Abstract

We study a large class of supersymmetric solutions in four-dimensional $N=5$ gauged supergravity with $SO(5)$ gauge group. There is only one $N=5$ supersymmetric $AdS_4$ vacuum preserving the full $SO(5)$ symmetry dual to an $N=5$ SCFT in three dimensions. We give a number of domain walls interpolating between this $AdS_4$ fixed point and singular geometries in the IR with $SO(4)$ and $SO(3)$ symmetries. These solutions describe RG flows from the $N=5$ SCFT to non-conformal field theories driven by mass deformations. The $SO(4)$ solutions are precisely in agreement with the previously known mass deformations within the dual $N=5$ SCFT. We also find supersymmetric Janus solutions describing two-dimensional conformal defects in the $N=5$ SCFT with $N=(4,1)$ and $N=(1,1)$ supersymmetries on the defects. Finally, we study supersymmetric solutions of the form $AdS_2\times \Sigma^2$, with $\Sigma^2=S^2,H^2$ being a Riemann surface, corresponding to near horizon geometries of $AdS_4$ black holes. We consider both magnetic and dyonic solutions and find that there exists a class of magnetic $AdS_2\times H^2$ solutions with $SO(2)$ symmetry. It is rather remarkable that a complete analytic solution interpolating between $AdS_4$ and $AdS_2\times H^2$ with a running scalar can be obtained. The solution corresponds to a twisted compactification of $N=5$ SCFT to superconformal quantum mechanics. We also show that no purely magnetic or dyonic black holes with $AdS_2\times \Sigma^2$ horizon from $SO(2)\times SO(2)$ twist exist in $N=5$, $SO(5)$ gauged supergravity.

Highlights

  • Over the past twenty years, the AdS=CFT correspondence, originally proposed in [1], has provided holographic descriptions of various strongly coupled systems ranging fromconformal field theories, conformal defects, AdS-black holes, and condensed matter physics systems

  • These solutions describe holographic renormalization group (RG) flows from the dual N 1⁄4 5 superconformal field theory (SCFT) in the UV to nonconformal field theories in the IR obtained from mass deformations of the N 1⁄4 5 SCFT

  • We begin with holographic RG flow solutions in the form of domain walls interpolating between the supersymmetric AdS4 vacuum in the UV and singular geometries in the IR

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Summary

INTRODUCTION

Over the past twenty years, the AdS=CFT correspondence, originally proposed in [1] (see [2,3]), has provided holographic descriptions of various strongly coupled systems ranging from (non)conformal field theories, conformal defects, AdS-black holes, and condensed matter physics systems. According to the AdS=CFT duality, this AdS4 critical point is dual to an N 1⁄4 5 SCFT in three dimensions There is another nonsupersymmetric AdS4 vacuum with unbroken SOð3Þ gauge symmetry. We will study supersymmetric domain walls interpolating between the supersymmetric AdS4 vacuum and singular geometries These solutions describe holographic renormalization group (RG) flows from the dual N 1⁄4 5 SCFT in the UV to nonconformal field theories in the IR obtained from mass deformations of the N 1⁄4 5 SCFT. At the supersymmetric AdS4 vacuum, all scalars have masses m2L2 1⁄4 −2 corresponding to operators of dimensions Δ 1⁄4 1, 2 in the dual N 1⁄4 5 SCFT These operators are given by scalar and fermion bilinears (mass terms), respectively. We will look for various types of supersymmetric solutions which are asymptotic to the N 1⁄4 5 supersymmetric AdS4 vacuum

HOLOGRAPHIC RG FLOWS
RG flows with SOð4Þ symmetry
RG flows with SOð3Þ symmetry
RG flows with SOð2Þ symmetry
Comment on general supersymmetric domain wall solutions
SUPERSYMMETRIC JANUS SOLUTIONS
Janus solutions with SOð4Þ symmetry
Janus solutions with SOð3Þ symmetry
SUPERSYMMETRIC AdS4 BLACK HOLES
Magnetic solutions
Dyonic solutions
CONCLUSIONS AND DISCUSSIONS
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