Appl. Phys. Lett. 97, 033308 (2010); http://dx.doi.org/10.1063/1.3466916 (3 pages)
Terahertz complex conductivities of carriers with partial localization in doped polythiophenes
(Received 27 April 2010; accepted 27 June 2010; published online 21 July 2010)
(ω) of two p-doped polythiophenes—poly(3-hexylthiophene) and poly(3,4-ethylenedioxythiophene)—with various carrier densities by using terahertz time-domain spectroscopy. The real part of
(ω) is found to gradually decrease with decreasing frequency ω and to approach a finite value for ω→0 unlike the Drude conductivity behavior, suggesting that carriers in polythiophenes have a partially localized nature. By reproducing both the measured real and imaginary parts of
(ω) with the Drude–Smith model, we show that carriers become less localized with increasing carrier density up to ∼ 1.8×1020 cm−3.© 2010 American Institute of Physics
RELATED DATABASES
KEYWORDS and PACS
ARTICLE DATA
- L. B. Groenendaal, F. Jonas, D. Freitag, H. Pielartzik, and J. R. Reynolds, Adv. Mater. (Weinheim, Ger.) 12, 481 (2000).
- K. Lee, S. Cho, S. H. Park, A. J. Heeger, C. -W. Lee, and S. -H. Lee, Nature (London) 441, 65 (2006). [MEDLINE]
- T. -I. Jeon, D. Grischkowsky, A. K. Mukherjee, and R. Menon, Appl. Phys. Lett. 77, 2452 (2000)APPLAB000077000016002452000001. [ISI]
- E. Hendry, J. M. Schins, L. P. Candeias, L. D. A. Siebbeles, and M. Bonn, Phys. Rev. Lett. 92, 196601 (2004) [MEDLINE]
E. Hendry, M. Koeberg, J. M. Schins, H. K. Nienhuys, V. Sundström, L. D. A. Siebbeles, and M. Bonn, Phys. Rev. B 71, 125201 (2005). - X. Ai, M. C. Beard, K. P. Knutsen, S. E. Shaheen, G. Rumbles, and R. J. Ellingson, J. Phys. Chem. B 110, 25462 (2006).
- P. D. Cunningham and L. M. Hayden, J. Phys. Chem. C 112, 7928 (2008).
- P. Parkinson, J. Lloyd-Hughes, M. B. Johnston, and L. M. Herz, Phys. Rev. B 78, 115321 (2008).
- H. Němec, H. -K. Nienhuys, E. Perzon, F. Zhang, O. Inhanäs, P. Kužel, and V. Sundström, Phys. Rev. B 79, 245326 (2009).
- N. V. Smith, Phys. Rev. B 64, 155106 (2001).
- The chemicals were purchased from Sigma-Aldrich.
- Y. Furukawa, J. Phys. Chem. 100, 15644 (1996).
- The spectral shape of the broad peak can be reproduced by neither Lorentzian nor Gaussian function. The present estimation of the low-energy tail edge indicates that its contribution is negligible in the THz frequency range.
- K. Lee, R. Menon, C. O. Yoon, and A. J. Heeger, Phys. Rev. B 52, 4779 (1995). [Inspec]
- G. M. Turner, M. C. Beard, and C. A. Schmuttenmaer, J. Phys. Chem. B 106, 11716 (2002).
- J. B. Baxter and C. A. Schmuttenmaer, J. Phys. Chem. B 110, 25229 (2006).
- D. G. Cooke, A. N. MacDonald, A. Hryciw, J. Wang, Q. Li, A. Meldrum, and F. A. Hegmann, Phys. Rev. B 73, 193311 (2006).
- M. Walther, D. G. Cooke, C. Sherstan, M. Hajar, M. R. Freeman, and F. A. Hegmann, Phys. Rev. B 76, 125408 (2007). [ISI]
Figures (click on thumbnails to view enlargements)
FIG.1 Download High Resolution Image (.zip file) |
Export Figure to PowerPoint
FIG.2 Download High Resolution Image (.zip file) |
Export Figure to PowerPoint
(ω) of regioregular P3HT (circles) prepared with doping times of 30, 120, and 360 s. Also shown by curved lines are Drude–Smith conductivity fits to
(ω).
FIG.3 Download High Resolution Image (.zip file) |
Export Figure to PowerPoint
FIG.4 Download High Resolution Image (.zip file) |
Export Figure to PowerPoint















This Publication
Scitation
SPIN
Google Scholar
PubMed