Preprints
https://doi.org/10.5194/egusphere-2026-6375
https://doi.org/10.5194/egusphere-2026-6375
26 Oct 2026
 | 26 Oct 2026
Status: this preprint is open for discussion and under review for Atmospheric Measurement Techniques (AMT).

Looking up, looking down: zenith-to-nadir lidar comparisons for cloud scenes (IPRAL and ATLID/EarthCARE)

Artem G. Feofilov, Arezki Haddouche, Hélène Chepfer, Sergey Khaykin, Florian Lapouge, Patricia Delville, Marc-Antoine Drouin, Martial Haeffelin, Jean-Charles Dupont, Cheikh Dione, and Christophe Pietras

Abstract. Intercomparisons between spaceborne lidar instruments and ground-based lidars are essential for calibration/validation of these instruments and for data quality assurance. However, zenith-to-nadir viewing geometry differences can create systematic discrepancies between space-borne and ground-based observations, even under perfect spatiotemporal collocation. This is particularly true for clouds: unlike aerosols, which are comparatively well-mixed and spatially homogeneous, clouds are structured and short-lived, so both the observation geometry and the collocation quality strongly affect whether a spaceborne and a ground-based profile can be meaningfully compared. Still, clouds are valuable targets because they push the signal into a different dynamic range, from strong backscatter to near-saturation, that clear-sky or aerosol scenes never exercise. The present paper addresses three questions: which parameters retrieved from lidar observations are better suited to zenith-to-nadir comparisons, which atmospheric scenes are favorable for such a comparison, and how the choice of collocation approach affects the comparison's reliability.

We address these questions with a simulation framework that generates 15 synthetic cloud scenes, propagates them through the lidar simulator of the Cloud Feedback Model Intercomparison Project (CFMIP) Observation Simulator Package, version 2 (COSP2), for both nadir and zenith geometries, and adds instrument-specific daytime/nighttime noise. We compare attenuated backscatter (Level 1) and retrieved particulate backscatter βpart(z) (Level 2) using two scattering-ratio (SR) definitions, and introduce a Comparability Score (CS) quantifying profile similarity via correlation and shape. Thin clouds yield high CS and comparable zenith/nadir measurements; thicker and multi-layer clouds do not, due to directional attenuation and retrieval instabilities. We also found that βpart(z) comparisons remain valid over a broader range of conditions than SR(z).

In real collocations, spatiotemporal separation is rarely negligible, so we select the best-matched profile pair by maximizing cross-correlation. We estimate this method's false discovery rate (the fraction of selected pairs that do not sample the same cloud) at 10–20%, using both a theoretical null model and an empirical one built from mismatched-date collocations. Applied to real collocations at 355 nm between the Atmospheric Lidar (ATLID) on the Earth Cloud, Aerosol and Radiation Explorer (EarthCARE) and the IPSL Atmospheric Research Lidar (IPRAL) across four representative cases, βpart(z) again agrees better than native-geometry SR(z), consistent with the simulation results.

We conclude that a spaceborne-to-ground-based cloud lidar comparison is meaningful, that is, not dominated by viewing geometry or by mismatched scenes, when three conditions are met: (1) candidate collocations are screened using the correlation coefficient and cloud vertical structure, rather than accepted by spatiotemporal proximity alone; (2) the collocated scene has a Comparability Score above 50; (3) the comparison variable, SR(z) or βpart(z) is chosen according to the scene's optical depth: both variables are comparable below τ = 0.7 and only βpart(z) is comparable above this threshold. We propose this decision scheme, with its threshold values, as a starting point for other spaceborne-to-ground-based cloud lidar validations.

Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. While Copernicus Publications makes every effort to include appropriate place names, the final responsibility lies with the authors. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.
Share
Artem G. Feofilov, Arezki Haddouche, Hélène Chepfer, Sergey Khaykin, Florian Lapouge, Patricia Delville, Marc-Antoine Drouin, Martial Haeffelin, Jean-Charles Dupont, Cheikh Dione, and Christophe Pietras

Status: open (until 01 Dec 2026)

Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor | : Report abuse
Artem G. Feofilov, Arezki Haddouche, Hélène Chepfer, Sergey Khaykin, Florian Lapouge, Patricia Delville, Marc-Antoine Drouin, Martial Haeffelin, Jean-Charles Dupont, Cheikh Dione, and Christophe Pietras

Model code and software

IPRAL-Lidar-Processing v1.0 Haddouche, A., and Feofilov, A. https://doi.org/10.5281/zenodo.23387966

Artem G. Feofilov, Arezki Haddouche, Hélène Chepfer, Sergey Khaykin, Florian Lapouge, Patricia Delville, Marc-Antoine Drouin, Martial Haeffelin, Jean-Charles Dupont, Cheikh Dione, and Christophe Pietras
Metrics will be available soon.
Latest update: 26 Oct 2026
Download
Short summary
Do a satellite and a ground-based laser see a cloud the same way? Yes, but only under specific conditions. Seen from above and from below, light is weakened differently, so thick clouds look different in the backscatter even with perfect instruments. Using simulations and real measurements, we show which clouds can be compared. As the instruments are rarely at the same spot, we pair observations by the similarity of their vertical shapes, not by distance. Our rules help check satellite data.
Share