THE PHASE BOUNDARY BETWEEN WADSLEYITE AND RINGWOODITE IN MG2SIO4 DETERMINED BY IN SITU X-RAY DIFFRACTION

dc.contributor.authorInoue T.
dc.contributor.authorIrifune T.
dc.contributor.authorHigo Y.
dc.contributor.authorSanehira T.
dc.contributor.authorSueda Y.
dc.contributor.authorYamada A.
dc.contributor.authorShinmei T.
dc.contributor.authorYamazaki D.
dc.contributor.authorAndo J.
dc.contributor.authorFunakoshi K.
dc.contributor.authorUtsumi W.
dc.date.accessioned2025-04-25T03:22:02Z
dc.date.available2025-04-25T03:22:02Z
dc.date.issued2006
dc.description.abstractThe phase boundary between wadsleyite and ringwoodite in Mg2SiO4 has been determined in situ using a multi-anvil apparatus and synchrotron X-rays radiation at SPring-8. In spite of the similar X-ray diffraction profiles of these high-pressure phases with closely related structures, we were able to identify the occurrence of the mutual phase transformations based on the change in the difference profile by utilizing a newly introduced press-oscillation system. The boundary was located at ~18.9 GPa and 1,400°C when we used Shim’s gold pressure scale (Shim et al. in Earth Planet Sci Lett 203:729–739, 2002), which was slightly (~0.8 GPa) lower than the pressure as determined from the quench experiments of Katsura and Ito (J Geophys Res 94:15663–15670, 1989). Although it was difficult to constrain the Clapeyron slope based solely on the present data due to the kinetic problem, the phase boundary [P (GPa)=13.1+4.11×10−3×T (K)] calculated by a combination of a P–T position well constrained by the present experiment and the calorimetric data of Akaogi et al. (J Geophys Res 94:15671–15685, 1989) reasonably explains all the present data within the experimental error. When we used Anderson’s gold pressure scale (Anderson et al. in J Appl Phys 65:1535–1543, 1989), our phase boundary was located in ~18.1 GPa and 1,400°C, and the extrapolation boundary was consistent with that of Kuroda et al. (Phys Chem Miner 27:523–532, 2000), which was determined at high temperature (1,800–2,000°C) using a calibration based on the same pressure scale. Our new phase boundary is marginally consistent with that of Suzuki et al. (Geophys Res Lett 27:803–806, 2000) based on in situ X-ray experiments at lower temperatures (<1,000°C) using Brown’s and Decker’s NaCl pressure scales.
dc.identifierhttps://elibrary.ru/item.asp?id=52813073
dc.identifier.citationPhysics and Chemistry of Minerals, 2006, 33, 2, 106-114
dc.identifier.doi10.1007/s00269-005-0053-y
dc.identifier.issn0342-1791
dc.identifier.urihttps://repository.geologyscience.ru/handle/123456789/49040
dc.subjectWADSLEYITE
dc.subjectRINGWOODITE
dc.subjectPHASE TRANSFORMATION
dc.subjectHIGH PRESSURE
dc.subjectIN SITU X-RAY DIFFRACTION
dc.titleTHE PHASE BOUNDARY BETWEEN WADSLEYITE AND RINGWOODITE IN MG2SIO4 DETERMINED BY IN SITU X-RAY DIFFRACTION
dc.typeСтатья

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