2009 IEEE Pulsed Power Conference 2009
DOI: 10.1109/ppc.2009.5386292
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High temperature and high energy density dielectric materials

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Cited by 44 publications
(35 citation statements)
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“…Nevertheless, this image clearly revealed a well-ordered lamellar structure corresponding to the layer-bylayer assembly. We also note that the interface is clean and atomically sharp without interfacial dead layer between (Ti 0.87 O 2 ) n and SrRuO 3 . Such an interface quality realizes the full potential of high-¬ nanosheets.…”
Section: Resultsmentioning
confidence: 67%
“…Nevertheless, this image clearly revealed a well-ordered lamellar structure corresponding to the layer-bylayer assembly. We also note that the interface is clean and atomically sharp without interfacial dead layer between (Ti 0.87 O 2 ) n and SrRuO 3 . Such an interface quality realizes the full potential of high-¬ nanosheets.…”
Section: Resultsmentioning
confidence: 67%
“…Take various above mentioned analysis results into comprehensive consideration, when x = 10%, the energy storage density and energy efficiency reached 0.797 J/cm 3 and 92.5%, respectively, which were the maximum values in this study. If the single layer thickness was less than 5 μm in capacitors, with refined homogeneous grain and decreased grain size, it was expected to achieve higher energy density (>6 J/cm 3 ) …”
Section: Resultsmentioning
confidence: 99%
“…For instance, the weakly coupled relaxor behavior of 0.7 BaTiO 3 ‐0.3 BiScO 3 ceramics results in an energy density of approximately 6.1 J/cm 3 in a field of 730 kV/cm . The C0G‐type linear dielectric 0.8 CaZrO 3 ‐0.2 CaTiO 3 ceramics have shown energy densities of up to 5 J/cm 3 and breakdown strengths of 650‐1750 kV/cm. Mn‐doped 0.8 CaTiO 3 ‐0.2 CaHfO 3 ceramics display a higher energy density of 9.5 J/cm 3 .…”
Section: Introductionmentioning
confidence: 99%