optoelectronic devices in particular are an appealing alternative to current inorganic technologies, which suffer from limited modularity, intrinsic fragility, low speed, high power consumption, cryogenic cooling requirements, and epitaxial incompatibility with Si complementary metal-oxide-semiconductor (CMOS) processes. [12] The beneficial electronic properties of narrow gap OSCs, such as low exciton binding energies and facile charge extraction, stem from their strong intramolecular polarity and easily accessible carrier transport energy levels. [4,13,14] However, the strong intramolecular polarity also leads to dramatic and unexpected changes in photophysics, such as ultrafast exciton self-ionization, [13,14] emergence of low-energy dark states, [15] and singlet fission mediated by intramolecular charge-transfer character. [16,17] Rationally designing devices to employ these materials requires a deeper understanding of their unique photophysical properties.There is a nascent interest in polymeric materials with electronic absorption in the short-wave infrared (SWIR), where recent advances in synthetic techniques have pushed band gaps of solution-processable materials as low as ≈0.5 eV. [18][19][20][21][22] Although further development of structure-function relationships is required to reach even lower band gaps, thus far the successful engineering of narrow gap polymers has, in large part, followed a "push-pull" design strategy in which the energetic difference between the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) is controlled by varying the electron Infrared organic photodetector materials are investigated using transient absorption spectroscopy, demonstrating that ultrafast charge generation assisted by polymer aggregation is essential to compensate for the energy gap law, which dictates that excited state lifetimes decrease as the band gap narrows. Short sub-picosecond singlet exciton lifetimes are measured in a structurally related series of infrared-absorbing copolymers that consist of alternating cyclopentadithiophene electron-rich "push" units and strong electron-deficient "pull" units, including benzothiadiazole, benzoselenadiazole, pyridalselenadiazole, or thiadiazoloquinoxaline. While the ultrafast lifetimes of excitons localized on individual polymer chains suggest that charge carrier generation will be inefficient, high detectivity for polymer:PC 71 BM infrared photodetectors is measured in the 0.6 < λ < 1.5 µm range. The photophysical processes leading to charge generation are investigated by performing a global analysis on transient absorption data of blended polymer:PC 71 BM films. In these blends, charge carriers form primarily at polymer aggregate sites on the ultrafast time scale (within our instrument response), leaving quickly decaying single-chain excitons unquenched. The results have important implications for the further development of organic infrared optoelectronic devices, where targeting processes such as excited state delocalization ov...