Ising model

The Ising model (also known as the Lenz-Ising model) is commonly defined over an ordered lattice. Each site of the lattice can adopt two states, $S\in \{-1,+1\}$. Note that sometimes these states are referred to as spins and the values are referred to as down and up respectively. The energy of the system is the sum of pair interactions between nearest neighbors.

${\frac {U}{k_{B}T}}=-K\sum _{\langle ij\rangle }S_{i}S_{j}$

where $k_{B}$ is the Boltzmann constant, $T$ is the temperature, $\langle ij\rangle$ indicates that the sum is performed over nearest neighbors, and $S_{i}$ indicates the state of the i-th site, and $K$ is the coupling constant.

For a detailed and very readable history of the Lenz-Ising model see the following references: .

1-dimensional Ising model

• 1-dimensional Ising model (exact solution)

2-dimensional Ising model

Solved by Lars Onsager in 1944 . Rudolf Peierls had previously shown (1935) that, contrary to the one-dimensional case, the two-dimensional model must have a phase transition.

3-dimensional Ising model

Sorin Istrail has shown that the solution of Ising's model cannot be extended into three dimensions for any lattice

ANNNI model

The axial next-nearest neighbour Ising (ANNNI) model is used to study alloys, adsorbates, ferroelectrics, magnetic systems, and polytypes.

See also

• Critical exponents
• Potts model