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Fate of cobalt and nickel in mackinawite during diagenetic pyrite formation

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Published/Copyright: June 20, 2019
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Abstract

As iron sulfide mineral phases are important sedimentary sinks for naturally occurring or contaminant metals, it is important to know the fate of metals during the diagenetic transformation of primary sulfide minerals into more stable phases, such as pyrite (FeS2). Furthermore, the trace metal content of pyrite has been proposed as a marine paleoredox proxy. Given the diverse low-temperature diagenetic formation pathways for pyrite, this use of pyrite requires validation. We, therefore, studied nickel (Ni) and cobalt (Co) incorporation into freshly precipitated mackinawite (FeSm), and after experimental diagenesis to pyrite (FeS2) using S0 as an oxidant at 65 °C. Metal incorporation was quantified on bulk digests using ICP-OES or ICP-AES. Bulk mineralogy was characterized with micro-X‑ray diffraction (micro-XRD), documenting the transformation of mackinawite to pyrite. Epoxy grain mounts were made anoxically of mackinawite and pyrite grains. We used synchrotron-based micro-X‑ray fluorescence (µXRF) to map the distribution of Co and Ni, as well as to collect multiple energy maps throughout the sulfur (S) K-edge. Iron (Fe) and S K-edge micro-X‑ray absorption near edge spectroscopy (µXANES) was used to identify the oxidation state and mineralogy within the experimentally synthesized and diagenetically transformed minerals, and map end-member solid phases within the grain mounts using the multiple energy maps. Metal-free FeSm transformed to pyrite, with residual FeSm detectable. Co- and Ni-containing FeSm also transformed to pyrite, but with multiple techniques detecting FeSm as well as S0, implying less complete transformation to pyrite as compared to metal-free FeSm. These results indicate that Co and Ni may inhibit transformation for FeSm to pyrite, or slow it down. Cobalt concentrations in the solid diminished by 30% during pyrite transformation, indicating that pyrite Co may be a conservative tracer of seawater or porewater Co concentrations. Nickel concentrations increased several-fold after pyrite formation, suggesting that pyrite may have scavenged Ni from the dissolution of primary FeSm grains. Nickel in pyrites thus may not be a reliable proxy for seawater or porewater metal concentrations.

Introduction

Pyrite (FeS2) is the most abundant iron sulfide mineral on the surface of the Earth (Rickard and Luther 2007) and has formed in marine sediments (e.g., “diagenetic” pyrite) for at least 3.5 billion years (Gy) (Shen et al. 2001). The presence of pyrite, as well as its isotopic and elemental composition, has been applied to determining the redox conditions of the site of deposition, as well as the atmosphere and oceans. For instance, the presence of detrital pyrite in sediments >2 Gy old was one of the early indications of an anoxic Archean atmosphere (Holland 1984). Because of the enhanced mobilization of sulfate to the oceans from weathering of continental pyrite as oxygen appeared in the atmosphere, the presence of marine pyrite, formed either authigenically or diagenetically, tracks the timing of oxidation of the

Earth and atmosphere. Pyrite Fe and S isotopes are exploited to track the magnitude of pyrite burial through time (Rouxel et al. 2005; Tostevin et al. 2014), the amount of sulfate in the oceans (Canfield and Farquhar 2009), as well as atmospheric and ocean oxygenation (Mojzsis et al. 2003; Rouxel et al. 2005; Konhauser et al. 2011; Fakhraee et al. 2018).

Increasingly, though, scientists are also looking into the trace metal inventory of sedimentary pyrite as a reflection of the trace metal contents and redox conditions of the overlying water column. While investigations of trace metals in bulk clastic sediments, such as shales, are useful for this purpose, these studies tend to better highlight the utility of elements that undergo extreme authigenic enrichments in sediments under certain redox conditions (Algeo and Maynard 2004; Algeo and Rowe 2012), rather than those that are specifically incorporated by pyrite. The trace metals that become incorporated into pyrite by coprecipitation can reflect either the abundance of these elements in seawater (Huerta-Diaz and Morse 1992), and the metals can be sequentially extracted from existing sulfide phases (Huerta-Diaz and Morse 1990). Such targeted extractions can be extremely useful for modern sediments where multiple sulfide minerals may be present (e.g., Scholz and Neumann 2007; Olson et al. 2017).

As sediments lithify, there is a potential for resetting of the trace metal contents by diagenesis, fluid alteration, or metamorphism. Extraction of pyrites and associated trace elements in clastic rocks is subject to limitations based on extraction efficiency or extraction specificity (Harrison et al. 1973). In situ analysis of trace metals in pyrite by methods such as laser ablation ICP-MS (e.g., Large et al. 2014; Gregory et al. 2015) or electron microprobe microanalysis (EPMA) coupled to wavelength-dispersive spectroscopy (WDS) have the utility of unambiguously assigning metal enrichments to pyrite vs. other phases (e.g., organics, detrital minerals, or authigenic precipitates such as Fe- and/or Mn-oxides) (Chappaz et al. 2014). Laser ablation ICP-MS paths and quantitative elemental maps made by EPMA of individual pyrite grains, nodules, or framboids can also help to distinguish primary enrichments of trace metals from later overgrowths (Large et al. 2009; Swanner et al. 2013). Such findings are valuable to understanding pathways for economically significant trace metal enrichments (Tardani et al. 2017).

The availability of bioessential metals [e.g., Ni, Co, Cu, Mo, Zn, Se, etc.] in the Precambrian oceans is widely agreed to have controlled the origination and activity of microbial functional groups throughout Earth’s history, due to the use of metals as active centers in enzymes or in organic co-factors (Anbar and Knoll 2002). While there has been an effort to infer changes in the abundance of metals in the environment through the genomic and metallomic inventory of modern organisms (Dupont et al. 2006, 2010), direct sedimentary records of metal availability are necessary for constraining the availability of metals (Robbins et al. 2016). As with modern sediments discussed above, the bulk rock inventory or trace metals in shales deposited throughout Earth’s history is useful for informing general metal availability in the early oceans (e.g., Scott et al. 2008, 2012). Mineral specific metal analyses of chemical sediments, such as iron formations (Konhauser et al. 2009; Partin et al. 2013; Robbins et al. 2013; Swanner et al. 2014; Chi Fru et al. 2016), and in situ metal quantification directly from diagenetic pyrite (Large et al. 2014; Swanner et al. 2014; Long et al. 2016) can complement bulk analyses, and even provide direct estimates of seawater concentrations of some elements (Konhauser et al. 2009). Multiple, temporally resolved metal records from several sedimentary reservoirs highlight the co-evolution of life and its role in influencing ocean and atmospheric redox chemistry, in addition to its reaction to it (Robbins et al. 2016).

Co and Ni are a bioessential elements that are incorporated into iron sulfide precipitates (e.g., mackinawite), unlike metals that precipitate directly with sulfide (e.g., HgS) (Morse and Arakaki 1993), a result of the kinetics of exchange between water ligands for sulfide (S2–) (Morse and Luther 1999). This means that the incorporation of Co and Ni into mackinawite is predictable with a partition coefficient (Morse and Arakaki 1993), an observation validated by the near-quantitative incorporation of these elements from porewaters into sulfide minerals, including pyrite (Scholz and Neumann 2007; Olson et al. 2017). Changes in the marine Co reservoir through time determined from pyrite, bulk black shale, and iron formation Co contents are consistent, and indicate that pyrite Co contents may reflect concentrations in the water column (Swanner et al. 2014). Nickel is expected to behave similarly in the pyrite system (Morse and Arakaki 1993). Using the marine sedimentary record as an indicator of marine metal reservoirs presumes that diagenesis does not alter the original metal contents of these sediments. However, diagenetic metal mobilization is a possibility for iron (oxy)hydroxides (Frierdich et al. 2011), and loss, gain or redistribution of Co or Ni could occur as primary iron sulfides (e.g., mackinawite, greigite, or the aqueous FeS cluster, FeSaq) are transformed to pyrite during low-temperature diagenesis (i.e., <80 °C) or later fluid alteration.

The formation pathways of pyrite are debated, but it is generally understood that pyrite forms from an aqueous or precipitated FeS phase, such as mackinawite, greigite, or an aqueous or nanoparticulate FeS cluster (e.g., FeSaq) (Luther and Rickard 2005). At low temperatures (i.e., below 80 °C), hydrogen sulfide (H2S) is the product of microbial sulfate reduction at circumneutral pH (Jørgensen 1982), which can then precipitate with dissolved Fe2+ to form an FeS phase. The presence of S in the S1– oxidation state in pyrite indicates that S in any primary FeS precipitate must be oxidized from S2– and Fe removed (or S added) to form the mineral pyrite (Goldhaber and Kaplan 1974). This has been accomplished experimentally through oxidation of FeS solids (mackinawite or greigite) with S0 (Berner 1970; Sweeney 1972; Schoonen and Barnes 1991b), polysulfides (i.e., chains of S0 and S-1) (Rickard 1969; Hunger and Benning 2007), or H2S (Rickard 1997; Rickard and Luther 1997; Butler and Rickard 2000). Although the degree to which solid FeS minerals such as mackinawite actually exists in sediments has been questioned due to bias with the traditional acid-volatile sulfide (AVS) extraction (Rickard and Morse 2005), numerous studies have directly detected mackinawite (Burton et al. 2009; Morgan et al. 2012a; Kraal et al. 2013) and greigite (Keene et al. 2011) in the environment, justifying the use of these solids as precursor materials. Another possible formation route is direct pyrite formation through reductive dissolution or surface reactions of Fe(III) (oxyhydr)oxide minerals with H2S or polysulfides (Hellige et al. 2012; Peiffer et al. 2015; Wan et al. 2017). While specific mechanistic details vary, reaction of dissolved species and dissolution or recrystallization of an initial solid phase, such as mackinawite or greigite, and subsequent nucleation of pyrite are generally invoked (Wang and Morse 1996; Rickard and Luther 1997). Such reactions could mobilize trace metals co-precipitated or adsorbed with precursor phases.

In this study, two different pathways were used to convert freshly precipitated mackinawite (FeSm) containing Co and/or Ni into pyrite. The amount of metal in the FeSm and pyrite were quantified by bulk and microscale techniques to determine whether these metals are retained through diagenesis. Bulk and microscale techniques for both mineralogy and trace element quantification were coupled to give insights on the influence of these metals in promoting or inhibiting diagenetic pyrite formation.

Methods

Mineral synthesis

Mackinawite (FeSm) was synthesized from solutions of 0.6 M ferrous ammonium sulfate [Fe(NH4)2(SO4)2] and 0.6 M sodium sulfide (Na2S) (Rickard 1997). Both solutions were made with ultrapure water (conductivity 0.052 µS) that had been boiled and cooled under an N2 stream to make it anoxic. Sodium sulfide crystals were washed for 30 s with anoxic water to remove any oxidized S-species from the surface, then water was removed with a Pasteur pipette. Washed crystals were dried under an N2 stream and stored in a N2 atmosphere within a glass bottle with a butyl rubber stopper. Washed sodium sulfide crystals were weighed in an anoxic glovebox (100% N2). The ferrous ammonium sulfate and sodium sulfide solutions were made in glass serum bottles and sealed with butyl rubber stoppers with an N2 headspace. To synthesize FeSm, equal volumes of each solution were added via N2-purged syringes to a previously N2-purged and stoppered serum bottle under a slight vacuum (0.5 mbar). FeSm precipitated immediately. For the synthesis of FeSm that contained either Ni or Co, 4.7 mg NiCl2·6H2O or 190 mg CoCl2·6H2O powders were weighed into serum bottles and stoppered, then flushed with N2. This was accomplished by introducing N2 through a long needle, which bubbled the solution, and letting the overpressure escape through a second, shorter needle. An appropriate volume of the ferrous ammonium sulfate solution was added to achieve concentrations of 500 µM Ni or 2000 µM Co when mixed with the sodium sulfide solution. These solutions were then mixed with sodium sulfide as described above.

Pyrite synthesis was attempted by two different methods. The first, oxidation of FeSm with H2S (Rickard 1997) (hereafter “H2S oxidation”), was attempted to circumvent introduction of other solid S species (e.g., elemental sulfur, S0) that would be detected with later microanalysis. The reaction 13323-4 of Rickard (1997) was chosen (400 mg ferrous ammonium sulfate, 80 °C, pH 6, –250 mV, 4 mM H2S), as partial pyrite synthesis was reported from that reaction (80% pyrite and 20% mackinawite). Partial synthesis was desirable so that the partitioning of Co and Ni between the primary and secondary mineral could be evaluated. The anoxic solution of Ti(III) citrate and the phthalate buffer were made as described (Rickard 1997). The Na2S solution was made as described for mackinawite synthesis but then adjusted to pH 6 with anoxic 1 N HCl. Dry FeSm was weighed into a glass headspace vial with a small stir bar and closed with a stopper inside the glovebox. The buffer solution, Ti(III) citrate solution, and the Na2S solution were introduced via syringes that had been flushed with N2. The mixture was incubated in a sand bath at 80 °C on a temperature regulated hot plate, stirring, for either 4 or 20 days. At the end of the reaction, the headspace was flushed with N2.

The second pyrite synthesis method reacted FeSm with orthorhombic sulfur (S8, with sulfur in the S0 oxidation state) (Schoonen and Barnes 1991b), hereafter “sulfur oxidation.” FeSm was synthesized as described above. Dried FeSm (see below) was resuspended with pH 6 anoxic phthalate buffer in a stoppered serum vial. Orthorhombic sulfur was weighed and placed into a stoppered headspace vial, then the headspace was exchanged with N2. Inside the glovebox, the orthorhombic sulfur and a small stir bar were added to the FeSm-buffer solution and crimped with butyl rubber stoppers. The vials were placed in a sand bath at 65 °C on a temperature regulated hot plate, stirring, for 2 weeks. At the end of the reaction, the mineral suspension was centrifuged at 4000 rpm, the liquid removed with a 2-inch needle, and carbon disulfide (CS2) was introduced from a stock under N2 atmosphere to solubilize the unreacted orthorhombic sulfur. The suspension was centrifuged once again and CS2 removed prior to washing of the suspension with water (see below).

After synthesis, minerals in solution were spun at 4000 rpm for 10 min while still sealed in glass serum bottles. The liquid was removed with a 2-inch needle while N2 was being injected into the headspace using a second needle to maintain atmospheric pressure. Anoxic ultrapure water was added to the mineral suspension, and centrifugation repeated until the suspension had been washed twice. Then, vials were moved into the glovebox where the stoppers were removed. The serum bottles were covered with a paper tissue held in place by rubber bands. They were then placed in the vacuum chamber of the glovebox under a vacuum of –0.8 mbar until dried. Dried samples were stored in stoppered, N2-filled glass bottles at room temperature until further use.

All glassware used in the above protocols was acid washed for at least 24 h in 1 N HCl. This was followed by a 24 h soak in ultrapure water, followed by three rinses in fresh ultrapure water.

Embedding and polishing

Dried samples of synthetic mineral grains were sprinkled into plastic 1-inch diameter rounds either on the bench or inside a glovebox (90% N2/10% H2). Samples were then immediately placed under vacuum within a Polyvac vacuum impregnator (Presi GmbH) at 80 kPa for 15 min. Then, Araldite epoxy 2020 A/B was slowly added (100:35 vol) until the sample was covered. Embedding proceeded at 80 kPa for 90 min. Samples were left to set for 24 h before removing from the impregnator.

Embedded samples were first ground with abrasive papers: 1200 (15 µm), then 2500 (8 µm) using a PRESI Mecatech 334. Polishing utilized a PRESI diamond stick LD 33 (3 µm) and Presi RAM polishing cloth, followed by a final polish with 0.05 µm deagglomerated g alumina on a Buehler Chemomet I cloth (BUEHLER Micropolisch II 0.05 µm). Sample mounts were stored and transported in a nitrogen atmosphere. Just prior to synchrotron-based microanalysis, samples were polished with a 1 µm cloth to remove oxidized coatings.

Bulk analysis

Particle size of synthesized samples was analyzed with a Mastersizer 2000 (Malvern Instruments GmbH). The surface area of solids was analyzed using a Micromeritics ASAP 2000 BET analyzer. Dried samples were loaded onto a holder and kept anoxic (100% N2) until directly before analysis by m-X‑ray diffraction (XRD) on a Bruker D8 Discover instrument (Bruker, Germany) equipped with a CoKα X‑ray tube (k = 0.17902 nm, 30 kV, 30 mA) and GADDS area detector (Berthold et al. 2009). Mineral phases were identified using the International Center for Diffraction Data (ICDD) database.

Bulk trace element measurements were carried out by ICP-OES (Perkin Elmer Optima 5300 or Horiba Ultima 2) or an ICP-AES at University of Tübingen. Mineral samples (5–30 mg) were digested with aqua regia: 0.5 mL concentrated trace metal grade (TMG) HNO3 (65%) and 1.5 mL concentrated HCl at 60 °C. Residues were resuspended in 8 N TMG HNO3, and diluted 10-fold in 2% TMG HNO3. Elemental sulfur that did not dissolve was filtered through a 0.2 µm Whatman filter. Aqueous samples were preserved with and further diluted in 2% TMG HNO3.

Microscale analysis and spectroscopy

Elemental mapping by micro-X‑ray fluorescence (µXRF) and S and Fe K-edge X‑ray absorption near-edge structure (XANES) spectroscopy was performed at beamlines (BL) 14-3 and 2-3, respectively at Stanford Synchrotron Radiation Lightsource (SSRL). Sulfur distribution was mapped in approximately 1 × 1 mm areas at ~2500 eV on BL14-3, which has an energy range of 2100 to 5000 eV. The incident energy was selected using a Si(111) φ = 90 double crystal monochromator and the fluorescence signal was collected with a Si-drift diode Vortex detector (Hitachi) coupled to an Xspress3 pulse processing system (Quantum Detectors). The energy was calibrated to the thiosulfate pre-edge peak set to 2472.02 eV or a sulfate peak from CaSO4 set to 2483 eV. The spot size was 5 × 5 µm, unless otherwise noted, and dwell times were between 50 to 200 ms. For a subset of samples, S maps were collected at multiple energies (ME) around the S K-edge that corresponded to characteristic absorption features for monosulfides, pyrite, elemental sulfur, sulfite/metal monosulfides, sulfate, and total sulfur, in order of increasing energy. In 2013 these energies were 2470, 2471.5, 2472.5, 2476.5, 2483, and 2490 eV. In 2014 they were 2469.7, 2471.2, 2472.2, 2476.2, 2482.7, and 2499 eV. In 2015 and 2016 these energies were 2470.7, 2471.1, 2472.6, 2478.5, 2482.5, and 2499 eV. These maps were then deadtime corrected, and subjected to a principle component analysis (PCA) in the Microanalysis Toolkit (http://smak.sams-xrays.com) (Webb 2011). Compositionally diverse spots based on the absorption at different energies above the S K-edge were revealed by PCA, and these spots were chosen for S K-edge spectroscopy. Fluorescence spectra were collected from 2460 to 2500 eV. Spectra were deadtime corrected and normalized using the SIXPACK software package (Webb 2005). Within SIXPACK, the collected spectra from each sample (3 to 23 spectra per sample) were subjected to PCA to reveal the number of unique spectra. These end-members (EM), representing the compositional heterogeneity of all µXANES from an individual sample, were then fitted with spectra of reference sulfur compounds available from the ESRF (https://www.esrf.eu/home/UsersAndScience/Experiments/XNP/ID21/php.html) and additional samples from mineral collections and laboratory synthesis that were analyzed on BL 14-3 [these include mackinawite (FeS) and polysulfide]. Mackinawite was bulk dried powder from the FeSm synthesis described above, without added metals. The distribution of EM was then back-mapped using the characteristic fluorescence intensities at the specific energies in the MicroAnalysis Toolkit, similar to published methods (Mayhew et al. 2011; Farfan et al. 2018).

Iron, sulfur, and trace metals were mapped in approximately 0.5 × 0.5 mm areas at 8500 eV on BL2-3, which has an energy range of 4500 to 24 000 eV. The incident energy was selected using a Si(111) φ = 0 double crystal monochromator, and the fluorescence signal was collected with a Si-drift diode Vortex detector (Hitachi) coupled to an Xspress3 pulse processing system (Quantum Detectors). The energy was calibrated using the first inflection of an Fe0 foil as a standard (7112 eV). The spot size was either 2 × 2 or 5 × 5 µm, and dwell times were between 50 to 200 ms. Spots with different element intensities were chosen for Fe K-edge XANES (3 to 10 spectra per sample). Data were processed as described above.

Reference spectra used for fitting Fe K-edge XANES have been previously published (O’Day et al. 2004). Additional reference spectra were for Fe XANES collected as bulk samples on BL 4-1 at SSRL. Powdered samples were analyzed in sandwiches of “Kapton” tape, or in “Teflon” (polytetrafluoroethylene) holder windows sealed with Kapton tape. Where necessary, powders were diluted with boron nitride to reduce self-absorption effects. The XANES spectra were collected in transmission mode as well as in fluorescence mode using a Lytle detector. The E0 of an Fe0 metal foil placed behind the first transmission detector was adjusted to 7112 eV to energy calibrate the resulting spectra. Replicate spectra were then averaged and background subtracted in SIXPACK (Webb 2005).

Semi-quantitative analysis of elemental abundance was accomplished by calibrating to NIST-traceable standards of the elements of interest, which were deposited on mylar films measured at the same detector distance, incident energy, dwell time, spot size, and detector gain as the samples. A calibration file was assembled containing the information from the standard maps in the MicroAnalysis Toolkit, and applied to the sample. Because the samples were in thick mounts, the sample thickness was approximated as the absorption length for the mineral host, either FeSm or FeS2. Because individual grains may be thinner, especially on the margins than this absorption thickness, it is important to emphasize that this approach is only semi-quantitative. The amount of element per area was converted to concentrations as milligram metal per gram sample assuming one absorption length of either FeSm or pyrite as the sample depth. A mask was applied to the image to eliminate pixels that did not represent Fe- and S-containing particles, and the statistics were calculated on the selected pixels by the MicroAnalysis Toolkit.

Results

Characteristics of synthesized minerals

The bulk mineralogy of synthetic samples was determined by XRD. Reference minerals were mackinawite, greigite, pyrite, pyrrhotite, and elemental sulfur. Synthesized FeSm matched diffraction patterns for mackinawite, with minor greigite and pyrrhotite (Fig. 1). No peaks attributable to the iron oxides hematite, goethite, magnetite, or ferrihydrite were present (data not shown). The XRD pattern for FeSm with no metals was very similar to that with added Co or Ni. Transformation of FeSm with or without Co or Ni to pyrite via H2S oxidation (Rickard 1997) did not produce pyrite. However, peaks for mackinawite were sharpest in the FeSm sample with no metals that reacted the longest—20 days—whereas FeSm with either Co or Ni (reacted 4 days) had lower intensity peaks, the weakest in the sample that contained Ni. Pyrite was synthesized from FeSm both with and without Co or Ni using the sulfur oxidation protocol. Residual elemental sulfur was also detected in Co- and Ni-containing samples. The pyrite peaks had similar intensity irrespective of metal additions.

Figure 1 XRD of (a) FeS with and without Co and/or Ni, (b) FeS with and without Co and/or Ni after pyrite synthesis for 4 or 20 days using the H2S oxidation protocol, and after pyrite synthesis with and without Co and/or Ni formed using the sulfur oxidation protocol. Reference reflections are shown for mackinawite (red), pyrite (black), elemental sulfur (yellow), greigite (green), and pyrrhotite (blue). Elemental sulfur was a residual phase following the sulfur oxidation protocol.
Figure 1

XRD of (a) FeS with and without Co and/or Ni, (b) FeS with and without Co and/or Ni after pyrite synthesis for 4 or 20 days using the H2S oxidation protocol, and after pyrite synthesis with and without Co and/or Ni formed using the sulfur oxidation protocol. Reference reflections are shown for mackinawite (red), pyrite (black), elemental sulfur (yellow), greigite (green), and pyrrhotite (blue). Elemental sulfur was a residual phase following the sulfur oxidation protocol.

During synthesis with 0.1 L each of 0.6 M ferrous ammonium sulfate and Na2S solutions, 5.27 g of FeSm is calculated to have formed. FeSm had a BET surface area of 25.96 ± 0.29 m2/g, within the range of values reported in the literature for similar methodologies. Other BET measurements on synthetic freeze-dried FeSm resulted in 36.5 m2/g (Rickard 1997), 16–21 m2/g (Benning et al. 2000), and 47 m2/g (Wolthers et al. 2003). Particle size ranged from 2 to 138 µm, with greater than 90% of particles being less than 10 µm. Pyrite synthesized by sulfur oxidation had a BET surface area of 13.84 ± 0.21 m2/g. The surface area of Co-containing pyrite synthesized by sulfur oxidation was 18.06 ± 0.12 m2/g.

The results of S K-edge XRF and S XANES mapping of FeSm synthesized with Co or Ni are shown in Figure 2, with the composition and fitting results of identified EM spectra reported in Table 1. FeSm synthesized without metals was not mapped at ME through the S K-edge, so a similar map is not available. However, grains synthesized without metals were composed of FeS and sulfate, based on analysis of the spot S XANES spectra

Figure 2 Phase distribution maps generated from multiple XRF maps within the S K-edge and point XANES in FeSm synthesized with Co or Ni. For each sample, the end-member XANES points labeled on the map (numbers) correspond to the spectra at right, and their distribution is shown in the same color as the corresponding spectra. Fits are dotted black lines. The fit compositions, as reported in Table 1, are also given. Note that FeSm synthesized without metals was not mapped at multiple XRF energies. (a) Results of FeSm synthesis with Co added. (b) Results FeSm synthesis with Ni added.
Figure 2

Phase distribution maps generated from multiple XRF maps within the S K-edge and point XANES in FeSm synthesized with Co or Ni. For each sample, the end-member XANES points labeled on the map (numbers) correspond to the spectra at right, and their distribution is shown in the same color as the corresponding spectra. Fits are dotted black lines. The fit compositions, as reported in Table 1, are also given. Note that FeSm synthesized without metals was not mapped at multiple XRF energies. (a) Results of FeSm synthesis with Co added. (b) Results FeSm synthesis with Ni added.

Table 1

Sulfur XANES fit data

SampleNumber of spectraEnd-member (EM) IDFeSPyritePoly-sulfideSulfurSulfateaComp. sumχ2
FeS (embedded oxically; 2013)2610.680.371.056.71
FeS (embedded anoxically; 2014)10800.680.140.821.29
880.470.220.210.901.64
Pyrite (2015)880.200.740.050.991.33
100.060.780.110.950.51
FeS + Co (2015)7210.800.100.91.78
250.290.160.320.771.09
FeS + Co H2S (2013)8230.880.883.13
240.660.110.773.73
Pyrite + Co (2014)1240.120.630.220.961.02
70.290.690.983.17
FeS + Ni (2013)23270.680.140.821.63
310.620.411.0310.01
FeS + Ni H2S (2013)1020.820.060.882.84
40.830.080.9124.24
Pyrite + Ni (2015)9290.150.730.050.930.69
350.790.251.041.83
  1. a The sulfate standard was quenstedtite.

(Fig. 3; Table 1). The standard quenstedtite [a hydrated ferric sulfate, Fe2(SO4)3·11H2O] was used as a proxy for the presence of an inorganic sulfate, as this fit all of the samples in the study requiring it fairly well. Substituting another sulfate mineral (e.g., anhydrite) did not change the fit significantly (e.g., more than 10% improvement on Σ2 values; data not shown). It is important to note that inclusion of quenstedtite in the fit is not equivalent to detection of this mineral, as XANES is not a crystallographic technique. The use of quenstedtite in fits rather estimates the

Figure 3 (top) S XANES spectra from oxically embedded FeSm compared to the same sample embedded anoxically (bottom). Data are black circles, and fits are thin black lines.
Figure 3

(top) S XANES spectra from oxically embedded FeSm compared to the same sample embedded anoxically (bottom). Data are black circles, and fits are thin black lines.

amount of an inorganic sulfate-bearing phase (Zeng et al. 2013). The FeSm synthesized in the presence of Co or Ni similarly were fit with FeS and sulfate (Fig. 2). Although ME mapping was not performed at the Fe K-edge, Fe XANES from points on the FeSm with added Co sample map were fit by FeS and pyrrhotite (Table 2). In this case, the FeS spectra used was collected from a bulk powder of the FeSm synthesized without any metals. FeSm

Table 2

Iron XANES fit data

SampleNumber of spectraEnd-member (EM) IDFeSPyriteMarcasitePyrrhotiteMaghemiteComp. Sumχ2
Pyrite (2015)10151.011.011.55
160.620.401.020.05
200.570.431.002.91
FeS + Co (2013)820.700.321.030.49
FeS + Co H2S (2013)851.041.040.59
Pyrite + Co (2015)10530.990.991.20
540.990.992.16
580.420.591.010.17
FeS + Ni (2015)8260.700.301.000.24
300.480.541.021.06
FeS + Ni H2S (2013)310.950.956.85
Pyrite + Ni (2014)3430.830.140.970.93
450.370.510.879.11

with added Ni was fit with mostly FeS and some pyrrhotite.

The synthesized FeSm was sensitive to oxidation during embedding, polishing, and oxic handling during analysis. Figure 3 shows the EM S XANES spectrum of the FeSm embedded oxically, which was fit by the reference spectra for FeS (0.68) and sulfate (0.37) (Table 1). The EM spectra from FeSm embedded anoxically also fit with FeS and sulfate, but polysulfide was also necessary for a good fit (Fig. 3; Table 1). No ME map was collected, so it was not possible to assess the distribution of the phases. However, these spectra were determined to be representative of the 10 individual XANES collected on each sample by a PCA in SIXPACK. The FeSm with no metal sample was not analyzed at the Fe K-edge.

The results of S K-edge XRF and S XANES mapping on samples treated with the sulfur oxidation method are presented in Figure 4, with the EM spectra displayed and used to determine phase distributions and the spectral fitting results reported in Table 1. The FeSm with no metals added oxidized with the sulfur oxidation method resulted in predominately pyrite (Fig. 4a). Minor amounts of FeS were present in this and Co- and Ni-containing samples (Figs. 4b and 4c), visible as a shoulder at 2470 eV along the pyrite pre-edge absorption feature. Sulfate was also present, as with FeSm samples. No sulfur was detected by XRF/XANES, although it was observed by XRD (Fig. 1). When Co was present, the grains were predominantly pyrite, with some polysulfide and residual FeS (Fig. 4b). The matrix was composed of sulfur and polysulfide, which was not seen in the metal-free sample. When Ni was added, most grains were made of pyrite with some polysulfide, or pyrite with FeS (Fig. 4c).

Figure 4 Phase distribution maps generated from multiple XRF maps within the S K-edge and point XANES in experiments where pyrite was produced from sulfur oxidation. For each sample, the end-member XANES points labeled on the map (numbers) correspond to the spectra at right, and their distribution is shown in the same color as the corresponding spectra. Fits are dotted black lines. The fit compositions, as reported in Table 1, are also given. (a) Results of pyrite synthesis from FeSm with no metals added. (b) Results of pyrite synthesis from FeSm with Co added. (c) Results of pyrite synthesis from FeSm with Ni added.
Figure 4

Phase distribution maps generated from multiple XRF maps within the S K-edge and point XANES in experiments where pyrite was produced from sulfur oxidation. For each sample, the end-member XANES points labeled on the map (numbers) correspond to the spectra at right, and their distribution is shown in the same color as the corresponding spectra. Fits are dotted black lines. The fit compositions, as reported in Table 1, are also given. (a) Results of pyrite synthesis from FeSm with no metals added. (b) Results of pyrite synthesis from FeSm with Co added. (c) Results of pyrite synthesis from FeSm with Ni added.

The FeSm containing either Co or Ni treated with the H2S oxidation pathway did not produce pyrite, according to S XANES and XRF. The composition of EM S XANES spectra determined fitting was FeS with minor sulfate (Table 1). The Fe XANES spectra fit with an FeS standard (Table 2).

Trace element additions

The elemental concentrations of solutions used to synthesize FeSm were analyzed, but S was not calibrated, and Fe was often above the range of the calibration curve and could not be quantified (Table 3). The ferrous ammonium sulfate solutions with nickel chloride or cobalt chloride were measured before adding the sodium sulfide solution and had a concentration of 65.28 mg/L (1112 µM) Ni, which was diluted by an equal volume of sodium sulfide solution to achieve ca. 500 µM Ni final

Table 3

Elemental concentrations as determined on digests by ICP-OES or ICP-AES

ICP-OESFeCoNi
Solutions (ppm)
Ferrous ammonium sulfate (0.6 M)NA1.36 ± 2.364.39 ± 1.37
Hydrogen sulfide (0.6 M)1.67 ± 8.86BDBD
Ferrous ammonium sulfate (0.6 M) with 2 mM CoNA223.20 ± 0.334.40 ± 0.84
Ferrous ammonium sulfate (0.6 M) with 0.5 mM NiNA1.47 ± 0.4165.28 ± 0.97
Solids (mg element/g mineral)
FeS no metals327.53 ± 0.230.02 ± 0.020.05 ± 0.630
FeS+Co348.56 ± 0.073.71 ± 0.060.07 ± 0.11
FeS+Ni319.23 ± 0.360.023 ± 0.261.05 ± 0.26
FeS no metals H2S (20 days)480.87 ± 2.600.05 ± 6.450.06 ± 22.15
FeS no metals H2S (4 days)483.14 ± 1.650.03 ± 10.040.027 ± 68.14
FeS+Co H2S455.96 ± 0.854.05 ± 1.920.06 ± 2.82
FeS+Ni H2S493.71 ± 1.130.05 ± 0.401.43 ± 0.87
Pyrite no metalsNABDBD
Pyrite+CoNA1.1 ± 0.0BD
Pyrite+Ni327.7 ± 20.4BD3.4 ± 0.1
  1. Notes: NA = element was either not quantified, or element was above the range of quantification. BD = below detection. Detection limits were 0.0008, 0.0011, and 0.0015 ppm for Fe, Co, and Ni, respectively, for ICP-OES. Detection limits were 0.1, 0.1, and 0.2 ppm for Fe, Co, and Ni, respectively for ICP-AES. The relative standard deviations are also reported.

concentration. The solution with Co had 223.2 mg/L (3878 µM) Co, and was also diluted by an equal volume of the sodium sulfide solution to achieve ca. 2000 µM Co.

The Fe content of bulk solids determined with ICP-OES increased after applying the H2S oxidation protocol (Table 3). The Fe content was only quantified in the Ni-containing sample after sulfur oxidation, due to the range of ICP-AES and standard concentrations. For the Co- and Ni-bearing solids, Co and Ni were quantified in bulk by either ICP-OES (FeSm and H2S oxidation samples) or ICP-AES (sulfur oxidation samples; Table3) or semi-quantitatively mapped by X‑ray fluorescence at 11 keV on individual pixels (Table 4). The measured values of Co and Ni in FeSm, measured by ICP-OES were 1.05 ± 0.26 mg Ni per g FeSm, and 3.71 ± 0.06 mg Co per g FeSm, higher than the range of the median values obtained by synchrotron-based XRF mapping on beamline 2–3 at 11 keV: of 0.4 ± 0.2 mg Ni per g FeSm and 3.1 ± 0.7 mg Co per g FeSm. Quantification of Ni after sulfur oxidation diverged the most between methods. ICP-AES measured 3.4 ± 0.1 mg Ni per g mineral, while XRF maps contained median values of 0.5 ± 0.4 mg Ni per g mineral. Results for Co after sulfur oxidation were comparable by bulk and microscale methods. Maps of particles used for XRF quantification are shown in Supplementary[1] Figure S1.

Discussion

Mineral transformation

For the FeSm synthesized in this study, XRD documented the mineral mackinawite, with minor greigite and pyrrhotite (Fig. 1). The best fitting standard for S XANES spectra was with FeS, a mackinawite standard, occasional polysulfide, and varying amounts of sulfate (Table 1). Even after embedding in the glovebox, the FeSm still shows signs of oxidation, shown by the inclusion of sulfate and polysulfide in the fits, although it may be less oxidized than samples embedded in the air (Fig. 3). Less sulfate was needed to fit the anoxically embedded samples, however, indicating some success of the protection from oxygen. The presence of polysulfide may have resulted from some sample hydration during storage, as the sample was anoxically embedded a year after oxically embedded samples, although they were stored under dry N2 in airtight containers. As sulfate minerals were not detected in XRD (detection limit 5 wt%), oxidation likely occurred during the storage, embedding or analysis of samples, and not during synthesis or transformation protocols. There was a major reflection at about 35° in the FeSm that could be greigite or pyrite, but other major reflections for these minerals were absent. The addition of Co or Ni did not appear to alter the mineralogy of the FeSm, or to change the intensity or width of reflections (Fig. 1).

The attempts to transform FeSm, with or without Co and/or Ni,to pyrite via H2S oxidation were not successful. From XRD, the sample still appeared to be mackinawite, with the most intense reflections in the Co-containing samples (Fig. 1). The Ni- and Co-containing samples were only reacted 4 days and yet had much more intense reflections for mackinawite than FeSm without metals, reacted either 4 or 20 days. The failure of the H2S oxidation method to produce pyrite from FeSm synthesized with Co or Ni was also verified by S XANES and XRF mapping (Table 1), as well as by point Fe XANES analysis (Table 2). These results are consistent with several studies, which found very slow reactions between mackinawite and H2S to form pyrite (Berner 1970; Schoonen and Barnes 1991b; Wilkin and Barnes 1996; Benning et al. 2000). It has been suggested that the freeze-dried FeS, used in the successful synthesis of pyrite via H2S oxidation (Rickard 1997), underwent minor oxidation by oxygen during drying, providing oxidized surface sites for the formation of pyrite via reaction with H2S (Benning et al. 2000). Secondary electron microscopy (SEM) studies of freeze-dried mackinawite in that second study noted an oxidized sulfate mineral phase, as well as a change in morphology from freshly precipitated mackinawite (Benning et al. 2000). In this same study, the freeze-dried material produced pyrite in reaction with H2S (100% transformation after 9 days),

whereas freshly precipitated mackinawite reacted with H2S did not. Our finding that N2-dried mackinawite does not react with H2S to form pyrite further support the claim (i.e., Benning et al. 2000) that H2S oxidation of mackinawite is not a significant reaction in the formation of pyrite at low temperatures.

In contrast, pyrite was formed from the sulfur oxidation method, evident in clear reflections for pyrite from XRD in metal-free samples (Fig. 1). After pyritization, most XRD reflections for mackinawite had disappeared, indicating a near-complete reaction. From the S ME mapping and EM XANES, pyrite was also the main product (Fig. 4; Table 1), with minor FeS and sulfate, likely reflecting oxidation during sample mounting and/or analysis (e.g., Fig. 2). The spot Fe XANES analysis also documented pyrite, but the product still retained some FeSm (Table 4). In addition, marcasite was a component of Fe XANES fits (Table 4), which likely reflects the same sulfur oxidation state and similar orbital energy levels of Fe in pyrite and marcasite (Jones 2006), rather than the presence of marcasite. The Fe XANES of pyrite and marcasite are very similar (O’Day et al. 2004). The inclusion of pyrrhotite in some fits could reflect some oxidation during embedding, storage, or analysis.

Pyrite was also produced in the Co-containing solids, as shown by XRD, S XANES, and Fe XANES. In the Co-containing samples, an additional intense reflection for sulfur was present at about 26°, and several minor reflections between 30–35° in the XRD data (Fig. 1). These likely correspond to residual sulfur retained after CS2 washing. The single CS2 wash must have been insufficient to remove sulfur. It is significant that evidence for residual sulfur is not seen in the metal-free product. In Co-containing samples analyzed by S XANES, FeS was still present in pyrite grains (visible as a shoulder at 2470 eV), as was polysulfide (Fig. 4). Sulfur and polysulfide comprised the matrix, consistent with the intense reflections for sulfur by XRD. Polysulfides form in the reaction of elemental sulfur with water, and themselves react with FeSm to form pyrite (Schoonen and Barnes 1991b), and so are expected S phases during pyrite formation by the S0 oxidation method. By Fe XANES, both pyrite/marcasite and FeS were components of fits. Taken together, these data indicate that the presence of Co impeded reaction of FeSm to pyrite in the time course of the experiments (2 weeks). Although FeSm was still detectable in metal-free product, the absence of any detectable sulfur may signify that metal-free FeSm reacted more completely than Co-amended FeSm. Inhibition of FeS transformation to pyrite has been observed in the presence of arsenate [As(V)], although this is linked to arsenate oxidizing both Fe and S (Wolthers et al. 2007). An analogous pathway can be excluded for Co2+, as its reduction in the aqueous phase is unlikely. Arsenate and arsenite ([As(III)] can also prevent FeS transformation to pyrite by sorption and blockage of surface sites (Wolthers et al. 2007). Although, Co does not adsorb even as strongly to FeS as Ni (Morse and Arakaki 1993), yet Ni-containing FeS appears to have more completely reacted in our experiments (see below). The lower concentrations of Co in pyrite compared to FeS (Tables 3 and 4) indicate that some Co could have been mobilized from solid phases during the reaction and available for sorption. It is impossible to rule out inhibition of pyrite formation due to Co sorption with our data.

Table 4

Semi-quantitiative Co and Ni concentrations determined from XRF maps

Solids (mg element/g mineral)ElementMeanMediane.s.d.
FeS+Co (2013)Co43.61.6
FeS+Ni (2013)Ni0.50.40.3
FeS+Co+H2S (2013)Co3.23.10.7
FeS+Ni+H2S (2013)Ni0.50.40.2
Pyrite+Co (2014)Co1.61.30.5
Pyrite+Ni (2014)Ni0.60.50.4
  1. Analytical precision was 0.1 mg element/g FeSm, which is estimated detection limit.

For Ni-containing samples, the predominant product of sulfur oxidation was pyrite, based on XRD, S XANES, and Fe XANES analyses. Some residual FeSm was present based on S and Fe XANES (Tables 1 and 2). One Fe XANES EM also fit with maghemite, indicating Fe oxidation, which likely occurred during sample embedding, storage, or analysis, as it was not detected by XRD prior to these steps. Sulfur was also present based on XRD, but the diffraction peaks were not as sharp or as large as for the Co-containing product. Polysulfide was detectable in S XANES (Fig. 4). The reaction of FeSm to pyrite also seems to be incomplete in the presence of Ni, but may have progressed further given the evidence for more abundant sulfur/polysulfide in the Co-containing grains. Another line of evidence is the more abundant distribution of sulfur-rich grains in Co-containing product, as revealed by the 8000 eV XRF map (Supplementary[1] Fig. S2) as compared to the Ni-containing product, although the sample size is just a few grains.

These results of incomplete pyrite formation in Ni-containing samples are in contrast to the recent observation that the presence of Ni accelerates the rate of pyrite formation (Morin et al. 2017). In that work, pyrite was formed from de novo synthesis from slightly acidic (ca. pH = 5.5) solutions of ferric chloride and H2S (Noël et al. 2014, 2015). In this mechanism, Fe(III) must be the oxidant, whereas our protocol started with solid FeSm and utilized sulfur as the oxidant. The authors proposed that Ni impurities accelerated pyrite nucleation from solution (Morin et al. 2017), which is generally slow. However, formation of pyrite in marine sediments likely proceeds from the nucleation and subsequent sulfidization of FeS minerals, such as mackinawite and greigite (Schoonen and Barnes 1991a), rather than through reaction of aqueous Fe(III) and H2S. This inference is supported by the observation of FeS phases being converted to pyrite with depth in numerous anoxic sediments (Cutter and Velinsky 1988; Huerta-Diaz and Morse 1992; Scholz and Neumann 2007). Our experiments, therefore, suggest that Ni (and Co) impurities might impede the rate of pyritization in pH circum-neutral sediments, although others note that Ni and Co may more completely pyritize than other metals (Morgan et al. 2012b).

The weight percent of Fe in FeSm calculated from bulk digestion data in Table 3 was about 30–40%, less than the predicted 63.5% for a 1:1 Fe:S stoichiometry. This lower weight percent iron may have been caused by sulfate precipitation during drying, as discussed above. After the H2S oxidation protocol, the weight percent of iron increased to 42–51%, closer to stoichiometric FeS, but still lower than expected. This may be due to increasing crystallinity of the FeSm in the aqueous phase (Rickard 1995), which has support from the sharpening of diffraction peaks (Fig. 1) or washing out of excess sulfate with the fluids used for H2S oxidation. Although the Fe content was not determined on most solids produced by the sulfur oxidation protocol, the Fe content for pyrite for the Ni-containing sample was ca. 33 wt%, whereas stoichiometric pyrite should have 46.55% Fe. This likely reflects residual sulfur in the solid sample after the sulfur oxidation method, as well as the persistence of FeSm.

Trace element incorporation

The distribution coefficient for Co in FeSm at 25 °C is 29 ± 3 (Morse and Arakaki 1993), which predicted 16 ± 2 mg Co per g FeSm in our synthesized mineral. The measured values of Co were 2.6 to 3.7 mg Co per g mineral were well under this range. Based on the published distribution coefficient of 280 ± 181 for Ni in FeSm at 25 °C (Morse and Arakaki 1993), we expected to see 3.9 ± 2.5 mg Ni per g FeSm. The measured value of Ni in FeSm (0.6 to 1.05 mg Ni per g mineral) was below this range (Table 3). In those experiments, mackinawite was synthesized by slow titration, whereas our FeSm was synthesized rapidly by mixing a Co- or Ni-bearing iron solution with a sulfide solution. It is likely that this fast precipitation did not allow full uptake of the likely equilibrium values of Co and Ni observed in slow precipitation experiments (Morse and Arakaki 1993). This may be due to the slower exchange of H2O ligand for S2– on Co2+ and Ni2+ ions as compared to Fe2+ ions (Morse and Luther 1999).

After the H2S oxidation protocol, the measured value was 4.05 ± 1.92 mg Co per g mineral, and 1.1 mg Co per g mineral after the sulfur oxidation protocol. Cobalt enrichments in FeSm are generally present in all particles based on XRF mapping of the synthesized minerals at 8500 eV (Supplementary[1] Fig. S2). In the samples mapped after sulfur oxidation, Co was distributed throughout the Fe-rich particles. From cross-plots of the Fe and S pixels, the Fe-rich particles always contain some S, and so are inferred to be FeSm/pyrite. The sulfur-rich grains comprise a very low-Fe population of pixels and are likely sulfur/polysulfide-rich grains (analyses not shown). Cobalt is visible in the FeSm/pyrite grains, but absent in the sulfur/polysulfide grains, indicating that Co is preferentially incorporated into sulfide minerals. From the bulk (ICP-OES or ICP-AES) and XRF metal quantification, there was general agreement between the techniques for the quantity of Co in both FeSm and sulfur oxidation products (Fig. 5). However, Co was quantitatively lost from the samples during transformation. The lower concentration of Co in Fe-rich particles by XRF after pyrite transformation (Supplementary[1] Figs. S1 and S2) indicates this is not a phenomenon of solid-phase dilution with residual sulfur for the ICP analyses. Therefore, it seems likely that Co is lost from the sulfide phase during the transformation of FeSm to pyrite.

Figure 5 Amount of metal in the solids produced from FeSm and pyrite synthesis in the presence of Co or Ni. The average of triplicate bulk measurements by ICP-AES or ICP-OES are in black, with error bars representing the standard deviation. The median of individual pixels in grains determined on XRF maps collected at 8500 eV. The error bars are the standard deviation of these data.
Figure 5

Amount of metal in the solids produced from FeSm and pyrite synthesis in the presence of Co or Ni. The average of triplicate bulk measurements by ICP-AES or ICP-OES are in black, with error bars representing the standard deviation. The median of individual pixels in grains determined on XRF maps collected at 8500 eV. The error bars are the standard deviation of these data.

After treating FeSm with the H2S oxidation protocol, Ni increased to 1.43 ± 0.87 mg Ni per g mineral. The amount in pyrite produced from the sulfur oxidation protocol was 3.4 ± 0.1 mg Ni per g mineral. In Ni-containing samples, the FeSm has Ni distributed throughout all grains. In the Ni-containing product oxidized by sulfur, both S- and Fe-rich grains are visible in the XRF map, similar to the Co-containing sample (Supplementary[1] Fig. S2). In the product, some Fe-rich grains are preferentially enriched in Ni, while others are Ni-poor, distinct from the Co-rich product. The S-rich grains have little Ni. Asno multi-energy maps were made at these higher energies on BL2-3 (e.g., the Fe K-edge), it is not possible to say whether Ni preferentially incorporated into discrete iron sulfide phases, such as FeSm or pyrite. Other studies have documented a preference of Ni for the pyrite vs. mackinawite mineral (Noël et al. 2015). This may be consistent with preferential Ni concentration in pyrite-bearing grains, as opposed to FeSm grains, although we cannot validate this with the current data set. The ICP data always detected more Ni in the samples than is apparent with the synchrotron-based XRF maps (Fig. 5), likely indicating the need for further matrix correction for XRF standards. Both techniques show an increase of Ni in the solid after sulfur oxidation, although this increase is unlikely to be statistically significant in the XRF data. It is possible that in the case of dissolution of FeS, and incomplete pyrite formation, mobilized Ni was effectively sequestered in fewer grains, increasing the concentration.

A final observation is that the addition of Co or Ni shifted thepre-edge peak position of the FeS in the S XANES spectra to

more positive values (Fig. 6), which was more extreme for Ni. A similar peak shift was noted for pyrite, although only for Ni. Other authors noted longer bond distance (2.28 Å) for Ni-S than for Fe-S (2.26 Å) based on Ni EXAFS of mackinawite synthesized with Ni (Wilkin and Beak 2017). However, shorter bond distances generally require higher excitation energy. It may more likely reflect the ordering of stability constants of the transition metal series, e.g., the Irving-Williams order, Fe < Co < Ni < Cu > Zn (Rickard and Luther 2006). Although the amount of the non-Fe metal is small, these pre-edge peaks may reflect the increased energy needed to achieve electronic transitions to empty hybridized Me-S and S-S anti-bonding orbitals.

Figure 6 Overplots of end-member FeSm and pyrite S XANES from samples synthesized with and without Co and Ni. The presence of Ni causes a shift for the pre-edge feature of FeSm and pyrite to be shifted to higher energy. A subtle shift is observed with Co, but only for FeSm.
Figure 6

Overplots of end-member FeSm and pyrite S XANES from samples synthesized with and without Co and Ni. The presence of Ni causes a shift for the pre-edge feature of FeSm and pyrite to be shifted to higher energy. A subtle shift is observed with Co, but only for FeSm.

Implications

The experiments described herein attempt to determine how efficiently the trace metals Ni and Co are pyritized under low-temperature pyrite formation from mackinawite. A first and important result was that oxidation of FeSm by H2S did not produce pyrite, casting doubt on the validity of this as a pyrite formation pathway in the absence of oxidized surface sites. However, pyrite was successfully synthesized through oxidation of FeSm with elemental sulfur. The equilibrium concentration of Co and Ni in the initial FeSm predicted by the published distribution coefficients was not attained in our experiments due to the fast precipitation method used. Cobalt was lost from the solid during transformation, as shown by the diminished concentrations of Co in pyrite compared to FeSm. The concentration of Ni increased during transformation, possibly due to the dissolution of FeSm and preferential sequestration of Ni in pyrite. In both cases, pyrite formation was not complete in the presence of added metals, indicating a kinetic inhibition to the formation of pyrite in the presence of Co and Ni. Taken together, these results suggest that if the pyrite formation pathway can be determined to initiate from a precursor FeS phase, the concentration of Co in pyrite could serve as a conservative record of environmental concentrations. Nickel, however, seems unreliable in this capacity, as pyrite appears to take up additional Ni in comparison to precursor FeSm, during its formation, as well as incorporate in other phases, such as elemental sulfur. A caveat of this work is that other pyrite formation mechanisms are possible, e.g., from another solid-phase precursor mineral such as greigite or by reductive dissolution of Fe(III) (oxyhydr)oxides with hydrogen sulfide or an aqueous or colloidal species (e.g., FeSaq), and the fate of trace metals during transformation should also be evaluated under those conditions. Also, our results are specific only to Co and Ni, and should not be extrapolated to other metals.


Orcid 0000-0001-9507-0893

† Special collection papers can be found online at http://www.minsocam.org/MSA/AmMin/special-collections.html


Acknowledgments

We thank Ellen Roehm for performing BET, Mastersizer, and ICP-AES analysis of samples. James Byrne and Maximilian Halama analyzed samples by µXRD. Stefan Peiffer and Mali Wan gave helpful advice regarding the synthesis of pyrite. Tabea Schmid and Bertrand Ligous assisted in developing and performing the epoxy embedding and polishing of samples. The polysulfide standard was a gift of Greg Druschel and Fotios Kafantaris. Sümeyya Eroglu, Maximilian Halama, and Aude Picard assisted with measurements at the SSRL. Courtney Roach assisted with beamline optimization and data interpretation.

  1. Funding This work was funded by a Deutsche Forschungsgemeinschaft grant (KA 1736/24-1). Use of the Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, is supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Contract No. DE-AC02-76SF00515.

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Received: 2018-10-03
Accepted: 2019-03-18
Published Online: 2019-06-20
Published in Print: 2019-07-26

© 2019 Walter de Gruyter GmbH, Berlin/Boston

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