Properties of the density of shear transformations in driven amorphous solids

preprint2020arXivOpen access

Abstract

The strain load ΔγΔγ that triggers consecutive avalanches is a key observable in the slow deformation of amorphous solids. Its temporally averaged value ⟨Δγ⟩\langle Δγ\rangle displays a non-trivial system-size dependence that constitutes one of the distinguishing features of the yielding transition. Details of this dependence are not yet fully understood. We address this problem by means of theoretical analysis and simulations of elastoplastic models for amorphous solids. An accurate determination of the size dependence of ⟨Δγ⟩\langle Δγ\rangle leads to a precise evaluation of the steady-state distribution of local distances to instability xx. We find that the usually assumed form P(x)∼xθP(x)\sim x^θ (with θθ being the so-called pseudo-gap exponent) is not accurate at low xx and that in general P(x)P(x) tends to a system-size-dependent \textit{finite} limit as x→0x\to 0. We work out the consequences of this finite-size dependence standing on exact results for random-walks and disclosing an alternative interpretation of the mechanical noise felt by a reference site. We test our predictions in two- and three-dimensional elastoplastic models, showing the crucial influence of the saturation of P(x)P(x) at small xx on the size dependence of ⟨Δγ⟩\langle Δγ\rangle and related scalings.

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