Abstract
The shape of the α-relaxation spectra in supercooled liquids is discussed within the mode-coupling approach. The dynamical behaviour is ruled by properties of various bifurcation singularities in the non-linear equations of motion. The stretched exponential behaviour appears as the generic case, and is intimately related with the von Schweidler relaxation. The theory can also account for a double α, α′ peak scenario which is related to self-intersections of the bifurcation hypersurface. The cusp singularities are also briefly discussed and they can account for complex spectra which are observed in many polymeric systems.
| Originalsprache | Englisch |
|---|---|
| Seiten (von - bis) | 7-15 |
| Seitenumfang | 9 |
| Fachzeitschrift | Journal of Non-Crystalline Solids |
| Jahrgang | 172-174 |
| Ausgabenummer | PART 1 |
| DOIs | |
| Publikationsstatus | Veröffentlicht - 1 Sept. 1994 |
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