Much work has been devoted to studying the potential links that might exist between climate and surface processes, and in particular the erosion of high-relief, tectonically active mountain belts . This is in turn important to understand whether climate can affect tectonics as suggested by several now highly quoted studies . Because glacial erosion is more efficient than fluvial processes, it is now reasonably well established that Cenozoic climate cooling culminating in the onset of periodic glaciations in the Quaternary has led to enhanced erosion rates in many high-latitude or high-elevation mountain belts , as long as ice is not frozen to the bedrock . In non-glaciated environments, rainfall intensity plays an important role in controlling erosion , but there is growing evidence that variability in rainfall may be as important as mean precipitation in limiting or enhancing the rate of surface erosion by mountain streams and rivers . Variations in rainfall also affect the rate of chemical erosion as water availability is, with temperature, one of the main controls on silicate weathering . The thawing and freezing of soil-mantled slopes is also known to highly amplify the rate of soil creep , implying that variability in temperature at or near freezing point must affect the rate of transport of chemically weathered rocks. Vegetation type and cover are also a function of climate (and elevation) and there is now mounting evidence that vegetation and erosion are linked , providing another potential, and so far poorly studied, link between erosional efficiency and climate.

The climate of the late Cenozoic and of the Quaternary in particular is dominated by large variations in continental ice cover both near the poles and in regions of elevated topography, which are controlled by variations in the Earth's orbital parameters, the so-called Milankovitch cycles . Other aspects of the Earth's climate are also known to vary between glacial and non-glacial periods, such as the strength of the monsoon, or the latitudinal distribution of precipitation . There is clear evidence that since the onset of large amplitude, 100 ka period glacial cycles approximately 1 Ma ago, glacial erosion is strongly enhanced during periods of extended ice cover , but other potential effects of climatic variations at Milankovitch periods on the erosional response of mountain belts, such as variations in rainfall intensity and/or variability, have not been extensively studied, potentially because of the large difference between the Milankovitch orbital periods and the typical tectonics/erosion timescales (≥ 1 Ma).

The response of geomorphic systems to cyclic climate variations at either longer or shorter periods, has, however, been the subject of several studies. and showed that, under the assumption that sediment transport rate is related to slope and runoff, the response of an equilibrium system (i.e., having reached a steady-state form by balancing uplift and erosion) to a sinusoidal variation in rainfall depends on the period of forcing in comparison to the response time of the system (the time it takes to reach equilibrium). If the forcing is much faster than the response time, the system is constantly out of equilibrium; when the forcing is slow, the system is able to remain at equilibrium; for intermediary forcing timescales, the geomorphic system's response lags the rainfall variations. computed the response of a geomorphic system composed of an eroding mountain (obeying a linearized version of the stream power law) and a depositional foreland to demonstrate that an oscillating forcing (in precipitation for example) causes cyclic sedimentation patterns that show maximum amplitude at the contact point between the erosional and depositional systems. They also note that the time delay between forcing and response is mostly a function of the system size, not the period of forcing, and that the response is always damped in comparison with the forcing.

Using a more complex model combining the effects of soil formation and transport on hillslopes to the transport and erosion by river channels, demonstrated that cycles in runoff intensity cause a non-linear response of geomorphic system, which strongly depends on the period of the cycles in comparison with the response time of the system. They also confirmed the results of , who showed that drainage density varies during climate cycles as the balance between fluvial and hillslope transport and erosion evolves through time. Using a diffusive model for fluvial sediment transport by rivers, showed that Milankovitch-period variations in sedimentary supply from a high-relief, fast-eroding source (the mountain) are strongly buffered and therefore unlikely to be preserved in the depositional record. Using a more sophisticated model that includes the effect of grain size on transport capacity, demonstrated that variability in rainfall is mostly imprinted in the sedimentary record as variations in grain size and its distribution with distance to the source. In a more recent study, argue that high-frequency rainfall cycles can be propagated and amplified to sedimentary basins if one assumes a potentially strong feedback between discharge and channel gradient. Similarly, but focusing on Milankovitch cycles timescales, demonstrated, using a surface processes model that combines fluvial erosion and hillslope processes, that geomorphic systems behave as “forced oscillators” where climate forcing is amplified in the sedimentary response at a relatively specific range of frequencies, although their response to the relatively short-period Quaternary climate variability is strongly damped when diffusive processes become dominant over river incision.

Here we present an analytical solution to the stream power law equation forced by climate-driven cycles in precipitation. We show that it is a natural behavior of this equation to predict an amplification and introduce a time lag between forcing and response. We then use a simple numerical solution of the same equation to fully appreciate the response of a fast-eroding tectonic system to periodic perturbations in precipitation, with a particular focus on forcing at the Milankovitch periods. We then interpret these solutions in terms of the consequences they have on the behavior of natural systems and their response to cyclic rainfall variability at a range of forcing periods.

We will assume that bedrock incision is the dominant mode of erosion in an active mountain belt. Under the assumption that fluvial erosion can be represented by the stream power law and that drainage area increases as a power of the distance to the water divide , the evolution of bedrock height, h, as a function of time is given by the following partial differential equation, or PDE (see Appendix for a detailed derivation): ∂h∂t=U-Kνm(L-x)mp∂h∂xn, where L is the length of the river channel, U is rock uplift, ν is precipitation rate and K, n, m and p are constants. The distance x is measured from base level (h(x = 0) = 0). Let us note that, as drainage area tends towards zero at the divide, erosion rate is arbitrarily nil at x = L. This is commonly handled by defining a critical slope, Sc, beyond which the stream power law is no more valid and colluvial and hillslope processes become dominant . The slope (n) and area (m) exponents in the stream power law are not well constrained. Their commonly accepted ranges are 0.2 < m < 0.8 and 0.5 < n < 2. The ratio m/n controls the concavity of stream profiles that have reached an equilibrium between uplift and erosion (see Eq.  in the Appendix) and, where estimated, it ranges between 0.4 and 0.6. Independently, p, the exponent in Hack's law relating drainage area to distance to the divide can be extracted from digital elevation model analysis; its commonly accepted value is close to 2.

In the Appendix, we show that this equation can be written in dimensionless form as follows: ∂h′∂t′=1-(1-x′)mp∂h′∂x′n, where x′ = x/L, h′ = h/H, t′ = t/τ, and H = UKνm1/nL1-mp/n1-mp/n and τ = H/U. We also show that the variation in normalized height, δh′, resulting from a small perturbation in precipitation, δν′, obeys the following PDE: ∂δh′∂t′≈-mδν′-n1-mp/n(1-x′)mp/n∂δh′∂x′. The first term of the right-hand side of the equation corresponds to the direct response of the system to the perturbation (it is directly and linearly proportional to δν′), whereas the second term expresses how the resulting change in slope, ∂h′∂x′, modifies the response of the system to future perturbation.

In the Appendix, we show that there exists an approximate solution to this equation, which yields the response of the system to a small periodic perturbation in precipitation rate, ν = ν0 + δν0 sin⁡ 2πtP, in the form of the corresponding variation in the sedimentary flux, Q = Q0 + δQ0, i.e., the erosion rate integrated over the channel length. The solution can be expressed as δQ0/Q0δν0/ν0=δQ′δν′=Gsin⁡2π(t+θ)P, where G is a dimensionless gain and is given by G=2πτm/P(2πτ/P)2+mp1-mp/n2 and θ is a phase shift, or time lag, between the forcing (the perturbation in precipitation rate) and the response (the resulting perturbation in sedimentary flux), given by θ=P2πtan⁡-1P2πτmp1-mp/n. P is the period of forcing and τ is the characteristic time of the system, i.e., the time it takes for erosion to balance uplift (τ = H/U). Note that this solution is only valid for values of the ratio mp/n close to unity (see Appendix).

The predicted time lag and gain are shown in Fig.  as functions of the period of the perturbation, for various values of the exponent m and mp1-mp/n ≈ 1. We see that for very short periods, i.e., in comparison with the characteristic timescale of the system (P ≪ τ = H/U), the sedimentary flux is in phase with the perturbation. This is because the channel geometry does not have the time to respond to the perturbation in precipitation rate. As the forcing period increases, the time lag grows until it reaches a quarter of the forcing period and the two signals are completely out of phase. This can be derived from Eq. (), where lim⁡P≪τθ=0lim⁡P≫τθ=P/4. For intermediary periods (τ/100 < P < τ), the system is out of phase, with the sedimentary response lagging behind the climate forcing. These results are in agreement with the qualitative analysis of based on the results of a landscape evolution model where sediment transport is assumed proportional to slope and surface runoff (proportional to precipitation and drainage area). Our results also show that the time lag increases with m (compare the red curve corresponding to m = 1 with the black curve corresponding to m = 2 and the green curve corresponding to m = 0.5 in Fig. ).

We note also that the gain decreases with the forcing period. The gain is maximum and equal to m when the forcing period is small compared to τ and it tends towards zero when the forcing period is much larger than τ. This can be derived from Eq. (): lim⁡P≪τG=mlim⁡P≫τG=0. In this latter situation (P ≫ τ), the channel has the time to adjust to the variable precipitation and remains at steady state such that the sedimentary flux perfectly balances the uplift rate, U, and there is no perturbation (the gain is nil).

It is worth noting that this behavior is similar to the response of a general linear system with finite memory as described by see his Fig. 1 while considering the general response of geomorphological systems to step or periodic forcing. Although clearly derived from a non-linear equation, our solution could be regraded as the application of this general principle to bedrock channel incision parameterized by the stream power law.

To test the accuracy of this approximate solution, we have solved the stream power law using the following implicit finite difference scheme : hi(t+Δt)=hi(t)+UΔt-KΔtνm(L-x)mphi(t+δt)-hi-1(t+δt)δxn. The non-linear dependence of erosion rate on slope (when n ≠ 1) was dealt with by using a Newton–Raphson iterative scheme . We imposed the uplift rate and the mean precipitation rate. We adjusted the constant K such that the resulting steady-state topography reaches a set value, Hmax. Note that the value of the mean precipitation rate is not important, as it appears as a multiplier of the constant K in the stream power law. The model was run to steady state and a sinusoidal variation in precipitation rate was then imposed of amplitude equal to one-tenth of the mean precipitation rate. The amplitude of this perturbation is of no importance to the solutions we present, as long as it remains small in comparison with the mean precipitation rate. Increasing the amplitude of the perturbation towards values close to the assumed mean precipitation causes the time lag to increase and the amplification to decrease, but the characteristics of the solution remain unchanged. The channel length was set to 200 km but its value does not influence the solution either, implying that the response of an incising river to a perturbation in precipitation rate does not depend on its size or the size of its catchment. This is a consequence of using a value of mp/n ≈ 1.

We computed the gain as the ratio of the amplitude of the variations in sedimentary flux normalized by the mean sedimentary flux (at steady state) by the amplitude of the imposed variations in precipitation rate normalized by the mean precipitation rate. We also computed the phase shift between the imposed precipitations and the computed sedimentary flux by performing a cross-correlation between the two signals. The results are also shown in Fig.  where they are compared to the semi-analytical solution for different combinations of the parameters m, n and p.

The first interesting result is that the numerical solution is almost identical to the analytical solution when mp/n ≈ 1, implying that the analytical solution is a good approximation of the general behavior of the system. For values of the exponents such that mp/n ≠ 1, the analytical solution is not so accurate as shown in the case where m = 1, n = 3 and p = 2 (blue curve in Fig. ), but the shape of the solution is very similar with the analytical solution clearly overestimating the time lag. In all cases, the numerical solution predicts a time lag between climate and the resulting erosional response that is a function of the forcing period, reaching a maximum of P/4 when the forcing period is similar to the characteristic time, τ. Similar to the analytical solution, the gain, G, or ratio of the relative variation in sedimentary flux (normalized by its steady-state value) to relative variation in precipitation (normalized by its steady-state value), scales with m for periods that are small compared to the characteristic timescale of the system and tends towards zero for longer periods.

To better understand the solution and thus the behavior of the system, we show in Fig.  snapshots of the evolution of the models in terms of the departure in erosion rate from the mean (steady-state) value. We selected the model run in which n = 4, m = 2, p = 2, P = 100 ka and U = 6 mm a-1. We recognize that the values of m and n we selected are large and likely to be outside the range of acceptable values, but this choice produces a clear time lag and amplification of the erosional signal that we can more easily use to illustrate the behavior of the system. The solution shows the propagation of damped waves in erosion rate (Fig. b) with the erosion rate varying locally by as much as 50 % of the imposed mean value (here 6 mm a-1). As rainfall increases at the beginning of a cycle (black curve in Fig. b), the incision rate increases near the base level. The maximum in anomalous erosion rate propagates up the profile (blue curve in Fig. b) until the precipitation rate starts to decrease. The erosion rate decreases then drastically near the base level (red curve in Fig. b), and a similar but opposite-sign wave of reduced erosion rate propagates towards the head of the channel (purple curve in Fig. b). The cycle then repeats itself. Note that the height of the river profile is also affected by similar topographic waves but, interestingly, whereas the predicted erosion rate can vary by as much as 50 % locally, the topographic “waves” never exceed 100 m in amplitude (i.e., < 2 % of the maximum topography), anywhere along the profile. The wavelength of these waves is such that the topographic perturbation they cause is likely to be almost undetectable.

The formation of these waves corresponds to the response of a system at equilibrium to a small perturbation. If the rate of change of the perturbation is rapid (in comparison to the characteristic time of the system), the system does not have the time to adjust and the perturbation in rainfall results in an instantaneous and proportional response in erosion rate. Consequently, the erosional response is in phase and in proportion to the perturbation (here amplified by the power m to which the discharge, and thus rainfall, is raised in the stream power law). On the contrary, when the perturbation rate is very slow (in comparison to the characteristic time of the system), the system is able to adjust, the system remains at or close to steady state and the integrated rate of erosion remains constant and equal to the imposed uplift rate. These two end-member behaviors are shown in Fig.  (blue and red curves), as well as the case where the forcing period is similar to the characteristic time of the system (purple curves). We see that, for long forcing periods, the response is strongly damped as the system is able to change its shape (slope) and adjust to the variation in precipitation rate such that erosion rate remains almost equal to uplift rate along the entire length of the river profile; the only remaining anomaly in erosion rate is near the headwaters of the stream and is therefore strongly out of phase. For short forcing periods, the perturbation propagates rapidly over the entire length of the profile such that it is able to offset the erosion rate over its entire length, therefore leading to a large amplitude response that is, however, in phase with the forcing.

In Fig. , we show the geometry of these waves/perturbations at the start of a precipitation cycle (corresponding to point 1 on Fig. a) for a range of values of the exponents m and n. We kept all other parameters at constant values, i.e., U = 6 mm yr-1 and P = 100 ka. As usual the K parameter is adjusted such that the resulting steady-state river profile maximum height is 6000 m. We note that, to first order, the wavelength of these waves determines the time lag – i.e., the shorter the wavelength, the shorter the time lag – whereas their amplitude determines the gain.

Finally, we performed a large number of simulations, keeping the uplift rate constant at 6 mm a-1, but varying m, n and P. The results are shown in Fig. . For small forcing periods (Fig. a; P = 1 ka) compared to the characteristic time, the offset is nil and the gain is directly proportional to m (Fig. a). For intermediate values of the forcing period (Fig. b and c), which we arbitrarily selected to correspond to the 41 and 100 ka Milankovitch periods, the gain remains proportional to m, especially for values of m and n that are close to the limit m/n = 0.5 (or mp/n = 1). If we assume that the ratio between m and n is well constrained, this implies that the gain is also proportional to n. This simple relationship breaks down for large forcing periods (Fig. d) as the gain tends towards zero, independently of m or n.

The time lag, θ, is nil for small values of the forcing period. For intermediate values of the forcing period (Fig. a), it increases with m as well as with n, such that the increase in time lag along the m/n = 0.5 line is relatively small: it varies between 250 and 1000 a for P = 41 ka and between 1000 and 5500 a for P = 100 ka (Fig. b and c). These contour plots also show that the time lag increases mostly as the ratio m/n tends towards 1 (the thick black diagonal line).

Our solutions demonstrate that time lags are a natural response of erosional systems to climate (rainfall) variability if they obey and are controlled by the stream power law. The sedimentary flux responds to an external climate forcing – variable precipitation – in a way that depends on how the forcing period compares to the characteristic timescale of the system, τ, which is itself proportional to mountain height and inversely proportional to mean uplift rate. When the forcing period, P, is within the range τ/100 < P < τ, a substantial time lag is predicted in the erosional response to a cyclic precipitation pattern (see Fig. ). Time lags associated with forcing at Milankovitch periods should therefore be measurable in most orogenic systems that have a characteristic timescale of a few million years and, particularly, in fast uplifting/eroding mountain belts, such as the Southern Alps in New Zealand or the Taiwan orogen, which both experience uplift and erosion rates of the order of 10 mm a-1.

We also predict that the erosional response is multiplied by a factor m, the area exponent in the stream power law, for forcing at periods smaller than τ. Although m is likely to be smaller than unity, it is possible that, if m > 1, the sedimentary signal be enhanced, which may explain the strong imprint that Milankovitch cycles have on the sedimentary record despite the relatively small changes in both solar insulation and temperature that are associated with the corresponding variations in the Earth's orbital parameters. At long forcing periods (compared to τ), the gain tends towards zero, inhibiting detection of the time lag.

We have also shown that the erosive response of a river to a change in precipitation rate does not depend on its length. This ensures that all streams and catchments in a given mountain belt respond in a synchronous manner. It is a direct consequence of the stream power law combined with Hack's law. To test whether this still holds when taking into account the complex geometry and varied topology of river networks, we have used the plan-form two-dimensional landscape evolution model FastScape to perform a simulation similar to the 1-D models presented here above. We used the following model parameters: n = 4, m = 2, K = 3 × 10-14 m1-3m a-1-m and U = 6 mm a-1 to allow for a direct comparison with the results shown in Fig. . The solution is shown in Fig.  and is also provided as a small animation (see Supplement).

On the one hand, and as in the 1-D model, the computed topography (Fig. d–f) remains relatively unchanged throughout the precipitation cycle with local variations of the order of a few tens of meters only. On the other hand, the erosion rate (Fig. a–c) changes dramatically from step to step. The model predicts a wave of erosion rate in each of the model catchments. The wave propagates at the same rate in all catchments, regardless of their size or geometry (panels a to c) demonstrating that Hack's law, used in the 1-D analytical solution (Eq. ) and in the 1-D numerical model (Fig. ), is a good approximation to the topology of catchments and the plan-form relationship between drainage area and distance to the divide. We also note that drainage geometry and, a fortiori, drainage density does not change during a climate cycle. This is contrary to the results of simulations performed by and implying that hillslope processes (not included in the FastScape model runs presented here) must control drainage density in a varying climate.

Another important outcome of our study is that, although the response of the stream power law to small cyclic variations in precipitation produces nearly undetectable changes in river longitudinal profiles, the erosional waves they trigger are measurable and, potentially, amplified (depending on the value of m). These waves could cause in situ measurements of erosion rate by cosmogenic isotope methods, for example, to be strongly variable both in space and time, rendering estimates of local or catchment-averaged exhumation rate rather difficult.

A direct comparison of our results (Fig. ) with those of (see their Fig. 2) shows that the amplification of the climate cycles in the sedimentary record near the “forced oscillator” periods they evidenced is reproduced by our model; it corresponds to the slight increase in the gain (or amplitude response) that is seen on all curves presented in Fig.  ahead of the transition to low gain values. Note that this slight increase in gain is relatively subtle compared to the main one we evidence here, which scales with m.

Unlike , however, we did not include in our computations the effect of the hillslope response to variations in stream incision rate caused by rainfall cycles. Here, we focused our attention on the stream power law representing bedrock incision which we considered as the main controlling agent on the rate of landscape evolution in active mountain belts. In a mountain that has reached steady state between fast uplift and erosion, it is likely that hillslopes are close to or at a critical state (slope) and should therefore respond almost instantaneously to variations in stream incision rate, at least for forcing periods of the order of a few tens of thousands of years (the Milankovitch periods, for example). For slowly uplifting areas, this might not be the case and further work should concentrate on including a reasonable representation of hillslope process but also of sediment transport capacity by rivers in the calculations presented here.

Observations of a potential time lag between climate forcing and the erosional response of an active tectonic area are rare. In a recent paper, argue that they observe a time lag between δ18O and ϵNd records derived from a well-studied ODP site (ODP 758) located in the southern part of the Bengal Fan . This is, potentially, an appropriate site to observe changes in continental riverine input related to changes in the erosional flux from the Himalayas. The data sets they use are rather unique for they provide records of both climate and ϵNd (a proxy for the intensity of the riverine sedimentary input from Himalayan rivers) at high resolution and on the same samples. This allows for a direct time correlation between the two data sets, even if the exact age of each sample is only constrained by correlating the local δ18O signal with globally averaged sea surface temperature data . A careful spectral analysis of the two signals shows the existence of a well-defined time lag between δ18O and ϵNd at Milankovitch periods, which increases with the forcing period. This time lag is 1000, 2000 and 7000 (±500) years at the 23, 41, and 100 ka Milankovitch periods, respectively. argue that the delay between temperature changes recorded by δ18O and the erosion flux out of the Himalayas recorded by ϵNd must be a consequence of how the variability in summer monsoonal rainfall affects erosion in the Himalayas. Estimates from global circulation models suggest that Indian monsoonal rainfall intensity varies in phase with temperature at orbital cycle periods with an amplitude of a 1–2 mm day-1, which is approximately 10 % of the present-day precipitations.

Using the numerical model described above, we searched through parameter space to find the best fitting model parameters that would provide a close fit to the observed time lags. We varied m, n, p and U and, for each run, adjusted K so that the steady-state maximum mountain height is 6000 m. There is no single solution to this search. In Fig. , we show the fit of three model runs corresponding to various values of the model parameters.

We combined the solutions of many model runs performed at the three Milankovitch periods (23, 41 and 100 ka) (Fig. ) but assuming a constant value of U = 6 mm a-1 and p = 2, to show that the range of acceptable m and n values defines a region in [m, n] space (dark grey shaded area in Fig. ) that is sub-parallel to the commonly accepted range for m and n defined by m/n = 0.5. The corresponding gain factors range from 1 to 2, depending on the value chosen for m. For large n values, the optimum m/n ratio tends towards its more commonly accepted value of 0.5.

We note, however, that only a small sub-ensemble of the best fitting values of the m and n model parameters (dark grey shaded area) are within the most commonly accepted ranges (0.2 < m < 0.8 and 0.5 < n < 2, light grey-shaded area between light dashed lines). This could imply that the time lags observed between the geochemical data sets are not related to the erosional response of the Himalayas to a cyclic rainfall; the time lags could originate from the delayed transport in the Ganges plains, for example. The temporary storage of sediments in the Indian plains is best described by a transport limited or diffusive model . However, to fit the constraint provided by the two geochemical signals (i.e., that the time lag increases with the forcing period), the diffusivity parameter needs to be scaled in an ad hoc fashion with the period of fluctuations, which is difficult to justify. Alternatively and if we recall that the value of the m and n exponents is poorly constrained and remains the subject of much debate (see the recent review paper by on this subject), the observed time lags could be regarded as new, independent constraints on the value of the stream power law parameters.

Our best fitting models have values for m and n that are either very large, if imposed to be in the accepted ratio of 2, or that are not in this accepted ratio. If n is indeed large, the response of the erosional system to changes in slopes is strong. Interestingly, it has been recently demonstrated that the exponent n may depend on the variability of river discharge, and thus climate . In a variable climate, n and m should have low values, with n being close to unity, whereas, in locations where the climate is “steady”, n could be as large as 3 or 4 . Alternatively, it could be that the ratio m/n is not close to 0.5, but this is difficult to reconcile with the very numerous observations of the steady-state concavity of river profiles (see , for example), unless one calls into question the existence of steady-state conditions between uplift and erosion.

Based on both analytical and numerical solutions to the stream power law, we have shown that it is a natural behavior of this equation to produce a time lag between cycling climate forcing and the resulting erosional response. The main finding is that the time lag depends on the forcing period. If the forcing period is small compared to the characteristic timescale of the tectonic system (i.e., the time it takes for the system to approach steady state between uplift and erosion), the time lag is small; conversely, if the forcing period is large, the time lag tends towards a quarter of the period (the response is exactly out of phase with the forcing). The second important finding is that the erosional response is amplified in comparison with the amplitude of the climate forcing in a direct proportion to the parameter m, the discharge exponent in the stream power law when the forcing period is small. For large value of the forcing period (in comparison with the characteristic timescale of the system), the amplification tends towards 0, which means that very long-term variations in rainfall do not affect the erosional response of an active mountain belt and thus cannot be recorded, in the sedimentary record for example.

We have also demonstrated, based on simple 1-D and 2-D numerical landscape evolution experiments, that the response to climatic variations of an actively eroding mountain river, if it obeys the stream power equation, is independent of the size of its drainage basins, implying that, within a mountain belt, all rivers should respond in phase with each other to a periodic rainfall perturbation and, consequently, contribute constructively to the integrated sedimentary record.

We have shown that the response of a rapidly uplifting and eroding mountain belt to rainfall variations at Milankovitch periods can lag the climatic forcing by several thousands of years. This theoretical prediction should be used to interrogate the geological record and, potentially, test the validity of the stream power law as an adequate parameterization of fluvial erosion in active mountain belts. We have finally shown how geochemical signals could be used to extract such potential offsets under the assumption that they are adequate proxies for climate variability and the resulting erosional response. Potentially, such data sets could provide interesting and independent constraints on the slope and area exponents in the stream power law. We have also shown that the sedimentary flux fluctuations resulting from periodic rainfall variations can be amplified if m > 1, which may explain the strong imprint that Milankovitch cycles have on the sedimentary record despite the relatively small changes in both solar insulation and temperature that are associated with the corresponding variations in the Earth's orbital parameters.