Nontraditional aromatic molecules hold tremendous promise for the design and realization of advanced materials for organic electronics applications. In this report, we describe recent work with the 10 π-electron methano[10]annulene molecule. We used chemistry established by Vogel and by Neidlein to incorporate this molecule into organic semiconducting polymers and found that they provide for highly delocalized charge carriers upon electrochemical oxidation/doping into conductive materials. Extensions to a variety of annulene-heteroaromatic copolymers will be described along with pertinent optical and electrical characterization data. Fig. 1 UV-vis spectra of (a) MT (solid) and NT (dashed) and (b) MBT (solid) and NBT (dashed), taken in chloroform at room temperature. Extinction coefficients (λ max , log ε): MT (284 nm, 4.52; 375 nm, 4.34), NT (315 nm, 4.27), MBT (257 nm, 4.52; 306 nm, 4.50; 416 nm, 4.57) and NBT (351 nm, 4.52).the reference electrode at the same scan rate. For a p-channel conductive polymer, a drain current (I D ) will flow between the two electrodes once the polymer has been oxidized into a conductive state. The magnitude of the current is directly proportional to the conductivity of the polymer. Therefore, plotting the graph of I D vs. V G gives relative conductivities at specific points of the polymer CV (Fig. 6). Poly(MT) was conductive between 0.50 and 0.90 V with its peak conductivity observed at 0.74 V. Fig. 10 Cyclic voltammograms (solid) and in situ conductivity profiles (dashed) of (a) poly(FMF) and (b) poly(FBF), taken on Au interdigitated electrodes with conditions as reported in Figs. 2 and 6.