Benefitting from the development of nonfullerene acceptors (NFAs), the power conversion efficiency (PCE) approaching 19% has been achieved in single-junction organic solar cells (OSCs). [1,2] Compared with fullerene acceptors (FAs), NFAs present different aspects of advantages, such as the tunable energy levels, [3,4] strong absorption in the visible-to-near-infrared wavelength range, [5,6] and various molecular aggregation structures. [7,8] Despite molecular diversity, most of the highperformance NFA molecules (e.g., ITIC and Y6) have push-pull electronic structure, where the central group has stronger electron push ability, the terminal groups have stronger electron pull ability, and sometimes π-bridges connecting the central group and the terminal groups. [9,10] Up to now, different strategies have been explored to strengthen the electron push ability of the central group, such as extending the conjugation length, [11,12] introducing strong electron push group (e.g., alkoxy or alkyl amino side groups), [13,14] and inserting quinone resonance structure. [15] To strengthen the electron pull ability of the terminal groups, one usually introduces halogen atoms (e.g., fluorine and chlorine). [16][17][18][19] The push-pull electronic structure of NFA molecules can result in their intramolecular charge transfer character, reducing the binding energy of their excited states. [20][21][22][23] Recent works have successively reported that the excited states in NFA molecules might behave in intra-and intermolecular charge transfer (CT) states, [24,25] which can dissociate into free charges even at room temperature without the assistance of a donor/acceptor (D/A) energy offset. [24][25][26] In FA-based OSCs, we know that polymer donors usually act as the light-absorbing components due to the poor absorption of FA molecules, [27] such that charges mainly originate from the donor excitation via experiencing the interfacial electron transfer into FA molecules. [28] In NFA-based OSCs, polymer donors and NFA molecules usually have complementary absorption; thus, charge generation presents diverse channels. When the donor molecule is photoexcited, the excited electron transfers into NFA molecule. [20,22,23] When NFA molecule is photoexcited, the excited hole transfers into donor molecule. [10,21,25] Recently, a third charge generation channel was revealed in