A new solution processable, regioregular, alternate copolymer of fluorenone and dialkylbithiophene, namely poly[(5,5‘-(3,3‘-di- n -octyl-2,2‘-bithiophene))- alt -(2,7-fluoren-9-one)] (abbreviated as PDOBTF), was synthesized by three different preparation methods: chemical or electrochemical oxidation of 2,7-bis(4-octylthien-2-yl)-fluoren-9-one or polycondensation of 2,7-bis(5-bromo-4-octylthien-2-yl)-fluoren-9-one in the presence of Ni(0) reagent. Independent of the preparation method, the crude product is a mixture of high molecular weight fractions and short oligomers. It can be however easily fractionated into fractions differing in their molecular weight by sequential extractions with a series of solvents. The principal absorption band registered for the undoped polymer (λ max = 384 nm for the THF solution and 389 nm for the solid state) originates from the π−π* transition of the conjugated backbone and is blue-shifted because of the chain torsion effects caused by steric hindrance. This band is accompanied by a peak of smaller intensity (λ max = 476 nm for the THF solution and 485 nm for the solid state) attributed to the n−π* transition in the carbonyl group of the fluoren-9-one subunit. Preliminary photoluminescence studies show that PDOBTF exhibits a very large Stokes shift and emits red light (λ max = 631 nm in THF solution and 643 nm in the solid state). Upon chemical p-type doping with FeCl 4 -, the polymer reaches the conductivity of σ dc = 0.05 S cm -1 . Mössbauer spectroscopy studies of the doping process show that both structural subunits, i.e., the bithiophene subunit and the fluoren-9-one one, participate in the doping. PDOBTF can be relatively easily postfunctionalized by grafting aniline oligomers as pendant groups via the carbonyl groups of the fluoren-9-one subunit. By consequence, the spectrum of the modified polymer can be precisely tuned in the visible region by changing the grafting level.
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Demadrille et al. (2003) studied this question.
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