English

A direct comparison between the mixing time of the interchange process with "few" particles and independent random walks

Probability 2021-05-31 v1

Abstract

We consider the interchange process with kk particles (IP(k){\rm IP}(k)) on nn-vertex hypergraphs in which each hyperedge ee rings at rate rer_e. When ee rings, the particles occupying it are permuted according to a random permutation from some arbitrary law, where our only assumption is that IP(2){\rm IP}(2) has uniform stationary distribution. We show that tmixIP(k)(ϵ)=Ob(tmixIP(2)(ϵ/k))t_{\rm mix}^{{\rm IP}(k)}(\epsilon)=O_{b}(t_{\rm mix}^{{\rm IP}(2)}(\epsilon/k)), where tmixIP(i)(ϵ)t_{\rm mix}^{{\rm IP}(i)}(\epsilon) is the ϵ\epsilon total-variation mixing time of IP(i){\rm IP}(i), provided that kn2RtmixIP(2)(ϵ/k)=O((ϵ/k)b)kn^{-2}Rt_{\rm mix}^{{\rm IP}(2)}(\epsilon/k)=O((\epsilon/k)^b) for some b>0b>0, where R=eree(e1)R=\sum_e r_e|e|(|e|-1) is n(n1)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 ϵ\epsilon mixing time of IP(k){\rm IP}(k) to that of kk independent particles, each evolving according to IP(1){\rm IP}(1), denoted RW(k){\rm RW}(k), and of Caputo about comparison of the spectral-gap of IP(k){\rm IP}(k) to that of a single particle IP(1)=RW(1){\rm IP}(1)={\rm RW}(1). We also show that tmixIP(k)(ϵ)tmixRW(1)(ϵ)tmixRW(k)(ϵk/4)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 kn1Ω(1)k\lesssim n^{1-\Omega(1)} and all ϵ1k14\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 ee are permuted uniformly at random when ee rings we obtain results bounding the spectral gap of IP(k){\rm IP}(k) in terms of that RW(1){\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 kk independent particles.

Keywords

Cite

@article{arxiv.2105.13486,
  title  = {A direct comparison between the mixing time of the interchange process with "few" particles and independent random walks},
  author = {Jonathan Hermon and Richard Pymar},
  journal= {arXiv preprint arXiv:2105.13486},
  year   = {2021}
}

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24 pages