Supersymmetric marginal deformations yielding a renormalizable SGYM theory
Determine whether supersymmetry-preserving marginal deformations of the three-dimensional supersymmetric Galilean Yang–Mills theory can render it renormalizable and simultaneously preserve Schrödinger symmetry at the quantum level.
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A question that should be dealt with is the fate of supersymmetry-preserving marginal deformations in the three-dimensional theory that render the theory renormalizable. As mentioned previously, it does not appear that one can find a well-defined nine-dimensional supersymmetric extension whose reduction to three dimensions is free of logarithmic divergences, and the structure of divergences means such an approach will not encompass all required counterterms. A more complete analysis of the possible three-dimensional terms that can be added is therefore desirable, though obviously far more complex; the hope would be that within this set lies a theory in which the Schr"odinger symmetry is preserved at the quantum level.
This is a supersymmetric Chern-Simons matter theory which (like three-dimensional SGYM) is classically invariant under the Schr"odinger algebra. All 24 generators of the original theory's superconformal transformations\footnote{Enhanced to 32 supercharges for the non-Lorentzian limit of BLG.} are also (classically) preserved by the limit, and it would be fascinating to see whether this holds once quantum corrections are included. Additionally, it is believed that relativistic three-dimensional $U(N)$ $#1{N}=8$ SYM flows to $U(N)1 \times U(N){-1}$ ABJM in the IR, which for the $N=2$ case considered in this paper is the BLG theory. Whether such a connection holds between the non-Lorentzian limits of the two theories is an intriguing one.