Abstract
We consider the nonlinear Hartree equation for an interacting gas containing infinitely many particles and we investigate the large-time stability of the stationary states of the form f (-δ), describing a homogeneous quantum gas. Under suitable assumptions on the interaction potential and on the momentum distribution f , we prove that the stationary state is asymptotically stable in dimension 2. More precisely, for any initial datum which is a small perturbation of f (-δ) in a Schatten space, the system weakly converges to the stationary state for large times.
| Original language | English |
|---|---|
| Pages (from-to) | 1339-1363 |
| Number of pages | 25 |
| Journal | Analysis and PDE |
| Volume | 7 |
| Issue number | 6 |
| DOIs | |
| Publication status | Published - 1 Jan 2014 |
| Externally published | Yes |
Keywords
- Hartree equation
- Infinite quantum systems
- Lindhard function
- Scattering
- strichartz inequality