Electrode-MediatedPhotochemical Disproportionationof a Polypyridylruthenium(II) Chromophore

On a metallic electrode embedded within a Nafion film, excitation at 470 nm of Ru­(bpy)<sub>2</sub>(dppn)<sup>2+</sup> (bpy = 2,2′-bipyridine; dppn = benzo­[<i>i</i>]­dipyrido­[3,2-<i>a</i>:2′,3′-<i>c</i>]­phenazine) produced photocurrents indicative of tunable charge transfer between the electrode and photosensitizer, with the direction and magnitude of current dependent on the applied bias potential. At a bias potential of 0.85 V vs dppn/dppn<sup>•–</sup>, the oxidative and reductive photocurrents cancel, yielding no net current; transient spectroscopy under these conditions reveals the photoelectrochemical disproportionation of the sensitizer to Ru<sup>3+</sup> and Ru<sup>+</sup>. The ∼2.8 eV photon energy could thus be coupled to the ground-state reduction potentials of the photosensitizer, <i>simultaneously</i> generating electrons and holes on a monolithic electrode at potentials milder than the formal potentials.

Publication Details

Journal
Figshare
Published
2025-03-21
DOI
https://doi.org/10.1021/acs.inorgchem.5c00113.s001
Primary Topic
Molecular Sensors and Ion Detection
Type
article
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article

Electrode-MediatedPhotochemical Disproportionationof a Polypyridylruthenium(II) Chromophore

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Molecular Sensors and Ion Detection
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Electrode-MediatedPhotochemical Disproportionationof a Polypyridylruthenium(II) Chromophore

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Abstract

On a metallic electrode embedded within a Nafion film, excitation at 470 nm of Ru­(bpy)<sub>2</sub>(dppn)<sup>2+</sup> (bpy = 2,2′-bipyridine; dppn = benzo­[<i>i</i>]­dipyrido­[3,2-<i>a</i>:2′,3′-<i>c</i>]­phenazine) produced photocurrents indicative of tunable charge transfer between the electrode and photosensitizer, with the direction and magnitude of current dependent on the applied bias potential. At a bias potential of 0.85 V vs dppn/dppn<sup>•–</sup>, the oxidative and reductive photocurrents cancel, yielding no net current; transient spectroscopy under these conditions reveals the photoelectrochemical disproportionation of the sensitizer to Ru<sup>3+</sup> and Ru<sup>+</sup>. The ∼2.8 eV photon energy could thus be coupled to the ground-state reduction potentials of the photosensitizer, <i>simultaneously</i> generating electrons and holes on a monolithic electrode at potentials milder than the formal potentials.

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