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Organic Light Emitting Diodes

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This break leads to a free radical defect, a so-called neutral soliton which is relatively stable<br />

(Figure 9). Addition of an acceptor removes an electron and creates a positive soliton (or a neutral one<br />

if the electron removed is not the free electron). The resulting carbocation is stabilised by having the<br />

charge spread over several monomer units and the charged solitons are responsible for making<br />

polyacetylene a conductor<br />

Figure 9: Charge defects in polyacetylene and oxidative doping.<br />

A further type of charge storage occurs when the generated charge and the radical are coupled to<br />

each other via local resonance of the charge and the radical. This type of charge transport is present in<br />

polymers like PPV. This combination of a charge site and a radical dependent of each other is called a<br />

polaron. A new localised electronic state is created in the band gap, with the lower energy states being<br />

occupied by a single unpaired electron. Unlike the soliton, the polaron cannot move without first<br />

overcoming an energy barrier so movement is by a hopping motion.<br />

FIGURE 10: Radical cation (”polaron”) formed by removal of one electron on the 5th carbon<br />

atom of a undecahexaene chain (a ―> b). The polaron migration shown in c ―> e.<br />

If a second electron is removed from an already oxidised section of the polymer, either a second<br />

independent polaron may be created or, if it is the unpaired electron of the first polaron that is<br />

removed, a bipolaron is formed (with lower energy than 2 polarons) (Figure 11). The two positive<br />

charges of the bipolaron are not independent, but move as a pair, like the Cooper pair in the theory of<br />

superconductivity. While a polaron, being a radical cation, has a spin of 1/2, the spins of the<br />

bipolarons sum to S = 0.<br />

8

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