Quasi-One Dimensional in-Plane Conductivity in Filamentary Films of PEDOT:PSS

被引:36
|
作者
van de Ruit, Kevin [1 ]
Cohen, Racheli Itzhak [2 ]
Bollen, Dirk [3 ]
van Mol, Ton [4 ]
Yerushalmi-Rozen, Rachel [2 ,5 ]
Janssen, Rene A. J. [1 ]
Kemerink, Martijn [1 ]
机构
[1] Eindhoven Univ Technol, Dept Appl Phys, NL-5600 MB Eindhoven, Netherlands
[2] Ben Gurion Univ Negev, Dept Chem Engn, IL-84105 Beer Sheva, Israel
[3] Agfa Gevaert NV, B-2640 Mortsel, Belgium
[4] Holst Ctr TNO, NL-5656 AE Eindhoven, Netherlands
[5] Ben Gurion Univ Negev, Ilze Kats Inst Nanoscale Sci & Technol, IL-84105 Beer Sheva, Israel
关键词
charge transport; conducting polymers; organic electronics; PSS THIN-FILMS; TRANSPORT-PROPERTIES; ELECTRICAL-CONDUCTIVITY; POLYMER BLENDS; POLY(3,4-ETHYLENEDIOXYTHIOPHENE)/POLY(STYRENESULFONATE); ENHANCEMENT; PERFORMANCE; NANOWIRES; MODEL;
D O I
10.1002/adfm.201301174
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
The mechanism and magnitude of the in-plane conductivity of poly(3,4-ethylenedioxythiophene): poly(styrenesulfonate) (PEDOT: PSS) thin fi lms is determined using temperature dependent conductivity measurements for various PEDOT: PSS weight ratios with and without a high boiling solvent (HBS). Without the HBS the in-plane conductivity of PEDOT: PSS is lower and for all studied weight ratios well described by the relation s = s0exp[-T0 T 0.5] with T 0 a characteristic temperature. The exponent 0.5 indicates quasi-one dimensional (quasi-1D) variable range hopping (VRH). The conductivity prefactor s 0 varies over three orders of magnitudes and follows a power law s 0. c 3.5 PEDOT with c PEDOT the weight fraction of PEDOT in PEDOT: PSS. The fi eld dependent conductivity is consistent with quasi-1D VRH. Combined, these observations suggest that conductance takes place via a percolating network of quasi-1D fi laments. Using transmission electron microscopy (TEM) fi lamentary structures are observed in vitrifi ed dispersions and dried fi lms. For PEDOT: PSS fi lms with HBS, the conductivity also exhibits quasi-1D VRH behavior when the temperature is less than 200 K. The low characteristic temperature T 0 indicates that HBStreated fi lms are close to the critical regime between a metal and an insulator. In this case, the conductivity prefactor scales linearly with c PEDOT, indicating the conduction is no longer limited by a percolation of fi laments. The lack of observable changes in TEM upon processing with the HBS suggests that the changes in conductivity are due to a smaller spread in the conductivities of individual fi laments, or a higher probability for neighboring fi laments to be connected rather than being caused by major morphological modifi cation of the material.
引用
收藏
页码:5778 / 5786
页数:9
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