Classical Heisenberg model

The classical Heisenberg model can be formulated as follows: take a d-dimensional lattice, and place a set of spins of unit length,

${\displaystyle {\vec {s}}_{i}\in \mathbb {R} ^{3},|{\vec {s}}_{i}|=1\quad (1)}$ ,

on each lattice node.

The model is defined through the following Hamiltonian:

${\displaystyle {\mathcal {H}}=-\sum _{i,j}{\mathcal {J}}_{ij}{\vec {s}}_{i}\cdot {\vec {s}}_{j}\quad (2)}$ 

where

${\displaystyle {\mathcal {J}}_{ij}={\begin{cases}J&{\mbox{if }}i,j{\mbox{ are neighbors}}\\0&{\mbox{else.}}\end{cases}}}$ 

is a coupling between spins.

• The general mathematical formalism used to describe and solve the Heisenberg model and certain generalizations is developed in the article on the Potts model.
• In the continuum limit the Heisenberg model (2) gives the following equation of motion

${\displaystyle {\vec {S}}_{t}={\vec {S}}\wedge {\vec {S}}_{xx}.}$ 

This equation is called the continuous classical Heisenberg ferromagnet equation or, more shortly, the Heisenberg model and is integrable in the sense of soliton theory. It admits several integrable and nonintegrable generalizations like the Landau-Lifshitz equation, the Ishimori equation, and so on.

• In the case of a long-range interaction, ${\displaystyle J_{x,y}\sim |x-y|^{-\alpha }}$ , the thermodynamic limit is well defined if ${\displaystyle \alpha >1}$ ; the magnetization remains zero if ${\displaystyle \alpha \geq 2}$ ; but the magnetization is positive, at a low enough temperature, if ${\displaystyle 1<\alpha <2}$  (infrared bounds).
• As in any 'nearest-neighbor' n-vector model with free boundary conditions, if the external field is zero, there exists a simple exact solution.

• In the case of a long-range interaction, ${\displaystyle J_{x,y}\sim |x-y|^{-\alpha }}$ , the thermodynamic limit is well defined if ${\displaystyle \alpha >2}$ ; the magnetization remains zero if ${\displaystyle \alpha \geq 4}$ ; but the magnetization is positive at a low enough temperature if ${\displaystyle 2<\alpha <4}$  (infrared bounds).
• Polyakov has conjectured that, as opposed to the classical XY model, there is no dipole phase for any ${\displaystyle T>0}$ ; namely, at non-zero temperatures the correlations cluster exponentially fast.^[1]

Independently of the range of the interaction, at a low enough temperature the magnetization is positive.

Conjecturally, in each of the low temperature extremal states the truncated correlations decay algebraically.

• Heisenberg model (quantum)
• Ising model
• Classical XY model
• Magnetism
• Ferromagnetism
• Landau–Lifshitz equation
• Ishimori equation

• Absence of Ferromagnetism or Antiferromagnetism in One- or Two-Dimensional Isotropic Heisenberg Models Archived 2020-06-08 at the Wayback Machine
• The Heisenberg Model - a Bibliography
• Monte-Carlo simulation of the Heisenberg, XY and Ising models with 3D graphics (requires WebGL compatible browser)