arXiv · quant-ph/9812084
Optimal squeezing, pure states, and amplification of squeezing in resonance fluorescence
Abstract
It is shown that 100% squeezed output can be produced in the resonance fluorescence from a coherently driven two-level atom interacting with a squeezed vacuum. This is only possible for $N=1/8$ squeezed input, and is associated with a pure atomic state, i.e., a completely polarized state. The quadrature for which optimal squeezing occurs depends on the squeezing phase $Φ,$ the Rabi frequency $Ω,$ and the atomic detuning $Δ$. Pure states are described for arbitrary $Φ,$ not just $Φ=0$ or $π$ as in previous work. For small values of $N,$ there may be a greater degree of squeezing in the output field than the input - i.e., we have squeezing amplification.
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Peng Zhou, S. Swain. 1998-12-30. Optimal squeezing, pure states, and amplification of squeezing in resonance fluorescence. https://doi.org/10.1103/physreva.59.3745
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