Fractional heat content asymptotics for Carnot groups
Rohan Sarkar
TL;DR
This work extends small-time fractional heat-content asymptotics to Carnot groups by linking the deficit |Ω|−Q^{(α)}_Ω(t) to the horizontal perimeter |∂Ω|_H via a universal rate μ_α(t). The authors represent the fractional heat content through subordination of horizontal Brownian motion and develop a Taylor-based Carnot-group framework plus precise exit-time estimates to obtain both lower and upper bounds. For 1≤α≤2, they prove lim_{t→0} (|Ω|−Q^{(α)}_Ω(t))/μ_α(t) = |∂Ω|_H, with μ_α(t) matching the Euclidean rate; the lower bound holds for any finite horizontal perimeter, while the upper bound is established for C^2 domains with no characteristic points. The results highlight a universal, geometry-driven mechanism in sub-Riemannian settings and demonstrate how probabilistic constructions combined with Carnot-group Taylor expansions can yield sharp heat-content asymptotics on non-Euclidean spaces.
Abstract
We propose a novel approach for studying small-time asymptotics of the fractional heat content of $C^2$ non-characteristic domains in Carnot groups. Denoting the sub-Laplacian operator by $\mathcal{L}$, the fractional heat content of a bounded domain $Ω$ is defined as $Q^{(α)}_Ω(t)=\int_Ω u_α(t,x)dx$, where $u_α$ is the solution to the heat equation corresponding to the fractional sub-Laplacian $\mathcal{L}_α:=\mathcal{L}^{α/2}$ with Dirichlet boundary condition on $Ω$. We prove that for $1\leα\le 2$, there exists explict rate function $μ_α: (0,\infty)\to (0,\infty)$ such that \[ \lim_{t\to 0}\frac{|Ω|-Q^{(α)}_Ω(t)}{μ_α(t)}=|\partialΩ|_H, \] where $|\partialΩ|_H$ is the horizontal perimeter of $Ω$. Moreover, the rate function $μ_α$ coincides with the same for the Euclidean case.
