1999
DOI: 10.1177/1045389x9901000302
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Domain Wall Theory for Ferroelectric Hysteresis

Abstract: This paper addresses the modeling of hysteresis in ferroelectric materials through consideration of domain wall bending and translation. The development is considered in two steps. In the rst step, dielectric constitutive relations are obtained through consideration of Langevin, Ising spin and preferred orientation theory with domain interactions incorporated through mean eld relations. This yields a model for the anhysteretic polarization that occurs in the absence of domain wall pinning. In the second step, … Show more

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Cited by 67 publications
(52 citation statements)
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“…The model is based on the so-called "limiting" (or anhysteretic) curve, derived analytically on the basis of Weiss theory and Boltzmann statistics [60][61][62][63][64][65][66][67]. If in the polycrystalline ferroelectric material were no mechanisms for locking the walls of the domains, then after the removal of the electric field, the polarization of the representative volume would be zero.…”
Section: The Giles-atherton Modelmentioning
confidence: 99%
“…The model is based on the so-called "limiting" (or anhysteretic) curve, derived analytically on the basis of Weiss theory and Boltzmann statistics [60][61][62][63][64][65][66][67]. If in the polycrystalline ferroelectric material were no mechanisms for locking the walls of the domains, then after the removal of the electric field, the polarization of the representative volume would be zero.…”
Section: The Giles-atherton Modelmentioning
confidence: 99%
“…Techniques for choosing α to avoid oversmoothing solutions as well as a solution algorithm for (26) can be found in Vogel [33]. We do not consider the convergence of approximate parameters as discretization levels are increased but instead let the infinite-dimensional analysis motivate potential sources of ill-posedness in the discrete least-squares formulations.…”
Section: Parameter Identification Problemmentioning
confidence: 99%
“…For a fixed parameter value q, the modelled polarization P ( E k ; q) = Aq at the measured field values E k was determined via (12). The residual 1 2 P ( E k ; q) − P k 2 = 1 2 Aq − P k 2 was subsequently minimized in the unregularized minimization problem (25) and regularized formulation (26).…”
Section: Materials Characterizationmentioning
confidence: 99%
See 1 more Smart Citation
“…As detailed by , there exists a wide range of techniques for modeling the hysteresis inherent to ferroelectric (e.g., PZT, PMN below the glass transition temperature), ferromagnetic (e.g., Terfenol-D, steel), and ferroelastic (e.g., SMA) compounds. Three modeling classes which provide unified characterization frameworks for ferroelectric, ferromagnetic, and ferroelastic -collectively termed as ferroic -compounds are domain wall models (Jiles and Atherton, 1986;Smith and Hom, 1999;Massad and Smith, 2003), Preisach models (Preisach, 1935;Hughes and Wen, 1997;Robert et al, 2001), and homogenized energy models Seelecke and Mu¨ller, 2004). The domain wall models are efficient to implement but require a priori knowledge of turning points to guarantee closure of biased minor loops.…”
Section: Introductionmentioning
confidence: 99%