Photoelectric Performance Optimization of Dye‐Sensitized Solar Cells Based on ZnO‐TiO 2 Composite Nanofibers
As the electron transport layer of dye‐sensitized solar cells (DSSCs), the photoanode is an important component that affects photoelectric conversion efficiency (PCE). The commonly used material titanium dioxide (TiO 2 ) is difficult to prepare as nanostructures with large specific surface area, whi...
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Veröffentlicht in: | Journal of nanomaterials 2022-01, Vol.2022 (1) |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | As the electron transport layer of dye‐sensitized solar cells (DSSCs), the photoanode is an important component that affects photoelectric conversion efficiency (PCE). The commonly used material titanium dioxide (TiO 2 ) is difficult to prepare as nanostructures with large specific surface area, which affects dye loading and electrolyte diffusion. Herein, TiO 2 nanofibers and ZnO‐TiO 2 composite nanofibers with different molar ratios are synthesized by electrospinning technology. The above nanofibers are coated on photoanodes by the doctor blade method to assemble DSSCs. The influence of the composite ratio of ZnO‐TiO 2 composite nanofibers on the photoelectric performance of the assembled DSSCs is explored. The ZnO‐TiO 2 composite nanofibers with a molar ratio of 1 : 2 have large specific surface area and porosity and have the smallest charge transfer resistance at the photoanode‐electrolyte interface. The PCE of the nanofiber‐modified DSSCs reaches a maximum of 3.66%, which is 56% higher than that of the TiO 2 nanofiber‐modified DSSCs. The photovoltaic parameters such as open circuit voltage (V OC ), current density (J SC ), and fill factor (FF) are 0.58 V, 10.36 mA/cm 2 , and 0.61, respectively. Proper compounding of zinc oxide (ZnO) can not only make the nanofibers absorb more dyes and enhance the light‐harvesting ability but also improve the diffusion of the electrolyte and enhance the electron transport, thus successfully improving the power conversion efficiency of DSSCs. |
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ISSN: | 1687-4110 1687-4129 |
DOI: | 10.1155/2022/7356943 |