Semilinear Schrodinger equation: Difference between revisions
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* [[NLS wellposedness|Local and global well-posedness theory]] | * [[NLS wellposedness|Local and global well-posedness theory]] | ||
* [[NLS scattering|Scattering theory]] | * [[NLS scattering|Scattering theory]] | ||
* [[NLS stability|Stability of solitons]] | |||
* [[NLS blowup|Blowup]] | * [[NLS blowup|Blowup]] | ||
* [[Unique continuation]] | * [[Unique continuation]] |
Revision as of 22:08, 5 August 2006
[Many thanks to Kenji Nakanishi with valuable help with the scattering theory portion of this section. However, we are still missing many references and results, e.g. on NLS blowup. - Ed.]
The semilinear Schrodinger equation (NLS) is
for p>1. There are many specific cases of this equation which are of interest, but in this page we shall focus on the general theory. The sign choice is the defocusing case; is focussing. There are also several variants of NLS, such as NLS with potential or NLS on manifolds and obstacles; see the general page on Schrodinger equations for more discussion.
Theory
- Algebraic structure (Symmetries, conservation laws, transformations, Hamiltonian structure)
- Local and global well-posedness theory
- Scattering theory
- Stability of solitons
- Blowup
- Unique continuation