\begin{document}${\text{μ}}{\rm{m}}$\end{document} to 8.8 \begin{document}${\text{μ}}{\rm{m}}$\end{document}, the real part of the effective refractive index decreases monotonically, the propagation lengths of the fundamental mode and the 1st order modes increase, and the 2nd order modes first increase and then decrease. When changing the elliptical nanowire structure parameters—the length of semi-major axis and semi-minor axis, there are slight influence on the mode characteristics of the fundamental mode and the 1st order modes, but greater influence on those of the 2nd order modes. As the Fermi energy of graphene increases from 0.45 eV to 0.72 eV, in the first five modes, the real part of the effective refractive index decreases, the propagation lengths of the fundamental mode and the 1st order modes increase, the propagation lengths of the 2nd order modes decrease. In addition, the propagation length approaches to 2 \begin{document}${\text{μ}}{\rm{m}}$\end{document} approximately. When the semi-minor axis b = 100 nm and ​\begin{document}${E_{\rm F}} \;{\rm{ = 0}}{\rm{.5}}\;{\rm{eV}}$\end{document}, the curves of the circular nanowire (a = 100 nm) and the elliptical nanowire (a = 140 nm), the real part of the effective refractive index and propagation length with the operating wavelength and the Fermi energy of graphene are compared. Then, the advantages of elliptical nanowire over the circular nanowire are verified. The results of the separation variable method are in good agreement with the results of the finite element method. This work can provide a theoretical basis for the design, fabrication and application of optical waveguides based on graphene-coated elliptical dielectric nanowires."> - 必威体育下载

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    Cheng Xin, Xue Wen-Rui, Wei Zhuang-Zhi, Dong Hui-Ying, Li Chang-Yong
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    • Abstract views:7197
    • PDF Downloads:55
    • Cited By:0
    Publishing process
    • Received Date:26 November 2018
    • Accepted Date:27 December 2018
    • Available Online:01 March 2019
    • Published Online:05 March 2019

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