Normalized ground states for the NLS equation with combined nonlinearities: the Sobolev critical case
Nicola Soave
TL;DR
This work develops a constrained variational framework for normalized ground states of the Sobolev-critical nonlinear Schrödinger equation with combined nonlinearities on $\mathbb{R}^N$, under a prescribed mass $a^2$. It introduces the Pohozaev manifold $\mathcal{P}_{a,\mu}$ as a natural constraint and analyzes the fiber maps $\Psi_u^\mu$ to study energy geometry under $L^2$-preserving dilations, obtaining existence results across $L^2$-subcritical, critical, and supercritical perturbations. A key contribution is the precise threshold condition $\mu a^{(1-\gamma_q)q}<\alpha(N,q)$, with explicit $\alpha$ depending on $N$ and $q$, which yields ground states that are real, positive, and radially symmetric with negative or positive energy according to the regime; the analysis covers both compactness of PS sequences and a Brezis–Nirenberg–type dichotomy in the critical setting. The paper also proves nonexistence results for defocusing perturbations and studies the asymptotic behavior of ground states as $\mu\to0^+$, connecting normalized solutions to the homogeneous Sobolev-critical problem and highlighting discontinuities in ground-state levels. Dynamical implications are discussed, including stability/instability and blow-up criteria, illustrating how the constrained critical points govern long-time behavior in the Sobolev-critical regime.
Abstract
We study existence and properties of ground states for the nonlinear Schrödinger equation with combined power nonlinearities \[ -Δu= λu + μ|u|^{q-2} u + |u|^{2^*-2} u \qquad \text{in $\mathbb{R}^N$, $N \ge 3$,} \] having prescribed mass \[ \int_{\mathbb{R}^N} |u|^2 = a^2, \] in the \emph{Sobolev critical case}. For a $L^2$-subcritical, $L^2$-critical, of $L^2$-supercritical perturbation $μ|u|^{q-2} u$ we prove several existence/non-existence and stability/instability results. This study can be considered as a counterpart of the Brezis-Nirenberg problem in the context of normalized solutions, and seems to be the first contribution regarding existence of normalized ground states for the Sobolev critical NLSE in the whole space $\mathbb{R}^N$.
