• Photonics Research
  • Vol. 10, Issue 3, 618 (2022)
Jun Ye1, Xiaoya Ma1, Yang Zhang1, Jiangming Xu1、2、*, Hanwei Zhang1, Tianfu Yao1, Jinyong Leng1, and Pu Zhou1、3、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2e-mail: jmxu1988@163.com
  • 3e-mail: zhoupu203@163.com
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    DOI: 10.1364/PRJ.445432 Cite this Article Set citation alerts
    Jun Ye, Xiaoya Ma, Yang Zhang, Jiangming Xu, Hanwei Zhang, Tianfu Yao, Jinyong Leng, Pu Zhou. Revealing the dynamics of intensity fluctuation transfer in a random Raman fiber laser[J]. Photonics Research, 2022, 10(3): 618 Copy Citation Text show less

    Abstract

    Temporal intensity fluctuation is one of the inherent features of fiber lasers. When utilizing the fiber lasers to pump a random Raman fiber laser (RRFL), the intensity fluctuation transfer from the pump to the random lasing could affect the output performance significantly. In this paper, we comprehensively compared the spectral, temporal, and power characteristics of an RRFL pumped by two different fiber lasers—a temporally unstable fiber oscillator and a temporally stable amplified spontaneous emission (ASE) source. Owing to less impact of the intensity fluctuation transfer, the ASE source-pumped RRFL shows 45.3% higher maximum output power, higher spectral purity (>99.9%) and optical signal-to-noise ratio (>40 dB), weaker spectral broadening, and more stable temporal behavior compared to the fiber oscillator-pumped RRFL. Furthermore, based on the temporal-spatial-coupled Raman equations and the generalized nonlinear Schrödinger equations, we numerically revealed the impact of the pump intensity fluctuations on the output characteristics of RRFLs, and found that the temporal walk-off effect played an important role in the dynamics of intensity fluctuation transfer. This work may provide a reference for designing and implementing high-performance RRFLs and promote their practicability in sensing, telecommunications, and high-power applications.
    dP0+dz+1vg0dP0+dt=α0P0+λ1λ0gR1(P1++P1+4hν1Δν1B1)P0+,

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    dP1±dz±1vg1dP1±dt=±gR1P0+(P1±+2hν1Δν1B1)±ε1P1λ2λ1gR2(P2++P2+4hν2Δν2B2)P1±α1P1±,

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    dP2±dz±1vg2dP2±dt=±gR2(P1++P1)(P2±+2hν2Δν2B2)±ε2P2α2P2±,

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    Bj=1+1exp[h(νj1νj)kBT]1(j=1,2),

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    P0+(z=0,t)=Pin(t),

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    P1,2+(z=0,t)=RL1,2P1,2(z=0,t),

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    P1,2(z=L,t)=RR1,2P1,2+(z=L,t),

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    Pin(t)=Pavg+Afsin(2πftπ/2),

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    A0z=d01A0ti2β2p2A0t2+iγ0[|A0|2+(2fR)|A1+|2]A0α02ApgR1λ12λ0(|A1+|2+|A1|2)A0,

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    A1+z=i2β2s2A1+t2+iγ1[|A1+|2+(2fR)(|A0|2+|A2+|2)]A1+α12A1++gR12|A0|2A1++ε12A1gR2λ22λ1(|A2+|2+|A2|2)A1+,

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    A1z=i2β2s2A1t2+iγ1[|A1|2+(2fR)|A2|2]A1α12A1+gR12|A0|2A1+ε12A1+gR2λ22λ1(|A2|2+|A2+|2)A1,

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    A2+z=i2β2h2A2+t2+iγ2[|A2+|2+(2fR)|A1+|2]A2+α22A2++ε22A2+d12A2+t+gR22(|A1+|2+|A1|2)A2+,

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    A2z=i2β2h2A2t2+iγ2[|A2|2+(2fR)|A1|2]A2α22A2+ε22A2++d12A2t+gR22(|A1|2+|A1+|2)A2,

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    A0(0,t)=Ain,

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    A˜1,2+(0,ω)=RL1,2(ω)A˜1,2(0,ω),

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    A˜1,2(L,ω)=RR1,2(ω)A˜1,2+(L,ω),

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    Ain=mX^mexp(imΔωt),

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    φ1(ωm)=(1q)×φ0(ωm)+q×φ1(ωm1),

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    |A˜in(ω)|2=n0exp[4ln(2)ω2ΩL2].

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    Jun Ye, Xiaoya Ma, Yang Zhang, Jiangming Xu, Hanwei Zhang, Tianfu Yao, Jinyong Leng, Pu Zhou. Revealing the dynamics of intensity fluctuation transfer in a random Raman fiber laser[J]. Photonics Research, 2022, 10(3): 618
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