The charge dependent hard-sphere model: Polycrystals as low-energy configurations
cond-mat.stat-mech, cond-mat.mes-hall, math-ph, math.MP
Submitted: 2026-09-18
Updated: 2026-09-18
Comments: 46 pages, 12 figures
License: http://creativecommons.org/licenses/by/4.0/
The gist: We investigate the emergence of rigid polycrystalline structures in atomistic ionic particle systems as low-energy configurations.
Terminology
Abstract
We investigate the emergence of rigid polycrystalline structures in atomistic ionic particle systems as low-energy configurations. The interaction between particles of opposite charge is modeled by hard spheres that interact when they are tangential. The interaction between particles of same charge is modeled as a hard repulsion that forces a minimal distance between them. The atomistic energy is frame invariant, and no underlying reference lattice is assumed on the ionic configurations. The asymptotic behavior of configurations with finite surface energy scaling is identified by means of Γ-convergence. The related continuum theory is described by piecewise constant fields that encode the local orientation of the configuration. The limiting energy is local and concentrates at grain boundaries, which correspond to the boundaries of the regions where the underlying configuration has a constant orientation. The limiting energy density is anisotropic and depends on the relative misorientation of the two grains, their translation misfit, and the normal to their interface. Furthermore, we perform a fine analysis of surface energies for solid-solid and solid-vacuum phase transitions and determine energetically favorable orientation mismatches. This relies on a structure result for our grain boundaries, which shows that, due to the rigid setup, interpolating layers near the grain interface are energetically not favorable.
Sources
- Phase-field approximation of sharp-interface energies accounting for lattice symmetry
- Crystallization in the Winterbottom shape and sharp fluctuation laws
- An Energy Estimate for Dislocation Configurations and the Emergence of Cosserat-Type Structures in Metal Plasticity
- Emergence of rigid Polycrystals from atomistic Systems with general Interactions
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