PCE of PSCs has not yet reached its limit (30.5%), implying there is still much room for further improve the performance of PSCs.To obtain PSCs with higher photoelectric performance and higher stability, various strategies have been developed to optimize the perovskite layer and charge carrier transport layers. [10][11][12] Exploring appropriate materials as efficient electron transport layers (ETLs) is also vital to promote the rapid development of PSCs. Titanium dioxide (TiO 2 ) was initially used as ETL material in PSCs, owing to the advantages of low cost, high stability, and superior ability able to effectively transferring of electrons from the perovskite layer to the bottom electrode. However, the energy levels of TiO 2 and perovskite are not matched well. Meanwhile and the annealing temperature of TiO 2 is high (above 450 °C), which is energy consuming and incompatible with flexible devices. [13][14][15] Alternatively, tin dioxide (SnO 2 ), has become the most commonly used ETL material, due to its advantages of low-temperature manufacturing, good energy level matching, and high electron mobility. However, using SnO 2 as ETL is inevitable to encounter defects (oxygen vacancy defects) pinholes at the film surface. These defects have a significantly negative impact on the photovoltaic performance and stability performance of perovskite solar cells. [16,17] Based on this, interfacial modification and doping strategies were applied to PSCs. Ogomi et al. introduced a monolayer HOCO-R-NH 3
The buried interface between perovskite light absorbing layer (PVK) and electron transport layer (ETL) plays an utmost important role for further improving the efficiency and stability of planar perovskite solar...
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