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0.9~1.0 μm近红外连续光纤激光器的研究进展

党文佳 李哲 卢娜 李玉婷 张蕾 田晓

党文佳, 李哲, 卢娜, 李玉婷, 张蕾, 田晓. 0.9~1.0 μm近红外连续光纤激光器的研究进展[J]. 中国光学, 2021, 14(2): 264-274. doi: 10.37188/CO.2020-0193
引用本文: 党文佳, 李哲, 卢娜, 李玉婷, 张蕾, 田晓. 0.9~1.0 μm近红外连续光纤激光器的研究进展[J]. 中国光学, 2021, 14(2): 264-274. doi: 10.37188/CO.2020-0193
DANG Wen-jia, LI Zhe, LU Na, LI Yu-ting, ZHANG Lei, TIAN Xiao. Research progress of 0.9 ~ 1.0 μm near-infrared continuous-wave fiber lasers[J]. Chinese Optics, 2021, 14(2): 264-274. doi: 10.37188/CO.2020-0193
Citation: DANG Wen-jia, LI Zhe, LU Na, LI Yu-ting, ZHANG Lei, TIAN Xiao. Research progress of 0.9 ~ 1.0 μm near-infrared continuous-wave fiber lasers[J]. Chinese Optics, 2021, 14(2): 264-274. doi: 10.37188/CO.2020-0193

0.9~1.0 μm近红外连续光纤激光器的研究进展

doi: 10.37188/CO.2020-0193
基金项目: 陕西省自然科学基础研究计划资助项目(No. 2019JQ-914);陕西省创新能力支撑计划项目(No. 2019KRM093);陕西省教育厅专项科研计划项目(No. 17JK0394,No. 19JK0429);陕西省科技厅重点研发计划项目(No. 2018ZDXM-GY-051)
详细信息
    作者简介:

    党文佳(1983—),女,陕西西安人,博士,讲师,2015年于西安电子科技大学获得工学博士学位,主要从事光外差探测、光纤激光器及光电子技术等方面的研究。E-mail:wenjia_dang@126.com

  • 中图分类号: O436

Research progress of 0.9 ~ 1.0 μm near-infrared continuous-wave fiber lasers

Funds: Supported by the Natural Science Basic Research Program of Shaanxi (No. 2019JQ-914); Innovation Capability Support Program of Shaanxi (No. 2019KRM093); Scientific Research Program Funded by Shaanxi Provincial Education Department (No. 17JK0394, No. 19JK0429); Key Research and Development Program Fund of Shaanxi Science and Technology Department (No. 2018ZDXM-GY-051)
More Information
  • 摘要: 波长为0.9~1.0 μm的近红外连续光纤激光器在高功率蓝光和紫外激光产生、高功率单模泵浦源、生物医学以及激光雷达等领域具有重要的应用前景,成为近年来的一个研究热点。目前,0.9~1.0 μm光纤激光器的增益机制主要有稀土离子增益和非线性效应增益,本文详细梳理了基于这两类增益机制的0.9~1.0 μm连续光纤激光器的研究进展,并深入分析了各类激光器存在的技术瓶颈及解决途径,最后对0.9~1.0 μm光纤激光器的发展趋势和应用前景进行了展望。
  • 图  1  (a)掺钕光纤激光器系统原理图;(b)双波长泵浦掺钕光纤激光器的输出功率[13]

    Figure  1.  (a) Schematic diagram Nd-doped fiber laser; (b) output power of dual wavelength pumped Nd fiber laser[13]

    图  2  (a)实验结构示意图;(b)输出功率与注入抽运光功率的关系;(c)最高输出功率时的光谱图[26]

    Figure  2.  (a) Diagram of the experimental setup; (b) output power versus pump power; (c) spectrum at the highest output power[26]

    图  3  (a)光纤激光器示意图;(b)测量的输出功率与泵浦功率的关系;(c)不同功率下的输出光谱[39]

    Figure  3.  (a) Schematic diagram of the monolithic fiber laser; (b) measured output versus pump power; (c) measured output spectra for the double-pumped laser under various output powers[39]

    图  4  (a)光纤激光器系统结构;(b) 976 nm激光在不同功率下的输出光谱;(c) 976 nm激光输出功率[41]

    Figure  4.  (a) Configuration of the monolithic fiber laser; (b) output spectra for 976 nm laser at different average output powers; (c) output power for the 976 nm signal[41]

    图  5  (a) LD直接泵浦的全光纤拉曼激光器结构;(b)不同渐变折射率光纤长度下的拉曼光纤激光输出功率[53]

    Figure  5.  (a) All-fiber configurations of Raman fiber lasers with direct LD pumping; (b) output power of the Raman fiber laser at different GRIN fiber lengths versus input pump power[53]

    图  6  (a) LD直接泵浦的级联全光纤随机激光器;(b)二阶随机光纤激光输出功率与输入泵浦功率的关系[64]

    Figure  6.  (a) All-fiber configuration of the cascaded random fiber laser with direct LD pumping; (b) measured output power at 2nd-order random lasing wavelengths versus the input pump power[64]

    表  1  976 nm单频光纤激光器研究进展

    Table  1.   Research progress of the 976 nm single frequency fiber laser

    年份研究单位波长/nm功率/W参考文献
    2012NP Photonics9760.143
    2013University of Arizona9760.3544
    2016976445
    20179763.4146
    201897610.147
    下载: 导出CSV
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  • 收稿日期:  2020-10-27
  • 修回日期:  2020-12-09
  • 网络出版日期:  2021-03-01
  • 刊出日期:  2021-03-23

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