Spectral projector kernel bounds on narrow windows for the two-dimensional torus

From papers

Let T2=R2/Z2\mathbb{T}^2=\mathbb{R}^2/\mathbb{Z}^2, let λ>2\lambda>2 and δ<1\delta<1, and define

Aλ,δ={xR2:λδ<x<λ+δ}.\mathcal{A}_{\lambda,\delta}=\{x\in\mathbb{R}^2: \lambda-\delta<|x|<\lambda+\delta\}.

Let

Φλ,δ(x)=kAλ,δZ2e2πikx,\Phi_{\lambda,\delta}(x)=\sum_{k\in\mathcal{A}_{\lambda,\delta}\cap\mathbb{Z}^2}e^{2\pi i k\cdot x},

so that Pλ,δf=Φλ,δfP_{\lambda,\delta}f=\Phi_{\lambda,\delta}*f. Kernel conjecture. If p2p\geq2 and κ>0\kappa>0, then, whenever δ>λ1+κ\delta>\lambda^{-1+\kappa},

Φλ,δLpp,κλ12pδ+(λδ)12.\|\Phi_{\lambda,\delta}\|_{L^p}\lesssim_{p,\kappa}\lambda^{1-\frac2p}\delta+(\lambda\delta)^{\frac12}.

Equivalently, the bound is governed by (λδ)1/2(\lambda\delta)^{1/2} for 2p42\leq p\leq4, by that term for p4p\geq4 and δ<λ4/p1\delta<\lambda^{4/p-1}, and by λ12/pδ\lambda^{1-2/p}\delta for p4p\geq4 and δ>λ4/p1\delta>\lambda^{4/p-1}. The conjecture is partially equivalent to the spectral projector conjecture and is connected to additive energies of lattice points in thin annuli.

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Sources & referencesView supporting material

Primary source

Ciprian Demeter and Pierre Germain, “L^2 to L^p bounds for spectral projectors on the Euclidean two-dimensional torus”, arXiv:2306.14286 (2024).

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