We show that for every $0<\delta <1$
, the Fourier extension conjecture on the paraboloid in three dimensions is equivalent to a local single scale smooth Alpert trilinear inequality of the form: $$\begin{align*}&\left\Vert \mathcal{E}\mathsf{Q}_{s,U_{1}}^{\eta}f_{1}\ \mathcal{E} \mathsf{Q}_{s,U_{2}}^{\eta}f_{2}\ \mathcal{E}\mathsf{Q}_{s,U_{3}}^{\eta} f_{3}\right\Vert _{L^{\frac{q}{3}}\left( B_{\mathbb{R}^{3}}\left( 0,2^{\frac{s}{1-\delta}}\right) \right) }\\ &\quad \leq C_{\delta,\varepsilon,\nu}2^{\varepsilon s}\left\Vert f_{1}\right\Vert _{L^{\infty}\left( U_{1}\right) }\left\Vert f_{2} \right\Vert _{L^{\infty}\left( U_{2}\right) }\left\Vert f_{3}\right\Vert _{L^{\infty}\left( U_{3}\right) }, \end{align*}$$
which is a variant of the analogous multiscale trilinear inequality in Rios and Sawyer (2025, Equivalence of linear and trilinear Kakeya conjectures in three dimensions), where the smooth Alpert projections $\mathsf {Q}_{s,U_{k}}^{\eta }$
were replaced more generally with $\mathsf {Q}_{s_{k},U_{k}}^{\eta }$
, where $s_{k}$
was close to $s$
.