Statement

Let ω:RdR0\omega:\mathbb R^d\to\mathbb R_{\le0} vanish on B2B_2, and suppose that for 0a30\le a\le3

Daω(x)Cregx1a,|D^a\omega(x)|\le C_{\mathrm{reg}}\langle x\rangle^{1-a},

while its satisfies

0G(r)1+r2drCgr.\int_0^\infty\frac{G^*(r)}{1+r^2}\,dr\le C_{\mathrm{gr}}.

For every σ>0\sigma>0, there is fL2(Rd)f\in L^2(\mathbb R^d) with

suppf^Bσ,f(x)Cecσω(x),f(x)12(xBrmin).\operatorname{supp}\widehat f\subseteq B_\sigma, \qquad |f(x)|\le C e^{c\sigma\omega(x)}, \qquad |f(x)|\ge\tfrac12\quad(x\in B_{r_{\min}}).

One may take cdmax(Creg,Cgr)1c\asymp_d\max(C_{\mathrm{reg}},C_{\mathrm{gr}})^{-1}, rmindmin(σ,σ1)r_{\min}\asymp_d\min(\sigma,\sigma^{-1}), and an explicit CC depending on dd and σ\sigma.

Proof chain

The constructs a plurisubharmonic minorant of the weight. The converts it to an entire L2L^2 function. Finally the gives the required Fourier support.

Why this is weaker than the one-dimensional theorem

The classical theorem needs only Lipschitz regularity and a logarithmic integral. The higher-dimensional result imposes symbol-type bounds through third derivatives; these are nevertheless satisfied by the weights built from line-porous sets.

References
  1. Alex Cohen, “Fractal uncertainty in higher dimensions,” 2024. arXiv record. Relevant: Theorem 1.4.