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      Dynamical correlations near dislocation jamming

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          Abstract

          Dislocation assemblies exhibit a jamming or yielding transition at a critical external shear stress value \(\sigma=\sigma_c\). Nevertheless the nature of this transition has not been ascertained. Here we study the heterogeneous and collective nature of dislocation dynamics within a crystal plasticity model close to \(\sigma_c\), by considering the first-passage properties of the dislocation dynamics. As the transition is approached in the moving phase, the first passage time distribution exhibits scaling, and a related peak {\it dynamical} susceptibility \(\chi_4^*\) diverges as \(\chi_4^* \sim (\sigma-\sigma_c)^{-\alpha}\), with \(\alpha \approx 1.1\). We relate this scaling to an avalanche description of the dynamics. While the static structural correlations are found to be independent of the external stress, we identify a diverging dynamical correlation length \(\xi_y\) in the direction perpendicular to the dislocation glide motion.

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          Direct experimental evidence of a growing length scale accompanying the glass transition

          Understanding glass formation is a challenge because the existence of a true glass state, distinct from liquid and solid, remains elusive: Glasses are liquids that have become too viscous to flow. An old idea, as yet unproven experimentally, is that the dynamics becomes sluggish as the glass transition approaches because increasingly larger regions of the material have to move simultaneously to allow flow. We introduce new multipoint dynamical susceptibilities to estimate quantitatively the size of these regions and provide direct experimental evidence that the glass formation of molecular liquids and colloidal suspensions is accompanied by growing dynamic correlation length scales.
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            How to simulate the quasistationary state

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              Rate-dependent avalanche size in athermally sheared amorphous solids.

              We perform an extensive numerical study of avalanche behavior in a two-dimensional Lennard-Jones glass at T = 0, sheared at finite strain rates gamma[over]. From the finite size analysis of stress fluctuations and of transverse diffusion we show that flip-flip correlations remain relevant at all realistic strain rates. We predict that, in steady flow, the avalanche size scales as gamma[over];{-1/d}, with d the space dimension.
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                Author and article information

                Journal
                12 February 2010
                Article
                10.1103/PhysRevLett.105.015501
                1002.2587
                958914fe-50d4-4ec8-b830-77fa2cd71845

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                Phys. Rev. Lett. 105, 015501 (2010)
                4 pages, 5 figures
                cond-mat.stat-mech cond-mat.mtrl-sci

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