Tuning donor/acceptor interfacial arrangements and electron-transfer processes in the active layers is crucial to improve the performance of organic solar cells (OSCs). Here, the impact of different molecular architectures (i.e., A-π -D-π -A, D-π-A-π -D and π-A-D-A-π ) of the donors on the interfacial arrangements and electronic processes in small-molecule (SM) OSCs is elucidated by means of multiscale theoretical simulations. An A-π-D-π-A structured donor with sizable terminal units, extended π bridges, and bulky side groups on the backbone core is proved to be able to simultaneously obtain both efficient charge generation and migration as well as suppressed charge recombination, thus paving the way for the rational design of electron donors toward high-performance SM OSCs.Solution-processed bulk heterojunction (BHJ) organic solar cells (OSCs) have achieved remarkable progress in the past decade. [1][2][3][4][5][6][7][8][9] For fullerene-based small-molecule (SM) OSCs, power conversion efficiencies (PCEs) have exceeded 11%, which is in stark contrast to the highest value of 1% in 2006 (Figure 1a). [4,5,[10][11][12][13][14][15][16][17][18][19] This significant improvement is attributed to the great efforts in developing new SM donors and device optimizations. [20][21][22][23][24][25][26][27][28] To date, three typical push-pull molecular structures, namely, D-π -A-π -D, π -A-D-A-π , and A-π -D-π -A, have been successfully used as SM donors. It is noteworthy that most of the donors with PCEs over 9% are of A-π -D-π -A structures. [4,5,18,[29][30][31][32][33] Inspired by the success of fullerene-based SM OSCs, nonfullerene counterparts have shown faster progress in the past few years (Figure 1a). [8,9,[34][35][36][37] Similarly, for nonfullerene SM OSCs with PCEs over 9%, both the donors and acceptors adopt A-π -D-π -A and/or Aπ -A structures. [8,9,[38][39][40] To realize solution processing in organic solvents, alkyl side chains are necessary to attach to the