Electroactive organic polymers are not only attractive from the viewpoint of their solid-state propertiesÐlike electrical conduction or electrochromism [1] Ðbut also as promising candidates in molecular electronics, [2] including as switches for information storage, an area dominated by smaller molecules.[3±5] While photochemically induced switching in polymers has received much attention, [6] other external stimuli like thermal treatment, [7] chemical or redox interactions, [8] and their combination to make multifunctional polymers [9] are also attractive. Motivated by this promise, one of our objectives is the preparation of chiral redox-polymer systems.[10]Tetrathiafulvalene (TTF) derivatives are good candidates as components of these polymers because of their reversible and tunable redox properties. [11,12] They show two reversible one-electron oxidation processes to form the cation radical and the dication. As a scaffold for these units we chose the poly(isocyanide)s, [13] which can assume chiral conformations and organize electroactive groups. [8,12,14] This manuscript describes a chiral TTF-substituted poly(isocyanide) [15] that shows reversible interconversion between three univalent and two very broad mixed-valence redox states ( Fig. 1) that have different chiroptical properties, behavior that is not shown by the monomer. The TTF derivative, 2 (Scheme 1), bearing a phenyl isocyanide group and two stereogenic centers to induce diastereoselectivity in the polymerization, acts as our monomer. Long alkyl chains are present to ensure the solubility of the resulting polymer. The synthesis of 2 was performed following a multistep synthetic route, [16] the last step of which is the conversion of the formamide 1 to the isocyanide 2 by dehydration with diphosgene. Treatment of 2 with NiCl 2´6 H 2 O as a catalyst in CH 2 Cl 2 gave poly(isocyanide) 3 in 85 % yield (Scheme 1). The conversion of the monomer into the polymer was confirmed analytically.The IR spectrum of 3 showed a broad band from the imine groups attached to the polymer backbone at approximately 1642 cm ±1 and no signal corresponding to the isocyanide moi-