Ions transport and self-doping in layer-by-layer conducting polymer films
The self-doping mechanism for charge transport is investigated in layer-by-layer (LBL) films from two conducting polymers, namely poly( o-methoxyaniline) (POMA) and poly(3-thiophene acetic acid) (PTAA). The efficiency of charge intercalation, defined as the ratio between the charge and the mass chan...
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Veröffentlicht in: | Synthetic metals 2005-12, Vol.155 (3), p.648-651 |
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Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
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Zusammenfassung: | The self-doping mechanism for charge transport is investigated in layer-by-layer (LBL) films from two conducting polymers, namely poly(
o-methoxyaniline) (POMA) and poly(3-thiophene acetic acid) (PTAA). The efficiency of charge intercalation, defined as the ratio between the charge and the mass change, is twice for the POMA/PTAA LBL film in comparison with a cast POMA film. This is attributed to differences in the diffusion-controlled charge and mass transport, where distinct ionic species participate in the LBL films, as demonstrated with experiments using a quartz crystal microbalance. The doping efficiency for LBL film is the same, i.e., 3.93
×
10
−4 and 3.56
×
10
−4
g/C for the Li
+ and (C
2H
5)
4N
+ doped films, and is different for the cast POMA film, i.e., 11.3
×
10
−4 for Li
+ and 6.45
×
10
−4
g/C for (C
2H
5)
4N
+. Therefore, once no significant differences in the intercalation mechanism are observed when different cations, Li
+ or (C
2H
5)
4N
+, are used with the LBL films, this indicates that the self-doping mechanism is controlled by the exchange of anions. |
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ISSN: | 0379-6779 1879-3290 |
DOI: | 10.1016/j.synthmet.2005.08.021 |