Abstract
Low-temperature thermochronology can be applied to a wide range of geologic problems. In this chapter, we provide an overview of different approaches, underlying assumptions and suitable sampling strategies for bedrock and detrital thermochronologic analyses, with particular emphasis on the fission-track (FT) method. Approaches to bedrock thermochronology are dependent on the goals of the project and the regional geologic setting, and include application of: (i) multiple methods (e.g., FT, (U–Th)/He and U–Pb) on various mineral phases (e.g., apatite and zircon) from the same sample, (ii) single methods on multiple samples collected over significant relief or across a geographic region (regional approach) or (iii) multiple methods on multiple samples. The cooling history of rock samples can be used to constrain exhumation paths and provides thermochronologic markers to determine fault offset, timing of deformation and virtual tectonic configurations above the present-day topography. Detrital samples can be used to constrain erosion patterns of sediment source regions on both short-term (103–105 yr) and long-term (106–108 yr) timescales, and their evolution through time. The full potential of the detrital thermochronology approach is best exploited by the integrated analysis of samples collected from a stratigraphic succession, samples of modern sediment and independent mineral fertility determinations.
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Keywords
- Fault Offsets
- Detrital Thermochronology
- Thermochronological Analyses
- Thermochronological Ages
- Exhumation Rates
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
1 Bedrock Thermochronology Studies
Low-temperature thermochronology studies fall into two general categories: those where samples are collected from bedrock and those where samples are essentially detrital. Within each of these two groups there are also natural subdivisions such as: for bedrock studies, applying a key-locality/outcrop approach (e.g., collecting over significant relief (the vertical profile approach) to determine age-elevation relationships) and/or a more regional sampling approach, all of which are dependent on the objectives of the study, the available geologic information, if other methods are also to be applied and if subsequent thermal modelling might also be applied. The geologic problem being addressed ideally helps shape the sampling strategy. Typically, the part of a study that has the longest longevity is the data itself. For example, modelling methods change and evolve, but the data remains the same, all things being equal.
1.1 Multiple-Method Versus Age-Elevation Approach for the Analysis of Exhumation Rates
When bedrock samples are collected on a regional basis, an exhumation rate for single samples may be estimated by assuming that the ages represent closure temperature (Tc) ages, and by assuming (or knowing) the paleogeothermal gradient to calculate depth to Tc. Hence, the depth divided by the ages yields an apparent exhumation rate (e.g., Reiners and Brandon 2006). This approach is not applied quite so much to basement samples, especially if inverse thermal models are available (Chap. 3, Ketcham 2018). However, it still remains the fundamental approach for many detrital thermochronology studies (e.g., Garver et al. 1999) (see Sect. 10.2).
More common approaches in studies utilising low-temperature thermochronology on bedrock samples involve the combination of multiple methods with different Tc, and sampling along vertical profiles (Fig. 10.1). The multiple-method approach (Fig. 10.1a) is based on the analysis of different thermochronologic systems in minerals retrieved from the same sample (e.g., Wagner et al. 1977; Hurford 1986; Moore and England 2001). Different mineral/systems with progressively lower Tc generally yield progressively younger thermochronologic ages, constraining a cooling history that is generally related to the exhumation of the sample towards the Earth’s surface. In a diagram showing Tc versus the thermochronologic ages yielded by the analysed sample (Fig. 10.1a), the gradient of the slope is a function of the cooling rate in the selected time interval and is steeper for faster cooling. Converting this average cooling rate into an exhumation rate is not straightforward, as the paleogeothermal gradient during cooling has to be independently known (see Chap. 8, Malusà and Fitzgerald 2018). The multiple-method approach is generally more applicable for samples that have cooled across a wider temperature range (i.e., several hundreds of °C), which makes this approach suitable for the analysis of rocks exhumed from greater depths (see Chap. 13, Baldwin et al. 2018). Higher temperature thermochronologic methods are slower to respond to changes in exhumation rates (Moore and England 2001). Thus, if there is a step-wise increase in erosion rates at the surface, different methods on the same sample may give the appearance of a gradually increasing erosion rate with time as the Tc isotherms migrate at different rates to their new steady-state depths.
The age-elevation (vertical profile) approach is based on the analysis of an array of samples collected across a significant elevation range (and a short horizontal distance) employing the same dating method (e.g., Wagner and Reimer 1972; Naeser et al. 1983; Gleadow and Fitzgerald 1987; Fitzgerald and Gleadow 1988, 1990; Fitzgerald et al. 1995; Ruiz et al. 2009). During exhumation from depths greater than the Tc isothermal surface, samples collected from higher elevations cross the Tc isothermal surface before those from lower elevations, leading to a normal age-elevation relationship (i.e., samples collected at higher elevation have older ages). The gradient of the slope in an age-elevation diagram provides an apparent average exhumation rate for the time interval between the age yielded by the uppermost sample (t1 in Fig. 10.1b) and the age yielded by the lowermost one (t2 in Fig. 10.1b). The slope is generally steeper for faster exhumation rates. This estimate does not require any explicit assumption about the paleogeothermal gradient, but converting an apparent exhumation rate to a true exhumation rate using the age-elevation approach is not straightforward and requires a careful analysis of the relationships between the topography and the thermal reference frame (see Chap. 9, Fitzgerald and Malusà 2018).
An important assumption underlying the age-elevation approach is that the spatial relationships between samples have remained unchanged since the time of exhumation. Therefore, this approach should not be applied, for example, across faults that may have modified these original relationships: Samples from different fault blocks must be considered separately. Conversely, this approach can be used to detect faults between samples with contrasting or unexpected ages. Additionally, the difference in elevation between the lowest and the highest samples should be sufficiently large to allow a significant spread in thermochronologic ages, at least compared to the standard error associated with each age. This is particularly important for rapidly exhuming areas, where thermochronologic ages tend to be invariant with elevation. The most favourable conditions for a successful application of the age-elevation method are thus represented by a combination of high topographic relief and relatively slow exhumation rates, which allows for a larger spread of thermochronologic ages in the array of analysed samples. However, the time interval constrained by the age-elevation approach using one dating method only (t1 to t2 in Fig. 10.1b) may be quite short. In order to constrain the exhumation history over a longer time interval, multiple methods may be applied to the same array of samples (Fig. 10.1b). The time intervals constrained by different thermochronologic methods may either overlap, thus providing complementary constraints to specific segments of the exhumation path, or leave unconstrained time intervals between different methods, as often observed when the relief covered by samples is not sufficiently large. Different age-elevation slopes may be recorded for different thermochronologic methods even if the same exhumation rate is ongoing. This is because of the effects of topography and the bending of isothermal surfaces under ridges and valleys (e.g., Stüwe et al. 1994; Mancktelow and Grasemann 1997; Braun 2002), which can be investigated by suitable sampling strategies as discussed in Chaps. 9 (Fitzgerald and Malusà 2018) and 19 (Schildgen and van der Beek 2018).
The vertical spacing between samples is also important, and should be sufficiently small to highlight any change in slope, either ascribed to variations in exhumation rates or to the presence of a paleo-PAZ (Partial Annealing Zone) (see Chap. 9, Fitzgerald and Malusà 2018). For the calculation of an apparent exhumation rate, thermochronologic ages yielded by partly reset or unreset samples, i.e., by samples collected within or above a paleo-PAZ (as revealed, e.g., by grain age over dispersion or by confined track-length distributions) should not be included (see Chap. 6, Vermeesch 2018; Chap. 9, Fitzgerald and Malusà 2018).
Plots displaying the measured FT age against the mean track length (MTL) provide a useful approach to visualise the occurrence of partly reset or unreset samples lying within or above a paleo-PAZ (Fig. 10.1c). Samples collected from a range of initial paleodepths in a region that has undergone broadly coeval cooling will define a concave-up “boomerang” shape (Green 1986). This boomerang trend includes: (i) old ages with long MTLs corresponding to samples that have spent most time above the PAZ; (ii) intermediate ages with the shortest MTLs, corresponding to samples that have spent most time within the PAZ; and (iii) young ages with long MTLs that have experienced the highest initial paleotemperatures. The timing of the most recent cooling event is constrained by the transition from samples with “intermediate” FT ages and MTLs in the 12–13 µm range to samples with younger FT ages and MTLs in the range of 14–15 μm (e.g., Brown et al. 1994; Fitzgerald 1994; Gallagher and Brown 1997; Hendriks et al. 2007). These latter samples can be used to estimate an apparent exhumation rate using the age-elevation approach, provided these samples are collected from the same fault block and fulfil the criteria described in Chap. 9 (Fitzgerald and Malusà 2018).
1.2 Virtual Configuration of Rock Units by FT Thermochronology
Low-temperature thermochronology can also be used to envisage a paleo-thermal structure and infer the original thickness of overburden, which may include partly eroded stratigraphic successions or eroded thrust sheets (Fig. 10.2a–c). This is one application of FT stratigraphy, with “stratigraphy” represented by the variation of age with elevation or depth (in case of boreholes) (e.g., Brown 1991).
The radial plots in Fig. 10.2a illustrate the grain-age distributions normally expected in samples of sedimentary rocks collected at increasing depths down a borehole in a sedimentary basin. Samples that have experienced minor burial and have remained above the PAZ of the chosen thermochronologic system (black circles in Fig. 10.2a) will show either unimodal or polymodal grain-age distributions, with grain-age populations systematically older than the stratigraphic age of the sample. Samples that have experienced burial within the PAZ (grey circles in Fig. 10.2a) will display partly reset FT ages that with increasing temperature become progressively younger than the stratigraphic age of the sample. Samples located below the PAZ, i.e., at higher temperatures (white circles in Fig. 10.2a), will yield a zero FT age because the fission tracks have been totally annealed.
Subsequent to burial, and following rapid exhumation to the surface, let us now examine age/length trends on this exhumed stratigraphic succession (Fig. 10.2b). Sedimentary rocks originally located below the PAZ (white circles in Fig. 10.2b) yield unimodal grain-age distributions with a central age that is equal to, or slightly younger (although often not much younger) than this rapid exhumation. Samples that have experienced burial within the PAZ (grey circles in Fig. 10.2b) will display FT ages ranging between the stratigraphic age of the sample and the time of exhumation. The timing of the transition between the completely reset and the partially reset samples typically marks the timing of the initiation of more rapid cooling and exhumation. Samples that have remained above the PAZ will provide information on older exhumation/crystallisation events in the sediment source areas, which can be investigated by using the detrital thermochronology approaches described in Sect. 10.2 (see also Chap. 14, Carter 2018; Chap. 15, Bernet 2018; Chap. 16, Malusà 2018 and Chap. 17, Fitzgerald et al. 2018 for more details). Clues for the interpretation of partially reset detrital samples can be found in Brandon et al. (1998) and in Chap. 18 (Schneider and Issler 2018).
The occurrence of partly or fully reset detrital samples in the uppermost levels of a stratigraphic sequence provides evidence of overburden removal by denudation (Fig. 10.2b). When the paleogeothermal gradient is reasonably assumed or independently known, the FT stratigraphy approach provides a useful way to estimate the depth of erosional denudation and the virtual configuration of eroded rock units above the present-day topography (Fig. 10.2c). Examples include studies in the central Alaska Range to estimate the amount of rock present above the summit of Denali prior to the onset of rapid exhumation in the Late Miocene (Fitzgerald et al. 1995, see also Chap. 9, Fitzgerald and Malusà 2018); in the Apennines to infer the virtual configuration of the Ligurian wedge on top of the Adriatic foredeep units (Zattin et al. 2002); in eastern Anti-Atlas to infer the past configuration of the Variscan belt on top of the Precambrian basement of the West African Craton (Malusà et al. 2007); in the Canadian Cordillera to infer the initial thickness of the Lewis thrust sheet (Feinstein et al. 2007); in SE France to infer the virtual configuration of the Alpine nappes on top of the Paleogene sedimentary succession of the European foreland (Labaume et al. 2008; Schwartz et al. 2017). The number of samples required for a reliable reconstruction of these virtual configurations is often quite high, and datasets will ideally include samples from different levels of the stratigraphic succession.
1.3 The Analysis of Fault Offsets Using Thermochronologic Markers
Low-temperature thermochronology often provides time constraints on fault activity and markers for the analysis of fault offsets (e.g., Gleadow and Fitzgerald 1987; Gessner et al. 2001; Raab et al. 2002; Fitzgerald et al. 2009; Niemi et al. 2013; Ksienzyk et al. 2014; Balestrieri et al. 2016, and Chap. 11, Foster 2018). Such markers are particularly useful in case of monotonous sequences of sedimentary, magmatic and metamorphic rocks, where geologic markers are absent, and in regions of poor outcrop where other markers are not available (e.g., forested or glaciated areas). Thermochronologic markers may include a paleo-PAZ and FT stratigraphy (Fig. 10.2d) (e.g., Brown 1991; Fitzgerald 1992; Foster et al. 1993; Bigot-Cormier et al. 2000; Stockli et al. 2002; Thiede et al. 2006; Richardson et al. 2008; Fitzgerald et al. 2009; Kounov et al. 2009; Miller et al. 2010), which potentially constrain fault activity in the uppermost few kilometres of the crust (Chap. 11, Foster 2018). Both the multiple-method and age-elevation approaches described in Sect. 10.1.1, when applied to distinct crustal blocks, are potentially able to highlight episodes of differential exhumation across major faults, thus constraining the age of fault activity (e.g., Gleadow and Fitzgerald 1987; Fitzgerald 1992, 1994; Foster et al. 1993; Foster and Gleadow 1996; Viola et al. 2001; West and Roden-Tice 2003; Malusà et al. 2005, 2009a; Niemi et al. 2013; Riccio et al. 2014). Given the precision of the ages on either side of the fault, which is typically ±5% (±1σ) for apatite FT (AFT) ages, faults with small offsets will not be revealed. Whether a fault offset is revealed often depends on the age-elevation relationship. If the slope is shallow (ages vary considerably with change in elevation) age-offsets due to faulting are often revealed, whereas when the slope is steep (ages do not vary much with elevation) faults are typically not revealed, as there is little age-offset across the fault unless the vertical fault offset is extremely large (i.e., several kilometres). Constraints on the fault offsets are usually more reliable when the local FT stratigraphy is well documented and multiple samples (if possible collected over a significant elevation range on either side of the fault to confirm the local age-elevation slope) are used. Observations of age trends such as these can be integrated by information provided by temperature-time paths, based on the modelling of confined track lengths in samples collected on the opposite sides of the fault (e.g., Thomson 2002; Balestrieri et al. 2016). If the paleogeothermal gradient is independently known, the multiple-method analysis of distinct fault blocks may provide reliable estimates of fault throws accommodated through time (e.g., Malusà et al. 2006).
In a well-known example, Fitzgerald (1992) tested the FT stratigraphy approach across the Transantarctic Mountain Front in the Dry Valleys area where the location and offset of normal faults are well-delineated by step-faulted horizontal dolerite sills (see also Chap. 9, Fitzgerald and Malusà 2018). There, reconstruction of the ~100 Ma isochron from samples collected systematically along the faulted ridge was used to reliably document fault offsets as small as ~200 m. This was, however, an ideal situation where the slope of the age-elevation relationship (an exhumed PAZ) was ~15 m/Myr; thus, an offset of 300–400 m represents a discernable age difference of 20–25 Ma. Miller et al. (2010) undertook a similar study across the Transantarctic Mountain Front at Cape Surprise near the Shackleton Glacier, distinguishing between the presence of one master fault with offset of ~5 km or a series of smaller faults, as it proved to be.
Fault offsets can be also constrained by mineral-age stratigraphy (Malusà et al. 2011), which is based on the specific combinations of crystallisation and exhumation ages that are yielded by different thermochronometers (and minerals) at different depths in the crust (see Chap. 8, Malusà and Fitzgerald 2018, their Fig. 8.7). Such combinations allow one to define, on a thermochronologic basis, a stratigraphy of increasingly deeper crustal levels (Levels 1–4 in Fig. 10.2e) that may be able to constrain fault offsets in homogeneous rock sequences. Mineral-age stratigraphy can be particularly useful in cases where plutonic rocks dominate the geology (Fig. 10.2e). Use of mineral-age stratigraphy may also, when compared to FT stratigraphy, constrain greater offsets across faults because the data spans a greater temperature interval. In the case of the Insubric Fault in the European Alps, this approach provides evidence of >10–15 km fault offset of the uplifted crustal block north of the fault, relative to the downthrown southern side. On the north, the Periadriatic Bergell/Bregaglia pluton, emplaced in the Oligocene, is now unroofed down to a crustal level that was lying below the Tc of the K–Ar system on biotite at the time of intrusion (level 4 in Fig. 10.2e). This is attested by biotite K–Ar ages (26–21 Ma, Villa and von Blanckenburg 1991) that are much younger than the intrusion age provided by zircon U–Pb dating (30 ± 2 Ma, Oberli et al. 2004). In comparison, the block south of the Insubric Fault has Periadriatic dykes now exposed at the surface. These dykes show zircon U–Pb and AFT ages, yielding two clusters at 42–39 Ma and 35–34 Ma, that are generally indistinguishable within error (D’Adda et al. 2011; Malusà et al. 2011; Zanchetta et al. 2015), because they were emplaced at crustal levels lying within or just below the AFT PAZ at the time of intrusion (level 1 or 2 in Fig. 10.2e). These constraints integrate previous estimates of fault offsets based on the multiple-method approach (Hurford 1986).
The mineral-age stratigraphy observed in an orogen undergoing erosion may subsequently be observed as a “reverse” age stratigraphy in sedimentary basins fed from that eroding source. This reverse age trend can thus be used as a marker to detect tectonic repetitions and fault offsets in the absence of other stratigraphic markers (Fig. 10.2e, right panel). For example, application of this approach to the Oligocene–Miocene Gonfolite Group derived from the erosion of the Bergell pluton (Wagner et al. 1979; Bernoulli et al. 1989) provided evidence for a major and previously undetected thrust fault in the Gonfolite Group (Lake Varese backthrust in Fig. 10.2e) (Malusà et al. 2011).
Thermochronologic analyses across major faults can ideally constrain the timing of deformation thanks to a detailed reconstruction of the differential exhumation paths experienced by different fault blocks through time. In the example of Fig. 10.3 (left panel), the activity of a reverse fault before time t3 is well constrained by apatite (U–Th)/He (AHe) and AFT analyses in rock samples A and B collected on the opposite sides of the fault, and by inverse modelling using age and confined track-length data from the same samples. AHe ages in samples A and B are equal to t3, and indistinguishable across the fault, which is in line with the cessation of fault activity not later than time t3. Importantly, there is usually only clear thermochronologic evidence for fault offset when faults accommodate differential exhumation (Fig. 10.3a), but such evidence is not observed when faults accommodate differential subsidence (Fig. 10.3b). Such an observation, with respect to cooling rather than exhumation/subsidence, has long been established (e.g., Green et al. 1989). The situation of faults accommodating differential subsidence is typical, for instance, of rapidly subsiding foreland basins such as the Po Plain north of the Apennines (Pieri and Groppi 1981). In Fig. 10.3b, the reverse fault indicated in red is active at the same time interval as the fault in Fig. 10.3a, and when the analysed samples (C and D) at the time of faulting were at the same crustal level as samples A and B. However, the thermochronologic analysis of samples C and D provides no useful constraint on the timing of deformation.
In the case where fault motion is dominantly strike-slip, differential exhumation between fault blocks is usually minimal. As a consequence, thermochronologic evidence for faulting along strike-slip systems is generally observed particularly at restraining bends or step-overs, or where there is transpression. Well-known examples of these situations have been documented along the Denali Fault (e.g., Riccio et al. 2014), the San Andreas Fault (e.g., Niemi et al. 2013) and the Alpine Fault (e.g., Herman et al. 2007; Warren-Smith et al. 2016).
Sampling strategies to provide timing constraints on fault activity, and markers for the analysis of fault offsets (see Chap. 11, Foster 2018), must be designed to minimise the bias arising from the complexity of isotherms close to major faults (see Chap. 8, Malusà and Fitzgerald 2018). Large (crustally penetrative) faults are most likely to have a thermal perturbation (Ehlers 2005), and for these faults, it is advisable to collect samples tens to hundreds of metres from the main deformation zone. In contrast, some studies seek to exploit the thermal perturbation along the faults to constrain the fault activity (Tagami et al. 2001; Murakami and Tagami 2004), and samples are best collected from a closely spaced array across the fault plane (see Chap. 12, Tagami 2018).
1.4 FT Thermochronology as a Correlation Tool for Mesoscale Structural Data
In tectonically complex areas, the analysis of post-metamorphic deformation is particularly challenging, because deformation is often partitioned within different crustal blocks, fault orientation is not scale invariant, and the strain field inferred from mesoscale structures (i.e., outcrop scale) may differ from strain on a regional scale (Eyal and Reches 1983; Rebai et al. 1992; Martinez-Diaz 2002). Regional reconstructions thus require structural analysis at different scales, including field mapping of the network of major (km-scale) faults, and a dense distribution of time-constrained mesoscale strain axes that are derived from the kinematic analysis of fault-slip data in outcrops from high-strain and low-strain domains (Marrett and Allmendinger 1990). Within this framework, low-temperature thermochronology provides not only time constraints for the analysis of major faults, but also an effective tool to constrain the age of mesoscale deformation (e.g., Malusà et al. 2009a).
Fault-rock types and related deformation mechanisms show a generalised progression with depth (Fig. 10.4a); from gouge/breccias to cataclasites to mylonites, or to describe the mechanisms, from frictional-plastic to viscous flow (Sibson 1983; Snoke et al. 1998). The transition from frictional to viscous flow partly depends on strain rate, but it is dominantly controlled by lithology and temperature in the crust (Schmid and Handy 1991; Scholz 1998; Raterron et al. 2004). Therefore, the analysis of fault rocks in a specific lithology gives indications on the crustal level where mesoscale structures have formed. Because FT analysis provides chronological constraints on the passage of a rock through a given crustal level, the timing of both mesoscale structures and their associated strain axes can thus be constrained.
Crustal rocks are commonly dominated by quartz rheology; thus, the transition from frictional to viscous flow takes place at ~300 °C (Scholz 1998; Chen et al. 2013). The temperature of this change in deformational mechanism correlates well with the Tc of the FT system in low-damage zircon (Fig. 10.4a). Therefore, in general, mylonites will form at temperatures higher than the Tc of the zircon FT (ZFT) system. Cohesive cataclasites will form at temperatures that are higher than the Tc of the AFT system. Fault gouges and fault breccias are typical of the uppermost kilometres of the crust, i.e., of the temperature range best constrained by the AHe system (Fig. 10.4a). Because the frictional-to-viscous transition controls the thickness of the seismogenic zone (Priestley et al. 2008; Chen et al. 2013), the maximum depth extent for pseudotachylite formation in quartz-dominated crustal rocks also correlates with the Tc of the ZFT system (Fig. 10.4a). Fault rocks are often associated with veins and hydrothermal mineralisation that can provide additional constraints on the temperature of fault-rock formation (Wiltschko 1998).
Figure 10.4a conceptually illustrates the application of FT thermochronology to constrain the timing of mesoscale deformation and related strain axes, in a region where the exhumation history is independently constrained by AFT and ZFT ages. The rock mass (shown as a cube) in the right panel, during progressive exhumation is cut by a right-lateral shear zone marked by mylonitic rocks (phase D1), then by a normal fault marked by cohesive cataclasite (phase D2), and finally by a normal fault marked by gouge (phase D3). When combined with FT data, we can conclude that phase D1 is likely older than the ZFT age, phase D2 may have taken place within a time range delimited by AFT and ZFT ages, whereas deformation phase D3 is likely younger than the AFT age. If pseudotachylites are found along these faults, they must be coeval or younger than the age provided by ZFT. The resolution of these constraints can be improved by using additional thermochronologic systems, and by considering not only rock types controlled by quartz rheology, but also other rock types controlled by the rheology of calcite, feldspar or olivine.
Interpreting mesoscale deformation on a regional scale solely based on deformation style, and without reliable time constraints provided by thermochronology, is potentially misleading. Deformation at the outcrop scale may be coeval in different crustal blocks, yet marked by different types of fault rock. Such a scenario may be possible if deformation occurred at the same time in different crustal blocks, but at different crustal levels (Malusà et al. 2009a). In the example of Fig. 10.4b, mylonites formed at time t1 in one crustal block, are exposed at the surface together with cataclasites formed at the same time, but at shallower levels, in a nearby crustal block exhumed at slower rates. Therefore, deformation style should not be used for correlations of mesoscale structural data over large areas, unless integrated with low-temperature thermochronology data. The sampling strategy for this kind of study, that incorporates thermochronology and structural analysis, is similar to that required for the multiple-method approach (cf. Sect. 10.1.1). Samples should preferably be collected far enough away from major faults to avoid major perturbations of the background thermal field. Compared to the direct, typically more precise dating of synkinematic minerals grown along a fault plane (e.g., Freeman et al. 1997; Zwingmann and Mancktelow 2004), this approach generally requires a lower number of samples but does require multiple methods. However, it may provide constraints not only on single deformation steps, but on the whole deformation history recorded by sets of mesoscale faults.
2 Detrital Thermochronology Studies
Modern sediments and sedimentary rocks can provide invaluable information on the provenance and exhumation of the sediment sources (e.g., Baldwin et al. 1986; Cerveny et al. 1988; Brandon et al. 1998; Garver et al. 1999; Bernet et al. 2001; Willett et al. 2003; Ruiz et al. 2004; van der Beek et al. 2006). Sedimentary rocks for detrital thermochronology studies are typically collected through a stratigraphic succession. If sedimentary rocks have remained above the PAZ or partial retention zone (PRZ) of the chosen thermochronologic system since their deposition, the stratigraphic succession should reflect, in inverted order, the thermochronologic age structure observed in the sediment source area. Eroded detritus is generally distributed over a much wider area compared to that of the eroding source. Sedimentary successions thus record the erosional history of a much thicker crustal section. Today, such crustal sections may be completely eroded away, and thus impossible to investigate by the bedrock approach.
Detrital grain-age distributions represent the source rocks. Depending on the geologic evolution of the source rocks, these distributions can be unimodal or polymodal. Polymodal distributions are usually deconvolved into different grain-age populations (e.g., Brandon 1996; Dunkl and Székely 2002; Vermeesch 2009), which are generally older than the depositional age of the analysed sample (Bernet et al. 2004a; Bernet and Garver 2005).
2.1 Approaches to Detrital Thermochronology Studies
Figure 10.5a provides a summary of potential approaches to detrital thermochronology studies by using either modern sediment samples (1 and 2 in Fig. 10.5a) and samples from a stratigraphic succession (3–5 in Fig. 10.5a). Detrital thermochronology can provide information on:
Average long-term erosion rates (1 in Fig. 10.5a) Analysing minerals from samples of modern river sediments allows one to construct grain-age distributions from each catchment sampled (e.g., Garver et al. 1999; Brewer et al. 2003). These grain-age distributions are representative, under certain conditions, of the FT stratigraphy within the drainage (e.g., Bernet et al. 2004a; Resentini and Malusà 2012). The age of the youngest detrital age component, if interpreted as an exhumation-related cooling age, can be used to provide preliminary, although sometimes imprecise constraints on the average long-term (106–108 yr) erosion rate of the source area, using the lag-time approach (Garver et al. 1999) and a zero stratigraphic age (see below). Notably, grain-age distributions are influenced by the drainage hypsometry. Ages will be generally older in grains eroded from summits, and younger in grains eroded from valleys, depending on the age-elevation relationship in bedrock. In the case of well-developed age-elevation relationships, it is hypothetically possible to constrain the elevation from where sediment grains were eroded (e.g., Stock et al. 2006; Vermeesch 2007). Grain-age distributions will also vary depending on the mineral fertility of different upstream eroding lithologies. The mineral fertility, which can be defined as the variable propensity of different parent rocks to yield detrital grains of specific minerals when exposed to erosion (Moecher and Samson 2006; Malusà et al. 2016), can be quite inhomogeneous. The main advantage of using the detrital approach to constrain an average long-term erosion rate is the possibility of getting a first-order picture of the erosion pattern over large areas by using a relatively low number of samples (e.g., Bernet et al. 2004a; Malusà and Balestrieri 2012; Asti et al. 2018). However, ages related to exhumational cooling should be distinguished from cooling ages that are independent from exhumation, such as those provided by volcanic grains. These grains can be effectively detected by double-dating (see Chap. 5, Danišík 2018; Chap. 7, Malusà and Garzanti 2018), as shown in Chap. 15 (Bernet 2018).
Modern short-term erosion patterns (2 in Fig. 10.5a) Grain-age distributions in modern river sediments can be analysed to constrain sediment budgets and erosion patterns on timescales typical of bedload river transport (generally 103–105 yr). This approach exploits the size of grain-age populations rather than the age of mineral grains, which is utilised instead as a provenance marker (Garver et al. 1999; Bernet et al. 2004b; Malusà et al. 2009b). Samples are either collected along the trunk of the river or at major confluences, and grain-age distributions are compared by statistical methods in order to determine the percentage of mineral grains derived from different sub-basins (see Sect. 10.2.2). This percentage, when integrated with the area of each sub-basin and its mineral fertility, which is independently derived (see Chap. 7, Malusà and Garzanti 2018), can be used to calculate the relative erosion rates of the sub-basins (Malusà et al. 2016; 2017; Glotzbach et al. 2017, Braun et al. 2018). Relative erosion rates can be converted into absolute rates after integration with gauging data or cosmogenic-derived sediment fluxes for selected basins (e.g., Lupker et al. 2012; Wittmann et al. 2016). The same approach can be ideally applied to ancient alluvial sediments, using samples from lithified clastic sequences, whenever it can be reasonably assumed that the past mountain catchment was not markedly different from its present-day configuration (4 in Fig. 10.5a).
Evolution of long-term erosion rates (3 in Fig. 10.5a) The same approach utilised to constrain the average long-term erosion rate within a catchment (1 in Fig. 10.5a) can be extrapolated to ancient sedimentary successions to investigate the evolution of long-term erosion (106–108 yr timescales) in an adjacent orogen (e.g., Garver et al. 1999; Bernet et al. 2001; van der Beek et al. 2006). Samples are collected through a stratigraphic succession, and single minerals are analysed. The resulting grain-age distributions, when polymodal, are deconvolved into different grain-age populations (red and blue in Fig. 10.5), and these populations are then plotted on a lag-time diagram where the lag time is the difference between the cooling age and the depositional age (Garver et al. 1999), which is independently derived (e.g., by biostratigraphy or magnetostratigraphy). The lag time provides an estimate of the average exhumation rate of the analysed detrital grains from the depth of the Tc isothermal surface to the Earth’s surface (Garver et al. 1999; Ruiz et al. 2004). The lag-time trend is often used to infer whether an eroding mountain belt is under a constructional, steady state or decay phase of evolution (Bernet et al. 2001; Carrapa et al. 2003; Spotila 2005; Ruiz and Seward 2006; Rahl et al. 2007; Zattin et al. 2010; Lang et al. 2016). More details and examples are provided in Chap. 15 (Bernet 2018) and Chap. 17 (Fitzgerald et al. 2018).
Depositional age (5 in Fig. 10.5a) Detrital thermochronology can be also used to constrain the depositional age of barren sedimentary successions (e.g., Carter et al. 1995; Rahn and Selbekk 2007). The depositional age of a sedimentary sample must be younger than the central age of the youngest grain-age population, provided that post-depositional annealing can be excluded.
2.2 Sediment Budgets Using Modern River Sediments
Constraining sediment budgets based on detrital thermochronology analysis of modern river sediments requires detrital sources with “thermochronologically distinct fingerprints”. Such fingerprints are generally the result of different geologic or upper crustal exhumation histories (red and blue tectonic blocks in Fig. 10.5a). In a detrital sample exclusively derived from one of these sources (e.g., the fast exhuming red block sampled in catchment C), the grain-age distribution depends on the catchment hypsometry and on the catchment age-elevation relationship. Detrital samples derived from the mixing of various sources (e.g., samples SA+B and SC+D, Fig. 10.5a) likely yield polymodal grain-age distributions including different grain-age populations. Two alternative sampling strategies are employed for an effective partitioning of mineral grains (i.e., to determine the relative proportion of grains from each source), and to perform a sediment budget starting from the analysis of grain-age distributions. These are the confluence sampling and the along-trunk sampling approaches (Malusà et al. 2016).
Confluence sampling approach This requires collecting samples from major tributaries (SA and SB in Fig. 10.5a) and from the trunk river downstream of their confluence (SA+B in Fig. 10.5a). Partitioning of detrital grains is based on a linear combination of grain-age distributions upstream of the confluence (e.g., Bernet et al. 2004b). The best-fit solution is defined by the mixing proportion that minimises the misfit between the modelled distributions resulting from the linear combination, and the empirical grain-age distribution observed downstream of the confluence (squares and black line, respectively, in the cumulative probability diagram in Fig. 10.5b). The goodness of fit between modelled and empirical grain-age distributions can be evaluated using the parameter Dn,n′ of the Kolmogorov–Smirnov statistics (Dunkl and Székely 2002; Malusà et al. 2013; Vermeesch 2013), which shows a minimum in correspondence of the best-fit solution. In order to avoid meaningless linear combinations between indistinguishable grain-age distributions, a two-sample Kolmogorov–Smirnov test can be used to check whether grain-age distributions in samples SA and SB are statistically different or not. The confluence sampling approach requires at least three samples at each node (SA, SB, and SA+B). It allows a direct measurement of mineral fertility in sub-basins A and B using the same samples collected for thermochronologic analysis (see Chap. 7, Malusà and Garzanti 2018) and does not require any independent information on the thermochronologic fingerprint of the parent bedrock.
Along-trunk approach This approach can be used when a river cuts across rock units that have distinct, independently known thermochronologic signatures that do not overlap. Thus, the age populations can be used to unequivocally discriminate the provenance of detrital grains (Resentini and Malusà 2012). The relative proportion of grains from each source, according to the along-trunk approach is based on the deconvolution of grain-age distributions in individual age components of specific size (m and n in Fig. 10.5a, c) (e.g., Brandon 1996; Dunkl and Székely 2002). Only two samples (SC and SC+D) are needed for unmixing the thermochronologic signal and characterising sub-basins C and D in terms of mineral fertility. Fertility of sub-basin C (FC) is directly measured, fertility of sub-basin D (FD) is calculated by the formula in Fig. 10.5c.
2.3 Assumptions in Detrital Thermochronology Studies
The approaches to detrital thermochronologic analysis illustrated in Fig. 10.5a rely on a range of assumptions that should be carefully considered and independently tested (see Table 10.1). When the age of a detrital population in a modern sediment sample is employed to constrain the long-term exhumation of bedrock exposed upstream of the sampling site (1 in Fig. 10.5a), the assumption is that the thermochronologic fingerprint of eroded bedrock reflects cooling during erosion. However, this assumption is not always valid. Thermochronologic ages may also reflect past transient changes in the thermal structure of the crust (Braun 2016), episodes of metamorphic or magmatic crystallisation within the eroded bedrock (Malusà et al. 2011; Kohn et al. 2015), or the cooling history of a different (distant) eroding source that provided detritus to sedimentary rocks now exposed within the drainage (Bernet and Garver 2005; von Eynatten and Dunkl 2012). Beside a careful evaluation of the geologic setting, the risk of misinterpretation can be minimised by multiple dating of detrital mineral grains (see Chap. 5, Danišík 2018), by the integration with thermochronologic analyses of cobbles (Chap. 17, Fitzgerald et al. 2018) and bedrock (Chap. 13, Baldwin et al. 2018), and by complementing detrital thermochronology analysis with thermal modelling (Ehlers et al. 2005; Braun et al. 2012).
The assumption of uniform mineral fertility in the catchment upstream of a sampling site, which is common to many detrital thermochronology studies (e.g., Glotzbach et al. 2013), should be carefully tested even in small basins, because grain ages sourced from elevation ranges characterised by low-fertility rocks would be under-represented in corresponding detrital grain-age distributions. This is particularly important when detrital and bedrock thermochronology data are compared to test if a mountain range is in steady state (e.g., Brewer et al. 2003; Ruhl and Hodges 2005). The analysis of the short-term erosion pattern based on the relative proportion of different grain-age populations in polymodal samples (2, Fig. 10.5a) relies on the additional assumption that the sediment is effectively mixed, and that the potential bias possibly introduced by hydraulic processes during sediment transport and deposition is negligible. These assumptions can be tested using the strategies described in Chap. 7 (Malusà and Garzanti 2018).
The number of often untestable assumptions underlying the detrital thermochronologic approach largely increases in ancient sedimentary successions (see Table 10.1 and references therein). Compared to approaches 1 and 2 in Fig. 10.5a, lag-time analysis (3 in Fig. 10.5a) additionally implies that: (i) the time elapsed during sediment transport is negligible; (ii) the isothermal surfaces relevant for the chosen thermochronologic system have remained steady during exhumation; (iii) major changes in provenance can be excluded or can be detected and accounted for; (iv) the thermochronologic signal is not modified by post-depositional annealing.
Apart from transport by turbidity currents, the zero transport time assumption from erosion to deposition should be evaluated on a case-by-case basis. As an example, the transportation of apatite and zircon as river bedload in the Amazon basin may require a few millions of years, as attested by cosmogenic data (Wittmann et al. 2011). Thus, transportation time may become relevant for lag-time interpretation. The behaviour of isothermal surfaces during exhumation is generally difficult to predict (see Chap. 8, Malusà and Fitzgerald 2018) and may require an integrated approach including thermochronologic data from the source region and thermal modelling. A reliable assessment of detritus provenance generally requires a multiple-method approach to single-grain analysis (see Chap. 5, Danišík 2018; Chap. 14, Carter 2018) and a careful inspection of thermochronologic age trends along a stratigraphic succession (see Chap. 16, Malusà 2018). Lag-time analysis of detrital mineral grains is often utilised to infer the long-term evolution of an entire mountain range, but it is noteworthy that it may emphasise the cooling history of small parts of the mountain range that are characterised by highest mineral fertility (Malusà et al. 2017). The potential impact of post-depositional annealing may represent a problem not only for lag-time analysis, but also for the determination of the depositional age of a sedimentary rock by thermochronologic methods (5 in Fig. 10.5a). However, post-depositional annealing produces age trends that can be recognised when multiple samples are analysed along a stratigraphic succession (van der Beek et al. 2006, see Chap. 16, Malusà 2018 and Chap. 17, Fitzgerald et al. 2018). In this perspective, information on burial-related annealing derived from AFT length distributions gives this method a further advantage over other thermochronology methods that rely on age values only.
3 Conclusions
Low-temperature thermochronology can be used to constrain a range of geologic processes using bedrock and/or detrital samples. In bedrock studies, the multiple-method and age-elevation approaches provide useful constraints on the exhumation history of rocks now exposed at the surface, provided that a range of assumptions are properly evaluated. The multiple-method approach provides direct constraints on the cooling history of a sample, but the paleogeothermal gradient must be independently known to convert an average cooling rate to an average exhumation rate. The age-elevation approach does not require explicit assumptions on the paleogeothermal gradient. A careful analysis of the relationships between the topography and the thermal reference frame is anyway required, as is an understanding of the various factors that may change the slope of an age-elevation profile. Multiple methods can be applied to the same array of vertical profile samples, which allows exhumation to be constrained over longer time intervals. FT stratigraphy provides a suitable reference frame to constrain virtual configurations of eroded rock units above the present-day topography. A range of thermochronologic markers can be used to highlight episodes of differential exhumation across a major fault and constrain the timing of fault activity. However, in some cases, major episodes of faulting are not revealed by low-temperature thermochronology. FT data combined with the analysis of fault rocks also provide useful constraints on the timing of mesoscale deformation, and a reliable tool for the correlation over large areas of mesoscale strain axes derived from fault-slip analysis.
Detrital thermochronologic analysis can be used to provide an averaged image of the thermochronologic age structure in bedrock and to constrain the erosion pattern of the sediment sources on short-term (103–105 yr) and long-term (106–108 yr) timescales. Detrital thermochronologic analysis can also be used to constrain the provenance of the dated grains. The analysis of modern sediment samples provides the baseline for the thermochronologic interpretation of older stratigraphic levels. The lag-time approach to detrital thermochronology provides information that can be used to investigate the evolutionary stage of an entire orogenic belt, and infer whether it is under a constructional, steady state or decay phase of evolution. Different approaches to detrital thermocronology are based on a range of assumptions that should be independently tested to avoid meaningless geologic interpretations. Depending on the objectives, the full potential of the detrital thermochronologic approach is best exploited by the integrated analysis of samples collected along a sedimentary succession, samples of modern river sediment, and independent mineral fertility determinations.
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Acknowledgements
This work benefited from constructive reviews by Maria Laura Balestrieri and Shari Kelley, comments on an early version of the manuscript by an anonymous reviewer, and comments by Suzanne Baldwin and students in her 2016 thermochronology class. PGF thanks the National Science Foundation for funding through the years as well as support from Jarg Pettinga and the Erksine Program at the University of Canterbury.
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Malusà, M.G., Fitzgerald, P.G. (2019). Application of Thermochronology to Geologic Problems: Bedrock and Detrital Approaches. In: Malusà, M., Fitzgerald, P. (eds) Fission-Track Thermochronology and its Application to Geology. Springer Textbooks in Earth Sciences, Geography and Environment. Springer, Cham. https://doi.org/10.1007/978-3-319-89421-8_10
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