conditions, such as the solvent and dopants used, as well as the doping concentrations. [ 5 ] Therefore, it is imperative to develop low-cost, dopant-free HTMs for effi cient PSCs. Most recently, impressive photovoltaic performance has been reported for different HTMs, such as small molecule-based HTMs, [29][30][31][32][33][34][35][36] polymer-based HTMs, [37][38][39][40] and inorganic hole conductors. [ 41,42 ] However, the vast majority of these reported HTMs require doping and the highest effi ciency reported in PSCs so far is less than 13%. Some novel HTMs, besides good hole mobilities, simultaneously show strong light absorbtion in the visible and near-infrared region. [ 34,35 ] Thus, these materials also have the potential to act as photoactive donor materials (PDMs) in bulk heterojunction (BHJ) organic solar cells (OSCs). [ 43,44 ] Herein, we report the design and synthesis of an acceptordonor-acceptor (A-D-A) structured small-molecule material M1 based on a rigid benzo[1,2b:4,5b′]-dithiophene (BDT) central building block and phenoxazine (POZ) linkers. With its unique properties, such as suitable energy levels, strong optical absorption in the visible region, and high hole mobility, M1 has been used both as HTM in (CH 3 NH 3 )PbI 3 -perovskite-based solar cells and as PDM in BHJ OSCs. Excellent PCE of 13.2% under 100 mW cm −2 irradiation was achieved using M1 as dopant-free HTM in PSCs, as compared to 12.4% obtained for devices containing the p-type doped Spiro-OMeTAD as HTM and 7.14% for the devices not containing any HTM. When applied in BHJ OSCs, a PCE of 6.91% was achieved using an optimized device structure of ITO/ZnO/polyethylenimine, 80% ethoxylated (PEIE)/ M1 :PC 70 BM (1:1.2)/MoO 3 /Ag. To the best of our knowledge, this is the fi rst case where a small-molecule organic material has been shown to act both as an HTM in PSCs and as a PDM in BHJ OSCs and showing excellent conversion effi ciencies in both types of solar cell systems.The structure and route of synthesis of the small-molecule material M1 are shown in Figure 1 and Scheme 1 , respectively. The BDT unit is rigid and fl at and is widely used as central building block in the construction of small-molecule donor materials for the application in BHJ OSCs, and this class of materials tend to exhibit high hole mobility and overall conductivity. [45][46][47][48][49] POZ is a well conjugated heterocyclic ring system with a butterfl y conformation and it is widely used in dyesensitized solar cells, possessing unique electronic and optical properties. [50][51][52][53] The BDT core unit was functionalized with ( Z )-3-(3-ethylrhodanine-5-alkenyl)-10-(2-ethylhexyl)-phenoxazine groups in order to generate a low band gap material. The symmetrical structure is expected to enhance π−π stacking interactions, which could be benefi cial for promoting a high hole The development of cost-effective, high-effi ciency solar cells that can meet the ever increasing demand of sustainable energy is one of the great challenges in the 21st century. Over the past two ye...