Résumé
The thermal equilibrium state of a charged, isentropic quantum fluid in a bounded domain Ω is entirely described by the particle density n minimizing the total energy where ϕ = V[n] + Ve solves Poisson’s equation - Δϕ = n - C subject to mixed Dirichlet-Neumann boundary conditions. It is shown that for given N > 0 (i. e. for prescribed total number of particles) this energy functional admits a unique minimizer in Furthermore it is proven that n ε Cloc1(Ω) H L∞(Ω) for all λ ε (0,1) and n > 0 in Ω.
| langue originale | Anglais |
|---|---|
| Pages (de - à) | 885-900 |
| Nombre de pages | 16 |
| journal | Communications in Partial Differential Equations |
| Volume | 20 |
| Numéro de publication | 5-6 |
| Les DOIs | |
| état | Publié - 1 janv. 1995 |
| Modification externe | Oui |
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