Abstract

Assessing the impact of uncertainties in ice-sheet models is a major and challenging issue that needs to be faced by the ice-sheet community to provide more robust and reliable model-based projections of ice-sheet mass balance. In recent years, uncertainty quantification (UQ) has been increasingly used to characterize and explore uncertainty in ice-sheet models and improve the robustness of their projections. A typical UQ analysis involves first the (probabilistic) characterization of the sources of uncertainty followed by the propagation and sensitivity analysis of these sources of uncertainty. Previous studies concerned with UQ in ice-sheet models have generally focused on the last two steps but paid relatively little attention to the preliminary and critical step of the characterization of uncertainty. Sources of uncertainty in ice-sheet models, like uncertainties in ice-sheet geometry or surface mass balance, typically vary in space and potentially in time. For that reason, they are more adequately described as spatio(-temporal) random fields, which account naturally for spatial (and temporal) correlation. As a means of improving the characterization of the sources of uncertainties in ice-sheet models, we propose in this paper to represent them as Gaussian random fields with Matérn covariance function. The class of Matérn covariance functions provides a flexible model able to capture statistical dependence between locations with different degrees of spatial correlation or smoothness properties. Samples from a Gaussian random field with Matérn covariance function can be generated efficiently by solving a certain stochastic partial differential equation. Discretization of this stochastic partial differential equation by the finite element method results in a sparse approximation known as a Gaussian Markov random field. We solve this equation efficiently using the finite element method within the Ice-sheet and Sea-level System Model (ISSM). In addition, spatio-temporal samples can be generated by combining an autoregressive temporal model and the Matérn field. The implementation is tested on a set of synthetic experiments to verify that it captures well the desired spatial and temporal correlations. Finally, we demonstrate the interest of this sampling capability in an illustration concerned with assessing the impact of various sources of uncertainties on the Pine Island Glacier, West Antarctica. We find that both larger spatial and temporal correlations lengths will likely result in increased uncertainty in the projections.

Highlights

  • Despite large improvements in ice-sheet modeling in recent years, model-based estimates of ice-sheet mass balance remain 25 characterized by large uncertainty

  • As a 10 means of improving the characterization of the sources of uncertainties in ice-sheet models, we propose in this paper to represent them as Gaussian random fields with Matérn covariance function

  • We assume without loss of generality the mean function to be zero, so that x(s) = (s), and we model the stochastic term as a Gaussian random field

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Summary

Introduction

Despite large improvements in ice-sheet modeling in recent years, model-based estimates of ice-sheet mass balance remain 25 characterized by large uncertainty. In order to provide more robust and reliable model-based estimates of ice-sheet mass balance, we need to understand how model outputs are 30 affected by or sensitive to input parameters To this aim, uncertainty quantification (UQ) methods have become a powerful and popular tool to deduce the impact of sources of uncertainty on ice-sheet projections (propagation of uncertainty) or to ascertain and rank the impact of each source of uncertainty on the projection uncertainty (sensitivity analysis) (Bulthuis et al, 2019, 2020; Edwards et al, 2019, 2021; Larour et al, 2012b; Ritz et al, 2015; Schlegel et al, 2018). Uncertainties in input parameters are generally lumped into uncertain (lumped) parameters that represent one or several sources of parametric and/or unmodeled dynamics uncertainty (Bulthuis et al, 2019; Edwards et al, 2019, 2021; Ritz et al, 2015) These uncertain lumped parameters appear in parameterizations and reduced-order models of complex physical processes such as basal friction or ocean induced melting. The number of partitions controls the spatial scale of the random perturbation; the larger the number of the partitions, the more local the perturbation

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