The fluorescence field from one of the two allowed transitions in a th
ree-level atom can sense squeezed fluctuations of a vacuum field coupl
ed to the other transition. We examine the fluorescence spectra of str
ongly driven three-level atoms in Lambda, V, and cascade configuration
s in which one of the two one-photon transitions is coupled to a finit
e-bandwidth squeezed vacuum field, when the bandwidth is much smaller
than the difference in the atomic transition frequencies, though much
larger than atomic decay rates and Rabi frequencies of the driving fie
lds. The driving fields are on one-photon resonance, and the squeezed
vacuum field is generated by a degenerate parameter oscillator. Detail
s are only given for the Lambda configuration. The extension to the V
and cascade configurations is straightforward. We find that in all con
figurations the fluorescence spectra of the transition not coupled to
the squeezed vacuum field are composed of five lines, one central and
two pairs of sidebands, with intensities and widths strongly influence
d by the squeezed vacuum field. However, only the central component an
d the outer sidebands exhibit a dependence on the squeezing phase. We
also examine the fluorescence spectrum for the cascade configuration w
ith a squeezed vacuum field on resonance with the two-photon transitio
n between the ground and the most excited states and now generated by
a nondegenerate parametric oscillator. In this case, where the squeeze
d vacuum field can be made coupled to both transitions, all spectral l
ines depend on the squeezing phase. The spectral features are explaine
d in terms of the dressed-atom model of the system. We show that the c
oherent mixing of the atomic states by the strong driving fields modif
ies transition rates between the dressed states, which results in the
selective phase dependence of the spectral features.