Non-local modulus of continuity on a bounded convex domain

Let Ω\Omega be a bounded convex domain in Rn\mathbb R^n with diameter DD. Choose rectangular coordinates whose z1z_1-axis is aligned with the compact interval I=[D/2,D/2]I=[-D/2,D/2]. For each z1Iz_1\in I, define the slice

Ωz1={pRn1:(z1,p)Ω}.\Omega_{z_1}=\{p\in\mathbb R^{n-1}:(z_1,p)\in\Omega\}.

Suppose u:Ω×[0,)Ru:\Omega\times[0,\infty)\to\mathbb R satisfies the non-local regional heat equation, and let φ\varphi be as in the one-dimensional modulus-of-continuity theorem. Assume that its odd extension φ~\tilde\varphi satisfies

φ~t(r,t)=Iρ~(wr)(φ~(w)φ~(r))dw,rI, t>0,\tilde\varphi_t(r,t)=\int_I\tilde\rho(w-r)\bigl(\tilde\varphi(w)-\tilde\varphi(r)\bigr)\,dw,\qquad r\in I,\ t>0,

where

ρ~(z1)=Ωz1ρ(z1,p)dp.\tilde\rho(z_1)=\int_{\Omega_{z_1}}\rho(z_1,p)\,dp.

Non-local modulus of continuity conjecture. Then φ(,t)\varphi(\cdot,t) is a modulus of continuity for u(,t)u(\cdot,t) on Ω×[0,)\Omega\times[0,\infty). This proposes that the higher-dimensional regional non-local heat flow on a bounded convex domain admits the same type of modulus-of-continuity control as the associated one-dimensional sliced equation. The statement is presented as a conjecture; no resolution is supplied in the source.

Sources & referencesView supporting material

Primary source

Ben Andrews and Sophie Chen, “Modulus of continuity for solutions of non-local heat equations”, arXiv:2507.19023 (2026).

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