Following the last glacial maximum (LGM), the demise of continental ice sheets induced crustal rebound in tectonically stable regions of North America and Scandinavia that is still ongoing. Unlike the ice sheets, the Alpine ice cap developed in an orogen where the measured uplift is potentially attributed to tectonic shortening, lithospheric delamination and unloading due to deglaciation and erosion. Here we show that ∼90% of the geodetically measured rock uplift in the Alps can be explained by the Earth’s viscoelastic response to LGM deglaciation. We modelled rock uplift by reconstructing the Alpine ice cap, while accounting for postglacial erosion, sediment deposition and spatial variations in lithospheric rigidity. Clusters of excessive uplift in the Rhône Valley and in the Eastern Alps delineate regions potentially affected by mantle processes, crustal heterogeneity and active tectonics. Our study shows that even small LGM ice caps can dominate present-day rock uplift in tectonically active regions.
Recent vertical movements of the Earth’s crust are mostly due to tectonic deformation along plate boundaries, volcanism and changes in crustal loading from water, ice and sediments1. The decay of continental ice sheets caused uplift of the formerly glaciated regions and was the primary cause for the Holocene eustatic sea level rise, which is one of the main concerns of the impacts of global warming on coastal communities worldwide2. Changes in the ice load of tectonically active mountain ranges, such as the Alps, the Alaska Range or the Himalaya, although much smaller, nevertheless trigger an isostatic response. The induced surface uplift and/or subsidence is thought to have caused changes in fluvial networks3, and the resulting stress changes in the Earth’s crust can influence crustal deformation and seismicity4 and might have triggered some of the largest intraplate earthquakes since last glacial maximum (LGM) deglaciation5. The key controls on how the Earth responds to changes in crustal loading are the viscosity of the upper mantle and the lithospheric effective elastic thickness (EET)—a geometric measure of the flexural rigidity of the lithosphere, which describes the resistance to bending under the application of vertical loads1. Most previous estimates of mantle viscosity come from old and tectonically stable continents, where the vertical motion can almost entirely be attributed to postglacial rebound6. In contrast, the complexity of the uplift signal in tectonically active orogens requires the relative contribution of different potential driving mechanisms to be disentangled.
For half a century, the cause for recent uplift of the European Alps has been debated. Possible drivers of uplift include postglacial rebound7, erosional unloading8, tectonic deformation9, lithospheric slab dynamics10 and combinations thereof (Fig. 1). Some of these processes, such as lithospheric delamination, manifest themselves on timescales of ∼106–107 years, whereas others, such as postglacial rebound, occur relatively rapidly (∼103 years). New approaches to modelling orogen-scale sediment storage11, glaciation12 and spatial variations in EET (ref. 13) provide new constraints for estimating the contribution of glacial isostatic adjustment (GIA) to present-day uplift rates in the European Alps.
Mountain building in the European Alps is due to the convergence of Africa and Eurasia beginning in the Mesozoic with continental collision culminating in the Eo-Oligocene14. A late phase of outward tectonic growth in the Early Miocene created the Jura Mountains and thrusting of the Swiss Plateau14 (Fig. 2). Further tectonic shortening was accompanied by eastward extrusion of the Eastern Alps and exhumation of metamorphic domes in the Central Alps15. The cessation of outward tectonic expansion of the Western and Central Alps during the Late Miocene might reflect an increase in the ratio of erosional to accretionary material flux and the onset of orogenic decay16. During the Pleistocene, the Alps were repeatedly glaciated with ice caps that covered almost the entire mountain belt and substantial parts of the northern foreland17. Locally, glaciation was presumably associated with a twofold increase in exhumation rates18,19 and topographic relief20, which may be controlled by feedbacks between glacial erosion, crustal unloading, isostatic uplift and deep-seated processes.
Permanent global positioning system (GPS) stations indicate ongoing crustal convergence of 1–2 mm yr−1 across the Eastern Alps (Fig. 2) that is controlled by the counterclockwise rotation of the Adriatic plate21. The convergence is accommodated by thrusting in the Italian Friuli and Lombardy regions and by eastward extrusion along strike-slip faults15,21. In the Central and Western Alps, however, only minor or no crustal shortening can be detected22 and earthquake focal plane solutions are dominated by extensional and strike-slip mechanisms (Fig. 2).
In this study, we re-evaluate the effect of GIA on the present-day rock uplift in the Alps while accounting for postglacial erosion, sediment deposition and variations in lithospheric strength. We show that most of the postglacially eroded material was trapped within the mountain belt and did not contribute to erosional unloading as previously suggested8. Instead our results demonstrate that the long-wavelength uplift signal is best explained by the Earth’s viscoelastic response to ice unloading after the LGM. We conclude that present-day uplift rates in other tectonically active and glaciated mountain belts could also carry a component related to LGM deglaciation.
Alpine valley fills and postglacial erosion
Among the most prominent features of the Alpine landscape are overdeepened valleys that were carved by glaciers and are now partially buried by thick sedimentary deposits. The isostatic adjustment to deglaciation was likely attenuated by the postglacial accumulation of sediments in these valleys8. We used an artificial neural network (ANN) algorithm11 to estimate the sediment thickness within all Alpine valleys (see ‘Methods’ section; Fig. 3a). Our estimates agree well with fill thicknesses observed in boreholes or estimated from seismic and gravimetric surveys (Supplementary Table 1), and they yield consistently similar or higher thicknesses where boreholes did not reach bedrock (Fig. 3c). Very shallow valley fills (<200 m) show the largest relative discrepancies, which can be attributed to distances between observation sites and valley walls that are smaller than the spatial resolution of the model (90 m). Compared with an independent sediment-thickness reconstruction at much higher spatial resolution (10 m) in the region around Bern23 our reconstruction yields a fill volume of 29 km3, which is ∼20% higher than the previous estimate of 24 km3, and thus reasonably consistent when considering the differences in spatial resolution. According to our estimate, the total volume of valley-filling sediments is 1,800±202 km3. This volume is a minimum bound on postglacial erosion; yet it is likely only a small underestimate because a large fraction of all postglacially eroded material was trapped in a closed system of overdeepened valleys and marginal lake basins24. To account for dissolved fluxes and for catchments that were only temporarily closed, we added another 10% to our volume estimate24, resulting in 1,980±222 km3 of material eroded after deglaciation. Assuming mean densities of 2,000 kg m−3 for unconsolidated sediments and 2,700 kg m−3 for bedrock, we computed a total eroded mass of ∼4 × 103 Gt. Evenly distributed over the Alps (∼123,000 km2, excluding valley-fill areas) this volume corresponds to a rock column of 11.9±1.3 m. With the assumption that the valley fills have formed following ice retreat ∼17 kyr before the present (BP) (ref. 24), this eroded column corresponds to a mean postglacial denudation rate of 0.7±0.08 mm yr−1. To create a mass-conserving topographic basis for modelling the Alpine ice cap, we redistributed the calculated sediment volume catchment-wise and as a power-law function of local relief25 back onto the hillslopes (Fig. 3b). Our valley fill-derived erosion rates from six lake-bordered catchments are comparable to or somewhat higher than erosion rates estimated from modern river loads26, cosmogenic nuclides27,28,29 and thermochronology18 (Fig. 3d). Furthermore, because there might be also older sediments that predate the LGM30 incorporated in our valley-fill estimate, our estimate of postglacial erosion and sediment redistribution is at the upper limit of probable values.
Reconstructing the LGM ice cap
Based on mapped ice extent and thickness indicators, such as terminal moraines31 and trimline elevations32,33,34, we reconstructed the LGM ice cover using a numerical ice-flow model12. Because it is not our aim to derive paleoclimatic conditions during the LGM, we used modern precipitation maps and an Alpine-wide average glacial mass-balance profile together with an iteratively adjusted equilibrium-line altitude to fit the observations (see ‘Methods’ section). The steady-state LGM ice cap, which best fits available ice-extent indicators (Fig. 4) has a mean and a maximum ice thickness of 415 and 2,445 m, respectively. The maximum ice thickness is higher than previously reported values of ∼2,000 m (refs 32, 34) due to our removal of thick post-LGM valley fills from the underlying topography. When compared with the existing reconstruction of the LGM ice cover in the Central Alps35 (V=25,000 km3), our modelled ice volume is only ∼8% larger (27,000 km3), which has negligible effects on our final results. The total reconstructed ice mass is 62 × 103 Gt, which is ∼16 times the mass of the postglacially eroded sediments.
The LGM Alpine ice cap started growing before 30 kyr BP and reached its maximum ∼21 kyr BP, followed by rapid deglaciation with ∼80% ice loss over the course of 3 kyr (ref. 36). This chronology is consistent with the dated onset of marginal lake formation, which indicates ice retreat to the mountain interior at 16–18 kyr BP (ref. 24). Because durations of ice-cap growth are long (>10 kyr) compared with maximum expected viscoelastic relaxation times of 3–6 kyr6, we assume that the Alpine ice cap reached full isostatic compensation. We calculated the lithospheric equilibrium deflection37, due to the ice loading, while accounting for a variable EET13. Although relative spatial variations in EET are well constrained13, the absolute values are not, because they strongly depend on the assumed rheology and geothermal gradient. For the Alps, a range of 10–50 km has been reported in previous studies1. Therefore, we solve for a range of possible average EETs while maintaining the spatial pattern (see ‘Methods’ section). An increase of the EET results in a smaller amplitude but a larger wavelength of the deflection, which approximately follows the ice extent. With an EET of 10 km (70 km), the maximum depression is 279 m (105 m) near the centre of the ice cap and the elevated forebulge has a height of 7 m (3 m), (Supplementary Fig. 1). The effect of spatial variations of the EET on the deflection decreases with an increasing average EET. Compared with the flexural pattern that results from a constant EET of 70 km, the deflection using a variable EET of 61–80 km is up to 2 m higher in the centre, and 1.5 m lower at the periphery (Supplementary Fig. 2). Because the EET only reflects the flexural properties of the lithosphere, it does not account for deeper-seated processes, which potentially modulate the isostatic response to loading and unloading. We address these aspects in the ‘Discussion’ section.
Due to the relatively small dimensions of the Alpine ice cap, the upper mantle viscosity determines isostatic uplift and relaxation rates. For a range of mantle viscosities of 1019–1021 Pa s, we calculated the corresponding uplift rates associated with deglaciation, which we assume to have occurred at 17±2 kyr BP (see above paragraph on postglacial erosion). To account for the isostatic component related to erosional unloading, we calculated the lithospheric response to the estimated erosion/deposition for average EETs of 10–70 km, assuming that the erosional mass redistribution is compensated by the mantle at a steady rate. We finally compared the combined uplift signal of GIA and erosional unloading with measurements obtained from precise levelling38,39,40, which were adjusted to a common reference frame using data from permanent GPS stations41 (see ‘Methods’ section).
With an average EET of 50 km and an upper mantle viscosity of 2.2±0.5 × 1020 Pa s, we are able to reproduce virtually all of the geodetically measured uplift with ∼90% of this uplift caused by deglaciation and only ∼10% by erosional unloading (Fig. 5f). Comparison with independent measurements from the French Alps42 shows that 70% of the observed uplift rates are near the model-predicted values (Fig. 5f). The derived viscosity is reasonable, as it is lower than the viscosity estimated for an old craton (3–10 × 1020 Pa s, Fennoscandia), but higher than that for a region with recent crustal thinning (0.18 × 1020 Pa s, Basin and Range province, Supplementary Table 2). For illustrative purposes, we repeated our calculation assuming that 90% of the postglacially eroded material has been exported from the Alps. Similar to our previous results, the best fit with the data is achieved with an EET of 50 km and an upper mantle viscosity of 1.8 × 1020 Pa s, whereas the erosional contribution to the total uplift rates increases to a maximum of 35% (Supplementary Fig. 3).
It has been argued that the geodetically measured uplift of the Alps is dominated by its isostatic response to erosional unloading8, which is supposed to have increased threefold from Pliocene to Quaternary times43, although some of this increase may be an artefact of incomplete preservation of older deposits44,45. Several thermochronometric studies point to an increase in exhumation rates of similar magnitude over the last 2 Ma, which has been attributed to a positive feedback between glacial incision, isostatic rebound, rock uplift and exhumation rates18,19,20. However, we argue that much of the material eroded from the Alps since deglaciation was deposited within Alpine valleys and therefore does not contribute to erosional unloading. Our models show that the LGM ice load (∼62 × 103 Gt) was much larger than postglacially eroded sediments (∼4 × 103 Gt) and suggest the dominance of ice melting over erosional unloading in contributing to the total recent uplift rate. Furthermore, erosion rate estimates based on our valley-fill volumes exceed long-term rates based on thermochronology (Fig. 3d). This could be explained by a peak in erosion rates at the onset of deglaciation due to intensified paraglacial processes that can be expected for a landscape that is adjusting to new boundary conditions. Even in the unreasonable case that 90% of the postglacially eroded material had been exported from the orogen, the erosional contribution to the recent uplift rate would not exceed 35%.
The most sensitive parameter in our modelling that is not well constrained is the average EET. A low average EET does not change the best-fit viscosity by much (1.7–2.2 × 1020 Pa s), but leads to systematically lower modelled uplift rates in the northwestern periphery of the Alps (Fig. 6a). Active tectonic shortening across this region is <1 mm yr−1 and contributes <0.2 mm yr−1 of rock uplift8. If other processes, such as lithospheric delamination10 or ongoing tectonic shortening46 were to account for some of the observed uplift in the northwest periphery of the Alps, these would have to generate the same uplift pattern as the ice unloading, which we think is rather unlikely. We therefore favour our model results with a relatively thick EET (50 km), in which ∼90% of the present-day uplift of the Alps is due to GIA. However, we acknowledge that the Alpine lithosphere has a complex architecture47 that our elastic thin-plate approach may not be able to fully account for.
For example, we observe a conspicuous cluster of residual uplift in the Swiss Rhône Valley, which is close to a zone of enhanced seismicity and may thus have a tectonic origin (Supplementary Fig. 4). Recent analysis of geodetic data in the Western Alps has revealed a narrow zone of particularly high uplift rates (1.5–2.5 mm yr−1) that exceed the combined signal of GIA and erosional unloading by up to 1.5 mm yr−1 (ref. 22) (Supplementary Fig. 4b). This excess uplift may be attributed to a contrast in crustal viscosities between the foreland and the mountains, which could enhance the isostatic response to crustal unloading48. Because the zone of high uplift coincides with a low-P-wave velocity anomaly at 100–150 km depth10 and with high Quaternary exhumation rates18, it may also (or alternatively) be related to deep-seated mantle processes that act on million-year timescales22. We thus speculate that the excess rock uplift we observe in the Swiss Rhône Valley may be linked to crustal heterogeneity, or deep-seated processes.
Because of the ongoing N–S convergence, we expect a larger tectonic contribution to the recent uplift rates in the Eastern Alps. Estimated rock uplift rates in the Tauern Window (Fig. 2) and along the eastern edge of the Alps since 4 Ma are <1 mm yr−1 (ref. 9) and 0.1–0.15 mm yr−1 (ref. 49), respectively, and thus one order of magnitude lower than geodetically observed uplift rates. Adding this tectonic component to our modelled uplift rate would in both cases improve the fit with the measurements. Therefore, the mismatch between modelled and observed uplift rates in parts of Austria could be explained by the ongoing convergence in the Eastern Alps that is related to the counterclockwise rotation of the Adriatic microplate, and by the eastward extrusion of the Eastern Alps that is associated with a complex pattern of transtensional and transpressional zones15,21(Fig. 2). We thus conclude that the recent long-wavelength uplift of the European Alps is predominantly due to GIA with a small erosional contribution of probably <10% and that observed residuals are likely due to local tectonic activity and deep-seated mantle processes.
Although the Alpine LGM ice cap was much smaller than the northern hemisphere ice sheets, the Earth’s response to its demise dominates the vertical motion over broad regions of the Alps even today. Other mountain belts that were similarly affected by glaciation, such as the Alaska Range, the Himalaya or the Southern Alps in New Zealand, might therefore also exhibit such a long-wavelength uplift component.
Estimation of valley-fill thicknesses
Based on the assumption of geometric similarity between the exposed and the buried parts of the landscape, we used an ANN algorithm11 and a 90- m-resolution digital elevation model (DEM) to explicitly estimate the depth to bedrock for grid cells that include valley fill. We expect geometric similarity of the bedrock surface, because the entire landscape was subject to glacial erosion before deposition of the valley fill. For each cell in the DEM that is part of a valley fill, the depth to bedrock is estimated from the horizontal distance to the nearest hillslope, calculated for different directions. Training and validation of the ANN was initially performed on the presently exposed topography using synthetic fills. We created a mask of all valley fills by a combination of slope thresholds and manual digitization using geological maps with a scale of 1:25,000 (https://map.geo.admin.ch) and 1:50,000 (https://www.geologie.ac.at, http://infoterre.brgm.fr, http://www.geoviewer.isprambiente.it). To calculate the eroded rock column for each cell since the LGM, we adopted the proposed relation between erosion rate (E) and mean local relief (R, determined in a window with 10 km diameter) of E=1.4 × 10−6 R1.8 (ref. 25) and multiplied this by 17,000 years. We then calculated the fractional contribution of each cell by multiplying with the rock volume derived from the valley-fill approach.
To reconstruct the Alpine ice cap during the LGM, we employed a numerical ice-flow model12 to solve the shallow ice approximation (SIA)50. The SIA simplifies ice dynamics but allows for computational efficiency at sufficiently high spatial resolution (3 km). We acknowledge that the SIA-approach may not be suitable concerning the calculation of the ice velocity and flow patterns in steep terrain. GIA, however, is ultimately controlled by the ice geometry and is insensitive to the ice velocity and flow pattern. Compared with higher-order models, only slight differences in glacier geometry are expected during steady-state51. The ice rheology is governed by Glen’s flow law, ɛij=Aτe2 τij, where ɛij are the components of the strain rate tensor, τij are the components of the deviatoric stress tensor, τe is the effective stress and A=1 × 10−16 Pa−3 yr−1. The sliding velocity us is assumed to be proportional to the basal shear stress τs, and given by: us=Asτs2 N−1. As is a sliding coefficient depending inversely on the bed roughness and N is the effective pressure at the base of the ice and set to 40% of the ice overburden pressure. In reality N would be highly variable in both space and time52 with lower values leading to increased decoupling between ice and bed, which permits faster sliding. Tests with N being 80% of the ice overburden pressure indicate only a small increase in the resulting ice volume. The surface mass balance is modelled with an accumulation/ablation gradient of 0.7 m snow water equivalent per year (100 m)−1 (ref. 53) and a spatially variable maximum accumulation rate, using the recent pattern of mean annual precipitation54 (Supplementary Fig. 5). To achieve the best match between modelled and mapped ice extent and thickness, we iteratively adjusted equilibrium line altitudes for each catchment that drains the Alps according to the areal misfit determined after each model run (Supplementary Fig. 6). This adjustment was repeated for As=25, 75, 100, 150 and 200 × 10−10 m yr−1 Pa−2. The best agreement between mapped trimline elevations32,33,34 and the modelled ice-surface was reached with As=100 × 10−10 m yr−1 Pa−2. Furthermore, we increased As stepwise within the foreland to prevent the Alpine ice cap from overtopping the Jura Mountains. Field observations clearly document that two branches of ice were flowing to the northeast and to the southwest of the Jura Mountains55. This pattern was reproduced when As in the foreland was increased by a factor of 15, which is similar to the value used in a reconstruction of the Laurentide ice sheet56. We attribute differences in the sliding coefficient between the foreland and mountain interior to deformable sediments57 and higher amounts of meltwater52, which both are likely associated with higher sliding velocities.
Flexure of the lithosphere
Because the lithospheric deflection due to glacier growth has a direct effect on the slope and elevation of the ice surface and hence on the ice flow and mass balance, we reconstructed the ice cap for uniform EETs of 20, 30, 40 and 50 km, respectively. We calculated the flexural isostatic adjustment, Wf(x,y), for every 10 model time steps (∼30 days) using the two-dimensional elastic thin-plate equation:
Here Df=YEET3/12(1−ν) denotes the flexural rigidity, where EET is the effective elastic thickness of the lithosphere, Y=100 GPa is Young’s modulus and ν=0.25 is the Poisson ratio. L(x,y)=ρigH(x,y)−ρagWf(x,y) is the vertical load where ρi=917 kg m−3 is the density of ice, H(x,y) is the ice thickness in each model cell and ρa=3,300 kg m−3 is the density of the compensating asthenosphere. The variation in total ice volume and maximum ice thickness due to an increase of the EET from 20 to 50 km is <5%. To further investigate the effect of a laterally heterogeneous lithosphere, we introduced variations in EET13, and calculated the isostatic depression due to the load of the steady-state ice cap using the algorithm gFlex37, which uses finite difference solutions for the problem of elastic plate bending under arbitrarily shaped surface loads. To account for the effect of the differences in the resulting flexural patterns on the ice geometry, we adjusted the glacier bed according to the results from gFlex and continued running the ice model to find the new steady-state ice geometry (Fig. 4). Imposing a variable EET results in 1 × 103 km3 more ice, which is small when compared with the total ice volume of 68 × 103 km3. The larger ice volume can be attributed to thicker ice (up to 160 m) in the foreland lobes.
Effective elastic thickness
EET of the lithosphere exerts a primary control on the plate’s flexural rigidity, which in turn determines the magnitude and pattern of the isostatic response. Reflecting the long-term and often complex history of the continental plate, the EET depends mostly on the combined effects of rheological and thermal heterogeneity. In this study we use EET estimates13 obtained by following the approach of ref. 58. The crustal rheology, corresponding to quartzite in the upper crust and diorite in the lower crust59, was assigned using the velocity distribution of the crustal model EuCRUST-07, which is based on integration of several hundred seismic profiles and receiver-function data60. For the mantle lithosphere, a ‘dry’ olivine rheology was used. Lithospheric temperatures were derived from the inversion of a tomographic model of seismic velocities for Europe61. The EET ranges from 14 to 27 km in the Alpine region, with overall higher values in the Eastern Alps compared with the Central and Western Alps (Supplementary Fig. 1a). However, these values reflect only a lower bound endmember, assuming a high geothermal gradient and a ‘soft’ rheology (‘dry’ quartzite and ‘wet’ diorite)13. Therefore, we modified the corresponding EET by adding 10, 20, 30, 40 and 50 km to the absolute values to account for lower geothermal gradients and a stiffer rheology. Larger values of EET than 50–70 km imply a significant contribution of the upper mantle to the rigidity of the lithosphere and are likely more representative of the Precambrian cratons than of active Phanerozoic regions like the Alps59.
The viscoelastic decay of the lithospheric deflection after removal of the surface load results in uplift at a rate u, which we calculated with an exponential decay model:
where W0 is the equilibrium deflection, τ is a characteristic timescale of relaxation and t is the time since unloading62. The timescale of relaxation is defined as:
where μ is the mantle viscosity, ρ=3,300 kg m−3 is the mantle density, g is the gravitational acceleration and λ=320 km is the wavelength of the load, which we calculated from the average transverse extent of the LGM ice cap. We used uplift rates determined by precise levelling in Switzerland38,39 and Austria40, obtained from repeated measurements of benchmarks since the beginning and the middle of the 20th century, respectively. Thus, they represent vertical velocities in relation to arbitrarily chosen reference points. The reference point for the Swiss data is located near the city of Aarburg on the Swiss Plateau and the Austrian data refer to a point near the city of Horn ∼70 km northwest of Vienna (Fig. 3a). Direct comparison of both datasets requires that the vertical velocities of the respective reference points can be determined. For this purpose, we used data from the permanent GPS stations Zimmerwald (Z) and Linz (L), which are located on the Swiss Plateau and the Bohemian Massif, respectively. Both stations provide continuous time series of ground motion from 1998to 2015 (17 yr) and from 2005 to 2013 (8 yr), with vertical velocities of 1±0.08 mm yr−1 (Z) and 0.8±0.15 mm yr−1 (L) in the global reference frame IGb08 (ref. 41). To adjust the measurements to a common reference frame we subtracted the GPS rates with the uplift rates of the nearest levelling benchmarks, which resulted in uplift of 0.94±0.08 mm yr−1 for the Swiss reference point and 1±0.15 mm yr−1 for the Austrian reference point. We inverted the adjusted uplift rates for the mantle viscosity using equation (2) with t=17±2 kyr, resulting in a viscosity of 1.4–2.8±0.5 × 1020 Pa s, depending on the assumed EET (20–50 km), with larger EETs leading to higher viscosities (Supplementary Fig. 7).
gFlex is available from Andrew Wickert’s GitHub repository at https://github.com/awickert/gFlex.
The data that support the findings of this study are available from the corresponding author upon request.
How to cite this article: Mey, J. et al. Glacial isostatic uplift of the European Alps. Nat. Commun. 7, 13382 doi: 10.1038/ncomms13382 (2016).
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This research was funded by the Potsdam Research Cluster for Georisk Analysis, Environmental Change and Sustainability (PROGRESS) through a grant of the German Federal Ministry for Education and Research (BMBF) to M.R.S., J.M. and T.F.S. acknowledge funding by the Deutsche Forschungsgemeinschaft (DFG) through Emmy Noether grant SCHI 1241/1-1 awarded to T.F.S., M.T. acknowledges Utrecht University and the Netherlands Research Centre for Integrated Solid Earth Science (ISES) for funding through grants ISES-2014-UU-08 and ISES-2016-UU-19. This work benefited from discussions with J.P. Avouac, J. Braun, M. Handy, P. van der Beek and F. von Blanckenburg. We acknowledge constructive comments by Fritz Schlunegger and two anonymous reviewers.
The authors declare no competing financial interests.
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Mey, J., Scherler, D., Wickert, A. et al. Glacial isostatic uplift of the European Alps. Nat Commun 7, 13382 (2016). https://doi.org/10.1038/ncomms13382
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