Solvent and Temperature Effects on Photoinduced Proton-Coupled Electron Transfer in the Marcus Inverted Region
Author(s) -
Laura F. Cotter,
Belinda Pettersson Rimgard,
Giovanny A. Parada,
James M. Mayer,
Leif Hammarström
Publication year - 2021
Publication title -
the journal of physical chemistry a
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.756
H-Index - 235
eISSN - 1520-5215
pISSN - 1089-5639
DOI - 10.1021/acs.jpca.1c05764
Subject(s) - chemistry , anthracene , marcus theory , reaction rate constant , solvent effects , solvent , reactivity (psychology) , excited state , proton , photochemistry , dielectric , electron transfer , kinetics , atomic physics , materials science , organic chemistry , medicine , physics , alternative medicine , optoelectronics , pathology , quantum mechanics
Concerted proton-coupled electron transfer (PCET) in the Marcus inverted region was recently demonstrated ( Science 2019 , 364 , 471-475). Understanding the requirements for such reactivity is fundamentally important and holds promise as a design principle for solar energy conversion systems. Herein, we investigate the solvent polarity and temperature dependence of photoinduced proton-coupled charge separation (CS) and charge recombination (CR) in anthracene-phenol-pyridine triads: 1 (10-(4-hydroxy-3-(4-methylpyridin-2-yl)benzyl)anthracene-9-carbonitrile) and 2 (10-(4-hydroxy-3-(4-methoxypyridin-2-yl)benzyl)anthracene-9-carbonitrile). Both the CS and CR rate constants increased with increasing polarity in acetonitrile: n -butyronitrile mixtures. The kinetics were semi-quantitatively analyzed where changes in dielectric and refractive index, and thus consequently changes in driving force (-Δ G °) and reorganization energy (λ), were accounted for. The results were further validated by fitting the temperature dependence, from 180 to 298 K, in n -butyronitrile. The analyses support previous computational work where transitions to proton vibrational excited states dominate the CR reaction with a distinct activation free energy (Δ G * CR ∼ 140 meV). However, the solvent continuum model fails to accurately describe the changes in Δ G ° and λ with temperature via changes in dielectric constant and refractive index. Satisfactory modeling was obtained using the results of a molecular solvent model [ J. Phys. Chem. B 1999 , 103 , 9130-9140], which predicts that λ decreases with temperature, opposite to that of the continuum model. To further assess the solvent polarity control in the inverted region, the reactions were studied in toluene. Nonpolar solvents decrease both Δ G ° CR and λ, slowing CR into the nanosecond time regime for 2 in toluene at 298 K. This demonstrates how PCET in the inverted region may be controlled to potentially use proton-coupled CS states for efficient solar fuel production and photoredox catalysis.
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