Photonics Research, Volume. 12, Issue 3, 505(2024)

Wafer-level substrate-free YIG single crystal film for a broadband tunable terahertz isolator Editors' Pick

Xilai Zhang1、†, Dan Zhao2、†, Ding Zhang1, Qiang Xue1,3, Fei Fan2,4, Yulong Liao1, Qinghui Yang1, and Qiye Wen1,3、*
Author Affiliations
  • 1School of Electronic Science and Engineering, State Key Laboratory of Electronic Thin Film and Integrated Devices, University of Electronic Science and Technology of China, Chengdu 610054, China
  • 2Tianjin Key Laboratory of Optoelectronic Sensor and Sensing Network Technology, Institute of Modern Optics, Nankai University, Tianjin 300350, China
  • 3Shenzhen Institute for Advanced Study, University of Electronic Science and Technology of China, Shenzhen 518110, China
  • 4e-mail: fanfei_gdz@126.com
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    Figures & Tables(9)
    Schematic diagram. (a) Polarized THz-TDS system with an adjustable magnetic field. (b) THz wave transfer through the sample. (c) Magnetic Faraday rotation effect. (d) Device formed after packaging a sample.
    (a) Photograph of La:YIG sample. (b) SEM image. (c) XRD pattern of La:YIG and GGG film. (d) Hysteresis curve of a La:YIG sample.
    (a) Time domain THz pulses of air and La:YIG film on GGG substrate. (b) Effective refractive index of La:YIG. (c) Transmission and absorption coefficient of one sample under different EMFs. (d) Transmission and absorption coefficient of different numbers of samples (stacked together).
    (a), (b) Phase change of left-handed rotation and right-handed rotation of one La:YIG sample at different EMFs. (c) Faraday rotation angle spectra of one La:YIG sample under the EMF range from −0.22 to 0.22 T. (d) Verdet constant spectrum of La:YIG calculated from the polarization rotation angle at an EMF of 0.22 T.
    (a), (b) Phase change of left-handed rotation and right-handed rotation of different numbers of YIG samples (stacked together) under ±0.22 T. (c) Faraday rotation angle spectra of different numbers of YIG samples (stacked together) under ±0.22 T. (d) Faraday rotation angle changes with the number of sample stacks. (e), (f) Polarization states of the transmitted THz wave through one to four stacked La:YIG films at 0.6 THz under ±0.22 T.
    (a) ±45° LP time domain THz pulses of four stacked La:YIG films under the EMF of ±0.22 T. (b) −45° transmission under the EMF of ±0.22 T. (c) +45° transmission under the EMF of ±0.22 T. (d) Isolation of four stacked La:YIG films under the EMF of 0.22 T.
    (a), (b) Transmission of eight La:YIG samples (stacked together) with ±45° linearly polarized light. (c) Faraday rotation angle spectra of eight La:YIG samples (stacked together) under the EMF range from −0.26 to 0.26 T. (d) Isolation of eight stacked La:YIG films under the EMF range from 0 to 0.26 T. (e), (f) Polarization states of the transmitted THz wave through eight stacked La:YIG films at 0.6 THz from 0 to ±0.26 T. (g) Faraday rotation angle spectrum of eight La:YIG samples changes with magnetic field. (h) Isolation of eight stacked La:YIG films changes with magnetic field.
    • Table 1. Optimized Growth Parameters for La:YIG Films

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      Table 1. Optimized Growth Parameters for La:YIG Films

      Flux CompositionTemperature (°C)Growth Rate (μm·min1)Rotation Rate (r·min1)Growth Time (min)Thickness (μm)
      LaxY3xFe5O12960±0.50.660508305
    • Table 2. Y, La, Fe, O Mole Fractions Obtained by EPMA from the Surface of La:YIG Sample (in %)

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      Table 2. Y, La, Fe, O Mole Fractions Obtained by EPMA from the Surface of La:YIG Sample (in %)

      PositionYLaFeOPb
      114.66150.171016.985468.18210
      214.65110.164817.035868.14830
      313.90170.163914.561271.17670.1965
      Average14.40480.166616.224169.16900.0655
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    Xilai Zhang, Dan Zhao, Ding Zhang, Qiang Xue, Fei Fan, Yulong Liao, Qinghui Yang, Qiye Wen. Wafer-level substrate-free YIG single crystal film for a broadband tunable terahertz isolator[J]. Photonics Research, 2024, 12(3): 505

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    Paper Information

    Category: Optical and Photonic Materials

    Received: Oct. 23, 2023

    Accepted: Dec. 24, 2023

    Published Online: Feb. 29, 2024

    The Author Email: Qiye Wen (qywen@uestc.edu.cn)

    DOI:10.1364/PRJ.509876

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