Generalized supergravity equations for the WZW model

Generalized supergravity equations (GSEs) were originally proposed as a modification of the standard IIB supergravity equations to satisfy the background of η-deformed AdS5×S5 introduced by Arutyunov et al. In this study, we proceed to write down the GSEs for the Wess-Zumino-Witten (WZW) models based on Lie groups. First, we simplify the GSEs for the WZW model by imposing the conditions for vanishing of the one-loop beta function equations. Then, by introducing an Ansatz for the Killing vector field I, it is shown that the Killing equation LIGμν=0 is held. In addition, we introduce a generalized Killing vector such that the existence of a solution to the GSEs requires that this vector be light-like. In this way, we solve the simplified GSEs for the WZW models constructed on Lie groups up to dimension five. Unfortunately, two of the groups do not have light-like vectors and therefore do not admit the GSEs.

Authors

Publication Details

Journal
Physics Letters B
Published
2024-11-28
DOI
https://doi.org/10.1016/j.physletb.2024.139159
Citations
2
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
1.32

Funders

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article

Generalized supergravity equations for the WZW model

A. Rezaei-Aghdam, Ali Eghbali, Simin Ghasemi-Sorkhabi
2 citations
Physics Letters B
Black Holes and Theoretical Physics
1.32
article

Generalized supergravity equations for the WZW model

A. Rezaei-Aghdam, Ali Eghbali, Simin Ghasemi-Sorkhabi
article en
2 citations

Abstract

Generalized supergravity equations (GSEs) were originally proposed as a modification of the standard IIB supergravity equations to satisfy the background of η-deformed AdS5×S5 introduced by Arutyunov et al. In this study, we proceed to write down the GSEs for the Wess-Zumino-Witten (WZW) models based on Lie groups. First, we simplify the GSEs for the WZW model by imposing the conditions for vanishing of the one-loop beta function equations. Then, by introducing an Ansatz for the Killing vector field I, it is shown that the Killing equation LIGμν=0 is held. In addition, we introduce a generalized Killing vector such that the existence of a solution to the GSEs requires that this vector be light-like. In this way, we solve the simplified GSEs for the WZW models constructed on Lie groups up to dimension five. Unfortunately, two of the groups do not have light-like vectors and therefore do not admit the GSEs.

Physics Letters BVol. 860
Azarbaijan Shahid Madani University
Openalex Percentile: Top 10%
Black Holes and Theoretical Physics
1.32
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