{"title":"Charge transfer in conducting polymers. Striving toward intrinsic properties","authors":"A. Heeger","doi":"10.1039/DC9898800203","DOIUrl":null,"url":null,"abstract":"A principal goal of the field of conducting polymers is to strive for advances in materials quality that will enable the exploration of the intrinsic electrical properties. In this context, we summarize the requirements for achieving high performance conducting polymers with electrical conductivities greater than that of copper. To avoid localization onto one-dimensioal polymer chains (with bandwidth 4t0), interchain charge transfer (t3d) is required. For crystalline materials in which the chains have precise phase order, the mean distance along the chain between defects must be L/acrystalline≫t0/t3d. In the case where there is good chain extension and good chain alignment, but when that alignment is nematic (i.e. with random interchain phase along the chain), the criterion is more severe: L/anematic≫(t0/t3d)2. When the appropriate inequality is satisfied the transport is that of an anisotropic three-dimensional metal, and the conductivity will increase in proportion to the mean distance between chain interruptions, cross-links, sp3 defects etc. If the mean defect scattering time, τdef=(L/vF), becomes sufficiently long that phonon scattering limits the mean free path, then the conductivity takes on a metallic temperature dependence, and the system is in the clean and intrinsic transport limit.","PeriodicalId":12210,"journal":{"name":"Faraday Discussions of The Chemical Society","volume":"17 1","pages":"203-211"},"PeriodicalIF":0.0000,"publicationDate":"1989-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"57","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Faraday Discussions of The Chemical Society","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1039/DC9898800203","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 57
Abstract
A principal goal of the field of conducting polymers is to strive for advances in materials quality that will enable the exploration of the intrinsic electrical properties. In this context, we summarize the requirements for achieving high performance conducting polymers with electrical conductivities greater than that of copper. To avoid localization onto one-dimensioal polymer chains (with bandwidth 4t0), interchain charge transfer (t3d) is required. For crystalline materials in which the chains have precise phase order, the mean distance along the chain between defects must be L/acrystalline≫t0/t3d. In the case where there is good chain extension and good chain alignment, but when that alignment is nematic (i.e. with random interchain phase along the chain), the criterion is more severe: L/anematic≫(t0/t3d)2. When the appropriate inequality is satisfied the transport is that of an anisotropic three-dimensional metal, and the conductivity will increase in proportion to the mean distance between chain interruptions, cross-links, sp3 defects etc. If the mean defect scattering time, τdef=(L/vF), becomes sufficiently long that phonon scattering limits the mean free path, then the conductivity takes on a metallic temperature dependence, and the system is in the clean and intrinsic transport limit.