Organic solar cells (OSCs) have attracted enormous research interest due to their promise for the realization of lightweight, mechanically flexible, and portable power generators using low-cost printing techniques. [1-3] Solution-processable OSCs are typically based on a bulk heterojunction (BHJ) architecture comprising electron-donating (donor) and electronaccepting (acceptor) semiconductors. In recent years, the continual development of innovative photovoltaic materials, [4-14] device and interface engineering [15-19] in conjunction with better understanding of fundamental mechanisms [20-23] have contributed to the rapid progress of BHJ OSCs. Their power conversion efficiencies (PCEs) have now reached more than 17% for both single-junction [24-28] and tandem [29] devices, providing great prospects for practical applications. The achievable performance of OSCs is strongly dependent on the BHJ blend morphology, wherein the donor and acceptor are expected to form nanoscale phase separation and bicontinuous pathways for maximizing charge generation and transport. [30] At present, BHJ photoactive layers are fabricated normally via spin-coating of the mixture of donor and acceptor materials, which usually leads to complicated dynamics and kinetics during the morphological evolution. [31,32] One of the long-standing challenges in realizing optimum BHJ configuration through such a method is to strike a delicate balance between the miscibility and self-organization of two active components during processing, thus imposing stringent requirements on the treatment conditions. Specifically, in the state-of-the-art nonfullerene systems, the donor and acceptor typically possess similar planar molecular structures and good miscibility, which enhances the difficulty in controlling the BHJ morphology. [33] An alternative way is to deposit neat donor and acceptor sequentially trying to reduce the complexity of interaction between two components. Previous studies have indicated that this sequential deposition method is feasible to create a p-in like structure due to the interdiffusion of top layer into bottom one and higher gradient concentration of acceptors near the cathode and donors near the anode. [34-36] Additionally, the two-step procedure allows each layer to be regulated and optimized independently, affording new opportunities for Bulk-heterojunction (BHJ) organic solar cells (OSCs) are prepared by a common one-step solution casting of donor-acceptor blends often encounter dynamic morphological evolution which is hard to control to achieve optimal performance. To overcome this hurdle, a generally applicable, sequential processing approach has been developed to construct high-performance OSCs without involving tedious processes. The morphology of photoactive layers comprising a polymer donor (PM6) and a nonfullerene acceptor (denoted as Y6-BO) can be precisely manipulated by tuning Y6-BO layer with a small amount of 1-chloronaphthalene additive to induce the structural order of Y6-BO molecules to impact the blend phase. Th...