Timing and conditions of brittle faulting on the Silltal-Brenner Fault Zone, Eastern Alps (Austria)
Swiss Journal of Geosciences volume 108, pages 305–326 (2015)
The Silltal Fault is the northern brittle continuation of the Brenner Fault Zone, marked by a narrow zone of cataclasis and, in three locations, clay-rich fault gouges. The clay mineral composition of these gouges is dominated by higher temperature 2M1 polytype illite/muscovite, with no 1M/1Md illite or mixed layer illite/smectite detected. Smectite is limited to the northern samples from the Stephansbrücke location, whereas chlorite is present in all samples. The K–Ar ages from the different sample size fractions (<0.1, <0.4, <2, 2–6, 6–10 μm, “whole rock gouge”) show a wide spread, from ca. 115 to 12 Ma, with ages consistently decreasing with grain size. Although the ranges overlap, ages from the northern Stephansbrücke samples are generally older (115–36 Ma) than those from the south near Matrei (55–12 Ma), possibly reflecting increasing regional metamorphic temperatures to the south. The well-defined linear relationship between apparent age and hydrogen stable isotope (δD) values establishes a direct correlation between rejuvenation of the K–Ar system and increased interaction with meteoric water introduced and focussed within the fault zone. The dependence of both apparent age and δD on grain size also indicates that radiogenic and stable isotope exchange was controlled by grain size, reflecting new 2M1 illite growth, mechanical grinding of protolith muscovite during cataclastic faulting, or both. The results demonstrate the advantages of combining radiogenic and stable isotope analysis in interpretation of K–Ar ages from clay fault gouges. The combined approach was necessary to establish the crucial influence on apparent K–Ar ages of meteoric water influx focussed on the fault zone and its interaction with clay-size-fraction grains.
The Silltal Fault is usually taken to be the direct continuation along strike of the younger brittle part of the Brenner Fault Zone, which forms the western boundary of the Tauern Window (Fig. 1; Schmidegg 1953, 1964; Frank et al. 1987; Behrmann 1988; Selverstone 1988; Fügenschuh et al. 1997, 2000; Rosenberg and Garcia 2011). The Brenner Fault Zone is one of two major low-angle normal faults that mark the western boundaries of regional-scale tectonic windows in the Alps: the other example is the Simplon Fault Zone limiting the Lepontine Metamorphic Dome in the Central Alps. These two fault systems appear to be directly analogous, developing mainly in the period from ~20 Ma to present and reflecting important orogen-parallel extension during ongoing Alpine convergence (Mancktelow 1985, 1992; Behrmann 1988; Selverstone 1988; Prey 1989; Grasemann and Mancktelow 1993; Fügenschuh et al. 1997, 2000; Campani et al. 2010a, b). The two fault zones involve regional exhumation of both hanging wall and footwall but whereas the hanging wall remained brittle, the more rapidly exhuming footwall underwent a transition from a broad zone of higher grade ductile mylonites to more localized brittle faulting during cooling. The latest relative displacement was localized on a discrete brittle fault marked by cataclasites and locally by clay fault gouge, as investigated here along the Silltal Fault.
Foliated clay fault gouges from the Stephansbrücke clay pit (e.g. Schmidegg 1953) preserve kinematic indicators indicating a normal sense typical of the Brenner Fault Zone further to the south and have been used as geological field evidence for quite recent movement on a continuous Silltal-Brenner Fault Zone (Reiter et al. 2005). However, until now there were no age data available to constrain the time of formation of this fault gouge. Clay fault gouges are typical of many important brittle faults active under relatively low metamorphic grade, near surface conditions (e.g. Engelder 1974; Rutter et al. 1986). If authigenic illite is present, such gouges can reliably date the timing of fault activity (e.g. Lyons and Snellenburg 1971; Kralik et al. 1987; Van der Pluijm et al. 2001; Zwingmann and Mancktelow 2004; Zwingmann et al. 2004, 2010a, 2011; Solum et al. 2005; Solum and van der Pluijm 2007; Surace et al. 2011; Pleuger et al. 2012; Clauer 2013; Viola et al. 2013; Yamasaki et al. 2013; Bense et al. 2014; Torgersen et al. 2014a). In this study, samples of clay fault gouge associated with the Silltal Fault were collected for K–Ar dating from the Stephansbrücke clay pit in the north and from two exposures some 8 km further to the SE.
Undeformed and recrystallized phyllosilicates (white mica, biotite, chlorite) were also collected along a broad profile from the brittle hanging wall into the mylonitic footwall of the Brenner Fault Zone further to the south (Fig. 1), with this profile corresponding to a telescoped crustal section through the detachment system. Similar to Hetzel et al. (2013), H-isotope data were obtained from the dated clay fractions, as well as from phyllosilicates collected across the wider shear zone, in order to identify the fluid source(s) involved and possible syndeformational fluid pathway(s) within the crustal detachment. A particular aim was to assess the possible deep influx of surface-derived water along or close to the detachment, as had previously been established for the Simplon Fault Zone (Campani et al. 2012).
The measured (apparent) K–Ar ages for different clay size fractions generally decrease with decreasing grain size, as also reported in many studies from other areas (e.g. Hower et al. 1963; Pevear 1999), and range from Early Cretaceous to Middle Miocene. There are various possible interpretations of this grain size dependence in clay fault gouges, including physical mixtures of protolith and authigenic mica and clay (Pevear 1999; Vrolijk and van der Pluijm 1999; Van der Pluijm et al. 2001; Haines and van der Pluijm 2008), growth of different clays and polytypes during ongoing fault movement (Zwingmann et al. 2010a; Viola et al. 2013; Bense et al. 2014; Torgersen et al. 2014a), and grain-size dependent loss of Ar, due to thermally activated diffusion (Dodson 1973) or promoted by intracrystalline deformation in a hydrothermal environment (Villa 1998; Mulch et al. 2002; Mulch and Cosca 2004). The current study employs a multi-faceted approach to investigate the relationship of measured K–Ar ages to clay mineralogy, potential protolith contamination, fluid source (e.g. metamorphic or meteoric) and degree of fluid-rock interaction. Such a broad approach is crucial for (1) critically assessing different possible interpretations of K–Ar dates from clay fault gouges developed in protoliths that contain metamorphic white mica, and (2) constraining the timing and conditions of brittle faulting on the Silltal-Brenner Fault Zone in the Eastern Alps.
The fault gouge samples collected for this study come from clay-rich zones developed at, or immediately adjacent to, the contact between hanging and footwall units of the Silltal Fault. The Silltal Fault runs NNW from the NW corner of the Tauern Window in the Eastern Alps and marks the boundary between two distinctly different units, the Ötztal Crystalline Complex to the west and the Innsbruck Quartz Phyllite to the east (Fig. 1). The fault is marked by a cataclastic zone and locally by clay-bearing gouge (Fügenschuh 1995), though outcrop conditions along the fault trace are generally poor (Decker et al. 2009).
In more recent publications, the Silltal Fault is invariably considered to be the northerly continuation of the brittle component of the Brenner Fault Zone, with an effectively normal (i.e., top-down-to-W) sense of movement (Behrmann 1988; Selverstone 1988; Prey 1989; Ratschbacher et al. 1991; Fügenschuh 1995; Fügenschuh et al. 2000; Linzer et al. 2002; Reiter et al. 2005; Glodny et al. 2008; Rosenberg and Garcia 2011). However, there is a change in the units comprising the footwall at the junction of the continuous Silltal-Brenner Fault Zone with the northern boundary of the Tauern Window (Fig. 1): south of this triple-point, the footwall dominantly consists of calc-schists from the Penninic Glockner nappe (e.g. Frisch 1974) and, north of here, generally of upper Austroalpine Innsbruck Quartz Phyllite. In the area directly north of the Tauern Window, units of the lower Austroalpine Tarntal and Reckner nappes locally also occur in the immediate footwall of the Silltal Fault (Fig. 1) (Koller 2003; Töchterle et al. 2011). Further to the north, the Patscherkofel Crystalline Complex (Rockenschaub et al. 2003; Piber et al. 2008; Decker et al. 2009) occurs as a klippe on top of the Innsbruck Quartz Phyllite (Fig. 1). This klippe crops out on a slope dipping ca. 20°–30° to the west and projection down-dip suggests that it should be transected by the Silltal Fault near the Stephansbrücke clay pit locality (Location A, Fig. 1).
In general, the Innsbruck Quartz Phyllite preserves a pre-Alpine greenschist facies metamorphic mineral assemblage, whereas units from the Tauern Window record later Alpine greenschist to amphibolite facies metamorphism (e.g. Hoernes and Friedrichsen 1974). Radiometric mineral ages reflect this difference in Alpine metamorphic grade on the northern boundary of the Tauern Window: in the Innsbruck Quartz Phyllite, 40Ar/39Ar results for white mica typically give Late Permian or Triassic to Jurassic ages, whereas the corresponding ages in the Tauern Window are Oligocene to Miocene (Fig. 2). There is also a marked jump in fission track ages, for zircon from ca. 10 to 16 Ma in the Tauern Window to ca. 35–60 Ma north of it and for apatite from ca. 9 to 13 Ma (Fig. 2; Fügenschuh 1995; Fügenschuh et al. 1997). The 40Ar/39Ar white mica ages in the Patscherkofel Crystalline Complex klippe show a wide range but with two main peaks at around 149–180 Ma (Middle Jurassic) and 123–136 Ma (Early Cretaceous) (Rockenschaub et al. 2003). One retrograde mylonitic gneiss from the base of the Patscherkofel Crystalline Complex shows a white mica 40Ar/39Ar age spectrum with steps between 50 and 120 Ma, and two marked plateaux at 51 and 72 Ma (Rockenschaub et al. 2003). Rockenschaub et al. (2003) note that these ages are markedly younger than those from the overlying Patscherkofel Crystalline Complex and interpret these younger ages down to 50 Ma to reflect retrograde metamorphism and mylonitization at the base of this allochthonous klippe, possibly related to its top-to-west final emplacement. From the similarity in lithology and thermobarometric estimates, Piber et al. (2008) suggest the Patscherkofel Crystalline Complex to be a fragment of the Ötztal Crystalline Complex, which has been thrusted onto the Innsbruck Quartz Phyllite after the peak of Late Cretaceous metamorphism.
South of Matrei (Fig. 1), the footwall of the Brenner Fault Zone forms the Tauern Window, which was exhumed during movement on the Brenner Fault Zone from depths corresponding to amphibolite facies metamorphic conditions in the last ca. 20 Ma (Behrmann 1988; Selverstone 1988; Fügenschuh et al. 1997). It follows that the hanging wall in this region was already at temperatures below those necessary for annealing of apatite fission tracks (ca. 90–110 °C) and therefore brittle throughout the Brenner Fault Zone history. In contrast, the immediate footwall of the Brenner Fault Zone involved a transition from a broad zone of ductile mylonites to more localized shearing and eventually to movement on a discrete brittle detachment during exhumation and cooling (Fügenschuh et al. 1997). Unfortunately, no preserved clay fault gouge has yet been found associated with the Brenner Fault Zone detachment at the western end of the Tauern Window, although the clear topographic expression (a well-developed dip-slope and valley incision) certainly suggests that it is marked by a narrow zone of weaker material.
The hanging wall of the Silltal-Brenner Fault Zone consists of the Ötztal Crystalline Complex overlain by parautochtonous “Brenner Mesozoic” (meta-) sediments and the allochthonous Steinach and Blaser “nappes”. Metamorphism in the Ötztal Crystalline Complex and Brenner Mesozoic increases progressively from lowermost greenschist in the north to amphibolite facies in the south (Frank et al. 1987; Purtscheller et al. 1987; Fügenschuh et al. 2000). Mineral ages reflect this, with white mica 40Ar/39Ar ages in the north still retaining pre-Alpine ages of ca. 270 Ma whereas in the south they have been reset to Cretaceous ages of around 90 Ma (Fig. 2; Rockenschaub et al. 2003). The anchimetamorphic Steinach and Blaser “nappes” (Teichmüller and Teichmüller 1978) are allochthons transported to the ESE on low-angle normal detachments during exhumation at the end of the Cretaceous (Fügenschuh et al. 2000) and preserve pre-Alpine white mica 40Ar/39Ar ages (Rockenschaub et al. 2003). In the area of the hanging wall shown in Fig. 2, zircon fission track ages range from 55 to 85 Ma and apatite fission track ages from 22 to 54 Ma (Fügenschuh 1995; Fügenschuh et al. 2000).
Sample location and description
Clay-rich samples from the Silltal Fault were collected from in and around the Stephansbrücke clay pit (location A on Fig. 1) and from two other locations around 8 km to the SSE, north of Matrei (locations B and C on Fig. 1). In total six gouge samples were investigated: four samples from Stephansbrücke (SB1, SB2, SB3, SB4) and one sample each from locations B (BF1) and C (BF2) near Matrei.
Clay from the quarry of Stephansbrücke was worked in former times as a raw material for ceramics, bricks and roofing tiles and was of excellent quality and plasticity due to the high clay mineral content (up to 80 % according to Czurda and Bertha 1984). Blaas (1885, p. 101) was the first to describe the blue-grey clay geologically, recognizing the sharp contact to the sand and gravel of the overlying glacial terrace sediments and the more gradational contact to the underlying solid rock of the Innsbruck Quartz Phyllite. He interpreted this transition, with common clasts of vein-quartz from the underlying Quartz Phyllite (Fig. 3; cf. Figure 3C in Reiter et al. 2005), as a clear example of a ground moraine reworking components from below. The blue-grey foliated clay is >15 m thick (Paschinger 1953), with common vein-quartz clasts covering a wide range of sizes up to several centimetres (Fig. 3). Below it is more-or-less contiguous with the Innsbruck Quartz Phyllite and above it is overlain by ca. 200 m of Quaternary Inntal terrace sediments, with a sharp contact to the clay (Paschinger 1953). The nearest outcrops of metamorphic rocks above the clay quarry are mica schists of the Ötztal Crystalline Complex (Decker et al. 2009). Although the common vein-quartz clasts already convinced Blaas (1885) and von Klebelsberg (1935) that the clay derived directly from the Innsbruck Quartz Phyllite below, it was Paschinger (1953) and Schmidegg (1953) who were the first to propose that the clay developed as the result of movement on a major fault zone. At the time, the grain size reduction was assigned to “mylonitization”, whereas now we would refer to the process they envisaged as cataclasis. Paschinger (1953) considered the movements to reflect (west-directed) overthrusting of the Ötztal nappe onto the Innsbruck Quartz Phyllite, in a similar manner to what has been more recently proposed by Rockenschaub et al. (2003) and Piber et al. (2008) for the klippe of Patscherkofel Crystalline Complex overlying the Innsbruck Quartz Phyllite east of Stephansbrücke (Fig. 1). Von Klebelsberg (1935), Schmidegg (1953), and Horninger and Weiss (1980) all proposed that clay formation could be totally or partly due to alteration of earlier “mylonite” by meteoric water derived from the overlying glacial terrace sediments.
From the Stephansbrücke locality, samples SB1 and SB2 were collected within ca. 1 m of each other on the western rim of the old clay pit (now filled as a waste disposal site), sample SB3 was collected from a trench dug a few metres to the west (Fig. 3) and sample SB4 was taken from a steep wall ca. 20 m further southwest. This outcrop shows a well-developed foliation and S–C–C′ (Berthé et al. 1979) or “shear band” structure, indicating normal (top-down-to-W) sense of movement (Fig. 3a, b in Reiter et al. 2005).
For the Matrei samples further SSE, BF1 was collected a few metres below the surface in a small tunnel on the west side of the main Brenner freeway (Location B, Fig. 1). Here, the fault gouge is derived from reworked Ötztal Crystalline Complex in the immediate hanging wall of the Silltal Fault. BF2 (Location C, Fig. 1) came from a drainage tunnel below the Brenner freeway, some 30 m below the surface, and is situated in the footwall within the Reckner nappe (Fig. 1).
Different clay-size fault gouge fractions ranging from <0.1 to 6–10 µm were analysed for their hydrogen isotope ratios (δD), in particular to assess the possible influence of meteoric water during formation of the clay-size fractions. The δD of undeformed and recrystallized phyllosilicates sampled through the entire crustal section affected by Brenner Fault Zone deformation were also investigated, with the aim of constraining the pathway of fluid infiltration both along and across the detachment system. Rock samples containing white mica, biotite and chlorite were collected from both the brittle hanging wall and the mylonitic footwall of the Brenner Fault Zone at three different localities near Steinach, Gries and close to the Brenner Pass (Fig. 1). Samples were taken from immediately adjacent to the Brenner Fault Zone detachment and from up to ca. 660 m into the hanging wall and up to ca. 1 km into the footwall. All the hanging wall outcrops considered in this study have been affected by intense brittle deformation and the chosen samples were essentially rich in chlorite. Rock samples collected within the footwall were strongly ductilely deformed with a sense-of-shear (top-down-to-W) consistent with Brenner Fault Zone movement, as was especially clear for the mica-schists and calc-schists. The phyllosilicate grains separated for hydrogen isotope analysis are generally recrystallized.
The procedures applied in this study are based on Zwingmann and Mancktelow (2004) and Zwingmann et al. (2010a). Approximately 200 g of fresh gouge and cataclastically ground rock material was collected from each sample site. Samples were gently disaggregated using a repetitive freezing and heating technique to avoid artificial reduction of rock components with K-bearing minerals, such as micas or K-feldspars (Liewig et al. 1987). Grain size fractions <2, 2–6 and 6–10 μm were separated in distilled water according to Stoke’s law and <0.4 and <0.1 μm were separated using a high-speed centrifuge. For “whole-rock gouge” (WR) analysis a small amount of sample material was crushed in an agate mortar by hand. Samples were characterized by X-ray diffraction (XRD) (normal and glycolated runs), environmental scanning electron microscopy (ESEM) on original wet gouge material, and transmission electron microscopy (TEM).
The mineralogy of the size fractions was determined by XRD on air-dried and glycolated samples following the approach outlined in Moore and Reynolds (1997). For clay polytype investigations the samples were lightly pressed into shallow stainless steel holders for XRD analysis. Oriented samples were prepared by dispersing approximately 40 mg of material using ultrasonic agitation in approximately 5 ml of deionised water. The slurries were deposited under suction onto 0.22 μm Duropore© filter membranes and then saturated with magnesium twice using 1 M MgCl2. The films were washed five times with deionised water and then five drops of glycerol added and gently spread over the entire clay surface. The samples remained on the vacuum manifold until all traces of liquid glycerol were gone. The oriented samples were placed onto absorbent paper towels to remove excess glycerol on the backs of the samples before mounting onto 25 mm aluminium discs with double sided tape. XRD patterns were recorded with a PANalytical X’Pert Pro microprocessor-controlled diffractometer using Fe filtered Co Kα radiation, 0.25° divergence slit, 0.50° anti-scatter slit and X’Celerator fast Si strip detector. The diffraction patterns were recorded in steps of 0.016° 2θ with a 1 s counting time per step, and logged to data files on a PC for analysis using HighScore Plus and CSIRO XPLOT software.
Freshly broken surfaces of moist gouge sample chips were examined by ESEM using a Zeiss EVO equipped with an energy dispersive system X-ray analyzer (EDS). Transmission electron microscopy (TEM) was used to identify and distinguish possible authigenic clays from finely ground protolith micas, feldspars and other contaminants, allowing the detection of traces of contaminant phases below the XRD detection limit. To this end, a JEOL 2010 TEM (200 kV) was used for detailed, grain-by-grain morphological characterization of selected <0.1 μm clay fractions. Samples were prepared by placing one drop of clay solution on a microcarbon grid film and drying under air. The chemical composition of individual particles was investigated by an attached EDS system.
The K–Ar dating technique follows standard methods described in detail by Dalrymple and Lanphere (1969). K content was determined by atomic absorption. The pooled error of duplicate K determinations on several samples and standards is better than 2.0 %. Ar isotopic determinations were performed using a procedure similar to that described by Bonhomme et al. (1975). Samples were pre-heated under vacuum at 80 °C for several hours to reduce the amount of atmospheric Ar adsorbed onto the mineral surfaces during sample preparation. Ar was extracted from the mineral fractions by fusing samples using a low blank resistance furnace within a vacuum line serviced by an on-line 38Ar spike pipette. The 38Ar spike was calibrated against GA1550 biotite (McDougall and Roksandic 1974). The isotopic composition of the spiked Ar was measured with an on-line VG3600 mass spectrometer via Faraday cup. The released gases were subjected to a two-stage purification procedure via CuO and Ti getters. Blanks for the extraction line and mass spectrometer were systematically determined and the mass discrimination factor was determined by airshots. About 25 mg of sample material was required for Ar analyses. Due to the hygroscopic nature of clays, special care was taken in the preparation of both K and Ar sample splits. For Ar analysis by noble gas spectrometry, sample splits were loaded into clean Mo-foil (Goodfellow molybdenum foil, thickness 0.0125 mm, purity 99.9 %), weighed and subsequently preheated to 80 °C overnight to remove moisture, and re-weighted using a Mettler AT20 balance. The measured dry weight was used in the K–Ar age calculation. Samples were stored prior to loading into the Ar purification line in a desiccator. During the course of the study, 10 international standards comprising 6 HD-B1 (Hess and Lippolt 1994) and 4 GLO (Odin et al. 1982) were measured. Standard and airshot data are listed in the table of Online Resource 1. The error for Ar analyses is below 1 % (Online Resource 1) and the 40Ar/36Ar value for airshots averaged 295.02 ± 0.28 (n = 10). K–Ar ages were calculated using 40K abundance and decay constants recommended by Steiger and Jäger (1977).
Stable isotope geochemistry
Micas (muscovite and biotite) and chlorite with a grain size of 600–250 µm were selected for isotopic analysis by crushing, grinding, and hand picking of individual mineral grains. For the phyllosilicate samples from the country rocks, a sample weight of 1 mg for chlorite and 2 mg for micas was wrapped into silver foil and placed into a He-purged autosampler. For the fine-grained clay separates, a sample weight of 1 mg was wrapped into silver foil and dried overnight at 150 °C in a stainless steel tray. Samples were rapidly transferred to a zero-blank autosampler in the stainless steel tray and the autosampler was immediately purged with Helium gas to avoid re-hydration with ambient air moisture. δD values were measured at Leibniz Universität Hannover using a Thermo Electron delta V advantage mass spectrometer in continuous flow mode coupled to a high temperature conversion elemental analyser (TC-EA). Clay samples BF1 and BF2 were analysed following the same procedure at Goethe University Frankfurt on a ThermoFinnigan MAT 253 mass spectrometer. In-house and three international standards were run with the samples and yielded δD = −65.5 ‰ (n = 21; NBS30 biotite), δD = −119.4 ‰ (n = 21; NBS22 oil), and δD = −102.7 ‰ (n = 21; CH7 polyethylene foil). Standards were run in-line with unknowns and reproduced with an error below ±2 ‰. All δD values are reported relative to standard mean ocean water (VSMOW).
Mineralogy and chemical composition of the dated fault gouge samples
The modal mineral compositions determined by X-ray Diffraction (XRD) of the clay size fractions dated in this study are listed in Table 1. The striking observation is that there is no detectable 1M (including 1Md) polytype illite or mixed-layer illite/smectite (I/S) in any of the fault gouge samples: only 2M1 illite/muscovite and chlorite are observed in all the samples, with smectite also present in samples from the Stephansbrücke area. This is unusual because a progression from smectite to random I/S to ordered I/S to illite is typically observed with increasing depth of burial and temperature, corresponding to the transition from diagenesis to anchimetamorphism to epizone (greenschist) metamorphism (e.g. Kisch 1983; Hunziker et al. 1986; Merriman and Frey 1999; Wilson 2013). Correspondingly, on a prograde path illite should evolve through an overlapping sequence of polytypes with increasing temperature, from 1Md to 1M to 2M1 (Yoder and Eugster 1955; Yoder 1957; Reynolds 1963; Velde 1965; Maxwell and Hower 1967; Merriman and Roberts 1985; Hunziker et al. 1986; Dalla Torre and Frey 1997; Wilson 2013). The gradational prograde transformation to 2M1 begins in the lowermost anchizone and is effectively completed by the transition to the epizone (Hunziker et al. 1986; cf. their Fig. 5), corresponding to a temperature range of ca. 200–300 °C (Merriman and Frey 1999). On the retrograde path, neocrystallization and recrystallization of clay due to cataclasis and fluid-rock interaction in an active brittle fault exhumed to the surface should produce the reverse sequence, although the reaction kinetics may be sluggish (Yoder and Eugster 1955; Yoder 1957). Most clay fault gouges are therefore a mixture of comminuted protolith (“detrital”) clay/mica/chlorite and different authigenic clay-sized minerals and polytypes (Vrolijk and van der Pluijm 1999; Ylagan et al. 2002; Zwingmann et al. 2010a; Surace et al. 2011; Bense et al. 2014). However, this is not what is observed in Silltal Fault gouges. In all samples, higher temperature 2M1 illite/muscovite is the dominant clay mineral present and in the southern Matrei samples BF1 and BF2, it is the only clay mineral that occurs.
Muscovite and 2M1 illite are not distinguishable by XRD and the transition is anyway gradational. Both are dioctahedral micas but differ in their chemistry, with illite having lower K and correspondingly less Al and more Si. In the “standard nomenclature” for micas, illite has the simplified (i.e. not considering possible Fe2+ or Mg2+ substitution, or vacancies) general formula K x Al2(Al x Si4–x O10(OH)2, with 0.6 < x < 0.85, whereas muscovite has x > 0.85 and an idealized end-member composition when x = 1 (Bailey 1984; Rieder et al. 1999). However, this “standard nomenclature” is not universally accepted, and the range assigned to illite has been extended by some authors to cover a significantly larger range of 0.31 < x < 0.89 (Yates and Rosenberg 1998), with the apparent end-member of the illite series regarded as having x = 0.88 ± 0.01 interlayer cations per half cell (Yates and Rosenberg 1997, 1998; Ylagan et al. 2000; Rosenberg 2002).
It follows that the most characteristic chemical difference between 2M1 illite and 2M1 muscovite is that illite is deficient in K compared to muscovite. Since 2M1 polytype illite/muscovite is effectively the only K-bearing mineral in the separated and dated clay fractions, it is possible to estimate the K content of this illite/muscovite component by plotting the amount of the polytype present in the samples (as determined by XRD analysis; Table 1) against the measured bulk % K in the same samples (as determined by K–Ar dating; Table 2). This should give a mixing line, with the mineral composition corresponding to 100 % 2M1. The result is shown in Fig. 4, with K content presented as wt% K2O. For comparison, the plot also shows the range of wt% K2O measured by electron microprobe on samples of metamorphic footwall muscovites from the Innsbruck Quartz Phyllite (Piber and Tropper 2007) and from the Patscherkofel Crystalline Complex (Piber et al. 2008), which show the same range in composition. In addition, a single representative analysis for illite from the online resource www.webmineral.com is shown. Figure 4 indicates that the composition of 2M1 polytype in most samples from the Stephansbrücke locality is identical to that of the muscovite from the metamorphic rocks in the footwall. Only the two samples richest in 2M1 component (SB3 <2 μm and SB4 <0.1 μm) are deficient in K and plot within the illite field. In contrast, the samples from the southern Matrei localities are all K-deficient, with compositions typical of illite and distinctly different from the protolith muscovite compositions of the footwall Innsbruck Quartz Phyllite.
SEM and TEM observations on clay morphology
Under the ESEM, original wet “whole rock” samples show large, 10–20 μm sized, irregular grains surrounded by a finer grained matrix, both of which appear to have developed by mechanical comminution (Fig. 5a), rather than the well-crystallized fibrous, lath-shaped or platelet forms more typical of authigenic clay minerals (Inoue et al. 1988; Clauer and Chaudhuri 1995; Pevear 1999). However, TEM investigations of selected <0.1 µm clay fractions show that the finest separated clay mineral particles have a relatively equant platelet form, generally with rather irregular diffuse boundaries but also with some straight, idiomorphic, euhedral edges (arrowed in Fig. 5b). The particles investigated by both SEM and TEM contain Al, Si, O, K and Fe as determined by EDS, so that these characteristic forms must correspond to the 2M1 illite/muscovite component identified by XRD.
Previous experimental and field studies show that there is a gradual change from more fibrous and lath-shaped forms to hexagonal-shaped platelets with evolution to the higher temperature 2M1 polytype (Inoue et al. 1988; Clauer and Chaudhuri 1995; Bauer et al. 2000; Clauer et al. 2014). Schleicher et al. (2006) also observed that, in a hydrothermally altered granite, authigenic 2M1 illite in vein fillings had a platy pseudohexagonal form, whereas 1M illite filling pores was fibrous. The morphology of the finest clay particles (Fig. 5b) is therefore typical of the higher temperature 2M1 polytype, confirming the quantitative XRD determinations showing that this is the only illite polytype present. The preserved idiomorphic forms and the K-deficient chemistry of this sample size fraction (BF2 <0.1 µm; see Fig. 4) is direct evidence for neocrystallization of fine 2M1 illite. The diffuse, irregular edges of many grains are more characteristic of protolith or “detrital” grains (e.g. Clauer and Chaudhuri 1995), but authigenic illite grains affected by ongoing fault movement would also be deformed and their edges may become irregular. The SEM and TEM observations therefore confirm the clay mineralogy and indicate that at least some of the finest clay fraction in the fault gouge is authigenic 2M1 illite. However, an additional component of comminuted protolith (“detrital”) muscovite (perhaps corresponding to the grains with irregular diffuse boundaries) cannot be unequivocally excluded on the basis of the TEM observations alone.
In total 32 K–Ar analyses comprising 5 whole rock splits and 27 clay fractions from <0.1 to 6–10 μm were obtained in this study (Table 2). The whole rock ages range from 45.0 to 99.2 Ma, whereas the clay fraction ages range from 12.3 to 114.9 Ma. For the clay-size fractions, there is a consistent decrease in age with decreasing grain size (Fig. 6). Ages for the Stephansbrücke samples range from 114.9 Ma (SB3, 6–10 µm) to 35.9 Ma (SB4, <0.1 µm) whereas for the Matrei samples further south the range extends down to significantly younger ages. The oldest ages for the Matrei samples are 54–55 Ma for the “whole rock sample” (WR) and 6–10 µm fraction of BF2 and the youngest age is 12.3 Ma for the <0.1 µm fraction of BF1. It follows that the oldest ages of the Matrei samples (BF1-2) overlap with the youngest ages of the Stephansbrücke samples (SB1-4) but reach down to much younger (Neogene) ages for the finest fractions.
The overstepping age ranges for the different sample sites are also seen in Fig. 7, where the measured K–Ar ages for the size fractions less than 6 µm are plotted against the interpreted wt% K2O of the dated 2M1 polytype. However, Fig. 7 also shows that (1) there is a general trend (although with significant scatter) to younger ages with decreasing K content of the dated 2M1 polytype; (2) the samples with the oldest ages from the Stephansbrücke locality overlap in both composition and age with results from the Patscherkofel Crystalline Complex, which, from its location as a klippe on the Innsbruck Quartz Phyllite and from its shallow dip to the SW, could be interpreted to intersect the Silltal-Brenner Fault Zone at the general level of the Stephansbrücke samples; and (3) the oldest K–Ar ages from Stephansbrücke locality are much younger than the pre-Alpine ages obtained from muscovite 40Ar/39Ar in the Innsbruck Quartz Phyllite from the underlying footwall.
Hydrogen isotope geochemistry
White mica (ms), biotite (bt) and chlorite (chl) separates across the Brenner Fault Zone from within both the footwall and hanging wall yield δD values averaging −59 ‰ (ms), −68 ‰ (bt) and −64 ‰ (chl), respectively (Table 3). In contrast, all clay gouge fractions have consistently lower δD values that range between −77 and −108 ‰ (Table 4). Similarly to the K–Ar results, there is a clear correlation between δD values and grain size of the analysed fractions for both the Stephansbrücke and the Matrei samples (Fig. 8), with δD values decreasing with grain size. It follows that there is also a direct correlation between K–Ar age and δD values (Fig. 9). It is particularly striking that all four Stephansbrücke samples, collected within a few tens of metres of each other from the same contiguous clay gouge location, plot on a very well-defined linear trend (Fig. 9a, R 2 = 0.995). The youngest Stephansbrücke sample (SB4 <0.1 μm; Table 2) was not analysed for δD, but extrapolation of the correlation line in Fig. 9a to its K–Ar age of 35.9 Ma would return a value of around −111 ‰. The Matrei samples BF1 and BF2 plot on similar, but uniquely different, linear trends (Fig. 9b; BF1: R 2 = 0.969, BF2: R 2 = 0.935). The δD value for the youngest age from sample BF1 (12.3 Ma for BF1 <0.1 μm; Table 2) is −106 ‰ and extrapolation of the line for BF2 to the same age would give a value of about −109 ‰. The finest grained fractions (<0.1 μm) in all the samples from Stephansbrücke and near Matrei give both the youngest K–Ar ages and the lowest δD values, in a quite limited range from ca. −106 to −110 ‰ (within error of ca. ±2 ‰).
The broad correlation of K–Ar age with calculated wt% K2O for the 2M1 polytype illite/muscovite component (Fig. 7) together with the strong correlation of δD with age (Fig. 9) implies that there should also be a decrease in δD values with decreasing wt% K2O. However, as seen from the plot of Fig. 10, this correlation is weak, especially within the different size fractions from the northern and southern localities. In effect, Fig. 10 only highlights the distinction between the higher values of wt% K2O in the 2M1 component for samples from the Stephansbrücke locality compared to the southerly Matrei samples, as already seen in Fig. 4, together with the tendency for the smallest size fractions in these southerly samples to return the most negative values of δD.
The major clay component in the fault gouge samples, as determined by quantitative XRD analysis, is 2M1 illite/muscovite, but there are variable amounts of smectite in the Stephansbrücke (SB) samples and secondary chlorite in all samples (Table 1). Chlorite is not a K-bearing mineral (e.g. see typical chemical analyses in Deer et al. 1992) and smectite in the Stephansbrücke samples is without discernible mixed-layers of illite and should also be effectively K-free. The K–Ar dates presented in Table 2 therefore only derive from the K-bearing 2M1 illite/muscovite component. However, there remains a correlation in the SB samples between the measured K–Ar ages and both the modal % smectite (Fig. 11a) and % chlorite (Fig. 11b). Inspecting Table 1 reveals the reason for this observation: the modal % of these minerals is an effective proxy for the grain size of the dated fraction, with chlorite decreasing in abundance and smectite increasing in abundance as the grain size decreases, and in turn the K–Ar age decreases with the grain size of different fractions separated from each sample (Table 2; Fig. 6). The indirect nature of this correlation is emphasized by the one clear outlier in Fig. 11a. There is apparently a lower limit to the grain size distribution of the smectite, because this finest-grained sample (SB4 <0.1 μm) does not continue the trend of increasing smectite component: it has only 9 % smectite, but returns the youngest age (35.9 Ma). The real correlation is therefore with grain size, as shown in Fig. 6, and not directly with modal % smectite or chlorite.
Relatively pure smectite without mixed illite/smectite layers only develops at low temperatures, well below ~80 °C (Pytte and Reynolds 1989; Huang et al. 1993) and, under these near-surface conditions, probably crystallized due to interaction of existing cataclastic fault gouge with meteoric water. It may even have developed at or very near the surface during glaciation and deposition of the overlying glacial moraine sediments, as was previously proposed for the development of clay in the Stephansbrücke location by von Klebelsberg (1935), Schmidegg (1953), and Horninger and Weiss (1980). If smectite formed near surface by interaction with meteoric water, the δD values of the smectite component should reflect this origin: increasing amounts of smectite in the SB samples should be reflected in increasingly negative δD values for the bulk grain-size fraction. There is indeed a broad trend, as shown in Fig. 11c, but it is much weaker than the correlation between age and δD (Fig. 9a). This strong correlation between age and δD is also seen in the southern Matrei samples (BF1 and BF2, Fig. 9b), where there is no smectite present. Again it appears that the observed trend in Fig. 11c actually reflects the grain size (for which the amount of smectite is a proxy), which in turn is reflected in the age and δD, rather than a direct influence of the amount and isotopic composition of the smectite itself.
TEM images of the finest (<0.1 μm) clay fractions show that the dated K-bearing illite/muscovite grains have a pseudohexagonal platelet form (Fig. 5b) typical of the 2M1 polytype (Inoue et al. 1988; Schleicher et al. 2006), confirming the quantitative XRD results that 2M1 is the only polytype present. The idiomorphic morphology of some of these very fine grains (Fig. 5b), together with their K-deficient chemistry relative to muscovite (Fig. 4), is direct evidence for authigenic growth of 2M1 illite, at least in the southerly Matrei samples (BF1, BF2), which generally give the younger K–Ar ages. The lack of any mixed layer illite/smectite or lower temperature 1M/1Md polytype illite is rather atypical of clay fault gouges: most other reported examples show a variable mixture of clay minerals and polymorphs, reflecting the range of initial and retrograde conditions during faulting and exhumation (Kralik et al. 1987; Zwingmann and Mancktelow 2004; Zwingmann et al. 2010a, b; Surace et al. 2011; Pleuger et al. 2012; Bense et al. 2014). Considering only the dateable K-bearing illite in such mixtures, many authors have argued that the 1M/1Md polytype represents the authigenic component grown during faulting, whereas the 2M1 part represents relict protolith or “detrital” grains. Based on this principle, extrapolation of a plot of vol% 2M1/(2M1 + 1 M + 1Md) versus apparent K–Ar age, Ar–Ar age, or eλt − 1 (where λ is the decay constant and t is time) can provide both the protolith (100 %) and authigenic (0 %) ages (Pevear 1999; Van der Pluijm et al. 2001, 2006; Ylagan et al. 2002; Haines and van der Pluijm 2010; Solum et al. 2010; Duvall et al. 2011; Hnat and van der Pluijm 2014).
However, it has also been clearly demonstrated in a range of natural examples that authigenic 2M1 illite can form in fault gouges derived from metamorphic or magmatic protoliths that were initially devoid of such illite (Zwingmann and Mancktelow 2004; Zwingmann et al. 2010a; Viola et al. 2013; Bense et al. 2014; Song et al. 2014; Torgersen and Viola 2014; Torgersen et al. 2014a). In particular, Viola et al. (2013) have recently described a clay fault gouge in the Palaeoproterozoic basement of Finland that contained almost exclusively 2M1 illite/muscovite as authigenic clay, developed from a protolith gneiss that contained no illite and <4 % protolith muscovite. In all these reported cases, authigenic 2M1 illite must have grown under higher temperature hydrothermal conditions, presumably during the initial stages of fault zone development at depths close to the ductile–brittle transition. For quartz-rich rocks, this occurs around 280–300 °C (Sibson et al. 1979; White and White 1983; Mancktelow 1985; Stipp et al. 2002). Velde (1965) established experimentally that 2M1 muscovite is stable down to 125 °C. As shown by Yoder and Eugster (1955) and Yoder (1957), the retrograde polymorphic transformation of 2M1 to 1M is also very sluggish (and not attainable experimentally). In natural examples of regional metamorphism in pelitic rocks, the gradational prograde transformation of 1M/1Md illite to 2M1 illite/muscovite begins in the lowermost anchizone and is effectively completed by the transition to the epizone (e.g. Hunziker et al. 1986; cf. their Fig. 5), corresponding to a temperature range of ca. 200–300 °C (Merriman and Frey 1999). Initiation of brittle faulting and gouge development in the upper continental crust can therefore occur within the stability field of 2M1 illite, which may be authigenic and not invariably represent an inherited “detrital” or protolith component.
The δD values of phyllosilicates (muscovite, biotite and chlorite) collected within the footwall and hanging wall of the Brenner Fault Zone are typical of a rock-buffered metamorphic system and do not indicate any interaction with meteoric fluids away from the fault zone (Table 3). However, compared to δD values of around −60 ‰ for 2M1 white micas from the footwall and hanging wall, δD values from the fault gouges are much more negative (Fig. 8c). They are especially negative (down to <−108 ‰) within samples BF1 and BF2 from the southern Matrei region, which are only composed of 2M1 illite/muscovite. Low δD in white micas (δD <−80 ‰) can only be explained by hydrogen isotope exchange with a meteoric fluid with low δD values (e.g. Mulch et al. 2004; Gébelin et al. 2015) and an important influence of meteoric water in samples BF1 and BF2 is thus clearly established. For both gouge samples, a well-defined linear relationship between δD values and K–Ar (apparent) ages is observed (Fig. 9b). This correlation between (apparent) age and isotopic composition indirectly reflects the influence of grain size on both isotopic composition and K–Ar age, with the finest fractions yielding the youngest K–Ar ages (Fig. 6) and the lowest δD values, which in turn implies the strongest (meteoric) fluid-rock interaction (Fig. 8). A similar relationship between K–Ar age of illite, grain size and δ18O was reported by Cathelineau et al. (2004) in fractured and altered plutonites from the French Massif Central, although in their case the value of δ18O increased with decreasing grain size and K–Ar age.
The Stephansbrücke samples from further north are dominantly composed of the same 2M1 polytype. However, they also contain smectite that must have formed near-surface at low temperatures (<80 °C) and is therefore likely to record strong isotopic exchange with surface-derived fluids, which should lower the measured δD values. Despite this, the δD values for comparable size fractions are generally higher in the Stephansbrücke samples than in the southern Matrei samples (Fig. 8). As seen from Fig. 9a, a clear linear relationship between δD values and K–Ar (apparent) ages of the 2M1 illite/muscovite component is still observed and in fact the correlation is even stronger than that for samples BF1 and BF2 (Fig. 9b). It follows that the presence of smectite seems to have had only a minor impact on the overall δD values. As discussed already in Sect. 5.4 above, all samples trend towards a value of around −108 ‰ for the finest grained fractions returning the youngest apparent K–Ar ages (Fig. 9).
In summary, the hydrogen isotope results in this study clearly document that meteoric water has infiltrated the Silltal fault gouge during brittle faulting, but that this infiltration was localised at the contact between hanging wall and footwall and did not reach deeper structural levels of the detachment system. The brittle fault gouge that marks the contact between hanging wall and footwall therefore appears to be the main pathway for fluid infiltration. This fluid infiltration pattern is in contrast to that from the other directly comparable major Alpine low-angle detachment in the Central Alps, the Simplon Fault Zone (SFZ), where surface-derived fluid infiltrated the detachment via a wide zone of brittle deformation and reached the depth of the ductile-to-brittle transition (Campani et al. 2012).
In interpreting the observations from the Silltal Fault on the clay mineralogy, chemistry, morphology, H-isotopes, and apparent K–Ar ages, as well as their dependence on grain size, two end-member models need to be critically assessed. (1) The 2M1 polytype found in all samples is metamorphic muscovite derived from the Innsbruck Quartz Phyllite and the only authigenic clay is the low-grade smectite developed in samples from the Stephansbrücke locality. The 2M1 grains in all size fractions are original protolith muscovite whose grain size has been mechanically reduced by cataclasis and grinding in the fault zone. The dependence of apparent age on grain size reflects grain-size dependent loss of radiogenic argon during deformation and comminution in a hydrothermal environment (Dodson 1973; Villa 1998). (2) The 2M1 polytype in the finest fractions is higher temperature illite that has neocrystallized due to fluid-rock interaction in the cataclastic fault zone. The dependence of apparent age on grain size reflects either a variable mixture with coarser grained protolith 2M1 muscovite or with earlier formed, coarser authigenic illite (e.g. Clauer et al. 2012), or both.
At least for the northern samples from near Stephansbrücke, the implied composition of most clay-sized fractions is identical to the composition of muscovite from the adjacent footwall Innsbruck Quartz Phyllite and Patscherkofel Crystalline Complex (Figs. 4, 7). The K–Ar ages also overlap with those from the Patscherkofel Crystalline Complex (Fig. 7). However, the two Stephansbrücke samples richest in 2M1 component (SB3 <2 μm and SB4 <0.1 μm) are deficient in K and lie within the illite field. These two samples contain respectively 75 and 88 % 2M1 illite/muscovite, whereas the usual Innsbruck Quartz Phyllite typically contains 25–30 % muscovite (see photomicrograph in Fig. 4b of Madritsch and Millen 2007). If the 2M1 component in the clay gouge samples is entirely metamorphic muscovite, it must have been concentrated by a factor two or more relative to the protolith Innsbruck Quartz Phyllite, presumably by dissolution of original quartz and plagioclase. Quartz dissolution is reported from fault gouge zones, but only to a more limited extent (e.g. Chester and Logan 1986). It should also be noted that although the 2M1 component generally increases with decreasing grain size, the opposite is the case for chlorite (Table 1), which is the other phyllosilicate originally present in the Innsbruck Quartz Phyllite. Bense et al. (2014) argued that diminution of coarse protolith muscovite to micron or sub-micron grain sizes is unlikely, because of the very strong mechanical resistance of this mineral. However, direct experiments on synthetic muscovite fault gouges contradict this supposition, with lower temperature runs (300 °C) under hydrothermal conditions developing fine grained shear bands with matrix grain sizes <2 μm (Van Diggelen et al. 2010).
As noted above, the two samples richest in 2M1 component from the Stephansbrücke, as well as all the samples from the southern Matrei area, are deficient in K and fall within the compositional range of illite (Fig. 4). However, muscovite can also be leached and lose K by interaction with low-K-activity, slightly acid water (Scott and Reed 1966; Scott and Smith 1966; Feigenbaum et al. 1981; Song and Huang 1988; Derkowski et al. 2014), which could be possible for meteoric water fluxing a fault zone developed in schist and gneiss. Such leaching would change the chemical composition of cataclastically comminuted muscovite grains towards more K-deficient illite without neocrystallization. In particular, Feigenbaum et al. (1981) found that the relative rate of K release from muscovite (and biotite and phlogopite) is much higher than the rate of K release from illite (Feigenbaum and Shainberg 1975) in 0.001 N HCl solutions, despite the fact that in their experiments the illite particles were clay size (<2 μm) and the mica particles were 5–20 μm. Scott and Smith (1966) note, however, that very low values of dissolved K are required for K release by muscovite (and illite), although more than 90 % of the K in muscovite (and biotite and phlogopite) is in fact exchangeable with Na (and other cations, e.g. Graf von Reichenbach and Rich 1969). In summary, numerous studies considering weathering (Scott and Reed 1966; Scott and Smith 1966; Graf von Reichenbach and Rich 1969) and hydrothermal alteration (Meyer and Hemley 1957; Hemley 1959) have demonstrated that K leaching from muscovite is possible in fluids of appropriate composition. However, preferentially leaching K and largely retaining the radiogenic argon, as considered by Derkowski et al. (2014), would lead to older apparent ages with increasing fluid-rock interaction in the finest grains, which is the opposite of what is observed. The experiments of Clauer et al. (1993) and Clauer and Mongodin (2012) show that acidic leaching does not induce a preferential release of radiogenic isotopes or a significant effect on the concentration of Al and K (and Mg) in illite/muscovite. They therefore argue that such leaching should not substantially modify K–Ar and 40Ar/39Ar ages.
Argon loss due to diffusion is a function of grain size and temperature (Dodson 1973) and can be strongly affected by intracrystalline deformation and fluid interaction (Villa 1998; Mulch et al. 2002). For fine-grained white mica <2 μm, Hunziker et al. (1986) reported a closure temperature interval (corresponding to the end of significant diffusion of Ar) of 260 ± 30 °C, whereas Wemmer and Ahrendt (1997) considered it to lie somewhere between 275 and 350 °C. The stability field of 2M1 illite and the temperature of its transition to muscovite, as well as the brittle-ductile transition in quartz-rich rocks, overlaps with this proposed closure temperature range. Zircon fission track ages from both the footwall and the hanging wall of the Silltal Fault north of Matrei are rather similar and indicate that this region had already cooled below ~300 °C in the early Palaeocene (Fügenschuh et al. 1997), which is markedly older than the youngest K–Ar ages obtained in the finest fractions from both the Stephansbrücke and (especially) the Matrei area. Nevertheless, it cannot be excluded that the observed decrease in apparent K–Ar age with grain size in the analysed fault gouges may reflect partial loss of Ar from protolith muscovite grains during deformation, comminution and interaction with water in the fault zone. Ar loss would be promoted by damage to the crystal lattice, caused by grain size reduction, as well as by the decreased diffusion distance in such defect-rich grains. Ar loss would also be aided by interaction with water in the fault zone, due to infiltration of water along cracks, cleavage planes and dislocation cores. Geothermal waters of higher temperature in the fault zone could also have promoted Ar loss.
However, the temperature range above 260–280 °C for which Ar loss in fine grained muscovite may start to be significant is also well within the temperature range of 125–350 °C for which 2M1 illite is known to form in epithermal conditions (e.g. Velde 1965; Schleicher et al. 2006). The observed idiomorphic grain boundaries in the finest analysed fractions with typical 2M1 pseudohexagonal platelet forms (Fig. 5b) is direct evidence for authigenic 2M1 illite growth, as is the K-deficient illite chemical composition of all the southern Matrei samples (which return the youngest ages). The trend of decreasing Tertiary ages in apatite fission track ages from north to south in the hanging wall of the Silltal Fault (Fig. 2) (Fügenschuh et al. 2000) indicates increasing depth of post-Tertiary exhumation to the south and therefore that temperatures during fault gouge formation in the southern samples from the Silltal Fault were higher. This would promote new higher temperature 2M1 illite growth, as seen directly in the TEM images, as well as potentially accelerate argon loss from finer grained protolith muscovite grains, both of which would result in younger apparent ages in the finest fractions from the southern samples.
In summary, there is direct evidence for new 2M1 illite growth in the finest fraction (<0.1 μm) of the higher temperature southern samples, and it is this fraction that has the highest vol% of the 2M1 polytype and the youngest age (12.3 ± 0.4 Ma). If there was no subsequent argon loss, the age of this finest fraction (<0.1 μm) in general corresponds to growth of the finest, and usually most recently nucleated, illite in the fault gouge (Zwingmann and Mancktelow 2004; Zwingmann et al. 2010a; Torgersen et al. 2014a). However, faults always accumulate displacement over a finite time span and, in some cases, may be intermittently active over long times (Mulch et al. 2005; Viola et al. 2013; Torgersen and Viola 2014; Torgersen et al. 2014a, b). Particularly when dates derive from the higher temperature 2M1 illite polytype, developed closer to the brittle-ductile transition, it is unlikely that K–Ar ages correspond only to the very last deformation increments on the fault (Zwingmann et al. 2010a), which may have continued to be active under retrograde conditions during exhumation to the surface. For the example of the Silltal Fault presented here, apparent K–Ar ages from the finest to the coarsest size fractions (and “whole-rock gouge” samples) range from Middle Miocene (~12 Ma) to Cretaceous (~115 Ma). The question then arises whether this range reflects extended activity on the fault or simply a mixture of authigenic young clay, reflecting the time of actual movement, and older protolith grains, which may be partly reset by Ar-loss during grain deformation and fluid rock interaction in the cataclastic fault zone. As discussed in some detail above, this cannot be unequivocally established—the youngest ages are taken to reflect active fault movement around 12 Ma, but initiation of faulting could certainly have been significantly earlier.
The K–Ar fault gouge ages from the current study are broadly consistent with regional constraints on the possible time of activity of the Silltal Fault. 40Ar/39Ar ages on white mica separates from both the hanging wall and the footwall of the Silltal Fault give mixed Permian to Cretaceous ages, in the range of 270–130 Ma (Fig. 2) (Thöni 1980, 1999; Thöni and Hoinkes 1987; Rockenschaub et al. 2003), which are generally older than the oldest ages obtained from the Silltal Fault in this study. The only exception is sample 77/97 from the mylonitic base of the Patscherkofel Crystalline Complex klippe (Fig. 2), which shows a series of steps in the 40Ar/39Ar spectrum between 120 and 50 Ma (Rockenschaub et al. 2003). As noted above, extrapolation of this contact to the west downslope suggests it should intersect the Silltal Fault in the vicinity of the Stephansbrücke samples, but outcrop conditions do not allow direct confirmation of this in the field. However, it certainly is the case that both the composition of the 2M1 illite/muscovite and the K–Ar age of the “whole-rock gouge” and coarser separates from the Stephansbrücke clay gouges overlap with the composition and 40Ar/39Ar ages on white mica from the retrograde mylonitic shear zone at the base of the Patscherkofel Crystalline Complex (e.g. Fig. 7). As noted in the Geological overview (Sect. 2), Rockenschaub et al. (2003) interpret these younger ages down to 50 Ma to reflect retrograde metamorphism and mylonitization related to top-to-west final emplacement of the Patscherkofel Crystalline Complex. This top-down-to-the-west kinematics is identical to that related to the Silltal Fault at Stephansbrücke. It follows that the oldest measured K–Ar ages in the “whole-rock gouge” and coarser grained separates from the Stephansbrücke area, spanning the range from 65 to 155 Ma, most likely represent inherited protolith muscovite grains from the Patscherkofel Crystalline Complex basal shear zone. The decreasing age spectrum with grain size could represent: (1) partial Ar loss from cataclastically comminuted protolith muscovite grains interacting with the documented influx of hydrothermal meteoric water into the fault zone—these partially reset apparent ages would have no real geological significance; (2) authigenic growth of higher temperature 2M1 illite/muscovite reflecting ongoing but possibly intermittent activity of the Patscherkofel Crystalline Complex basal shear zone, and its transition to brittle faulting and fault gouge formation on the Silltal Fault; (3) a mixture between comminuted protolith muscovite grains and authigenic new illite, whose minimum age is given by the youngest ages from the finest fractions—in this case only the youngest ages would have a geological significance.
The probable time of brittle faulting on the Brenner Fault Zone south of Matrei (Fig. 1) can be derived from the cooling history of the western Tauern window, which represents the footwall of the Brenner Fault Zone in this area. Here, the footwall cools through 300 °C at around 13–14 Ma and 200 °C at around 12 Ma (Fig. 2b of Fügenschuh et al. 1997), so that protracted brittle movements on the Brenner Fault Zone are expected to be around 13 Ma or younger. However, zircon fission track ages from both the footwall and the hanging wall of the Silltal Fault north of Matrei are rather similar and indicate that this area had already cooled below ~300 °C in the early Palaeocene (Fügenschuh et al. 1997). The transition to brittle behaviour in the region of the current Silltal Fault may therefore be older, both in the hanging wall and in the footwall, than further to the south. Unlike the Brenner Fault Zone south of Matrei, which forms the western boundary of the Tauern window, the Silltal Fault north of Matrei does not juxtapose markedly different crustal levels, any vertical component must have been modest, and brittle faulting may have initiated at higher crustal levels and at lower temperatures (at least in the footwall) compared to the Brenner Fault Zone continuation further south. The finest grained fault gouge samples from the Silltal Fault samples near Matrei give ages around 12–18 Ma, consistent with the independently estimated time of movement on the Brenner Fault Zone <20 Ma (Fügenschuh et al. 1997), with the youngest age corresponding to the interpreted transition to brittle faulting in the Tauern window footwall of Brenner Fault Zone at around 12–13 Ma.
The results presented here from the Silltal Fault in the Eastern Alps form an internally consistent data set, but one that is challenging both with regard to the common assumptions involved in fault gouge dating and in applying the results to interpreting the tectonic history of this fault. Many authors have argued that in clay fault gouges the 2M1 polytype is entirely derived from “detrital” higher temperature illite or protolith metamorphic muscovite and should preserve a pre-faulting age for faults developed under relatively cool (<~250–280 °C), near-surface brittle conditions. In this interpretation, the authigenic clay component that is newly grown during faulting should consist of lower temperature 1M/1Md polytypes and mixed layer illite/smectite. Only the age information from these polytypes would therefore reflect the time of fault activity. A plot of percentage of 2M1 polytype against apparent K–Ar or 40Ar/39Ar age for several size fractions can thus be extrapolated to pure authigenic and pure “detrital” illite end member ages, if these are the only two K-bearing components within the sample.
In samples from the Silltal Fault there is no lower temperature 1M/1Md polytype, only 2M1, but there is a strong correlation of decreasing age with decreasing grain size of the clay fraction. There is also a very well-defined linear correlation between δD values and the K–Ar ages of the 2M1 illite/muscovite component, implying a direct relationship between decreased age and increased (meteoric) fluid-rock interaction. The low δD values indicative of strong interaction with meteoric water are entirely restricted to the narrow fault gouge and are not observed in the adjacent footwall and hanging wall, where values are typical of fluids buffered against metamorphic rocks. We conclude, particularly based on the amount of 2M1 polytype present and from direct TEM observation of the grain morphology, that there has been new 2M1 illite growth in the clay gouge of the Silltal Fault, especially in the southern samples from near Matrei that return the youngest ages in the finest fractions. From the regional metamorphic gradient, the Silltal Fault near Matrei probably initiated under slightly higher temperatures, conducive to authigenic 2M1 illite growth. The youngest ages around 12 Ma are geologically meaningful and reflect the time of Neogene brittle displacement on the Silltal-Brenner Fault Zone system. The increasing age with increasing grain size in other sample size fractions may reflect either a mixture with older, coarser authigenic illite/muscovite grown during a more extended period of fault activity or a mixture with protolith (“detrital”) white mica. This protolith mica component may have suffered partial, grain-size-dependent, radiogenic Ar loss (and possibly also K loss) during cataclastic grain comminution and deformation, with this leaching enhanced by hydrothermal interaction with channelized meteoric water in the fault zone. In this case, the older apparent K–Ar ages are not geologically meaningful but only record partial reset of protolith muscovite incorporated from adjacent muscovite-bearing phyllites during faulting.
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A. Todd and M. Raven, CSIRO, are thanked for technical assistance. The study was part of the collaborative Topo-Alps project within the framework of the European Science Foundation (ESF) Eurocores Programme TOPO-EUROPE, and was funded by the Swiss National Science Foundation (SNF projects 200021-134469 and 200021-120502). AM also acknowledges support through DFG Mu2845/2-1 in the framework of the ESF TOPO-EUROPE Program and the LOEWE program of Hesse’s Ministry of Higher Education, Research, and the Arts. We also thank J. Fiebig (Goethe University Frankfurt) at the Joint Goethe University—BiK-F Stable Isotope Facility. HZ acknowledges the use of equipment of the Curtin University Electron Microscope Facility, which is partially funded by the University, State and Commonwealth Governments. Constructive reviews by E. Torgersen and an anonymous reviewer helped to improve the manuscript and are gratefully acknowledged.
Editorial handling: E. Gnos.
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Mancktelow, N., Zwingmann, H., Campani, M. et al. Timing and conditions of brittle faulting on the Silltal-Brenner Fault Zone, Eastern Alps (Austria). Swiss J Geosci 108, 305–326 (2015). https://doi.org/10.1007/s00015-015-0179-y
- Clay fault gouge
- K–Ar dating
- Silltal-Brenner Fault Zone
- Eastern Alps