Martin Gärttner, Jörg Evers
Light propagation through an ensemble of ultra-cold Rydberg atoms in electromagnetically induced transparency (EIT) configuration is studied. In strongly interacting Rydberg EIT media, non-linear optical effects lead to a non-trivial dependence of the degree of probe beam attenuation on the medium density and on its initial intensity. We develop a Monte Carlo rate equation model that self-consistently includes the effect of the probe beam attenuation to investigate the steady state of the Rydberg medium driven by two laser fields. We compare or results to recent experimental data and to results of other state-of-the-art models for light propagation in Rydberg EIT-media. We find that for low probe field intensities, our results match the experimental data best if a density-dependent dephasing rate is included in the model. At higher probe intensities, our model deviates from other theoretical approaches, as it predicts a spectral asymmetry together with line broadening. These are due to off-resonant excitation channels, which however have not been observed in recent experiments. We interpret these results as signatures for atomic motion and effects beyond the frozen gas approximation. At resonant driving with low probe intensity, the motion is consistent with the required additional density-dependent dephasing. At higher probe intensities and off-resonant driving, the motion renders off-resonant excitation channels ineffective, suppressing the spectral asymmetry.
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http://arxiv.org/abs/1305.1458
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