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Diagrammatic representation of the two‐spin correlation function for the generalized heisenberg model
Author(s) -
Stanley H. Eugene,
Lee M. Howard
Publication year - 2009
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.560050744
Subject(s) - diagrammatic reasoning , heisenberg model , hamiltonian (control theory) , physics , spins , ising model , statistical physics , mathematical physics , correlation function (quantum field theory) , series expansion , spin (aerodynamics) , quantum mechanics , thermodynamic limit , mathematics , condensed matter physics , thermodynamics , ferromagnetism , mathematical optimization , philosophy , linguistics , dielectric
Abstract We consider a “generalized Heisenberg model”, with a Hamiltonian given by ℋ (D) = – J Σ ij S ( D ) j , where the quantities S i are isotropically‐interacting D‐dimensional classical spins and the summation is restricted to nearest‐neighbor pairs of sites . Thus when D = 1, 2, and 3, this model reduces to the S = 1/2 Ising, plane rotator, and classical Heisenberg models which are useful for describing phase transitions in, respectively, liquid‐gas systems, Bose fluids, and magnetic materials. Unfortunately this Hamiltonian is exactly soluble only in the limit D → ∞, in which case the solution corresponds to the spherical model of Berlin and Kac. For finite D , we must consider approximation procedures in order to obtain any useful information. In this paper we develop a diagrammatic representation, valid for arbitrary D , for successive terms in the high‐temperature expansions of the free energy and the spin‐spin correlation function—from which we can obtain series expansions for all the thermodynamic properties of the system.