3 research outputs found
Mesoporous BaTiO<sub>3</sub>/TiO<sub>2</sub> Double Layer for Electron Transport in Perovskite Solar Cells
We
report on the effect of BaTiO<sub>3</sub>/TiO<sub>2</sub> mesoporous
double layer (MDL) in the electron transport layer (ETL) of perovskite
solar cells and enhancement of the photovoltaic performance. The conversion
efficiency was enhanced from 9.89% for TiO<sub>2</sub> mesoporous
single layer (MSL) to 12.4% for BaTiO<sub>3</sub>/TiO<sub>2</sub> MDL.
The CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> crystal size on the
BaTiO<sub>3</sub>/TiO<sub>2</sub> MDL was larger. The larger CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> crystals resulted in the better
light absorption and improved <i>J</i><sub>SC</sub>. Moreover, <i>V</i><sub>OC</sub> was also improved by suppressing a charge
recombination, which is attributable to the fewer CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> crystal boundaries and band structure of BaTiO<sub>3</sub>/TiO<sub>2</sub> MDL. The results suggest that using BaTiO<sub>3</sub> as the second layer of the TiO<sub>2</sub> mesoporous layer
is a promising way to boost the performance of perovskite solar cells
Mesoporous BaTiO<sub>3</sub>/TiO<sub>2</sub> Double Layer for Electron Transport in Perovskite Solar Cells
We
report on the effect of BaTiO<sub>3</sub>/TiO<sub>2</sub> mesoporous
double layer (MDL) in the electron transport layer (ETL) of perovskite
solar cells and enhancement of the photovoltaic performance. The conversion
efficiency was enhanced from 9.89% for TiO<sub>2</sub> mesoporous
single layer (MSL) to 12.4% for BaTiO<sub>3</sub>/TiO<sub>2</sub> MDL.
The CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> crystal size on the
BaTiO<sub>3</sub>/TiO<sub>2</sub> MDL was larger. The larger CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> crystals resulted in the better
light absorption and improved <i>J</i><sub>SC</sub>. Moreover, <i>V</i><sub>OC</sub> was also improved by suppressing a charge
recombination, which is attributable to the fewer CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> crystal boundaries and band structure of BaTiO<sub>3</sub>/TiO<sub>2</sub> MDL. The results suggest that using BaTiO<sub>3</sub> as the second layer of the TiO<sub>2</sub> mesoporous layer
is a promising way to boost the performance of perovskite solar cells
Perovskite Solar Cells Prepared by Advanced Three-Step Method Using Additional HC(NH<sub>2</sub>)<sub>2</sub>I Spin-Coating: Efficiency Improvement with Multiple Bandgap Structure
In
the conventional two-step prepared perovskite solar cells, the CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> (MAPbI<sub>3</sub>) film usually
contains an unreacted PbI<sub>2</sub> at the interface between an
electron transport layer (ETL) and a perovskite active layer. To reduce
the unreacted PbI<sub>2</sub> in the two-step prepared MAPbI<sub>3</sub> film, we have recently reported a new three-step method, which was
realized by an additional MAÂ(I,Br) spin-coating. Here, we propose
an advanced three-step method, viz., an additional HCÂ(NH<sub>2</sub>)<sub>2</sub>I (FAI) spin-coating on the two-step prepared MAPbI<sub>3</sub> film. The additional FAI spin-coating formed a FA<sub><i>x</i></sub>MA<sub>1–<i>x</i></sub>PbI<sub>3</sub> solid solution by the incorporation of FA ion into MAPbI<sub>3</sub>. Also, the additional FAI spin-coating yielded a FA<sub><i>y</i></sub>MA<sub>1–<i>y</i></sub>PbI<sub>3</sub> layer (<i>y</i> > <i>x</i>) by converting
the unreacted PbI<sub>2</sub>, which resulted in the layered structure
with different FA concentrations and hence, with the multiple bandgap
structure. The best PCE of 18.1% was achieved by optimizing the FAI
spin-coating process