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Planar THz electromagnetic graphene pass-band filter with low polarization and angle of incidence dependencies

机译:具有低极化和入射角依赖性的平面THz电磁石墨烯通带滤波器

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摘要

We propose and analyze a graphene electromagnetic filter for the terahertz ( THz) region. The filter represents a planar square array of graphene elements. A unit cell of the array is formed by two coaxial graphene rings placed on the opposite sides of a thin dielectric substrate. The two electromagnetically coupled rings resonate with dipole plasmonic modes. The rings have slightly different dimensions and consequently different yet close individual resonant frequencies. At a frequency lying between these two resonances, the currents in the two interacting rings have opposite directions. This leads to a suppression of the reflected from the array waves and consequently to a high transmission through the array. For the chemical potential of the graphene mu(c) = 0.6 eV, the calculated quality factor of this resonant mode is Q = 5 at the frequency f = 0.8 THz. At this frequency, the reflection coefficient of the array equals -36 dB and the transmission peak which is defined by the graphene losses is -1.8 dB. We show that the frequency position of the transmission peak can be varied in a wide range by the graphene chemical potential. (C) 2015 Optical Society of America
机译:我们提出并分析了太赫兹(THz)区域的石墨烯电磁滤波器。过滤器代表石墨烯元素的平面正方形阵列。阵列的晶胞由放置在薄介电基板相对两侧的两个同轴石墨烯环形成。两个电磁耦合的环以偶极子等离子体模式共振。环的尺寸略有不同,因此各个谐振频率也不同但接近。在这两个共振之间的频率处,两个相互作用的环中的电流具有相反的方向。这导致抑制了来自阵列波的反射,并因此导致通过阵列的高透射率。对于石墨烯的化学势mu(c)= 0.6 eV,在频率f = 0.8 THz时,该共振模式的计算品质因数为Q = 5。在此频率下,阵列的反射系数等于-36 dB,由石墨烯损耗定义的透射峰为-1.8 dB。我们表明,透射峰的频率位置可以通过石墨烯化学势在很宽的范围内变化。 (C)2015年美国眼镜学会

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