Shock-driven amorphization and melting in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Fe</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math>
/ Authors
C. Crépisson, A. Amouretti, M. Harmand, C. Sanloup, P. Heighway, Sam Azadi, D. McGonegle, T. Campbell, J. Pintor, D. Chin
and 22 more authors
Ethan Smith, L. Hansen, A. Forte, T. Gawne, Hae Ja Lee, B. Nagler, YuanFeng Shi, G. Fiquet, François Guyot, Mikako Makita, A. Benuzzi-Mounaix, T. Vinci, K. Miyanishi, N. Ozaki, T. Pikuz, H. Nakamura, K. Sueda, T. Yabuuchi, M. Yabashi, J. Wark, D. Polsin, S. Vinko
/ Abstract
We present measurements on Fe2O3 amorphization and melt under laser-driven shock compression up to 209(10) GPa via time-resolved x-ray diffraction. At 122(3) GPa, a diffuse signal is observed indicating the presence of a noncrystalline phase. Structure factors have been extracted up to 182(6) GPa showing the presence of two well-defined peaks. A rapid change in the intensity ratio of the two peaks is identified between 145(12) and 151(12) GPa, indicative of a phase change. The noncrystalline diffuse scattering is consistent with shock amorphization of Fe2O3 between 122(3) and 145(12) GPa, followed by an amorphous-to-liquid transition above 151(12) GPa. Upon release, a noncrystalline phase is observed alongside crystalline α−Fe2O3. The extracted structure factor and pair distribution function of this release phase resemble those reported for Fe2O3 melt at ambient pressure. Published by the American Physical Society 2025
Journal: Physical Review B