• Acta Optica Sinica
  • Vol. 40, Issue 6, 0623002 (2020)
Da Teng1、2、*, Kai Wang3、**, Zhe Li4, Qing Cao4, Yanan Tang1、***, Yongzhe Zhao1, Ziyi Liu1, Yunwen Zhang1, and Rongzhen Guo1
Author Affiliations
  • 1School of Physics and Electronic Engineering, Zhengzhou Normal University, Zhengzhou, Henan 450044, China
  • 2Quantum materials research Center, School of Physics and Electronic Engineering, Zhengzhou Normal University, Zhengzhou, Henan 450044, China
  • 3Key Laboratory of Infrared Imaging Materials and Detectors, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
  • 4College of Sciences, Shanghai University, Shanghai 200444, China
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    DOI: 10.3788/AOS202040.0623002 Cite this Article Set citation alerts
    Da Teng, Kai Wang, Zhe Li, Qing Cao, Yanan Tang, Yongzhe Zhao, Ziyi Liu, Yunwen Zhang, Rongzhen Guo. Graphene Gap Plasmonic Waveguide for Deep-Subwavelength Transmission of Mid-Infrared Waves[J]. Acta Optica Sinica, 2020, 40(6): 0623002 Copy Citation Text show less
    Schematic of waveguide structure
    Fig. 1. Schematic of waveguide structure
    Normalized energy distribution of fundamental mode. (a) Normalized energy distribution; (b) |Sz| along y direction
    Fig. 2. Normalized energy distribution of fundamental mode. (a) Normalized energy distribution; (b) |Sz| along y direction
    Graphene plasmon modal properties with respect to frequency. (a) Re(neff) and LP; (b) Aeff/A0 and FM. Here, we set μc=0.5 eV, T=300 K, τ=0.5 ps, R=30 nm, ε1=3, ε2=1, W= 200 nm, H=100 nm, and D=20 nm
    Fig. 3. Graphene plasmon modal properties with respect to frequency. (a) Re(neff) and LP; (b) Aeff/A0 and FM. Here, we set μc=0.5 eV, T=300 K, τ=0.5 ps, R=30 nm, ε1=3, ε2=1, W= 200 nm, H=100 nm, and D=20 nm
    Modal transmission properties with respect to R and D. (a) Re(neff) and LP versus R when D=20 nm; (b) Aeff/A0 and FM versus R when D=20 nm; (c) Re(neff) and LP versus D when R= 30 nm; (d) Aeff/A0 and FM versus D when R= 30 nm
    Fig. 4. Modal transmission properties with respect to R and D. (a) Re(neff) and LP versus R when D=20 nm; (b) Aeff/A0 and FM versus R when D=20 nm; (c) Re(neff) and LP versus D when R= 30 nm; (d) Aeff/A0 and FM versus D when R= 30 nm
    Modal transmission properties with respect to nanowire permittivity and chemical potential of graphene. (a) Re(neff) and LP as functions of ε1 when μc=0.5 eV; (b) Aeff/A0 and FM as functions of ε1 when μc=0.5 eV; (c) Re(neff) and LP as functions of μc when ε1=2; (d)
    Fig. 5. Modal transmission properties with respect to nanowire permittivity and chemical potential of graphene. (a) Re(neff) and LP as functions of ε1 when μc=0.5 eV; (b) Aeff/A0 and FM as functions of ε1 when μc=0.5 eV; (c) Re(neff) and LP as functions of μc when ε1=2; (d)
    Value of permittivityEffective mode index neffMode area Aeff /m2
    237.062+0.278i1.832×10-15
    448.950+0.441i1.616×10-15
    663.776+0.626i1.213×10-15
    879.689+0.811i0.959×10-15
    Table 1. Impact of permittivity of rectangular dielectric on graphene plasmon mode
    Da Teng, Kai Wang, Zhe Li, Qing Cao, Yanan Tang, Yongzhe Zhao, Ziyi Liu, Yunwen Zhang, Rongzhen Guo. Graphene Gap Plasmonic Waveguide for Deep-Subwavelength Transmission of Mid-Infrared Waves[J]. Acta Optica Sinica, 2020, 40(6): 0623002
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