Electro-optical properties of electropolymerized poly(3-hexylthiophene)/carbon nanotube composite thin films

✍ Scribed by Romesh J. Patel; Timothy B. Tighe; Ilia N. Ivanov; Michael A. Hickner

• Publisher: John Wiley and Sons
• Year: 2011
• Tongue: English
• Weight: 511 KB
• Volume: 49
• Category: Article
• ISSN: 0887-6266
• DOI: 10.1002/polb.22307

✦ Synopsis

Abstract

3‐hexylthiophene was electropolymerized on a carbon nanotube (CNT)‐laden fluorine‐doped tin oxide substrate. Scanning electron microscopy and Raman spectroscopy revealed that the polymer was infused throughout the thickness of the 150‐nm thick CNT mat, resulting in a conducting composite film with a dense CNT network. The electropolymerized poly(3‐hexylthiophene) (e‐P3HT)/CNT composites exhibited photoluminescence intensity quenching by as much as 92% compared to the neat e‐P3HT, which provided evidence of charge transfer from the polymer phase to the CNT phase. Through‐film impedance and J‐V measurements of the composites gave a conductivity (σ) of 1.2 × 10^−10^ S cm^−1^ and zero‐field mobility (μ~0~) of 8.5 × 10^−4^ cm^2^ V^−1^ s^−1^, both of which were higher than those of neat e‐P3HT films (σ = 9.9 × 10^−12^ S cm^−1^, μ~0~ = 3 × 10^−5^ cm^2^ V^−1^ s^−1^). In electropolymerized samples, the thiophene rings were oriented in the (010) direction (thiophene rings parallel to substrate), which resulted in a broader optical absorbance than for spin coated samples, however, the lack of long‐range conjugation caused a blueshift in the absorbance maximum from 523 nm for unannealed regioregular P3HT (rr‐P3HT) to 470 nm for e‐P3HT. Raman spectroscopy revealed that π‐π stacking in e‐P3HT was comparable to that in rr‐P3HT and significantly higher than in regiorandom P3HT (ran‐P3HT) as shown by the principal Raman peak shift from 1444 to 1446 cm^−1^ for e‐P3HT and rr‐P3HT to 1473 cm^−1^ for ran‐P3HT. This work demonstrates that these polymer/CNT composites may have interesting properties for electro‐optical applications. © 2011 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 49: 1269–1275, 2011