Hairy black-holes in shift-symmetric theories

Abstract Scalar hair of black holes in theories with a shift symmetry are constrained by the no-hair theorem of Hui and Nicolis, assuming spherical symmetry, time-independence of the scalar field and asymptotic flatness. The most studied counterexample is a linear coupling of the scalar with the Gau...

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Main Authors: Paolo Creminelli, Nicolás Loayza, Francesco Serra, Enrico Trincherini, Leonardo G. Trombetta
Format: Article
Language:English
Published: SpringerOpen 2020-08-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP08(2020)045
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spelling doaj-524b225362f5407088fe1851f53276d72020-11-25T02:50:28ZengSpringerOpenJournal of High Energy Physics1029-84792020-08-012020812410.1007/JHEP08(2020)045Hairy black-holes in shift-symmetric theoriesPaolo Creminelli0Nicolás Loayza1Francesco Serra2Enrico Trincherini3Leonardo G. Trombetta4ICTP, International Centre for Theoretical PhysicsIFIC, Universitat de Valencia — CSICScuola Normale SuperioreScuola Normale SuperioreScuola Normale SuperioreAbstract Scalar hair of black holes in theories with a shift symmetry are constrained by the no-hair theorem of Hui and Nicolis, assuming spherical symmetry, time-independence of the scalar field and asymptotic flatness. The most studied counterexample is a linear coupling of the scalar with the Gauss-Bonnet invariant. However, in this case the norm of the shift-symmetry current J 2 diverges at the horizon casting doubts on whether the solution is physically sound. We show that this is not an issue since J 2 is not a scalar quantity, since J μ is not a diffinvariant current in the presence of Gauss-Bonnet. The same theory can be written in Horndeski form with a non-analytic function G 5 ∼ log X . In this case the shift-symmetry current is diff-invariant, but contains powers of X in the denominator, so that its divergence at the horizon is again immaterial. We confirm that other hairy solutions in the presence of non-analytic Horndeski functions are pathological, featuring divergences of physical quantities as soon as one departs from time-independence and spherical symmetry. We generalise the no-hair theorem to Beyond Horndeski and DHOST theories, showing that the coupling with Gauss-Bonnet is necessary to have hair.http://link.springer.com/article/10.1007/JHEP08(2020)045Black HolesClassical Theories of Gravity
collection DOAJ
language English
format Article
sources DOAJ
author Paolo Creminelli
Nicolás Loayza
Francesco Serra
Enrico Trincherini
Leonardo G. Trombetta
spellingShingle Paolo Creminelli
Nicolás Loayza
Francesco Serra
Enrico Trincherini
Leonardo G. Trombetta
Hairy black-holes in shift-symmetric theories
Journal of High Energy Physics
Black Holes
Classical Theories of Gravity
author_facet Paolo Creminelli
Nicolás Loayza
Francesco Serra
Enrico Trincherini
Leonardo G. Trombetta
author_sort Paolo Creminelli
title Hairy black-holes in shift-symmetric theories
title_short Hairy black-holes in shift-symmetric theories
title_full Hairy black-holes in shift-symmetric theories
title_fullStr Hairy black-holes in shift-symmetric theories
title_full_unstemmed Hairy black-holes in shift-symmetric theories
title_sort hairy black-holes in shift-symmetric theories
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2020-08-01
description Abstract Scalar hair of black holes in theories with a shift symmetry are constrained by the no-hair theorem of Hui and Nicolis, assuming spherical symmetry, time-independence of the scalar field and asymptotic flatness. The most studied counterexample is a linear coupling of the scalar with the Gauss-Bonnet invariant. However, in this case the norm of the shift-symmetry current J 2 diverges at the horizon casting doubts on whether the solution is physically sound. We show that this is not an issue since J 2 is not a scalar quantity, since J μ is not a diffinvariant current in the presence of Gauss-Bonnet. The same theory can be written in Horndeski form with a non-analytic function G 5 ∼ log X . In this case the shift-symmetry current is diff-invariant, but contains powers of X in the denominator, so that its divergence at the horizon is again immaterial. We confirm that other hairy solutions in the presence of non-analytic Horndeski functions are pathological, featuring divergences of physical quantities as soon as one departs from time-independence and spherical symmetry. We generalise the no-hair theorem to Beyond Horndeski and DHOST theories, showing that the coupling with Gauss-Bonnet is necessary to have hair.
topic Black Holes
Classical Theories of Gravity
url http://link.springer.com/article/10.1007/JHEP08(2020)045
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