2006
DOI: 10.1016/j.solidstatesciences.2006.04.005
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Why is SrTiO3 much stronger at nanometer than at centimeter scale?

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Cited by 19 publications
(10 citation statements)
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“…It was found that the larger d 33f value of the PZT film on CNOns/glass than those on CNOns/Si and STO. For these relatively thin films a large fraction of the clamping is due to the substrate, that is expected to be proportional to the Young’s modulus ( Y s ) of the substrate ( Y s = 238 GPa for STO substrate, 44 which is much higher than that of Si ( Y s = 150 GPa) 45 and glass ( Y s = 67.6 GPa) 42 substrates). Thus, one may expect with decreasing Y s the effective piezoelectric coefficient of the film increases, as is observed.…”
Section: Resultsmentioning
confidence: 99%
“…It was found that the larger d 33f value of the PZT film on CNOns/glass than those on CNOns/Si and STO. For these relatively thin films a large fraction of the clamping is due to the substrate, that is expected to be proportional to the Young’s modulus ( Y s ) of the substrate ( Y s = 238 GPa for STO substrate, 44 which is much higher than that of Si ( Y s = 150 GPa) 45 and glass ( Y s = 67.6 GPa) 42 substrates). Thus, one may expect with decreasing Y s the effective piezoelectric coefficient of the film increases, as is observed.…”
Section: Resultsmentioning
confidence: 99%
“…For our case, where the film is much thinner than the substrate ( t f ≪ t s )30–32 and the electrode/film covers the whole active area, a simple formula is valid: where L is the distance from the anchoring point, E f and E s , are Young's moduli of the substrate and the film respectively and t s is thicknesses of the substrate. In the d 31 calculations, the Young's modulus of the substrate (Nb doped bulk STO) is E s = 238 GPa 33. Equation (1) is applicable for all samples studied in this work.…”
Section: Methodsmentioning
confidence: 99%
“…Experiments of Paufler et al [18] for different crystal orientations resulted in a hardness ranging from H = 11.5 GPa to 12.2 GPa. Young's modulus can also be derived from single crystal data of the elastic compliance [19] giving E <100> = 1/s 11 = (265 ± 2) GPa for the <100> direction of SrTiO 3 .…”
Section: Measurementmentioning
confidence: 98%
“…This is related to an increasing possibility of encountering material defects or a surface layer hardened by polishing [21]. Paufler et al [18] gave the similar argument that mobile dislocations are only available in macroscopic indentation depths, so that SrTiO 3 is stronger at the nanometer scale. We observed a maximum hardness at a depth of about 135 nm nearly independent of the applied electric field.…”
Section: Measurementmentioning
confidence: 98%