Abstract
We identify the unique stress tensor deformation which preserves zero-birefringence conditions in non-linear electrodynamics, which is a 4d4d version of the T\overline{T}TT¯ operator. We study the flows driven by this operator in the three Lagrangian theories without birefringence - Born-Infeld, Plebanski, and reverse Born-Infeld - all of which admit ModMax-like generalizations using a root-T\overline{T}TT¯-like flow that we analyse in our paper. We demonstrate one way of making this root-T\overline{T}TT¯-like flow manifestly supersymmetric by writing the deforming operator in \mathcal{N} = 1𝒩=1 superspace and exhibit two examples of superspace flows. We present scalar analogues in d = 2d=2 with similar properties as these theories of electrodynamics in d = 4d=4. Surprisingly, the Plebanski-type theories are fixed points of the classical T\overline{T}TT¯-like flows, while the Born-Infeld-type examples satisfy new flow equations driven by relevant operators constructed from the stress tensor. Finally, we prove that any theory obtained from a classical stress-tensor-squared deformation of a conformal field theory gives rise to a related “subtracted” theory for which the stress-tensor-squared operator is a constant.
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