2013
DOI: 10.2140/apde.2013.6.1213
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Nodal count of graph eigenfunctions via magnetic perturbation

Abstract: Abstract. We establish a connection between the stability of an eigenvalue under a magnetic perturbation and the number of zeros of the corresponding eigenfunction. Namely, we consider an eigenfunction of discrete Laplacian on a graph and count the number of edges where the eigenfunction changes sign (has a "zero"). It is known that the n-th eigenfunction has n − 1 + s such zeros, where the "nodal surplus" s is an integer between 0 and the number of cycles on the graph.We then perturb the Laplacian by a weak m… Show more

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Cited by 32 publications
(57 citation statements)
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“…Numerical evidence suggests that this should be the case for discrete graphs as well and it is interesting to prove (or maybe disprove) such an inverse result. A possible approach might be to check whether a similar magnetic-nodal connection exists for the nodal domain count as well (which would form a nontrivial generalization of other work [26][27][28]) and to apply it for the inverse problem. Another generalization direction of the magnetic-nodal link, from which inverse problems would benefit, is to give some treatment for non-simple eigenvalues and for eigenfunctions which vanish at vertices.…”
Section: Discussionmentioning
confidence: 99%
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“…Numerical evidence suggests that this should be the case for discrete graphs as well and it is interesting to prove (or maybe disprove) such an inverse result. A possible approach might be to check whether a similar magnetic-nodal connection exists for the nodal domain count as well (which would form a nontrivial generalization of other work [26][27][28]) and to apply it for the inverse problem. Another generalization direction of the magnetic-nodal link, from which inverse problems would benefit, is to give some treatment for non-simple eigenvalues and for eigenfunctions which vanish at vertices.…”
Section: Discussionmentioning
confidence: 99%
“…In the discrete case, such perturbations include changing the non-zero entries of the matrix L. For a metric graph, one may perturb either the vertex conditions, the edge lengths or the electric potential. Further discussions can be found in [23,26,42], where this assumption was used.…”
Section: Assumption 11 the Eigenvalue λ N Is Simple And The Correspmentioning
confidence: 99%
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“…In the recent paper [2], Gregory Berkolaiko proves a nice formula for the nodal defect of an eigenfunction of a Schrödinger operator on a finite graph in terms of the Morse index of the corresponding eigenvalue as a function of a magnetic deformation of the operator. His proof remains mysterious and rather indirect.…”
Section: Introductionmentioning
confidence: 99%