Extreme pressures unlock the secrets of solidified xenon, helium, and hydrogen
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| Fig 1: Schematic of a Diamond Anvil Cell |
Simple, ‘inert’ gas atoms can solidify, alloy or bond under extreme pressures in a diamond-anvil cell (DAC) [See Fig.1] and allows scientists to explore the forced condensation of molecular solids having extreme contrast in molecular weight and size. In this study, Prof. Andrew Jephcoat, the Principal Beamline Scientist for I15, and his colleagues, Dr Annette Kleppe and Dr Mónica Amboage, studied xenon compressed with a mixture of light gases under extremely high pressures to near 150 GigaPascals (1.5 million times atmospheric pressure).
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| Fig. 2: Excited ruby fluorescence band provides pressure scale. |
Helium is the lightest noble gas and xenon one of the heaviest. The noble gases have filled electron shells, and are generally considered not to form compounds, except for the reactive halogens chlorine and fluorine. However, they are subject to weak, van der Waals bonding forces, which could allow formation of molecules and solid molecular crystals under extremely high pressures. A complex morphology of crystalgrowth patterns was observed in the DAC [See Fig.3].
The DAC was brought to Diamond’s I15 beamline for structure determination with an intense and collimated X-ray beam. In the case of the xenon-helium mix, the studies found that the xenon behaves just as it does when pure, forming crystals that are face-centred cubic (fcc) at lower pressures, changing to hexagonal close packed (hcp) above 16 GPa in a continuous transformation process. Contrary to some predictions, no Xe-He molecular compound was observed. For the xenon-hydrogen mix, the story is more complicated. Two distinct H2-Xe solids were identified depending on the initial concentration of xenon in hydrogen. The precise molecular composition and crystalline form of these new compounds is still under investigation.
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| Fig.3a). Micro-crystals of solid xenon condensing in fluid helium and associated powder/single-crystal diffraction patterns. Fig.3b). Phase separation and single-crystal growth of solid xenon in helium. Fig.3c). Xenon in fluid and solid hydrogen at room temperature: Solid xenon crystallite (hexagon) and growth of a new, bonded H2-Xe molecular phase. |
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| Fig. 4. Optical spectra showing the Raman-active, H-H stretching vibration (vibron mode) in H2-Xe. The vibron turns over in frequency and crosses that of pure hydrogen at 50 GPa. |
Prof Andrew Jephcoat, Diamond Light Source
Learn more about Beamline I15 - Extreme Conditions
Structural and Vibrational Properties of Condensed Phases in Xenon Molecular Binary Systems: He-Xe, H2-Xe Journal of Physics: Conference Series. Andrew P Jephcoat, Mónica Amboage, Annette K Kleppe.
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