Journal of Physics Condensed Matter · 2011 · 13 citations · 14 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsMaterials PhysicsSolid State PhysicsInorganic MaterialsMagnetic Properties Of SolidsMagnetism In SolidsPerovskite MaterialsPhase TransitionsSolid-state Phase TransitionsElectrical Transport PropertiesInsulator-to-metal TransitionMetal-insulator TransitionPerovskite Crystal StructurePerovskite SemiconductorsRietveld RefinementStructural Phase TransitionsTetragonal System
Polycrystalline samples of the perovskite family Sr(1-x)Ca(x)CrO(3) have been prepared at high pressure and temperature in steps of 1/6 over the range 0 ≤ x ≤ 1. Rietveld analysis shows a series of structural phase transitions from cubic to tetragonal to orthorhombic with increasing x. The cubic samples have no long-range magnetic order; the other samples become antiferromagnetically ordered below a T(N) that increases with x. At ambient pressure, the electric transport properties of the cubic and tetragonal phases are semiconducting with a small (meV range) activation energy that increases with x; the orthorhombic phase exhibits variable-range hopping rather than the small-polaron behavior typically found for mixed-valent, localized-electron configurations. Above a pressure P=P(C), a smooth insulator-metal transition is found at a T(IM) that decreases with increasing P for a fixed x; P(C) increases with x. These phenomena are rationalized qualitatively with a π(∗)-band model having a width W(π) that approaches crossover from itinerant-electron to localized-electron behavior as W(π) decreases with increasing x. The smaller size of the Ca(2+) ion induces the structural changes and the greater acidity of the Ca(2+) ion is primarily responsible for narrowing W(π) as x increases.
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Absence of Diffusion in Certain Random Lattices
P. W. Anderson · Physical Review · 1958 · 12.3K citations
John B. Goodenough · Progress in Solid State Chemistry · 1971 · 1.2K citations