Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant

We investigate the phase space of topological black hole solutions of su(N) Einstein–Yang–Mills theory in anti-de Sitter space with a purely magnetic gauge potential. The gauge field is described by N−1 magnetic gauge field functions ωj, j=1,…,N−1. For su(2) gauge group, the function ω1 has no zeros...

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Main Authors: J. Erik Baxter, Elizabeth Winstanley
Format: Article
Language:English
Published: Elsevier 2016-02-01
Series:Physics Letters B
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269315009715
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author J. Erik Baxter
Elizabeth Winstanley
author_facet J. Erik Baxter
Elizabeth Winstanley
author_sort J. Erik Baxter
collection DOAJ
description We investigate the phase space of topological black hole solutions of su(N) Einstein–Yang–Mills theory in anti-de Sitter space with a purely magnetic gauge potential. The gauge field is described by N−1 magnetic gauge field functions ωj, j=1,…,N−1. For su(2) gauge group, the function ω1 has no zeros. This is no longer the case when we consider a larger gauge group. The phase space of topological black holes is considerably simpler than for the corresponding spherically symmetric black holes, but for N>2 and a flat event horizon, there exist solutions where at least one of the ωj functions has one or more zeros. For most of the solutions, all the ωj functions have no zeros, and at least some of these are linearly stable.
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spelling doaj.art-b56e22cf6e1946b18e5efc0a3b7103842022-12-21T23:26:43ZengElsevierPhysics Letters B0370-26931873-24452016-02-01753C26827310.1016/j.physletb.2015.12.023Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constantJ. Erik Baxter0Elizabeth Winstanley1Norfolk Building, Sheffield Hallam University, 1 Howard Street, Sheffield, S1 1WB, United KingdomConsortium for Fundamental Physics, School of Mathematics and Statistics, The University of Sheffield, Hicks Building, Hounsfield Road, Sheffield, S3 7RH, United KingdomWe investigate the phase space of topological black hole solutions of su(N) Einstein–Yang–Mills theory in anti-de Sitter space with a purely magnetic gauge potential. The gauge field is described by N−1 magnetic gauge field functions ωj, j=1,…,N−1. For su(2) gauge group, the function ω1 has no zeros. This is no longer the case when we consider a larger gauge group. The phase space of topological black holes is considerably simpler than for the corresponding spherically symmetric black holes, but for N>2 and a flat event horizon, there exist solutions where at least one of the ωj functions has one or more zeros. For most of the solutions, all the ωj functions have no zeros, and at least some of these are linearly stable.http://www.sciencedirect.com/science/article/pii/S0370269315009715Topological black holesEinstein–Yang–Mills theory
spellingShingle J. Erik Baxter
Elizabeth Winstanley
Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant
Physics Letters B
Topological black holes
Einstein–Yang–Mills theory
title Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant
title_full Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant
title_fullStr Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant
title_full_unstemmed Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant
title_short Topological black holes in su(N) Einstein–Yang–Mills theory with a negative cosmological constant
title_sort topological black holes in su n einstein yang mills theory with a negative cosmological constant
topic Topological black holes
Einstein–Yang–Mills theory
url http://www.sciencedirect.com/science/article/pii/S0370269315009715
work_keys_str_mv AT jerikbaxter topologicalblackholesinsuneinsteinyangmillstheorywithanegativecosmologicalconstant
AT elizabethwinstanley topologicalblackholesinsuneinsteinyangmillstheorywithanegativecosmologicalconstant