[S-MP47_1AM1] Physics and Chemistry of Minerals

[SMP47-04] A new high pressure phase of Fe2SiO4 and the relationship between spin and structural transitions

*Takamitsu YAMANAKA¹, Atsushi KYONO², Yuki NAKAMOTO³, Svetlana KHARLAMOVA¹, Viktor STRUZKIN¹, Ho-kwang MAO¹, Russell HEMLY¹ (1.Carnegie Institution of Washington Geophysical Laboratory, 2.Division of Earth Evolution Sciences, Life and Environment Sciences, University of Tsukuba, 3.Center for Quantum Science and Technology Under Extreme Conditions, Osaka University)

Keywords:Fe2SiO4 spinel, new high-pressure phase, spin transition, X-ray emission, martensitic transition

A structural change in Fe₂SiO₄ spinel (ringwoodite) has been found by synchrotron powder diffraction study and the structure of a new high-pressure phase was determined by Monte-Carlo simulation method and Rietveld profile fitting of x-ray diffraction data up to 64 GPa at ambient temperature. A transition from the cubic spinel structure to a body centered orthorhombic phase (I-Fe₂SiO₄) with space group Imma and Z=4 was observed at approximately 34 GPa. The structure of I-Fe₂SiO₄ has two crystallographically independent FeO₆ octahedra. Iron resides in two different sites of six-fold coordination: Fe1 and Fe2, which are arranged in layers parallel to (101) and (011), and very similar to the layers of FeO₆ octahedra in the spinel structure. Silicon is located in the six-fold coordination in I-Fe₂SiO₄. The transformation to the new high-pressure phase is reversible under decompression at ambient temperature. A martensitic transformation of each slab of the spinel structure with transition vector < 1/8 1/8 1/8 > generates the I-Fe₂SiO₄ structure. Laser heating of I-Fe₂SiO₄ at 1500 K results in a decomposition of the material to rhombohedral FeO and SiO₂ stishovite.Fe K beta x-ray emission measurements at high pressure up to 65GPa show that the transition from a high spin (HS) to an intermediate spin (IS) state begins at 17 GPa in the spinel phase. The IS electron spin state is gradually enhanced with pressure. The Fe2+ ion at the octahedral site changes the iron radius under compression from 0.78 A at the high-spin state to 0.61 A at the low spin, which results in the changes of the lattice parameter and the deformation of the octahedra of the spinel structure. The compression curve of the lattice parameter of the spinel is discontinuous at approximately 20 GPa. The spin transition induces an isostructural change.