XY model

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The XY model is a generalization of the Ising model of statistical mechanics , with which magnetism and other physical phenomena can be described. The XY model is the special case of the more general n-vector model (the other special cases of this model are the Ising model with and the Heisenberg model with ).

It was already considered in 1950 by Yōichirō Nambu in connection with the two-dimensional Ising model. In 1961 Elliott Lieb , Daniel Mattis and T. Schultz gave an exact solution to the XY model of spin 1/2 particles in one dimension. They used the Jordan-Wigner transformation .

The XY model consists of spins that are represented by unit vectors. They are arranged on the points of a grid of any dimension, but can only be aligned in one plane; hence the designation  XY and the special case .

The Hamiltonian for the XY model is given by:

in which

The order parameter of the XY model is the magnetization and thus a vector in the XY plane. A phase transition can occur for two- and higher-dimensional lattices. In two dimensions, this is not a normal continuous phase transition or first-order phase transition , but the Kosterlitz-Thouless transition that cannot be described by any conventional local order parameter . This is the main reason why the XY model is interesting for theoretical physics .

See also

Web links

Individual evidence

  1. ^ Daniel Mattis, The many-body problem, World Scientific 1993, p. 683
  2. ^ Lieb, Schultz, Mattis, Annals of Physics, Volume 16, 1961, p. 407