To constrain the thermodynamics and melting relations of the siderite-magnesite (FeCO 3-MgCO 3) system, 27 piston cylinder experiments were conducted at 3.5 GPa and 1170-1575 °C. Fe-rich compositions were also investigated with 13 multi anvil experiments at 10, 13.6 and 20 GPa, 1500-1890 °C. At 3.5 GPa, the solid solution siderite-magnesite coexisting with melt over a compositional range of X Mg (=Mg/(Mg+Fe tot)) = 0.38-1.0, while at ≥10 GPa solid solution appears to be complete. At 3.5 GPa the system is pseudo-binary because of the limited stability of siderite or liquid FeCO 3 , Fe-rich carbonates decomposing at subsolidus conditions to magnetite-magnesioferrite solid solution, graphite and CO 2. Similar reactions also occur with liquid FeCO 3 resulting in melt species with ferric iron components, but the decomposition of the liquid decreases in importance with pressure. 2 At 3.5 GPa the metastable melting temperature of pure siderite is located at 1264 °C whereas pure magnesite melts at 1629 °C. The melting loop is non-ideal on the Fe-side where the dissociation reaction resulting in Fe 3+ in the melt depresses melting temperatures and causes a minimum. Over the pressure range of 3.5-20 GPa, this minimum is 20-35 °C lower than the (metastable) siderite melting temperature. By merging all present and previous experimental data, standard state (298.15 K, 1 bar) thermoydynamic properties of the magnesite melt (MgCO 3 L) end-member are calculated and the properties of (Fe,Mg)CO 3-melt fit by a regular solution model with an interaction parameter of-7600 J/mol. The solution model reproduces the asymmetric melting loop and predicts the thermal minimum at 1240 °C near the siderite side at X Mg =0.2 (3.5 GPa). The solution model is applicable to pressures reaching to the bottom of the upper mantle and allows calculation of phase relations in the FeO-MgO-O 2-C system.