• Chinese Optics Letters
  • Vol. 14, Issue 8, 081901 (2016)
Wulong Zhao, Hongjun Liu*, Qibing Sun, Nan Huang, Zhaolu Wang, Jing Han, and Heng Sun
Author Affiliations
  • State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinademy of Sciences, Xi’an 710119, China
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    DOI: 10.3788/COL201614.081901 Cite this Article Set citation alerts
    Wulong Zhao, Hongjun Liu, Qibing Sun, Nan Huang, Zhaolu Wang, Jing Han, Heng Sun. Extracting signal via stochastic resonance in the semiconductor optical amplifier[J]. Chinese Optics Letters, 2016, 14(8): 081901 Copy Citation Text show less
    Schematic diagram of the stochastic resonance system.
    Fig. 1. Schematic diagram of the stochastic resonance system.
    Optical bistable hysteresis in the SOA with α=20 cm−1, η=0.75, g0=280 cm−1, L=300 μm, b=2, φ0=π4, and R=0.3.
    Fig. 2. Optical bistable hysteresis in the SOA with α=20cm1, η=0.75, g0=280cm1, L=300μm, b=2, φ0=π4, and R=0.3.
    Bistable output characteristics with different system parameters of the SOA: (a) b=3, φ0=π4, R=0.3, and L=100 μm (red), 200 μm (green), 300 μm (blue), and 400 μm (black); (b) L=300 μm, b=3, φ0=π4, and R=0.1 (red), 0.2 (green), 0.3 (blue), and 0.4 (black).
    Fig. 3. Bistable output characteristics with different system parameters of the SOA: (a) b=3, φ0=π4, R=0.3, and L=100μm (red), 200 μm (green), 300 μm (blue), and 400 μm (black); (b) L=300μm, b=3, φ0=π4, and R=0.1 (red), 0.2 (green), 0.3 (blue), and 0.4 (black).
    Bistability characteristics with different parameters: (a) R=0.3, L=300 μm, b=3, and φ0=0 (red), π4 (green), π3 (blue), and π2 (black); (b) R=0.3, L=300 μm, φ0=π4, and b=1.5 (red), 2 (green), 3 (blue), and 4 (black).
    Fig. 4. Bistability characteristics with different parameters: (a) R=0.3, L=300μm, b=3, and φ0=0 (red), π4 (green), π3 (blue), and π2 (black); (b) R=0.3, L=300μm, φ0=π4, and b=1.5 (red), 2 (green), 3 (blue), and 4 (black).
    Transmission properties of the stochastic resonance system with increasing noise intensities. (a)–(d) input signals S0=0.5 MW/cm2 with noise, in which normalized noise intensities D are 0∶1, 1∶1, 5∶1, and 10∶1, respectively; (a′)–(d′) the corresponding output signals through the stochastic resonance system with parameters L=300 μm, R=0.3, φ0=π4, and b=3.
    Fig. 5. Transmission properties of the stochastic resonance system with increasing noise intensities. (a)–(d) input signals S0=0.5MW/cm2 with noise, in which normalized noise intensities D are 01, 11, 51, and 101, respectively; (a′)–(d′) the corresponding output signals through the stochastic resonance system with parameters L=300μm, R=0.3, φ0=π4, and b=3.
    (a) Cross-correlation coefficients and (b) the cross-correlation gain as functions of the normalized noise intensity D at system parameters L=300 μm, R=0.3, φ0=π4, and b=3. The solid curves are the optimal fitted curves neglecting the random fluctuation.
    Fig. 6. (a) Cross-correlation coefficients and (b) the cross-correlation gain as functions of the normalized noise intensity D at system parameters L=300μm, R=0.3, φ0=π4, and b=3. The solid curves are the optimal fitted curves neglecting the random fluctuation.
    Wulong Zhao, Hongjun Liu, Qibing Sun, Nan Huang, Zhaolu Wang, Jing Han, Heng Sun. Extracting signal via stochastic resonance in the semiconductor optical amplifier[J]. Chinese Optics Letters, 2016, 14(8): 081901
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