Like the even chirality correlation functions of, say, the two vector curre
nts, one can also consider odd chirality correlation functions to write the
rmal QCD sum rules. They contain fewer non-perturbative corrections, at lea
st to the leading order. Here we write such a sum rule for the correlation
function of vector and tensor "currents." The odd and even chirality sum ru
les are taken together to evaluate the effective parameters of the rho meso
n to second order in temperature.