Abstract
The possible existence of so-called “squeezed” states in two-atom resonance fluorescence is discussed in Lehmberg's master equation approach. It is shown that squeezing strongly depends on interatomic separations r 12. For large r 12 one of the quadrature components is squeezed, and as r 12 decreases its squeezing decreases in order to appear in the other quadrature component for certain value of r 12. For very small r 12 fluctuations in both components tend to zero.
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