Broadband polarization-insensitive amplitude and phase modulators based on graphene-covered buried and ridge silicon waveguides
Autor: | Mahmood Hosseini-Farzad, Mohamad Najafi-Hajivar |
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Rok vydání: | 2020 |
Předmět: |
Materials science
Graphene business.industry 02 engineering and technology 021001 nanoscience & nanotechnology Polarization (waves) 01 natural sciences Atomic and Molecular Physics and Optics Electronic Optical and Magnetic Materials law.invention 010309 optics Amplitude modulation Wavelength Amplitude Optics Optical modulator law 0103 physical sciences Electrical and Electronic Engineering Physical and Theoretical Chemistry 0210 nano-technology business Phase modulation Waveguide |
Zdroj: | Optics Communications. 472:125860 |
ISSN: | 0030-4018 |
DOI: | 10.1016/j.optcom.2020.125860 |
Popis: | In this paper, four easy-to-fabricate graphene-based Si waveguide modulators are presented to overcome the strong polarization dependency of graphene-based modulators. The modulation features of two newly proposed structures, i.e. two graphene-based buried silicon waveguides in addition to two standard ridge silicon waveguides at the telecommunication wavelength of λ = 1 . 55 μ m are studied. The results show that for certain widths of each waveguide (the height is constant), the amplitude and phase modulations clearly become polarization-insensitive. The amplitude modulation depths for both the TE and TM modes are equal for these optimized waveguides with the precision of 1 0 − 3 dB/ μ m . Moreover, in the proposed modulators, the maximum variations of the real parts of the effective mode indices (EMI) for both the TE and TM modes coincide with each other with an excellent precision ( 1 0 − 4 ). This precision value is much smaller than the standard criterion value for confirming a polarization-insensitive phase modulation. For proposed structures, the average modulation depth (MD) and maximum variation of the real parts of EMI are about 0 . 3 dB/ μ m and 0.02 respectively. Thus, it means to clearly imply small footprints for both amplitude and phase modulations. Furthermore, the performances of all the structures are studied for all optical telecommunication wavelengths. Even without making any changes to the structures designed at 1 . 55 μ m at appropriate wavelength intervals, the structures exhibit polarization-insensitive behaviors. |
Databáze: | OpenAIRE |
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