Crossover of quasi-localized dynamics and diffusion in supercooled liquids
Secondary relaxation, also known as βJG relaxation, is a dynamical process observed in supercooled liquids and glasses. It is distinct from the slower, so-called α relaxation, which is associated with particles escaping the cages formed by their surrounding neighbours. The secondary relaxation affects several properties of the glass, including the crystallization propensity and mechanical response. Traditionally studied via dielectric and mechanical spectroscopy, the βJG rela
Secondary relaxation, also known as βJG relaxation, is a dynamical process observed in supercooled liquids and glasses. It is distinct from the slower, so-called α relaxation, which is associated with particles escaping the cages formed by their surrounding neighbours. The secondary relaxation affects several properties of the glass, including the crystallization propensity and mechanical response. Traditionally studied via dielectric and mechanical spectroscopy, the βJG relaxation is often linked to quasi-localized particle motion. Here we use a wavevector-resolved X-ray technique to access microscopic, real-space information on the βJG relaxation in a hydrogen-bonded glass former and show that the α and βJG relaxations cannot be described as two independent processes. Moreover, we provide evidence that the βJG relaxation is associated with a sublinear growth of the mean-squared molecular displacement preceding the onset of diffusion. Our findings thus clarify that the βJG relaxation can be described as the critical rattling of molecules within the cage formed by their neighbours just before escaping from it. Relaxation processes in glasses display two distinct components—fast localized motions versus slower diffusive dynamics. Time-domain interferometry experiments with a typical glass former now show that the two processes are coupled.
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