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| animation:seminaires:2010:accueil [2013/01/29 10:18] – [Séminaires 2010] sbarends | animation:seminaires:2010:accueil [2013/02/19 13:56] (Version actuelle) – sbarends | ||
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| ====== Séminaires 2010 ====== | ====== Séminaires 2010 ====== | ||
| - | **On the spectroscopy, | + | {{: |
| Séminaire du Centre Blaise Pascal \\ | Séminaire du Centre Blaise Pascal \\ | ||
| Location: Salle de réunion LR6 C 023, Centre Blaise Pascal, ENS-Lyon, France \\ | Location: Salle de réunion LR6 C 023, Centre Blaise Pascal, ENS-Lyon, France \\ | ||
| **November 16, 2010 - 13:45** | **November 16, 2010 - 13:45** | ||
| - | * FLORENT | + | * Florent |
| Abstract: Quantum nuclear effects are usually manifested in weakly-bound compounds or at low temperatures. The role of nuclear delocalization has thus been emphasized in situations involving the hydrogen or neon atoms, for which the classical treatment is likely to be approximate. The path integral (PI) approach to quantum statistics at finite temperature offers a convenient theoretical framework to address such effects in molecular dynamics (MD) simulations of complex systems. In this talk, we will review the basics of the PIMD method and its variants, as well as some of its recent improvements. Several applications will be presented and discussed, ranging from the diffusion of hydrogen in palladium nanoparticles, | Abstract: Quantum nuclear effects are usually manifested in weakly-bound compounds or at low temperatures. The role of nuclear delocalization has thus been emphasized in situations involving the hydrogen or neon atoms, for which the classical treatment is likely to be approximate. The path integral (PI) approach to quantum statistics at finite temperature offers a convenient theoretical framework to address such effects in molecular dynamics (MD) simulations of complex systems. In this talk, we will review the basics of the PIMD method and its variants, as well as some of its recent improvements. Several applications will be presented and discussed, ranging from the diffusion of hydrogen in palladium nanoparticles, | ||
| - | **A spectral fictitious domain method with internal forcing for solving elliptic PDEs** \\ | + | {{: |
| Séminaire du Centre Blaise Pascal \\ | Séminaire du Centre Blaise Pascal \\ | ||
| Location: Salle de réunion LR6 C 023, Centre Blaise Pascal, ENS-Lyon, France \\ | Location: Salle de réunion LR6 C 023, Centre Blaise Pascal, ENS-Lyon, France \\ | ||
| **October 19, 2010 - 15:00** \\ | **October 19, 2010 - 15:00** \\ | ||
| - | * MARC BUFFAT, Laboratoire de Mécanique des fluides et acoustique, Université Claude Bernard Lyon I, France | + | * Marc BUFFAT, Laboratoire de Mécanique des fluides et acoustique, Université Claude Bernard Lyon I, France |
| Abstract: A fictitious domain method is presented for solving elliptic partial differential equations using Galerkin spectral approximation. The fictitious domain approach consists in immersing the original domain into a larger and geometrically simpler one in order to avoid the use of boundary fitted or unstructured meshes. In the present study, boundary constraints are enforced using Lagrange multipliers and the novel aspect is that the Lagrange multipliers are associated with smooth forcing functions, compactly supported inside the fictitious domain. This allows the accuracy of the spectral method to be preserved, unlike the classical discrete Lagrange multipliers method, in which the forcing is defined on the boundaries. In order to have a robust and efficient method, equations for the Lagrange multipliers are solved directly with an influence matrix technique. Using a Fourier-Chebyshev Petrov-Galerkin approximation, | Abstract: A fictitious domain method is presented for solving elliptic partial differential equations using Galerkin spectral approximation. The fictitious domain approach consists in immersing the original domain into a larger and geometrically simpler one in order to avoid the use of boundary fitted or unstructured meshes. In the present study, boundary constraints are enforced using Lagrange multipliers and the novel aspect is that the Lagrange multipliers are associated with smooth forcing functions, compactly supported inside the fictitious domain. This allows the accuracy of the spectral method to be preserved, unlike the classical discrete Lagrange multipliers method, in which the forcing is defined on the boundaries. In order to have a robust and efficient method, equations for the Lagrange multipliers are solved directly with an influence matrix technique. Using a Fourier-Chebyshev Petrov-Galerkin approximation, | ||
| - | **Simulation numérique des écoulements complexes ; importance de l' | + | {{: |
| Séminaire du Centre Blaise Pascal \\ | Séminaire du Centre Blaise Pascal \\ | ||
| Location: Salle de réunion LR6 C 023, Centre Blaise Pascal, ENS-Lyon, France \\ | Location: Salle de réunion LR6 C 023, Centre Blaise Pascal, ENS-Lyon, France \\ | ||
| **Septembre 14, 2010 - 15:00** \\ | **Septembre 14, 2010 - 15:00** \\ | ||
| - | * EMMANUEL | + | * Emmanuel |
| - | **Physique statistique du repliement et de la dénaturation des acides nucléiques** \\ | + | {{: |
| Location: Amphi A, ENS-Lyon, France \\ | Location: Amphi A, ENS-Lyon, France \\ | ||
| **June 23, 2010** \\ | **June 23, 2010** \\ | ||
| - | * DANIEL | + | * Daniel |
| Abstract: L' | Abstract: L' | ||