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Overview no. 61 On geometric criteria for low interfacial energy
Affiliation:1. Mechanical and Materials Engineering, University of Nebraska–Lincoln, Lincoln, NE 68588, USA;2. Department of Materials Science and Engineering, and Department of Mechanical Engineering, College of Engineering, University of Michigan, Ann Arbor, MI 48109-2136, USA;1. Marc De Graef, Department of Materials Science and Engineering, Carnegie Mellon University, 5000 Forbes Avenue, Pittsburgh, PA 15213-3890, USA;2. Department of Materials Science and Engineering, Carnegie Mellon University, Pittsburgh, PA 15213, USA;3. CNRS, Arts et Métiers ParisTech, LEM3, F-57000 Metz, France;4. Laboratory of Excellence on Design of Alloy Metals for low-mAss Structures (DAMAS), Université de Lorraine, France
Abstract:A review of geometric criteria for low interfacial energy which have been proposed in the literature is given. These include, (i) low reciprocal volume density of coincidence sites; (ii) high planar density of coincidence sites, Γ; (iii) high Γ at constant interplanar spacing, d; (iv) large d; and (v) high density of locked-in rows of atoms. These criteria are then tested against available experimental results which include measurements of: (a) interfacial energy; (b) rotations of crystallites on flat crystal substrates; (c) boundary faceting; (d) boundary dissociation; and (e) observations of grain boundary dislocations. No support for the general usefulness of criteria (i), (ii), (iv) and (v) is found. In all cases, significant numbers of results violating these criteria are found or else it is demonstrated that their range of validity is undefined, and, hence, their predictive power is highly limited. Criterion (iii) is found to apply for a limited number of cases involving metal/metal or ionic/ionic interfaces but fails for metal/ionic interfaces. Further testing and consideration of this criterion seems called for. It is concluded that no general and useful criterion for low energy can be enshrined in a simple geometric framework. Any understanding of the variations of interfacial energy must take account of the atomic structure and the details of the bonding at the interface.
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