期刊
SOFT MATTER
卷 17, 期 45, 页码 10242-10253出版社
ROYAL SOC CHEMISTRY
DOI: 10.1039/d0sm01575j
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资金
- National Cancer Institute of the National Institutes of Health under Physical Sciences Oncology Center (PSOC) [U54 CA193417]
- National Science Foundation [DMR-1506625]
- Simons Foundation [454945, 327939]
Machine learning techniques have been utilized to study the relationship between local structural features and variations in local dynamical activity in disordered glass-forming materials. The study focuses on the Voronoi model and reveals a strong connection between softness and the temperature dependence of relaxation time. Softness accurately predicts the likelihood of rearrangements and captures nearly all relevant information about rearrangements from structure.
Machine learning techniques have been used to quantify the relationship between local structural features and variations in local dynamical activity in disordered glass-forming materials. To date these methods have been applied to an array of standard (Arrhenius and super-Arrhenius) glass formers, where work on soft spots indicates a connection between the linear vibrational response of a configuration and the energy barriers to non-linear deformations. Here we study the Voronoi model, which takes its inspiration from dense epithelial monolayers and which displays anomalous, sub-Arrhenius scaling of its dynamical relaxation time with decreasing temperature. Despite these differences, we find that the likelihood of rearrangements can nevertheless vary by several orders of magnitude within the model tissue and extract a local structural quantity, softness, that accurately predicts the temperature dependence of the relaxation time. We use an information-theoretic measure to quantify the extent to which softness determines impending topological rearrangements; we find that softness captures nearly all of the information about rearrangements that is obtainable from structure, and that this information is large in the solid phase of the model and decreases rapidly as state variables are varied into the fluid phase.
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