Abstract
High-temperature series are presented for the spin-spin correlation function of the spin-infinity nearest-neighbor Heisenberg ferromagnet on the fcc lattice. Our zero-field series are to tenth order in the interaction, while our finite field series are to eighth order in the interaction. Previous analysis of these series indicated γ=1.405±0.020 and ν=0.717±0.007. These series are used to determine the true correlation length. Further examination of these series indicates that, where the inverse correlation length κ is not much smaller than the momentum transfer κ (explicitly κ2k2>0.08, the correlations in momentum space are well represented by the Ornstein-Zernike form μη(k2+μ2), where η has been found to be 0.040 ± 0.008, not zero as in mean-field theories.