{ "id": "2306.03585", "version": "v1", "published": "2023-06-06T11:03:08.000Z", "updated": "2023-06-06T11:03:08.000Z", "title": "Selection principle for the Fleming-Viot process with drift $-1$", "authors": [ "Oliver Tough" ], "comment": "25 pages", "categories": [ "math.PR", "math.AP" ], "abstract": "We consider the Fleming-Viot particle system consisting of $N$ identical particles evolving in $\\mathbb{R}_{>0}$ as Brownian motions with constant drift $-1$. Whenever a particle hits $0$, it jumps onto another particle in the interior. It is known that this particle system has a hydrodynamic limit as $N\\rightarrow\\infty$ given by Brownian motion with drift $-1$ conditioned not to hit $0$. This killed Brownian motion has an infinite family of quasi-stationary distributions (QSDs), with a Yaglom limit given by the unique QSD minimising the survival probability. On the other hand, for fixed $N<\\infty$, this particle system converges to a unique stationary distribution as time $t\\rightarrow\\infty$. We prove the following selection principle: the empirical measure of the $N$-particle stationary distribution converges to the aforedescribed Yaglom limit as $N\\rightarrow\\infty$. The selection problem for this particular Fleming-Viot process is closely connected to the microscopic selection problem in front propagation, in particular for the $N$-branching Brownian motion. The proof requires neither fine estimates on the particle system nor the use of Lyapunov functions.", "revisions": [ { "version": "v1", "updated": "2023-06-06T11:03:08.000Z" } ], "analyses": { "subjects": [ "35C07", "35K57", "35Q92", "60J80", "60J85" ], "keywords": [ "fleming-viot process", "selection principle", "brownian motion", "particle stationary distribution converges", "yaglom limit" ], "note": { "typesetting": "TeX", "pages": 25, "language": "en", "license": "arXiv", "status": "editable" } } }