English

Nonlocal $s$-minimal surfaces and Lawson cones

Analysis of PDEs 2014-02-19 v1 Differential Geometry

Abstract

The nonlocal ss-fractional minimal surface equation for Σ=E\Sigma= \partial E where EE is an open set in RNR^N is given by HΣs(p):=RNχE(x)χEc(x)xpN+sdx = 0for all pΣ. H_\Sigma^ s (p) := \int_{R^N} \frac {\chi_E(x) - \chi_{E^c}(x)} {|x-p|^{N+s}}\, dx \ =\ 0 \quad \text{for all } p\in \Sigma. Here 0<s<10<s<1, χ\chi designates characteristic function, and the integral is understood in the principal value sense. The classical notion of minimal surface is recovered by letting s1s\to 1. In this paper we exhibit the first concrete examples (beyond the plane) of nonlocal ss-minimal surfaces. When ss is close to 11, we first construct a connected embedded ss-minimal surface of revolution in R3R^3, the {\bf nonlocal catenoid}, an analog of the standard catenoid x3=log(r+r21)|x_3| = \log (r + \sqrt{r^2 -1}). Rather than eventual logarithmic growth, this surface becomes asymptotic to the cone x3=r1s|x_3|= r\sqrt{1-s}. We also find a two-sheet embedded ss-minimal surface asymptotic to the same cone, an analog to the simple union of two parallel planes. On the other hand, for any 0<s<10<s<1, n,m1n,m\ge 1, ss-minimal Lawson cones v=αu|v|=\alpha|u|, (u,v)Rn×Rm(u,v)\in R^n\times R^m, are found to exist. In sharp contrast with the classical case, we prove their stability for small ss and n+m=7n+m=7, which suggests that unlike the classical theory (or the case ss close to 1), the regularity of ss-area minimizing surfaces may not hold true in dimension 77.

Keywords

Cite

@article{arxiv.1402.4173,
  title  = {Nonlocal $s$-minimal surfaces and Lawson cones},
  author = {Juan Dávila and Manuel del Pino and Juncheng Wei},
  journal= {arXiv preprint arXiv:1402.4173},
  year   = {2014}
}

Comments

92 pages, 2 figures

R2 v1 2026-06-22T03:10:09.141Z