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Rock magnetic characterization of ferrimagnetic iron sulfides in gas hydrate-bearing marine sediments at Site C0008, Nankai Trough, Pacific Ocean, off-coast Japan
© Kars and Kodama. 2015
- Received: 27 February 2015
- Accepted: 30 June 2015
- Published: 29 July 2015
A high-resolution rock magnetic study was carried out in Integrated Ocean Drilling Program (IODP) Expedition 316 Hole C0008A located in the Megasplay Fault Zone of the Nankai Trough, SW offshore Japan, in order to document changes in magnetic properties throughout gas hydrate-bearing horizons. A total of 169 Pleistocene discrete samples were collected from ~110 to 153 m core depth below sea floor (CSF), and their magnetic minerals concentration, grain size, composition, and rock magnetic parameters were estimated. Results showed the presence of iron oxides ((titano)-magnetite), iron sulfides (greigite and pyrrhotite), and their mixture, among which single-domain greigite is the most major magnetic mineral present in the samples. Two horizons containing ferrimagnetic iron sulfides (114.5–127.5 and 129.5–150 m CSF) covering almost the entire studied interval were identified, both associated with slight local pore water anomalies, suggesting occurrence of gas hydrates and anoxic conditions. These results are different from the neighboring Hole C0008C (215 m away from Hole C0008A) where four pore water anomalies and six iron sulfide-rich intervals were identified for the same time slice. Comparison of the lithology, physical properties, and geochemical data of the two boreholes at Site C0008 suggests that a combination of processes (e.g., availability of reactive iron, microbial activity) is responsible for such laterally varying distribution of the ferrimagnetic iron sulfides.
- Iron sulfides
- Gas hydrate
- IODP Expedition 316
- Nankai Trough
Gas hydrates, composed mainly of methane, have been paid growing attention for the last decades because of their potential value as an energy resource (e.g., Kvenvolden 1993) and their possible impact on submarine landslides and climate change (Kennett et al. 2003). Low temperature, relatively high pressure, and sufficient concentration of methane are required for gas hydrate formation, although the mechanisms are not well understood (Hesse 2003).
Accretionary prisms, such as the Cascadia Margin (offshore Oregon, USA) and the Nankai Trough (SW Japan) are favorable locations for gas hydrates accumulation. The Nankai accretionary complex off the coast of SW Japan is formed by the subduction of the Philippine Sea plate beneath the Eurasian plate along the Nankai Trough.
On seismic profiles, gas hydrates horizons are recognized by the occurrence of high amplitude bottom simulating reflectors (BSRs) that are regarded as the base of a gas hydrate stability field (e.g., Ashi et al. 2002). BSRs indicate the boundary between contrasting high velocity gas hydrates zone above and low velocity free gas zone below.
In the Nankai Trough, BSRs are continuous in the fore arc Kumano Basin and intermittent in the imbricate fault zone. No BSRs are recognized in the megasplay fault zone (MSFZ) and the frontal thrust zone of the Nankai accretionary prism (Kinoshita et al. 2011). Gas hydrates dissociate rapidly during drill core recovery, and their identification is mostly indirect. Various analytical approaches on cores and during drilling are indicative of gas hydrate occurrences such as isotopic and pore water anomalies (essentially chlorinity anomalies) (Hesse 2003), lower core temperature, well logging data (Collett 2001), heat flow and thermal anomalies (Yamano et al. 2014; Kinoshita et al. 2015), and characteristic rock magnetic variations (e.g., Housen and Musgrave 1996; Larrasoaña et al. 2007).
The magnetic index DJH characterizes the occurrence of fine-grained (single domain-pseudo single domain) magnetic iron sulfides (Housen and Musgrave 1996). It is defined as the hysteresis parameters ratio (M rs/M s)/(B cr/B c) with M rs is the remanence at saturation, M s is the magnetization at saturation, B c is the coercive field, and B cr is the remanent coercive field. In the Cascadia Margin marine sediments, DJH displays high values within low chlorinity zones and indicates the occurrence of gas hydrates (Housen and Musgrave 1996). Widespread occurrence of greigite (Fe3S4) and pyrrhotite (Fe7S8), associated with gas hydrates has later been reported in the Cascadia Margin (e.g., Musgrave et al. 2006; Larrasoaña et al. 2006; Larrasoaña et al. 2007).
Rock magnetic properties of gas hydrate-bearing sediments in the Nankai Trough at Site C0008 have been recently investigated. A high-resolution magnetic study in Hole C0008C (33° 12.7313′ N, 136° 43.6727′ E; water depth = 2797 m), drilled during Integrated Ocean Drilling Program (IODP) Expedition 316 by the D/V Chikyu (Kinoshita et al. 2009), has been conducted between 70 and 110 m core depth below sea floor (CSF) (i.e. 2867–2907 m below sea level) to document the downcore mineralogy, grain size, and concentration variations of the magnetic minerals through the gas hydrate horizons in Pleistocene sediments (Kars and Kodama 2015). The peaks of DJH outline six layers bearing greigite and/or pyrrhotite, separated by sediments containing mainly coarse-grained (titano)-magnetite. Four of these layers correspond to intervals where pore water anomalies were identified and hence correspond undoubtedly to gas hydrate horizons. The two remaining intervals are believed to be also gas hydrate horizons that were not identified by pore water geochemistry because of the low sampling resolution for pore water analysis. The downcore variations of the magnetic properties in Hole C0008C have been explained by different diagenetic stages related to upward gas migration (Kars and Kodama 2015).
In this study, 169 discrete samples (7 cc plastic cubes) were collected at approximately 20-cm interval covering the 110–153 m CSF depth interval on sections 13H-1 to 19H-3 of Hole C0008A (2861–2904 mbsl). Slope sediments at Site C0008 are divided into three stratigraphic units (Ia, Ib, Ic) (Fig. 1). The samples studied in this paper belong to unit Ib that is constituted of hemipelagic silty clays interbedded with coarse turbidite and fine ash layers (Kimura et al. 2011; Strasser et al. 2011). The mean grain size at Site C0008 is 5–12 μm, with values up to 20 μm (Kopf et al. 2011). Based on the occurrence of calcareous nannofossils, the age of the collected samples ranges between 1.34 Ma at 90.39 m CSF and 1.46 Ma at 152.69 m CSF (Mid Pleistocene) (Expedition 316 Scientists 2009). This is supported by the onboard magnetostratigraphy that yields an age between 1.24 and 1.77 Ma (C1r.2r) (Expedition 316 Scientists 2009). The sampling depth includes two pore water chlorinity minima at ~120 and ~136 m CSF (Expedition 316 Scientists 2009).
Magnetic measurements were performed at the paleomagnetic laboratory of the Center for Advanced Marine Core Research (CMCR), Kochi University, Japan. Low field-low frequency magnetic susceptibility (χ) was measured with a MS2 Bartington apparatus. Natural remanent magnetization (NRM) and anhysteretic remanent magnetization (ARM) were measured with a 2G SQUID cryogenic magnetometer in the shielded room (noise level ~10−10 Am2). ARM was imparted in a direct current (DC) bias field of 50 μT in presence of an 80 mT peak alternating field. Isothermal remanent magnetization (IRM) was subsequently imparted at 0.9 and 1.2 T by using a MMPM10 impulse magnetizer before being measured at each step with a Natsuhara Giken spinner magnetometer (noise level ~10−8 Am2). Then, the samples were subsequently remagnetized in a DC reverse field of 0.3 T and measured again, in order to calculate the S-ratio S = (−IRM−0.3T)/IRM1.2T, an indication of the relative proportion of hard coercive minerals (e.g., hematite, goethite, ferrimagnetic iron sulfides) in a mixture with soft ferrimagnetic minerals (e.g. magnetite, maghemite).
Hysteresis loops with a maximum applied field of 1 T were measured at room temperature with a Princeton Vibrating Sample Magnetometer (VSM) (noise level ~10−7 Am2). First order reversal curves (FORC) were also measured for 76 selected samples every 5–10 cm, with a 1-T saturating field (averaging time 200 ms, field increment 5 mT, slew rate limit 1 T/s, number of FORCs 66). FORC diagrams were processed by using the software FORCInel (Harrison and Feinberg 2008).
Low-temperature measurements (down to 5 K) were made with a Quantum Design Magnetic Properties Measurements System (MPMS) (noise level ~10−10 Am2) for 21 selected samples representing the three types of magnetic assemblages (described hereafter) and covering the entire studied interval. A cooling-warming cycle of a saturation isothermal remanent magnetization (SIRM) imparted at room temperature (300 K) at 2.5 T was first measured in a zero magnetic field (trapped field <150 μT). A low temperature (LT)-SIRM was imparted at 5 K at 2.5 T. The sample was then warmed up to room temperature in a zero magnetic field and measured (called ZFC for zero field cooled). The sample is then cooled down to 5 K in a 2.5 T magnetic field, and the LT-SIRM is measured during warming to 300 K (FC for field cooled).
NRM, χ, ARM/χ, and S-ratio
The ARM/χ ratio, an indicator of the grain size variations, shows, unlike NRM and χ, greater variations and varies from ~50 to ~1170 A/m (Fig. 2d). The higher values of ARM/χ span two depth intervals, ~115–122 and 135–140 m CSF, and suggest the occurrence of fine-grained particles. However, because χ is low, it might be possible that this ratio may reflect both grain size and ferrimagnetic concentration.
The S-ratio generally displays high values above 0.9, suggesting the dominance of low coercive magnetic minerals (Fig. 2e). The intervals 110–113 and 127.5–129.5 m CSF are characterized by lower S-ratio values (~0.85).
For type 1 samples, the Verwey transition of magnetite is not well marked and occurs at ~110–115 K on the RT-SIRM curves (Fig. 4a; Muxworthy and McClelland 2000; Özdemir et al. 2002). During warming of the RT-SIRM, the remanence is not fully recovered when passing the temperature of the Verwey transition. The transition is hardly visible on ZFC and FC curves (Fig. 4b). Similarly to Hole C0008C (Kars and Kodama 2015) and nearby Site C0004 in the MSFZ (Zhao and Kitamura 2011), between 50 and 60 % of the LT-SIRM imparted at 5 K is lost upon warming between 5 and 35 K (Fig. 4b), suggesting the presence of very small magnetic (superparamagnetic) particles (e.g., Passier and Dekkers 2002).
Type 2 samples, contrary to the samples from types 1 and 3, display a very well developed Verwey transition on the RT-SIRM (Fig. 4c) that are also recognizable on both ZFC and FC (Fig. 4d). The transition occurs at ~120 K suggesting stoichiometric magnetite, probably of pseudo-single domain (PSD) to multidomain (MD) size, because the remanence is not fully recovered upon warming of the RT-SIRM.
For the type 3 samples containing iron sulfides, two different low-temperature behaviors can be identified. One is characterized by the occurrence of the Besnus transition of pyrrhotite at ~35 K on cooling of the RT-SIRM (Fig. 4e) (Dekkers et al. 1989; Rochette et al. 1990; Wolfers et al. 2011). The grain size of the pyrrhotite is probably single domain (SD) because the remanence is almost fully recovered upon warming of the RT-SIRM (Dekkers et al. 1989; Rochette et al. 1990). No particular feature can be identified on ZFC and FC (Fig. 4f). The second magnetic signature of type 3 samples is similar to that of type 1 samples (Fig. 4g, h). These samples contain mainly greigite that does not have low-temperature magnetic transition (Roberts et al. 2011).
For all types of the samples, the rapid increase observed at very low temperature (<50 K) on the RT-SIRM is actually an induced magnetization caused by the trapped magnetic field inside the MPMS and a strong paramagnetic contribution of the samples (e.g., clays) or submicron pyrrhotite (Aubourg and Pozzi 2010; Kars et al. 2011).
Hysteresis properties and DJH
As indicated by the IRM measurements (Fig. 3) and FORC analyses (Fig. 6), ferrimagnetic iron sulfides (greigite and pyrrhotite) are abundant in the samples. The index DJH, (M rs/M s)/(B cr/B c), derived from the hysteresis properties and sensitive to the occurrence of fine-grained ferrimagnetic iron sulfides, is reported on Fig. 7. The samples displaying high DJH values >0.2 belong to two intervals (~116–128 and 130–148 m CSF) that host all type 3 samples and some type 1 samples (probable mixture of both iron oxides and ferrimagnetic iron sulfides) (Fig. 2h). This finding suggests that these two depth ranges that represent almost the entire studied interval are constituted of fine-grained (SD) ferrimagnetic iron sulfides.
The studied interval in Hole C0008A roughly laterally correspond to the 70–110 m CSF (2867–2907 mbsl) interval in Hole C0008C studied previously by the authors (Kars and Kodama 2015). No correlation between the two holes was attempted by the IODP Expedition 316 Scientists because of the distance between the holes (215 m apart), presence of normal faults, and possible slumped sediments in Hole C0008A (e.g., Kinoshita et al. 2009; Strasser et al. 2011). One motivation for the magnetic study of Hole C0008A was to use the rock magnetic properties of the sediments in order to correlate Holes C0008A and C0008C.
Distribution of the ferrimagnetic iron sulfides, Site C0008
Based on the occurrence of the peaks of DJH, high values of M rs/χ (>40 kA/m) and IRM0.9/χ (>15–85 kA/m), two intervals containing ferrimagnetic iron sulfides, referred as IS (for Iron Sulfides) layers hereafter, are identified in Hole C0008A, 114.5–127.5 m CSF (2865.5–2878.5 mbsl) and 129.5–150 m CSF (2880.5–2901 mbsl), separated by a ~2 m wide interval mainly constituted of detrital iron oxides (PSD-MD magnetite) (Fig. 2).
Single-domain (SD) greigite is the main magnetic iron sulfide identified over the interval studied from the analysis of the FORC diagrams. SD pyrrhotite is identified at ~2887 and ~2891 mbsl.
The observations made in Hole C0008A differ from Hole C0008C (Kars and Kodama 2014, 2015). Indeed, two IS layers are identified in Hole C0008A whereas six IS zones are identified in Hole C0008C. DJH is higher in Hole C0008A indicating that there is a higher proportion of fine-grained SD ferrimagnetic minerals in Hole C0008A compared to Hole C0008C. The values of Mrs/χ up to ~220 kA/m, i.e., ~10 times higher than in Hole C0008C, suggest that greigite content is higher in Hole C0008A. Hole C0008A samples also display higher values of the ARM/χ ratio (>120 A/m against ~ A/m for Hole C0008C). Except for the 2869–2873.5 mbsl interval in Hole C0008C, referred as IS1 in Kars and Kodama (2015), all the IS intervals in Hole C0008C are characterized by lower values of IRM0.9/χ, compared to Hole C0008A.
Greigite is more abundant than pyrrhotite in both Holes C0008A and C0008C. The conditions for the formation and preservation of greigite and pyrrhotite differ. Limited organic carbon (which limits microbial production of dissolved sulfide) and high concentration of reactive iron favor the preservation of greigite, whereas more reducing environments with higher H2S concentration and more important organic matter consumption favor pyrrhotite (Kao et al. 2004). Moreover, their occurrence depends also on the sediment grain size. Greigite occurs mainly in fine-grained sediments, whereas pyrrhotite is present in coarser grained sediments (Horng et al. 1998). In the following paragraph, the differences in the magnetic mineralogy, i.e., greigite versus pyrrhotite, are not taken into account for understanding the distribution of the IS layers at Site C0008.
Possible leads for the distribution of the IS layers
The rock magnetic study conducted in Hole C0008A shows different results compared to Hole C0008C. The most important finding is the difference in the spatial distribution of the IS layers. In the following, possible leads that may explain this distribution are proposed.
The trends of the mineral abundance in the studied interval in Hole C0008A for the clay size fraction are similar to the trends identified in the studied interval in Hole C0008C (Fig. 8). Because the studied intervals cover a time interval of ~120 kyr, it is reasonable to assume that the detrital clay assemblage does not differ significantly in the sediments. The IS layers recognized in both holes are not characterized by any significant changes in clays assemblage, compared to the non-IS layers.
However, as stated above, the availability of reactive iron is very important for the formation of iron sulfides. It might be possible that a secondary non-identified source of iron (e.g., Fe-rich silicates such as glauconite) is present. Indeed, it has been shown previously that glauconite is often associated with iron sulfides (Shipboard Scientific Party 1994).
Grain size variations
Clay and silt are the dominant lithologies in the studied interval of Hole C0008A (Kopf et al. 2011) and represent ~35 and ~55 %, respectively of the grain size distribution. Approximately ten percent correspond to the sand fraction. There is no particular enrichment in one or the other grain size fraction, with respect to the occurrence of the IS layers. Finer and coarser fractions alternate over the studied interval (Kopf et al. 2011).
Physical properties measurements are another way to indicate lithological variations (e.g., natural gamma ray radiation, magnetic susceptibility) and grain size (e.g., gamma ray attenuation, porosity) and provide also information on state of consolidation, deformation, and strain. The wet bulk density measured by gamma ray attenuation increases downhole from ~1.60 g/cm3 just below seafloor to 1.95 g/cm3 at ~3023 mbsl in Hole C0008A (Expedition 316 Scientists 2009). The slight variations of the bulk density in the studied intervals at Site C0008 (i.e., 2867–2907 mbsl in Hole C0008C and 2861–2904 mbsl m CSF in Hole C0008A) are not significant to explain the occurrence of the IS layers.
In addition to the given P-T conditions and methane content for the formation of gas hydrate, porosity is considered as an important factor favoring the formation and concentration of gas hydrate (e.g., Ginsburg et al. 2000; Jin et al. 2002). High porosity should favor occurrence of gas hydrate. Porosity decreases monotonically downhole from ~63 % just below seafloor to ~47 % at ~3021 mbsl in Hole C0008A (Expedition 316 Scientists 2009). Expedition 316 Scientists do not observe significant deviations from the downhole trend. Moreover, porosity does not show any particular trend related to the occurrence of the IS layers. In Hole C0008C, porosity does not vary significantly over the studied interval (~60 %), although higher value (~65 %) intervals are present (Fig. 8). In Hole C0008A, porosity is also ~60 %, except for the ~2889–2906 mbsl interval where porosity is ~65 % on average (Fig. 8). The intervals that present higher measured porosity values host ferrimagnetic iron sulfides in both holes. Because the overall slightly decreasing trend of porosity cannot explain the spatial distribution of the IS layers, the possibility that localized slight changes in porosity occur cannot be ruled out. The intervals with higher porosity would favor the formation of gas hydrate leading to the formation of ferrimagnetic iron sulfides.
Methane content and microbial activity
At Site C0008, the occurrence of ferrimagnetic iron sulfides is associated with gas hydrate. It is reasonable to assume that the gas content may play a role on the distribution of the IS layers.
Below the sulfate-methane transition zone (at ~4–8 m below sea floor in Holes C0008A and C0008C), the methane concentration decreases to ~2 mM at 60 m depth and remains at this value downhole (Expedition 316 Scientists 2009). Exception is a local enrichment up to 15 m M at ~140 m CSF (~2891 mbsl) in Hole C0008A. This corresponds to a pore water anomaly (low chlorinity) that indicates the occurrence of gas hydrate. Then changes in methane concentration over the studied intervals cannot explain the distribution of the IS layers. Gas hydrates are rather disseminated throughout the holes, rather than being localized at some particular depth intervals.
In the Nankai Trough, CH4 formation is mainly by microbial hydrogenotropic methanogenesis (Toki et al. 2012). Methanogenic Archaea are inactive below 100 m depth and prevent organic matter decomposition (Toki et al. 2012). Because organic matter content is low over the studied intervals (<0.6 %; Expedition 316 Scientists 2009), organic matter is not the main factor controlling the magnitude of hydrogenotropic methanogenesis (Toki et al. 2012). Presence of gas hydrate enhances microbial activity that results in the formation of ferrimagnetic iron sulfides (high values of DJH), as shown by lower concentration of pyrite and higher concentration of iron monosulfides (mainly greigite) in the studied intervals in Holes C0008A and C0008C (Riedinger and Brunner 2014).
The microbial cell abundance is almost double in Hole C0008C, compared to Hole C0008A (Expedition 316 Scientists 2009). More gas hydrate occurrences and IS layers are identified in Hole C0008C, compared to Hole C0008A, but the total width covered by the IS layers is lesser (17.3 against 33.5 m). At the authors’ knowledge, no interpretation has been given yet for the distinct microbial content, which could be a probable explanation for clarifying the distribution of the IS layers at Site C0008, as a result of probable different environmental and geochemical conditions prevailing in the two holes.
Two thick IS layers, covering almost entirely the sampling interval, are then recognized in Hole C0008A, whereas six IS layers were identified in Hole C0008C for roughly the same depth interval in Mid Pleistocene sediments. One has to keep in mind that the age of the host sediments is not the age of gas hydrate formation (Kars and Kodama 2015). The IS intervals are not uniform laterally. So will be the gas hydrate horizons, by assuming the IS layers as potential reservoirs of gas hydrates. The conditions controlling the formation of the ferrimagnetic iron sulfides then differ between the two boreholes, although the mechanism(s) responsible could be the same. This indicates that not only are the pressure-temperature conditions responsible for the formation of ferrimagnetic iron sulfides and gas hydrates but also environmental (diagenetic) and geochemical conditions (e.g., redox conditions, reactive iron) as a result of possible microbially mediated process.
The rock magnetic study conducted from 110 to 153 m CSF in Hole C0008A in the Nankai Trough highlighted a widespread occurrence of magnetic iron sulfides, particularly greigite. Two thick IS layers, containing greigite and pyrrhotite, were identified both associated with the occurrence of gas hydrate. In the neighboring Hole C0008C, six IS layers were identified for the same lateral horizon, all corresponding to gas hydrate-bearing horizons. Both holes present also distinct magnetic properties that result from diagenesis. Possible leads for explaining the spatial distribution of the IS layers at Site C0008 were proposed. However, to date, no satisfying explanation can be expressed to report the occurrence of the multiple IS layers. It is likely that a combination of many factors (availability of reactive iron, microbial activity) favor the formation of ferrimagnetic iron sulfides in the presence of gas hydrates. Future work on the role of the microbial activity in gas hydrate-bearing sediments, as well as on the factors controlling the formation of iron sulfides, is needed in order to better understand the relationship between gas hydrate and iron sulfide.
Samples used in this study were provided by the Integrated Ocean Drilling Program (IODP). We would like to thank the Marine Works Japan staff for their help during the sampling party in Kochi Core Center.
We are grateful to Dr. Mark J. Dekkers and an anonymous reviewer for their constructive comments and to Dr. Qingsong Liu for editorial handling.
This is contribution PMG15–04 from the Center for Advanced Marine Core Research, Kochi University.
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