On the rigidity of a hard sphere glass near random close packing

dc.creatorBrito, Carolina
dc.creatorWyart, Matthieu
dc.date2005-12-09
dc.date2006-10-27
dc.date.accessioned2026-07-07T06:53:15Z
dc.date.available2026-07-07T06:53:15Z
dc.descriptionWe study theoretically and numerically the microscopic cause of the mechanical stability of hard sphere glasses near their maximum packing. We show that, after coarse-graining over time, the hard sphere interaction can be described by an effective potential which is exactly logarithmic at the random close packing $ϕ_c$. This allows to define normal modes, and to apply recent results valid for elastic networks: mechanical stability is a non-local property of the packing geometry, and is characterized by some length scale $l^*$ which diverges at $ϕ_c$ [1, 2]. We compute the scaling of the bulk and shear moduli near $ϕ_c$, and speculate on the possible implications of these results for the glass transition.
dc.description7 pages, 4 figures. Figure 4 had a wrong unit in abscissa, which was corrected
dc.identifierhttps://arxiv.org/abs/cond-mat/0512197
dc.identifierhttp://arxiv.org/abs/cond-mat/0512197
dc.identifierEurophys. Lett., 76 (1), pp. 149-155 (2006)
dc.identifierdoi:10.1209/epl/i2006-10238-x
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/105515
dc.subjectSoft Condensed Matter
dc.subjectDisordered Systems and Neural Networks
dc.subjectStatistical Mechanics
dc.titleOn the rigidity of a hard sphere glass near random close packing
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