Abstract
Carbonates are the major hosts of carbon on Earth's surface and their fate during subduction needs to be known to understand the deep carbon cycle. Magnesite (${\mathrm{MgCO}}_{3}$) is thought to be an important phase participating in deep Earth processes, but its phase stability is still a matter of debate for the conditions prevalent in the lowest part of the mantle and at the core mantle boundary. Here, we have studied the phase relations and stabilities of ${\mathrm{MgCO}}_{3}$ at these $P,T$ conditions, using Raman spectroscopy at high pressures ($\ensuremath{\sim}148\phantom{\rule{0.16em}{0ex}}\mathrm{GPa}$) and after heating to high temperatures ($\ensuremath{\sim}3600\phantom{\rule{0.16em}{0ex}}\mathrm{K}$) in laser-heated diamond anvil cell experiments. The experimental Raman experiments were supplemented by x-ray powder diffraction data, obtained at a pressure of 110 GPa. Density-functional-theory-based model calculations were used to compute Raman spectra for several ${\mathrm{MgCO}}_{3}$ high-pressure polymorphs, thus allowing an unambiguous assignment of Raman modes. By combining the experimental observations with the density-functional-theory results, we constrain the phase stability field of ${\mathrm{MgCO}}_{3}$ with respect to the high-pressure polymorph, ${\mathrm{MgCO}}_{3}$-II. We further confirm that Fe-free ${\mathrm{MgCO}}_{3}$-II is a tetracarbonate with monoclinic symmetry (space group $C2/m$), which is stable over the entire $P,T$ range of the Earth's lowermost mantle geotherm.
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