2006
DOI: 10.1063/1.2174100
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Ferroelectric properties of SrRuO3∕BaTiO3∕SrRuO3 ultrathin film capacitors free from passive layers

Abstract: thicknesses of between 5 nm and 30 nm, show well-defined interfaces between ferroelectric BaTiO 3 and electrode SrRuO 3 layers. In these capacitors, we cannot observe any extrinsic electrical effects due to either the formation of an insulating interfacial passive layer or passive-layer-induced charge injection. Such high quality interfaces result in very good fatigue endurance, even for the 5 nm thick BaTiO 3 capacitor.

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Cited by 60 publications
(45 citation statements)
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“…In particular, the observation of a negligible intercept at one temperature 52 does not represent a convincing proof for the absence of "dead" layers in the capacitor. Indeed, such zero intercept may result from the mutual compensation of the positive and negative contributions to c t −1 ͑t → 0͒, but not from the zero interfacial capacitance c i .…”
Section: Discussionmentioning
confidence: 96%
“…In particular, the observation of a negligible intercept at one temperature 52 does not represent a convincing proof for the absence of "dead" layers in the capacitor. Indeed, such zero intercept may result from the mutual compensation of the positive and negative contributions to c t −1 ͑t → 0͒, but not from the zero interfacial capacitance c i .…”
Section: Discussionmentioning
confidence: 96%
“…13,14 At this point, let us compare the observed E C values with the thermodynamic intrinsic limit using the LD model. To check for the possibility of homogeneous switching in our ultrathin films, we calculated E C using LD theory with the free energy density functional (Ĝ):…”
Section: -7mentioning
confidence: 99%
“…The polar axis of the material is perpendicular to the film plane and the electrodes are 'real' meaning that the electric field penetrates into them, although only over tiny depths < 1Å. This is an adequate model for the perovskite ferroelectric films on a substrate with compressive strain, like BaTiO 3 /SrRuO 3 /SrTiO 3 (BTO/SRO/STO) [1][2][3][4][5] where the misfit strain drives the FE film into a uniaxial state. We supplement our analytical results with the relevant numerical estimates for BaTiO 3 (BTO), PbTiO 3 (PTO), and Pb(Zr 0.5 Ti 0.5 )O 3 (PZT) using the material constants available in the literature Incomplete screening of the depolarizing field by SrRuO 3 electrode leads to an absolute instability of a single domain state and formation of a sinusoidal domain structure when thickness of BaTiO 3 film is slightly above the minimal thickness compatible with ferroelectricity in this system [5][6][7] .…”
Section: Introductionmentioning
confidence: 99%
“…We shall also discuss this stability among other questions This makes sense because of several reasons. First, Pertsev and Kohlstedt performed numerical calculations using material constants for BaTiO 3 and Pb(Zr 0.5 Ti 0.5 )O 3 and the electrode parameters of SrRuO 3 while our results are analytical and apply to any material of the same symmetry. Moreover, our method applies to other symmetries as well.…”
Section: Introductionmentioning
confidence: 99%