{ "id": "2105.13486", "version": "v1", "published": "2021-05-27T22:47:36.000Z", "updated": "2021-05-27T22:47:36.000Z", "title": "A direct comparison between the mixing time of the interchange process with \"few\" particles and independent random walks", "authors": [ "Jonathan Hermon", "Richard Pymar" ], "comment": "24 pages", "categories": [ "math.PR" ], "abstract": "We consider the interchange process with $k$ particles (${\\rm IP}(k)$) on $n$-vertex hypergraphs in which each hyperedge $e$ rings at rate $r_e$. When $e$ rings, the particles occupying it are permuted according to a random permutation from some arbitrary law, where our only assumption is that ${\\rm IP}(2)$ has uniform stationary distribution. We show that $t_{\\rm mix}^{{\\rm IP}(k)}(\\epsilon)=O_{b}(t_{\\rm mix}^{{\\rm IP}(2)}(\\epsilon/k))$, where $t_{\\rm mix}^{{\\rm IP}(i)}(\\epsilon)$ is the $\\epsilon$ total-variation mixing time of ${\\rm IP}(i)$, provided that $kn^{-2}Rt_{\\rm mix}^{{\\rm IP}(2)}(\\epsilon/k)=O((\\epsilon/k)^b)$ for some $b>0$, where $R=\\sum_e r_e|e|(|e|-1)$ is $n(n-1)$ times the particle-particle interaction rate at equilibrium. This has some consequences concerning the validity in this regime of conjectures of Oliveira about comparison of the $\\epsilon$ mixing time of ${\\rm IP}(k)$ to that of $k$ independent particles, each evolving according to ${\\rm IP}(1)$, denoted ${\\rm RW}(k)$, and of Caputo about comparison of the spectral-gap of ${\\rm IP}(k)$ to that of a single particle ${\\rm IP}(1)={\\rm RW}(1)$. We also show that $t_{\\rm mix}^{\\mathrm{IP}(k)}(\\epsilon) \\asymp t_{\\rm mix}^{{\\rm RW}(1)}(\\epsilon)\\asymp t_{{\\rm mix}}^{{\\rm RW}(k)}(\\epsilon k/4)$ for all $k\\lesssim n^{1-\\Omega(1)}$ and all $\\epsilon\\le\\frac 1k\\wedge\\frac 14$ for vertex-transitive graphs of constant degree, as well as for general graphs satisfying a mild (\"transience-like\") heat-kernel condition. In the case where the particles occupying a hyperedge $e$ are permuted uniformly at random when $e$ rings we obtain results bounding the spectral gap of ${\\rm IP}(k)$ in terms of that ${\\rm RW}(1)$. The proof does not use Morris' chameleon process. It can be seen as a rigorous and direct way of arguing that when the number of particles is fairly small, the system behaves similarly to $k$ independent particles.", "revisions": [ { "version": "v1", "updated": "2021-05-27T22:47:36.000Z" } ], "analyses": { "subjects": [ "60J27", "60K35", "82C22" ], "keywords": [ "independent random walks", "interchange process", "direct comparison", "independent particles", "uniform stationary distribution" ], "note": { "typesetting": "TeX", "pages": 24, "language": "en", "license": "arXiv", "status": "editable" } } }