Pm. Borsenberger et al., ELECTRON-TRANSPORT IN -BUTYL-9,10-N,N'-DICYANOANTHRAQUINONEDIIMINE-DOPED POLYMERS, Journal of imaging science and technology, 39(1), 1995, pp. 6-12
Electron mobilities have been measured in 2-t-butyl-9,10-N,N,N'-dicyan
oanthraquinonediimine (DCAQ)-doped bisphenol-A-polycarbonate and poly(
styrene) over a range of fields, temperatures, and DCAQ concentrations
. The results agree with predictions of a model based on disorder, acc
ording to Bassler and coworkers. The model is premised on the assumpti
on that charge transport occurs by hopping through a manifold of local
ized states with superimposed energetic and positional disorder. The k
ey parameters of the model are the energy width of the hopping site ma
nifold, the degree of positional disorder, and a prefactor mobility. D
escribing the results by the disorder model leads to the conclusion th
at the width of the hopping site manifold is 0.136 eV and independent
of both the host polymer and DCAQ concentration. The width comprises a
dipolar component of 0.085 eV and a van der Waals component of 0.106
eV. Agreement with experimental requires that the dipolar effect be pu
rely intramolecular and the van der Waals component be independent of
both the DCAQ concentration and the host polymer. The degree of positi
onal disorder is between 3.0 and 4.2, increasing with decreasing DCAQ
concentration, and is independent of the polymer. The prefactor mobili
ties are between 10(-3) and 10(-9) cm(2)/Vsec and can be described by
wavefunction decay constants of approximately 1 Angstrom that are also
independent of the polymer.