2022
DOI: 10.1111/jace.18616
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High piezoelectricity with broad temperature insensitivity in BiScO3–PbTiO3‐based piezoceramics

Abstract: The surge of interest in searching for high-temperature piezoceramics has proved that BiScO 3 -PbTiO 3 ceramics with high piezoelectric constant and high Curie temperature are promising for high-temperature nondestructive inspection (NDT) applications. However, their inferior temperature stability limits the applications. In this paper, 0.365BiScO 3 -0.635(Pb 1-3x/2 Bi x ) (Ti 0.99 Zn 0.01 )O 3 (BS-xBPZnT) system has been investigated by doping Bi ions to A-site and Zn ions to B-site based on the lattice disto… Show more

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Cited by 15 publications
(20 citation statements)
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“…S6(c)†), which was relevant to the hierarchical nanodomains with flexible domain walls in the multiphase existence. 32 Moreover, the ε r P s as a function of temperature was calculated, and the results are shown in Fig. S6(d) †.…”
Section: Resultsmentioning
confidence: 99%
“…S6(c)†), which was relevant to the hierarchical nanodomains with flexible domain walls in the multiphase existence. 32 Moreover, the ε r P s as a function of temperature was calculated, and the results are shown in Fig. S6(d) †.…”
Section: Resultsmentioning
confidence: 99%
“…To characterize the degree of diffusion of the BSPT-LWx ceramics, the modified Curie-Weiss relationship, and the parameters of ΔT m and ΔT dif were applied. 2 As shown in Equations (1-3): where C is the Curie-Weiss constant and γ the is diffusion coefficient. The value of γ is 1 for normal ferroelectrics and a real relaxor ferroelectric has the γ value of 2.…”
Section: Resultsmentioning
confidence: 99%
“…With an increase in Li + /W 6+ content, the dielectric peaks show broadening and the temperature of the maximum ε r ( T m ) shows a clear shift with frequency, suggesting a diffuse phase transition. To characterize the degree of diffusion of the BSPT–LW x ceramics, the modified Curie–Weiss relationship, and the parameters of Δ T m and Δ T dif were applied 2 . As shown in Equations (): 1/εrgoodbreak−1/εmgoodbreak=TTmγ/C,$$\begin{equation}1/{\varepsilon _r} - 1/{\varepsilon _m} = {\left( {T - {T_m}} \right)^\gamma }/C,\end{equation}$$ normalΔTmbadbreak=Tmfalse(1MHzfalse)goodbreak−Tmfalse(1kHzfalse),$$\begin{equation}\Delta {T_m} = {T_{m(1 MHz)}} - {T_{m(1 kHz)}},\end{equation}$$ normalΔTdiffalse(10kHzfalse)badbreak=T0.9εmaxfalse(10kHzfalse)goodbreak−Tεmaxfalse(10kHzfalse),$$\begin{equation}\Delta {T_{dif(10 kHz)}} = {T_{0.9\varepsilon max(10 kHz)}} - {T_{\varepsilon max(10 kHz)}},\end{equation}$$where C is the Curie–Weiss constant and γ the is diffusion coefficient.…”
Section: Resultsmentioning
confidence: 99%
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