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dc.contributor.authorYamamoto, Shunsukeen
dc.contributor.authorOhkita, Hideoen
dc.contributor.authorBenten, Hiroakien
dc.contributor.authorIto, Shinzaburoen
dc.contributor.alternative山本, 俊介ja
dc.contributor.alternative大北, 英生ja
dc.contributor.alternative辨天, 宏明ja
dc.contributor.alternative伊藤, 紳三郎ja
dc.date.accessioned2024-10-17T02:27:36Z-
dc.date.available2024-10-17T02:27:36Z-
dc.date.issued2012-07-24-
dc.identifier.urihttp://hdl.handle.net/2433/289911-
dc.description.abstractThe charge carrier dynamics in blend films of [6, 6]-phenyl-C₆₁-butyric acid methyl ester (PCBM) and conjugated polymers with different ionization potentials are measured using transient absorption spectroscopy to study the formation mechanism of PCBM radical cation, which was previously discovered for blend films of poly[2-methoxy-5-(3, 7-dimethyloctyloxy)-1, 4-phenylenevinylene] (MDMO-PPV) and PCBM. On a nanosecond time scale after photoexcitation, polymer hole polaron and PCBM radical anion are observed but no PCBM radical cation is found in the blends. Subsequently, the fraction of polymer hole polarons decreases and that of PCBM radical cations increases with time. Finally, the fraction of PCBM radical cations becomes constant on a microsecond time scale. The final fraction of PCBM radical cation is dependent on the ionization potential of polymers but independent of the excitation wavelength. These findings show that the formation of PCBM radical cation is due to hole injection from polymer to PCBM domains. Furthermore, the energetic conditions for such hole injection in polymer/PCBM blend films are discussed on the basis of Monte Carlo analysis for hole hopping in a disordered donor/acceptor heterojunction with varying energetic parameters.en
dc.language.isoeng-
dc.publisherWileyen
dc.rightsThis is the peer reviewed version of the following article: [Yamamoto, S., Ohkita, H., Benten, H. and Ito, S. (2012), Formation Mechanism of Fullerene Cation in Bulk Heterojunction Polymer Solar Cells. Adv. Funct. Mater., 22: 3075-3082.], which has been published in final form at https://doi.org/10.1002/adfm.201200086 This article may be used for non-commercial purposes in accordance with Wiley Terms and Conditions for Use of Self-Archived Versions. This article may not be enhanced, enriched or otherwise transformed into a derivative work, without express permission from Wiley or by statutory rights under applicable legislation. Copyright notices must not be removed, obscured or modified. The article must be linked to Wiley’s version of record on Wiley Online Library and any embedding, framing or otherwise making available the article or pages thereof by third parties from platforms, services and websites other than Wiley Online Library must be prohibited.en
dc.rightsThe full-text file will be made open to the public on 17 April 2013 in accordance with publisher's 'Terms and Conditions for Self-Archiving'.en
dc.rightsThis is not the published version. Please cite only the published version. この論文は出版社版でありません。引用の際には出版社版をご確認ご利用ください。en
dc.subjectconjugated polymersen
dc.subjectfullerenesen
dc.subjectfullerene cationsen
dc.subjectpolymer solar cellsen
dc.subjecthole injectionen
dc.titleFormation Mechanism of Fullerene Cation in Bulk Heterojunction Polymer Solar Cellsen
dc.typejournal article-
dc.type.niitypeJournal Article-
dc.identifier.jtitleAdvanced Functional Materialsen
dc.identifier.volume22-
dc.identifier.issue14-
dc.identifier.spage3075-
dc.identifier.epage3082-
dc.relation.doi10.1002/adfm.201200086-
dc.textversionauthor-
dcterms.accessRightsopen access-
datacite.date.available2013-04-17-
dc.identifier.pissn1616-301X-
dc.identifier.eissn1616-3028-
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