LaAlO3: A substrate material with unusual ferroelastic propeties

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dc.contributor.author Kustov,S.
dc.contributor.author Liubimova, Iu.
dc.contributor.author Salje, E.K.H.
dc.date.accessioned 2020-03-18T07:22:48Z
dc.identifier.uri http://hdl.handle.net/11201/151058
dc.description.abstract [eng] Twin boundary dynamics in LaAlO3 is associated with non-linear anelasticity. Ultrasonic studies of non-linear twin boundary dynamics between 80 and 520 K show that cooling substrates from temperatures near the ferroelastic transition at 813 K generate three characteristic thermal regimes with different non-linear dynamics. Twin boundaries are initially highly mobile. Anelastic strain amplitudes versus stress are power law distributed with an exponent of 2.5. No de-pinning was found down to elastic strain amplitudes of ε0 ∼ 10−7. The power law is gradually replaced between 370 K and 280 K by few large singularities (jerks) due to massive rearrangements of the domain structure for ε0 larger than ca. 5 × 10−5. At lower temperatures, the domain structure is pinned with well-defined thresholds for de-pinning. The de-pinning is not accompanied by global rearrangements of twin patterns below room temperature. Unexpectedly, the low-temperature critical de-pinning strain amplitude decreases with decreasing temperature, which may indicate an additional, so far unknown phase transition near 40 K.
dc.format application/pdf
dc.relation.isformatof Reproducció del document publicat a: https://doi.org/10.1063/1.5017679
dc.relation.ispartof Applied Physics Letters, 2018, vol. 112, num. 042902, p. 1-5
dc.subject.classification 53 - Física
dc.subject.other 53 - Physics
dc.title LaAlO3: A substrate material with unusual ferroelastic propeties
dc.type info:eu-repo/semantics/article
dc.type info:eu-repo/semantics/publishedVersion
dc.date.updated 2020-03-18T07:22:48Z
dc.date.embargoEndDate info:eu-repo/date/embargoEnd/2026-12-31
dc.embargo 2026-12-31
dc.rights.accessRights info:eu-repo/semantics/embargoedAccess
dc.identifier.doi https://doi.org/10.1063/1.5017679


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