A stability-reversibility map unifies elasticity, plasticity, yielding, and jamming in hard sphere glasses

A stability-reversibility map unifies the response of amorphous solids to volume and shear deformations. Amorphous solids, such as glasses, have complex responses to deformations, with substantial consequences in material design and applications. In this respect, two intertwined aspects are important: stability and reversibility. It is crucial to understand, on the one hand, how a glass may become unstable due to increased plasticity under shear deformations, and, on the other hand, to what extent the response is reversible, meaning how much a system is able to recover the original configuration once the perturbation is released. Here, we focus on assemblies of hard spheres as the simplest model of amorphous solids such as colloidal glasses and granular matter. We prepare glass states quenched from equilibrium supercooled liquid states, which are obtained by using the swap Monte Carlo algorithm and correspond to a wide range of structural relaxation time scales. We exhaustively map out their stability and reversibility under volume and shear strains using extensive numerical simulations. The region on the volume-shear strain phase diagram where the original glass state remains solid is bounded by the shear yielding and the shear jamming lines that meet at a yielding-jamming crossover point. This solid phase can be further divided into two subphases: the stable glass phase, where the system deforms purely elastically and is totally reversible, and the marginal glass phase, where it experiences stochastic plastic deformations at mesoscopic scales and is partially irreversible. The details of the stability-reversibility map depend strongly on the quality of annealing of the glass. This study provides a unified framework for understanding elasticity, plasticity, yielding, and jamming in amorphous solids.

[1]  Francesco Concetti The full replica symmetry breaking solution in mean-field spin glass models , 2019, 1911.00557.

[2]  G. Biroli,et al.  Random critical point separates brittle and ductile yielding transitions in amorphous materials , 2018, Proceedings of the National Academy of Sciences.

[3]  P. Wolynes,et al.  Aging, Jamming, and the Limits of Stability of Amorphous Solids. , 2017, The journal of physical chemistry. B.

[4]  A. Nicolas,et al.  Deformation and flow of amorphous solids: Insights from elastoplastic models , 2017, Reviews of Modern Physics.

[5]  M. .. Moore,et al.  Gardner Transition in Physical Dimensions. , 2017, Physical review letters.

[6]  Y. Oono First-Order Phase Transition , 2017 .

[7]  Christopher J. Fullerton,et al.  Density controls the kinetic stability of ultrastable glasses , 2017, 1706.10081.

[8]  Absence of Marginal Stability in a Structural Glass. , 2017, Physical review letters.

[9]  L. Berthier,et al.  Configurational entropy measurements in extremely supercooled liquids that break the glass ceiling , 2017, Proceedings of the National Academy of Sciences.

[10]  G. Biroli,et al.  Liu-Nagel phase diagrams in infinite dimension , 2017, 1704.04649.

[11]  H. Shiba,et al.  Continuum limit of the vibrational properties of amorphous solids , 2017, Proceedings of the National Academy of Sciences.

[12]  G. Parisi,et al.  Shear bands as manifestation of a criticality in yielding amorphous solids , 2017, Proceedings of the National Academy of Sciences.

[13]  S. Sastry,et al.  The yielding transition in amorphous solids under oscillatory shear deformation , 2016, Nature Communications.

[14]  H. Yoshino,et al.  Exploring the complex free-energy landscape of the simplest glass by rheology , 2016, Nature Communications.

[15]  P. Urbani,et al.  Shear Yielding and Shear Jamming of Dense Hard Sphere Glasses. , 2016, Physical review letters.

[16]  S. Franz,et al.  Mean-field avalanches in jammed spheres. , 2016, Physical review. E.

[17]  P. Charbonneau,et al.  Nontrivial Critical Fixed Point for Replica-Symmetry-Breaking Transitions. , 2016, Physical review letters.

[18]  Ludovic Berthier,et al.  Yield Stress Materials in Soft Condensed Matter , 2015, 1502.05281.

[19]  Andrea J. Liu,et al.  Emergent SO(3) Symmetry of the Frictionless Shear Jamming Transition , 2016, 1609.00280.

[20]  Giorgio Parisi,et al.  Glass and Jamming Transitions: From Exact Results to Finite-Dimensional Descriptions , 2016, 1605.03008.

[21]  A. Seguin,et al.  Experimental Evidence of the Gardner Phase in a Granular Glass. , 2016, Physical review letters.

[22]  E. Lerner,et al.  Statistics and Properties of Low-Frequency Vibrational Modes in Structural Glasses. , 2016, Physical review letters.

[23]  H. Jaeger,et al.  Direct observation of dynamic shear jamming in dense suspensions , 2016, Nature.

[24]  Pierfrancesco Urbani,et al.  Breakdown of elasticity in amorphous solids , 2016, Nature Physics.

[25]  I. Procaccia,et al.  Mechanical Yield in Amorphous Solids: A First-Order Phase Transition. , 2016, Physical review letters.

[26]  Ludovic Berthier,et al.  Equilibrium Sampling of Hard Spheres up to the Jamming Density and Beyond. , 2015, Physical review letters.

[27]  Giorgio Parisi,et al.  Growing timescales and lengthscales characterizing vibrations of amorphous solids , 2015, Proceedings of the National Academy of Sciences.

[28]  L. Berthier,et al.  Macroscopic yielding in jammed solids is accompanied by a nonequilibrium first-order transition in particle trajectories. , 2015, Physical review. E.

[29]  Corrado Rainone,et al.  Following the evolution of glassy states under external perturbations: the full replica symmetry breaking solution , 2015, 1512.00341.

[30]  K. Dahmen,et al.  Reversibility and criticality in amorphous solids , 2015, Nature Communications.

[31]  M. Wyart,et al.  Criticality in the Approach to Failure in Amorphous Solids. , 2015, Physical review letters.

[32]  Corrado Rainone,et al.  Following the evolution of hard sphere glasses in infinite dimensions under external perturbations: compression and shear strain. , 2014, Physical review letters.

[33]  Pierfrancesco Urbani,et al.  Gardner transition in finite dimensions , 2015 .

[34]  Matthieu Wyart,et al.  Marginal Stability in Structural, Spin, and Electron Glasses , 2014, 1406.7669.

[35]  H. Yoshino,et al.  Shear modulus of glasses: results from the full replica-symmetry-breaking solution. , 2014, Physical review. E, Statistical, nonlinear, and soft matter physics.

[36]  S. Sastry,et al.  Oscillatory athermal quasistatic deformation of a model glass. , 2013, Physical review. E, Statistical, nonlinear, and soft matter physics.

[37]  Juan J de Pablo,et al.  Ultrastable glasses from in silico vapour deposition. , 2013, Nature materials.

[38]  P. Wolynes,et al.  On the strength of glasses , 2012, Proceedings of the National Academy of Sciences.

[39]  Ludovic Berthier,et al.  Unified study of glass and jamming rheology in soft particle systems. , 2012, Physical review letters.

[40]  R. Behringer,et al.  Jamming by shear , 2011, Nature.

[41]  Gareth H. McKinley,et al.  A review of nonlinear oscillatory shear tests: Analysis and application of large amplitude oscillatory shear (LAOS) , 2011 .

[42]  G. Biroli,et al.  Dynamical Heterogeneities in Glasses, Colloids, and Granular Media , 2011 .

[43]  D. Rodney,et al.  Modeling the mechanics of amorphous solids at different length scale and time scale , 2011, 1107.2022.

[44]  H. Hentschel,et al.  Do athermal amorphous solids exist? , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[45]  A. J. Liu,et al.  Vibrational modes identify soft spots in a sheared disordered packing. , 2010, Physical review letters.

[46]  A. Lemaître,et al.  Heterogeneities in amorphous systems under shear , 2010, 1009.5774.

[47]  Andrea J. Liu,et al.  The Jamming Transition and the Marginally Jammed Solid , 2010 .

[48]  I. Procaccia,et al.  Statistical physics of elastoplastic steady states in amorphous solids: finite temperatures and strain rates. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[49]  R. Candelier,et al.  Creep motion of an intruder within a granular glass close to jamming. , 2009, Physical review letters.

[50]  Andrea Cavagna,et al.  Supercooled liquids for pedestrians , 2009, 0903.4264.

[51]  J. Roux,et al.  Frictionless bead packs have macroscopic friction, but no dilatancy. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[52]  T. Hufnagel,et al.  Mechanical behavior of amorphous alloys , 2007 .

[53]  Weihua Wang,et al.  Bulk metallic glasses , 2004 .

[54]  L. Cipelletti,et al.  Jamming phase diagram for attractive particles , 2001, Nature.

[55]  Paul F. McMillan,et al.  Relaxation in glassforming liquids and amorphous solids , 2000 .

[56]  Andrea J. Liu,et al.  Nonlinear dynamics: Jamming is not just cool any more , 1998, Nature.

[57]  J. Langer,et al.  Dynamics of viscoplastic deformation in amorphous solids , 1997, cond-mat/9712114.

[58]  Daan Frenkel,et al.  Computer simulation of solid-liquid coexistence in binary hard sphere mixtures , 1991 .

[59]  B. Lubachevsky,et al.  Geometric properties of random disk packings , 1990 .

[60]  H. R. Harrison,et al.  Low-dc-field susceptibility of CuMn spin glass , 1979 .

[61]  S. Edwards,et al.  The computer study of transport processes under extreme conditions , 1972 .

[62]  J. Maxwell,et al.  The Scientific Papers of James Clerk Maxwell: On the Calculation of the Equilibrium and Stiffness of Frames , 1864 .