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Differential erosion and sediment fluxes in the Landquart basin and possible relationships to lithology and tectonic controls

Abstract

This paper focuses on the Landquart drainage basin, where we explore geomorphic signals related to the spatial differences in bedrock lithology and differential uplift. We use concentrations of cosmogenic 10Be to quantify the sediment flux patterns in the region. Furthermore we use the chemical composition of the fine fraction (< 63 μm) of the river sediment to determine the provenance of the material, and we quantify the landscape properties through the calculation of normalized steepness values for the tributary basins. The results show that the upstream segment of the Landquart basin is a glacially imprinted landscape and contributes to about 20–50% of the total modern sediment flux of the Landquart River. Contrariwise, the landscape of the downstream part is dominated by a V-shaped landscape where tributary basins are characterized by a generally high steepness. This downstream area has delivered about 50–80% of the total eroded material. Because this lowermost part of the Landquart basin is c. 50% smaller than the upstream region (200 km2 downstream versus 400 km2 upstream), the sediment budget points to very high erosion at work in this lowermost segment. Interestingly, the bedrock of this area comprises flysch and particularly ‘Bündnerschiefer’ deposits that have a high erodibility. In addition, apatite fission track ages are much younger (c. 5–10 Ma) than in the headwater reaches (10–30 Ma). This suggests the occurrence of ongoing yet long-term rock uplift that has occurred at higher rates in the downstream segment than in the headwaters. It appears that the landscape shape and denudation rate pattern in the Landquart basin reflect the combined effect of tectonic processes and fast surface response, where uplift has promoted the exhumation of bedrock with high erodibilities, and where the low erosional resistance of the exposed lithologies has promoted the streams to respond by fast erosion.

1 Introduction

There is a general consensus that the topography of a mountain belt results from the erosional response to the tectonic advection of crustal material (e.g., Schmidt and Montgomery 1995; Willet and Brandon 2002; Ouimet et al. 2009; Champagnac et al. 2012). Erosional processes are different in nature and mainly operate in response to gravitational forces (Strahler 1952), thereby causing streams to incise into the bedrock and to create relief (e.g., Tucker and Whipple 2002; Whipple 2004; Valla et al. 2010a, b). However, it has also been reported that erosion and rock uplift are coupled through a positive feedback where enhanced erosional unloading accelerates rock uplift through an isostatic compensation of the eroded material (Whipple 2009). Such feedback mechanisms between erosion and uplift have been invoked for the Central European Alps (Schlunegger and Hinderer 2001; Wittmann et al. 2007; Champagnac et al. 2009; Korup and Schlunegger 2009). However, other authors suggested that the present pattern of rock uplift in the Central Alps is more likely related either to neotectonic shortening (Persaud and Pfiffner 2004) or to isostatic compensations related to the melting of the LGM glaciers and thus to glacial unloading (Gudmundsson 1994; Barletta et al. 2006; Mey et al. 2016). Although these mechanisms have been well explored in the past years, less research has been conducted on exploring how lithology controls the denudation rates and patterns (e.g., Norton et al. 2011; Stutenbecker et al. 2016) and how the occurrence of rock uplift in combination with variations in bedrock lithologies can be recognized based on the landscape properties and the erosion rate patterns at a drainage basin scale within the Central European Alps.

Here, we present evidence for the combined controls of rock uplift and lithology on surface erosion, sediment flux and landscape form within the Landquart basin, a tributary system of the Rhine headwaters situated in the eastern Alps of Switzerland (Fig. 1). We quantify spatially averaged denudation rates using the concentrations of in situ produced cosmogenic 10Be in alluvial sediments. We complement this dataset with sediment-provenance fingerprinting techniques and investigate the geochemical composition of the eroded materials at different sites within the catchment. Finally, we extract morphometric data from the topography of the tributary catchments, which potentially record the controls of the combined effect of lithology and rock uplift.

Fig. 1
figure 1

(modified after Schmid et al. 1996)

Geological setting, showing a map of the large-scale tectonic architecture of the Alps and the studied drainage basin

2 Local setting

2.1 Geomorphology

The SE to NW-oriented Landquart basin, which is the focus of this study, is a tributary system within the headwaters of the Rhine River and covers an area of c. 610 km2. It can be subdivided into a lower and upper headwater segment (Fig. 1). In a general sense, the headwater streams incise mainly in rocks of the Austroalpine cover nappes, while the lower reaches are located in the Prättigau half-window where Flysch and ‘Bündnerschiefer’ units are exposed. Uplift and exhumation of the latter units resulted in the bending of the basal thrust that separates the Austroalpine cover nappes from the Flysch and ‘Bündnerschiefer’ units in the footwall (Fig. 2).

Fig. 2
figure 2

Tectonic units underlying the Landquart drainage basin. The figure also illustrates the sites where the samples for the provenance analysis and the estimation of 10Be-based sediment fluxes and denudation rates have been collected. The tributary streams are indicated with italic letters

The Landquart River, which is the trunk stream in the basin (Fig. 2), originates at 2700 m a.s.l. and flows into the Rhine River at 530 m a.s.l. In the headwaters, the Landquart basin hosts four small glaciers situated at elevations above c. 2000–2200 m a.s.l. The largest of them is referred to as the Silvretta glacier and is only 3 km long. Farther downstream from the glaciers, the Landquart basin hosts 11 major tributary systems with various sizes ranging from 7 to c. 30–60 km2 (Fig. 2). The five tributary basins in the lower part of the Landquart system (Schranggabach, Taschinasbach, Schraubbach, Buchner Tobel and Furner Bach; Fig. 2) are deeply incised, V-shaped basins, while the remaining six tributary basins farther upstream (Ariesch Bach, Schanielabach, Schlappinbach, Stützbach, Verstanclabach and Vernelabach) have more gently curved hillslopes particularly in their headwaters.

During the Quaternary and particularly during the Last Glacial Maximum (LGM) c. 20 ka ago, the central Alps including the Landquart basin have been covered by a km-thick ice sheet (Bini et al. 2009). This resulted in the formation of glacial landforms with curved valley flanks, U-shaped cross-sectional geometries in some places, and multiple bedrock steps (Ivy-Ochs et al. 2008; Montgomery and Korup 2010). The LGM and previous glaciers in the tributary valleys did not incise as deeply as the main glacier in the trunk channel. The consequence is that hanging valleys with V-shaped inner gorges were formed along the downstream ends of the tributary systems (Korup and Schlunegger 2007), as is the case in many locations in the Alps (e.g., Valla et al. 2010a, b).

2.2 Bedrock geology

The bedrock of the study area (Figs. 1, 2) is made up of a stack of tectonic units dipping towards the southeast (Schmid et al. 1996). In the northwest, the Helvetic nappes cover the Aar massif (exposed in the Vättis window) and its autochthonous sedimentary cover including the Infrahelvetic nappe stack. During Mesozoic times, these units were deposited on the stretched margin of the European continental plate adjacent to the Valais basin in an offshore environment. Farther to the southeast, the Helvetic units are overlain by the Penninic nappe stack, which in turn is divided into three groups according to their palaeogeographic position during Mesozoic times (Schmid et al. 2004). The lower Penninic units cover directly the Helvetic nappes and consist of the Mesozoic (Jurassic to Cretaceous) meta-sedimentary fill of the Valais basin, where sedimentation occurred in a hemipelagic environment and partly by turbidity currents. The related deposits comprise the Mesozoic ‘Bündnerschiefer’. These deposits, in turn, are overlain by the Cenozoic Prättigau Flysch that is part of the same sedimentary sequence (Schmid et al. 1996). The overlying middle Penninic units consist of Mesozoic limestones deposited on a distal spur of the Iberian micro-continent, which has been referred to as the Briançonnais zone in the literature (Schmid et al. 1996). These sediments are found in the Sulzfluh and Falknis thrust sheets and currently mark the northern boundary of the study area (Fig. 2). The third and tectonically highest Penninic unit, referred to as the Arosa nappe, had its origin in the Alpine Tethys ocean situated to the south of the Briançonnais micro-continent during Mesozoic times, but to the north of the distal margin of the Adriatic microplate. The Mesozoic phase of extensional faulting resulted in the formation of pillow lavas and ophiolitic rock sequences (Trümpy 1975; Pfiffner 2015). The Penninic units are overlain by the Austroalpine sedimentary and crystalline units, which delineated the northern stretched margin of the Adriatic plate during Mesozoic times. They comprise the Schafläger, Dorfberg, Gotschna and Schiahorn imbricates with Paleozoic crystalline rocks and Mesozoic sediments (Mählmann and Giger 2012), the overlying Silvretta nappe with Paleozoic basement units, and a Mesozoic suite of limestones farther to the north (Pfiffner 2015).

Seismic surveys have shown that the crystalline basement of the external massifs underlying the Landquart basin dips towards the SE and is part of the northeastern spur of the Aar massif (Pfiffner and Hitz 1997; Pfiffner 2015; Fig. 3a). The Aar massif is a large crystalline unit made up of Variscan basement rocks of the European continental plate, which stretches from the SE to the NW. In addition, this unit has been interpreted as a laterally propagating large-scale fold (e.g. Herwegh et al. 2017; Nibourel et al. 2018), whereby the northeastern tip is situated beneath the Landquart basin (Fig. 3a). Approximately 4–2 Ma-old apatite fission track ages (Wagner and Reimer 1972; Weh 1998; Weh and Froitzheim 2001; Fig. 3b), which record the cooling of the host rocks to temperatures between 110-90°, indicate that this unit has experienced the fastest exhumation rates in the Central European Alps during the past millions of years, possibly until the present (Vernon et al. 2008; Pfiffner 2015; Fox et al. 2016). These young ages are centred in the Chur region, from where the ages get older than > 10 Ma over a distance of c. 50 km. Interestingly, the contour lines of fission track ages follow the exhumation pattern of the Prättigau half-window (Fig. 3b), where the basement thrusts of the Austroalpine units are bent (Weh and Froitzheim 2001). This suggests that the formation of this half-window is likely to have occurred during the past few millions of years. This pattern of uplift and exhumation is likewise seen by the results of geodetic surveys (Fig. 3c) that disclosed high modern surface uplift rates of > 1.4 mm a−1 (Kahle et al. 1997; Schlatter et al. 2005). Persaud and Pfiffner (2004) invoked the occurrence of neotectonic shortening in the area of the eastern extension of the Aar massif to explain this uplift pattern. However, based on a recent analysis of fault plane solutions from earthquakes, Marschall et al. (2013) suggested a strike-slip to extensional regime in this region. Alternatively, the Prättigau half-window exposes Flysch and ‘Bündnerschiefer’ units with high bedrock erodibilities, while the headwaters are underlain by lithologies with a larger erosional resistance (Kühni and Pfiffner 2001). It is quite likely that these contrasts in erodibility could have influenced the pattern of erosion and sediment production with the consequence that the fast uplift surrounding the ‘Bündnerschiefer’ units could reflect a positive feedback response to accelerated erosion (Korup and Schlunegger 2009). We thus aim to explore the relative importance of lithology and uplift as controls on landscape form, surface erosion and sediment flux in the Landquart basin.

Fig. 3
figure 3

Landquart drainage basin within a the tectonic framework, showing a map of top crystalline basement (Pfiffner 2015), b pattern of apatite fission track ages (Weh 1998), and c geodetic uplift rates, indicated as mm per year (Kahle et al. 1997; Schlatter et al. 2005). Please refer to Fig. 1 for explanation of colours and geological units

3 Methods

3.1 Basin-averaged denudation rates using concentrations of in situ cosmogenic 10Be

We estimated catchment-wide denudation rates using the concentrations of in situ 10Be in detrital quartz grains of river-born sediments (von Blanckenburg 2005). To this extent, we collected three stream-sediment samples in the Landquart trunk stream (Lan-1, Lan-5 and Lan-10) and four samples in tributary channels (Lan-2, Schranggabach; Lan-11, Stützbach; Lan-12, Vernelabach; and Lan-13, Schlappinbach), as close to the trunk channel as possible (Fig. 2). Stream sediment samples were taken where sufficient quartz grains could be identified with hand lenses in the field. Upon sampling, special attention was paid to collect the samples from stream material, transported by fluvial processes only, to avoid perturbations of the 10Be concentrations by local processes, as for example landslides or erosion of riverbanks. After sampling, the material was processed following the lab protocol reported in Akçar et al. (2012). The samples were sieved to the size-fraction of 0.25–0.5 mm. The non-magnetic fraction was separated from each sample using a Franz isodynamic magnetic separator. In order to extract only the pure quartz grains, a sequential chemical dissolution was performed. First the non-magnetic fraction was leached with 5% hydrochloric acid (HCl) to dissolve the carbonates and organic components. All samples were then treated three times with 5% hydrofluoric acid (HF), followed by three subsequent steps using 2.5% HF. The etching of the samples with HF resulted in the removal of mineral impurities (e.g. feldspar, oxides and residual carbonates). In addition, it leached out the atmospheric 10Be adsorbed to the quartz grains. The last step of quartz purification was conducted using Aqua Regia in order to dissolve remaining metallic components as well as residual carbonate and organic materials.

The chemical separation of 10Be was then performed using the lab protocol of Akçar et al. (2012). First c. 0.2 mg of a 1 g/l Be carrier was added to the purified quartz samples, which were then dissolved in concentrated HF. After complete evaporation of the solution, the sample was fumed with HNO3, Aqua Regia and HCl. The separation protocol was followed by ion-chromatography columns. Beryllium and iron were then co-precipitated as hydroxides at a pH ~ 8. After mixing the Be/Fe precipitate with silver nitrate (AgNO3) the suspension was dried and baked in a furnace at 675 °C before the resulting Beryllium oxide (BeO) was finally pressed into copper targets. 10Be/9Be ratios were measured using the 500 kV TANDY AMS facility at ETH Zurich (Christl et al. 2013) and normalized to ETH in-house standard S2007N (Kubik and Christl 2010) using the 10Be half-life of 1.387 ± 0.012 Ma (Korschinek et al. 2010; Chmeleff et al. 2010). The full process blank ratio of (2.41 ± 0.13) × 10−15 was then subtracted from the measured ratios in order to calculate 10Be concentrations for each sample (Table 1).

Table 1 Cosmogenic nuclide data

Spatially averaged denudation rates (Table 2) were calculated using the concentrations of in situ 10Be and the CAIRN software (Mudd et al. 2016) in which 10Be production and shielding effects are computed on a pixel-by-pixel basis. Calculations were accomplished using the default parameters in CAIRN, which include a SLHL 10Be production rate of 4.30 at g−1 a−1, consider the neutrons, fast and slow muons attenuation lengths and contributions following Braucher et al. (2011). A rock density of 2.65 g cm−3 was used. Snow shielding factors were estimated based on annual snow thickness derived from Auer (2003) and converted to snow water equivalent thickness according to Jonas et al. (2009).

Table 2 10Be derived denudation rates

3.2 Provenance tracing and mixing modelling

In order to allocate sediment sources and to quantify their relative contributions to the sediment budget of the Landquart basin, we applied a provenance tracing technique. This was conducted based on the chemical composition of the fine fraction (< 63 μm) of riverine sediments following a tributary sampling approach (e.g., Stutenbecker et al. 2018): Sediment was collected from 10 major tributary basins with different bedrock lithologies (Lan-2, 3, 4, 6, 7, 8, 9, 11, 12 and 13) and 3 additional locations within the trunk river (Lan-1, 5 and 10; Fig. 2). The < 63 μm fraction was extracted through wet-sieving, and the material was dried and sent to the Bureau Veritas Commodities in Vancouver (Canada) for inductively coupled plasma mass spectrometry (ICP-MS) analysis. This yielded concentrations of the main element oxides (SiO2, Al2O3, Fe2O3, MgO, CaO, Na2O, K2O, TiO2, P2O3, MnO and Cr2O3) as well as of selected trace elements (Ba, Ni, Sr, Zr, Y, Nb and Sc) (Tables 3, 4). Compositional end-members were then defined based on principal component analysis techniques (PCA). PCA allows to reduce the data dimensionality and to examine the variance of a dataset (Aitchison 1983, Vermeesch and Garzanti 2015). In order to visualize intra- and inter-sample variability, the compositional data were transformed using the centered-log-ratio-transformation (clr) and plotted in a compositional biplot using the software CoDaPack (Comas and Thió-Henestrosa 2011) (Fig. 4).

Table 3 Content of oxides (%)
Table 4 Content of oxides and elements (ppm)
Fig. 4
figure 4

Compositional biplot of the principal component analysis using a centered-log-ratio-transformation. The first two principal components (PC1 and PC2) sum up to 85%

The contributions of each end-member to the three in-stream samples Lan-1, Lan-5 and Lan-10 (pie plots on Fig. 5a) were estimated using the mixing modelling R package “fingerPro” developed by Lizaga et al. (2018). In order to choose input element concentrations that provide maximum discrimination between the three defined sources we followed standard statistical procedures in fingerprinting techniques (e.g. Collins et al. 1996, Collins and Walling 2002). This includes (1) the range test, (2) the Kruskal–Wallis-H-test and (3) the stepwise discriminant analysis based on the minimization of Wilks’ Lambda. The range test is used to ensure that only mass-conservative elements enter the mixing model. If elements get enriched during transport (e.g. through hydraulic sorting that might favour heavy minerals such as zircon, rich in Zr, or apatite, rich in P2O5) or depleted (e.g. through the destruction of cleaved rock fragments or dissolution of carbonates/evaporates), their concentration can be higher or lower, respectively, in the in-stream sediment compared to the concentration range present in the sources. Accordingly, we calculated the maximum and minimum concentrations of each element for all sources and the in-stream samples. If the minimum or the maximum concentration of any element in the in-stream sediment was higher or lower than the ones in the sources, the element was removed from the input data.

Fig. 5
figure 5

a Relative contribution of the three major litho-tectonic units (sedimentary, ophiolitic and crystalline nappes) on the composition of the material at the sites Lan-10, Lan-5 and Lan-1. The composition has been determined for the silt fraction, and the relative contribution of these litho-tectonic units on the bulk composition of the material is based on the results of the composition modelling (results of model run 2 of Table 5). b Results of mixing modelling, where the material derived between the sites Lan-10 and Lan-5 has been assigned a composition made up of 100% of sedimentary constituents. The relative contribution of the various segments on the downstream changes of the material composition has been iteratively changed until the calculated compositions correspond to the measured ones. DEM ©swisstopo

The non-parametric Kruskal–Wallis H-test, which does not require a Gaussian data distribution, identifies single tracer elements that do not show significant differences amongst two or more of the sources (e.g. Collins and Walling 2002). Elements that do not pass the Kruskal–Wallis H-test (at p values > 0.05) and that do not provide discrimination amongst sources should be excluded from the mixing model. Because the Kruskal–Wallis H-test only tests single elements, the stepwise linear discriminant analysis is used in addition to identify pairings of elements that together provide the largest end-member discrimination based on the minimization of Wilk’s lambda (e.g. Collins and Walling 2002, Collins et al. 2012; Palazón et al. 2015). All tests were performed in R, version 3.5.

Finally, the relative contribution of material from tributary basins to the trunk stream at the sites Lan-1, Lan-5, and Lan-10 were estimated using a simplified end-member mixing model (Fig. 5b; see also Savi et al. 2014). We thus assigned relative abundances, x and y where x + y = 1, to the contribution of material from upstream segments and estimated the compositions C of the sedimentary, ophiolitic and crystalline constituents farther downstream at the sites Lan-1 and Lan-5. For these calculations, we employed the measured concentrations Cmeasured of the three constituents (sedimentary, crystalline, and ophiolitic, expressed as relative contribution) at the sites Lan-5 and Lan-10. We assigned a relative abundance of 100% of sedimentary material to the material derived from the tributary basins C(trib) between Lan-10 and Lan-1, because the bedrock of the area of the Landquart catchment downstream of location Lan-10 is almost entirely composed of (meta)sedimentary rocks and flysch units (Fig. 2). This then leads to the following end-member mixing equations:

$$ C({\text{Lan-}}1) = {\text{x}}\left[ {C_{measured} ({\text{Lan-}}5)} \right] + {\text{y}}\left[ {C({\text{trib}}\;{\text{between}}\;{\text{Lan-}}5\;{\text{and}}\;{\text{Lan-}}1)} \right], $$
(1a)
$$ C({\text{Lan-}}1) = {\text{x}}[C_{measured} ({\text{Lan}}10)] + {\text{y}}[C({\text{trib}}\;{\text{between}}\;{\text{Lan-}}10\;{\text{and}}\;{\text{Lan-}}1)], $$
(1b)
$$ C({\text{Lan-}}5) = {\text{x[}}C_{measured} ({\text{Lan}}10) ]+ {\text{y}}[C({\text{trib}}\;{\text{between}}\;{\text{Lan-}}10\;{\text{and}}\;{\text{Lan-}}5)]. $$
(1c)

We iterated these calculations until the calculated, or alternatively theoretical concentrations C(Lan-1) and C(Lan-5) corresponded to the measured ones Cmeasured(Lan-1) and Cmeasured(Lan-5) at these sites. As an illustration, the composition at Lan-1 comprises 72% sedimentary particles, 7% ophiolitic fragments and 21% crystalline constituents. Such a composition can be achieved through a 50–70% contribution of material from tributary basins, which contain 100% of sedimentary material (tributary basins between Lan-1 and Lan-5), and a 30–50% contribution of sediment from Lan-5 where sedimentary, ophiolitic and crystalline constituents make up 37%, 32% and 31% of the total composition, respectively.

3.3 Topographic variables

An undisturbed river exhibits a concave-up shaped river profile along the entire channel length. However, processes such as rock uplift, glacial sculpting, lithologic contacts, landslide dams and orographic rainfall can disturb the idealized concave shaped river profile (Whipple and Tucker 1999; Korup and Montgomery 2008; Schlunegger et al. 2011; Walsh et al. 2012). A river is forming a steep segment, referred to as knickzone, along its channel profile upon adjusting to these disturbances. These knickzones then propagate upstream after a disturbance, thereby separating a re-adjusted landscape downstream of the knickzone from an upstream segment that still records the landscape properties prior to the perturbation. In our case, the change form the LGM c. 20,000 years ago to the Holocene represents such a perturbation and conditioned the erosional mechanisms and landscape forms during the Holocene (Salcher et al. 2014). We expect that the erosional processes have adjusted the landscape after glacial retreat through headward erosion, where the knickzones are predicted to have shifted farther upstream and where the related distances most likely depend on the erosion rates.

Knickzones are generally identified from longitudinal stream profiles, which can be characterized through Flint’s relationships (Flint 1974):

$$ S = k_{s} \times A^{ - \theta } . $$
(2)

Here, S is the local slope, A corresponds to the upstream area, and θ and ks denote the concavity and steepness index, respectively. In order to compare different basins with each other, it has proven convenient to normalize the steepness index with a constant concavity value of 0.45 (Wobus et al. 2006). This approach removes a possible bias introduced particularly by differences in the upstream size of a drainage basin. In this regard, differences in normalized steepness indices could then be used to identify variations in erosional efficiencies, conditioned by either uplift rates (Safran et al. 2005) or the litho-tectonic architecture (Chittenden et al. 2014), as the aforementioned studies have shown.

We determined the occurrences of knickzones along the thalwegs of the tributary and trunk streams on longitudinal stream profiles. We verified these locations on aerial photographs, in the field and on topographic maps. Topographic profiles along streams were extracted from a 10-m-resolution DEM resampled from the 2-m-resolution LIDAR DEM provided by Swisstopo. We then calculated the regression line within a Log(S) − Log(A) plot to quantify the normalized steepness ksn indices by setting the concavity θ index to 0.45 (e.g., Wobus et al. 2006). We finally calculated the normalized steepness index separately for the stream segments above and below these knickzones where the data on the Log(S) − Log(A) show clear correlations. To do so, we used the river gradient derived from the 10-m-resolution DEM together with the calculated drainage area for each river nodes, thereby limiting our analyses to > 1-km2 drainage areas. We expect that within individual basins, normalized steepness values ksn are higher downstream of the knickzones were erosion rates have supposedly been enhanced than in their headwaters (e.g., Chittenden et al. 2014; Vanacker et al. 2015). We then calculated both the horizontal and vertical relative propagation of the knickzones from the trunk channel toward the interfluves. Respective values are calculated as the ratio between the horizontal (or vertical) propagation distance of the knickzones and the total tributary length (or relief).

4 Results

4.1 10Be derived denudation rates

The 10Be concentrations, which we have measured in the seven samples, range from 1.33 ± 0.12 × 104 to 3.97 ± 0.29 × 104 atoms g−1 (Table 1). The resulting catchment-wide denudation rates vary between 0.33 ± 0.07 mm a−1 (Lan-11) and 1.26 ± 0.26 mm a−1 (Lan-12) (Table 2). They are in the same range as the denudation rates measured in the Eastern Alps (Norton et al. 2010a, 2011; Cruz Nunes et al. 2015) or the Central European Alps (Wittmann et al. 2007; Stutenbecker et al. 2018). The related minimum apparent ages, which correspond to the residence time of rock within the uppermost 60 cm where most nuclides are produced (e.g. von Blanckenburg 2005), range between c. 600 and 2300 a.

4.2 Provenance tracing and mixing modelling

Tables 3 and 4 present the results of the ICP–MS analysis. Table 3 displays the contents of different major element oxides in weight percentage, while Table 4 illustrates the results for the trace elements as well as Cr2O3 and MnO, which we report in parts per million (ppm) due to their low concentrations.

The ICP-MS analysis reveals that all sediment-derived samples (Lan-2, 3, 4, 6, 7, 8, and 9) have much higher contents of CaO and Sr than the samples derived from the crystalline and ophiolitic basins. The material encountered in Lan-11, which is derived from an ophiolitic basin, is characterized by its very high content of Fe2O3, MgO, Cr2O3 and Ni. Lan-12 and 13, both of which are sourced from crystalline basins, show relatively high contents of SiO2, Al2O3, Na2O, MnO, Sc, Y and Nb.

The ICP-MS results of sample Lan-1, 5 and 10 from the trunk channel can be characterized by two major observations. First, compared to the samples derived from sediment-type lithologies, they have elevated contents of Na2O and Cr2O3, while the concentration of these two oxides decreases between sites Lan-10 and Lan-1. The second observation is the relatively high concentration of CaO and Sr compared to the samples derived from basins made up of crystalline and ophiolitic lithologies. Here the related concentrations in the stream sediments increase between sites Lan-10 and Lan-1.

The biplot of the ICP-MS analysis in Fig. 4 yields three clusters. The first cluster contains the sample Lan-11 sourced in the basin that hosts ophiolitic bedrock. The material collected at Lan-11 is characterized by high concentrations of MgO, Cr2O3, Fe2O3 and Ni. The samples from the sedimentary basins (Lan2, 3, 4, 6, 7, 8 and 9) generally plot on the left side of the biplot and are dominated by the components CaO and Sr. There is no detectable compositional difference between sediments derived from ‘Bündnerschiefer’ basins (Lan-2, 3 and 4) and North Penninic flysch basins (Lan-6, 7, 8 and 9), which is why these basins will be treated as one compositional end-member throughout the following sections. The remaining samples Lan-12 and Lan-13 derived from crystalline basins plot in the upper right corner of the biplot. They are defined by the remaining components Na2O, Y, P2O5, MnO, Sc, TiO2 and Zr.

The range test confirmed that all element concentrations in the in-stream samples were within the range of the three source end-members. None of the elements passed the Kruskal–Wallis-H-test, which is probably due to the low number of samples for the ophiolitic (n = 1) and the crystalline (n = 2) end-member. However, the stepwise selection algorithm suggested a combination of four tracers (Na2O, Ni, Sr and Sc) to provide sufficient end-member discrimination. Sherriff et al. (2015) showed that mixing model accuracy can be improved by maximizing the number of tracers rather than minimizing them through a stepwise selection algorithm. Accordingly, we decided to run the mixing model twice, once with all available elements (run 1) and once with the four selected elements Na2O, Ni, Sr and Sc as input tracers (run 2). The relative contributions of the three end-member sources as well as the respective model performance of both runs are displayed in Table 5. The two model runs differ mostly with regard to the ophiolitic contribution, which was calculated to be higher in the first model run. However, we prefer the mixing model solution of the second run characterized by a much better goodness of fit (GOF, Table 5).

Table 5 Relative contributions (and uncertainty expressed as the standard deviation) of the three end member sources in the catchment to the three in-stream locations Lan-1, Lan-5 and Lan-10 (see Fig. 2)

The relative contribution of sediment derived from the three litho-tectonic units is illustrated in the pie charts of Fig. 5a for each trunk stream sample location (Lan-1, Lan-5 and Lan-10, results of model run 2, Table 5). At site Lan-10, 42 ± 16% of the sediment originates from tributaries draining the area composed of crystalline rocks. The basins situated in sedimentary bedrock rock upstream of location Lan-10 deliver 32 ± 10% of the material, while the basin made up of ophiolitic lithologies contributes 26 ± 11% to the bulk composition of the material at site Lan-10. At location Lan-5, the trunk stream sediment consists of 30 ± 12% crystalline, 32 ± 8% ophiolitic and 37 ± 8% sedimentary material (Fig. 5a). Therefore, the ophiolitic constituents remain constant in a relative sense, and the decrease of crystalline material is compensated by a corresponding increase in sedimentary material. At the outlet of the Landquart stream, the relative abundances of crystalline and ophiolitic constituents are significantly lower than at site Lan-5. In particular, at this lowermost site Lan-1, the sediment leaving the Landquart basin consists of 21 ± 8% of crystalline, 7 ± 7% of ophiolitic and 72 ± 7% of sedimentary particles (Fig. 5a).

4.3 Sediment budgeting

The three in-stream sample locations Lan-1, 5 and 10 define the three sub-catchments illustrated in the mixing model of Fig. 5a. The three pie charts show the relative amount of sediment supplied from the three litho-tectonic units to the in-stream sample locations Lan-1, 5 and 10. The results of the mixing model then base on the change of the sediment composition from Lan-10 downstream to Lan-5, and finally to Lan-1 (Fig. 5b). Every factor is normalized to its corresponding sub-catchment area (see methods where x + y=1). At the sample location Lan-1, two cases are possible (Fig. 5b). The mixing model suggests that either 40–50% of the sediment originates from upstream of location Lan-10 and 50–60% downstream of location Lan-10, or alternatively 30–50% arrives from upstream of location Lan-5 and 50–70% downstream of location Lan-5. The third case shows that at the sample location Lan-5, 70–90% of the sediment originates from upstream of location Lan-10 and 10–30% from downstream of location Lan-10. Please note that these budget values only yield first-order approximations based on the silt fraction and hence on the suspension loads of one sample survey only. Accordingly, they have to be treated with caution. Nevertheless, the values yield a distinct picture where a large fraction of the material has been supplied by the tributary basins situated in the downstream segment of the Landquart drainage basin. The relatively high material contribution from this lower region is independently supported by 10Be-based sediment budgets measured on in situ quartz extracted from the sand fraction and thus from the bedload. The corresponding sediment budget is presented in the next section.

Annual sediment fluxes were calculated from the mean denudation rates without any error propagation. Hence, they represent estimates only that are shown here as rounded on 10,000 m3 a−1 for a better overview (Table 6). The average denudation rate from the entire basin of 1.13 mm a−1 yields a total sediment flux of 700,000 m3 a−1. This value can be compared with the actual suspended sediment concentrations measured at the BAFU station Landquart-Felsenbach (Schlunegger and Hinderer 2003; Hinderer et al. 2013). There, the annual concentration ranges from 159,000 to 3,450,000 tons between 1994 and 2003 (on average ca. 900,000 tons a−1). If the ca. 700,000 m3 derived from the cosmo data is converted into tons (using a density of 2700 kg/m3), then the cosmo-based flux is ca. 1,890,000 tons a−1, which is not too far off the measured values, in particular if the usual uncertainties such as grain size, sediment storage, integrating time scales and solute versus mechanical loads are considered (Hinderer et al. 2013). The cosmo-based flux estimates also reveal that the contribution of the basins upstream of the sample site Lan-10 is approximately 240,000 m3 a−1. The flux in the trunk stream remains nearly constant, or slightly decreases farther downstream to site Lan-5 (210,000 m3 a−1). This decrease more likely reflects the large uncertainties (10-30%) that are associated with this methodology rather than the consequence of in-channel storage of material, for which there is no evidence in the field. Nevertheless, this suggests that a large budgetary contribution of > 400,000 m3 a−1 (based on cosmo data and a density of 2700 kg m−3) has to be inferred for the lowermost tributary basins of the Landquart River, which amounts to c. 70% of the total sediment flux while it represents < 30% of the entire basin drainage area. The lowermost tributary basins can thus be considered as the most important erosional hotspot in the region. The second most significant sediment source is situated in the catchment upstream of the sampling site Lan-12 in the SE of the Landquart basin. This basin produces approximately 140,000 m3 a−1 of sediment (Table 6) corresponding to 20–30% of the total sediment flux.

Table 6 Sediment budget based on the results of 10Be-based denudation rates

4.4 Topographic variables

The shape of river profiles of each tributary basin is characterized by the location of a major knickzone, together with the normalized steepness values (Fig. 6). The knickzones of the Taschinasbach, Schraubbach, and Furner Bach are located in the upper part of the individual catchments with a relative knickzone propagation distance in the order of c. 70–90% (Fig. 6, Table 7). Alternatively the knickzones of the Schanielabach, Schlappinbach, Verstanclabach, Vernelabach and Stützback are situated close to the confluence with the trunk channel of the Landquart River, i.e. with relative knickzone propagation values in the order of 10–30%. Interestingly, the situation for the Arieschbach appears intermediate, with a relative knickzone propagation in the order of 60%. Furthermore, no remarkable knickzones are present in the Schranggabach (Fig. 6), which suggests that a possible knickzone might have propagated through the entire drainage basin up to the headwaters. An analysis of the normalized steepness indices reveals that within the individual basins, the ksn values are systematically larger in the downstream reaches than above the identified knickzones (Fig. 6, Table 7). ksn above the knickzones yield values < 150 m0.9 while downstream reaches yield ksn values > c. 200 m0.9. At the scale of individual tributaries, ksn values are thus increasing by a factor ranging from 1.3 to 3.7 between the upper and the lower segments.

Fig. 6
figure 6figure 6

Longitudinal stream profiles of tributary basins and corresponding normalized steepness values. The two numbers next to the knickzones (KZ) indicate the relative KZ distance propagation (distance towards upstream, first number) and the relative KZ relief propagation (relative vertical propagation, second number). Please refer to Table 7 for dataset

Table 7 Normalized steepness ksn values of tributary basins and extent to which the knickzones have propagated toward the headwaters

Once mapped, the knickzones particularly of the Taschinasbach and Schraubbach are situated at the boundary between the Penninic and Austroalpine cover nappes in the hangingwall, and the Flysch units in the footwall (Fig. 7). Because the limestone suites of the Austroalpine und Penninic limestones display much lower erodibilities than the underlying Flysch units, the location of the knickzones at the tectonic boundaries are likely to be conditioned by the contrasts in the erosional resistance between these litho-tectonic units.

Fig. 7
figure 7

Simplified litho-tectonic framework of the Landquart drainage basin, location of knickzones along the various tributary basins and the longitudinal stream profiles of selected basins

5 Discussion

5.1 Landscape metrics disclose differences in erosion rates

The landscape of the Swiss Alps is still adjusting to the perturbation of the last glaciation, which is expressed by upstream migrating knickzones in the tributary channels but also in the trunk channel. This has been documented at the scale of individual drainage basins (e.g., Chittenden et al. 2014) and at that of the entire Alps (Salcher et al. 2014) through the analysis of longitudinal stream profiles of streams, and it has also been confirmed through the mapping of knickzones across the Central Alps (Norton et al. 2010b). These mechanisms at work can also be observed in the Landquart basin if the locations of the knickzones are considered (Fig. 7). The sections of the catchments located above the knickzones are characterized by a flattened and less steep topography, multiple bedrock steps along the thalwegs, and U-shaped cross-sectional valley geometries at several locations, all of which are indicative of a glacial landscape (Whipple et al. 1999). Below the knickzones the occurrence of deeply concave-upward incised channels and V-shaped valley geometries suggests that the streams have rejuvenated the landscapes by fluvial erosion and associated hillslope processes. This interpretation of fluvial adjustment, most likely through fast erosion, is also supported by the morphometric data where within individual basins, the normalized steepness values are generally larger in the rejuvenated downstream reaches compared to the river segments above the knickzones (Whipple et al. 1999; Norton et al. 2010b). In addition, Abbühl et al. (2011) argued that the celerity of knickzone retreat is positively correlated to the rate at which denudation operates within a basin. In this context, the knickzones of the Taschinasbach, Schraubbach, Furner Bach and to a less degree of the Arieschbach have propagated close to their headwaters, or have already propagated through the entire basin (Schranggabach). This suggests that a large portion of these basins has already rejuvenated since the termination of the Last Glacial Maximum c. 20 ka ago. Contrariwise, the knickzones of the basins father to the SE are still situated close to the trunk channel (e.g., Schanielabach, Stützbach; Fig. 7). In addition, the shape of these basins, characterized by U-shaped cross-sectional geometries in some places, display features related to glacial sculpting. This suggests that these basins have to large extents preserved their original glacial topography, and that erosion in these catchments has been lower in comparison to the basins farther to the NW (downstream of site Lan-5).

5.2 Sediment budget of the Landquart basin

The sediment budget of the Landquart basin was established through two different methods. Estimates of the present day sediment fluxes were achieved using the chemical composition of the river sediment along the basin. Furthermore an average annual sediment flux over the past 600–2300 years was calculated based on the inferred 10Be-derived denudation rates. In order to compare these data in a quantitative way, the Landquart catchment was divided into three sections, defined by the sample sites Lan-1, Lan-5 and Lan-10. The results (Fig. 8) suggest that the total sediment budget of the entire Landquart basin is made up of a 60−70 ± 10% contribution derived from the lowermost segment (green colour), while 10 ± 10% and 20−30 ± 10% of the material has been derived from the middle (yellow colour) and headwater sections (red colour), respectively. We note that the uncertainties on these values are relatively high, but the budget does disclose a distinct trend regarding the provenance of the material. Accordingly, c. 50–80% of the total sediment from the Landquart basin has been derived from the lowermost part of the catchment, while the relative spatial extent of this region is only one-third of the total area of the Landquart basin. This implies that modern denudation rates in this lowermost segment are likely to be much higher compared to the rates inferred for the middle and headwater regions of the basin. This interpretation is supported by the sediment budget that is based on the denudation and sediment flux patterns derived from in situ 10Be. Indeed, these budgets suggest that most of the sediment (up to 70%, based on denudation rate estimates) has been delivered from the lowermost part of the Landquart basin, while the contribution of the headwater and middle region is much less (Fig. 8). Accordingly, both approaches yield the same patterns whereby sediment input from the lowermost portion of the Landquart basin has been relatively high. This pattern seems to have existed at least since several hundred years, which corresponds to the integration time scale of the 10Be methodology (see above).

Fig. 8
figure 8

Summary figure, showing the relative contribution of the various segments to the bulk sediment budget of the Landquart basin

5.3 The role of bedrock erodibility

In the lowermost part of the Landquart basin, the bedrock mainly consists of ‘Bündnerschiefer’ and North Penninic Flysch with high bedrock erodibilities (Kühni and Pfiffner 2001). Here the Penninic units reach the surface in a tectonic window referred to as the ‘Prättigau half-window’ (Weh and Froitzheim 2001). Korup and Schlunegger (2009) claimed that mechanically weak bedrock such as the ‘Bündnerschiefer’ and the North Penninic Flysch may have promoted erosion by fluvial dissection and landsliding. According to these authors, the accelerated erosion could be explained through a mechanism where mechanically weak bedrock may have amplified both erosion and rock uplift through a positive feedback. The sediment budget of this study supports this interpretation. Furthermore, in this part of the Landquart basin, the ‘Bündnerschiefer’ comprise the Valzeina series (Nänny 1948) where the relative abundance of shales is much higher than in the rest of the “Bündnerschiefer” and in the Flysch units. We see the consequence in our sediment budget where material fluxes from basins underlain by the ‘Bündnerschiefer’ is greater than the material contributions of drainage systems sourced within the Flysch units.

A second lithology control is seen in the longitudinal stream profiles within the Taschinasbach and Schraubbach basins, where the knickzones of these streams are located near the tectonic boundaries (Fig. 7) separating bedrock lithologies with low (Austroalpine cover nappes) and high erodibilities (‘Bündnerschiefer’ and Flysch in the footwall). We envisage a scenario where the Austroalpine cover nappes are likely to have served as cap rock with a high erosional resistance, thereby decelerating the celerity at which the knickzones propagate towards the headwaters as they approach the lithological contacts. Ongoing fluvial dissection in the lower stream segments where the bedrock is made up of Flysch and ‘Bündnerschiefer’ might have steepened the stream profiles particularly downstream of the knickzones. This possibly resulted in an increase of the curvature and the gradients of the channel profiles, and also in an amplification of the normalized steepness indices in comparison to the segments upstream of the knickzones (Fig. 6). If such a mechanism is additionally accompanied by faster rock uplift rates in the area where ‘Bündnerschiefer’ units are exposed, then a deeply dissected landscape with steep and highly curved channels and V-shaped hillslopes will form, as is the case in the lower part of the Landquart basin (see below).

It has been suggested that the eastward-directed tilt of the tectonic units has a measurable influence on the erosional pattern and the resulting landscape form of a drainage system (Cruz Nunes et al. 2015). In addition, non-dip slopes can maintain very steep hillslopes where shallow landsliding can regularly occur as suggested by e.g. Brardinoni et al. (2009) and Hassan et al. (2019). Because the exposure pattern of the bedrock does suggest the occurrence of an eastward tilt, particularly in the units of the lower part of the Landquart basin, we cannot fully exclude the possibility that such a scenario does have an influence on the erosional mass flux. If it does, then it will not modify the picture proposing that an erosional hotspot is located in the lower part of the Landquart basin with elevated long-term exhumation rates and fast modern rock uplift.

As a final mechanism, it is possible that recycling of previously deposited terrace sediments could contribute to the erosional flux patterns observed in the Landquart basin. We currently lack the required quantitative dataset to test this hypothesis. However, field inspections showed that terrace deposits are more frequent in the upstream part of the Landquart basin where the relative contribution of material to the sediment budget is low. Accordingly, we do not consider the possibility that a possible recycling of previously deposited material will weaken our statement that high sediment production in the downstream part of the Landquart basin is the result of active downcutting where denudation rates are much higher than in the upstream part.

5.4 Possible controls of uplift on the denudation pattern

As discussed above, the lower part of the Landquart basin can be considered as an erosional hotspot where most of the sediment has been derived from (Fig. 8). In this lower part, the knickzones of the tributary streams have propagated close to the headwaters, and the landscape downstream of these knickzones has adapted V-shaped cross-sectional geometries with steep slopes. This is different from the shape of the tributary catchments in the middle and headwater segments of the Landquart basin where sediment supply has been relatively low, where the characteristic glacially scoured landscape remains, and where multiple bedrock steps along the thalwegs are well preserved. Also in these basins, the knickzones are still located close to the confluence with the trunk stream, thus supporting the inferred lower denudation and incision rates. Interestingly, the geomorphologically very active lowermost zone lies exactly within the Prättigau half-window, which could have formed in response to the updoming of the basement units underlying the Chur area at greater depths (Fig. 3). Based on the pattern of apatite fission track ages in the region, Weh (1998), Vernon et al. (2008) and Fox et al. (2016) proposed that this phase of updoming may have started c. 4–5 Ma ago and would have resulted in the fast exhumation of ‘Bündnerschiefer’ and Flysch units that are underlying the Austroalpine and Penninic cover nappes. Geodetic surveys (Kahle et al. 1997; Schlatter et al. 2005) have disclosed that the Chur area has experienced the fastest uplift of the region during the past decades, suggesting that advection of crustal material to the surface is still ongoing. We use these observations to propose a mechanism whereby the occurrence of an erosional hotspot in the lower part of the Landquart basin can be understood as a combined effect of uplift and the exposure of bedrock with lower erosional resistance. In such a scenario, updoming and fast rock uplift have resulted in the formation of the Prättigau half-window, thereby exposing Flysch and particularly ‘Bündnerschiefer’ units with high erodibilities to the surface. A possible positive feedback between rock uplift and erosional unloading could have contributed to the amplification of both processes (Korup and Schlunegger 2009). In such a scenario, the Austroalpine and Penninic cover nappes, delineating the eastern boundary of this erosional hotspot, have most likely operated as cap rock, thereby retarding the celerity at which the knickzones have migrated towards the headwaters. The combination of a cap rock with high erosional resistance in the headwaters together with the exposure of highly erodible lithologies farther downstream resulted in a landscape where (1) channels have a high steepness, (2) hillslopes are V-shaped and where (3) sediment fluxes are large. The occurrence of high rock uplift rates in the region surrounding Chur where ‘Bündnerschiefer’ and Flysch are exposed could then reflect a positive feedback response of uplift to fast erosion (Korup and Schlunegger 2009). It thus appears that these conditions have likely prevailed during the past millions of years and could have started when Penninic and Austroalpine cap rocks were removed, thereby giving way to the exposure of highly erodible ‘Bündnerschiefer’ and Flysch lithologies to the surface.

6 Summary and conclusion

The sediment budget presented in this study suggests the occurrence of a positive feedback mechanism between erosion and rock uplift in the lower part of the Landquart basin, eastern Swiss Alps, where bedrock with high erodibilities are exposed. The local topography shows that the upstream part of the Landquart basin, made up of bedrock lithologies resilient to erosional processes, still preserves most of the glacial imprints, while the landscape in the downstream segment where highly erodible ‘Bündnerschiefer’ and Flysch lithologies are predominant, is in a more mature state with respect to the Holocene climate conditions and dominated by fluvial dissection. The measured denudation pattern and the sediment provenance support the observed trends in the landscape. The main part of the fluvial sediment in the Landquart catchment has been derived from the downstream part of the basin. As a first observation, the sediment budget and the erosional pattern of the Landquart basin therefore appear to be strongly influenced by the patterns of the exposed lithologies. As a second major observation, we find that the inferred erosional hotspot in this region is located within the Chur area that is currently affected by high rock uplift rates. This region has additionally been characterized by high exhumation rates, as indicated by some of the youngest apatite fission track ages in the Alps. Based on these findings, we suggest that: (1) this uplift is a long-lived signal and could have been amplified by higher erosion rates in this window, conditioned by the strong erodibility of the exposed lithologies, and that (2) the Austroalpine cover nappe could have operated as cap rock, thereby maintaining a steep morphology farther downstream where fast erosion proceeds. Accordingly, this part of the European Alps offers a nice example where mechanically weak bedrock may have amplified both erosion and rock uplift through a long lasting yet ongoing positive feedback.

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Acknowledgements

Financial support to pay the costs associated with the cosmo and geochemical analysis has been offered by the Swiss National Science Foundation (SNF Project 147689 awarded to Schlunegger). The very constructive comments and suggestions by two anonymous reviewers and A. Pfiffner greatly improved the science of this article. Additional very constructive comments by the editor S. Schmid are greatly acknowledged.

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Glaus, G., Delunel, R., Stutenbecker, L. et al. Differential erosion and sediment fluxes in the Landquart basin and possible relationships to lithology and tectonic controls. Swiss J Geosci 112, 453–473 (2019). https://doi.org/10.1007/s00015-019-00344-3

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