A. Deyasi, Ratul Ghosh, P. Chakraborty, Anwesha Adhikary, A. Sarkar
{"title":"填充因子对超材料基二维光子晶体布里渊区影响的研究","authors":"A. Deyasi, Ratul Ghosh, P. Chakraborty, Anwesha Adhikary, A. Sarkar","doi":"10.2174/1876402913666210210155312","DOIUrl":null,"url":null,"abstract":"\n\nFill factor in the negative permittivity materials are tailored within physically permissible limit to characterize the Brillouin zone for two-dimensional crystal under propagation of both s and p-polarized waves. Two lowermost bandgaps are computed along with corresponding midband frequencies, where plane wave expansion method is invoked for computational purpose. Rectangular geometrical shape is considered for the simulation, and all the results are calculated inside the ‘Γ’ point and ‘X’ point of first Brillouin zone. Simulated findings depict monotonous variations of both bandgap width as well as midband frequency for higher negative permittivity materials, when magnitude of fill factor is comparatively low, for both TE (Transverse Electric)and TM (Transverse Magnetic)mode of propagations. Lower negative permittivity leads to random fluctuations which makes it unsuitable for photonic component design. Multiple forbidden regions may be observed for some specific artificial materials which can be utilized in antenna or multi-channel filter design in higher THz region.\n\n\n\nThe present paper aims to compute the shape of the first Brillouin zone from the fill factor for a two-dimensional photonic crystal structure.\n\n\n\n\nEBG (Electromagnetic Band gap) of a photonic crystal plays a major role in determining its candidature for optical applications, which is critically controlled by fill factor. Therefore, it is significant to investigate the effect of F.F on the wave propagation characteristics of 2D PhC(Two-dimensional photonic crystal). \n\n\n\nInvestigation of metamaterial based photonic crystal structure for electromagnetic bandgap analysis in the desired spectrum of interest as a function of fill factor inside the first Brillouin zone \nMethod:Maxwell’s equations are solved using plane wave propagation method to solve the problem, and simulation is carried out in MATLAB® software. \n\n\n\nBoth the first and second photonic bandgaps are simultaneously computed with variation of refractive index differences of the constituent materials as well as with the fill factors. Results are extremely significant about the formation of narrowband and wideband filters on certain material combinations and structural designs. \n\n\n\nBetter tenability is observed for metamaterial structure compared to conventional positive index materials, and fill factor has a great role in shaping the Brillouin zone and corresponding bandgap width. \n\n","PeriodicalId":18543,"journal":{"name":"Micro and Nanosystems","volume":" ","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2021-02-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Investigating Fill Factor Effect on Brillouin Zone of Metamaterial-based 2D Photonic Crystal\",\"authors\":\"A. Deyasi, Ratul Ghosh, P. Chakraborty, Anwesha Adhikary, A. 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引用次数: 0
摘要
负介电常数材料的填充因子在物理允许的范围内进行调整,以表征二维晶体在s和p极化波传播下的布里渊区。计算了两个最低带隙以及相应的中频,其中采用平面波展开法进行计算。模拟采用矩形几何形状,所有结果均在第一布里色区' Γ '点和' X '点内进行计算。模拟结果描述了高负介电常数材料的带隙宽度和中频的单调变化,当填充因子的幅度相对较低时,对于TE(横向电)和TM(横向磁)传播模式。较低的负介电常数导致随机波动,不适合光子元件的设计。对于某些特定的人造材料,可以观察到多个禁区,这些人造材料可以用于天线或高太赫兹区域的多通道滤波器设计。本文的目的是从二维光子晶体结构的填充因子计算第一布里渊带的形状。光子晶体的电磁带隙(EBG)在决定其光学应用的候选性方面起着重要作用,其关键是由填充因子控制的。因此,研究f - f对二维PhC(二维光子晶体)波传播特性的影响具有重要意义。基于超材料的光子晶体结构研究用于电磁带隙分析的期望频谱作为第一布里渊区内填充因子的函数方法:采用平面波传播法求解麦克斯韦方程组,并在MATLAB®软件中进行仿真。根据组成材料折射率差的变化以及填充因子的变化,同时计算了第一和第二光子带隙。窄带和宽带滤波器的形成在一定的材料组合和结构设计上具有重要意义。与传统的正折射率材料相比,超材料结构具有更好的可维持性,填充因子对布里渊带的形成和相应的带隙宽度有很大的影响。
Investigating Fill Factor Effect on Brillouin Zone of Metamaterial-based 2D Photonic Crystal
Fill factor in the negative permittivity materials are tailored within physically permissible limit to characterize the Brillouin zone for two-dimensional crystal under propagation of both s and p-polarized waves. Two lowermost bandgaps are computed along with corresponding midband frequencies, where plane wave expansion method is invoked for computational purpose. Rectangular geometrical shape is considered for the simulation, and all the results are calculated inside the ‘Γ’ point and ‘X’ point of first Brillouin zone. Simulated findings depict monotonous variations of both bandgap width as well as midband frequency for higher negative permittivity materials, when magnitude of fill factor is comparatively low, for both TE (Transverse Electric)and TM (Transverse Magnetic)mode of propagations. Lower negative permittivity leads to random fluctuations which makes it unsuitable for photonic component design. Multiple forbidden regions may be observed for some specific artificial materials which can be utilized in antenna or multi-channel filter design in higher THz region.
The present paper aims to compute the shape of the first Brillouin zone from the fill factor for a two-dimensional photonic crystal structure.
EBG (Electromagnetic Band gap) of a photonic crystal plays a major role in determining its candidature for optical applications, which is critically controlled by fill factor. Therefore, it is significant to investigate the effect of F.F on the wave propagation characteristics of 2D PhC(Two-dimensional photonic crystal).
Investigation of metamaterial based photonic crystal structure for electromagnetic bandgap analysis in the desired spectrum of interest as a function of fill factor inside the first Brillouin zone
Method:Maxwell’s equations are solved using plane wave propagation method to solve the problem, and simulation is carried out in MATLAB® software.
Both the first and second photonic bandgaps are simultaneously computed with variation of refractive index differences of the constituent materials as well as with the fill factors. Results are extremely significant about the formation of narrowband and wideband filters on certain material combinations and structural designs.
Better tenability is observed for metamaterial structure compared to conventional positive index materials, and fill factor has a great role in shaping the Brillouin zone and corresponding bandgap width.