residual Coulomb attraction with holes, enabling ultrafast charge separation. [ 21 ] Therefore, it is very important to understand and ultimately control the active layer morphologies and the D/A interface confi gurations at the molecular level. [8][9][10][11][12][13][14][15][17][18][19][20][21][22][23][24] Although modulation of the active layer morphologies has been successfully achieved by several different preparation procedures, [ 1,12,13,[25][26][27][28] it still remains experimentally diffi cult to accurately probe the molecular self-assembly processes and packing structures, [ 29 ] which severely hinders obtaining reliable structure-property relationships and further improving the device performance.Over the past a few years, a series of small-molecule donors with a simple D-A-A structure have been synthesized by Wong and co-workers for high-effi ciency vacuum-deposition OSCs; [30][31][32][33] in conjunction with the C 60 or C 70 acceptor, the highest power conversion effi ciency (PCE) has reached 6.8% for a single junction cell, [ 31 ] 10.0% and 11.1% for a tandem and a triple junction cell, [ 34 ] respectively. Among these donor materials, 2-{[7-(5-N , N -ditolylaminothiophen-2-yl)-2,1,3-benzothiadiazol-4-yl]methylene}malononitrile (DTDCTB, see Figure 1 a) has gained intensive attention. [ 30,31,[34][35][36][37][38][39][40][41][42] Here, interesting to us is the antiparallel packing mode in the DTDCTB crystal (see Figure 1 b), which can provide a variety of model surfaces with different features to systematically probe the infl uence of donor surfaces on the fullerene packing and interface morphologies.In this contribution, we have mimicked vapor-phase deposition and growth of C 60 on different DTDCTB substrate surfaces via nonequilibrium atomistic molecular dynamics (MD) simulations. [ 43,44 ] Using this scheme, Muccioli and co-workers have investigated the crystal growth of pentacene or sexithiophene on the C 60 (001) substrate, while the relationship between different surface properties and thin-fi lm morphologies is yet to be revealed. [ 43,44 ] Our simulated results point to that, both the interfacial and thin-fi lm morphologies substantially depend on a combinational role of the stability, ordering, landscape, and local molecular orientation of the substrate surfaces. This work will be helpful to understand and control the formation of crystalline fullerene in the active layer toward achieving effi cient separation of the photogenerated charges for organic photovoltaics.The initial DTDCTB substrate surfaces with different molecular orientations, i.e., nearly "fl at," "upright," and "edge-on" confi gurations (see Figure S1, Supporting Information) were constructed by cleaving the DTDCTB crystal along the (100), (010), and (001) crystallographic planes, respectively. Each type of confi guration has two opposite facets, labeled as A and B (i.e., obtained by cutting the cell at full and half cell, respectively), because the molecules stack in an antiparallel manner Organic solar cells offer considerab...