Dynamics of coalescence in hyperquenched glassy water probed by x-rays
Johannes Giebelmann1, Tobias Eklund2,3,4, Christina M Tonauer1,5
1Institute of Physical Chemistry, University of Innsbruck, Innrain 52c, 6020 Innsbruck, Austria.
Abstract:
Dynamics, morphology, and structure of glassy water are highly relevant for cryochemical techniques, in particular for cryo-electron microscopy. Here, we study the structural dynamics of a deposit consisting of thousands of micrometer-sized glassy water droplets during and after droplet coalescence using x-ray photon correlation spectroscopy at the micro- and meso-scale. We cover the temperature range from 94 to 161 K, encompassing droplet coalescence, the glass transition, and crystallization to ice I. Our experimental protocol involves heating beyond the coalescence regime, followed by recooling and reheating beyond crystallization, which allows us to disentangle the dynamics of coalescence from those associated with the glass transition. During coalescence, we observe an irreversible ballistic process in the temperature range between 130 and 145 K, with characteristic velocities of ∼0.1-0.2 Å s-1. In addition, samples that are not annealed below 125 K exhibit a q-independent mode (q0) at 130-145 K, which only appears while coalescence is progressing. We regard this to be a collective relaxation connected to a mobile surface layer at the droplet interfaces. After coalescence is complete, we observe significant diffusive dynamics. In particular, we find a sharp increase in diffusivity to ∼2 Å2 s-1 at around 148 K, indicating the onset of pronounced diffusive motion. From these results, we conclude droplet coalescence is primarily governed by ballistic, non-diffusive dynamics below ∼136 K, whereas strongly heterogeneous diffusive dynamics emerge at higher temperatures. We associate the abrupt increase in diffusivity after coalescence with the bulk glass-to-liquid transition.
Related Concept Videos
X-ray Crystallography
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
Determination of Crystal Structures
X-ray Diffraction of Biological Samples
According to Bragg's law, when X-rays strike the sample positioned on a stage, the rays are scattered by the electron clouds around the sample atoms. The X-ray diffraction or scattering is caused by constructive interference of the X-ray waves that reflect off the internal...


