In this work, (Pb1 − 1.5xLax)(Zr0.80Ti0.20)O3 (abbreviated as PLZT, x = 0.01, 0.03, 0.04, 0.06, 0.07) ceramics are designed on the base of chemical composition modification and prepared by solid-state reaction. The effect of composition, temperature, and hydrostatic pressure on ferroelectric-antiferroelectric (FE-AFE) phase transition is investigated. It is obtained that phase transition from ferroelectric rhombohedral phase to antiferroelectric tetragonal phase as a function of La3+ doping content, especially, the PLZT ceramics of x = 0.04, 0.06, and 0.07 are the coexistence of FE-AFE phase. It is also found the FE-AFE phase transition driven by increased temperature in poled PLZT ceramics (x = 0.04, 0.06). Furthermore, static charges density (Pr) of PLZT (x = 0.04, 0.06) are decreased from 29.11 µC/cm2 and 31.52 µC/cm2 to 19.76 {\mu }C/cm2, 6.45 {\mu }C/cm2 under 400 MPa hydrostatic pressure due to the pressure-induced FE-AFE phase transition. The depolarization rates are 32.12% and 79.54%, respectively. Meanwhile, the phase diagram of (Pb1 − 1.5xLax)(Zr0.80Ti0.20)O3 ceramics is acquired roughly. These results provide guidance for the engineering application of (Pb1 − 1.5xLax)(Zr0.80Ti0.20)O3 ceramics.

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Posted 06 May, 2020
Posted 06 May, 2020
In this work, (Pb1 − 1.5xLax)(Zr0.80Ti0.20)O3 (abbreviated as PLZT, x = 0.01, 0.03, 0.04, 0.06, 0.07) ceramics are designed on the base of chemical composition modification and prepared by solid-state reaction. The effect of composition, temperature, and hydrostatic pressure on ferroelectric-antiferroelectric (FE-AFE) phase transition is investigated. It is obtained that phase transition from ferroelectric rhombohedral phase to antiferroelectric tetragonal phase as a function of La3+ doping content, especially, the PLZT ceramics of x = 0.04, 0.06, and 0.07 are the coexistence of FE-AFE phase. It is also found the FE-AFE phase transition driven by increased temperature in poled PLZT ceramics (x = 0.04, 0.06). Furthermore, static charges density (Pr) of PLZT (x = 0.04, 0.06) are decreased from 29.11 µC/cm2 and 31.52 µC/cm2 to 19.76 {\mu }C/cm2, 6.45 {\mu }C/cm2 under 400 MPa hydrostatic pressure due to the pressure-induced FE-AFE phase transition. The depolarization rates are 32.12% and 79.54%, respectively. Meanwhile, the phase diagram of (Pb1 − 1.5xLax)(Zr0.80Ti0.20)O3 ceramics is acquired roughly. These results provide guidance for the engineering application of (Pb1 − 1.5xLax)(Zr0.80Ti0.20)O3 ceramics.

Figure 1

Figure 2

Figure 3

Figure 4

Figure 5

Figure 6
This is a list of supplementary files associated with this preprint. Click to download.
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