• Chinese Optics Letters
  • Vol. 14, Issue 6, 061301 (2016)
Mengning Hu, Yuping Chen*, Guangzhen Li, and Xianfeng Chen
Author Affiliations
  • State Key Laboratory of Advanced Optical Communication Systems and Networks, Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
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    DOI: 10.3788/COL201614.061301 Cite this Article Set citation alerts
    Mengning Hu, Yuping Chen, Guangzhen Li, Xianfeng Chen. Multichannel polarization-entangled photon-pair source for entanglement distribution[J]. Chinese Optics Letters, 2016, 14(6): 061301 Copy Citation Text show less
    Spectral emission rate of type I (black solid) and type II (red solid) QPM SPDC in a 2 cm-long 5% MgO:PPLN waveguide at the temperature of 20°C versus the signal wavelength. Curves of type 0, type I, and II have an FWHM of 54.3, 48.5, and 0.4 nm, respectively.
    Fig. 1. Spectral emission rate of type I (black solid) and type II (red solid) QPM SPDC in a 2 cm-long 5% MgO:PPLN waveguide at the temperature of 20°C versus the signal wavelength. Curves of type 0, type I, and II have an FWHM of 54.3, 48.5, and 0.4 nm, respectively.
    Scheme of the proposed source. The red arrows show the propagation direction of the pump laser, and the blue arrows show that of the fiber communication band photon pairs created in the crystal.
    Fig. 2. Scheme of the proposed source. The red arrows show the propagation direction of the pump laser, and the blue arrows show that of the fiber communication band photon pairs created in the crystal.
    Tuning curves of the photon pairs generation rate of type I QPM SPDC as a function of the crystal temperature in a 2 cm-long MgO:PPLN crystal. Two non-overlapping channel bands (black arrows) are supported at 20°C and 21°C.
    Fig. 3. Tuning curves of the photon pairs generation rate of type I QPM SPDC as a function of the crystal temperature in a 2 cm-long MgO:PPLN crystal. Two non-overlapping channel bands (black arrows) are supported at 20°C and 21°C.
    Comparisons between QPM SPDC bandwidths of type 0, type I, and type II. The red, black, and blue solid lines represent type 0, type I, and type II, respectively. (a) The phase mismatching parameters as functions of the signal wavelengths of type 0, type I, and type II. (b) QPM SPDC bandwidths as functions of the interaction lengths of type 0, type I and type II.
    Fig. 4. Comparisons between QPM SPDC bandwidths of type 0, type I, and type II. The red, black, and blue solid lines represent type 0, type I, and type II, respectively. (a) The phase mismatching parameters as functions of the signal wavelengths of type 0, type I, and type II. (b) QPM SPDC bandwidths as functions of the interaction lengths of type 0, type I and type II.
    Mengning Hu, Yuping Chen, Guangzhen Li, Xianfeng Chen. Multichannel polarization-entangled photon-pair source for entanglement distribution[J]. Chinese Optics Letters, 2016, 14(6): 061301
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