about
Existence of isostatic, maximally random jammed monodisperse hard-disk packingsThe structural origin of the hard-sphere glass transition in granular packing.Dense colloidal fluids form denser amorphous sedimentsBond orientational order in liquids: Towards a unified description of water-like anomalies, liquid-liquid transition, glass transition, and crystallization: Bond orientational order in liquids.Spontaneous crystallization in athermal polymer packings.Droplet-droplet interactions investigated using a combination of electrochemical and dynamic light scattering techniques. The case of water/BHDC/benzene:n-heptane system.Attractive particle interaction forces and packing density of fine glass powders.Minkowski tensor shape analysis of cellular, granular and porous structures.Glass transition of dense fluids of hard and compressible spheres.Simple effective rule to estimate the jamming packing fraction of polydisperse hard spheres.Crystallization time scales for polydisperse hard-sphere fluids.Pore Size Distribution in Granular Material Microstructure.Crowding-based rheological model for suspensions of rigid bimodal-sized particles with interfering size ratios.Relevance of packing to colloidal self-assembly.Subjamming transition in binary sphere mixtures.Universal behaviour of the glass and the jamming transitions in finite dimensions for hard spheres.Equilibrium Sampling of Hard Spheres up to the Jamming Density and Beyond.Fundamental challenges in packing problems: from spherical to non-spherical particles.Random-close packing limits for monodisperse and polydisperse hard spheres.Equilibrium theory of the hard sphere fluid and glasses in the metastable regime up to jamming. I. Thermodynamics.Jammed spheres: Minkowski tensors reveal onset of local crystallinity.Temperature-pressure scaling for air-fluidized grains near jamming.Equation of state and jamming density for equivalent bi- and polydisperse, smooth, hard sphere systems.Glass transition and random close packing above three dimensions.Tuning jammed frictionless disk packings from isostatic to hyperstatic.Effect of long-range repulsive Coulomb interactions on packing structure of adhesive particles.Equilibrium equation of state of a hard sphere binary mixture at very large densities using replica exchange Monte Carlo simulations.Fractal heterogeneous media.Shear-Rate-Independent Diffusion in Granular Flows.Geometrical frustration in two dimensions: idealizations and realizations of a hard-disk fluid in negative curvature.Hard disks on the hyperbolic plane.Hard-sphere crystallization gets rarer with increasing dimension.Structural evolution in the packing of uniform spheres.Understanding the ideal glass transition: lessons from an equilibrium study of hard disks in a channel.Upper bound on the Edwards entropy in frictional monodisperse hard-sphere packings.Pushing the glass transition towards random close packing using self-propelled hard spheres.The other entropyDirect Determination of the Size of Basins of Attraction of Jammed SolidsNumerical detection of the Gardner transition in a mean-field glass formerUniversal Microstructure and Mechanical Stability of Jammed Packings
P2860
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P2860
description
2007 nî lūn-bûn
@nan
2007年の論文
@ja
2007年学术文章
@wuu
2007年学术文章
@zh
2007年学术文章
@zh-cn
2007年学术文章
@zh-hans
2007年学术文章
@zh-my
2007年学术文章
@zh-sg
2007年學術文章
@yue
2007年學術文章
@zh-hant
name
Why is random close packing reproducible?
@en
Why is random close packing reproducible?
@nl
type
label
Why is random close packing reproducible?
@en
Why is random close packing reproducible?
@nl
prefLabel
Why is random close packing reproducible?
@en
Why is random close packing reproducible?
@nl
P2860
P1476
Why is random close packing reproducible?
@en
P2860
P304
P356
10.1103/PHYSREVLETT.99.155501
P407
P577
2007-10-09T00:00:00Z
P698
P818
cond-mat/0701343