Chinese Journal of Lasers, Volume. 50, Issue 17, 1714013(2023)

Terahertz Time‐Domain Spectroscopy of Warm Dense Gold

Xu Sun1, Haizhong Wu1, Xiaowei Wang1, Lü Zhihui1, Dongwen Zhang1、*, Dongxiao Liu2, Wei Fan2, Jingqin Su2, Weimin Zhou2, Yuqiu Gu2, Zengxiu Zhao1、**, and Jianmin Yuan1,3、***
Author Affiliations
  • 1College of Science, National University of Defense Technology, Changsha 410073, Hunan, China
  • 2Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, CAEP, Mianyang 621900, Sichuan, China
  • 3Graduate School of China Academy of Engineering Physics, Beijing 100193, China
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    Figures & Tables(5)
    Schematic diagrams of single-shot optical pump-terahertz detection system. (a) A schematic illustration of the setup (KDP: KH2PO4; DM: dichroic mirror; BS: beam splitter; LN: lithium niobate wafer; OAP: off-axis parabolic mirror; MM: metal mirror; TD1, TD2: terahertz detection delay line and pump delay line; RE: reflective echelon; W1, W2: wire grid polarizers; ITO: indium tin oxide thin film; ZnTe: zinc telluride detector crystal; QWP: 1/4 wave plate); (b)(c) reflection and transmission imaging results of free-standing gold foils with the diameter of 2 mm and the thickness of 30 nm, respectively; (d) spatial arrangement of optical pump and terahertz probe; (e) schematic diagram of the surface structure of the reflective echelon
    Comparison of terahertz waveform between single-shot detection and traditional multi-shot scanning detection. (a) Single-shot signal with THz on; (b) single-shot background signal with THz off; (c) single-shot terahertz modulation signal,ΔI/I0=ITHz on-ITHz off/ITHz off; (d) comparison between the single-shot waveform (solid line, ΔI/I0) obtained by vertical integration of Fig. 2 (c) and the multi-shot waveform obtained by traditional multi-shot scanning (dot dash line)
    Terahertz energy characterization. (a) The dependence of laser pulse duration on the grating position, and the variation of terahertz pulse energy with grating position for different pump laser energies (from top to bottom: 1, 0.8, 0.7, 0.6, and 0.4 J); (b) at a pulse duration of 126 fs, the terahertz energy fluence and conversion efficiency as a function of pump laser intensity
    Transmitted terahertz signal of the free-standing gold foil and the hole at the pump delay of 3 ps. (a)(b) Changes in probe optical intensity (ΔI=ITHz on-ITHz off) with and without THz radiation for the gold foil and the hole, respectively; (c)(d) THz time-domain waveforms obtained from ΔI/I0 for the gold foil and the hole, respectively; (e)(f) the corresponding frequency spectra of Figs.4(c) and (d)
    Variations in the electrical conductivity σ0 and THz transmittance of the free-standing gold foil as a function of pump-probe delay (negative delay indicates that the terahertz wave arrives at the free-standing gold foil before the pump laser), where the solid line represents the time-resolved electrical conductivity at different pump-probe delay obtained from a double exponential function fit and the DC electrical conductivity of bulk pure gold at room temperature (300 K) is shown with five-pointed star symbols[49], σdc bulk=4.403×107 S/m
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    Xu Sun, Haizhong Wu, Xiaowei Wang, Lü Zhihui, Dongwen Zhang, Dongxiao Liu, Wei Fan, Jingqin Su, Weimin Zhou, Yuqiu Gu, Zengxiu Zhao, Jianmin Yuan. Terahertz Time‐Domain Spectroscopy of Warm Dense Gold[J]. Chinese Journal of Lasers, 2023, 50(17): 1714013

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    Paper Information

    Category: terahertz technology

    Received: May. 4, 2023

    Accepted: Jun. 19, 2023

    Published Online: Sep. 13, 2023

    The Author Email: Zhang Dongwen (dwzhang@nudt.edu.cn), Zhao Zengxiu (zhaozengxiu@nudt.edu.cn), Yuan Jianmin (jmyuan@gscaep.ac.cn)

    DOI:10.3788/CJL230791

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