Stochastic Approach to Plasticity and Yield in Amorphous Solids

TL;DR

This paper investigates the probability distribution of strain intervals between plastic events in amorphous solids, revealing discontinuous transitions at specific strains and establishing scaling relations between key exponents.

Contribution

It introduces a stochastic framework linking the distribution of plastic strain intervals to the eigenvalues of the Hessian, highlighting discontinuous transitions during plasticity.

Findings

Distributions of strain intervals and eigenvalues are discontinuous functions of strain.

Two distinct transitions occur in slowly quenched amorphous solids at specific strains.

The second transition is absent in quickly quenched amorphous solids due to the lack of a stress peak.

Abstract

We focus on the probability distribution function (pdf) $P(\Delta \gamma; \gamma)$ where $\Delta \gamma$ are the {\em measured} strain intervals between plastic events in an athermal strained amorphous solids, and $\gamma$ measures the accumulated strain. The tail of this distribution as $\Delta \gamma\to 0$ (in the thermodynamic limit) scales like $\Delta \gamma^\eta$. The exponent $\eta$ is related via scaling relations to the tail of the pdf of the eigenvalues of the {\em plastic modes} of the Hessian matrix $P(\lambda)$ which scales like $\lambda^\theta$, $\eta=(\theta-1)/2$. The numerical values of $\eta$ or $\theta$ can be determined easily in the unstrained material and in the yielded state of plastic flow. Special care is called for in the determination of these exponents between these states as $\gamma$ increases. Determining the $\gamma$ dependence of the pdf $P(\Delta \gamma; \gamma)$ can shed important light on plasticity and yield. We conclude that the pdf's of both $\Delta \gamma$ and $\lambda$ are not continuous functions of $\gamma$. In slowly quenched amorphous solids they undergo two discontinuous transitions, first at $\gamma=0^+$ and then at the yield point $\gamma=\gamma_{_{\rm Y}}$ to plastic flow. In quickly quenched amorphous solids the second transition is smeared out due to the non existing stress peak before yield. The nature of these transitions and scaling relations with the system size dependence of $\langle \Delta \gamma\rangle$ are discussed.