Abstract
We performed a series of experiments at high pressures and temperatures to determine the partitioning of a wide range of
trace elements between ilmenite (Ilm), armalcolite (Arm) and anhydrous lunar silicate melt, to constrain geochemical models
of the formation of titanium-rich melts in the Moon. Experiments were performed in graphite-lined platinum capsules
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at pressures
and temperatures ranging from 1.1 to 2.3 GPa and 1300–1400 C using a synthetic Ti-enriched Apollo ‘black glass’ composition
in the CaO–FeO–MgO–Al2O3–TiO2–SiO2 system. Ilmenite–melt and armalcolite–melt partition coefficients (D) show
highly incompatible values for the rare earth elements (REE) with the light REE more incompatible compared to the heavy
REE (DIlm–melt
La 0.0020 ± 0.0010 to DIlm–melt
Lu 0.069 ± 0.010 for ilmenite; DArm–melt
La 0.0048 ± 0.0023 to DArm–melt
Lu 0.041 ± 0.008 for
armalcolite). D values for the high field strength elements vary from highly incompatible for Th, U and to a lesser extent W
(for ilmenite: DIlm–melt
Th 0.0013 ± 0.0008, DIlm–melt
U 0.0035 ± 0.0015 and DIlm–melt
W 0.039 ± 0.005, and for armalcolite DArm–melt
Th
0.008 ± 0.003, DArm–melt
U 0.0048 ± 0.0022 and DArm–melt
W 0.062 ± 0.03), to mildly incompatible for Nb, Ta, Zr, and Hf (e.g.
DIlm–melt
Hf 0.28 ± 0.05 and : DArm–melt
Hf 0.76 ± 0.07). Both minerals fractionate the high field strength elements with DTa/DNb
and DHf/DZr between 1.3 and 1.6 for ilmenite and 1.3 and 1.4 for armalcolite. Armalcolite is slightly more efficient at fractionating
Hf from W during lunar magma ocean crystallisation, with DHf/DW = 12–13 compared to 6.7–7.5 for ilmenite.
The transition metals vary from mildly incompatible to compatible, with the highest compatibilities for Cr in ilmenite
(D 7.5) and V in armalcolite (D 8.1). D values show no clear variation with pressure in the small range covered.
Crystal lattice strain modelling of D values for di-, tri- and tetravalent trace elements shows that in ilmenite, divalent elements
prefer to substitute for Fe while armalcolite data suggest REE replacing Mg. Tetravalent cations appear to preferentially
substitute for Ti in both minerals, with the exception of Th and U that likely substitute for the larger Fe or Mg cations.
Crystal lattice strain modelling is also used to identify and correct for very small ( 0.3 wt.%) melt contamination of trace
element concentration determinations in crystals.
Our results are used to model the Lu–Hf–Ti concentrations of lunar high-Ti mare basalts. The combination of their subchondritic
Lu/Hf ratios and high TiO2 contents requires preferential dissolution of ilmenite or armalcolite from late-stage,
lunar magma ocean cumulates into low-Ti partial melts of deeper pyroxene-rich cumulates.
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