NPG Asia Materials · 2020 · 36 citations · 42 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsMaterials ChemistryPhysical ChemistryCoordination NumberCrystallographyMolecular DynamicsPhase TransitionsX-ray CrystallographyX-ray DiffractionCrystalline Phase FormationCrystalline StructureElectronic Structure DeterminationGlass TransitionGlass Transition StructureLiquid-glass TransitionStructural Glass TransitionX-ray Diffraction Analysis
Abstract Understanding the liquid structure provides information that is crucial to uncovering the nature of the glass-liquid transition. We apply an aerodynamic levitation technique and high-energy X-rays to liquid ( l )-Er 2 O 3 to discover its structure. The sample densities are measured by electrostatic levitation at the International Space Station. Liquid Er 2 O 3 displays a very sharp diffraction peak (principal peak). Applying a combined reverse Monte Carlo – molecular dynamics approach, the simulations produce an Er–O coordination number of 6.1, which is comparable to that of another nonglass-forming liquid, l -ZrO 2 . The atomic structure of l -Er 2 O 3 comprises distorted OEr 4 tetraclusters in nearly linear arrangements, as manifested by a prominent peak observed at ~180° in the Er–O–Er bond angle distribution. This structural feature gives rise to long periodicity corresponding to the sharp principal peak in the X-ray diffraction data. A persistent homology analysis suggests that l -Er 2 O 3 is homologically similar to the crystalline phase. Moreover, electronic structure calculations show that l -Er 2 O 3 has a modest band gap of 0.6 eV that is significantly reduced from the crystalline phase due to the tetracluster distortions. The estimated viscosity is very low above the melting point for l -ZrO 2 , and the material can be described as an extremely fragile liquid.
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