A Critical Centre-Stable Manifold for Schroedinger's Equation in R^3
arXiv:0909.1180
Abstract
Consider the focusing cubic semilinear Schroedinger equation in R^3 i \partial_t ψ+ Δψ+ | ψ|^2 ψ= 0. It admits an eight-dimensional manifold of special solutions called ground state solitons. We exhibit a codimension-one critical real-analytic manifold N of asymptotically stable solutions in a neighborhood of the soliton manifold. We then show that N is centre-stable, in the dynamical systems sense of Bates-Jones, and globally-in-time invariant. Solutions in N are asymptotically stable and separate into two asymptotically free parts that decouple in the limit --- a soliton and radiation. Conversely, in a general setting, any solution that stays close to the soliton manifold for all time is in N. The proof uses the method of modulation. New elements include a different linearization and an endpoint Strichartz estimate for the time-dependent linearized equation. The proof also uses the fact that the linearized Hamiltonian has no nonzero real eigenvalues or resonances. This has recently been established in the case treated here --- of the focusing cubic NLS in R^3 --- by the work of Marzuola-Simpson and Costin-Huang-Schlag.
Substantially revised from previous version
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- Numerical study of the blowup/global existence dichotomy for the focusing cubic nonlinear Klein-Gordon equation
- On asymptotic stability of moving ground states of the nonlinear Schrodinger equation
- Global dynamics above the ground state energy for the focusing nonlinear Klein-Gordon equation
- Blow-up criteria for the 3d cubic nonlinear Schrödinger equation
- Invariant manifolds around soliton manifolds for the nonlinear Klein-Gordon equation