• Photonics Research
  • Vol. 3, Issue 3, 86 (2015)
Rumao Tao1, Pengfei Ma1, Xiaolin Wang1、*, Pu Zhou1、2, and Zejin Liu1
Author Affiliations
  • 1College of Optoelectric Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, China
  • 2e-mail: zhoupu203@163.com
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    DOI: 10.1364/PRJ.3.000086 Cite this Article Set citation alerts
    Rumao Tao, Pengfei Ma, Xiaolin Wang, Pu Zhou, Zejin Liu. 1.3  kW monolithic linearly polarized single-mode master oscillator power amplifier and strategies for mitigating mode instabilities[J]. Photonics Research, 2015, 3(3): 86 Copy Citation Text show less

    Abstract

    We report on the high-power amplification of a 1064 nm linearly polarized laser in an all-fiber polarization-maintained master oscillator power amplifier, which can operate at an output power level of 1.3 kW. The beam quality (M2) was measured to be <1.2 at full power operation. The polarization extinction rate of the fiber amplifier was measured to be above 94% before mode instabilities (MIs) set in, which reduced to about 90% after the onset of MI. The power scaling capability of strategies for suppressing MI is analyzed based on a semianalytical model, the theoretical results of which agree with the experimental results. It shows that mitigating MI by coiling the gain fiber is an effective and practical method in standard double-cladding large mode area fiber, and, by tight coiling of the gain fiber to the radius of 5.5 cm, the MI threshold can be increased to three times higher than that without coiling or loose coiling. Experimental studies have been carried out to verify the idea, which has proved that MI was suppressed successfully in the amplifier by proper coiling.
    E(r,ϕ,z,t)=m=0l=1Aml(z,t)ψml(r,ϕ)ej(βmlzωmlt)+c.c.,(1)

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    Is(r,ϕ,z,t)=2n0ε0cE(r,ϕ,z,t)E(r,ϕ,z,t)*=I0+I˜(2)

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    I0=I11(z,t)ψ1(r,ϕ)ψ1(r,ϕ)+I22(z,t)ψ2(r,ϕ)ψ2(r,ϕ),(3a)

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    I˜=I12(z,t)ψ1(r,ϕ)ψ2(r,ϕ)ej(qzΩt)+I21(z,t)ψ1(r,ϕ)ψ2(r,ϕ)ej(qzΩt),(3b)

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    Ikl(z,t)=4n0ε0cAk(z,t)Al*(z,t),(3c)

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    q=β1β2,Ω=ω1ω2.(3d)

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    2T(r,ϕ,z,t)+Q(r,ϕ,z,t)κ=1αT(r,ϕ,z,t)t,(4)

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    Q(r,ϕ,z,t)g(r,ϕ,z,t)(vpvsvs)Is(r,ϕ,z,t),(5a)

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    g(r,ϕ,z,t)=[(σsa+σse)nu(r,ϕ,z,t)σsa]NYb(r,ϕ),(5b)

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    κTr+hqT=0,(6)

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    T(r,ϕ,z,t)=1πασηvm=1Jv(δmr)H(δm)t=0t[B11(ϕ,z)I11(z,t)+B22(ϕ,z)I22(z,t)+B12(ϕ,z)I12(z,t)ej(qzΩt)+B12(ϕ,z)I12*(z,t)ej(qzΩt)]eαδm2(tt)dt(7)

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    Bkl(ϕ,z)={02πdϕ0Rg0Jv(δm,r)cosv(ϕϕ)ψk(r,ϕ)ψk(r,ϕ)1+I0/Isaturationdr,k=l02πdϕ0Rg0Jv(δm,r)cosv(ϕϕ)ψk(r,ϕ)ψl(r,ϕ)(1+I0/Isaturation)2dr,kl,(8a)

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    H(δm)=0RrJv2(δm,r)dr,σ=ηκ(vpvsvs),(8b)

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    n2=(n0+ng+nNL)2n02jg(r,ϕ,z,t)n0k0+2n0nNL,(9)

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    nNL(r,ϕ,z,t)=ηT(r,ϕ,z,t)=h11(r,ϕ,z,t)+h22(r,ϕ,z,t)+h12(r,ϕ,z,t)ejqz+h21(r,ϕ,z,t)ejqz(10)

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    hkl(r,ϕ,z,t)={ασπvm=1Jv(δmr)H(δm)0tBkk(ϕ,z)Ikk(z,t)eαδm2(tt)dt,k=lασπvm=1Jv(δmr)H(δm)0tBkl(ϕ,z)Ikl(z,t)eαδm2(tt)jΩtdt,kl.(11)

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    ξ(L)ω0P1(L)2π0LP1(z)|χ(Ω0)|dzexp{0L[g(r,ϕ,z)ψ2ψ2rdrdϕ]dz+0LP1(z)χ(Ω0)dz},(14)

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    ξ(L)ξ0exp[0Ldzg(r,ϕ,z)(ψ2ψ2ψ1ψ1)rdrdϕαcoilLcoil]+ξ042π0LP1(z)|χ(Ω0)|dzRN(Ω0)×exp[0Ldzg(r,ϕ,z)(ψ2ψ2ψ1ψ1)rdrdϕ+0LP1(z)χ(Ω0)dzαcoilLcoil],(15)

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    Rumao Tao, Pengfei Ma, Xiaolin Wang, Pu Zhou, Zejin Liu. 1.3  kW monolithic linearly polarized single-mode master oscillator power amplifier and strategies for mitigating mode instabilities[J]. Photonics Research, 2015, 3(3): 86
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