Journal of the American Ceramic Society · 1968 · 95 citations · 6 references
Natural SciencesMaterials SciencePhysicsCeramic MaterialsCondensed Matter PhysicsSolid State PhysicsCrystal ChemistryCrystal LatticeFerroelectric MaterialsPerovskite MaterialsPhase TransitionsSolid-state Phase TransitionsCompositionCoupling CoefficientFerroelectric CrystalsFerroelectric Phase TransitionsFerroelectric PropertiesFerroelectric StructurePerovskite Crystal StructurePhase Transition Temperature
Extensive solid solution was observed in the system Pb(Sc 1/2 /,Nb 1/2 ,) 1‐x ,Ti x ,O 3 . In the range 0 ≤ x ≤ 0.425 a rhombohedral ferroelectric phase was stable at 25° C. In the range 0.45 ≤ x ≤ 1.00 a tetragonal ferroelectric phase was stable at this temperature. The phase diagram of the system below 500° C strongly resembles that of PbZrO 3 −PbTiO 3 . The compound Pb(Sc 1/2 Nb 1/2 )O 3 exhibited rhombohedral perovskite cell symmetry below the ferroelectric ↔ paraelectric transition temperature, and the angle a was acute. The radial coupling coefficient was 0.46 for the composition Sc 1/2 Nb 1/2 ) 0.575 Ti 0.4250 O 3 . At 25°C this composition consisted primarily of the rhombohedral phase with a small amount of the tetragonal phase present. The ferroelectric ↔ paraelectric transition occurred over a temperature range in the rhombohedral phase field. The spontaneous polarization was finite at temperatures considerably above the temperature of the permittivity maximum for a given rhombohedral solid solution.
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BERNARD JAFFE, R. Roth, S. Marzullo · Journal of research of the National Bureau of Standards · 1955 · 574 citations · Full text
Natural Sciences, Materials Engineering, Materials Science +17
On the Phase Transition in Lead Titanate
G. Shirane, Sadao Hoshino · Journal of the Physical Society of Japan · 1951 · 394 citations