Phase equilibria in the (1−
x)BaZrO
3-
xCaZrO
3 system were analyzed using a combination of X-ray and neutron powder diffraction, and transmission electron microscopy. The proposed phase diagram features two extended two-phase fields containing mixtures of a Ba-rich cubic phase and a tetragonal, or orthorhombic Ca-rich phase, all having perovskite-related structures. The symmetry differences in the Ca-rich phases are caused by different tilting patterns of the [ZrO
6] octahedra. In specimens quenched from 1650°C, CaZrO
3 dissolves only a few percent of Ba, whereas the solubility of Ca in BaZrO
3 is approximately . The BaZrO
3-CaZrO
3 system features at least two tilting phase transitions,
Pm3
m→
I4/
mcm and
I4/
mcm→
Pbnm. Rietveld refinements of the Ba
0.8Ca
0.2ZrO
3 structure using variable-temperature neutron powder diffraction data confirmed that the
Pm3
m→
I4/
mcm transition corresponds to a rotation of octahedra about one of the cubic axes; successive octahedra along this axis rotate in opposite directions. In situ variable-temperature electron diffraction studies indicated that the transition temperature increases with increasing Ca-substitution on the
A-sites, from approximately −120°C at Ca to 225°C at Ca. Dielectric measurements revealed that the permittivity increases monotonically from 36 for BaZrO
3 to 53 for Ba
0.9Ca
0.1ZrO
3, and then decreases to 50 for Ba
0.8Ca
0.2ZrO
3. This later specimen was the Ca-richest composition for which pellets could be quenched from the single-phase cubic field with presently available equipment. Strongly non-monotonic behavior was also observed for the temperature coefficient of resonant frequency; however, in this case, the maximum occurred at a lower Ca concentration, 0.05?
x?0.1. The non-linear behavior of the dielectric properties was attributed to two competing structural effects: a positive effect associated with substitution of relatively small Ca cations on the
A-sites, resulting in stretched Ca-O bonds, and a negative effect, related to the distortion of the
A-site environment (bond strain relaxation) upon octahedral tilting.
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