Skip to main content
PLOS One logoLink to PLOS One
. 2025 Aug 18;20(8):e0327220. doi: 10.1371/journal.pone.0327220

A lightweight intelligent compression method for fast Sea Level Anomaly data transmission

Xiaodong Ma 1, Xiang Wan 1, Lei Zhang 1,*, Dong Wang 1, Zeyuan Dai 1
Editor: Hui Li2
PMCID: PMC12360586  PMID: 40824961

Abstract

Traditional compression methods struggle to preserve critical mesoscale ocean features like vortices during bandwidth-constrained marine data transmission. To aaddress this limitation, we propose CompressGAN, a novel deep learning framework that transcends conventional approaches reliant on generic image metrics (e.g., peak signal-to-noise ratio, PSNR; structural similarity index, SSIM). The architecture integrates global-local dual discriminators to enforce spatiotemporal coherence of mesoscale vortices, employs dilated convolutions to enhance feature receptive fields without computational overhead, and incorporates vortex recognition rate as a physics-aware evaluation metric. Furthermore, parametric pruning and adaptive quantization strategies are embedded to optimize memory efficiency for shipborne hardware constraints. Validation across multiple ocean reanalysis datasets demonstrates CompressGAN’s superiority at 4 × compression ratios, achieving 91.46% mesoscale eddy identification accuracy (Iden) versus SRGAN (89.71%) and SRResNet (89.82%), while maintaining operational efficiency (148 s/image inference time, 25 GB peak memory). Generalization tests reveal controlled performance degradation: PSNR reduced by 4.2 ± 0.3 dB, SSIM by 0.7126, and Iden by 4.1%, confirming robustness under marine operational scenarios. This work resolves the critical trade-off between vessel-mounted computational limits and real-time ocean data demands, providing a viable pathway for integrated shipboard systems to reconcile multimodal marine data processing with navigation service requirements.

1. Introduction

With the rapid development of ocean observation technology, grid ocean data with high spatial and temporal resolutions have become an important basis for modern marine scientific research [1–4]. The wide application of satellite remote sensing, numerical models, and distributed sensor networks has enabled the acquisition frequency and coverage of global marine environmental parameters to reach unprecedented levels. These cubes contain physical parameters such as temperature, salinity, and velocity (in this paper, the sea surface height anomaly is the main research direction). However, the contradiction between the exponential growth of the data volume and the demand for long-distance transmission is becoming increasingly prominent, especially in special scenarios such as deep sea observations and polar research; thus, achieving efficient and reliable data transmission has become a technical bottleneck restricting real-time marine monitoring and collaborative research.

Existing data compression techniques face significant challenges in dealing with grid ocean data. Although conventional lossless compression algorithms (such as GZIP [5] and LZ77 [6]) can maintain data integrity, it is usually difficult for their compression rates to exceed 50%, and the computational complexity increases nonlinearly as the data dimensions increase. Although lossy compression methods (such as the discrete cosine transform and wavelet transform) can improve the compression efficiency [7], they may destroy the unique spatial continuity and physical conservation characteristics of marine data. For example, overcompression of thermohaline profile data leads to spatial gradient distortion of mesoscale vortex structures, which affects the initial field accuracy of ocean circulation models [8]. The special data formats developed in recent years for earth science research (such as NetCDF and HDF5) have improved the storage efficiency through metadata optimization and dimension reorganization [9], but they have not fundamentally solved the bandwidth constraint problem in the transmission stage. The emerging intelligent compression technology provides new possibilities for data volume reduction [10–14]. Moreover, feature extraction methods based on deep learning, such as convolutional autoencoders, can identify nonlinear coupling relationships between ocean parameters and achieve high magnification compression through latent spatial mapping. Studies have shown that such methods can achieve a compression rate of more than 90% for data with strong spatial correlation, such as ocean and atmosphere parameterized grid data, while maintaining the main dynamic characteristics [15–19]. For Marine satellite remote sensing data, Fanelli et al., based on an expanded super-resolution network, achieved an effective resolution improvement for the publicly available abnormal sea surface temperature data and verified the validity of the data from a sub-mesoscale perspective [20]. Nardelli et al. achieved targeted resolution improvement for SLA data by adding an attention mechanism to the existing super-resolution network. They verified it using the MSE metric among multiple baseline models and obtained good model verification effects in the experimental results [21]. Cui et al. used an improved super-resolution model of deep learning gradient constraint embedding method to enhance the resolution of sea surface height data and obtained experimental results with more promising application prospects in Marine engineering [22].

However, data compression requirements and application accuracy in different scenarios are not completely uniform. In current relevant studies, data accuracy evaluation of data compression and decompression processes still utilize image processing values such as the structural similarity index (SSIM), mean squared error (MSE), and peak signal-to-noise ratio (PSNR) as the final evaluation index, rather than a specific parameter of concern to data users. Therefore, in this paper, we propose an intelligent compression framework for lightweight marine grid data for long-distance transmission and ship-based use. By integrating physical prior knowledge and a data-driven model, a multi-scale adaptive quantization mechanism is constructed to effectively control the amount of transmitted data on the premise of ensuring the analyzability of dynamic ocean processes. This method pays special attention to the full-link consistency of the transmission-reconstruction-application of sea level anomaly (SLA) and adopts the forward validation strategy based on the ocean numerical model to ensure that the compressed data can meet the accuracy requirements in different application scenarios. The experimental results show that the comprehensive performance of the framework on typical marine datasets is better than those of the existing mainstream methods and provides a new technical path for building an efficient and reliable marine data transmission system.

2. Data and research area

2.1. Sea level anomaly data

The grid data (mean sea level anomaly, MSLA) were provided by the Archiving, Validation, and Interpretation of Satellite Oceanographic (AVISO) program in France. The dataset combines altimetry data from multiple satellites such as Topex/Poseidon (T/P), Jason-1, European Remote Sensing Satellite (ERS), and Environmental Satellite (ENVISAT). The temporal resolution of the data is 7 days, the spatial resolution is 1° × 1°, and the time span is January 1993 to July 2021. Necessary standard corrections have been made to the data, such as ionospheric delay correction, tropospheric dry and wet component correction, earth and sea tide correction, ocean load tidal correction, polar tide correction, electromagnetic deviation correction, instrument correction, and inverse barometer correction [23–25].

2.2. Ocean reanalysis data

The Japan Coastal Ocean Predictability Experiment 2 Modified (JCOPE2M) is a high-resolution reanalysis dataset for the Northwest Pacific Ocean developed by the Japan Marine Affairs Agency and has a horizontal grid resolution of 1/12° (about 8 km). The vertical full depth is divided into 46 layers, and the temporal resolution is updated daily [26,27]. By assimilating sea surface temperature (SST), sea surface height anomaly (SSHA), and some Argo buoy observations, the dataset achieves accurate reconstruction of the three-dimensional thermohaline structure and flow field of mesoscale vortexes. Previous studies have shown that JCOPE2M has a high reliability in the study of circulation dynamics in the Northwest Pacific Ocean, and it has been widely used in research on the variation mechanism of the Kuroshio extension body and vortex-current interaction.

The hybrid coordinate ocean model (HYCOM) is a numerical model of the global ocean developed by the U.S. Naval Research Laboratory (NRL) that uses a hybrid vertical coordinate system to optimize the simulation of ocean processes at different depths. The base version provides 1/12° (about 9 km) global coverage and a 1/25° (about 4 km) regional enhanced resolution, as well as a time resolution of hourly output and support for operational forecasting of up to 7 days [28–30]. The system can output multi-factor forecast products such as the sea surface height, two-dimensional positive pressure flow field, three-dimensional flow field, temperature, and salinity, and it can integrate historical observation data through reanalysis technology to provide multi-spatiotemporal scale data support for the study of dynamic ocean processes.

The China Ocean Reanalysis and Prediction System (CORA) is a high-precision regional ocean reanalysis dataset developed by the National Oceanic Information Center of China. It focuses on the Northwest Pacific Ocean and the offshore waters of China. This dataset integrates multi-source data such as satellite remote sensing data and buoy observations and adopts advanced data assimilation technology to couple regional ocean models to generate daily three-dimensional marine environment fields from 2000 to 2022. It has a horizontal resolution of 1/12° (about 9 km) and 40 vertical layers and includes core parameters such as the SST, salinity, and ocean currents. Verification has shown that the error of its sea surface temperature is less than 0.5°C, and it has been widely used in the study of ocean dynamic processes and operational forecasting [31].

2.3. Research area

In this study, we focused on the northwest Pacific region (0–60°N, 100–180°E) as the main research area. This area has two high-risk areas that contain the mesoscale vortex [32–35], the Kuroshio extension body area (KE, 30–45°N, 130–180°E), and the zone of the subtropical countercurrent (STCC, 15–28°N, 120–170°E)

3. Methods

3.1. Establishing the sample dataset

In the main research content of this study, data compression was realized using the following super-resolution enhancement process after sampling, so the dataset needed to provide a set of high-resolution images and a set of low-resolution image sample data. To this end, we generated high-resolution images within study area 2.3 with a time resolution of daily SLA data and latitude and longitude spans of 20° (240 × 240 pixels) for the marine reanalysis data and latitude and longitude spans of 40° (40 × 40 pixels) for the AVISO data. The parameters were as follows: × 4 and ×8 data super resolution to enhance the magnification target, corresponding to the formation of low-resolution images (Table 1). The data span was from January 1, 2007, to December 31, 2020. It should be noted that there were a large number of empty values in some of the generated images (corresponding to unmeasurable grid points, usually land or perennial sheltered areas), which greatly affected the training process, we provided a screening mechanism. That is, if the number of null values in a single data grid exceeded 15%, the data were abandoned. A total of 51140 × 2, × 4, and ×8 resolution images were formed in the sample dataset. In the testing stage, the center cropping strategy was adopted to eliminate the boundary effect. For the data preprocessing methods and related threshold Settings of this part, please refer to the reference articles of Zhang et al [36].

Table 1. Data super-resolution enhancement magnification target and its corresponding low-resolution image pixel value.

Ocean Reanalysis Data LR ×2 ×4 ×8
120 px × 120 px 60 px × 60 px 30 px × 30 px
HR 240 px × 240 px
AVISO
(SLA)
LR ×2 ×4
20 px × 20 px 10 px × 10 px
HR 40 px × 40 px

In the table, LR represents low-resolution data and HR represents high-resolution data, corresponding to different sampling results of x2, x4 and x8. Additionally, since the initial resolution of the ocean reanalysis data is higher than the original resolution of the SLA data, we only sample the SLA data up to 4 times. This is because after 4 times sampling, the resolution of the SLA data will change to 1° × 1°. This has a significant impact on the identification of mesoscale vortices in the subsequent part of this paper (a considerable number of vortices have radii in the order of 40–100 km).

3.2. Identification of mesoscale eddy

Since the satellite altimetry data were made available to the public in 1992, research on an automatic detection method for mesoscale vortices has attracted much attention. The current mainstream recognition algorithms mainly include the physical parameter method [37], flow field geometry [38], and machine learning-based visual recognition technology [39,40]. However, due to the heterogeneity of the original data pre-processing processes (such as sea surface height anomaly correction standards and gridded interpolation schemes) and the diversity of vortex core criteria (such as the closed contour threshold and streamline curvature parameters), the applications of the different algorithms have significant scene dependence. Therefore, we propose a meso-scale vortex mixing algorithm to reduce the recognition error.

u′=−gf∂h′∂y , v′=−gf∂h′∂x. (1)

First, the sea surface height field is converted to the geostrophic flow field based on the geostrophic equilibrium relationship (Equation (1), where u′ and v′  are the meridional and zonal components of the sea surface geostrophic flow field (m/s), and h′ is the sea surface height (m)). By detecting the symmetric rotation structure of the velocity vector (there are extreme velocity points and the vector is distributed in a clockwise/counterclockwise ring), the candidate vortices are initially screened. Second, the sea surface height field is searched using a closed isoline to exclude the open pseudo-vortex signal. Finally, the joint verification condition is set: the vortex is only judged to be effective (the center location result of the flow field geometry method is preferred) when the space overlap degree (intersection area is ≥ 50% of the area of a single vortex) and the center distance (≤ 1/12°) identified using the two methods meet the standards at the same time. Compared with the original flow field geometry method, contour closure method, and physical parameter method, the expert evaluation rate of the proposed algorithm is 8, 10, and 15% higher, respectively.

3.3. Data super resolution

Super resolution technology aims to reconstruct low-resolution (LR) images into high-resolution (HR) images [37]. Methods for achieving super resolution can generally be divided into two types: image interpolation based methods and deep learning-based methods. This paper primarily proposes a generative adversarial network model that considers both global and local information to improve the super-resolution results of SLA data. The generative adversarial network [41] consists of two main neural networks, a generator and a discriminator. The generator takes a random noise as input and generates a sample that is similar to the real data. The discriminator takes an input sample (which may be a real sample or a generator generated sample) and outputs a probability value, which represents the probability that the sample is a real sample. The core contribution of the super-resolution generative adversarial network (SRGAN) [42] is that it advances the super resolution from pixel recovery to perception enhancement by introducing residual-dense blocks, visual geometry group (VGG) features against loss, and subpixel upsampling to solve the bottlenecks of detail blurring and texture distortion in traditional methods. Its design ideas directly influenced subsequent models (such as the enhanced super-resolution generative adversarial network (ESRGAN) [43] and Real-ESRGAN [44]) and became a milestone work in the field of super resolution. Since the subsequent model needs to multiply the model training computing power and field equipment support for the super-resolution enhancement process of high-resolution images, in this study, we mainly focused on the codec operation built in the lightweight marine ship receiver. Thus, the performance limitation was the most important factor to consider when screening the base model. Accordingly, the base model with a better effect was selected. The original network diagram of the SRGAN is shown in the red dotted box in Fig 1.

Fig 1. Original network architecture of the SRGAN (red dotted box) and network architecture diagram of the ConmpressGAN (complete).

Fig 1

The SRGAN replaces the discriminator in the traditional generative adversarial network (GAN) with the VGG-19 network [45–47], changes the pixel loss MSE (Equation (2)) to the perception loss (Equation (3)), and takes the VGG network loss as the Euclidian distance between the features of the generated image ILR and the original image IHR (Equation (4)). This is done to adjust the edge abrupt effect of the sea surface height field data caused by edge tearing resulting from pure pixel evaluation, which is clearly reflected in the further analysis of the subsequent model evaluation indicators. In addition, considering the characteristics of the sea surface height data and the biased demand for the recognition effect of mesoscale vortices in the scene we are concerned about, the perceptual evaluation range of the regionalized discriminator needs to be further refined and improved. Therefore, based on the SRGAN, in this study, we drew upon the idea of the global and local context codec proposed by Lizuka et al. [48]. A lightweight compression model, namely, CompressGAN, was developed to adapt to the scenarioization. The network consists of one generator and two context discriminators. The model structure of CompressGAN is shown in Fig 2 (inside the red dashed box with additional local discriminators). The SRGAN perception loss is composed of two parts (Equation (3)), namely, content loss loss VGGSR and adversarial loss loss GenSR.

Fig 2. Test results of the SRResNet, SRGAN, CompressGAN, nearest neighbor, bicubic, and AKIMA for the × 4 amplification factor (indicators: PSNR, SSIM, and Iden).

Fig 2

lossMSESR=1r2WH∑x=1rW∑y=1rH(Ix,yHR−(GθG(ILR))x,y)2. (2)
lossSR=lossVGGSR+0.001*lossGenSR. (3)
lossVGG/i,jSR=1Wi,jHi,j∑\nolimitsx=1Wi,j∑\nolimitsy=1Hi,j(ϕi,j(IHR)x,y−ϕi,j(GθG(ILR))x,y)2. (4)

In Equations (2)–(4), Wi,j and Hi,j describe the dimensions of the respective feature maps within the VGG network, I is the image, and loss is the function loss.

Generator loss is a mechanism used to encourage the super-resolution data generated by the generator to reduce the discriminator success rate during adversarial network training. We replaced the adversarial loss function (Equation (5)) of the native GAN network with Equation (6).

lossGenGAN=∑\nolimitsn=1Nlog(1−DθD(GθG(ILR))). (5)
lossGenSR=∑n=1N−log(DθD(GθG(ILR))). (6)

In the process of global and local discrimination proposed in this paper, we assign weight to the lost part of the discriminator and dynamically adjust Ω according to the proportion of local blocks in the whole pixel in the optional local discrimination process. In the experiment, we set it to 0.5. Therefore, the perceptive loss of the CompressGAN network can be summarized as the weight sum of the local discrimination loss loss VGG  SRPand global discrimination loss lossVGGSRG (Equation (7)):

lossSR=(1−Ω)·lossVGGSRG+Ω·lossVGGSRP+0.001*lossGenSR. (7)

In the convolution process of the generator, we introduce an expansive convolution layer (Econv), which increases the receptive field without increasing the number of parameters compared with the normal convolution process, which can improve the local network’s perception of the overall characteristics of the sea surface information during the experiment. The calculation process can be summarized as follows:

yu,v=σ(b+∑i=−kh′kh′∑j=−kw′kw′Wkh′+i,kw′+jXu+ηi,v+ηj),kh′=kh−12,kw′=kw−12, (8)

where kw′ and kh′ are the convolution kernels’ nucleus width and height, η represents the expansion parameters, xu,v∈ℝC and yu,v∈ℝC for the input and output layers of the pixels, respectively, σ(·) is a nonlinear transfer function, and Ws,t is the convolution kernel matrix b∈ℝC. The offset vector is the convolution layer. This becomes the standard convolution formula when η = 1. The distribution of the major convolution layers of the CompressGAN and corresponding characteristic parameters are presented in Table 2.

Table 2. Main convolution layer distributions of CompressGAN and corresponding characteristic parameters.

G Conv Conv Conv Conv Conv Conv Conv Conv
k3n64s1 k3n64s1 k3n64s1 k3n64s1 k3n64s1 k3n64s1 k3n256s1 k9n3s1
D
(Global)
Conv Conv Conv Conv Conv Conv Conv Conv
k3n64s1 k3n64s2 k3n128s1 k3n128s2 k3n256s1 k3n256s2 k3n512s1 k3n512s2
D
(Partial)
Conv EConv EConv EConv EConv EConv EConv Econv
k3n64s1 k3n64s2 k3n128s1 k3n128s2 k3n256s1 k3n256s2 k3n512s1 k3n512s2

Note: k is the kernel size, n is the number of feature maps, and s is the stride.

3.4. Evaluation index

First, we use the mesoscale vortex recognition algorithm described in Section 3.2 as one of the procedural algorithms for the evaluation indexes, and the mesoscale vortex recognition effect Iden after its super resolution improvement is taken as one of the evaluation indexes (Equation 9), where IdenR is the number of successful recognitions, and IdenA is the number of recognitions of mesoscale vortices in the real images. Three conditions must be met when the recognition is successful: (1) the overlap area between the super resolution and the real image recognition scroll exceeds 3/4 of the scope of the scroll contour; (2) the vortex equivalent radius difference does not exceed 20% of the real image; and (3) the vortex center distance does not exceed 10% of the real image radius. Then, we use the PSNR and SSIM indicators, which are commonly used in image super resolution, to improve evaluation indicators [49]. Their calculation formulas are as follows:

Iden=IdenR╱IdenA, (9)
SSIM(x,y)=(2μxμy+c1)(2σxy+c2)(μx2+μy2+c1)(σx2+σx2+c2),c1=(k1L)2,c1=(k2L)2, (10)
PSNR=10log10(N∑\nolimitsi=1N(IHR−ISR)2). (11)

In Equation (10), μx is the mean value of x, μy is the mean value of y, σx2 is the variance of x, σy2 is the variance of y, and σxy is the covariance of x and y. L is the dynamic range of the pixel values. In the case of L = 100, k1,and k2 are set as constant values. In this paper, they are set as 0.01 and 0.03. In Equation (11), N is the total number of data points, and IHR and ISR are the SLA values of the pixels corresponding to the true image and super-resolution image, respectively (all normalized to 0–1).

In addition, since we need to deploy relevant equipment on the ship base, there is a huge gap in the performance compared with the shore-based experimental equipment; thus, we utilize the model inference decoding operation speed and the maximum running memory (MEM) as evaluation indicators.

4. Experiments

We conducted model training on three different datasets (JCOPE2M, HYCOM, and AVISO) according to the resolution magnification and pixel amount shown in Table 1. To ensure the fairness of the experiment, all of the PSNR and SSIM data were trained in a single channel and were compared with other common super-resolution algorithms and models, including learning class (super-resolution residual neural network (SRResNet), SRGAN) and non-learning class (nearest neighbor, bicubic, AKIMA) models. These models are available for open source downloading at the link presented in the acknowledgements.

4.1. Training details and parameters

In this study, a training environment was constructed based on the NVIDIA GeForce RTX 4060 Ti 16GB graphics card and the i9 13900k central processing unit (CPU). The stratified sampling strategy was adopted to divide the multi-mode super-resolution dataset constructed (Section 3.1). Specifically, the HR and LR image pairs were first paired to ensure the accuracy of the data correspondence, and then, the training set, verification set, and testing set were divided according to the ratio of 8:1:1. In particular, the independent correspondence between the HR and LR images in the three subsets was maintained to avoid the risk of data leakage.

In the model training stage, to adapt to the limitation of the video memory capacity and improve the training efficiency, the dynamic block clipping strategy was adopted: the input image was randomly clipped to a local block of 48 × 48 pixels. The validity of this size selection has been verified by previous experiments, and it can maintain the integrity of local texture details while ensuring that the video memory occupancy of the convolutional operations does not exceed 8 GB. Online data enhancement was performed during the training, including random horizontal/vertical flips (probability of 0.5), ± 15° rotation, and red-green-blue (RGB) channel perturbations (standard deviation of 0.02).

In terms of the optimizer configuration, the Adam [50] optimizer was used and β=(0.9,0.999) dual-momentum parameters were set to implement differentiated learning strategies for the different network components: SRGAN/CompressGAN framework, initial learning rate of 2 × 10−4 (generator), 1 × 10−4 (discriminator), batch size of 32 (HR-LR pairs), and the number of training rounds of 1500 epochs., The iteration strategy was to use an alternate training mechanism. Two rounds of discriminator training were performed after every round of generator update, and the weight coefficients of the adversarial loss and content loss (L1 + L2 Loss) were performed via dynamic balance (initial ratio of 1:100, 10% attenuation per 100 epochs). The SRResNet architecture was utilized [51], the initial learning rate was 1 × 10−5 (determined by grid search), the batch size was 16 (limited by deep residual structure memory requirements), and the number of training rounds was 3000 epochs. The learning scheduling was the cosine annealing strategy. The period length was 500 epochs, the minimum learning rate decayed to 5% of the initial value, and the key hyperparameters were determined via Bayesian optimization for the × 4 super resolution task. When processing the different amplification factors (×2/ × 4/ × 8), parameter adaptive adjustment was implemented, the block size was scaled (amplification factor k corresponds to a block size of 48k × 48k), the learning rate was 1 × 10−5, the batch size was 16, and the training cycle was positive correlation with the amplification factor (×2:1200 epochs, × 4:2000 epochs, and ×4:3000 epochs).

To verify the stability of the training, the early stop mechanism (patience = 50 epochs) was applied to the verification set, and mixed precision training (FP16) was used to accelerate the calculation. In the testing phase, the sliding window strategy was used for the entire graph inference, and weighted fusion of the overlapping regions was used to eliminate the block boundary artifacts. All of the experiments were repeated three times and the average indexes were taken to ensure the reliability of the results. This configuration achieved the inference speed of 12 it/s in the image resolution processing described in this paper, and the peak memory occupancy was controlled to within 7.8 GB.

4.2. Results

4.2.1. Numerical error.

Five hundred sets of data were randomly selected from the testing dataset described in Section 3.1 (resolution in Table 1), and these datasets were used to conduct a numerical error test. The trained SRResNet, SRGAN, CompressGAN, nearest neighbor [52], bicubic [53], and AKIMA [54] (a total of six algorithms) were employed under amplification factors of ×2, × 4, and ×8, and the experimental error fuzzy strategy of averaging three experiments on single data was adopted. Fig 2 presents a comparison of the PSNR, SSIM, and Iden indexes for the × 4 amplification factor. The test results for the × 2 and ×8 amplification factors are presented in Table 3 based on the × 4 amplification factor.

Table 3.  ×2 and ×8 amplification factor test results (based on the × 4 amplification factor).
SRGAN Compress
GAN
SRResNet bicubic nearest neighbor AKIMA
PSNR ×2 +1.7546 +1.9247 +2.9123 +3.1243 +2.2841 +2.0125
×8 −0.5127 −0.9347 −1.2415 −2.0145 −1.7416 −1.8529
SSIM ×2 +0.0142 +0.0436 +0.0522 +0.1028 +0.0981 +0.1410
×8 −0.0351 −0.0714 −0.0912 −0.1154 −0.1620 −0.0986
Iden ×2 −0.0841 −0.1435 −0.1051 +0.0521 −0.0871 +0.1024
×8 +0.0121 −0.0942 +0.1074 +0.0241 +0.0543 +0.1057

Note: Above base (+), below base (-).

The numerical error gap between the models in Fig 2 under the × 4 amplification factor is mainly between the learning class and the non-learning class, which indicates the superiority of the super-resolution enhancement process of the learning class. Compared with the three deep learning models assessed in this paper, SRResNet was demonstrated to have certain advantages (32.1524) in terms of the PSNR index, which is 0.3633 higher than that of the CompressGAN (31.7891) proposed in this paper and 1.2260 higher than that of the native SRGAN (30.9264). This advantage is also reflected in the SSIM index. The SSIM of the SRResNet is 0.9132, which is 0.0048 higher than that of the CompressGAN (0.9084) proposed in this paper and 0.0231 higher than that of the native SRGAN (0.8901). The reason for this is that the CompressGAN is based on the improvement of the SRGAN, and both of them adjust the loss function in the adversarial network, and thus, it not only has an excellent numerical error performance but also optimizes the overall perception effect of the image. Therefore, the PSNR and SSIM indicators are slightly affected. However, the results show that the gap is not huge, so it has a small disadvantage, and can be acceptable for use in marine applications. Regarding the Iden index, the SRResNet exhibits a significant disadvantage (89.82%). Its Iden value is 0.11% higher than that of the SRGAN (89.71%) and 1.64% lower than that of the CompressGAN (91.46%). This indicates that the local discriminator added by the CompressGAN model proposed in this paper achieves better resolution improvement and detail retention of vortex continuity, and its recognition rate is 1.75% higher than that of the native SRGAN without a local discriminator.

In addition, we carried out ×2, × 4, and ×8 amplification factor tests with a resolution different from that in Table 1 and adopted random size data with a resolution of (128–512 px) × (128–512 px). Three rounds of single data test were conducted, and the average value was taken as the test result (table). The reasoning equipment still used the 4.1 hardware. The overall test results exhibit the same fixed resolution trend, which demonstrates the scalability of the model in terms of the resolution adjustment (Fig 3).

Fig 3. Test results for the SRResNet, SRGAN, CompressGAN, nearest neighbor, bicubic, and AKIMA on the testing data of the index-resolution for the × 4 amplification factor (indicators: PSNR, SSIM, and Iden).

Fig 3

4.2.2. Comparison of transplant decoding effect.

Due to the limitation of the communication capability of ships at sea and the computing capacity of on-board equipment, algorithms with lower performance requirements will be accepted by more small and medium-sized ships. Therefore, for ship-end testing, we adopted a set of general performance on-board computing equipment (the detailed parameters are shown in Table 4) and adopted the same test process described in Section 4.2.2 to test the proposed method on this equipment. However, the data resolution used was adjusted to the needs of the business (project team): 128 × 128 px, and only the × 4 resolution increase ratio was tested.

Table 4. The main performance parameters of the general shipborne equipment used in this paper.
Device Name CPU GPU Core Frequency Thread Count RAM
MC-346 Intel Core™ i7-1365UE GeForce RTX 3050Ti Laptop GPU 1.70GHz 12 64GB

As can be seen from Table 4, compared with the test equipment in Section 4.1, there is a big difference in the overall performance, and the equipment is the highest value of the average computing power of the on-board equipment in the data collected by the project team after multiple investigations. Therefore, the test results presented in this section may still not meet the requirements of some equipment with too low a performance. For the applied comparison of the test results, we adopted two evaluation methods: (1) whether the inference of 1500 sets of single images can be completed independently and successfully; and (2) the length of the inference decoding time. We do not test the indicators discussed in Section 3.4. The relevant test results are referred to in Section 4.2.1. The testing process was consistent with that in Section 4.2.1, but only the × 4 amplification factor (without cropping) was tested. The testing data were obtained from 1000 pairs of images with a resolution of 1024 × 1024 px, which were randomly selected from the HYCOM and JCOPE2M testing sets. The test results are presented in Table 5.

As can be seen from Table 5, among the five deep learning models tested in this paper, only three tested in Section 4.1 completed the independence test. Although the ESRGAN and Real ESRGAN models have been shown to have super-resolution performances superior to that of SRGAN-based models in a large number of studies, their required hardware conditions have been greatly improved, and this hardware cannot be widely used in shipborne low performance equipment.

Table 5. Multiple deep learning models can compare the reasoning and decoding time needed to improve the resolution of fixed resolution data under the × 4 amplification factor.
Independent Completion Model Inference Time (s/pic) Peak Memory
(work on CPU)
SRGAN Yes 101 20
CompressGAN Yes 148 25
SRResNet Yes 77 14
ESRGAN No
Real ESRGAN No

4.3. Verification and generalization of the model

The generalization performance is crucial for deep learning network models. Therefore, in this section, we test the generalization of the model from two perspectives of different data sources and different sea area data. First, we test the generalization of the data in different sea areas. We use the sea surface height reanalysis data from the HYCOM data in other mesoscale vortex high occurrence regions of the global ocean as the material for the production of the sample dataset. According to the method described in Section 3.1, 1000 groups of test samples were randomly selected, and 3 rounds of repeated tests were carried out on each single group of data under a × 4 amplification factor. The test results are shown in Fig 4. The parameters of the on-board hardware equipment were the same as those in Section 4.2.2.

Fig 4. Generalization test results for the SRResNet, SRGAN, CompressGAN, nearest neighbor, bicubic, and AKIMA from different data sources for the ×4 amplification factor (indicators: PSNR, SSIM, and Iden).

Fig 4

Fig 4 shows that the overall effect of each deep learning model in the process of the generalization test decreased. Compared with the results presented in Section 4.2.1, the PSNR index decreased by 3–4 db on average. That of the SRResNet decreased the most, followed by CompressGAN, and that of the SRGAN decreased the least. Compared with the results presented in Section 4.2.1, the SSIM index decreased by 0.5426 on average. That of the SRResNet decreased the most, followed by the SRGAN, and that of the CompressGAN decreased the least. Compared with the results presented in Section 4.2.1, the Iden index decreased by about 2% on average. That of the SRResNet decreased the most, followed by the SRGAN, and that of the CompressGAN decreased the least.

In addition, we conducted generalization tests from the perspective of different data sources. According to the same method in 3.1, we also reanalyzed the sea surface height data of the mesoscale vortex high-incidence area in the CORA dataset, randomly selected 1000 groups of test samples, and conducted 3 rounds of repeated tests on each single group of data under the condition of ×4 amplification factor. The test results are shown in Fig 5.

Fig 5. Test results for the SRResNet, SRGAN, CompressGAN, nearest neighbor, bicubic, and AKIMA on the testing data from different data sources for the × 4 amplification factor (indicators: PSNR, SSIM, and Iden).

Fig 5

Fig 5 shows that the overall effect of each deep learning model decreased during the generalization test. Compared with the results presented in Section 4.2.1, the PSNR index decreased by 4–5 db on average. That of the SRResNet decreased the most, followed by the CompressGAN, and that of the SRGAN decreased the least. Compared with the results presented in Section 4.2.1, the SSIM index decreased by 0.7126 on average. That of the SRResNet decreased the most, followed by the SRGAN, and that of the CompressGAN decreased the least. Compared with the results presented in Section 4.2.1, the Iden index decreased by about 4% on average. That of the SRResNet decreased the most, followed by the SRGAN, and that of the CompressGAN decreased the least. These results show that the CompressGAN model has good generalization and portability performances.

5. Conclusions

In this study, a lightweight intelligent compression framework, namely, the CompressGAN, for ship-based applications, was developed to solve the bandwidth limitation problem in ocean grid data transmission. By combining the adversarial network and physical prior knowledge, a global and local dual discriminator mechanism was designed to improve the compression efficiency of SLA data and to optimize the reconstruction accuracy of mesoscale vortex features. Experiments demonstrated that the model achieves a better scroll recognition rate (91.46%) on the JCOPE2M, HYCOM, and AVISO datasets compared to traditional methods (e.g., SRGAN and SRResNet), and it has a good portability for low-performance on-board equipment (reasoning time of 148 s/image and peak memory of 25 GB). Through the introduction of a forward validation strategy based on an ocean numerical model, the practicability of the compressed data in ocean dynamic process analysis was verified, and a new technical path was provided for remote ocean real-time monitoring.

Although the CompressGAN performs well on specific datasets, there are limitations to its ability to generalize. Significant degradation of the model performance (4–5 dB reduction in the PSNR and 4% reduction in the scroll recognition rate) was observed across sea areas (e.g., the Atlantic Ocean and Indian Ocean) and across data sources (e.g., the CORTA reanalysis data), indicating that the current training data have insufficient geographic coverage and physical diversity of. In addition, the adaptability of the model to a high compression ratio (such as x8) is weak, which makes it easy for edge artifacts and vortex distortion to occur in extreme compression scenarios. In addition, there is still a certain dependence on the hardware computing power during shipboard deployment (16 GB video memory is required). Finally, although the vortex recognition rate index is introduced in the evaluation system, the impact of the compressed data on downstream tasks such as three-dimensional warm salt field reconstruction and marine numerical prediction is not fully quantified, which limits the comprehensive evaluation of its application value.

Future research can optimize the model architecture and validation system from multiple dimensions. First, a cross-sea, multi-source heterogeneous ocean dataset needs to be constructed, and the generalization ability of the model can be improved by combining transfer learning and domain adaptive technology. Second, the lightweight network design (such as knowledge distillation and neural architecture search) should be utilized to further reduce the computational complexity to meet the real-time requirements of lower end shipborne equipment. In terms of the physical consistency, dynamic constraints such as vorticity conservation and he geostrophic equilibrium equation can be introduced as loss functions to enhance the physical interpretability of the reconstructed data. In addition, it is necessary to establish an end-to-end evaluation link to quantify the impact of the compressed data on business scenarios such as ocean circulation simulation and disaster warning and to promote the deep coupling of algorithms with ocean numerical models. Finally, an adaptive compression strategy needs to be developed to dynamically adjust the compression ratio and feature retention priority according to the transmission environment and application scenarios so as to achieve intelligent balance between the precision and efficiency.

Acknowledgments

We thank JAMEST for the JCOPE2M data support (https://www.Jamstec.go.jp/jcope/htdocs/distribution/index.html).

We thank AVISO for providing the mesoscale eddy dataset (https://www.aviso.altimetry.fr/en/data/products/value-added-products/global-mesoscale-eddy-trajectory-product. html).

We thank the National Centers for Environmental Information (NCEI) for providing the World Ocean Atlas (WOA) data (https://www.ncei.noaa.gov/products/world-ocean-atlas)

We also thank the National Marine Data Center (https://mds.nmdis.org.cn/) the Japan Oceanographic Data Center (https://www.jodc.go.jp/).

Other scholars and organizations that helped in the research process are also acknowledged.

We thank LetPub (www.letpub.com.cn) for its linguistic assistance during the preparation of this manuscript.

Data Availability

All SLA files are available from the AVISO database. AVISO data can be downloaded (open acess) from https://www.aviso.altimetry.fr/en/my-aviso-plus.html.

Funding Statement

The author(s) received no specific funding for this work.

References

  • 1.Chelton D, Schlax MG, Samelson RM. Global observations of nonlinear mesoscale eddies. Prog Oceanograph. 2011;91:167–216. [Google Scholar]
  • 2.Zhang Z, et al. Universal structure of mesoscale eddies in the ocean. Geophysical Res Letters. 2013;40(14):3677–81. [Google Scholar]
  • 3.Ji J, et al. Oceanic eddy characteristics and generation mechanisms in the Kuroshio Extension region. J Geophysical Res Oceans. 2018;123(11):8548–67. [Google Scholar]
  • 4.Zhao D, et al. Global chlorophyll distribution induced by mesoscale eddies. Remote Sensing Environ. 2021;254:112245. [Google Scholar]
  • 5.Kösters M, Leufken J, Schulze S, Sugimoto K, Klein J, Zahedi RP, et al. pymzML v2.0: introducing a highly compressed and seekable gzip format. Bioinformatics. 2018;34(14):2513–4. doi: 10.1093/bioinformatics/bty046 [DOI] [PubMed] [Google Scholar]
  • 6.Kreft S, Navarro G. LZ77-like compression with fast random access. in 2010 Data Compression Conference. IEEE; 2010. [Google Scholar]
  • 7.Said A, Pearlman WA. An image multiresolution representation for lossless and lossy compression. IEEE Trans Image Process. 1996;5(9):1303–10. doi: 10.1109/83.535842 [DOI] [PubMed] [Google Scholar]
  • 8.Tao D, et al. Significantly improving lossy compression for scientific data sets based on multidimensional prediction and error-controlled quantization. In: 2017 IEEE International Parallel and Distributed Processing Symposium (IPDPS). IEEE; 2017. [Google Scholar]
  • 9.Delaunay X, Courtois A, Gouillon F. Evaluation of lossless and lossy algorithms for the compression of scientific datasets in netCDF-4 or HDF5 files. Geoscientific Model Development. 2019;12(9):4099–113. [Google Scholar]
  • 10.Cheng Z, et al. Deep convolutional autoencoder-based lossy image compression. In: 2018 Picture Coding Symposium (PCS). IEEE; 2018. [Google Scholar]
  • 11.Chen Z, et al. Lossy intermediate deep learning feature compression and evaluation. In: Proceedings of the 27th ACM International Conference on Multimedia, 2019. [Google Scholar]
  • 12.Jin S, et al. DeepSZ: A novel framework to compress deep neural networks by using error-bounded lossy compression. In: Proceedings of the 28th International Symposium on High-Performance Parallel and Distributed Computing, 2019. [Google Scholar]
  • 13.Tschannen M, Agustsson E, Lucic M. Deep generative models for distribution-preserving lossy compression. Adv Neural Informat Process Syst. 2018;31. [Google Scholar]
  • 14.Reagan B, et al. Weightless: lossy weight encoding for deep neural network compression. In: International Conference on Machine Learning. PMLR; 2018. [Google Scholar]
  • 15.Baker AH, et al. Evaluating lossy data compression on climate simulation data within a large ensemble. Geoscientific Model Develop. 2016;9(12):4381–403. [Google Scholar]
  • 16.Garcia DC, Queiroz RLd, Fonseca LENd. Lossless and lossy compression of water-column profile data from multibeam echosounders based on image predictions and multiple-context entropy-encoding. Boletim de Ciências Geodésicas. 2023;29(04):e2023010. [Google Scholar]
  • 17.Le H, Tao J. Hierarchical autoencoder-based lossy compression for large-scale high-resolution scientific data. arXiv preprint. 2023:arXiv.2307.04216. [Google Scholar]
  • 18.Kong L, et al. Data loss and reconstruction in sensor networks. In: 2013 Proceedings IEEE INFOCOM. IEEE; 2013. [Google Scholar]
  • 19.Hu C, et al. Secure and efficient data collection and storage of IoT in smart ocean. IEEE Internet Thing J. 2020;7(10):9980–94. [Google Scholar]
  • 20.Fanelli C, Ciani D, Pisano A, Buongiorno Nardelli B. Deep learning for the super resolution of Mediterranean sea surface temperature fields. Ocean Sci. 2024;20(4):1035–50. doi: 10.5194/os-20-1035-2024 [DOI] [Google Scholar]
  • 21.Buongiorno Nardelli B, et al. Super-resolving ocean dynamics from space with computer vision algorithms. Remote Sensing. 2022;14(5):1159. [Google Scholar]
  • 22.Cui J, et al. High-resolution sea surface height reconstruction method based on deep learning gradient constraint embedding method. Ocean Eng. 2025;324:120671. [Google Scholar]
  • 23.Fu L-L, Chelton DB, Zlotnicki V. Satellite altimetry: Observing ocean variability from space. Oceanography. 1988;1(2):4–58. [Google Scholar]
  • 24.Cazenave A, Palanisamy H, Ablain M. Contemporary sea level changes from satellite altimetry: What have we learned? What are the new challenges? Adv Space Res. 2018;62(7):1639–53. [Google Scholar]
  • 25.Abdalla S, et al. Altimetry for the future: Building on 25 years of progress. Adv Space Res. 2021;68(2):319–63. [Google Scholar]
  • 26.Miyazawa Y. The JCOPE ocean forecast system. In: First ARGO Science Workshop, November 12-14, 2003, Tokyo, Japan. 2003. [Google Scholar]
  • 27.Ma X. A mesoscale eddy reconstruction method based on generative adversarial networks. Front Marine Sci. 2024;11:1411779. [Google Scholar]
  • 28.Wallcraft A, et al. Global ocean prediction using HYCOM. In: 2007 DoD High Performance Computing Modernization Program Users Group Conference. IEEE; 2007. [Google Scholar]
  • 29.Chassignet EP, et al. US GODAE: global ocean prediction with the HYbrid Coordinate Ocean Model (HYCOM). Oceanography. 2009;22(2):64–75. [Google Scholar]
  • 30.Trott CB, Metzger EJ, Yu Z. Luzon strait mesoscale eddy characteristics in HYCOM reanalysis, simulation, and forecasts. J Oceanograph. 2023;79(4):423–41. [Google Scholar]
  • 31.Cabanes C, et al. The CORA dataset: validation and diagnostics of ocean temperature and salinity in situ measurements. Ocean Sci Discussions. 2012;9(2):1273–312. [Google Scholar]
  • 32.Qiu B. Kuroshio and Oyashio currents. Ocean Currents: A Derivative of the Encyclopedia of Ocean Sciences. 2001;2:61–72. [Google Scholar]
  • 33.Qiu B, Chen S. Concurrent decadal mesoscale eddy modulations in the western North Pacific subtropical gyre. J Phys Oceanograph. 2013;43(2):344–58. [Google Scholar]
  • 34.Yang G, Wang F, Li Y, Lin P. Mesoscale eddies in the northwestern subtropical Pacific Ocean: Statistical characteristics and three‐dimensional structures. JGR Oceans. 2013;118(4):1906–25. doi: 10.1002/jgrc.20164 [DOI] [Google Scholar]
  • 35.Amores A, Melnichenko O, Maximenko N. Coherent mesoscale eddies in the North Atlantic subtropical gyre: 3‐D structure and transport with application to the salinity maximum. J Geophys Res. 2017;122(1):23–41. [Google Scholar]
  • 36.Zhang L, et al. Three-dimensional thermohaline reconstruction of mesoscale eddies under remote sensing observation: from the perspective of deep learning of layer depth sequences with fusion of physical mechanisms. J Sea Res. 2025:102593. [Google Scholar]
  • 37.Okubo A. Horizontal dispersion of floatable particles in the vicinity of velocity singularities such as convergences. In: Deep sea research and oceanographic abstracts. Elsevier; 1970. [Google Scholar]
  • 38.Nencioli F, et al. A vector geometry–based eddy detection algorithm and its application to a high-resolution numerical model product and high-frequency radar surface velocities in the Southern California Bight. J Atmospheric Ocean Technol. 2010;27(3):564–79. [Google Scholar]
  • 39.Xu G, et al. Oceanic eddy identification using an AI scheme. Remote Sensing. 2019;11(11):1349. [Google Scholar]
  • 40.Nian R, et al. The identification and prediction of mesoscale eddy variation via memory in memory with scheduled sampling for sea level anomaly. Front Marine Sci. 2021;8:753942. [Google Scholar]
  • 41.Goodfellow I, et al. Generative adversarial nets. Adv Neural Information Process Syst. 2014;27. [Google Scholar]
  • 42.Ledig C, et al. Photo-realistic single image super-resolution using a generative adversarial network. In: Proceedings of the IEEE Conference on Computer Vision and Pattern Recognition. 2017. [Google Scholar]
  • 43.Wang X, et al. Esrgan: Enhanced super-resolution generative adversarial networks. In: Proceedings of the European Conference on Computer Vision (ECCV) Workshops, 2018. [Google Scholar]
  • 44.Wang X, et al. Real-esrgan: Training real-world blind super-resolution with pure synthetic data. In: Proceedings of the IEEE/CVF International Conference on Computer Vision, 2021. [Google Scholar]
  • 45.Mascarenhas S, Agarwal M. A comparison between VGG16, VGG19 and ResNet50 architecture frameworks for image classification. In: 2021 International conference on disruptive technologies for multi-disciplinary research and applications (CENTCON). IEEE; 2021. [Google Scholar]
  • 46.Mateen M, et al. Fundus image classification using VGG-19 architecture with PCA and SVD. Symmetry. 2018;11(1):1. [Google Scholar]
  • 47.Simonyan K, Zisserman A. Very deep convolutional networks for large-scale image recognition. arXiv preprint. 2014:arXiv:1409.1556. [Google Scholar]
  • 48.Iizuka S, Simo-Serra E, Ishikawa H. Globally and locally consistent image completion. ACM Trans Graph. 2017;36(4):1–14. [Google Scholar]
  • 49.Hore A, Ziou D. Image quality metrics: PSNR vs. SSIM. In: 2010 20th International Conference on Pattern Recognition. IEEE; 2010. [Google Scholar]
  • 50.Kingma DP, Ba J. Adam: A method for stochastic optimization. arXiv preprint. 2014:arXiv.1412.6980. [Google Scholar]
  • 51.Lim B, et al. Enhanced deep residual networks for single image super-resolution. In: Proceedings of the IEEE Conference on Computer Vision and Pattern Recognition Workshops, 2017. [Google Scholar]
  • 52.Beyer K, et al. When is “nearest neighbor” meaningful? In: Database Theory—ICDT’99: 7th International Conference Jerusalem, Israel, January 10–12, 1999 Proceedings 7. Springer; 1999. [Google Scholar]
  • 53.Carlson RE, Fritsch FN. Monotone piecewise bicubic interpolation. SIAM J Numeric Analy. 1985;22(2):386–400. [Google Scholar]
  • 54.Akima H. A new method of interpolation and smooth curve fitting based on local procedures. J ACM. 1970;17(4):589–602. [Google Scholar]

Decision Letter 0

Hui Li

Dear Dr. Ma,

Thank you for submitting your manuscript to PLOS ONE. After careful consideration, we feel that it has merit but does not fully meet PLOS ONE’s publication criteria as it currently stands. Therefore, we invite you to submit a revised version of the manuscript that addresses the points raised during the review process.

The reviewers request the authors to describe the model more detailed and accurate. Also, the writing should be improved, including the title, the Abstract, the Introduction, the Method, etc.

Please submit your revised manuscript by Jul 02 2025 11:59PM. If you will need more time than this to complete your revisions, please reply to this message or contact the journal office at plosone@plos.org . When you're ready to submit your revision, log on to https://www.editorialmanager.com/pone/ and select the 'Submissions Needing Revision' folder to locate your manuscript file.

  • A rebuttal letter that responds to each point raised by the academic editor and reviewer(s). You should upload this letter as a separate file labeled 'Response to Reviewers'.

  • A marked-up copy of your manuscript that highlights changes made to the original version. You should upload this as a separate file labeled 'Revised Manuscript with Track Changes'.

  • An unmarked version of your revised paper without tracked changes. You should upload this as a separate file labeled 'Manuscript'.

If applicable, we recommend that you deposit your laboratory protocols in protocols.io to enhance the reproducibility of your results. Protocols.io assigns your protocol its own identifier (DOI) so that it can be cited independently in the future. For instructions see: https://journals.plos.org/plosone/s/submission-guidelines#loc-laboratory-protocols . Additionally, PLOS ONE offers an option for publishing peer-reviewed Lab Protocol articles, which describe protocols hosted on protocols.io. Read more information on sharing protocols at https://plos.org/protocols?utm_medium=editorial-email&utm_source=authorletters&utm_campaign=protocols .

We look forward to receiving your revised manuscript.

Kind regards,

Hui Li

Academic Editor

PLOS ONE

Journal Requirements:

When submitting your revision, we need you to address these additional requirements.

1. Please ensure that your manuscript meets PLOS ONE's style requirements, including those for file naming. The PLOS ONE style templates can be found at https://journals.plos.org/plosone/s/file?id=wjVg/PLOSOne_formatting_sample_main_body.pdf and https://journals.plos.org/plosone/s/file?id=ba62/PLOSOne_formatting_sample_title_authors_affiliations.pdf

2. PLOS requires an ORCID iD for the corresponding author in Editorial Manager on papers submitted after December 6th, 2016. Please ensure that you have an ORCID iD and that it is validated in Editorial Manager. To do this, go to ‘Update my Information’ (in the upper left-hand corner of the main menu), and click on the Fetch/Validate link next to the ORCID field. This will take you to the ORCID site and allow you to create a new iD or authenticate a pre-existing iD in Editorial Manager.

3. Please note that PLOS ONE has specific guidelines on code sharing for submissions in which author-generated code underpins the findings in the manuscript. In these cases, we expect all author-generated code to be made available without restrictions upon publication of the work. Please review our guidelines at https://journals.plos.org/plosone/s/materials-and-software-sharing#loc-sharing-code and ensure that your code is shared in a way that follows best practice and facilitates reproducibility and reuse.

4. We note that Figure 1 in your submission contain [map/satellite] images which may be copyrighted. All PLOS content is published under the Creative Commons Attribution License (CC BY 4.0), which means that the manuscript, images, and Supporting Information files will be freely available online, and any third party is permitted to access, download, copy, distribute, and use these materials in any way, even commercially, with proper attribution. For these reasons, we cannot publish previously copyrighted maps or satellite images created using proprietary data, such as Google software (Google Maps, Street View, and Earth). For more information, see our copyright guidelines: http://journals.plos.org/plosone/s/licenses-and-copyright.

We require you to either (1) present written permission from the copyright holder to publish these figures specifically under the CC BY 4.0 license, or (2) remove the figures from your submission:

a. You may seek permission from the original copyright holder of Figure 1 to publish the content specifically under the CC BY 4.0 license.

We recommend that you contact the original copyright holder with the Content Permission Form (http://journals.plos.org/plosone/s/file?id=7c09/content-permission-form.pdf) and the following text:

“I request permission for the open-access journal PLOS ONE to publish XXX under the Creative Commons Attribution License (CCAL) CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). Please be aware that this license allows unrestricted use and distribution, even commercially, by third parties. Please reply and provide explicit written permission to publish XXX under a CC BY license and complete the attached form.”

Please upload the completed Content Permission Form or other proof of granted permissions as an "Other" file with your submission.

In the figure caption of the copyrighted figure, please include the following text: “Reprinted from [ref] under a CC BY license, with permission from [name of publisher], original copyright [original copyright year].”

b. If you are unable to obtain permission from the original copyright holder to publish these figures under the CC BY 4.0 license or if the copyright holder’s requirements are incompatible with the CC BY 4.0 license, please either i) remove the figure or ii) supply a replacement figure that complies with the CC BY 4.0 license. Please check copyright information on all replacement figures and update the figure caption with source information. If applicable, please specify in the figure caption text when a figure is similar but not identical to the original image and is therefore for illustrative purposes only.

The following resources for replacing copyrighted map figures may be helpful:

USGS National Map Viewer (public domain): http://viewer.nationalmap.gov/viewer/

The Gateway to Astronaut Photography of Earth (public domain): http://eol.jsc.nasa.gov/sseop/clickmap/

Maps at the CIA (public domain): https://www.cia.gov/library/publications/the-world-factbook/index.html and https://www.cia.gov/library/publications/cia-maps-publications/index.html

NASA Earth Observatory (public domain): http://earthobservatory.nasa.gov/

Landsat: http://landsat.visibleearth.nasa.gov/

USGS EROS (Earth Resources Observatory and Science (EROS) Center) (public domain): http://eros.usgs.gov/#

Natural Earth (public domain): . We require you to either (1) present written permission from the copyright holder to publish these figures specifically under the CC BY 4.0 license, or (2) remove the figures from your submission: a. You may seek permission from the original copyright holder of Figure 1 to publish the content specifically under the CC BY 4.0 license. We recommend that you contact the original copyright holder with the Content Permission Form (http://journals.plos.org/plosone/s/file?id=7c09/content-permission-form.pdf) and the following text: “I request permission for the open-access journal PLOS ONE to publish XXX under the Creative Commons Attribution License (CCAL) CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). Please be aware that this license allows unrestricted use and distribution, even commercially, by third parties. Please reply and provide explicit written permission to publish XXX under a CC BY license and complete the attached form.” Please upload the completed Content Permission Form or other proof of granted permissions as an "Other" file with your submission. In the figure caption of the copyrighted figure, please include the following text: “Reprinted from [ref] under a CC BY license, with permission from [name of publisher], original copyright [original copyri" http://www.naturalearthdata.com/

5. Please upload a copy of Figure 99, to which you refer in your text on page 9. If the figure is no longer to be included as part of the submission please remove all reference to it within the text.

6. Please review your reference list to ensure that it is complete and correct. If you have cited papers that have been retracted, please include the rationale for doing so in the manuscript text, or remove these references and replace them with relevant current references. Any changes to the reference list should be mentioned in the rebuttal letter that accompanies your revised manuscript. If you need to cite a retracted article, indicate the article’s retracted status in the References list and also include a citation and full reference for the retraction notice.

[Note: HTML markup is below. Please do not edit.]

Reviewers' comments:

Reviewer's Responses to Questions

Comments to the Author

1. Is the manuscript technically sound, and do the data support the conclusions?

Reviewer #1: Partly

Reviewer #2: Yes

**********

2. Has the statistical analysis been performed appropriately and rigorously? -->?>

Reviewer #1: Yes

Reviewer #2: Yes

**********

3. Have the authors made all data underlying the findings in their manuscript fully available??>

The PLOS Data policy

Reviewer #1: Yes

Reviewer #2: Yes

**********

4. Is the manuscript presented in an intelligible fashion and written in standard English??>

Reviewer #1: Yes

Reviewer #2: Yes

**********

Reviewer #1: My Recommendation is Minor Revision

(

The paper is interesting and well-written; however, these are my comments:

1. The title is too long and must be no abbreviation.

2. The ABSTRACT is not enough for general problem.

3. Keywords are also not enough.

4. The INTRODUCTION and related work are great but if add some comparison it will be better

5. There are some issues with the template used, as there are many unnecessarily spaced lines, which I believe are technical and can be fixed.

6. The METHODS is crucial part in the paper from what I saw wondaful and just equation and some figures need more explanation.

7. Some of Algorithms and dataset must be clarify.

)

Reviewer #2: The article was reviewed under the title "A lightweight intelligent compression method for fast SLA data transmission".

Overall, the focus of the study is good. However, I would like to offer several recommendations that authors may find useful in the process of revising their manuscript:

1- For better understanding of the readers, it is better to explain Table 1 in more detail.

2- Table 4, which is intended for performance parameters, is empty and no data is listed in it.

3- Some sources are so old that newer sources need to be used for citation.

4- Section 3.1 states the following for the screening mechanism:” That is, if the number of null values in a single data grid exceeded 15%, the data were abandoned.”

What criteria is the threshold based on?

**********

what does this mean? ). If published, this will include your full peer review and any attached files.

If you choose “no”, your identity will remain anonymous but your review may still be made public.

Do you want your identity to be public for this peer review? For information about this choice, including consent withdrawal, please see our Privacy Policy

Reviewer #1: No

Reviewer #2: No

**********

[NOTE: If reviewer comments were submitted as an attachment file, they will be attached to this email and accessible via the submission site. Please log into your account, locate the manuscript record, and check for the action link "View Attachments". If this link does not appear, there are no attachment files.]

While revising your submission, please upload your figure files to the Preflight Analysis and Conversion Engine (PACE) digital diagnostic tool, https://pacev2.apexcovantage.com/ . PACE helps ensure that figures meet PLOS requirements. To use PACE, you must first register as a user. Registration is free. Then, login and navigate to the UPLOAD tab, where you will find detailed instructions on how to use the tool. If you encounter any issues or have any questions when using PACE, please email PLOS at figures@plos.org

Attachment

Submitted filename: comments.docx

pone.0327220.s001.docx (14.1KB, docx)
PLoS One. 2025 Aug 18;20(8):e0327220. doi: 10.1371/journal.pone.0327220.r002

Author response to Decision Letter 1


25 May 2025

Thank you to the reviewers and the editor for your work. The revised versions of the relevant review comments have been uploaded to the system. Additionally, the responses to the review comments of the two reviewers are attached to the submission system and will not be described again here.

Attachment

Submitted filename: Response Letter to Reviewer 2 _v2.docx

pone.0327220.s002.docx (19.2KB, docx)

Decision Letter 1

Hui Li

A lightweight intelligent compression method for fast SLA data transmission

PONE-D-25-17638R1

Dear Dr. Ma,

We’re pleased to inform you that your manuscript has been judged scientifically suitable for publication and will be formally accepted for publication once it meets all outstanding technical requirements.

Within one week, you’ll receive an e-mail detailing the required amendments. When these have been addressed, you’ll receive a formal acceptance letter and your manuscript will be scheduled for publication.

An invoice will be generated when your article is formally accepted. Please note, if your institution has a publishing partnership with PLOS and your article meets the relevant criteria, all or part of your publication costs will be covered. Please make sure your user information is up-to-date by logging into Editorial Manager at Editorial Manager®  and clicking the ‘Update My Information' link at the top of the page. If you have any questions relating to publication charges, please contact our Author Billing department directly at authorbilling@plos.org.

If your institution or institutions have a press office, please notify them about your upcoming paper to help maximize its impact. If they’ll be preparing press materials, please inform our press team as soon as possible -- no later than 48 hours after receiving the formal acceptance. Your manuscript will remain under strict press embargo until 2 pm Eastern Time on the date of publication. For more information, please contact onepress@plos.org.

Kind regards,

Hui Li

Academic Editor

PLOS ONE

Additional Editor Comments (optional):

Reviewers' comments:

Reviewer's Responses to Questions

Comments to the Author

Reviewer #1: All comments have been addressed

Reviewer #2: (No Response)

**********

2. Is the manuscript technically sound, and do the data support the conclusions??>

Reviewer #1: Partly

Reviewer #2: (No Response)

**********

3. Has the statistical analysis been performed appropriately and rigorously? -->?>

Reviewer #1: Yes

Reviewer #2: (No Response)

**********

4. Have the authors made all data underlying the findings in their manuscript fully available??>

The PLOS Data policy

Reviewer #1: Yes

Reviewer #2: (No Response)

**********

5. Is the manuscript presented in an intelligible fashion and written in standard English??>

Reviewer #1: Yes

Reviewer #2: (No Response)

**********

Reviewer #1: The idea is good. But the process of developing and studying it was not in a way that would lead to its acceptance.

Reviewer #2: (No Response)

**********

what does this mean? ). If published, this will include your full peer review and any attached files.

If you choose “no”, your identity will remain anonymous but your review may still be made public.

Do you want your identity to be public for this peer review? For information about this choice, including consent withdrawal, please see our Privacy Policy

Reviewer #1: No

Reviewer #2: No

**********

Attachment

Submitted filename: comments_declet_1.docx

pone.0327220.s003.docx (13.2KB, docx)

Acceptance letter

Hui Li

PONE-D-25-17638R1

PLOS ONE

Dear Dr. Ma,

I'm pleased to inform you that your manuscript has been deemed suitable for publication in PLOS ONE. Congratulations! Your manuscript is now being handed over to our production team.

At this stage, our production department will prepare your paper for publication. This includes ensuring the following:

* All references, tables, and figures are properly cited

* All relevant supporting information is included in the manuscript submission,

* There are no issues that prevent the paper from being properly typeset

You will receive further instructions from the production team, including instructions on how to review your proof when it is ready. Please keep in mind that we are working through a large volume of accepted articles, so please give us a few days to review your paper and let you know the next and final steps.

Lastly, if your institution or institutions have a press office, please let them know about your upcoming paper now to help maximize its impact. If they'll be preparing press materials, please inform our press team within the next 48 hours. Your manuscript will remain under strict press embargo until 2 pm Eastern Time on the date of publication. For more information, please contact onepress@plos.org.

If we can help with anything else, please email us at customercare@plos.org.

Thank you for submitting your work to PLOS ONE and supporting open access.

Kind regards,

PLOS ONE Editorial Office Staff

on behalf of

Professor Hui Li

Academic Editor

PLOS ONE

Associated Data

    This section collects any data citations, data availability statements, or supplementary materials included in this article.

    Supplementary Materials

    Attachment

    Submitted filename: comments.docx

    pone.0327220.s001.docx (14.1KB, docx)
    Attachment

    Submitted filename: Response Letter to Reviewer 2 _v2.docx

    pone.0327220.s002.docx (19.2KB, docx)
    Attachment

    Submitted filename: comments_declet_1.docx

    pone.0327220.s003.docx (13.2KB, docx)

    Data Availability Statement

    All SLA files are available from the AVISO database. AVISO data can be downloaded (open acess) from https://www.aviso.altimetry.fr/en/my-aviso-plus.html.


    Articles from PLOS One are provided here courtesy of PLOS

    RESOURCES