2019
DOI: 10.1007/jhep01(2019)021
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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 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 (n) 1 and m (n) 2 , due to the existence of the two extra dimensi… Show more

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Cited by 11 publications
(25 citation statements)
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“…Following the method in ref. [58], we proved that there is no contradiction among the consistency conditions in our model. It means that a fourdimensional free U(1) gauge field theory can be obtained by reducing the six-dimensional action.…”
Section: Jhep05(2021)017supporting
confidence: 50%
See 3 more Smart Citations
“…Following the method in ref. [58], we proved that there is no contradiction among the consistency conditions in our model. It means that a fourdimensional free U(1) gauge field theory can be obtained by reducing the six-dimensional action.…”
Section: Jhep05(2021)017supporting
confidence: 50%
“…propose a braneworld model which satisfies both the consistency conditions [58] and the localization conditions [35] of the free U(1) gauge field. We expect that our model has the following properties.…”
Section: Jhep05(2021)017mentioning
confidence: 99%
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“…Generally, for most of the models in co-dimendion 2 or higher, the free U (1) gauge field is already naturally confined just by minimum couplings with gravity [34][35][36][37]64,[70][71][72]. Thus, there are not many localization mechanisms for this field in those dimensional configurations.…”
Section: (Iv) Localization In Codimension 2 or Higher Modelsmentioning
confidence: 99%