This shows you the differences between two versions of the page.
Both sides previous revision Previous revision Next revision | Previous revision | ||
percolation [2021/04/11 20:35] Scott Lawrence [Computational methods] |
percolation [2021/05/05 19:06] (current) Scott Lawrence [Bethe lattice] |
||
---|---|---|---|
Line 6: | Line 6: | ||
Percolation is a [[tag: | Percolation is a [[tag: | ||
- | This page focuses on " | + | This page focuses on " |
- | ===== Lattice | + | ===== Lattice |
- | Percolation | + | Percolation |
- | Because percolation is not a unitary CFT, there is no Hamiltonian lattice theory that flows to percolation in the IR. | + | Because percolation is not a unitary CFT, there is no Hamiltonian lattice theory that flows to percolation in the IR. All lattices in this section are spacetime lattices. |
+ | |||
+ | Usually percolation is defined on a square lattice. Many other possibilities exist, with the same critical behavior. | ||
+ | |||
+ | ==== Site percolation ==== | ||
+ | |||
+ | ==== Bond percolation ==== | ||
Line 18: | Line 24: | ||
==== Lattice ==== | ==== Lattice ==== | ||
+ | |||
+ | The most straightforward computational method is to instantiate a random lattice of some finite size and compute cluster sizes. This gives a single sample, and the procedure can be repeated as much as desired to improve the statistics. Note that although this is a Monte Carlo method, there is no (non-trivial) Markov chain. In other words, there is no " | ||
==== Epsilon expansion ==== | ==== Epsilon expansion ==== | ||
Line 27: | Line 35: | ||
===== Two dimensions ===== | ===== Two dimensions ===== | ||
+ | For bond percolation on a 2-dimensional square lattice, $p_c = 0.5$ is known exactly. | ||
===== Six or more dimensions ===== | ===== Six or more dimensions ===== | ||
In six or more dimensions critical percolation is described by [[mean-field theory|mean-field theory]]. | In six or more dimensions critical percolation is described by [[mean-field theory|mean-field theory]]. | ||
+ | |||
+ | ===== Bethe lattice ===== | ||
+ | |||
+ | The Bethe lattice can be thought of as the $d\rightarrow\infty$ lattice. It is the infinite tree in which each vertex has the same number ($z$ --- called the coordination number) of neighbors. Note that $z=1$ is invalid, and $z=2$ is just a one-dimensional lattice. | ||
+ | |||
+ | As with many statistical models, percolation can be exactly solved on a Bethe lattice: see for instance [[https:// | ||
===== Related theories ===== | ===== Related theories ===== | ||
* [[Directed percolation]] | * [[Directed percolation]] | ||
+ | |||
+ | ===== External links ===== | ||
+ | * [[https:// |