We use the so-called lace expansion of mathematical random walk theory to d
erive several generalizations of dynamical mean-field theory (DMFT) for str
ongly correlated electron systems (SCES). DMFT is based on a self-consisten
ce condition. by which a lattice Hamiltonian for SCES is mapped onto the co
rresponding impurity problem. It is a local theory with a density of states
of the impurity problem following from the local band Green function. So i
n the Fourier-transformed version the self-energy is independent of momenta
. From a mathematical point of view. the self-consistence condition follows
from a physical self-avoiding loop. We discuss non-local as well as local
corrections and examine them numerically for the Anderson lattice in the la
rge U limit. All calculations are performed at finite spatial dimensions. (
C) 2001 Elsevier Science B.V. All rights reserved.