• Chinese Optics Letters
  • Vol. 19, Issue 9, 091401 (2021)
Renchong Lü1、2, Hao Teng2、5、*, Jiangfeng Zhu1、**, Yang Yu1、2, Wei Liu4, Guoqing Chang2, and Zhiyi Wei2、3、5、***
Author Affiliations
  • 1School of Physics and Optoelectronic Engineering, Xidian University, Xi’an 710071, China
  • 2Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 3School of Physical Science, University of Chinese Academy of Sciences, Beijing 100049, China
  • 4School of Physics and Astronomy, Sun Yat-sen University, Zhuhai 519082, China
  • 5Songshan Lake Materials Laboratory, Dongguan 523808, China
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    DOI: 10.3788/COL202119.091401 Cite this Article Set citation alerts
    Renchong Lü, Hao Teng, Jiangfeng Zhu, Yang Yu, Wei Liu, Guoqing Chang, Zhiyi Wei. High power Yb-fiber laser amplifier based on nonlinear chirped-pulse amplification at a repetition rate of 1 MHz[J]. Chinese Optics Letters, 2021, 19(9): 091401 Copy Citation Text show less
    Schematic of the NCPA system. BPF, bandpass filter; WDM, wavelength division multiplex; SM-LD, single-mode laser diode; YDF, Yb-doped gain fiber; PDG, pulse delay generator; AOM, acoustic optical modulator; PDOI, polarization dependent optical isolator; MM-LD, multi-mode laser diode; DM, dichromic mirror; TG, transmission grating; HR, high reflecting mirror; PCF, photonic crystal fiber.
    Fig. 1. Schematic of the NCPA system. BPF, bandpass filter; WDM, wavelength division multiplex; SM-LD, single-mode laser diode; YDF, Yb-doped gain fiber; PDG, pulse delay generator; AOM, acoustic optical modulator; PDOI, polarization dependent optical isolator; MM-LD, multi-mode laser diode; DM, dichromic mirror; TG, transmission grating; HR, high reflecting mirror; PCF, photonic crystal fiber.
    (a) RF spectrum of the oscillator. (b) The AC trace of the laser pulses from the oscillator.
    Fig. 2. (a) RF spectrum of the oscillator. (b) The AC trace of the laser pulses from the oscillator.
    Comparison of the transmission spectra after the BPF and the oscillator.
    Fig. 3. Comparison of the transmission spectra after the BPF and the oscillator.
    (a) Spectral distribution from amplified pulses on linear and logarithmic (inset) scale; (b) AC trace of compressed pulses.
    Fig. 4. (a) Spectral distribution from amplified pulses on linear and logarithmic (inset) scale; (b) AC trace of compressed pulses.
    (a) Dependence of output power versus the pump power for the main amplifier; (b) measured power stability and pulse train; (c) M2 value of this NCPA system.
    Fig. 5. (a) Dependence of output power versus the pump power for the main amplifier; (b) measured power stability and pulse train; (c) M2 value of this NCPA system.
    AC traces at different pulse energies (a)–(c) with BPF and (d)–(f) without BPF.
    Fig. 6. AC traces at different pulse energies (a)–(c) with BPF and (d)–(f) without BPF.
    Renchong Lü, Hao Teng, Jiangfeng Zhu, Yang Yu, Wei Liu, Guoqing Chang, Zhiyi Wei. High power Yb-fiber laser amplifier based on nonlinear chirped-pulse amplification at a repetition rate of 1 MHz[J]. Chinese Optics Letters, 2021, 19(9): 091401
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