Abstract
Icosahedral quasicrystals spontaneously form from the melt in simulations of Al--Cu--Fe alloys. We model the interatomic interactions using oscillating pair potentials tuned to the specific alloy system based on a database of density functional theory (DFT)-derived energies and forces. Favored interatomic separations align with the geometry of icosahedral motifs that overlap to create face-centered icosahedral order on a hierarchy of length scales. Molecular dynamics simulations, supplemented with Monte Carlo steps to swap chemical species, efficiently sample the configuration space of our models, which reach up to 9846 atoms. Exchanging temperatures of independent trajectories (replica exchange) allows us to achieve thermal equilibrium at low temperatures. By optimizing structure and composition we create structures whose DFT energies reach to within $\sim$2 meV/atom of the energies of competing crystal phases. Free energies obtained by adding contributions due to harmonic and anharmonic vibrations, chemical substitution disorder, phasons, and electronic excitations, show that the quasicrystal becomes stable against competing phases at temperatures above 600K. The average structure can be described succinctly as a cut through atomic surfaces in six-dimensional space that reveal specific patterns of preferred chemical occupancy. Atomic surface regions of mixed chemical occupation demonstrate the proliferation of phason fluctuations, which can be observed in real space through the formation, dissolution and reformation of large scale icosahedral motifs -- a picture that is hidden from diffraction refinements due to averaging over the disorder and consequent loss of information concerning occupancy correlations.
Highlights
IntroductionExcellent descriptions of their average structures are possible in terms of cuts through higher-dimensional periodic lattices obtained by single-crystal diffraction refinements [4]
Since the discovery of quasicrystals as a distinct phase of matter [1], and recognition of their quasiperiodicity [2], two fundamental questions remain to be definitively answered: Where are the atoms [3]? What stabilizes their quasiperiodic order? Excellent descriptions of their average structures are possible in terms of cuts through higher-dimensional periodic lattices obtained by single-crystal diffraction refinements [4]
Three important ingredients enable the success of our atomistic simulations: realistic density functional theory (DFT)-derived interatomic interactions; appropriately sized simulation cells with periodic boundary conditions; efficient hybrid Monte Carlo/molecular dynamics augmented by replica exchange
Summary
Excellent descriptions of their average structures are possible in terms of cuts through higher-dimensional periodic lattices obtained by single-crystal diffraction refinements [4]. Quasicrystalline structures can only be reliably equilibrated at high temperatures; these models contain ambiguous atomic positions with uncertain occupation and chemistry. They omit important correlations in the case of mixed or partial occupation, and they omit atomic vibrations and diffusion. As regards their thermodynamic stability, local icosahedral motifs are clearly favored energetically. Local preference need not force long-range quasiperiodicity, as is illustrated by the prevalence of periodic “approximants,”
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