with CYTOP dielectric though the BT units have less planarity than the TVT and Np units. The reasons for the different mobility in IIG-based polymers are studied by analyzing the energy structure by absorption spectra, calculating transport levels by density functional theory, investigating the in-and out-of-plane crystallinity of thin film by grazing-incidence wideangle X-ray scattering, and extracting key transport parameters via lowtemperature measurements. By combining theoretical, optical, electrical, and structural analyses, this study finds that the large difference in OFET mobility mainly originates from the transport disorders determined by the different microcrystal structure, rather than the intrinsic transport properties in isolated chains for different polymers. bithiophene (BT), and thiophene-vinylene-thiophene (TVT). These three groups are selected because they are of the similar size and thus should give similar contribution to electron density to the semiconducting polymers, simplifying the comparative study. In addition, these groups have been widely adapted in synthesizing D-A semiconducting polymers. PIIG-Np, PIIG-BT, and PIIG-TVT polymers were synthesized by Pd-catalyzed Suzuki (PIIG-Np) and Stille (PIIG-BT and PIIG-TVT) cross-coupling according to the literature [5a,6,8] and applied in the active layer of top-gate and bottom-contact (TG/BC) OFETs with poly(methyl methacrylate) (PMMA) or CYTOP as a gate dielectric layer.All OFETs showed stable p-type transistor characteristics, but a huge mobility difference was observed among polymers with different donor units. Though the BT unit has less planarity than the Np and TVT units and is not considered the best partner for charge transport, PIIG-BT OFETs showed 50 times higher hole mobility (0.63 cm 2 V −1 s −1 ) than PIIG-TVT and PIIG-Np ones of ≈ 0.01 cm 2 V −1 s −1 (with CYTOP dielectric). The reasons for the structure-property relationship are studied here by a combination of various analyses: (i) Analyzing energy structure by absorption spectra; (ii) calculating transport levels by density functional theory (DFT); (iii) investigating the inand out-of-plane crystallinity of thin film by grazing-incidence wide-angle X-ray scattering (GIWAXS); and (iv) extracting key transport parameters via low-temperature measurements. The large difference in OFET mobility mainly originates from the transport disorders determined by the different microcrystal structure, rather than the intrinsic transport properties in isolated chains for different polymers. In particular, PIIG-BT polymer exhibits a special crystal structure and the highest crystalline degree, which apparently benefits the charge transport occurring in both in-plane and out-of-plane directions.