Infrared and Laser Engineering, Volume. 50, Issue 4, 20190565(2021)

Effects of gain distribution on self-similar amplification of picosecond pulses

Yun Zhang, Bowen Liu, Huanyu Song, Yuan Li, Lu Chai, and Minglie Hu
Author Affiliations
  • Ultrafast Laser Laboratory, College of Precision Instruments and Opto-Electronics Engineering, Tianjin University, Tianjin 300072, China
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    Figures & Tables(8)
    Self-similar amplification in different pump schemes. (a) Forward pump, (b) backward pump
    M-factors versus pulse central wavelength and input energy of amplified pulses in different pump schemes. (a) Forward pump, (b) backward pump. Point A and B represent the minimum value of M-factors in (a) and (b), which are the best points of self-similar evolution
    Amplification results of seed pulses in different pump schemes. (a) De-chirped pulse profile of the seed pulse of point A transmitting to the end of the 2 m-long fiber in forward-pumping scheme, (b) de-chirped pulse profile of the seed pulse of point B transmitting to the end of the 2 m-long fiber in backward-pumping scheme. Black lines and red lines are seed pulses and transform-limited pulses. Insets: corresponding spectra (left) and amplified pulses before compression (right). Black lines and red lines are seed pulses and parabolic fittings
    Evolution of the seed pulse of point A in forward-pumping and backward-pumping schemes. (a) Peak power (solid) and M-factor (dash-dot), (b) 10 dB spectral width (solid) and pulse width(dash-dot). Black lines and red lines represent forward pump and backward pump. (c) Spectral evolution in forward-pumping scheme, (d) Spectral evolution in backward-pumping scheme
    Evolution of the seed pulse of point B in forward-pumping and backward-pumping schemes. (a) Peak power (solid) and M-factor(dash-dot), (b) 10 dB spectral width (solid) and pulse width(dash-dot). Black lines and red lines represent forward pump and backward pump. (c) Spectral evolution in forward-pumping scheme, (d) Spectral evolution in backward-pumping scheme
    M-factors versus central wavelength and input energy of amplified pulses in different pump schemes with different fiber lengths. In forward-pumping scheme, the M-factors of amplified pulses with the fiber length of (a) 2 m, (b) 3 m, (c) 4 m. In backward-pumping scheme, the M-factors of amplified pulses with the fiber length of (d) 2 m, (e) 3 m, (f) 4 m
    M-factors versus central wavelength and input energy of amplified pulses in different pump schemes with different total gain coefficients. In forward-pumping scheme, the M-factors of amplified pulses with the total gain coefficient of (a) 20 dB, (b) 25 dB, (c) 30 dB. In backward-pumping scheme, the M-factors of amplified pulses with the total gain coefficient of (d) 20 dB, (e) 25 dB, (f) 30 dB
    • Table 1. [in Chinese]

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      Table 1. [in Chinese]

      ParameterValueParameterValue
      c/m•s−13×108h/J•s 6.63×10−34
      Ap/m23.14×10−8As/m21.256×10−9
      β2/ps2•m−10.023γ/W−1 m−12.14×10−4
      τ/ms 0.8n2/W−1 m22.3×10−20
      NYb/m−33.8×10−25λp/nm 976
      σa(λ)/m2Ref. [18] σe(λ)/m2Ref. [18]
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    Yun Zhang, Bowen Liu, Huanyu Song, Yuan Li, Lu Chai, Minglie Hu. Effects of gain distribution on self-similar amplification of picosecond pulses[J]. Infrared and Laser Engineering, 2021, 50(4): 20190565

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    Paper Information

    Category: Lasers & Laser optics

    Received: Dec. 25, 2019

    Accepted: --

    Published Online: Jul. 30, 2021

    The Author Email:

    DOI:10.3788/IRLA20190565

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