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On the Dual Geometry of Laplacian Eigenfunctions

Published 25 Apr 2018 in eess.SP, cs.LG, math.AP, and math.SP | (1804.09816v1)

Abstract: We discuss the geometry of Laplacian eigenfunctions −Δϕ=λϕ-\Delta \phi = \lambda \phi on compact manifolds (M,g)(M,g) and combinatorial graphs G=(V,E)G=(V,E). The 'dual' geometry of Laplacian eigenfunctions is well understood on T<sup>d\mathbb{T}<sup>d (identified with Z<sup>d\mathbb{Z}<sup>d) and R<sup>n\mathbb{R}<sup>n (which is self-dual). The dual geometry is of tremendous role in various fields of pure and applied mathematics. The purpose of our paper is to point out a notion of similarity between eigenfunctions that allows to reconstruct that geometry. Our measure of 'similarity' α(ϕλ,ϕμ) \alpha(\phi_{\lambda}, \phi_{\mu}) between eigenfunctions ϕλ\phi_{\lambda} and ϕμ\phi_{\mu} is given by a global average of local correlations α(ϕλ,ϕμ)<sup>2</sup>=∣ϕλϕμ∣<em>L<sup>2<sup>−2∫</sup></sup></em>M(∫Mp(t,x,y)(ϕλ(y)−ϕλ(x))(ϕμ(y)−ϕμ(x))dy)<sup>2</sup>dx, \alpha(\phi_{\lambda}, \phi_{\mu})<sup>2</sup> = | \phi_{\lambda} \phi_{\mu} |<em>{L<sup>2}<sup>{-2}\int</sup></sup></em>{M}{ \left( \int_{M}{ p(t,x,y)( \phi_{\lambda}(y) - \phi_{\lambda}(x))( \phi_{\mu}(y) - \phi_{\mu}(x)) dy} \right)<sup>2</sup> dx}, where p(t,x,y)p(t,x,y) is the classical heat kernel and e<sup>−t</sup>λ+e<sup>−t</sup>μ=1e<sup>{-t</sup> \lambda} + e<sup>{-t</sup> \mu} = 1. This notion recovers all classical notions of duality but is equally applicable to other (rough) geometries and graphs; many numerical examples in different continuous and discrete settings illustrate the result.

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