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Poling Field Dependence of Ferroelectric Domains in Tetragonal Lead Zirconate Titanate Ceramics
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The ferroelectric domain structures of tetragonal lead zirconate
titanate (PZT) ceramics were evaluated by investigating the poling field (E)
dependence of the planar coupling factor (k
p) and the relative intensity of
X-ray diffraction (002) peak, I
002. Fifteen typical domain configurations were
proposed. Furthermore, we selected the two patterns which make a domain
configuration model with 90° and 180° domains. It was thought that the
change in domain structure due to poling could be explained by calculating
the change in area of domain for each axis. Therefore, the total number of
domains oriented along the c axis was estimated from using the relationship
between I
002, k
p, the normalized polarization and E. Using our domain
configuration model, it was confirmed that there were two peaks
corresponding to 90° domain rotation and one peak corresponding to 180°
domain switching. After the 90° domain rotation occurred, the domains along
the c axis were changed mainly by 180° switching. As a result, the degree of
90° domain rotation decreased and that of 180° domain switching increased.
Our study on domain structures in bulk ceramics is useful for understanding
the degradation characteristics of PZT thin films.
Title: Poling Field Dependence of Ferroelectric Domains in Tetragonal Lead Zirconate Titanate Ceramics
Description:
The ferroelectric domain structures of tetragonal lead zirconate
titanate (PZT) ceramics were evaluated by investigating the poling field (E)
dependence of the planar coupling factor (k
p) and the relative intensity of
X-ray diffraction (002) peak, I
002.
Fifteen typical domain configurations were
proposed.
Furthermore, we selected the two patterns which make a domain
configuration model with 90° and 180° domains.
It was thought that the
change in domain structure due to poling could be explained by calculating
the change in area of domain for each axis.
Therefore, the total number of
domains oriented along the c axis was estimated from using the relationship
between I
002, k
p, the normalized polarization and E.
Using our domain
configuration model, it was confirmed that there were two peaks
corresponding to 90° domain rotation and one peak corresponding to 180°
domain switching.
After the 90° domain rotation occurred, the domains along
the c axis were changed mainly by 180° switching.
As a result, the degree of
90° domain rotation decreased and that of 180° domain switching increased.
Our study on domain structures in bulk ceramics is useful for understanding
the degradation characteristics of PZT thin films.
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