We compute spinning four point functions in the quasi-fermionic three dimensional conformal field theory with slightly broken higher spin symmetry at finite t'Hooft coupling. More concretely, we obtain a formula for $\langle j_s j_{ \tilde{ 0}} j_{ \tilde{ 0}} j_{ \tilde{ 0}} \rangle$, where $j_s$ is a higher spin current and $j_{ \tilde{ 0}}$ is the scalar single trace operator. Our procedure consists in writing a plausible ansatz in Mellin space and using crossing, pseudo-conservation and Regge boundedness to fix all undetermined coefficients. Our method can potentially be generalised to compute all spinning four point functions in these theories.
Categories: hep-th