在有机设备中,电光发射和光伏转换的共存之路
Taku Oono1, Yusuke Aoki2, Tsubasa Sasaki1
1Japan Broadcasting Corporation (NHK), Science & Technology Research Laboratories, Setagaya-ku, Tokyo, Japan.
Nature communications
|December 7, 2025
概括
这项研究引入了新型有机材料,可以同时实现高电解发光 (EL) 和功率转换效率 (PCE). 这些进步克服了以前的权衡,使高效的多功能光电子设备成为可能.
科学领域:
- 有机电子学有机电子学
- 材料科学是一种材料科学.
- 光电学是指光电子产品.
背景情况:
- 在单个有机器件中实现高电解发光 (EL) 效率和功率转换效率 (PCE) 是具有挑战性的,因为设计原则相互矛盾.
- 传统的方法往往会导致妥协,限制设备的性能.
研究的目的:
- 开发具有高EL和PCE的多功能有机设备.
- 为了克服有机光电子产品中固有的效率权衡.
主要方法:
- 使用具有强吸收和高排放效率的多重共振热激活延迟光 (TADF) 材料.
- 精确控制的电荷转移状态在输送器/接收器接口.
- 制造的多功能设备具有可调节的发射颜色.
主要成果:
- 在单个设备中实现了高EL和光伏 (PV) 效率的共存.
- 证明了全谱可见的电解发光 (蓝色到红色,包括白色).
- 优化的设备实现了EL的外部量子效率 (EQE) 超过8.5%,绿色和色发射器的PCE约为0.5%.
结论:
- 通过战略性材料设计,成功地减轻了有机设备的效率权衡.
- 开辟了诸如自动供电显示器和照明等应用的新可能性.
- 进步了有机光电子技术领域.
相关概念视频
Photoluminescence: Applications
962
Photoluminescence offers a wide range of applications due to its inherent sensitivity and selectivity. This technique allows for both direct and indirect analyses of the analyte. Direct quantitative analysis is possible when the analyte exhibits a favorable quantum yield for fluorescence or phosphorescence. However, an indirect analysis may be feasible if the analyte is not fluorescent or phosphorescent, or if the quantum yield is unfavorable. Indirect methods include reacting the analyte with...
962
Photoluminescence: Fluorescence and Phosphorescence
3.4K
Photoluminescence is a process where a molecule absorbs light energy and re-emits it in the form of light. This phenomenon occurs when a substance absorbs photons, promoting its electrons to higher energy level excited states, followed by a relaxation process in which the electrons return to their original ground state energy levels and emit light. Photoluminescence is widely observed in various materials, including semiconductors, and organic and inorganic compounds.
A pair of electrons in a...
A pair of electrons in a...
3.4K
P-N junction
1.1K
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...
1.1K
Photoelectric Effect
38.7K
When light of a particular wavelength strikes a metal surface, electrons are emitted. This is called the photoelectric effect. The minimum frequency of light that can cause such emission of electrons is called the threshold frequency, which is specific to the metal. Light with a frequency lower than the threshold frequency, even if it is of high intensity, cannot initiate the emission of electrons. However, when the frequency is higher than the threshold value, the number of electrons ejected...
38.7K
Thermal and Photochemical Electrocyclic Reactions: Overview
2.9K
Electrocyclic reactions are reversible reactions. They involve an intramolecular cyclization or ring-opening of a conjugated polyene. Shown below are two examples of electrocyclic reactions. In the first reaction, the formation of the cyclic product is favored. In contrast, in the second reaction, ring-opening is favored due to the high ring strain associated with cyclobutene formation.
2.9K
Photochemical Electrocyclic Reactions: Stereochemistry
2.2K
The absorption of UV–visible light by conjugated systems causes the promotion of an electron from the ground state to the excited state. Consequently, photochemical electrocyclic reactions proceed via the excited-state HOMO rather than the ground-state HOMO. Since the ground- and excited-state HOMOs have different symmetries, the stereochemical outcome of electrocyclic reactions depends on the mode of activation; i.e., thermal or photochemical.
Selection Rules: Photochemical Activation
Selection Rules: Photochemical Activation
2.2K


