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Article

High-Resolution Inversion of GOSAT-2 Retrievals for Sectoral Methane Emission Estimates During 2019–2022: A Consistency Analysis with GOSAT Inversion

1
Satellite Observation Center, National Institute for Environmental Studies, Tsukuba 305-8506, Japan
2
The Cooperative Institute for Research in Environmental Sciences, University of Colorado Boulder, Boulder, CO 80309, USA
3
Global Monitoring Laboratory, National Oceanic and Atmospheric Administration (NOAA), Washington, DC 20230, USA
*
Author to whom correspondence should be addressed.
Remote Sens. 2025, 17(17), 2932; https://doi.org/10.3390/rs17172932
Submission received: 1 July 2025 / Revised: 16 August 2025 / Accepted: 18 August 2025 / Published: 23 August 2025

Abstract

We employed a global high-resolution inverse model to estimate sectoral methane emissions, integrating observations from the GOSAT-2 satellite for the first time, along with observations from the surface observation network. A similar set of inversions using GOSAT observations was carried out to evaluate the consistency between emissions estimates derived from these two satellites and to ensure that GOSAT-2 data could seamlessly integrate with the existing data series without disrupting the continuity of flux estimates. This analysis, covering the period from 2019 to 2022, utilized prior anthropogenic emissions data mainly from EDGAR v6 and incorporated additional natural sources and sinks as outlined by global methane budget, 2020. Our analysis reveals a general agreement between total methane emissions estimates from GOSAT and GOSAT-2. However, on a sectoral basis, we found notable regional differences in the flux estimates. While GOSAT inversion estimates ~8 Tg a−1 more anthropogenic emissions for China and around 4 Tg a−1 more wetland emissions for Brazil and Indonesia, the posterior error distribution suggests that GOSAT-2 inversion is closer to surface observations over Asia. These discrepancies are found in regions with significant differences in XCH4 data from the two satellites, such as East Asia and North America, tropical South America, and tropical Africa. These regional biases persist due to limited representative surface reference sites for Level 2 bias correction. The relatively lower data volume from GOSAT also introduces seasonal biases in the flux estimates when the quality filtering of Level 2 data persistently reduces usable observations during certain seasons, resulting in inadequate representation of the seasonal cycle in regions such as East Asia. Similarly, in tropical South America, where the model is relatively under-constrained by the limited surface observations, the lower data volume of GOSAT-2 suffers. While the two inversions exhibit consistent overall performance across North America and Europe, the GOSAT-2-based inversion demonstrates a better performance over East Asia. Therefore, while the two satellite datasets are broadly consistent, considering the fact that the biases in the XCH4 data overlap with regions under-constrained by surface observations, establishing additional surface reference measurement sites is desirable to ensure consistent inversion results.

1. Introduction

Methane is a potent greenhouse gas that has been increasing at a steeper rate of 8.6 ppb a year during recent years (2011–2020) [1,2]. Rising concentrations of methane have contributed to a 0.6 °C rise in global temperatures since pre-industrial times [3]. Hence, the emission mitigation efforts require more realistic emission quantification. Its sources are diverse, encompassing natural processes such as wetlands and geological seepage, as well as anthropogenic activities including agriculture, fossil fuel extraction, and waste management. Effective monitoring and quantification of methane emissions are essential for understanding climate change impacts and guiding mitigation. While bottom-up emission inventories form the basis of these efforts, their accuracy varies by country due to uncertainties. Inverse modeling, which assimilates observations from multiple platforms (e.g., [3,4]), helps assess these emissions. Accurate predictions of future methane growth depend on thoroughly understanding emission sources and processes. Anthropogenic and natural sources contribute by their pathways to the global growth rate. Anthropogenic emissions are influenced by the growing activities in agriculture, fossil fuel exploitation, and waste production. Natural sources, such as wetlands, are, on the other hand, influenced by climate change itself, such as the recent increase in wetland emissions reported by several studies (e.g., [5,6]). National greenhouse gas inventories are fundamental for countries to report their emissions and commitments under international agreements. However, these inventories often rely on uncertain assumptions and sparse ground-based measurements, highlighting the need for independent verification and refinement using advanced observational tools like atmospheric measurements and inverse modeling.
Satellite observations are attractive in the top-down emission estimation due to their coverage over global regions without ground-based measurements. Recent studies have used data from various satellites to constrain global [7,8,9] and regional methane fluxes [10,11]. Quite often, these top-down estimates are diverse and found to differ from bottom-up inventories [12], particularly in regions where the data coverage is insufficient to constrain the emissions. The Greenhouse gases Observing SATellite (GOSAT), launched by the Japan Aerospace Exploration Agency (JAXA) in 2009, marked a significant milestone in satellite-based methane observation. The GOSAT series comprises satellites observing atmospheric greenhouse gases jointly developed and operated by the Ministry of the Environment, Japan, JAXA, and the National Institute for Environmental Studies (NIES) [13,14]. Equipped with the thermal and near-infrared sensor for carbon observation (TANSO), GOSAT provides XCO2 and XCH4 retrievals for the total atmospheric column. Its successor, GOSAT-2, launched in 2018, builds upon this legacy with improved capabilities, including a slightly higher spatial footprint (9.7 versus 10.5 km), better spatial coverage, and enhanced sensitivity to methane emissions. The comparative analysis of GOSAT and GOSAT-2 inversions is pivotal for assessing the consistency and reliability of methane emission estimates derived from these satellites. This comparison not only validates the advancements made in satellite technology but also identifies areas for improvement in future missions. As satellite missions evolve and new technologies emerge, continuity and consistency in methane monitoring are essential for maintaining long-term datasets and ensuring the robustness of emission estimates.
Consistency between observations from various space-based instruments is crucial because varying regional biases in different products used together in inversion may counteract to inform the model differently. Many recent studies have demonstrated the potential and limitations of joint inversions of retrievals from various satellite instruments [1,15,16]. Although consistency is important, studies have pointed out that even when satellite retrievals agree reasonably well, data coverage (an adequate number of observations in a region) plays an important role in estimated emissions. For example, in a comparison of GOSAT and TROPOMI inversion, [1] found that better coverage over the Indo-Gangetic plain helped the TROPOMI-based inversion to correctly attribute the mode-observation difference over Bangladesh to local emissions instead of the upwind region of the Indo-Gangetic plain, as GOSAT inversion did. It is expected that there will be such an advantage of better coverage for GOSAT-2. Also, because successor missions like GOSAT-2 follow their predecessors (like GOSAT) after their nominal operational period, it is desirable to investigate temporal and spatial consistency in their inverted fluxes. When using such data for emission inversions, ensuring compatibility between datasets from consecutive missions is vital for reliable estimates. Differences due to major improvements in the remote sensing instruments or retrieval algorithms may change the data, but for other reasons, such as systematic errors (biases), ideally, we expect them to be minor so that both datasets have similar information content.
In this study, we examine the results of inverting methane observations from two satellite instruments in the same series to evaluate their regional consistency and to find out any potential statistically significant differences and their possible reasons. Regarding this point, in this study, we report the results of inverse modeling of GOSAT-2 for the first time and the analysis results of its sectoral comparison with the inversion of GOSAT for the period 2019–2022. As satellite Level 2 products are retrieved from radiance spectra, unlike direct measurements, they need to be corrected for biases based on reference observations. For a similar reason, we also include direct surface-based CH4 measurements from the same surface observation network for both inversions. That is, the experimental setup is the same in both cases, except for the satellite Level 2 data. This paper has the following structure. Section 2 describes the data used and the methods involved in this study, and Section 3 shows the results, including the comparison of sectoral emission estimates, validation with independent observations, and discussion of the causes behind regional inconsistencies, followed by the conclusion in Section 4.

2. Data and Methods

2.1. Observations

CH4 observations were collected from a network of surface monitoring stations, as compiled in the GLOBALVIEWplus_v4.0_2021-10-14 dataset [17], with additional data from the ICOS network [18]. A list of sites along with site-specific information is given in Table S1 (used for assimilation) and Table S2 (used for validation). Surface sites used in the inversion are also marked in Figure S1a. We have used observations from 89 stationary sites, with some stations having more than one measurement type (e.g., flask, in situ, etc.), and additional observations from ships, aircraft, etc. The spatial representativeness of the data used is given in Supplementary Figure S5. There is a glaring shortage of observation sites in Asia, southern Africa, and large parts of South America and Australia. Maximum coverage is in Europe, followed by North America. To ensure that the measurements were representative of well-mixed atmospheric conditions, continuous observations were averaged between 12:00 and 16:00 local time. For high-altitude sites, early morning averages (00:00–04:00 local time) were used to minimize the influence of local emissions transported upslope due to daytime heating. Data uncertainties for surface sites were assessed using the root mean squared error (RMSE) from prior forward simulations, with a minimum threshold of 6 ppb applied to provide greater flexibility for inversion in the southern hemisphere. Rejection criteria for surface, aircraft, and ship observations were based on data variance, with a threshold set at double the observed variance.
The satellite observations for this study were obtained from the GOSAT and its successor, GOSAT-2. We utilized the National Institute for Environmental Studies (NIES) short-wavelength infrared (SWIR) bias-corrected Level 2 product V02.95/96 for GOSAT [19] and the GOSAT-2 NIES full-physics-based bias-uncorrected Level 2 product V02.00 [20]. Ref. [20] proposed an empirical formula for correcting the systematic biases in the GOSAT-2 Level 2 product. However, for this study, this bias correction has not been applied. Both GOSAT and GOSAT-2 are sun-synchronous satellites, with GOSAT having a revisit cycle of three days and GOSAT-2 a cycle of six days. The TANSO-FTS onboard GOSAT provides observations with a nadir footprint diameter of approximately 10.5 km, while the newer TANSO-FTS-2 [21] has a footprint diameter of 9.7 km. TANSO-FTS-2 includes an advanced “intelligent pointing” function, which shifts the instrument’s line of sight to avoid clouds detected within its field of view, enhancing the availability of cloud-free data. A plot of one month (October 2019) of GOSAT and GOSAT-2 XCH4 observations is given in Supplementary Figure S1.

2.2. Prior Fluxes

Anthropogenic prior fluxes we used were from the Emission Database for Global Atmospheric Research (EDGAR v6, [22]), excluding emissions from the oil and gas sector. For oil and gas, we used data from the greenhouse gas and air pollution interactions and synergies (GAINS) model [23]. Biomass burning emissions were taken from the Global Fire Emission Database (GFED v4, [24]). Wetlands and termites were taken from [25]. Geological and oceanic emissions were taken from [26] and [27], respectively. The methane sink in the soil was taken from MeMo v1.0 [28]. All prior fluxes were provided to the model at 0.1° spatial resolution. Climatological maps of major emission sectors used in the model are given in Figure 1. Monthly climatologies were used for wetlands, geological, termite, and oceanic fluxes. All other fluxes were given at the monthly time step. The prior uncertainties were prescribed as 30% of the climatology of each anthropogenic sector and 50% for wetland emissions.

2.3. Meteorological Data

The meteorological data used for the transport model were obtained from the Japanese Reanalysis (JRA-55) [29], which provides the required parameters, such as three-dimensional wind fields, temperature, and humidity at 1.25° × 1.25° spatial resolution, 40 vertical hybrid sigma-pressure levels, and a temporal resolution of 6 h. The Japanese Meteorological Agency (JMA) has revised the meteorological product from earlier JRA-25 by improving the data assimilation system and including newly prepared data of past observations. Therefore, JMA states that JRA-55 has advantages over the previous version. Also, our modeling system has usually been driven by Japanese Reanalysis meteorology, unless there is a requirement for high resolution in horizontal or vertical coordinates.

2.4. Inverse Modeling System

2.4.1. NIES-TM-FLEXPART-VAR (NTFVAR) Inverse Modeling System

We utilized a global Eulerian–Lagrangian coupled inverse model known as NTFVAR, which integrates the National Institute for Environmental Studies (NIES) model with FLEXPART (FLEXible PARTicle dispersion model), representing an Eulerian three-dimensional transport model and a Lagrangian particle dispersion model, respectively. The development of this model was documented by [30]. Our version of the transport model is a modified iteration of the one previously described. This coupled model combines NIES-TM v21, which features a horizontal resolution of 3.75° and 42 hybrid-pressure vertical levels, with the FLEXPART model v.8.0, run in backward mode with a surface flux resolution of 0.1°. The resolution of the Lagrangian model is decided based on the resolution of the available surface fluxes. The current version incorporates revisions to the transport matrix, and indexing and sorting algorithms to enhance memory efficiency for managing large matrices of Lagrangian responses to surface fluxes, particularly for utilizing GOSAT and GOSAT-2 data in the inversion process. Additional details can be found in [31]. Different variants of this model have been used for methane inversion previously (e.g., [32], but this study uses a modified version used by [33].

2.4.2. The Inverse Modeling Scheme

We employed a high-resolution version of the transport model and its adjoint as detailed by [30], combined with the optimization schemes proposed by [34,35]. Following their methodology, flux corrections were estimated separately for anthropogenic and natural emissions. Variational optimization was utilized to derive six sets of scaling factors for monthly varying prior uncertainty fields at a resolution of 0.1° × 0.1°, applied independently to five anthropogenic and natural wetland emissions with a bi-weekly time step. Corrections to anthropogenic emissions were based on the monthly climatology provided by EDGAR sectors, while wetland emissions were adjusted according to the monthly climatology from the VISIT model, defined as the prior uncertainty fields for optimized sectors. The grid-scale flux uncertainty was set at 30% of EDGAR v6 climatology for anthropogenic emission sectors and 50% of VISIT climatological emissions for wetland emissions. Other natural flux categories, such as biomass burning, geological sources, termites, and soil sinks, were not optimized due to their significantly lower amplitude compared to wetlands. A spatial correlation length of 50 km and a temporal correlation of two weeks were applied. The inverse modeling problem was formulated to find the optimal values of x, which represent the corrections to prior fluxes, minimizing the cost function J(x).
J x = 1 2 H · x r T R 1 H · x r + 1 2 x T B 1 x
In this context, H represents the atmospheric transport operator, r denotes the difference between the observed concentrations and the forward simulations conducted using prior fluxes without any corrections, R is the covariance matrix of the observations, and B is the covariance matrix of the prior fluxes. The design of the B matrix involves representing it as a product of a non-dimensional covariance matrix C and a diagonal flux uncertainty matrix D, such that:
B = DT·C·D
The C matrix is typically implemented as a band matrix, where the non-diagonal elements decrease according to ~exp(−l2/d2), with l representing the distance between grid cells and d the correlation distance. The optimal solution, defined as the minimum of the cost function J was determined iteratively using the Broyden–Fletcher–Goldfarb–Shanno (BFGS) algorithm, as described by [36]. For additional details on the implementation, refer to [31].

2.4.3. Posterior Uncertainties

For calculating the posterior flux uncertainty, we used an ensemble of fifteen simulations by randomly perturbing the observations and the prior fluxes and taking the spread in the resulting flux as a measure of the posterior uncertainty, as in the method described by [37]. Pseudo-observations were prepared by perturbing the observations with their uncertainty at each site. Also, prior monthly perturbed fluxes were prepared, applying random scaling factors separately for each global carbon project (GCP) region and month. Inversions were carried out using the perturbed pseudo-observations and the perturbed fluxes (perturbed anthropogenic and wetlands with non-perturbed soil sink, biomass burning, and other natural emissions from the ocean, geological sources, and termites) as the prior fluxes.

2.5. Statistical Significance Test for Difference in Mean

To assess whether the mean flux corrections from the two inversions differ significantly, we performed Welch’s t-test ([38]) on the monthly flux corrections at 0.1° resolution. The formula for the test statistic is
t = X ¯ 1 X ¯ 2 S E X 1 2 + S E X 2 2
where
S E X i = S D i n i
in which SDi is the standard deviation and ni is the number of the sample. The analysis was conducted separately for each of the six optimized source sectors. Results are shown in Figure 2, with hatched areas indicating regions where the differences are statistically significant.

3. Results and Discussion

3.1. Methane Emission Estimates by GOSAT and GOSAT-2 Inversions

Figure 2 illustrates the grid-wise differences in flux corrections inferred from GOSAT and GOSAT-2 inversions to the prior sectoral methane emissions. Statistically significant differences are observed in the agriculture, waste, and wetland sectors, the most notable being the lower estimate for wetland emissions. We estimated a mean (2019–2022) global total emission of 605.2 Tg yr−1 for GOSAT and 601.8 Tg yr−1 for GOSAT-2 compared to the prior total of 615.3 Tg yr−1. Table 1 presents the global total sectoral emissions averaged over the study period for the prior and the two sets of inversions. Our estimate is in good agreement with the ensemble mean of the recent global methane synthesis [39]. Any mention of emission estimate in the following sections follows the order, GOSAT followed by GOSAT-2. When comparing the sectoral posterior emissions estimated by the GOSAT and GOSAT-2 inversions, there is a noticeable trend; GOSAT-2 generally estimates lower emissions for Southeast Asia (Figure 2) than GOSAT. The monthly mean XCH4 from GOSAT and GOSAT-2 is given in Supplementary Figure S7. GOSAT-2 provides lower estimates for the agriculture sector in Southeast Asia, parts of Europe, and tropical America. For instance, in China, GOSAT estimated 23.18 ± 1.54 Tg yr−1 of methane emissions from agriculture, while GOSAT-2 estimated 16.82 ± 1.12 Tg yr−1 (Table 2). This estimate is lower than recent studies, such as the one by [40] on TROPOMI inversion, which reported 17.8 Tg yr−1 from livestock and 11.9 Tg yr−1 from rice paddies using GOSAT as a reference to omit outliers in the inversion. Therefore, it is reasonable that our GOSAT inversion is on the upper side, closer to [40]. The primary reason for the difference with GOSAT-2 inversion is the lower XCH4 observed by GOSAT-2 over eastern China and the surrounding regions. In addition to the lower XCH4 in GOSAT-2, there is a bias introduced by the seasonal sampling differences. For example, over Southeast Asia, there is a clear seasonality in XCH4 due to agricultural emissions. By limiting the GOSAT-2 data volume to match that of GOSAT (see Supplementary Information for more details), we estimate around 3.2 ppm higher mean XCH4 for GOSAT due to limited observations during the monsoon. This also contributes to the differences seen in China or Southeast Asia in general. In contrast, for other regions of the globe, GOSAT-2 inversion estimates higher emissions compared to GOSAT, particularly in central North America, eastern temperate South America (Argentina 2.34 ± 0.25; 2.97 ± 0.31 Tg yr−1, Brazil 13.52 ± 0.36; 14.29 ± 0.38 Tg yr−1), tropical Africa, and Southwest Asia (Pakistan). However, the difference in the posterior agricultural emission in the two inversions for Pakistan is greater than the uncertainty level (5.34 ± 0.37; 5.87 ± 0.41 Tg yr−1).
In the waste sector, the largest emitter is China, with GOSAT estimating 14.36 ± 0.7 Tg yr−1 and GOSAT-2 estimating 13.35 ± 0.65 Tg yr−1, followed by USA (4.29 ± 0.05; 4.62 ± 0.06 Tg yr−1), India (6.56 ± 0.15; 6.44 ± 0.15 Tg yr−1), and Brazil (4.91 ± 0.09; 5.06 ± 0.09 Tg yr−1). GOSAT-2 also estimates lower emissions for Mexico, northern South American countries, and East, South, and Southeast Asia. Generally, GOSAT-2 has a good agreement with GOSAT over Australia, boreal Eurasia, and South Africa, while GOSAT-2 suggests higher emissions over Europe and eastern North America. For the coal sector, GOSAT estimates higher emissions than GOSAT-2 for India, China, Southeast Asia, and Australia. Conversely, GOSAT-2 provides higher emission estimates for the USA, Europe, and Russia. Emissions from coal mining in China are consistent between GOSAT and GOSAT-2 (18.97 ± 0.98 and 18.31 ± 0.95 Tg yr−1, respectively), aligning with recent studies such as [40], which reported 16.6 Tg yr−1. The differences between the inversions are within the estimation uncertainty for China. Additionally, slight variations in coal emission estimates between the two inversions are observed for Indonesia.
In the oil and gas sector, GOSAT-2 suggests higher emissions from localized sources in the United States, Europe, Russia, the Middle East, and parts of Africa. Conversely, GOSAT estimates higher emissions in Southeast Asian countries. The largest differences between the two inversions are observed for Nigeria (2.08 ± 0.37 Tg yr−1 vs. 2.86 ± 0.51 Tg yr−1, p < 0.05), one of Africa’s largest producers, and similar differences are noted for oil and gas producers in the Middle East, such as Iraq and Saudi Arabia. GOSAT-2 estimates higher emissions from major sources in the Middle East, Africa, and the United States. However, at the country level, the differences generally fall within the uncertainties of the inversions.
For wetland emissions, GOSAT estimates higher emissions in Amazonia, Southeast Asia, central Africa, and Australia. Figure 3b illustrates a slight bias remaining in the GOSAT-optimized forward simulation compared to observations in Amazonia and Southeast Asia, in contrast to the GOSAT-2 inversion (Figure 3d). GOSAT-2 suggests higher emissions in Canada, Russia, tropical Africa, and southern South America. The most notable differences at the country level are seen for Brazil (30.50 ± 1.67 Tg yr−1 vs. 26.19 ± 1.44 Tg yr−1, p < 0.1), Colombia (6.19 ± 0.35 Tg yr−1 vs. 4.71 ± 0.27 Tg yr−1), and Indonesia (12.12 ± 0.77 Tg yr−1 vs. 7.72 ± 0.49 Tg yr−1). Previous estimates for Brazil’s wetland emissions using GOSAT inversions ([41] were higher (e.g., ~39 Tg yr−1) compared to ~13 Tg yr−1 by [10]. In the present study with GOSAT and GOSAT-2 inversions, the estimates are 30.5 Tg yr−1 and 26.2 Tg yr−1, respectively. Figure 3d shows that the posterior simulation by GOSAT-2 exhibits less bias over Brazil compared to the optimized forward simulation by GOSAT, whereas GOSAT-2 estimates lower emissions in central African countries compared to GOSAT.
In East Asia and adjacent oceanic regions, GOSAT often shows higher XCH4 values, especially over China. Figure 4 highlights this, with some months showing XCH4 values exceeding 30 ppb or more in GOSAT compared to GOSAT-2. This discrepancy may account for the elevated emissions in sectors like agriculture, waste, and coal in the east China region. Figure 3 compares the differences between prior forward and optimized forward simulations of GOSAT and GOSAT-2. It is evident that the prior forward simulation for GOSAT-2 was more biased over North American and Asian regions (Figure 3c,h,j) compared to GOSAT, possibly due to the biases in the GOSAT-2 Level 2 data over North America and Asia [20]. These regions, having a bias in the XCH4 data identified by [20], exhibit biases in the prior forward also. The reasons for the spatial and temporal biases in these two datasets are still under investigation.
The analysis of the residual for forward and optimized simulations for GOSAT and GOSAT-2 reveals that both the inversions, on average, work well for North America and Europe (Figure 3e,f), but for East Asia, the posterior fit of the surface observations is handled better by GOSAT-2 inversion (Figure 3g). We have analyzed the results for these three regions defined as North America (60–135°W; 15–85°N), Europe (60°E–30°W; 35–72°N), and Asia (60–160°E; 10–75°N) to evaluate the estimated fluxes (Figure 3e–j). The figure shows the spatial distribution and the density curves for prior and optimized residuals for these three regions for GOSAT and GOSAT-2 inversions. The ability of the two inversions to reduce the posterior mean residuals for surface sites over North America is quite similar, and the distribution curves shift to neutral for both inversions. Similar observations can be made over Europe as well, but with almost indistinguishable performance by the two inversions in bias reduction (Figure 3f). The reason behind this is reflected in the analysis by [20] in their bias estimation of GOSAT and GOSAT-2 relative to the TCCON sites over Europe; both satellite products showed similar performance in the region. This means that both inversions could reduce the biases to the same degree. However, for Asia, there is a distinct difference between the two inversions. All other inputs being the same, GOSAT-2 inversion brings the biases to a minimum in this region compared to GOSAT inversion. This means that despite GOSAT being more mature and evolved in the retrieval processes over the years, GOSAT-2 performs well for the Asian region, which is less constrained by the limited surface observations.
Prior forward simulations for GOSAT show differences from GOSAT-2 prior simulations (Figure 3). GOSAT-2 prior residuals are more biased than GOSAT over North America and Asia. But this can be due to a combination of biases in prior emissions and the Level 2 data itself. However, considering the ability of the two inversions to represent the surface observations (Figure 3e,f,g), it is likely that GOSAT-2 inversions perform better for Asia, while GOSAT and GOSAT-2 are similar in Europe and North America.

3.2. Evaluation with Independent Observations

We used a set of observations that were not assimilated in the inversion process to have an independent evaluation of the posterior emissions in the two sets of inversions. The dataset includes surface and aircraft data across the globe. But a lack of coverage over the southern hemisphere generally and in the northern hemisphere over Asia, Africa, and South America is noted. The locations of the data are given in Figure 5a, and additionally, the details are tabulated in the Supplementary Table S2. Globally, the two inversions are consistent with similar residual statistics. Prior RMSE and bias were 32.1 and −3.95 ppb, respectively, while after optimization by GOSAT, RMSE and bias were 30.8 and −4.8 ppb, and with GOSAT-2 were 31.1 and −3.5 ppb. The detailed RMSE and BIAS for each validation site is given in Supplementary Figure S4. The probability density plot of prior and optimized residuals of the two inversions shows that the distribution of the residuals shifts closer to zero after optimization (Figure 5b). Moreover, the two inversions have similar posterior residual distributions. However, we found that for the validation sites in Russia and the northeastern USA, the bias has increased in both the inversions (Figure S5). Over northern African validation sites, GOSAT-2 optimization has increased bias. However, RMSE was found to have generally reduced except over the northeast USA and Mexico regions. The opposite biases in the African region are attributable mainly to the difference in GOSAT and GOSAT-2 Level 2 products. Over Russia, we have few ground observations, and the use of the oil and gas emissions from the GAINS model as prior over Russia introduces some unreasonably high posterior emissions for this sector over the region (Table 2). Unfortunately, there is not enough observation coverage over East Asia, Africa, or South America for validation.
In order to check the performance of the models in representing the marine boundary layer latitudinal profile, we sampled our posterior simulations by GOSAT and GOSAT-2 inversions at the same sites as those used in the NOAA marine boundary layer reference. The marine boundary layer reference (MBLR) is a reference for CH4 concentrations [42] represented by latitude and constructed from air samples of the Cooperative Air Sampling Network [43,44,45,46]. It is created by using selected marine boundary layer sites with measurements representative of a large volume of air masses for each trace gas, providing a latitudinally smoothed distribution of CH4. A detailed explanation can be found on the NOAA website https://gml.noaa.gov/ccgg/mbl/mbl.html (accessed on 28 October 2024) [42]. In the northern latitudes, GOSAT-2-based inversions show a better match to the MBLR, but in the southern hemisphere, GOSAT optimization brings the simulation closer to the reference (Figure 5c). However, inversion results for the southern hemisphere deviate more from the MBLR due to sparse observational constraints in this region.

3.3. Attribution of Regional Differences in Posterior Emissions

Since the two sets of inversions differ only by the set of satellite observations used, the estimated flux differences can be attributed to the regional differences in the Level 2 products. Another aspect that could influence the estimated flux is the data volume during the 4 years of analysis. That is the representativeness of satellite data in regions not covered by surface observations. Generally, GOSAT-2 has more observations than GOSAT, and sometimes, GOSAT has very little coverage over certain regions during certain times. We will examine the influence of these two aspects on the regional inconsistencies between the two inversions.

3.3.1. Regional Inconsistency Between XCH4 Retrieval Products

Though observations were retrieved using similar algorithms from two satellites, there can be regional inconsistencies between the products. Figure 4 presents the monthly perspective of the difference between GOSAT and GOSAT-2 XCH4 products (averaged on a 10° × 10° grid). We can see that there exist considerable regional differences between the two Level 2 products, especially over Africa, Europe, and eastern Asia. GOSAT-2 XCH4 is higher over northern Africa, the Middle East, Europe, and India during most of the months (January–September). GOSAT-2 XCH4 is lower than GOSAT over Russia, China, Southeast Asia, and adjoining oceanic regions from March to September (Figure 4). Over the United States, GOSAT-2 has lower XCH4 for almost all months. These seasonally persistent differences in the XCH4 influence the estimated fluxes, as can be seen in Figure 2. We should, however, note that the differences in the two data products shown in the mean picture need not be only due to regional biases in Level 2 products, but also due to any seasonally dependent quality control filter applied to each observation. For example, over regions with seasonal cloud cover, such as monsoon Asia, filtering out observations from cloudy scenes can leave the remaining data not representative of the whole year. To quantify the effect of seasonal sampling biases for Southeast Asia (85–135°E; 10°S–40°N), where we have persistent cloud cover, we performed an analysis by randomly sub-sampling the GOSAT-2 data to match the monthly data count to that of GOSAT. By taking the mean of the whole data and a thousand sub-samples, we estimate the mean XCH4 difference to be around 3.2 ppb. With a scale factor estimated by weighted regression of the monthly difference in XCH4 and estimated flux, we arrive at around 7.3 Tg yr−1 flux difference due to the difference in sampling (Figure S8). In Figure 6, we present the time series evolution of average XCH4 roughly over Amazonia (80–50°W; 10°S–10°N) and East Asia (80–120°E; 20–60°N). For both regions, there is a seasonal minimum concentration from June to September. So, if observations are cleared for cloud cover, there is a chance that the majority of observations represent a slightly elevated XCH4 over East Asia than they would be in the actual case. On the contrary, the convective season over Amazonia is from December to April. Filtering observations during this season will reduce observations of peak wetland methane emissions following the inundation. For satellites having a large number of observations, such as GOSAT-2 (almost double compared to GOSAT), there will still be more observations to compensate for the filtered-out data (Figure 7). These differences become crucial when the region is poorly constrained by surface observations. For example, for almost half of the year, the east and Southeast Asian and tropical African regions have significant differences in the representative XCH4, as shown in Figure 4. This can be seen reflected in the difference in the flux corrections with the two sets of Level 2 products (Figure 2).
Ref. [20] examined the consistency of XCO2 and XCH4 retrievals between GOSAT and GOSAT-2 and found an overall agreement between the two satellites, but pointed out the need for additional surface-based validation sites in light of the regional differences in bias between them. In their validation of GOSAT and GOSAT-2 XCH4 products with TCCON observations, they found a negative bias of −5.7 ppb around the Darwin TCCON site for GOSAT-2, but no sufficient data is available for GOSAT. A similar negative bias was found over Burgos for GOSAT-2, while a strong positive BIAS was found for Saga (Table 2 of [20]). In summary, though there are only a few sites for validation, their results indicate that there is likely considerable bias for both GOSAT and GOSAT-2 over East Asia remaining in the products. Comparatively lower emissions by GOSAT-2 inversion over the region covering Southeast Asia and Australia indicate that this is influenced by the lower GOSAT-2 XCH4 data. They have attributed the higher Xgas concentration in GOSAT-2 over northern Africa (similar to biases in Figure 4) to the bias in the aerosol optical thickness in GOSAT-2 retrieval compared to GOSAT.

3.3.2. Regional Differences in Data Density

Comparing the data volume for composite months (Figure 7), there is apparently a lower number of GOSAT-2 observations over Northern North America, Russia, and southern South America. Apart from these regions, all other regions have a higher data count for GOSAT-2. This means that these regions have additional observational constraints by GOSAT-2, especially over regions not adequately observed by surface sites. Though there is a reduction in GOSAT-2 data over Russia, the differences in posterior emissions are not statistically significant. Instead, there are statistically significant differences in the other regions, e.g., Canada, Argentina, Chile, etc. The XCH4 over the southern part of South America, North America, and Russia is remarkably lower (Figure 4); however, the GOSAT-2 inversion allocates more emissions over southern South America and boreal North America. The higher emission over southern South America in GOSAT-2 inversions is attributable to the anomalously low number of satellite observations (Figure 7), which makes this region the most under-constrained when comparing the two inversions. In the case of boreal North America, both satellite datasets have limited observations. This makes this region yet another under-constrained area, and the model allocates more flux there. Over Africa, GOSAT-2 is biased (higher than GOSAT) and has the largest regional data volume, so that this region is normally under-constrained by the surface observation network and has larger emissions across all sectors in GOSAT-2 inversion. A major reason for the observed differences in the regionally inferred fluxes could potentially be the seasonal dependence in quality filtering of Level 2 data between these products. For example, the cloud screening of the Level 2 products can be seasonally dependent over monsoon Asia during the northern hemispheric summer. Since GOSAT has a lower data volume compared to GOSAT-2 per month (Figures S2 and S3), cloud filtering during the monsoon season increases the fraction of available observations during non-monsoon months. A monthly mean picture of the data retrieval rate over East Asia is given in Supplementary Figure S4. Considering that this is a data-sparse region as far as surface observations are concerned, this region remains under-constrained during summer. However, for the East Asian domain, the average XCH4 has a seasonal low during the monsoon (Figure 6) and hence has an inherent tendency to infer higher aggregated emissions over this region. In other words, this leads to an insufficient representation of the CH4 seasonal cycle. On the other hand, GOSAT-2 has a higher number of observations to compensate for the filtered-out observations. Considering that these regions are poorly constrained by the surface networks, there is an apparent difference in the estimated fluxes.
The GOSAT and GOSAT-2 Level 2 products exhibit considerable regional differences (Figure 4) that need to be fixed. The African continent has high CH4 for GOSAT-2 from February to August, while it has lower XCH4 over and adjoining regions of East Asia from May through September. Figure 7 shows the difference in the number of observations between GOSAT and GOSAT-2 during the 2019–2022 period, counted in 10° × 10° grids over the globe. The actual data count for them can be seen in Figures S2 and S3. The difference is not very significant during the northern winter months (Nov-Feb) but is apparent in the months from March to September, especially over Africa, South America, and regions of India and China. GOSAT-2 has twice as the observations per day as GOSAT and thus retains more observations after filtering out cloudy scenes. Therefore, GOSAT-2 has higher data volume during warmer months in Africa and Southeast Asia. However, despite GOSAT-2 having more data overall, GOSAT has higher data density over southern South America. This depends on the higher sensitivity of FTS-2 onboard GOSAT-2 to abundant cosmic ray influx over the South Atlantic Anomaly of the geomagnetic field and the resultant contamination of spectra, which are filtered out during the retrieval process. From Figure 4, we can see that there are some significant regional biases from March to September over Asia, Africa, and South American regions between the observations from the two instruments. Figure 6 gives the time series of XCH4 averaged over the spatial regions represented by 80–50°W, 10°S–10°N, and 80–120°E, 0–30°N, respectively, over Amazonia and East Asian regions. We focus only on these two regions because the difference in flux corrections by the inversions using the two satellite data is sizable (Figure 2). Over East Asia, the time series has a seasonal minimum during the June to September period, or close to northern summer. Similarly, over the Amazon region, the averaged XCH4 by GOSAT and GOSAT-2 shows a seasonal minimum during this season, though the cycle is not well defined. The ultimate effect of this seasonally dependent quality filtering is inadequate representation of the seasonal cycle in XCH4 data, leading to biased estimates in the fluxes, where GOSAT-2 has an advantage in East Asia due to its larger volume of data.

4. Conclusions

In this paper, for the first time, we use GOSAT-2 observations along with observations from a surface observation network for inverse estimation of sectoral methane emissions for the 2019–2022 period. We have analyzed the results of GOSAT-2 inversion together with methane emissions estimated using GOSAT observations. The objective of the study was a comparative analysis of estimated sectoral fluxes from these two inversions and their regional consistency, identifying the potential causes of any inconsistency, and noting which dataset performs better over large regions such as North America, East Asia, and Europe. Overall, the two inversions generally agree over the global sectoral emissions, while they have differences from a regional point of view. Major differences in the estimated sectoral fluxes are generally over East and Southeast Asia, Africa, and tropical South America. These regions coincide with the areas where GOSAT and GOSAT-2 have inconsistencies in the XCH4 product. GOSAT-2 tends to have lower XCH4 over East and Southeast Asia and the neighboring oceanic regions, while GOSAT-2 has higher XCH4 values over Africa, the Middle East, and India. Although validation of the sectoral optimized fluxes is difficult using independent observations, we analyze the plausible reasons for the regional differences in the total fluxes inferred by the two sets of satellite observations. Most of our independent data are from North America and Europe, and the distribution of residuals after optimization shows reduced bias than prior residuals over these two spatial domains. However, there are other regions, such as Asia, where GOSAT-2 performs better. The most valuable contribution of satellite observations in flux inversion is over such regions with sparse surface-based observation coverage. The NIES retrieval algorithm used for the two satellite Level 2 products is similar, but there are regional differences in the XCH4 data. Remaining biases in Level 2 products significantly affect flux estimates, especially in regions with limited surface network constraints. Recent studies emphasized the causes for such regional differences in XCH4 products, such as the simultaneously retrieved aerosol optical depth over, for example, the African continent, and the need for further corrections of biases in the Level 2 data. Apart from the differences in the retrieval products, quality filtering that removes data for a particular season in one product can also make a difference. We have found that the net annual emissions inferred from the satellite products can be influenced by the regional biases in the data from different sources when the region has poor coverage by the surface observations included in the inversion, as well as when surface-based total column observation sites like TCCON used for bias correction of the satellite data do not represent the region adequately. This difficulty is exacerbated if the region’s XCH4 has a lower data volume due to quality filtering, which depends on seasonal cloud cover, such as monsoon Asia. Therefore, as a first comparison between inverse modeling of methane using GOSAT and GOSAT-2, this study is a key step in further improving the XCH4 retrievals from these satellite observations, so that inversions based on these two datasets produce minimal biases in the inferred sectoral fluxes. From the results of the analysis in this study, we emphasize the need for establishing key observation sites in data-sparse regions such as Asia, including reference sites used for the validation of satellite observations, and ensuring sufficient data volume during cloudy seasons, especially for the utility of the combined use of satellite data from different platforms in inferring surface fluxes.
The limitations of the study include the fact that additional bias corrections proposed for GOSAT-2 XCH4 data by the retrieval group were not applied, while we used bias-corrected GOSAT data. However, we do apply a bias correction based on a surface-optimized forward model to both the data. However, this surface optimization could also leave some regions, such as East Asia or Amazonia, not adequately constrained by the surface observation network. Another point is that, for validation, we have quite a few observations in the Asian region, especially East Asia, where we found a better performance for GOSAT-2.

Supplementary Materials

The following supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/rs17172932/s1, Figure S1: Observation locations; Figure S2: Number of GOSAT observations per month on 10° × 10° grid; Figure S3: Number of GOSAT-2 observations per month on 10° × 10° grid; Figure S4: RMSE and BIAS for assimilated surface sites; Figure S5: Spatial representativeness of observation sites in 10° × 10° regions; Figure S6: Monthly fraction of GOSAT and GOSAT-2 successful retrievals; Figure S7: Monthly climatological mean of GOSAT and GOSAT-2 XCH4 over East Asia; Figure S8: Estimation of seasonal sampling biases on inferred fluxes over southeast Asia; Table S1: Details of observations used in inversion; Table S2: Details of observations used for validating the inversion.

Author Contributions

R.J. conducted the inversions, analyzed the data, and prepared the initial manuscript. S.M. developed the model, prepared the Lagrangian simulations, and provided discussions during the preparation of the manuscript. F.W. and L.N. provided critical discussions and revised the manuscript. Y.Y. prepared the satellite Level 2 data and revised the manuscript. X.L. contributed several observations used in this inversion and shared constructive comments during the analysis and revision of the manuscript. T.M. supervised the project and the study. All authors have read and agreed to the published version of the manuscript.

Funding

This study was financially supported by the NIES GOSAT and GOSAT-2 projects and the Ministry of the Environment, Japan.

Data Availability Statement

Restrictions apply to the datasets: The datasets presented in this article are not readily available because of administrative restrictions. Requests to access the observational datasets should be directed to the principal investigators.

Acknowledgments

We thank the Ministry of the Environment, Japan, for the financial support for the GOSAT project, under which this work was carried out. The simulations were carried out at the supercomputing facility at the National Institute for Environmental Studies, Tsukuba, Japan. The authors acknowledge the PIs and contributors related to the operations in the compilations of the Obspack CH4 dataset (obspack_ch4_1_GLOBALVIEWplus_v4.0_2021-10-14) and the ICOS network. The contributions from the following people and institutions are thankfully acknowledged: A. di Sarra and S. Piacentino (ENEA); A. Zahn, F. Obersteiner, H. Boenisch, and T. Gehrlein (KIT/IMK); A. Desai (UofWI); A. Karion (NIST); A. Andrews, B. Baier, C. Sweeney, E. Dlugokencky, E. Hintsa, F. Moore, J. B. Miller, K. McKain, and K. N. Schuldt (NOAA); A. Colomb and J. M. Pichon (OPGC); B. Scheeren and H. Chen (RUG); B. Viner (SRNL); B. Stephens (NCAR); C. Labuschagne (SAWS); C. L. Myhre, K. Tørseth, and O. Hermanssen (NILU); C. E. Miller (NASA-JPL); C.-H. Lee, H. Lee, H.-Y. Kang, and M.-Y. Ko (KMA); C. Plass-Duelmer, D. Kubistin, M. Schumacher, and M. Lindauer (DWD); C. Gerbig (MPI-BGC); C. D. Sloop (EN); D. Jaffe (UofWA); D. Munro (NOAA-CIRES); D. Worthy (ECCC); E. Kozlova (CEDA); E. Gloor (UoL); E. Cuevas, and P. P. Rivas (AEMET); E. Kort (UoM); G. Vitkova, K. Kominkova, and M. V. Marek (CAS); G. Manca and P. Bergamaschi (JRC); G. Brailsford and S. Nichol (NIWA); H. Matsueda (MRI); I. Lehner, T. Biermann, and M. Heliasz (LUND-CEC); I. Mammarella and P. Keronen (UHELS); J. W. Elkins (HATS); J. Müller-Williams (HPB); J. Arduini (UNIURB); J. Turnbull (GNS); J. Lee (UofME); J. P. DiGangi (NASA-LaRC); J. Hatakka, T. Laurila, and T. Aalto (FMI); J. Holst and M. Mölder (LUND-NATEKO); K. Saito (JMA); K. Davis, N. Miles, S. Richardson, and T. Lauvaux (PSU); L. V. Gatti (INPE); L. Emmenegger and M. Steinbacher (EMPA); L. Haszpra (RCAES); M. K. Sha, and M. De Mazière (BIRA-IASB); J. M. Metzger (LACy); M. Delmotte, M. Ramonet, M. Lopez, and V. Kazan (LSCE); M. L. Fischer and M. Torn (LBNL); M. Leuenberger (KUP); M. Sasakawa, T. Machida, and Y. Niwa (NIES); O. Laurent (ICOS-ATC); P. Trisolino, P. Cristofanelli (CNR-ISAC); P. Krummel, R. Langenfelds, and Z. Loh (CSIRO); P. Shepson (PU); P. Smith (SLU); S. C. Biraud (LBNL-ARM); S. Morimoto and S. Aoki (TU); S. O’Doherty (UNIVBRIS); S. Wofsy (HU); S. Conil (Andra); T. Schuck (IAU); V. Ivakhov (MGO); and D. Goto (NIPR). NOAA measurements are supported in part by the NOAA cooperative agreement NA22OAR4320151. The statements, findings, conclusions, and recommendations are those of the author(s) and do not necessarily reflect the views of NOAA or the U.S. Department of Commerce.

Conflicts of Interest

The authors declare no conflict of interest.

Correction Statement

This article has been republished with a minor correction to the Data Availability Statement. This change does not affect the scientific content of the article.

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Figure 1. Climatological sectoral prior fluxes used in this study (gCH4 m−2 day−1, scale different for each panel).
Figure 1. Climatological sectoral prior fluxes used in this study (gCH4 m−2 day−1, scale different for each panel).
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Figure 2. The sectoral mean (2019–2022) difference in the flux corrections (gCH4 m−2 d−1) in the inversion of GOSAT and GOSAT-2 (GOSAT-2−GOSAT). The hatchings indicate regions where the mean differences are statistically significant at p < 0.01. The country maps may not represent the actual political boundaries, but only a software-dependent approximate outline.
Figure 2. The sectoral mean (2019–2022) difference in the flux corrections (gCH4 m−2 d−1) in the inversion of GOSAT and GOSAT-2 (GOSAT-2−GOSAT). The hatchings indicate regions where the mean differences are statistically significant at p < 0.01. The country maps may not represent the actual political boundaries, but only a software-dependent approximate outline.
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Figure 3. The mean difference of prior and optimized forward model with GOSAT and GOSAT-2 observations gridded on a 4° × 4° grid (ad). Frequency distribution curves of prior (lighter color) and optimized (darker color) forward residuals corresponding to GOSAT (red) and GOSAT-2 (blue) inversions, for surface (eg) and satellite (hj) observations for three regions, North America (e,h), Europe (f,i), and Asia (g,j). The country maps may not represent the actual political boundaries.
Figure 3. The mean difference of prior and optimized forward model with GOSAT and GOSAT-2 observations gridded on a 4° × 4° grid (ad). Frequency distribution curves of prior (lighter color) and optimized (darker color) forward residuals corresponding to GOSAT (red) and GOSAT-2 (blue) inversions, for surface (eg) and satellite (hj) observations for three regions, North America (e,h), Europe (f,i), and Asia (g,j). The country maps may not represent the actual political boundaries.
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Figure 4. The difference in mean XCH4 (GOSAT-2−GOSAT) averaged on a 10° × 10° grid for each calendar month. The country maps may not represent the actual political boundaries.
Figure 4. The difference in mean XCH4 (GOSAT-2−GOSAT) averaged on a 10° × 10° grid for each calendar month. The country maps may not represent the actual political boundaries.
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Figure 5. Validation of the two inversions with observations that were not assimilated in the inversion step. Locations of the observation sites used in this validation are presented in (a), and the kernel density estimates of the prior and posterior residuals are given in (b). More details on the sites selected for validation are given in Table S2. (c) Comparison of the NOAA marine boundary layer reference with the latitude-wise average of optimized simulations using GOSAT and GOSAT-2 data. The sites used for averaging are a subset of the list.
Figure 5. Validation of the two inversions with observations that were not assimilated in the inversion step. Locations of the observation sites used in this validation are presented in (a), and the kernel density estimates of the prior and posterior residuals are given in (b). More details on the sites selected for validation are given in Table S2. (c) Comparison of the NOAA marine boundary layer reference with the latitude-wise average of optimized simulations using GOSAT and GOSAT-2 data. The sites used for averaging are a subset of the list.
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Figure 6. Time series of monthly area-averaged XCH4 values over Amazonia and East Asia regions. The months from June to September are shaded, which indicates the dry season for Brazil and the wet season for East Asia.
Figure 6. Time series of monthly area-averaged XCH4 values over Amazonia and East Asia regions. The months from June to September are shaded, which indicates the dry season for Brazil and the wet season for East Asia.
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Figure 7. The difference in the number of observations of GOSAT and GOSAT-2 in each 10° grid (GOSAT-2—GOSAT). The country maps may not represent the actual political boundaries.
Figure 7. The difference in the number of observations of GOSAT and GOSAT-2 in each 10° grid (GOSAT-2—GOSAT). The country maps may not represent the actual political boundaries.
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Table 1. Global totals of sectoral emission estimates for prior, GOSAT, and GOSAT-2 inversions in units of Tg yr−1. The values are the mean for the 2019–2022 period. Sectors marked with an asterisk were not optimized.
Table 1. Global totals of sectoral emission estimates for prior, GOSAT, and GOSAT-2 inversions in units of Tg yr−1. The values are the mean for the 2019–2022 period. Sectors marked with an asterisk were not optimized.
SectorsPriorGOSAT InversionGOSAT-2 Inversion
Total615.27605.20601.83
Agriculture159.85156.23154.72
Waste82.3480.0280.28
Biomass burning26.8622.7822.79
Coal37.8136.5036.14
Geological *23.0223.0223.02
Other microbial *9.919.919.91
Ocean *11.4811.4811.48
Oil and gas90.0283.5287.79
Wetlands173.99177.84171.80
Soil sink *−35.51−35.51−35.51
Table 2. Comparison of country-level sectoral emissions inferred by inversion of GOSAT and GOSAT-2 data and the associated uncertainties for selected major emitting countries in units of Tg yr−1.
Table 2. Comparison of country-level sectoral emissions inferred by inversion of GOSAT and GOSAT-2 data and the associated uncertainties for selected major emitting countries in units of Tg yr−1.
SectorsAgricultureWasteBiomass and BiofuelCoalOil and GasWetland
CountryGOSATGOSAT-2GOSATGOSAT-2GOSATGOSAT-2GOSATGOSAT-2GOSATGOSAT-2GOSATGOSAT-2
ARG2.34 ± 0.252.97 ± 0.310.52 ± 0.010.55 ± 0.010.11 ± 0.000.11 ± 0.000.00 ± 0.000.00 ± 0.000.44 ± 0.010.47 ± 0.013.58 ± 0.153.86 ± 0.16
AUS1.89 ± 0.242.04 ± 0.260.31 ± 0.010.31 ± 0.010.88 ± 0.020.88 ± 0.020.79 ± 0.050.79 ± 0.050.27 ± 0.000.26 ± 0.003.84 ± 0.163.40 ± 0.14
BOL0.72 ± 0.020.75 ± 0.020.08 ± 0.000.08 ± 0.000.44 ± 0.000.44 ± 0.000.00 ± 0.000.00 ± 0.000.12 ± 0.000.12 ± 0.004.68 ± 0.274.38 ± 0.26
BRA13.52 ± 0.3614.29 ± 0.384.91 ± 0.095.06 ± 0.091.85 ± 0.041.85 ± 0.040.05 ± 0.000.05 ± 0.000.22 ± 0.010.23 ± 0.0130.50 ± 1.6726.19 ± 1.44
CAN1.06 ± 0.021.15 ± 0.020.57 ± 0.010.62 ± 0.010.46 ± 0.000.46 ± 0.000.08 ± 0.010.08 ± 0.012.68 ± 0.112.84 ± 0.1211.20 ± 0.7013.49 ± 0.84
CHN23.18 ± 1.5416.82 ± 1.1214.36 ± 0.7013.35 ± 0.652.47 ± 0.032.42 ± 0.0318.97 ± 0.9818.31 ± 0.952.69 ± 0.022.75 ± 0.023.03 ± 0.092.92 ± 0.09
COL1.89 ± 0.051.80 ± 0.050.82 ± 0.010.80 ± 0.010.07 ± 0.000.07 ± 0.000.20 ± 0.000.20 ± 0.000.44 ± 0.020.43 ± 0.026.19 ± 0.354.71 ± 0.27
COG0.02 ± 0.000.03 ± 0.000.03 ± 0.000.03 ± 0.000.08 ± 0.000.08 ± 0.000.00 ± 0.000.00 ± 0.000.06 ± 0.000.07 ± 0.005.97 ± 0.255.95 ± 0.25
COD0.30 ± 0.000.31 ± 0.000.64 ± 0.020.64 ± 0.021.35 ± 0.041.35 ± 0.040.00 ± 0.000.00 ± 0.000.02 ± 0.000.02 ± 0.0013.59 ± 0.8013.44 ± 0.79
IND16.37 ± 1.6315.73 ± 1.566.56 ± 0.156.44 ± 0.151.23 ± 0.051.23 ± 0.051.11 ± 0.051.05 ± 0.050.47 ± 0.010.47 ± 0.013.92 ± 0.174.06 ± 0.17
IDN3.70 ± 0.343.20 ± 0.302.04 ± 0.111.89 ± 0.102.17 ± 0.012.17 ± 0.014.83 ± 0.304.53 ± 0.280.79 ± 0.060.60 ± 0.0412.12 ± 0.777.72 ± 0.49
IRQ0.13 ± 0.020.14 ± 0.030.44 ± 0.010.46 ± 0.010.00 ± 0.000.00 ± 0.000.00 ± 0.000.00 ± 0.006.38 ± 0.966.91 ± 1.040.09 ± 0.000.10 ± 0.00
MEX2.67 ± 0.052.65 ± 0.052.48 ± 0.032.43 ± 0.030.21 ± 0.000.21 ± 0.000.01 ± 0.010.01 ± 0.010.29 ± 0.020.30 ± 0.021.35 ± 0.051.29 ± 0.05
NGA1.85 ± 0.042.25 ± 0.051.47 ± 0.021.57 ± 0.020.85 ± 0.010.90 ± 0.010.00 ± 0.000.00 ± 0.002.08 ± 0.372.86 ± 0.511.77 ± 0.112.09 ± 0.13
PAK5.34 ± 0.375.87 ± 0.411.30 ± 0.031.33 ± 0.040.32 ± 0.010.33 ± 0.010.03 ± 0.000.03 ± 0.000.53 ± 0.030.56 ± 0.040.16 ± 0.010.16 ± 0.01
PER0.53 ± 0.000.52 ± 0.000.27 ± 0.000.27 ± 0.000.04 ± 0.000.04 ± 0.000.00 ± 0.000.00 ± 0.000.03 ± 0.000.03 ± 0.007.80 ± 0.536.18 ± 0.42
RUS1.59 ± 0.021.67 ± 0.023.36 ± 0.033.53 ± 0.042.93 ± 0.352.93 ± 0.353.15 ± 0.133.24 ± 0.1315.78 ± 0.4116.36 ± 0.4314.54 ± 1.1915.50 ± 1.27
SDN2.58 ± 0.032.98 ± 0.040.44 ± 0.010.45 ± 0.010.34 ± 0.000.34 ± 0.000.00 ± −0.000.00 ± −0.000.59 ± 0.020.61 ± 0.023.13 ± 0.233.40 ± 0.25
THA2.50 ± 0.492.01 ± 0.390.95 ± 0.030.87 ± 0.030.13 ± 0.030.13 ± 0.030.01 ± 0.000.01 ± 0.000.12 ± 0.010.08 ± 0.011.10 ± 0.080.89 ± 0.06
USA9.63 ± 0.2910.79 ± 0.324.29 ± 0.054.62 ± 0.060.68 ± 0.080.68 ± 0.081.44 ± 0.281.60 ± 0.3120.57 ± 0.2821.09 ± 0.295.58 ± 0.286.20 ± 0.32
VEN1.17 ± 0.021.12 ± 0.020.36 ± 0.000.36 ± 0.000.15 ± 0.010.15 ± 0.010.01 ± 0.000.01 ± 0.000.47 ± 0.010.45 ± 0.014.52 ± 0.353.44 ± 0.26
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Janardanan, R.; Maksyutov, S.; Wang, F.; Nayagam, L.; Yoshida, Y.; Lan, X.; Matsunaga, T. High-Resolution Inversion of GOSAT-2 Retrievals for Sectoral Methane Emission Estimates During 2019–2022: A Consistency Analysis with GOSAT Inversion. Remote Sens. 2025, 17, 2932. https://doi.org/10.3390/rs17172932

AMA Style

Janardanan R, Maksyutov S, Wang F, Nayagam L, Yoshida Y, Lan X, Matsunaga T. High-Resolution Inversion of GOSAT-2 Retrievals for Sectoral Methane Emission Estimates During 2019–2022: A Consistency Analysis with GOSAT Inversion. Remote Sensing. 2025; 17(17):2932. https://doi.org/10.3390/rs17172932

Chicago/Turabian Style

Janardanan, Rajesh, Shamil Maksyutov, Fenjuan Wang, Lorna Nayagam, Yukio Yoshida, Xin Lan, and Tsuneo Matsunaga. 2025. "High-Resolution Inversion of GOSAT-2 Retrievals for Sectoral Methane Emission Estimates During 2019–2022: A Consistency Analysis with GOSAT Inversion" Remote Sensing 17, no. 17: 2932. https://doi.org/10.3390/rs17172932

APA Style

Janardanan, R., Maksyutov, S., Wang, F., Nayagam, L., Yoshida, Y., Lan, X., & Matsunaga, T. (2025). High-Resolution Inversion of GOSAT-2 Retrievals for Sectoral Methane Emission Estimates During 2019–2022: A Consistency Analysis with GOSAT Inversion. Remote Sensing, 17(17), 2932. https://doi.org/10.3390/rs17172932

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