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Graphene-based optical absorbers in middle-infrared wavelengths

机译:基于石墨烯的光学吸收器中的中红外波长

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In the visible and near infrared regions, graphene is essentially transparent with a constant absorptivity of 2.3%. On contrast, in longer wavelengths, the absorptivity can be enhanced by graphene plasmons motivated by simple nanostructures. Besides, the graphene plasmons can be further enhanced via electrostatic doping when voltage is applied. This work numerically demonstrates that in optimized configuration the absorptance in monolayer graphene can be greatly enhanced and reach to 98.6% of the impinging light for transverse magnetic (TM) polarizations. Graphene can interact with light via plasmonic resonance. Towards this, we utilize a subwavelength-thick optic cavity, which composed of graphene grating, a dielectric spacing layer and a metal film to further enhance the interaction. When we use the TM mode source, the incident light matched the graphene plasmons, a strong drastic cut in the energy of the reflected light, which means obvious resonance absorption occurred. Meanwhile, the reflection can approach 0 when voltage applied. Finally, great absorption in 6.94 μm has been achieved by the graphene grating with the addition of a subwavelength-thick optic cavity via different voltage.
机译:在可见光和近红外区域中,石墨烯基本上是透明的,恒定吸收率为2.3%。相比之下,在更长的波长中,通过简单的纳米结构激励的石墨烯等离子体可以增强吸收性。此外,当施加电压时,可以通过静电掺杂进一步增强石墨烯等离子体。这项工作以数字方式表明,在优化配置中,可以大大提高单层石墨烯的吸收率,达到横向磁(TM)偏振的撞击光的98.6%。石墨烯可以通过等离子体共振与光相互作用。朝向这一点,我们利用了由石墨光栅,介电空间层和金属膜构成的亚壳长厚的光学腔,以进一步增强相互作用。当我们使用TM模式源时,入射光匹配石墨烯等离子体,在反射光的能量中匹配强烈的切割,这意味着发生明显的共振吸收。同时,当施加电压时,反射可以接近0。最后,通过通过不同电压加入亚波长厚的光学腔的石墨烯光栅实现了6.94μm的极大吸收。

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