• High Power Laser Science and Engineering
  • Vol. 12, Issue 5, 05000e65 (2024)
Haiyang Wang1,2,3, Mengxia Wang2,3,*, Zhen Zhang4, Yuanan Zhao2,3,*..., Dawei Li2,3, Kun Shuai2,3, Hailong Qiu1,*, Zhonghan Zhang4, Liangbi Su4 and Jianda Shao2,3,5|Show fewer author(s)
Author Affiliations
  • 1Tianjin Key Laboratory of Functional Crystal Materials, Institute of Functional Crystals, Tianjin University of Technology, Tianjin, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
  • 3Laboratory of Thin Film Optics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 4Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
  • 5Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou, China
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    DOI: 10.1017/hpl.2024.44 Cite this Article Set citation alerts
    Haiyang Wang, Mengxia Wang, Zhen Zhang, Yuanan Zhao, Dawei Li, Kun Shuai, Hailong Qiu, Zhonghan Zhang, Liangbi Su, Jianda Shao, "976 nm continuous-wave laser damage of Er:CaF2 crystals," High Power Laser Sci. Eng. 12, 05000e65 (2024) Copy Citation Text show less

    Abstract

    Er:CaF2 crystals are crucial gain media for producing 3 μm mid-infrared (MIR) lasers pumped by 976 nm continuous-wave (CW) lasers owing to their low phonon energy and high conversion efficiency. This study investigated the damage characteristics and mechanism of Er:CaF2 crystals irradiated with a 976 nm CW laser. The laser-induced damage threshold of Er:CaF2 crystals with different Er3+ doping levels was tested; the damage morphology consists of a series of regular 70° cracks related to the angle of the crystal slip system on the surface. A finite-element model was used to calculate the temperature and stress fields of the crystals. The results indicated that the damage can be attributed to surface tensile stresses caused by the temperature gradient, and crystals with higher doping concentrations were more susceptible to damage owing to stronger light absorption. These findings provide valuable insights into the development of high-power MIR lasers.
    ρCpTt+ρCp\boldsymboluT=Qv+k2T, ((1))

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    Q(x,y,z)=(1R)2Pπw(z)2exp(2(x2+y2)w(z)2)exp(αz)w02w(z)2α, ((2))

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    w(z)=w01+(zzR)2, ((3))

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    kTl=hs(TT0), ((4))

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    σ+f=ρ2ut2. ((5))

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    σij=Cεij. ((6))

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    σx=E1+ν(εxx+ν12ν(εxx+εyy+εzz)),σy=E1+ν(εyy+ν12ν(εxx+εyy+εzz)),σz=E1+ν(εzz+ν12ν(εxx+εyy+εzz)),τxy=2Gεxy,τyz=2Gεyz,τxz=2Gεxz. ((7))

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    Haiyang Wang, Mengxia Wang, Zhen Zhang, Yuanan Zhao, Dawei Li, Kun Shuai, Hailong Qiu, Zhonghan Zhang, Liangbi Su, Jianda Shao, "976 nm continuous-wave laser damage of Er:CaF2 crystals," High Power Laser Sci. Eng. 12, 05000e65 (2024)
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