Metal-halide perovskites were firstly introduced to a dye-sensitized solar cell (DSSC) as visible-light absorbers by Miyasaka and his coworkers in 2009. At that time, the device demonstrated a light-to-electricity power conversion efficiency (PCE) of 3.8%. [1] Subsequently, based on these perovskites, Park et al. developed a solid-state DSSC by substituting the liquid electrolytes with spiro-MeOTAD as the hole conductors. [2] The PCE of the photovoltaic device is boosted to 9.7% and the device stability is also greatly enhanced. In 2013, the researches further revealed that these solution-processed metal-halide perovskites possess long-range balanced electron-and hole-transport lengths, [3,4] which suggests that the DSSC architecture designed for decoupling light absorption and charge carrier transport is not necessarily needed. In the same year, Snaith and his coworkers constructed high efficiency (over 15%) perovskite solar cell (PSC) with a planar heterojunction (PHJ) architecture, [5] which confirms the previous finding. Up to now, highly efficient perovskite-based solar cells with a broad range of configurations have been demonstrated. [6] The highest certified PCE value is over 25%. [7] Since the perovskites have been revealed as super semiconductors, most of the reported PSCs were constructed with a traditional p-i-n device structure. The photo-induced charge carrier dynamics within the device could be described by the classic physics in a traditional thin-film solar cell.Recently, due to the excellent environmental stability of all-inorganic PSCs, related research is getting more and more attention. Unfortunately, the performance of the device is limited, especially for the J SC , because of the narrow visible-light absorption spectral window. [8] In this issue of Energy & Environmental Materials, Guo et al. increased the J SC of PSCs around 19% (from 7.51 to 8.92 mA cm −2 ) by employing high target utilization sputtering Nb-doped SnO 2 ETLs. [9] The carrier concentration of ETLs can be increased from 10 18 to 10 19 cm −3 by 3%