High Power Laser Science and Engineering, Volume. 11, Issue 5, 05000e57(2023)

Laser chirp controlled relativistic few-cycle mid-infrared pulse generation

Dongao Li1, Guobo Zhang2、*, Jie Zhao1, Yanting Hu1, Yu Lu1, Hao Zhang1, Qianni Li1, Dongze Zhang1, Rong Sha1, Fuqiu Shao1, Zhengming Sheng3,4,5, and Tongpu Yu1、*
Author Affiliations
  • 1Department of Physics, National University of Defense Technology, Changsha, China
  • 2Department of Nuclear Science and Technology, National University of Defense Technology, Changsha, China
  • 3Key Laboratory for Laser Plasmas (MOE) and School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai, China
  • 4Collaborative Innovation Center of IFSA, Shanghai Jiao Tong University, Shanghai, China
  • 5Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, China
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    Figures & Tables(6)
    Schematic of laser chirp controlled few-cycle mid-IR pulse generation. Due to the special curving profile of the refractive index of the NCLP and the plasma etching, the pulse is rapidly compressed longitudinally. As a result, a large number of photons approach the photon deceleration phase, and produce the mid-infrared frequency component, which then slips backwards into the bubble and moves forward together with the bubble. The red curves represent the distribution of the laser electric field on-axis, and the green curves represent the corresponding distribution of the refractive index of the NCLP. The blue arrows denote the photon emission directions relative to the bubble.
    2D simulation of mid-IR generation with the NCLP. (a)–(c) Distributions of the plasma density () and transverse electric field () at different times. The orange curve is the electron density on-axis. (d) Spectral evolution as a function of the propagation time. (e) Spectral distribution of the on-axis laser electric field at (blue), (black) and (red). (f) Temporal profile of the mid-IR electric field at .
    Comparison of refractive index and evolution of the NCLP and un-chirped pulse. Longitudinal distribution of the laser electric field and refractive index in the cases of (a) and (b) an un-chirped laser. (c), (d) The corresponding locations of the rise edge and the fall edge, corresponding to the case with and without chirp, respectively. The insets of (c) and (d) show the evolution of the laser peak electric field .
    The evolution of the CEP at . (a) The generated mid-IR electric field as a function of the initial drive pulse phase . The inset shows the electric field waveform for different of the initial drive pulse (, blue dashed; , black solid; , red dot dash). (b) The phase evolution of the mid-IR electric field with variation.
    3D simulation of mid-IR generation with the NCLP. (a)–(c) The distributions of the plasma density () and the transverse electric field () at different times obtained from 3D PIC simulation. (d) Spectral distribution of the on-axis laser electric field at (blue) and (red). The inset is the temporal profile of the mid-IR electric field at .
    • Table 1. The maximum energy conversion efficiency () of the generated mid-IR pulse with different chirp parameters.

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      Table 1. The maximum energy conversion efficiency () of the generated mid-IR pulse with different chirp parameters.

      ${t}_{\mathrm{MIR}}$ ${\mathrm{Effi}}_{\mathrm{max}}$ Width ( $\unicode{x3bc} \mathrm{m}$ )
      b = –0.07 $4125{T}_0$ 5.0%4.2–20.0
      b = –0.06 $4300{T}_0$ 4.6%4.4–20.0
      b = –0.04 $4725{T}_0$ 2.7%6.2–26.6
      b = –0.02 $5500{T}_0$ 2.3%6.2–26.6
      b = 0 $6350{T}_0$ 1.9%6.2–26.6
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    Dongao Li, Guobo Zhang, Jie Zhao, Yanting Hu, Yu Lu, Hao Zhang, Qianni Li, Dongze Zhang, Rong Sha, Fuqiu Shao, Zhengming Sheng, Tongpu Yu. Laser chirp controlled relativistic few-cycle mid-infrared pulse generation[J]. High Power Laser Science and Engineering, 2023, 11(5): 05000e57

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    Paper Information

    Category: Research Articles

    Received: Jan. 29, 2023

    Accepted: Jun. 12, 2023

    Posted: Jun. 15, 2023

    Published Online: Sep. 5, 2023

    The Author Email: Guobo Zhang (zgb830@163.com), Tongpu Yu (tongpu@nudt.edu.cn)

    DOI:10.1017/hpl.2023.51

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