2014
DOI: 10.1134/s1063774514060145
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Formation of unusual nonferroic domains in TeO2 single crystals under external electric field

Abstract: The formation of unusual slowly relaxing domains under an external dc electric field has been revealed in paratellurite (TeO 2 ) crystals. These domains differ from those arising in ferroics (ferromagnets, ferroelectrics, ferroelastics, etc.). The effect is characterized by the existence of a threshold field strength (at which domains begin to be formed) and long equilibrium settling times (up to a few hours, depending on the electric field strength). A crystal returns to the initial single domain state also a… Show more

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Cited by 17 publications
(2 citation statements)
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“…This phase transition is a result of oxygen vacancies migration, and the mechanism paves the way for managing the physical properties of materials. Structural changes observed in paratellurite TeO 2 in applied electric field [22][23][24][25] also are associated with oxygen vacancy migration. Contrary to SrTiO 3 , the TeO 2 crystal intrinsically possesses piezoelectric properties and its symmetry is described by a non-symmorphic space group, which provides a set of forbidden reflections in the reciprocal space.…”
Section: Introductionmentioning
confidence: 89%
“…This phase transition is a result of oxygen vacancies migration, and the mechanism paves the way for managing the physical properties of materials. Structural changes observed in paratellurite TeO 2 in applied electric field [22][23][24][25] also are associated with oxygen vacancy migration. Contrary to SrTiO 3 , the TeO 2 crystal intrinsically possesses piezoelectric properties and its symmetry is described by a non-symmorphic space group, which provides a set of forbidden reflections in the reciprocal space.…”
Section: Introductionmentioning
confidence: 89%
“…These techniques make it possible to obtain qualitative information about the defect structure of crystals, and they have already been used for the study of various objects, including the natural faces (edges) of grown crystals, 20) and samples under ultrasonic loading 21,22) and electric fields. 23) We used a laboratory X-ray tube with a molybdenum anode as the radiation source. The slits and monochromator crystalsymmetric Si(400) for RC measurements and asymmetric Si(440) for X-ray topographywere used to select only the Mo Kα 1 spectral line λ = 0.7039 Å.…”
Section: Experimental Methodsmentioning
confidence: 99%