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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.creator조원호-
dc.date.accessioned2013-01-25T01:57:12Z-
dc.date.available2013-01-25T01:57:12Z-
dc.date.issued2012-02-
dc.identifier.citationJOURNAL OF APPLIED PHYSICS Vol.111 No.4, 043710-
dc.identifier.issn0021-8979-
dc.identifier.urihttps://hdl.handle.net/10371/81080-
dc.descriptionCopyright (2012) American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics.-
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]en
dc.language.isoenen
dc.publisherAMER INST PHYSICSen
dc.subject공학en
dc.titleCharge transport in amorphous low bandgap conjugated polymer/fullerene filmsen
dc.typeArticle-
dc.contributor.AlternativeAuthor김정용-
dc.contributor.AlternativeAuthor조현덕-
dc.contributor.AlternativeAuthor노승욱-
dc.contributor.AlternativeAuthor이윤규-
dc.contributor.AlternativeAuthor남영민-
dc.contributor.AlternativeAuthor이창희-
dc.contributor.AlternativeAuthor조원호-
dc.identifier.doi10.1063/1.3686633-
dc.description.srndOAIID:oai:osos.snu.ac.kr:snu2012-01/102/0000001236/2-
dc.description.srndSEQ:2-
dc.description.srndPERF_CD:SNU2012-01-
dc.description.srndEVAL_ITEM_CD:102-
dc.description.srndUSER_ID:0000001236-
dc.description.srndADJUST_YN:Y-
dc.description.srndEMP_ID:A004558-
dc.description.srndDEPT_CD:445-
dc.description.srndCITE_RATE:2.168-
dc.description.srndFILENAME:2. Charge Transport in Amorphous.pdf-
dc.description.srndDEPT_NM:재료공학부-
dc.description.srndEMAIL:whjpoly@snu.ac.kr-
dc.description.srndSCOPUS_YN:Y-
dc.description.srndCONFIRM:Y-
dc.identifier.srnd2012-01/102/0000001236/2-
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