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学術論文

Gating effects of conductive polymeric ionic liquids

MPS-Authors

Cui,  Bin
Nano-Systems from Ions, Spins and Electrons, Max Planck Institute of Microstructure Physics, Max Planck Society;

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Gao,  Fang
Nano-Systems from Ions, Spins and Electrons, Max Planck Institute of Microstructure Physics, Max Planck Society;

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Parkin,  Stuart S. P.       
Nano-Systems from Ions, Spins and Electrons, Max Planck Institute of Microstructure Physics, Max Planck Society;

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引用

Chen, S., Frenzel, F., Cui, B., Gao, F., Campanella, A., Funtan, A., Kremer, F., Parkin, S. S. P., & Binder, W. H. (2018). Gating effects of conductive polymeric ionic liquids. Journal of Materials Chemistry C, 6(30), 8242-8250. doi:10.1039/C8TC01936C.


引用: https://hdl.handle.net/21.11116/0000-0009-272A-D
要旨
Poly(ionic liquid)s (POILs) belong to one of the most promising materials class in electrochemistry. In this study, we investigate POILs as a gating material within a field-effect transistor, additionally describing their glassy dynamics and charge transport properties. Four different imidazolium-based POILs have been investigated, ranging from homopolymers with varied counterions, i.e. POIL 1: P(APMIN(Tf)2) poly(1-[2-acryloylpropyl]-3-methylimidazolium bis(trifluoromethane)sulfonamide) and POIL 2: P(APMIPF6) poly(1-[2-acryloylpropyl]-3-methylimidazolium hexafluorophosphate, to semifluorinated random copolymers, i.e. POIL 3: P(APMIN(Tf)2-co-TFEA) (TFEA: 2,2,2-trifluoroethyl acrylate), and finally to semifluorinated triblock copolymers, POIL 4: P(APMIN(Tf)2-co-TFEA)-b-PPFS-b-P(APMIN(Tf)2-co-TFEA) (PPFS: polypentafluorostyrene). Their glassy dynamics and charge transport mechanism are investigated by broadband dielectric spectroscopy (BDS), differential scanning calorimetry (DSC) and alternating current chip-calorimetry (ACC). The gating effects of these POILs are studied in detail, showing for the first time a reversible phase transition between thin films formed from the brownmillertite phase SrCoO2.5 and the perovskite phase SrCoO3 by use of such POILs, being especially pronounced for POIL 1: P(APMIN(Tf)2) homopolymer displaying gate voltages (VG) of 3–4 V and a gating time of ∼4 h. In the case of the POIL 3, P(APMIN(Tf)2-co-TFEA) as a random copolymer, higher VG (−8/+5 V) and a longer gating time (∼16 h) are revealed. Phase transition between SrCoO2.5 and SrCoO3 could not be observed from POILs 2 & 4 even using very large gate voltages (−10/+8 V) for a much longer time (48 h), indicating that primarily charge density and charge-carrier mobility are decisive in ionic liquid gating.