Absence of T2lnT term in spin susceptibility of nearly ferromagnetic Fermi systems

Abstract
Several recent treatments of the temperature dependence of the spin susceptibility chi (T) of nearly ferromagnetic Fermi systems suggest that there is a T2lnT term in chi (T). It is shown, in a simple microscopic model, that such a term arises from retaining only one class of contributions to xi (T), and is exactly cancelled by another class, present in a spin-conserving calculation.