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The coercive field is determined as (0.8 ± 0.1) Oe.
They also have a coercive field smaller than 1 mT.
At this stage, changes in the coercive field are determined by the crystalline grain coarsening.
These arrays demonstrate unusual properties including an oscillatory dependence of the coercive field on film thickness.
We found significant increase in the coercive field for the sample with the smallest antidot spacing.
More interestingly, an increase in the coercive field Ec and remanent polarization Pr is observed.
This is supported by the derivative of the hysteresis loops, which show two components, one with a high coercive field and another with a small coercive field.
The obtained maximum coercive field is about 250 Oe at 300 K.
For the as prepared film, the derivative shows a peak centred at 19 Oe, corresponding to its coercive field.
As the annealing temperature increased, the remnant polarization value increased whereas the coercive field was reduced.
8/65/35 PLZT is characterized under stress and electric field loading above the coercive field.
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