Short Excited-State Lifetimes Mediate Charge-Recombination Losses in Organic Solar Cell Blends with Low Charge-Transfer Driving Force

dc.bibliographicCitation.articleNumber2101784
dc.bibliographicCitation.date2022
dc.bibliographicCitation.firstPage2101784eng
dc.bibliographicCitation.issue22
dc.bibliographicCitation.journalTitleAdvanced materialseng
dc.bibliographicCitation.volume34
dc.contributor.authorShivhare, Rishi
dc.contributor.authorMoore, Gareth John
dc.contributor.authorHofacker, Andreas
dc.contributor.authorHutsch, Sebastian
dc.contributor.authorZhong, Yufei
dc.contributor.authorHambsch, Mike
dc.contributor.authorErdmann, Tim
dc.contributor.authorKiriy, Anton
dc.contributor.authorMannsfeld, Stefan C.B.
dc.contributor.authorOrtmann, Frank
dc.contributor.authorBanerji, Natalie
dc.date.accessioned2021-12-06T08:26:05Z
dc.date.available2021-12-06T08:26:05Z
dc.date.issued2021
dc.description.abstractA blend of a low-optical-gap diketopyrrolopyrrole polymer and a fullerene derivative, with near-zero driving force for electron transfer, is investigated. Using femtosecond transient absorption and electroabsorption spectroscopy, the charge transfer (CT) and recombination dynamics as well as the early-time transport are quantified. Electron transfer is ultrafast, consistent with a Marcus-Levich-Jortner description. However, significant charge recombination and unusually short excited (S1 ) and CT state lifetimes (≈14 ps) are observed. At low S1 -CT offset, a short S1 lifetime mediates charge recombination because: i) back-transfer from the CT to the S1 state followed by S1 recombination occurs and ii) additional S1 -CT hybridization decreases the CT lifetime. Both effects are confirmed by density functional theory calculations. In addition, relatively slow (tens of picoseconds) dissociation of charges from the CT state is observed, due to low local charge mobility. Simulations using a four-state kinetic model entailing the effects of energetic disorder reveal that the free charge yield can be increased from the observed 12% to 60% by increasing the S1 and CT lifetimes to 150 ps. Alternatively, decreasing the interfacial CT state disorder while increasing bulk disorder of free charges enhances the yield to 65% in spite of the short lifetimes.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/7640
dc.identifier.urihttps://doi.org/10.34657/6687
dc.language.isoengeng
dc.publisherWeinheim : Wiley-VCHeng
dc.relation.doihttps://doi.org/10.1002/adma.202101784
dc.relation.essn1521-4095
dc.rights.licenseCC BY 4.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/eng
dc.subject.ddc540eng
dc.subject.ddc660eng
dc.subject.othercharge transfereng
dc.subject.otherenergy materialseng
dc.subject.otherorganic solar cellseng
dc.subject.otherphotophysicseng
dc.subject.otherultrafast spectroscopyeng
dc.titleShort Excited-State Lifetimes Mediate Charge-Recombination Losses in Organic Solar Cell Blends with Low Charge-Transfer Driving Forceeng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorIPFeng
wgl.subjectChemieeng
wgl.typeZeitschriftenartikeleng
Files
Original bundle
Now showing 1 - 1 of 1
Loading...
Thumbnail Image
Name:
adma.202101784.pdf
Size:
1.72 MB
Format:
Adobe Portable Document Format
Description:
Collections