U(1) gauge vector field on a codimension-2 brane

Abstract In this paper, we obtain a gauge invariant effective action for a bulk massless U(1) gauge vector field on a brane with codimension two by using a general Kaluza-Klein (KK) decomposition for the field. It suggests that there exist two types of scalar KK modes to keep the gauge invariance of...

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Main Authors: Chun-E Fu, Yuan Zhong, Yu-Xiao Liu
Format: Article
Language:English
Published: SpringerOpen 2019-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP01(2019)021
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author Chun-E Fu
Yuan Zhong
Yu-Xiao Liu
author_facet Chun-E Fu
Yuan Zhong
Yu-Xiao Liu
author_sort Chun-E Fu
collection DOAJ
description Abstract In this paper, we obtain a gauge invariant effective action for a bulk massless U(1) gauge vector field on a brane with codimension two by using a general Kaluza-Klein (KK) decomposition for the field. It suggests that there exist two types of scalar KK modes to keep the gauge invariance of the action for the massive vector KK modes. Both the vector and scalar KK modes can be massive. The masses of the vector KK modes m (n) contain two parts, m 1 (n) and m 2 (n) , due to the existence of the two extra dimensions. The masses of the two types of scalar KK modes m ϕ (n) and m φ (n) are related to the vector ones, i.e., m ϕ (n)  = m 1 (n) and m φ (n)  = m 2 (n) . Moreover, we derive two Schrödinger-like equations for the vector KK modes, for which the effective potentials are just the functions of the warp factor.
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spelling doaj.art-d0146ba6427949e9adbb8d62a96ebcb62022-12-21T18:01:51ZengSpringerOpenJournal of High Energy Physics1029-84792019-01-012019111610.1007/JHEP01(2019)021U(1) gauge vector field on a codimension-2 braneChun-E Fu0Yuan Zhong1Yu-Xiao Liu2School of Science, Xi’an Jiaotong UniversitySchool of Science, Xi’an Jiaotong UniversityInstitute of Theoretical Physics & Research Center of Gravitation, Lanzhou UniversityAbstract In this paper, we obtain a gauge invariant effective action for a bulk massless U(1) gauge vector field on a brane with codimension two by using a general Kaluza-Klein (KK) decomposition for the field. It suggests that there exist two types of scalar KK modes to keep the gauge invariance of the action for the massive vector KK modes. Both the vector and scalar KK modes can be massive. The masses of the vector KK modes m (n) contain two parts, m 1 (n) and m 2 (n) , due to the existence of the two extra dimensions. The masses of the two types of scalar KK modes m ϕ (n) and m φ (n) are related to the vector ones, i.e., m ϕ (n)  = m 1 (n) and m φ (n)  = m 2 (n) . Moreover, we derive two Schrödinger-like equations for the vector KK modes, for which the effective potentials are just the functions of the warp factor.http://link.springer.com/article/10.1007/JHEP01(2019)021Field Theories in Higher DimensionsSolitons Monopoles and Instantons
spellingShingle Chun-E Fu
Yuan Zhong
Yu-Xiao Liu
U(1) gauge vector field on a codimension-2 brane
Journal of High Energy Physics
Field Theories in Higher Dimensions
Solitons Monopoles and Instantons
title U(1) gauge vector field on a codimension-2 brane
title_full U(1) gauge vector field on a codimension-2 brane
title_fullStr U(1) gauge vector field on a codimension-2 brane
title_full_unstemmed U(1) gauge vector field on a codimension-2 brane
title_short U(1) gauge vector field on a codimension-2 brane
title_sort u 1 gauge vector field on a codimension 2 brane
topic Field Theories in Higher Dimensions
Solitons Monopoles and Instantons
url http://link.springer.com/article/10.1007/JHEP01(2019)021
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AT yuanzhong u1gaugevectorfieldonacodimension2brane
AT yuxiaoliu u1gaugevectorfieldonacodimension2brane