Abstract
The energy-energy correlation function C(k) is calculated to O(4d) in an exponentiated crossover form for n-component spin systems. The result is exact for the Gaussian (n=2) and spherical (n=) models which form symmetrically placed anchors for the calculation for general n. The error is proprotional to the small critical-point exponent η and is likely to be small in three dimensions. A dispersion-theory representation of C(k) is used to correct the large-k behavior to the expected Fisher-Langer asymptotic form. The result gives a direct method for the measurement of the correlation length in liquid helium.