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This relation provides the volume conservation in strained Terfenol-D. It holds for the macroscopic deformations resulting from magnetization reorientations in a model polycrystal, where the crystallites have a cubic lattice with the same spatial orientation and a randomly oriented magnetization with fixed magnitude.
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This relation provides the volume conservation in strained Terfenol-D. It holds for the macroscopic deformations resulting from magnetization reorientations in a model polycrystal, where the crystallites have a cubic lattice with the same spatial orientation and a randomly oriented magnetization with fixed magnitude.
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24
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We suppose that the single-domain state can be created in an epitaxial ferroelectric film even at small misfit strains near um =0, where the formation of ferroelastic (non- 180°) domains becomes energetically favorable [10.1103/PhysRevB.73.214103
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The strain sensitivities S1 and S2 of the in-plane polarization components are not further discussed in this paper. These sensitivities differ from zero in the monoclinic r phase and the orthorhombic aa phase and give rise to nonzero transverse ME coefficients α13 and α23.
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The strain sensitivities S1 and S2 of the in-plane polarization components are not further discussed in this paper. These sensitivities differ from zero in the monoclinic r phase and the orthorhombic aa phase and give rise to nonzero transverse ME coefficients α13 and α23.
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