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Three-point functions of a superspin-2 current multiplet in 3D, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="script">N</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math> superconformal theory

Three-point functions of a superspin-2 current multiplet in 3D, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="script">N</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math> superconformal theory

We consider $\mathcal{N}=1$ superconformal field theories in three dimensions possessing a conserved current multiplet ${\mathcal{F}}_{({\ensuremath{\alpha}}_{1}{\ensuremath{\alpha}}_{2}{\ensuremath{\alpha}}_{3}{\ensuremath{\alpha}}_{4})}$, which we refer to as the superspin-2 current multiplet. At the component level it contains a conserved spin-2 current different from the energy-momentum tensor and a conserved fermionic higher-spin current of spin $5/2$. Using a …