2017
DOI: 10.1002/polb.24530
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Charge transport and structure in semimetallic polymers

Abstract: Owing to changes in their chemistry and structure, polymers can be fabricated to demonstrate vastly different electrical conductivities over many orders of magnitude. At the high end of conductivity is the class of conducting polymers, which are ideal candidates for many applications in low‐cost electronics. Here, we report the influence of the nature of the doping anion at high doping levels within the semi‐metallic conducting polymer poly(3,4‐ethylenedioxythiophene) (PEDOT) on its electronic transport proper… Show more

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Cited by 64 publications
(82 citation statements)
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“…The different PEDOT:Tos morphologies studied in this work were generated by molecular dynamics simulations (MD) following the methodology developed in previous works [42][43][44]. The initial systems are mixtures of positively charged PEDOT oligomers, Tosylate anions and water molecules; the system has a neutral charge when the total positive charge carried by the PEDOT oligomers exactly compensate the Tosylate anionic charge.…”
Section: A From Morphology To Resistive Networkmentioning
confidence: 99%
“…The different PEDOT:Tos morphologies studied in this work were generated by molecular dynamics simulations (MD) following the methodology developed in previous works [42][43][44]. The initial systems are mixtures of positively charged PEDOT oligomers, Tosylate anions and water molecules; the system has a neutral charge when the total positive charge carried by the PEDOT oligomers exactly compensate the Tosylate anionic charge.…”
Section: A From Morphology To Resistive Networkmentioning
confidence: 99%
“…[28][29][30] Recent All Atomistic (AA) Molecular Dynamics (MD) calculations for PEDOT doped with different molecular counterions (including Tos) reveal a complex morphology where small crystallites consisting of several p-p stacking PEDOT chains are embedded in a polymer matrix including PEDOT chains, Tos counterions and water molecules. 16,31 Because of computational limitations, AA MD simulations do not always allow one to reach a lengthscale needed to study the morphology of a realistic material. For example, a formation of PEDOT-rich and PSS-rich phases in PEDOT:PSS that happens on the scale of B20-30 nm 32 is beyond the reach of AA MD.…”
Section: Introductionmentioning
confidence: 99%
“…We thus observe the same speed increase if the cells are in a CP environment in a redox state. Moreover, vapor‐phase polymerized PEDOT:TOS CP is known to have a bulk conductivity as high as 100–1000 S cm −1 . In our case, the bulk conductivity of the PEDOT:PSS microstripes is decreased by one order of magnitude after plasma oxygen processing.…”
Section: Resultsmentioning
confidence: 58%