  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.
