概括
这项研究引入了一种新的光学交换机,使用拓光子晶体和奇拉极化光来实现高效的芯片内光学通信. 新的设计使复杂的逻辑操作具有较小的足迹和比传统方法更高的对比度.
科学领域:
- 光子学和光学工程 光子学和光学工程
- 凝聚物质物理学 凝聚物质物理学
- 纳米技术 纳米技术
背景情况:
- 芯片上的光通信和网络需要高效的光学交换机来进行逻辑操作和通道控制.
- 传统的波长选择性光学开关用于复杂的逻辑操作通常涉及重的设计和复杂的系统集成.
- 现有的光学开关方法可能受到设备足迹和系统复杂性的限制.
研究的目的:
- 提出和演示基于拓光子晶体的紧而高效的1x1和2x1光学交换机.
- 为了利用由奇拉极化光激发的单向合,以提高光学开关性能.
- 使用拟议的光学开关设计实现基本逻辑门 (NOR,AND,NAND,XOR,OR).
主要方法:
- 制造一个六边形的光子晶体,通过打破空间反转对称来创建一个山谷拓边缘.
- 使用单向合,由左手/右手循环偏振光激发,在三角共振腔内.
- 实现频率共振和空腔长度调整,以实现所需的逻辑门功能.
主要成果:
- 实现了1x1拓光子晶体光学开关,具有22.8dB的高开关对比度.
- 使用2x1光学开关成功演示了五种类型的逻辑门 (NOR,AND,NAND,XOR,OR).
- 实现的逻辑门在一个紧的足迹 (<14.76 × 12.78 μm2) 中显示了5.9dB和19.3dB之间的逻辑对比.
结论:
- 建议使用拓光子晶体的极化转换策略为芯片上的被动光学网络提供了一条新的途径.
- 该设备利用单向激发和拓性质的稳定性来实现高效的光学切换.
- 这项工作为开发先进的芯片上光学计算和通信系统提供了基础.
相关概念视频
Dielectric Polarization in a Capacitor
4.5K
The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
4.5K
Potential Due to a Polarized Object
349
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
349
Biasing of P-N Junction
361
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
361
P-N junction
410
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
410


