Morse theory for discrete magnetic operators and nodal count distribution for graphs

Abstract

Given a discrete Schrödinger operator $h$ on a finite connected graph $G$ of $n$ vertices, the nodal count $\varphi (h,k)$ denotes the number of edges on which the $k$-th eigenvector changes sign. A signing $h^{\prime }$ of $h$ is any real symmetric matrix constructed by changing the sign of some off-diagonal entries of $h$, and its nodal count is defined according to the signing. The set of signings of $h$ lie in a naturally defined torus ${\mathbb{T}}_h$ of “magnetic perturbations” of $h$. G. Berkolaiko [Anal. PDE 6 (2013), 1213–1233] discovered that every signing $h^{\prime }$ of $h$ is a critical point of every eigenvalue ${\lambda }_k:{\mathbb{T}}_h\to \mathbb{R}$, with Morse index equal to the nodal surplus. We add further Morse theoretic information to this result. We show if $h_{\alpha }\in {\mathbb{T}}_h$ is a critical point of ${\lambda }_k$ and the eigenvector vanishes at a single vertex $v$ of degree $d$, then the critical point lies in a non-degenerate critical submanifold of dimension $d+n-4$, closely related to the configuration space of a planar linkage. We compute its Morse index in terms of spectral data. The average nodal surplus distribution is the distribution of values of $\varphi (h^{\prime },k)-(k-1)$, averaged over all signings $h^{\prime }$ of $h$. If all critical points correspond to simple eigenvalues with nowhere-vanishing eigenvectors, then the average nodal surplus distribution is binomial. In general, we conjecture that the nodal surplus distribution converges to a Gaussian in a CLT fashion as the first Betti number of $G$ goes to infinity.