Différences
Ci-dessous, les différences entre deux révisions de la page.
| Les deux révisions précédentes Révision précédente | Prochaine révisionLes deux révisions suivantes | ||
| anr-efi:publications [2022/11/24 17:44] – Jean Dolbeault | anr-efi:publications [2022/11/24 17:50] – Jean Dolbeault | ||
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| ** 2022 ** | ** 2022 ** | ||
| - | * // Eyring-Kramers exit rates for the overdamped Langevin dynamics: the case with saddle points on the boundary.// Lelièvre, T. & Le Peutrec, D. & Nectoux, B. [[https:// | + | * // Eyring-Kramers exit rates for the overdamped Langevin dynamics: the case with saddle points on the boundary.// Lelièvre, T. & Le Peutrec, D. & Nectoux, B. [[https:// |
| - | * // Convergence of the kinetic annealing for general potentials.// | + | * // Convergence of the kinetic annealing for general potentials.// |
| - | * // Almost sure contraction for diffusions on $\mathbb R^d$.// Application to generalised Langevin diffusions.// | + | * // Almost sure contraction for diffusions on $\mathbb R^d$. Application to generalised Langevin diffusions.// |
| - | * // Uniform convergence of the Fleming-Viot process in a hard killing metastable case.// Journel, L. & Monmarché, P. [[https:// | + | * // Uniform convergence of the Fleming-Viot process in a hard killing metastable case.// Journel, L. & Monmarché, P. [[https:// |
| * // Wasserstein contraction and Poincaré inequalities for elliptic diffusions at high temperature.// | * // Wasserstein contraction and Poincaré inequalities for elliptic diffusions at high temperature.// | ||
| * // From kinetic to fluid models of liquid crystals by the moment method.// Degond, P. & Frouvelle, A. & Liu, J.-G. [[https:// | * // From kinetic to fluid models of liquid crystals by the moment method.// Degond, P. & Frouvelle, A. & Liu, J.-G. [[https:// | ||