• Chinese Journal of Lasers
  • Vol. 50, Issue 17, 1714016 (2023)
Pai Peng1、2, Zhilin Li1, and Xinbo Wang1、*
Author Affiliations
  • 1Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2Department of Physics, Tsinghua University, Beijing 100084, China
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    DOI: 10.3788/CJL230830 Cite this Article Set citation alerts
    Pai Peng, Zhilin Li, Xinbo Wang. Terahertz-Field-Induced Second Harmonic Generation in Weyl Semimetal TaAs[J]. Chinese Journal of Lasers, 2023, 50(17): 1714016 Copy Citation Text show less
    Schematic diagram of the experimental setup, using wavefront tilt technology to generate strong electric field terahertz, and carrying electro-optic sampling and second harmonic generation detection at the sample position (grating: reflective diffraction grating, 1800 line/mm; HWP: half-wave plate; QWP: quarter-wave plate; CL: plano-convex cylindrical lens; MgO∶LiNbO3: magnesium oxide doped lithium niobate crystal; OAPM: off-axis parabolic mirror; WGP: terahertz wire grid polarizer; PMT: photomultiplier tube; WP:Wollaston prism; EOS:electro-optic sampling)
    Fig. 1. Schematic diagram of the experimental setup, using wavefront tilt technology to generate strong electric field terahertz, and carrying electro-optic sampling and second harmonic generation detection at the sample position (grating: reflective diffraction grating, 1800 line/mm; HWP: half-wave plate; QWP: quarter-wave plate; CL: plano-convex cylindrical lens; MgO∶LiNbO3: magnesium oxide doped lithium niobate crystal; OAPM: off-axis parabolic mirror; WGP: terahertz wire grid polarizer; PMT: photomultiplier tube; WP:Wollaston prism; EOS:electro-optic sampling)
    Strong THz profiles generated by LiNbO3 crystal in time-domain and frequency-domain (inset)
    Fig. 2. Strong THz profiles generated by LiNbO3 crystal in time-domain and frequency-domain (inset)
    Image of the focused THz spot at sample position and the experimental and Gaussian fitting results of pixel-cutting along the horizontal and vertical directions through the center of the THz spot
    Fig. 3. Image of the focused THz spot at sample position and the experimental and Gaussian fitting results of pixel-cutting along the horizontal and vertical directions through the center of the THz spot
    SHG intensity of TaAs (112) surface as a function of polarization angle under normal incidence
    Fig. 4. SHG intensity of TaAs (112) surface as a function of polarization angle under normal incidence
    Temporal profile of TFISHG signal (inset: TFISHG peak intensity as a funciton of THz electric field intensity along with a linear fit)
    Fig. 5. Temporal profile of TFISHG signal (inset: TFISHG peak intensity as a funciton of THz electric field intensity along with a linear fit)
    Experimental results of TFISHG signals of the TaAs (112) surface under different measurement configurations at room temperature. TFISHG signal as a function of polarization angle when the intensity terahertz electric field is along the [1, 1, -1] direction (a) and [1, -1, 0] direction (b) of the sample where the incident polarization is either parallel or perpendicular to detection polarization. Hollow circles and solid lines represent the experimental data and the fitting results using formula (8)‒(13), respectively. (c) SHG intensity as a function of polarization angle measured under the same experimental condition except the THz pump beam is blocked. Solid circles and solid lines represent the experimental data and the fitting results using formula (5)‒(7), respectively. (d) The relative amplitude of the fitted third-order nonlinear susceptibility coefficient. Green and orange data are fitting results of (a) and (b), respectively
    Fig. 6. Experimental results of TFISHG signals of the TaAs (112) surface under different measurement configurations at room temperature. TFISHG signal as a function of polarization angle when the intensity terahertz electric field is along the [1, 1, -1] direction (a) and [1, -1, 0] direction (b) of the sample where the incident polarization is either parallel or perpendicular to detection polarization. Hollow circles and solid lines represent the experimental data and the fitting results using formula (8)‒(13), respectively. (c) SHG intensity as a function of polarization angle measured under the same experimental condition except the THz pump beam is blocked. Solid circles and solid lines represent the experimental data and the fitting results using formula (5)‒(7), respectively. (d) The relative amplitude of the fitted third-order nonlinear susceptibility coefficient. Green and orange data are fitting results of (a) and (b), respectively
    Pai Peng, Zhilin Li, Xinbo Wang. Terahertz-Field-Induced Second Harmonic Generation in Weyl Semimetal TaAs[J]. Chinese Journal of Lasers, 2023, 50(17): 1714016
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