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Abstract
As a new class of multi-principal component oxides with high chemical disorder, high-entropy oxides (HEOs) have attracted much attention. The stability and tunability of their structure and properties are of great interest and importance, but remain unclear. By using in situ synchrotron radiation X-ray diffraction, Raman spectroscopy, ultraviolet–visible absorption spectroscopy, and ex situ high-resolution transmission electron microscopy, here we show the existence of lattice distortion in the crystalline (Ce0.2La0.2Pr0.2Sm0.2Y0.2)O2−δ HEO according to the deviation of bond angles from the ideal values, and discover a pressure-induced continuous tuning of lattice distortion (bond angles) and band gap. As continuous bending of bond angles, pressure eventually induces breakdown of the long-range connectivity of lattice and causes amorphization. The amorphous state can be partially recovered upon decompression, forming glass–nanoceramic composite HEO. These results reveal the unexpected flexibility of the structure and properties of HEOs, which could promote the fundamental understanding and applications of HEOs.
High entropy oxides can exhibit remarkable properties which may be amenable to pressure tuning. Here a fluorite-type high entropy oxide is shown to undergo pressure-induced lattice distortion with associated changes to optical behaviour.
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1 Center for High Pressure Science and Technology Advanced Research, Pudong, P. R. China (GRID:grid.410733.2); Shanghai Institute of Laser Plasma, Shanghai, P. R. China (GRID:grid.410733.2)
2 Center for High Pressure Science and Technology Advanced Research, Pudong, P. R. China (GRID:grid.410733.2)
3 Joint Research Laboratory Nanomaterials–Technische Universität Darmstadt and Karlsruhe Institute of Technology, Darmstadt, Germany (GRID:grid.410733.2); Karlsruhe Institute of Technology, Institute of Nanotechnology, Eggenstein-Leopoldshafen, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874)
4 Center for High Pressure Science and Technology Advanced Research, Pudong, P. R. China (GRID:grid.410733.2); University of Science and Technology Beijing, State Key Laboratory for Advanced Metals and Materials, Beijing, P. R. China (GRID:grid.69775.3a) (ISNI:0000 0004 0369 0705)
5 University of Chicago, Center for Advanced Radiation Sources, Chicago, USA (GRID:grid.170205.1) (ISNI:0000 0004 1936 7822)
6 Argonne National Laboratory, Center for Nanoscale Materials, Argonne, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)
7 Joint Research Laboratory Nanomaterials–Technische Universität Darmstadt and Karlsruhe Institute of Technology, Darmstadt, Germany (GRID:grid.187073.a); Heraeus Deutschland GmbH & Co. KG, Hanau, Germany (GRID:grid.439024.8)
8 Joint Research Laboratory Nanomaterials–Technische Universität Darmstadt and Karlsruhe Institute of Technology, Darmstadt, Germany (GRID:grid.439024.8); Karlsruhe Institute of Technology, Institute of Nanotechnology, Eggenstein-Leopoldshafen, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874)
9 Center for High Pressure Science and Technology Advanced Research, Pudong, P. R. China (GRID:grid.410733.2); Southeast University, Jiangsu Key Laboratory of Advanced Metallic Materials, School of Materials Science and Engineering, Nanjing, P. R. China (GRID:grid.263826.b) (ISNI:0000 0004 1761 0489)