Abstract

Martensitic phase transitions in which there is a group–subgroup relationship between the parent and product structures are driven by combinations of soft-mode and electronic instabilities. These have been analysed from the perspective of symmetry, by considering possible order parameters operating with respect to a parent structure which has space group Im{\bar 3} m. Heusler structures with different stoichiometries are derived by operation of order parameters belonging to irreducible representations {\rm H}^{+}_{1}and P1 to describe the atomic ordering configurations. Electronic instabilities are ascribed to an order parameter belonging to the Brillouin zone centre, \Gamma^{+}_{3}, which couples with shear strains to give tetragonal and orthorhombic distortions. An additional zone centre order parameter, with \Gamma^{+}_{5} symmetry, is typically a secondary order parameter but in some cases may drive a transition. Soft-mode instabilities produce commensurate and incommensurate structures for which the order parameters have symmetry properties relating to points along the Σ line of the Brillouin zone for the cubic I lattice. The electronic and soft-mode order parameters have multiple components and are coupled in a linear–quadratic manner as \lambda q_{\Gamma}q_{\Sigma}^{2}. As well as providing comprehensive tables setting out the most important group–subgroup relationships and the order parameters which are responsible for them, examples of NiTi, RuNb, Ti50Ni50−x Fe x , Ni2+x Mn1−x Ga and Ti50Pd50−x Cr x are used to illustrate practical relevance of the overall approach. Variations of the elastic constants of these materials can be used to determine which of the multiple order parameters is primarily responsible for the phase transitions that they undergo.

Highlights

  • Ferroelastic phase transitions in functional oxides are accompanied by symmetry-breaking shear strains which typically fall in the range $0.1–5% (Salje, 1993; Carpenter et al, 1998)

  • The primary objective of the present paper is to present a group theoretical treatment of martensitic materials which can be derived from the simplest b.c.c. parent structure with space group Im3"m

  • Most of the observed product structures appear to be understandable in terms of separate order parameters which have symmetry properties related to the Brillouin zone centre (À point in Fig. 1) and points along one of the h110i* directions of the reciprocal lattice for Im3"m structures (Æ line of Fig. 1)

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Summary

Introduction

Ferroelastic phase transitions in functional oxides are accompanied by symmetry-breaking shear strains which typically fall in the range $0.1–5% (Salje, 1993; Carpenter et al, 1998). Most can be understood in terms of some structural or electronic instability with a driving order parameter that gives rise to the strain by coupling. Depends on symmetry and is determined by rigorous group theoretical rules. The same symmetry rules apply to coupling between two or more order parameters in materials with multiple instabilities, and the form of this coupling determines how, for example, multiferroic materials may respond to an external electric or magnetic field. As set out for the cases of transitions in perovskites driven by combinations of octahedral tilting, ferroelectric displacements, atomic ordering and cooperative Jahn–Teller distortions, the group theory program ISOTROPY (Stokes et al, 2007) has allowed such relationships to be tabulated even for the most.

B2 L21 DO3 B32a X Y
Parent structures
Martensite structures
33 Pna21 4 P21
Primary and secondary order parameters
Some examples of real materials
Ti50Pd50ÀxCrx
Patterns of elastic anomalies due to strain–order parameter coupling
Conclusions
Full Text
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