English

Normalized ground states for NLS equations with mass critical nonlinearities

Analysis of PDEs 2025-10-30 v2

Abstract

We study normalized solutions (μ,u)R×H1(RN)(\mu,u)\in \mathbb{R} \times H^1(\mathbb{R}^N) to nonlinear Schr\"odinger equations Δu+μu=g(u)in RN,12RNu2dx=m, -\Delta u + \mu u = g(u)\quad \hbox{in}\ \mathbb{R}^N, \qquad \frac{1}{2}\int_{\mathbb{R}^N} u^2 dx = m, where N2N\geq 2 and the mass m>0m>0 is given. Here gg has an L2L^2-critical growth, both at the origin and at infinity, that is g(s)sp1sg(s)\sim |s|^{p-1}s as s0s\sim 0 and ss\sim\infty, where p=1+4Np=1+\frac{4}{N}. We continue the analysis started in [Cingolani-Gallo-Ikoma-Tanaka, 2024], where we found two (possibly distinct) minimax values b0b\underline{b} \leq 0 \leq \overline{b} of the Lagrangian functional. In this paper we furnish explicit examples of gg satisfying b<0<b\underline{b}<0<\overline{b}, b=0<b\underline{b}=0<\overline{b} and b<0=b\underline{b}<0=\overline{b}; notice that b=0=b\underline{b}=0=\overline{b} in the power case g(t)=tp1tg(t)=|t|^{p-1}t. Moreover, we deal with the existence and non-existence of a solution with minimal energy. Finally, we discuss the assumptions required on gg to obtain the existence of a positive solution for perturbations of gg.

Keywords

Cite

@article{arxiv.2507.00639,
  title  = {Normalized ground states for NLS equations with mass critical nonlinearities},
  author = {Silvia Cingolani and Marco Gallo and Norihisa Ikoma and Kazunaga Tanaka},
  journal= {arXiv preprint arXiv:2507.00639},
  year   = {2025}
}
R2 v1 2026-07-01T03:41:22.532Z