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N-vector model : ウィキペディア英語版
N-vector model

The ''n''-vector model or O(''n'') model has been introduced by H. Eugene Stanley 〔H. E. Stanley, "Dependence of Critical Properties upon Dimensionality of Spins," Phys. Rev. Lett. 20, 589-592 (1968).〕 is one of the many highly simplified models in the branch of physics known as statistical mechanics. In the ''n''-vector model, ''n''-component, unit length, classical spins \mathbf_i are placed on the vertices of a lattice. The Hamiltonian of the n-vector model is given by:
:H = -J_\mathbf_i \cdot \mathbf_j
where the sum runs over all pairs of neighboring spins and \cdot denotes the standard Euclidean inner product. Special cases of the n-vector model are:
:n=0 || The Self-Avoiding Walks (SAW)
:n=1 || The Ising model
:n=2 || The XY model
:n=3 || The Heisenberg model
: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.
==References==

() H. E. Stanley, "Dependence of Critical Properties upon Dimensionality of Spins," (Phys. Rev. Lett. 20, 589-592 (1968) ).
This paper is the basis of many articles in field theory and is reproduced as Chapter 1 of Brèzin/Wadia () ''(The Large-N expansion in Quantum Field Theory and Statistical Physics )'' (World Scientific, Singapore, 1993). Also described extensively in the text Pathria RK ''(Statistical Mechanics: Second Edition )'' (Pergamon Press, Oxford, 1996).
* P.G. de Gennes, Phys. Lett. A, 38, 339 (1972) noticed that the n=0 case corresponds to the SAW.
* George Gaspari, Joseph Rudnick, Phys. Rev. B, 33, 3295 (1986) discuss the model in the limit of n going to 0.

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