2010
DOI: 10.5488/cmp.13.23701
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Possibility of soft-matter effects in solids

Abstract: Shape variation under the action of small external fields is a peculiar feature of soft matter. In the present paper we demonstrate a possibility of the analogous shape variation in the solids that combine the properties of antiferro-and ferromagnetic materials and show strong magnetoelastic coupling. The antiferromagnetic subsystem provides a macroscopic deformation of a sample in the external magnetic field while the ferromagnetic component ensures high susceptibility of the domain structure. 75.60.Ch, 46.25… Show more

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Cited by 4 publications
(4 citation statements)
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“…Position ξ 0 of the DW center is calculated from the boundary conditions (see below). In (15) we neglect the possible difference between the DW width ξ DW = (1/2) α/K ⊥ in the near-surface region and in the core. Substituting (15) in (11), we obtain the following equation for ϕ…”
Section: A Seed Distribution and Magnetoelastic Chargesmentioning
confidence: 99%
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“…Position ξ 0 of the DW center is calculated from the boundary conditions (see below). In (15) we neglect the possible difference between the DW width ξ DW = (1/2) α/K ⊥ in the near-surface region and in the core. Substituting (15) in (11), we obtain the following equation for ϕ…”
Section: A Seed Distribution and Magnetoelastic Chargesmentioning
confidence: 99%
“…Understanding the mechanisms of the shape effects specific to AFM ordered systems is crucial for optimizing and finetuning the properties of AFM-based devices and clarifying the fundamental questions whether the shape effects reside in AFM with vanishingly small macroscopic magnetization, and which of peculiar AFM properties might depend on the particle shape. For this purpose we investigate the finite-size and shape effects in AFM particles, regardless of their macroscopic magnetization, combining two previously shown statements: i) the shape effects in AFM materials may originate from the long-range fields of "magnetoelastic" charges due to spontaneous magnetostriction below the Néel temperature (so called destressing fields) 14 ; ii) "magnetoelastic" charges may arise from the surface magnetic anisotropy 15 . We consider the particles with the characteristic size below the several critical lengths of monodomainization (which, for convenience, are referred to as "nanoparticles").…”
Section: Introductionmentioning
confidence: 99%
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“…In the case of an FM+AFM phase mixture, the inclusions of a new (FM or AFM, depending upon the direction of a phase transition) phase could be considered as elastic dipoles (due to the strain misfit between the FM and AFM phases). In the case of AFM+FM multiferroic, the analogous dipoles arise at the sample surface (see [14] for details). In both cases, the elastic dipoles produce long-range fields that could be taken into account phenomenologically with the use of the destressing energy…”
Section: Combined Influence Of a Magnetic Field And A Stress On The Mmentioning
confidence: 99%