4.2 Article

OH-defects in Al- and Cr- doped synthetic enstatites and defect geobarometry on natural orthopyroxenes from the Earth's mantle

Journal

EUROPEAN JOURNAL OF MINERALOGY
Volume 24, Issue 3, Pages 471-481

Publisher

E SCHWEIZERBARTSCHE VERLAGSBUCHHANDLUNG
DOI: 10.1127/0935-1221/2012/0024-2208

Keywords

enstatite; high-pressure; IR-spectroscopy; geobarometry; OH point defect; water storage

Categories

Funding

  1. Austrian Science Fund [FWF:P22367-N21]
  2. Austrian Science Fund (FWF) [P22367] Funding Source: Austrian Science Fund (FWF)
  3. Austrian Science Fund (FWF) [P 22367] Funding Source: researchfish

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Hydrogen incorporation mechanisms in synthetic enstatite (Mg2Si2O6), doped with Al or Cr and Al and Cr, and coexisting with forsterite were studied experimentally at 4-8 GPa at 1150 degrees C. The IR spectra show two different groups of OH-absorption bands: group 1 (wavenumbers between 3500 and 3730 cm(-1)) and group 2 (wavenumbers between 2800 and 3500 cm(-1)). The intensity ratio of group 2 to group 1 bands (e.g., (A(3362))/(A(3692))) is sensitive to pressure and to the Al/Cr ratio incorporated in enstatite. In addition, for samples doped with Al and Cr, the OH content is not a simple function of Al and Cr, suggesting OH-defect annihilation if both trivalent cations are present. Modelling of OH-incorporation into enstatite suggests that the water storage capacity in mantle orthopyroxene under average conditions of a continental geotherm is higher than in pure enstatite, but much lower than simple substitution mechanisms would suggest. Based on the observed pressure trend in the OH-absorption spectra of the synthetic samples, IR spectra of eleven natural samples were evaluated. Even if synthetic and natural samples do not show the same trend, a pressure trend for the natural samples could be established, and a geobarometer for the OH-characteristics of natural orthoenstatite from the Earth's mantle (coexisting with forsterite) can be formulated as P[GPa] = 63.4. A((3487-3240)) + A((3570-3487))/ A((3487-3240)) + A((3570-3487)) + A((3730-3570)) -48.8, where A((a-b)) is the integral absorbance of the component E parallel to n(gamma) + E parallel to n(beta) of the absorption bands between a cm(-1) and b cm(-1), respectively.

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