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How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches

Density functional theory (DFT) was used to investigate the electronic and optical properties of the ortho, meta, and para derivatives of 2,2′,7,7′-tetrakis-(N,N-di-4-methoxyphenylamino)-9,9′spirobifluorene (spiro-OMeTAD) and its two oxidized forms (+1 and +2). The energy level, distribution shape,...

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Autores principales: Ashassi-Sorkhabi, Habib, Salehi-Abar, Parvin
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9080512/
https://www.ncbi.nlm.nih.gov/pubmed/35541152
http://dx.doi.org/10.1039/c8ra01879k
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author Ashassi-Sorkhabi, Habib
Salehi-Abar, Parvin
author_facet Ashassi-Sorkhabi, Habib
Salehi-Abar, Parvin
author_sort Ashassi-Sorkhabi, Habib
collection PubMed
description Density functional theory (DFT) was used to investigate the electronic and optical properties of the ortho, meta, and para derivatives of 2,2′,7,7′-tetrakis-(N,N-di-4-methoxyphenylamino)-9,9′spirobifluorene (spiro-OMeTAD) and its two oxidized forms (+1 and +2). The energy level, distribution shape, and density of highest occupied molecular orbital (HOMO) and of lowest unoccupied molecular orbital (LUMO) were computed for all three derivatives and compared in the neutral and oxidized forms. Results indicated that the different positions of OMe in the spiro-OMeTAD framework lead to different optical properties. It was also found that compared to the neutral form, in the oxidized forms, the maximum absorption band red shifts, new signals in the visible range between 500 and 850 nm appear, and the Stokes shift values reduce for all three derivatives. The exciton binding energy of spiro-OMeTAD with an o-OMe substituent is 0.52 eV, being smaller than that of p-OMe and m-OMe, indicating easier generation of free charge carriers. The hole mobility was calculated for all three molecules, and the obtained data revealed that the hole mobility of the o-OMe substituent has a value of 7.90 × 10(−3) cm(2) V(−1) s(−1), which is respectively 3 and 11 times larger than that of p-OMe and m-OMe. The smaller exciton binding energy and larger hole mobility of the o-OMe substituent will result in a higher short-circuit current density (J(sc)) and a higher fill factor, respectively, demonstrating that po-spiro-OMeTAD is a promising candidate for use in perovskite solar cells. The reorganization energy, electron affinity, and ionization potential were also calculated and discussed.
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spelling pubmed-90805122022-05-09 How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches Ashassi-Sorkhabi, Habib Salehi-Abar, Parvin RSC Adv Chemistry Density functional theory (DFT) was used to investigate the electronic and optical properties of the ortho, meta, and para derivatives of 2,2′,7,7′-tetrakis-(N,N-di-4-methoxyphenylamino)-9,9′spirobifluorene (spiro-OMeTAD) and its two oxidized forms (+1 and +2). The energy level, distribution shape, and density of highest occupied molecular orbital (HOMO) and of lowest unoccupied molecular orbital (LUMO) were computed for all three derivatives and compared in the neutral and oxidized forms. Results indicated that the different positions of OMe in the spiro-OMeTAD framework lead to different optical properties. It was also found that compared to the neutral form, in the oxidized forms, the maximum absorption band red shifts, new signals in the visible range between 500 and 850 nm appear, and the Stokes shift values reduce for all three derivatives. The exciton binding energy of spiro-OMeTAD with an o-OMe substituent is 0.52 eV, being smaller than that of p-OMe and m-OMe, indicating easier generation of free charge carriers. The hole mobility was calculated for all three molecules, and the obtained data revealed that the hole mobility of the o-OMe substituent has a value of 7.90 × 10(−3) cm(2) V(−1) s(−1), which is respectively 3 and 11 times larger than that of p-OMe and m-OMe. The smaller exciton binding energy and larger hole mobility of the o-OMe substituent will result in a higher short-circuit current density (J(sc)) and a higher fill factor, respectively, demonstrating that po-spiro-OMeTAD is a promising candidate for use in perovskite solar cells. The reorganization energy, electron affinity, and ionization potential were also calculated and discussed. The Royal Society of Chemistry 2018-05-18 /pmc/articles/PMC9080512/ /pubmed/35541152 http://dx.doi.org/10.1039/c8ra01879k Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Ashassi-Sorkhabi, Habib
Salehi-Abar, Parvin
How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches
title How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches
title_full How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches
title_fullStr How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches
title_full_unstemmed How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches
title_short How the change of OMe substituent position affects the performance of spiro-OMeTAD in neutral and oxidized forms: theoretical approaches
title_sort how the change of ome substituent position affects the performance of spiro-ometad in neutral and oxidized forms: theoretical approaches
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9080512/
https://www.ncbi.nlm.nih.gov/pubmed/35541152
http://dx.doi.org/10.1039/c8ra01879k
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