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dc.contributor.authorCarpenter, Michael A.
dc.contributor.authorEvans, Donald
dc.contributor.authorSchiemer, J. A.
dc.contributor.authorWolf, Thomas
dc.contributor.authorAdelmann, P.
dc.contributor.authorBöhmer, A. E.
dc.contributor.authorMeingast, C.
dc.contributor.authorDutton, S. E.
dc.contributor.authorMukherjee, P.
dc.contributor.authorHoward, Christopher J.
dc.date.accessioned2019-03-21T14:39:38Z
dc.date.available2019-03-21T14:39:38Z
dc.date.created2019-02-13T11:38:14Z
dc.date.issued2019
dc.identifier.citationJournal of Physics: Condensed Matter. 2019, 31 155401-?.nb_NO
dc.identifier.issn0953-8984
dc.identifier.urihttp://hdl.handle.net/11250/2591133
dc.description.abstractThe hypothesis that strain has a permeating influence on ferroelastic, magnetic and superconducting transitions in 122 iron pnictides has been tested by investigating variations of the elastic and anelastic properties of a single crystal of Ba(Fe0.957Co0.043)2As2 by resonant ultrasound spectroscopy as a function of temperature and externally applied magnetic field. Non-linear softening and stiffening of C66 in the stability fields of both the tetragonal and orthorhombic structures has been found to conform quantitatively to the Landau expansion for a pseudoproper ferroelastic transition which is second order in character. The only exception is that the transition occurs at a temperature (TS ≈ 69K) ~10K above the temperature at which C66 would extrapolate to zero (T∗ cE ≈ 59K). An absence of anomalies associated with antiferromagnetic ordering below TN ≈ 60K implies that coupling of the magnetic order parameter with shear strain is weak. It is concluded that linear-quadratic coupling between the structural/electronic and antiferromagnetic order parameters is suppressed due to the effects of local heterogeneous strain fields arising from the substitution of Fe by Co. An acoustic loss peak at ~50–55K is attributed to the influence of mobile ferroelastic twin walls that become pinned by a thermally activated process involving polaronic defects. Softening of C66 by up to ~6% below the normal—superconducting transition at Tc ≈ 13K demonstrates an effective coupling of the shear strain with the order parameter for the superconducting transition which arises indirectly as a consequence of unfavourable coupling of the superconducting order parameter with the ferroelastic order parameter. Ba(Fe0.957Co0.043)2As2 is representative of 122 pnictides as forming a class of multiferroic superconductors in which elastic strain relaxations underpin almost all aspects of coupling between the structural, magnetic and superconducting order parameters and of dynamic properties of the transformation microstructures they contain.nb_NO
dc.language.isoengnb_NO
dc.publisherIOP Publishingnb_NO
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleFerroelasticity, anelasticity and magnetoelastic relaxation in Co-doped iron pnictide: Ba(Fe0.957Co0.043)2As2nb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionpublishedVersionnb_NO
dc.source.pagenumber155401-?nb_NO
dc.source.volume31nb_NO
dc.source.journalJournal of Physics: Condensed Matternb_NO
dc.identifier.doi10.1088/1361-648X/aafe29
dc.identifier.cristin1676875
dc.description.localcodeOriginal content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.nb_NO
cristin.unitcode194,66,35,0
cristin.unitnameInstitutt for materialteknologi
cristin.ispublishedfalse
cristin.fulltextoriginal
cristin.qualitycode1


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