Cooperative atom-light interaction in a blockaded Rydberg ensemble
J. D. Pritchard, D. Maxwell, A. Gauguet, K. J. Weatherill, M. P. A., Jones, C. S. Adams

TL;DR
This paper demonstrates how strong dipole-dipole interactions in a Rydberg ensemble induce cooperative optical non-linearity, requiring an N-atom model for accurate description, with experimental validation and limits on dephasing rates.
Contribution
It introduces an N-atom cooperative model for Rydberg blockade effects and validates it experimentally, surpassing mean-field approximations.
Findings
Good quantitative agreement with three atoms per blockade
Upper limit on dephasing rate of 110 kHz
Observation of cooperative optical non-linearity
Abstract
By coupling a probe transition to a Rydberg state using electro-magnetically induced transparency (EIT) we map the strong dipole-dipole interactions onto an optical field. We characterize the resulting cooperative optical non-linearity as a function of probe strength and density. We show that the effect of dipole blockade cannot be described using a mean-field but requires an -atom cooperative model. Good quantitative agreement is obtained for three atoms per blockade with the Rydberg state. We place an upper-limit on the dephasing rate of the blockade spheres of kHz.
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