Abstract
The feasibility of using Monte Carlo methods in finite fermion systems has been investigated. The basic tool is a (recently suggested) functional integral representation of Z=tr[exp(βII)] using real coherent states of Slater determinants. Conditions for using the discretized (N-point lattice) version as a starting point for Monte Carlo integrations are studied. The limit of large β is achieved only with large N. For a two-fermion system numerical calculations of the ground-state energy agree farily well with the exact value.