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. 2022 Jul 4;13(1):3779.
doi: 10.1038/s41467-022-31586-9.

Oxygen isotope (δ18O, Δ'17O) insights into continental mantle evolution since the Archean

Affiliations

Oxygen isotope (δ18O, Δ'17O) insights into continental mantle evolution since the Archean

Ilya N Bindeman et al. Nat Commun. .

Abstract

Oxygen isotopic ratios are largely homogenous in the bulk of Earth's mantle but are strongly fractionated near the Earth's surface, thus these are robust indicators of recycling of surface materials to the mantle. Here we document a subtle but significant ~0.2‰ temporal decrease in δ18O in the shallowest continental lithospheric mantle since the Archean, no change in Δ'17O is observed. Younger samples document a decrease and greater heterogeneity of δ18O due to the development and progression of plate tectonics and subduction. We posit that δ18O in the oldest Archean samples provides the best δ18O estimate for the Earth of 5.37‰ for olivine and 5.57‰ for bulk peridotite, values that are comparable to lunar rocks as the moon did not have plate tectonics. Given the large volume of the continental lithospheric mantle, even small decreases in its δ18O may explain the increasing δ18O of the continental crust since oxygen is progressively redistributed by fluids between these reservoirs via high-δ18O sediment accretion and low-δ18O mantle in subduction zones.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. Evolution of oxygen isotopes in lithospheric continental mantle (CLM).
Temporal trends of δ18O olivine (a, b), orthopyroxene and bulk (b), and CLM corrected for melt depletion (b, c) in studied mantle nodules. Bulk is computed based on modal mineral abundances and δ18O values of olivine and orthopyroxene (T Supplementary Table 1). Zircon from the Archean Kaapvaal cratonic mantle is from ref. , and zircon and basalts from the moon are from refs. ,, lunar mantle estimate is based on zircon, olivine, and basalts (see the text). Notice decreasing trends (95% conf. interval error envelope in line fit) and inbox diagrams.
Fig. 2
Fig. 2. Locality-averaged δ18O values for the studied samples of olivine (Ol), bulk, and reconstructed original undepleted peridotite (see Fig. 3).
Line fit statistics indicate decreasing trends.
Fig. 3
Fig. 3. Computed isotope effects of batch (continuous lines) and fractional (dashed lines) peridotite melting from 0 to 45‰ on the equilibrium isotope values of melt and the residual mineral assemblage.
a Isotope effects on minerals and the residual bulk. Starting composition at low-T has 56% olivine, 26% Opx, 15% Cpx, and 3% of Spinel. Isotope fractionation factors are from refs. ,. For melt, we assumed A = 1.3. Isotope effects are computed against phase change and proportions (% melt) trends observed in ref. in their peridotite melting experiments, also modeled in ref. in pMELTS. Fractional melting assumed the removal of equilibrium fractional melt shown on the diagram. Flux melting trends are computed using Rayleigh melting by water fluxing and up to 5% fractional melt removal with shown effect on bulk peridotite and residual olivine δ18O values. In this case, it is assumed that water fluxing generates silica-rich andesitic hydrous melt/fluid with δ18O = 6.1–7.3‰ in equilibrium with the ambient assemblage. The upper bound of the flux melting triangle is computed by assuming decreasing δ18O from 7.3‰ to 6.1‰, while the lower bound assumes that the hydrous melts maintain a constant high δ18O = 7.3‰. Notice that melt depletion results in lowering bulk δ18O, but it also results in higher modal olivine and the δ18OOl values which are higher (closer to the bulk), while δ18OOpx is also higher; Δ18OOpx-Ol are constant. b effect of melt depletion along the melting path shown in (a) for δ18OOl or δ18Obulk. Notice the nearly linear change. Upon melt extraction, δ18Odunite < δ18Oharzburgite < δ18Olherzolite. cooling will not affect δ18Obulk (blue horizontal lines) but will increase Δ18Omineral-mineral. fractionation as is shown. c Thin sections of samples showing enriched and depleted harzburgites that lost melt, and the final residual assemblage is olivine-richer. The horizontal width is 3 cm.
Fig. 4
Fig. 4. Triple oxygen isotope analyses of Archean and post-Archean olivines and orthopyroxenes showing overlap with San Carlos olivine.
Expected trends to higher-Δ′17O and lower and higher δ18O subduction fluids, derived from subducting slabs are shown. The δ18O in orthopyroxenes is higher than equilibrium olivine by 0.5–0.7‰ and nearly identical in Δ′17O at mantle temperatures (Fig. 3, ref. ).
Fig. 5
Fig. 5. A cartoon that explains the cooling of the Earth and rehydration of the mantle by low-δ18O fluids in spreading centers,, plate bending zones, and subduction zones,, generating progressively lower δ18O (and overall heterogeneous) continental lithospheric mantle (darker blue) after initiation of plate tectonics.
Δ′17O is not significantly modified by these processes (Fig. 4). Color code: yellow: low-δ18O peridotites, red: high-δ18O sediments, basalts, and eclogites, green: primitive mantle plumes, light blue: oceans. a Early Earth and moon regimes: degassed mantle, plume tectonics, rudimentary subduction around plumes, and intense hot mantle convection. The δ18O of the original peridotites is 5.57 ± 0.07‰, and Bulk Silicate Earth=Bulk Silicate Moon. b Modern plate tectonics regime: rehydration of mantle, plate accretion, and imbrication, lower-δ18O peridotites in the subcontinental lithospheric mantle samples by studied xenolith suites.
Fig. 6
Fig. 6. Co-evolution of the continental lithospheric mantle (CLM, this work) and the Earth’s crust as expressed by three proxies: granites, bulk shales, and zircons.
Note change in δ18O scale. Inset shows mass balance of CLM and crust during growth and evolution; 1:10 and 1:20 are assumed crust/CLM proportions based on the modern average lithospheric thickness of 150 km. BSE is estimated in this work and corresponds to the starting point of crustal growth after the Giant Impact. Unidirectional temporal loss of low-δ18O to the large reservoir of CLM helps to explain the accumulation of heavy δ18O in the crust and potentially hydrosphere (e.g., 57–60).

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