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Charge transport in amorphous low bandgap conjugated polymer/fullerene films

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dc.contributor.authorKim, Jung Yong-
dc.contributor.authorCho, Hyunduck-
dc.contributor.authorNoh, Seunguk-
dc.contributor.authorLee, Yoonkyoo-
dc.contributor.authorNam, Young Min-
dc.contributor.authorLee, Changhee-
dc.contributor.authorJo, Won Ho-
dc.date.accessioned2023-12-11T07:46:14Z-
dc.date.available2023-12-11T07:46:14Z-
dc.date.created2020-08-26-
dc.date.issued2012-02-
dc.identifier.citationJournal of Applied Physics, Vol.111 No.4, p. 043710-
dc.identifier.issn0021-8979-
dc.identifier.urihttps://hdl.handle.net/10371/198650-
dc.description.abstractThe structural and charge transport properties of a low bandgap copolymer poly(3-hexylthiophene-alt-6,7-dimethyl-4,9-bis-(4-hexylthien-2yl)-[1,2,5]thiadiazolo[3,4-g]quinoxaline) (P(3HT-MeTDQ)) and its blend with [6,6]-phenyl-C-61-butyric acid methyl ester (PCBM) are investigated. Thermal analysis, X-ray scattering diffraction (XRD), atomic force microscopy and transmission electron microscopy (TEM) of P(3HT-MeTDQ) reveal that the polymer is amorphous in solid state. As the hole mobility of P(3HT-MeTDQ) was measured by the time-of-flight photoconductivity method, the mobility was 3.35 x 10(-4) cm(2)/Vs, which is very comparable to that of semicrystalline poly(3-hexylthiophene). When the mobility of amorphous P(3HT-MeTDQ) was analyzed according to the Gaussian disorder model, the polymer has the energetic and positional disorders with the values of sigma = 62 meV and Sigma = 1.7, respectively, indicating that the polymer has a relatively narrow Gaussian distribution of transport states. Interestingly, when P(3HT-MeTDQ) is blended with PCBM, the amorphous P(3HT-MeTDQ) becomes partially ordered, as evidenced by observation of two discernible XRD peaks at 20 = 5 degrees (d = 17.7 angstrom) and 25.5 degrees (d = 3.5 angstrom) corresponding to the interchain distance and pi-stacking distance, respectively. The bicontinuous network morphology was identified at the blend with 60 wt.% PCBM by TEM, at which the charge carrier transport changes from hole-only to ambipolar. (C) 2012 American Institute of Physics. [doi:10.1063/1.3686633]-
dc.language영어-
dc.publisherAmerican Institute of Physics-
dc.titleCharge transport in amorphous low bandgap conjugated polymer/fullerene films-
dc.typeArticle-
dc.identifier.doi10.1063/1.3686633-
dc.citation.journaltitleJournal of Applied Physics-
dc.identifier.wosid000300948600048-
dc.identifier.scopusid2-s2.0-84863275894-
dc.citation.number4-
dc.citation.startpage043710-
dc.citation.volume111-
dc.description.isOpenAccessN-
dc.contributor.affiliatedAuthorLee, Changhee-
dc.contributor.affiliatedAuthorJo, Won Ho-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.subject.keywordPlusHETEROJUNCTION SOLAR-CELLS-
dc.subject.keywordPlusFIELD-EFFECT TRANSISTORS-
dc.subject.keywordPlusPOLYMER-FULLERENE BLENDS-
dc.subject.keywordPlusHIGH-PERFORMANCE-
dc.subject.keywordPlusPHOTOVOLTAIC CELLS-
dc.subject.keywordPlusMOBILITY-
dc.subject.keywordPlusDERIVATIVES-
dc.subject.keywordPlusINSULATORS-
dc.subject.keywordPlusENERGY-
dc.subject.keywordPlusSEMICONDUCTORS-
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