Structure dependence of dielectric properties in Ca-doped bismuth magnesium niobate pyrochlores

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Gao, Libin [1 ,2 ]
Liang, Kexin [1 ,2 ]
Liu, Zhongzhe [1 ,2 ]
Chen, Hongwei [1 ,2 ]
Zhang, Jihua [1 ,2 ]
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[1] School of Energy Science and Engineering, University of Electronic Science and Technology of China, Chengdu,610054, China
[2] State Key Laboratory of Electronic Thin Films and Integrated Devices, University of Electronic Science and Technology of China, Chengdu,610054, China
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The cubic pyrochlore Bi1.5MgNb1.5O7 (BMN) materials have large permittivity; good temperature stability; and extremely low dielectric loss. The structure and dielectric properties of Bi1.5Mg1−xCaxNb1.5O7 (BMCN; x = 0.0–0.5) are discussed systematically. All the samples except x = 0.5 were found that the dominant crystalline phase was cubic pyrochlore structure. The BMN (x = 0.0) cubic pyrochlore phase contained little impurity Mg4Nb2O9. Although Ca-doping inhibited the formation of the impurity phase Mg4Nb2O9; excessive Ca-doping (x ≥ 0.4) led to another second phase CaBi2Nb2O9 in BMCN structure. The substitution of Ca2+ brought about the reduction of structure disorder which were caused by abnormal cell shrinkage. It evidenced that Ca2+ ions are prone to substitute Mg2+ ions on A-site; then take on the B-site when the more Ca2+ ions doping in the pyrochlores. The permittivity of doped BMCN (x = 0.1–0.5) was smaller than that of BMN; and decreased with the increase of Ca2+ doping. The dielectric loss of doped BMCN increased due to the lattice defects caused by larger Ca2+ substitution for Mg2+; and the existence of the second phase with x = 0.4–0.5. The temperature dependence of the dielectric properties become unstable by Ca-doping. The Ca2+ substitution led to a closer association of BO6 octahedra; which had adverse impact on temperature stability of BMCN (x = 0.1–0.3). The coexistence of the second phase with positive temperature coefficient improved the dielectric temperature stability of the BMCN (x = 0.4–0.5). The dielectric loss was interpreted on the basis of the interfacial polarization at the grain-boundary region; which would become sensitive to temperature/frequency. © 2022;
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