• Laser & Optoelectronics Progress
  • Vol. 56, Issue 4, 043002 (2019)
Yuanyuan Song1, Ding Chen2, and Shuang Cong1、*
Author Affiliations
  • 1 Department of Automation, University of Science and Technology of China, Hefei, Anhui 230027, China
  • 2 State Key Laboratory of Space-Ground Integrated Information Technology, Beijing Institute of Satellite Information Engineering, Beijing 100086, China
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    DOI: 10.3788/LOP56.043002 Cite this Article Set citation alerts
    Yuanyuan Song, Ding Chen, Shuang Cong. Property of Entangled Photon Pairs Generated via Spontaneous Parametric Down Conversion[J]. Laser & Optoelectronics Progress, 2019, 56(4): 043002 Copy Citation Text show less
    Schematic of experimental device for generation of entangled photon pairs via type-II spontaneous parametric down conversion. (a) Collinear matching; (b) non-collinear matching
    Fig. 1. Schematic of experimental device for generation of entangled photon pairs via type-II spontaneous parametric down conversion. (a) Collinear matching; (b) non-collinear matching
    Illustration of type-II SPDC light field
    Fig. 2. Illustration of type-II SPDC light field
    Single photon spectra of signal light (s) and idle light (i) under different parameters. (a) Ω>0; (b) Ω<0; (c) D+≠0; (d) D+=0
    Fig. 3. Single photon spectra of signal light (s) and idle light (i) under different parameters. (a) Ω>0; (b) Ω<0; (c) D+≠0; (d) D+=0
    Source function graphs when continuous light used as pump. (a1) (a2) 3D and 2D plots of phase matching function; (b1) (b2) 3D and 2D plots of pumping linear function; (c1) (c2) 3D and 2D plots of combined spectral function; (d) single photon spectra
    Fig. 4. Source function graphs when continuous light used as pump. (a1) (a2) 3D and 2D plots of phase matching function; (b1) (b2) 3D and 2D plots of pumping linear function; (c1) (c2) 3D and 2D plots of combined spectral function; (d) single photon spectra
    3D plots of pumping linear functions, 3D plots and 2D plots of combined spectral functions, single photon spectra under different spectral widths of pulsed laser. (a1) (b1) (c1) (d1) σp=0.5 nm; (a2) (b2) (c2) (d2) σp=2 nm; (a3) (b3) (c3) (d3) σp=5 nm
    Fig. 5. 3D plots of pumping linear functions, 3D plots and 2D plots of combined spectral functions, single photon spectra under different spectral widths of pulsed laser. (a1) (b1) (c1) (d1) σp=0.5 nm; (a2) (b2) (c2) (d2) σp=2 nm; (a3) (b3) (c3) (d3) σp=5 nm
    3D plots of pumping linear functions, 3D plots of phase matching functions, 3D plots and 2D plots of combined spectral functions, single photon spectra under different crystal thicknesses. (a) σp=1 nm; (b1) (c1) (d1) (e1) L=0.5 nm; (b2) (c2) (d2) (e2) L=1 mm; (b3) (c3) (d3) (e3) L=3 mm
    Fig. 6. 3D plots of pumping linear functions, 3D plots of phase matching functions, 3D plots and 2D plots of combined spectral functions, single photon spectra under different crystal thicknesses. (a) σp=1 nm; (b1) (c1) (d1) (e1) L=0.5 nm; (b2) (c2) (d2) (e2) L=1 mm; (b3) (c3) (d3) (e3) L=3 mm
    Combined two-photon spectra under different frequency correlation. (a) Non-correlation; (b) positive correlation
    Fig. 7. Combined two-photon spectra under different frequency correlation. (a) Non-correlation; (b) positive correlation
    σp /nmΔνc /THzΔνs /THzRV
    0.50.675.868.750.96
    21.136.946.140.77
    52.2612.585.570.69
    Table 1. Frequency entanglement and interference visibility under different spectral widths of pulsed laser
    L /mmΔνc /THzΔνs /THzRV
    0.51.7411.206.440.99
    10.916.427.050.84
    30.292.528.690.58
    Table 2. Frequency entanglement and interference visibility under different crystal thicknesses
    Yuanyuan Song, Ding Chen, Shuang Cong. Property of Entangled Photon Pairs Generated via Spontaneous Parametric Down Conversion[J]. Laser & Optoelectronics Progress, 2019, 56(4): 043002
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