Chinese Journal of Lasers, Volume. 51, Issue 19, 1901008(2024)

Research Progress of Highly RE‐Doped Silica Fibers and Short‐Cavity Fiber Lasers (Invited)

Yafei Wang1, Mengting Guo1, Fan Wang1, Chongyun Shao1, Yan Jiao3, Meng Wang1, Lei Zhang1, Hehe Dong1, Suya Feng1, Shikai Wang1, Danping Chen1, Chunlei Yu1,2、*, and Lili Hu1,2、**
Author Affiliations
  • 1Research Center of Specialty Glass and Fiber, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2School of Physics and Optoelectronic Engineering, Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, Zhejiang , China
  • 3Juxin Photonics Technology (Taizhou) Co., Ltd., Taizhou 318000, Zhejiang , China
  • show less
    Figures & Tables(32)
    Schematic diagram of MCVD technique[31]
    Schematic diagram of MCVD combined sol-doping[32]
    Schematic diagram of MCVD system with vapor phase doping[33]
    Schematic diagram of DND manufacturing fiber[34]
    Schematic diagram of the REPUSIL process[31]
    Fabrication procedure of RE-doped silica glasses and fibers by sol-gel combined high temperature sintering[36]
    Schematic diagram of laser sintering RE-doped silica powder[37]
    Schematic diagram of glass phase-separation technology[39]
    Single-frequency DBR Nd3+-doped silica fiber laser at 930 nm[44]. (a) Experimental setup; (b) laser spectrum; (c) output power
    Watt-level single-frequency tunable MOPA Nd3+-doped fiber laser operating at 915‒937 nm[45]
    Single-frequency DBR Nd3+-doped silica fiber laser at 910 nm[58]. (a) Experimental setup; (b) laser spectrum, the inset is the longitudinal characteristic; (c) output power
    920 nm passively mode-locked Nd3+-doped fiber laser with 207 MHz fundamental repetition rate[61]. (a) Experimental setup; (b) pulse train; (c) laser spectra, the inset is the measurement result of 2 h spectrum stability; (d) radio frequency (RF) spectra, the inset is the RF spectrum from 0 to 5 GHz; (e) autocorrelation curve; (f) output power
    Single-frequency DBR laser based on commercial Yb406 Yb3+-doped silica fiber[67]. (a) Experimental setup; (b) output power, the inset is the power stability in 10 min time span; (c) laser spectra, the inset is the laser spectrum in 3 nm span
    Structure comparison of single-frequency DBR cavity. (a) Conventional DBR cavity; (b) monolithic single-frequency DBR cavity
    Monolithic single-frequency DBR laser based on photosensitive Yb3+-doped silica fiber[71]. (a) Experimental setup, the inset is the photograph of the monolithic cavity; (b) transmission spectra of HR-FBG and LR-FBG; (c) output power
    Dissipative soliton mode-locked laser with 3.3 GHz fundamental repetition rate by high absorption Yb3+-doped silica fiber[72]. (a) Experimental setup; (b) structure of the dispersive dielectric mirror (DDM), the Ta2O5-SiO2 multilayer coating designed and deposited onto the end facet of the fiber ferrule segment; (c) group velocity dispersion and transmissivity of the DDM versus wavelength between 970 nm and 1100 nm; (d) laser spectra versus pump power; (e) RF spectrum
    Dual-frequency DBR 1.5 μm fiber laser based on Er3+-doped silica fiber[76]. (a) Experimental setup; (b) reflective spectra of high- and low-reflection superimposed fiber Bragg gratings; (c) laser output power; (d) verification of dual-wavelength laser single frequency operation using a scanning Fabry‒Pérot interferometer; (e) frequency spectrum of the two-wavelength beating signal within 1 GHz span
    Highly Er3+-doped silica fiber developed by Shanghai Institute of Optics and Fine Mechanics via MCVD combined sol-gel doping method[32]. (a) Radial refractive index profile, the inset shows micrograph of fiber end-face; (b) distribution of Al and Er elements in the end-face; (c) core absorption coefficient; (d) propagation loss
    Monolithic single-frequency fiber laser at 1540 nm based on photosensitive Er3+/Yb3+ co-doped silica fiber[80]. (a) Experimental setup; (b) single longitudinal mode characteristic measured by Fabry‒Pérot interferometer; (c) laser spectrum
    Passively mode-locked Er3+-doped fiber laser at 1.5 μm with 5 GHz fundamental repetition rate[86]. (a) Experimental setup; (b) laser spectra, the inset shows the magnification of the optical spectrum in 0.3 nm range; (c) RF spectra, the inset shows the RF spectra from 0 to 12 GHz
    Schematic of single-frequency DFB fiber laser at 2.0 μm[91]
    Monolithic single-frequency DBR fiber laser at 2.0 μm[92]. (a) Experimental setup; (b) transmission spectra of high- and low-reflection fiber Bragg gratings; (c) output power
    Single-frequency DBR fiber laser at 1908-2050 nm based on commercial Tm3+-doped silica fiber[93]. (a) Cavity structure;
    Single-frequency DBR fiber laser at 2.0 μm based on commercial Tm3+-doped silica fiber[94]. (a) Experimental setup; (b) laser spectra, the inset show the laser spectrum in 2 nm range; (c) output power
    Single-frequency DBR fiber laser at 2.0 μm[96]. (a) Structure diagram; (b) photo of laser adiabatic package; (c) photo of the laser prototype
    • Table 1. Typical results of 0.9‒2.0 μm single-frequency laser by RE-doped soft glass fibers

      View table

      Table 1. Typical results of 0.9‒2.0 μm single-frequency laser by RE-doped soft glass fibers

      Fiber

      Wavelength /

      nm

      Cavity

      Fiber

      length /cm

      Power /

      mW

      Efficiency /

      %

      InstituteYearRef.
      Nd3+-doped phosphate fiber880DBR2.544.520.4University of Arizona202223
      Yb3+-doped phosphate fiber1064DBR1.8115066University of Arizona202112
      Er3+/Yb3+ co-doped phosphate fiber1550DBR230030.9South China University of Technology201018
      Tm3+-doped germanate fiber1950DBR1.861742.2South China University of Technology201824
    • Table 2. Typical results of 0.9‒2.0 μm high-repetition-rate passively mode-locked laser by RE-doped soft glass fibers

      View table

      Table 2. Typical results of 0.9‒2.0 μm high-repetition-rate passively mode-locked laser by RE-doped soft glass fibers

      Fiber

      Wavelength /

      nm

      Cavity

      Fiber

      length /cm

      Repetition

      rate /GHz

      InstituteYearRef.
      Nd3+-doped silicate fiber920F‒P81.6Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences202325
      Yb3+-doped phosphate fiber1064F‒P0.812.5South China University of Technology201921
      Er3+/Yb3+ co-doped phosphate fiber1556F‒P0.519.5The University of Tokyo201122
      Tm3+-doped germanate fiber1915F‒P0.911.2South China University of Technology202226
    • Table 3. Typical splicing loss between soft glass fiber and silica fiber

      View table

      Table 3. Typical splicing loss between soft glass fiber and silica fiber

      Spliced fiberSplicing loss /dBInstituteRef.
      Phosphate fiber+silica fiber0.3Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences27
      Silicate fiber+silica fiber0.6Tianjin University20
      Tellurite fiber+silica fiber0.7University of Arizona29
      Germanate fiber+silica fiber0.8NP Photonics30
      Fluorotellurite fiber+silica fiber0.08Harbin Engineering University28
    • Table 4. Commercial high-absorption RE-doped silica fibers

      View table

      Table 4. Commercial high-absorption RE-doped silica fibers

      ManufacturerRare earthTypeNumerical apertureDiameter /μmCore absorption
      NufernNdPM-NDF-5/1250.145/125450 dB/m@808 nm
      CoractiveYbYb4060.164/1252400 dB/m@976 nm
      LiekkiErEr-1100.24/125110 dB/m@1530 nm
      NufernTmSM-TDF-10P/130-M0.1510/1301521 dB/m@793 nm*
    • Table 5. Single-frequency Yb3+-doped silica fiber laser at 1.0 μm

      View table

      Table 5. Single-frequency Yb3+-doped silica fiber laser at 1.0 μm

      Fiber

      Wavelength /

      nm

      Cavity

      Fiber

      length /cm

      Power /

      mW

      Efficiency /

      %

      InstituteYearRef.
      Coractive, DCF-YB-7/128-FA1063DBR1.044.530Beijing University of Technology201662
      Commercial Yb3+-doped silica fiber*1150DFB5.0104.5National University of Defense Technology202163
      Fibercore, DF11001030DBR1.414.43Northwest University202364
      Commercial Yb3+-doped silica fiber*1030DBR0.87.42Aerospace Information Research Institute202365
      Coractive, Yb4061064DBR1.264266.4Tianjin University202367
      Self-developed Yb3+-doped silica fiber1064DBR1.07516.4Shanghai Institute of Optics and Fine Mechanics, Chinese Academy Sciences202366
    • Table 6. Typical results of 1.0 μm passively mode-locked Yb3+-doped fiber lasers with high repetition rate

      View table

      Table 6. Typical results of 1.0 μm passively mode-locked Yb3+-doped fiber lasers with high repetition rate

      Fiber

      Wavelength /

      nm

      Cavity

      Cavity

      length /cm

      Repetition

      rate /GHz

      InstituteYearRef.
      Coractive, DCF-Yb-7/1281064F‒P3.23.1Beijing University of Technology201773
      Self-developed Yb3+-doped silica fiber1066F‒P8.41.2Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences202366
      Coractive, Yb401-PM1040F‒P8.01.3Xiamen University202374
      Coractive, Yb5501064F‒P3.03.3Xiamen University202372
    • Table 7. Typical results of 1.5 μm passively mode-locked Er3+-doped fiber laser with high repetition rate

      View table

      Table 7. Typical results of 1.5 μm passively mode-locked Er3+-doped fiber laser with high repetition rate

      Fiber

      Wavelength /

      nm

      Cavity

      Cavity

      length /cm

      Repetition

      rate /GHz

      InstituteYearRef
      Liekki Er-801573F‒P10.31.0Massachusetts Institute of Technology201082
      Liekki Er-801554F‒P101.0Xi’an Institute of Optics and Precision Mechanics, Chinese Academy Sciences201983
      Liekki Er-801610F‒P101.0Xi’an Institute of Optics and Precision Mechanics, Chinese Academy Sciences201984
      Liekki Er-1101558F‒P3.82.7Xi’an Institute of Optics and Precision Mechanics, Chinese Academy Sciences201985
      Liekki Er-1101560F‒P25Shangdong Univeristy202186
      Er3+/Yb3+ co-doped silica fiber*1535F‒P81.6Xiamen Univeristy202388
    Tools

    Get Citation

    Copy Citation Text

    Yafei Wang, Mengting Guo, Fan Wang, Chongyun Shao, Yan Jiao, Meng Wang, Lei Zhang, Hehe Dong, Suya Feng, Shikai Wang, Danping Chen, Chunlei Yu, Lili Hu. Research Progress of Highly RE‐Doped Silica Fibers and Short‐Cavity Fiber Lasers (Invited)[J]. Chinese Journal of Lasers, 2024, 51(19): 1901008

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category: laser devices and laser physics

    Received: Jul. 18, 2024

    Accepted: Sep. 2, 2024

    Published Online: Oct. 11, 2024

    The Author Email: Chunlei Yu (sdycllcy@siom.ac.cn), Lili Hu (hulili@siom.ac.cn)

    DOI:10.3788/CJL241063

    CSTR:32183.14.CJL241063

    Topics