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TDDFT versus GW/BSE Methods for Prediction of Light Absorption and Emission in a TADF Emitter
[Image: see text] Design concepts for organic light emitting diode (OLED) emitters, which exhibit thermally activated delayed fluorescence (TADF) and thereby achieve quantum yields exceeding 25%, depend on singlet–triplet splitting energies of order kT to allow reverse intersystem crossing at ambien...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9806837/ https://www.ncbi.nlm.nih.gov/pubmed/36515973 http://dx.doi.org/10.1021/acs.jpca.2c06403 |
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author | Chaudhuri, D. Patterson, C. H. |
author_facet | Chaudhuri, D. Patterson, C. H. |
author_sort | Chaudhuri, D. |
collection | PubMed |
description | [Image: see text] Design concepts for organic light emitting diode (OLED) emitters, which exhibit thermally activated delayed fluorescence (TADF) and thereby achieve quantum yields exceeding 25%, depend on singlet–triplet splitting energies of order kT to allow reverse intersystem crossing at ambient temperatures. Simulation methods for these systems must be able to treat relatively large organic molecules, as well as predict their excited state energies, transition energies, singlet–triplet splittings, and absorption and emission cross sections with reasonable accuracy, in order to prove useful in the design process. Here we compare predictions of TDDFT with M06-2X and ωB97X-D exchange-correlation functionals and a G(o)W(o)@HF/BSE method for these quantities in the well-studied DPTZ-DBTO2 TADF emitter molecule. Geometry optimization is performed for ground state (GS) and lowest donor–acceptor charge transfer (CT) state for each functional. Optical absorption and emission cross sections and energies are calculated at these geometries. Relaxation energies are on the order of 0.5 eV, and the importance of obtaining excited state equilibrium geometries in predicting delayed fluorescence is demonstrated. There are clear trends in predictions of G(o)W(o)@HF/BSE, and TDDFT/ωB97X-D and M06-2X methods in which the former method favors local exciton (LE) states while the latter favors DA CT states and ωB97X-D makes intermediate predictions. G(o)W(o)@HF/BSE suffers from triplet instability for LE states but not CT states relevant for TADF. Shifts in HOMO and LUMO levels on adding a conductor-like polarizable continuum model dielectric background are used to estimate changes in excitation energies on going from the gas phase to a solvated molecule. |
format | Online Article Text |
id | pubmed-9806837 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-98068372023-01-03 TDDFT versus GW/BSE Methods for Prediction of Light Absorption and Emission in a TADF Emitter Chaudhuri, D. Patterson, C. H. J Phys Chem A [Image: see text] Design concepts for organic light emitting diode (OLED) emitters, which exhibit thermally activated delayed fluorescence (TADF) and thereby achieve quantum yields exceeding 25%, depend on singlet–triplet splitting energies of order kT to allow reverse intersystem crossing at ambient temperatures. Simulation methods for these systems must be able to treat relatively large organic molecules, as well as predict their excited state energies, transition energies, singlet–triplet splittings, and absorption and emission cross sections with reasonable accuracy, in order to prove useful in the design process. Here we compare predictions of TDDFT with M06-2X and ωB97X-D exchange-correlation functionals and a G(o)W(o)@HF/BSE method for these quantities in the well-studied DPTZ-DBTO2 TADF emitter molecule. Geometry optimization is performed for ground state (GS) and lowest donor–acceptor charge transfer (CT) state for each functional. Optical absorption and emission cross sections and energies are calculated at these geometries. Relaxation energies are on the order of 0.5 eV, and the importance of obtaining excited state equilibrium geometries in predicting delayed fluorescence is demonstrated. There are clear trends in predictions of G(o)W(o)@HF/BSE, and TDDFT/ωB97X-D and M06-2X methods in which the former method favors local exciton (LE) states while the latter favors DA CT states and ωB97X-D makes intermediate predictions. G(o)W(o)@HF/BSE suffers from triplet instability for LE states but not CT states relevant for TADF. Shifts in HOMO and LUMO levels on adding a conductor-like polarizable continuum model dielectric background are used to estimate changes in excitation energies on going from the gas phase to a solvated molecule. American Chemical Society 2022-12-14 2022-12-29 /pmc/articles/PMC9806837/ /pubmed/36515973 http://dx.doi.org/10.1021/acs.jpca.2c06403 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Chaudhuri, D. Patterson, C. H. TDDFT versus GW/BSE Methods for Prediction of Light Absorption and Emission in a TADF Emitter |
title | TDDFT versus GW/BSE Methods for Prediction
of Light Absorption and Emission in a TADF Emitter |
title_full | TDDFT versus GW/BSE Methods for Prediction
of Light Absorption and Emission in a TADF Emitter |
title_fullStr | TDDFT versus GW/BSE Methods for Prediction
of Light Absorption and Emission in a TADF Emitter |
title_full_unstemmed | TDDFT versus GW/BSE Methods for Prediction
of Light Absorption and Emission in a TADF Emitter |
title_short | TDDFT versus GW/BSE Methods for Prediction
of Light Absorption and Emission in a TADF Emitter |
title_sort | tddft versus gw/bse methods for prediction
of light absorption and emission in a tadf emitter |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9806837/ https://www.ncbi.nlm.nih.gov/pubmed/36515973 http://dx.doi.org/10.1021/acs.jpca.2c06403 |
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