Supersymmetric domain walls in maximal 6D gauged supergravity III

We continue our study of gaugings the maximal \(N=(2,2)\) supergravity in six dimensions with gauge groups obtained from decomposing the embedding tensor under \(\mathbb{R}^+\times SO(4,4)\) subgroup of the global symmetry \(SO(5,5)\). Supersymmetry requires the embedding tensor to transform in \(\m...

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Published inarXiv.org
Main Authors Karndumri, Parinya, Nuchino, Patharadanai
Format Paper Journal Article
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 15.10.2024
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ISSN2331-8422
DOI10.48550/arxiv.2312.15777

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Abstract We continue our study of gaugings the maximal \(N=(2,2)\) supergravity in six dimensions with gauge groups obtained from decomposing the embedding tensor under \(\mathbb{R}^+\times SO(4,4)\) subgroup of the global symmetry \(SO(5,5)\). Supersymmetry requires the embedding tensor to transform in \(\mathbf{144}_c\) representation of \(SO(5,5)\). Under \(\mathbb{R}^+\times SO(4,4)\) subgroup, this leads to the embedding tensor in \((\mathbf{8}^{\pm 3}\), \(\mathbf{8}^{\pm 1},\mathbf{56}^{\pm 1})\) representations. Gaugings in \(\mathbf{8}^{\pm 3}\) representations lead to a translational gauge group \(\mathbb{R}^8\) while gaugings in \(\mathbf{8}^{\pm 1}\) representations give rise to gauge groups related to the scaling symmetry \(\mathbb{R}^+\). On the other hand, the embedding tensor in \(\mathbf{56}^{\pm 1}\) representations gives \(CSO(4-p,p,1)\sim SO(4-p,p)\ltimes \mathbb{R}^4\subset SO(4,4)\) gauge groups with \(p=0,1,2\). More interesting gauge groups can be obtained by turning on more than one representation of the embedding tensor subject to the quadratic constraints. In particular, we consider gaugings in both \(\mathbf{56}^{-1}\) and \(\mathbf{8}^{+3}\) representations giving rise to larger \(SO(5-p,p)\) and \(SO(4-p,p+1)\) gauge groups for \(p=0,1,2\). In this case, we also give a number of half-supersymmetric domain wall solutions preserving different residual symmetries. The solutions for gaugings obtained only from \(\mathbf{56}^{-1}\) representation are also included in these results when the \(\mathbf{8}^{+3}\) part is accordingly turned off.
AbstractList Eur. Phys. J. C84 (2024) 333 We continue our study of gaugings the maximal $N=(2,2)$ supergravity in six dimensions with gauge groups obtained from decomposing the embedding tensor under $\mathbb{R}^+\times SO(4,4)$ subgroup of the global symmetry $SO(5,5)$. Supersymmetry requires the embedding tensor to transform in $\mathbf{144}_c$ representation of $SO(5,5)$. Under $\mathbb{R}^+\times SO(4,4)$ subgroup, this leads to the embedding tensor in $(\mathbf{8}^{\pm 3}$, $\mathbf{8}^{\pm 1},\mathbf{56}^{\pm 1})$ representations. Gaugings in $\mathbf{8}^{\pm 3}$ representations lead to a translational gauge group $\mathbb{R}^8$ while gaugings in $\mathbf{8}^{\pm 1}$ representations give rise to gauge groups related to the scaling symmetry $\mathbb{R}^+$. On the other hand, the embedding tensor in $\mathbf{56}^{\pm 1}$ representations gives $CSO(4-p,p,1)\sim SO(4-p,p)\ltimes \mathbb{R}^4\subset SO(4,4)$ gauge groups with $p=0,1,2$. More interesting gauge groups can be obtained by turning on more than one representation of the embedding tensor subject to the quadratic constraints. In particular, we consider gaugings in both $\mathbf{56}^{-1}$ and $\mathbf{8}^{+3}$ representations giving rise to larger $SO(5-p,p)$ and $SO(4-p,p+1)$ gauge groups for $p=0,1,2$. In this case, we also give a number of half-supersymmetric domain wall solutions preserving different residual symmetries. The solutions for gaugings obtained only from $\mathbf{56}^{-1}$ representation are also included in these results when the $\mathbf{8}^{+3}$ part is accordingly turned off.
We continue our study of gaugings the maximal \(N=(2,2)\) supergravity in six dimensions with gauge groups obtained from decomposing the embedding tensor under \(\mathbb{R}^+\times SO(4,4)\) subgroup of the global symmetry \(SO(5,5)\). Supersymmetry requires the embedding tensor to transform in \(\mathbf{144}_c\) representation of \(SO(5,5)\). Under \(\mathbb{R}^+\times SO(4,4)\) subgroup, this leads to the embedding tensor in \((\mathbf{8}^{\pm 3}\), \(\mathbf{8}^{\pm 1},\mathbf{56}^{\pm 1})\) representations. Gaugings in \(\mathbf{8}^{\pm 3}\) representations lead to a translational gauge group \(\mathbb{R}^8\) while gaugings in \(\mathbf{8}^{\pm 1}\) representations give rise to gauge groups related to the scaling symmetry \(\mathbb{R}^+\). On the other hand, the embedding tensor in \(\mathbf{56}^{\pm 1}\) representations gives \(CSO(4-p,p,1)\sim SO(4-p,p)\ltimes \mathbb{R}^4\subset SO(4,4)\) gauge groups with \(p=0,1,2\). More interesting gauge groups can be obtained by turning on more than one representation of the embedding tensor subject to the quadratic constraints. In particular, we consider gaugings in both \(\mathbf{56}^{-1}\) and \(\mathbf{8}^{+3}\) representations giving rise to larger \(SO(5-p,p)\) and \(SO(4-p,p+1)\) gauge groups for \(p=0,1,2\). In this case, we also give a number of half-supersymmetric domain wall solutions preserving different residual symmetries. The solutions for gaugings obtained only from \(\mathbf{56}^{-1}\) representation are also included in these results when the \(\mathbf{8}^{+3}\) part is accordingly turned off.
Author Nuchino, Patharadanai
Karndumri, Parinya
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BackLink https://doi.org/10.48550/arXiv.2312.15777$$DView paper in arXiv
https://doi.org/10.1140/epjc/s10052-024-12676-y$$DView published paper (Access to full text may be restricted)
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Snippet We continue our study of gaugings the maximal \(N=(2,2)\) supergravity in six dimensions with gauge groups obtained from decomposing the embedding tensor under...
Eur. Phys. J. C84 (2024) 333 We continue our study of gaugings the maximal $N=(2,2)$ supergravity in six dimensions with gauge groups obtained from decomposing...
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Embedding
Mathematical analysis
Physics - High Energy Physics - Theory
Representations
Subgroups
Supergravity
Supersymmetry
Symmetry
Tensors
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