energy. Since the first report by Miyasaka and co-workers in 2009, [1] the perovskites (e.g., CH 3 NH 3 PbI 3 ) have been widely studied due to their good light absorption capability from visible to near-infrared, long charge diffusion lengths, and high carrier mobilities as well as solutionprocessabilities. [2][3][4][5][6][7][8][9][10] Benefited from careful modification of perovskite, delicate design of device configuration, and in-depth understanding of interfacial interactions, the power conversion efficiencies (PCEs) of PVSCs have been skyrocketed from initial 3.8% to above 20% to date. [11][12][13][14][15][16][17][18][19] Nowadays, as a necessary component in the most studied conventional n-i-p junction PVSCs, the hole-transporting materials (HTMs) play an even more critical role in efficiently extracting holes separated from perovskite layer and simultaneously transmitting to anode in order to avoid loss in open-circuit voltage (V oc ) and decrease in charge recombination. [20][21][22][23] Currently, most of the highly efficient PVSCs utilize 2,2′,7,7′-tetrakis(N,N-di-p-methoxyphenylamine)-9,9′-spirobifluorene (Spiro-OMeTAD) as the HTM owing to its matched energy level with the valence band edge of the perovskite, and high compatibility with lithium bis(trifluoromethanesulfonyl)imide (LiTFSI) dopant. Nevertheless, the low synthetic yield and high cost for Spiro-OMeTAD will inevitably obviate the large-scale production and practical commercialization of PVSCs. As a result, efforts have been executed in developing cheaper, more stable, and efficient organic HTMs to replace Spiro-OMeTAD. When focusing on their intrinsic properties, these small molecular HTMs can be divided into three categories: (i) donor-acceptor type structures to form intramolecular charge transfer character, which usually show decent PCEs in dopant-free devices; [24][25][26][27] (ii) 2D (quasi) planar molecular structures to enhance intermolecular π-π interactions, which lead to excellent hole-transporting properties; [28,29] (iii) arylamines derivatives with different central building blocks such as pyrene, [30] 1,1,2,2-tetraphenylethene, [31] bifluorenylidene, [32] 4,4-N,N′-dicarbazole-1,1′-biphenyl, [33] quinolizino acridine, [34] thiophene, and derivatives, etc., [35][36][37][38] and di(4-methoxyphenyl)amine as the peripheral functional groups to endow adequate hole-transporting properties via radical cation species. [39] It is worth noting that the efficient HTMs in the state-of-the-art PVSCs usually contain spiro-arranged Perovskite solar cells have emerged as a promising technique for low-cost, light weight, and highly efficient photovoltaics. However, they still largely rely on 2,2′,7,7′-tetrakis(N,N-di-p-methoxyphenylamine)-9,9′-spirobifluorene (Spiro-OMeTAD) to serve as hole-transporting materials (HTMs). Here, a series of HTMs with small molecular weight is designed, which are constructed on a spiro core involving phenylpyrazole and a second heteroaromatics, i.e., xanthene (O atom), thioxanthene (S atom), and acridine (N atom)....