• High Power Laser Science and Engineering
  • Vol. 12, Issue 4, 04000e38 (2024)
Ruixian Li1, Hanshuo Wu1,2,3, Hu Xiao1,2,3,*, Zilun Chen1,2,3..., Jinyong Leng1,2,3, Liangjin Huang1,2,3, Zhiyong Pan1,2,3 and Pu Zhou1,*|Show fewer author(s)
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, Changsha, China
  • show less
    DOI: 10.1017/hpl.2024.21 Cite this Article Set citation alerts
    Ruixian Li, Hanshuo Wu, Hu Xiao, Zilun Chen, Jinyong Leng, Liangjin Huang, Zhiyong Pan, Pu Zhou, "Design and optimization methods towards a 10 kW high beam quality fiber laser based on the counter tandem pumping scheme," High Power Laser Sci. Eng. 12, 04000e38 (2024) Copy Citation Text show less

    Abstract

    In this study, we investigated the influence of fiber parameters on stimulated Raman scattering (SRS) and identified a unique pattern of SRS evolution in the counter tandem pumping configuration. Our findings revealed that the SRS threshold in counter-pumping is predominantly determined by the length of the output delivery fiber rather than the gain fiber. By employing the counter tandem pumping scheme and optimizing the fiber parameters, a 10 kW fiber laser was achieved with beam quality M2 of 1.92. No mode instability or severe SRS limitation was observed. To our knowledge, this study achieved the highest beam quality in over 10 kW fiber lasers based on conventional double-clad Yb-doped fiber.
    N2(z)N={[Pp+(z)+Pp(z)]σapλpΓphcAc+[Ps+(z)+Ps(z)]σasλsΓshcAc+[PR+(z)+PR(z)]σaRλRΓRhcAc}{1τ+[Pp+(z)+Pp(z)](σap+σep)λpΓphcAc+[Ps+(z)+Ps(z)](σes+σas)λsΓshcAc+[PR+(z)+PR(z)](σRs+σRs)λRΓRhcAc}1, ((1))

    View in Article

    ±dPp±(z)dz=Γp{σa(λp)N[σa(λp)+σe(λp)]N2(z)}×Pp±(z)α(λp)Pp±(z), ((2))

    View in Article

    ±dPs±(z)dz=Γs{[σe(λs)+σa(λs)]N2(z)σa(λs)N}Ps±(z)+Γsσe(λs)N2(z)P0gRAeffsλRλs[PR+(z)+PR(z)]×Ps±(z)α(λs)Ps±(z), ((3))

    View in Article

    ±dPR±(z)dz=ΓR{[σe(λR)+σa(λR)]N2(z)σa(λR)N}PR±(z)+ΓRσe(λR)N2(z)P0+gRAeffR[Ps+(z)+Ps(z)]×PR±(z)α(λR)PR±(z). ((4))

    View in Article

    dPs±(z)dz=gRAcλRλs[PR+(z)+PR(z)]PR±(z)α(λs)Ps±(z), ((5))

    View in Article

    dPR±(z)dz=gRAc[Ps+(z)+Ps(z)]PR±(z)α(λR)PR±(z). ((6))

    View in Article

    GSRS(z)={ΓR{[σe(λR)+σa(λR)]N2(z)σa(λR)N}+gRAc[Ps+(z)+Ps(z)], in YDF,gRAc[Ps+(z)+Ps(z)], in DF. ((7))

    View in Article

    Ruixian Li, Hanshuo Wu, Hu Xiao, Zilun Chen, Jinyong Leng, Liangjin Huang, Zhiyong Pan, Pu Zhou, "Design and optimization methods towards a 10 kW high beam quality fiber laser based on the counter tandem pumping scheme," High Power Laser Sci. Eng. 12, 04000e38 (2024)
    Download Citation