Abstract

To distinguish between order and disorder is of fundamental importance to understanding solids. It becomes more significant with recent observations that solids with high structural order can behave like disordered solids, while properties of disordered solids can approach crystals under certain circumstance. It is then imperative to understand when and how disorder takes effect to deviate the properties of a solid from crystals and what the correct factors are to control the behaviours of solids. Here we answer these questions by reporting the finding of a hidden order-disorder transition from crystals to disordered crystals for static packings of frictionless spheres. While the geometric indicators are mostly blind to the transition, disordered crystals already exhibit properties apart from crystals. The transition approaches the close packing of hard spheres, giving rise to the singularity of the close packing point. We evidence that both the transition and properties of disordered crystals are jointly determined by the structural order and density. Near the transition, the elastic moduli and coordination number of disordered crystals show particular pressure dependence distinct from known behaviours of both crystals and jammed solids. The discovery of the transition therefore reveals some unknown aspects of solids.

Highlights

  • One may distinguish disordered solids from crystals based on the structural order and classify solids with high structural order to crystals

  • Our model systems consist of frictionless particles interacting via finite range repulsions, which mimic experimental systems like granular and colloidal solids[17,18,19]

  • The finding and characterization of the transition from crystals to disordered crystals reveals some unknown features: (i) The close packing point is singular in terms of the transition, implying that it is the only point satisfying the physics of crystals for rigid packings of hard spheres, (ii) the structural order and density interplay to determine the transition and properties of disordered solids, and (iii) disordered crystals near the transition exhibit unique pressure scalings apart from the physics of crystals and the physics of jamming

Read more

Summary

Introduction

One may distinguish disordered solids from crystals based on the structural order and classify solids with high structural order to crystals. Indicates that in addition to the structural order there exist other possible controlling parameters of the manifestation of disordered solids, while the density is a candidate. How the density works together with the structural order to determine properties of disordered solids is still an open question. Bearing in mind the questions mentioned above, we numerically investigate the evolution from perfect crystals to disordered solids, by using the particle-size polydispersity as the control parameter. We focus on another hidden order-disorder transition at a rather small polydispersity from crystals to disordered crystals, namely solids with extremely high crystalline order in structure but mechanical and vibrational properties resembling disordered solids. We denote disordered solids with strong structural amorphisation as amorphous solids to distinguish them from disordered crystals

Methods
Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.