Abstract

We derive an equivalence between the (2,0) superconformal M5-brane field theory dimensionally reduced on a squashed three-sphere, and Chern-Simons theory with complex gauge group. In the reduction, the massless fermions obtain an action which is second order in derivatives and are reinterpreted as ghosts for gauge fixing the emergent non-compact gauge symmetry. A squashing parameter in the geometry controls the imaginary part of the complex Chern-Simons level.

Highlights

  • Scalars make up the remainder of gC

  • We derive an equivalence between the (2,0) superconformal M5-brane field theory dimensionally reduced on a squashed three-sphere, and Chern-Simons theory with complex gauge group

  • We find that it is consistent with supersymmetry to set this quantized flux parameter to zero

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Summary

The M5-brane on a squashed three-sphere

We construct a Euclidean continuation of the six-dimensional (2, 0) theory on a three-dimensional spherical background. We consider a squashed three-sphere which preserves the round form of the metrics on the base and the fiber, but takes their ratio of radii to be l/2, where l ∈ R+ is a parameter of the construction. Preserving supersymmetry on a squashed three sphere will require us to activate various background supergravity fields, and we describe the precise form of these. We wish to study a configuration which is compatible with replacing R3 with a general threemanifold M3 while preserving supersymmetry It follows that our choice of background supergravity fields must be compatible with topological twisting.

Supergravity configuration
Analysis of supersymmetry constraints
Zero modes and the three-dimensional action
Gauge field
Scalars
Fermions
Non-abelian interaction terms
The 3d effective action: complex Chern-Simons theory
The fermion action
Supersymmetry transformations and a Q exact deformation
Ghosts and gauge fixing
Discussion
B Clifford algebra
Useful properties of 3d and 2d Clifford algebra
Full Text
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