• Chinese Optics Letters
  • Vol. 22, Issue 4, 041201 (2024)
Yanru Zhou1、2、*, Lifan Fan1、3, Kai Xu1、3, Wenyao Liu1、3, Enbo Xing1、3, Jun Tang1、3, and Jun Liu1、3、**
Author Affiliations
  • 1State Key Laboratory of Dynamic Measurement Technology, North University of China, Taiyuan 030051, China
  • 2School of Information & Communication Engineering, North University of China, Taiyuan 030051, China
  • 3School of Instrument & Electronics, North University of China, Taiyuan 030051, China
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    DOI: 10.3788/COL202422.041201 Cite this Article Set citation alerts
    Yanru Zhou, Lifan Fan, Kai Xu, Wenyao Liu, Enbo Xing, Jun Tang, Jun Liu. Dynamic range expansion for optical frequency shift detection based on multiple harmonics[J]. Chinese Optics Letters, 2024, 22(4): 041201 Copy Citation Text show less

    Abstract

    Sensors based on optical resonators often have their measurement range limited by their cavity linewidth, particularly in the measurement of time-varying signals. This paper introduces a method for optical frequency shift detection using multiple harmonics to expand the dynamic range of sensors based on optical resonators. The proposed method expands the measurement range of optical frequency shift beyond the cavity linewidth while maintaining measurement accuracy. The theoretical derivation of this method is carried out based on the equation of motion for an optical resonator and the recursive relationship of the Bessel function. Experimental results show that the dynamic range is expanded to 4 times greater than the conventional first harmonic method while still maintaining accuracy. Furthermore, we present an objective analysis of the correlation between the expansion factor of the method and the linewidth and free spectrum of the optical resonator.

    da(t)dt={i[ΔG(t)]Γt2}a(t)+iΓexAin,

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    a(t)=iΓexAin0dτexp[(iΔΓt2)τ]exp[i0τdτG(tτ)].

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    a(t)=iΓexAin0dτexp[(iΔΓt2)τ]exp[2iΓtG(t)].

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    a(t)=iΓexAiniΔΓt2exp[2iΩΓtsin(ω0t)].

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    P(t)=|Ain+iΓexa(t)|2.

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    P(t)=|Ain|2|1+ΓexΔ2+(Γt2)2exp[i(Φ0+Φm)]|2,

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    P(t)=|Ain|2{1+[ΓexΔ2+(Γt2)2]2+2ΓexΔ2+(Γt2)2cos(Φ0+Φm)},

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    P(t)=PDC+δP(t),

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    δP(t)=2ΓexΔ2+(Γt2)2[cos(Φ0)cos(Φm)sin(Φ0)sin(Φm)].

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    cos(Φm)=cos[2ΩΓtsin(ω0t)]=J0(2ΩΓt)+2n=1J2n(2ΩΓt)cos(2nω0t),

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    sin(Φm)=sin[2ΩΓtsin(ω0t)]=2n=0J2n+1(2ΩΓt)cos[(2n+1)ω0t].

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    P(t)=2ΓexΔ2+(Γt2)2{J0(2ΩΓt)cos(Φ0)+2n=1J2n(2ΩΓt)cos(Φ0)cos(2nω0t)2n=0J2n+1(2ΩΓt)sin(Φ0)sin[(2n+1)ω0t]}.

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    2nJn(η)=η[Jn+1(η)+Jn1(η)],

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    4P2cos(Φ0)=2ΩΓt(P1+P3sin(Φ0)),

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    Ω=2Γttan(Φ0)P2P1+P3.

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    Ω=4ΔP2P1+P3.

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    Yanru Zhou, Lifan Fan, Kai Xu, Wenyao Liu, Enbo Xing, Jun Tang, Jun Liu. Dynamic range expansion for optical frequency shift detection based on multiple harmonics[J]. Chinese Optics Letters, 2024, 22(4): 041201
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