首页> 外文期刊>Journal of the Ceramic Society of Japan >Variation in crystal structure of Ln2Ni1?xCuxO4+δ (Ln: La, Pr, Nd, Sm, Eu, and their solid solution) based on type of Ln: Relationship between crystal structure and tolerance factor
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Variation in crystal structure of Ln2Ni1?xCuxO4+δ (Ln: La, Pr, Nd, Sm, Eu, and their solid solution) based on type of Ln: Relationship between crystal structure and tolerance factor

机译:基于Ln的类型的Ln2Ni1?xCuxO4 +δ(Ln:La,Pr,Nd,Sm,Eu及其固溶体)的晶体结构变化:晶体结构与公差因子之间的关系

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The variation in the crystal structure of Ln sub2/subNisub1?/sub subx/sub Cu subx/sub Osub4+δ/sub, which has great potential as a new cathode material for solid oxide fuel cells, based on the type of Ln (La, Pr, Nd, Sm, Eu, and their solid solution), was investigated. For Ln with ionic radius larger than 1.21 ? (1 ? = 0.1 nm), a single-phase Ksub2/subNiFsub4/sub structure called T-phase was prepared for 0.0 ≤ x ≤ 1.0. For Ln with ionic radius between 1.21 and 1.15 ?, the crystal structure changed from single T-phase to single Ndsub2/subCuOsub4/sub structure called T′-phase, through the mixture of T-phase and T′-phase, along with increasing Cu content. The range of Cu content, in which the mixture phase was obtained because of the miscibility gap, increased with the decreasing size of Ln . The single T-phase was never prepared for Ln with ionic radius below 1.15 ?. Rough tendencies were observed, indicating that the single T-phase was obtained or was not prepared if the tolerance factor was above or below 0.865, respectively. The mixture of T-phase and T′-phase was obtained because of the miscibility gap by decreasing the tolerance factor slightly below about 0.865. The T-phase was never generated by decreasing the tolerance factor any further. The change of the crystal structure by Cu content and kind of Ln can also be explained by using Jahn–Teller effect of Cusup2+/sup ion.
机译:Ln 2 Ni 1? x Cu x O 4 +δ的晶体结构变化基于Ln的类型(La,Pr,Nd,Sm,Eu及其固溶体),作为固体氧化物燃料电池的新型正极材料具有很大的潜力。对于离子半径大于1.21的Ln? (1θ= 0.1nm),制备了称为T-相的单相K 2 NiF 4 结构,其中0.0≤x≤1.0。对于离子半径在1.21和1.15?之间的Ln,通过混合,晶体结构从单T相变为单Nd 2 CuO 4 结构,称为T'相。 T相和T'相的变化,以及Cu含量的增加。由于可混溶间隙而获得混合相的Cu含量范围随Ln尺寸的减小而增加。对于离子半径低于1.15的Ln,从未准备过单一的T相。观察到粗糙的趋势,表明如果容限因子分别高于或低于0.865,则将获得或未制备单个T相。由于混溶性间隙,通过将公差因子降低到略低于约0.865,获得了T相和T'相的混合物。不再通过进一步减小公差因子来生成T相。利用Cu 2 + 离子的Jahn-Teller效应也可以解释由于Cu含量和Ln的种类引起的晶体结构的变化。

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