Optically active polymers represent a class of materials of importance because of their unique properties and potential application as chiral chromatographic stationary phases, as supports for or ligands in asymmetric catalysts, and as components in nonlinear optical and liquid-crystalline materials. However, vinyl and related polymers that are optically active as a result of the configuration of their main chains, rather than chiral side-chain substituents, are very rare as this requires very special stereoregular symmetries of consecutive repeat units.In general, symmetry operations are more difficult to recognize in a long polymer chain made up of uniformly repeating units than in low-molecular-weight compounds. Wulff, however, recognized that only one specific sequence of eight possible hexad sequences of a homopolymer of a monosubstituted vinyl monomer is chiral.[1] Not surprisingly it is extremely difficult to control a vinyl polymerization to introduce such a chiral hexad sequence in a polymer backbone. One of the methods proposed by Wulff to reduce this difficulty was to introduce a second repeat unit in the polymer backbone to help break down the overall symmetry. For such copolymers, triad sequences (Figure 1) in which a syndiotactic