Lowest eigenvalues and formally self-adjoint fourth order elliptic differential operators
Abstract
Let be a closed, smooth, Riemannian manifold of dimension . Let be a smooth -tensor field on . The divergence of is defined as . Now let be a differential operator on that is given on functions by . We will call the Laplace-Beltrami operator. With this definition in place, it is not difficult to produce an example of a formally self-adjoint elliptic differential operator on that has a sign-changing eigenfunction that is associated with the operator's lowest eigenvalue. Indeed, let be the second lowest eigenvalue of , and let be a differential operator on that is given on functions by . Then will possess a sign-changing eigenfunction that is associated with 's lowest eigenvalue.. The question that remains is given a smooth, closed manifold of dimension , how rare are formally self-adjoint elliptic differential operators on that have sign-changing eigenfunctions that are associated with the operators' lowest eigenvalues. In this paper, we will see that if , where is a smooth, symmetric, negative semi-definite -tensor field on , then , the differential operator on given on functions by , will have the property that it possesses a sign-changing eigenfunction that is associated with the lowest eigenvalue of the operator. This suggests that on any smooth, closed manifold of dimension there exists a lot of formally self-adjoint fourth order elliptic differential operators on the manifold that possess sign-changing eigenfunctions that are associated with the lowest eigenvalues of the operators.
Cite
@article{arxiv.2601.11882,
title = {Lowest eigenvalues and formally self-adjoint fourth order elliptic differential operators},
author = {David Raske},
journal= {arXiv preprint arXiv:2601.11882},
year = {2026}
}
Comments
7 pages. This paper is the fourth version of the paper that was originally called "Lowest eigenvalues and higher order elliptic differential operators". It differs from the third version in that the differential operators used in the fourth version are defined differently than those used in the third version