International
Tables for Crystallography Volume D Physical properties of crystals Edited by A. Authier © International Union of Crystallography 2006 |
International Tables for Crystallography (2006). Vol. D. ch. 3.3, pp. 443-444
Section 3.3.10.9. Coherent and incoherent twin interfaces
a
Institut für Kristallographie, Rheinisch–Westfälische Technische Hochschule, D-52056 Aachen, Germany, and bMineralogisch-Petrologisches Institut, Universität Bonn, D-53113 Bonn, Germany |
At the start of Section 3.3.10, the terms compatible and incompatible twin boundaries were introduced and clearly defined. There exists another pair of terms, coherent and incoherent interfaces, which are predominantly used in bicrystallography and metallurgy for the characterization of grain boundaries, but less frequently in mineralogy and crystallography for twin boundaries. These terms, however, are defined in different and often rather diffuse ways, as the following examples show.
The above definitions have one feature in common: coherent twin boundaries are planar interfaces, which are either rational or irrational, as stated explicitely by Christian (1965, p. 332). Beyond this, the various definitions are rather vague. In particular, they do not distinguish between ferroelastic and non-ferroelastic (strictly merohedral) twins and do not consider the twin displacement vector discussed in Section 3.3.10.4.
As an attempt to fill this gap, the following elucidations of the term `coherence' are suggested here. These proposals are based on the definitions summarized above, as well as on the concepts of compatibility of interfaces (Sections 3.3.10.1 and 3.3.10.3) and on the notion of twin displacement vector (Section 3.3.10.4).
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It is apparent from these discussions of coherent twin interfaces that several features have to be taken into account, some readily available by experiments and observations, whereas others require geometric models (lattice matching) or even physical models (structure matching), including determination of twin displacement vectors t.
The definitions of coherence, as treated here, often do not satisfactorily agree with reality. Two examples are given:
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These examples demonstrate that the above formal definitions of coherence, based on geometrical viewpoints alone, are not always satisfactory and require consideration of individual cases.
With these discussions of rather subtle features of twin interfaces, this chapter on twinning is concluded. It was our aim to present this rather ancient topic in a way that progresses from classical concepts to modern considerations, from three dimensions to two and from macroscopic geometrical arguments to microscopic atomistic reasoning. Macroscopic derivations of orientation and contact relations of the twin partners (twin laws, as well as twin morphologies and twin genesis) were followed by lattice considerations and structural implications of twinning. Finally, the physical background of twinning was explored by means of the analysis of twin interfaces, their structural and energetic features. It is this latter aspect which in the future is most likely to bring the greatest progress toward the two main goals, an atomistic understanding of the phenomenon `twinning' and the ability to predict correctly its occurrence and non-occurrence.
All considerations in this chapter refer to analysis of twinning in direct space. The complementary aspect, the effect of twinning in reciprocal space, lies beyond the scope of the present treatment and, hence, had to be omitted. This concerns in particular the recognition and characterization of twinning in diffraction experiments, especially by X-rays, as well as the consideration of the problems that twinning, especially merohedral twinning, may pose in single-crystal structure determination (cf. Buerger, 1960a). Several powerful computer programs for the solution of these problems exist. For a case study, see Herbst-Irmer & Sheldrick (1998).
References
Barrett, C. S. & Massalski, T. B. (1966). Structure of metals, 3rd edition, especially pp. 406–414. New York: McGraw-Hill.Google ScholarBuerger, M. J. (1960a). Crystal-structure analyses, especially ch. 3. New York: Wiley.Google Scholar
Cahn, R. W. (1954). Twinned crystals. Adv. Phys. 3, 202–445.Google Scholar
Chalmers, B. (1959). Physical metallurgy, especially ch. 4.4. New York: Wiley.Google Scholar
Christian, J. W. (1965). The theory of transformations in metals and alloys, especially chs. 8 and 20. Oxford: Pergamon.Google Scholar
Cottrell, A. H. (1955). Theoretical structural metallurgy, 2nd edition, especially ch. 14.5. London: Edward Arnold.Google Scholar
Friedel, J. (1964). Dislocations, especially ch. 6. Oxford: Pergamon.Google Scholar
Herbst-Irmer, R. & Sheldrick, G. M. (1998). Refinement of twinned structures with SHELXL97. Acta Cryst. B54, 443–449.Google Scholar
Kelly, A. & Groves, G. W. (1970). Crystallography and crystal defects, especially chs. 10 and 12.5. London: Longman.Google Scholar
Klassen-Neklyudova, M. V. (1964). Mechanical twinning of crystals. New York: Consultants Bureau.Google Scholar
Porter, D. A. & Easterling, K. E. (1992). Phase transformations in metals and alloys, 2nd edition, especially ch. 3. London: Chapman & Hall.Google Scholar
Putnis, A. (1992). Introduction to mineral sciences, especially chs. 7.3 and 12.4. Cambridge University Press.Google Scholar
Shektman, V. Sh. (1993). Editor. The real structure of high-Tc superconductors, especially ch. 3, Twins and structure of twin boundaries, by I. M. Shmyt'ko & V. Sh. Shektman. Berlin: Springer.Google Scholar
Sutton, A. P. & Balluffi, R. W. (1995). Interfaces in crystalline materials, Section 1.5, pp. 25–41. Oxford: Clarendon Press.Google Scholar
Van Bueren, H. G. (1961). Imperfections in crystals, especially chs. 13.4 and 19. Amsterdam: North-Holland.Google Scholar