1994
DOI: 10.1143/jpsj.63.1031
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A Theory of D-E Hysteresis Loop Based on the Avrami Model

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Cited by 240 publications
(142 citation statements)
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“…The problem of analysis is that polycrystalline ferroelectrics typically exhibit a complicated dispersive switching response which cannot be interpreted in terms of the classical nucleation and growth theory often referred to as the Kolmogorov-Avrami-Ishibashi (KAI) model. 3 To obtain microscopic parameters providing the macroscopic switching process, more sophisticated theories are required, which account for a statistical distribution of local switching times in a system. [4][5][6][7][8] To this end, the inhomogeneous field mechanism (IFM) model is used in this paper, which derives the distribution of times from the distribution of randomly distributed local field values.…”
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confidence: 99%
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“…The problem of analysis is that polycrystalline ferroelectrics typically exhibit a complicated dispersive switching response which cannot be interpreted in terms of the classical nucleation and growth theory often referred to as the Kolmogorov-Avrami-Ishibashi (KAI) model. 3 To obtain microscopic parameters providing the macroscopic switching process, more sophisticated theories are required, which account for a statistical distribution of local switching times in a system. [4][5][6][7][8] To this end, the inhomogeneous field mechanism (IFM) model is used in this paper, which derives the distribution of times from the distribution of randomly distributed local field values.…”
mentioning
confidence: 99%
“…Traditionally, the polarization switching kinetics is described by the KAI model, 3 which suggests a temporal dependence of the reversed polarization as follows:…”
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confidence: 99%
“…143,144 It is noted that the removal of the electric field leads to a decay of 65 % in the polarization of BNT-0.25ST, indicating that although in BNT-0.25ST is higher than in BNT-0.28ST, it still has considerably lower values than its . Domain switching is a time-dependent kinetic process 73,[441][442][443] , while a first order phase transition is an infinitely fast discontinuous process occurring in the terahertz range. 39,48,444 Therefore, a feasible way to give insight into the nature of the phase transition and the origin of the volume change is to perform polarization and strain measurements at a rate faster than the time domain where the switching processes should occur.…”
Section: Quasi-static Large Signal Propertiesmentioning
confidence: 99%
“…242 Although, the induced phase transition is of first order, the subsequent switching of the domains formed is a kinetic process that requires time. 73,[441][442][443] Therefore, it is expected that each sub-cycle allows a gradual increase in the amount of switching. The gradual increase of the values after each sub-cycle is analogous to the increase of the values observed with increasing field strength in pulse experiments ( Figure 5.46).…”
Section: Quasi-static Large Signal Propertiesmentioning
confidence: 99%
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