Elsevier

Lithos

Volumes 326–327, February 2019, Pages 435-445
Lithos

Effect of water on the magnesite–iron interaction, with implications for the fate of carbonates in the deep mantle

https://doi.org/10.1016/j.lithos.2019.01.004Get rights and content

Highlights

  • We studied the effect of hydrous fluid on the carbonate-iron reaction at 6–16 GPa

  • We observed formation of magnesiowüstite, graphite and carbide

  • In peridotite, pyroxenes react with magnesiowüstite resulting in olivine enrichment.

  • MgCO3 in hydrous system will be reduced during subduction to the transition zone.

  • MgCO3 can survive only at the coldest subduction P-T path or in anhydrous systems.

Abstract

The subduction of carbonates beyond 250–300 km, where redox conditions favour the presence of metallic iron (Fe), will result in redox reactions with the Fe dispersed in the silicate rocks. Here, we studied the effect of water on the carbonate–Fe interaction in the hydromagnesite–Fe system at 6, 8 and 16 GPa and the peridotite–CO2–H2O–Fe system at 8 GPa, using a multianvil apparatus. In all of the studied samples, we observed the formation of magnesiowüstite, graphite and carbide. Additionally, in the peridotite–CO2–H2O–Fe system, magnesiowüstite reacted with pyroxenes, resulting in olivine enrichment.

Kinetic calculations performed at 8 GPa showed that, at the pressure–temperature (PT) parameters of the ‘hot’, ‘medium’ and ‘cold’ subduction, about 40, 12 and 4 vol% of carbonates, respectively, would be reduced in the hydrous system within 1 Myr, assuming direct contact with Fe. Based on the present results, it is suggested that carbonates will largely be consumed during the characteristic subduction time to the mantle transition zone by reaction with the reduced mantle in the presence of hydrous fluid.

Graphical abstract

Interaction of carbonate containing subducting slab with the Fe–saturated mantle peridotites in the presence of the water-bearing fluid. The fluid phase in the described systems is an active reagent and a solvent, responsible for the transport of the components. The studied interactions occur due to the counter transport of oxidised and reduced components through the fluid phase. Carbonates in the hydrous systems will likely be totally reduced with the formation of diamond in the upper mantle and transition zone. CO2 – oxidised form of carbon dissolved in water fluid. H2 – reduced fluid, which can also contain hydrocarbons.

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Introduction

Investigations of mantle xenoliths, carbonatite and kimberlite and numerous experimental studies have revealed an important role of carbonates in the formation of the Earth's mantle heterogeneity and source regions for sublithospheric magmatism (Dasgupta and Hirschmann, 2010; Litasov, 2011; Yaxley et al., 1991). Carbonates drastically reduce the melting temperature of mantle rocks, peridotites and eclogites (Dasgupta and Hirschmann, 2010; Litasov, 2011), which leads to the formation of kimberlites and related alkaline rocks (Shatskiy et al., 2017). Due to their low density, viscosity and high reactivity, alkaline magmas affect the geochemistry of the surrounding mantle, and play a significant role in diamond formation (Stachel and Harris, 2008; Yaxley et al., 1991).

The subduction of oceanic slabs delivers a large amount of carbonates, predominantly calcite (Cal), dolomite (Dol) and magnesite (Mgs), into the mantle (Dasgupta and Hirschmann, 2010; Staudigel, 2014). Roughly 20–80% of the initial amount of carbonates may survive decarbonation beneath island arcs, and be further transported, beyond ~150 km depth, to the deep mantle (Kerrick and Connolly, 2001a, Kerrick and Connolly, 2001b). Indeed, findings of syngeneic inclusions of Ca- and Mg-carbonates in super-deep diamonds (Brenker et al., 2007; Bulanova et al., 2010) and carbonate-bearing marbles, gneisses, eclogites and ultramafic rocks from ultrahigh pressure metamorphic complexes (Shatsky et al., 1995), confirm the existence of carbonates in the upper mantle, transition zone and even in the lower mantle.

Cal and Dol are predominant among the carbonates of subduction zones at near-surface conditions (Plank and Langmuir, 1998; Staudigel, 2014). However, at high pressure, Cal reacts with silicates, such as garnet (Grt), enstatite or bridgmanite, forming Dol or Mgs (Brey et al., 1983; Yaxley and Brey, 2004). After the decomposition of Dol at about 4.5 GPa and 1000 °C (Sato and Katsura, 2001), Mgs remains as a major oxidised carbon phase in the peridotites and eclogites. However, although it has been experimentally confirmed that polymorphs of Mg‑carbonate are stable at extremely high temperatures and pressures (Fiquet et al., 2002), their presence in mantle assemblages mostly depends on the redox conditions.

Oxygen thermobarometry measurements on peridotites from the cratonic lithosphere have revealed that mantle rocks become progressively more reduced with depth due to the effect of pressure on the Fe3+/Fe2+ equilibrium (Frost and McCammon, 2008; Woodland and Koch, 2003). Stabilisation of the Fe3+-bearing end-members in the solid solutions of Grt, pyroxene and bridgmanite leads to the disproportionation of Fe2+ (Fe2+ → Fe3+ + Fe0), with the release of metallic Fe. Thermodynamic calculations and experiments have suggested that the mantle becomes metal saturated at depths exceeding 250–300 km (Ballhaus, 1995; Frost et al., 2004; Rohrbach et al., 2007). Studies on diamond inclusions have confirmed the presence of metallic Fe in the mantle. Inclusions of native Fe and Fe-Ni alloy have been detected in diamonds, together with carbide, wüstite (Wus), magnetite and sulphides, in equilibrium with typical upper mantle peridotite mineral assemblages, including olivine (Ol), Grt, and chromite (Sobolev et al., 1981; Stachel et al., 1998), and with Ca-perovskite in diamonds with a lower mantle origin (Kaminsky and Wirth, 2011; Smith et al., 2016).

Consequently, significant chemical heterogeneity in the redox conditions exists in the mantle, and the oxygen fugacity varies from approximately C–CO2 buffer (CCO) in the carbonate–bearing subducting slabs to the Fe–FeO buffer (IW) in the metal-saturated surrounding mantle. As a result of the existing redox gradient, redox reactions occur, and diamonds, or other reduced carbon species, can be formed directly by the reduction of carbonates or carbonatite melts (Palyanov et al., 2013; Rohrbach and Schmidt, 2011; Stachel and Harris, 2008). The mechanism and kinetics of these processes are extremely important for understanding carbon behaviour and its distribution in the deep Earth.

Carbonate–Fe interaction represents a simplified model of the processes that occur between the Fe-saturated mantle and the carbonate-bearing subducting slabs. Most of the previous experimental and theoretical studies have examined simplified carbonate–Fe systems, including MgCO3–Fe (Martirosyan et al., 2015a, Martirosyan et al., 2018; Zhu et al., 2018), CaCO3–Fe (Martirosyan et al., 2015b, Martirosyan et al., 2016) and (Ca,Mg)CO3–Fe (Dorfman et al., 2018; Palyanov et al., 2013). These works revealed the occurrence of redox reactions, with the formation of graphite (Gr)/diamond, Fe3C/Fe7C3 carbide and magnesiowüstite (Mws) or calcium Wus, depending on the initial composition of the carbonate. It is evident that, in order to further understand the carbonate–Fe reaction, an experimental study of the natural-like systems is required. This would include investigations on silicate- and H2O-containing systems.

Water is the dominant volatile component in the subduction zone (Peacock, 1990). The amount of water that survives dehydration at shallow depths is poorly constrained. Thermodynamic calculations have shown that the slab may retain from 7% to 35% of initial H2O, concentrated in basaltic crust, gabbro and peridotites, to 200–300 km depth (Schmidt and Poli, 1998; van Keken et al., 2011). Furthermore, the finding of fluid inclusions containing H2O in diamonds indicates the existence of hydrous fluid in the mantle (e.g.Izraeli et al., 2001 ; Klein-BenDavid et al., 2004 ; Navon et al., 1988). H2O in such fluids is commonly associated with C-bearing compounds, such as CO2 and carbonates, revealing that the C and H cycles are intimately related (Izraeli et al., 2001; Klein-BenDavid et al., 2004; Navon et al., 1988).

High-pressure peridotites with hydrous phases, phlogopite and amphibole, together with carbonates, discovered in ultrahigh-pressure terranes, provide another link between the carbon and water cycles in the deep Earth (Naemura et al., 2009; van Roermund et al., 2002; Zhang et al., 2007). The peridotite–COH system has been experimentally studied under oxidised conditions up to 32 GPa, with the main focus being on the melting relations (Litasov, 2011; Tumiati et al., 2012). However, the existing data for the systems with reduced COH fluid under the conditions relevant to the IW buffer are limited (Litasov et al., 2014; Taylor and Green, 1988).

Despite the fact that reactions in the MgCO3–Fe and CaCO3–Fe systems have been carefully studied, only a few works have been published that model the process in systems containing H2O. (Mukhina et al., 2017; Sonin et al., 2014) or in the peridotite–COH system (Rohrbach and Schmidt, 2011). In this study we explored the effect of water on the carbonate–Fe redox interaction in the hydromagnesite (hMgs)–Fe and peridotite–CO2–H2O–Fe systems under upper mantle and transition zone pressure–temperature conditions.

Section snippets

Experimental methods

High-pressure experiments were carried out using uniaxial presses equipped with the split-sphere guide blocks, USSA-1000 and USSA-5000, installed at the Institute for Planetary Materials, Okayama University, Misasa, Japan (IPM). Octahedra made of Cr-doped MgO semi-sintered ceramics were employed as pressure-transmitting media. Eight tungsten carbide (WC) cubes (F08 grade, Fujiloy Corp., Japan), with truncated corners, were used as Kawai-type anvils. Two cell assemblies, with a/b = 18/11 and

Results

Two series of experiments were conducted in the hMgs–Fe system: 1) isothermal experiments at 1100 °C and 6, 8 GPa, and at 1200 °C, 16 GPa, with the duration (t) varying from 1 to 720 min; and 2) for t = 60 min, at various temperatures ranging from 650 to 1100 °C at 8 GPa, and from 900 to 1200 °C at 16 GPa. In addition, two experiments in the peridotite–CO2–H2O–Fe system were conducted at 8 GPa and 1100 °C for t = 360 and 720 min. The experimental conditions and phase assemblages of the

Carbonate–Fe–H2O system

The presented data allow a reconstruction of the sequence of the processes in the carbonate–Fe system in the presence of hydrous fluid at 6, 8 and 16 GPa and 650–1200 °C. We start the discussion with an interpretation of the results obtained in the hMgs–Fe system (Fig. 5).

At the experimental pressure–temperature parameters, hMgs decomposes with the formation of Mgs, hydrous fluid and Brc or magnesium oxide:Mg5CO34OH2·4H2OhMgs=4MgCO3Mgs+MgOH2Brc+4H2OFl

This reaction (1) occurs up to 900 °C at

Conclusions

The experimental modeling of the hMgs–Fe and peridotite–CO2–H2O–Fe systems allowed the reconstruction of possible chemical processes that occur when fluids are involved in mantle–slab redox interactions under the P–T conditions of the upper mantle (6 and 8 GPa) and transition zone (16 GPa). A multistage reaction mechanism in both systems has been proposed: (i) an Fe + H2O reaction, with the formation of a reduced fluid and Wus; (ii) the reaction of MgCO3 with H2 transported in the hydrous

Nomenclature

    Alm

    almandine

    Brc

    brucite

    Cal

    calcite

    Cpx

    clinopyroxene

    Dol

    dolomite

    Fl

    fluid

    Grt

    garnet

    Gr

    graphite

    Grs

    grossular

    hMgs

    hydromagnesite, Mg5(CO3)4(OH)2·4H2O

    Mgs

    magnesite

    Mws

    magnesiowüstite

    Ol

    olivine

    Opx

    orthopyroxene

    Pyr

    pyrope

    Sp

    spinel

    Wus

    wüstite

Acknowledgements

We thank two anonymous reviewers for helpful comments which significantly improved the manuscript. The work is performed under the state assignment of IGM SB RAS. NM and IP were supported by the Russian Foundation for Basic Research RFBR project no. 18-35-00104. This study was performed using the joint facilities of the Institute for Planetary Materials, Okayama University.

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