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Domain reversal in stoichiometric prepared by vapor transport equilibration
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10.1063/1.1814436
/content/aip/journal/apl/85/19/10.1063/1.1814436
http://aip.metastore.ingenta.com/content/aip/journal/apl/85/19/10.1063/1.1814436

Figures

Image of FIG. 1.
FIG. 1.

Composition dependence of forward and reverse coercive fields, and the Curie temperature in lithium tantalate single crystals.

Image of FIG. 2.
FIG. 2.

(a) Hysteresis loops for 1st experimental cycle and 22nd experimental cycle of stoichiometric single crystals (SLT-VTE). Cycling frequency was . (b) Coercive fields and spontaneous polarization measured in 22 successive experimental cycles. Coercive fields and coercive field do not change with cycling.

Image of FIG. 3.
FIG. 3.

The switching time as a function of field , where the negative sign is for forward poling and the positive sign for reverse poling. The measured internal field .

Tables

Generic image for table
Table I.

A comparison of congruent (CLT), near-stoichiometric (NSLT-CZ), and stoichiometric (SLT-VTE) crystals. Measurements not referenced below are from this study.

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/content/aip/journal/apl/85/19/10.1063/1.1814436
2004-11-08
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Domain reversal in stoichiometric LiTaO3 prepared by vapor transport equilibration
http://aip.metastore.ingenta.com/content/aip/journal/apl/85/19/10.1063/1.1814436
10.1063/1.1814436
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