• Photonics Research
  • Vol. 12, Issue 5, 995 (2024)
Yang Zhang1, Jiangming Xu1、4、*, Junrui Liang1, Sicheng Li1, Jun Ye1、2、3, Xiaoya Ma1, Tianfu Yao1、2、3, Zhiyong Pan1、2、3, Jinyong Leng1、2、3, and Pu Zhou1、5、*
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, National University of Defense Technology, Changsha 410073, China
  • 4e-mail: jmxu1988@163.com
  • 5e-mail: zhoupu203@163.com
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    DOI: 10.1364/PRJ.510057 Cite this Article Set citation alerts
    Yang Zhang, Jiangming Xu, Junrui Liang, Sicheng Li, Jun Ye, Xiaoya Ma, Tianfu Yao, Zhiyong Pan, Jinyong Leng, Pu Zhou. High power cladding-pumped low quantum defect Raman fiber amplifier[J]. Photonics Research, 2024, 12(5): 995 Copy Citation Text show less

    Abstract

    Heat generated by the quantum defect (QD) in optically pumped lasers can result in detrimental effects such as mode instability, frequency noise, and even catastrophic damage. Previously, we demonstrated that boson-peak-based Raman fiber lasers have great potential in low QD laser generation. But their power scalability and heat load characteristics have yet to be investigated. Here, we demonstrate a boson-peak-based Raman fiber amplifier (RFA) with 815 W output power and a QD of 1.3%. The low heat generation characteristics of this low QD RFA are demonstrated. Both experimental and simulation results show that at this power level, the heat load of the low QD RFA is significantly lower than that of the conventional RFA with a QD of 4.8%. Thanks to its low heat generation characteristics, the proposed phosphosilicate-fiber-based low QD RFA provides an effective solution for the intractable thermal issue in optically pumped lasers, which is of significance in reducing the laser’s noise, improving the laser’s stability and safety, and solving the challenge of heat removing.
    dP0dz=α0P0gR01Acladλ1λ0P0P1gR02Acladλ2λ0P0P2,

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    dP1dz=α1P1+gR01AcladP0P1gR12Acoreλ2λ1P1P2,

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    dP2dz=α2P2+gR12AcoreP1P2+gR02AcladP0P2,

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    2T+Qκ=0,(A1)

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    1rr(rT1(r)r)+Q1κ1=0,0rr1,(A2)

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    1rr(rT2(r)r)+Q2κ2=0,r1rr2,(A3)

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    1rr(rT3(r)r)=0,r2rr3,(A4)

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    1rr(rT4(r)r)=0,r3rr4,(A5)

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    Q1=α0P0Aclad+α1P1Acore+α2P2Acore+gR01AcladAcoreλ1λ0λ1P0P1+gR02AcladAcoreλ2λ0λ2P0P2+gR02AcoreAcoreλ2λ1λ2P1P2,(A6)

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    Q2=α0P0Aclad.(A7)

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    Ti(ri)=Ti+1(ri),i=1,2,3,(A8)

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    κiTi(ri)=κi+1Ti+1(ri),i=1,2,3,(A9)

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    T4(r4)=hκ4(T0T4(r4)),(A10)

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    T1(r)=T0+Q1(r12r2)4κ1(Q1Q2)r122κ2lnr1+((Q1Q2)r122κ2Q1r12+Q2(r22r12)2κ3)lnr2+Q2(r22r12)4κ2+(Q1r12+Q2(r22r12))(12hr4+lnr42κ4+lnr32κ3lnr32κ4),0rr1,(A11)

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    T2(r)=T0+Q2(r22r2)4κ2(Q1Q2)r122κ2lnr+((Q1Q2)r122κ2Q1r12+Q2(r22r12)2κ3)lnr2+(Q1r12+Q2(r22r12))(12hr4+lnr42κ4+lnr32κ3lnr32κ4),r1rr2,(A12)

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    T3(r)=T0Q1r12+Q2(r22r12)2κ3lnr+(Q1r12+Q2(r22r12))(12hr4+lnr42κ4+lnr32κ3lnr32κ4),r2rr3,(A13)

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    T4(r)=T0Q1r12+Q2(r22r12)2κ4lnr+(Q1r12+Q2(r22r12))(12hr4+lnr42κ4),r3rr4.(A14)

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    Yang Zhang, Jiangming Xu, Junrui Liang, Sicheng Li, Jun Ye, Xiaoya Ma, Tianfu Yao, Zhiyong Pan, Jinyong Leng, Pu Zhou. High power cladding-pumped low quantum defect Raman fiber amplifier[J]. Photonics Research, 2024, 12(5): 995
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