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Study on the structural and electrical properties of the double perovskite oxide SrMn0.5Nb0.5O3-delta

机译:钙钛矿双氧化物SrMn0.5Nb0.5O3-δ的结构和电学性能研究

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摘要

The new non-stoichiometric mixed perovskite SrMn0.5Nb0.5O3-delta has a cubic double perovskite structure similar to that of Sr2CrNbO6 with space group Fm (3) over barm (225), a = 7.9338(3) Angstrom, V = 499.39(6) Angstrom(3) according to X-ray diffraction. The material is redox stable and maintains its structure in a reducing atmosphere. After reducing in 5% H-2 at 900 degreesC for 6 hours, SrMn0.5Nb0.5O3-delta still exhibits a cubic structure with space group Pm (3) over barm (221), a = 4.0022(5) Angstrom, V = 64.10(8) Angstrom(3). A lattice volume expansion of 2.7% was observed during the reduction. TGA analysis indicates SrMn0.5Nb0.5O3-delta loses 0.125 oxygen per formula unit from 500 to 950 degreesC in 5% H,. This weight change is consistent with a reduction from SrMn0.5Nb0.5O3 to SrMn0.5Nb0.5O2.875. The morphology of this material does not significantly change on reduction according to SEM observation. A.c. impedance measurements indicate that electronic conduction is probably dominant both in air and 5% H-2.(.) The conductivities of this material in air, humidified 5% H-2 and 5%, H-2 were 1.23, 6.4 x 10(-2) and 3.1 x 10(-2) S cm(-1) respectively at 900 degreesC. The decrease of d.c. conductivity of SrMn0.5Nb0.5O3-delta at p(o2), below 10(-12) atm indicates p-type electronic conduction. The higher apparent conduction activation energy and lower conductivity in H-2 than in air may be due to the contribution of lattice expansion which results in poorer overlap of both sigma and Tu bonds, which makes the hopping of electron holes more difficult. The d.c. conductivity of SrMn0.5Nb0.5O3-delta at low p(o2) exhibits a p(o2)(1/6) dependence that is interpreted by a simple defect chemistry model. [References: 19]
机译:新型非化学计量混合钙钛矿SrMn0.5Nb0.5O3-δ具有立方双钙钛矿结构,类似于Sr2CrNbO6的结构,其空间群Fm(3)超过巴姆(225),a = 7.9338(3)埃,V = 499.39( 6)根据X射线衍射的埃(3)。该材料是氧化还原稳定的,并在还原气氛中保持其结构。在900°C下于5%H-2中还原6小时后,SrMn0.5Nb0.5O3-δ仍显示立方结构,其空间群Pm(3)超过巴姆(221),a = 4.0022(5)埃,V = 64.10(8)埃(3)。在还原过程中观察到2.7%的晶格体积膨胀。 TGA分析表明,SrMn0.5Nb0.5O3-δ在5%H中从500到950摄氏度每配方单位损失0.125氧气。这种重量变化与从SrMn0.5Nb0.5O3减少到SrMn0.5Nb0.5O2.875一致。根据SEM观察,该材料的形态在还原时没有显着变化。交流电阻抗测量表明,电子传导可能在空气和5%H-2中均占主导地位。(。)这种材料在空气中的电导率(加湿5%H-2和5%H-2)分别为1.23、6.4 x 10( -2)和在900摄氏度下分别为3.1 x 10(-2)S cm(-1)。直流电的减少在低于10(-12)atm的p(o2)处SrMn0.5Nb0.5O3-δ的电导率表明p型电子导电。 H-2中比空气中更高的表观传导活化能和更低的传导率可能是由于晶格膨胀的作用,这导致sigma键和Tu键的重合较差,这使电子空穴的跃迁更加困难。直流电低p(o2)时SrMn0.5Nb0.5O3-delta的电导率表现出p(o2)(1/6)依赖性,这可以通过简单的缺陷化学模型来解释。 [参考:19]

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