5 years ago

Diffusive dynamics during the high-to-low density transition in amorphous ice [Physics]

Diffusive dynamics during the high-to-low density transition in amorphous ice [Physics]
Thomas Loerting, Michael Sprung, Chris J. Benmore, Gerhard Grubel, Flora Aubree, Alexander Spah, Daniel Mariedahl, Anders Nilsson, Lars G. M. Pettersson, Felix Lehmkuhler, Bernhard Massani, Alessandro Ricci, Katrin Amann–Winkel, Avni Jain, Fivos Perakis, Daniel Schlesinger, Jonas A. Sellberg, Filippo Cavalca, Harshad Pathak

Water exists in high- and low-density amorphous ice forms (HDA and LDA), which could correspond to the glassy states of high- (HDL) and low-density liquid (LDL) in the metastable part of the phase diagram. However, the nature of both the glass transition and the high-to-low-density transition are debated and new experimental evidence is needed. Here we combine wide-angle X-ray scattering (WAXS) with X-ray photon-correlation spectroscopy (XPCS) in the small-angle X-ray scattering (SAXS) geometry to probe both the structural and dynamical properties during the high-to-low-density transition in amorphous ice at 1 bar. By analyzing the structure factor and the radial distribution function, the coexistence of two structurally distinct domains is observed at T = 125 K. XPCS probes the dynamics in momentum space, which in the SAXS geometry reflects structural relaxation on the nanometer length scale. The dynamics of HDA are characterized by a slow component with a large time constant, arising from viscoelastic relaxation and stress release from nanometer-sized heterogeneities. Above 110 K a faster, strongly temperature-dependent component appears, with momentum transfer dependence pointing toward nanoscale diffusion. This dynamical component slows down after transition into the low-density form at 130 K, but remains diffusive. The diffusive character of both the high- and low-density forms is discussed among different interpretations and the results are most consistent with the hypothesis of a liquid–liquid transition in the ultraviscous regime.

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