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Volumn 19, Issue 9, 2007, Pages 1196-1200

Microscopic understanding of the anisotropic conductivity of PEDOT:PSS thin films

Author keywords

[No Author keywords available]

Indexed keywords

ATOMIC FORCE MICROSCOPY; ELECTRIC CONDUCTIVITY; MAGNETIC ANISOTROPY; SCANNING TUNNELING MICROSCOPY; SPIN COATING;

EID: 34250661692     PISSN: 09359648     EISSN: None     Source Type: Journal    
DOI: 10.1002/adma.200602575     Document Type: Article
Times cited : (501)

References (25)
  • 1
    • 34250678209 scopus 로고    scopus 로고
    • For a review on PEDOT see for example, a L. B. Groenendaal, F. Jonas, D. Freitag, H. Pielartzik, J. R. Reynolds, Adv. Mater. 2000, 12, 48l.
    • For a review on PEDOT see for example, a) L. B. Groenendaal, F. Jonas, D. Freitag, H. Pielartzik, J. R. Reynolds, Adv. Mater. 2000, 12, 48l.
  • 18
    • 34250683153 scopus 로고    scopus 로고
    • last accessed March 2007
    • H. C. Starck, http://www.baytron.com (last accessed March 2007).
    • Starck, H.C.1
  • 21
    • 34250689216 scopus 로고    scopus 로고
    • Unlike AFM, STM topography reflects a surface of equal conductivity, which, in low-conductivity materials, does not necessarily coincide with the sample surface. The current setpoint and bias used in this work, 10 pA and 2.3 V, respectively, were enough to penetrate the insulating PSS-rich surface layer, while maintaining stable imaging of the deeper, more conducting bulk layers. See S. Timpanaro et al. [16] for more details.
    • Unlike AFM, STM topography reflects a surface of equal conductivity, which, in low-conductivity materials, does not necessarily coincide with the sample surface. The current setpoint and bias used in this work, 10 pA and 2.3 V, respectively, were enough to penetrate the insulating PSS-rich surface layer, while maintaining stable imaging of the deeper, more conducting bulk layers. See S. Timpanaro et al. [16] for more details.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.