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Normalized solutions for the nonlinear Schr\"odinger equation with potential: the purely Sobolev critical case

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arxiv 2505.05357 v1 pith:7XDZSJM7 submitted 2025-05-08 math.AP

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keywords existencepotentialsolutionsolutionscasecriticalequationmountain
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abstract

We study the existence and multiplicity of positive solutions in $H^1(\mathbb{R}^N)$, $N\ge3$, with prescribed $L^2$-norm, for the (stationary) nonlinear Schr\"odinger equation with Sobolev critical power nonlinearity. It is well known that, in the free case, the associated energy functional has a mountain pass geometry on the $L^2$-sphere. This boils down, in higher dimensions, to the existence of a mountain pass solution which is (a suitable scaling of) the Aubin-Talenti function. In this paper, we consider the same problem, in presence of a weakly attractive, possibly irregular, potential, wondering (i) whether a local minimum solution appears, thus providing an orbitally stable family of solitons, and (ii) if the existence of a mountain-pass solution persists. We provide positive answers, depending on suitable assumptions on the potential and on the mass value. Moreover, by the Hopf-Cole transform, we give some applications of our results to the existence of multiple solutions to ergodic Mean Field Games systems with potential and quadratic Hamiltonian.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Normalized solutions for the NLS equation with potential in higher dimension: the purely Sobolev critical case

    math.AP 2025-07 conditional novelty 7.0 of 10

    For N≥6, the normalized Sobolev-critical NLS with potential has a positive mountain-pass solution; for N≥3, a negative-energy local minimizer exists under weaker conditions than in the cited preprint.

  2. Energy local minimizers for the nonlinear Schr\"{o}dinger equation on product spaces

    math.AP 2025-06 conditional novelty 7.0 of 10

    Energy local minimizers with prescribed L2 norm exist in the mass-supercritical NLS on R^N x M^k; for small mass they are the Euclidean ground states, and in certain cases they become nontrivial along M^k.

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