English

A Metric Sturm-Liouville theory in Two Dimensions

Analysis of PDEs 2019-12-02 v2 Classical Analysis and ODEs Spectral Theory

Abstract

A central result of Sturm-Liouville theory (also called the Sturm-Hurwitz Theorem) states that if ϕk\phi_k is a sequence of eigenfunctions of a second order differential operator on the interval IRI \subset \mathbb{R}, then any linear combination satisfies a uniform bound on the roots #{xI:knakϕk(x)=0}n1. \# \left\{x \in I:\sum_{k \geq n}{ a_k \phi_k(x)} = 0 \right\} \geq n-1. We provide a sharp (up to logarithmic factors) generalization to two dimensions: let (M,g)(M,g) be a compact two-dimensional manifold (with or without boundary), let (ϕk)(\phi_k) denote the sequence of eigenfunctions of a uniformly elliptic operator \mboxdiv(a())-\mbox{div}(a(\cdot) \nabla) (with Dirichlet or Neumann boundary conditions). Then, for any linear combination of eigenfunctions above a certain index nn, f=knakϕk \mboxwehaveH1{x:f(x)=0}nlognlog(nfL2(M)fL1(M))1/2fL1(M)fL(M). f = \sum_{k \geq n}{a_k \phi_k} ~ \mbox{we have} \quad \mathcal{H}^1 \left\{ x: f(x) = 0\right\} \gtrsim_{} \frac{\sqrt{n}}{\sqrt{\log{n}}} \log \left(n \frac{\|f\|_{L^2(M)}}{\|f\|_{L^1(M)}} \right)^{-1/2} \frac{\|f\|_{L^1(M)}}{\| f \|_{L^{\infty}(M)}} . Examples on M=T2M=\mathbb{T}^2 and M=S2M=\mathbb{S}^2 shows that this is optimal up to the logarithmic factors. The proof is using optimal transport and a new inequality for the Wasserstein metric WpW_p: if f(x)dxf(x)dx and g(x)dxg(x)dx are two absolutely continuous measures on a two-dimensional domain MM with continuous densities and the same total mass, then, for all 1p<1 \leq p <\infty, Wp(f(x)dx,g(x)dx)H1{xM:f(x)=g(x)}M,pfgL1(M)1+1/pfgL(M). W_p(f(x)dx, g(x) dx) \cdot \mathcal{H}^1 \left\{x \in M: f(x) = g(x) \right\} \gtrsim_{M,p} \frac{\|f-g\|_{L^1(M)}^{1+1/p}}{\|f-g\|_{L^{\infty}(M)}}.

Keywords

Cite

@article{arxiv.1809.01044,
  title  = {A Metric Sturm-Liouville theory in Two Dimensions},
  author = {Stefan Steinerberger},
  journal= {arXiv preprint arXiv:1809.01044},
  year   = {2019}
}