Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect

The complexity of Ni-Mn-Ga single crystal originates from the interplay between ferromagnetic domain structure and ferroelastic twinned microstructure. Magnetic domain structure in the vicinity of single twin boundary was studied using magneto-optical indicator film and magnetic force microscopy tec...

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Main Authors: V. Kopecký, L. Fekete, O. Perevertov, O. Heczko
Format: Article
Language:English
Published: AIP Publishing LLC 2016-05-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4943363
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spelling doaj-91e167424ba24d35b0da4ce720441eb02020-11-24T20:51:55ZengAIP Publishing LLCAIP Advances2158-32262016-05-0165056208056208-610.1063/1.4943363070691ADVChanges in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effectV. Kopecký0L. Fekete1O. Perevertov2O. Heczko3Department of Functional Materials, Institute of Physics ASCR, Na Slovance 1999/2, 182 21 Prague 8, Czech RepublicDepartment of Functional Materials, Institute of Physics ASCR, Na Slovance 1999/2, 182 21 Prague 8, Czech RepublicDepartment of Functional Materials, Institute of Physics ASCR, Na Slovance 1999/2, 182 21 Prague 8, Czech RepublicDepartment of Functional Materials, Institute of Physics ASCR, Na Slovance 1999/2, 182 21 Prague 8, Czech RepublicThe complexity of Ni-Mn-Ga single crystal originates from the interplay between ferromagnetic domain structure and ferroelastic twinned microstructure. Magnetic domain structure in the vicinity of single twin boundary was studied using magneto-optical indicator film and magnetic force microscopy technique. The single twin boundary of Type I was formed mechanically and an initial magnetization state in both variants were restored by local application of magnetic field (≈40 kA/m). The differently oriented variants exhibited either stripe or labyrinth magnetic domain pattern in agreement with the uniaxial magnetocrystalline anisotropy of the martensite. The twin boundary was then moved by compressive or tensile stress. The passage of the boundary resulted in the formation of granular or rake domains, respectively. Additionally, the specific magnetic domains pattern projected by twin boundary gradually vanished during twin boundary motion.http://dx.doi.org/10.1063/1.4943363
collection DOAJ
language English
format Article
sources DOAJ
author V. Kopecký
L. Fekete
O. Perevertov
O. Heczko
spellingShingle V. Kopecký
L. Fekete
O. Perevertov
O. Heczko
Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect
AIP Advances
author_facet V. Kopecký
L. Fekete
O. Perevertov
O. Heczko
author_sort V. Kopecký
title Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect
title_short Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect
title_full Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect
title_fullStr Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect
title_full_unstemmed Changes in magnetic domain structure during twin boundary motion in single crystal Ni-Mn-Ga exhibiting magnetic shape memory effect
title_sort changes in magnetic domain structure during twin boundary motion in single crystal ni-mn-ga exhibiting magnetic shape memory effect
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2016-05-01
description The complexity of Ni-Mn-Ga single crystal originates from the interplay between ferromagnetic domain structure and ferroelastic twinned microstructure. Magnetic domain structure in the vicinity of single twin boundary was studied using magneto-optical indicator film and magnetic force microscopy technique. The single twin boundary of Type I was formed mechanically and an initial magnetization state in both variants were restored by local application of magnetic field (≈40 kA/m). The differently oriented variants exhibited either stripe or labyrinth magnetic domain pattern in agreement with the uniaxial magnetocrystalline anisotropy of the martensite. The twin boundary was then moved by compressive or tensile stress. The passage of the boundary resulted in the formation of granular or rake domains, respectively. Additionally, the specific magnetic domains pattern projected by twin boundary gradually vanished during twin boundary motion.
url http://dx.doi.org/10.1063/1.4943363
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AT lfekete changesinmagneticdomainstructureduringtwinboundarymotioninsinglecrystalnimngaexhibitingmagneticshapememoryeffect
AT operevertov changesinmagneticdomainstructureduringtwinboundarymotioninsinglecrystalnimngaexhibitingmagneticshapememoryeffect
AT oheczko changesinmagneticdomainstructureduringtwinboundarymotioninsinglecrystalnimngaexhibitingmagneticshapememoryeffect
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