelian gauge theories including (super-) gravities is fairly straightforward: the 2n-brane couples to a (2n + 1) ChernSimons form. The construction suggests a generic role for ChernSimons forms as the natural way to couple a gauge connection to a brane and avoids the inconsistency that results from the minimal coupling between a brane and a fundamental p-form field. © 2011 World Scientific Publishing Company. 2011 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_02182718_v20_n5_p839_Edelstein http://hdl.handle.net/20.500.12110/paper_02182718_v20_n5_p839_Edelstein
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic brane couplings
Naked singularities
topological defects
spellingShingle brane couplings
Naked singularities
topological defects
Naked singularities, topological defects and brane couplings
topic_facet brane couplings
Naked singularities
topological defects
description A conical defect in 2 + 1 anti-de Sitter space is a BTZ solution with a negative mass parameter. This is a naked singularity, but a rather harmless one: it is a point particle. Naturally, the energy density and the spacetime curvature have a δ-like singularity at the conical defect, but that does not give rise to any unphysical situations. Since the conical solution implies the presence of a source, applying reverse enginnering, one can identify the coupling term that is required in the action to account for that source. In that way, a relation is established between the identification operation that gives rise to the topological defect and the interaction term in the action that produces it. This idea has a natural extension to higher dimensions, where instead of a point particle (zero-brane) one finds membranes of even spatial dimensions (p-branes, with p = 2n). The generalization to other abelian and nonabelian gauge theories including (super-) gravities is fairly straightforward: the 2n-brane couples to a (2n + 1) ChernSimons form. The construction suggests a generic role for ChernSimons forms as the natural way to couple a gauge connection to a brane and avoids the inconsistency that results from the minimal coupling between a brane and a fundamental p-form field. © 2011 World Scientific Publishing Company.
title Naked singularities, topological defects and brane couplings
title_short Naked singularities, topological defects and brane couplings
title_full Naked singularities, topological defects and brane couplings
title_fullStr Naked singularities, topological defects and brane couplings
title_full_unstemmed Naked singularities, topological defects and brane couplings
title_sort naked singularities, topological defects and brane couplings
publishDate 2011
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_02182718_v20_n5_p839_Edelstein
http://hdl.handle.net/20.500.12110/paper_02182718_v20_n5_p839_Edelstein
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