By utilizing our previous operator solution [17], we have investigated
the squeezing in the radiation field of the Tavis-Cummings model (col
lective N much greater than 1 two-level atoms interacting with a reson
ant single cavity quantized mode). With field and atoms initially in c
oherent field state strong or weak and atomic coherent state (of few e
xcited atoms), periodic time-dependent squeezing in the field and the
macroscopic polarization is expressed in terms of Jacobian elliptic fu
nctions of the first kind. The statistical investigations are carried
out for the quasiprobability distribution functions (Wigner function a
nd Q function). The distribution function of the field quadrature has
a variance less (greater) than that for a coherent state if this quadr
ature is squeezed (unsqueezed).