0Introduction

III Schramm--Loewner Evolutions



0 Introduction
Schramm–Loewner evolution is a random curve in a complex domain
D
(which
we will often take to be
H
for convenience), parametrized by a positive real
number
κ
. This was introduced by Schramm in 1999 to describe various scaling
limits that arise in probability theory and statistical physics.
Recall that if we take a random walk on the integer lattice
Z
d
, and take the
scaling limit as the grid size tends to 0, we converge towards a Brownian motion.
There are other discrete models that admit a scaling limit, and the limit is often
something that is not Brownian motion.
Schramm showed that if the scaling limit satisfies certain conformal invariance
properties, which many models do, then it must be
SLE
κ
for some
κ
. If we can
identify exactly which
κ
it belongs to, then this will completely determine what
the scaling limit is, and often conveys a lot of extra information such as the
critical exponents. This has been done for several discrete models:
The scaling limit of loop-erased random walk is SLE
2
The scaling limit of hexagonal percolation is SLE
6
(see chapter 5)
It is conjectured that the scaling limit of self-avoiding random walk is
SLE
8/3
(see chapter 6)
The “level sets” of a Gaussian free field are SLE
4
’s (see chapter7).
In this course, we will prove some basic properties of
SLE
κ
, and then establish
the last three results/conjectures.