• Acta Physica Sinica
  • Vol. 69, Issue 17, 174204-1 (2020)
Yan-Qiang Guo1、3, Li-Jing Wang1, Yu Wang2, Xin Fang1, Tong Zhao1, and Xiao-Min Guo1、*
Author Affiliations
  • 1Key Laboratory of Advanced Transducers and Intelligent Control System, Ministry of Education, College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan 030024, China
  • 2State Key Laboratory of Cryptology, Beijing 100878, China
  • 3State Key Laboratory of Quantum Optics and Quantum Optics Devices, Shanxi University, Taiyuan 030006, China
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    DOI: 10.7498/aps.69.20200325 Cite this Article
    Yan-Qiang Guo, Li-Jing Wang, Yu Wang, Xin Fang, Tong Zhao, Xiao-Min Guo. Analysis and measurement of high-order photon correlations of light fields[J]. Acta Physica Sinica, 2020, 69(17): 174204-1 Copy Citation Text show less
    Theoretical model of double HBT scheme. B0, B1, B2, B3: Beamsplitter; D1, D2, D3, D4: Detector. The letters in parentheses L, N,K, et al, denote the photon numbers of splitting light paths, respectively.
    Fig. 1. Theoretical model of double HBT scheme. B0, B1, B2, B3: Beamsplitter; D1, D2, D3, D4: Detector. The letters in parentheses L, N,K, et al, denote the photon numbers of splitting light paths, respectively.
    (a) Third-order, and (b) fourth-order photon correlations and of single-mode thermal state versus the mean photon number .
    Fig. 2. (a) Third-order, and (b) fourth-order photon correlations and of single-mode thermal state versus the mean photon number .
    (a) Second-order, (b) third-order, and (c) fourth-order photon correlations of single-mode squeezed vacuum state versus the squeezing parameter r.
    Fig. 3. (a) Second-order, (b) third-order, and (c) fourth-order photon correlations of single-mode squeezed vacuum state versus the squeezing parameter r.
    The third-order (blue hollow square) and fourth-order (red solid circle) photon correlations of Fock state versus the photon number: (a) , ; (b) , .
    Fig. 4. The third-order (blue hollow square) and fourth-order (red solid circle) photon correlations of Fock state versus the photon number: (a) , ; (b) , .
    Schematic illustration of the experimental setup (ISO, isolator; HWP, half-wave plate; PBS, polarized beam splitter; M1, M2, mirror; L, optical lens; RGGD, rotating ground glass disk; BS1, BS2, BS3, beam splitter; D1, D2, D3 and D4, single photon counting module, SPCM; DAS, data acquisition system).
    Fig. 5. Schematic illustration of the experimental setup (ISO, isolator; HWP, half-wave plate; PBS, polarized beam splitter; M1, M2, mirror; L, optical lens; RGGD, rotating ground glass disk; BS1, BS2, BS3, beam splitter; D1, D2, D3 and D4, single photon counting module, SPCM; DAS, data acquisition system).
    Measured (a) third-order and (b) fourth-order photon correlations of thermal state and coherent state versus the counting rate for resolution time of 210 ns. The red and blue solid lines are the ideal results of the high-order photon correlations of thermal state and coherent state.
    Fig. 6. Measured (a) third-order and (b) fourth-order photon correlations of thermal state and coherent state versus the counting rate for resolution time of 210 ns. The red and blue solid lines are the ideal results of the high-order photon correlations of thermal state and coherent state.
    Measured (a) third-order and (b) fourth-order photon correlations of thermal state and coherent state versus the resolution time for counting rate of 80 kc/s. The red and blue solid lines are the ideal results of the high-order photon correlations of thermal state and coherent state.
    Fig. 7. Measured (a) third-order and (b) fourth-order photon correlations of thermal state and coherent state versus the resolution time for counting rate of 80 kc/s. The red and blue solid lines are the ideal results of the high-order photon correlations of thermal state and coherent state.
    Measured third-order photon correlation of thermal state versus delay times for resolution times of 210 ns and counting rate of 80 kc/s. The blue dots and black solid curves are the experimental and theoretical results, respectively: (a) τ2 = 0 μs; (b) τ2 = –10 μs; (c) τ2 = 10 μs. The peak value of g(3) in Fig. (a) is .
    Fig. 8. Measured third-order photon correlation of thermal state versus delay times for resolution times of 210 ns and counting rate of 80 kc/s. The blue dots and black solid curves are the experimental and theoretical results, respectively: (a) τ2 = 0 μs; (b) τ2 = –10 μs; (c) τ2 = 10 μs. The peak value of g(3) in Fig. (a) is .
    The fourth-order photon correlations of thermal state at complete time delays for (a) τ3 = 0 μs, (b) τ3 = –10 μs, (c) τ3 = 10 μs. The peak value of g(4) in Fig. (a) is .
    Fig. 9. The fourth-order photon correlations of thermal state at complete time delays for (a) τ3 = 0 μs, (b) τ3 = –10 μs, (c) τ3 = 10 μs. The peak value of g(4) in Fig. (a) is .
    Measured fourth-order photon correlation of thermal state versus delay time τ1 for resolution times of 210 ns and counting rate of 80 kc/s. The dots are the experimental results, and the black solid curves are the theoretical fittings.
    Fig. 10. Measured fourth-order photon correlation of thermal state versus delay time τ1 for resolution times of 210 ns and counting rate of 80 kc/s. The dots are the experimental results, and the black solid curves are the theoretical fittings.
    Yan-Qiang Guo, Li-Jing Wang, Yu Wang, Xin Fang, Tong Zhao, Xiao-Min Guo. Analysis and measurement of high-order photon correlations of light fields[J]. Acta Physica Sinica, 2020, 69(17): 174204-1
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