quantum-dot solids, and dye-sensitized metal oxides. [1][2][3][4][5] In recent years, a major breakthrough in performance enhancement has been achieved using lead organo halide perovskite light absorbers which has taken the spotlight in the broad area of emerging thin fi lm photovoltaics. [6][7][8][9][10][11][12][13][14][15][16] Perovskite materials promise to yield inexpensive solar cells owing to the earthabundance and low cost of the primary materials and to the opportunity to solution-manufacture large area panels via continuous and high throughput roll-toroll methods. [ 17 ] To achieve highly effi cient and low cost perovskite cells, efforts have been made mainly in two distinct directions; to modify either electron-injecting nanostructured oxide layers or to develop the nonelectron-injecting-type layers. In the case of electron injecting oxide systems mesoscopic TiO 2 is still one of the most widely employed electron transporting materials (ETMs) in mesoscopic devices. [ 18,19 ] It would be of great interest if all the layers used to fabricate the perovskite devices could be solution-processed at low temperature, thus opening up the routes for high throughput and continuous manufacturing on glass and on plastic substrates at a very low cost. [ 20 ] In this regard, ZnO-based nanostructures have attracted great attention in the dye-sensitized solar cell (DSSC) area as an alternative ETM to the conventional TiO 2 , because of their excellent electrical/optical characteristics that can be tuned easily by manipulating the morphology, doping, and composition. [21][22][23] Moreover, ZnO has several orders of magnitude higher conductivity than TiO 2 which can promote faster electron transport and can be easily solution-processed at low temperature with high structural quality and in a wide range of microstructures using different techniques. [24][25][26][27] Kelly and co-workers [ 28 ] have obtained remarkably effi cient (15.4%, in the reverse direction) perovskite devices based on planar spin-coated ZnO electron transporting layers (ETLs) approaching the performance (19.3%, in the reverse direction) of TiO 2 -based ETL. [ 29 ] However, recent progress in the development of effi cient perovskite solar cells based on ZnO as a mesostructured ETM (e.g., nanoparticulate fi lm or nanorod (NR) array) has pushed the power conversion effi ciency (PCE) to 12% (in reverse direction), [30][31][32][33][34] which is still inferior to comparable mesostructured TiO 2 ETMs (with
Signifi cant effi ciency improvements are reported in mesoscopic perovskite solar cells based on the development of a low-temperature solution-processedZnO nanorod (NR) array exhibiting higher NR aspect ratio, enhanced electron density, and substantially reduced work function than conventional ZnO NRs. These features synergistically result in hysteresis-free, scan-independent, and stabilized devices with an effi ciency of 16.1%. Electron-rich, nitrogendoped ZnO (N:ZnO) NR-based electron transporting materials (ETMs) with enhanced electron mobility produced...