School of Chemistry, University of Birmingham, Birmingham, B15 2TT, UK.
Dalton Trans. 2013 Apr 21;42(15):5421-9. doi: 10.1039/c3dt32561j. Epub 2013 Feb 19.
In this paper we report the successful incorporation of silicon into Sr1-yCayMnO3-δ perovskite materials for potential applications in cathodes for solid oxide fuel cells. The Si substitution onto the B site of a (29)Si enriched Sr1-yCayMn1-xSixO3-δ perovskite system is confirmed by (29)Si MAS NMR measurements at low B0 field. The very large paramagnetic shift (~3000-3500 ppm) and anisotropy (span ~4000 ppm) suggests that the Si(4+) species experiences both Fermi contact and electron-nuclear dipolar contributions to the paramagnetic interaction with the Mn(3+/4+) centres. An improvement in the conductivity is observed for low level Si doping, which can be attributed to two factors. The first of these is attributed to the tetrahedral coordination preference of Si leading to the introduction of oxide ion vacancies, and hence a partial reduction of Mn(4+) to give mixed valence Mn. Secondly, for samples with high Sr levels, the undoped systems adopt a hexagonal perovskite structure containing face sharing of MnO6 octahedra, while Si doping is shown to help to stabilise the more highly conducting cubic perovskite containing corner linked octahedra. The level of Si, x, required to stabilise the cubic Sr1-yCayMn1-xSixO3-δ perovskite in these cases is shown to decrease with increasing Ca content; thus cubic symmetry is achieved at x = 0.05 for the Sr0.5Ca0.5Mn1-xSixO3-δ series; x = 0.075 for Sr0.7Ca0.3Mn1-xSixO3-δ; x = 0.10 for Sr0.8Ca0.2Mn1-xSixO3-δ; and x = 0.15 for SrMn1-xSixO3-δ. Composites with 50% Ce0.9Gd0.1O1.95 were examined on dense Ce0.9Gd0.1O1.95 pellets. For all series an improvement in the area specific resistances (ASR) values is observed for the Si-doped samples. Thus these preliminary results show that silicon can be incorporated into perovskite cathode materials and can have a beneficial effect on the performance.
本文报道了成功地将硅掺入 Sr1-yCayMnO3-δ钙钛矿材料中,以应用于固体氧化物燃料电池的阴极。通过在低 B0 场下进行的 (29)Si MAS NMR 测量,证实了 Si 取代 (29)Si 富集 Sr1-yCayMn1-xSixO3-δ钙钛矿体系中的 B 位。非常大的顺磁位移(3000-3500 ppm)和各向异性(跨度4000 ppm)表明 Si(4+) 物种同时经历费米接触和电子-核偶极对与 Mn(3+/4+)中心的顺磁相互作用的贡献。在低水平 Si 掺杂时观察到电导率的提高,这可以归因于两个因素。第一个因素归因于 Si 的四面体配位偏好,导致引入氧离子空位,从而部分还原 Mn(4+)以产生混合价态 Mn。其次,对于 Sr 水平较高的样品,未掺杂的系统采用具有面共享 MnO6 八面体的六方钙钛矿结构,而 Si 掺杂被证明有助于稳定具有更高导电性的包含顶角相连八面体的立方钙钛矿。在这些情况下,稳定 Sr1-yCayMn1-xSixO3-δ立方钙钛矿所需的 Si 水平,x,随着 Ca 含量的增加而降低;因此,Sr0.5Ca0.5Mn1-xSixO3-δ 系列中 x = 0.05 时达到立方对称;x = 0.075 用于 Sr0.7Ca0.3Mn1-xSixO3-δ;x = 0.10 用于 Sr0.8Ca0.2Mn1-xSixO3-δ;x = 0.15 用于 SrMn1-xSixO3-δ。在致密的 Ce0.9Gd0.1O1.95 颗粒上研究了与 50% Ce0.9Gd0.1O1.95 的复合材料。对于所有系列,Si 掺杂样品的比面积电阻(ASR)值都有所提高。因此,这些初步结果表明,硅可以掺入钙钛矿阴极材料中,并对性能产生有益影响。