A model of itinerant lattice electrons interacting with classical nucl
ei is studied. The electrons can interact between themselves via a Hub
bard on-site term. It is shown that, in the ground state of the half-f
illed band, the nuclei form a periodic crystal. More precisely for a c
ubic lattice they form a chessboard state under some appropriate condi
tion on the hopping matrix. This generalizes known results previously
obtained for the Falicov-Kimball model. The case where fermions are re
placed by hard-core bosons in this later model is also discussed. More
generally models of fermions interacting with classical scalar or vec
tor fields are briefly considered. The mathematical technique used is
''reflection positivity'' adapted to the case of Fermi statistics.