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616                                                    Carraher’s Polymer Chemistry








                                                     Doped


                                            C +             C            C              CH +










                        HC               C +                    C              C +











                                             C +                      C +


                 FIGURE 19.2  Poly-p-phenylene resonance structures after doping.
                    A critical structural feature for conductive polymers is the presence of conjugated double bonds.
                 For polyacetylene, every backbone carbon is connected by a stronger localized sigma bond. They
                 are also connected by a network of alternating less localized and weaker pi bonds. While conjuga-
                 tion is present, it is localized enough to prevent ready delocalization of the pi-bond electrons. The

                 dopants cause the introduction of sites of increased or deficiency of electrons (Figure 19.2). When
                 there is a deficiency of electrons, or holes, created electrons flow to fill this hole with the newly cre-



                 ated hole causing other electrons to fl ow to fill the new hole, and so on allowing charge to migrate

                 within and between the polyacetylene chains.
                    In general, the Huckel theory predicts that pi electrons can be delocalized over an entire chain
                 containing adjacent pi bonds with the activation energy for delocalization decreasing as the chain
                 length increases. The basic mechanism of electrical conductance is often explained in terms of the
                 band theory borrowed from more classical semiconductors. As noted before, for essentially all con-
                 ductive polymers, pi bonds are critical for conductance with the overlapping of pi clouds, allowing
                 conductivity of the electric current to occur. Highly delocalized electronic structures with conju-
                 gated pi electrons along the backbones are the norm for good conductivity. The ionization potential
                 to move from the valence band to the conduction band should be small.
                    Doping provides a ready mechanism for delocalization to occur. Doping is the mode of creat-

                 ing electron sinks or deficiencies and electron excesses that are necessary to breach, or get to, the
                 conductive band. The list of often used oxidant dopants includes I  (probably the most widely used
                                                                      2
                                                                                             −
                 because of the ease of using it), AsF , AlCl , Br , and O . Anionic counterions include Sb F , I ,
                                                                                                3
                                                                2
                                                         2
                                                                                           2 11
                                               5
                                                     3
                 and AsF . These dopants create defects that can be viewed as either a radical cation for oxidation
                        −
                        6
                 dopants (the doping agents acting to remove electrons), or radical anion for reduction doping (the
                 doping agents acting to increase the number of electrons). This is referred to as polaron with the
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