Nowadays photodetectors primarily rely on inorganic semiconductors including silicon and III-V compounds. [6][7][8][9][10] But the fabrication of these devices requires costly, size-limited epitaxial growth methods that are not compatible with on-chip integration and mass production. [11,12] Therefore, increasing interests have been evoked recently to produce cost-effective photodetectors consisting of solution-processable materials. [1,[13][14][15] Metal-halide perovskites have emerged with considerable potential as the next-generation materials of photodetectors because of their ease of processing, tailorable optoelectronic properties, and compatibility with flexible substrates. [12,16] Following the development pathway of perovskite photovoltaics, material scientists have reported perovskite photodetectors with an n-i-p structure using mesoporous TiO 2 (meso-TiO 2 ) at the early stage. [14,17,18] Although being an excellent electron transporting layer (ETL) for photovoltaics, meso-TiO 2 has been found to show large capacitance leading to slow response to an Monolithic integration of nanostructured metalenses with broadband light transmission and good charge transport can simultaneously enhance the sensitivity, speed, and efficiency of photodetectors. The realization of built-in broadband metalenses in perovskite photodetectors, however, has been largely challenged by the limited choice of materials and the difficulty in nanofabrication. Here a new type of broadband-transmitting built-in TiO 2 metalens (meta-TiO 2 ) is devised, which is readily fabricated by one-step and lithographfree glancing angle deposition. The meta-TiO 2 , which comprises of sub-100 nm TiO 2 nanopillars randomly spaced with a wide range of sub-wavelength distances in 5-200 nm, shows high transmittance of light in the wavelength range of 400-800 nm. The meta-TiO 2 also serves as an efficient electron transporting layer to prevent the exciton recombination and facilitate the photoinduced electron extraction and transport. Replacing the conventional mesoporous TiO 2 with the meta-TiO 2 comprehensively leads to enhancing the detection speed by three orders of magnitude to a few hundred nanoseconds, improving the responsivity and detectivity by one order of magnitude to 0.5 A W −1 and 10 13 Jones, respectively, and extending the linear dynamic range by 50% to 120 dB.