Kernel density plot of eddy nonlinearity (r) versus normalized eddy scale Lη/Ld for eddies identified by the automated eddy detection algorithm. The nonlinearity parameter (r) is defined as r=U/c following Chelton et al 2007. Colors blue, red, and gray represent eddies in the 35°, 45°, and 55° latitudinal band, respectively. This regime diagram is adapted from Klocker et al. (2016). This plot combines data corresponding to 4,680 and 3,755 detected eddy structures for (top) NATL60 and (bottom) HYCOM50 respectively.

Kernel density plot of eddy nonlinearity (r) versus normalized eddy scale Lη/Ld for eddies identified by the automated eddy detection algorithm. The nonlinearity parameter (r) is defined as r=U/c following Chelton et al 2007. Colors blue, red, and gray represent eddies in the 35°, 45°, and 55° latitudinal band, respectively. This regime diagram is adapted from Klocker et al. (2016). This plot combines data corresponding to 4,680 and 3,755 detected eddy structures for (top) NATL60 and (bottom) HYCOM50 respectively.

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Ocean circulation is dominated by turbulent geostrophic eddy fields with typical scales ranging from 10 to 300 km. At mesoscales (>50 km), the size of eddy structures varies regionally following the Rossby radius of deformation. The variability of the scale of smaller eddies is not well known due to the limitations in existing numerical simulations...

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... The considered simulation data set relies on a nature run of the NATL60 configuration of the NEMO (Nucleus for European Modeling of the Ocean) model (Madec et al., 2022). This simulation delivers a realistic hindcast simulation of ocean dynamics, including mesoscale-to-submesoscale ocean dynamics (Ajayi et al., 2020), over 1 year from October 2012 to September 2013 for a North Atlantic domain with a 1/60°and hourly resolution. The initial and open boundary conditions rely on GLORYS2v3 ocean reanalysis and the atmospheric forcing is based on DFS5.2 (Dussin et al., 2018). ...
... The initial and open boundary conditions rely on GLORYS2v3 ocean reanalysis and the atmospheric forcing is based on DFS5.2 (Dussin et al., 2018). We refer the reader to (Ajayi et al., 2020) for a more detailed description and analysis of NATL60 simulation. It has been used in numerous studies regarding the reconstruction and observability of sea surface dynamics (see below for the related OSSE data challenge stated in Le Guillou et al. (2020)). ...
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... So the same CCN (UNet variant) was retrained on a more realistic training dataset: less random noise than in prelaunch simulations, training on the eNATL60 model with tides (Ajayi et al., 2020;Brodeau et al., 2020) to better simulate the SWOT observations. The re-training was performed with a random wave-modulated white noise at 250-m, with a Hamming filter to 440 mimic the downscaling to 2-km that is performed in the ground segment. ...
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... It is well recognized that mesoscale eddies capture approximately 80% of the total kinetic energy, exerting a significant influence on the ocean circulation, the air-sea interaction, and the marine ecosystem (Dong et al., 2014;Zhang et al., 2014;Zhang & Qiu, 2020). However, the nadir-looking altimeter is limited in its ability to resolve other ocean energetic motions at submesoscale or smaller scales (Amores et al., 2018;Ballarotta et al., 2019;Dufau et al., 2016;Vergara et al., 2019), even though these motions play a crucial role in the cascade and dissipation of ocean energy (Ajayi et al., 2020;Klein et al., 2019;Zhang et al., 2023). To improve the observational capabilities of satellite altimetry, the next generation of wide-swath imaging altimeter has been proposed, including the Surface Water and Ocean Topography (SWOT) satellite launched on 16 December 2022 , as well as the Guanlan mission proposed by China . ...
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... These methods are generally trained on simulated data, and are then evaluated either on simulated data from an excluded test set or on real data such as drifters. System Simulation Experiments (OSSEs) such as [37][38][39] are based on geophysical models and have proven essential in training data-driven methods. An OSSE is a modeling experiment used to evaluate the value of a new observing system when actual observational data are not available. ...
... The OSSE setup comprises a nature run, a data assimilation system, and software tasked with simulating 'observations' derived from the nature run while incorporating realistic observation errors. Numerous studies train models to reconstruct SSH using simulated data from the Gulf Stream [37], such as 4DVarNet (Fablet et al. [8]) and the CNN-based method RESAC (Thiria et al. [40]). Nardelli et al. [7] use simulated data from the Mediterranean Sea [38] to reconstruct SSH and surface currents. ...
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... Our primary experiments utilized the eNATL60 configuration of the Nucleus for the European Modelling of the Ocean (NEMO) model (Gurvan et al., 2022), featuring a 1/60°horizontal resolution and 300 vertical levels across the North Atlantic. This highresolution configuration is essential for understanding ocean dynamics, particularly for surface oceanic motions down to 15 km, which aligns with SWOT observations (Ajayi et al. (2020)). We direct readers to this work for a detailed understanding of NATL60's capabilities. ...
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... Initial conditions were taken from the 1/12 • MERCATOR ocean reanalysis. The output of NATL60 was analyzed in Ajayi et al. (2020). In the present research, we studied the Gulf-stream region (26 • N, 45 • N; 40 • W, 65 • W, Fig. 1) which is the most energetic region of the North Atlantic Ocean. ...
... It relies on an Observing System Simulation Experiment (OSSE) for nadir and wide-swath satellite altimetry data. We exploit one-year NATL60 numerical simulation dataset [3] for a 10 • x10 • area along the Gulf Stream from October 2012 to September 2013 with a daily time resolution and a 1/20 • spatial resolution. Nadir altimetry data involves the space-time sampling of a real 4-altimeter configuration, whereas wide-swath SWOT data rely on SWOT simulator [25]. ...
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... Torres et al. (2019) make use of a spatial scale threshold above which BMs dominate and below which ITs dominate. This spectral technique is less effective when the common spatial scale interval extends too much, which is particularly the case in winter due to the emergence of small vortices (<50 km) associated with mixed layer instabilities (Ajayi et al., 2020). Gonzalez-Haro et al. (2019) and Ponte et al. (2017) explore multi-sensor approaches with altimetry and sea surface temperature observations, motivated by the fact that BMs and ITs have distinct signature on both fields. ...
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Wide‐swath altimetry, for example, the Surface Water and Ocean Topography mission is expected to provide Sea Surface Height (SSH) measurements resolving scales of a few tens of kilometers. Over a large fraction of the globe, the SSH signal at these scales is essentially a superposition of a component due to balanced motions (BMs) and another component due to internal tides (ITs). Several oceanographic applications require the separation of these components and their mapping on regular grids. For that purpose, the paper introduces an alternating minimization algorithm that iteratively implements two data assimilation techniques, each specific to the mapping of one component: a quasi‐geostrophic model with Back‐and‐Forth Nudging for BMs, and a linear shallow‐water model with 4‐Dimensional Variational assimilation for ITs. The algorithm is tested with Observation System Simulation Experiments where the truth is provided by a primitive‐equation ocean model in an idealized configuration simulating a turbulent jet and mode‐one ITs. The algorithm reconstructs almost 80% of the variance of BMs and ITs, the remaining 20% being mostly due to dynamics that cannot be described by the simple models used. Importantly, in addition to the reconstruction of stationary ITs, the amplitude and phase of nonstationary ITs are reconstructed. Sensitivity experiments show that the quality of reconstruction significantly depends upon the timing of observations. Although idealized, this study represents a step forward towards the disentanglement of BMs and ITs signals from real wide‐swath altimetry data.