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Published on: December 11, 2014
The jamming transition is a k-core percolation transition.
Flaviano Morone1, Kate Burleson-Lesser1, H A Vinutha2
1Levich Institute and Physics Department, City College of New York, New York, NY 10031.
The jamming transition in matter is driven by the emergence of k-cores, not the isostatic point. This structural change, explained by k-core percolation theory, dictates rigidity in jammed systems.
Area of Science:
- Physics
- Materials Science
- Network Theory
Background:
- Jammed matter exhibits a critical transition point where rigidity emerges.
- Understanding the structural origins of this jamming transition is crucial for materials science.
- Existing theories often relate rigidity to the isostatic point, but this study explores an alternative mechanism.
Purpose of the Study:
- To elucidate the structural origin of the jamming transition in jammed matter.
- To investigate the role of k-cores and k-core percolation theory in rigidity.
- To compare 3D simulation results with mean-field k-core percolation theory.
Main Methods:
- Analysis of k-core structures in jammed matter simulations.
- Application of k-core percolation theory to identify critical coordination numbers.
- Comparison of finite-dimensional simulation data with infinite-dimensional (mean-field) network models.
Main Results:
- The jamming transition is characterized by the sudden appearance of k-cores at specific coordination numbers.
- Rigidity in jammed matter is dominated by the emergence of giant 3- and 4-cores.
- 3D simulation results align with mean-field k-core percolation predictions for random networks.
Conclusions:
- The jamming transition's origin lies in the emergence of k-cores, not the isostatic point.
- K-core percolation theory accurately describes the onset of rigidity in jammed systems.
- Jammed pack structures exhibit properties consistent with random networks, as explained by infinite-dimensional k-core theory.
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