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To investigate the physical property of Fe 7 C 3 , we carried out in situ X‑ray diffraction experiments using a Kawai-type multi-anvil apparatus and a diamond anvil cell up to 71.5 GPa and 1973 K. The carbide was found to be stable under these experimental conditions. However, we found anomalous behavior in its isothermal compression and thermal expansivity. These anomalies could be due to the magnetic phase transition in Fe 7 C 3  from a ferromagnetic (fm) to a paramagnetic (pm) phase. The Curie temperature of 523 K at 1 bar (Tsuzuki et al. 1984) decreases with pressure, and the pressure-induced magnetic transition is estimated to occur at ~18 GPa and 300 K. The pressure-volume-temperature (P-V-T) data set for the pm-Fe 7 C 3  was fitted by the Mie-Grüneisen-Debye (MGD) equation of state (EOS) and the following parameters were obtained: unit-cell volume V 0  = 184.2 ± 0.3 Å 3 , bulk modulus K 0  = 253 ± 7 GPa, the pressure derivative of bulk modulus K' 0  = 3.6 ± 0.2, Grüneisen parameter γ 0  = 2.57 ± 0.05, Debye temperature θ 0  = 920 ± 140 K, and q = 2.2 ± 0.5, respectively, at zero pressure. The calculated density for Fe 7 C 3  provides a good explanation for the density of the Earth’s inner core obtained from seismological observations.

Thermoelastic property and high-pressure stability of Fe 7 C 3 : Implication for iron-carbide in the Earth’s core