R-current three-point functions in 4d $\mathcal{N}=1$ superconformal theories

3Schematically we have: Xij = Xi · Xj, Iij = SiSj, Ji,jk = SiXjXkSi/Xjk, Ki,jk = SjXiSkpXjk/(Xij Xik). In

addition, Xab is obtained contracting XM with the 6d gamma matrices. Finally J1 ≡ J1,23, J2 ≡ J2,13, J3 ≡ J3,12

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