to the long chemical readsorption process (oxygen molecules readsorption) occurred at the surface. [10,11] In contrast, the photo voltaic PDs including p-n homojunctions, p-n heterojunctions, and Schottky barrier diodes show a fast response speed and a possible selfpowered function due to the photovoltaic effect. Furthermore, as there is an increasing emphasis on low energy consumption, selfpowered PDs which can operate without an external power source are particularly appealing in applications like submarine oil leakage monitoring and forest fires prevention. [12] Thus, researchers are highly motivated to develop highperformance UV PDs with selfpowered characteristics.Thanks to the continuous innovations in semiconductor technology, various widebandgap materials such as diamond, ZnO, TiO 2 , ZnS, etc., have drawn great attention in the field of UV PDs. [13][14][15][16] Among them, SnO 2 , a conventional metal oxide with a direct bandgap, is generally regarded as a ntype material in its undoped form because of the intrinsic defects. It possesses unique chemical, electrical, and optoelectronic properties, thus having vast applications in gas sensors, transparent conductors, and optoelectronic devices. [17][18][19] In particular, with a wide bandgap of ≈3.6 eV (at 300 K), SnO 2 exhibits good UV light absorption characteristics and high vis ible light transparency, making it an ideal candidate for UV PD, especially under acidic or alkalic circumstances in comparison with ZnO. [20] Up to now, various efforts have been devoted to demonstrate the excellent UV photosensitivity of SnO 2 . Previ ously, our group presented thin SnO 2 nanowire UV PDs with a high external quantum efficiency. [21] Chen et al. [22] fabricated monolayer SnO 2 nanonets with a high UV photocurrent. Tian et al. [23] reported ZnOSnO 2 heterojunction nanofibers with a high UV photodark current ratio. However, the response time of the works mentioned above is still dissatisfactory, of which the decay time is >50 s, [22] ≈50 s, [21] and 7.8 s, [23] respectively. Recently, Ling et al. [24] constructed a SnO 2 nanoparticle thin film/ SiO 2 /pSi heterojunction, which exhibited a short response time (<0.1 s) and a high UV photocurrent (≈4.0 × 10 −5 A), however, it suffered from a low photosensitivity (≈40) due to the high dark current. Thus, a combination of a high photosensitivity and a fast response speed has not been realized in SnO 2 PDs, not to men tion additional functions including selfpowered property and flexibility.Herein, a single-crystal SnO 2 microwire photodetector (PD) is demonstrated with a fast response speed owing to a low concentration of point defects. However, the presence of surface defects (e.g., oxygen vacancies) still limits its optoelectronic performance. To further improve the photoresponse of such device, a core-shell p-n junction is constructed by simply coating a new p-type transparent conductive (CuS) 0.35 :(ZnS) 0.65 nanocomposite film (CuZnS) on n-type SnO 2 microwire. As a result, not only the surface of SnO 2 is modified...