Abstract

Crystal defects induce strong distortions in diffraction patterns. A single defect alone can yield strong and fine features that are observed in high-resolution diffraction experiments such as coherent X-ray diffraction. The case of face-centred cubic nanocrystals is studied numerically and the signatures of typical defects close to Bragg positions are identified. Crystals of a few tens of nanometres are modelled with realistic atomic potentials and 'relaxed' after introduction of well defined defects such as pure screw or edge dislocations, or Frank or prismatic loops. Diffraction patterns calculated in the kinematic approximation reveal various signatures of the defects depending on the Miller indices. They are strongly modified by the dissociation of the dislocations. Selection rules on the Miller indices are provided, to observe the maximum effect of given crystal defects in the initial and relaxed configurations. The effect of several physical and geometrical parameters such as stacking fault energy, crystal shape and defect position are discussed. The method is illustrated on a complex structure resulting from the simulated nanoindentation of a gold nanocrystal.

Highlights

  • The microstructure of materials plays a large role in determining their physical properties (Hull & Bacon, 2001; Hirth & Lothe, 1968)

  • For a direct analysis of coherent X-ray diffraction (CXD) patterns we suggested that a single decade of intensity is sufficient to show a distortion or a splitting of the Bragg peak, while two decades are needed for the modification of fringes due to a stacking fault

  • We carried out a detailed numerical analysis of the effect of defects in f.c.c. nanocrystals on their CXD patterns in the

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Summary

Introduction

The microstructure of materials plays a large role in determining their physical properties (Hull & Bacon, 2001; Hirth & Lothe, 1968). Transmission electron microscopy (TEM) is routinely used to produce various imaging contrasts of dislocations in real space by selecting pertinent diffraction vectors, according to well known invisibility criteria (Wiliams & Carter, 1996). It has atomic resolution and can evidence individual crystal defects. The use of TEM is hindered by strong experimental constraints on the sample environment and thickness. These restrictions are relaxed for X-rays, which have a great potential for the study of defects in crystals

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