Transparent organic semiconductors are desirable for organic optoelectronic devices. While electrical performance is often improved by increasing the p-conjugation length, the resulting red-shifted absorption profile typically leads to loss of transparency. Therefore, it is a great challenge to design and develop organic semiconductor materials that possess both high electrical performance and transparency in visible light region. We have previously developed promising transparent hole-transporting materials (HTMs) based on the quasiplanar skeletons of partially oxygen-bridged triphenylamines.In the present study, we have designed new transparent HTMs by introducing diarylamines into the 7-position of a quasiplanar partially oxygen-bridged triphenylamine. The combination of an oxygen-bridged triphenylamine strong donor and a diarylamine weak donor makes the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) localize on the oxygen-bridged triphenylamine and diarylamine, respectively, leading to minimal orbital overlap between the HOMO and the LUMO, therefore, weak absorption. Three HTMs, namely, HND-Cbz, HND-DTP, and HND-NOMe, were synthesized by connecting a partially oxygen-bridged triphenylamine structure to carbazole, dithieno[3,2-b:2′,3′-d]pyrrole, and bis(4-methoxyphenyl)amine through Buchwald-Hartwig amination with yields of 91%, 70%, and 88%, respectively. All of three materials are amorphous and thermally stable with decomposition temperatures higher than 350 °C. The vacuum-deposited thin films are transparent, with absorption edges from 405 nm to 419 nm. The space-charge limited current (SCLC) hole mobilities of HND-Cbz, HND-DTP, and HND-NOMe are 1.3 x 10- 7, 3.5 x 10- 5 and 1.4 x 10- 4 cm2 V- 1 s- 1, respectively while the HOMO energy levels are –5.34, –5.30 and –5.08 eV. The HOMO levels lie above the corresponding valence band of typical perovskites (e.g. –5.45 eV for MAPbI3 or –5.56 for Cs0.05FA0.15MA0.80PbI2.75Br0.25), making these molecules potentially good candidates for hole-transporting materials in perovskite solar cells. To verify this, perovskite solar cells having the structures ITO/SnO2/Cs0.05FA0.15MA0.80PbI2.75Br0.25/HTM/Au for the solution processed HTM and ITO/SnO2/Cs0.05FA0.15MA0.80PbI2.75Br0.25/HTM/MoO3/Au/MoO3 for the vacuum processed HTM layer, were fabricated. With HND-Cbz, HND-DTP and HND-NOMe as the HTM, the best power conversion efficiency reached 13.7%, 15.0% and 17.2%, respectively. Figure 1