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1 Institute of Precambrian Geology and Geochronology RAS, nab. Makarova, 2, St. Petersburg, 199034, Russian Federation e-mail: dkrylov{at}dk1899.spb.edu
2 Institute of Geochemistry, Mineralogy and Ore Formation UAS, ul. Palladina 34, Kiev, 252142, Ukraine
3 Institut fur Mineralogie und Petrologie, Rheinische Friedrich Wilhelms Universitat Bonn, Poppelsdorfer Schloß, D-53115 Bonn, Germany
Oxygen isotope fractionation between synthesised zircon and water has been experimentally quantified at 700, 800, 900, and 1000 °C. The results are interpolated by:
zm-H20 = 3.70 + 2.74 ± 0.19x2, where x = 103/T (K). Combined with the fractionation between quartz and water (Bottinga & Javoy, 1973) this yields:
qtz-zm= 1.36x2.
Theoretical evaluations of the reduced partition function ratios for zircon and two (a- and ß-) modifications of quartz are expressed in terms of the following polynomials: 1000 lnfzm= 8.3306x2+ 1.9402 x 0.6896 (400 < T < 1100°C) 1000 lnfa-qtz= 7.8963 x2+7.4091 x-3.6015 (200°C < T < a-quartz stability field) 1000 lnfß-qtz= 9.3362 x2+ 2.4514 x 0.7844 (ß-quartz stability field up to 1100 °C).
These expressions are in excellent agreement both with the experimentally derived factors of oxygen isotope fractionation for ß-quartz and zircon, and the incremental calibrations for a-quartz and zircon (Hoffbauer et al., 1994). The effect of a-ß-quartz transition on oxygen isotope fractionation implies, that those calculations, anchored to the theoretically evaluated reduced partition function ratios of quartz (e.g., Zheng, 1993), can predict fractionations only within the P-T stability field of the respective modification of quartz (i.e. a-quartz).
Key-words: oxygen isotopes, zircon water fractionation, quartz, geothermometry.
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