2019
DOI: 10.1007/s12043-019-1739-x
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High-sensitivity measurement of Rydberg population via two-photon excitation in atomic vapour using optical heterodyne detection technique

Abstract: We demonstrate a technique based on optical heterodyne detection to measure Rydberg population in thermal atomic vapour. The technique used a probe beam far off resonant to the D2 line of rubidium along with a reference beam with frequency offset by 800 MHz in the presence of a coupling laser that couples to Rydberg state via two-photon resonance. The polarizations of the probe, reference and coupling beams are suitably chosen such that only the probe beam goes through a non-linear phase shift due to two-photo… Show more

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Cited by 3 publications
(2 citation statements)
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“…Similarly, partial suppression in the Rydberg excitation has also been reported as an evidence of Rydberg blockade using a thermal atomic beam [37]. High sensitive measurement of the Rydberg population due to two-photon excitation in thermal vapor is reported using the optical heterodyne detection technique [38,39]. A single-photon source based on strongly interacting Rydberg atoms at room temperature has also been reported [40].…”
Section: Introductionmentioning
confidence: 90%
“…Similarly, partial suppression in the Rydberg excitation has also been reported as an evidence of Rydberg blockade using a thermal atomic beam [37]. High sensitive measurement of the Rydberg population due to two-photon excitation in thermal vapor is reported using the optical heterodyne detection technique [38,39]. A single-photon source based on strongly interacting Rydberg atoms at room temperature has also been reported [40].…”
Section: Introductionmentioning
confidence: 90%
“…The possibility to all-optical detection of highlyexcited state population with high-precision has opened a new avenue to the investigation of different excitation facilitation mechanisms [1][2][3]. If detecting a single twolevel atom of weak driving ω < |δ| (ω denotes the excitation Rabi frequency and δ is the detuning to the upper level), the steady-state excitation probability of the upper-level can be well characterized by a Lorentzian function of detuning δ [4] P A = 4ω 2 1 + 8ω 2 + 4δ 2 (1) with the frequency unit γ.…”
Section: Introductionmentioning
confidence: 99%