The naive perturbation expansion for many-fermion systems is infrared
divergent. One can remove these divergences by introducing counterterm
s. To do this without changing the model, one has to solve an inversio
n equation. We call this procedure Fermi surface renormalization (FSR)
. Whether or not FSR is possible depends on the regularity properties
of the fermion self-energy. When the Fermi surface is nonspherical, th
is regularity problem is rather nontrivial. Using improved power count
ing at all orders in perturbation theory, we have shown sufficient dif
ferentiability to solve the FSR equation for a class of models with a
non-nested, non-spherical Fermi surface. I will first motivate the pro
blem and give a definition of FSR, and then describe the combination o
f geometric and graphical facts that lead to the improved power counti
ng bounds. These bounds also apply to the four-point function. They im
ply that only ladder diagrams can give singular contributions to the f
our-point function.