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Phase diagram of elastic spheres

Experiments show that polymeric nanoparticles often self-assemble into several non-close-packed lattices in addition to the face-centered cubic lattice. Here, we explore theoretically the possibility that the observed phase sequences may be associated with the softness of the particles, which are mo...

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Bibliographic Details
Published in:Soft matter 2017-02, Vol.13 (7), p.1463-1471
Main Authors: Athanasopoulou, L, Ziherl, P
Format: Article
Language:English
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Summary:Experiments show that polymeric nanoparticles often self-assemble into several non-close-packed lattices in addition to the face-centered cubic lattice. Here, we explore theoretically the possibility that the observed phase sequences may be associated with the softness of the particles, which are modeled as elastic spheres interacting upon contact. The spheres are described by two finite-deformation theories of elasticity, the modified Saint-Venant-Kirchhoff model and the neo-Hookean model. We determine the range of indentations where the repulsion between the spheres is pairwise additive and agrees with the Hertz theory. By computing the elastic energies of nine trial crystal lattices at densities far beyond the Hertzian range, we construct the phase diagram and find the face- and body-centered cubic lattices as well as the A15 lattice and the simple hexagonal lattice, with the last two being stable at large densities where the spheres are completely faceted. These results are qualitatively consistent with observations, suggesting that deformability may indeed be viewed as a generic property that determines the phase behavior in nanocolloidal suspensions. On compression, elastic spheres push against their neighbors and transform into completely faceted polyhedra. Shape deformation drives phase transitions between different crystal lattices and the phase diagram contains the face- and body-centered cubic lattices as well as the A15 and the simple hexagonal lattice.
ISSN:1744-683X
1744-6848
DOI:10.1039/c6sm02474b