• Journal of Infrared and Millimeter Waves
  • Vol. 40, Issue 3, 297 (2021)
Rong-Guo LU1、*, Rui LIN1, Li-Ming SHEN1, Song-Wei CAI1, Yu-Jiao WANG1, Jin-Zhan CHEN1, Zhong-Hua YANG2, Jiang-Bo LYU1, Yong ZHOU1, Xiao-Ju WANG1, and Yong LIU1
Author Affiliations
  • 1State Key Laboratory of Electronic Thin Films and Integrated Devices, School of Optoelectronic Science and Engineering, University of Electronic Science and Technology of China, Chengdu 610054, China
  • 2Chongqing United Microelectronics Center, Chongqing 401332, China
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    DOI: 10.11972/j.issn.1001-9014.2021.03.003 Cite this Article
    Rong-Guo LU, Rui LIN, Li-Ming SHEN, Song-Wei CAI, Yu-Jiao WANG, Jin-Zhan CHEN, Zhong-Hua YANG, Jiang-Bo LYU, Yong ZHOU, Xiao-Ju WANG, Yong LIU. 3-μm mid-infrared polarization-independent and CMOS-compatible graphene modulator[J]. Journal of Infrared and Millimeter Waves, 2021, 40(3): 297 Copy Citation Text show less
    (a) Schematic diagram of our proposed device,(b) schematic diagram of mode conversion structure,(c) cross-sectional schematic diagram of the graphene modulator
    Fig. 1. (a) Schematic diagram of our proposed device,(b) schematic diagram of mode conversion structure,(c) cross-sectional schematic diagram of the graphene modulator
    (a) Under the wavelength of 2.95 μm, 3 μm, 3.05 μm, the in-plane dielectric constant changes with the applied voltage,(b) the variation of the absorption coefficient for both TE0 and TM0 mode of graphene modulator under different chemical potential
    Fig. 2. (a) Under the wavelength of 2.95 μm, 3 μm, 3.05 μm, the in-plane dielectric constant changes with the applied voltage,(b) the variation of the absorption coefficient for both TE0 and TM0 mode of graphene modulator under different chemical potential
    (a) The variation of effective refractive index for the first five modes in the width range from 1.4 μm to 3.4 μm,(b) analyzing the influence on coupling efficiency by sweeping the coupling length,(c) analyzing the influence on conversion efficiency by sweeping the length of three parts
    Fig. 3. (a) The variation of effective refractive index for the first five modes in the width range from 1.4 μm to 3.4 μm,(b) analyzing the influence on coupling efficiency by sweeping the coupling length,(c) analyzing the influence on conversion efficiency by sweeping the length of three parts
    (a) The variation of insertion loss of various parts for the device under the wavelength from 2.95 μm to 3.05 μm,(b) the normalized transmission of the device under the wavelength from 2.95 μm to 3.05 μm
    Fig. 4. (a) The variation of insertion loss of various parts for the device under the wavelength from 2.95 μm to 3.05 μm,(b) the normalized transmission of the device under the wavelength from 2.95 μm to 3.05 μm
    Rong-Guo LU, Rui LIN, Li-Ming SHEN, Song-Wei CAI, Yu-Jiao WANG, Jin-Zhan CHEN, Zhong-Hua YANG, Jiang-Bo LYU, Yong ZHOU, Xiao-Ju WANG, Yong LIU. 3-μm mid-infrared polarization-independent and CMOS-compatible graphene modulator[J]. Journal of Infrared and Millimeter Waves, 2021, 40(3): 297
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