Dynamic of Threshold Solutions for Energy-Critical NlS
By Thomas Duyckaerts, F. Merle. 2007
161 citations recorded by the source corpus.
Abstract.We consider the energy-critical non-linear focusing Schrödinger equation in dimension N = 3, 4, 5. An explicit stationary solution, W, of this equation is known. In [KeM], the energy E(W) has been shown to be a threshold for the dynamical behavior of solutions of the equation. In the present article, we study the dynamics at the critical level E(u) = E(W) and classify the corresponding solutions. This gives in particular a dynamical characterization of W.
Subfields: Control and Systems Engineering, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/9dfc3a937d1c4a312f462bbed11d6eae1a794252
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In Control and Systems Engineering
In Mathematical Physics
- F. Merle
- Pierre Raphael
- Yvan Martel
- Jérémie Szeftel
- Carlos E. Kenig
- Aynur Bulut
- Vianney Combet
- Xiaoyi Zhang
Citations in the corpus
- Existence and uniqueness of minimal blow-up solutions to an inhomogeneous mass critical NLS (2010, methodology): “[23] Merle, F., Determination of minimal blow-up solutions with minimal mass for nonlinear Schrödinger equations with critical power.”
- Multi-Soliton Solutions for the Supercritical gKdV Equations (2010, result): “[14] Y. Martel and F. Merle.”
- Blow up for the critical gKdV equation II: minimal mass dynamics (2012, methodology): “Related rigidity theorems near the solitary wave were recently obtained by Nakanishi and Schlag [46], [47] for super critical wave and Schrödinger equations using the invariant set methods of Beresticky, Cazenave [2], the Kenig-Merle concentration compactness approach [14], the classification of min”
- Stability and Unconditional Uniqueness of Solutions for Energy Critical Wave Equations in High Dimensions (2009, methodology): “he energy threshold E (u0,u1) = E (W,0) in high dimensions. Such dynamics were analyzed by Duyckaerts and Merle [5] for 3 ≤ d ≤ 5, and recently by Li and Zhang [20] in high dimensions d ≥ 6 (see also [6] and [21] for the NLS case). 2In Theorem 3.6 we do not assume smallness in exotic Strichartz spac”