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Study on Transmission Characteristics and Bandgap Types of Plasma Photonic Crystal
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A plasma photonic crystal (PPC) was formed using an array of discharge plasma tubes. The transmission spectra and bandstructure of PPCs with different lattice types under different polarization modes were studied through simulation and measurement. To study the types of bandgap in PPCs, the bandstructure of the PPC is calculated using symplectic finite difference time domain (SFDTD), a modified plane wave expansion (PWE) method, and a finite element method (FEM) based on weak form equations. The bandstructure of the PPC is compared with the transmission curve results. The results show that the bandgap is stable in the PPC, and the experimental and numerical results of the transmission spectra agree well. There are different types of bandgap in the PPC; the bandgap under TE-like polarization is caused by localized surface plasmon (LSP) and Bragg scattering. The bandgap under TM-like polarization is caused by the cutoff effect of plasma on the electromagnetic wave and Bragg scattering. The lattice type also affects the position and number of the bandgap. The three methods have their advantages and disadvantages when calculating bandstructure. Therefore, it is necessary to combine the results of three methods and experimental results to accurately determine the bandgap type of the PPC.
Title: Study on Transmission Characteristics and Bandgap Types of Plasma Photonic Crystal
Description:
A plasma photonic crystal (PPC) was formed using an array of discharge plasma tubes.
The transmission spectra and bandstructure of PPCs with different lattice types under different polarization modes were studied through simulation and measurement.
To study the types of bandgap in PPCs, the bandstructure of the PPC is calculated using symplectic finite difference time domain (SFDTD), a modified plane wave expansion (PWE) method, and a finite element method (FEM) based on weak form equations.
The bandstructure of the PPC is compared with the transmission curve results.
The results show that the bandgap is stable in the PPC, and the experimental and numerical results of the transmission spectra agree well.
There are different types of bandgap in the PPC; the bandgap under TE-like polarization is caused by localized surface plasmon (LSP) and Bragg scattering.
The bandgap under TM-like polarization is caused by the cutoff effect of plasma on the electromagnetic wave and Bragg scattering.
The lattice type also affects the position and number of the bandgap.
The three methods have their advantages and disadvantages when calculating bandstructure.
Therefore, it is necessary to combine the results of three methods and experimental results to accurately determine the bandgap type of the PPC.
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