Large ensemble decoupling for the paraboloid

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Let RR be a large parameter, let BRB_R be a ball or cube of radius or side length RR in R3{\mathbb R}^3, and let ESFE_SF denote the Fourier extension operator associated to the two-dimensional paraboloid, restricted to S⊂[0,1]2S\subset[0,1]^2. A large ensemble is a disjoint union of 1/R1/\sqrt{R}-squares from the partition QR{\mathcal Q}_R of [0,1]2[0,1]^2. Let N=O(R)N=O(R), and let S1,…,SNS_1,\ldots,S_N be a partition of [0,1]2[0,1]^2 into large ensembles. Large ensemble decoupling for the paraboloid. For 2≤p≤32\le p\le3, one has

∥EF∥Lp(BR)≲ϵRϵ(∑i=1N∥ESiF∥Lp(BR)2)1/2.\|EF\|_{L^p(B_R)}\lesssim_{\epsilon}R^{\epsilon}\left(\sum_{i=1}^N\|E_{S_i}F\|_{L^p(B_R)}^2\right)^{1/2}.

This would extend canonical l2l^2 decoupling from canonical caps to arbitrary unions of such caps, including thin rectangles and disconnected sets. The source provides no resolution status for this conjecture.

References

Primary source

Ciprian Demeter, “Beyond canonical decoupling”, arXiv:2402.04989 (2024).

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