Author Affiliations
1Institute of Fundamental and Frontier Sciences, University of Electronic Science and Technology of China, Chengdu 610054, China2Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China3Southwest Institute of Technical Physics, Chengdu 610041, China4CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China5e-mail: c.z.yuan@uestc.edu.cn6e-mail: youwang_2007@aliyun.com7e-mail: zhouqiang@uestc.edu.cnshow less
Fig. 1. Conceptual illustration of the HOM interference to reveal the dispersion effect on the indistinguishability between single-photon wave-packets. (a) HOM interferometer with dispersive manipulation modules. Two identical single-photon wave-packets are manipulated with dispersion modules along two optical paths, i.e., path A and path B, and then are sent into an HOM interferometer; (b) HOM interference curves without the second-order dispersion along two paths; (c) with the same second-order dispersion along two paths, i.e., balanced HOM interferometer; (d) with unbalanced second-order dispersions along two paths. To obtain the HOM interference curve, the travel time of the wave-packet in path A is fixed, and that in path B is varied and the time axis is in reference to the center of the pulse in path A. To guide eyes, envelopes of three sub-wave-packets are depicted with solid and dashed lines in red, green, and blue, respectively, and the black envelope covering the three sub-wave-packets is used to illustrate the widths of the wave-packets.
Fig. 2. Experimental setup. The setup consists of attenuated mode-locked laser pulses, HOM interferometer, and photon detection with a dispersion module. VOA, variable optical attenuator; SMC, single-mode fiber coupler; PBS, polarization beam splitter; PMC, polarization-maintaining fiber coupler; PC, polarization controller; SNSPD, superconducting nanowire single photon detector; TDC, time to digital convertor.
Fig. 3. HOM interference curves (a) without a dispersion module, and (b) with 50 km long fiber as the dispersion module at the output of the mode-locked laser, respectively. The blue dots are experimental results. The solid purple lines are Gaussian fitting curves obtained via Monte Carlo method with 1000-time random sampling around each measured data assumed as Poissonian distribution.
Fig. 4. HOM interference curves with a 80 m long single-mode fiber inserted in one path, which corresponds to 16 periods of mode-locked laser pulses.
Fig. 5. (a) Output of a mode-locked pulse laser, measured by a second-order autocorrelator. (b) Output of a mode-locked pulse laser after the dispersive manipulation, recorded by the single-photon detection and a TDC.