In the $D$-dimensional Vicsek graph, we prove that the Riesz-like inequality $ \|\nabla f\|_p \leq C \|Δ^γf\|_p $ holds for every $p\in(1,\infty)$ and every $ 0<γ<γ^*(p):=\frac{1}{D+1}+\frac{D-1}{D+1}\,\frac{1}{p}, $ while it fails whenever $p\in(1,\infty)$ and $γ^*(p)<γ<1$. Thus, the validity of the inequality remains open only at the critical exponent $γ=γ^*(p)$. This provides the first example of an $L^p$-bounded ``super-Riesz transform'', namely an operator of the form $\nabla Δ^{-γ}$ with $γ$ strictly larger than the Euclidean threshold $\frac12$. To achieve this, we establish a more general result linking the diffusion escape rate and a Poincaré inequality on balls to the validity of the reverse Riesz-like inequality $\|Δ^γf\|_p \leq C \|\nabla f\|_p.$