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

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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={x∈R2:λ−δ<∣x∣<λ+δ}.\mathcal{A}_{\lambda,\delta}=\{x\in\mathbb{R}^2: \lambda-\delta<|x|<\lambda+\delta\}.

Let

Φλ,δ(x)=∑k∈Aλ,δ∩Z2e2πik⋅x,\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,δ∗fP_{\lambda,\delta}f=\Phi_{\lambda,\delta}*f. Kernel conjecture. If p≥2p\geq2 and κ>0\kappa>0, then, whenever δ>λ−1+κ\delta>\lambda^{-1+\kappa},

∥Φλ,δ∥Lp≲p,κλ1−2pδ+(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 2≤p≤42\leq p\leq4, by that term for p≥4p\geq4 and δ<λ4/p−1\delta<\lambda^{4/p-1}, and by λ1−2/pδ\lambda^{1-2/p}\delta for p≥4p\geq4 and δ>λ4/p−1\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.

References

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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