Skip to content
DraconiticResearch
Search Sources API
197,768 studies31 sourcesUpdated 29 min ago
PreprintarXiv licencearXiv

Almost-sure quenched KAM tori for cubic NLS with a spatial white-noise potential

Abstract

Let Aω=−∂x2+ρḂx(ω), ρ≠0, be the Dirichlet Schrödinger operator on (0,π) with a spatial Gaussian white-noise potential, realized pathwise via quasi-derivatives. Here Ḃx denotes the distributional derivative of Brownian motion with respect to the spatial variable x. For κ≠0, we consider the cubic nonlinear Schrödinger equation i ut=Aωu+κ|u|2u. We first prove a zero-set theorem for locally real-analytic functions on classical Wiener space. As a consequence, on a single event of probability one, no nontrivial finitely supported integer combination of the random eigenvalues vanishes, and the quartic twist matrix is nonsingular for every finite tangential set. After fixing a path in this event, we combine these qualitative nondegeneracy properties with a partial quartic Birkhoff normal form adapted to the KAM scheme. For every finite nonempty tangential set J of cardinality b, we obtain a Cantor family of linearly stable, real-analytic, small-amplitude invariant b-tori. The family is parametrized by a Cantor subset of [ν,2ν]b whose relative measure tends to one as ν→0.

Related

  1. Blow-up or grow-up for the focusing 3D cubic NLS with a repulsive inverse-power potential at the mass--energy threshold
    Alex H. Ardila, Zuyu Ma, Ying Wang
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  2. Soliton Dynamics for the Cubic-Quintic Nonlinear Schrödinger Equation with a Potential
    Alex H. Ardila, Rémi Carles
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  3. Overcoming the spatial order barrier for nonlinear SPDEs with additive space-time white noise
    Lukas Anzeletti, Máté Gerencsér, Helena Kremp
    arXivPreprintCC BY 4.0Full textNumerical analysis & scientific computingProbabilityarXiv
  4. Modeling soliton-potential interactions for the 1-D cubic NLS via an invariant-preserving finite-difference method
    Anthony D. Stone Jr., Christopher C. Hogan
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  5. Polytopic symmetric interior-penalty approximation of elliptic SPDEs driven by spatial white noise
    Tristan Pryer
    arXivPreprintCC BY 4.0Full textNumerical analysis & scientific computingarXiv
BibTeX
@misc{dong2026almostsure,
  title = {{Almost-sure quenched KAM tori for cubic NLS with a spatial white-noise potential}},
  author = {Yingdu Dong and Wenwen Jian and Xiaoping Yuan},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.22808},
  eprint = {2609.22808},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.22808},
}
RIS
TY  - UNPB
TI  - Almost-sure quenched KAM tori for cubic NLS with a spatial white-noise potential
AU  - Yingdu Dong
AU  - Wenwen Jian
AU  - Xiaoping Yuan
PY  - 2026
DA  - 2026/09/19
PB  - arXiv
DO  - 10.48550/arxiv.2609.22808
UR  - https://arxiv.org/abs/2609.22808
AB  - Let A_ω=−∂_x^2+ρḂ_x(ω), ρ≠0, be the Dirichlet Schrödinger operator on (0,π) with a spatial Gaussian white-noise potential, realized pathwise via quasi-derivatives. Here Ḃ_x denotes the distributional derivative of Brownian motion with respect to the spatial variable x. For κ≠0, we consider the cubic nonlinear Schrödinger equation i u_t=A_ωu+κ|u|^2u. We first prove a zero-set theorem for locally real-analytic functions on classical Wiener space. As a consequence, on a single event of probability one, no nontrivial finitely supported integer combination of the random eigenvalues vanishes, and the quartic twist matrix is nonsingular for every finite tangential set. After fixing a path in this event, we combine these qualitative nondegeneracy properties with a partial quartic Birkhoff normal form adapted to the KAM scheme. For every finite nonempty tangential set J of cardinality b, we obtain a Cantor family of linearly stable, real-analytic, small-amplitude invariant b-tori. The family is parametrized by a Cantor subset of [ν,2ν]^b whose relative measure tends to one as ν→0.
ER  -