  The interaction of a quantized field with three-level atoms in $\Lambda$
configuration inside a two mode cavity is analyzed. We calculate the stationary
quadrature noise spectrum of the field outside the cavity in the case where the
input probe field is in a squeezed state and the atoms show electromagnetically
induced transparency (EIT). If the Rabi frequencies of both dipole transitions
of the atoms are different from zero, we show that the output probe field have
four maxima of squeezing absorption. We show that in some cases two of these
frequencies can be very close to the transition frequency of the atom, in a
region where the mean value of the field entering the cavity is hardly altered.
Furthermore, part of the absorbed squeezing of the probe field is transfered to
the pump field. For some conditions this transfer of squeezing can be complete.
