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Sub-Second Long Lifetime Triplet Exciton Reservoir for Highly Efficient and Stable Organic Light-Emitting Diode.
Tang, Zhenyu; Lyu, Fang; Gu, Jiannan; Guo, Haoqing; Yu, Wenjin; Zou, Yu; Gong, Lefan; Tang, Rong; Qu, Bo; Guo, Xuan; Chen, Yan; Deng, Yongkai; Bian, Mengying; Li, Yan; Zhang, Dongdong; Wei, Mingyang; Park, So Min; Xia, Pan; Lv, Yao; Gong, Qihuang; Wang, Shufeng; Chen, Zhijian; Xiao, Lixin.
Afiliação
  • Tang Z; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Lyu F; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Gu J; Department of Physics, The University of Tokyo, Tokyo, 113-0033, Japan.
  • Guo H; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Yu W; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Zou Y; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Gong L; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Tang R; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Qu B; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Guo X; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Chen Y; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Deng Y; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Bian M; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Li Y; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Zhang D; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Wei M; Yangtze Delta Institute of Optoelectronics, Peking University, Nantong, 226010, P. R. China.
  • Park SM; Key Lab of Organic Optoelectronics and Molecular Engineering of Ministry of Education, Department of Chemistry, Tsinghua University, Beijing, 100084, P. R. China.
  • Xia P; Department of Electrical and Computer Engineering, University of Toronto, Toronto, M5S 3G4, Canada.
  • Lv Y; Department of Electrical and Computer Engineering, University of Toronto, Toronto, M5S 3G4, Canada.
  • Gong Q; Department of Electrical and Computer Engineering, University of Toronto, Toronto, M5S 3G4, Canada.
  • Wang S; Beijing Green Guardee Technology Co. Ltd., Beijing 102299, P. R. China.
  • Chen Z; State Key Laboratory of Artificial Microstructure and Mesoscopic Physics, School of Physics, Peking University, Beijing, 100871, P. R. China.
  • Xiao L; Yangtze Delta Institute of Optoelectronics, Peking University, Nantong, 226010, P. R. China.
Adv Mater ; 36(21): e2313746, 2024 May.
Article em En | MEDLINE | ID: mdl-38332722
ABSTRACT
In organic light-emitting diode (OLED), achieving high efficiency requires effective triplet exciton confinement by carrier-transporting materials, which typically have higher triplet energy (ET) than the emitter, leading to poor stability. Here, an electron-transporting material (ETM), whose ET is 0.32 eV lower than that of the emitter is reported. In devices, it surprisingly exhibits strong confinement effect and generates excellent efficiency. Additionally, the device operational lifetime is 4.9 times longer than the device with a standard ETM, 1,3,5-tri(1-phenyl-1H-benzo[d]imidazol-2-yl) phenyl (whose ET 0.36 eV is higher than the emitter). This anomalous finding is ascribed to the exceptionally long triplet state lifetime (≈0.2 s) of the ETM. It is named as long-lifetime triplet exciton reservoir effect. The systematic analysis reveals that the long triplet lifetime of ETM can compensate the requirement for high ET with the help of endothermic energy transfer. Such combination of low ET and long lifetime provides equivalent exciton confinement effect and high molecular stability simultaneously. It offers a novel molecular design paradigm for breaking the dilemma between high efficiency and prolonged operational lifetime in OLEDs.
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Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Adv Mater Assunto da revista: BIOFISICA / QUIMICA Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Adv Mater Assunto da revista: BIOFISICA / QUIMICA Ano de publicação: 2024 Tipo de documento: Article
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