• Acta Physica Sinica
  • Vol. 69, Issue 15, 154205-1 (2020)
Feng Wu1,2, Zhi-Wei Guo1, Jia-Ju Wu1, Hai-Tao Jiang1,*, and Gui-Qiang Du3
Author Affiliations
  • 1Ministry of Education Key Laboratory of Advanced Microstructure Materials, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 2School of Optoelectronic Engineering, Guangdong Polytechnic Normal University, Guangzhou 510665, China
  • 3School of Space Science and Physics, Shandong Univeristy, Weihai 264209, China
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    DOI: 10.7498/aps.69.20200084 Cite this Article
    Feng Wu, Zhi-Wei Guo, Jia-Ju Wu, Hai-Tao Jiang, Gui-Qiang Du. Band gap engineering and applications in compound periodic structure containing hyperbolic metamaterials[J]. Acta Physica Sinica, 2020, 69(15): 154205-1 Copy Citation Text show less
    Schematic of the compound periodic structure containing hyperbolic metamaterials.
    Fig. 1. Schematic of the compound periodic structure containing hyperbolic metamaterials.
    Schematic of the conventional all-dielectric one-dimensional photonic crystal (AB)N.
    Fig. 2. Schematic of the conventional all-dielectric one-dimensional photonic crystal (AB)N.
    Iso-frequency curves of isotropic dielectrics A and B (TM and TE polarizations).
    Fig. 3. Iso-frequency curves of isotropic dielectrics A and B (TM and TE polarizations).
    Calculated reflectance spectrum of (AB)10 as a function of incident angle (TM and TE polarizations).
    Fig. 4. Calculated reflectance spectrum of (AB)10 as a function of incident angle (TM and TE polarizations).
    Schematic of the one-dimensional photonic crystal containing hyperbolic metamaterials [(CD)SB]N.
    Fig. 5. Schematic of the one-dimensional photonic crystal containing hyperbolic metamaterials [(CD)SB]N.
    Iso-frequency curves of (a) hyperbolic metamaterial A and (b) isotropic dielectric B (TM polarization).
    Fig. 6. Iso-frequency curves of (a) hyperbolic metamaterial A and (b) isotropic dielectric B (TM polarization).
    Reflectance spectra of [(CD)2B]3 under different incident angles (TM polarization): (a) Simulated result[107]; (b) experimental result[107].
    Fig. 7. Reflectance spectra of [(CD)2B]3 under different incident angles (TM polarization): (a) Simulated result[107]; (b) experimental result[107].
    Reflectance spectrum of [(CD)2B]3 as a function of incident angle (TM polarization)[107]. Background color represents the calculated result. Black hollow circle represents measured gap edge extracted from the reflectance dip.
    Fig. 8. Reflectance spectrum of [(CD)2B]3 as a function of incident angle (TM polarization)[107]. Background color represents the calculated result. Black hollow circle represents measured gap edge extracted from the reflectance dip.
    Calculated reflectance spectrum of [(CD)2B]3 as a function of incident angle (TM and TE polarizations)[108].
    Fig. 9. Calculated reflectance spectrum of [(CD)2B]3 as a function of incident angle (TM and TE polarizations)[108].
    Experimental reflectance spectra of [(CD)2B]3 under different incident angles: (a) TM polarization[108]; (b) TE polarization[108].
    Fig. 10. Experimental reflectance spectra of [(CD)2B]3 under different incident angles: (a) TM polarization[108]; (b) TE polarization[108].
    (a) Schematic of the heterostructure M[(CD)2B]3[109]; (b) experimental absorptance spectra of M[(CD)2B]3 under different incident angles (TM polarization)[109].
    Fig. 11. (a) Schematic of the heterostructure M[(CD)2B]3[109]; (b) experimental absorptance spectra of M[(CD)2B]3 under different incident angles (TM polarization)[109].
    Experimental absorptance of M[(CD)2B]3 as a function of incident angle at nm (TM polarization)[109].
    Fig. 12. Experimental absorptance of M[(CD)2B]3 as a function of incident angle at nm (TM polarization)[109].
    (a) Experimental reflectance of M[(CD)2B]3 as a function of incident angle for TM and TE polarizations at nm[108]; (b) corresponding polarization selection ratio as a function of incident angle[108].
    Fig. 13. (a) Experimental reflectance of M[(CD)2B]3 as a function of incident angle for TM and TE polarizations at nm[108]; (b) corresponding polarization selection ratio as a function of incident angle[108].
    Calculated reflectance spectrum of M[(CD)2B]9 as a function of incident angle (TM and TE polarizations)[114].
    Fig. 14. Calculated reflectance spectrum of M[(CD)2B]9 as a function of incident angle (TM and TE polarizations)[114].
    (a) Schematic of the refractive index sensor[114]; (b) calculated minimal refractive index resolution as a function of incident angle[114].
    Fig. 15. (a) Schematic of the refractive index sensor[114]; (b) calculated minimal refractive index resolution as a function of incident angle[114].
    Feng Wu, Zhi-Wei Guo, Jia-Ju Wu, Hai-Tao Jiang, Gui-Qiang Du. Band gap engineering and applications in compound periodic structure containing hyperbolic metamaterials[J]. Acta Physica Sinica, 2020, 69(15): 154205-1
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