Energy transfer processes in hyperfluorescent organic light-emitting diodes
Affiliation
Department of Chemistry and Biochemistry, The University of ArizonaIssue Date
2022
Metadata
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Royal Society of ChemistryCitation
Cho, E., Hong, M., Yang, Y. S., Cho, Y. J., Coropceanu, V., & Brédas, J.-L. (2022). Energy transfer processes in hyperfluorescent organic light-emitting diodes. Journal of Materials Chemistry C.Journal
Journal of Materials Chemistry CRights
Copyright © The Author(s). This journal is copyright © The Royal Society of Chemistry 2022.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
Hyperfluorescent organic light-emitting diodes (OLEDs) are based on a combination of molecules displaying thermally activated delayed fluorescence (TADF) and of fluorescent emitters embedded into a host matrix; excitons formed on the TADF molecules are expected to transfer to the fluorescent emitters. As a result, device performance strongly depends on the efficiency of the relevant energy transfer processes. Here, we investigate the morphology, excited-state properties, and energy-transfer processes in a ternary TBRb:4CzIPN:mCBP blend by using complementary molecular dynamics simulations and density functional theory calculations. The results indicate that the rate constants for singlet exciton energy transfer from 4CzIPN (TADF) molecules to TBRb fluorescent emitters are about three orders of magnitude larger than both the intersystem crossing (ISC) and radiative decay rate constants of 4CzIPN; thus, the vast majority of the singlet 4CzIPN excitons can efficiently transfer to the emitters. In contrast, the transfer of triplet excitons from 4CzIPN to the emitters is limited due to a fast reverse ISC (RISC) transition. Also, it is found that singlet and triplet energy transfer from mCBP to 4CzIPN and TBRb is very efficient. As a result of quasi resonance between the emissive first excited state and the second triplet state of TBRb, not all triplet excitons that reach TBRb are lost since part of them can convert into singlet excitons via a RISC process. © 2022 The Royal Society of ChemistryNote
12 month embargo; first published: 10 January 2022ISSN
2050-7534Version
Final published versionae974a485f413a2113503eed53cd6c53
10.1039/d1tc05090g

