Physical review. B, Solid state · 1970 · 184 citations · 23 references
Natural SciencesPhysicsComputational PhysicsCondensed Matter PhysicsQuantum MechanicsApproximation MethodsComputational Quantum MechanicsElectron CorrelationQuantum SimulationStatistical MechanicsStrongly Correlated Electron SystemsAnalytic ApproximationsAutocorrelation FunctionCorrelation FunctionsExchange Interactions In Heisenberg ModelsHeisenberg MagnetismHeisenberg ModelSimple Cubic LatticeSpin Systems
The study discusses the physical motivation of the approximations used and the special mathematical aspects of the problem. The paper proposes a self‑consistent method for calculating correlation functions in the high‑temperature Heisenberg model. Based on a straightforward physical picture, the technique derives a simple analytic approximation for the short‑time autocorrelation function, reproduces the R\'esibois–DeLeener equation, and formulates integrodifferential equations for general correlation functions. Numerical solutions of these equations for a simple cubic lattice with nearest‑neighbor interactions agree excellently with computer‑simulation results.
A method for the self-consistent calculation of correlation functions is described and applied to the Heisenberg model at high temperatures. The technique is based on a straightforward physical picture. It is used (i) to derive a simple analytic approximation for the autocorrelation function valid at times $t\ensuremath{\lesssim}\frac{2JS}{\ensuremath{\hbar}}$; (ii) to derive an equation given by R\'esibois and DeLeener which is shown to be valid at short times also; (iii) to derive a set of integrodifferential equations for the general correlation functions $〈{\mathrm{S}}_{\ensuremath{-}\mathrm{q}}\ifmmode\cdot\else\textperiodcentered\fi{}\{\mathrm{S}}_{\mathrm{q}}(t)〉$. The latter equations are solved numerically for the case of a simple cubic lattice with nearest-neighbor interactions, and are shown to give results in excellent agreement with computer simulation calculations for the same model. A discussion is given of the physical motivation of the approximations employed and the special mathematical aspects of the problem.
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