1,2Kyusei Tsuno, 3Hideharu Kuwahara, 1Varun Manilal, 2Axel Wittmann, 2,4Kurt Leinenweber, 3Tetsuo Irifune, 1Damanveer S Grewal
Earth and Planetary Science Letters (in Press) Link to Article [DOI: 10.1016/j.epsl.2026.120246]
1Department of Earth and Planetary Sciences, Yale University, New Haven, CT, 06511, United States
2Eyring Materials Center, Arizona State University, Tempe, AZ, 85287, United States
3Geodynamic Research Center, Ehime University, Matsuyama, 790-8577, Japan
4School of Molecular Sciences, Arizona State University, Tempe, AZ, 85287, United State
Copyright Elsevier
Geochemical constraints imply that a solid silicate layer existed between the base of the Martian magma ocean (∼14 GPa) and the core-mantle boundary (∼18–20 GPa) during early differentiation. Both S-poor metallic melts segregated during core formation and S-rich sulfide melts exsolved upon subsequent magma ocean cooling must have percolated through this layer to the core, but the efficiency of this process is poorly constrained. At ∼18 GPa, this layer comprises roughly equal proportions of ringwoodite and majorite garnet, yet no dihedral angles in majorite garnet have been reported. We conducted experiments at 18 GPa and 1723–2200 K to determine dihedral angles between Fe(-Ni)-S-O alloy melts (25–46 mol% S+O) and both ringwoodite and majorite garnet. Dihedral angles decrease with increasing temperature, S+O content, and oxygen fugacity, while Ni has no effect. Dihedral angles in majorite garnet are systematically ∼10° lower than in ringwoodite under comparable conditions. Despite this, all dihedral angles (89°-126°) remain above the 60° threshold for melt interconnection, so the entire mineral assemblage acts as a percolation barrier. Because our experimental S+O contents exceed those of the S-poor core-forming alloy (∼15 mol% S), the measured angles represent a lower bound; the barrier for core-forming metal was even more severe. Theoretical models predict that for such angles, a few (> ∼1–2) vol.% of melt remains trapped as isolated pockets upon network disconnection. Such melts constitute a hidden deep mantle reservoir of highly siderophile elements (HSEs) and siderophile volatiles (C, N), explaining their abundances in bulk silicate Mars without requiring a late veneer.