Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities

Abstract We study supersymmetric $$AdS_4$$ A d S 4 black holes in matter-coupled $$N=3$$ N = 3 and $$N=4$$ N = 4 gauged supergravities in four dimensions. In $$N=3$$ N = 3 theory, we consider $$N=3$$ N = 3 gauged supergravity coupled to three vector multiplets and $$SO(3)\times SO(3)$$ S O ( 3 ) × S...

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Autor principal: Parinya Karndumri
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spelling oai:doaj.org-article:46d7f23cf8714197825f0d3dc101bc532021-11-21T12:10:10ZSupersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities10.1140/epjc/s10052-021-09757-71434-60441434-6052https://doaj.org/article/46d7f23cf8714197825f0d3dc101bc532021-11-01T00:00:00Zhttps://doi.org/10.1140/epjc/s10052-021-09757-7https://doaj.org/toc/1434-6044https://doaj.org/toc/1434-6052Abstract We study supersymmetric $$AdS_4$$ A d S 4 black holes in matter-coupled $$N=3$$ N = 3 and $$N=4$$ N = 4 gauged supergravities in four dimensions. In $$N=3$$ N = 3 theory, we consider $$N=3$$ N = 3 gauged supergravity coupled to three vector multiplets and $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) gauge group. The resulting gauged supergravity admits two $$N=3$$ N = 3 supersymmetric $$AdS_4$$ A d S 4 vacua with $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) and SO(3) symmetries. We find an $$AdS_2\times H^2$$ A d S 2 × H 2 solution with $$SO(2)\times SO(2)$$ S O ( 2 ) × S O ( 2 ) symmetry and an analytic solution interpolating between this geometry and the $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) symmetric $$AdS_4$$ A d S 4 vacuum. For $$N=4$$ N = 4 gauged supergravity coupled to six vector multiplets with $$SO(4)\times SO(4)$$ S O ( 4 ) × S O ( 4 ) gauge group, there exist four supersymmetric $$AdS_4$$ A d S 4 vacua with $$SO(4)\times SO(4)$$ S O ( 4 ) × S O ( 4 ) , $$SO(4)\times SO(3)$$ S O ( 4 ) × S O ( 3 ) , $$SO(3)\times SO(4)$$ S O ( 3 ) × S O ( 4 ) and $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) symmetries. We find a number of $$AdS_2\times S^2$$ A d S 2 × S 2 and $$AdS_2\times H^2$$ A d S 2 × H 2 geometries together with the solutions interpolating between these geometries and all, but the $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) , $$AdS_4$$ A d S 4 vacua. These solutions provide a new class of $$AdS_4$$ A d S 4 black holes with spherical and hyperbolic horizons dual to holographic RG flows across dimensions from $$N=3,4$$ N = 3 , 4 SCFTs in three dimensions to superconformal quantum mechanics within the framework of four-dimensional gauged supergravity.Parinya KarndumriSpringerOpenarticleAstrophysicsQB460-466Nuclear and particle physics. Atomic energy. RadioactivityQC770-798ENEuropean Physical Journal C: Particles and Fields, Vol 81, Iss 11, Pp 1-27 (2021)
institution DOAJ
collection DOAJ
language EN
topic Astrophysics
QB460-466
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
spellingShingle Astrophysics
QB460-466
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
Parinya Karndumri
Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities
description Abstract We study supersymmetric $$AdS_4$$ A d S 4 black holes in matter-coupled $$N=3$$ N = 3 and $$N=4$$ N = 4 gauged supergravities in four dimensions. In $$N=3$$ N = 3 theory, we consider $$N=3$$ N = 3 gauged supergravity coupled to three vector multiplets and $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) gauge group. The resulting gauged supergravity admits two $$N=3$$ N = 3 supersymmetric $$AdS_4$$ A d S 4 vacua with $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) and SO(3) symmetries. We find an $$AdS_2\times H^2$$ A d S 2 × H 2 solution with $$SO(2)\times SO(2)$$ S O ( 2 ) × S O ( 2 ) symmetry and an analytic solution interpolating between this geometry and the $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) symmetric $$AdS_4$$ A d S 4 vacuum. For $$N=4$$ N = 4 gauged supergravity coupled to six vector multiplets with $$SO(4)\times SO(4)$$ S O ( 4 ) × S O ( 4 ) gauge group, there exist four supersymmetric $$AdS_4$$ A d S 4 vacua with $$SO(4)\times SO(4)$$ S O ( 4 ) × S O ( 4 ) , $$SO(4)\times SO(3)$$ S O ( 4 ) × S O ( 3 ) , $$SO(3)\times SO(4)$$ S O ( 3 ) × S O ( 4 ) and $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) symmetries. We find a number of $$AdS_2\times S^2$$ A d S 2 × S 2 and $$AdS_2\times H^2$$ A d S 2 × H 2 geometries together with the solutions interpolating between these geometries and all, but the $$SO(3)\times SO(3)$$ S O ( 3 ) × S O ( 3 ) , $$AdS_4$$ A d S 4 vacua. These solutions provide a new class of $$AdS_4$$ A d S 4 black holes with spherical and hyperbolic horizons dual to holographic RG flows across dimensions from $$N=3,4$$ N = 3 , 4 SCFTs in three dimensions to superconformal quantum mechanics within the framework of four-dimensional gauged supergravity.
format article
author Parinya Karndumri
author_facet Parinya Karndumri
author_sort Parinya Karndumri
title Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities
title_short Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities
title_full Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities
title_fullStr Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities
title_full_unstemmed Supersymmetric $$AdS_4$$ A d S 4 black holes from matter-coupled $$N=3,4$$ N = 3 , 4 gauged supergravities
title_sort supersymmetric $$ads_4$$ a d s 4 black holes from matter-coupled $$n=3,4$$ n = 3 , 4 gauged supergravities
publisher SpringerOpen
publishDate 2021
url https://doaj.org/article/46d7f23cf8714197825f0d3dc101bc53
work_keys_str_mv AT parinyakarndumri supersymmetricads4ads4blackholesfrommattercoupledn34n34gaugedsupergravities
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