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Sökning: WFRF:(Wang Shenghao) > (2016) > Role of the dopants...

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FältnamnIndikatorerMetadata
00003735naa a2200397 4500
001oai:DiVA.org:kau-83187
003SwePub
008210222s2016 | |||||||||||000 ||eng|
024a https://urn.kb.se/resolve?urn=urn:nbn:se:kau:diva-831872 URI
024a https://doi.org/10.1021/acs.chemmater.6b017772 DOI
040 a (SwePub)kau
041 a engb eng
042 9 SwePub
072 7a ref2 swepub-contenttype
072 7a art2 swepub-publicationtype
100a Juarez-Perez, Emilio J.u Okinawa Institute of Science and Technology Graduate University, JPN4 aut
2451 0a Role of the dopants on the morphological and transport properties of Spiro-MeOTAD hole transport layer
264 c 2016-08-04
264 1b American Chemical Society (ACS),c 2016
338 a print2 rdacarrier
520 a The use of a solid hole transport layer (HTL) was transformational for the recent perovskite solar cell (PSC) revolution in solar energy technology. Often high efficiency PSC devices employ heavily doped hole transport materials such as spiro-MeOTAD. Independent of HTL chemistry, lithium-bis-trifluoromethanesulfonyl-imide (LiTFSI) and tert-butylpyridine (TBP) are commonly used as additives in HTL formulations for PSCs. LiTFSI and TBP were originally optimized for dye sensitized solar cells, where their roles have been extensively studied. However, in the case of PSCs, the function of TBP is not clearly understood. In this study, properties of the HTL composite deposited on flat silicon substrates were systematically measured at several length scales, e.g., macroscopically (profilometry, 4-point probe conductivity, and thermogravimetrydifferential thermal analysis), microscopically, and at the nanoscale to investigate film morphology, conductivity, and dopant distribution. Microscopic distributions of spiro-MeOTAD, LiTFSI, and TBP were determined using 2D Fourier transform infrared (FTIR) microscopy and electrostatic atomic force microscopy (EFM). Our findings reveal that the main role of TBP is to prevent phase segregation of LiTFSI and Spiro-MeOTAD, resulting in a homogeneous hole transport layer. These properties are critical for charge transport in the HTL bulk film as well as at the perovskite/HTL and HTL/electrode interfaces and for efficient solar cell performance.
650 7a TEKNIK OCH TEKNOLOGIERx Materialteknik0 (SwePub)2052 hsv//swe
650 7a ENGINEERING AND TECHNOLOGYx Materials Engineering0 (SwePub)2052 hsv//eng
653 a Physics
653 a Fysik
700a Leyden, Matthew R.u Okinawa Institute of Science and Technology Graduate University, JPN4 aut
700a Wang, Shenghaou Okinawa Institute of Science and Technology Graduate University, JPN4 aut
700a Ono, Luis K.u Okinawa Institute of Science and Technology Graduate University, JPN4 aut
700a Hawash, Zaferu Okinawa Inst Sci & Technol Grad Univ GIST, Energy Mat & Surface Sci Unit EMSS, 1919-1 Tancha, Okinawa 9040495, Japan.4 aut0 (Swepub:kau)zafehawa
700a Qi, Yabingu Okinawa Institute of Science and Technology Graduate University, JPN4 aut
710a Okinawa Institute of Science and Technology Graduate University, JPNb Okinawa Inst Sci & Technol Grad Univ GIST, Energy Mat & Surface Sci Unit EMSS, 1919-1 Tancha, Okinawa 9040495, Japan.4 org
773t Chemistry of Materialsd : American Chemical Society (ACS)g 28:16, s. 5702-5709q 28:16<5702-5709x 0897-4756x 1520-5002
856u https://doi.org/10.1021/acs.chemmater.6b01777y Fulltext
856u https://pubs.acs.org/doi/pdf/10.1021/acs.chemmater.6b01777
8564 8u https://urn.kb.se/resolve?urn=urn:nbn:se:kau:diva-83187
8564 8u https://doi.org/10.1021/acs.chemmater.6b01777

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