C Prigent
email: cprigent@udel.edu

J M Warren

A H Kohli

C Teyssier

Fracture-mediated deep seawater flow and mantle hydration on oceanic transform faults

Keywords: Fluid-rock interaction, Peridotite, Mylonite, Oceanic transform fault, Southwest Indian Ridge, Serpentinization

Fluid-rock interaction on oceanic transform faults (OTFs) is important for both the deformation behavior of the lithosphere and volatile cycling in the Earth. Rocks deformed and exhumed at OTFs preserve information about the depth extent of fluid percolation and the nature of fluid-rock interactions within these fault zones. In this study, we focus on five dredges from the Shaka and Prince Edward OTFs on the ultraslow spreading Southwest Indian Ridge that recovered significant volumes of deformed mantle rocks. Samples are predominantly mylonites that have been deformed to high strains in the fault zone, but also contain several generations of fractures. Based on the mineral assemblages in fractures and shear bands combined with thermobarometry analysis, we identified three distinct temperature ranges of fluid-mantle interactions associated with deformation. At low temperature (LT), this leads to crystallization of serpentine (± talc ± amphibole ± chlorite) at <500-550°C. At medium temperature (MT), chlorite and amphibole crystallized at ~500-750°C. At high temperature (HT), amphibole (± second generation peridotitic minerals) crystallized. The composition of minerals in HT fractures and shear bands indicate that fracturing and fluid flow occur up to temperatures of at least 850-875°C. Combining these results with modeled geotherms for both faults suggests that seawater percolation extended to depths of 20-25 km and that serpentinization extended to ~11-13 km. The evolution of fault zone structure induced by deep fluid-rock interaction and progressive formation of LT, MT and HT mylonites on OTFs results in weakening and strain localization within the oceanic lithosphere, and suggests that the global transform system may represent a large reservoir of volatiles in the Earth's lithosphere.

Introduction

Fault zones serve as pathways for fluid migration through the lithosphere owing to enhanced permeability caused by brittle fracturing (e.g., [START_REF] Caine | Fault zone architecture and permeability structure[END_REF][START_REF] Sibson | Seismic pumping-a hydrothermal fluid transport mechanism[END_REF] and ductile flow (e.g., [START_REF] Fusseis | Creep cavitation can establish a dynamic granular fluid pump in ductile shear zones[END_REF][START_REF] Mccaig | Deep fluid circulation in fault zones[END_REF]. The resulting fluid-rock interactions and metamorphic reactions are crucial controls on the long-term mechanical behavior and composition of fault zones [START_REF] Faulkner | A review of recent developments concerning the structure, mechanics and fluid flow properties of fault zones[END_REF]. For oceanic faults, which have an unlimited overlying supply of seawater, the extent of fluid flow controls both fault rheology and volatile cycling between the Earth's surface and the mantle (e.g., [START_REF] Hacker | Subduction factory 1. Theoretical mineralogy, densities, seismic wave speeds, and H2O contents[END_REF][START_REF] Rüpke | Serpentine and the subduction zone water cycle[END_REF][START_REF] Scambelluri | Serpentinite subduction: implications for fluid processes and trace-element recycling[END_REF].

At slow-spreading mid-ocean ridges, studies of fluid-rock interaction have shown that detachment faults are sites of enhanced fluid flow and mantle hydration. Hydrothermal fluids have been found to percolate down to 600-800°C (e.g., [START_REF] Mccaig | Detachment fault control on hydrothermal circulation systems: Interpreting the subsurface beneath the TAG hydrothermal field using the isotopic and geological evolution of oceanic core complexes in the Atlantic[END_REF][START_REF] Miranda | Strain localization along the Atlantis Bank oceanic detachment fault system, Southwest Indian Ridge[END_REF][START_REF] Picazo | Deformation associated with the denudation of mantle-derived rocks at the Mid-Atlantic Ridge 13°-15° N: The role of magmatic injections and hydrothermal alteration[END_REF], corresponding to ~7 km depth on the Mid-Atlantic Ridge (MAR) (e.g., [START_REF] Hansen | Mylonitic deformation at the Kane oceanic core complex: Implications for the rheological behavior of oceanic detachment faults: Rheology of Kane Oceanic Core Complex[END_REF], resulting in mantle serpentinization up to ~400°C and crystallization of amphibole-chloritetalc assemblages at higher temperatures [START_REF] Picazo | Deformation associated with the denudation of mantle-derived rocks at the Mid-Atlantic Ridge 13°-15° N: The role of magmatic injections and hydrothermal alteration[END_REF][START_REF] Rouméjon | Serpentinization of mantle-derived peridotites at mid-ocean ridges: Mesh texture development in the context of tectonic exhumation[END_REF].

Observations from oceanic transform faults (OTFs) also suggest the occurrence of enhanced hydrothermal circulation and deep fluid flow within the fault zone. Seafloor exposures of exhumed mantle rocks along the Vema OTF on the MAR indicate that the upper mantle can be highly serpentinized at shallow depths [START_REF] Boschi | Serpentinization of mantle peridotites along an uplifted lithospheric section, Mid Atlantic Ridge at 11[END_REF]. The presence of syn-deformational amphibole at Vema [START_REF] Cannat | Transform tectonics, metamorphic plagioclase and amphibolitization in ultramafic rocks of the Vema transform fault (Atlantic Ocean)[END_REF][START_REF] Cipriani | A 19 to 17 Ma amagmatic extension event at the Mid-Atlantic Ridge: Ultramafic mylonites from the Vema Lithospheric Section[END_REF] and at the Shaka OTF [START_REF] Kohli | Evidence for a deep hydrologic cycle on oceanic transform faults[END_REF] on the Southwest Indian Ridge (SWIR) suggests that seawater may percolate to even higher temperatures. Geophysical observations also indicate that some OTFs at intermediate and fast spreading ridges have negative gravity anomalies [START_REF] Gregg | Spreading rate dependence of gravity anomalies along oceanic transform faults[END_REF][START_REF] Pickle | Thermo-mechanical control of axial topography of intra-transform spreading centers[END_REF] and low seismic wave velocities compared to the surrounding lithosphere [START_REF] Froment | Imaging along-strike variations in mechanical properties of the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Roland | Seismic velocity constraints on the material properties that control earthquake behavior at the Quebrada-Discovery-Gofar transform faults, East Pacific Rise[END_REF], both of which are interpreted as evidence of high porosity and/or extensive serpentinization of fault material. Studies of subduction zones where oceanic fracture zones are subducting have also hypothesized that higher slab seismicity [START_REF] Paulatto | Dehydration of subducting slow-spread oceanic lithosphere in the Lesser Antilles[END_REF][START_REF] Schlaphorst | Water, oceanic fracture zones and the lubrication of subducting plate boundaries-insights from seismicity[END_REF] and geochemical enrichments of arc volcano lavas erupting above these faults (e.g., [START_REF] Manea | Subduction of fracture zones controls mantle melting and geochemical signature above slabs[END_REF] could be due to enhanced hydration of the mantle on OTFs and their fracture zones.

Despite the potential importance of hydration of the oceanic lithosphere for OTF deformation and for the subduction zone water budget, limited work has been done to systematically characterize fluid-rock interactions on OTFs. Dredging campaigns along the SWIR ridge-transform system have recovered significant volumes of deformed mantle rocks (serpentinites and peridotite mylonites) in three dredges from the Shaka OTF and two dredges from the Prince (Pr.) Edward OTF.

Microstructural analysis of four peridotite mylonites from Shaka [START_REF] Kohli | Evidence for a deep hydrologic cycle on oceanic transform faults[END_REF] revealed that some of the mylonites underwent relatively high temperature deformation and hydration within the fault zone prior to exhumation. In this paper, we focus on the full range of deformed mantle rocks that were recovered in the five SWIR dredges. We characterize sample mineralogy and chemistry to estimate the pressure-temperature-fluid-deformation path of mantle rocks, understand the nature of fluid-mantle interaction processes, and determine the depth extent of fluid percolation on OTFs.

Finally, we assess the consequences of fluid-rock interaction processes for oceanic lithosphere composition and deformation.

Sample selection

The Shaka and Pr. Edward OTFs on the SWIR (Fig. 1) were sampled during two cruises in the 1980s.

Cruise 107, leg 6, on the R/V Atlantis II in 1980 [START_REF] Farmer | Description of WHOI rock dredge samples: volume 3[END_REF] collected seven full and one empty dredges (60-67) across the Shaka OTF (Fig. 1d). The Protea expedition, leg 5, on the R/V Melville in 1984 [START_REF] Fisher | Mafic and ultramafic rock assemblages from the Antarctic Plate boundary, southwest Indian Ocean[END_REF][START_REF] Fisher | Mafic/Ultramafic Suites of the Slowly Spreading Southwest Indian Ridge: Protea Exploration of the Antarctic Plate Boundary, 24E-47[END_REF]Scripps Institution of Oceanography, 1984) collected four dredges (17-20) across the Pr. Edward OTF (Fig. 1e). Large amounts of peridotite mylonites were recovered in the five dredges that sampled the E-SE walls of each transform (60, 61, 63, 18 and 19), spanning a vertical distance of 1-3 km and a lateral extent of ~25 km.

From available multibeam bathymetry data (GMRT basemap v3.6), we constructed topographic profiles perpendicular to the trace of each fault (Figs. 1d-e). These profiles show that dredges containing peridotite mylonites were collected at distances ranging from <1 km up to ~7 km away from the deepest point in the transform fault valley. The mylonite-bearing dredges contain 29-100% ultramafic samples, with the remaining samples mainly consisting of basalts, diabases and greenstones (i.e., altered mafic rocks). We have not assessed the extent of deformation in the crustal lithologies; the sample descriptions from the cruise reports [START_REF] Farmer | Description of WHOI rock dredge samples: volume 3[END_REF]Scripps Institution of Oceanography, 1984) indicate that they have only been affected by brittle deformation. Among the ultramafic samples, 0-56% are porphyroclastic peridotites, 25-96% are mylonitic peridotites and 0-17% are foliated serpentinites (See Supplementary Table 1 for dredge sample descriptions). Breccias make up 0 to 9% of the dredges and exhibit either carbonate or serpentine matrices. All mantle rocks underwent intense deformation, mainly through ductile processes, but exhibit varying degrees of strain (i.e. grain size reduction). The proportion of highly deformed peridotites compared to protogranular and porphyroclastic peridotites decreases away from the center of the fault zone for both OTFs (Figs.

1d-e).

The samples used in this study come from the seafloor sample repository at Woods Hole Oceanographic Institution. From the five dredges that sampled the fault zones along the Shaka and Pr.

Edwards OTFs, we classified the textures of 34 deformed samples. These samples were chosen as representative of the range of lithologies and textures found within each dredge (Supplementary Table 1). In the cruise reports, 10 samples were classified as porphyroclastic peridotites (from dredges 61, 63 and 19), 22 as mylonites (from dredges 60, 61 and 18) and 2 as serpentinites (dredge 61). Based on analysis of hand samples and thin sections, we re-classified all these samples as mylonites. Our updated descriptions along with the original dredge descriptions are in Supplementary Table 1. We then subdivided the samples into three groups based on the intensity of grain size reduction through the proportion of fine-grained matrix: <50% for protomylonites, 50-90% for mylonites and >90% for ultramylonites (e.g., [START_REF] Passchier | Microtectonics[END_REF]. In this classification, samples that were described as porphyroclastic are now termed protomylonitic. Photos of the different mylonitic textures in hand sample and thin section are shown in Figs. A1 andA2.

Of the 34 hand samples evaluated (Supplementary Table 1), 7 from Shaka and 4 from Pr.

Edward were selected for detailed geochemical analysis (Table 1). The samples represent four of the five mylonite-bearing dredges and cover the range of observed textures. Samples from dredge 63 were not selected for further analysis because they are too weathered.

Methods

Sample mineralogy

We used a combination of optical microscopy and energy-dispersive X-ray spectroscopy (EDS)

analysis to determine sample mineralogy and phase distribution. For EDS analysis, we used a Zeiss Auriga 60 CrossBeam scanning electron microscope (SEM) equipped with an Oxford Synergy X-MAX 80 mm 2 EDS detector at the Keck Center for Advanced Microscopy at the University of Delaware (USA). Measurements were made at an accelerating voltage of 15 kV, an aperture of 30 µm (which controls the beam current) and a working distance of 8-10 mm. For EDS analyses, dwell time and process time were set in order to get a deadtime of ~20%. AZtec v3.3 software from Oxford Instruments (UK) was used to collect and process EDS spectra and to construct phase maps.

Mineral composition

Quantitative compositional analysis of minerals was performed on two different electron microprobes: a JEOL JXA-8900R at the Department of Earth Sciences, University of Minnesota (USA) and a JEOL JXA-8230 at ISTerre, Grenoble-Alpes University (France). Data are reported in Supplementary Table 2.

At the University of Minnesota, data were collected with an accelerating voltage of 15 kV, a beam current of 20 nA on a tungsten filament and beam diameters of 1 µm. The on-peak counting time was 20 s for all elements and mean atomic number (MAN) backgrounds were utilized [START_REF] Donovan | A new EPMA method for fast trace element analysis in simple matrices[END_REF]. Standardization was made using synthetic and natural oxides as well as natural minerals.

Unknown and standard intensities were corrected for deadtime and standard intensities were corrected for drift over time. The matrix correction was calculated with a Phi-Rho-Z method using an

Armstrong/Love Scott algorithm [START_REF] Armstrong | Quantitative analysis of silicate and oxide minerals: comparison of Monte Carlo, ZAF and phi-rho-z procedures[END_REF] and the mass attenuation coefficients from the FFAST database [START_REF] Chantler | X-ray form factor, attenuation and scattering tables (version 2.1)[END_REF]. Oxygen abundance was calculated by cation stoichiometry and included in the matrix correction.

At ISTerre, data were collected with an accelerating voltage of 20 kV and a field emission gun with a beam current of 300 nA for olivine (see detailed procedure in [START_REF] Sobolev | The amount of recycled crust in sources of mantle-derived melts[END_REF], 20 kV and 50 nA for spinel, and 15 kV and 12 nA for other silicates. Beam diameters ranged from 1-5 µm depending on the target grain size. Standardization was made using synthetic oxides and natural minerals. The matrix correction was calculated with a ZAF method (e.g., [START_REF] Batanova | Trace element analysis of olivine: High precision analytical method for JEOL JXA-8230 electron probe microanalyser[END_REF].

Thermobarometry

To determine the P-T conditions during mylonite deformation, we used empirical thermometers to evaluate temperature and construct pseudosections to determine the stability fields of mineral assemblages associated with deformation. We applied two thermometers, both of which are based on orthopyroxene composition: TAl-Cr in Opx of [START_REF] Witt-Eickschen | Solubility of Ca and Al in orthopyroxene from spinel peridotite: an improved version of an empirical geothermometer[END_REF] and TCa in Opx of [START_REF] Brey | Geothermobarometry in four-phase lherzolites II. New thermobarometers, and practical assessment of existing thermobarometers[END_REF]. TCa in Opx reported in Table 2 was calculated for a pressure of 5 kbars.

Pseudosections were constructed using Perple_X software [START_REF] Connolly | The geodynamic equation of state: What and how[END_REF] in the NCFMASH (Na2O-CaO-FeO-MgO-Al2O3-SiO2-H2O) chemical system. As whole rock major element compositions are needed to define the system composition, we obtained the composition of one protomylonite, three mylonites, and three ultramylonites through analysis of samples at the Washington State University GeoAnalytical Lab (Table B.1). Details of the thermodynamic solid solution models used in Perple_X are provided in Appendix B.

Results

All mylonites show both ductile and brittle deformation features. We classified the samples into three categories based on the mineral assemblages associated with their ductile deformation, which we interpret as representative of distinct temperature ranges of deformation (Table 1). We therefore term the categories as low-temperature (LT), medium-temperature (MT) and high-temperature (HT) mylonites (Fig. 2). This classification scheme is based primarily on mineralogy, so different rock textures from proto-to ultra-mylonite may be grouped together.

Petrographic observations of ductile deformation

All samples in this study are composed of coarser-grained porphyroclasts and finer-grained material (rock matrix). Thin sections were cut orthogonal to the foliation plane defined by alternating coarseand fine-grained layers, which we interpret as the shear plane (Figs. 2a-c), and parallel to the lineation defined by the long axis of porphyroclasts. The rock matrix consists of bands of very fine-grained material that are oriented parallel to the interpreted shear plane (Figs. 2d-i), which we will refer to as shear bands. In higher strain samples (mylonites and ultramylonites), shear bands alternate with coarser-grained olivine-rich domains within the matrix. We classified samples as LT, MT, or HT based on the mineralogy of the shear bands, as these features developed during ductile deformation (Fig. 2).

Porphyroclasts of orthopyroxene (Opx1), clinopyroxene (Cpx1), and Al-Cr spinel (Spl1) are present in samples from all three categories. In protomylonitic samples, olivine (Ol1) is also present as porphyroclasts, but is only present in the matrix in mylonites and ultramylonites. In the two samples from dredge 19, plagioclase (Plg1) is present as coronas around Spl1.

LT mylonites are characterized by serpentine-rich bands oriented parallel to the shear plane (Fig. 2). The serpentine layers occasionally contain talc, chlorite, amphibole, and oxides, in textural equilibrium with serpentine (Fig. C.1). MT mylonites (Fig. 2e,h) are characterized by amphibole and chlorite aligned and elongated parallel to the shear plane. Amphibole-rich bands may be continuous on the thin section scale, whereas chlorite is less abundant and dispersed, usually forming coronas around Al-free Cr-spinel (Figs. 2e andh). HT mylonites (Fig. 2) contain amphibole in their shear bands (Fig. 2i), but otherwise have the standard anhydrous mineral assemblage of peridotites. In contrast to MT mylonites, chlorite is absent in HT mylonites, and spinel is unaltered and Al-rich.

Grain size of serpentine and chlorite could not be determined microscopically. Other phases located in shear bands have <20 µm mean grain sizes, with no clear relationship between shear band grain size and rock texture. Shear bands in rocks with protomylonitic and ultramylonitic textures have average grain sizes of 5-10 µm, while mylonitic textures seem to have slightly higher grain sizes, on the order of 10-20 µm.

Petrographic observations of brittle deformation

All samples underwent brittle deformation in addition to ductile deformation, as evidenced by the presence of crosscutting intra-and trans-granular fractures (Fig. 2). All three types of mylonites are crosscut by serpentine ± magnetite ± talc filled fractures, which are classified as LT fractures based on their mineral assemblage (Table 1). In addition, the MT and HT mylonites are crosscut by chlorite + amphibole-filled fractures, which are classified as MT fractures (Table 1).

In addition to LT and MT fractures, we also identified HT fractures in the microstructures of the HT mylonites. In these samples, porphyroclasts are often fractured and fragmented (Fig. 3). Many of these fractured grains show evidence of intra-crystalline plasticity prior to fracturing, based on the occurrence of grains that are elongated, bent, or have undulose extinction (Figs. 3a andc). These intragranular fractures are filled with the same mineral assemblage that is present in the shear bands in these rocks (Figs. 3b andd): amphibole, sulfide, olivine, orthopyroxene (Opx2), clinopyroxene (Cpx2), spinel (Spl2) ± plagioclase (Plg2). These minerals are also found to have similar chemical compositions to minerals in the shear bands (Supplementary Table 2).

HT mylonites also contain fractures that crosscut the samples and are filled with amphibole ± sulfides (Fig. 2c). We refer to these as transgranular fractures, as they crosscut many grains without following grain boundaries. We observed them in the four HT samples that have mylonitic and ultramylonitic textures (Table 1), and in great number in mylonite PROT5-18-11. Interestingly, some of these HT transgranular fractures were subsequently offset by ductile deformation within shear bands (e.g., Fig. 4).

Amphibole composition

Amphibole is present in shear bands and fractures in all the mylonites and has a wide compositional range that reflects a range of formation conditions (Fig. 5). In HT mylonites, amphibole is pargasite or Mg-hornblende in composition and no intragranular zoning is observed (Fig. 5a). Amphibole composition varies between the proto-and ultra-mylonites (Fig. 5a), with the Si content of amphibole increasing with increasing intensity of deformation. However, amphibole composition does not vary between the fractures and the fine-grained ductile shear bands (Fig. 5a).

In MT mylonites, amphibole is Mg-hornblende to tremolite in composition (Fig. 5b) and has a Si content between 7.1 and 7.6 apfu. Only samples AII107-6-60-07 (Si, 6.7-6.8 apfu) and AII107-6-60-68 (Si, 7.8-7.9 apfu) fall outside this range (Fig. 5b). In both these samples, amphibole grains have concentric chemical zoning, with the cores having lower Si and higher alkali contents (Fig. 5b), as well as higher Al and Ti contents (Supplementary Table 2) than the rims. The transition from core to rim composition is sharp, occurring over a distance <3 µm (Fig. C.2). In AII107-6-60-07, cores and rims are both Mg-hornblende, but the core composition is similar to amphibole in HT mylonites, while the rim composition is similar to the majority of other MT mylonites (Figs. 5a-b). In AII107-6-60-68, cores are Mg-hornblende and rims are tremolite in composition (Fig. 5b).

Amphibole was only analyzed in one LT mylonite (sample AII107-6-61-89). This sample has two generations of amphibole: a first generation found in textural equilibrium with minerals in the coarser-grained olivine-rich zones of the matrix, and a second generation located in the shear bands in textural equilibrium with serpentine (Fig. C.1). The first generation is of Mg-hornblende to tremolite composition (Si, 7.4-7.6 apfu; Fig. 5b). The second generation of amphibole, associated with LT deformation, is tremolite in composition and has Si contents of 7.9-8.0 apfu (Fig. 5b).

Amphiboles in LT to HT mylonites have chlorine concentrations ranging from below the detection limit up to 0.67 wt% (Fig. 5c). Chlorine shows an overall trend of decreasing concentration with increasing silica, i.e. from amphibole in HT to LT mylonites (Fig. 5c). In addition, chlorine decreases with increasing Fe#, Fe 2+ /(Fe 2+ +Mg), (Fig. C.3). These variations are interpreted to reflect the structural control of Cl incorporation in amphibole (e.g., [START_REF] Campanaro | An experimental study of chlorine incorporation in amphibole synthesized along the pargasite-ferro-pargasite join[END_REF]. The overall amount of Cl in the amphiboles is relatively high, with up to 10 5 times the predicted concentration of Cl in the Depleted Mantle (ClDM = 0.14-0.38 μg/g; [START_REF] Urann | Fluorine and chlorine in mantle minerals and the halogen budget of the Earth's mantle[END_REF].

P-T-fluid conditions during deformation

To evaluate the P-T conditions during mylonitic deformation, we used two empirical geothermometers that are based on the composition of orthopyroxene. Temperatures were calculated for porphyroclasts (cores and rims) for all categories of mylonites and for matrix shear bands in samples where orthopyroxene was found, totaling five HT and one MT samples (Table 2). Both TCa-in-Opx and TAl-Cr in Opx thermometers indicate that, in each sample, porphyroclast cores have higher temperatures than porphyroclast rims, and that porphyroclast rim temperatures are systematically higher than matrix grain temperatures (Fig. 6a). The composition of grains located in HT shear bands imply higher temperatures than that of grains located in shear bands of the MT mylonite samples (Fig. 6a).

Temperatures in HT mylonites range from 600 to 875°C with an average of ~700°C for TAl-Cr in Opx, and range from 700 to 850°C with an average of ~760°C for TCa-in-Opx (Fig. 6a). For the composition of 7 orthopyroxene grains found in the shear bands of one MT mylonite sample, both thermometers give an average temperature of ~600°C (Fig. 6a).

P-T pseudosections were built using Perple_X and provide constraints on the stability of phases associated with LT, MT and HT mylonite deformation. Fig. 6b shows the pseudosection of sample PROT5-19-08 calculated under water-saturated conditions. We also calculated pseudosections for six other samples (Fig. B.1) and found that the compositional variations among peridotites in this study do not significantly influence the stability fields of the observed hydrous phases. The stability of hydrous phases (serpentine, talc, chlorite, pargasite/Mg-hornblende and tremolite) is mainly temperature-dependent and is only slightly sensitive to pressure (Fig. 6b). The presence of syndeformational serpentine suggests that the LT mylonites formed at temperatures <500-650°C. This corresponds to the upper stability limit of antigorite and thus the highest temperature conditions at which any serpentine polymorph can be present (Guillot et al., 2015 and references therein). The presence of chlorite in MT mylonites constrains their deformation temperatures between 500 and 800°C. In HT mylonites, the only hydrous phase is pargasite to Mg-hornblende amphibole, which implies deformation at temperatures >750-800°C.

The pseudosection results agree well with the mineral thermometry estimate of ~600°C for the deformation temperature of matrix grains in MT mylonites (Fig. 6). For matrix grains in the HT mylonites, thermometry suggests a temperature range of 600-700 to 850-875°C (Fig. 6a). However, thermometric estimates below <750°C are not consistent with mylonite deformation under watersaturated conditions because chlorite is expected to form (Fig. 6b). These lower temperature estimates can be either explained by continued subsolidus diffusive re-equilibration of orthopyroxene

Discussion

Our petrological and geochemical observations indicate that peridotite mylonites and serpentinites dredged from the Shaka and Pr. Edward OTFs deformed by brittle and ductile processes within three distinct temperature ranges, forming LT (<500-650°C), MT (~500-800°C) and HT (>750-800°C)

mylonites. The following discussion focuses first on the evidence for seawater-peridotite interaction during deformation from LT to HT conditions. We then use our microstructural and chemical analyses of the mylonite to evaluate the depth extent and mechanism of seawater percolation and mantle hydration on OTF. Finally, we discuss the implications of fluid-mantle interaction for fault zone structure, rheology and geochemistry.

Seawater-mantle interaction from LT to HT conditions

Mylonites from the Shaka and Pr. Edward OTFs show evidence of interaction with seawater over a wide range of temperatures. The mylonite protolith is assumed to have been typical coarse-grained upper mantle peridotite, which does not contain hydrous phases (e.g., [START_REF] Dick | Mineralogic variability of the uppermost mantle along midocean ridges[END_REF][START_REF] Warren | Global variations in abyssal peridotite compositions[END_REF]. The absence of porphyroclasts of hydrous phases also suggests that no hydrous phase was present in the protolith prior to deformation. In contrast, hydrous phases are systematically present, and commonly abundant, in the shear bands of the mylonites, indicating that they crystallized during mylonite formation (Fig. 2). Serpentine (± talc, chlorite, amphibole) formed at LT conditions, chlorite and amphibole at MT conditions, and amphibole at HT conditions. Amphibole is present in LT to HT mylonites and has high concentrations of chlorine (Fig. 5c), which in HT mylonites is up to 10 5 times the predicted concentration of the upper mantle [START_REF] Urann | Fluorine and chlorine in mantle minerals and the halogen budget of the Earth's mantle[END_REF]. At lower temperature, amphibole contains less chlorine due to structural controls of Cl incorporation in amphibole (e.g., [START_REF] Campanaro | An experimental study of chlorine incorporation in amphibole synthesized along the pargasite-ferro-pargasite join[END_REF]. The abundance of chlorine in amphibole and the overall abundance of hydrous minerals suggest that hydrous minerals formed within the shear bands formed as a result of syndeformational interaction of peridotite with seawater.

The continuous spectrum of amphibole compositions suggests that mylonite formation and mantle hydration occurred over a continuous temperature range from LT to HT conditions.

Experiments have shown that the Si content of amphibole in peridotites is inversely proportional to its crystallization temperature [START_REF] Fumagalli | Alkali in phlogopite and amphibole and their effects on phase relations in metasomatized peridotites: a high-pressure study[END_REF]. The continuous decrease in Si from HT pargasite to LT tremolite (Fig. 5) is therefore consistent with continuous amphibole crystallization and mantlefluid interaction from LT to HT conditions. Some amphiboles have sharp zoning, with cores and rims having distinct compositions (Fig. B.1), which suggests that some rocks underwent two separate episodes of fluid/rock interaction during deformation, at two distinct temperatures during rock cooling and uplift to the seafloor.

Our thermometry estimates argue for formation of HT mylonites, and therefore seawatermantle interaction, at temperatures >850-875°C. The maximum temperature calculated for minerals in HT shear bands using the TCa in Opx and the TAl-Cr in Opx thermometers is 850°C and 875°C, respectively (Fig. 6a). In each sample, the estimated deformation temperatures of matrix grains are lower than those estimated for both the cores and rims of porphyroclasts (Table 2). This suggests that orthopyroxene matrix grains chemically (re)equilibrated during deformation and thus provide information on the temperature of HT mylonite deformation. [START_REF] Linckens | Linking temperature estimates and microstructures in deformed polymineralic mantle rocks[END_REF] used 1D diffusion modelling to estimate a closure temperature of ~800°C for orthopyroxene major element-based thermometers for a grain size of 50 µm. Hence, our estimates of 850-875°C are above the closure temperature of the two thermometers and thus represent minimum estimates of the maximum temperature of HT mylonite deformation.

Our results support seawater percolation and continuous fluid-mantle interaction up to high temperature conditions on transform faults. Analysis of rock samples from the Vema OTF on the MAR (Fig. 1f) supports our interpretations as serpentinite (LT), amphibole-chlorite (MT) and amphibole-bearing (HT) mylonites have also been dredged in large proportions on the Vema southern transform valley walls [START_REF] Cannat | A geological cross-section of the Vema fracture zone transverse ridge, Atlantic ocean[END_REF][START_REF] Cannat | Transform tectonics, metamorphic plagioclase and amphibolitization in ultramafic rocks of the Vema transform fault (Atlantic Ocean)[END_REF][START_REF] Cipriani | A 19 to 17 Ma amagmatic extension event at the Mid-Atlantic Ridge: Ultramafic mylonites from the Vema Lithospheric Section[END_REF].

Amphibole in the Vema samples has similar compositions [START_REF] Cipriani | A 19 to 17 Ma amagmatic extension event at the Mid-Atlantic Ridge: Ultramafic mylonites from the Vema Lithospheric Section[END_REF] to SWIR mylonite amphiboles, suggesting a similar temperature range for fluid-mantle interaction. Overall, observations of mylonites from OTFs indicate that hydrothermal fluids interact with the mantle up to at least 850-875°C and that this might be a common process on OTFs.

Depth of seawater percolation and mylonite formation

The depth of LT, MT and HT mylonite deformation cannot be directly estimated from our samples, as hydrous mineral stability in peridotites is mainly temperature-dependent (Fig. 6b), and mineral-based empirical barometers are not available for spinel-bearing peridotites. Therefore, to convert temperature constraints to depth, we use numerical models of fault thermal structure for the Shaka and Pr. Edward OTFs (Fig. 7a).

To evaluate the thermal structure of these two SWIR OTFs, we first use the results of a 3D viscoplastic, thermomechanical model (e.g., [START_REF] Behn | Thermal structure of oceanic transform faults[END_REF][START_REF] Roland | Thermal-mechanical behavior of oceanic transform faults: Implications for the spatial distribution of seismicity[END_REF] Based on the thermal models of the two OTFs, serpentinization and LT deformation occurs up to temperatures of 500-550°C, which corresponds to depths of ~11-13 km in the thermal model. LT mylonites formed somewhere within this domain and characterization of the serpentine polymorph (antigorite versus lizardite and/or chrysotile) could provide more specific constraints on the temperature of formation (e.g., [START_REF] Guillot | Tectonic significance of serpentinites[END_REF]. MT mylonite formation occurs at up to 700-750°C (16-19 km). Finally, our maximum estimate of >850-875°C for HT mylonite formation, and the limit of mantle hydration on OTFs, corresponds to depths >22-25 km. All together, these results prove that seawater can percolate deep into OTFs.

Fracturing as a mechanism for deep hydrothermal fluid percolation

Our results highlight seawater percolation and mantle hydration up to at least 850-875°C on OTFs. As discussed in Kohli and Warren (In Press), this observation contradicts the traditional view of the 600°C isotherm as the limit of brittle behavior in the oceanic lithosphere [START_REF] Abercrombie | Earthquake slip on oceanic transform faults[END_REF][START_REF] Boettcher | Olivine friction at the base of oceanic seismogenic zones[END_REF][START_REF] Jaroslow | Abyssal peridotite mylonites: implications for grain-size sensitive flow and strain localization in the oceanic lithosphere[END_REF][START_REF] Mckenzie | Thermal structure of oceanic and continental lithosphere[END_REF], and thereby the limit of seawater percolation on OTFs (e.g., [START_REF] Sibson | Seismic pumping-a hydrothermal fluid transport mechanism[END_REF]. In contrast, we show direct evidence of brittle deformation of peridotites at higher temperature, which is consistent with observations of deep earthquakes from recent seismic surveys [START_REF] Kuna | Mode of slip and crust-mantle interaction at oceanic transform faults[END_REF][START_REF] Mcguire | Variations in earthquake rupture properties along the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Wolfson-Schwehr | The relationship between seismicity and fault structure on the Discovery transform fault, East Pacific Rise[END_REF].

Our microstructural observations of HT mylonites reveal HT fracturing events coeval with mylonitic ductile deformation (Figs. 3 and4). In every sample, porphyroclasts can be crosscut by fractures (Fig. 3). These fractures are filled with the same mineral assemblage as observed in the mylonitic shear bands (Fig. 3) and show similar chemical compositions (e.g., Fig. 5a),. This high temperature semi-brittle behavior is also shown by the offset of amphibole-filled transgranular veins by HT shear bands in HT mylonites and ultramylonites (Fig. 4). This provides additional support for the idea that fractures developed during ductile deformation within the shear bands.

We propose that this HT fracturing process was the driving force for the deep downward migration of hydrothermal fluids, which resulted in HT mylonite hydration. Our results show that amphibole systematically occurs in the sealing material of porphyroclast fractures (Fig. 3) and is the dominant phase sealing transgranular fractures (Fig. 2i). This indicates that, at the sample scale, brittle failure locally enhanced rock permeability, driving fluid flow and amphibole crystallization in HT mylonites. Accordingly, we propose that this HT brittle behavior of peridotites leads to the formation of hydrothermal fluid pathways, allowing for deep seawater percolation and mantle hydration within the fault zone (Fig. 7b). In HT and MT mylonites, amphibole is concentrated in fine-grained shear zones and absent from coarser-grained zones (Figs. 2h andi; Kohli et al, in press). This might suggest that, after fracturing and fluid flow, subsequent ductile deformation is localized and possibly drives fluid flow preferentially through mylonitic regions [START_REF] Fusseis | Creep cavitation can establish a dynamic granular fluid pump in ductile shear zones[END_REF]Précigout et al., 2017).

Brittle behavior of peridotites in fault zones is thought to be limited to ~600°C, which corresponds to the temperature of the brittle-ductile transition of olivine at tectonic strain rates (10 -12 -10 -15 s -1 ). This temperature was determined by extrapolating the results of deformation experiments on olivine aggregates from laboratory strain rates (10 -4 -10 -7 s -1 ) to tectonic strain rates [START_REF] Boettcher | Olivine friction at the base of oceanic seismogenic zones[END_REF]. Here, we provide evidence for brittle behavior of mantle peridotites at much higher temperatures. This suggests that the mechanism for HT fracturing of the coarse-grained peridotite protolith is deformation at strain rates higher than tectonic strain rates. The experiments of [START_REF] Boettcher | Olivine friction at the base of oceanic seismogenic zones[END_REF] show that brittle deformation in olivine at temperatures up to ~900°C requires strain rates of 10 -8 s -1 or higher, which is consistent with estimates from [START_REF] Kohli | Evidence for a deep hydrologic cycle on oceanic transform faults[END_REF] based on rheological modeling of the Shaka mylonites.

Our observations of high temperature brittle failure in the mylonites agrees with the results of two recent ocean bottom seismometer campaigns on the Gofar and Discovery OTFs on the fast slipping East Pacific Rise [START_REF] Mcguire | Variations in earthquake rupture properties along the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Wolfson-Schwehr | The relationship between seismicity and fault structure on the Discovery transform fault, East Pacific Rise[END_REF] and on the Blanco OTF on the intermediate slipping Juan de Fuca Ridge [START_REF] Kuna | Mode of slip and crust-mantle interaction at oceanic transform faults[END_REF]. Based on similar thermal models as in Fig. 7, earthquakes located within the mantle imply brittle failure above 600°C on both faults, and possibly up to 1000-1100°C on Gofar [START_REF] Guo | Structural control on earthquake behaviors revealed by highresolution Vp/Vs imaging along the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Roland | Seismic velocity constraints on the material properties that control earthquake behavior at the Quebrada-Discovery-Gofar transform faults, East Pacific Rise[END_REF]. Brittle deformation of mantle peridotites at temperatures above their long-term brittle-ductile transition therefore seems to characteristic of both fast-to ultraslow slipping OTFs, from, which suggests that deep seawater percolation exists across the global transform system.

Evolution of fault zone structure and slip behavior due to fluid-rock interaction

In the ocean bottom seismometer campaigns, spatial variations have been observed in the seismic behavior of the mantle. The mantle at temperatures below 600°C deforms by aseismic creep or can slip seismically in either large, quasi-periodic mainshocks or micro-earthquakes [START_REF] Kuna | Mode of slip and crust-mantle interaction at oceanic transform faults[END_REF].

Above the 600°C isotherm, the mantle deforms aseismically in some sections of the faults, while micro-earthquakes are recorded on other sections [START_REF] Guo | Structural control on earthquake behaviors revealed by highresolution Vp/Vs imaging along the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Kuna | Mode of slip and crust-mantle interaction at oceanic transform faults[END_REF][START_REF] Roland | Seismic velocity constraints on the material properties that control earthquake behavior at the Quebrada-Discovery-Gofar transform faults, East Pacific Rise[END_REF]. Some of these variations may be explained by spatial variations in the intensity of mantle deformation and hydration.

An important implication of the fluid-mantle interaction recorded in mylonites from the Shaka and Pr. Edward OTFs is that the structure and the rheology of the mantle evolves as a function of time, strain and hydration. With increasing intensity of peridotite deformation and hydration, mantle deformation transitions from being accommodated by deformation of dry, coarse-grained peridotites, mainly olivine, to being controlled by the rheology of interconnected, weak LT, MT and HT mylonitic shear zones (Fig. 7b).

In the LT domain, progressive accommodation of fault slip by serpentinite shear zones on active OTFs is consistent with observations of the exhumed Southern Troodos Transform Fault Zone (Cyprus). Studies have highlighted that the dominant structures in the mantle section of this ~5 km wide fault zone are serpentinite mélange [START_REF] Macleod | On the sense of slip of the Southern Troodos transform fault zone, Cyprus[END_REF], with the proportion of serpentinite matrix to embedded blocs increasing with strain [START_REF] Fagereng | On Seismicity and Structural Style of Oceanic Transform Faults: A Field Geological Perspective From the Troodos Ophiolite, Cyprus[END_REF].

Serpentine is a mechanically weak mineral and, in contrast to olivine, can steadily creep at tectonic strain rates and LT temperature conditions (Guillot et al., 2015 and references therein). These observations recently lead [START_REF] Fagereng | On Seismicity and Structural Style of Oceanic Transform Faults: A Field Geological Perspective From the Troodos Ophiolite, Cyprus[END_REF] to propose that spatio-temporal variations in mantle serpentinization could explain lateral variations observed in the seismic behavior of OTFs at temperatures less than 600°C (e.g., [START_REF] Wolfson-Schwehr | Global Characteristics of Oceanic Transform Fault Structure and Seismicity[END_REF]. Serpentinized segments of the fault zone would have low seismic coupling and would creep aseismically, whereas segments composed of dry peridotites would be locked interseismically between seismic events.

Deeper on the OTFs, deformation in hydrated shear zones is mainly accommodated by chlorite and amphibole assemblages at MT conditions (Fig. 2h) and by fine-grained, amphibole-bearing assemblages at HT conditions (Fig. 2i). The mechanical behavior of such assemblages has not been studied experimentally. We know, however, that chlorite is a mechanically weak phyllosilicate owing to its planar crystallographic structure, and the presence of chlorite can therefore trigger peridotite weakening (e.g., [START_REF] Amiguet | Creep of phyllosilicates at the onset of plate tectonics[END_REF]. In contrast, [START_REF] Tommasi | Hydrous melts weaken the mantle, crystallization of pargasite and phlogopite does not: Insights from a petrostructural study of the Finero peridotites, southern Alps[END_REF] found no evidence of peridotite weakening associated with increasing amounts of amphibole in a study of a natural upper mantle shear zone containing pargasitic amphibole. However, this result may not be applicable the MT mylonites where tremolitic amphibole forms continuous bands at the sample scale. In addition, Kohli and Warren (In Press) found that the presence of amphibole promoted olivine grain size reduction and thus weakening through a transition from grain-size insensitive to grain-size sensitive creep. In this study, we also found that the grain size reduction associated with both MT and HT mylonite deformation provides a weakening mechanism. Kohli et al. (subm.) also noted that this switch causes a shallowing of the brittle-ductile transition in the mantle lithosphere. Variations in the depth extent of microseismicity in the mantle on OTFs [START_REF] Guo | Structural control on earthquake behaviors revealed by highresolution Vp/Vs imaging along the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Kuna | Mode of slip and crust-mantle interaction at oceanic transform faults[END_REF][START_REF] Mcguire | Variations in earthquake rupture properties along the Gofar transform fault, East Pacific Rise[END_REF][START_REF] Roland | Seismic velocity constraints on the material properties that control earthquake behavior at the Quebrada-Discovery-Gofar transform faults, East Pacific Rise[END_REF] could therefore be explained by variations in the degree of strain and hydration within the fault zones, with aseismic (ductile) zones being more deformed and hydrated than seismic (brittle) patches.

We conclude that increasing hydration and strain of mantle rocks on OTFs leads to weakening from LT to HT conditions and changes in seismic behavior. Lateral variations in mantle seismicity may thus be explained by lateral variations in the intensity of mantle deformation and fluid-rock interaction.

Implications of deep fluid-rock interaction for volatile cycling and subduction zone dynamics

Oceanic fracture zones (OFZs) are the relict trace of OTFs that extend beyond mid-ocean ridge offsets and eventually enter the mantle at subduction zones (e.g., [START_REF] Manea | Subduction of fracture zones controls mantle melting and geochemical signature above slabs[END_REF]. The depth and extent of hydration of the lithosphere at OTFs is therefore important to the global volatile cycle and the geochemical budget of subduction zones. Phases precipitating after hydrothermal fluid-mantle interaction, especially serpentine, chlorite and amphibole, are able to host large amounts of volatiles in their mineral structures. This includes water (~13 wt% for serpentine; e.g., [START_REF] Ulmer | Serpentine stability to mantle depths and subduction-related magmatism[END_REF] and fluid-mobile elements such as boron, chlorine, strontium (e.g., [START_REF] Scambelluri | Serpentinite subduction: implications for fluid processes and trace-element recycling[END_REF][START_REF] Urann | Fluorine and chlorine in mantle minerals and the halogen budget of the Earth's mantle[END_REF]. Our observations of deep and intense mantle hydration on OTFs indicate a depth range of 11-13 km for serpentinization on ultra-slow slipping OTFs, which has important implications for subduction. At slab de-serpentinization temperatures (~600-700°C; e.g., [START_REF] Ulmer | Serpentine stability to mantle depths and subduction-related magmatism[END_REF], higher water flux into the overlying mantle wedge would be promoted in regions of subducting OFZs compared to the surrounding oceanic lithosphere. This could explain the overall higher rate of seismicity [START_REF] Schlaphorst | Water, oceanic fracture zones and the lubrication of subducting plate boundaries-insights from seismicity[END_REF] and clustering of deep intra-slab seismicity [START_REF] Paulatto | Dehydration of subducting slow-spread oceanic lithosphere in the Lesser Antilles[END_REF] observed in sub-arc regions along the Lesser Antilles subduction zone where several MAR OFZs are subducting.

In addition to water, modeling results of [START_REF] Mccaig | No significant boron in the hydrated mantle of most subducting slabs[END_REF] suggest that the process of deep and intense hydrothermal fluid flow on OTFs, as we observe in this study, is needed to add significant boron to the mantle. On fault systems which are not long-lived and/or permeable (e.g., bending faults found in the outer rise of subduction zones), boron is completely consumed through crustal alteration before hydrothermal fluids reach the mantle. Deep fluid flow and mantle serpentinization on OTFs, as well as deserpentinization at sub-arc depths, therefore could account for the observation that volcanoes located above subducting OFZs along the Aleutian and Andean margins have lavas relatively enriched in boron compared to other arc volcanoes [START_REF] Manea | Subduction of fracture zones controls mantle melting and geochemical signature above slabs[END_REF].

Conclusion

Our 1: Some samples were previously studied: AII107-6-61-83, PROT5-18-10 and PROT5-18-11 by [START_REF] Jaroslow | Abyssal peridotite mylonites: implications for grain-size sensitive flow and strain localization in the oceanic lithosphere[END_REF], AII107-6-61-83 by Warren and Hirth (2006), and AII107-6-60-4, AII107-6-60-5, AII107-6-60-7 and AII107-6-61-83 by Kohli and Warren (subm).

  compositions after deformation or by deformation of HT mylonites at water-undersaturated conditions (<0.5 wt%; Fig. B.2).

  of Shaka OTF. The model is composed of two ridge segments offset by a transform fault. Three-dimensional mantle flow is driven kinematically by imposing a half-slip rate on either side of the transform fault at the surface of the model. As Shaka and Pr. Edward faults have similar slip rates and offsets and neither are segmented (e.g., Wolfson-Schwehr and Boettcher, 2019), we consider their thermal structures to be similar (Fig. 7a) and calculate the Pr. Edward thermal structure from the scaling relations developed by Wolfson-Schwehr et al. (2017) based on fault slip rate. The full slip rates of the two faults are from the NUVEL-1 model (Argus and Gordon, 1991) and fault lengths are from the database of Wolfson-Schwehr and Boettcher (2019).

  study of deformed peridotites and serpentinites dredged from the Shaka and Pr. Edward OTFs indicate deep and intense fluid-rock interaction during deformation of peridotites on OTFs. By combining observations of the mineral assemblages present in fractures and shear bands with thermometric and thermodynamic calculations, we identified three domains of deformation corresponding to different temperature conditions. They are characterized by crystallization of (i) serpentine (± talc ± tremolitic amphibole ± chlorite ± oxides) at <500-550°C (LT domain), (ii) chlorite, Mg-hornblende to tremolitic amphibole and oxides at ~500-750°C (MT domain), and (iii) pargasitic to Mg-hornblende amphibole, sulfides and new peridotitic minerals at >750°C (HT domain).The crystallization of Cl-rich amphibole in each domain indicates that the peridotite reacted with seawater-derived fluids during deformation.In each domain, samples record evidence of deformation by both brittle and ductile mechanisms, with fracturing and fluid-mantle interaction leading to the progressive formation of LT, MT and HT mylonites. Empirical thermometers indicate HT semi-brittle deformation and mantle hydration extended to temperatures up to at least 850-875°C, beyond the long-term brittle-ductile transition of olivine, and likely results from high strain rates in the fault zones. We applied our temperature constraints on the mylonites to modeled geotherms of Shaka and Pr. Edward OTFs, which indicates that mantle serpentinization extends to ~11-13 km and deep seawater percolation extends to ~25-30 km.The evolution in fault zone structure induced by progressive fracturing and fluid-rock interaction leads to the crystallization of weak phases at shallow levels and grain size reduction deeper on the fault, providing mechanisms to account for weakening and strain localization processes within the hydrated portions of the mantle on OTFs. Due to intense and deep fluid-rock interaction, the mantle lithosphere on OTFs also likely represents very large reservoirs for volatiles and are thus important elements of the Earth's volatile cycle.

Fig. 1 .

 1 Fig. 1. Location (a) and bathymetric maps of the Shaka (b) and Pr. Edward (c) OTFs. (d-e) Map

Fig. 2 .

 2 Fig. 2. Texture and mineralogy of low temperature (LT), medium-T (MT) and high-T (HT) mylonites.

Fig. 3 .

 3 Fig.3.Textures in shear zones of LT mylonites. Optical photomicrographs in cross-polarized light (a)

Fig. 4 .

 4 Fig. 4. Evidence for HT fracturing of porphyroclasts in (a-b) protomylonite PROT5-19-08 and (c-d)

Fig. 5 .

 5 Fig. 5. Polarized optical photomicrograph showing transgranular fractures in a HT mylonite (PROT5-

Fig. 6 .

 6 Fig. 6. Composition of amphibole in LT, MT and HT shear bands (circles) and fractures (crosses).

Fig. 7 .Fig. 8 .

 78 Fig. 7. Thermobarometry of HT, MT and LT mylonites. (a) Temperatures of porphyroclasts and grains

2:

  Low temperature (LT) deformation domain is characterized by the presence of serpentine (Serp). Medium-T (MT) domain is marked by crystallization of chlorite (Chl) and tremolitic to Mg-hornblende amphibole (Amp).The high temperature (HT) domain is defined by crystallization of Mg-hornblende to pargasitic amphibole. D, B/D and B if the sample deformed in the deformation domain by ductile, semi-brittle or brittle mechanisms, respectively. A blank means that the sample has not experienced or has not preserved evidence of deformation within the corresponding deformation domain. Table2. Temperature estimates based on orthopyroxene (Opx) composition (TCa in Opx of[START_REF] Brey | Geothermobarometry in four-phase lherzolites II. New thermobarometers, and practical assessment of existing thermobarometers[END_REF] and TAl-Cr in Opx of Witt-Eickschen and Seck (1991)). The average temperatures are written in °C and the number of averaged grains is in parentheses.

Table 1 .

 1 Location of dredges, rock type and deformation features of selected samples.

						Deformation 2
	OTF	Cruise	# Dredge	# 1 sample	Rock Type	HT	MT	LT
						(Amp)	(Chl + Amp) (Serp)
	Shaka	AII107-6	60	4	MT mylonite		B/D	B
				5	MT mylonite		B/D	B
				7	MT mylonite	B/D	B/D	B
				68	MT mylonite		B/D	B
			61	80	HT ultramylonite	B/D		B
				83	HT ultramylonite	B/D		B
				89	LT (ultra)mylonite		B/D	B/D
	Pr Edward	PROT5	18	10	HT mylonite	B/D		B
				11	HT mylonite	B/D	B	B
			19	1	HT protomylonite	B/D	B	B
				8	HT protomylonite	B/D		B

Acknowledgments

We are grateful to Anette van der Handt, Valentina Batanova and Valérie Magnin for their technical support and advice on EPMA analyses and to Yong Zhao for assistance with the University of Delaware SEM. This work was supported by National Science Foundation grants EAR-1347696 and EAR-1619880, and funds provided to Jessica Warren as part of the University Startup funding.