具有各向同性液晶的偏振无关电光波导

F. Costache, Martin Blasl, K. Bornhorst
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引用次数: 1

摘要

电光诱导波导可用于光纤网络中的光功率控制和光信号的分配。这种类型的波导由于其非机械的工作原理而确保了可靠的工作。然而,由场致双折射效应引起的极化依赖行为限制了它们的实际应用。本文报道了一种减少各向同性液晶芯电光诱导波导中极化相关损耗的方法。该概念设计通过采用优化的电极排列,可以对电场分布进行可控调整,电场分布负责诱导和塑造光学模式。在这种新的波导结构中,TM和TE模式在空间上共存,并且以类似的方式被引导。为了证明这一概念,已经设计和制造了1×1和1×2光输入输出配置的直波导和弯曲波导。利用有限元模拟对电极排列和单模波导几何结构进行了优化。采用体硅微加工技术制备了这些波导。特别地,所制造的器件由两个加工过的硅衬底组成,其中包含一个液晶层。在不同驱动电压下测试的器件显示出TE和TM模式的传输功率相当。在超过20 dB宽的动态衰减范围内获得了极低的极化相关损耗。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Polarization independent electro-optical waveguides with liquid crystals in isotropic phase
Electro-optically induced waveguides can be used in fiber optic networks for optical power control and the distribution of optical signals transmitted over optical fibers. Reliable operation is ensured with this type of waveguides due to their non-mechanical principle of operation. Their polarization dependent behavior caused by field-induced birefringence effects may limit however their practical applications. We report on a method to reduce the polarization dependent loss in electro-optically induced waveguides with a core made of liquid crystals in isotropic phase. The concept design enables a controlled adjustment of the electric field distribution, which is responsible for inducing and shaping the optical mode, by employing an optimized electrode arrangement. In this new waveguide structure, the TM and TE modes coexist spatially and are guided in a similar way. In order to demonstrate this concept, straight and bending waveguides in 1×1 and 1×2 light input to output configurations have been designed and fabricated. The electrode arrangement and single mode waveguide geometry were optimized using FEM simulations. Bulk silicon micromachining was used to fabricate these waveguides. In particular, the manufactured device consisted of two processed silicon substrates with a liquid crystal layer enclosed in between. Devices tested with varying driving voltage have revealed comparable transmitted power for both TE and TM modes. Very low polarization dependent losses over a more than 20 dB wide dynamic attenuation range have been obtained.
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