控制在石墨烯中的光热电定向光电流,带宽超过400 GHz
Stefan M Koepfli1, Michael Baumann2, Robin Gadola2
1ETH Zurich, Institute of Electromagnetic Fields (IEF), Zurich, Switzerland. stefan.koepfli@ief.ee.ethz.ch.
Nature communications
|August 26, 2024
概括
我们开发了一种自动供电的石墨烯光探测器,其频率响应超过400GHz. 该设备利用光热电效应进行快速,零偏差的红外探测,性能优于其他技术.
科学领域:
- 光电学是指光电子产品.
- 材料科学 材料科学 材料科学
- 纳米技术纳米技术
背景情况:
- 红外光探测需要具有特定吸收性质的成本效益高的材料.
- 石墨烯独特的光电子特性为宽带红外探测提供了潜力.
- 现有的石墨烯光探测器往往需要复杂的优化,以实现高速,低噪音的操作.
研究的目的:
- 为了演示具有超高频响应的自动供电石墨烯光探测器.
- 调查光热电流用于快速光检测的使用.
- 探索石墨烯在先进的红外传感应用中的潜力.
主要方法:
- 石墨烯与超材料完美吸收架构的整合.
- 使用不对称的共振器来诱导定向光电流.
- 光探测器的频率响应和检测机制的特征.
主要成果:
- 实现了一种自动供电的石墨烯光探测器,其频率响应超过400 GHz.
- 观察到与光热电效应相关的近似瞬间反应.
- 证明漂移/扩散时间优化对于高速性能是不必要的.
结论:
- 石墨烯中的光热电定向光电流为超快,零偏差光探测器提供了一条道路.
- 这种方法超过了许多现有的石墨烯光探测器的带宽限制.
- 开发的技术对下一代红外传感有前途.
相关概念视频
Biasing of Metal-Semiconductor Junctions
230
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
230
Biasing of P-N Junction
469
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...
469


