and optical properties, such as direct-toindirect band gap transition with thickness decreasing, [1] orbit-spin coupling, [2] and spin-valley locking [3] heralding the great potential of TMDs in optical and optoelectronic applications. [4][5][6] The band alignment semiconducting heterojunction is divided into three categories according to the relative positions of their energy bands, that is, type I (straddling), type II (staggered), and type III (broken). Type II structure can efficiently separate electrons and holes on two sides of the heterojunction, extending the photoexcited carrier lifetime, [7] therefore are preferable for field-effect-transistor-based photodetector, solar cell, photocatalyst, etc. In a type I heterostructure, both electrons and holes tend to transfer from wide to narrow bandgap side, largely increasing the chance of recombination of electrons and holes and facilitating photon generation and luminescent efficiency, therefore are suitable for devices like light-emitting diodes . [8] Heterojunctions composed of two monolayer TMDs are usually type II structures, while type I structures are rarely observed [9] and only reported on MoTe 2 /WSe 2 , [10] ReS 2 /MoS 2 , [11] etc. The limitations to obtaining vertical type I TMD heterostructures mainly originate from Atomically thin monolayer semiconducting transition metal dichalcogenides (TMDs), exhibiting direct band gap and strong light-matter interaction, are promising for optoelectronic devices. However, an efficient band alignment engineering method is required to further broaden their practical applications as versatile optoelectronics. In this work, the band alignment of two vertically stacked monolayer TMDs using the chemical vapor deposition (CVD) method is effectively tuned by two strategies: 1) formulating the compositions of MoS 2(1-x) Se 2x alloys, and 2) varying the twist angles of the stacked heterobilayer structures. Photoluminescence (PL) results combined with density functional theory (DFT) calculation show that by changing the alloy composition, a continuously tunable band alignment and a transition of type II-type I-type II band alignment of TMD heterobilayer is achieved. Moreover, only at moderate (10°-50°) twist angles, a PL enhancement of 28%-110% caused by the type I alignment is observed, indicating that the twist angle is coupled with the global band structure of heterobilayer. A heterojunction device made with MoS 0.76 Se 1.24 /WS 2 of 14° displays a significantly high photoresponsivity (55.9 A W -1 ), large detectivity (1.07 × 10 10 Jones), and high external quantum efficiency (135%). These findings provide engineering tools for heterostructure design for their application in optoelectronic devices.