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中红外光学参量振荡器技术进展

李充 谢冀江 潘其坤 陈飞 何洋 张阔

李充, 谢冀江, 潘其坤, 陈飞, 何洋, 张阔. 中红外光学参量振荡器技术进展[J]. 中国光学, 2016, 9(6): 615-624. doi: 10.3788/CO.20160906.0615
引用本文: 李充, 谢冀江, 潘其坤, 陈飞, 何洋, 张阔. 中红外光学参量振荡器技术进展[J]. 中国光学, 2016, 9(6): 615-624. doi: 10.3788/CO.20160906.0615
LI Chong, XIE Ji-jiang, PAN Qi-kun, CHEN Fei, HE Yang, ZHANG Kuo. Progress of mid-infrared optical parametric oscillator[J]. Chinese Optics, 2016, 9(6): 615-624. doi: 10.3788/CO.20160906.0615
Citation: LI Chong, XIE Ji-jiang, PAN Qi-kun, CHEN Fei, HE Yang, ZHANG Kuo. Progress of mid-infrared optical parametric oscillator[J]. Chinese Optics, 2016, 9(6): 615-624. doi: 10.3788/CO.20160906.0615

中红外光学参量振荡器技术进展

doi: 10.3788/CO.20160906.0615
基金项目: 

中国科学院长春光机所创新基金资助项目 No. Y44222C150

吉林省科技发展计划资助项目 No.20140203010GX

详细信息
    作者简介:

    李充(1992-),女,吉林长春人,硕士研究生,2014年于吉林大学获得学士学位,主要从事中红外固体激光器方面的研究。E-mail:18843109663@163.com

    通讯作者:

    谢冀江(1959—),男,江苏镇江人,学士,研究员,硕士生导师,1983 年于哈尔滨科学技术大学获得学士学位,主要从事激光器及其应用技术方面的研究。E-mail:laserxjj@163.com

  • 中图分类号: TN248.1

Progress of mid-infrared optical parametric oscillator

Funds: 

Supported by Innovation foundation Project of CIOMP,CAS No. Y44222C150

Jilin provincial Science and Technology Development Project No.20140203010GX

More Information
  • 摘要: 3~5 μm中红外激光器在环境污染检测、医疗、工业等领域具有重要的应用价值。本文总结了基于ZnGeP2、MgO∶PPLN晶体的光参量振荡器(OPO)的国内外发展现状,分析了其各自不同结构系统设计的优势和发展前景。指出高功率、小体积、轻重量的光学参量振荡器是未来重要发展方向,发展的技术核心是生长更大尺寸的中红外激光晶体以及研制更高性能指标的OPO泵浦源,并对中红外激光器的发展趋势进行了展望。
  • 图  1  Nd:YAG泵浦级联KTP和ZGP

    Figure  1.  Cascaded KTP and ZGP pumped by Nd:YAG

    图  2  Ho:YAG泵浦的ZGP-OPO

    Figure  2.  ZGP-OPO pumped by Ho:YAG

    图  3  2.09 μm调Q钬激光泵浦ZGP-OPO

    Figure  3.  ZGP-OPO pumped by Q-switch Ho laser at 2.09 μm

    图  4  Ho:YAG激光器泵浦四镜环形腔OPO

    Figure  4.  Four-mirror ring cavity OPO pumped by Ho:YAG laser

    图  5  掺Tm3+光纤激光器泵浦的ZGP-OPO

    Figure  5.  ZGP-OPO pumped by Tm3+ doped fiber

    图  6  二极管泵浦调Q Tm:YAG晶体泵浦ZGP

    Figure  6.  ZGP pumped by diode-pumped Q-switch Tm:YAG

    图  7  调Q掺Tm3+光纤激光器泵浦单通双谐振OPO

    Figure  7.  Single pass double resonant OPO pumped by Q-switch Tm3+ doped fiber laser

    图  8  Yb光纤激光器泵浦四镜环形腔OPO

    Figure  8.  Four-mirror ring cavity OPO pumped by Yb fiber laser

    图  9  光纤激光器泵浦DPSR型OPO实验原理图

    Figure  9.  DPSR OPO pumped by fiber laser

    图  10  声光调Q固体激光器泵浦MgO:PPLN-OPO实验装置

    Figure  10.  MgO:PPLN-OPO pumped by Q-switch solid lasser

    图  11  1.06 μm连续泵浦V形PPLN-OPO实验装置

    Figure  11.  Schematic diagram of V cavity PPLN-OPO pumped by CW-laser at 1.06 μm

    图  12  高功率1.06 μm激光泵浦单谐PPLN-OPO结构图

    Figure  12.  Schematic diagram of single-oscillator PPLN-OPO pumped by high power 1.06 μm laser

    图  13  跨周期参量光输出的多参量振荡器实验装置图

    Figure  13.  Schematic diagram of multi-OPO output crossing periods

    表  1  光纤激光器泵浦中红外PPLN-OPO国内外研究现状

    Table  1.   Development of mid-infrared PPLN-OPO pumped by fiber laser at home and abroad

    年份研究单位泵浦源参数晶体尺寸中红外输出参数
    2008年University of Helsinki1 064 nmMgO:PPLN2.7~3.45 μm
    光纤激光器50 mm×1 mm瓦级的中红外输出[28]
    20 W
    2010年E.L.Ginzton Laboratory,Yb光纤激光器PPLN3.8 μm附近1.8~2W[29]
    Stanford University20 W50 mm
    2010年ICFO-Institut de Yb光纤激光MgO:PPLN3.07 μm闲频光9.8 W,M2<1.28
    Ciencies Fotoniques30 W50 mm×1 mm光-光转换效率61%[30]
    2014年山东大学Yb光纤激光器MgO:PPLN3.8 μm处1 W
    20 W多极化周期光-光转换效率高于10%
    50 mm×1 mm 波长可调谐[31]
    2014年浙江大学线偏振脉冲YDFLMgO:PPLN3.83 μm处3.3 W
    平均25 W50 mm×1 mm×10 mmM2为1.98和1.44[27]
    下载: 导出CSV
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  • 收稿日期:  2016-06-17
  • 修回日期:  2016-07-28
  • 刊出日期:  2016-12-01

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