Turn off MathJax
Article Contents
ZHOU Tian-chen, LI Ke-xue, CHEN Yi, ZHANG Xin, YU Jing-hua, ZHANG Yi-wen, SUN Jun-jie, CHEN Fei, WANG Xiao-hua, WEI Zhi-peng. Research progress on high-power, high-beam-quality short-pulse/ultrashort-pulse solid-state green laser technology[J]. Chinese Optics. doi: 10.37188/CO.2025-0050
Citation: ZHOU Tian-chen, LI Ke-xue, CHEN Yi, ZHANG Xin, YU Jing-hua, ZHANG Yi-wen, SUN Jun-jie, CHEN Fei, WANG Xiao-hua, WEI Zhi-peng. Research progress on high-power, high-beam-quality short-pulse/ultrashort-pulse solid-state green laser technology[J]. Chinese Optics. doi: 10.37188/CO.2025-0050

Research progress on high-power, high-beam-quality short-pulse/ultrashort-pulse solid-state green laser technology

cstr: 32171.14.CO.2025-0050
Funds:  National Key R&D Program of China (No. 2023YFB4604400), the National Natural Science Foundation of China (No. 62434001, 62027820), the Science and Technology Development Project of Jilin Province (No. SKL202402019), the Natural Science Foundation of Jilin Province (No. 20230101352JC), the “111” Project of China (No. D17017).
More Information
  • High-power, high-beam-quality short-pulse/ultrashort-pulse green lasers have wide applications in industry, medicine, and scientific research. To clarify the research progress of green light sources based on second-harmonic generation (SHG, frequency doubling), this paper systematically reviews the latest advancements in SHG green light sources at kilohertz repetition rates, categorized by pulse width and doubling scheme into four types: nanosecond intracavity doubling, nanosecond extracavity doubling, picosecond extracavity doubling, and femtosecond extracavity doubling. For nanosecond intracavity doubling, crystals such as KTP and LBO are used, with power increased to 51.1 W (energy 50 mJ, repetition rate 1 kHz) and efficiency of 50%. Nanosecond extracavity doubling primarily employs LBO, where tandem frequency-doubling crystals can elevate the doubling power to 1.04 kW (energy 1.04 J, efficiency 89%). Picosecond extracavity doubling achieves the highest average power of 1460 W (energy 259 mJ, efficiency 71%). Femtosecond doubling, by employing thin crystals, boosts power to 29 W (energy 440 μJ, efficiency >52%). The advancements in SHG-based green light sources and related application technologies will continually expand their boundaries in scientific research, industry, medicine, and other fields.

     

  • loading
  • [1]
    WU Y, WU H P, WANG Y, et al. 1.21-W 532-nm picosecond green laser generated by second-harmonic generation using K3B6O10Cl as a nonlinear optical crystal[J]. Optical Engineering, 2018, 57(6): 066112. doi: 10.1117/1.oe.57.6.066112
    [2]
    DING X, WANG R, ZHANG H, et al. Generation of 3.5W high efficiency blue-violet laser by intracavity frequency-doubling of an all-solid-state tunable Ti: sapphire laser[J]. Optics Express, 2008, 16(7): 4582-4587. doi: 10.1364/oe.16.004582
    [3]
    FAN ZH W, LIU X P, ZHANG ZH P, et al. 10 kHz repetition rate picosecond green laser for high-accuracy satellite ranging[J]. Frontiers in Physics, 2023, 10: 1115330. doi: 10.3389/fphy.2022.1115330
    [4]
    LEONE C, LOPRESTO V, DE IORIO I. Wood engraving by Q-switched diode-pumped frequency-doubled Nd: YAG green laser[J]. Optics and Lasers in Engineering, 2009, 47(1): 161-168. doi: 10.1016/j.optlaseng.2008.06.019
    [5]
    BREDILLET K, RIPORTO F, GUO T, et al. Dual second harmonic generation and up-conversion photoluminescence emission in highly-optimized LiNbO3 nanocrystals doped and co-doped with Er3+ and Yb3+[J]. Nanoscale, 2024, 16(13): 6739-6747. doi: 10.1039/D4NR00431K
    [6]
    ZHANG A N, WANG Y P, LI ZH L, et al. Concept for power scaling by harmonic beam coaxial combination in an intra-cavity frequency doubling laser[J]. Optics Letters, 2024, 49(16): 4669-4672. doi: 10.1364/OL.531047
    [7]
    HUBKA Z, ANTIPENKOV R, BOGE R, et al. 120 mJ, 1 kHz, picosecond laser at 515 nm[J]. Optics Letters, 2021, 46(22): 5655-5658.
    [8]
    JI B, ZHENG X S, CAI Z P, et al. Compact high conversion efficiency Nd: YAG/LBO green laser using unstable V cavity[J]. Laser Physics, 2012, 22(2): 406-410. doi: 10.1134/S1054660X12020119
    [9]
    SHEN J P, HUANG X, XU SH C, et al. High average power green laser based on LED-side-pumped Q-switched Nd: YAG laser[J]. IEEE Photonics Technology Letters, 2023, 35(13): 721-724. doi: 10.1109/LPT.2023.3274576
    [10]
    LIU Q, YAN X P, GONG M L, et al. 103W high beam quality green laser with an extra- cavity second harmonic generation[J]. Optics Express, 2008, 16(19): 14335-14340. doi: 10.1364/OE.16.014335
    [11]
    BAER T. Large-amplitude fluctuations due to longitudinal mode coupling in diode-pumped intracavity-doubled Nd: YAG lasers[J]. Journal of the Optical Society of America B, 1986, 3(9): 1175-1180. doi: 10.1364/JOSAB.3.001175
    [12]
    JIANG SH B, WANG Q, JIANG L J, et al. Frequency-doubled short nanosecond fiber lasers for glass drilling and grinding[J]. International Journal of Applied Ceramic Technology, 2022, 19(3): 1208-1213. doi: 10.1111/ijac.13994
    [13]
    KHRIPUNOV S, KOBTSEV S, RADNATAROV D. Efficiency of different methods of extra-cavity second harmonic generation of continuous wave single-frequency radiation[J]. Applied Optics, 2016, 55(3): 502-506. doi: 10.1364/AO.55.000502
    [14]
    BAI S C, DONG J. GTR-KTP enhanced stable intracavity frequency doubled Cr, Nd: YAG self-Q-switched green laser[J]. Laser Physics, 2015, 25(2): 025002. doi: 10.1088/1054-660X/25/2/025002
    [15]
    FU Q, ZHANG X Y, LIU ZH J, et al. An efficient frequency-doubled Nd: KLu(WO4)2 laser at 535 nm[J]. Optics & Laser Technology, 2016, 77: 193-197. doi: 10.1016/j.optlastec.2015.09.026
    [16]
    CHANG J H, YANG ZH B, LI H H, et al. Passively Q-switched Nd: YVO4/PPLN green laser with a few-layered MoS2 saturable absorber[J]. Optical Review, 2017, 24(6): 765-771. doi: 10.1007/s10043-017-0380-5
    [17]
    孙瑛璐, 段延敏, 程梦瑶, 等. 自拉曼混频黄绿波段三波长可切换激光[J]. 物理学报, 2020, 69(12): 124201. doi: 10.7498/aps.69.20200324

    SUN Y L, DUAN Y M, CHENG M Y, et al. Triple wavelength-switchable lasing in yellow-green based on frequency mixing of self-Raman operation[J]. Acta Physica Sinica, 2020, 69(12): 124201. (in Chinese). doi: 10.7498/aps.69.20200324
    [18]
    DUAN Y M, SUN Y L, ZHU H Y, et al. YVO4 cascaded Raman laser for five-visible-wavelength switchable emission[J]. Optics Letters, 2020, 45(9): 2564-2567. doi: 10.1364/OL.392566
    [19]
    SHILOVA G V, ZVEREV P G, SIROTKIN A A. Diode pumped Nd: YVO4/LBO/Ba(NO3)2 Raman laser at 563 nm[J]. Laser Physics Letters, 2020, 17(6): 065801. doi: 10.1088/1612-202X/ab8932
    [20]
    SONG M Y, CHOO H T, CHOI J H. Operational characteristics of the doubly Q-switched Nd: YAG laser and intra-cavity frequency doubled laser[J]. New Physics: Sae Mulli, 2022, 72(3): 245-251. doi: 10.3938/npsm.72.245
    [21]
    PANG Y J, XUE R X, LU W, et al. Intracavity frequency doubling acousto-optic Q-switched high repetition rate high-energy Nd: YLF laser[J]. Applied Optics, 2024, 63(6): 1572-1576. doi: 10.1364/AO.516321
    [22]
    WU ZH CH, ZHANG X L. High power 100 kHz electro-optic cavity empty green laser[J]. Optik, 2019, 178: 25-28. doi: 10.1016/j.ijleo.2018.10.051
    [23]
    ZHU J Q, XIE X L, SUN M ZH, et al. Analysis and construction status of SG-II 5PW laser facility[J]. High Power Laser Science and Engineering, 2018, 6: e29. doi: 10.1017/hpl.2018.23
    [24]
    CHI H, WANG Y, DAVENPORT A, et al. Demonstration of a kilowatt average power, 1 J, green laser[J]. Optics Letters, 2020, 45(24): 6803-6806. doi: 10.1364/OL.412975
    [25]
    CHA Y H, KIM Y, PARK H, et al. 80-W dual-wavelength green pulsed laser based on a Yb-doped rod-type fiber amplifier[J]. Applied Physics B, 2021, 127(5): 78. doi: 10.1007/s00340-021-07628-3
    [26]
    CHA Y H, CHUN B, PARK H. 40-W 352-nm single-frequency nanosecond pulsed rod-type fiber laser[J]. Journal of the Korean Physical Society, 2023, 82(12): 1157-1162. doi: 10.1007/s40042-023-00780-3
    [27]
    LIU H Y, ZHOU Z H, BIAN Q, et al. High-efficiency nanosecond green laser based on extra-cavity second-harmonic generation of a Nd: YAG MOPA system[J]. IEEE Photonics Journal, 2023, 15(5): 1502005. doi: 10.2139/ssrn.4411865
    [28]
    LI X D, ZHOU Y P, XU H B, et al. High-stability, high-pulse-energy MOPA laser system based on composite Nd: YAG crystal with multiple doping concentrations[J]. Optics & Laser Technology, 2022, 152: 108080. doi: 10.1016/j.optlastec.2022.108080
    [29]
    JIANG Y W, YANG J, LI P L, et al. High energy LiDAR source for long distance, high resolution range imaging[J]. Microwave and Optical Technology Letters, 2020, 62(12): 3655-3661. doi: 10.1002/mop.32650
    [30]
    NEGEL J P, LOESCHER A, VOSS A, et al. Ultrafast thin-disk multipass laser amplifier delivering 1.4 kW (4.7 mJ, 1030 nm) average power converted to 820 W at 515 nm and 234 W at 343 nm[J]. Optics Express, 2015, 23(16): 21064-21077. doi: 10.1364/OE.23.021064
    [31]
    FATTAHI H, ALISMAIL A, WANG H CH, et al. High-power, 1-ps, all-Yb: YAG thin-disk regenerative amplifier[J]. Optics Letters, 2016, 41(6): 1126-1129. doi: 10.1364/OL.41.001126
    [32]
    RÖCKER C, LOESCHER A, BIENERT F, et al. Ultrafast green thin-disk laser exceeding 1.4 kW of average power[J]. Optics Letters, 2020, 45(19): 5522-5525. doi: 10.1364/OL.403781
    [33]
    MA N, CHEN M, YANG C, et al. High-efficiency 50 W burst-mode hundred picosecond green laser[J]. High Power Laser Science and Engineering, 2020, 8: e1. doi: 10.1017/hpl.2020.2
    [34]
    WALCH P, MAHIEU B, MORENO V, et al. Long distance laser filamentation using Yb: YAG kHz laser[J]. Scientific Reports, 2023, 13(1): 18542. doi: 10.1038/s41598-023-45660-9
    [35]
    GORBUNOV I A, KULAGIN O V. Picosecond hybrid laser based on semiconductor laser, fibre and Nd: YVO4 amplifiers. Investigation of effects limiting the peak power[J]. Quantum Electronics, 2021, 51(10): 886-893. doi: 10.1070/QEL17627
    [36]
    DUDA M, NOVÁK O, CHYLA M, et al. Balancing the conversion efficiency and beam quality of second harmonic generation of a two-picosecond Yb: YAG thin-disk laser[J]. Laser Physics, 2020, 30(2): 025405. doi: 10.1088/1555-6611/ab60b0
    [37]
    CHEN Y, LI F Q, LIU K, et al. High-efficiency 2-mJ 5-kHz picosecond green laser generation by Nd: YAG innoslab amplifier[J]. IEEE Photonics Technology Letters, 2015, 27(14): 1531-1534. doi: 10.1109/LPT.2015.2424230
    [38]
    NOVÁK O, TURČIČOVÁ H, SMRŽ M, et al. Picosecond green and deep ultraviolet pulses generated by a high-power 100 kHz thin-disk laser[J]. Optics Letters, 2016, 41(22): 5210-5213. doi: 10.1364/OL.41.005210
    [39]
    HUANG Y T, ZHANG H B, YAN X CH, et al. A high peak power and high beam quality sub-nanosecond Nd: YVO4 laser system at 1 kHz repetition rate without SRS process[J]. Applied Sciences, 2019, 9(23): 5247. doi: 10.3390/app9235247
    [40]
    NOVÁK J, GREEN J T, METZGER T, et al. Thin disk amplifier-based 40 mJ, 1 kHz, picosecond laser at 515 nm[J]. Optics Express, 2016, 24(6): 5728-5733. doi: 10.1364/OE.24.005728
    [41]
    ALISMAIL A, WANG H CH, BRONS J, et al. 20 mJ, 1 ps Yb: YAG thin-disk regenerative amplifier[J]. Journal of Visualized Experiments, 2017(125): 55717. doi: 10.3791/55717-v
    [42]
    DESCAMPS D, GUICHARD F, PETIT S, et al. High-power sub-15 fs nonlinear pulse compression at 515 nm of an ultrafast Yb-doped fiber amplifier[J]. Optics Letters, 2021, 46(8): 1804-1807. doi: 10.1364/OL.419683
    [43]
    XIE G H, LIU Y, ZHANG C C, et al. Temporal envelope programmable burst-mode Ytterbium all-fiber amplifier based, ultraviolet source at 260 nm[J]. Optics & Laser Technology, 2022, 151: 108032. doi: 10.1016/j.optlastec.2022.108032
    [44]
    KARST M, PFALLER P, KLAS R, et al. 22-W average power high pulse energy multipass-cell-based post-compression in the green spectral range[J]. Optics Letters, 2023, 48(5): 1300-1303. doi: 10.1364/OL.482600
    [45]
    ZHANG L, LONG Y, ZHANG M, et al. Femtosecond green and ultraviolet lasers generated using second-harmonic generation based on K3B6O10Br nonlinear optical crystals[J]. Optical Engineering, 2020, 59(5): 056107. doi: 10.1117/1.oe.59.5.056107
    [46]
    DIDENKO N V, KONYASHCHENKO A V, KOSTRYUKOV P V, et al. Temporal compression of pulses from a 100-KHz-repetiton-rate femtosecond ytterbium laser[J]. Quantum Electronics, 2016, 46(8): 675-678. doi: 10.1070/qel16147
    [47]
    TAWFIEQ M, HANSEN A K, JENSEN O B, et al. Intensity noise transfer through a diode-pumped titanium sapphire laser system[J]. IEEE Journal of Quantum Electronics, 2018, 54(1): 1700209.
    [48]
    KUMAR S C, BAUTISTA E S, EBRAHIM-ZADEH M. Stable, high-power, Yb-fiber-based, picosecond ultraviolet generation at 355 nm using BiB3O6[J]. Optics Letters, 2015, 40(3): 403-406. doi: 10.1364/OL.40.000403
    [49]
    程梦尧, 王兆华, 何会军, 等. 高效率三倍频产生355 nm皮秒激光的实验研究[J]. 物理学报, 2019, 68(12): 124205. doi: 10.7498/aps.68.20190513

    CHENG M Y, WANG ZH H, HE H J, et al. Efficient third harmonic generation of 355 nm picosecond laser pulse[J]. Acta Physica Sinica, 2019, 68(12): 124205. (in Chinese). doi: 10.7498/aps.68.20190513
    [50]
    上官爱红, 张昊苏, 曹钰, 等. 空间高功率激光二极管泵浦源阵列的相变热控系统[J]. 光学 精密工程, 2024, 32(19): 2877-2888.

    SHANGGUAN A H, ZHANG H S, CAO Y, et al. Phase change thermal control system for space high-power laser diode pumping source array[J]. Optics and Precision Engineering, 2024, 32(19): 2877-2888. (in Chinese).
    [51]
    CHIOW S W, KOVACHY T, HOGAN J M, et al. Generation of 43 W of quasi-continuous 780 nm laser light via high-efficiency, single-pass frequency doubling in periodically poled lithium niobate crystals[J]. Optics Letters, 2012, 37(18): 3861-3863. doi: 10.1364/OL.37.003861
    [52]
    KIRIYAMA H, INOUE N, YAMAKAWA K. High energy second-harmonic generation of Nd: glass laser radiation with large aperture CsLiB6O10 crystals[J]. Optics Express, 2002, 10(19): 1028-1032. doi: 10.1364/oe.10.001028
    [53]
    YANG X Z, ZHANG L, CUI S Z, et al. Sodium guide star laser pulsed at Larmor frequency[J]. Optics Letters, 2017, 42(21): 4351-4354. doi: 10.1364/OL.42.004351
    [54]
    张益嘉, 付鑫鹏, 阮迪, 等. 固体MOPA激光器光束质量优化技术研究进展[J]. 发光学报, 2025, 46(10): 1916-1929.

    ZHANG Y J, FU X P, RUAN D, et al. Research progress of beam quality optimization technology for solid-state MOPA lasers[J]. Chinese Journal of Luminescence, 2025, 46(10): 1916-1929. (in Chinese).
    [55]
    王英广, 张激扬, 张强, 等. 旋变二次谐波测角误差自校正[J]. 光学 精密工程, 2024, 32(2): 184-192.

    WANG Y G, ZHANG J Y, ZHANG Q, et al. Self-correction for resolver second harmonic angle measurement error[J]. Optics and Precision Engineering, 2024, 32(2): 184-192. (in Chinese).
    [56]
    宋佳齐. 高平均功率单频824nm纳秒光学参量振荡器的研究[D]. 太原: 山西大学, 2024.

    SONG J Q. Investigation of the high-average-power single-frequency 824 nm nanosecond optical parametric oscillator[D]. Taiyuan: Shanxi University, 2024. (in Chinese).
    [57]
    RIEDEL R, ROTHHARDT J, BEIL K, et al. Thermal properties of borate crystals for high power optical parametric chirped-pulse amplification[J]. Optics Express, 2014, 22(15): 17607-17619. doi: 10.1364/OE.22.017607
    [58]
    ZHANG Y, ZHANG L C, LIU M, et al. Revealing the mechanical properties of potassium dihydrogen phosphate crystals by nanoindentation[J]. Journal of Materials Research, 2016, 31(8): 1056-1064. doi: 10.1557/jmr.2016.91
    [59]
    ZHANG ZH CH, WANG B, TAO G H, et al. Water dissolution ultra-precision continuous polishing of potassium dideuterium phosphate (DKDP) crystal[J]. Proceedings of SPIE, 2023, 12982: 129820G. doi: 10.1117/12.3021149
    [60]
    BEASLEY J D. Thermal conductivities of some novel nonlinear optical materials[J]. Applied Optics, 1994, 33(6): 1000-1003. doi: 10.1364/AO.33.001000
  • 加载中

Catalog

    通讯作者: 陈斌, bchen63@163.com
    • 1. 

      沈阳化工大学材料科学与工程学院 沈阳 110142

    1. 本站搜索
    2. 百度学术搜索
    3. 万方数据库搜索
    4. CNKI搜索

    Figures(9)  / Tables(4)

    Article views(21) PDF downloads(2) Cited by()
    Proportional views
    Related

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return