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Bifunctional Highly Uniform Core/double-shell Structured B-NaYF4:Er3+, Yb3+ @ SiO2@TiO2 Hexagonal Submicroprisms Upconversion Nanoparticles for High-performance Dye Sensitized Solar Cells

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We designed a highly uniform core double-shell (CDS) structure consisting of -NaYF4:Er3+,Yb3+ crystal as core (~400 nm in diameter and ~470 nm in height), amorphous SiO2 as inner shell (~10 nm in thickness), and interconnected anatase TiO2 grains as outer shell (~30 nm in thickness). For device application, various amount of these hexagonal submicroprisms (HSMs) were introduced into TiO2nanoparticles (20-40 nm in diameter) to form a bifunctional nano-submicron composite (NSMC) layer upon a prior prepared transparent TiO2 layer. By utilization of these efficient -NaYF4:Er3+,Yb3+ upconversion cores, near-infrared irradiation can be absorbed and harvested indirectly by dye molecules to broaden the absorption region and produce more electrons. Owing to the excellent insulating properties, SiO2 shell creates a perfect electrical isolation for the UCP cores. Through this method, the problem of electron trapping and capture caused by ligands and defects on the surface of NaYF4:Er3+,Yb3+ crystals can be thoroughly overcome. However, employment of this submicron sized composites can seriously reduce the internal surface area, leading to a less amount of dye loading. By coating of the outer TiO2 shell, the disadvantage of SiO2 shell can be avoided to the utmost extent. Computer simulation results have shown that scattering of 10-25 nm TiO2particles is negligible and effective Mie scatterers are those particles whose dimensions are comparable to the wavelength of light. With the increasing of mixing amount of these submicron sized HSMs, these bifunctional layers become white gradually, indicating their significant scattering effect of incident light. It is experimentally damostrated that performance of DSCs can be effectively enhanced by employing these bifunctional highly uniform core/double-shell(CDS) structure in the photoelectrodes, an efficiency of 8.65% was obtained, which is 120% higher than the device based on bare NaYF4:Er3+,Yb3+ employed photoelectrode.

© 2013 Optical Society of America

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