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Energy Transfer Mechanism and Quantitative Modeling of Rate from an Antenna to a Lanthanide Ion
[Image: see text] The excitation energy transfer (ET) pathway and mechanism from an organic antenna to a lanthanide ion has been the subject of discussion for many decades. In the case of europium (Eu(3+)), it has been suggested that the transfer originates from the ligand singlet state or a triplet...
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/PMC9589723/ https://www.ncbi.nlm.nih.gov/pubmed/36200840 http://dx.doi.org/10.1021/acs.jpca.2c03965 |
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author | Tanner, Peter A. Thor, Waygen Zhang, Yonghong Wong, Ka-Leung |
author_facet | Tanner, Peter A. Thor, Waygen Zhang, Yonghong Wong, Ka-Leung |
author_sort | Tanner, Peter A. |
collection | PubMed |
description | [Image: see text] The excitation energy transfer (ET) pathway and mechanism from an organic antenna to a lanthanide ion has been the subject of discussion for many decades. In the case of europium (Eu(3+)), it has been suggested that the transfer originates from the ligand singlet state or a triplet state. Taking the lanthanide complex Eu(TTA)(3)(H(2)O)(2) as an example, we have investigated the spectra and luminescence kinetics, mainly at room temperature and 77 K, to acquire the necessary experimental data. We put forward an experimental and theoretical approach to measure the energy transfer rates from the antenna to different Eu(3+) levels using the Dexter formulation. We find that transfer from the ligand singlet state to Eu(3+) may account for the ET pathway, by combined electric dipole–electric dipole (ED–ED) and ED-electric quadrupole (EQ) mechanisms. The contributions from the triplet state by these mechanisms are very small. An independent systems rate equation approach can effectively model the experimental kinetics results. The model utilizes the cooperative processes that take place on the metal ion and ligand and considers S(0), S(1), and T(1) ligand states in addition to (7)F(0,1), (5)D(0), (5)D(1), and (5)DJ (=(5)L(6), (5)D(3), (5)D(2) combined) Eu(3+) states. The triplet exchange ET rate is estimated to be of the order 10(7) s(–1). The observation of a nanosecond risetime for the Eu(3+ 5)D(1) level does not enable the assignment of the ET route or the mechanism. Furthermore, the (5)D(1) risetime may be contributed by several processes. Observation of its temperature dependence and also that of the ground-state population can supply useful information concerning the mechanism because the change in metal-ion internal conversion rate has a greater effect than changes in singlet or triplet nonradiative rates. A critical comparison is included for the model of Malta employed in the online software LUMPAC and JOYSpectra. The theoretical treatment of the exchange mechanism and its contribution are now being considered. |
format | Online Article Text |
id | pubmed-9589723 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-95897232022-10-25 Energy Transfer Mechanism and Quantitative Modeling of Rate from an Antenna to a Lanthanide Ion Tanner, Peter A. Thor, Waygen Zhang, Yonghong Wong, Ka-Leung J Phys Chem A [Image: see text] The excitation energy transfer (ET) pathway and mechanism from an organic antenna to a lanthanide ion has been the subject of discussion for many decades. In the case of europium (Eu(3+)), it has been suggested that the transfer originates from the ligand singlet state or a triplet state. Taking the lanthanide complex Eu(TTA)(3)(H(2)O)(2) as an example, we have investigated the spectra and luminescence kinetics, mainly at room temperature and 77 K, to acquire the necessary experimental data. We put forward an experimental and theoretical approach to measure the energy transfer rates from the antenna to different Eu(3+) levels using the Dexter formulation. We find that transfer from the ligand singlet state to Eu(3+) may account for the ET pathway, by combined electric dipole–electric dipole (ED–ED) and ED-electric quadrupole (EQ) mechanisms. The contributions from the triplet state by these mechanisms are very small. An independent systems rate equation approach can effectively model the experimental kinetics results. The model utilizes the cooperative processes that take place on the metal ion and ligand and considers S(0), S(1), and T(1) ligand states in addition to (7)F(0,1), (5)D(0), (5)D(1), and (5)DJ (=(5)L(6), (5)D(3), (5)D(2) combined) Eu(3+) states. The triplet exchange ET rate is estimated to be of the order 10(7) s(–1). The observation of a nanosecond risetime for the Eu(3+ 5)D(1) level does not enable the assignment of the ET route or the mechanism. Furthermore, the (5)D(1) risetime may be contributed by several processes. Observation of its temperature dependence and also that of the ground-state population can supply useful information concerning the mechanism because the change in metal-ion internal conversion rate has a greater effect than changes in singlet or triplet nonradiative rates. A critical comparison is included for the model of Malta employed in the online software LUMPAC and JOYSpectra. The theoretical treatment of the exchange mechanism and its contribution are now being considered. American Chemical Society 2022-10-06 2022-10-20 /pmc/articles/PMC9589723/ /pubmed/36200840 http://dx.doi.org/10.1021/acs.jpca.2c03965 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 | Tanner, Peter A. Thor, Waygen Zhang, Yonghong Wong, Ka-Leung Energy Transfer Mechanism and Quantitative Modeling of Rate from an Antenna to a Lanthanide Ion |
title | Energy Transfer
Mechanism and Quantitative Modeling
of Rate from an Antenna to a Lanthanide Ion |
title_full | Energy Transfer
Mechanism and Quantitative Modeling
of Rate from an Antenna to a Lanthanide Ion |
title_fullStr | Energy Transfer
Mechanism and Quantitative Modeling
of Rate from an Antenna to a Lanthanide Ion |
title_full_unstemmed | Energy Transfer
Mechanism and Quantitative Modeling
of Rate from an Antenna to a Lanthanide Ion |
title_short | Energy Transfer
Mechanism and Quantitative Modeling
of Rate from an Antenna to a Lanthanide Ion |
title_sort | energy transfer
mechanism and quantitative modeling
of rate from an antenna to a lanthanide ion |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9589723/ https://www.ncbi.nlm.nih.gov/pubmed/36200840 http://dx.doi.org/10.1021/acs.jpca.2c03965 |
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