Higher-dimensional logarithmic-phase fractal uncertainty conjecture

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For n=2n=2, let X,Y⊂BR2(0,1)X,Y\subset B_{\mathbb R^2}(0,1) be ν\nu-porous on scales hh to 11. Let U⊂R2nU\subset\mathbb R^{2n} be open, let b∈Cc∞(U)b\in C_c^\infty(U), and define

Bhf(x)=(2πh)−n/2∫RneiΦ(x,y)/hb(x,y)f(y) dy,\mathcal B_hf(x)=(2\pi h)^{-n/2}\int_{\mathbb R^n}e^{i\Phi(x,y)/h}b(x,y)f(y)\,dy,

where

Φ(x,y)=log⁡∣x−y∣.\Phi(x,y)=\log|x-y|.

Higher-dimensional logarithmic-phase FUP conjecture. For each ν>0\nu>0 there exists β=β(ν)>0\beta=\beta(\nu)>0 such that

∥1XBh1Y∥L2(Rn)→L2(Rn)=O(hβ)as h→0.\|\mathbf 1_X\mathcal B_h\mathbf 1_Y\|_{L^2(\mathbb R^n)\to L^2(\mathbb R^n)}=\mathcal O(h^\beta)\quad\text{as }h\to0.

The claim concerns a genuinely higher-dimensional phase for which the standard reduction to the Fourier transform may lose information; it is proposed as a generalization relevant to higher-dimensional hyperbolic manifolds.

References

Primary source

Semyon Dyatlov, “An introduction to fractal uncertainty principle”, arXiv:1903.02599 (2019).

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