English

Supersymmetric $AdS_5$ black holes and strings from 5D $N=4$ gauged supergravity

High Energy Physics - Theory 2019-03-20 v2

Abstract

We study supersymmetric AdS3×Σ2AdS_3\times \Sigma_2 and AdS2×Σ3AdS_2\times \Sigma_3 solutions, with Σ2=S2,H2\Sigma_2=S^2,H^2 and Σ3=S3,H3\Sigma_3=S^3,H^3, in five-dimensional N=4N=4 gauged supergravity coupled to five vector multiplets. The gauge groups considered here are U(1)×SU(2)×SU(2)U(1)\times SU(2)\times SU(2), U(1)×SO(3,1)U(1)\times SO(3,1) and U(1)×SL(3,R)U(1)\times SL(3,\mathbb{R}). For U(1)×SU(2)×SU(2)U(1)\times SU(2)\times SU(2) gauge group admiting two supersymmetric N=4N=4 AdS5AdS_5 vacua, we identify a new class of AdS3×Σ2AdS_3\times \Sigma_2 and AdS2×H3AdS_2\times H^3 solutions preserving four supercharges. Holographic RG flows describing twisted compactifications of N=2N=2 four-dimensional SCFTs dual to the AdS5AdS_5 vacua to the SCFTs in two and one dimensions dual to these geometries are numerically given. The solutions can also be interpreted as supersymmetric black strings and black holes in asymptotically AdS5AdS_5 spaces with near horizon geometries given by AdS3×Σ2AdS_3\times \Sigma_2 and AdS2×H3AdS_2\times H^3, respectively. These solutions broaden previously known black brane solutions including half-supersymmetric AdS5AdS_5 black strings recently found in N=4N=4 gauged supergravity. Similar solutions are also studied in non-compact gauge groups U(1)×SO(3,1)U(1)\times SO(3,1) and U(1)×SL(3,R)U(1)\times SL(3,\mathbb{R}).

Keywords

Cite

@article{arxiv.1812.10122,
  title  = {Supersymmetric $AdS_5$ black holes and strings from 5D $N=4$ gauged supergravity},
  author = {H. L. Dao and Parinya Karndumri},
  journal= {arXiv preprint arXiv:1812.10122},
  year   = {2019}
}

Comments

35 pages, 12 figures, substantial extension of the results in arXiv:1811.01608, typos corrected, references added