Holographic vector superconductor in Gauss–Bonnet gravity

In the probe limit, we numerically study the holographic p-wave superconductor phase transitions in the higher curvature theory. Concretely, we study the influences of Gauss–Bonnet parameter α on the Maxwell complex vector model (MCV) in the five-dimensional Gauss–Bonnet–AdS black hole and soliton b...

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Main Authors: Jun-Wang Lu, Ya-Bo Wu, Tuo Cai, Hai-Min Liu, Yin-Shuan Ren, Mo-Lin Liu
Format: Article
Language:English
Published: Elsevier 2016-02-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321316000110
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spelling doaj-178010c49b234dea9e166b074d738de62020-11-24T21:41:37ZengElsevierNuclear Physics B0550-32131873-15622016-02-01903C36037310.1016/j.nuclphysb.2016.01.010Holographic vector superconductor in Gauss–Bonnet gravityJun-Wang Lu0Ya-Bo Wu1Tuo Cai2Hai-Min Liu3Yin-Shuan Ren4Mo-Lin Liu5Department of Physics and Electronic Science, Qiannan Normal College for Nationalities, Duyun 558000, PR ChinaDepartment of Physics, Liaoning Normal University, Dalian 116029, PR ChinaDepartment of Physics and Electronic Science, Qiannan Normal College for Nationalities, Duyun 558000, PR ChinaDepartment of Physics and Electronic Science, Qiannan Normal College for Nationalities, Duyun 558000, PR ChinaDepartment of Physics and Electronic Science, Qiannan Normal College for Nationalities, Duyun 558000, PR ChinaCollege of Physics and Electronic Engineering, Xinyang Normal University, Xinyang 464000, PR ChinaIn the probe limit, we numerically study the holographic p-wave superconductor phase transitions in the higher curvature theory. Concretely, we study the influences of Gauss–Bonnet parameter α on the Maxwell complex vector model (MCV) in the five-dimensional Gauss–Bonnet–AdS black hole and soliton backgrounds, respectively. In the two backgrounds, the improving Gauss–Bonnet parameter α and dimension of the vector operator Δ inhibit the vector condensate. In the black hole, the condensate quickly saturates a stable value at lower temperature. Moreover, both the stable value of condensate and the ratio ωg/Tc increase with α. In the soliton, the location of the second pole of the imaginary part increases with α, which implies that the energy of the quasiparticle excitation increases with the improving higher curvature correction. In addition, the influences of the Gauss–Bonnet correction on the MCV model are similar to the ones on the SU(2) p-wave model, which confirms that the MCV model is a generalization of the SU(2) Yang–Mills model even without the applied magnetic field to some extent.http://www.sciencedirect.com/science/article/pii/S0550321316000110
collection DOAJ
language English
format Article
sources DOAJ
author Jun-Wang Lu
Ya-Bo Wu
Tuo Cai
Hai-Min Liu
Yin-Shuan Ren
Mo-Lin Liu
spellingShingle Jun-Wang Lu
Ya-Bo Wu
Tuo Cai
Hai-Min Liu
Yin-Shuan Ren
Mo-Lin Liu
Holographic vector superconductor in Gauss–Bonnet gravity
Nuclear Physics B
author_facet Jun-Wang Lu
Ya-Bo Wu
Tuo Cai
Hai-Min Liu
Yin-Shuan Ren
Mo-Lin Liu
author_sort Jun-Wang Lu
title Holographic vector superconductor in Gauss–Bonnet gravity
title_short Holographic vector superconductor in Gauss–Bonnet gravity
title_full Holographic vector superconductor in Gauss–Bonnet gravity
title_fullStr Holographic vector superconductor in Gauss–Bonnet gravity
title_full_unstemmed Holographic vector superconductor in Gauss–Bonnet gravity
title_sort holographic vector superconductor in gauss–bonnet gravity
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
1873-1562
publishDate 2016-02-01
description In the probe limit, we numerically study the holographic p-wave superconductor phase transitions in the higher curvature theory. Concretely, we study the influences of Gauss–Bonnet parameter α on the Maxwell complex vector model (MCV) in the five-dimensional Gauss–Bonnet–AdS black hole and soliton backgrounds, respectively. In the two backgrounds, the improving Gauss–Bonnet parameter α and dimension of the vector operator Δ inhibit the vector condensate. In the black hole, the condensate quickly saturates a stable value at lower temperature. Moreover, both the stable value of condensate and the ratio ωg/Tc increase with α. In the soliton, the location of the second pole of the imaginary part increases with α, which implies that the energy of the quasiparticle excitation increases with the improving higher curvature correction. In addition, the influences of the Gauss–Bonnet correction on the MCV model are similar to the ones on the SU(2) p-wave model, which confirms that the MCV model is a generalization of the SU(2) Yang–Mills model even without the applied magnetic field to some extent.
url http://www.sciencedirect.com/science/article/pii/S0550321316000110
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AT tuocai holographicvectorsuperconductoringaussbonnetgravity
AT haiminliu holographicvectorsuperconductoringaussbonnetgravity
AT yinshuanren holographicvectorsuperconductoringaussbonnetgravity
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