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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESSD</journal-id><journal-title-group>
    <journal-title>Earth System Science Data</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESSD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Sci. Data</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1866-3516</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/essd-17-4305-2025</article-id><title-group><article-title>ESA CCI Soil Moisture GAPFILLED: an independent global gap-free satellite climate data record with uncertainty estimates</article-title><alt-title>ESA CCI Soil Moisture GAPFILLED</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Preimesberger</surname><given-names>Wolfgang</given-names></name>
          <email>wolfgang.preimesberger@geo.tuwien.ac.at</email>
        <ext-link>https://orcid.org/0000-0002-6655-0588</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Stradiotti</surname><given-names>Pietro</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Dorigo</surname><given-names>Wouter</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8054-7572</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Geodesy and Geoinformation, TU Wien, Wiedner Hauptstraße 8, 1040 Vienna, Austria</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Wolfgang Preimesberger (wolfgang.preimesberger@geo.tuwien.ac.at)</corresp></author-notes><pub-date><day>5</day><month>September</month><year>2025</year></pub-date>
      
      <volume>17</volume>
      <issue>9</issue>
      <fpage>4305</fpage><lpage>4329</lpage>
      <history>
        <date date-type="received"><day>23</day><month>December</month><year>2024</year></date>
           <date date-type="rev-request"><day>16</day><month>January</month><year>2025</year></date>
           <date date-type="rev-recd"><day>28</day><month>April</month><year>2025</year></date>
           <date date-type="accepted"><day>5</day><month>June</month><year>2025</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2025 Wolfgang Preimesberger et al.</copyright-statement>
        <copyright-year>2025</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025.html">This article is available from https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025.html</self-uri><self-uri xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025.pdf">The full text article is available as a PDF file from https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e95">The ESA CCI Soil Moisture multi-satellite climate data record is a widely used dataset for large-scale hydrological and climatological applications and studies. However, data gaps in the record can affect derived statistics such as long-term trends and – if not taken into account – can potentially lead to inaccurate conclusions. Here, we present a novel gap-free dataset, covering the period from January 1991 to December 2023. Our dataset distinguishes itself from other gap-filled products, as it is purely based on the available soil moisture (SM) measurements (independent of ancillary variables to make predictions), and further due to the inclusion of uncertainty estimates for all interpolated data points.</p>

      <p id="d2e98">Our gap-filling framework is based on a well-established univariate discrete cosine transform with the penalized least-squares (DCT-PLS) algorithm. This ensures that the dataset remains fully independent of other soil moisture and biogeophysical datasets and eliminates the risk of introducing non-soil-moisture features from other variables. We apply DCT-PLS on a spatial moving window basis to predict missing data points based on temporal and regional neighbourhood information. The challenge of providing gap-free estimates during extended periods of frozen soils is addressed by applying a linear interpolation for these periods, which approximates the retention of frozen water in the soil. To quantify the inherent uncertainties in our predictions, we developed an uncertainty estimation model that considers the input observations quality and the performance of the gap-filling algorithm under different surface conditions. We evaluate our algorithm through performance metrics with independent in situ reference measurements and by its ability to restore GLDAS Noah reanalysis data in artificially introduced satellite-like gaps. We find that the gap-filled data perform comparably to the original observations in terms of correlation and unbiased root mean squared difference (ubRMSD) with in situ data (global median <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.72</mml:mn></mml:mrow></mml:math></inline-formula>, ubRMSD <inline-formula><mml:math id="M2" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.05 m<sup>3</sup> m<sup>−3</sup>). However, in some complex environments with sparse observation coverage, performance is lower.</p>

      <p id="d2e141">The new ESA CCI SM v09.1 GAPFILLED dataset is publicly available at <ext-link xlink:href="https://doi.org/10.48436/hcm6n-t4m35" ext-link-type="DOI">10.48436/hcm6n-t4m35</ext-link> <xref ref-type="bibr" rid="bib1.bibx99" id="paren.1"/> and will see yearly updates due to its inclusion in the operational ESA CCI SM production.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>European Space Agency</funding-source>
<award-id>4000126684/19/I-NB</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e159">Satellite soil moisture data are relevant for a wide range of applications, including water resource management, agriculture, disaster risk assessment and response, weather prediction, and climate monitoring <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx110" id="paren.2"/>. Soil moisture (SM) is classified as an essential climate variable (ECV) <xref ref-type="bibr" rid="bib1.bibx41" id="paren.3"/>, and dedicated satellite missions such as ESA's SMOS <xref ref-type="bibr" rid="bib1.bibx61" id="paren.4"/> or NASA's SMAP <xref ref-type="bibr" rid="bib1.bibx37" id="paren.5"/> have been launched to measure it. However, the data coverage of individual satellites is limited by their lifespan and revisit frequency, requiring multiple days for a complete set of global measurements. Long-term analyses of climate variability and change require at least 30 years of data <xref ref-type="bibr" rid="bib1.bibx41" id="paren.6"/>, which surpasses the lifespan of any single Earth observation satellite. Measurements from multiple platforms are therefore harmonized and merged to create consistent multi-decadal records, such as the ESA CCI soil moisture (ESA CCI SM) products <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx47 bib1.bibx98" id="paren.7"/>. Despite the high number of currently operational satellites integrated in ESA CCI SM, it is still impossible to provide global gap-free daily soil moisture because of several physical limitations to measure soil moisture, as discussed below. Leaving these data gaps unfilled can perturb derived statistics such as anomalies or long-term trends and, in the worst case, lead to incorrect conclusions <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx72" id="paren.8"/>. Yet, observational datasets like ESA CCI SM are still valued in addition to gap-free reanalysis products because they can capture features that models might miss <xref ref-type="bibr" rid="bib1.bibx123" id="paren.9"/>. This creates a challenge as gap-free satellite data are often required, especially in various machine learning frameworks, such as those used for spatial downscaling <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx84" id="paren.10"/>, or for applications that require water balance closure <xref ref-type="bibr" rid="bib1.bibx32" id="paren.11"/>. In an attempt to fill these gaps, users unfamiliar with the underlying geophysical processes may resort to oversimplified approaches, such as filling missing values (“NaNs”) with zeros, which risks introducing further bias into the analysis. Understanding the underlying causes of data gaps in ESA CCI SM is therefore a prerequisite for filling them.</p>
      <p id="d2e193">As mentioned above, there are several reasons for data gaps in ESA CCI SM. Apart from missing satellite overpasses in earlier periods, data gaps originate from the underlying retrieval models to convert raw satellite measurements (radiances, backscatter) into soil moisture. These models become unreliable under certain surface conditions, leading to flagged/masked data points and, therefore, gaps in the final record. The most common cause are frozen soils <xref ref-type="bibr" rid="bib1.bibx124" id="paren.12"/>. Retrieval models are designed to estimate the amount of liquid water in the soil <xref ref-type="bibr" rid="bib1.bibx90 bib1.bibx128 bib1.bibx37" id="paren.13"/>. The dielectric properties of water change drastically between liquid and frozen aggregate state <xref ref-type="bibr" rid="bib1.bibx85" id="paren.14"/>. Consequently, measured soil moisture normally drops when part of the satellite footprint is frozen <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx33" id="paren.15"/>. The second-most-common cause for unreliable retrievals is dense vegetation, which can mask contributions from the soil. This issue is more pronounced at shorter wavelengths (K- and X-band), while L- and C-band measurements are less affected <xref ref-type="bibr" rid="bib1.bibx122 bib1.bibx59" id="paren.16"/>. Other reasons for failed retrievals include signal perturbation due to radio frequency interference (RFI), mainly for C- and L-band and overly densely populated areas <xref ref-type="bibr" rid="bib1.bibx119 bib1.bibx87" id="paren.17"/>, as well as barren, dry soils, where the received signal is noise-like and sometimes dominated by responses from sub-surface sediments <xref ref-type="bibr" rid="bib1.bibx130 bib1.bibx95" id="paren.18"/>.</p>
      <p id="d2e218">Data gaps can be broadly classified into two – not strictly separable – categories (based on <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx103 bib1.bibx31" id="altparen.19"/>): (i) (quasi-)random and (ii) systematic retrieval gaps. Random gaps appear noise-like over time and affect only short periods. They are not directly related to processes at the surface. Members of this category include cases where there is no satellite overpass for a given day, when the retrieval model does not converge for various reasons or when it converges at soil moisture values outside the physically possible boundaries, and RFI. Systematic gaps are related to the surface state and, therefore, usually cover longer periods. In the most extreme cases, systematic gaps can be permanent, meaning no data are available for a location (e.g. rainforests in ESA CCI SM). Systematic gaps are more likely to obscure spatial and/or temporal features in the data than random gaps. Gap-filling methods aim to restore these features as accurately as possible without introducing artificial (non-soil-moisture) patterns and without overfitting the data.</p>
      <p id="d2e224">There are generally two approaches to fill gaps in satellite soil moisture records: (i) univariate, stand-alone interpolation methods and (ii) multivariate, covariate-enhanced interpolation methods. The former uses only the available (neighbourhood) information to predict missing values with (geo)statistical methods, while the latter relies on supporting data to improve predictions. For soil moisture, most recent gap-filling studies focus on the applicability of different multivariate machine learning (ML) methods in small to medium-sized study regions. Random forest (RF) has been the dominant algorithm <xref ref-type="bibr" rid="bib1.bibx84 bib1.bibx72 bib1.bibx84 bib1.bibx133 bib1.bibx75 bib1.bibx8" id="paren.20"/> and was found to outperform other covariate supported approaches such as neural networks (NNs), XGBoost, support vector machines (SVMs), or multivariate linear regression <xref ref-type="bibr" rid="bib1.bibx69 bib1.bibx115 bib1.bibx117 bib1.bibx4" id="paren.21"/>. To predict missing soil moisture, these studies use physically related variables such as air or land surface temperature, precipitation, soil type, topography, land cover, and vegetation properties. While multivariate approaches can leverage additional datasets to improve predictions, univariate methods such as ordinary kriging (OK) or multiple linear regression (MLR) do not. However, they remain viable alternatives. In homogeneous areas, they have often been found to perform similarly to multivariate methods <xref ref-type="bibr" rid="bib1.bibx117 bib1.bibx115 bib1.bibx137" id="paren.22"/>.</p>
      <p id="d2e237">In this study, we adopt a univariate approach to fill gaps in ESA CCI SM. The choice of using a univariate method is motivated by the fact that it allows for being totally independent of any ancillary data and therefore mitigating the risk of introducing spurious features. The greatest possible independence of ancillary or model data is also one of the top priorities expressed by the climate user community <xref ref-type="bibr" rid="bib1.bibx31" id="paren.23"/>. Gap filling of ESA CCI SM is based on discrete cosine transform with penalized least squares (DCT-PLS) <xref ref-type="bibr" rid="bib1.bibx40" id="paren.24"/> because (i) even without the use of any ancillary data, it often performs similarly to multivariate methods such as XGBoost, LSTM, ANN, or CNN <xref ref-type="bibr" rid="bib1.bibx107 bib1.bibx137" id="paren.25"/>. (ii) It is considered a well-proven method that has been successfully applied to gap fill soil moisture <xref ref-type="bibr" rid="bib1.bibx131 bib1.bibx137" id="paren.26"/> and other geophysical variables such as land surface temperature (LST) <xref ref-type="bibr" rid="bib1.bibx68 bib1.bibx96" id="paren.27"/>, ocean surface current <xref ref-type="bibr" rid="bib1.bibx62" id="paren.28"/>, chlorophyll-<inline-formula><mml:math id="M5" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> concentration <xref ref-type="bibr" rid="bib1.bibx132" id="paren.29"/>, and lake surface water temperature <xref ref-type="bibr" rid="bib1.bibx38" id="paren.30"/> data.</p>
      <p id="d2e272">The multitude of gap-filling studies highlights the importance of this topic and the community's need for a gap-free ESA CCI SM data record. With the ESA CCI SM v09.1 GAPFILLED product, we aim to meet this community requirement by providing an independent, gap-filled, global, long-term, and satellite-based record. Consistently with other ESA CCI SM products, we also provide uncertainty estimates to quantify potential errors associated with the interpolation process – a feature which to our knowledge has not yet been included in any gap-filled satellite soil moisture record. This will allow users to account for the expected accuracy of our predictions and, for example, weigh them accordingly in their analyses.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>ESA CCI SM</title>
      <p id="d2e290">ESA CCI SM is a multi-satellite climate data record of daily global surface soil moisture. The latest release, v09.1, covers the period from 1 November 1978 to 31 December 2023 <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx47 bib1.bibx98 bib1.bibx34" id="paren.31"/>. The COMBINED product merges soil moisture derived from radiometer measurements in the L-, C-, X-, and K-bands by the Land Parameter Retrieval Model (LPRM) <xref ref-type="bibr" rid="bib1.bibx90 bib1.bibx120 bib1.bibx121 bib1.bibx122" id="paren.32"/> and from C-band scatterometer observations using the TU Wien change detection method <xref ref-type="bibr" rid="bib1.bibx50 bib1.bibx128 bib1.bibx129 bib1.bibx51" id="paren.33"/>. A timeline of all used satellite sensors and frequency bands is shown in Fig. <xref ref-type="fig" rid="F1"/>a. Soil moisture values are provided in volumetric units (m<sup>3</sup> m<sup>−3</sup>). ESA CCI SM data include quality flags, which are applied to mask unreliable data points and inform users about the underlying cause. Currently, there are quality flags for (i) frozen soils, (ii) dense vegetation, (iii) unsuccessful retrievals in all sensors, (iv) low signal-to-noise ratio in all sensors, and (v) barren ground <xref ref-type="bibr" rid="bib1.bibx124 bib1.bibx91" id="paren.34"/>. While flags (i)–(iv) coincide with missing data points in ESA CCI SM, flag (v) only tags the observations but does not remove them. ESA CCI SM data come with associated estimates of measurement uncertainties <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx47" id="paren.35"/>. These uncertainties are propagated from sensor-level estimates through triple collocation analysis on a day-of-year basis <xref ref-type="bibr" rid="bib1.bibx112" id="paren.36"/>. ESA CCI SM represents moisture in the upper soil layer (<inline-formula><mml:math id="M8" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 0–5 cm) with a regular spatial sampling of 0.25° (<inline-formula><mml:math id="M9" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 25 km). The algorithm is regularly updated with new data from available sensors to incorporate the latest scientific advances and extend the product's temporal coverage. This study aims to fill data gaps in the period from 1 January 1991 onward, chosen to make the data suitable for long-term (multi-decadal) studies <xref ref-type="bibr" rid="bib1.bibx41" id="paren.37"/>. From 1978 to 1991, no overlapping sensors were available (Fig. <xref ref-type="fig" rid="F1"/>a), resulting in very low data coverage (Fig. <xref ref-type="fig" rid="F1"/>b) and high measurement uncertainties <xref ref-type="bibr" rid="bib1.bibx31" id="paren.38"/>. As this would lead to even higher uncertainties after gap filling, this period is excluded.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e362">Availability of satellites and sensor frequency bands over time as of ESA CCI SM v09.1 <bold>(a)</bold> and data coverage over time of the merged COMBINED product averaged by latitude <bold>(b)</bold>.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Model and reanalysis data</title>
      <p id="d2e385">We use daily mean top-layer (0–7 cm) soil temperature from ERA5 at a 0.25° resolution <xref ref-type="bibr" rid="bib1.bibx54" id="paren.39"/>. In our study, these data are used to classify which gaps occurred during periods of frozen soils and which did not and to subsequently choose one of two different interpolation approaches. ERA5 is a global reanalysis product that integrates in situ and satellite observations into an open-loop run of the HTESSEL land surface model, producing hourly, gap-free estimates of various surface variables since 1940.</p>
      <p id="d2e391">We further use ERA5-Land top-layer (0–7 cm) soil moisture from 1991 to 2023 for a comparison of zonal anomalies and long-term trends after gap filling <xref ref-type="bibr" rid="bib1.bibx83" id="paren.40"/>. ERA5-Land has been produced by replaying the land component of ERA5 and provides surface variables with an increased spatial resolution (0.1°).</p>
      <p id="d2e397">Additionally, as reference data to assess the impact of gap distribution and size on interpolation quality, we use daily averages of gap-free soil moisture simulations for the 0–10 cm layer (given in kg m<sup>−2</sup>) from the GLDAS Noah v2.1 model <xref ref-type="bibr" rid="bib1.bibx101" id="paren.41"/>. The original data are available at a 3 h temporal sampling and 0.25° spatial resolution for the period after 2000. Notably, GLDAS Noah surface soil moisture serves as the scaling reference for the ESA CCI SM COMBINED product <xref ref-type="bibr" rid="bib1.bibx31" id="paren.42"/>. Hence, there is no bias between the two.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Vegetation optical depth</title>
      <p id="d2e426">We utilize vegetation optical depth (VOD) from the VODCA v2 CXKu dataset <xref ref-type="bibr" rid="bib1.bibx146 bib1.bibx79" id="paren.43"/> to predict the uncertainty in gap-filled values under different vegetation conditions. VOD is a satellite-derived, unitless measure of vegetation density closely related to vegetation water content and biomass. VODCA v2 CXKu harmonizes and merges VOD retrievals from nine passive sensors operating in the 6.8–19.4 GHz frequency range, creating a consistent long-term record from 1987 to 2023.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>In situ measurements</title>
      <p id="d2e440">The International Soil Moisture Network (ISMN) is a data hosting facility that collaborates with partners worldwide to collect in situ measurements of soil moisture and other geophysical variables into a harmonized, quality-controlled database <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx30 bib1.bibx36" id="paren.44"/>. ISMN in situ measurements serves as the primary source of ground reference data for global satellite soil moisture validation activities. An overview is provided by <xref ref-type="bibr" rid="bib1.bibx33" id="text.45"/>. In our study, we use ISMN data to evaluate the quality of our gap-filled soil moisture product. We use a subset of the full ISMN database for the 0–10 cm depth range, downloaded in March 2024. Specifically, we use a subset of the available data labelled as fiducial reference measurements (FRMs), which are point measurements found to be representative of soil moisture at the radiometer scale and therefore recommended for satellite validation <xref ref-type="bibr" rid="bib1.bibx55 bib1.bibx44" id="paren.46"/>. This subset consists of 1314 high-quality time series (Fig. <xref ref-type="fig" rid="FA3"/> in the Appendix). Soil moisture measurements are provided with associated quality flags for each time stamp and station metadata, such as land cover information extracted from ESA's CCI land cover v1.6.1 dataset. ISMN measurements are unevenly distributed both temporally (with different stations covering different periods) and geographically. This uneven distribution means that our validation results are spatially and temporally biased towards regions and periods with dense station coverage, primarily North America and Europe after the year 2000 <xref ref-type="bibr" rid="bib1.bibx33" id="paren.47"/>.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Preprocessing</title>
      <p id="d2e466">The following steps are applied to the original ESA CCI SM v09.1 COMBINED data before the interpolation process takes place.</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Additional retrievals under dense vegetation conditions</title>
      <p id="d2e476">Soil moisture values in areas covered by tropical rainforests are associated with high uncertainties <xref ref-type="bibr" rid="bib1.bibx118" id="paren.48"/>. Consequently, these areas are masked out in ESA CCI SM, leading to permanent gaps <xref ref-type="bibr" rid="bib1.bibx31" id="paren.49"/>. Such large gaps are particularly difficult to fill for any algorithm, regardless of whether covariates are used or not <xref ref-type="bibr" rid="bib1.bibx117" id="paren.50"/>. However, soil moisture is still retrieved, e.g. from deforested patches, and therefore available for some frequency bands in which electromagnetic waves can – at least to some degree – penetrate through vegetation. Specifically, C-band data from ASCAT-A, B, and C, as well as L-band data from SMOS and SMAP – despite the overall lower data quality compared to other global regions – can serve as useful support points for the interpolation algorithm when available. Hence, these lower-quality observations, despite being masked out in the original ESA CCI v9.1 COMBINED data, are included now in the gap filling to serve as anchor points (compare Fig. <xref ref-type="fig" rid="F2"/>e). This is preferred over large-scale interpolation without any support data <xref ref-type="bibr" rid="bib1.bibx49" id="paren.51"/>.</p>
      <p id="d2e493">Similar to the rest of the ESA CCI SM data, the additional retrievals available for densely vegetated areas are error-characterized via triple collocation analysis, harmonized through scaling to a common reference, and merged when more than one measurement is available for a grid point on a given day <xref ref-type="bibr" rid="bib1.bibx70 bib1.bibx31 bib1.bibx46 bib1.bibx47" id="paren.52"/>.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Gap analysis</title>
      <p id="d2e507">The observation density of ESA CCI SM depends on the number of available satellites and surface conditions that affect retrieval success rates. Figure <xref ref-type="fig" rid="F1"/>b shows the temporal coverage of the product. At the start of the data record, data from only few sensors were available, leading to relatively low data coverage. After 2002, coverage increases significantly, culminating in up-to-daily (i.e. gap-free) measurements for certain latitude bands in recent years. However, some regions still show large data gaps (Fig. <xref ref-type="fig" rid="F2"/>e), especially around the Equator and above 50° N, due to the dense vegetation cover and seasonally frozen soils, respectively.</p>
      <p id="d2e514">Figure <xref ref-type="fig" rid="F2"/>a–d evaluate data gaps in ESA CCI SM in terms of their 3-dimensional (Euclidean) distance from the nearest available valid data point. Gaps are analysed separately depending on whether the corresponding reanalysis soil temperature is above or below 0 °C. While in most cases a valid observation is found within a range of a few pixels or days, in some exceptional cases, the combined gap size in days and pixels can reach up to 350.</p>
      <p id="d2e519">The so derived distances are required for the initial guess for gap filling (nearest neighbour), which is then further adjusted by the DCT-PLS. They are also essential for deriving uncertainty estimates.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e525">Distance to the nearest neighbour for each missing data point (excluding Greenland) in ESA CCI SM along each dimension: time <bold>(a)</bold>, longitude <bold>(b)</bold>, latitude <bold>(c)</bold>, and Euclidean distance across dimensions <bold>(d)</bold>. Very large gaps (40–350 days/pixels) exist but are too rare to be visible in the histograms. The temporal coverage for each grid point with additional anchor observations over tropical rainforests is shown in <bold>(e)</bold>. Gap classification (frozen vs. non-frozen) based on ERA5 soil temperature.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f02.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Gap-filling methods</title>
      <p id="d2e558">To fill data gaps between observations in ESA CCI SM and assign uncertainty estimates to the predicted values, we follow the processing chain in Fig. <xref ref-type="fig" rid="F3"/>. We start from daily ESA CCI SM data with additional observations in the tropics (Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/>). We then compute the gap statistics (Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>) required for all subsequent steps: (i) for each gap, we compute the distance to the nearest observation (across 3 dimensions), and (ii) we differentiate between gaps due to frozen soils and other reasons based on (gap-free) ERA5 temperature information. We then fill data gaps in ESA CCI SM by applying the DCT-PLS algorithm with local parameterization (Sect. <xref ref-type="sec" rid="Ch1.S4.SS1"/>) but overwrite the so-derived values with a linear interpolation over time in periods where soil moisture is frozen in a certain place (discussed in Sect. <xref ref-type="sec" rid="Ch1.S4.SS1.SSS1"/>). Prediction uncertainty models are derived based on the performance of our method in restoring GLDAS Noah soil moisture data after introducing gaps from ESA CCI SM (Sect. <xref ref-type="sec" rid="Ch1.S5"/>). Finally, the gap-filled soil moisture and uncertainty estimates from gap statistics and pre-computed models are combined in the final GAPFILLED product.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e576">Flow chart of the main process steps to derive the ESA CCI SM GAPFILLED product (blue box). Dashed lines indicate optional processing steps that – once the model parameters are known – can be left out.</p></caption>
        <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f03.png"/>

      </fig>

<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Core algorithm: DCT-PLS</title>
      <p id="d2e592">We only provide a summary of the DCT-PLS algorithm here. For the full description with all intermediate steps, see <xref ref-type="bibr" rid="bib1.bibx40" id="text.53"/>. Initially designed as a data smoother, DCT-PLS can also provide estimates for missing data points by predicting a set of smoothed values <inline-formula><mml:math id="M11" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> for the original/input data <inline-formula><mml:math id="M12" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>. The algorithm optimizes for (i) minimal residual sum of squares (RSS) between the input and smoothed observations and (ii) optimal reduced roughness <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> between (smoothed) elements (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>). DCT-PLS therefore ideally removes noise in the data while retaining relevant information, i.e. finding smoothed versions of input observations <inline-formula><mml:math id="M14" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> so that <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is minimized.

            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M16" display="block"><mml:mrow><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi mathvariant="normal">RSS</mml:mi><mml:mo>+</mml:mo><mml:mi>s</mml:mi><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>‖</mml:mo><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>‖</mml:mo><mml:mo>+</mml:mo><mml:mi>s</mml:mi><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e726">The penalty term  <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is based on (temporal and spatial) neighbourhood information as differences (<inline-formula><mml:math id="M18" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>) between elements of <inline-formula><mml:math id="M19" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula>, thus optimizing for smoothed transitions between them (Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>).

            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M20" display="block"><mml:mrow><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>‖</mml:mo><mml:mi>D</mml:mi><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:msup><mml:mo>‖</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e797">Solving the linear system (Eq. <xref ref-type="disp-formula" rid="Ch1.E3"/>, where <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> indicates the identity matrix) to minimize <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mi>F</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is a computationally extensive task when <inline-formula><mml:math id="M23" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> is large.

            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M24" display="block"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>I</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi>s</mml:mi><mml:msup><mml:mi>D</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mi>D</mml:mi><mml:mo>)</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e871"><xref ref-type="bibr" rid="bib1.bibx40" id="text.54"/> provides a step-by-step description of the required (matrix) operations to find <inline-formula><mml:math id="M25" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> and discusses modifications to the base algorithm for improved performance. In particular, computing <inline-formula><mml:math id="M26" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> and performing eigenvalue (<inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula>) decomposition thereof is greatly simplified by the use of equally spaced input data such as ESA CCI SM. In fact, a predefined formulation for <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of <inline-formula><mml:math id="M29" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> can be used (Eq. <xref ref-type="disp-formula" rid="Ch1.E4"/>) where <inline-formula><mml:math id="M30" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> are the values along the dimension and <inline-formula><mml:math id="M31" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> the value count.

            <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M32" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mi mathvariant="italic">π</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>n</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e989">In the 3-dimensional case (<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>; time, latitude, longitude), this leads to tensor <inline-formula><mml:math id="M34" display="inline"><mml:mi mathvariant="normal">Λ</mml:mi></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E5"/>).

            <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M35" display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="normal">Λ</mml:mi><mml:mrow><mml:msub><mml:mi>i</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:msub><mml:mi>i</mml:mi><mml:mi>N</mml:mi></mml:msub></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mrow><mml:msub><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1061">Together with a realization of the smoothing parameter <inline-formula><mml:math id="M36" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>, we can define the tensor <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Γ</mml:mi><mml:mi>N</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E6"/>; <inline-formula><mml:math id="M38" display="inline"><mml:mo>÷</mml:mo></mml:math></inline-formula> and <inline-formula><mml:math id="M39" display="inline"><mml:mo>∘</mml:mo></mml:math></inline-formula> symbolize the element-by-element division and multiplication).

            <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M40" display="block"><mml:mrow><mml:msup><mml:mi mathvariant="normal">Γ</mml:mi><mml:mi>N</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:msup><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:msup><mml:mo>÷</mml:mo><mml:mo>(</mml:mo><mml:msup><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:msup><mml:mo>+</mml:mo><mml:mi>s</mml:mi><mml:msup><mml:mi mathvariant="normal">Λ</mml:mi><mml:mi>N</mml:mi></mml:msup><mml:mo>∘</mml:mo><mml:msup><mml:mi mathvariant="normal">Λ</mml:mi><mml:mi>N</mml:mi></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1144">This allows us to efficiently solve for <inline-formula><mml:math id="M41" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> using the discrete cosine transform matrix (DCTN) of <inline-formula><mml:math id="M42" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> and the inverse form (IDCTN) for data with the dimension <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>, respectively <xref ref-type="bibr" rid="bib1.bibx113" id="paren.55"/>. As data gaps are present in ESA CCI SM, assigning weights (<inline-formula><mml:math id="M44" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula>) to observations is required (Eq. <xref ref-type="disp-formula" rid="Ch1.E7"/>). Data gaps are assigned a weight of zero and therefore interpolated as part of the (robust) smoothing process, while observations have an initial weight of 1. <inline-formula><mml:math id="M45" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> here refers to one realization of <inline-formula><mml:math id="M46" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> because this step is repeated multiple times when optimizing <inline-formula><mml:math id="M47" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>, as explained later.

            <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M48" display="block"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">IDCTN</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi mathvariant="normal">Γ</mml:mi><mml:mi>N</mml:mi></mml:msup><mml:mo>∘</mml:mo><mml:mi mathvariant="normal">DCTN</mml:mi><mml:mo>(</mml:mo><mml:mi>W</mml:mi><mml:mo>∘</mml:mo><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1281">Finally, having an estimate for <inline-formula><mml:math id="M49" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula>, the generalized cross-validation (GCV) score is computed (Eq. <xref ref-type="disp-formula" rid="Ch1.E8"/>), where <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">miss</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the number of missing values of <inline-formula><mml:math id="M51" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> overall samples.

            <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M52" display="block"><mml:mtable class="split" rowspacing="5.690551pt" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">GCV</mml:mi><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">wRSS</mml:mi><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">miss</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>T</mml:mi><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi>H</mml:mi><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mi>n</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>‖</mml:mo><mml:msup><mml:mi>W</mml:mi><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mo>‖</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">miss</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>T</mml:mi><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi>H</mml:mi><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mi>n</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

          <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi>H</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is computed from <inline-formula><mml:math id="M54" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E4"/>) as described in Eq. (<xref ref-type="disp-formula" rid="Ch1.E9"/>).

            <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M55" display="block"><mml:mrow><mml:mi>T</mml:mi><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi>H</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>s</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mi mathvariant="italic">π</mml:mi><mml:mo>/</mml:mo><mml:mi>n</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mo>]</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1573">A bounded minimization – as implemented in SciPy's “optimize” module <xref ref-type="bibr" rid="bib1.bibx125" id="paren.56"/> – is now applied to find the smoothing parameter <inline-formula><mml:math id="M56" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> for minimal GCV, and <inline-formula><mml:math id="M57" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula> is computed again using this <inline-formula><mml:math id="M58" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M59" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> is the only free parameter in the model that needs to be tuned using GCV.</p>
      <p id="d2e1610">As outliers can be present in ESA CCI SM data, we use the “robust” implementation of DCT-PLS <xref ref-type="bibr" rid="bib1.bibx40" id="paren.57"/>, which includes further iterations of the above described process to detect outliers in the data and gradually reduce weights assigned to these observations until the optimization converges at <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mrow><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>k</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, meaning that no more relevant changes between <inline-formula><mml:math id="M61" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M62" display="inline"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula> – before and after calibrating <inline-formula><mml:math id="M63" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>, respectively – are found.</p>
      <p id="d2e1674">DCT-PLS can take <inline-formula><mml:math id="M64" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>-dimensional tensors of any size. We apply it to (3-dimensional) spatial subsets of the dataset via a <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mn mathvariant="normal">15</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula>° moving window. We prefer a moving window over a global <inline-formula><mml:math id="M66" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> value to locally allow for different degrees of smoothing and therefore reducing potential overfitting or over-smoothing when using a global <inline-formula><mml:math id="M67" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> value <xref ref-type="bibr" rid="bib1.bibx131" id="paren.58"/>. Therefore, local parameterization of <inline-formula><mml:math id="M68" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> is also expected to improve the interpolation results between areas with different levels of autocorrelation. In most cases, the chosen window is large enough to provide sufficient data for a robust estimation. However, for some edge cases, such as remote islands, the initial window size is gradually extended by 5° (in eight directions, in practice, the maximum was 35°) until the GCV minimization process has sufficient data to converge for <inline-formula><mml:math id="M69" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>.</p>
      <p id="d2e1728">Predictions are made not only for missing data points, but also at locations where observations are available. While these (smoothed) observations are not used in the final gap-filled product (because the original observations are kept when available), they can be used to further harmonize predictions and observations before they are combined (see Sect. <xref ref-type="sec" rid="Ch1.S4.SS1.SSS2"/>).</p>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>Frozen soils</title>
      <p id="d2e1740">During periods of frozen soil moisture, it is a matter of definition whether a dataset should represent only the liquid or the total (frozen and non-frozen) soil moisture content. In the first case, soil moisture would start to decline as soon as water begins to freeze in a scene until it reached <inline-formula><mml:math id="M70" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0 m<sup>3</sup> m<sup>−3</sup>. Factors such as freezing point depression due to solutes can result in the presence of liquid soil moisture even when the soil temperature is below 0 °C <xref ref-type="bibr" rid="bib1.bibx5" id="paren.59"/>. In the second case, which we try to cover in our data record, soil moisture remains constant over the period when it is frozen; i.e. there is no soil water loss due to evaporation of percolation. However, when predicted observations are based on insufficiently-masked, low, and often noisy soil moisture observations from transitional zones/periods around a frozen soil gap, these are often too low <xref ref-type="bibr" rid="bib1.bibx131 bib1.bibx69" id="paren.60"/>. In addition, since DCT-PLS does not use any information on soil temperature, it may predict temporal fluctuations in soil moisture even when the soil is frozen. One could argue that this is the result of regional (sub-pixel) freeze/thaw processes, but there is no reason to assume that univariate algorithms, which do not account for soil temperature on a sub-pixel scale, can accurately predict this.</p>
      <p id="d2e1777">We therefore carry the last (observed or interpolated) soil moisture level before freezing starts forward over time until thawing occurs and soil moisture changes can be measured again directly by the satellite. In practice, there can be differences between the last and first available observations around a period of frozen soil, e.g. due to measurement noise. We therefore use the mean of 30 d before and after an affected period to perform a simple linear interpolation over time between these points. This is in line with our definition of frozen soil moisture content, deals with the expected noise in observations around the affected period, and avoids temporal fluctuations in predictions when soil moisture should remain stable. These values are then used to replace those from the DCT-PLS algorithm.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>Combining predictions and observations</title>
      <p id="d2e1788">For the final GAPFILLED product, we use the predictions (from either DCT-PLS or linear interpolation) to fill data gaps in the original record. The available original observations are not replaced. However, since DCT-PLS uses temporal and spatial neighbourhood information to create predictions, the mean and variance of the predictions for a grid point are adjusted towards those of its neighbours, giving the data a (spatially) smooth appearance. This characteristic, typical of any spatial interpolation method <xref ref-type="bibr" rid="bib1.bibx73" id="paren.61"/>, can lead to temporal inconsistencies between predictions and observations. To address this, we apply a linear transformation (derived from linear regression on shared data points) to scale the mean and variance of the predictions to match those of the observations <xref ref-type="bibr" rid="bib1.bibx111 bib1.bibx93" id="paren.62"/>. Finally, the scaled predictions are used to fill gaps in the observation time series.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Validation</title>
      <p id="d2e1808">The gap-filled ESA CCI SM product is compared to ISMN in situ reference measurements using the QA4SM online validation platform (<uri>https://qa4sm.eu</uri>, last access: 20 August 2025). Time series for grid points collocated with FRMs (see Appendix Fig. <xref ref-type="fig" rid="FA3"/>) are extracted from the original ESA CCI SM COMBINED and the GAPFILLED product. For the latter, we extracted four different subsets: (i) all available data points from the GAPFILLED product (original observations plus filled values), (ii) only the filled values, (iii) only the filled values from “small” gaps (classification based on the Euclidean distance (ED) to the nearest observation) with <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi mathvariant="normal">ED</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> (i.e. adjacent to a valid data point in any dimension), and (iv) only the filled values within “medium/large” gaps (<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi mathvariant="normal">ED</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>). All four datasets were uploaded to the service. We select a temporal matching window of <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> h around 00:00 UTC to align in situ measurements with the satellite data (temporal reference). QA4SM offers filtering options to include only in situ time stamps flagged as “good” – excluding erroneous measurements from, for example, frozen soils <xref ref-type="bibr" rid="bib1.bibx30" id="paren.63"/> – and “(very) representative” time series in terms of FRM qualification. Biases between satellite and in situ time series are removed by matching their mean and standard deviation using the in situ data as the (scaling) reference <xref ref-type="bibr" rid="bib1.bibx48" id="paren.64"/>. QA4SM validation results include ESA CCI land cover information at the in situ sites, which we use to stratify our results.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Uncertainty estimation</title>
      <p id="d2e1867">An uncertainty estimate is provided for each interpolated value. This uncertainty depends on the uncertainty of the observations used (<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">observations</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the availability of support data and other inherent factors affecting the quality of DCT-PLS predictions (summarized as <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). Combining both as in Eq. (<xref ref-type="disp-formula" rid="Ch1.E10"/>) yields the uncertainty for our predictions.

          <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M78" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">prediction</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">observations</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:msqrt></mml:mrow></mml:math></disp-formula>

        <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">observations</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is characterized in ESA CCI SM using triple collocation analysis and uncertainty propagation <xref ref-type="bibr" rid="bib1.bibx45" id="paren.65"/>. The random error level of observations mainly depends on the merged sensor frequency bands in conjunction with surface characteristics, such as vegetation cover <xref ref-type="bibr" rid="bib1.bibx91" id="paren.66"/>. Recently, a temporal component was added to account for (sub)seasonal error dynamics <xref ref-type="bibr" rid="bib1.bibx112" id="paren.67"/>. We use <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">observations</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as the baseline for uncertainties in the gap-filled values. For a conservative estimate, we choose the 95th percentile of measurement uncertainties for any grid point series (or the nearest-neighbour series in the case of a permanent gap).</p>
      <p id="d2e1957">To estimate <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, we impose the gaps in the satellite data on gap-free GLDAS Noah soil moisture and subsequently restore these gaps using the presented methodology (Fig. <xref ref-type="fig" rid="F3"/>). This approach preserves the original satellite gap systematics as opposed to randomly splitting the input data into training and validation sets, as is commonly done (e.g. <xref ref-type="bibr" rid="bib1.bibx131 bib1.bibx71 bib1.bibx143" id="altparen.68"/>). The goal of this analysis is to derive a set of model functions for the expected discrepancy between predictions and observations based on the gap size. Uncertainty models are preferred over empirical values because they remain applicable even in scenarios where GLDAS data are unavailable, ensuring broader utility of the methodology (e.g. for the period before 2000, when GLDAS Noah v2.1 data are not available). For improved accuracy, these functions should account for both realistic gap conditions and varying surface complexities. To address the former, we use the previously computed gap statistics (Euclidean distances). To address the latter, we use a static VOD classification map for low, medium, and high VOD based on the 2000–2023 average, derived from the VODCA v2 CXKu archive (compare Fig. <xref ref-type="fig" rid="FA1"/> in the Appendix). We therefore assume that prediction uncertainty will generally increase for larger gaps and with denser vegetation cover, consistent with the observations <xref ref-type="bibr" rid="bib1.bibx91" id="paren.69"/>.</p>
      <p id="d2e1981">From analysing the differences between original and restored values with regard to the gap systematics and VOD level (compare Fig. <xref ref-type="fig" rid="F4"/>a), a log-like function of form <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>b</mml:mi><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is fitted for different vegetation conditions. Each <inline-formula><mml:math id="M83" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M84" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is found from fitting 1000 realizations of this function (least squares with boundary conditions for <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>a</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>) to randomly drawn samples without replacement. Using the medians of the obtained parameter sets for <inline-formula><mml:math id="M87" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M88" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> (Table <xref ref-type="table" rid="T1"/>), we defined the required models for the uncertainty of the gap-filling process (<inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) itself as shown in Fig. <xref ref-type="fig" rid="F4"/>b.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e2096">Absolute differences between original and restored GLDAS Noah soil moisture after gap filling <bold>(a)</bold> and function fits <bold>(b)</bold> (median and standard deviation from 1000 randomly drawn samples) to predict <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for high, medium, and low VOD conditions.</p></caption>
        <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f04.png"/>

      </fig>

<table-wrap id="T1"><label>Table 1</label><caption><p id="d2e2125">Model parameters found from fitting <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for different VOD levels (VOD classification in Fig. <xref ref-type="fig" rid="FA1"/> in the Appendix).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>b</mml:mi><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M93" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M94" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">high VOD</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M95" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.089</oasis:entry>
         <oasis:entry colname="col3">0.128</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">medium VOD</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M96" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.218</oasis:entry>
         <oasis:entry colname="col3">0.08</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">low VOD</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M97" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.234</oasis:entry>
         <oasis:entry colname="col3">0.035</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S6">
  <label>6</label><title>Results</title>
<sec id="Ch1.S6.SS1">
  <label>6.1</label><title>DCT-PLS parameterization</title>
      <p id="d2e2289">Figure <xref ref-type="fig" rid="F5"/> shows the result of the local parameterization of the DCT-PLS model. A lower <inline-formula><mml:math id="M98" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> means that more (day-to-day temporal and/or regional spatial) variability is found in the prediction (Fig. <xref ref-type="fig" rid="F5"/>a). The highest <inline-formula><mml:math id="M99" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> values are found in arid climates, in northeast Africa and Arabia. This coincides with the expected low variability in soil moisture in these regions. Low <inline-formula><mml:math id="M100" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> values (i.e. high variability) are found in subtropical regions in central Africa and South America, South Asia, and East Australia. The GCV scores in Fig. <xref ref-type="fig" rid="F5"/>b were minimized to find the optimal <inline-formula><mml:math id="M101" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> in each cell. For most regions, the GCV score is close to zero, which indicates a good fit. Higher scores are found in subtropical regions, which indicates a slightly larger discrepancy between the predictions and available observations in these areas. This could be due to underestimating the seasonal and/or overfitting of the day-to-day soil moisture variability in the measurements.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e2329">Local parameterization of the DCT-PLS function to find the optimal value for <inline-formula><mml:math id="M102" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> <bold>(a)</bold> that minimizes the GCV score <bold>(b)</bold>.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f05.png"/>

        </fig>

</sec>
<sec id="Ch1.S6.SS2">
  <label>6.2</label><title>Spatial data characteristics</title>
      <p id="d2e2359">The GAPFILLED product provides full daily coverage for both soil moisture and uncertainty estimates. For a selected day, Fig. <xref ref-type="fig" rid="F6"/> shows both fields before and after gap filling, respectively. The gap filling has produced a smooth, spatially consistent image without any outlier values or edges that could arise from sudden differences in regional parameterization of the DCT-PLS model. As expected, soil moisture in tropical latitudes is high as a result of interpolating anchor retrievals from L- and C-band measurements within and surrounding these areas. In high northern latitudes, the predictions come mainly from linear time interpolation between autumn values of the preceding year and spring values observed later in the year.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e2366">Soil moisture and uncertainty before <bold>(a, b)</bold> and after <bold>(c, d)</bold> gap filling on 1 March 2007. Ice sheets (Greenland, Antarctica) are excluded from the GAPFILLED product. Hatched regions indicate ERA5 soil temperature below 0 °C.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f06.png"/>

        </fig>

      <p id="d2e2381">The uncertainties are within the range of 0 to 0.1 m<sup>3</sup> m<sup>−3</sup>, which is expected from the defined models for <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the value range of the original (triple collocation) error estimates <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">observations</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx45 bib1.bibx47" id="paren.70"/>. The highest values are found in (sub)tropical and boreal ecozones, the Tibetan Plateau, and southeast Asia. This is due to the low data coverage and quality of the used retrievals in these regions, which are noisy for dense vegetation and often missing in mountainous regions.</p>
      <p id="d2e2431">While uncertainties increase as expected in most regions covered by dense vegetation, an inverse effect appears in some areas of the northwestern Amazon and the central African rainforest (Fig. <xref ref-type="fig" rid="FA2"/> in the Appendix), where the uncertainties of the GAPFILLED product are lower than in parts of the surrounding subtropical zones. Our analysis of this phenomenon shows that – although uncertainties in the GAPFILLED product increase according to <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> – the initial uncertainty estimates based on triple collocation analysis <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">observations</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in the affected regions are too low (Fig. <xref ref-type="fig" rid="FA2"/>a). This likely results from the poor agreement between satellite and model data in these areas, whereas similar soil moisture climatologies are found in the (independent) active and passive satellite products (Fig. <xref ref-type="fig" rid="FA2"/>d).</p>
<sec id="Ch1.S6.SS2.SSS1">
  <label>6.2.1</label><title>Time series characteristics</title>
      <p id="d2e2469">Figure <xref ref-type="fig" rid="F7"/> shows temporal subsets for five grid points in the Northern Hemisphere, where also in situ measurements are available. The locations were selected to represent a wide range of environments and gap types as far as the spatial distribution of in situ sensors allows (for more information on the chosen sites, see Table <xref ref-type="table" rid="TA1"/> in the Appendix). For visualization purposes, a linear least-squares regression scaling was applied to remove biases between point- and satellite-scale time series <xref ref-type="bibr" rid="bib1.bibx111 bib1.bibx93" id="paren.71"/>. Anomalies are computed relative to the 1991–2023 average conditions. All <inline-formula><mml:math id="M109" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> scores are based only on data points from the visualized period and are statistically significant (<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). Figure <xref ref-type="fig" rid="F7"/>a illustrates the performance of the gap-filling algorithm in predicting soil moisture for gaps because of frozen conditions and gaps emerging for other reasons in an area with a moderate number of missing data points (40 %). The predicted values align reasonably well with the available in situ data, with an anomaly correlation of 0.59 between the in situ measurements and the filled values only (<inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">FILLED</mml:mi><mml:mspace width="0.33em" linebreak="nobreak"/><mml:mi mathvariant="normal">VALUES</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, without the original observations). This is lower than the 0.70 correlation between in situ measurements and original satellite observation anomalies. However, this is hardly surprising, as systematic gaps appear during more challenging conditions. This plot also shows how combining data from both the DCT-PLS and linear interpolation in a single time series based on soil temperature can lead to inconsistencies for some edge cases (February 2018). In this case, an individual, unobserved “non-frozen” data point is found in the middle of a prolonged frozen period. Differences in the predictions of the two interpolation algorithms can lead to outliers in this case. Figure <xref ref-type="fig" rid="F7"/>b is an example of a location affected strongly by seasonally missing data. The periods of linear interpolation (frozen) align well with missing in situ values due to the (independent) quality-flag-based masking based on in situ temperature measurements <xref ref-type="bibr" rid="bib1.bibx33" id="paren.72"/>. The reanalysis temperature data below 0 °C therefore, for this location, provides a good approximation of the period when soil moisture is frozen and kept at an almost constant level. However, it also means that a direct comparison between gap-filled values and in situ measurements is usually not possible during winter. For the onset and termination of this period, the absolute values between gap-filled and in situ data match well. Figure <xref ref-type="fig" rid="F7"/>c represents a location with only few missing data points and no relevant periods of frozen soil moisture. In this case, we find a higher correlation with the in situ data for the gap-filled values compared to the original data (0.89 vs. 0.80), which we attribute to the smoothing effect of DCT-PLS and therefore reduced noise in the predictions. Figure <xref ref-type="fig" rid="F7"/>d is for a location near the Equator, where ESA CCI SM is normally permanently masked due to the presence of dense vegetation (i.e. 100 % filled values). The example time series shows how the additional C- and L-band retrievals in this region form a consistent although somewhat noisy record, which matches reasonably well with the in situ data (anomaly correlation of 0.54). Figure <xref ref-type="fig" rid="F7"/>e is located in a complex topography on the Tibetan Plateau, with significant amounts of missing data points due to soil freezing. The performance of ESA CCI SM is generally poor in this region and the gap-filled product shows only little variation and often contradicts the (sparse) in situ measurements. The available observations are very noisy in this location, and hence do not form a consistent time series with the gap-filled data points.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e2530">Selection of soil moisture anomaly time series from the original and gap-filled ESA CCI SM data set and available in situ measurements (relative to the 1991–2023 climatological average). The locations of <bold>(a)</bold>–<bold>(e)</bold> are indicated in <bold>(f)</bold>. All statistics are based only on data from the shown sub-periods. <inline-formula><mml:math id="M112" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> scores shown in bold are statistically significant (<inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and are based on the number of data points indicated in parentheses. For more information about the chosen locations, see Table <xref ref-type="table" rid="TA1"/> in the Appendix.</p></caption>
            <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f07.png"/>

          </fig>

</sec>
<sec id="Ch1.S6.SS2.SSS2">
  <label>6.2.2</label><title>Global anomalies and uncertainties</title>
      <p id="d2e2578">Global monthly anomalies and uncertainties over time are shown in Fig. <xref ref-type="fig" rid="F8"/>. The similarity in anomalies before (Fig. <xref ref-type="fig" rid="F8"/>a) and after (Fig. <xref ref-type="fig" rid="F8"/>c) gap filling indicates that large-scale deviations from normal conditions are equally well represented in the gap-filled as in the original data. The main differences (Fig. <xref ref-type="fig" rid="F8"/>e) are found in equatorial regions (mainly due to the additional observations used) and in transition zones/periods between frozen and unfrozen soil moisture.</p>
      <p id="d2e2589">Uncertainties are high at the start of the record, when data coverage is lowest (compare Fig. <xref ref-type="fig" rid="F8"/>b, d  to Fig. <xref ref-type="fig" rid="F1"/>b), and for equatorial latitudes due to reduced coverage and observation quality. Uncertainties in the gap-filled values often exceed 0.1 m<sup>3</sup> m<sup>−3</sup> in areas where ESA CCI SM measurements are seasonally masked due to frozen soils, and linear interpolation potentially does not sufficiently account for diurnal freeze–thaw processes, evaporation, and other factors. However, it is important to note that these higher uncertainties reflect the inclusion of additional data points rather than a decline in dataset quality.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e2619">Time-latitude diagrams of monthly soil moisture anomalies and soil moisture uncertainties as in the original COMBINED <bold>(a, b)</bold> and GAPFILLED <bold>(c, d)</bold> product. Differences between <bold>(a)</bold> and <bold>(c)</bold> are shown in <bold>(e)</bold>.</p></caption>
            <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f08.png"/>

          </fig>

</sec>
<sec id="Ch1.S6.SS2.SSS3">
  <label>6.2.3</label><title>Zonal anomalies and trends</title>
      <p id="d2e2651">Figure <xref ref-type="fig" rid="F9"/> shows annual anomalies expressed as <inline-formula><mml:math id="M116" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores <xref ref-type="bibr" rid="bib1.bibx127" id="paren.73"/> for different latitude bands of the original observation-only ESA CCI dataset, its gap-filled counterpart, and two reanalysis products. Gap filling can influence annual anomaly estimates, particularly when large portions of observational data are (systematically) masked. This effect is evident in the global estimates (Fig. <xref ref-type="fig" rid="F9"/>a), where the 1991–2023 trend shifts from negative to neutral after gap filling. The most significant discrepancies between the original and gap-filled ESA CCI SM data occur during the first third of the time series (1992–2002), a period with limited observation coverage compared to the era following the launch of AMSR-E in 2002. The gap-filled data are drier than the original and the reanalysis products. From 2002 to 2016, we find good agreement between all four datasets until the two CCI (and reanalysis) records start to diverge again, with gap-filled anomalies exceeding those of the original data. The extreme dry anomaly in the original dataset in 2019 is mitigated after gap filling, resulting in a closer alignment with reanalysis. During the last 4 years, CCI and GLDAS agree well, while ERA5-Land reached the lowest value on record in 2023. For the Southern Hemisphere (Fig. <xref ref-type="fig" rid="F9"/>b), we find only minor differences between the original and gap-filled data, mainly in the beginning and at the end of the time series. We attribute this partly to the good initial data coverage, but it also indicates that the integration of additional observations for the previously permanently masked tropical rainforest regions was successful. The gap-filled time series is now slightly less variable and closer to GLDAS Noah. The overall trend for the Southern Hemisphere has slightly changed, from neutral to negative, in line with the reanalysis products. Looking at <inline-formula><mml:math id="M117" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores for the tropical zone (Fig. <xref ref-type="fig" rid="F9"/>c) separately, we find a negative soil moisture trend after gap filling. This trend, as well as the annual anomalies in general, align better with the reanalysis products, compared to the original data. Some differences are found during the first 5 and the last 10 years, when gap filling has a better aligned CCI with GLDAS. Figure <xref ref-type="fig" rid="F9"/>d comprises the data from a wide range of climatic regions, from arid over temperate to boreal conditions. This subset contains the majority of points over land for the Northern Hemisphere (excluding Greenland). From 1991 to 2003 we find drier and from 2013 to 2020 wetter conditions after gap filling, which matches the observations from Fig. <xref ref-type="fig" rid="F9"/>a in the same period, where it had a similar effect on the long-term trend in the data. The largest discrepancies between the original and gap-filled data are found for the boreal zone (Fig. <xref ref-type="fig" rid="F9"/>e). The effect of the interpolation of seasonally missing values is clearly visible and has led to a switch from a slight negative to a strong positive trend, which is in contrast to ERA5-Land. However, it should be noted that the reliability of reanalyses in this case is also unknown. This is also evident from the discrepancies between GLDAS Noah and ERA5-Land in this zone.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e2688">Annual soil moisture anomaly <inline-formula><mml:math id="M118" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores across different latitude bands: <bold>(a)</bold> global, <bold>(b)</bold> Southern Hemisphere, <bold>(c)</bold> (sub)tropical zone, <bold>(d)</bold> arid/temperate zone, <bold>(e)</bold> boreal zone. The dotted coloured lines indicate the zonal trends in the original and gap-filled data.</p></caption>
            <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f09.png"/>

          </fig>

      <p id="d2e2720">We further assess global trend changes in Fig. <xref ref-type="fig" rid="F10"/>, showing Theil–Sen slopes computed from annual averages between 1991 and 2023, with a Mann–Kendall test for statistical significance <xref ref-type="bibr" rid="bib1.bibx29" id="paren.74"/>. Figure <xref ref-type="fig" rid="F10"/>a is for the original ESA CCI SM data (with gaps), and Fig. <xref ref-type="fig" rid="F10"/>b is the same for the gap-filled product. Figure <xref ref-type="fig" rid="F10"/>c summarizes the differences in terms of change in trend direction and significance. Only a very small number of initially detected significant trends changed their direction due to gap filling, either from positive to negative (1.5 %) or vice versa (1.4 %). Affected regions are in the northwest United States, Siberia, and Myanmar, where positive trends are found after gap filling, as well as central Africa and some spots in South America, where the trend direction was inverted to negative. More prominently, large parts of the Northern Hemisphere, where previously no significant increase in soil moisture was found, now show a positive trend. This is the case for large parts of Russia, Alaska, the northwest United States, and Canada. The opposite is often found in the Southern Hemisphere, mainly in central and western Africa and South America and also in northeast China and Mongolia. The previously masked regions covered by tropical rainforest do not show spatially consistent trends after gap filling. For parts of Brazil and Columbia in particular, trends vary spatially, while a consistent negative trend is found for the lower half of South America, which only changed in some spots in the far south due to gap filling.</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e2737">Significant (<inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) long-term (1991–2023) soil moisture trends before <bold>(a)</bold> and after <bold>(b)</bold> gap filling. Panel <bold>(c)</bold> shows the change in trend direction and significance: “<inline-formula><mml:math id="M120" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>” indicates wetting, “–” drying, and “0” non-significant trends before and after gap-filling, respectively. Inset numbers (%) are relative to the total number of points with a significant trend.</p></caption>
            <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f10.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S6.SS3">
  <label>6.3</label><title>Evaluation of <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></title>
      <p id="d2e2798">Figure <xref ref-type="fig" rid="F11"/> shows Pearson's <inline-formula><mml:math id="M122" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> (masked for <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and unbiased root mean squared difference (ubRMSD), between original daily soil moisture from GLDAS Noah and restored GLDAS Noah points for the imposed ESA CCI SM gaps. The gap-filling algorithm manages to restore the data well (global median <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.81</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mi mathvariant="normal">ubRMSD</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.69</mml:mn></mml:mrow></mml:math></inline-formula> kg m<sup>−2</sup>, corresponding to <inline-formula><mml:math id="M127" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 10 % relative error). When data from gaps classified as “frozen” (Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>) are excluded, i.e. without values filled by linear interpolation, performance metrics improve (global median <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.89</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mi mathvariant="normal">ubRMSD</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.24</mml:mn></mml:mrow></mml:math></inline-formula> kg m<sup>−2</sup>). By design, regions with a low <inline-formula><mml:math id="M131" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> and high ubRMSD in this analysis match with regions where our uncertainty models predict a lower gap-filling accuracy (Figs. <xref ref-type="fig" rid="F6"/>d, <xref ref-type="fig" rid="F8"/>d).</p>

      <fig id="F11" specific-use="star"><label>Figure 11</label><caption><p id="d2e2918">Agreement between original and restored GLDAS Noah surface soil moisture obtained after imposing data gaps from ESA CCI SM and subsequent filling. The top row is based on all restored data points, and the bottom row is with frozen periods excluded. Pearson's <inline-formula><mml:math id="M132" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> in <bold>(a)</bold> and <bold>(d)</bold> is masked if <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M134" display="inline"><mml:mo lspace="0mm">≈</mml:mo></mml:math></inline-formula> 3 % of all grid cells). ubRMSD is shown in <bold>(b)</bold> and <bold>(e)</bold>, and the respective sample sizes (i.e. number of gaps over time) over the period 2000–2023 are shown in <bold>(c)</bold> and <bold>(f)</bold>.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f11.png"/>

        </fig>

</sec>
<sec id="Ch1.S6.SS4">
  <label>6.4</label><title>GAPFILLED soil moisture validation with in situ data</title>
      <p id="d2e2980">Figure <xref ref-type="fig" rid="F12"/> shows aggregated performance metrics (<inline-formula><mml:math id="M135" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> and ubRMSD) between FRM in situ sites and the original ESA CCI SM COMBINED product, the new GAPFILLED product (original data with filled values), and the subset consisting only of the filled values. All three datasets generally perform on a similar level. In terms of absolute value correlations, the GAPFILLED product slightly outperforms the original data. Note, however, that the temporal and spatial coverage differs among the three products. Logically, there is no overlap in observations between the original and the filled values. Fill values typically comprise challenging cases, where satellite retrievals were not possible in the first place. Consequently, it is unsurprising that the performance of only the filled values slightly lags behind the original dataset in terms of absolute values <inline-formula><mml:math id="M136" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> (Fig. <xref ref-type="fig" rid="F12"/>a) and ubRMSD (Fig. <xref ref-type="fig" rid="F12"/>c), especially for stations near or under dense vegetation (“Tree Cover”). Metrics are slightly more spread for the filled values. A good performance of the GAPFILLED product is also found in terms of anomaly <inline-formula><mml:math id="M137" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> and ubRMSD, indicating that the gap-filling algorithm manages to capture not only the seasonality, but also short-term events on par with the observations (based on the same 1991–2023 reference period as in Sect. <xref ref-type="sec" rid="Ch1.S6.SS2.SSS1"/>). The station count for anomaly metrics can be lower than for absolute values as QA4SM excludes time series for which a reliable anomaly cannot be computed (e.g. due to insufficient temporal coverage).</p>

      <fig id="F12" specific-use="star"><label>Figure 12</label><caption><p id="d2e3015">Performance metrics between ISMN soil moisture time series and the “original” ESA CCI SM v09.1 COMBINED product, the GAPFILLED product, and the “filled values” of the GAPFILLED product only. Pearson's <inline-formula><mml:math id="M138" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) based on absolute values <bold>(a)</bold> and anomalies <bold>(b)</bold> and ubRMSD <bold>(c, d)</bold>, respectively. The numbers in each box indicate the count of contributing time series.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f12.png"/>

        </fig>

      <p id="d2e3052">In Fig. <xref ref-type="fig" rid="F13"/>, we assess the performance of the filled values separately in “small” and “medium/large” gaps with respect to the same in situ reference measurements. Figure <xref ref-type="fig" rid="F13"/>a shows that the temporal agreement between in situ and filled values decreases for larger gaps. However, it is less distinct in terms of ubRMSD (Fig. <xref ref-type="fig" rid="F13"/>b), which barely increases for larger gaps. Note, however, that there is a severe lack of reference data for the larger gaps, mainly due to the unavailability of in situ measurements during winter. Hence, it was not possible to evaluate “medium” and “large” gaps separately.</p>

      <fig id="F13"><label>Figure 13</label><caption><p id="d2e3064">Performance metrics between ISMN soil moisture and only the filled values in the GAPFILLED product, separated by their Euclidean distance (ED) to the nearest observation: small gaps (<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi mathvariant="normal">ED</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>) and medium/large gaps (<inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mi mathvariant="normal">ED</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>). The shown metrics are <bold>(a)</bold> Pearson's <inline-formula><mml:math id="M142" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> (only <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and <bold>(b)</bold> ubRMSD. Narrow boxes indicate the upper and lower boundary values of the 95 % confidence interval for each data point. The numbers in each box refer to the sample size (number of time series).</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f13.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S7">
  <label>7</label><title>Code and data availability</title>
      <p id="d2e3132">The ESA CCI SM v09.1 GAPFILLED dataset is available at <ext-link xlink:href="https://doi.org/10.48436/hcm6n-t4m35" ext-link-type="DOI">10.48436/hcm6n-t4m35</ext-link> <xref ref-type="bibr" rid="bib1.bibx99" id="paren.75"/>. It contains the gap-filled original soil moisture observations, gap-free uncertainty estimates, and the pure predictions before reimposing the observations (i.e. for missing data points as well as in place of the original measurements). We also provide two binary masks in the data to separate (original) observations and filled values in the gap-filled soil moisture field and to differentiate between DCT-PLS predictions and linear interpolation values over frozen periods.</p>
      <p id="d2e3141">Our Python implementation of the DCT-PLS algorithm is based on the original MATLAB implementation by <xref ref-type="bibr" rid="bib1.bibx40" id="text.76"/> and is provided as part of the pytesmo soil moisture toolbox package in v0.18.0 (<ext-link xlink:href="https://doi.org/10.5281/zenodo.14975386" ext-link-type="DOI">10.5281/zenodo.14975386</ext-link>, <xref ref-type="bibr" rid="bib1.bibx93" id="altparen.77"/>), available at <uri>https://github.com/TUW-GEO/pytesmo</uri> (last access: 20 August 2025).</p>
</sec>
<sec id="Ch1.S8" sec-type="conclusions">
  <label>8</label><title>Discussion and conclusions</title>
      <p id="d2e3164">The gap-filling framework around the DCT-PLS algorithm effectively estimates soil moisture for data gaps in the ESA CCI SM dataset. Choosing a univariate algorithm ensures that the resulting product relies solely on soil moisture observations independent of external satellite or model datasets. Additionally, DCT-PLS is a performant algorithm suitable for operational data production as envisaged for the Copernicus Climate Change Service (C3S) <xref ref-type="bibr" rid="bib1.bibx35" id="paren.78"/>.</p>
      <p id="d2e3170">We incorporated additional soil moisture retrievals from L- and C-band in equatorial latitudes with dense vegetation cover as anchor measurements for the interpolation algorithm. Although these measurements are often noisy and therefore justifiably excluded from the original ESA CCI SM data, they serve as viable support points for gap filling, leading to a moderate agreement with available in situ measurements in the area. However, we found that the retrieval uncertainty estimates based on triple collocation analysis for these areas are often too low, which can also affect the (propagated) uncertainties of the GAPFILLED product. We conclude that not only the retrieval of soil moisture under very dense vegetation layers remains challenging, but also that the estimation of associated uncertainties warrants further research. Studies utilizing these retrieval uncertainties, including ours, could apply them to provide better estimates of the quality of derived products based on these data.</p>
      <p id="d2e3173">Linear interpolation during periods when soil moisture is frozen may appear simplistic but follows the logic that there is no loss of water from the soil resulting in short-term changes. We use the average of observations from 30 d before and after periods when soil moisture is frozen as bounding points for linear interpolation. The threshold was determined based on regional experiments with satellite and in situ data and was selected as the best compromise between stable interpolation and a smooth transition between interpolated and observed data. However, it could be further refined, for example, by considering different onset periods for different climates globally. Our approach has the drawback that it relies on external soil temperature information, which can introduce outliers in the time series when prolonged periods of frozen soils (<inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> °C) are interrupted by brief thawing events. This issue could be mitigated by adopting a slightly stricter threshold value (e.g. 4 °C, in line with <xref ref-type="bibr" rid="bib1.bibx48" id="altparen.79"/>) and/or by setting a minimum number of consecutive days above 0 °C before a data point is classified as “unfrozen”. Moreover, our method does not account for potential sub-pixel freeze–thaw dynamics. Further research is needed to better understand soil moisture dynamics at coarse scales in such cases, enabling satellite retrievals and improved gap-filling predictions in the future. In the final data files, we provide a separate flag to identify cases where linear interpolation was applied so that users can filter them out or replace them if necessary.</p>
      <p id="d2e3189">To provide users with a quality estimate for the gap-filled values, we developed a method to quantify the uncertainties in our predictions (<inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">gapfilling</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). These uncertainties are generally higher for larger gaps and regions with dense vegetation compared to areas with better initial coverage. They are combined with the observation uncertainties and included as a separate field in the dataset. In order to quantify uncertainties associated with the gap-filling process, we used 3-dimensional Euclidean distances to the nearest valid data point as an estimate of gap size, but in practice, it could matter whether this point is close temporally or spatially due to different levels of soil moisture autocorrelation in these dimensions <xref ref-type="bibr" rid="bib1.bibx97" id="paren.80"/>. Evaluating these uncertainties remains challenging due to limited reference data. While correlation with in situ measurements decreases for larger gaps, this could not be confirmed in terms of ubRMSD. We do not consider the current uncertainty estimates final and encourage further research on this topic. Methods such as Gaussian process regression <xref ref-type="bibr" rid="bib1.bibx42" id="paren.81"/> have been used to fill measurement gaps in time series data in the past <xref ref-type="bibr" rid="bib1.bibx27" id="paren.82"/>. They provide uncertainty estimates based on the variance of multiple predictions but for the same reason were also found to be computationally too demanding <xref ref-type="bibr" rid="bib1.bibx53" id="paren.83"/> for operational application in a global record such as ESA CCI and C3S SM.</p>
      <p id="d2e3216">We observed that the GAPFILLED product performs similarly to the original observations for the absolute values (including the climatological signals) and short-term fluctuations (anomalies). In some cases, the filled values match better with independent reference data than the original observations, likely due to the smoothing effect of DCT-PLS. Similar outcomes have been observed with other smoothing algorithms, such as the exponential filter model, which is used to estimate root-zone soil moisture from surface measurements <xref ref-type="bibr" rid="bib1.bibx92 bib1.bibx128 bib1.bibx2" id="paren.84"/>. These conclusions are based on evaluations using in situ data and from successfully restoring artificially introduced gaps in the gap-free GLDAS Noah dataset. One downside of the latter approach is that model and satellite soil moisture can differ, for example, in terms of noise level, representation of extreme events, or autocorrelation. This can be due to limited model representations, for example, due to disregarded irrigation signals <xref ref-type="bibr" rid="bib1.bibx142" id="paren.85"/> or unaccounted for latent water influx from rivers <xref ref-type="bibr" rid="bib1.bibx123" id="paren.86"/>. Thus, conclusions drawn from the restoration of model-based data may not fully apply to satellite observations in some regions, but they still give valuable insights. Regional parameterization of the DCT-PLS algorithm resulted in spatial variations in <inline-formula><mml:math id="M146" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>. The use of GCV score optimization for <inline-formula><mml:math id="M147" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx40" id="paren.87"/> follows the recommendation of <xref ref-type="bibr" rid="bib1.bibx131" id="text.88"/>. While the impact on the predictive skill compared to using a single global <inline-formula><mml:math id="M148" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> value was not extensively evaluated, we found a good global performance in restoring artificially excluded data.</p>
      <p id="d2e3256">The GAPFILLED dataset is suitable for both long-term and event-based studies. Our comparisons, as well as other studies, have shown that derived statistics (such as changes in annual anomalies) can be affected by gap filling <xref ref-type="bibr" rid="bib1.bibx9" id="paren.89"/>. However, in complex environments with little or no input observations, such as mountainous regions, minimal variability is observed in our data. Similarly, using a smoothing algorithm such as DCT-PLS for interpolation may be detrimental in terms of preserving small-scale extreme events. For applications that do not require a pure soil-moisture-based dataset, multivariate methods might therefore still be preferred. These studies could potentially use our data as starting values for further adjustment.</p>
</sec>

      
      </body>
    <back><app-group>

<app id="App1.Ch1.S1">
  <label>Appendix A</label><title/>

      <fig id="FA1"><label>Figure A1</label><caption><p id="d2e3274">VOD classification based on VODCA v2 CXKu multiband 2000–2023 average conditions. Threshold values are 0.18 for low/medium and 0.57 for medium/high VOD (<inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
        
        <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f14.png"/>

      </fig>

<fig id="FA2"><label>Figure A2</label><caption><p id="d2e3302">1991–2023 average uncertainty estimates in parts of the tropical climate zone of <bold>(a)</bold> satellite observations used for the GAPFILLED product (based on triple collocation analysis), <bold>(b)</bold> the filled (propagated) values in the GAPFILLED product only, and <bold>(c)</bold> the final GAPFILLED product overall (circles indicate areas with uncertainty estimates that are too low). Panel <bold>(d)</bold> shows the mean soil moisture climatologies of SMAP, ASCAT, and GLDAS Noah over the area outlined by the red bounding box in <bold>(a)</bold>.</p></caption>
        
        <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f15.png"/>

      </fig>

      <fig id="FA3"><label>Figure A3</label><caption><p id="d2e3331">ISMN Fiducial reference measurements (0–0.1 m depth) in ISMN v20240314 on <uri>http://qa4sm.eu</uri> (last access: 20 August 2025) (network references in Table <xref ref-type="table" rid="TA2"/> in the Appendix).</p></caption>
        
        <graphic xlink:href="https://essd.copernicus.org/articles/17/4305/2025/essd-17-4305-2025-f16.png"/>

      </fig>

<table-wrap id="TA1"><label>Table A1</label><caption><p id="d2e3352">ISMN sensor locations and properties from Fig. <xref ref-type="fig" rid="F7"/>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="10">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Network</oasis:entry>
         <oasis:entry colname="col3">Station</oasis:entry>
         <oasis:entry colname="col4">Sensor  Type</oasis:entry>
         <oasis:entry colname="col5">Latitude</oasis:entry>
         <oasis:entry colname="col6">Longitude</oasis:entry>
         <oasis:entry colname="col7">Elevation</oasis:entry>
         <oasis:entry colname="col8">Depth</oasis:entry>
         <oasis:entry colname="col9">Land Cover</oasis:entry>
         <oasis:entry colname="col10">Climate</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Name</oasis:entry>
         <oasis:entry colname="col3">Name</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">[°]</oasis:entry>
         <oasis:entry colname="col6">[°]</oasis:entry>
         <oasis:entry colname="col7">[m]</oasis:entry>
         <oasis:entry colname="col8">[cm]</oasis:entry>
         <oasis:entry colname="col9">Class</oasis:entry>
         <oasis:entry colname="col10">Class</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">(a)</oasis:entry>
         <oasis:entry colname="col2">TERENO</oasis:entry>
         <oasis:entry colname="col3">Schoeneseiffen</oasis:entry>
         <oasis:entry colname="col4">Hydraprobe-II-Sdi-12</oasis:entry>
         <oasis:entry colname="col5">50.5149</oasis:entry>
         <oasis:entry colname="col6">6.37559</oasis:entry>
         <oasis:entry colname="col7">612</oasis:entry>
         <oasis:entry colname="col8">5</oasis:entry>
         <oasis:entry colname="col9">130</oasis:entry>
         <oasis:entry colname="col10">Cfb</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">(b)</oasis:entry>
         <oasis:entry colname="col2">RISMA</oasis:entry>
         <oasis:entry colname="col3">SK2</oasis:entry>
         <oasis:entry colname="col4">Hydraprobe-II-Sdi-12</oasis:entry>
         <oasis:entry colname="col5">51.33504</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M150" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>106.5639</oasis:entry>
         <oasis:entry colname="col7">590</oasis:entry>
         <oasis:entry colname="col8">0–5</oasis:entry>
         <oasis:entry colname="col9">130</oasis:entry>
         <oasis:entry colname="col10">Dfb</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">(c)</oasis:entry>
         <oasis:entry colname="col2">SCAN</oasis:entry>
         <oasis:entry colname="col3">Stephenville</oasis:entry>
         <oasis:entry colname="col4">Hydraprobe-Digital-Sdi-12-(2.5-Volt)</oasis:entry>
         <oasis:entry colname="col5">32.25</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M151" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>98.2</oasis:entry>
         <oasis:entry colname="col7">407.896</oasis:entry>
         <oasis:entry colname="col8">5.08</oasis:entry>
         <oasis:entry colname="col9">130</oasis:entry>
         <oasis:entry colname="col10">Cfa</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">(d)</oasis:entry>
         <oasis:entry colname="col2">TAHMO</oasis:entry>
         <oasis:entry colname="col3">BiaSHTSDebiso</oasis:entry>
         <oasis:entry colname="col4">TEROS12</oasis:entry>
         <oasis:entry colname="col5">6.66462</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M152" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>3.09725</oasis:entry>
         <oasis:entry colname="col7">228.0</oasis:entry>
         <oasis:entry colname="col8">10</oasis:entry>
         <oasis:entry colname="col9">130</oasis:entry>
         <oasis:entry colname="col10">Aw</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">(e)</oasis:entry>
         <oasis:entry colname="col2">NGARI</oasis:entry>
         <oasis:entry colname="col3">SQ08</oasis:entry>
         <oasis:entry colname="col4">5TM</oasis:entry>
         <oasis:entry colname="col5">32.55603</oasis:entry>
         <oasis:entry colname="col6">79.84004</oasis:entry>
         <oasis:entry colname="col7">4308.0</oasis:entry>
         <oasis:entry colname="col8">5</oasis:entry>
         <oasis:entry colname="col9">200</oasis:entry>
         <oasis:entry colname="col10">Dsb</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<table-wrap id="TA2"><label>Table A2</label><caption><p id="d2e3647">Soil moisture FRM networks available through QA4SM.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="16cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Network</oasis:entry>
         <oasis:entry colname="col2">Reference</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">AMMA-CATCH</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx94" id="text.90"/>, <xref ref-type="bibr" rid="bib1.bibx82" id="text.91"/>, <xref ref-type="bibr" rid="bib1.bibx24" id="text.92"/>, <xref ref-type="bibr" rid="bib1.bibx102" id="text.93"/>, <xref ref-type="bibr" rid="bib1.bibx66" id="text.94"/>, <xref ref-type="bibr" rid="bib1.bibx39" id="text.95"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ARM</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx25" id="text.96"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">COSMOS</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx147 bib1.bibx148" id="text.97"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CTP_SMTMN</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx136" id="text.98"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">DAHRA</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx116" id="text.99"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FLUXNET-AMERIFLUX</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FMI</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx57" id="text.100"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FR_Aqui</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx1" id="text.101"/>, <xref ref-type="bibr" rid="bib1.bibx134" id="text.102"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GROW</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx135" id="text.103"/>, <xref ref-type="bibr" rid="bib1.bibx140 bib1.bibx141" id="text.104"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">HOAL</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx13" id="text.105"/>, <xref ref-type="bibr" rid="bib1.bibx126" id="text.106"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">HOBE</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx12" id="text.107"/>, <xref ref-type="bibr" rid="bib1.bibx60" id="text.108"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ICN</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx56" id="text.109"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">IMA_CAN1</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx11" id="text.110"/>, <xref ref-type="bibr" rid="bib1.bibx23" id="text.111"/>, <xref ref-type="bibr" rid="bib1.bibx100" id="text.112"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">IPE</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx3" id="text.113"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">KIHS_CMC</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">KIHS_SMC</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">LAB-net</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx78 bib1.bibx77" id="text.114"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MAQU</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx114" id="text.115"/>, <xref ref-type="bibr" rid="bib1.bibx28" id="text.116"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MOL-RAO</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx10" id="text.117"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NAQU</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx114" id="text.118"/>, <xref ref-type="bibr" rid="bib1.bibx28" id="text.119"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NGARI</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx114" id="text.120"/>, <xref ref-type="bibr" rid="bib1.bibx28" id="text.121"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">OZNET</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx109" id="text.122"/>, <xref ref-type="bibr" rid="bib1.bibx138" id="text.123"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PTSMN</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx52" id="text.124"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">REMEDHUS</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx43" id="text.125"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RISMA</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx86" id="text.126"/>, <xref ref-type="bibr" rid="bib1.bibx67" id="text.127"/>, <xref ref-type="bibr" rid="bib1.bibx22" id="text.128"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RSMN</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SASMAS</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx104" id="text.129"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SCAN</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx105" id="text.130"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SD_DEM</oasis:entry>
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       <oasis:row>
         <oasis:entry colname="col1">SMN-SDR</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx144" id="text.132"/>, <xref ref-type="bibr" rid="bib1.bibx145" id="text.133"/></oasis:entry>
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       <oasis:row>
         <oasis:entry colname="col1">SMOSMANIA</oasis:entry>
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       <oasis:row>
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         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx65" id="text.137"/>, <xref ref-type="bibr" rid="bib1.bibx64" id="text.138"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SOILSCAPE</oasis:entry>
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       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SWEX_POLAND</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx76" id="text.141"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">TAHMO</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
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       <oasis:row>
         <oasis:entry colname="col1">TERENO</oasis:entry>
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       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">UDC_SMOS</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx106" id="text.145"/>, <xref ref-type="bibr" rid="bib1.bibx74" id="text.146"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">UMBRIA</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx17 bib1.bibx18" id="text.147"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">UMSUOL</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">USCRN</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx7" id="text.148"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">VAS</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">VDS</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">iRON</oasis:entry>
         <oasis:entry colname="col2"><xref ref-type="bibr" rid="bib1.bibx89 bib1.bibx88" id="text.149"/></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>


</app>
  </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e4184">WP, PS, and WD designed the study. WP performed the analysis and wrote the paper. All authors contributed to discussions about the methods and results and provided feedback on the paper and data.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e4190">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e4197">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. While Copernicus Publications makes every effort to include appropriate place names, the final responsibility lies with the authors.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e4203">The initial dataset was designed under the Horizon 2020 Global Gravity-based Groundwater Product (G3P) project supported by the European Commission (grant no. 870353). Operational implementation is supported by the Copernicus Climate Change Service implemented by ECMWF through C3S2 312a/313c.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e4208">This dataset was produced with funding from the European Space Agency (ESA) Climate Change Initiative (CCI) Plus Soil Moisture Project (CCN 3 to ESRIN contract no. 4000126684/19/I-NB ESA CCI+ Phase 1 New R&amp;D on CCI ECVS Soil Moisture). The authors acknowledge the TU Wien Bibliothek for financial support through its Open Access Funding Programme.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e4214">This paper was edited by Jiafu Mao and reviewed by two anonymous referees.</p>
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