2018
DOI: 10.1107/s2052520618012970
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Fundamental aspects of symmetry and order parameter coupling for martensitic transition sequences in Heusler alloys

Abstract: The combinations of phase transitions which occur in Heusler alloys in terms of order parameters and symmetry have been analysed using a group theoretical approach. It is shown how this approach can be applied to relevant examples.

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Cited by 16 publications
(3 citation statements)
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“…The formalities of how this coupling leads to the observed pattern have been set out in full in the literature (see, for example, [28]). The structural/electronic order parameter, Q E , has the symmetry properties of irreducible representation Γ + 3 of the parent L2 1 cubic state with space group Fm 3m and couples bilinearly with tetragonal and orthorhombic shear strains, i.e., as λeQ [7,8,29]. Here, softening and stiffening of the combination of elastic constants C 11 -C 12 arises by bilinear coupling between Q E and the symmetry breaking shear strain of DO 22 -type tetragonal state (space group I4/mmm, con rmed by the diffraction pattern shown in gure S1).…”
Section: Resultsmentioning
confidence: 99%
“…The formalities of how this coupling leads to the observed pattern have been set out in full in the literature (see, for example, [28]). The structural/electronic order parameter, Q E , has the symmetry properties of irreducible representation Γ + 3 of the parent L2 1 cubic state with space group Fm 3m and couples bilinearly with tetragonal and orthorhombic shear strains, i.e., as λeQ [7,8,29]. Here, softening and stiffening of the combination of elastic constants C 11 -C 12 arises by bilinear coupling between Q E and the symmetry breaking shear strain of DO 22 -type tetragonal state (space group I4/mmm, con rmed by the diffraction pattern shown in gure S1).…”
Section: Resultsmentioning
confidence: 99%
“…In another type of symmetry analysis related to incommensurate structures, Carpenter and Howard modelled the coupling between different types (concretely: first‐order (structural) and second‐order (shear‐strain)) of order parameters whose coupling has led to martensitic transition sequences in Heusler alloys. Despite the fact that they have perfectly applied the group–subgroup technique frequently used in the descriptions of structural phase transitions in modulated crystal structures, the use of line group theoretical methods is absent in this study, too.…”
Section: A Note On Possible Future Experimental Applicationsmentioning
confidence: 99%
“…Lastly, the Heusler compounds were taken into consideration due to their various properties including the half-metals [1,2], spin-gapless half-metals, spin-gapless semiconductors [3,4] and topology insulators [5,6]. These compounds have several crystal structures such as full-Heusler (X 2 YZ) [7,8], half-Heusler (XYZ) [9,10], DO3 [11,12] and tetragonal [13,14] which all of these structures have the same crystallography structures.…”
Section: Introductionmentioning
confidence: 99%