2018
DOI: 10.1080/10586458.2018.1538911
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On the Dual Geometry of Laplacian Eigenfunctions

Abstract: We discuss the geometry of Laplacian eigenfunctions −∆φ = λφ on compact manifolds (M, g) and combinatorial graphs G = (V, E). The 'dual' geometry of Laplacian eigenfunctions is well understood on T d (identified with Z d ) and R 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(φ λ , φµ) be… Show more

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Cited by 9 publications
(27 citation statements)
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References 29 publications
(30 reference statements)
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“…Already the simpler question of understanding L 2 −size of the product is highly nontrivial: a seminal result of Burq-Gérard-Tzetkov [8] states e µ e λ L 2 min(λ 1/4 , µ 1/4 ) e λ L 2 e µ L 2 on compact two-dimensional manifolds without boundary (this has been extended to higher dimensions [4,7]). A recent result of the third author [23] (see also [9]) shows that one would generically (i.e., on typical manifolds in the presence of quantum chaos) expect e i (x)e j (x) to be mainly supported at eigenfunctions having their eigenvalue close to max {λ i , λ j } and that deviation from this phenomenon, as in the case of Fourier series on T for example, requires eigenfunctions to be strongly correlated at the wavelength in a precise sense.…”
Section: Introductionmentioning
confidence: 98%
“…Already the simpler question of understanding L 2 −size of the product is highly nontrivial: a seminal result of Burq-Gérard-Tzetkov [8] states e µ e λ L 2 min(λ 1/4 , µ 1/4 ) e λ L 2 e µ L 2 on compact two-dimensional manifolds without boundary (this has been extended to higher dimensions [4,7]). A recent result of the third author [23] (see also [9]) shows that one would generically (i.e., on typical manifolds in the presence of quantum chaos) expect e i (x)e j (x) to be mainly supported at eigenfunctions having their eigenvalue close to max {λ i , λ j } and that deviation from this phenomenon, as in the case of Fourier series on T for example, requires eigenfunctions to be strongly correlated at the wavelength in a precise sense.…”
Section: Introductionmentioning
confidence: 98%
“…However, one important drawback of the above method is that the construction of the spectral filters F j solely depends on the eigenvalue distribution (except some flexibility in choosing the filter pair (h, g), and the dilation parameters {s j }) and does not reflect how the eigenvectors behave. [5,20,31,40,[48][49][50][51].…”
Section: A Motivating Examplementioning
confidence: 99%
“…Second, in the long term, this is a first method of systematically using the novel concept of eigenvector dual geometry [5,31,49]. This direction can set a path for future modification of spectral graph theory applications to incorporate dual geometry.…”
Section: Introductionmentioning
confidence: 95%
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