The nonrelativistic many-electron system in the forward, exchange and
BCS approximation is considered. In this approximation, the model is e
xplicitly solvable for arbitrary space dimension d. The partition func
tion and the correlation functions are given by finite-dimensional int
egral representations. Renormalization effects as well as symmetry bre
aking can be seen explicitly. It is shown that the usual mean field ap
proach, based on approximating the Hamiltonian by a quadratic expressi
on, may be misleading if the electron-electron interaction contains hi
gher angular momentum terms and the space dimension is d = 3. The pert
urbation theory of the solvable model is discussed. There are cases wh
ere the logarithm of the partition function has positive radius of con
vergence but the sum of all connected diagrams has radius of convergen
ce zero implying that the linked cluster theorem is not applicable in
these cases.