Near-infrared photoluminescence from undoped trans-polyacetylene was attributed to emission from ``cis defects,'' structures composed of isolated cis-(-CH?CH-) bonds embedded within conjugated trans-(CH)ₓ segments. Spectra were found to be independent of residual transition-metal impurities in the polymer, but quantum efficiencies decreased with increasing concentrations of neutral defects and free carriers. The percolation limit for free carriers was achieved at about 30% overall trans-(CH)ₓ. The photoluminescence energy varied inversely with the length of the conjugated cis defects, with a different dependence than for polyenes in solution. Interchain interactions were found to be significant in the solid state, distorting bonding geometries and perturbing the electronic structure of the chains; we postulate they are essential for bulk conduction. H\"uckel calculations yielded β₀=1.08 eV for the {π} interaction energy, predicting an energy of 0.39--0.43 eV for the {π}-π* transition of a typical bound neutral soliton. The band gap for trans-polyacetylene of infinite conjugation length was estimated to be 1.20 eV by extrapolation of the solid-state luminescence data. We conclude that thermally isomerized trans-polyacetylene is best described as being a three-dimensional ensemble of short, conjugated segments that are bounded and interconnected by defects and crosslinks. Mean segment lengths are probably less than 13 (-CH?CH-) units.
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Carter et al. (1991) studied this question.
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