0.9~1.0 μm近红外连续光纤器的研究进展 -

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0.9~1.0 μm近红外连续光纤器的研究进展

doi:10.37188/CO.2020-0193

党文佳^1,,,
李哲^{2, 3},
卢娜¹,
李玉婷¹,
张蕾¹,
田晓¹

1.
西安航空学院理学院，陕西西安 710077
2.
中国科学院西安光学精密机械研究所瞬态光学与光子技术国家重点实验室，陕西西安 710119
3.
中国科学院大学，北京 100049

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
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出版历程
- 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

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

DANG Wen-jia^1,,,
LI Zhe^{2, 3},
LU Na¹,
LI Yu-ting¹,
ZHANG Lei¹,
TIAN Xiao¹

1.
School of Science, Xi’an Aeronautical University, Xi’an 710077, China
2.
State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
3.
University of Chinese Academy of Sciences, Beijing 100049, China

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)

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Corresponding author:wenjia_dang@126.com

摘要

摘要:波长为0.9~1.0 μm的近红外连续光纤器在高功率蓝光和紫外产生、高功率单模泵浦源、生物医学以及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连续光纤器的研究进展，并深入分析了各类器存在的技术瓶颈及解决途径，最后对0.9~1.0 μm光纤器的发展趋势和应用前景进行了展望。
- 光纤器/
- 0.9~1.0 μm近红外/
- 稀土离子增益/
- 非线性效应增益
Abstract:Near-infrared continuous-wave fiber lasers with wavelengths of 0.9~1.0 μm have important application prospects in the fields of high-power blue and ultraviolet laser generation, high-power single-mode pump sources, biomedicine and lidars. They have thus become a heavily researched topic in recent years. At present, their gain mechanisms mainly include a rare earth ion gain or a nonlinear effect gain. In this paper, the research progress of 0.9~1.0 μm fiber lasers based on these two kinds of gain mechanisms are reviewed in detail, and the technical bottlenecks and solutions of these lasers are analyzed. Furthermore, the potential directions for the future of their research are proposed.
- fiber laser/
- near-infrared laser with a wavelength of 0.9~1.0 μm/
- rare earth ion gain/
- nonlinear effect gain

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图 1（a）掺钕光纤器系统原理图；（b）双波长泵浦掺钕光纤器的输出功率^[13]

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

下载: 全尺寸图片幻灯片

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]

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图 3（a）光纤器示意图；（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]

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图 4（a）光纤器系统结构；（b） 976 nm 在不同功率下的输出光谱；（c） 976 nm 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]

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

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图 6（a） LD直接泵浦的级联全光纤随机器；（b）二阶随机光纤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]

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表 1976 nm单频光纤器研究进展

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
2012	NP Photonics	976	0.1	43
2013	University of Arizona	976	0.35	44
2016		976	4	45
2017		976	3.41	46
2018		976	10.1	47

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参考文献 (64)

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