High Power Laser Science and Engineering, Volume. 12, Issue 5, 05000e61(2024)
High-repetition-rate strong-field terahertz source by optical rectification in DSTMS crystals
Fig. 1. The experimental setup consists of an ultrafast Yb:YAG laser, a laser pulse compressor, THz generation and detection geometry. MPC, multi-pass cell; Cv. M1 and Cv. M2, concave mirrors; CM1 and CM2, chirped mirrors; BS, beam splitter; L1 and L2, lenses; NDF, neutral density filter; HDPE, high-density polyethylene; OAP1–OAP3, off-axis parabolic mirrors; TDL, time delay line; QWP, quarter wave plate; WP, Wollaston polarizer; BPD, balanced photodetector.
Fig. 2. Laser spectrum and pulse duration characterization. (a) The spectrum of the Yb:YAG laser (grey), after the MPC compressor (blue) and after the DSTMS crystal (purple). (b) The pulse duration before (yellow) and after (red) the MPC compressor.
Fig. 3. THz electric field (a) and the corresponding spectrum (b). The inset shows the THz focus spot. (c) The coherence length between the generated THz wave and the pump laser in the DSTMS crystal. (d) The absorption coefficient in the THz (red) and optical (purple) band in the DSTMS crystal.
Fig. 4. THz power (a) and pulse energy (b) at different repetition rates.
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Zhuorui Zheng, Kang Wang, Hongyang Li, Xianze Meng, Ye Tian, Liwei Song. High-repetition-rate strong-field terahertz source by optical rectification in DSTMS crystals[J]. High Power Laser Science and Engineering, 2024, 12(5): 05000e61
Category: Research Articles
Received: Jan. 27, 2024
Accepted: Jul. 25, 2024
Published Online: Nov. 14, 2024
The Author Email: Ye Tian (tianye@siom.ac.cn), Liwei Song (slw@siom.ac.cn)
CSTR:32185.14.hpl.2024.50