2020
DOI: 10.1016/j.jeurceramsoc.2020.06.038
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Remarkably enhanced energy storage properties of lead-free Ba0.53Sr0.47TiO3 thin films capacitors by optimizing bottom electrode thickness

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Cited by 14 publications
(17 citation statements)
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“…With the rapid developments in microelectronics and micro-electromechanical systems, there is a great demand for integrated energy devices at a miniaturized scale. Perovskite ferroelectric (FE)-based film capacitors have attracted a great deal of attention due to their high power density (ultrafast charge and discharge speed), superior thermal and mechanical stability, and long work life. , With a large dielectric constant ε r and relatively small remnant polarization P r , BaTiO 3 -based film capacitors have raised a research upsurge internationally in recent years. Generally speaking, charge–discharge efficiency and energy densities of a FE film capacitor can be calculated from its characteristic P – E curve by the following equations: the efficiency η is defined as , while the recyclable energy density , the charged energy density , and the energy loss density W loss = W c – W rec , where P r is the remnant polarization (polarization at zero electric field), E is the applied electric field, and P max is the electric polarization under the maximum electric field E max .…”
Section: Introductionmentioning
confidence: 99%
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“…With the rapid developments in microelectronics and micro-electromechanical systems, there is a great demand for integrated energy devices at a miniaturized scale. Perovskite ferroelectric (FE)-based film capacitors have attracted a great deal of attention due to their high power density (ultrafast charge and discharge speed), superior thermal and mechanical stability, and long work life. , With a large dielectric constant ε r and relatively small remnant polarization P r , BaTiO 3 -based film capacitors have raised a research upsurge internationally in recent years. Generally speaking, charge–discharge efficiency and energy densities of a FE film capacitor can be calculated from its characteristic P – E curve by the following equations: the efficiency η is defined as , while the recyclable energy density , the charged energy density , and the energy loss density W loss = W c – W rec , where P r is the remnant polarization (polarization at zero electric field), E is the applied electric field, and P max is the electric polarization under the maximum electric field E max .…”
Section: Introductionmentioning
confidence: 99%
“…Pan et al obtained a large W rec of ∼112 J/cm 3 and η ∼80% in the BiFeO 3 –BaTiO 3 –SrTiO 3 solid-solution films deposited on Nb:SrTiO 3 substrates at 700 °C via a polymorphic nanodomain design. Zhu et al reported W rec ∼51.2 J/cm 3 with efficiency η ∼54.3% in Ba 0.53 Sr 0.47 TiO 3 thin-film capacitors prepared at 700 °C on SrTiO 3 substrates. Through domain engineering, Cheng et al achieved a giant W rec of ∼133 J/cm 3 in thin films and η ∼96% in thick films of epitaxial Ba­(Zr 0.2 Ti 0.8 )­O 3 , which were deposited on SrTiO 3 substrates at 650 °C.…”
Section: Introductionmentioning
confidence: 99%
“…Here, Ba 0.53 Sr 0.47 TiO 3 (BST) films were deposited on LSMO bottom electrodes of different thicknesses on a (001) SrTiO 3 (STO). The BDS and J r increased from 3075 to 4822 kV/cm and 31 to 51 J/cm 3 , respectively, for an LSMO thickness ranging from 30 to 140 nm [ 169 ]. Increase in LSMO thickness ensured a smooth interface and better stress relaxation that profited the ED properties.…”
Section: Tuning Energy Density By Processing Methodsmentioning
confidence: 99%
“…High Curie temperature BFO‐, NBT‐, KNN‐, BIT‐based materials with notable electromechanical coupling factor/piezoelectric coefficient values, high polarization etc, can be achieved using suitable site engineering, sintering aids or a new synthesis technique etc 6,7 . These materials are difficult to sinter using ordinary conditions.…”
Section: Introductionmentioning
confidence: 99%
“…Extensive literature review reveals that the improvement in such properties can be achieved with suitable site engineering. Examples of solid solutions include but not limited to those mentioned here: BST, BCT, BZT, (Ba 1− x Sr x )(Ti 1− y Sn y )O 3 (BSTS), (1 − x )Ba(Ti 0.8 Zr 0.2 )O 3 − x (Ba 0.7 Ca 0.3 )TiO 3 [BZT‐BCT] 4‐8,12‐18 …”
Section: Introductionmentioning
confidence: 99%