English

Blow-up analysis and a priori bounds for NLS equations on metric graphs

Analysis of PDEs 2026-05-05 v1

Abstract

We consider, on a connected metric graph G\mathcal{G}, a family of nonlinear Schr\"odinger equations u+Wn(x)u+λnu=ρn(x)up2u,nN.() -u'' + W_n(x) u + \lambda_n u = \rho_n(x)|u|^{p-2}u, \quad n \in \mathbb{N}. \qquad (*) We assume that p>2p > 2, (Wn)(W_n), (ρn)L(G)(\rho_n) \subseteq L^{\infty}(\mathcal{G}) with ρn0\rho_n \geq 0, WnL(G)|W_n|_{L^\infty(\mathcal{G})} and ρnL(G)|\rho_n|_{L^\infty(\mathcal{G})} are bounded and λn+\lambda_n \to +\infty. Given nNn \in \mathbb{N}, we call "solution" a function unH1(G)u_n \in H^1(\mathcal{G}) which satisfies (*) for that nNn\in \mathbb{N} together with the Kirchhoff conditions at the vertices. Focusing on the limiting behavior of sequences (un)H1(G)(u_n) \subseteq H^1(\mathcal{G}) of solutions as λn+\lambda_n \to + \infty and assuming that the Morse index m(un)m(u_n) of unu_n is uniformly bounded, we establish, the existence of a finite subset of blow-up points away from which, up to a subsequence, un|u_n| has a global exponential decay. These points are generally a strict subset of the blow-up points, and their number is estimated by the bound on the Morse index of (un)(u_n). It is the first time that this global exponential decay property is established on graphs even if one consider only signed solutions. In the last part of the paper we derive various results of a priori bounds on the solutions in LL^\infty and L2L^2. Our blow-up analysis, combined with ODE arguments allows, for frequently considered classes of graphs, to obtain a fairly complete picture of the relationships between the number of nodal regions, Morse index, LL^\infty and L2L^2 norms of solutions.

Keywords

Cite

@article{arxiv.2605.02879,
  title  = {Blow-up analysis and a priori bounds for NLS equations on metric graphs},
  author = {Pablo Carrillo and Colette De Coster and Damien Galant and Louis Jeanjean and Christophe Troestler},
  journal= {arXiv preprint arXiv:2605.02879},
  year   = {2026}
}