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Excited‐State Dynamics of [Ru(bpy)(3)](2+) Thin Films on Sensitized TiO(2) and ZrO(2)
The excited state dynamics of Tris(2,2′‐bipyridine)ruthenium(II) hexafluorophosphate, [Ru(bpy)(3)(PF(6))(2)], was investigated on the surface of bare and sensitized TiO(2) and ZrO(2) films. The organic dyes LEG4 and MKA253 were selected as sensitizers. A Stern–Volmer plot of LEG4‐sensitized TiO(2) s...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6593980/ https://www.ncbi.nlm.nih.gov/pubmed/30623544 http://dx.doi.org/10.1002/cphc.201801010 |
Sumario: | The excited state dynamics of Tris(2,2′‐bipyridine)ruthenium(II) hexafluorophosphate, [Ru(bpy)(3)(PF(6))(2)], was investigated on the surface of bare and sensitized TiO(2) and ZrO(2) films. The organic dyes LEG4 and MKA253 were selected as sensitizers. A Stern–Volmer plot of LEG4‐sensitized TiO(2) substrates with a spin‐coated [Ru(bpy)(3)(PF(6))(2)] layer on top shows considerable quenching of the emission of the latter. Interestingly, time‐resolved emission spectroscopy reveals the presence of a fast‐decay time component (25±5 ns), which is absent when the anatase TiO(2) semiconductor is replaced by ZrO(2). It should be specified that the positive redox potential of the ruthenium complex prevents electron transfer from the [Ru(bpy)(3)(PF(6))(2)] ground state into the oxidized sensitizer. Therefore, we speculate that the fast‐decay time component observed stems from excited‐state electron transfer from [Ru(bpy)(3)(PF(6))(2)] to the oxidized sensitizer. Solid‐state dye sensitized solar cells (ssDSSCs) employing MKA253 and LEG4 dyes, with [Ru(bpy)(3)(PF(6))(2)] as a hole‐transporting material (HTM), exhibit 1.2 % and 1.1 % power conversion efficiency, respectively. This result illustrates the possibility of the hypothesized excited‐state electron transfer. |
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