Oxygen Isotope Fractionation During Evaporation of Mg- and Si-rich CMAS-Liquids in Vacuum
Oxygen Isotope Fractionation During Evaporation of Mg- and Si-rich CMAS-Liquids in Vacuum
复制标题
真空蒸发富镁和富硅 CMAS 液体过程中的氧同位素分馏
DOI:
--
复制
发表时间:
2010
期刊:
影响因子:
--
通讯作者:
A. Davis
中科院分区:
文献类型:
--
作者:
R. Mendybaev;F. Richter;M. Spicuzza;J. Valley;A. Davis
Introduction: FUN CAIs are similar to Type B CAIs chemically and mineralogically, but characterized by large mass-dependent fractionations in Mg, Si and O isotopes as well as by unidentified nuclear effects in number of elements (e.g., [1, 2]). The heavy isotope enrichment is usually attributed to the isotopic fractionation caused by the partial evaporation of volatile components of CAI precursors during high temperature molten stage (e.g. [2]). To test this hypothesis we conducted an experimental study in which Mgand Si-rich CMAS liquids were evaporated in a vacuum [3,4]. Evaporation of extremely forsterite-rich melt (FUN1) and a melt with composition close to the bulk composition of Vig1623-5 FUN CAI (FUN2) resulted in a trajectory passing close to the compositions of 1623-5 and C1 FUN CAI, correspondingly. Moreover, Mgand Si-isotopic compositions in the evaporation residues with chemical compositions close to 1623-5 (produced by evaporation of FUN1 melt), and C1 (produced by evaporation of FUN2 melt) are close to the values measured in 1623-5 (δMg~62‰ and δSi~21‰) and C1 (δMg~60‰ and δSi~28‰) FUN CAIs [2, 5]. The bulk oxygen isotopic composition has been reported for several FUN CAIs (e.g., [2, 5]). On a three oxygen isotope diagram for individual grains of Vig1623-5, the isotopic composition of spinel, forsterite and fassaite lie on a mass fractionation line that intersects the CCAM line at about δO= -48‰. We use this point to estimate the degree of O enrichment of the bulk oxygen of a given FUN CAI. Here we report oxygen isotopic composition of evaporation residues from starting compositions that are possible precursors of Vig1623-5 and C1 FUN inclusions. Experimental: Evaporation experiments were conducted in a vacuum furnace at 1900°C. 2.5 mm dia Irwire loops with the starting materials were first placed into a cold furnace which was then pumped out and temperature increased to 1900°C in an automated mode. The sample was allowed to evaporate at this temperature for a predetermined period of time (0 min to 1 hr) and furnace then cooled at several hundred degrees per minute (see [6,7] for the experimental details). Oxygen isotopic compositions were measured at the University of Wisconsin-Madison. Oxygen (from ~2 mg chips of the evaporation residues) produced by laser fluorination with BrF5 as the fluorinating agent was cryogenically purified, passed through an in-line Hg diffusion pump and collected on 5Å mole sieve held at -196°C. The trap was then warmed using a liquid pentane slush (-131°C), and the gas was transferred to a second trap (at -196°C) to remove NF3. The purified O2 was then analyzed for three oxygen isotopes with a Finnigan MAT 251 mass spectrometer. The data were standardized as described in [8]. Each day, the δO and the δO values of unknowns were adjusted based on the average of 3-4 analyses of UWG-2 garnet standard [8, 9] analyzed on the same day. Results and Discussion: Measured oxygen isotope data are presented in Table below and Fig.1.