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Spherical model : ウィキペディア英語版
Spherical model
The spherical model in statistical mechanics is a model of ferromagnetism similar to the Ising model, which was solved in 1952 by T. H. Berlin and M. Kac. It has the remarkable property that when applied to systems of dimension ''d'' greater than four, the critical exponents that govern the behaviour of the system near the critical point are independent of ''d'' and the geometry of the system. It is one of the few models of ferromagnetism that can be solved exactly in the presence of an external field.
== Formulation ==
The model describes a set of particles on a lattice \mathbb containing ''N'' sites. For each site ''j'' of \mathbb , a spin \sigma_j which interacts only with its nearest neighbours and an external field ''H''. It differs from the Ising model in that the \sigma_j are no longer restricted to \sigma_j \in \ , but can take all real values, subject to the constraint that
: \sum_^N \sigma_j^2 = N
which in a homogeneous system ensures that the average of the square of any spin is one, as in the usual Ising model.
The partition function generalizes from that of the Ising model to
: Z_N = \int_^ \ldots \int_^ d\sigma_1 \ldots d\sigma_N exp \left(K \sum_ \sigma_j \sigma_l + h \sum_j \sigma_j \right ) \delta \left(- \sum_j \sigma_j^2 \right )
where \delta is the Dirac delta function, \langle jl \rangle are the edges of the lattice, and K=J/kT and h= H/kT , where ''T'' is the temperature of the system, ''k'' is Boltzmann's constant and ''J'' the coupling constant of the nearest-neighbour interactions.
Berlin and Kac saw this as an approximation to the usual Ising model, arguing that the \sigma-summation in the Ising model can be viewed as a sum over all corners of an ''N''-dimensional hypercube in \sigma-space. The becomes an integration over the surface of a hypersphere passing through all such corners.
It was rigorously proved by Kac and C. J. Thompson that the spherical model is a limiting case of the N-vector model.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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