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Angular selection of incident waves by photonic crystals with position-varying Dirac points at the Brillouin zone boundary

机译:在布里渊区边界处具有位置变化的狄拉克点的光子晶体对入射波的角度选择

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摘要

We demonstrate the angular selection of incident electromagnetic waves using photonic crystals (PCs) composed of a square lattice of dielectric rods which exhibit position-varying Dirac conical dispersion at the Brillouin zone boundary. At the frequency of the Dirac point, the transmittance can reach unity at a particular incident angle associated with the Dirac dispersion, while for all other incident angles the waves are reflected due to the existence of a directional photonic band gap. By changing the size of the dielectric rods, the position of the Dirac point at the Brillouin zone boundary is variable, which makes the unity transmission angle customizable. Interestingly, we show that such a scheme of angular selection is almost independent of the refractive index of the background medium, as long as it is not too large so that a diffraction effect emerges. By investigating the PC being sandwiched by two different types of media, we find it actually acts as an optical 0 or π phase modulator at that particular incident angle. By attaching a metasurface to the PC, angular selection in the reflection geometry can also be achieved. Our work establishes a systematic and efficient method to achieve angular selection of arbitrary incident waves based on Dirac dispersions.
机译:我们演示了使用光子晶体(PCs)入射电磁波的角度选择,该光子晶体由电介质棒的方格子组成,这些电棒在布里渊区边界处表现出随位置变化的狄拉克圆锥形弥散。在狄拉克点的频率处,在与狄拉克色散相关的特定入射角处,透射率可以达到单位,而对于所有其他入射角,由于方向性光子带隙的存在,反射波。通过改变电介质棒的尺寸,在布里渊区边界处的狄拉克点的位置是可变的,这使得可定制统一的透射角。有趣的是,我们证明了这种角度选择方案几乎与背景介质的折射率无关,只要它不会太大而出现衍射效应即可。通过研究被两种不同类型的介质夹在中间的PC,我们发现它实际上在该特定入射角下充当光学0或π相位调制器。通过将超表面连接到PC,还可以实现反射几何形状的角度选择。我们的工作建立了一种系统且有效的方法,以基于Dirac色散实现对任意入射波的角度选择。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2016年第24期|245116.1-245116.5|共5页
  • 作者单位

    College of Physics, Optoelectronics and Energy & Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China;

    Department of Physics, Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong;

    College of Physics, Optoelectronics and Energy & Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China;

    College of Physics, Optoelectronics and Energy & Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China;

    Department of Physics, Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong;

    College of Physics, Optoelectronics and Energy & Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China;

    College of Physics, Optoelectronics and Energy & Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China;

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