to the electronic and morphological parameters in the active perovskite layer, the electron transport layer (ETL) and hole transport layer (HTL) are significantly important in determining the photovoltaic performance in perovskite solar cells. [3][4][5][6] Specifically, the role of a transport layer in solar cells is to facilitate charge transport and assist charge collection toward the respective electrodes as well as inhibiting from recombination of charge carriers on the path to the electrodes. [3] Meanwhile, the open circuit voltage (V oc ) is normally determined by the energy differences between the Fermi levels of the ETL and the HTL. There are certain prerequisites for a hole transport material in order to perform more efficiently in perovskite solar cells, such as energy band alignment, suitable hole mobility, chemical compatibility with the perovskite layer as well as good thermal and photochemical stability. [5,6] In addition, morphology and crystallinity of this layer plays an important role. The importance and influence of these parameters in the transport layer on perovskite solar cells performance have been extensively investigated. [3,[5][6][7][8][9][10] In this article, we demonstrate the importance of photogenerated dipoles in the HTL as a new strategy to improve the photovoltaic performance of planar perovskite solar cells. In order to explore this effect, we select two HTLs with similar conjugated thiophene backbones, namely PTB7 and P3HT with significant and negligible optically generated dipoles. Moreover, our measurements based on space charge limited current model indicate that PTB7 and P3HT have hole mobilities in the same order in agreement with previous publications (Figure S1, Supporting Information). [11][12][13][14] It has been shown that PTB7 has a relatively large internal dipoles through intrachain charge transfer from benzodithiophene to thienothiophene moieties under photoexcitation. [15] The dipole moments (D) in ground and excite states have been measured to be 3.76 and 7.13 for PTB7 and 0.19 and 0.43 for P3HT, respectively. [15] In general, perovskites have the advantage of both bulk polarization and semiconducting properties. [16][17][18][19][20] It was shown that the presence of a polar molecule, methylammonium at the center of perovskite introduces the possibility of orientational P3HT-poly(3-hexylthiophene) are separately used as the HTL with significant and negligible photoinduced dipoles, respectively. Electric field-induced photoluminescence quenching provides the first-hand evidence to indicate that the photoinduced dipoles are partially aligned in the amorphous PTB7 layer under the influence of device built-in field. By monitoring the recombination process through magneto-photocurrent measurements under device operation condition, it is shown that the photoinduced dipoles in PTB7 layer can decrease the recombination of photogenerated carriers in the active layer in perovskite solar cells. Furthermore, the capacitance measurements suggest that the photoinduced dipoles ...