Volume 56, Issue 4 pp. 1125-1130
research papers

Structure evolution of Bi4O7 under high pressure

Jianzong Wang

Jianzong Wang

Center for High Pressure Science and Technology Advanced Research, People's Republic of China

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Luhong Wang

Corresponding Author

Luhong Wang

Shanghai Advanced Research in Physical Sciences, Shanghai 201203, People's Republic of China

Luhong Wang, e-mail: [email protected]; Haozhe Liu, e-mail: [email protected]Search for more papers by this author
Fuyang Liu

Fuyang Liu

Center for High Pressure Science and Technology Advanced Research, People's Republic of China

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Shuhua Yuan

Shuhua Yuan

Center for High Pressure Science and Technology Advanced Research, People's Republic of China

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Dongzhou Zhang

Dongzhou Zhang

University of Hawaii at Manoa, Honolulu, Hawaii, USA

University of Chicago, Chicago, Illinois, USA

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Vitali B. Prakapenka

Vitali B. Prakapenka

University of Chicago, Chicago, Illinois, USA

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Wilhelm Klein

Wilhelm Klein

Technical University of Munich, Germany

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Haozhe Liu

Corresponding Author

Haozhe Liu

Center for High Pressure Science and Technology Advanced Research, People's Republic of China

Luhong Wang, e-mail: [email protected]; Haozhe Liu, e-mail: [email protected]Search for more papers by this author
First published: 20 July 2023

Abstract

X-ray diffraction and Raman spectroscopy measurements were used to study the structure evolution of Bi4O7 during compression. Two isostructural phase transitions were observed under high pressure, with the first transition to phase II occurring at approximately 3.0 (2) GPa and the second to phase III occurring at approximately 13.0 (5) GPa. The pressure–volume (PV) curve was found to be discontinuous at those two pressure transition boundaries. By fitting the PV curves in three different stages, the bulk moduli were estimated to be approximately 101 (2), 68 (2) and 172 (3) GPa. Such large differences in the bulk moduli confirm two isostructural phase changes in the three stages. An irreversible amorphization process was found to start at approximately 20 (1) GPa, and the sample gradually becomes fully amorphous during compression at 30 (1) GPa.

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