We present a novel Sr-doped TiO 2 /SrTiO 3 nanorod array heterostructures for dye sensitized solar cells (DSSCs) via a facile two-step hydrothermal process, with a tunable microstructure, optical response and photoelectrical conversion properties. The chemical composition components and microstructures of Sr-doped TiO 2 /SrTiO 3 nanorod array heterostructures are investigated using XRD, XPS, SEM and TEM characterization techniques, respectively. It is shown that the treatment of rutile TiO 2 nanorod arrays in Sr(NO 3 ) 2 solution results in the self-doping of Sr into lattice of TiO 2 and formation of Sr-doped TiO 2 /SrTiO 3 nanorod array heterostructures, inducing a transition of optical response property from ultraviolet region to visible region. The photogenerated electrons and holes can be effectively separated due to the formation of SrTiO 3 /Sr-doped TiO 2 heterostructure with uniquely matched band-gap energy structure, resulting in greatly enhanced photoelectric conversion efficiency performance. Electrochemical impedance spectroscopy and photoluminescence results show the formation of Sr-doped TiO 2 /SrTiO 3 heterostructure can effectively prolong the charge carriers' lifetime. The dye loading capacity on the Sr-doped TiO 2 /SrTiO 3 heterostructures can be improved through the functionalization bonding of the hydroxide group on surface of the electrode material. DSSCs based on optimized Sr-doped TiO 2 /SrTiO 3 heterostructure photoanode achieves the highest energy conversion efficiency of 4.70% (one sun illumination), nearly 1.5 times higher than the bare rutile TiO 2 photoanode (3.10%). 9 samples show two arcs in high frequency and low frequency region. It is reported that the first arc implies the charge-transfer resistance of the electrode, and the diameter of the second arc implies the electron life time. 38,39 Accordingly, the resistance of the electrode is about 3.4 (T0), 1.5 (T1) and 4.7 (T3) ohm, respectively, which proves that the Sr-doped TiO 2 /SrTiO 3 heterostructures can effectively improve the charge transfer performance.More importantly, the diameter of the second arcs is in the order of D 1 >D 0 >D 3 , demonstrating that Sr-doped TiO 2 /SrTiO 3 heterostructure can effectively prolong the charge carriers' lifetime, but excess SrTiO 3 may result in the counter effect.The Sr-doping into lattice of TiO 2 could create impurity energy level and narrow the band gap for a wide light absorption. The energy band diagram of DSSCs based on Sr-doped TiO 2 /SrTiO 3 heterostructure is shown in Fig. 9.Due to the matched band gap energy structure between TiO 2 and SrTiO 3 , the formation of Sr-doped TiO 2 /SrTiO 3 heterostructure can effectively suppress the recombination rate of light-induced electrons-holes. The conduction band (CB) of SrTiO 3 locates higher position than that of the rutile TiO 2 , while the valence band (VB) of SrTiO 3 lays lower position than that of rutile TiO 2 . 38, 41 Therefore, the photoinduced electrons from the lowest unoccupied molecular orbital (LUMO) of the dye molecule will t...