The new non-stoichiometric mixed perovskite SrMn0.5Nb0.5O3−δ has a cubic double perovskite structure similar to that of Sr2CrNbO6 with space group Fmm (225), a = 7.9338(3) Å, V = 499.39(6) Å3 according to X-ray diffraction. The material is redox stable and maintains its structure in a reducing atmosphere. After reducing in 5% H2 at 900 °C for 6 hours, SrMn0.5Nb0.5O3−δ still exhibits a cubic structure with space group Pmm (221), a = 4.0022(5) Å, V = 64.10(8) Å3. A lattice volume expansion of 2.7% was observed during the reduction. TGA analysis indicates SrMn0.5Nb0.5O3−δ loses 0.125 oxygen per formula unit from 500 to 950 °C in 5% H2. 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% H2. The conductivities of this material in air, humidified 5% H2 and 5% H2 were 1.23, 6.4 × 10−2 and 3.1 × 10−2 S cm−1 respectively at 900 °C. The decrease of d.c. conductivity of SrMn0.5Nb0.5O3−δ at pO2 below 10−12 atm indicates p-type electronic conduction. The higher apparent conduction activation energy and lower conductivity in H2 than in air may be due to the contribution of lattice expansion which results in poorer overlap of both σ and π bonds, which makes the hopping of electron holes more difficult. The d.c. conductivity of SrMn0.5Nb0.5O3−δ at low pO2 exhibits a pO21/6 dependence that is interpreted by a simple defect chemistry model.
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Tao et al. (2002) studied this question.
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