Abstract

Athermal systems across a large range of length scales, ranging from foams and granular bead packings to crumpled metallic sheets, exhibit slow stress relaxation when compressed. Experimentally they show a non-monotonic stress response when decompressed somewhat after an initial compression, i.e., under a two-step, Kovacs-like protocol. It turns out that from this response one can tell for how long the system was in a compressed state, suggesting an interpretation as a memory effect. In this paper we use a model of an athermal jammed solid, specifically a binary mixture of soft harmonic particles, to explore this phenomenon through in silico experiments. Using extensive simulations under conditions analogous to those in experiment, we observe identical phenomenology in the stress response under a two-step protocol. Our model system also recovers the behavior under a more recently studied three-step protocol, which consists of a compression followed by a decompression and then a final compression. We show that the observed response in both two-step and three-step protocols can be understood using linear response theory. In particular, a linear scaling with age for the two-step protocol arises generically for slow linear responses with power law or logarithmic decay and does not in itself point to any underlying aging dynamics.

Highlights

  • Memory in the context of physical systems refers to the ability to encode, access, and erase signatures of past history in the state of a system [1]

  • We first demonstrate that our simulations lie in the linear response limit, and we show that using linear response theory (LRT) we can correctly predict the observed phenomenology via Eqs. (7) and (8)

  • In this paper we demonstrate that a model athermal solid made of a binary mixture of soft particles can serve as a canonical model for understanding the non-monotonic response seen recently in a diverse type of athermal systems subjected to multistep variations of the control parameter

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Summary

Protocols

To explore the memory-like response we deform the system using three different protocols. The protocols are named according to the number of times in which the control parameter h(t ) is changed instantaneously

One-step protocol
Two-step protocol
Three-step protocol
LINEAR RESPONSE PREDICTION
RESULTS
DISCUSSION
Fit of simulation data
Nonlinear Response
Full Text
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