Room-temperature proton transport and its effect on thermopower in a solid ionic semiconductor, TTFCOONH sub(4)
Ammonium proton in a solid ionic semiconductor, TTFCOONH sub(4), is shown to be mobile under anhydrous conditions at room temperature by the hydrogen concentration cell method. Isotope substituted TTFCOOND sub(4) exhibits a 2.2 H/D isotope effect in ion carrier mobility with TTFCOONH sub(4). First-p...
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Veröffentlicht in: | Journal of materials chemistry. A, Materials for energy and sustainability Materials for energy and sustainability, 2013-03, Vol.1 (16), p.5089-5096 |
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creator | Kobayashi, Yuka Fujii, Takenori Terasaki, Ichiro Kino, Hiori Jin, Yongcheng Hibino, Takashi Kobayashi, Tetsuya Nishibori, Eiji Sawa, Hiroshi Yoshikawa, Hideki Terauchi, Takeshi Sumi, Satoshi |
description | Ammonium proton in a solid ionic semiconductor, TTFCOONH sub(4), is shown to be mobile under anhydrous conditions at room temperature by the hydrogen concentration cell method. Isotope substituted TTFCOOND sub(4) exhibits a 2.2 H/D isotope effect in ion carrier mobility with TTFCOONH sub(4). First-principles calculations reveal that an efficient proton-transfer pathway vialow-barrier N...H super(+)...N hydrogen bonds reduces the activation energy to 0.12 eV, which is quite small and comparable to that reported in a bulk water system. The ac conductivity of TTFCOONH sub(4) and TTFCOOND sub(4) is similar at room temperature, reflecting similar hole carrier concentrations. In sharp contrast, the thermopower exhibits a large isotope effect: TTFCOONH sub(4) shows 260 mu V K super(-1), which is twice as large as that predicted by the hole carrier concentration and the value of TTFCOOND sub(4), with 138 mu V K super(-1). The 1.9 H/D isotope effect in thermopower closely relates to the 2.2 H/D isotope effect in ion carrier mobility. Proton carriers in the temperature gradient enhance thermopower without cancelling out the effect of holes in the solid state owing to possession of the same positive charge. |
doi_str_mv | 10.1039/c3ta00011g |
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Isotope substituted TTFCOOND sub(4) exhibits a 2.2 H/D isotope effect in ion carrier mobility with TTFCOONH sub(4). First-principles calculations reveal that an efficient proton-transfer pathway vialow-barrier N...H super(+)...N hydrogen bonds reduces the activation energy to 0.12 eV, which is quite small and comparable to that reported in a bulk water system. The ac conductivity of TTFCOONH sub(4) and TTFCOOND sub(4) is similar at room temperature, reflecting similar hole carrier concentrations. In sharp contrast, the thermopower exhibits a large isotope effect: TTFCOONH sub(4) shows 260 mu V K super(-1), which is twice as large as that predicted by the hole carrier concentration and the value of TTFCOOND sub(4), with 138 mu V K super(-1). The 1.9 H/D isotope effect in thermopower closely relates to the 2.2 H/D isotope effect in ion carrier mobility. Proton carriers in the temperature gradient enhance thermopower without cancelling out the effect of holes in the solid state owing to possession of the same positive charge.</description><identifier>ISSN: 2050-7488</identifier><identifier>EISSN: 2050-7496</identifier><identifier>DOI: 10.1039/c3ta00011g</identifier><language>eng</language><ispartof>Journal of materials chemistry. 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A, Materials for energy and sustainability</title><description>Ammonium proton in a solid ionic semiconductor, TTFCOONH sub(4), is shown to be mobile under anhydrous conditions at room temperature by the hydrogen concentration cell method. Isotope substituted TTFCOOND sub(4) exhibits a 2.2 H/D isotope effect in ion carrier mobility with TTFCOONH sub(4). First-principles calculations reveal that an efficient proton-transfer pathway vialow-barrier N...H super(+)...N hydrogen bonds reduces the activation energy to 0.12 eV, which is quite small and comparable to that reported in a bulk water system. The ac conductivity of TTFCOONH sub(4) and TTFCOOND sub(4) is similar at room temperature, reflecting similar hole carrier concentrations. In sharp contrast, the thermopower exhibits a large isotope effect: TTFCOONH sub(4) shows 260 mu V K super(-1), which is twice as large as that predicted by the hole carrier concentration and the value of TTFCOOND sub(4), with 138 mu V K super(-1). The 1.9 H/D isotope effect in thermopower closely relates to the 2.2 H/D isotope effect in ion carrier mobility. 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A, Materials for energy and sustainability</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kobayashi, Yuka</au><au>Fujii, Takenori</au><au>Terasaki, Ichiro</au><au>Kino, Hiori</au><au>Jin, Yongcheng</au><au>Hibino, Takashi</au><au>Kobayashi, Tetsuya</au><au>Nishibori, Eiji</au><au>Sawa, Hiroshi</au><au>Yoshikawa, Hideki</au><au>Terauchi, Takeshi</au><au>Sumi, Satoshi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Room-temperature proton transport and its effect on thermopower in a solid ionic semiconductor, TTFCOONH sub(4)</atitle><jtitle>Journal of materials chemistry. A, Materials for energy and sustainability</jtitle><date>2013-03-01</date><risdate>2013</risdate><volume>1</volume><issue>16</issue><spage>5089</spage><epage>5096</epage><pages>5089-5096</pages><issn>2050-7488</issn><eissn>2050-7496</eissn><abstract>Ammonium proton in a solid ionic semiconductor, TTFCOONH sub(4), is shown to be mobile under anhydrous conditions at room temperature by the hydrogen concentration cell method. Isotope substituted TTFCOOND sub(4) exhibits a 2.2 H/D isotope effect in ion carrier mobility with TTFCOONH sub(4). First-principles calculations reveal that an efficient proton-transfer pathway vialow-barrier N...H super(+)...N hydrogen bonds reduces the activation energy to 0.12 eV, which is quite small and comparable to that reported in a bulk water system. The ac conductivity of TTFCOONH sub(4) and TTFCOOND sub(4) is similar at room temperature, reflecting similar hole carrier concentrations. In sharp contrast, the thermopower exhibits a large isotope effect: TTFCOONH sub(4) shows 260 mu V K super(-1), which is twice as large as that predicted by the hole carrier concentration and the value of TTFCOOND sub(4), with 138 mu V K super(-1). The 1.9 H/D isotope effect in thermopower closely relates to the 2.2 H/D isotope effect in ion carrier mobility. Proton carriers in the temperature gradient enhance thermopower without cancelling out the effect of holes in the solid state owing to possession of the same positive charge.</abstract><doi>10.1039/c3ta00011g</doi></addata></record> |
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title | Room-temperature proton transport and its effect on thermopower in a solid ionic semiconductor, TTFCOONH sub(4) |
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