A fluorene-terminated hole-transporting material for highly efficient and stable perovskite solar cells

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dc.contributor.authorJeon, Nam Joongko
dc.contributor.authorNa, Hyejinko
dc.contributor.authorJung, Eui Hyukko
dc.contributor.authorYang, Tae-Youlko
dc.contributor.authorLee, Yong Gukko
dc.contributor.authorKim, Geunjinko
dc.contributor.authorShin, Hee-Wonko
dc.contributor.authorSeok, Sang Ilko
dc.contributor.authorLee, Jaeminko
dc.contributor.authorSeo, Jangwonko
dc.date.accessioned2021-05-04T05:30:13Z-
dc.date.available2021-05-04T05:30:13Z-
dc.date.created2021-05-04-
dc.date.created2021-05-04-
dc.date.issued2018-08-
dc.identifier.citationNATURE ENERGY, v.3, no.8, pp.682 - +-
dc.identifier.issn2058-7546-
dc.identifier.urihttp://hdl.handle.net/10203/282744-
dc.description.abstractPerovskite solar cells (PSCs) require both high efficiency and good long-term stability if they are to be commercialized. It is crucial to finely optimize the energy level matching between the perovskites and hole-transporting materials to achieve better performance. Here, we synthesize a fluorene-terminated hole-transporting material with a fine-tuned energy level and a high glass transition temperature to ensure highly efficient and thermally stable PSCs. We use this material to fabricate photovoltaic devices with 23.2% efficiency (under reverse scanning) with a steady-state efficiency of 22.85% for small-area (-0.094 cm(2)) cells and 21.7% efficiency (under reverse scanning) for large-area (-1 cm(2)) cells. We also achieve certified efficiencies of 22.6% (small-area cells, -0.094 cm(2)) and 20.9% (large-area, -1 cm(2)). The resultant device shows better thermal stability than the device with spiro-OMeTAD, maintaining almost 95% of its initial performance for more than 500 h after thermal annealing at 60 degrees C.-
dc.languageEnglish-
dc.publisherNATURE PUBLISHING GROUP-
dc.titleA fluorene-terminated hole-transporting material for highly efficient and stable perovskite solar cells-
dc.typeArticle-
dc.identifier.wosid000441098100017-
dc.identifier.scopusid2-s2.0-85049614452-
dc.type.rimsART-
dc.citation.volume3-
dc.citation.issue8-
dc.citation.beginningpage682-
dc.citation.endingpage+-
dc.citation.publicationnameNATURE ENERGY-
dc.identifier.doi10.1038/s41560-018-0200-6-
dc.contributor.localauthorSeo, Jangwon-
dc.contributor.nonIdAuthorJeon, Nam Joong-
dc.contributor.nonIdAuthorNa, Hyejin-
dc.contributor.nonIdAuthorJung, Eui Hyuk-
dc.contributor.nonIdAuthorYang, Tae-Youl-
dc.contributor.nonIdAuthorLee, Yong Guk-
dc.contributor.nonIdAuthorKim, Geunjin-
dc.contributor.nonIdAuthorShin, Hee-Won-
dc.contributor.nonIdAuthorSeok, Sang Il-
dc.contributor.nonIdAuthorLee, Jaemin-
dc.description.isOpenAccessN-
dc.type.journalArticleArticle-
dc.subject.keywordPlusHALIDE PEROVSKITES-
dc.subject.keywordPlusTHERMAL-STABILITY-
dc.subject.keywordPlusSPIRO-OMETAD-
dc.subject.keywordPlusLOW-COST-
dc.subject.keywordPlusPERFORMANCE-
dc.subject.keywordPlusLENGTHS-
dc.subject.keywordPlusLAYERS-
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