• Chinese Optics Letters
  • Vol. 20, Issue 4, 043201 (2022)
Yunqing Jiang1、2, Xiaoqiang Zhang1、2、*, Yongshan Liu1、2, Pierre Vallobra1, Sylvain Eimer1, Fan Zhang1、2, Yinchang Du2、3, Fengguang Liu1、2, Yong Xu1、2、**, and Weisheng Zhao1、2、***
Author Affiliations
  • 1School of Integrated Circuit Science and Engineering, Hefei Innovation Research Insititute, Beihang University, Beijing 100191, China
  • 2Anhui High Reliability Chips Engineering Laboratory, Hefei 230013, China
  • 3Key Laboratory of Geospace Environment, University of Science and Technology of China, Hefei 230026, China
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    DOI: 10.3788/COL202220.043201 Cite this Article Set citation alerts
    Yunqing Jiang, Xiaoqiang Zhang, Yongshan Liu, Pierre Vallobra, Sylvain Eimer, Fan Zhang, Yinchang Du, Fengguang Liu, Yong Xu, Weisheng Zhao. Spintronic terahertz emitter with integrated electromagnetic control[J]. Chinese Optics Letters, 2022, 20(4): 043201 Copy Citation Text show less
    Schematic of spintronic film THz emission with alternating electromagnetic coils.
    Fig. 1. Schematic of spintronic film THz emission with alternating electromagnetic coils.
    (a) Power supply circuit for the electromagnetic coils to produce the alternating magnetic field. (b) Magnetic field versus current and corresponding theoretical calculation for electromagnetic coils.
    Fig. 2. (a) Power supply circuit for the electromagnetic coils to produce the alternating magnetic field. (b) Magnetic field versus current and corresponding theoretical calculation for electromagnetic coils.
    (a) Square waveforms detected from the function generator and the oscilloscope. (b) Simplified waveforms for laser modulation by a chopper and electromagnetic field modulation by a function generator. (c) THz signal waveforms from the W/CoFeB/Pt spintronic film measured by a THz emission system, where two reverse directions of the direct current (DC) and alternating current (AC) flow in coils with chopper (w/ chopper) and without chopper (w/o chopper), respectively. (d) THz signal waveforms from the W/CoFeB/Pt spintronic emitter with the original start level (orange line) and a π phase difference start level (gray dash line).
    Fig. 3. (a) Square waveforms detected from the function generator and the oscilloscope. (b) Simplified waveforms for laser modulation by a chopper and electromagnetic field modulation by a function generator. (c) THz signal waveforms from the W/CoFeB/Pt spintronic film measured by a THz emission system, where two reverse directions of the direct current (DC) and alternating current (AC) flow in coils with chopper (w/ chopper) and without chopper (w/o chopper), respectively. (d) THz signal waveforms from the W/CoFeB/Pt spintronic emitter with the original start level (orange line) and a π phase difference start level (gray dash line).
    (a) THz signal waveforms and (b) the peak value of the THz signal under different frequencies from 84 Hz to 6884 Hz. (c) THz signal waveforms and (d) the peak value of the THz signal under different square wave amplitudes from 2 mV to 300 mV.
    Fig. 4. (a) THz signal waveforms and (b) the peak value of the THz signal under different frequencies from 84 Hz to 6884 Hz. (c) THz signal waveforms and (d) the peak value of the THz signal under different square wave amplitudes from 2 mV to 300 mV.
    Yunqing Jiang, Xiaoqiang Zhang, Yongshan Liu, Pierre Vallobra, Sylvain Eimer, Fan Zhang, Yinchang Du, Fengguang Liu, Yong Xu, Weisheng Zhao. Spintronic terahertz emitter with integrated electromagnetic control[J]. Chinese Optics Letters, 2022, 20(4): 043201
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