On the Dynamics of Large Particle Systems in the Mean Field Limit

By François Golse. 2013

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This course explains how the usual mean field evolution partial differential equations (PDEs) in Statistical Physics—such as the Vlasov-Poisson system, the vorticity formulation of the two-dimensional Euler equation for incompressible fluids, or the time-dependent Hartree equation in quantum mechanics—can be rigorously derived from the fundamental microscopic equations that govern the evolution of large, interacting particle systems. The emphasis is put on the mathematical methods used in these derivations, such as Dobrushin’s stability estimate in the Monge-Kantorovich distance for the empirical measures built on the solution of the N-particle motion equations in classical mechanics, or the theory of BBGKY hierarchies in the case of classical as well as quantum problems. We explain in detail how these different approaches are related; in particular we insist on the notion of chaotic sequences and on the propagation of chaos in the BBGKY hierarchy as the number of particles tends to infinity.

Subfields: Applied Mathematics, Astronomy and Astrophysics, Computational Mechanics

View Paper: https://www.semanticscholar.org/paper/c9f34244e41be310a266c589c44ffc48fc719fcc

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In Applied Mathematics

  1. Zhenfu Wang
  2. Pierre-Emmanuel Jabin
  3. Daniel Lacker
  4. Didier Bresch
  5. Benoit Perthame
  6. M. Hauray

In Astronomy and Astrophysics

  1. Zhenfu Wang
  2. Pierre-Emmanuel Jabin

In Computational Mechanics

  1. Zhenfu Wang
  2. Pierre-Emmanuel Jabin
  3. Benoit Perthame

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