Physics:Conformal loop ensemble

In critical percolation on the honeycomb lattice, each hexagon face is colored red or black independently with equal probability. Every interface separating a black cluster from a red cluster is shown in green. This random collection of interfaces converges in law to CLE₆ as the lattice spacing goes to zero.

To define a random interface converging to SLE, we fix the colors of the hexagons along the boundary of the domain. This procedure defines a single interface separating red hexagons from black hexagons. This path converges in law to SLE₆ as the lattice spacing goes to zero.

A conformal loop ensemble (CLE_κ) is a random collection of non-crossing loops in a simply connected, open subset of the plane. These random collections of loops are indexed by a parameter κ, which may be any real number between 8/3 and 8. CLE_κ is a loop version of the Schramm–Loewner evolution: SLE_κ is designed to model a single discrete random interface, while CLE_κ models a full collection of interfaces.

In many instances for which there is a conjectured or proved relationship between a discrete model and SLE_κ, there is also a conjectured or proved relationship with CLE_κ. For example:

• CLE₃ is the limit of interfaces for the critical Ising model.
• CLE₄ may be viewed as the 0-set of the Gaussian free field.
• CLE_16/3 is a scaling limit of cluster interfaces in critical FK Ising percolation.
• CLE₆ is a scaling limit of critical percolation on the triangular lattice.

Constructions

For 8/3 < κ < 8, CLE_κ may be constructed using a branching variation of an SLE_κ process. When 8/3 < κ ≤ 4, CLE_κ may be alternatively constructed as the collection of outer boundaries of Brownian loop soup clusters.

Properties

CLE_κ is conformally invariant, which means that if [math]\displaystyle{ \varphi:D\to D' }[/math] is a conformal map, then the law of a CLE in D' is the same as the law of the image of all the CLE loops in D under the map [math]\displaystyle{ \varphi }[/math].

Since CLE_κ may be defined using an SLE_κ process, CLE loops inherit many path properties from SLE. For example, each CLE_κ loop is a fractal with almost-sure Hausdorff dimension 1 + κ/8. Each loop is almost surely simple (no self intersections) when 8/3 < κ ≤ 4 and almost surely self-touching when 4 < κ < 8.

The set of all points not surrounded by any loop, which is called the gasket, has Hausdorff dimension 1 + 2/κ + 3κ/32 almost surely (random soups, carpets and fractal dimensions by Nacu and Werner. Since this dimension is strictly greater than 1+κ/8, there are almost surely points not contained in or surrounded by any loop. However, since the gasket dimension is strictly less than 2, almost all points (with respect to area measure) are contained in the interior of a loop.

CLE is sometimes defined to include only the outermost loops, so that the collection of loops is non-nested (no loop is contained in another). Such a CLE is called a simple CLE to distinguish it from a full or nested CLE. The law of a full CLE can be recovered from the law of a simple CLE as follows. Sample a collection of simple CLE loops, and inside each loop sample another collection of simple CLE loops. Infinitely many iterations of this procedure gives a full CLE.

References

• Sheffield, Scott (2009), "Exploration trees and conformal loop ensembles", Duke Math J 147 (1): 79–129, doi:10.1215/00127094-2009-007, http://projecteuclid.org/DPubS?service=UI&version=1.0&verb=Display&handle=euclid.dmj/1235657189 
• Miller, Jason; Sun, Nike; Wilson, David (2012). "Hausdorff dimension of the CLE gasket". The Annals of Probability 42 (4): 1644–1665. doi:10.1214/12-AOP820. 
• Sheffield, Scott; Werner, Wendelin (2010). "Conformal Loop Ensembles: The Markovian characterization and the loop-soup construction". arXiv:1006.2374 [math.PR].