Iron isotope tracing of mantle heterogeneity within the source regions of oceanic basalts

Mineralogical variations in the Earth's mantle and the relative proportions of peridotitic versus enriched and potentially crustally-derived pyroxenitic domains within the mantle have important implications for mantle dynamics, magma generation, and the recycling of surface material back into the mantle. Here we present iron (Fe) stable isotope data (delta Fe-57, deviation in Fe-57/Fe-54 from the IRMM-014 standard in parts per thousand) for peridotite and garnet-pyroxenite xenoliths from Oahu, Hawaii and explore Fe isotopes as tracer of both peridotitic and pyroxenitic components in the source regions of oceanic basalts. The pyroxenites have delta Fe-57 values that are heavy (0.10 to 0.27 parts per thousand) relative to values for mid-ocean ridge and ocean island basalts (MORB; OIB; delta Fe-57 similar to 0.16 parts per thousand) and the primitive mantle (PM; delta Fe-57 similar to 0.04 parts per thousand). Pyroxenite delta Fe-57 values are positively correlated with bulk pyroxenite titanium and heavy rare earth element (REE) abundances, which can be interpreted in terms of stable isotope fractionation during magmatic differentiation and pyroxene cumulate formation. In contrast, the peridotites have light delta Fe-57 values (-0.34 to 0.14 parts per thousand) that correlate negatively with degree of melt depletion and radiogenic hafnium isotopes, with the most depleted samples possessing the most radiogenic Hf isotope compositions and lightest delta Fe-57 values. While these correlations are broadly consistent with a scenario of Fe isotope fractionation during partial melting, where isotopically heavy Fe is extracted into the melt phase, leaving behind low-delta Fe-57 peridotite residues, the extent of isotopic variation is far greater than predicted by partial melting models. One possibility is derivation of the samples from a heterogeneous source containing both light-delta Fe-57 (relative to PM) and heavy-delta Fe-57 components. While pyroxenite is a viable explanation for the heavy-delta Fe-57 component, the origin of the depleted light-delta Fe-57 component is more difficult to explain, as melting models predict that even large (>30%) degrees of melt extraction do not generate strongly fractionated residues. Multiple phases of melt extraction or other processes, such as metasomatism, melt percolation or the assimilation of xenocrystic olivine with light delta Fe-57 values may need to be invoked to explain these light delta Fe-57 values; a caveat to this is that these processes must either preserve, or generate correlations between delta Fe-57 and Hf isotopes. Published variations in delta Fe-57 in mantle melting products, such as MORB and OIB, are also greater than predicted by melting models assuming derivation from delta Fe-57-homogeneous mantle. For example, OIB from the Society and Cook-Austral islands, which have radiogenic Pb and Sr isotope compositions indicative of recycled components such as subduction modified, low-Pb oceanic crust and terrigenous sediments have heavy mean delta Fe-57 values (-0. 21 parts per thousand) significantly distinct to those of other OIB and MORB, which could explained by the presence of heavy-delta Fe-57 pyroxenite cumulate or pyroxenitic melt components, whereas large degree partial melts, such as komatiites and boninites, display light Fe-isotopic compositions which may reflect sampling of refractory, light-delta Fe-57 mantle components. Iron stable isotopes may therefore provide a powerful new means of fingerprinting mineralogical variations within the Earth's mantle and identifying the mineralogy of depleted and enriched components within the source regions of volcanic rocks. (C) 2014 The Authors. Published by Elsevier B.V.