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新型过渡金属硫化物在超快激光中的应用

孙俊杰 陈飞 何洋 丛春晓 曲家沂 季艳慧 鲍赫

孙俊杰, 陈飞, 何洋, 丛春晓, 曲家沂, 季艳慧, 鲍赫. 新型过渡金属硫化物在超快激光中的应用[J]. 中国光学, 2020, 13(4): 647-659. doi: 10.37188/CO.2019-0241
引用本文: 孙俊杰, 陈飞, 何洋, 丛春晓, 曲家沂, 季艳慧, 鲍赫. 新型过渡金属硫化物在超快激光中的应用[J]. 中国光学, 2020, 13(4): 647-659. doi: 10.37188/CO.2019-0241
SUN Jun-jie, CHEN Fei, HE Yang, CONG Chun-xiao, QU Jia-yi, JI Yan-hui, BAO He. Application of emerging transition metal dichalcogenides in ultrafast lasers[J]. Chinese Optics, 2020, 13(4): 647-659. doi: 10.37188/CO.2019-0241
Citation: SUN Jun-jie, CHEN Fei, HE Yang, CONG Chun-xiao, QU Jia-yi, JI Yan-hui, BAO He. Application of emerging transition metal dichalcogenides in ultrafast lasers[J]. Chinese Optics, 2020, 13(4): 647-659. doi: 10.37188/CO.2019-0241

新型过渡金属硫化物在超快激光中的应用

doi: 10.37188/CO.2019-0241
基金项目: 国家重点研发计划资助项目(No.2016YFB0500100;No.2018YFE0203203);国家自然科学基金面上项目(No. 61975203);中科院青年创新促进会(No. 2017259);民用航天预研项目(No. D040101)
详细信息
    作者简介:

    孙俊杰(1994—),女,吉林长春人,硕士,研究实习员,2015年于武汉大学获得学士学位,2017年于国防科技大学获得硕士学位,主要从事新型激光技术方面的研究。E-mail:15143115236@163.com

    陈 飞(1982—),男,河南南阳人,博士,研究员,博士生导师,2005年于长春理工大学获得学士学位,2007年于哈尔滨工业大学获得硕士学位,2011年于哈尔滨工业大学获得博士学位,主要从事激光技术及应用方面的研究。E-mail:feichenny@126.com

  • 中图分类号: TN248

Application of emerging transition metal dichalcogenides in ultrafast lasers

Funds: Supported by National Key R&D Program of China (No. 2016YFB0500100; No. 2018YFE0203203); National Natural Science Foundation of China (No. 61975203); Youth Innovation Promotion Association of CAS (No. 2017259); Civil Aerospace Pre-research Project (No. D040101)
More Information
  • 摘要: 超快激光技术是目前激光乃至物理学和信息科学领域最活跃的研究前沿之一,在工业加工、生物医学和激光雷达等领域具有广泛应用。二维材料具有独特的物理结构及优异的光电特性,作为可饱和吸收体应用于超快激光器时,具备工作波段宽、调制深度可控和恢复时间快等优势。其中,过渡金属硫化物因具有带隙连续可调等特点,已成为二维材料研究领域的重点。本文从过渡金属硫化物的特性出发,介绍了可饱和吸收器件的制作方法,综述了基于新型过渡金属硫化物的超快激光器的研究进展,并对其发展趋势进行了展望。
  • 图  1  典型TMD图像。(a)光学图像;(b)扫描电镜图像;(c)原子力显微镜图像;(d、e)低倍、高倍透射电镜图像[40]

    Figure  1.  Typical images of TMD. (a) Optical image. (b) SEM image. (c) AFM image. (d, e) Low- and high-magnification TEM images

    图  2  TMD可饱和吸收体转移示意图

    Figure  2.  Schematic diagram of transfer for TMD saturable absorber

    图  3  基于ReS2可饱和吸收体的固体激光器装置图

    Figure  3.  Solid-state laser setup based on ReS2 saturable absorber

    图  4  基于ReS2可饱和吸收体的光纤激光器装置示意图

    Figure  4.  Schematic of fiber laser setup based on ReS2 saturable absorber

    表  1  基于新型TMD可饱和吸收体的超快固体激光器

    Table  1.   Ultrafast solid-state lasers with emerging TMD saturable absorbers

    TMD饱和能量调制深度调制方式增益介质中心波长重复频率脉冲宽度单脉冲能量/平均功率参考
    文献
    ReS222.6 μJ/cm29.7%调QEr:YSGG2.8 μm126 kHz324 ns104 mW[69]
    58.2 μJ/cm2 21.5 μJ/cm2 2.7 μJ/cm23%
    5.2%
    2.9%
    调Q/锁模Pr:YLF、
    Nd:YAG、
    Tm:YAP
    调Q:0.64 μm、1.064 μm、1.991 μm,锁模:
    1.06 μm
    调Q:520 kHz、644 kHz、67.7 kHz,锁模:
    50.7 MHz
    调Q:160 ns、139 ns、415 ns,锁模:323 fs调Q:0.625 W、1.34 W、8.72 W,锁模:350 mW
    11.89 GW/cm248%调QNd:YAG0.95 μm/
    1.06 μm
    165 kHz834 ns81 mW[70]
    23.5 μJ/cm210.2%调QHo,Pr:LiLuF42.95 μm91.5 kHz676 ns1.13 μJ[44]
    15.6 μJ/cm215%调QNd:YAG1.3 μm214 kHz403 ns0.42 μJ[71]
    PtSe217.1 μJ/cm212.6%锁模Nd:LuVO41066 nm61.3 MHz15.8 ps180 mW[72]
    3.2 μJ/cm26.6%调QTm:YAP1 987 nm58 kHz244 ns24.3 μJ[73]
    0.47 GW/cm21.9%调Q锁模Nd:YAG1064 nm8.8 GHz27 ps127 mW[74]
    ReSe2调QTm:YLF/Tm:Y2O31 900 nm/
    2050 nm
    54 kHz/
    106 kHz
    527.9 ns/
    727 ns
    862 mW/
    1.04 W
    [75]
    12.8 GW/cm22.9%调QNd:Y3Al5O121.06 μm274 MHz1.08 μs2.5 μJ[76]
    14.5 μJ/cm27.5%调QEr:YAP2.73 μm/
    2.8 μm
    244.6 kHz202.8 ns526 mW[77]
    12.8 GW/cm22.9%锁模固体波导1064 nm6.5 GHz29 ps250 mW[78]
    6.37 MW/cm21.89%调QNd:YVO41064.4 nm84.16 kHz682 ns125 mW[79]
    4.3 μJ/cm27.3%调QTm:YAP2 μm89.4 kHz925.8 ns17.6 μJ[46]
    MoTe20.14 mJ/cm222%调QHo,Pr:LiLuF42.95 μm76.46 kHz670 ns0.95 μJ[80]
    1.71 MW/cm2调QYb:LaCa4O(BO3)31.03~1.04 μm357 kHz103 ns6.6 μJ[81]
    18 MW/cm24%调QTm:CaYAlO41 929 nm70.9 kHz0.69 μs10.58 μJ[82]
    6.87 mJ/cm21.3%调QEr:YAG1645 nm41.59 kHz1.048 μs27.4 μJ[83]
    2.26 μJ/cm26.0%调QTm:YAP2 μm144 kHz380 ns8.4 μJ[84]
    1.71 MW/cm20.9%调QYb:YCOB1.03 μm704 kHz52 ns2.25 μJ[85]
    1.71 MW/cm20.9%调QYb:KLu(WO4)21030.6 nm2.18 MHz36 ns1.3 μJ[86]
    WTe25.1 μJ/cm27.2%调QTm:YAP1 938 nm78 kHz368 ns4.8 μJ[87]
    1.97 mJ/cm220.9%调QHo,Pr:LiLuF42 954.7 nm92 kHz366 ns1.4 μJ[88]
    TiS23.37 mJ/cm28%调QEr:YAG1645 nm38 kHz1.2 μs37.4 μJ[89]
    下载: 导出CSV

    表  2  基于新型TMD可饱和吸收体的超快光纤激光器

    Table  2.   Ultrafast fiber lasers with emerging TMD saturable absorbers

    TMD饱和能量调制深度调制方式光纤掺杂中心波长重复频率脉冲宽度单脉冲能量/平均功率参考
    文献
    ReS227 μJ/cm21%锁模Er1564 nm3.43 MHz1.25 ps[91]
    74 MW /cm20.12%调Q/锁模Er1558.6 nm12.6~19 kHz/
    5.48 MHz
    23~5.49 μs/1.6 ps22~62.8 μJ[92]
    锁模Er1.5 μm1.896 MHz12 mW[93]
    8.4 MW/cm244%调QYb1047 nm134 kHz1.56 μs13.02 nJ[94]
    27.5 μJ/cm26.9%锁模Er1573.6 nm/
    1591.1 nm/
    1592.6 nm
    13.39 MHz[95]
    PtSe20.346 GW/cm226%锁模Yb1064.47 nm4.08 MHz470 ps2.31 nJ[96]
    9.48 MW/cm26.9%锁模Er1550 nm8.24 MHz861 fs78.52 nJ[45]
    0.34~1.23 GW/cm21.11%~4.9%调Q/锁模Er1560 nm锁模:23.3 MHz锁模:1.02 ps调Q:143.2 nJ
    锁模:0.53 nJ
    [97]
    ReSe2调QYb1.06 μm17.89~39.86 kHz2.27 μs30.4 nJ[98]
    3.9%锁模Er1560 nm14.97 MHz862 fs0.5 mW[99]
    7%调QEr1566 nm16.64 kHz4.98 μs36 nJ[100]
    MoTe23.46 MW/cm248.85%锁模Er1559 nm1.8 MHz2.46 ps0.11 mW[101]
    0.969 MW/cm226.97%锁模Er1561 nm96.323 MHz111.9 fs23.4 mW[102]
    26.45 MW/cm217.47%调QEr1559 nm148~228 kHz677 ns109 nJ[103]
    8.3 MW /cm25.7%锁模Tm1 930 nm14.353 MHz952 fs2.56 nJ[47]
    9.6 MW/cm2@
    1.5 μm、12.3 MW/cm2@2 μm
    25.5%@1.5 μm、22.1%@
    2 μm
    锁模Er/Tm1.5 μm/2 μm25.601 MHz/
    15.37 MHz
    229 fs/1.3 ps2.14 nJ/13.8 nJ[104]
    WTe27.6 MW/cm231%锁模Tm1915.5 nm18.72 MHz1.25 ps39.9 mW[48]
    2.18%调QYb1044 nm19~79 kHz1 μs28.3 nJ[105]
    0.515 MW/cm231.06%调QEr1531 nm144.7~240 kHz583 ns58.625 nJ[106]
    TiS28.3%锁模/调QEr1563.3 nm/
    1560.2 nm
    22.7 MHz/
    33.387 kHz
    1.25 ps/4.01 μs25.3 pJ/9.5 nJ[107]
    772.2 GW /cm2锁模Er1550 nm5.7 MHz618 fs0.28~1.2 mW[49]
    下载: 导出CSV
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  • 收稿日期:  2019-12-17
  • 修回日期:  2020-02-07
  • 刊出日期:  2020-08-01

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