the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
All-day global cloud physical properties products with 0.07° resolution retrieved from geostationary satellite imagers covering the period from 2000 to 2022
Lingxiao Zhao
Feng Zhang
Zhijun Zhao
Feng Lu
Jingwei Li
Wenwen Li
Clouds play a crucial role in the Earth's energy budget and the hydrological cycle. However, differences in the spatiotemporal resolution of satellite sensors and in retrieval algorithms lead to substantial heterogeneity among retrieved cloud products. Based on global geostationary satellite thermal infrared brightness temperature data from the Gridded Satellite (GridSat-B1) project, this study applied the single-layer Cloud retrieval model – Small Attention-UNet (Cloud-SmaAtUNet) algorithm in the DaYu CLoud Analysis System (DaYu-CLAS) to retrieve a global cloud product with a 3 h temporal resolution, 0.07° spatial resolution, and 23 year temporal span (2000–2022). This product is referred to as the DaYu Global Cloud physical properties Products (DaYu-GCP). The DaYu-GCP includes CLoud Phase (CLP), Cloud Top Height (CTH), Cloud Optical Thickness (COT), and Cloud Effective Radius (CER), covering all regions between 70° S–70° N and 180° W–180° E. Evaluation based on the Moderate-resolution Imaging Spectroradiometer (MODIS) official cloud products shows that the annual CLP identification accuracy of DaYu-GCP remains stable at 85 % ± 0.7 %, while the annual RMSE for CTH, COT, and CER stabilize at 1.50 ± 0.03 km, 10.71 ± 0.15, and 6.75 ± 0.10 µm, respectively. The multi-year variations in accuracy are within 2 %, with no evident interannual differences, and the spatiotemporal distributions are continuous. In addition, evaluation based on observations from the Cloud Profiling Radar and the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) indicates that the DaYu-GCP products show reasonable day–night consistency for optically thin cloud. Furthermore, the DaYu-GCP products are compared with other global cloud products. Taking the Northern Hemisphere as an example, the interannual variations of Cloud Cover Frequency (CCF), CTH, COT, and CER retrieved from DaYu-GCP show correlation coefficients of 0.760, 0.486, 0.764, and 0.514 with the ISCCP product, respectively, and 0.444, 0.778, 0.171, and 0.412 with the CLARA-A3 product. The DaYu-GCP dataset, which is stored in the Network Common Data Format (NetCDF), is freely available on the Science Data Bank at https://doi.org/10.57760/sciencedb.26292 (Zhao et al., 2026). The corresponding code can be found at https://github.com/lingxiao-zhao/DaYu-GCP (last access: 25 June 2025).
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Clouds within the Earth-atmosphere system play a vital role in regulating the planetary radiation balance (Wang et al., 2024; Zhang et al., 2025a) and in the global hydrological cycle (Liu et al., 2024; Viggiano et al., 2025). Therefore, obtaining a high-accuracy, long-term global dataset of cloud physical properties is essential for weather forecasting and climate-change research (Shi et al., 2025; Letu et al., 2023; Tang et al., 2025).
Satellite remote sensing is the primary means of obtaining cloud physical properties. Among these platforms, geostationary satellites can continuously monitor approximately one-third of the Earth's surface day and night, providing high-frequency observations at the minute scale for long-term cloud variability studies. For example, the Advanced Geostationary Radiation Imager (AGRI) onboard the FengYun (FY)-4A/B satellites operated by the National Satellite Meteorological Center of the China Meteorological Administration (NSMC-CMA) (Min et al., 2017; Min et al., 2020), as well as the Advanced Himawari Imager (AHI) onboard the Himawari-8/9 (H8/9) satellites operated by the Japan Aerospace Exploration Agency (JAXA), can monitor East Asia and the Pacific region (Bessho et al., 2016; Iwabuchi et al., 2018). The Spinning Enhanced Visible and Infra-Red Imager (SEVIRI) onboard the Meteosat Second Generation (MSG) satellites operated by the European Organisation for the Exploitation of Meteorological Satellites (EUMETSAT) provides observations over Africa and Europe (Donny Maladji et al., 1997; Coste et al., 2017; Kocaman et al., 2022). The Geostationary Operational Environmental Satellites (GOES)-R series operated by the National Oceanic and Atmospheric Administration (NOAA), including GOES-16 to GOES-19, are equipped with the Advanced Baseline Imager (ABI) to monitor the Americas (Bin et al., 2018, 2019, 2020; Heidinger et al., 2020). These geostationary satellite sensors provide observations every 10–15 min, with spatial resolutions of 0.5–1 km in the visible channels and 2–5 km in the infrared channels. In contrast to geostationary satellites, polar-orbiting satellites, such as the Moderate-resolution Imaging Spectroradiometer (MODIS) onboard Aqua and Terra (Platnick et al., 2015), cannot provide high-frequency continuous observations over a given region; however, since 2000 they have offered observations with higher spatial resolution (0.25–1 km).
Table 1Specifications of our DaYu-GCP dataset and the latest cloud physical property product dataset.
As shown in Table 1, based on satellite observation data, these sensors all provide official cloud physical characteristics product datasets, such as official products from the AGRI, AHI, ABI, and SEVIRI, as well as datasets from research initiatives like the Cloud Remote Sensing, Atmospheric Radiation and Renewable Energy (CARE). Most include physical characteristics such as CLoud Phase (CLP), Cloud Top Height (CTH), Cloud Optical Thickness (COT), and Cloud Effective Radius (CER), with spatial resolutions of 2–5 km and temporal resolutions of 10–15 min. However, these are all regional cloud products, and most lack night-time cloud coverage. In addition, channel spectral responses differ among sensors, and the official cloud product algorithms also vary across platforms. For example, the official AHI cloud products are mainly retrieved using the Comprehensive Analysis Program for Cloud Optical Measurement (CAPCOM) multifunctional algorithm system, which integrates multi-channel threshold methods and a dual visible-near-infrared Look-Up Table (LUT) approach. For liquid water clouds, the Mie-Lorenz scattering model is applied (Nakajima and Nakajma, 1995; Kawamoto et al., 2001), while for ice clouds, an extended Voronoi irregular ice crystal scattering model is used (Letu et al., 2020b), enabling daytime cloud detection and the retrieval of COT and CER (Imai and Yoshida, 2016; Mouri et al., 2016). The ABI official products are developed by the GOES-R Algorithm Working Group, which employs LUT-based retrievals constructed from visible and near-infrared radiances during daytime, while nighttime retrievals rely on thermal infrared channels (Walther and Heidinger, 2012; Minnis and Heck, 2012; Walther et al., 2013), ultimately achieving the retrieval of CLP, CTH, COT, and CER (Pavolonis, 2010; Heidinger, 2012). These differences prevent the direct integration of official geostationary satellite cloud products into a spatiotemporally continuous global cloud product.
Although several global cloud physical property datasets have been developed, such as the third edition of the Satellite Application Facility on Climate Monitoring's (CM SAF) cloud, albedo, and surface radiation dataset from Advanced Very High Resolution Radiometer (AVHRR) observations (CLARA-A3), which retrieves cloud amount, CTH, COT, and CER based on AVHRR measurements, its coverage is global but the temporal resolution is limited to 24 h and the spatial resolution to 0.25° (Karlsson et al., 2023a; Karlsson et al., 2023b). The International Satellite Cloud Climatology Project (ISCCP) uses AVHRR and approximately 10 km geostationary imagery to produce cloud amount, cloud types, Cloud Top Temperature (CTT), and COT products. However, the D series (3 h; 2.5°) (Schiffer and Rossow, 1983; Rossow et al., 1985; Rossow and Schiffer, 1991) and H series (3 h; 1°) (Young et al., 2018; Rossow et al., 2022) were discontinued in 2009 and 2017, respectively. Recent years have witnessed a surge in the application of machine learning and deep learning techniques for cloud property retrieval from satellite data (e.g., Iwabuchi et al., 2018; Wang et al., 2019, 2022a, b; Liu et al., 2022; Viggiano et al., 2025). For instance, the National Aeronautics and Space Administration (NASA) Satellite ClOud and Radiation Property retrieval System (SatCORPS) leverages such techniques with multiple sensors, including AHI and SEVIRI, to generate CLP, CTH, COT, and CER products. Although its temporal and spatial resolutions can reach 1 h and 3 km, respectively, the data are currently only available from 2023 onward (Trepte et al., 2019; Yost et al., 2021). These facts indicate that existing global cloud products are unable to simultaneously achieve both long temporal coverage and high spatiotemporal resolution.
Therefore, this study employs the single-layer Cloud retrieval model – Small Attention-UNet (Cloud-SmaAtUNet), within the DaYu CLoud Analysis System (DaYu-CLAS) to develop an all-day Global Cloud physical properties Products (GCP) retrieval algorithm (DaYu-CLAS) (Zhao et al., 2023, 2024; Tong et al., 2023; Li et al., 2023a). Further details about the DaYu-CLAS can be accessed at its project website: https://fdu-crias.fudan.edu.cn/ (last access: 21 February 2026). The Cloud-SmaAtUNet model of DaYu-CLAS takes globally mosaicked thermal infrared channel brightness temperature data from the Gridded Satellite (GridSat-B1) project as input, and is trained using MODIS official cloud products as labels. This approach not only combines the global coverage of the geostationary satellite product GridSat-B1 with the high-precision observation advantages of the polar-orbiting satellite MODIS, but also maximizes the extraction of spatial structural information within clouds, thereby enabling all-day, high-accuracy global retrievals of CLP, CTH, CER, and COT products, collectively referred to as DaYu-GCP. The DaYu-GCP products achieve a temporal resolution of 3 h, a spatial resolution of 0.07°, and a time span of 23 years (2000–2022), covering all regions between 70° S–70° N in latitude and 180° W–180° E in longitude, and can provide essential data support for studies of radiative balance, the hydrological cycle, and related processes.
This paper provides further details on the DaYu-GCP dataset records, including input data, algorithm explanations, product examples, and validation results. Section 2 briefly introduces data preparation and methods, while Sect. 3 introduces, discusses and evaluates four major products: CLP, CTH, COT and CER. Additionally, DaYu-GCP was compared with existing global cloud datasets ISCCP and CLARA-A3. Section 4 describes the availability of the data. Section 5 is the conclusion.
2.1 Data
This study employed three datasets: GridSat-B1 geostationary satellite data, polar-orbiting satellite data, and reanalysis data. Further details are provided in Table 2.
2.1.1 GridSat-B1 data
The primary source of geostationary infrared-channel brightness temperature data used in this study is the GridSat-B1 dataset. Over the 23 year study period (2000–2022), a total of 24 satellites from four countries or regions contributed to the construction of the GridSat-B1 dataset, as shown in Fig. 1. This global dataset integrates observations from multiple geostationary satellites to provide Top-of-Atmosphere (TOA) infrared brightness temperatures from two bands: the Infrared Water-Vapor band (IRWVP, 6.7 µm) and the Infrared Window band (IRWIN, 11 µm). In addition to IRWVP and IRWIN, and in consideration of the physical generation mechanisms and developmental processes of clouds, the satellite identifiers (Satid) associated with the infrared brightness temperature data, together with the corresponding Satellite Zenith (SAZ) angles, have been included in the input data. The parsing procedure for Satid and SAZ in the auxiliary data is described in the GridSat-B1 documentation (Knapp et al., 2011). Additionally, the official documentation indicates that zenith-angle correction for infrared brightness temperature images may be referenced in Joyce et al. (2001). Because the IRWVP and IRWIN grid integrated products may originate from different satellites, Satid is divided into IRWVP satellite identifiers (Satid_VP) and IRWIN satellite identifiers (Satid_IN), and SAZ is similarly separated into IRWVP SAZ (SAZ_VP) and IRWIN SAZ (SAZ_IN). GridSat-B1 has a standard spatial grid resolution of 0.07° and a temporal resolution of 3 h, corresponding to standard synoptic times of 00:00, 03:00, …, 21:00 UTC. For each grid point, the measurement closest to the satellite nadir is selected. Missing data at these specified times are supplemented from ISCCP (Young et al., 2018) using the temporally nearest available image.
2.1.2 Polar orbit satellite data
The MODIS instrument operates aboard two polar-orbiting satellites: Terra (launched in December 1999) and Aqua (launched in April 2002). With 36 spectral channels and a global revisit frequency of 1–2 d, MODIS's broad spectral coverage supports a wide range of applications, including vegetation-health monitoring, land-cover classification, sea-surface temperature retrieval, and cloud analysis (Menzel et al., 2008; Cai et al., 2011; Hosen et al., 2023). In this study, cloud physical properties from the MODIS Level-2 cloud product (Collection 6.1) were used as training labels, specifically CLP, CTH, CER, and COT. This product, identified by the code “06”, provides data from the Terra platform (MOD06) and the Aqua platform (MYD06). Owing to its well-characterized accuracy and high data quality, the MODIS Collection 6.1 product is widely utilized as a benchmark in remote-sensing studies (Zhang et al., 2017). The Cloud Profiling Radar and Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) instrument, mounted on the Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observation (CALIPSO) satellite, was launched in April 2006 and ceased operations in June 2023 (Winker et al., 2010). CALIPSO provides global observations of the vertical structure and characteristics of aerosols and thin clouds (Hagihara et al., 2010; Zhang et al., 2017). The assessment of model accuracy primarily utilized official cloud products from MODIS and CALIOP.
The CLP, CTH, COT, and CER selected from the MODIS official cloud products in this study originate from the Cloud_Phase_Infrared_1km, cloud_top_height_1km, Cloud_Optical_Thickness, and Cloud_Effective_Radius variables, respectively. The CLP, CTH, and COT from the CALIOP official cloud product are derived from the Feature_Classification_Flags, Layer_Top_Altitude, and Column_Optical_Depth_Cloud_532 variables, respectively.
2.1.3 ERA5 data
Meteorological field data are obtained from the European Center for Medium-Range Weather Forecasts (ECMWF) Reanalysis v5 (ERA5) dataset (Hersbach et al., 2020). This study selected ERA5 hourly Air Temperature Profiles (ATP), Relative Humidity Profiles (RHP), Skin Temperature (SKT), Total Column Water Vapor (TCWV) and Land Cover with a spatial resolution of 0.25°. Excessively dense pressure levels in the input data may introduce unnecessary model redundancy and adversely affect training and operational efficiency. Therefore, ATP and RHP were each extracted at four identical pressure levels: 1000, 850, 500, and 300 hPa (Zhao et al., 2024; Liu et al., 2025).
Figure 2Flowchart of DaYu-GCP production. It is worth noting that the input data consists of 19 channels, including GridSat-B1 and ERA5, while the target is CLP, CTH, COT, and CER images from MODIS official product processed to the same resolution. The training input and output image sizes are both 64 × 64. For each target, this study conducted model training, validation and evaluation separately. Finally, a sliding window fusion strategy was used to produce global-scale cloud product data.
2.2 Method
In our earlier work, we introduced the DaYu Cloud-Radiation-Precipitation analysis Systems (DaYu-CRPS), which includes three core components: the DaYu Radiative Transfer Model (DaYu-RTM) (Zhang et al., 2019; Li et al., 2020; Li et al., 2023b; Cai et al., 2023, 2025; Wu et al., 2026), the DaYu-CLAS (Zhao et al., 2023, 2024; Tong et al., 2023; Li et al., 2023a; Xiao et al., 2025b; Li et al., 2022, 2024), and the DaYu PRecipitation Analysis System (DaYu-PRAS) (Xiao et al., 2025a; Yang et al., 2026). The DaYu-RTM is dedicated to simulating the imager measurements and radiative transfer calculations. DaYu-CLAS integrates both single-layer and double-layer cloud retrieval models. DaYu-PRAS incorporates the TPWDiff-CB (Xiao et al., 2025a) and RePPIC-Net (Yang et al., 2026) models for precipitation monitoring and nowcasting. Specifically, the DaYu-CLAS framework integrates several single-layer cloud retrieval models, including Cloud-ResUNet (Zhao et al., 2023, 2024; Tong et al., 2023), Cloud-SmaAtUNet (Li et al., 2023a), CloudDiff (Xiao et al., 2025b). For double-layer cloud retrieval, it employs two models: Overlap-CloudDiff (Li et al., 2026) and the hybrid algorithm that combines DaYu-RTM simulation with deep learning (Li et al., 2022, 2024). Cloud-SmaAtUNet is an improved version of UNet, in which depthwise separable convolutions and convolutional block attention modules (CBAM) are integrated into both the encoder and decoder paths. Li et al. (2023a) applied Cloud-SmaAtUNet to H8-AHI data and demonstrated that Cloud-SmaAtUNet achieves high accuracy and efficiency in cloud physical properties retrieval tasks. However, that study focused on a single sensor and produced cloud products for only one year (2017), which is insufficient to support studies of global cloud physical properties at high spatiotemporal resolution.
Therefore, in this study, the Cloud-SmaAtUNet model is applied to achieve global all-day cloud physical properties retrievals, as shown in Fig. 2. Due to the different institutional sources of the datasets, they may have different projection methods and spatiotemporal resolutions. To ensure the correct correspondence of pixels and data consistency, the data were first aligned to a unified 0.07° latitude and longitude grid before model construction. Temporal matching was conducted based on the respective temporal characteristics of the datasets. MODIS and ERA5 data, available at synoptic hours (00:00, 03:00, …, 21:00 UTC), were directly matched. In contrast, CALIOP data, were included by selecting profiles within a ± 2 min window around each corresponding synoptic hour. Because the GridSat-B1 images are too large to be directly used as model inputs, each image is divided into multiple 64 pixel × 64 pixel sub-images. After data preprocessing, Cloud-SmaAtUNet is trained using brightness temperature (BT) from the 6.7 and 11 µm channels and the SAZ as the primary inputs, with CLP, CTH, COT, and CER from the MODIS official cloud products as labels. Considering the influence of meteorological conditions on cloud formation and development, additional meteorological variables, such as temperature and humidity profiles, are incorporated as auxiliary inputs. In this way, a DaYu-GCP dataset with a temporal resolution of 3 h and a spatial resolution of 0.07° is retrieved. Finally, the products are validated using the MODIS and CALIOP official cloud products to evaluate their spatiotemporal continuity and day–night consistency.
During model parameter training, the spatiotemporally matched dataset comprised approximately 700 000 sample pairs. Data spanning 2000–2021 were used as the training set, while the entire dataset from 2022 constituted the testing-set. These samples were evenly distributed across the spatial domain, and the strategy for selecting the training and testing-sets satisfied the basic requirements of Cloud-SmaAtUNet. This selection strategy, together with the large overall sample size, jointly reduces the risk of model overfitting. To further expand the training data, data augmentation operations – including horizontal flipping, vertical flipping, and rotations of 90, 180, and 270° – were applied to the training set, increasing its size to 6 times the original. Meanwhile, the testing-set remained unchanged, without any augmentation, in order to objectively evaluate the effectiveness of data augmentation in improving model performance. Indeed, the application of data augmentation led to improved accuracy. Detailed information on the dataset is provided in Table 3.
Key parameters for model training include: batch size = 512, maximum epochs = 300, and learning rate = 0.001. An early-stopping strategy was adopted, whereby training was terminated if the loss on the testing-set did not decrease by more than 0.1 for 15 consecutive epochs. All models converged and stopped before reaching the maximum of 300 epochs. The loss functions used for model training varied by task. Cross-Entropy Loss was employed for the CLP classification task, whereas MSE Loss was applied to the CTH, COT, and CER regression tasks. To achieve seamless global coverage of the cloud products, an image sliding-window fusion strategy was implemented to eliminate gaps between adjacent small samples; details of this method are provided in Sect. S1 in the Supplement. For model evaluation, statistical metrics for classification performance included Accuracy, Recall, Precision, and F1-score, while regression performance was assessed using root mean squared error (RMSE), mean absolute error (MAE), mean bias error (MBE), and Pearson correlation coefficients (R).
Figure 3Detailed distribution of testing-set evaluations on Cloud-SmaAtUNet (left column) and Cloud-RF (right column). (a, b) Confusion matrix for CLP. Scatter density distribution diagram under the kernel density estimation of (c, d) CTH. (e, f) COT. (g, h) CER between MODIS official and DaYu-CLAS Cloud-SmaAtUNet or DaYu-CLAS Cloud-RF products.
3.1 Evaluation of model performance in testing-set
To enhance the physical interpretability of the model, the pixel-based (point-to-point) Cloud retrieval machine learning model Random Forest (Cloud-RF) (Breiman, 2001) was employed as a comparative benchmark. Here, a grid-search approach was used to determine the Cloud-RF model parameters, with n_estimators = 200, max_depth = 50, min_samples_split = 3, and min_samples_leaf = 1. Using the 2022 test dataset, we compared the performance of the Cloud-SmaAtUNet and Cloud-RF models. Compared with the MODIS official products, Cloud-SmaAtUNet achieved an overall accuracy of 82.3 % in the CLP classification task. The recognition accuracies of Cloud-SmaAtUNet for clear sky, water clouds, and ice clouds reached 81.52 %, 80.21 %, and 86.38 %, respectively (Fig. 3a). In addition, Cloud-SmaAtUNet also exhibited relatively dense joint probability density distributions aligned along the diagonal in the regression tasks for CTH, COT, and CER. Although Cloud-SmaAtUNet showed a systematic underestimation (MBE < 0), the estimation errors for CTH, COT, and CER remained within acceptable ranges (Fig. 3c, e, and g). The RMSE (MAE) values were 1.617 km (0.954 km), 11.314 (6.871), and 7.181 µm (5.133 µm), respectively, with R of 0.926, 0.617, and 0.799. These results indicate that Cloud-SmaAtUNet exhibits excellent performance in the retrieval of cloud physical properties.
In contrast, the performance of the Cloud-RF model in cloud retrieval declined across all products. The overall accuracy of Cloud-RF in the CLP classification task decreased to 78.1 % (Fig. 3b). Among the classes, the recognition accuracy for water clouds decreased most markedly (73.44 %), while those for clear sky and ice clouds also showed slight reductions (78.93 % and 85.19 %, respectively). This indicates that Cloud-RF performs worse than Cloud-SmaAtUNet in CLP classification. Moreover, in the regression tasks for CTH, COT, and CER, Cloud-RF exhibited more pronounced underestimation than Cloud-SmaAtUNet (MBE < 0 with larger magnitude), and the joint probability density distributions aligned along the diagonal were less concentrated (Fig. 3d, f, and h). The RMSE (MAE) values were 2.369 km (1.483 km), 13.370 (8.935), and 8.860 µm (6.535 µm), respectively, with R of 0.843, 0.565, and 0.719. These results demonstrate that, compared with Cloud-SmaAtUNet, the Cloud-RF model shows inferior performance in retrieving cloud physical properties.
Compared with the conventional Cloud-RF, Cloud-SmaAtUNet can leverage the spatial structure information of clouds to improve cloud physical properties retrievals. The accuracy of CLP is increased by 5.4 %, while the RMSE of CTH, COT, and CER are reduced by 31.7 %, 18.2 %, and 23.4 %, respectively. Beyond the performance differences, Cloud-SmaAtUNet requires only about 100 s to retrieve a single global image, whereas Cloud-RF takes nearly 6 times longer, approximately 630 s. These findings are also reflected in other studies (Zhao et al., 2024).
3.2 Physical interpretability of the Cloud-SmaAtUNet model
To elucidate the physical interpretability of the model, we investigated the roles of BT and meteorological fields in cloud retrieval. This experiment involved feature ablation testing, comparing model performance across different input combinations (BT only, ERA5 only, BT and ERA5) to analyze each data source's contribution to retrieval accuracy. Specifically, for both the Cloud-SmaAtUNet and Cloud-RF models, three distinct input configurations were employed: Group 1 incorporated 11 and 6.7 µm BT along with the full set of ERA5 meteorological fields; Group 2 comprised solely 11 and 6.7 µm BT data; Group 3 comprised solely ERA5 meteorological field data. These experiments utilized both Cloud-SmaAtUNet and Cloud-RF models for training and evaluation, with results presented in Table S1 in the Supplement and Fig. 4.
Figure 4Cloud-SmaAtUNet was evaluated for RMSE across three distinct input datasets, with results presented for different value ranges. Group 1 inputs comprise 11 and 6.7 µm BT alongside ERA5. Group 2 inputs comprise 11 and 6.7 µm BT. Group 3 inputs comprise ERA5. (a) CTH. (b) COT. (c) CER.
Figure 5Evaluation of (a) CLP classification accuracy and Recall (b) CTH (c) COT (d) CER regression RMSE and MBE results based on training-set and testing-set of Aqua and Terra MODIS official cloud products.
The CLP classification results in Table S1 indicate that when using only ERA5, the Cloud-SmaAtUNet classification Accuracy for clear sky, water cloud, and ice cloud were 66.06 %, 63.64 %, and 68.16 %, respectively; when using only BT, the Accuracy was 78.86 %, 79.43 %, and 83.96 %. Using BT and ERA5 together, the classification Accuracy for clear sky, water cloud, and ice cloud improved to 81.52 %, 80.21 %, and 86.38 %, representing increases of 23.4 %, 26.0 %, and 26.7 % compared to using ERA5 alone, and increases of 19.4 %, 24.8 %, and 23.2 % compared to using BT alone.
The results of the regression tasks are shown in Fig. 4. When using ERA5 alone, the RMSE of CTH, COT, and CER retrieved by Cloud-SmaAtUNet across different ranges were 2.1–7.2 km, 12.9–82.9, and 7.0–25.3 µm, respectively. When using only BT, the RMSE was 1.5–6.0 km, 9.2–63.7, and 4.8–24.1 µm. When using BT and ERA5 together, the RMSE of CTH, COT, and CER decreased to 1.1–5.1 km, 6.0–45.9, and 2.8–21.4 µm. These results indicate that using BT and ERA5 together, compared to using only BT (or only ERA5), reduces the RMSE of CTH, COT, and CER on average by 21.0 % (63.5 %), 39.5 % (90.3 %), and 42.6 % (85.6 %), respectively.
The above experimental results indicate that satellite-observed BT represents an integrated signature of clouds, the atmosphere, and surface types. In the cloud retrieval process based on BT, incorporating atmospheric background fields and surface information contributes to the accurate retrieval of cloud physical properties.
3.3 Evaluation of DaYu-GCP with MODIS official products
To assess the interannual stability of the DaYu-GCP products, we validated them using the Aqua/Terra MODIS official cloud products over the period 2000–2022, as shown in Fig. 5. In terms of CLP identification, the Accuracy and Recall for all years are approximately 0.85 ± 0.007. Although there are slight fluctuations in accuracy across years – for example, slightly lower in 2004 and slightly higher in 2010 – the differences are minor. This demonstrates that the Cloud-SmaAtUNet model possesses robust cloud detection capability. For the retrievals of CTH, COT, and CER, the annual RMSE values remain stable at 1.50 ± 0.03 km, 10.71 ± 0.15, and 6.75 ± 0.10 µm, respectively, with coefficients of variation (standard deviation/mean) of 2.0 %, 1.4 %, and 1.5 %. These results indicate that DaYu-GCP exhibits stable accuracy across years. The MBE for CTH, COT, and CER across all years range from −0.007 to −0.059 km, −0.536 to −0.649, and −0.069 to −0.283, respectively. Although the MBE deviations are very small, the dataset still exhibits a slight systematic negative bias.
Figure 7Variation in 23 year average accuracy of (a) CLP and RMSE for (b) CTH, (c) COT, and (d) CER across different longitudes.
We also analyzed the spatiotemporal distribution of spatial discrepancies between DaYu-GCP and MODIS official cloud products from 2000 to 2022. Figure 6 shows the latitudinal distribution of differences between DaYu-GCP and MODIS official cloud products, with statistical results averaged every 3°. Figure 7 shows the longitudinal distribution of differences between DaYu-GCP and MODIS official products, with statistical results averaged every 5°. In both Figs. 6 and 7, the mean values (blue dots), one Standard Deviation (STD) above and below the mean (blue shading), and box plots (upper bound, lower bound, upper quartile, lower quartile, and median) are presented.
Firstly, the latitudinal distribution of CLP exhibits minimal variation, with overall accuracy reaching approximately 0.85. Accuracy increases slightly with increasing latitude. Additionally, the spatial error distributions of CTH and CER in Fig. 6b and d are relatively consistent, showing higher values near the equator than in other regions. This is primarily because CTH and CER values near the equator are inherently larger, leading to correspondingly larger error margins during model evaluation (Fig. 11l and o). Mitra et al. (2021) compared MODIS CTH with Lidar observations and found that CTH errors are smaller for low clouds and larger for high clouds. Since cloud heights near the equator are inherently higher, this results in larger errors in CTH retrieval. Zhang et al. (2025b) also found that in equatorial and low-latitude regions, the high mixing of ice and water clouds and complex infrared absorption patterns lead to higher CER values, which in turn result in larger errors during model evaluation. Finally, as shown in Fig. 6c, COT errors are smaller near the equator and gradually increase with latitude.
Figure 7 shows that for all products, the indicators exhibit clear peak-trough cycles along the longitudinal direction, with the mean Accuracy of CLP fluctuating between 0.82 and 0.88. The mean RMSE of CTH, COT, and CER vary between 1.3–2.1 km, 7–13, and 6.7–8.2 µm, respectively. This may be because regions with larger fluctuations correspond to fewer samples in the MODIS products, resulting in less stable evaluation results.
Figure 8CLP accuracy and RMSE of CTH and COT for DaYu-GCP during daytime and nighttime using CALIPSO/CALIOP data: (a) CLP accuracy, (b) CTH RMSE, (c) COT RMSE. The COT evaluation employs optically thin clouds labeled as “transparent” in CALIOP. The blue bar chart shows the model's daytime accuracy, and the yellow bar chart shows the model's nighttime accuracy.
3.4 Evaluation of DaYu-GCP with CALIOP official products
In this study, we evaluated the consistency of daytime and nighttime performance of the DaYu-GCP results using CALIPSO/CALIOP data in 2022. Compared with the active sensors CALIPSO/CALIOP, the Accuracy of CLP during the day and night are 0.787 and 0.775, respectively (Fig. 8a). The daytime and nighttime RMSE of CTH are 3.384 and 3.568 km, respectively (Fig. 8b). For the evaluation of COT, given that CALIOP cannot penetrate thick cloud layers, this assessment considered only optically thin cloud layers labeled as transparent in the CALIOP data as ground-truth references. Correspondingly, within DaYu-GCP, only optically thin cloud regions with a thickness less than 5 were compared against CALIOP measurements. Finally, the daytime and nighttime RMSE of the COT product are 2.836 and 3.002, respectively (Fig. 8c). Overall, the model results demonstrate good consistency between day and night.
Figure 9Comparison of MODIS and DaYu-GCP annual accuracy against CALIOP standards for (a) CLP, (b) CTH RMSE, and (c) COT RMSE. The COT evaluation is restricted to optically thin clouds, defined as CALIOP “transparent” layers and MODIS clouds with COT < 5.
Figure 9 presents the validation of DaYu-GCP and MODIS official products against the CALIOP official products for three variables: CLP, CTH, and COT. For CLP, the overall Accuracy of DaYu-GCP shows relatively small variation, with a mean value of approximately 0.76. The Accuracy for clear sky, water clouds, and ice clouds are about 0.74, 0.76, and 0.77, respectively, which are slightly lower than those of MODIS, whose overall Accuracy is around 0.80, with clear sky, water cloud, and ice cloud Accuracy of approximately 0.76, 0.79, and 0.81, respectively (Table 4). For CTH, the multi-year RMSE of DaYu-GCP ranges from 3.35 to 3.53 km, slightly higher than that of MODIS (3.09–3.32 km). For COT, the multi-year RMSE of DaYu-GCP ranges from 3.59 to 4.08, also slightly higher than MODIS (2.57–3.18). Using the CALIOP official products as the reference, the annual RMSE for CTH and COT remain stable at 3.42 ± 0.15 km and 3.84 ± 0.16, with coefficients of variation of 4.4 % and 4.1 %, respectively. Overall, the DaYu-GCP products demonstrate stability in both day–night accuracy and interannual variations.
3.5 Spatiotemporal distribution characteristics of clouds
Since MODIS is carried on polar-orbiting satellites, the spatial coverage of cloud products at any given time is limited, making large-scale, synchronous global observations difficult. Consequently, the spatiotemporal distribution characteristics of the retrieved cloud physical properties lack representativeness.
Here, we initially defined and calculated three physical quantities characterizing cloud cover based on the CLP product: Ice Cloud Fraction (ICF), Water Cloud Fraction (WCF), and Total Cloud Fraction (TCF) (Zhao et al., 2024). To ensure that spatiotemporally matched samples achieve global coverage, this study employed a 1.5 h temporal resolution and used MODIS transit times as the reference for spatiotemporal matching between DaYu-GCP and MODIS data. Monthly and annual average distributions were subsequently calculated.
Figure 10Annual average spatial distribution of global cloud physical products from 2020 to 2022, respectively: ICF (a–c), WCF (d–f), TCF (g–i), CTH (j–l), COT (m–o), and CER (p–r). Vertically, these are the averages of the MODIS official cloud products with a 1.5 h transit time interval (a, d, g, j, m, and p), the averages of DaYu-GCP at the same MODIS transit time and coverage location (b, e, h, k, n, and q), and the averages of DaYu-GCP's all-day global products at all times (c, f, i, l, o, and r).
Annual mean values for each year from 2020 to 2022 are presented in Fig. 10, while the corresponding seasonal means (DJF, MAM, JJA, and SON) are shown in Figs. S1–S4 in the Supplement. Comparison of the results indicates that the MODIS official product and the DaYu-GCP product are highly consistent with respect to ICF, WCF, TCF, CTH, COT, and CER at MODIS transit times (Fig. 10a, d, g, j, m, p and Fig. 10b, e, h, k, n, q), particularly in equatorial regions. Since MODIS transits only at 10:30 AM and 1:30 PM local time, these annual averages do not fully capture the spatiotemporal characteristics of cloud physical properties throughout the day. In contrast, the all-day global DaYu-GCP, which provides complete spatial coverage, compensates for this limitation, representing a significant improvement over the official MODIS products (Fig. 10a, d, g, j, m, p and Fig. 10c, f, i, l, o, r).
Additionally, DaYu-GCP was compared with the global cloud datasets ISCCP and CLARA-A3. The four variables involved in the comparison were CCF, CTH, CER, and COT. For ISCCP, the base HGG data itself provides global 3 h CCF and COT. CTH can be derived from the provided CTT, and CER can be calculated from the available COT and Cloud Water Path (CWP) (Schiffer and Rossow, 1983; Rossow et al., 1996; Young et al., 2018). For CLARA-A3, the dataset provides global daily mean CCF and CTH directly, whereas COT and CER can be derived from Ice Water Path (IWP) and Liquid Water Path (LWP) (Nakajima and King, 1990).
Figure 11CCF, CTH, COT and CER anomaly change curves for the period 2000 to 2022 across the 60° N to 60° S latitude zone, derived from DaYu-GCP, ISCCP and CLARA-A3 products. Statistical data are presented separately for the Northern and Southern Hemispheres. The black, red and blue curves represent DaYu-GCP, ISCCP and CLARA-A3, respectively. In the corner, we have labelled the Pearson correlation coefficients RISCCP and RCLARA-A3. RISCCP denotes the correlation coefficient between DaYu-GCP and ISCCP. RCLARA-A3 denotes the correlation coefficient between DaYu-GCP and CLARA-A3. (a) and (e) are CCF variables. (b) and (f) are CTH variables. (c) and (g) are COT variables. (d) and (h) are CER variables.
To clearly compare the annual variability of cloud physical properties among different products, monthly anomaly time series of each parameter were constructed for the Northern and Southern Hemispheres based on the monthly mean data from each product, and R between DaYu-GCP and the other two datasets were calculated (Fig. 11). DaYu-GCP exhibits higher correlations with ISCCP in CCF, COT, and CER; for the Northern Hemisphere, the R reach 0.760, 0.764, and 0.514, respectively. DaYu-GCP shows higher correlation with CLARA-A3 in CTH, with R = 0.778 for the Northern Hemisphere. The Southern Hemisphere exhibits similar results. Among all R values, CER shows the lowest correlation compared to CCF and CTH; for the Northern Hemisphere, R values between DaYu-GCP and ISCCP, DaYu-GCP and CLARA-A3, and ISCCP and CLARA-A3 are 0.514, 0.412, and 0.219, respectively. This indicates that CER remains a challenging parameter in future cloud physical properties datasets. These comparison results demonstrate that, as a new cloud product, DaYu-GCP exhibits reasonable consistency in the spatiotemporal variability of major cloud parameters with the two long-standing global datasets, ISCCP and CLARA-A3. This underscores the reliable data quality of DaYu-GCP and its potential as a consistent data source for global cloud-climate studies.
The DaYu-GCP data described in this paper have been made publicly available. We would like to express our special thanks to Science Data Bank and its staff for their help and support in the data publication process. DaYu-GCP can be accessed at https://doi.org/10.57760/sciencedb.26292 (Zhao et al., 2026). Moreover, the matching dataset employed to train the models in this study is also publicly available and can be accessed at https://doi.org/10.57760/sciencedb.27171 (Zhao, 2025).
This study developed and released the first all-day, high spatiotemporal resolution global cloud physical properties product, DaYu-GCP. The product spans the period from 2000 to 2022, with a temporal resolution of 3 h and a spatial resolution of 0.07°, covering all regions between 70° S and 70° N. It includes four key cloud physical properties: CLP, CTH, COT, and CER. Systematic quality assessments indicate that the DaYu-GCP product demonstrates reliable accuracy, strong stability, and good consistency. The specific conclusions are as follows:
- 1.
Compared with the MODIS official products, the classification Accuracy of CLP reaches 82.3 %, and the RMSE of CTH, COT, and CER are 1.617 km, 11.314, and 7.181 µm, respectively. Interannual evaluations show that the CLP Accuracy remains stable at approximately 0.85 ± 0.007, while the RMSE of CTH, COT, and CER remain stable at 1.50 ± 0.03 km, 10.71 ± 0.15, and 6.75 ± 0.10 µm, with coefficients of variation of 2.0 %, 1.4 %, and 1.5 %, respectively. This indicates that the accuracy of DaYu-GCP exhibits no significant interannual differences.
- 2.
Compared with the CALIOP official products, the day–night Accuracy of CLP are 0.787 and 0.775, respectively; the day–night RMSE of CTH are 3.384 and 3.568 km, and the day–night RMSE of COT are 2.836 and 3.002 for optically thin cloud. These results demonstrate reasonable day–night consistency of the product.
- 3.
The product shows reasonable correlations with ISCCP and CLARA-A3 datasets in both hemispheres. For example, in the Northern Hemisphere, the correlations of CCF and COT with ISCCP are high (R = 0.760 and 0.764), while CTH shows a stronger correlation with CLARA-A3 (R = 0.778). The correlations of CER between DaYu-GCP and ISCCP, DaYu-GCP are slightly lower (R = 0.514 and 0.412), whereas the R between ISCCP and CLARA-A3 themselves is only 0.219, indicating that DaYu-GCP maintains higher spatiotemporal consistency with global cloud products ISCCP and CLARA-A3, although the CER retrieval algorithm still requires further development in future studies.
In summary, DaYu-GCP fills the gap in existing global cloud property products that simultaneously offer high spatiotemporal resolution and long-term coverage. The dataset combines high accuracy, strong stability, and robust consistency, and is publicly accessible, making it a valuable resource for studies of cloud-climate feedbacks and the global energy and water cycles. Furthermore, additional research is required in the future to explore how to enhance the data for cloud physical property products in the polar regions and continuously improve observational capabilities to obtain more reliable COT and CER products.
The supplement related to this article is available online at https://doi.org/10.5194/essd-18-1813-2026-supplement.
LZ contributed to conceptualization, methodology, writing-original draft, investigation, validation, data curation, drawing. FZ contributed to supervision, writing-review and editing, funding acquisition. ZZ contributed to investigation, discussion, writing-review and editing. FL contributed to supervision, discussion. JL contributed to investigation, validation. BG contributed to discussion, writing-review and editing. WL contributed to discussion, investigation. All authors reviewed the manuscript.
The contact author has declared that none of the authors has any competing interests.
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. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.
We thank the National Centers for Environmental Information and European Centre for Medium-Range Weather Forecasts for the provided datasets. We are also deeply grateful to the two anonymous reviewers for their constructive suggestions, and to the editor and ESSD editorial staff for their assistance.
This work was supported by the National Key Research and Development Program of China (grant no. 2024YFF0808303) and National Natural Science Foundation of China (grant no. 42305146). The computations in this research were performed using the CFFF platform of Fudan University.
This paper was edited by Jing Wei and reviewed by two anonymous referees.
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