有机极化发光晶体管
Zhengsheng Qin1,2, Tianyu Wang1, Haikuo Gao1
1Beijing National Laboratory for Molecular Sciences, Key Laboratory of Organic Solids, Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190, China.
Advanced materials (Deerfield Beach, Fla.)
|June 26, 2023
概括
新型有机极化发光晶体管 (OPLET) 实现高极化 (DOP高达0.97),将多个功能集成到单个设备中. 这一突破使先进的光学成像和防伪安全应用成为可能.
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
- 有机电子 有机电子
背景情况:
- 电驱动的极化光源对于量子计算,光通信和3D显示器至关重要.
- 由于复杂的光学元件,传统设备面临着挑战.
- 有机极化发光晶体管 (OPLET) 提供了一个新的,集成的解决方案.
研究的目的:
- 为了展示具有高极化度 (DOP) 的OPLET.
- 调查OPLETs中高效极化辐射背后的机制.
- 展示OPLET在光学成像和安全方面的实际应用.
主要方法:
- 制造集成晶体管和发光功能的有机设备.
- 通过门电压对极化辐射进行电调制.
- 极化特性和设备性能的表征.
主要成果:
- 达到0.97的高极化度 (DOP),接近完全线性极化光.
- 通过门电压调节的强大和高效的极化辐射.
- 成功实施了用于高对比度光学成像和防伪安全的OPLET.
结论:
- OPLET为集成光子和电子设备提供了一个有前途的平台.
- 有机半导体的内平面异极性是实现高极化的关键.
- OPLETs为小型化,芯片上的光电子应用铺平了道路.
相关概念视频
Bipolar Junction Transistor
825
Bipolar Junction Transistors (BJTs) are essential elements in electronic circuits, playing a crucial role in the functionality of amplifiers, memories, and microprocessors. These transistors can be designed as NPN or PNP based on their doping patterns. They consist of three layers: the emitter, base, and collector. The configuration of these layers and their respective doping levels—with N-type or P-type impurities—define the transistor's type and its operational...
825
Biasing of P-N Junction
619
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...
619
MOSFET: Enhancement Mode
391
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
391
Field Effect Transistor
485
Field-effect transistors (FETs) are integral to electronic circuits and distinguished by their three-terminal setup: the gate, drain, and source. These transistors operate as unipolar devices, which utilize either electrons or holes as charge carriers, in contrast to bipolar transistors, which use both types of carriers. The primary function of the FET is to modulate the flow of these carriers from the source to the drain through a channel. The voltage difference between the gate and source...
485
P-N junction
590
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...
590
Working Principle of BJT
593
A Bipolar Junction Transistor (BJT), specifically a PNP transistor in a common-base configuration, effectively amplifies or switches electronic signals by controlling the flow of charge carriers. This discussion focuses on its operation in the active mode.
In the PNP configuration, the emitter is heavily doped with positive charge carriers (holes), while the base is lightly doped with negative carriers (electrons). This setup allows for a forward bias across the emitter-base junction,...
In the PNP configuration, the emitter is heavily doped with positive charge carriers (holes), while the base is lightly doped with negative carriers (electrons). This setup allows for a forward bias across the emitter-base junction,...
593


