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Top-emitting thermally activated delayed fluorescence organic light-emitting devices with weak light-matter coupling

  • Chunxiu Zang
  • , Shihao Liu*
  • , Mengxin Xu
  • , Ruifang Wang
  • , Chen Cao
  • , Zelin Zhu
  • , Jiaming Zhang
  • , Hui Wang
  • , Letian Zhang
  • , Wenfa Xie*
  • , Chun-Sing Lee*
  • *Corresponding author for this work

Research output: Journal Publications and Reviews › RGC 21 - Publication in refereed journal › peer-review

125 Downloads (CityUHK Scholars)

Abstract

Resonance interaction between a molecular transition and a confined electromagnetic field can lead to weak or strong light-matter coupling. Considering the substantial exciton–phonon coupling in thermally activated delayed fluorescence (TADF) materials, it is thus interesting to explore whether weak light-matter coupling can be used to redistribute optical density of states and to change the rate of radiative decay. Here, we demonstrate that the emission distribution of TADF emitters can be reshaped and narrowed in a top-emitting organic light-emitting device (OLED) with a weakly coupled microcavity. The Purcell effect of weak microcavity is found to be different for TADF emitters with different molecular orientations. We demonstrate that radiative rates of the TADF emitters with vertical orientation can be substantial increased in weakly coupled organic microcavity. These observations can enhance external quantum efficiencies, reduce efficiency roll-off, and improve color-purities of TADF OLEDs, especially for emitters without highly horizontal orientation.
Original languageEnglish
Article number116
JournalLight: Science and Applications
Volume10
Online published3 Jun 2021
DOIs
Publication statusPublished - 2021

Publisher's Copyright Statement

  • This full text is made available under CC-BY 4.0. https://creativecommons.org/licenses/by/4.0/

RGC Funding Information

  • RGC-funded

ESI Highly Cited Papers

  • Highly Cited Paper 2022

ESI Highly Cited Paper Designation Date(s)

  • 20220512
  • 20220908
  • 20220714

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