2016
DOI: 10.1111/jace.14592
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(Pb,Sm)(Zr,Sn,Ti)O3 Multifunctional Ceramics with Large Electric‐Field‐Induced Strain and High‐Energy Storage Density

Abstract: Recently, the progress of integrated electronics has led to a strong demand for materials and devices with multiple functions. In this study, we achieved Pb0.985Sm0.01 (Zr0.64Sn0.28Ti0.08)O3 (PSZST) multifunctional ceramics which showed simultaneously large electric‐field‐induced strain (0.63%) and high recoverable energy density (1.743 J/cm3) at room temperature. Moreover, the strain and recoverable energy density exhibited a slight frequency fluctuation in the frequency range of 1–10 Hz. Their variations wer… Show more

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Cited by 31 publications
(20 citation statements)
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“…Lead-based dielectric ceramics have already proven to have potential in the application of energy-storage capacitors, with high Wrec (6.4 J/cm -3 ) reported in Ladoped Pb(Zr,Ti)O3-based AFE ceramics fabricated by spark plasma sintering (SPS). [10][11][12][13][14][15] However, environmental issues, health concerns and regulations against hazardous substances in electric and electronic equipment have stimulated research in lead-free materials for energy-storage. [16][17][18] Lead-free energy storage ceramics such as BaTiO3 (BT), (Bi0.5Na0.5)TiO3 (BNT) and (K0.5Na0.5)NbO3…”
Section: Introductionmentioning
confidence: 99%
“…Lead-based dielectric ceramics have already proven to have potential in the application of energy-storage capacitors, with high Wrec (6.4 J/cm -3 ) reported in Ladoped Pb(Zr,Ti)O3-based AFE ceramics fabricated by spark plasma sintering (SPS). [10][11][12][13][14][15] However, environmental issues, health concerns and regulations against hazardous substances in electric and electronic equipment have stimulated research in lead-free materials for energy-storage. [16][17][18] Lead-free energy storage ceramics such as BaTiO3 (BT), (Bi0.5Na0.5)TiO3 (BNT) and (K0.5Na0.5)NbO3…”
Section: Introductionmentioning
confidence: 99%
“…According to Pan's theory, the variation (▵ V / V ) in the unit‐cell volume during AFE‐ferroelectric (FE) phase transition process can be expressed by the formula:false(normalΔVfalse/Vfalse)=QnormalhΩP2normalindwhere P ind is the induced polarization by the electric field, Q h is the electrostrictive coefficient, and Ω is the coupling coefficient between the anti‐parallel dipoles in AFEs. It means that more stable AFE phase will lead to larger field‐induced strains . At the same time, the stable AFE phase is also companied by larger AFE‐FE phase switching field (EF), which results in improved energy‐storage density.…”
Section: Introductionmentioning
confidence: 99%
“…3(c) illustrates the capacitance C of PLZST10 versus E. At low field the value of C only increase slightly, but when E approaches 8kV/mm, the value of C grows rapidly due to the AFE-FE phase transition. 16,17 According to the expression of I max and equation (6), the increase of both E and C will result in a rise of increase rate of I max . Above 8 kV/mm, the field-induced FE phase becomes stable.…”
Section: Resultsmentioning
confidence: 99%
“…Generally, the energy density of AFEs is higher than those of FEs and linear dielectrics because the total stored charges can be released due to the absence of any remnant polarization. 3 Many efforts [4][5][6][7] have been made to investigate the energy store performance of these dielectric materials and improve the energy density.…”
Section: Introductionmentioning
confidence: 99%