2016
DOI: 10.1364/oe.24.003365
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Correlated photon pair generation in AlGaAs nanowaveguides via spontaneous four-wave mixing

Abstract: Abstract:We demonstrate a source of correlated photon pairs which will have applications in future integrated quantum photonic circuits. The source utilizes spontaneous four-wave mixing (SFWM) in a dispersion-engineered nanowaveguide made of AlGaAs, which has merits of negligible two-photon absorption and low spontaneous Raman scattering (SpRS). We observe a coincidence-to-accidental (CAR) ratio up to 177, mainly limited by propagation losses. Experimental results agree well with theoretical predictions of the… Show more

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Cited by 36 publications
(28 citation statements)
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“…The ZDW is located at ~1550 nm with the width of 700 nm (see Fig. 1c, and we have shown that this waveguide delivers efficient and broadband classical four-wave mixing (FWM) 24 . On the other hand, the TM mode is only slightly affected by the waveguide widths since the major electric field aligns vertically and experience less index contrast from the core-cladding interface.…”
Section: Resultsmentioning
confidence: 94%
See 1 more Smart Citation
“…The ZDW is located at ~1550 nm with the width of 700 nm (see Fig. 1c, and we have shown that this waveguide delivers efficient and broadband classical four-wave mixing (FWM) 24 . On the other hand, the TM mode is only slightly affected by the waveguide widths since the major electric field aligns vertically and experience less index contrast from the core-cladding interface.…”
Section: Resultsmentioning
confidence: 94%
“…We can estimate the bandwidth of SFWM using a classical FWM measurement 26 . Previously we reported co-polarized, continuous-wave FWM efficiencies measured from the 700-nm-wide waveguide 24 . The TE mode exhibited a bandwidth of at least 80 nm while the TM mode operated with a bandwidth of 60 nm.…”
Section: Resultsmentioning
confidence: 96%
“…Sources capable of these schemes need to emit photon pairs in a probabilistic manner with high brightness and low noise, preferably operating at telecom wavelengths that fit the high transmittance window of the optical fiber networks. In the past decades, photon-pair sources have been achieved through a variety of spontaneous nonlinear processes, including the spontaneous parametric down-conversion in optical crystals [6] and quasimatched waveguides [7], and the spontaneous fourwave mixing (SpFWM) in highly nonlinear fibers [8][9][10][11] and integrated waveguides [12][13][14][15][16][17][18][19][20]. Although the fiberbased source via SpFWM is more compatible with the optical fiber networks than the source via spontaneous * guokai07203@hotmail.com † yanglin61s@126.com parametric down-conversion, it suffers from the huge noise induced by the spontaneous Raman scattering of amorphous silica at room temperature [9].…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, a number of photon-pair generation experiments have been carried out in on-chip platforms, due to the advantages of designable dispersion and highly nonlinear response. The materials of these platforms include crystalline silicon [12][13][14][15][16], amorphous silicon [17], silica [18], silicon nitride [19], and (Al,Ga)As [20]. It is appealing to integrate significant building blocks for quantum communication on a single chip, the functionalities of which include photon-pair generation, photonpair modulation, cryptogram coding, and cryptogram decoding [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…As current data center communications systems use 850 nm vertical cavity lasers, monolithic integration would enable efficient wavelength division multiplexing devices [2]. AlGaAs has also been identified as the promising semiconductor system for quantum optics [3][4][5][6]. The integration of pump lasers, nonlinear optical elements, and signal processing waveguides opens the possibility of a true quantum optics technology.…”
mentioning
confidence: 99%