论文标题
阻抗匹配的平面超材料光束转向Terahertz Wave
Impedance-Matched Planar Metamaterial Beam Steerer for Terahertz Waves
论文作者
论文摘要
Terahertz结构域中具有可量身定制电磁特性的平面超材料提供了定制的光学溶液,这些解决方案是成像和光谱系统开发所需的。特别是,超材料具有替代常规笨重光学元件的潜力,或者可能是完全新颖的设备的基本构建块。在这方面,可以将超材料设计成与其他有关其电磁特性的材料的阻抗匹配是有利的。在这里,我们设计,制造和调查具有可定制的折射率和阻抗匹配空间的超材料。单位电池由两对切割系组成,这些切割线几乎可以独立控制电磁波的电和磁反应。对于具有均匀有效折射率为1.18的超材料的示例,我们在实验上证明了超过90%的振幅传播,在工作频率为0.444THz的情况下,振幅传播约为90%,反射率约为5%。作为一种更具功能的设备,我们用线性折射率梯度从1.14到2.66制造了Terahertz梯度指数梁驱动器。我们通过数值模拟电磁波传播通过光束转向器,并将偏转波的电场幅度与Terahertz场分布进行比较,该电场幅度在横梁转向器后面测量的Terahertz Terahertz时间域光谱仪后面测量。 6.1°的数值模拟挠度角与测得的挠度角度为5.95°非常吻合。测得的峰值转向器的峰值振幅传输近90%,这也与模拟值约为88%非常吻合。
Planar metamaterials with tailorable electromagnetic properties in the terahertz domain offer customized optics solutions that are needed for the development of imaging and spectroscopy systems. In particular, metamaterials carry the potential to substitute conventional bulky optics or can be basic building blocks for completely novel devices. In this respect it is advantageous that metamaterials can be devised to be impedance-matched to another material regarding their electromagnetic properties. Here, we design, fabricate and investigate a metamaterial with tailorable refractive index and impedance-matching to free space. The unit cell is comprised of two different pairs of cut-wires that provide almost independent control over the electric and magnetic response to an electromagnetic wave. For the example of a metamaterial with a uniform effective refractive index of 1.18, we experimentally demonstrate an amplitude transmission of more than 90% and a reflectivity of about 5% at a working frequency of 0.444THz. As a more functional device, we fabricate a terahertz gradient index beam steerer with a linear refractive index gradient from 1.14 to 2.66. We numerically simulate the electromagnetic wave propagation through the beam steerer and compare the electric field amplitude of the deflected wave with the terahertz field distribution that is measured behind the beam steerer in an imaging terahertz time-domain spectroscope. The numerically simulated deflection angle of 6.1° agrees well with the measured deflection angle of 5.95°. The measured peak amplitude transmission of the beam steerer amounts to almost 90%, which also agrees well with a simulated value of approximately 88%.