Abstract
We study a population of N particles, which evolve according to a diffusion process and interact through a dynamical network. In turn, the evolution of the network is coupled to the particles' positions. In contrast with the mean-field regime, in which each particle interacts with every other particle, i.e., with O(N) particles, we consider the a priori more difficult case of a sparse network; that is, each particle interacts, on average, with O(1) particles. We also assume that the network's dynamics is much faster than the particles' dynamics, with the time-scale of the network described by a parameter ∊ > 0. We combine the averaging (∊ → 0) and the many-particles (N → ∞ ) limits and prove that the evolution of the particles' empirical density is described (after taking both limits) by a nonlinear Fokker-Planck equation; moreover, we give conditions under which such limits can be taken uniformly in time, hence providing a criterion under which the limiting nonlinear Fokker-Planck equation is a good approximation of the original system uniformly in time. The heart of our proof consists of controlling precisely the dependence on N of the averaging estimates.
| Original language | English |
|---|---|
| Pages (from-to) | 937–972 |
| Number of pages | 36 |
| Journal | SIAM Journal on Mathematical Analysis |
| Volume | 53 |
| Issue number | 1 |
| Early online date | 8 Feb 2021 |
| DOIs | |
| Publication status | Published - 2021 |
Keywords
- Averaging methods
- Interacting particle systems
- Markov semigroups
- Nonlinear Fokker-Plank equation
- Sparse interaction
ASJC Scopus subject areas
- Analysis
- Computational Mathematics
- Applied Mathematics