Data

Data from: Electron, hole, singlet, and triplet energy transfer in photoexcited porphyrin-naphthalenediimide dyads

RMIT University, Australia
Sheshanath Vishwanath Bhosale (Aggregated by)
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ctx_ver=Z39.88-2004&rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Adc&rfr_id=info%3Asid%2FANDS&rft_id=https://figshare.com/articles/Electron_Hole_Singlet_and_Triplet_Energy_Transfer_in_Photoexcited_Porphyrin_Naphthalenediimide_Dyads/2157115&rft.title=Data from: Electron, hole, singlet, and triplet energy transfer in photoexcited porphyrin-naphthalenediimide dyads&rft.identifier=feb0a2a76bf4f40deca4b5c771c2b2c9&rft.publisher=RMIT University, Australia&rft.description=Attached file provides supplementary data for linked article. The excited-state dynamics of two molecular dyads, consisting of zinc (1) and free-base (2) porphyrin connected via a peptide linker to a core-substituted naphthalenediimide (NDI) have been investigated using optical spectroscopy. These dyads exhibit rich photophysics because of the large number of electronic excited states below 3 eV. In the case of 1 in apolar solvents, excitation energy transfer from the vibrationally hot singlet excited porphyrin to the NDI takes place with a 500 fs time constant. Electronic energy ends up in the NDI-localized triplet state, which decays to the ground state on a microsecond timescale. In polar solvents, ground-state recovery is faster by 5 orders of magnitude because of the occurrence of charge separation followed by recombination. On the other hand, excitation energy transfer in 2 takes place in the opposite direction, namely from the NDI to the porphyrin, which then undergoes intersystem crossing to the triplet state, followed by triplet energy transfer back to the NDI. Therefore, four distinct local electronic excited states are consecutively populated after excitation of the NDI unit of 2, with the energy shuttling between the two ends of the dyad.&rft.creator=Sheshanath Vishwanath Bhosale&rft.date=2018&rft.relation=https://dx.doi.org/10.1021/jp5108685&rft_rights=Further information about rights and usage of ACS publications and supplementary data can be found here: http://pubs.acs.org/page/copyright/permissions.html.&rft_rights=CC BY-NC: Attribution-Noncommercial 3.0 AU http://creativecommons.org/licenses/by-nc/3.0/au&rft_subject=Excited-state dynamics&rft_subject=Excitation energy&rft_subject=Light harvesting arrays&rft_subject=Reaction center complex&rft_subject=Charge separation pathways&rft_subject=Photosynthetic antenna&rft_subject=Multiporphyrin arrays&rft_subject=Photoinduced electron&rft_subject=Molecular electronics &rft_subject=Ultrafast dynamics &rft_subject=Organic Chemical Synthesis&rft_subject=CHEMICAL SCIENCES&rft_subject=ORGANIC CHEMISTRY&rft.type=dataset&rft.language=English Access the data

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CC BY-NC: Attribution-Noncommercial 3.0 AU
http://creativecommons.org/licenses/by-nc/3.0/au

Further information about rights and usage of ACS publications and supplementary data can be found here: http://pubs.acs.org/page/copyright/permissions.html.

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Attached file provides supplementary data for linked article. The excited-state dynamics of two molecular dyads, consisting of zinc (1) and free-base (2) porphyrin connected via a peptide linker to a core-substituted naphthalenediimide (NDI) have been investigated using optical spectroscopy. These dyads exhibit rich photophysics because of the large number of electronic excited states below 3 eV. In the case of 1 in apolar solvents, excitation energy transfer from the vibrationally hot singlet excited porphyrin to the NDI takes place with a 500 fs time constant. Electronic energy ends up in the NDI-localized triplet state, which decays to the ground state on a microsecond timescale. In polar solvents, ground-state recovery is faster by 5 orders of magnitude because of the occurrence of charge separation followed by recombination. On the other hand, excitation energy transfer in 2 takes place in the opposite direction, namely from the NDI to the porphyrin, which then undergoes intersystem crossing to the triplet state, followed by triplet energy transfer back to the NDI. Therefore, four distinct local electronic excited states are consecutively populated after excitation of the NDI unit of 2, with the energy shuttling between the two ends of the dyad.

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  • Local : feb0a2a76bf4f40deca4b5c771c2b2c9
ACN 633 798 857