Singlet Fission in Lycopene H‑Aggregates
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. Th...
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Veröffentlicht in: | The journal of physical chemistry letters 2023-11, Vol.14 (44), p.9842-9847 |
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description | 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 11 B u – state. Once populated, the 11 B u – state allows exothermic bimolecular singlet fission, while its internal conversion to the 21 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. |
doi_str_mv | 10.1021/acs.jpclett.3c02435 |
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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 11 B u – state. Once populated, the 11 B u – state allows exothermic bimolecular singlet fission, while its internal conversion to the 21 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.</description><identifier>ISSN: 1948-7185</identifier><identifier>EISSN: 1948-7185</identifier><identifier>DOI: 10.1021/acs.jpclett.3c02435</identifier><identifier>PMID: 37890074</identifier><language>eng</language><publisher>American Chemical Society</publisher><subject>Letter ; Physical Insights into Quantum Phenomena and Function</subject><ispartof>The journal of physical chemistry letters, 2023-11, Vol.14 (44), p.9842-9847</ispartof><rights>2023 The Author. Published by American Chemical Society</rights><rights>2023 The Author. 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Phys. Chem. Lett</addtitle><description>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 11 B u – state. Once populated, the 11 B u – state allows exothermic bimolecular singlet fission, while its internal conversion to the 21 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.</description><subject>Letter</subject><subject>Physical Insights into Quantum Phenomena and Function</subject><issn>1948-7185</issn><issn>1948-7185</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kM9LwzAUx4MoTqd_gZceRdiWNG2SnmQM54SBB3cPafpaO7qkJq2wm_-C_6J_idEV0YuX9x58fzz4IHRF8JTgmMyU9tNtqxvouinVOE5oeoTOSJaICSciPf51j9C591uMWYYFP0UjykWGMU_O0M1TbapQES1r72trotpE6722LRiIVh9v7_OqclCpDvwFOilV4-Fy2GO0Wd5tFqvJ-vH-YTFfT1QS0y5MUAoYjQVXOYGiZFQkVNNCMKYxVmWZFSTDwEiQYsUV5ZzlOi8EZjhP6BjdHmrbPt9BocF0TjWydfVOub20qpZ_FVM_y8q-SoJZQgSnoeF6aHD2pQffyV3tNTSNMmB7L2MhaCpYmrFgpQerdtZ7B-XPH4LlF2UZKMuBshwoh9TskPoWbe9M4PFv4hNPfYNe</recordid><startdate>20231109</startdate><enddate>20231109</enddate><creator>Barford, William</creator><general>American Chemical Society</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0002-7223-686X</orcidid></search><sort><creationdate>20231109</creationdate><title>Singlet Fission in Lycopene H‑Aggregates</title><author>Barford, William</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a423t-a4eaae63287ab1edf63843c3d866c00aff9d190e61df62a7a3776bcbd8060b43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Letter</topic><topic>Physical Insights into Quantum Phenomena and Function</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Barford, William</creatorcontrib><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>The journal of physical chemistry letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Barford, William</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Singlet Fission in Lycopene H‑Aggregates</atitle><jtitle>The journal of physical chemistry letters</jtitle><addtitle>J. Phys. Chem. Lett</addtitle><date>2023-11-09</date><risdate>2023</risdate><volume>14</volume><issue>44</issue><spage>9842</spage><epage>9847</epage><pages>9842-9847</pages><issn>1948-7185</issn><eissn>1948-7185</eissn><abstract>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 11 B u – state. Once populated, the 11 B u – state allows exothermic bimolecular singlet fission, while its internal conversion to the 21 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.</abstract><pub>American Chemical Society</pub><pmid>37890074</pmid><doi>10.1021/acs.jpclett.3c02435</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0002-7223-686X</orcidid><oa>free_for_read</oa></addata></record> |
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title | Singlet Fission in Lycopene H‑Aggregates |
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