Abstract
We report the extreme sensitivity of the resonance fluorescence spectra of a two level atom interacting with a detuned classical field to the presence of a very weak squeezed vacuum (which includes a black body field as a special case). Large asymmetries are induced by these very weak perturbations. For an appropriate choice of squeezing phase, a pronounced minimum is found in one of the peaks as the intensity of the squeezed field increases. The connection with population trapping in squeezed fields is established, and a physical interpretation provided.
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