S CT) or triplet ( T CT) character in a 1:3 ratio following the spin statistics. [8] These nearly energetically degenerate S CT and T CT excitons will recombine or separate again into FC. The recombination of S CT to the ground state (S0) can be effectively suppressed because of the high enough S CT energy (E CT ), according to the energygap law ( Figure S1a, Supporting Information). [9−12] Although the recombination from T CT to S0 is spin-forbidden, T CT can relax to the lower-lying triplet state (T1) on the material with lower S1 excitation energy (E S1 , which determines optical gap of the device, E g ) via back electron transfer (BET). [13−18] The singlet−triplet energy gap (ΔE ST = E S1 -E T1 , where E T1 is the T1 excitation energy) is usually very large (≈0.7 eV) in the organic π-conjugated molecules and polymers with strong optical absorption and emission. [19−21] If the CT driving force (ΔE CT = E S1 -E CT ) is small (as required to maximize open-circuit voltage, V OC ), the speed of T1 to thermalize back into T CT will be limited due to the large difference between E CT and E T1 (ΔE BET = E CT -E T1 , Figure S1b, Supporting Information); the decay of T1 to S0 via intersystem crossing (ISC) and tripletcharge annihilation can thus constitute a major terminal loss channel of photocurrent. [13−18] Therefore, in order to reduce both voltage loss and NG recombination, the ΔE ST needs to be minimized ( Figure 1b). [22,23] Here, we have investigated the critical role of end-group π−π stacking in reducing ΔE ST in the state-of-the-art narrowbandgap nonfullerene (NF) acceptors (ITIC, IT-4F, and Y6, [24−26] Figure 2a) by means of (time-dependent) density functional theory (TD)DFT calculations in combination with molecular dynamics (MD) simulations (see Supporting Information for details). Owing to a modest degree of intramolecular push−pull effect, these acceptors show moderate ΔE ST while large oscillator strength ( f, ≈3) in the isolated molecules. Importantly, the ΔE ST is further reduced to 0.3−0.4 eV in the end-group π−π stacking dimers that are frequently present in the films. Such small ΔE ST proves to be able to suppress the T1 decay even in the case of very low ΔE CT of 0.1−0.2 eV. Accordingly, high J SC (>20 mA cm −2 ) and fill factor (FF, 75-80%) as well as low ΔV OC (≈ 0.6 V) have been achieved simultaneously, leading to high power conversion efficiencies (PCEs) of 13-18% in the OPVs based on these acceptors. [25−40] In principle, the ΔE ST value is determined by the electron exchange energy. Normally, the S1 and T1 states are both To improve the power conversion efficiencies for organic solar cells, it is necessary to enhance light absorption and reduce energy loss simultaneously. Both the lowest singlet (S1) and triplet (T1) excited states need to energertically approach the charge-transfer state to reduce the energy loss in exciton dissociation and by triplet recombination. Meanwhile, the S1 energy needs to be decreased to broaden light absorption. Therefore, it is imperative to reduce the...