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连续/脉冲复合体制高功率固体激光技术研究

刘磊 王文涛 王超 王钢 刘洋 贾佑权 李宁 吕坤鹏 陈露

刘磊, 王文涛, 王超, 等. 连续/脉冲复合体制高功率固体激光技术研究[J]. 强激光与粒子束, 2022, 34: 031007. doi: 10.11884/HPLPB202234.210292
引用本文: 刘磊, 王文涛, 王超, 等. 连续/脉冲复合体制高功率固体激光技术研究[J]. 强激光与粒子束, 2022, 34: 031007. doi: 10.11884/HPLPB202234.210292
Liu Lei, Wang Wentao, Wang Chao, et al. High power solid state laser operating in continuous / pulse composite mode[J]. High Power Laser and Particle Beams, 2022, 34: 031007. doi: 10.11884/HPLPB202234.210292
Citation: Liu Lei, Wang Wentao, Wang Chao, et al. High power solid state laser operating in continuous / pulse composite mode[J]. High Power Laser and Particle Beams, 2022, 34: 031007. doi: 10.11884/HPLPB202234.210292

连续/脉冲复合体制高功率固体激光技术研究

doi: 10.11884/HPLPB202234.210292
基金项目: 中国电科创新基金项目
详细信息
    作者简介:

    刘 磊,cetc11_liulei@sina.com

    通讯作者:

    王文涛,wwntao@163.com

  • 中图分类号: TN241

High power solid state laser operating in continuous / pulse composite mode

  • 摘要: 常规高功率激光器以连续或者长脉冲方式工作,与物质作用主要是依靠单一“加热”模式,针对其对复杂目标作用能力有限的问题, 提出一种连续和脉冲激光同时输出,脉宽、重频可调的新体制高功率激光技术,激光放大链路以特殊时域模式工作,即高重频脉冲与连续运转同时输出,在重频10 kHz时,实现输出功率4800 W,其中连续激光功率3600 W,脉冲激光功率1200 W,脉冲宽度为3.6 ns;在重频100 kHz时,实现输出功率4920 W,其中连续激光功率3100 W,脉冲激光功率1820 W,脉冲宽度为7 ns,光束质量4.8倍衍射极限 。
  • 图  1  5 kW连续/脉冲高功率激光器实验装置示意图

    Figure  1.  5 kW continuous / pulse high power laser experimental device structure

    图  2  不同泵浦光通量下小信号增益系数随长度的变化

    Figure  2.  Small signal gain coefficient varies with length under different pump power

    图  3  单程和双程输出能量密度计算模型

    Figure  3.  Calculation model of one-way and two-way output energy density

    图  4  连续/脉冲复合激光输出时功率变化情况

    Figure  4.  Continuous / pulse composite laser output

    图  5  10 kHz时纯脉冲与连续/脉冲的激光脉冲

    Figure  5.  Laser pulse in pulse and continuous / pulse operation at 10 kHz

    图  6  100 kHz时纯脉冲与连续/脉冲的激光脉冲

    Figure  6.  Laser pulse in pulse and continuous / pulse operation at 100 kHz

  • [1] Kerse C, Kalaycıoğlu H, Elahi P, et al. Ablation-cooled material removal with ultrafast bursts of pulses[J]. Nature, 2016, 537(7618): 84-88. doi: 10.1038/nature18619
    [2] Liang Liang, Yuan Jiandong, Lin Guozhi. Effect of the scanning speed on the microgroove formation regime in nanosecond-pulsed laser scanning ablation of cermet[J]. Int J Adv Manuf Technol, 2020, 107(1/2): 97-107.
    [3] Fazeli R. Enhanced X-ray emission from laser-produced gold plasma by double pulses irradiation of nano-porous targets[J]. Phys Lett A, 2017, 381(5): 467-471. doi: 10.1016/j.physleta.2016.11.024
    [4] Schmidt B E, Hage A, Mans T, et al. Highly stable, 54 mJ Yb-InnoSlab laser platform at 0.5 kW average power[J]. Opt Express, 2017, 25(15): 17549-17555. doi: 10.1364/OE.25.017549
    [5] Reagan B A, Baumgarten C, Jankowska E, et al. Scaling diode-pumped, high energy picosecond lasers to kilowatt average powers[J]. High Power Laser Sci Eng, 2018, 6: 01000e11.
    [6] Sun L C, Liu T H, Fu X, et al. 1.57 times diffraction-limit high-energy laser based on a Nd: YAG slab amplifier and an adaptive optics system[J]. Chin Opt Lett, 2019, 17: 051403. doi: 10.3788/COL201917.051403
    [7] W. 克希耐尔. 固体激光工程[M]. 孙文, 江泽文, 程国祥, 译. 北京: 科学出版社, 2002

    Koechner W. Solid-state laser engineering[M]. Sun Wen, Jiang Zewen, Cheng Guoxiang, trans. Beijing: Science Press, 2002
    [8] 周炳琨, 高以智, 陈倜嵘, 等. 激光原理[M]. 4版. 北京: 国防工业出版社, 2000.

    Zhou Bingkun, Gao Yizhi, Chen Tirong, et al. The principle of laser[M]. 4th edition. Beijing: National Defense Industry Press, 2000.
    [9] Klimek D E, Mandl A. Nd: YAG ceramic ThinZag high-power laser development[M]//Injeyan H, Goodno G D. High-power laser handbook. New York: McGraw-Hill, 2011: 207-223.
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  • 被引次数: 0
出版历程
  • 收稿日期:  2021-07-15
  • 修回日期:  2021-11-25
  • 网络出版日期:  2021-12-07
  • 刊出日期:  2022-01-13

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