Abstract

The application of the Ti-in-zircon thermometer to granitic rock requires consideration of a_{{{text{TiO}}_{2} }} and a_{{{text{SiO}}_{2} }} during zircon crystallization. Thermodynamic software programs such as rhyolite-MELTS or Perple_X permit the estimation of a_{{{text{TiO}}_{2} }} and a_{{{text{SiO}}_{2} }} values from whole-rock geochemical data as a function of pressure and temperature. Model calculations carried out on a set of 14 different granite types at 2 kbar, 5 kbar, and H2O = 3 wt% show a_{{{text{SiO}}_{2} }} during zircon crystallization close to 1 (0.75–1) and a_{{{text{TiO}}_{2} }} generally far below unity (0.1–0.6). This would suggest that Ti-in-zircon temperatures for granites must be significantly upward corrected relative to the original TiO2- and SiO2-saturated calibration of the thermometer. Both the rhyolite-MELTS and Perple_X calculations indicate that a_{{{text{TiO}}_{2} }} is typically around 0.5 in ilmenite-bearing granites. Thus, for ilmenite-series granites (that is, almost all S-type and many I-type granites), it could be a reasonable first order approximation to apply a constant temperature correction of + 70 °C to the Ti-in-zircon thermometer. Granites lacking the paragenesis zircon–ilmenite, that is, some A-type granites and a few special I-type granites may have even lower a_{{{text{TiO}}_{2} }} (0.1–0.5) and some of them may require a huge upward correction of Ti-in-zircon temperatures on the order of 100–200 °C. Using a set of Ti-in-zircon measurements from a Variscan granite of the Bohemian Massif, we introduce a novel T-dependent a_{{{text{TiO}}_{2} }} and a_{{{text{SiO}}_{2} }} correction of Ti-in-zircon calculated temperatures which is based on a_{{{text{TiO}}_{2} }}-, a_{{{text{SiO}}_{2} }}–T functions modelled with rhyolite-MELTS. This method takes into account that early and late zircons in granitic systems may crystallize at different a_{{{text{SiO}}_{2} }} and a_{{{text{TiO}}_{2} }}. Furthermore, we highlight the usefulness of comparing the corrected results of Ti-in-zircon thermometry with bulk-rock-Zr-based zircon solubility thermometry and ideal zircon crystallization temperature distributions for granites, and we present a graphical method that enables this comparison. In addition, this paper addresses the problem that Ti-in-zircon measurements are commonly collected with only moderate spatial analytical resolution, which leads to an averaging effect and to difficulties in recording accurate crystallization temperatures. Therefore, we propose that Ti-in-zircon thermometry for granites should generally rely on the more representative median-T (Tmed) value of a series of zircon analyses. Peak magma temperatures will be, in general, 35–50 °C above Tmed, as can be modelled using zircon crystallization temperature distributions.

Highlights

  • The Ti-in-zircon thermometer (Watson et al 2006) could become a most interesting petrological tool for research on granitic rocks if we succeed to overcome a few ongoing problems

  • Our results clearly suggest that Ti-in-zircon temperatures for granites have to be significantly upward corrected relative to the original ­TiO2and ­SiO2-saturated calibration of the thermometer, due to generally low aTiO2

  • Most have ­TiO2 contents that correspond to aTiO2 values of around or just below 0.5 (Fig. 5), and this agrees very well with the rhyolite-MELTS calculations performed in the present paper for a series of granitic rocks

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Summary

Introduction

The Ti-in-zircon thermometer (Watson et al 2006) could become a most interesting petrological tool for research on granitic rocks if we succeed to overcome a few ongoing problems. While the thermometer is ideally suited for rocks that carry cogenetic zircon, rutile, and quartz (e.g., high-pressure granulites), its application to granites is not straightforward. Most granites lack rutile implying that aTiO2 must have been below unity when the zircons formed. Granites are ­SiO2-rich, aSiO2 can be below unity during early zircon crystallization, because quartz is normally not present at near liquidus conditions (Johannes and Holtz 1991). An equation that corrects the Ti-in-zircon thermometer for the effects of reduced aTiO2 and aSiO2 is given by Ferry and Watson (2007): log (ppm Ti) = 5.711 ± 0.072 − 4800(±86)

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