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532 nm皮秒脉冲激光对单晶硅的损伤特性研究

王佳敏 季艳慧 梁志勇 陈飞 郑长彬

王佳敏, 季艳慧, 梁志勇, 陈飞, 郑长彬. 532 nm皮秒脉冲激光对单晶硅的损伤特性研究[J]. 中国光学(中英文), 2022, 15(2): 242-250. doi: 10.37188/CO.2021-0160
引用本文: 王佳敏, 季艳慧, 梁志勇, 陈飞, 郑长彬. 532 nm皮秒脉冲激光对单晶硅的损伤特性研究[J]. 中国光学(中英文), 2022, 15(2): 242-250. doi: 10.37188/CO.2021-0160
WANG Jia-min, JI Yan-hui, LIANG Zhi-yong, CHEN Fei, ZHENG Chang-bin. Damage characteristics of a 532 nm picosecond pulse laser on monocrystalline silicon[J]. Chinese Optics, 2022, 15(2): 242-250. doi: 10.37188/CO.2021-0160
Citation: WANG Jia-min, JI Yan-hui, LIANG Zhi-yong, CHEN Fei, ZHENG Chang-bin. Damage characteristics of a 532 nm picosecond pulse laser on monocrystalline silicon[J]. Chinese Optics, 2022, 15(2): 242-250. doi: 10.37188/CO.2021-0160

532 nm皮秒脉冲激光对单晶硅的损伤特性研究

基金项目: 国家重点研发计划资助项目(No. 2018YFE0203203);中国科学院创新交叉团队(No. JCTD-2020-13);中科院长春光机所重大创新项目(No. E10302Y3M0)
详细信息
    作者简介:

    王佳敏(1995—),女,内蒙古呼和浩特人,博士研究生,2018年于内蒙古大学获得学士学位,主要从事激光辐照效应方面的研究。E-mail: wangjiamin18@mails.ucas.ac.cn

    郑长彬(1981—),男,黑龙江富锦人,博士,副研究员,2005年于吉林大学获得硕士学位,2011年于哈尔滨工业大学获得博士学位,主要从事激光辐照效应方面的研究。E-mail:zhengchangbin@ciomp.ac.cn

  • 中图分类号: TN249

Damage characteristics of a 532 nm picosecond pulse laser on monocrystalline silicon

Funds: Supported by National Key R&D Program Funded Project (No. 2018YFE0203203); Innovative Cross Team of the Chinese Academy of Sciences (No. JCTD-2020-13); Major Innovation Project of Changchun Institute of Optics and Mechanics, Chinese Academy of Sciences (No. E10302Y3M0)
More Information
  • 摘要: 随着光电对抗和超短脉冲激光技术的发展,研究超短脉冲激光与单晶硅相互作用具有非常重要的理论和实际意义。为了进一步明确532 nm皮秒脉冲激光对单晶硅的损伤机理,本文开展了532 nm皮秒脉冲激光辐照单晶硅的损伤效应实验研究,测定了损伤阈值,明确了损伤机理,探讨了低通量下的脉冲累积效应。首先,利用波长为532 nm、脉冲宽度为30 ps的激光器和金相显微镜,基于1-on-1的激光损伤测试方法,测定了单晶硅的零损伤概率阈值为0.52 J/cm2;其次,研究了皮秒激光辐照单晶硅在不同激光能量密度下的损伤形貌,发现532 nm皮秒脉冲激光对单晶硅的损伤表现为热影响损伤和等离子体冲击损伤,随着激光能量密度的增大,按主要的损伤机制可将损伤程度分为:热影响(0.52~3 J/cm2)、热烧蚀(3~50 J/cm2)和等离子烧蚀(>50 J/cm2),且不同情况下,损伤面积随激光能量密度分别对应不同的增长规律;最后,研究了低通量下多脉冲的累积效应,发现在0.52 J/cm2的激光能量密度下,连续辐照16个脉冲时表面形成热影响区,验证了多脉冲的累积效应可以降低单晶硅的激光损伤阈值。

     

  • 图 1  皮秒激光诱导损伤实验装置图

    Figure 1.  Schematic diagram of the picosecond laser induced damage experiment setup

    图 2  损伤区域尺寸随激光能量密度的变化规律

    Figure 2.  The size of the damaged area changes with the laser’s energy density

    图 3  不同能量密度下损伤形貌图

    Figure 3.  Damage morphography at different energy densities

    图 4  302 J/cm2能量密度的损伤形貌图

    Figure 4.  Damage morphography at the energy density of 302 J/cm2

    图 5  能量密度为21.9 J/cm2的损伤形貌图

    Figure 5.  Damage morpography at the energy density of 21.9 J/cm2

    图 6  能量密度为3.04 J/cm2的损伤形貌图

    Figure 6.  Damage morphography at the energy density of 3.04 J/cm2

    图 7  能量密度为0.52、1.07 J/cm2时脉冲累积效应的损伤形貌

    Figure 7.  Damage morphography from the pulse accumulation effect at the energy densities of 0.52 J/cm2、1.07 J/cm2

    图 8  烧蚀区域尺寸随脉冲数量的变化规律

    Figure 8.  Variation of the ablation zone size with the number of pulses

    图 9  脉冲累积效应的损伤形貌

    Figure 9.  Damage morphology from the pulse accumulation effect

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出版历程
  • 收稿日期:  2021-08-16
  • 修回日期:  2021-09-24
  • 录用日期:  2021-11-18
  • 网络出版日期:  2021-11-18
  • 刊出日期:  2022-03-21

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