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BY-NC-ND 4.0 license Open Access Published by De Gruyter September 20, 2020

Archean to Paleoproterozoic seawater halogen ratios recorded by fluid inclusions in chert and hydrothermal quartz

  • Ray Burgess ORCID logo , Sarah L. Goldsmith , Hirochika Sumino , Jamie D. Gilmour , Bernard Marty , Magali Pujol and Kurt O. Konhauser
From the journal American Mineralogist

Abstract

Past changes in the halogen composition of seawater are anticipated based on the differing behavior of chlorine and bromine that are strongly partitioned into seawater, relative to iodine, which is extremely depleted in modern seawater and enriched in marine sediments due to biological uptake. Here we assess the use of chert, a chemical sediment that precipitated throughout the Precambrian, as a proxy for halide ratios in ancient seawater. We determine a set of criteria that can be used to assess the primary nature of halogens and show that ancient seawater Br/Cl and I/Cl ratios can be resolved in chert samples from the 2.5 Ga Dales Gorge Member of the Brockman Banded Iron Formation, Hamersley Group, Western Australia. The values determined of Br/Cl ~2 × 10-3 M and I/Cl ~30 × 10-6 M are comparable to fluid inclusions in hydrothermal quartz from the 3.5 Ga North Pole area, Pilbara Craton, Western Australia, that were the subject of previous reconstructions of ancient ocean salinity and atmospheric isotopic composition. While the similar Br/Cl and I/Cl values indicate no substantial change in the ocean halide system over the interval 2.5–3.5Ga, compared to modern seawater, the ancient ocean was enriched in Br and I relative to Cl. The I/Cl value is intermediate between bulk Earth (assumed chondritic) and the modern seawater ratio, which can be explained by a smaller organic reservoir because this is the major control on marine iodine at the present day. Br/Cl ratios are about 30% higher than both modern seawater and contemporary seafloor hydrothermal systems, perhaps indicating a stronger mantle buffering of seawater halogens during the Archean.

Introduction

There have been relatively few studies of halogens in the Archean oceans, and no reliable record of seawater halogen evolution has been compiled. In particular, past salinity changes in the oceans are largely unconstrained, and the biologically controlled evolution of the iodine cycle remains unknown. Previous studies have analyzed fluid inclusions to determine halogen ratios in Precambrian seawater. However several factors have hampered the interpretation of these results for understanding the halogen composition of the early oceans, including: the challenges of delimiting primary seawater composition in mixed hydrothermal fluids formed during seawater-basalt interaction processes; possible overprinting during later metamorphic and deformation events; and the analytical difficulties of determining low halogen concentrations, especially for least-abundant iodine.

The limited halogen data that exist are mainly derived from fluids associated with volcanic-sedimentary successions. This includes mid-Archean (~3.2 Ga) ironstone pods, and silicified komatiites and sediments from the Barberton Greenstone Belt, Kapvaal, South Africa (Channer et al. 1997; de Ronde et al. 1997; Farber et al. 2015); hydrothermal quartz in metabasalts from the ~3.4 Ga North Pole area, Pilbara, Western Australia (Foriel et al. 2004); and volcanic-related quartz veins and pods in the Paleoproterozoic (2.22 Ga) Ongeluk Formation, Kapvaaal, South Africa (Gutzmer et al. 2003).

Fluid inclusions in quartz veins hosted in ironstone pods from Barberton have chemical compositions that approximately match modern seawater, except for higher Br/Cl and I/Cl (de Ronde et al. 1997; Channer et al. 1997). These fluids may have been trapped fluids from seafloor hydrothermal vent systems (de Ronde et al. 1997), however both their age and origin is contested (de Ronde et al. 2004; Lowe and Byerly 2004), leading to uncertainty for their use in reconstructing early ocean chemistry (Lowe and Byerly 2003, 2007; Hren et al. 2006).

Crush-leach analysis of fluid inclusions in chert and quartz veins in komatiites from Barberton yielded Br/Cl and I/Cl much higher than modern seawater and, although some overlap with the range reported by Channer et al. (1997), most are considerably higher, similar to those observed in organic-rich fluids (Farber et al. 2015) and also inclusion fluids present in minerals in rocks from Caledonides, western Norway (Svensen et al. 2001), perhaps indicative of a metamorphic overprint.

North Pole hydrothermal quartz contains several types of fluid inclusions with variable Br/Cl values that are 1–2 times modern seawater values (Foriel et al. 2004), and quartz-bearing fluid inclusions from the Onglevlauk Formation also have Br/Cl ratios ≥2 times the modern value (Gutzmer et al. 2003). In these studies, the elevated Br/Cl values are thought to reflect the influence of mantle-derived hydrothermal vent compositions, as there was likely insufficient organic matter present to fractionate Br from Cl toward the modern value. Only in settings isolated from the main oceans, such as in the lagoonal depositional environment proposed for the North Pole area, was there sufficient organic matter to decrease the Br/Cl ratio of seawater toward the modern value (Foriel et al. 2004).

Temporal changes in seawater Cl abundance (salinity) has also been a topic of interest, with suggestions that Precambrian oceans may have been between at least two times more saline than the modern value (Knauth 1998; Weiershäuser and Spooner 2005). Due to its formation in volcanic hydrothermal systems, quartz rarely contains primary seawater in fluid inclusions, making it difficult to reconstruct seawater salinity. However, Marty et al. (2018) used 36Ar/Cl/K mixing relationships in fluids extracted from 3.4 Ga North Pole quartz to show that Archean seawater had comparable Cl salinity to modern oceans.

Martin et al. (2006) reviewed available evidence for Archean and Proterozoic seawater chemistry noting the similarity with Ca-Na-Cl and Na-Ca-Cl brines found in most Precambrian shields including Finland, Sweden, Russia, and Canada. They considered that the chemical composition of Archean seawater may have been comparable to modern seawater but was modified by water-rock interactions or contamination by hydrothermal fluids. A common finding of previous studies is that Archaean ocean water chemistry was strongly buffered by mantle input by emission of dissolved ions from mid-oceanic vents and high-temperature water-rock interactions in the oceanic crust (Martin et al. 2006).

The approach and rationale used in this study is outlined as follows. First, we have determined the halogen ratios (Cl, Br, I) in fluid inclusion-bearing hydrothermal quartz from the North Pole area. These samples have been the subject of several previous studies, in particular to determine their fluid compositions and Br/Cl ratios (Foriel et al. 2004), seawater salinity (Marty et al. 2018), and ancient atmospheric isotopic compositions of Ar, Xe, and N2 (Pujol et al. 2011, 2013; Marty et al. 2013; Avice et al. 2018). Second, we analyzed halogens in cherts from the Dales Gorge Member of the Brockman Iron Formation, Hamersley Group, Western Australia. Chert in Banded Iron Formations (BIF) is considered to be an early diagenetic phase derived either from abiogenic amorphous silica or a siliceous Fe oxyhydroxide precursor phase. Silica precipitation occurred directly from Si-saturated seawater or via absorption of Si on Fe hydroxides (e.g., Morris 1993; Maliva et al. 2005; Posth et al. 2008). The microcrystalline nature of BIF chert means primary seawater is likely to be initially trapped between particles/colloids during deposition. Some of this fluid will subsequently be retained in intercrystalline porosity formed during diagenesis and dewatering. Fluid flow and particle redistribution in this microporous network has recently been considered by Egglseder et al. (2018) as a process that may lead to the formation of chert/iron-rich microbands. Cherts are widespread and common throughout the geological record and preserve the earliest fossils, single cell walls and filaments, e.g., those found in the 3.47 Ga old Apex Chert of Western Australia (Schopf et al. 2002). They also have low permeability and are resistant to later dissolution and reprecipitation, and even during metamorphic recrystallization water/rock ratios are usually so low that δ18O is unaffected (Knauth and Lowe 2003). Cherts have been used to investigate the physical and chemical conditions in past oceans in numerous studies (reviewed by Konhauser et al. 2017), although not previously for halogens, so they are assessed here as an alternative record of seawater halogen ratios, independent from that obtained from hydrothermal quartz.

Third, we pay particular attention to the I/Cl value of seawater. Iodine has a much higher affinity for organic matter, potentially making it a potent indicator of the biological influences on ocean water chemistry. There has been only one previous estimate of the I/Cl ratio of Archean oceans of ~40 × 10-6 M (Channer et al. 1997), which is higher than present day value of 0.86 × 10-6 M (Li 1991). The biophilic behavior of I has led to suggestions that the iodine abundance of the oceans may have decreased over time in response to evolutionary changes (e.g., de Ronde et al. 1997; Hardisty et al. 2014). Changes in reservoir size of biologically related iodine in the oceans would also have impacted atmospheric chemistry because volatile organohalides influence the oxidative capacity of the atmosphere and can form ultrafine aerosol particles, which are important as cloud condensation nuclei and provide a major pathway for transferring marine iodine to the continents (e.g., Saiz-Lopez et al. 2011).

Finally, to overcome the analytical challenges related to samples containing low halogen abundances and mixed fluid compositions, we used the neutron-irradiation noble gas technique. This method has low halogen detection limits (<1 ppb I) and, because it combines halogens with noble gas isotope measurements, can be used to obtain a range of insights into fluid systems including their origin, temperature, salinity, and age (Turner et al. 1993; Ballentine et al. 2002). As such, it has been applied to a wide range of ancient fluid systems (e.g., Kelley et al. 1986; Tuner et al. 1993; Bohlke and Irwin 1992a; Kendrick et al. 2001; Ballentine et al. 2002).

Samples and geological setting

Quartz samples PI-02-39 and PI-06 are from the 3.5 Ga old Dresser formation, Warrawoona Group, Pilbara Craton at North Pole, Western Australia (Foriel et al. 2004). The Dresser Formation is a sedimentary-volcanic succession comprising pillowed metabasalts and metakomatiites interbedded with cherty metasediments and is interpreted to have formed in a hydrothermal system associated with a volcanic caldera (Van Kranendonk 2006). Both quartz samples analyzed are from a drill core (Pilbara Drilling Project 2) and were collected at between 102 and 110 m depth. PI-06-39 and PI-06 are from quartz-carbonate aggregates forming pods in centimeter-sized vacuoles in a metakomatiite (Buick and Dunlop 1990; Pujol et al. 2011). The host rocks are undeformed and have experienced only low-grade metamorphism between 100–350 °C, probably occurring shortly after deposition 3.5 Ga ago (Terabayashi et al. 2003; Van Kranendonk 2006). Quartz contains abundant mixed aqueous-vapor fluid inclusions with variable salinity (average ~12 wt% NaCl) considered to be of primary origin (Foriel et al. 2004). The age of trapped fluids is likely >3.0 Ga, and probably contemporaneous with the Dresser formation (Pujol et al. 2013), they contain low atmospheric 40Ar/36Ar ratios (40Ar/36Ar = 143 ± 24, 1σ) and isotopically fractionated xenon characteristic of Archean atmosphere (Pujol et al. 2011, 2013; Avice et al. 2018). The fluids are interpreted as being mixtures of seawater and two or more different hydrothermal end-member mixtures (Foriel et al. 2004). The hydrothermal end-members are rich in metals (Fe, Ba), Cl, K, and parentless 40Ar (Foriel et al. 2004; Pujol et al. 2011). Marty et al. (2018) used noble gases released by crushing of neutron-irradiated samples of PI-06-39 and PI-06 to show that the salinity (Cl) of 3.5 Ga Archean seawater was comparable to modern seawater, with perhaps a 40% lower potassium abundance. Foriel et al. (2004) used the chemical composition to divide the fluid inclusions into three types, two hydrothermal fluids with Br/ Cl of ~2.6 × 10-3 M, and a low Br/Cl fluid considered to be representative of seawater.

Nine samples were selected from different depths in the DDH44 drill core at Paraburdoo from the ca. 2.5 Ga Dales Gorge Member, Brockman Banded Iron Formation, Hamersley Group, Western Australia (Ewers and Morris 1981). Samples 36.7–13, 96.8–14, and 146.7/8 were available from the previous study by Hamade et al. (2003). The Dales Gorge Member is one of the best-preserved BIFs, and has been extensively studied to make inferences about ancient environmental conditions and biological processes (e.g., Trendall and Blockley 1970; Ewers and Morris 1981; Morris 1993; Krapež et al. 2003; Pecoits et al. 2009; Rasmussen et al. 2013, 2014). It is ~150 m thick and divided into 17 depositional sequences. The BIF macrobands are themselves composed of mesobands (millimeter to centimeter thick) apparent as alternating iron oxide-rich (hematite, magnetite) and chert-rich bands that are laterally continuous. Chert mesobands are, in turn, often characterized by fine microbands (sub-millimeter thickness), also defined by alternation of iron oxides and chert (Rasmussen et al. 2013). Chert is interpreted to have formed from amorphous silica, which either precipitated directly from the water column (Ewers and Morris 1981) or formed below the sediment-water interface as a diagenetic replacement (Krapež et al. 2003; Rasmussen et al. 2013, 2014). The Dales Gorge Member has undergone very low- to low-grade metamorphism and minor deformation (Smith et al. 1982; Kaufman et al. 1990). Based on textural evidence, the hematite present in iron-rich bands either formed by dehydration of ferric oxyhydroxides that precipitated in the water column (Sun et al. 2015) or by secondary replacement growth during the 2.2 Ga Ophthalmian Orogeny (Rasmussen et al. 2005). While the movement of hydrothermal fluids is thought to be responsible for the deposition of microplaty hematite, which forms the major ore bodies in the region (Brown et al. 2004), the samples in this study are generally considered primary in nature (Robbins et al. 2019).

Since BIFs are marine sediments, not associated with lavas or other igneous bodies, they are less likely to be directly influenced by hydrothermal systems. The Hamersley samples studied have positive Eu/Eu* anomalies between 1.3–2.4 and elevated but variable Y/Ho of 34–62 (data from Hamade 2002 and given in Table 1). On a Y/Ho–Eu/Eu* diagram (Fig. 1), they are intermediate between crust and Archean seawater values, the latter represented by data from the 3.40 Ga Strelley Pool Chert (Van Kranendonk et al. 2003). The lack of evidence for a hydrothermal end-member in Figure 1 indicates the cherts did not precipitate directly from hot fluids. On this basis, Hamersley samples precipitated at least partially to mostly from Archean seawater, possibly contaminated with crustal material.

Figure 1 
          Y/Ho vs. Eu/Eu* ratio calculated as Eu/[(0.67Sm + 0.33Tb)]MUQ. MUQ = average mud from Queensland (Kamber et al. 2005). End-member compositions for crust and hydrothermal fluids from Pinti et al. (2009). The Strelley Pool stromatolite data are considered to precipitate from Archean seawater (Van Kranendonk et al. 2003).
Figure 1

Y/Ho vs. Eu/Eu* ratio calculated as Eu/[(0.67Sm + 0.33Tb)]MUQ. MUQ = average mud from Queensland (Kamber et al. 2005). End-member compositions for crust and hydrothermal fluids from Pinti et al. (2009). The Strelley Pool stromatolite data are considered to precipitate from Archean seawater (Van Kranendonk et al. 2003).

Table 1

Halogen data for Hamersley chert samples (1 St.dev. error)

Sample Fe2O3[a] wt% Hematite[a] wt% Magnetite[a] wt% Y/Ho[a] Eu/Eu*[a] T (°C)[b] Cl (ppm) % Cl release Br/Cl (×103) I/Cl (×106) 36Ar/Cl (×10–9)
36.7 61.9 21.2 27.3 1.364 61.9 1400 21.7 ± 0.1 47.7 1.94 ± 0.11 26.3 ± 0.6 74.7 ± 1.8
36.11 31.9 11.4 9.3 1.358 52.0 1400 14.2 ± 0.1 47.9 1.90 ± 0.02 32.4 ± 0.7 113.9 ± 1.9
36.12 59.5 23.7 14.3 1.535 52.9 1400 21.1 ± 0.2 45.3 2.04 ± 0.03 31.5 ± 2.6 95.5 ± 4.3
36.13 40.3 14.3 12.8 1.651 44.2 1600 14.3 ± 0.1 50.1 2.04 ± 0.01 30.2 ± 0.8 74.7 ± 2.3
96.8 34.0 17.7 12.4 1.469 38.4 1400 8.0 ± 0.1 43.4 1.97 ± 0.02 26.6 ± 1.0 84.9 ± 4.9
96.13 71.5 25.2 45.7 1.457 47.1 1600 16.9 ± 0.1 50.2 2.24 ± 0.01 28.7 ± 0.7 80.1 ± 2.5
96.14 53.3 11.4 26.7 1.726 52.4 1400 20.0 ± 0.1 46.3 2.06 ± 0.01 28.8 ± 0.8 74.0 ± 1.8
146.6 61.9 54.5 10.0 1.762 39.2 1400 18.2 ± 0.2 51.1 2.15 ± 0.02 20.3 ± 3.3 78.2 ± 1.5
146.7/8 45.6 28.7 4.4 2.429 33.6 1600 23.0 ± 0.1 59.1 1.84 ± 0.01 14.4 ± 0.4 55.8 ± 1.3

Experimental methods

Hamersley samples were hand-picked under a binocular microscope to ensure only vein-free chert was analyzed, and then crushed to a coarse powder. North Pole samples were prepared as millimeter-sized chips. Halogens were determined using neutron irradiation noble gas mass spectrometry (Turner 1965; Bohlke and Irwin 1992b; Kendrick 2012; Ruzié-Hamilton et al. 2016). The samples were irradiated at the Safari-1 reactor, NECSA, South Africa, for 24 h to receive an integrated neutron dose of ~1019 n cm-2. Noble gas isotopes 38ArCl, 80KrBr, 128XeI, 39ArK, and 37ArCa are formed following neutron reactions with parent isotopes of Cl, Br, I, K, and Ca, respectively. Following irradiation, noble gases were released either by in vacuo crushing (North Pole samples) or by furnace heating (Hamersley samples). Sample crushing was carried-out using modified Nupro valves (Stuart et al. 1994), by loading 10–50 mg of sample into a crucible placed in the body of the valve. Prior to crushing, the samples were evacuated and baked at 250 °C for 12 h. Samples were progressively crushed in 5–6 steps by repeatedly lowering and raising the valve stem with a modified tip designed to crush the sample.

During furnace heating, approximately 20–50 mg of sample powder was wrapped in pure Al foil and placed into the “Christmas” tree loading device of the furnace. The resistance furnace is manufactured from Ta metal components, contained in a secondary vacuum chamber to prevent oxidation during heating. Samples were dropped into the furnace by externally manipulating an iron slug placed behind each sample, using a hand magnet. Temperatures were monitored using a thermocouple positioned at the base of the furnace tube. Samples were heated to between 400–1800 °C in 200 °C steps, each of 30 min duration.

Noble gases released either by crushing or stepped heating were purified using the same procedure: initially using a hot SAES G50 getter in close proximity to the furnace or crusher devices; then with a hot SAES ST171 getter positioned close to the inlet of the mass spectrometer; and finally with an SAES NP10 getter at room temperature mounted adjacent to the mass spectrometer ion source. Isotopic analyses were made using the MS1 mass spectrometer, a custom-built single focusing magnetic sector mass spectrometer equipped with a continuous dynode channeltron and a Faraday detector (Ruzié-Hamilton et al. 2016). Peak height determinations were made by switching the magnetic field over the mass range for Ar, Kr, and Xe isotopes (m/z 36–136), using nine measurement cycles. Baseline readings at intermediate masses were also measured and subtracted from peak readings. Following isotopic analysis, raw data were regressed to mass spectrometer inlet time, corrected for blanks (determined by heating an empty Al foil wrapping, or in the static volume of the crushers), neutron interferences, radioactive decay and mass discrimination (the latter only for Ar isotopes), and converted to moles using calibrated volumes of air standard, analyzed daily during the period of the experiments. Methods used for converting neutron-produced noble gas isotopes to parent halogen, K, and Ca concentrations follow those described by Ruzié-Hamilton et al. (2016). Reported elemental ratios are in molar (M) units and uncertainties are one standard deviation unless otherwise stated.

Results and discussion

Data obtained from crushing and stepped heating are summarized in Table 1 and the full data set is available in Supplemental[1] Table S1. Data for the Hamersley samples do not show any correlation, or systematic differences, with sampling depth, mesoband mineralogy or Fe content (Table 1). For this reason, results obtained from different samples are not differentiated in the following discussion. Furthermore, in assessing the sample data for the presence of ancient seawater we make the same conservative assumptions of previous studies (Turner 1989; Pujol et al. 2013; Marty et al. 2018), that during the Archean the partial pressure of 36Ar in the atmosphere was similar to today, and that 36Ar concentrations in seawater are a primarily a function of temperature and salinity only.

Retention of a primary seawater halogen signature in chert

Stepped heating noble gas release patterns are similar for all chert samples. There are two main gas releases: (1) a fairly broad release between 600–1000 °C, representing the predominant release for 37ArCa (57–89%) and 39ArK (44–78%); and (2) a sharp release occurring at either 1400 or 1600 °C, normally corresponding to the main release of 38ArCl (43–59%); 80KrBr (41–69%) and 128XeI (55–78%).

The stepped release pattern indicates that halogens are hosted by at least two different phases in chert. The host(s) of the lower temperature release (600–1000 °C) is not known with certainty, but possible candidates include iron oxides that are able to adsorb halide ions or carbonate minerals, the latter implicated by the large 37ArCa release. Cherts are also known to contain noble gases dissolved in a fluid phase and, during previous stepped heating studies of irradiated cherts, this component has been shown to be retained until >1200 °C (Turner 1988). Further insights into the nature of the phase(s) releasing most of the halogen-derived noble gases at high temperature can be gained by considering the K-Ar-Cl relationships below.

K-40Ar age constraints

Figure 2a shows a plot of K/36Ar vs.40Ar/36Ar for heating steps from all samples, and Figure 2b shows data for high-temperature steps only (1200–1600 °C). The low temperature stepped heating data show a limited range of 40Ar/36Ar values (216–400), and do not correlate with K/36Ar (Fig. 2a). In contrast, high-temperature data form a reasonable linear relationship (Fig. 2b) indicating that 40Ar is composed of a mixture between a K-poor, low 40Ar/36Ar (<250) end-member, and a K-rich, radiogenic 40Ar end-member. The best fit line shown in Figure 2b was obtained by linear regression of the data obtained for steps above >1200 °C. The 1200 °C steps were excluded from the fit because some show evidence of mixing with the low-temperature component, these data are indicated in Figure 2b. The slope of the best-fit line corresponds to an age of 2383 ± 183 Ma (2σ) with an intercept 40Ar/36Ar of 142 ± 31 (MSWD = 1.6, p = 0.07). The linear regression is not considered to be a robust isochron because, even after excluding the 1200 °C step from the regression, it is possible that some residual gas is being released from the low temperature phase. Furthermore, the K-bearing phase is likely to be fine-grained, making 39Ar recoil into surrounding chert a strong possibility. Nevertheless, the age obtained is consistent with both the timing of hydrothermal vein formation in the Dales Gorge Member, considered to be related to the ca. 2.2 Ga Ophthalmian Orogeny (Brown et al. 2004), and the age of 2461 ± 6 Ma determined by U-Pb dating of zircons from an ash-fall tuff in macroband S13 (Trendall et al. 2004). The trapped 40Ar/36Ar value of 142 ± 31 is lower than modern atmosphere (296) and within error of the palaeo-atmospheric 40Ar/36Ar composition of sample PI-06 from the 3.4 Ga Dresser Formation of 143 ± 24 (Pujol et al. 2011). In summary, the high temperature release of Ar from Hamersley cherts is consistent with the presence of a ~2.4 Ga old K-bearing phase preserving an ancient atmospheric component.

Figure 2 
            
              40Ar/36Ar vs. K/36Ar plot for 9 chert samples from Dales Gorge Member, Brockman BIF, Hamersley Group, Western Australia. (a) Low T refers to heating steps 600–1000 °C; High T are steps at 1200–1600 °C; and Main is the dominant release step for K-derived 39Ar at either 1400 or 1600 °C (b) High temperature and Main release steps only, additionally the 1200 °C step for each sample is excluded from the regression. The line of best fit (dotted) yields a slope 40Ar*/K = (33.68 ± 1.3) × 10-6 and an intercept 40Ar/36Ar = 142 ± 31 (2σ errors).
Figure 2

40Ar/36Ar vs. K/36Ar plot for 9 chert samples from Dales Gorge Member, Brockman BIF, Hamersley Group, Western Australia. (a) Low T refers to heating steps 600–1000 °C; High T are steps at 1200–1600 °C; and Main is the dominant release step for K-derived 39Ar at either 1400 or 1600 °C (b) High temperature and Main release steps only, additionally the 1200 °C step for each sample is excluded from the regression. The line of best fit (dotted) yields a slope 40Ar*/K = (33.68 ± 1.3) × 10-6 and an intercept 40Ar/36Ar = 142 ± 31 (2σ errors).

Salinity of the trapped fluid released at high temperature

Hamersley heating data are shown on a plot of Cl/36Ar vs. K/36Ar in Figure 3, where it can be seen that there is a general positive correlation. Notably, the main release steps (at 1400 or 1600 °C) from each sample have Cl/36Ar values comparable to modern seawater salinity in the temperatures range 0–25 °C (calculated from equations in Hamme and Emerson 2004). This is similar to the finding of Marty et al. (2018) for North Pole fluids, which are also shown for comparison in Figure 3. However, K/36Ar of the Hamersley high temperature steps are about two orders of magnitude higher than modern seawater. This can be explained by the presence of a K-rich phase yielding the ~2.3 Ga age discussed earlier and implies that both sold and fluid inclusions are co-released during melting of the host chert. The fluid phase is likely to be paleo-seawater containing dissolved atmospheric noble gases based on the low 40Ar/36Ar ratio, seawater-like Cl/36Ar ratios, and the ~2.4 Ga 40Ar-39Ar age.

Figure 3 
            Cl/36Ar vs. K/36Ar data obtained by stepped heating of Hamersley chert and in vacuo crushing of North Pole (PI) quartz samples. Hamersley data are subdivided on the basis of low T = temperature steps between 600–1000 °C; High T = steps between 1200–1600 °C, and Main release at either 1400 or 1600 °C. Data from individual crushing steps are shown for North Pole samples. The solid line represents modern seawater salinity over the temperature range 0–75 °C calculated using equations from Hamme and Emerson (2004).
Figure 3

Cl/36Ar vs. K/36Ar data obtained by stepped heating of Hamersley chert and in vacuo crushing of North Pole (PI) quartz samples. Hamersley data are subdivided on the basis of low T = temperature steps between 600–1000 °C; High T = steps between 1200–1600 °C, and Main release at either 1400 or 1600 °C. Data from individual crushing steps are shown for North Pole samples. The solid line represents modern seawater salinity over the temperature range 0–75 °C calculated using equations from Hamme and Emerson (2004).

Fluid inclusions present in North Pole quartz are comprised of three fluid types having different salinities and metal composition (Foriel et al. 2004). The slightly elevated Cl/36Ar values obtained by crushing (Fig. 3) may reflect their hydrothermal origins, and the lower K/36Ar values compared to cherts indicates either an absence of a K-rich phase, or that this component is not released during crushing.

Halogen ratios of fluid inclusions

Br/Cl and I/Cl vs. 36Ar/Cl is shown for chert samples in Figure 4. Low-temperature heating steps give highly variable 36Ar/Cl values, and do not show any correlations (Fig. 4a). The variability in 36Ar/Cl ratios of the low-temperature release steps is attributed to the presence of a 36Ar-bearing component in the samples, most likely modern air contamination, as indicated by their air-like 40Ar/36Ar ratios (Fig. 2). The high temperature (>1200 °C) steps give lower and more consistent 36Ar/Cl values indicative of a single fluid component having a relatively uniform composition similar to that observed in the North Pole quartz samples (Fig. 4b). Assuming the main release step is representative of ~2.5 Ga seawater as discussed earlier, then Br/Cl = (2.02 ± 0.13) × 10-3 M and I/Cl = 26.6 ± 5.8 × 10-6 M, which are about 30% and 30 times higher than the present-day seawater values, respectively.

Figure 4 
            I-Br-Cl-36Ar relationships in Hamersley and North Pole samples. (a) Hamersley data only showing decreasing scatter with increasing temperature steps. Symbols are defined in Figure 2. (b) Expanded scale showing the main release step for the Hammersley cherts and total crushing release from North Pole (PI) quartz samples. The solid horizontal lines represent modern seawater salinity over the temperature range 0–75 °C calculated using equations from Hamme and Emerson (2004).
Figure 4

I-Br-Cl-36Ar relationships in Hamersley and North Pole samples. (a) Hamersley data only showing decreasing scatter with increasing temperature steps. Symbols are defined in Figure 2. (b) Expanded scale showing the main release step for the Hammersley cherts and total crushing release from North Pole (PI) quartz samples. The solid horizontal lines represent modern seawater salinity over the temperature range 0–75 °C calculated using equations from Hamme and Emerson (2004).

While the process of formation remains unknown for Hamersley BIF cherts, the main control on halogen fractionation does not appear to be related to the depositional processes causing mineralogical banding in the cherts (Table 1). Retention of halogen variations on the centimeter-scale further supports the view that cherts provide a reliable record of fluid compositions over long geological timescales.

Hamade et al. (2003) suggest that banding in the Dales Gorge Member is controlled by the varying influence of continental vs. hydrothermal inputs to the basin. Br/Cl and I/Cl of modern continental runoff is variable (e.g., Moran et al. 2002; Tagami and Uchida 2006) but mostly exceeds modern seawater and mantle ratios. Thus, it is possible that the relatively minor inter-sample variations result from changing fluxes of halogens from the basin, although there is no evidence for mixing relationships in our data or relationship with REE ratios (Fig. 1, Table 1) that may support the presence of these two end-members.

Changes in composition at the mesoband scale are also unlikely to be caused by fluctuations in the source because deposition rate is much shorter than the residence time of any of the halogens. There is considerable uncertainty about rates of deposition of BIF, with rates possibly differing between band types due to changes in clastic input. Sedimentation rates for the Dales Gorge Member have been estimated at 3–1000 m/Ma (Arndt et al. 1991; Barley et al. 1997; Martin et al. 1993; Trendall 2000; Trendall et al. 2004), meaning 1 cm of BIF represents 10–3000 yr of deposition. Note, these rates are not based on wet sediment deposition that would have been much higher, but instead on consolidated core that would have undergone approximately 95% compaction (see Trendall and Blockley 1970). Regardless of the high uncertainty, the suggested rates are orders of magnitude lower than the residence times of Cl, Br, and I in modern oceans of 1.1 × 108, 1.2 × 108, and 3.1 × 105 years, respectively (Martin and Whitfield 1983).

North Pole crushing gives Br/Cl values 1.9–2.0 × 10-3 M that are just above the range of 1.5–1.6 × 10-3 M obtained from two samples by crush leach analysis reported by Foriel et al. (2004). The minor disparity may reflect a higher proportion of hydrothermal fluid contributing to our determination, or perhaps be related to analytical differences between the techniques employed, e.g., crush leach may partially dissolve minor solid phases not sampled during noble gas crushing, or the noble gas technique may be biased toward release from larger inclusions having subtly different composition. Using synchrotron microanalysis, Foriel et al. (2004) determined Br/Cl values for individual fluid inclusions in North Pole quartz and found the composition of a low-metal bearing fluid to be similar to the bulk crush leach values. They interpreted this fluid type as being most representative of North Pole seawater on the basis having Br/Cl ratios similar to modern seawater values.

Halogen ratios of the ancient oceans: Biological and mantle influences

Based on the preceding discussion, halogens released at high temperature from Hamersley cherts, and during crushing release of North Pole quartz provide similar estimates for Br/Cl and I/Cl ratios of seawater for the time periods 2.5 and 3.5 Ga, respectively. Figure 5 plots I/Cl vs. Br/Cl for samples studied here, together with previously reported values of Archean seawater composition. Data from this study are reasonably consistent with previous values, although a comparison of I/Cl is only possible for Barberton (Channer et al. 1997), assuming the ironstone pods at Barberton are of Archean age, which is disputed (Lowe and Byerly 2003, 2007; Hren et al. 2006). The range of halogen ratios of Archean seawater are distinct from the modern mantle and chondrite values, which has relevance for understanding the distribution of halogens in the early Earth. Estimates suggest that 80–90% of terrestrial Cl, Br, and I are currently stored in surface reservoirs (Burgess et al. 2002; Kendrick et al. 2017), significantly higher compared to the ~50% mantle degassing of noble gases. To account for these differences, Clay et al. (2017) argued that halogens were degassed in a large pulse, probably early in terrestrial evolution, and then stabilized in fluid or solid phases to avoid the extreme early loss processes experienced by noble gases (Pepin and Porcelli 2006). In this scenario, the early oceans would be expected to have chondrite-like halogen ratios. However, the estimates shown in Figure 5 indicate that seawater halogen chemistry had already evolved from this initial state by 3.5 Ga.

Figure 5 
            I/Cl vs. Br/Cl plot for Hamersley chert and North Pole quartz samples. Data and end-member (SW = seawater; VF = vent fluid) estimates for Barberton, Kapvaal are from Channer et al. (1997); de Ronde et al. (1997). Gray symbols at top of the graph are Br/Cl data only: Pilbara SW and VF = Foriel et al. (2004); Kapvaal SW = Gutzmer et al. (2003). Reference values are mid-ocean ridge basalts (MORB, representative of the Earth’s depleted mantle) = Kendrick et al. (2017), chondrite meteorites = Clay et al. (2017), and modern seawater = (Li 1991).
Figure 5

I/Cl vs. Br/Cl plot for Hamersley chert and North Pole quartz samples. Data and end-member (SW = seawater; VF = vent fluid) estimates for Barberton, Kapvaal are from Channer et al. (1997); de Ronde et al. (1997). Gray symbols at top of the graph are Br/Cl data only: Pilbara SW and VF = Foriel et al. (2004); Kapvaal SW = Gutzmer et al. (2003). Reference values are mid-ocean ridge basalts (MORB, representative of the Earth’s depleted mantle) = Kendrick et al. (2017), chondrite meteorites = Clay et al. (2017), and modern seawater = (Li 1991).

Higher plume activity, production of voluminous mafic crust (Smithies et al. 2005), higher outgassing rates (Sleep and Zahnle 2001) and increased vigour of high-temperature hydrothermal activity (Shibuya et al. 2007) means there was probably a stronger connection between the mantle and ocean chemistry during the Archean. The halogen composition of the Archean mantle is unknown, and in modern seafloor hydrothermal systems Br/Cl ratios are not usually fractionated from mantle values by >10% during boiling and phases separation processes (see Kendrick 2018 for review). Higher than mantle Br/Cl ratios, similar to those estimated for Archean hydrothermal fluids (Channer et al. 1997; Gutzmer et al. 2003; Foriel et al. 2004; Farber et al. 2015) are present in fluids in hydrothermally altered ocean crust and may be explained by mixing of seawater ± mantle halogens followed by fractionation of Br and Cl during amphibole crystallization during high-temperature ocean crust alteration (Kendrick et al. 2015; Chavrit et al. 2016). In contrast to seafloor alteration processes that do not strongly affect the Br/Cl ratios, organic matter fractionates Cl and Br, and the lack of a significant organic reservoir was proposed to explain the high Br/Cl of Palaeoproterozoic seawater (Gutzmer et al. 2003).

An Archean marine reservoir of iodine much larger than today’s has previously been suggested based on the absence of, or more limited, biological control (de Ronde et al. 1997; Hardisty et al. 2014). The main iodine sink in the modern ocean is biological assimilation and burial in organic-rich marine sediments (Price and Calvert 1973; Price 1977; Muramatsu and Wedepohl 1998). In particular, marine algae accumulate iodine (and some bromine) with a concentration factor from seawater of around five orders of magnitude (and up to one order of magnitude for Br; Küpper et al. 2013). Most of the organically bound iodine is released back to into seawater during the decomposition of organic matter (Ullman and Aller 1980, 1983). Under anoxic conditions, which characterized early Archean oceans, seawater iodate is reduced to iodide, which adsorbs less readily on to organic matter making burial of iodine less efficient (Zhou et al. 2015). This is because in contrast to seafloor alteration processes that do not affect the Cl/Br ratios, organic matter fractionates Cl and Br. Overall, the relatively small iodine sink of sedimentary organic matter predicted for the Archean, is supported by our finding of I/Cl ratios much higher than the modern value.

Implications

This study addresses the Br/Cl and I/Cl composition of Archean and Palaeoproterozoic seawater by applying the noble gas neutron irradiation technique to chert and hydrothermal quartz samples. In addition to low detection levels for halogens, this technique has the potential advantage of being able to distinguish between primary and secondary components and provide age constraints on the timing of fluid entrapment. This is the first study to assess the potential of BIF cherts for reconstructing ancient seawater halogen compositions. Cherts containing preserved seawater exhibit the following characteristics: 36Ar/Cl values consistent with the range predicted for ocean water salinity and temperature; 40Ar-39Ar ages that are equivalent to the chert depositional age; presence of paleoatmospheric noble gases dissolved in the seawater component; and high temperature (≥1400 °C) co-release of these attributes during melting of the host chert. Although the hydrothermal quartz and BIF chert formed in different depositional environments at separate times, they nonetheless trapped seawater with similar halogen ratios (Br/Cl ~ 2 × 10-3 M and I/Cl ~ 30 × 10-6 M).

The strong affinity of I for organic matter makes this element a sensitive tracer for the evolution of biological activity in the ocean and is particularly influenced by marine algae. The Archean ocean I/Cl value is intermediate between the bulk Earth (represented by chondritic meteorites) and modern seawater consistent with a smaller organic iodine reservoir in the Archean and Paleoproterozoic. The Br/Cl value of ancient seawater is elevated above modern seawater and chondritic values, and the cause of this is not understood. However, given the likely buffering of seawater halogen ratios by mantle inputs, it is suggested this may reflect stronger Br and Cl fractionation during seafloor hydrothermal processes relative to the modern day.


† Current address: TOTAL, Centre Scientifique et Techniques Jean-Féger, Pau, France.

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


Acknowledgments and funding

We thank Zunli Lu and an anonymous reviewer for constructive reviews, and Anita Cadoux for editorial assistance. S.G. acknowledges funding from a NERC Ph.D. studentship that supported the analyses of the Hamersley chert samples. R.B. is grateful for a JSPS Fellowship that funded his stay at the University of Tokyo during which the manuscript was prepared.

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Received: 2019-07-31
Accepted: 2020-02-14
Published Online: 2020-09-20
Published in Print: 2020-09-25

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