Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity
Abstract We study supersymmetric $$AdS_3\times M^4$$ AdS3×M4 solutions of $$N=2$$ N=2 gauged supergravity in seven dimensions coupled to three vector multiplets with $$SO(4)\sim SO(3)\times SO(3)$$ SO(4)∼SO(3)×SO(3) gauge group and $$M^4$$ M4 being a four-manifold with constant curvature. The gauged...
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doaj-cccdce42d67e463db8d96fc4a97437072020-11-25T03:02:09ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-08-0179812310.1140/epjc/s10052-019-7170-0Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravityParinya Karndumri0Patharadanai Nuchino1String Theory and Supergravity Group, Department of Physics, Faculty of Science, Chulalongkorn UniversityString Theory and Supergravity Group, Department of Physics, Faculty of Science, Chulalongkorn UniversityAbstract We study supersymmetric $$AdS_3\times M^4$$ AdS3×M4 solutions of $$N=2$$ N=2 gauged supergravity in seven dimensions coupled to three vector multiplets with $$SO(4)\sim SO(3)\times SO(3)$$ SO(4)∼SO(3)×SO(3) gauge group and $$M^4$$ M4 being a four-manifold with constant curvature. The gauged supergravity admits two supersymmetric $$AdS_7$$ AdS7 critical points with SO(4) and SO(3) symmetries corresponding to $$N=(1,0)$$ N=(1,0) superconformal field theories (SCFTs) in six dimensions. For $$M^4=\Sigma ^2\times \Sigma ^2$$ M4=Σ2×Σ2 with $$\Sigma ^2$$ Σ2 being a Riemann surface, we obtain a large class of supersymmetric $$AdS_3\times \Sigma ^2\times \Sigma ^2$$ AdS3×Σ2×Σ2 solutions preserving four supercharges and $$SO(2)\times SO(2)$$ SO(2)×SO(2) symmetry for one of the $$\Sigma ^2$$ Σ2 being a hyperbolic space $$H^2$$ H2 , and the solutions are dual to $$N=(2,0)$$ N=(2,0) SCFTs in two dimensions. For a smaller symmetry SO(2), only $$AdS_3\times H^2\times H^2$$ AdS3×H2×H2 solutions exist. Some of these are also solutions of pure $$N=2$$ N=2 gauged supergravity with $$SU(2)\sim SO(3)$$ SU(2)∼SO(3) gauge group. We numerically study domain walls interpolating between the two supersymmetric $$AdS_7$$ AdS7 vacua and these geometries. The solutions describe holographic RG flows across dimensions from $$N=(1,0)$$ N=(1,0) SCFTs in six dimensions to $$N=(2,0)$$ N=(2,0) two-dimensional SCFTs in the IR. Similar solutions for $$M^4$$ M4 being a Kahler four-cycle with negative curvature are also given. In addition, unlike $$M^4=\Sigma ^2\times \Sigma ^2$$ M4=Σ2×Σ2 case, it is possible to twist by $$SO(3)_{\text {diag}}$$ SO(3)diag gauge fields resulting in two-dimensional $$N=(1,0)$$ N=(1,0) SCFTs. Some of the solutions can be uplifted to eleven dimensions and provide a new class of $$AdS_3\times M^4\times S^4$$ AdS3×M4×S4 solutions in M-theory.http://link.springer.com/article/10.1140/epjc/s10052-019-7170-0 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Parinya Karndumri Patharadanai Nuchino |
spellingShingle |
Parinya Karndumri Patharadanai Nuchino Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity European Physical Journal C: Particles and Fields |
author_facet |
Parinya Karndumri Patharadanai Nuchino |
author_sort |
Parinya Karndumri |
title |
Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity |
title_short |
Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity |
title_full |
Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity |
title_fullStr |
Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity |
title_full_unstemmed |
Two-dimensional SCFTs from matter-coupled $$7D~N=2$$ 7DN=2 gauged supergravity |
title_sort |
two-dimensional scfts from matter-coupled $$7d~n=2$$ 7dn=2 gauged supergravity |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2019-08-01 |
description |
Abstract We study supersymmetric $$AdS_3\times M^4$$ AdS3×M4 solutions of $$N=2$$ N=2 gauged supergravity in seven dimensions coupled to three vector multiplets with $$SO(4)\sim SO(3)\times SO(3)$$ SO(4)∼SO(3)×SO(3) gauge group and $$M^4$$ M4 being a four-manifold with constant curvature. The gauged supergravity admits two supersymmetric $$AdS_7$$ AdS7 critical points with SO(4) and SO(3) symmetries corresponding to $$N=(1,0)$$ N=(1,0) superconformal field theories (SCFTs) in six dimensions. For $$M^4=\Sigma ^2\times \Sigma ^2$$ M4=Σ2×Σ2 with $$\Sigma ^2$$ Σ2 being a Riemann surface, we obtain a large class of supersymmetric $$AdS_3\times \Sigma ^2\times \Sigma ^2$$ AdS3×Σ2×Σ2 solutions preserving four supercharges and $$SO(2)\times SO(2)$$ SO(2)×SO(2) symmetry for one of the $$\Sigma ^2$$ Σ2 being a hyperbolic space $$H^2$$ H2 , and the solutions are dual to $$N=(2,0)$$ N=(2,0) SCFTs in two dimensions. For a smaller symmetry SO(2), only $$AdS_3\times H^2\times H^2$$ AdS3×H2×H2 solutions exist. Some of these are also solutions of pure $$N=2$$ N=2 gauged supergravity with $$SU(2)\sim SO(3)$$ SU(2)∼SO(3) gauge group. We numerically study domain walls interpolating between the two supersymmetric $$AdS_7$$ AdS7 vacua and these geometries. The solutions describe holographic RG flows across dimensions from $$N=(1,0)$$ N=(1,0) SCFTs in six dimensions to $$N=(2,0)$$ N=(2,0) two-dimensional SCFTs in the IR. Similar solutions for $$M^4$$ M4 being a Kahler four-cycle with negative curvature are also given. In addition, unlike $$M^4=\Sigma ^2\times \Sigma ^2$$ M4=Σ2×Σ2 case, it is possible to twist by $$SO(3)_{\text {diag}}$$ SO(3)diag gauge fields resulting in two-dimensional $$N=(1,0)$$ N=(1,0) SCFTs. Some of the solutions can be uplifted to eleven dimensions and provide a new class of $$AdS_3\times M^4\times S^4$$ AdS3×M4×S4 solutions in M-theory. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-019-7170-0 |
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