have received broad research attention as promising candidates for renewableenergy conversion devices owing to their mechanical flexibility, lightweight, absence of toxic heavy metals, and the potential for large-scale fabrication by roll-to-roll printing methodologies. [1] Realization of high-performance BHJ-OSCs devices has relied on photoactive materials design, synthesis, and characterization, as well as thin-film processing advances and device architecture optimization. [2] Since nonfullerene acceptors (NFAs) have now surpassed fullerene acceptors in key properties affecting OSC performance, including strong optical absorption in the visible-near-infrared (vis-NIR) region, adjustable energy levels, charge transport magnitude, and facile structural modification, considerable efforts have been devoted to understanding and perfecting NFAs in recent years. [3] The development of narrow-bandgap (NBG) NFAs with strong optical oscillator strength in the vis-NIR range of 600-1000 nm has been pioneered by several groups; specifically Hou and co-workers reported ITIC-4F [4] and IEICO-4F, [5] and Zhou and co-workers developed Y6. [6] These NFAs when combined with the proper donor polymers have enabled power conversion efficiencies (PCEs) ≈18% for both single-junction and multijunction devices, [7] Fluorination of the donor and/or acceptor blocks of photoactive semiconducting polymers is a leading strategy to enhance organic solar cell (OSC) performance. Here, the effects are investigated in OSCs using fluorine-free (TPD-3) and fluorinated (TPD-3F) donor polymers, paired with the nonfullerene acceptor Y6. Interestingly and unexpectedly, fluorination negatively affects performance, and fluorine-free TPD-3:Y6 OSCs exhibit a far higher power conversion efficiency (PCE = 14.5%) than in the fluorine-containing TPD-3F:Y6 blends (PCE = 11.5%). Transmission electron microscopy (TEM) analysis indicates that the TPD-3F:Y6 blends have larger phase domain sizes than TPD-3:Y6, which reduces exciton dissociation efficiency to 81% for TPD-3F:Y6 versus 93% for TPD-3:Y6. Additionally, grazing incidence wideangle X-ray scattering (GIWAXS) reveals that the TPD-3F:Y6 blends are less textured than those of TPD-3:Y6, while space-charge limited currents reveal lower and unbalanced hole/electron mobility in TPD-3F:Y6 versus TPD-3:Y6 blends. Charge recombination dynamic, transient absorption, and donoracceptor miscibility assays additionally support this picture. Furthermore, conventional architecture TPD-3:Y6 OSCs deliver a PCE of 15.2%, among the highest to date for halogen-free polymer donor OSCs. Finally, a large-area (20.4 cm 2 ) TPD-3:Y6 blend module exhibits an outstanding PCE of 9.31%, one of the highest to date for modules of area >20 cm 2 .