Abstract

We show that the distribution of elements $H$ in the Hessian matrices associated with amorphous materials exhibit singularities $P(H) \sim {\lvert H \rvert}^{\gamma}$ with an exponent $\gamma < 0$, as $\lvert H \rvert \to 0$. We exploit the rotational invariance of the underlying disorder in amorphous structures to derive these exponents exactly for systems interacting via radially symmetric potentials. We show that $\gamma$ depends only on the degree of smoothness $n$ of the potential of interaction between the constituent particles at the cut-off distance, independent of the details of interaction in both two and three dimensions. We verify our predictions with numerical simulations of models of structural glass formers. Finally, we show that such singularities affect the stability of amorphous solids, through the distributions of the minimum eigenvalue of the Hessian matrix.

Highlights

  • Understanding and modeling the properties of amorphous solids such as glasses has remained a challenge due to their extreme nonequilibrium nature as well as the underlying disorder in the arrangement of particles [1,2,3,4,5,6,7,8,9,10]

  • We have presented analytic results for the distribution of Hessian elements in disordered amorphous media in 2D and 3D, and verified them with extensive numerical simulations

  • We have shown that the Hessian matrices of amorphous materials display a preponderance of small elements, characterized by a singularity whose strength depends on the smoothness of the interaction potential at the cutoff distance

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Summary

Introduction

Understanding and modeling the properties of amorphous solids such as glasses has remained a challenge due to their extreme nonequilibrium nature as well as the underlying disorder in the arrangement of particles [1,2,3,4,5,6,7,8,9,10]. In this Rapid Communication, we analyze the distributions of Hessian elements in structural glass formers analytically, as well as through numerical simulations. In the case of a disordered arrangement derived from simulations of glass formers as shown, this distribution is continuous, peaking at zero with a marked singularity.

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