Abstract
We study supersymmetric solutions in four-dimensional $N=6$ gauged supergravity with $SO(6)$ gauge group. There is a unique $N=6$ supersymmetric $AdS_4$ vacuum with $SO(6)$ symmetry dual to an $N=6$ SCFT in three dimensions. We find a number of domain walls interpolating between this $AdS_4$ vacuum and singular geometries in the IR with $SO(2)\times SO(4)$, $U(3)$, $SO(3)$ and $SO(2)\times SO(2)\times SO(2)$ symmetries. The $SO(3)$ case admits $N=6$ or $N=2$ solutions depending on whether the pseudoscalars are present or not. On the other hand, all the remaining solutions preserve $N=6$ supersymmetry. These solutions describe RG flows from the $N=6$ SCFT to non-conformal field theories driven by mass deformations. In particular, the $SO(2)\times SO(4)$ solution is in agreement with the previously known mass deformations of the dual $N=6$ SCFT. We also give a supersymmetric Janus solution with $SO(2)\times SO(4)$ symmetry, describing two-dimensional conformal defects in the $N=6$ SCFT with unbroken $N=(4,2)$ supersymmetry. Finally, we find an $N=2$ supersymmetric $AdS_2\times H^2$ solution with $SO(2)\times SO(4)$ symmetry and the corresponding domain wall interpolating between this fixed point and the $AdS_4$ vacuum. The solution describes an $AdS_4$ black hole with a magnetic charge and is dual to a twisted compactification of the $N=6$ SCFT on a hyperbolic space $H^2$. We also give a domain wall interpolating between a locally supersymmetric $AdS_4$ and a curved domain wall with $SO(2)\times SO(2)\times SO(2)$ symmetry dual to an RG flow across dimensions from the $N=6$ SCFT to a supersymmetric quantum mechanics.
Highlights
Supersymmetric solutions of gauged supergravities in various space-time dimensions play an important role in string and M theory
There is a unique N 1⁄4 6 supersymmetric AdS4 vacuum preserving the full SOð6Þ gauge symmetry. This can be identified with AdS4 × CP3 geometry in type IIA theory dual to an N 1⁄4 6 superconformal field theory (SCFT) in three dimensions
We have found a number of RG flow solutions with various symmetries from this N 1⁄4 6 SCFT to possible nonconformal phases in the IR
Summary
Supersymmetric solutions of gauged supergravities in various space-time dimensions play an important role in string and M theory. The N 1⁄4 6 gauged supergravity has been shown to admit a unique N 1⁄4 6 supersymmetric AdS4 vacuum, with the full SOð6Þ symmetry unbroken, dual to an N 1⁄4 6 superconformal field theory (SCFT) in three dimensions. In the dual field theory, the solutions describe RG flows from the N 1⁄4 6 SCFT to superconformal quantum mechanics in the IR which play a prominent role in microscopic computation of black hole entropy in asymptotically AdS4 spaces; see, for example, [67,68,69]. To define a proper gauging and preserve the full supersymmetry of the ungauged theory, the embedding tensor needs to satisfy the so-called linear and quadratic constraints given, respectively, by XðMNLΩPÞL 1⁄4 0 and θMmθNnfmnp þ XMNPθPp 1⁄4 0 ð12Þ with fmnp being the SOÃð12Þ structure constants. We will find solutions that are asymptotic to this AdS4 geometry and can be interpreted as different types of deformations of the dual N 1⁄4 6 SCFT
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