Single frequency laser with 100 MHz repetition rate and 1 ns pulse width using combined amplification

被引:0
作者
Liu, Chong [1 ]
Zhang, Xiang [1 ]
Ye, Zhibin [1 ]
Wang, Yi [1 ]
Xiang, Zhen [1 ]
Chen, Jun [1 ]
机构
[1] State Key Laboratory of Modern Optical Instrumentation, Zhejiang University, Hangzhou
来源
Zhongguo Jiguang/Chinese Journal of Lasers | 2014年 / 41卷 / 04期
关键词
High repetition rate; Lasers; Pulsed laser; Single frequency;
D O I
10.3788/CJL201441.0402006
中图分类号
学科分类号
摘要
Pulsed laser with 100 MHz repetition rate and 1 ns pulse width is obtained by intensity modulating a continous wave (CW) single frequency fiber laser with 70 kHz line width. The spectrum line width of the modulated pulsed laser is less than 0.8 GHz. A combined amplification setup with a fiber amplifier and two solid-state amplifiers is used to achieve power amplification of the pulsed laser. The output average powers are 13 W and 32.9 W after first and second solid-state laser amplifier, respectively. The small signal of the modulated pulsed laser is firstly amplified up to 2 W by a fiber pre-amplifier. The pre-amplified laser transmits the two solid-state main amplifiers for further power amplification. The combined amplification setup effectively weakens the stimulated scattering and amplified spontaneous emission (ASE) in the fiber amplifier. After amplification, the output laser preserves line width of 0.8 GHz with pulse width of 1 ns and repetition rate of 100 MHz. Such a laser output with single frequency, narrow pulse width and high repletion rate is required in many special applications.
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  • [1] Loftus T.H., Liu A., Hoffman P.R., Et al., 258 W of spectrally beam combined power with near-diffraction limited beam quality, SPIE, 6102, pp. 1-8, (2006)
  • [2] Nawatal K., Okidal M., Furuki K., Et al., Sub-100 W picosecond output from a phase-conjugate Nd:YVO<sub>4</sub> bounce amplifier, Optics Express, 17, 9, pp. 20816-20823, (2009)
  • [3] Nawatal K., Okidal M., Furuki K., Et al., MW ps pulse generation at sub-MHz repetition rates from a phase conjugate Nd:YVO<sub>4</sub> bounce amplifier, Optics Express, 15, 15, pp. 9123-9128, (2007)
  • [4] Liu X., Du S., Xue Y., Et al., High repetition rate nanosecond pulse fiber amplifier based on China-made large-mode-area fiber, Chinese J Lasers, 36, 7, pp. 1876-1879, (2009)
  • [5] Mao X., Mi G., Deng M., Et al., 200 kHz, 8 ns passively Q-switched high peak power Nd:YAG laser, Chinese J Lasers, 37, S1, pp. 20-23, (2010)
  • [6] Liu J., Liu J., Wang P., Cladding pumped nanosecond passively Q-switched Yb-doped fiber laser with Cr<sup>4+</sup>:YAG as saturable absorber, Chinese J Lasers, 38, 11, (2011)
  • [7] Xia J., Hu H., He J., Passively Q-switched laser operation of composite Cr<sup>4+</sup>:YAG-Nd<sup>3+</sup>:YAG crystal fiber, Chinese J Lasers, 32, 6, pp. 754-756, (2005)
  • [8] Ren F., Xiang W., Zu P., Et al., Experimental study on Er/Yb Co-doped double-clad all fiber laser, Chinese J Lasers, 37, 3, pp. 622-625, (2010)
  • [9] Liao M., Wang Z., Yu H., Et al., Nd:GdVO<sub>4</sub>/Cr:YAG microchip pulse laser, Chinese J Lasers, 37, 12, pp. 2954-2958, (2010)
  • [10] Su R., Zhou P., Xiao H., Et al., MOPA structured single-frequency nanosecond pulsed laser in all fiber format, Chinese J Lasers, 38, 11, (2011)