A Riemannian Autocorrelation Function and its Application to Non-Local Isoperimetric Energies
Michael Bleher, Denis Brazke, Sebastian Nill
TL;DR
This work extends non-local isoperimetric energies to curved geometries by introducing a Riemannian autocorrelation function $c_\Omega$ and characterising finite perimeter via a BV framework expressed through geodesic difference quotients. The approach replaces Euclidean translations with geodesic flows, leveraging Liouville invariance to relate the non-local term to $c_\Omega$, and proving that $c_\Omega$ is Lipschitz if and only if $\Omega$ has finite perimeter, with $c'_\Omega(0)$ proportional to the perimeter. On the round sphere, the authors prove a Gamma-convergence result as $\varepsilon\to0$ for $0<\gamma<\gamma_{\mathrm{crit}}$, with $\gamma_{\mathrm{crit}}=1$, and show the energy localises to a multiple of the perimeter, precluding fine-scale pattern formation in the subcritical regime. Overall, the paper provides a geometry-aware framework for analyzing pattern formation on curved membranes by linking BV theory, geodesic dynamics, and non-local interactions via the Riemannian autocorrelation function.
Abstract
We study a family of non-local isoperimetric energies $E_{γ,\varepsilon}$ on the round sphere $M = S^n$, where the non-local interaction kernel $K_\varepsilon$ is the fundamental solution of the Helmholtz operator $1 - \varepsilon^2 Δ$. To analyse these energies, we introduce a Riemannian autocorrelation function $c_Ω$ associated to a measurable set $Ω\subset M$, defined on any compact, connected, oriented Riemannian manifold without boundary $(M^n,g)$ of dimension $n\ge2$. This function is intimately linked to Matheron's set covariogram from convex geometry. By establishing a characterisation of functions of bounded variation $BV(M)$ in terms of geodesic difference quotients, we show that $Ω$ has finite perimeter if and only if $c_Ω$ is Lipschitz, and we relate the Lipschitz constant to the perimeter of $Ω$. We show that on the round sphere $E_{γ,\varepsilon}$ admits a reformulation in terms of $c_Ω$, which allows us to compute the limit as $\varepsilon \to 0$ in a variational sense, that is, in the framework of $Γ$-convergence.
