• Chinese Optics Letters
  • Vol. 18, Issue 3, 030601 (2020)
Zongfu Hu1, Zhiguo Jiang1、*, Jinfang Wang2、3, and Su Mei1
Author Affiliations
  • 1College of Electronics and Information Engineering, Tongji University, Shanghai 201806, China
  • 2Shanghai Aerospace Control Technology Institute, Shanghai 201109, China
  • 3Shanghai Engineering Research Center of Inertia, Shanghai 201109, China
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    DOI: 10.3788/COL202018.030601 Cite this Article Set citation alerts
    Zongfu Hu, Zhiguo Jiang, Jinfang Wang, Su Mei. Resonator fiber optic gyros with light time-division input and multiplexing output in clockwise and counterclockwise directions[J]. Chinese Optics Letters, 2020, 18(3): 030601 Copy Citation Text show less

    Abstract

    A resonator fiber optic gyro with the light time-division input and multiplexing output (TDM-RFOG) in the clockwise (CW) and counterclockwise (CCW) directions is proposed. The light time-division input in the CW and CCW directions can effectively suppress the backscattering induced noise. The TDM-RFOG is implemented with the 2 × 2 Mach–Zehnder interferometer (MZI) optical switch. The response time of the fiber ring resonator is analyzed, and it is demonstrated by experiments that light time-division input in the CW and CCW directions can reduce the backscattering induced noise. The suppression effectiveness of backscattering induced noise in the TDM-RFOG is determined by the extinction ratio of the optical switch, so a closed loop is designed to adjust the phase shift difference between the two arms of the MZI optical switch to control the extinction ratio. The method using two arms of the MZI optical switch with twin 90° polarization-axis rotated splices is proposed to make the extinction ratio along both slow and fast axes greater than ?70 dB.
    E(t)=EReiω0t,(1)

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    E(nτ)=EReiω0t(1γ)Km=n((1γ)(1K))mei(ω0+2πfw)mτ,(2)

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    F=π(1γ)(1K)1(1γ)(1K).(3)

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    E(nτ)=EReiω0t{(1γ)(1K)(1γ)K×m=1n[(1γ)(1K)]m1ei(ω0+2πfw)mτ}.(4)

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    Es=EDei(ω0t+φ1),(5a)

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    Eb=Rb·EDei(ω0t+ξ),(5b)

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    I=ED2+TEXT·Rb2ED2+2TEXT·RbED2cos(φ1ξ),(6)

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    E3(t)=E0[k1k2ei(ω0t)+1k11k2ei(ω0t+Δϕ+π)],(7a)

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    E4(t)=E0[k11k2ei(ω0t)+1k1k2ei(ω0t+Δϕ)],(7b)

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    P3=P0[k1k2+(1k1)(1k2)2k1(1k1)k2(1k2)cosΔϕ],(8a)

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    P4=P0[k1(1k2)+(1k1)k2+2k1(1k1)k2(1k2)cosΔϕ],(8b)

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    TEXT=10lg(P3/P4).(9)

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    PL(t)=P0{k1k2+(1k1)(1k2)2k1(1k1)k2(1k2)cos[Δϕ+ϕL(t)]},(10a)

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    ϕL(t)={φ,0t<1/2fLφ,1/2fLt<1/fL,(10b)

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    ΔPsyn(Δϕ)=01/2fLPL(t)dt1/2fL1/fLPL(t)dt,=P0{2k1(1k1)k2(1k2)×[cos(Δϕ+φ)cos(Δϕφ)]},(11)

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    φ||=2πλ(n||L1+nL2),(12)

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    φ=2πλ(nL1+n||L2).(13)

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    ΔφT=[2πλ(n||n)ΔLM]/T,(14)

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    Zongfu Hu, Zhiguo Jiang, Jinfang Wang, Su Mei. Resonator fiber optic gyros with light time-division input and multiplexing output in clockwise and counterclockwise directions[J]. Chinese Optics Letters, 2020, 18(3): 030601
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