In statistical mechanics, the n-vector model or O(n) model is a simple system of interacting spins on a crystalline lattice. It was developed by H. Eugene Stanley as a generalization of the Ising model, XY model and Heisenberg model.
Definition In the n-vector model, n-component unit-length classical spins s i {\displaystyle \mathbf {s} _{i}} are placed on the vertices of a d-dimensional lattice. The Hamiltonian of the n-vector model is given by:
H = K ∑ ⟨ i , j ⟩ s i ⋅ s j {\displaystyle H=K{\sum }_{\langle i,j\rangle }\mathbf {s} _{i}\cdot \mathbf {s} _{j}}
where the sum runs over all pairs of neighboring spins ⟨ i , j ⟩ {\displaystyle \langle i,j\rangle } and ⋅ {\displaystyle \cdot } denotes the standard Euclidean inner product. Special cases of the n-vector model are:
n = 0 {\displaystyle n=0} : The self-avoiding walk
n = 1 {\displaystyle n=1} : The Ising model
n = 2 {\displaystyle n=2} : The XY model
n = 3 {\displaystyle n=3} : The Heisenberg model
n = 4 {\displaystyle n=4} : Toy model for the Higgs sector of the Standard Model The general mathematical formalism used to describe and solve the n-vector model and certain generalizations are developed in the article on the Potts model. The Hamiltonian of the n-vector model is also the same as the potential term of the quantum rotor model.
Reformulation as a loop model In a small coupling expansion, the weight of a configuration may be rewritten as
e H ∼ K → 0 ∏ ⟨ i , j ⟩ ( 1 + K s i ⋅ s j ) {\displaystyle e^{H}{\underset {K\to 0}{\sim }}\prod _{\langle i,j\rangle }\left(1+K\mathbf {s} _{i}\cdot \mathbf {s} _{j}\right)}
Integrating over the vector s i {\displaystyle \mathbf {s} _{i}} gives rise to expressions such as
∫ d s i ∏ j = 1 4 ( s i ⋅ s j ) = ( s 1 ⋅ s 2 ) ( s 3 ⋅ s 4 ) + ( s 1 ⋅ s 4 ) ( s 2 ⋅ s 3 ) + ( s 1 ⋅ s 3 ) ( s 2 ⋅ s 4 ) {\displaystyle \int d\mathbf {s} _{i}\ \prod _{j=1}^{4}\left(\mathbf {s} _{i}\cdot \mathbf {s} _{j}\right)=\left(\mathbf {s} _{1}\cdot \mathbf {s} _{2}\right)\left(\mathbf {s} _{3}\cdot \mathbf {s} _{4}\right)+\left(\mathbf {s} _{1}\cdot \mathbf {s} _{4}\right)\left(\mathbf {s} _{2}\cdot \mathbf {s} _{3}\right)+\left(\mathbf {s} _{1}\cdot \mathbf {s} _{3}\right)\left(\mathbf {s} _{2}\cdot \mathbf {s} _{4}\right)}
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