Supersymmetric solutions of 7D maximal gauged supergravity

preprint2020arXivOpen access

Abstract

We study a number of supersymmetric solutions in the form of Mkw3×S3Mkw_3\times S^3- and AdS3×S3AdS_3\times S^3-sliced domain walls in the maximal gauged supergravity in seven dimensions. These solutions require non-vanishing three-form fluxes to support the AdS3AdS_3 and S3S^3 subspaces. We consider solutions with SO(4)SO(4), SO(3)SO(3), SO(2)×SO(2)SO(2)\times SO(2) and SO(2)SO(2) symmetries in CSO(p,q,5−p−q)CSO(p,q,5-p-q), CSO(p,q,4−p−q)CSO(p,q,4-p-q) and SO(2,1)⋉R4SO(2,1)\ltimes \mathbf{R}^4 gauge groups. All of these solutions can be analytically obtained. For SO(5)SO(5) and CSO(4,0,1)CSO(4,0,1) gauge groups, the complete truncation ansatze in terms of eleven-dimensional supergravity on S4S^4 and type IIA theory on S3S^3 are known. We give the full uplifted solutions to eleven and ten dimensions in this case. The solutions with an AdS3×S3AdS_3\times S^3 slice are interpreted as two-dimensional surface defects in six-dimensional N=(2,0)N=(2,0) superconformal field theory in the case of SO(5)SO(5) gauge group or N=(2,0)N=(2,0) nonconformal field theories for other gauge groups. For SO(4)SO(4) symmetric solutions, it is possible to find solutions with both the three-form fluxes and SO(3)SO(3) gauge fields turned on. However, in this case, the solutions can be found only numerically. For SO(3)SO(3) symmetric solutions, the three-form fluxes and SO(3)SO(3) gauge fields cannot be non-vanishing simultaneously.

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