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The effect of the chemical substitution of Ti, Zr, and Gd cations on the structure and properties of bismuth‐based pyrochlores was investigated for (Bi 1.5 Zn 1.0 Nb 1.5 )O 7 and Bi 2 (Zn 2/3 Nb 4/3 )O 7 . Broad ranges of solid solutions based on cubic (Bi 1.5 Zn 1.0 Nb 1.5 )O 7 were observed for Ti and Zr cations: (Bi 1.5 Zn 1−( x /3) Nb 1.5−(2 x /3) Zr x )O 7 (0.0 ≤ x ≤ 1.5) and (Bi 1.5 Zn 1−( x /3) Nb 1.5−(2 x /3) Ti x )O 7 (0.0 ≤ x ≤ 2.25). For Gd cations, the range of solid solution was quite limited in (Bi 1.5− x Gd x Zn 1.0 Nb 1.5 )O 7 (0.0 ≤ x ≤ 0.2); however, the range of solid solution is more extensive in the system that contains Ti and Gd cations ((Bi 1.5− x Gd x Zn 0.5 Ti 1.5 Nb 0.5 )O 7 (0.0 ≤ x ≤ 0.6)). The stability fields of the solid solutions could be interpreted by using the ratio of the ionic sizes of the A‐ and B‐site ions in the pyrochlore structure ( R A / R B ). The substituted phases exhibited permittivities (κ′) in the range of ∼100–200 and relatively low dielectric losses (tan δ < 7 × 10 −4 ) at 1 MHz. The temperature coefficients of permittivity (τ κ ) varied in accordance with the R A / R B value and could be tuned from −88 ppm/K to −1300 ppm/K. For the orthorhombic Bi 2 (Zn 2/3 Nb 4/3 )O 7 pyrochlore, the ranges of solid solution were very limited and the dielectric properties remained similar to those of the undoped phase (κ′= 90, τ κ = 150 ppm/K).
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Valant et al. (2000) studied this question.
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