Einstein-Gauss-Bonnet black strings at large D
Abstract We study the black string solutions in the Einstein-Gauss-Bonnet(EGB) theory at large D. By using the 1/D expansion in the near horizon region we derive the effective equations that describe the dynamics of the EGB black strings. The uniform and non-uniform black strings are obtained as the...
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doaj-ff708001e2c3446b8a2efa5bff3e23762020-11-25T00:36:10ZengSpringerOpenJournal of High Energy Physics1029-84792017-10-0120171012010.1007/JHEP10(2017)123Einstein-Gauss-Bonnet black strings at large DBin Chen0Peng-Cheng Li1Cheng-Yong Zhang2Department of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityDepartment of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityDepartment of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking UniversityAbstract We study the black string solutions in the Einstein-Gauss-Bonnet(EGB) theory at large D. By using the 1/D expansion in the near horizon region we derive the effective equations that describe the dynamics of the EGB black strings. The uniform and non-uniform black strings are obtained as the static solutions of the effective equations. From the perturbation analysis of the effective equations, we find that thin EGB black strings suffer from the Gregory-Laflamme instablity and the GB term weakens the instability when the GB coefficient is small, however, when the GB coefficient is large the GB term enhances the instability. Furthermore, we numerically solve the effective equations to study the non-linear instability. It turns out that the thin black strings are unstable to developing inhomogeneities along their length, and at late times they asymptote to the stable non-uniform black strings. The behavior is qualitatively similar to the case in the Einstein gravity. Compared with the black string instability in the Einstein gravity at large D, when the GB coefficient is small the time needed to reach to final state increases, but when the GB coefficient is large the time to reach to final state decreases. Starting from the point of view in which the effective equations can be interpreted as the equations for the dynamical fluid, we evaluate the transport coefficients and find that the ratio of the shear viscosity and the entropy density agrees with that obtained previously in the membrane paradigm after taking the large D limit.http://link.springer.com/article/10.1007/JHEP10(2017)123Black HolesClassical Theories of Gravity |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Bin Chen Peng-Cheng Li Cheng-Yong Zhang |
spellingShingle |
Bin Chen Peng-Cheng Li Cheng-Yong Zhang Einstein-Gauss-Bonnet black strings at large D Journal of High Energy Physics Black Holes Classical Theories of Gravity |
author_facet |
Bin Chen Peng-Cheng Li Cheng-Yong Zhang |
author_sort |
Bin Chen |
title |
Einstein-Gauss-Bonnet black strings at large D |
title_short |
Einstein-Gauss-Bonnet black strings at large D |
title_full |
Einstein-Gauss-Bonnet black strings at large D |
title_fullStr |
Einstein-Gauss-Bonnet black strings at large D |
title_full_unstemmed |
Einstein-Gauss-Bonnet black strings at large D |
title_sort |
einstein-gauss-bonnet black strings at large d |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2017-10-01 |
description |
Abstract We study the black string solutions in the Einstein-Gauss-Bonnet(EGB) theory at large D. By using the 1/D expansion in the near horizon region we derive the effective equations that describe the dynamics of the EGB black strings. The uniform and non-uniform black strings are obtained as the static solutions of the effective equations. From the perturbation analysis of the effective equations, we find that thin EGB black strings suffer from the Gregory-Laflamme instablity and the GB term weakens the instability when the GB coefficient is small, however, when the GB coefficient is large the GB term enhances the instability. Furthermore, we numerically solve the effective equations to study the non-linear instability. It turns out that the thin black strings are unstable to developing inhomogeneities along their length, and at late times they asymptote to the stable non-uniform black strings. The behavior is qualitatively similar to the case in the Einstein gravity. Compared with the black string instability in the Einstein gravity at large D, when the GB coefficient is small the time needed to reach to final state increases, but when the GB coefficient is large the time to reach to final state decreases. Starting from the point of view in which the effective equations can be interpreted as the equations for the dynamical fluid, we evaluate the transport coefficients and find that the ratio of the shear viscosity and the entropy density agrees with that obtained previously in the membrane paradigm after taking the large D limit. |
topic |
Black Holes Classical Theories of Gravity |
url |
http://link.springer.com/article/10.1007/JHEP10(2017)123 |
work_keys_str_mv |
AT binchen einsteingaussbonnetblackstringsatlarged AT pengchengli einsteingaussbonnetblackstringsatlarged AT chengyongzhang einsteingaussbonnetblackstringsatlarged |
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1725306481251713024 |