2020
DOI: 10.1088/1361-6455/ab728f
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Photon correlation transients in a weakly blockaded Rydberg ensemble

Abstract: The combination of electromagnetically-induced transparency (EIT) and Rydberg excitations in atomic media is a compelling and versatile platform for both applications in quantum information, and fundamental studies of nonlinear quantum optics and non-local quantum dynamics. In this paper, we study the dynamics of a Rydberg-EIT system in a medium that allows for more than one Rydberg excitation in the propagation direction. We study the cross-over between coherent collective emission ('flash') of two-level atom… Show more

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Cited by 12 publications
(8 citation statements)
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“…For 𝑅 in ≈ 10 𝜇s −1 (bottom row), saturation sets in even faster, but we observe a slight oscillation in the subsequent transmission, which reflects the superatom dynamics as the probe drives Rabi oscillations between |𝐺 and |𝑊 with strong damping due to 𝛾 𝐷 [16]. To suppress superradiant reemission of absorbed photons in the forward direction after the probe pulse [44,45], 𝛾 𝐷 has to be sufficiently strong not only compared to 1/𝜏, but also the coherent dynamics [16,34]. The dephasing is dominated by atomic motion, with additional contributions from elastic scattering of the Rydberg electron by ground state atoms [46][47][48] and the AC-Stark shift induced by the trapping light.…”
Section: Resultsmentioning
confidence: 86%
“…For 𝑅 in ≈ 10 𝜇s −1 (bottom row), saturation sets in even faster, but we observe a slight oscillation in the subsequent transmission, which reflects the superatom dynamics as the probe drives Rabi oscillations between |𝐺 and |𝑊 with strong damping due to 𝛾 𝐷 [16]. To suppress superradiant reemission of absorbed photons in the forward direction after the probe pulse [44,45], 𝛾 𝐷 has to be sufficiently strong not only compared to 1/𝜏, but also the coherent dynamics [16,34]. The dephasing is dominated by atomic motion, with additional contributions from elastic scattering of the Rydberg electron by ground state atoms [46][47][48] and the AC-Stark shift induced by the trapping light.…”
Section: Resultsmentioning
confidence: 86%
“…The probe and control beams are circularly polarized and counter-propagate. Before the probe is switched off, the control is ramped down to zero [15]. The spatial extent of the stored photon is of order 10 × 1 × 1 µm 3 .…”
Section: Experimental Demonstrationmentioning
confidence: 99%
“…1c is used to initialise a qubit into state |0 using the two-photon polariton storage technique, |g → |e → |r , with Rabi frequencies Ω p and Ω c , see Fig. 1b, Methods and previous work [20,[48][49][50][51]. The qubit can be manipulated during storage using fast microwave pulses, with 80%/20% switching time of 10 ns.…”
mentioning
confidence: 99%