Volume 30 Issue 4
Apr.  2018
Turn off MathJax
Article Contents
Zhang Xuguang, Wang Weimin, Lu Yanhua, et al. 440 nm solid-state blue laser produced by a monolithic periodically poled lithium niobate crystal based on cascaded third-harmonic generation[J]. High Power Laser and Particle Beams, 2018, 30: 041005. doi: 10.11884/HPLPB201830.170483
Citation: Zhang Xuguang, Wang Weimin, Lu Yanhua, et al. 440 nm solid-state blue laser produced by a monolithic periodically poled lithium niobate crystal based on cascaded third-harmonic generation[J]. High Power Laser and Particle Beams, 2018, 30: 041005. doi: 10.11884/HPLPB201830.170483

440 nm solid-state blue laser produced by a monolithic periodically poled lithium niobate crystal based on cascaded third-harmonic generation

doi: 10.11884/HPLPB201830.170483
  • Received Date: 2017-11-29
  • Rev Recd Date: 2018-01-04
  • Publish Date: 2018-04-15
  • A 440 nm solid-state blue laser produced by a periodically poled lithium niobate (PPLN) crystal based on cascaded third-harmonic generation (THG) is introduced. According to Sellmeier equation and phase-matching conditions of second-harmonic generation (SHG) and sum-frequency generation (SFG), two different poling periods of PPLN were designed to realize SHG and SFG at the same working temperature, and then the cascaded THG can be realized through SHG and SFG. The fundamental laser was produced by Nd: YAG, and had a 110 ns pulse width at 400 Hz pulse repetition rate with a measured beam quality of Mx2=1.81 and My2=2.65. It was coupled in PPLN and the 660 nm and 440 nm laser were detected after it passed through the crystal. The maximum output power of 440 nm laser was 2.4 mW where the working temperature was 55.5 ℃, and the power of 1319 nm laser was 530 mW. It is proved that a cascaded THG 440 nm blue laser can be realized by this method and it can realize a high power and high efficiency blue laser after optimization.
  • loading
  • [1]
    Sakuma J, Asakawa Y, Obara M. Generation of 5-W deep-UV continuous-wave radiation at 266 nm by an external cavity with a CsLiB6O10 crystal. [J]. Optics Letters, 2004, 29(1): 92-94. doi: 10.1364/OL.29.000092
    [2]
    Seyed, Ebrahim, Pourmand, et al. Effects of 946-nm thermal shift and broadening on Nd3+: YAG laser performance[J]. Chinese Physics B, 2015, 24(12): 342-345.
    [3]
    Wang G, Geng A, Bo Y, et al. 28.4 W 266 nm ultraviolet-beam generation by fourth-harmonic generation of an all-solid-state laser[J]. Optics Communications, 2006, 259(2): 820-822.
    [4]
    Shen Y R. Principles of nonlinear optics[M]. Hoboken: John Wiley, 1984: 261.
    [5]
    Risk W P, Lenth W. Room-temperature, continuous-wave, 946-nm Nd: YAG laser pumped by laser-diode arrays and intracavity frequency doubling to 473 nm[J]. Optics Letters, 1987, 12(12): 993-995. doi: 10.1364/OL.12.000993
    [6]
    Mu X D, Ding Y J, Zotova I B. All-solid-state, compact, and coherent blue source producing 118 mW at 440 nm by intracavity-frequency-tripling Nd: YAG laser beam[C]//Conference on Lasers and Electro-Optics. 2005, 1: 473-475.
    [7]
    罗国珍, 祝世宁, 何京良, 等. PPLT光学超晶格全固态蓝红双波长激光器的研制[J]. 中国激光, 2002, 29(s1): 142-144.

    Luo Guozhen, Zhu Shining, He Jingliang, et al. All-solid-state blue and red dual wavelength laser based on PPLT optical superlattice. Chinese Journal of Lasers, 2002, 29(s1): 142-144
    [8]
    Castaing M, Balembois F, Georges P. Continuous-wave laser at 440 nm based on frequency-doubled diode-pumped Nd: GdVO(4) crystal[J]. Optics Letters, 2008, 33(17): 1957-1959. doi: 10.1364/OL.33.001957
    [9]
    Myers L E. Efficient third-harmonic generation with PPLN and PPLT[C]//IEEE Lasers and Electro-Optics Society. 1999, 2: 586-587.
    [10]
    赵景山. 大功率蓝光激光器的研究[D]. 天津: 天津大学, 2009.

    Zhao Jingshan. Research on high-power blue laser. Tianjin: Tianjin University, 2009
    [11]
    王峰. 高功率准连续440 nm蓝光激光器的研究[D]. 长春: 长春理工大学, 2014.

    Wang Feng. Research on high-power quasi-CW 440 nm blue laser. Changchun: Changchun University of Science and Technology, 2014
    [12]
    Walter K. Solid-state laser engineering[M]. 5th ed. Beijing: World Book Inc, 2005.
    [13]
    Chen Q, Risk W P. Periodic poling of KTiOPO4 using an applied electric field[J]. Electronics Letters, 1994, 30(18): 1516-1517. doi: 10.1049/el:19941019
    [14]
    Burns W K, Mcelhanon W, Goldberg L. Second harmonic generation in field poled, quasi-phase-matched, bulk LiNbO3[J]. IEEE Photonics Technology Letters, 1994, 6(2): 252-254. doi: 10.1109/68.275441
    [15]
    Zhai K, Zhang S, Ma X, et al. Temperature dependence of fiber-format multiwavelength generation process in bulk MgO-PPLN crystal via high-power photonic crystal fiber laser[J]. IEEE Photonics Journal, 2016, 8(2): 1-7.
    [16]
    Fejer M M, Magel G A, Jundt D H, et al. Quasi-phase-matched second harmonic generation: tuning and tolerances[J]. IEEE Journal of Quantum Electronics, 1992, 28(11): 2631-2654. doi: 10.1109/3.161322
    [17]
    Gayer O, Sacks Z, Galun E, et al. Temperature and wavelength dependent refractive index equations for MgO-doped congruent and stoichiometric LiNbO3[J]. Applied Physics B, 2008, 91(2): 343-348. doi: 10.1007/s00340-008-2998-2
  • 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(6)  / Tables(1)

    Article views (1258) PDF downloads(176) Cited by()
    Proportional views
    Related

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return