Polarons conjugated polymers

For spin-1/2 excitations such as electrons and holes in normal semiconductors or polarons in conjugated polymers, a single resonance is found centered at the Field... 

We have studied the temporal dynamics of CPG in m-LPPP by performing field-assisted pump-probe experiments on LED structures, as described in Section 8.3.2. The narrow line-width PA assigned to polarons (see Section 8.5.2) is a fingerprint of charge generation in m-LPPP. Monitoring the dynamics of these PA band enables us, for the first time, to directly observe the CPG dynamics in a conjugated polymer with sub-picosecond time resolution [40],... 

The electrical conductivity in the solid state is determined by the product of the carrier concentration and the carrier mobility. In conjugated polymers both entities are material dependent and, i.e., are different for electrons and holes. Electrons or holes placed on a conjugated polymer lead to a relaxation of the surrounding lattice, forming so-called polarons which can be positive or negative. Therefore, the conductivity, o, is the sum of both the conductivity of positive (P+) and negative polarons (P ) ... 

EL), conjugated polymers are also of interest as materials for optically or electrically pumped stimulated emission. For effects of this type, the ratio of stimulated emission to photoinduced absorption (PA) is of particular interest for conjugated polymers. In this context, the orign of the PA is controversial the PA can be a result of the formation of either charge-separated polaron pair -states or excimers. Initial experiments support the conjecture that LPPP 26 is significantly superior [49], as the stimulated emission of LPPP 26 is markedly more intense than that of PPV under comparable conditions. 

W Wohlgenannt, XM Jiang, C Yang, OJ Korovyanko, and ZV Vardeny, Spin-dependent polaron pair recombination in TT-conjugated polymers enhanced singlet exciton densities, Synth. Met., 139 921-924, 2003. 

As we will see in Section 5, it is not a straightforward matter to obtain conjugated polymers with a high content of pendent radicals either chemical introduction of radicals into polymers is inefficient or radical centres cannot be kept intact during polymerization. A possible way out of this problem has been proposed by Fukutome, namely, doping of closed-shell cross-conjugated polymers to generate the open-shell centres. The polaronic interaction in these systems has been discussed (Fukutome et al., 1987). 

The polaronic strategy has also been applied to polymers, incorporating m-phenylene units as coupling links in n-conjugated polymer chains of polyfthienylene ketone) (Dal Colle et al. 1999) as well as of polyarylamine, polyacetylene, and polythiophene (Kaisaki et al. 1991, Murray et al. 1994, Bushby et al. 1997a). Scheme 1.44 represents these polaronic polymers. 

Radical cations and dications of oligothiophenes have been investigated by many research groups to understand the nature of polarons and bipolarons in polythiophenes which are responsible for the electrical and optical properties of these re-conjugated polymers. 

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