DI002-0005
Subsolidus phase relations for Mg2SiO4 at mantle transition zone conditions

Monday, 7 December 2020
Poster
Junjie Dong1, Rebecca A. Fischer1, Matthew Brennan1, Kierstin Daviau1, Terry-Ann Suer1, Katlyn M Turner1, Vitali B Prakapenka2 and Yue Meng3, (1)Harvard University, Cambridge, MA, United States, (2)University of Chicago, GeoSoilEnviroCARS, Chicago, IL, United States, (3)HPCAT, X-Ray Science Division, Argonne National Laboratory, Argonne, United States
Abstract:
Detailed knowledge of phase relations for (Mg,Fe)2SiO4 is required for a better understanding of the thermochemical structure across the 660-kilometer boundary between Earth’s transition zone and lower mantle. The phase diagram of Mg2SiO4 at mantle transition zone pressures has been extensively investigated up to temperatures of ~2000 K, while the wadsleyite ↔ bridgmanite boundary from ~2000 K to the solidus as well as the triple point at which wadsleyite (wd), ringwoodite (rw) and bridgmanite/periclase (bdg/per) co-exist are still poorly constrained. In this study, we report new experimental constraints on the phase relations for Mg2SiO4 at pressures between 17 and 23 GPa and temperatures from 1600 to 2500 K, with an exploration of the effect of iron on the phase transitions, using synchrotron X-ray diffraction collected in high-pressure and high-temperature laser-heated diamond anvil cell experiments. In combination with previously published datasets, we determined the Clapeyron slope of the wdbdg + per boundary and the location of the wdrwbdg/per triple point based on a logistic regression model. Our statistical analysis suggests that the wdbdg + per reaction occurs at 20.7 GPa and 2100 K and 20.4 GPa and 2300 K, with a Clapeyron slope of –1.8 MPa/K; the wdrwbdg triple point is located at 20.8 GPa and 2060 K. The combined effects of the multiple phase transitions in the system MgO–FeO–SiO2, including the wdbdg + per reaction and the wdrwbdg/per triple point, influence the proportions of stable mineral phases in the mantle rock assemblages and their thermo-physical properties across the 660-km boundary, which eventually controls the vigor and style of the mantle convection through this upper-lower mantle interface of Earth.