Universality classes: Difference between revisions

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==Ising==
==Ising==
The Hamiltonian of the Ising model is  
The Hamiltonian of the Ising model is  
\begin{equation}
\begin{equation}
{\cal H}=\sum{<i,j>}S_iS_j
{\cal H}=\sum{<i,j>}S_iS_j
\end{equation}
\end{equation}
where $S_i=\pm 1$ and the summation runs over the lattice sites.
where $S_i=\pm 1$ and the summation runs over the lattice sites.
The order parameter is  
The order parameter is  
\begin{equation}
\begin{equation}
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\end{equation}
\end{equation}
(In fact, the specific hear diverges logarithmically with the critical temperature)
(In fact, the specific hear diverges logarithmically with the critical temperature)
\begin{equation}
\begin{equation}
\beta=\frac{1}{8}
\beta=\frac{1}{8}

Revision as of 14:01, 20 July 2011

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name
3-state Potts
Ashkin-Teller
Chiral
Directed percolation
Ising
Local linear interface
Mean-field
Molecular beam epitaxy
Random-field

3-state Potts

Ashkin-Teller

Chiral

Directed percolation

Ising

The Hamiltonian of the Ising model is

\begin{equation} {\cal H}=\sum{<i,j>}S_iS_j \end{equation}

where $S_i=\pm 1$ and the summation runs over the lattice sites.

The order parameter is \begin{equation} m=\sum_i S_i \end{equation}

In two dimensions, Onsager obtained the exact solution in the absence of a external field, and the critical exponents are \begin{equation} \alpha=0 \end{equation} (In fact, the specific hear diverges logarithmically with the critical temperature)

\begin{equation} \beta=\frac{1}{8} \end{equation} \begin{equation} \gamma=\frac{7}{4} \end{equation} \begin{equation} \delta=15 \end{equation}

Local linear interface

Mean-field

Molecular beam epitaxy

See also

Random-field