The certified laboratory power conversion efficiency (PCE) of 25.2% has recently been achieved for hybrid organic-inorganic lead halide perovskite solar cells (PSCs), [1-5] which is now on par with that of the traditional photovoltaic (PV) devices. Despite their high efficiencies, the intrinsic volatility and thermal instability of organic components in hybrid perovskites are considered to be the important factors that limit their practical applications of PSCs. [6,7] As a potential solution to overcome the shortage of hybrid PSCs, allinorganic perovskites (CsPbX 3 , X ¼ Cl, Br, I, or mixed) have been developed in recent years. [8-10] Among them, mixedhalide inorganic perovskites, CsPbI 2 Br, feature excellent thermal stability and suitable direct bandgap (1.92 eV) for potential usage in tandem solar cells, and have gained increased attentions. [11,12] Much efforts have been dedicated to boost the PCEs of normal structured (n-i-p) CsPbI 2 Br PSCs to over 16% via interfacial engineering, crystallization tailoring, ion substitution, and/or doping of the perovskite. [13,14] Nevertheless, the PCEs for CsPbI 2 Br PSCs still lag far behind that of the hybrid PSCs, especially for the inverted structured devices (the latest developments for inverted CsPbI 2 Br PSCs are shown in Table S1, Supporting Information). [15] Compared with the n-i-p structured device, the development of inverted (p-in) structured PSCs is quite attractive and has recently drawn ever-increasingly research interests [16,17] because it can not only avoid using the unstable hole transport layers (HTLs), such as Spiro-OMeTAD (where 4-tert-butyl pyridine and lithium salts were traditionally adopted as the dopants), but also be more compatible with tandem solar cells. Up to date, most of the perovskite/perovskite tandem solar cells are fabricated with the p-in structures. [18,19] However, the development of inverted wide-bandgap PSCs remains limited. Therefore, it is highly desirable to develop novel strategies for high-efficiency inverted wide-bandgap PSCs. It is well known that the key factors influencing the overall device efficiency should be: 1) the film quality of all functional layers, especially for light absorber and charge transport layers (CTLs); 2) optoelectronic properties of CTLs, such as bandgaps, carrier mobility, and energy levels. [20-23] Therefore, obtaining high-quality perovskite film with reduced defects is the prerequisite for high-performance solar cells. Thus, far ion doping, such as Eu 2þ , [24] Mn 2þ , [25] Nb 5þ , [26] Cu 2þ , [27] Cl À , [25] and Br À , [28] has been proven to be an effective strategy to obtain large grains and in situ strengthen original octahedral structural stability in