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dc.contributor.authorChen, Mark S.
dc.contributor.authorLee, Olivia P.
dc.contributor.authorNiskala, Jeremy R.
dc.contributor.authorYiu, Alan T.
dc.contributor.authorTassone, Christopher J.
dc.contributor.authorSchmidt, Kristin
dc.contributor.authorBeaujuge, Pierre M.
dc.contributor.authorOnishi, Seita S.
dc.contributor.authorToney, Michael F.
dc.contributor.authorZettl, Alex K.
dc.contributor.authorFrechet, Jean
dc.date.accessioned2015-08-03T11:37:13Z
dc.date.available2015-08-03T11:37:13Z
dc.date.issued2013-12-26
dc.identifier.issn00027863
dc.identifier.doi10.1021/ja4088665
dc.identifier.urihttp://hdl.handle.net/10754/563162
dc.description.abstractEfficient charge carrier transport in organic field-effect transistors (OFETs) often requires thin films that display long-range order and close π-π packing that is oriented in-plane with the substrate. Although some polymers have achieved high field-effect mobility with such solid-state properties, there are currently few general strategies for controlling the orientation of π-stacking within polymer films. In order to probe structural effects on polymer-packing alignment, furan-containing diketopyrrolopyrrole (DPP) polymers with similar optoelectronic properties were synthesized with either linear hexadecyl or branched 2-butyloctyl side chains. Differences in polymer solubility were observed and attributed to variation in side-chain shape and polymer backbone curvature. Averaged field-effect hole mobilities of the polymers range from 0.19 to 1.82 cm2/V·s, where PDPP3F-C16 is the least soluble polymer and provides the highest maximum mobility of 2.25 cm2/V·s. Analysis of the films by AFM and GIXD reveal that less soluble polymers with linear side chains exhibit larger crystalline domains, pack considerably more closely, and align with a greater preference for in-plane π-π packing. Characterization of the polymer solutions prior to spin-coating shows a correlation between early onset nanoscale aggregation and the formation of films with highly oriented in-plane π-stacking. This effect is further observed when nonsolvent is added to PDPP3F-BO solutions to induce aggregation, which results in films with increased nanostructural order, in-plane π-π orientation, and field-effect hole mobilities. Since nearly all π-conjugated materials may be coaxed to aggregate, this strategy for enhancing solid-state properties and OFET performance has applicability to a wide variety of organic electronic materials. © 2013 American Chemical Society.
dc.description.sponsorshipThis work was supported in part by the Director, Office of Science, Office of Basic Energy Sciences, Materials Science and Engineering Division, of the U.S. Department of Energy under contract no. DE-AC02-05CH11231, within the SP2-bonded Materials Program, which provided for device fabrication and electrical characterization, the Center for Advanced Molecular Photovoltaics (CAMP) under award no. KUS-C1-015-21, supported by King Abdullah University of Science and Technology (KAUST), and the Frechet "various gifts" fund for the support of research in new materials. Portions of this research were carried out at the Stanford Synchrotron Radiation Lightsource user facility, operated on behalf of the U.S. Department of Energy, Office of Basic Energy Sciences. M.S.C. thanks the Camille and Henry Dreyfus Postdoctoral Program in Environmental Chemistry for a fellowship.
dc.publisherAmerican Chemical Society (ACS)
dc.titleEnhanced solid-state order and field-effect hole mobility through control of nanoscale polymer aggregation
dc.typeArticle
dc.contributor.departmentChemical Science Program
dc.contributor.departmentPhysical Sciences and Engineering (PSE) Division
dc.identifier.journalJournal of the American Chemical Society
dc.contributor.institutionDepartment of Chemistry, University of California, Berkeley, CA 94720, United States
dc.contributor.institutionDepartment of Chemical and Biomolecular Engineering, University of California, Berkeley, CA 94720, United States
dc.contributor.institutionMaterials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, United States
dc.contributor.institutionDepartment of Physics, University of California, Berkeley, CA 94720, United States
dc.contributor.institutionKavli Energy Nanosciences Institute, University of California, Berkeley, CA 94720, United States
dc.contributor.institutionStanford Synchrotron Radiation Lightsource, Menlo Park, CA 94025, United States
kaust.personFrechet, Jean


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