J. Simitzis et al., EFFECT OF DOPING SYSTEMS, HEAT, AND TIME ON THE ELECTRICAL-CONDUCTIVITY OF POLY-P-PHENYLENES, New polymeric materials, 5(1), 1996, pp. 81-91
Poly-p-phenylenes (PPPs) were synthesized by the Kovacic procedure usi
ng CuCl2 as the oxidant and AlCl3 as the catalyst. The alternating ele
ctrical conductivity of PPPs was investigated considering the doping s
ystem (dopant-solvent), heat treatment, and time. Doped poly-p-phenyle
nes remained semiconductors even 1 year after doping with a lower cond
uctivity compared to the initial one. The most effective doping system
s for PPPs were FeCl3-ACN (ACN: acetonitrile) and FeCl3-N (N: nitroben
zene), while SnCl4-ACN yielded material with a lower but comparable co
nductivity. FTIR spectra and X-ray diffractograms of doped materials h
aving a lower conductivity (i.e. PPP doped with SnCl4-ACN) approached
that of the undoped PPP. The conductivity depends on the stability of
the polymer-dopant complex, which is affected by the electron donor-ac
ceptor (EDA) interactions between the dopant and the solvent. Annealin
g after doping resulted in a decrease in conductivity, due to the ther
mal deactivation of the polymer-dopant complex. The ratio of sigma'(ta
u)/sigma'(0) (where sigma'(tau) and sigma'(0) are the real part of the
electrical conductivity at log f = 7 and log f = 1, respectively) ran
ges from 10(1) for the doped polymers at a time of t = 0 to 10(1)-10(2
) at t = 12 months, and to 10(4) for the heat-treated doped polymers.
The conductivity measurements suggested an indirect method to characte
rize the stability of the complexes formed.