Variable-range-hopping exponents 1/2, 2/5 and 1/4 in HCl-doped polyaniline pellets
We study the variable-range-hopping (VRH) charge transport in polyaniline pellets doped with HCl over a wide range. Increase of the doping not only enhances the electrical conductivity σ but also weakens the disorder, which affects the VRH mechanism. This is revealed in the σ vs temperature ( T) cha...
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Veröffentlicht in: | Synthetic metals 2009-04, Vol.159 (7), p.649-653 |
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Sprache: | eng |
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Zusammenfassung: | We study the variable-range-hopping (VRH) charge transport in polyaniline pellets doped with HCl over a wide range. Increase of the doping not only enhances the electrical conductivity
σ
but also weakens the disorder, which affects the VRH mechanism. This is revealed in the
σ
vs temperature (
T) characteristics
σ
∝
exp
[
−
(
T
0
/
T
)
α
]
, where
α
and
T
0
carry information on the underlying physics. Below
∼
200
K,
α
undergoes a significant disorder dependent change at
∼
60% of the full doping:
α
=
1
/
2
for lower doping, whereas more-doped samples exhibit
α
=
2
/
5
. From
∼
200
K up to room temperature, most of the samples (i.e., those doped below 80%) exhibit
α
=
1
/
4
regardless of the corresponding
α
at low
T. These results can be to a large extent explained by the VRH theory of Fogler et al. [M.M. Fogler, S. Teber, B.I. Shklovskii, Phys. Rev. B 69 (2004) 035413] (FTS). In particular,
α
=
1
/
2
,
2
/
5
,
1
/
4
are therein anticipated for three-dimensional transport together with crossovers between these values in response to changes in disorder and/or
T. The doping (disorder) dependence of
T
0
for a given
α
=
1
/
2
or
2
/
5
also follows the FTS predictions reasonably well. The appearance of
α
=
1
/
4
at high
T can be understood from an analysis of energy scales that are relevant to VRH as described by the FTS model. |
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ISSN: | 0379-6779 1879-3290 |
DOI: | 10.1016/j.synthmet.2008.12.010 |