Abstract

We report on the fabrication of dye-sensitized solar cells with a TiO2 buffer layer between the transparent conductive oxide substrate and the mesoporous TiO2 film, in order to improve the photovoltaic conversion efficiency of the device. The buffer layer was fabricated by pulsed laser deposition whereas the mesoporous film by the doctor blade method, using TiO2 paste obtained by the sol–gel technique. The buffer layer was deposited in either oxygen (10 Pa and 50 Pa) or argon (10 Pa and 50 Pa) onto transparent conducting oxide glass kept at room temperature. The cross-section scanning electron microscopy image showed differences in layer morphology and thickness, depending on the deposition conditions. Transmission electron microscopy studies of the TiO2 buffer layers indicated that films consisted of grains with typical diameters of 10 nm to 30 nm. We found that the photovoltaic conversion efficiencies, determined under standard air mass 1.5 global (AM 1.5G) conditions, of the solar cells with a buffer layer are more than two times larger than those of the standard cells. The best performance was reached for buffer layers deposited at 10 Pa O2. We discuss the processes that take place in the device and emphasize the role of the brush-like buffer layer in the performance increase.

Highlights

  • Dye-sensitized solar cell technology continues to be a key technological domain as it allows for the production of low-cost energy from renewable sources [1], under ambient lighting [2]

  • Dye-sensitized solar cells (DSSC) are photovoltaic devices consisting of a photoelectrode with a mesoporous layer of a nanocrystalline wide band gap semiconductor on transparent conducting oxide, sensitized with a dye, and a counter electrode, for example platinized conductive glass, with a liquid or solid state electrolyte in-between [3,4]

  • We present the photovoltaic performance of DSSC devices fabricated with buffer layers obtained by pulsed laser deposition (PLD), to take advantage of the good adherence and the control of stoichiometry, crystallinity and purity of ablated materials

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Summary

Introduction

Dye-sensitized solar cell technology continues to be a key technological domain as it allows for the production of low-cost energy from renewable sources [1], under ambient lighting [2]. Dye-sensitized solar cells (DSSC) are photovoltaic devices consisting of a photoelectrode with a mesoporous layer of a nanocrystalline wide band gap semiconductor (such as anatase TiO2) on transparent conducting oxide, sensitized with a dye, and a counter electrode, for example platinized conductive glass, with a liquid or solid state electrolyte in-between [3,4]. The working principle of the device is based on light absorption in the dye, followed by transfer of the resulting photoelectrons from the excited level of the dye into the conduction band of TiO2. The use of perovskite light absorbers and organic hole conductors in a solid state cell resulted in efficiencies larger than 15% [13], which was subsequently further increased by design changes away from the DSSC structure to more than 22% [14]

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