Meng Haiyu, Wang Lingling, Liu Guidong, Xue Xiongxiong, Lin Qi, Zhai Xiang
Appl Opt. 2017 Jul 20;56(21):6022-6027. doi: 10.1364/AO.56.006022.
We numerically investigate the optical performance of a periodically patterned H-shaped graphene array by the finite-difference time-domain (FDTD) in the mid-infrared region. The simulated results reveal that absorption spectra of the proposed structure consist of two dramatic narrowband perfect absorption peaks located at 6.3 μm (Mode 1) and 8.6 μm (Mode 2) with high absorption coefficients of 99.65% and 99.80%, respectively. Two impressive absorption bandwidths that are the full width at half-maximum (FWHM) of the resonant frequency of 90 nm and 188 nm are obtained. The dipole resonance mode is supported by graphene ribbon at a wavelength of 6.3 μm. While the other absorption, attributed to the hybridized mode, is a new resonance that is different from the dipole resonance. The spectral position of the absorption peaks can be dynamically tuned by controlling the refractive index of the dielectric and the Fermi energy of graphene. Furthermore, we can obtain multispectral absorption peaks by applying multilayer graphene arrays. These design approaches enable us to control the number of absorption spectra and such absorbers will benefit the easy-to-fabricate nanophotonic devices for optical filtering, thermal detectors, and electromagnetic wave energy storage.
我们采用时域有限差分法(FDTD)对周期性图案化的H形石墨烯阵列在中红外区域的光学性能进行了数值研究。模拟结果表明,所提出结构的吸收光谱由位于6.3μm(模式1)和8.6μm(模式2)处的两个显著的窄带完美吸收峰组成,其吸收系数分别高达99.65%和99.80%。获得了两个令人印象深刻的吸收带宽,即谐振频率半高宽(FWHM)分别为90nm和188nm。石墨烯带在波长6.3μm处支持偶极子共振模式。而另一种吸收归因于杂化模式,是一种不同于偶极子共振的新共振。通过控制电介质的折射率和石墨烯的费米能量,可以动态调节吸收峰的光谱位置。此外,通过应用多层石墨烯阵列,我们可以获得多光谱吸收峰。这些设计方法使我们能够控制吸收光谱的数量,并且这样的吸收器将有利于制造用于光学滤波、热探测器和电磁波能量存储的易于制造的纳米光子器件。