• Photonics Research
  • Vol. 6, Issue 10, 959 (2018)
Baolong Zhang1、2, Shangqing Li1、2, Shusu Chai3, Xiaojun Wu3、*, Jinglong Ma1, Liming Chen1、2、4, and Yutong Li1、2、4
Author Affiliations
  • 1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3School of Electronic and Information Engineering, Beihang University, Beijing 100191, China
  • 4Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai 200240, China
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    DOI: 10.1364/PRJ.6.000959 Cite this Article Set citation alerts
    Baolong Zhang, Shangqing Li, Shusu Chai, Xiaojun Wu, Jinglong Ma, Liming Chen, Yutong Li. Nonlinear distortion and spatial dispersion of intense terahertz generation in lithium niobate via the tilted pulse front technique[J]. Photonics Research, 2018, 6(10): 959 Copy Citation Text show less
    (a) Experimental setup for systematic characterization of the terahertz emission spectrum depends on the pump polarization, the emission position, as well as the input spectrum. The grating density is of 1500 lines/mm. The focal length of the imaging lens between the grating is 85 mm; HWP, half wave plate; SC, sheet copper; LN, lithium niobate crystal; OAP, 90° off-axis parabolic mirror; 1/4 WP, quarter-wave plate. (b) Photo of the lithium niobate crystal used in our experiment as well as its axis illustration.
    Fig. 1. (a) Experimental setup for systematic characterization of the terahertz emission spectrum depends on the pump polarization, the emission position, as well as the input spectrum. The grating density is of 1500 lines/mm. The focal length of the imaging lens between the grating is 85 mm; HWP, half wave plate; SC, sheet copper; LN, lithium niobate crystal; OAP, 90° off-axis parabolic mirror; 1/4 WP, quarter-wave plate. (b) Photo of the lithium niobate crystal used in our experiment as well as its axis illustration.
    (a) Normalized infrared (IR) input spectra for different GVD, and (b) their corresponding output terahertz spectra. (c) The detected terahertz signal as a function of the different GVD values of the pump pulses; (d) terahertz bandwidth and terahertz central frequency as functions of GVD values of the pump pulses; (e) calculated chirped pulse duration as a function of the different GVD values of the pump pulses.
    Fig. 2. (a) Normalized infrared (IR) input spectra for different GVD, and (b) their corresponding output terahertz spectra. (c) The detected terahertz signal as a function of the different GVD values of the pump pulses; (d) terahertz bandwidth and terahertz central frequency as functions of GVD values of the pump pulses; (e) calculated chirped pulse duration as a function of the different GVD values of the pump pulses.
    (a) Normalized output terahertz spectra for different rotation angles of the IR polarizer between the grating and the imaging lens. Zero degree means the pump laser is vertically polarized in the laboratory coordinate. (b) Normalized terahertz output spectra for the typical complementary angles, respectively. (c) Polarization angle dependence of the terahertz central frequency and spectral width. (d) Recorded terahertz signal as a function of the rotation angle of the IR polarizer.
    Fig. 3. (a) Normalized output terahertz spectra for different rotation angles of the IR polarizer between the grating and the imaging lens. Zero degree means the pump laser is vertically polarized in the laboratory coordinate. (b) Normalized terahertz output spectra for the typical complementary angles, respectively. (c) Polarization angle dependence of the terahertz central frequency and spectral width. (d) Recorded terahertz signal as a function of the rotation angle of the IR polarizer.
    (a) Terahertz signal as a function of the knife-edge position. (b) Detected terahertz temporal waveforms in knife-edge measurement directly recorded after the crystal emission plane, and (c) their corresponding normalized Fourier transform spectra.
    Fig. 4. (a) Terahertz signal as a function of the knife-edge position. (b) Detected terahertz temporal waveforms in knife-edge measurement directly recorded after the crystal emission plane, and (c) their corresponding normalized Fourier transform spectra.
    Baolong Zhang, Shangqing Li, Shusu Chai, Xiaojun Wu, Jinglong Ma, Liming Chen, Yutong Li. Nonlinear distortion and spatial dispersion of intense terahertz generation in lithium niobate via the tilted pulse front technique[J]. Photonics Research, 2018, 6(10): 959
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