1992
DOI: 10.1109/14.155796
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Effect of space charge on micro-macro domain transition of PLZT

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Cited by 23 publications
(7 citation statements)
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“…A layer of Pt/Ti bottom electrode was evaporated on p-type silicon substrate with a resistivity of [5][6][7][8][9] cm. Then a layer of PbZr 0.5 Ti 0.48 O 3 (PZT) film was fabricated on the bottom electrode by the PLD technique.…”
Section: Methodsmentioning
confidence: 99%
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“…A layer of Pt/Ti bottom electrode was evaporated on p-type silicon substrate with a resistivity of [5][6][7][8][9] cm. Then a layer of PbZr 0.5 Ti 0.48 O 3 (PZT) film was fabricated on the bottom electrode by the PLD technique.…”
Section: Methodsmentioning
confidence: 99%
“…From the electric point of view, it can be considered as an insulator because of its large bandgap (3.5 eV), especially as a pure dielectric in its bulk domain. Charge carriers (defects, charged particles etc) in domains move and separate under a dc field making the effective field on microdomains and polar microregions smaller than the applied field [9]. This process is called polarization.…”
Section: Radiation Theory For Pzt Filmmentioning
confidence: 99%
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“…One is that a large quantity of space charges would be generated in an FE film during irradiation [3,7]. Under the bias of an external electric field, these charges will redistribute and move to domain interfaces [9]; finally, they will be captured by defects of the interfaces and form parasitic dipoles whose direction is opposite to that of the external field, and aligned with that of spontaneous polarization. This means that the parasitic dipoles can result in the increasing of remanent polarization.…”
Section: Changes Of Hysteresis Loop During Irradiationmentioning
confidence: 99%