Journal of Physics Condensed Matter · 2004 · 143 citations · 42 references
Natural SciencesMaterials SciencePhysicsMaterials PhysicsSolid State PhysicsThin FilmsDielectric PropertiesDielectric ResponseDielectricsElectrical Properties Of CeramicsFerroelectric MaterialsPhase TransitionsBarium TitanateCurie-weiss LawFerroelectric CapacitorsFerroelectric Dielectric ResponseFerroelectric Phase TransitionsFerroelectric PropertiesFerroelectricityLoss Tangent
Measurements on 'free-standing' single-crystal barium titanate capacitors with thickness down to 75 nm show a dielectric response typical of large single crystals, rather than conventional thin films. There is a notable absence of any broadening or temperature shift of the dielectric peak or loss tangent. Peak dielectric constants of are observed, and Curie–Weiss analysis demonstrates first order transformation behaviour. This is in dramatic contrast to results on conventionally deposited thin film capacitor heterostructures, which show large dielectric peak broadening and temperature shifts (e.g. Parker et al 2002 Appl. Phys. Lett. 81 340), as well as an apparent change in the nature of the paraelectric–ferroelectric transition from first to second order. Our data are compatible with a recent model by Bratkovsky and Levanyuk (2004 Preprint cond-mat/0402100), which attributes dielectric peak broadening to gradient terms that will exist in any thin film capacitor heterostructure. The observed recovery of first order transformation behaviour is consistent with the absence of significant substrate clamping in our experiment, as modelled by Pertsev et al (1998 Phys. Rev. Lett. 80 1988), and illustrates that the second order behaviour seen in conventionally deposited thin films cannot be attributed to the effects of reduced dimensionality in the system, nor to the influence of an intrinsic universal interfacial capacitance associated with the electrode–ferroelectric interface.
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