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

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dc.contributor.author Inoue T.
dc.contributor.author Irifune T.
dc.contributor.author Higo Y.
dc.contributor.author Sanehira T.
dc.contributor.author Sueda Y.
dc.contributor.author Yamada A.
dc.contributor.author Shinmei T.
dc.contributor.author Yamazaki D.
dc.contributor.author Ando J.
dc.contributor.author Funakoshi K.
dc.contributor.author Utsumi W.
dc.date.accessioned 2025-04-25T03:22:02Z
dc.date.available 2025-04-25T03:22:02Z
dc.date.issued 2006
dc.identifier https://elibrary.ru/item.asp?id=52813073
dc.identifier.citation Physics and Chemistry of Minerals, 2006, 33, 2, 106-114
dc.identifier.issn 0342-1791
dc.identifier.uri https://repository.geologyscience.ru/handle/123456789/49040
dc.description.abstract The 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.subject WADSLEYITE
dc.subject RINGWOODITE
dc.subject PHASE TRANSFORMATION
dc.subject HIGH PRESSURE
dc.subject IN SITU X-RAY DIFFRACTION
dc.title THE PHASE BOUNDARY BETWEEN WADSLEYITE AND RINGWOODITE IN MG2SIO4 DETERMINED BY IN SITU X-RAY DIFFRACTION
dc.type Статья
dc.identifier.doi 10.1007/s00269-005-0053-y


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