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Elastic models for the non-arrhenius relaxation time of glass-forming liquids.
| Content Provider | CiteSeerX |
|---|---|
| Abstract | Abstract. We first review the phenomenology of viscous liquids and the standard models used for explaining the non-Arrhenius average relaxation time. Then the focus is turned to the so-called elastic models, arguing that these models are all equivalent in the Einstein approximation (where the short-time elastic properties are all determined by just one effective, temperature-dependent force constant). We finally discuss the connection between the elastic models and two well-established research fields of condensed-matter physics: point defects in crystals and solid-state diffusion. |
| File Format | |
| Access Restriction | Open |
| Subject Keyword | Elastic Model Non-arrhenius Relaxation Time Glass-forming Liquid Viscous Liquid Condensed-matter Physic Well-established Research Field Temperature-dependent Force Constant Non-arrhenius Average Relaxation Time Short-time Elastic Property Einstein Approximation So-called Elastic Model Standard Model Point Defect Solid-state Diffusion |
| Content Type | Text |
| Resource Type | Article |