• Chinese Physics B
  • Vol. 29, Issue 9, (2020)
Jian-Xing Zhao1, Jian-Lin Song1, Yao Zhou1, Rui-Long Zhao1, Yi-Chao Liu1, and Jian-Hong Zhou1、2、†
Author Affiliations
  • 1School of Photoelectric Engineering, Changchun University of Science and Technology, Changchun 30022, China
  • 2Key Laboratory of Optoelectric Measurement and Optical Information Transmission Technology of Ministry of Education, Changchun University of Science and Technology, Changchun 1300, China
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    DOI: 10.1088/1674-1056/abab6f Cite this Article
    Jian-Xing Zhao, Jian-Lin Song, Yao Zhou, Rui-Long Zhao, Yi-Chao Liu, Jian-Hong Zhou. Multi-functional vanadium dioxide integrated metamaterial for terahertz wave manipulation[J]. Chinese Physics B, 2020, 29(9): Copy Citation Text show less
    (a) Cross section view of the proposed metamaterial. The thickness of the upper part is the same as that of the lower part. (b) Front, (c) middle, and (d) back metallic grating layers of the proposed metamaterial. The front grating is parallel to the x axis, the middle grating is oriented at 45° with respect to the x axis and the back grating is vertical to the x axis.
    Fig. 1. (a) Cross section view of the proposed metamaterial. The thickness of the upper part is the same as that of the lower part. (b) Front, (c) middle, and (d) back metallic grating layers of the proposed metamaterial. The front grating is parallel to the x axis, the middle grating is oriented at 45° with respect to the x axis and the back grating is vertical to the x axis.
    (a) Moduli of the T matrix coefficients for forward propagation. (b) Transmission and PCR spectra for y-polarization (y-pol.) incidence. Insets are z-component electric field distributions in the middle x–y plane of the middle grating structure at the frequencies of 0.453 THz and 1.058 THz, respectively. (c) Reflection and PCR spectra for x-polarization (x-pol.) incidence.
    Fig. 2. (a) Moduli of the T matrix coefficients for forward propagation. (b) Transmission and PCR spectra for y-polarization (y-pol.) incidence. Insets are z-component electric field distributions in the middle xy plane of the middle grating structure at the frequencies of 0.453 THz and 1.058 THz, respectively. (c) Reflection and PCR spectra for x-polarization (x-pol.) incidence.
    (a) Absorption spectrum for y-polarization incidence. (b) Reflection spectrum for x-polarization incidence. (c) The z-component electric field distribution in the x–y plane of the front grating layer, (d) the z-component electric field distribution in the y–z plane of the structure, and (e) the magnetic |Hx| field distribution in the y–z plane at the frequency of 1.155 THz when illuminated with y-polarized wave.
    Fig. 3. (a) Absorption spectrum for y-polarization incidence. (b) Reflection spectrum for x-polarization incidence. (c) The z-component electric field distribution in the xy plane of the front grating layer, (d) the z-component electric field distribution in the yz plane of the structure, and (e) the magnetic |Hx| field distribution in the yz plane at the frequency of 1.155 THz when illuminated with y-polarized wave.
    (a) The absorption spectra with different tg when VO2 is at metal phase, and (b) the cross-polarization coefficient |Txy| with different ts when VO2 is at insulator phase for y-polarization incidence. (c) The absorption spectrum at metal phase and the cross-polarization coefficient at insulator phase for the optimized structure with w1 = 56 μm, ts = 49 μm when illuminated with y-polarized wave. (d) The reflection spectra of the optimized structure with w1 = 56 μm, ts = 49 μm at metal phase and insulator phase when illuminated with x-polarization wave.
    Fig. 4. (a) The absorption spectra with different tg when VO2 is at metal phase, and (b) the cross-polarization coefficient |Txy| with different ts when VO2 is at insulator phase for y-polarization incidence. (c) The absorption spectrum at metal phase and the cross-polarization coefficient at insulator phase for the optimized structure with w1 = 56 μm, ts = 49 μm when illuminated with y-polarized wave. (d) The reflection spectra of the optimized structure with w1 = 56 μm, ts = 49 μm at metal phase and insulator phase when illuminated with x-polarization wave.
    (a) The absorption spectra with different w1 when VO2 is at metal phase, and (b) the cross-polarization coefficient |Txy| with different ts when VO2 is at insulator phase for y-polarization incidence. (c) The absorption spectrum at metal phase and the cross-polarization coefficient at insulator phase for the optimized structure with w1 = 62 μm, ts = 56 μm when illuminated with y-polarized wave. (d) The reflection spectra of the optimized structure with w1 = 62 μm, ts = 56 μm at metal phase and insulator phase when illuminated with x-polarization wave.
    Fig. 5. (a) The absorption spectra with different w1 when VO2 is at metal phase, and (b) the cross-polarization coefficient |Txy| with different ts when VO2 is at insulator phase for y-polarization incidence. (c) The absorption spectrum at metal phase and the cross-polarization coefficient at insulator phase for the optimized structure with w1 = 62 μm, ts = 56 μm when illuminated with y-polarized wave. (d) The reflection spectra of the optimized structure with w1 = 62 μm, ts = 56 μm at metal phase and insulator phase when illuminated with x-polarization wave.
    Conditions for state 1Conditions for state 2Conditions for state 3
    Forward propagationy-pol. and 298 Ky-pol. and 378 Kx-pol.
    Backward propagationx-pol. and 298 Kx-pol. and 378 Ky-pol.
    Table 1. The corresponding conditionsfor the three states.
    Jian-Xing Zhao, Jian-Lin Song, Yao Zhou, Rui-Long Zhao, Yi-Chao Liu, Jian-Hong Zhou. Multi-functional vanadium dioxide integrated metamaterial for terahertz wave manipulation[J]. Chinese Physics B, 2020, 29(9):
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