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Singlet Fission in Lycopene H-Aggregates

[Image: see text] A theory of singlet fission (SF) in carotenoid dimers is applied to explain the SF in lycopene H-aggregates observed after high-energy photoexcitation. The explanation proposed here is that a high energy, delocalized bright (1)B(u)(+) state first relaxes and localizes onto a single...

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Autor principal: Barford, William
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10641873/
https://www.ncbi.nlm.nih.gov/pubmed/37890074
http://dx.doi.org/10.1021/acs.jpclett.3c02435
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author Barford, William
author_facet Barford, William
author_sort Barford, William
collection PubMed
description [Image: see text] A theory of singlet fission (SF) in carotenoid dimers is applied to explain the SF in lycopene H-aggregates observed after high-energy photoexcitation. The explanation proposed here is that a high energy, delocalized bright (1)B(u)(+) state first relaxes and localizes onto a single lycopene monomer. The high-energy intramonomer state then undergoes internal conversion to the 1(1)B(u)(–) state. Once populated, the 1(1)B(u)(–) state allows exothermic bimolecular singlet fission, while its internal conversion to the 2(1)A(g)(–) state is symmetry forbidden. The simulation of SF predicts that the intramonomer triplet-pair state undergoes almost complete population transfer to the intermonomer singlet-pair state within 100 ps. Simultaneously, ZFS interactions begin to partially populate the intermonomer quintet triplet-pair state up to ca. 2 ns, after which hyperfine interactions thermally equilibrate the triplet-pair states, thus forming free single triplets within 50 ns.
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spelling pubmed-106418732023-11-15 Singlet Fission in Lycopene H-Aggregates Barford, William J Phys Chem Lett [Image: see text] A theory of singlet fission (SF) in carotenoid dimers is applied to explain the SF in lycopene H-aggregates observed after high-energy photoexcitation. The explanation proposed here is that a high energy, delocalized bright (1)B(u)(+) state first relaxes and localizes onto a single lycopene monomer. The high-energy intramonomer state then undergoes internal conversion to the 1(1)B(u)(–) state. Once populated, the 1(1)B(u)(–) state allows exothermic bimolecular singlet fission, while its internal conversion to the 2(1)A(g)(–) state is symmetry forbidden. The simulation of SF predicts that the intramonomer triplet-pair state undergoes almost complete population transfer to the intermonomer singlet-pair state within 100 ps. Simultaneously, ZFS interactions begin to partially populate the intermonomer quintet triplet-pair state up to ca. 2 ns, after which hyperfine interactions thermally equilibrate the triplet-pair states, thus forming free single triplets within 50 ns. American Chemical Society 2023-10-27 /pmc/articles/PMC10641873/ /pubmed/37890074 http://dx.doi.org/10.1021/acs.jpclett.3c02435 Text en © 2023 The Author. 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 Barford, William
Singlet Fission in Lycopene H-Aggregates
title Singlet Fission in Lycopene H-Aggregates
title_full Singlet Fission in Lycopene H-Aggregates
title_fullStr Singlet Fission in Lycopene H-Aggregates
title_full_unstemmed Singlet Fission in Lycopene H-Aggregates
title_short Singlet Fission in Lycopene H-Aggregates
title_sort singlet fission in lycopene h-aggregates
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10641873/
https://www.ncbi.nlm.nih.gov/pubmed/37890074
http://dx.doi.org/10.1021/acs.jpclett.3c02435
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