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Nonlocal ss-minimal surfaces and Lawson cones

Published 17 Feb 2014 in math.AP and math.DG | (1402.4173v1)

Abstract: The nonlocal ss-fractional minimal surface equation for Σ=∂E\Sigma= \partial E where EE is an open set in R<sup>NR<sup>N is given by HΣs(p):=∫R<sup>N</sup>χE(x)−χE<sup>c(x)</sup>∣x−p∣<sup>N+s </sup>dx = 0for all p∈Σ. H_\Sigma^ s (p) := \int_{R<sup>N}</sup> \frac {\chi_E(x) - \chi_{E<sup>c}(x)}</sup> {|x-p|<sup>{N+s}}\,</sup> dx \ =\ 0 \quad \text{for all } p\in \Sigma. Here $0<s<1$, 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 s→1s\to 1. In this paper we exhibit the first concrete examples (beyond the plane) of nonlocal s−s-minimal surfaces. When ss is close to $1$, we first construct a connected embedded ss-minimal surface of revolution in R<sup>3R<sup>3, the {\bf nonlocal catenoid}, an analog of the standard catenoid ∣x3∣=log⁡(r+r<sup>2</sup>−1)|x_3| = \log (r + \sqrt{r<sup>2</sup> -1}). Rather than eventual logarithmic growth, this surface becomes asymptotic to the cone ∣x3∣=r1−s|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 $0<s<1$, n,m≥1n,m\ge 1, s−s-minimal Lawson cones ∣v∣=α∣u∣|v|=\alpha|u|, (u,v)∈R<sup>n×</sup>R<sup>m(u,v)\in R<sup>n\times</sup> R<sup>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 $7$.

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