Wide-bandgap perovskites are attractive top-cell materials for tandem photovoltaic applications. Comprehensive optical modeling is essential to minimize the optical losses of state-of-the-art perovskite/perovskite, perovskite/CIGS, and perovskite/silicon tandems. Such models require accurate optical constants of wide-bandgap perovskites.
View Article and Find Full Text PDFWe apply a series of transient measurements to operational perovskite solar cells of the architecture ITO/PTAA/FACsPb(IBr)/C60/BCP/Ag, and similar cells with FAMA. The cells show no detectable JV hysteresis. Using photocurrent transients at applied bias we find a ∼1 ms time scale for the electric field screening by mobile ions in these cells.
View Article and Find Full Text PDFWe demonstrate four- and two-terminal perovskite-perovskite tandem solar cells with ideally matched band gaps. We develop an infrared-absorbing 1.2-electron volt band-gap perovskite, FACsSnPbI, that can deliver 14.
View Article and Find Full Text PDFThe active layers of perovskite solar cells are also structural layers and are central to ensuring that the structural integrity of the device is maintained over its operational lifetime. Our work evaluating the fracture energies of conventional and inverted solution-processed MAPbI perovskite solar cells has revealed that the MAPbI perovskite exhibits a fracture resistance of only ∼0.5 J/m, while solar cells containing fullerene electron transport layers fracture at even lower values, below ∼0.
View Article and Find Full Text PDFA sputtered oxide layer enabled by a solution-processed oxide nanoparticle buffer layer to protect underlying layers is used to make semi-transparent perovskite solar cells. Single-junction semi-transparent cells are 12.3% efficient, and mechanically stacked tandems on silicon solar cells are 18.
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