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Electronic Structure and Properties of Poly- and Oligoazulenes
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    Electronic Structure and Properties of Poly- and Oligoazulenes
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    Department of Analytical Chemistry, Lund University, P.O. Box 124, SE-221 00 Lund, Sweden, Institut für Organische Chemie, Universität Regensburg, Universitätsstrasse 31, D-93053 Regensburg, Germany, and Institut für Organische Chemie, Julius-Maximilians-Universität Würzburg, Am Hubland, 97074 Würzburg, Germany
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    The Journal of Physical Chemistry C

    Cite this: J. Phys. Chem. C 2008, 112, 6, 2156–2164
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    https://doi.org/10.1021/jp074376b
    Published January 17, 2008
    Copyright © 2008 American Chemical Society

    Abstract

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    One of the most important research interests in the field of organic photovoltaic devices (OPVs) is the development of new materials which can serve as light-absorbing electron donors and hole-conducting (p-type) semiconductors. In this context, 1,3-polyazulenes were synthesized chemically and electrochemically. Their spectroscopic and electrochemical properties are compared with those of the 1,3-oligoazulenes Az1Az6. The UV−vis spectra of the neutral azulenes Az1Az6 show a linear correlation between the lowest absorption maximum and the inverse chain length 1/n leading to a band gap of Eg = 1.90 eV for infinite chain length. Derived from this correlation the effective conjugation length of chemically synthesized polyazulene is only about 10. By an alternative approach, a band gap of Eg = 1.46 eV was determined. Depending on the applied potential the oligomers Az2Az6 undergo up to two reversible oxidation processes or further polymerization which results in the formation of polymer films at the electrode. The potentiodynamic oxidation of chemically synthesized polyazulene leads to electrocrystallization at the electrode, whereas films of polyazulenes are obtained directly upon oxidation of Az1Az6. Chemically and electrochemically generated polyazulenes adsorbed on Pt show similar electrochemical behavior upon positive doping. The spectroelectrochemical investigations in combination with density functional theory (DFT) calculations lead to the conclusion that polyazulene can be oxidized up to a doping level of one charge per three or four azulene units. At this stage polarons or polaron pairs are formed (depending on the doping level) but not bipolarons. At higher doping levels the polymers start to decompose.

    Copyright © 2008 American Chemical Society

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     Corresponding author. Phone:  +46 46 222 0103. Fax:  +46 46 222 4544. E-mail:  [email protected].

     Lund University.

     Universität Regensburg.

    §

     Julius-Maximilians-Universität Würzburg.

    Supporting Information Available

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    The experimental part (details about synthesis, electrochemical setup, and DFT calculations), additional CV experiments (comparison between azulene and chemically and electrochemically synthesized polyazulene), the spectroelectrochemistry of films of PAz2 and PAz3 in monomer-free solution, and the bond distances and dihedral angles for neutral Az8. This material is available free of charge via the Internet at http://pubs.acs.org.

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    This article is cited by 27 publications.

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    The Journal of Physical Chemistry C

    Cite this: J. Phys. Chem. C 2008, 112, 6, 2156–2164
    Click to copy citationCitation copied!
    https://doi.org/10.1021/jp074376b
    Published January 17, 2008
    Copyright © 2008 American Chemical Society

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