Test of the Orbital-Based LI3 Index as a Predictorof the Height of the <sup>3</sup>MLCT →<sup>3</sup>MC Transition-StateBarrier for [Ru(N<sup>∧</sup>N)<sub>3</sub>]<sup>2+</sup> PolypyridineComplexes in CH<sub>3</sub>CN

Ruthenium(II) polypyridine compounds often have a relatively long-lived triplet metal–ligand charge transfer (<sup>3</sup>MLCT) state, making these complexes useful as chromophores for photoactivated electron transfer in photomolecular devices (PMDs). As different PMDs typically require different ligands and as the luminescence lifetime of the <sup>3</sup>MLCT is sensitive to the structure of the ligand, it is important to understand this state and what types of photoprocesses can lead to its quenching. Recent work has increasingly emphasized that there are likely multiple competing pathways involved, which should be explored in order to fully comprehend the <sup>3</sup>MLCT state. However, the lowest barrier that needs to be crossed to pass over to the nonluminescent triplet metal-centered (<sup>3</sup>MC) state has been repeatedly found to be a <i>trans</i> dissociation of the complex, at least in the simpler cases studied. This is the fourth in a series of articles investigating the possibility of an orbital-based luminescence index (LI3, because it was the most successful of three) for predicting luminescence lifetimes. In an earlier study of bidentate (N<sup>∧</sup>N) ligands, we showed that the gas-phase <sup>3</sup>MLCT → <sup>3</sup>MC mechanism proceeded via an initial charge transfer to a single N<sup>∧</sup>N ligand, which moves symmetrically away from the central ruthenium atom, followed by a bifurcation pathway to one of two <sup>3</sup>MC enantiomers. The actual transition state barrier was quite small and independent, to within the limits of our calculations, of the choice of ligand studied. Here, we investigate the same reaction in acetonitrile, CH<sub>3</sub>CN, solution and find that the mechanism differs from that in the gas phase in that the reaction passes directly via a <i>trans</i> mechanism. This has implications for the interpretation of LI3 via the Bell-Evans–Polanyi principle.

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Figshare
Published
2025-02-17
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https://doi.org/10.1021/acs.jpca.4c07424.s001
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Organic Light-Emitting Diodes Research
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Test of the Orbital-Based LI3 Index as a Predictorof the Height of the 3MLCT →3MC Transition-StateBarrier for [Ru(N∧N)3]2+ PolypyridineComplexes in CH3CN

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Organic Light-Emitting Diodes Research
article

Test of the Orbital-Based LI3 Index as a Predictorof the Height of the 3MLCT →3MC Transition-StateBarrier for [Ru(N∧N)3]2+ PolypyridineComplexes in CH3CN

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Abstract

Ruthenium(II) polypyridine compounds often have a relatively long-lived triplet metal–ligand charge transfer (<sup>3</sup>MLCT) state, making these complexes useful as chromophores for photoactivated electron transfer in photomolecular devices (PMDs). As different PMDs typically require different ligands and as the luminescence lifetime of the <sup>3</sup>MLCT is sensitive to the structure of the ligand, it is important to understand this state and what types of photoprocesses can lead to its quenching. Recent work has increasingly emphasized that there are likely multiple competing pathways involved, which should be explored in order to fully comprehend the <sup>3</sup>MLCT state. However, the lowest barrier that needs to be crossed to pass over to the nonluminescent triplet metal-centered (<sup>3</sup>MC) state has been repeatedly found to be a <i>trans</i> dissociation of the complex, at least in the simpler cases studied. This is the fourth in a series of articles investigating the possibility of an orbital-based luminescence index (LI3, because it was the most successful of three) for predicting luminescence lifetimes. In an earlier study of bidentate (N<sup>∧</sup>N) ligands, we showed that the gas-phase <sup>3</sup>MLCT → <sup>3</sup>MC mechanism proceeded via an initial charge transfer to a single N<sup>∧</sup>N ligand, which moves symmetrically away from the central ruthenium atom, followed by a bifurcation pathway to one of two <sup>3</sup>MC enantiomers. The actual transition state barrier was quite small and independent, to within the limits of our calculations, of the choice of ligand studied. Here, we investigate the same reaction in acetonitrile, CH<sub>3</sub>CN, solution and find that the mechanism differs from that in the gas phase in that the reaction passes directly via a <i>trans</i> mechanism. This has implications for the interpretation of LI3 via the Bell-Evans–Polanyi principle.

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