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In a wide temperature range around the phase transition, the<br>intermediate relaxor state comprises a mixture of randomly<br>oriented regions with ordered and disordered electric dipoles<br>embedded in the paraelectric matrix. When the randomly oriented<br>electric dipoles are arranged in antiparallel order, the structure is<br>antiferroelectric. An applied electric field induces the reorientation<br>of electric dipoles in the direction of the field and leads to a<br>transition to the polar state, although the formation of a<br>macrodomain ferroelectric state is inhibited by the nonpolar<br>regions along with the inner local field.
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