Necessary and sufficient condition for existence at resonance for eigenvalues of multiplicity two
Philip Korman
TL;DR
The paper addresses existence of solutions to semilinear Dirichlet problems at resonance for eigenvalues with two-dimensional eigenspaces. It extends the Landesman–Lazer framework by deriving a necessary and sufficient condition expressed through projections of the forcing term onto the two-dimensional eigenspace and a universal quantity $J_{n,m}$ that depends on the jumps $g(\infty) - g(-\infty)$. In the disc setting $B_a \subset \mathbb{R}^2$, where all nonprincipal eigenvalues have multiplicity two, the authors obtain an explicit criterion: $\sqrt{A_k^2 + B_k^2} < J_{n,m}(g(\infty) - g(-\infty))$, with $A_k,B_k$ the appropriate projections, and $J_{n,m}$ computed from the eigenfunction radial structure. They illustrate with a unit-disc example and apply the results to prove unboundedness of all steady states for the corresponding semilinear heat equation, highlighting a PDE analogue of the Lazer–Leach theorem.
Abstract
We establish necessary and sufficient condition for existence of solutions for a class of semilinear Dirichlet problems with the linear part at resonance at eigenvalues of multiplicity two. The result is applied to give a condition for unboundness of all solutions of the corresponding semilinear heat equation.
