2003
DOI: 10.1016/j.materresbull.2003.09.020
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Dielectric characteristics of Mg-replaced Pb[(Zn1/3Ta2/3)0.2(Zn1/3Nb2/3)0.6Ti0.2]O3 ceramics

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Cited by 1 publication
(2 citation statements)
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“…When the temperature is higher than the Curie temperature, the ferroelectric material will behave as a paraelectric. Therefore, the response of polarization to electric field becomes a nonlinear line rather than a hysteresis loop when the temperature increases to 600 • C. The dependence of the remnant polarization and coercive field on the temperature in figure 2 is consistent with the analytic predictions from Landau theory and many experimental observations [3][4][5][6][7][8][9][10]. room temperature in figures 3(a1)-(a3).…”
Section: Simulation Methodologysupporting
confidence: 83%
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“…When the temperature is higher than the Curie temperature, the ferroelectric material will behave as a paraelectric. Therefore, the response of polarization to electric field becomes a nonlinear line rather than a hysteresis loop when the temperature increases to 600 • C. The dependence of the remnant polarization and coercive field on the temperature in figure 2 is consistent with the analytic predictions from Landau theory and many experimental observations [3][4][5][6][7][8][9][10]. room temperature in figures 3(a1)-(a3).…”
Section: Simulation Methodologysupporting
confidence: 83%
“…Due to the complex nature of real experiments, the effects of temperature on the properties of ferroelectric material are inconsistent in different experiments. Based on the conventional mixed-oxide technique, Khemakhema et al [3] measured the polarization hysteresis loops of the BaTi 0.975 (Zn 1/3 Nb 2/3 ) 0.025 O 3 ceramic at different temperatures and found that the remnant polarization and coercive field decrease when the temperature increases from 280 to 330 K. Similar results have been found by many researchers [4][5][6][7][8][9][10], and are reasonable from the thermodynamics point of view.…”
Section: Introductionsupporting
confidence: 68%