• Chinese Optics Letters
  • Vol. 18, Issue 5, 051901 (2020)
Yuting Yang, Gang Zhao, Yue Huang, Liwen Feng, Senlin Huang*, and Kexin Liu
Author Affiliations
  • State Key Laboratory of Nuclear Physics and Technology and Institute of Heavy Ion Physics, School of Physics, Peking University, Beijing 100871, China
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    DOI: 10.3788/COL202018.051901 Cite this Article Set citation alerts
    Yuting Yang, Gang Zhao, Yue Huang, Liwen Feng, Senlin Huang, Kexin Liu. High repetition rate picosecond LiNbO3 THz parametric amplifier and parametric gain[J]. Chinese Optics Letters, 2020, 18(5): 051901 Copy Citation Text show less
    Sketch of the TPA experimental setup.
    Fig. 1. Sketch of the TPA experimental setup.
    Measurement results for THz radiation (a) wavelength and (b) bandwidth.
    Fig. 2. Measurement results for THz radiation (a) wavelength and (b) bandwidth.
    THz beam profile measurement results of the LN TPA. (a)–(d) THz beam profiles measured at 2.0, 5.0, 8.0, and 11.0 mm downstream of the THz radiation exit surface (S2) of the LN crystal. (e) The beam radii for the THz beam plotted as a function of the measurement distance. The solid curves were calculated according to the estimated M2 parameters.
    Fig. 3. THz beam profile measurement results of the LN TPA. (a)–(d) THz beam profiles measured at 2.0, 5.0, 8.0, and 11.0 mm downstream of the THz radiation exit surface (S2) of the LN crystal. (e) The beam radii for the THz beam plotted as a function of the measurement distance. The solid curves were calculated according to the estimated M2 parameters.
    (a) Measured THz pulse energy as a function of frequency for different effective parametric amplification lengths L. (b) Measured pulse energy of THz wave output as a function of L at four different THz frequencies.
    Fig. 4. (a) Measured THz pulse energy as a function of frequency for different effective parametric amplification lengths L. (b) Measured pulse energy of THz wave output as a function of L at four different THz frequencies.
    THz parametric gain (gTHz) versus frequency. The curves represent theoretical results calculated using Eq. (2), for which three different κ values were used.
    Fig. 5. THz parametric gain (gTHz) versus frequency. The curves represent theoretical results calculated using Eq. (2), for which three different κ values were used.
    Yuting Yang, Gang Zhao, Yue Huang, Liwen Feng, Senlin Huang, Kexin Liu. High repetition rate picosecond LiNbO3 THz parametric amplifier and parametric gain[J]. Chinese Optics Letters, 2020, 18(5): 051901
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