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Effect of Co-Adsorbate and Hole Transporting Layer on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine Interface
[Image: see text] Understanding the primary processes of charge separation (CS) in solid-state dye-sensitized solar cells (DSSCs) and, in particular, analysis of the efficiency losses during these primary photoreactions is essential for designing new and efficient photosensitizers. Phthalocyanines (...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2018
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6641689/ https://www.ncbi.nlm.nih.gov/pubmed/31458711 http://dx.doi.org/10.1021/acsomega.8b00600 |
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author | Virkki, Kirsi Tervola, Essi Medel, Maria Torres, Tomás Tkachenko, Nikolai V. |
author_facet | Virkki, Kirsi Tervola, Essi Medel, Maria Torres, Tomás Tkachenko, Nikolai V. |
author_sort | Virkki, Kirsi |
collection | PubMed |
description | [Image: see text] Understanding the primary processes of charge separation (CS) in solid-state dye-sensitized solar cells (DSSCs) and, in particular, analysis of the efficiency losses during these primary photoreactions is essential for designing new and efficient photosensitizers. Phthalocyanines (Pcs) are potentially interesting sensitizers having absorption in the red side of the optical spectrum and known to be efficient electron donors. However, the efficiencies of Pc-sensitized DSSCs are lower than that of the best DSSCs, which is commonly attributed to the aggregation tendency of Pcs. In this study, we employ ultrafast spectroscopy to discover why and how much does the aggregation affect the efficiency. The samples were prepared on a standard fluorine-doped tin oxide (FTO) substrates covered by a porous layer of TiO(2) nanoparticles, functionalized by a Pc sensitizer and filled by a hole transporting material (Spiro-MeOTAD). The study demonstrates that the aggregation can be suppressed gradually by using co-adsorbates, such as chenodeoxycholic acid (CDCA) and oleic acid, but rather high concentrations of co-adsorbate is required. Gradually, a few times improvement of quantum efficiency was observed at sensitizer/co-adsorbate ratio Pc/CDCA = 1:10 and higher. The time-resolved spectroscopy studies were complemented by standard photocurrent measurements of the same sample structures, which also confirmed gradual increase in photon-to-current conversion efficiency on mixing Pc with CDCA. |
format | Online Article Text |
id | pubmed-6641689 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-66416892019-08-27 Effect of Co-Adsorbate and Hole Transporting Layer on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine Interface Virkki, Kirsi Tervola, Essi Medel, Maria Torres, Tomás Tkachenko, Nikolai V. ACS Omega [Image: see text] Understanding the primary processes of charge separation (CS) in solid-state dye-sensitized solar cells (DSSCs) and, in particular, analysis of the efficiency losses during these primary photoreactions is essential for designing new and efficient photosensitizers. Phthalocyanines (Pcs) are potentially interesting sensitizers having absorption in the red side of the optical spectrum and known to be efficient electron donors. However, the efficiencies of Pc-sensitized DSSCs are lower than that of the best DSSCs, which is commonly attributed to the aggregation tendency of Pcs. In this study, we employ ultrafast spectroscopy to discover why and how much does the aggregation affect the efficiency. The samples were prepared on a standard fluorine-doped tin oxide (FTO) substrates covered by a porous layer of TiO(2) nanoparticles, functionalized by a Pc sensitizer and filled by a hole transporting material (Spiro-MeOTAD). The study demonstrates that the aggregation can be suppressed gradually by using co-adsorbates, such as chenodeoxycholic acid (CDCA) and oleic acid, but rather high concentrations of co-adsorbate is required. Gradually, a few times improvement of quantum efficiency was observed at sensitizer/co-adsorbate ratio Pc/CDCA = 1:10 and higher. The time-resolved spectroscopy studies were complemented by standard photocurrent measurements of the same sample structures, which also confirmed gradual increase in photon-to-current conversion efficiency on mixing Pc with CDCA. American Chemical Society 2018-05-07 /pmc/articles/PMC6641689/ /pubmed/31458711 http://dx.doi.org/10.1021/acsomega.8b00600 Text en Copyright © 2018 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Virkki, Kirsi Tervola, Essi Medel, Maria Torres, Tomás Tkachenko, Nikolai V. Effect of Co-Adsorbate and Hole Transporting Layer on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine Interface |
title | Effect of Co-Adsorbate and Hole Transporting Layer
on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine
Interface |
title_full | Effect of Co-Adsorbate and Hole Transporting Layer
on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine
Interface |
title_fullStr | Effect of Co-Adsorbate and Hole Transporting Layer
on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine
Interface |
title_full_unstemmed | Effect of Co-Adsorbate and Hole Transporting Layer
on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine
Interface |
title_short | Effect of Co-Adsorbate and Hole Transporting Layer
on the Photoinduced Charge Separation at the TiO(2)–Phthalocyanine
Interface |
title_sort | effect of co-adsorbate and hole transporting layer
on the photoinduced charge separation at the tio(2)–phthalocyanine
interface |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6641689/ https://www.ncbi.nlm.nih.gov/pubmed/31458711 http://dx.doi.org/10.1021/acsomega.8b00600 |
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