Fast and accurate determination of the singlet-triplet gap in donor-acceptor and multiresonance TADF molecules by using hole-hole Tamm-Dancoff approximated density functional theory

Document Type

Article

Publication Date

8-1-2022

Abstract

One of the requirements to design efficient emitters based on the multiresonance (MR)- or donor-acceptor (D-A) thermally activated delayed fluorescence (TADF) materials is a relatively small energy gap between the lowest singlet and triplet excited states (Delta E-ST). High-level ab initio calculations of their Delta E-ST provide benchmark results, but they are very time consuming and little practical for large-size systems. Here, the performances of hole-hole Tamm-Dancoff approximated density functional theory (hh-TDA-DFT) and the functional dependent accuracy of hh-TDA are examined on SE of a large number of MR- and D-A TADF molecules. The results indicate that hh-TDA combined with the hybrid functional B3LYP can predict Delta E-ST values for a wide number of MR-TADF molecules with mean absolute error (MAE) within 0.04 eV with correlation as high as 0.75. For D-A TADF molecules, Delta E-ST is less sensitive to the nature of the functionals, with MAE as low as 0.07 eV. The larger discrepancy between Delta E-ST obtained obtained from hh-TDA-DFT and experimental data in several oxygen-containing MR-TADF molecules is assumed to stem from the aggregation tendency of these compounds in solution. These findings provide important insights on the role of aggregation in reducing the Delta E-ST of of MR-TADF compounds.

Keywords

Aggregation, Hole-hole Tamm-Dancoff approximated density functional theory, Multiresonance thermally activated delayed fluorescence, Singlet-triplet splitting

Divisions

PHYSICS

Funders

Marie Curie Actions (Grant No: 823720),University Malaya Research University (Grant No: GPF086B-2020)

Publication Title

Advanced Theory and Simulations

Volume

5

Issue

8

Publisher

WILEY-V C H VERLAG GMBH

Publisher Location

POSTFACH 101161, 69451 WEINHEIM, GERMANY

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