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Solvent processed conductive polymer with single-walled carbon nanotube composites

Published online by Cambridge University Press:  30 October 2015

Zhe Jia
Affiliation:
Energy Technologies Area, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
Hui Zhao
Affiliation:
Energy Technologies Area, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
Ying Bai
Affiliation:
Energy Technologies Area, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA; and School of Chemical Engineering & Environment, Beijing Institute of Technology, Beijing 100081, China
Ting Zhang
Affiliation:
School of Optoelectronics, Beijing Institute of Technology, Beijing 100081, China
Amanda S. Lupinacci
Affiliation:
Department of Materials Science and Engineering, University of California, Berkeley, Berkeley, California 94720, USA; and National Center for Electron Microscopy, Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
Andrew M. Minor
Affiliation:
Department of Materials Science and Engineering, University of California, Berkeley, Berkeley, California 94720, USA; and National Center for Electron Microscopy, Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
Gao Liu*
Affiliation:
Energy Technologies Area, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
*
a)Address all correspondence to this author. e-mail: gliu@lbl.gov

Abstract

Single-walled carbon nanotube (SWNT) and conductive polymer composite were studied as a potential electrode candidate for plastic electronic devices such as organic light-emitting diodes (OLEDs) and solar cells. A novel conductive polymer, poly(2,7–9,9(di(oxy-2,5,8-trioxadecane))fluorene) (PFO), was synthesized and characterized as a surfactant to disperse SWNTs in solutions. The ethylene oxide (EO) side chain of rigid PFO backbone acts as a template to wrap around SWNTs in solution. Up to 0.02% (by weight) of SWNTs are stabilized and well separated in the solution phase. The carbon nanotube can be dispersed in solutions for over 4 mo. Transmission electron microscopy (TEM) images of solvent cast film suggest highly uniformed SWNT distribution incorporated in the conductive polymer matrix. Transmittance characterization shows the film is as transparent as indium tin oxide conducting glass. Conductivity measurement shows SWNTs can effectively inject charges into the PFO polymer matrix at low voltage. The current versus voltage profile of the SWNT/PFO composite film (2% SWNT in PFO by weight) shows that the majority current conducting is carried by SWNTs.

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Articles
Copyright
Copyright © Materials Research Society 2015 
Figure 0

SCHEME 1. Chemical structure of PF (left) and PFO (right) conducting polymers as stabilization agents studied in this work.

Figure 1

SCHEME 2. Synthesis of poly(2,7–9,9-(di(oxy-2,5,8-trioxadecane))fluorene) (PFO) conducting polymer.

Figure 2

FIG. 1. Photos of SWNT dispersion in polymer solutions. (a) SWNT/PF/CB solution; (b) SWNT/PF/CF solution; (c) SWNT/PFO/CB solution; (d) SWNT/PFO/CF solution.

Figure 3

FIG. 2. SEM images. (a) SWNT/PFO film was cast using the upper layer solution of SWNT/PFO/CB [Fig. 1(c)]; (b) SWNT/PFO film was cast using upper layer solution of SWNT/PFO/CF [Fig. 1(d)]; (c) AP grade SWNT. (The scale bar is 100 nm for all images.)

Figure 4

FIG. 3. Selective aggregations of PFO in (a) CF, (b) CB, (c) PFO preferred wrapping of SWNT, (d) a hypothetical SWNT polymer micelle. (In the drawings, the blue lines represent rigid PFO backbones; the flexible red branches represent methyltriethyleneoxide side chains; and the tubes represent SWNTs).

Figure 5

FIG. 4. TEM images of (a) PFO associated SWNT show smooth coating on surface of SWNTs. (The scale bar is 20 nm.) (b) PF associated SWNTs show aggregation of polymer. (c) Individual tubes can be seen after the PFO leached out.

Figure 6

FIG. 5. TEM image of the PFO/SWNT composite film on holey carbon grid.

Figure 7

FIG. 6. Transmittance of the SWNT/PFO is equivalent to that of the ITO film. The major absorbance at 380 nm is due to the PFO polymer.

Figure 8

FIG. 7. Conductivity of the pure PFO and the 0.1% by weight SWNT PFO composite.

Figure 9

FIG. 8. Current versus voltage behavior of the ITO/PEDOT; PSS/PFO; SWNT/Al device. (a) Low current density; (b) high current density.