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Evolution of topography, Be10 production rate, and erosion rate through time after response to basal accretion by duplex formation at depth, simulated using the TopoToolbox Landscape Evolution Model. (a and b) Transient topographies after initial (a) and further response (b) to basal accretion, simulated by moving a 10‐km‐wide high rock‐uplift zone across the model domain. The 10‐km‐wide hatched region experiences an uplift rate of 5 mm yr−1, whereas the model domain outside the hatched region experiences a constant rock uplift rate of 1 mm yr−1. (c) Evolution of the simulated mountain topography and the consequent variation of cosmogenic Be10 production rate through time. Blue arrows indicate times when both topographic snapshots (a and b) are created. Red arrows mark the onset of high rock‐uplift zone migration. (d) Simulated actual and Be10‐derived erosion rates through time (for details, see Appendix A).

Evolution of topography, Be10 production rate, and erosion rate through time after response to basal accretion by duplex formation at depth, simulated using the TopoToolbox Landscape Evolution Model. (a and b) Transient topographies after initial (a) and further response (b) to basal accretion, simulated by moving a 10‐km‐wide high rock‐uplift zone across the model domain. The 10‐km‐wide hatched region experiences an uplift rate of 5 mm yr−1, whereas the model domain outside the hatched region experiences a constant rock uplift rate of 1 mm yr−1. (c) Evolution of the simulated mountain topography and the consequent variation of cosmogenic Be10 production rate through time. Blue arrows indicate times when both topographic snapshots (a and b) are created. Red arrows mark the onset of high rock‐uplift zone migration. (d) Simulated actual and Be10‐derived erosion rates through time (for details, see Appendix A).

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The evolution of Earth's climate over geological timescales is linked to surface erosion via weathering of silicate minerals and burial of organic carbon. However, methodological difficulties in reconstructing erosion rates through time and feedbacks among tectonics, climate, and erosion spurred an ongoing debate on mountain erosion sensitivity to...

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... Also, sediment fluxes during the Neogene are compatible with rapid tectonic uplift in Myanmar. In addition, tectonic erosion and crustal removal show similar patterns in the evolution of Japanese forearc sediment provenance (Pastor-Galán et al. 2021) as well as with tectonic accretion processes (Mandal et al. 2021). ...
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... 4 of 26 and present-day erosion rates in the hinterland source regions (Mandal et al., 2021;Scherler et al., 2014). Fourth, geophysical data constrain the décollement geometry, which is the dominant cause for spatial variations in uplift rate across the range (Powers et al., 1998). ...
... The Asan and Suswa-Song Rivers set the base level for north-draining rivers, whereas the Gangetic Plain sets the base level for south-draining rivers (Figure 4a). The drainage divide reaches ∼800-900 m Mandal et al. (2021) and red circle shows location of sample analyzed for 10 Be by Lupker et al. (2012). B-B' = location of the balanced structural cross section shown in panel (c). ...
... The cumulative concentration of in situ-produced CRN in sediment recycled from an uplifted foreland succession (N) consists of concentrations acquired during paleoerosion in the hinterland (N E ), transport to the foreland (N T ), deposition and burial in the foreland (N B ), adjusted for radioactive decay losses, and augmented by renewed accumulation resulting from erosion of the uplifting foreland succession (N X ) ( Figure 2; steps 1-5) (e.g., Charreau et al., 2011;Mandal et al., 2021). Before reaching the foreland, sediments may be stored in intermontane valleys at the rapidly eroding front of the Himalaya for a considerable period. ...
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... tion of the kinematics of tectonic transport along the MHT similarly depends on the timescale considered. Orogenic wedges, like the Himalaya, grow primarily by frontal and basal accretion of crustal rocks, each of which lead to distinct rock-uplift patterns (Gutscher et al., 1996;Naylor & Sinclair, 2007;Mercier et al., 2017;Dal Zilio et al., 2020b;S. K. Mandal et al., 2021). Instantaneous to short-term (10 3 -10 4 y) deformation can be modelled satisfactorily by passive motion over a stable ramp-flat-ramp system (Cattin & Avouac, 2000;Lavé & Avouac, 2001;Grandin et al., 2012;Scherler et al., 2014;Dal Zilio et al., 2021), i.e., by frontal accretion. In contrast, balanced cross-sections imply a complex histo ...
... Both theoretical (Naylor & Sinclair, 2007;Mercier et al., 2017) and recent observational (S. K. Mandal et al., 2021) studies suggest that the Himalayan wedge may be experiencing cycles of frontal versus basal accretion on timespans of a few million years. Each cycle would then lead to migration of the active ramp in the MHT. ...
... Lesser Himalayan thrust nappes referred to as the Lesser Himalayan Duplex. These reconstructions also document that the ramp-flat structures are not a permanent structural feature over the time of its evolution, but rather migrate throughout Neogene times (Colleps et al., 2019), linked to the accretion cycles described above (Mercier et al., 2017;S. K. Mandal et al., 2021). ...
... To construct the 3D development of a folding landscape with both uplift and erosion, we carried out numerical simulations using the TopoToolbox Landscape Evolution Model (TTLEM) (Campforts et al., 2017). TTLEM is an open-access MATLAB-based landscape evolution model that has also been used to model drainage divide migration in response to tectonic forcing (He et al., 2021a(He et al., , 2021b, and erosion in the Himalayas (e.g., Mandal et al., 2021). The soil or regolith density moved by surfaces processes downslope is different to that of the bedrock. ...
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... In situ produced cosmogenic 10 Be and 26 Al are now routinely applied in the Earth sciences [1] and new applications demand higher accuracy and precision at increasingly lower nuclide abundances (e.g., [2][3][4][5][6]). Sample preparation procedures employed to isolate Be and Al for accelerator mass spectrometry (AMS) of 10 Be and 26 Al have a direct effect on sample throughput, background levels, and sample beam currents achieved during AMS measurement (e.g., [7][8][9][10][11]). ...
... Further complications arise in deciphering the primary driver of erosion in orogenic systems due to the common spatial coincidence between precipitation, topographic relief maxima, and deformational foci as a consequence of orographic effects 7 . excursions in climate [8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25] . Unfortunately, these studies are rarely straightforward, and commonly rely on less-than-ideal field exposures, temporal controls, and source-area and cosmogenic radionuclide systematic constraints. ...
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It has long been hypothesized that climate can modify both the pattern and magnitude of erosion in mountainous landscapes, thereby controlling morphology, rates of deformation, and potentially modulating global carbon and nutrient cycles through weathering feedbacks. Although conceptually appealing, geologic evidence for a direct climatic control on erosion has remained ambiguous owing to a lack of high-resolution, long-term terrestrial records and suitable field sites. Here we provide direct terrestrial field evidence for long-term synchrony between erosion rates and Milankovitch-driven, 400-kyr eccentricity cycles using a Plio-Pleistocene cosmogenic radionuclide paleo-erosion rate record from the southern Central Andes. The observed climate-erosion coupling across multiple orbital cycles, when combined with results from the intermediate complexity climate model CLIMBER-2, are consistent with the hypothesis that relatively modest fluctuations in precipitation can cause synchronous and nonlinear responses in erosion rates as landscapes adjust to ever-evolving hydrologic boundary conditions imposed by oscillating climate regimes.
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Sediment transfer from the interiors of the Himalaya is complex because the archives are influenced by both glacial and mon-soonal cycles. To deconvolve the coupling of glacial and monsoonal effects on sediment transfer processes, we investigate the Late Pleistocene-Holocene sediment archive in the Upper Chenab valley. Optically stimulated luminescence (OSL) ages from the archive indicate major aggradation during ca. 20-10 ka. Isotopic fingerprinting using Sr-Nd isotopes in silt fractions together with clast counts in boulder-pebble fractions indicate a decreasing Higher Himalayan sediment flux in the archive with time. Decreasing clast size, increasing clast roundness, increasing matrix to clast ratio, and dominance of the Higher Himalayan sourcing unequivocally suggest strong glacial influence during the initial stages of the archive formation. This evidence also agrees with the existing retreat ages of glaciers in the Upper Chenab valley. Results of our study also show that the upper parts of the archive contain significant fluvial sediment contribution from the Lesser Himalaya, which suggests an active role of the stronger Indian Summer Monsoon (ISM) in the region during the Early Holocene. The apparent decrease in sediment supply from the Higher Himalayan sources could have been due to longer source-to-sink transport in the Early Holocene and/or increased hillslope flux from Lesser Himalayan sources.
... The physical and thermal evolution of mountain belts is governed by the interplay between tectonic deformation, the production and transfer of heat, crustal metamorphism, and surface denudation. The extent to which surficial processes (e.g., climate and erosion) can modulate deep crustal metamorphic and tectonic processes is poorly known (1)(2)(3). The places on Earth where surface denudation is most likely to exert control on deeper crustal processes are the syntaxial massifs of the Himalaya-the Namche Barwa massif (NBM) in the east and the Nanga Parbat massif (NPM) in the west (Fig. 1). ...
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We combine monazite petrochronology with thermal modeling to evaluate the relative roles of crustal melting, surface denudation, and tectonics in facilitating ultrafast exhumation of the Nanga Parbat Massif in the western Himalayan syntaxis. Our results reveal diachronous melting histories between samples and a pulse of ultrafast exhumation (9 to 13 mm/year) that began ~1 Ma and was preceded by several million years of slower, but still rapid, exhumation (2 to 5 mm/year). Recent studies show that an exhumation pulse of similar timing and magnitude occurred in the eastern Himalayan syntaxis. A synchronous exhumation pulse in both Himalayan syntaxes suggests that neither erosion by rivers and/or glaciers nor a pulse of crustal melting was a primary trigger for accelerated exhumation. Rather, our results, combined with those of recent studies in the eastern syntaxis, imply that larger-scale tectonic processes impose the dominant control on the current tempo of rapid exhumation in the Himalayan syntaxes.