The state evolution in the two-photon atom-field interaction with larg
e initial fields is studied. It is shown that under certain conditions
, for the initial coherent field, at one-quarter and three-quarters of
the revival time the atom is converged into unique pure states, and a
t the revival time both the atom and field return to their initial sta
tes. The possibility for the field macroscopic superposition states to
be generated is discussed. The effects of tl;e cavity damping, photon
statistics, and dynamic Stark shifts are investigated. Our results gi
ve some further insight into the validity of the effective two-photon
Hamiltonian which neglects the Stark shifts.