Eur. Phys. J. B 33, 233-247 (2003)
https://doi.org/10.1140/epjb/e2003-00162-y

Elastic interaction between defects in thin and 2D films

¹ Laboratoire de Physique et de Modélisation des Milieux Condensés, Université Joseph Fourier (CNRS), BP 166, 38042 Grenoble Cedex 9, France
² GREPHE, Groupe de Recherche sur les Phénomènes Hors Équilibre, LSP, Université Joseph Fourier (CNRS), Grenoble I, Saint-Martin d'Hères, 38402 Cedex, France

Corresponding author: ^a chaouqi.misbah@ujf-grenoble.fr

Received: 7 October 2002
Published online: 4 June 2003

Abstract

Elastic interactions between defects is investigated at the surface of thin layers, a question on which we have given a brief account [P. Peyla et al. Phys. Rev. Lett. 82, 787 (1999)]. Two isotropic defects do not interact in an unlimited medium, regardless of the spatial dimension, a result which can be shown on the basis of the Gauss theorem in electrostatics. Within isotropic elasticity theory, defects interact only (i) if they are, for example, at a surface (or at least if they feel a boundary), or if their action on the material is anisotropic (e.g. they create a non central force distribution, though the material elasticity is isotropic). It is known that two identical isotropic defects on the surface of a semi-infinite material repel each other. The repulsion law behaves as ( defects separation). We first revisit the Lau-Kohn theory and extend it to anisotropic defects. Anisotropy is found to lead to attraction. We show that in thin films defects may either attract or repel each other depending on the local geometric force distribution caused by the defect. It is shown that the force distribution (or more precisely the forces configuration symmetry) fixes the exponent in the power law (e.g. for a four-fold symmetry ). We discuss the implication of this behaviour in various situations. We treat the interactions in terms of the symmetries associated with the defect. We argue that if the defects are isotropic, then their effective interaction in an unlimited 2D (or a thin film) medium arises from the induced interaction, which behaves as for any defect symmetry. We shall also comment on the contribution to the interaction which arises from flexion of thin films.