1971
DOI: 10.1080/00150197108234104
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The influence of the shape of domains on the ferroelectric hysteresis loop

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Cited by 16 publications
(10 citation statements)
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“…4(b-f)) is prominent and is a common feature, and has been previously reported for alanine and H 3 PO 4 Table 1 Crystallographic and morphological parameters, piezoelectric (d 22 ) and pyroelectric (l) coefficients of TGS and TGSP crystals doped (ATGSP) crystals [18]. The elongation in the shape of the domains may be attributed to the linear and volume defects introduced in the crystal due to H 3 PO 4 doping [19]. In comparison to TGS, the TGSP crystals have exhibited a wide variation in the domain sizes and also show a higher domain density (Table 1) in agreement with earlier observations [7].…”
Section: Structural Characterizationmentioning
confidence: 79%
“…4(b-f)) is prominent and is a common feature, and has been previously reported for alanine and H 3 PO 4 Table 1 Crystallographic and morphological parameters, piezoelectric (d 22 ) and pyroelectric (l) coefficients of TGS and TGSP crystals doped (ATGSP) crystals [18]. The elongation in the shape of the domains may be attributed to the linear and volume defects introduced in the crystal due to H 3 PO 4 doping [19]. In comparison to TGS, the TGSP crystals have exhibited a wide variation in the domain sizes and also show a higher domain density (Table 1) in agreement with earlier observations [7].…”
Section: Structural Characterizationmentioning
confidence: 79%
“…This property obviously also affects the overall macroscopic response of piezoelectric materials. Janta (1971) developed a model to estimate the influence of the domain shape and different loading frequencies on the amplitude of the hysteresis loop as well as on the coercive electric field. The reported results indicate that the coercive electric field is solely slightly affected by the shape of the domain structure itself.…”
Section: Introductionmentioning
confidence: 99%
“…For the sake of simplicity, a fixed number of nucleation sites N1 and the same extended area a (t) for every domain are assumed for a unit surface area. In a thin layer of ferroelectric material, the total extended area per unit area of the electrode (in the same sense as AexCt) in Equation (12) if Ao = 1 is assumed) for the positive half-period of a sinusoidal electric field can be expressed as (Janta, 1971):…”
Section: Basic Theories Of Polarization Reversal Dynamicsmentioning
confidence: 99%
“…Nucleation and forward wall motion are neglected. It has been shown that in the case of cylindrical domains, an expression similar to Equation (15) may be obtained (Janta, 1971). It should be noted that the above polarization reversal theories are only valid for single crystals.…”
Section: Basic Theories Of Polarization Reversal Dynamicsmentioning
confidence: 99%