2020
DOI: 10.1088/1361-6455/ab8717
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High nonclassical correlations of large-bandwidth photon pairs generated in warm atomic vapor

Abstract: Generation of nonclassical light suitable for interaction with atoms corresponds to a crucial goal pursued across the broad quantum optics community. We present the generation of nonclassical photon pairs using the process of spontaneous four-wave mixing in warm atomic vapor with an unprecedentedly high degree of nonclassical photon correlations. We show how the unique combination of excitation of atoms in the proximity of the vapor cell viewport, single excitation laser beam, double-Λ energy level scheme, aux… Show more

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Cited by 17 publications
(15 citation statements)
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“…1 depicts a simplified experimental scheme and main source characteristics. We have implemented several crucial improvements of our scheme [54] which contributed to the simultaneous enhancement of the overall two-photon coupling efficiency η 2ph = P C /P AS to up to 9.0 ± 0.2 % complemented by a more than a tenfold improvement of generated Stokes M S and anti-Stokes M AS photon detection rates and by a twofold increase in photon coincidence rates to C = 7.7 ± 0.1 kHz evaluated for the coincidence time window T bin = 486 ps. At the same time, sufficiently high nonclassical correlations between Stokes and anti-Stokes fields on the order of g…”
Section: Resultsmentioning
confidence: 99%
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“…1 depicts a simplified experimental scheme and main source characteristics. We have implemented several crucial improvements of our scheme [54] which contributed to the simultaneous enhancement of the overall two-photon coupling efficiency η 2ph = P C /P AS to up to 9.0 ± 0.2 % complemented by a more than a tenfold improvement of generated Stokes M S and anti-Stokes M AS photon detection rates and by a twofold increase in photon coincidence rates to C = 7.7 ± 0.1 kHz evaluated for the coincidence time window T bin = 486 ps. At the same time, sufficiently high nonclassical correlations between Stokes and anti-Stokes fields on the order of g…”
Section: Resultsmentioning
confidence: 99%
“…S,AS (0) ∼ 50, observable for low excitation powers, could be maintained. The combination of the interaction area corresponding to the spatial overlap of excitation lasers and detection mode within the atomic ensemble in the proximity of the vapor cell viewport [54], efficient auxiliary optical pumping (OP) with a help of atomic polarization preserving coating of vapor cell [47], and particular polarization, spectral, and spatial filtering (F S , F AS ), provide conditions for sufficient two-photon coupling efficiencies and, simultaneously, allow for the feasibility of generation of very high nonclassical correlations and low noise contribution in both Stokes and anti-Stokes fields.…”
Section: Resultsmentioning
confidence: 99%
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“…Two major physical mechanisms are used to produce biphotons: the spontaneous parametric down conversion (SPDC) [18][19][20][21][22][23][24][25][26][27][28][29][30] and spontaneous four-wave mixing (SFWM) [31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47] . The SPDC is employed for nonlinear crystals.…”
Section: Introductionmentioning
confidence: 99%
“…The counter-propagating scheme was commonly used in the previous hot-atom SFWM sources [41][42][43][44][45][46] .…”
Section: Introductionmentioning
confidence: 99%