English

Connection probabilities for conformal loop ensembles

Probability 2018-11-21 v5 Mathematical Physics math.MP

Abstract

The goal of the present paper is to explain, based on properties of the conformal loop ensembles CLEκ_\kappa (both with simple and non-simple loops, i.e., for the whole range κ(8/3,8)\kappa \in (8/3, 8)) how to derive the connection probabilities in conformal rectangles for a conditioned version of CLEκ_\kappa which can be interpreted as a CLEκ_{\kappa} with wired/free/wired/free boundary conditions on four boundary arcs (the wired parts being viewed as portions of to-be-completed loops). In particular, in the case of a conformal square, we prove that the probability that the two wired sides hook up so that they create one single loop is equal to 1/(12cos(4π/κ))1/(1 - 2 \cos (4 \pi / \kappa )). Comparing this with the corresponding connection probabilities for discrete O(N) models for instance indicates that if a dilute O(N) model (respectively a critical FK(q)-percolation model on the square lattice) has a non-trivial conformally invariant scaling limit, then necessarily this scaling limit is CLEκ_\kappa where κ\kappa is the value in (8/3,4](8/3, 4] such that 2cos(4π/κ)-2 \cos (4 \pi / \kappa ) is equal to NN (resp. the value in [4,8)[4,8) such that 2cos(4π/κ)-2 \cos (4\pi / \kappa) is equal to q\sqrt {q}). Our arguments and computations build on the one hand on Dub\'edat's SLE commutation relations (as developed and used by Dub\'edat, Zhan or Bauer-Bernard-Kyt\"ol\"a) and on the other hand, on the construction and properties of the conformal loop ensembles and their relation to Brownian loop-soups, restriction measures, and the Gaussian free field, as recently derived in works with Sheffield and with Qian.

Keywords

Cite

@article{arxiv.1702.02919,
  title  = {Connection probabilities for conformal loop ensembles},
  author = {Jason Miller and Wendelin Werner},
  journal= {arXiv preprint arXiv:1702.02919},
  year   = {2018}
}

Comments

37 pages, to appear in Comm. in Math. Phys

R2 v1 2026-06-22T18:14:08.698Z