有机发光二极管
材料科学
激子
电致发光
荧光
兴奋剂
光电子学
共发射极
原子物理学
激发态
单重态
量子效率
纳米技术
光学
物理
凝聚态物理
图层(电子)
作者
Chengwei Lin,Pengbo Han,Shu Xiao,Fenlan Qu,Jingwen Yao,Xianfeng Qiao,Dezhi Yang,Yanfeng Dai,Qian Sun,Dehua Hu,Anjun Qin,Yuguang Ma,Ben Zhong Tang,Dongge Ma
标识
DOI:10.1002/adfm.202106912
摘要
Abstract Aggregation‐induced emission (AIE) and hybridized local and charge‐transfer (HLCT) materials are two kinds of promising electroluminescence systems for the fabrication of high‐efficiency organic light‐emitting diodes (OLEDs) by harnessing “hot excitons” at the high‐lying triplet exciton states (T n , n ≥ 2). Nonetheless, the efficiency of the resulting OLEDs did not meet expectations due to the possible loss of T n →T n −1 . Herein, experimental results and theoretical calculations demonstrate the “hot exciton” process between the high‐lying triplet state T 3 and the lowest excited singlet state S 1 in an AIE material 4⁗‐(diphenylamino)‐2″,5″‐diphenyl‐[1,1″:4′,1″:4″,1′″:4′″,1⁗‐quinquephenyl]‐4‐carbonitrile (TPB‐PAPC) and it is found that the Förster resonance energy transfer (FRET) between two molecules can facilitate the “hot exciton” process and inhibit the T 3 →T 2 loss by doping a blue fluorescent emitter in TPB‐PAPC. Finally, the doped TPB‐PAPC blue OLEDs achieve a maximum external quantum efficiency (EQE max ) of 9.0% with a small efficiency roll‐off. Furthermore, doping the blue fluorescent emitter in a HLCT material 2‐(4‐(10‐(3‐(9 H ‐carbazol‐9‐yl)phenyl)anthracen‐9‐yl)phenyl)‐1‐phenyl‐1 H ‐phenanthro[9,10‐ d ] imidazole (PAC) is used as the emission layer, and the resulting blue OLEDs exhibit an EQE max of 17.4%, realizing the efficiency breakthrough of blue fluorescence OLEDs. This work establishes a physical insight in the design of high‐performance “hot exciton” molecules and the fabrication of high‐performance blue fluorescence OLEDs.
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