Abstract

AbstractFix constants $$\chi >0$$ χ > 0 and $$\theta \in [0,2\pi )$$ θ ∈ [ 0 , 2 π ) , and let h be an instance of the Gaussian free field on a planar domain. We study flow lines of the vector field $$e^{i(h/\chi +\theta )}$$ e i ( h / χ + θ ) starting at a fixed boundary point of the domain. Letting $$\theta $$ θ vary, one obtains a family of curves that look locally like $$\hbox {SLE}_\kappa $$ SLE κ processes with $$\kappa \in (0,4)$$ κ ∈ ( 0 , 4 ) (where $$\chi = \tfrac{2}{\sqrt{\kappa }} -\tfrac{ \sqrt{\kappa }}{2}$$ χ = 2 κ - κ 2 ), which we interpret as the rays of a random geometry with purely imaginary curvature. We extend the fundamental existence and uniqueness results about these paths to the case that the paths intersect the boundary. We also show that flow lines of different angles cross each other at most once but (in contrast to what happens when h is smooth) may bounce off of each other after crossing. Flow lines of the same angle started at different points merge into each other upon intersecting, forming a tree structure. We construct so-called counterflow lines ($$\hbox {SLE}_{16/\kappa }$$ SLE 16 / κ ) within the same geometry using ordered “light cones” of points accessible by angle-restricted trajectories and develop a robust theory of flow and counterflow line interaction. The theory leads to new results about $$\hbox {SLE}$$ SLE . For example, we prove that $$\hbox {SLE}_\kappa (\rho )$$ SLE κ ( ρ ) processes are almost surely continuous random curves, even when they intersect the boundary, and establish Duplantier duality for general $$\hbox {SLE}_{16/\kappa }(\rho )$$ SLE 16 / κ ( ρ ) processes.

Highlights

  • Background and settingLet D ⊆ C be a domain with harmonically non-trivial boundary and D

  • We will focus on the case that z is point on the boundary of the domain where h is defined and establish a more general set of results. (Flow lines beginning at interior points will be addressed in a subsequent paper.) In particular, we show that the paths exist and are determined by h even in settings where they hit and bounce off of the boundary, and we will describe the interaction of multiple flow lines that hit the boundary and cross or bounce off each other

  • We show that the flow lines started at the same point, corresponding to different θ values, may bounce off one another but almost surely do not cross one another, that flow lines started at distinct points with the same angle can “merge” with each other, and that flow lines started at distinct points with distinct angles almost surely cross at most once

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Summary

Overview

A complete description of all the rays and the way they interact with each other This will have a range of applications in SLE theory: in particular, this paper will establish continuity results for SLEκ (ρ) curves and generalizations of so-called Duplantier. We will use the flow-line geometry to construct so-called counterflow lines, which are forms of SLE16/κ (κ ∈ (0, 4)) that arise as the “light cones” of points accessible by certain angle-restricted SLEκ trajectories To use another metaphor, we say that a point y is “downstream” from another point x if it can be reached from x by an angle-varying flow line whose angles lie in some allowed range; the counterflow line is a curve that traces through all the points that are downstream from a given boundary point x, but it traces them in an “upstream” (or “counterflow”) direction.

Background and setting
Coupling of paths with the GFF
Main results
Outline
Overview of SLEκ
Construction and basic properties
Local sets
Dubédat’s argument
The non-boundary-intersecting regime
Monotonicity of flow and counterflow lines
Light cone construction of counterflow lines
Interacting flow lines
The conditional mean
Existence and continuity of Loewner driving functions
Proofs of main theorems
Two boundary force points
Continuity for many boundary force points
Counterflow lines
Many boundary force points
Light cones with general boundary data
The fan is not space filling
Full Text
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