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  <front>
    <journal-meta><journal-id journal-id-type="publisher">TC</journal-id><journal-title-group>
    <journal-title>The Cryosphere</journal-title>
    <abbrev-journal-title abbrev-type="publisher">TC</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">The Cryosphere</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1994-0424</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/tc-20-3187-2026</article-id><title-group><article-title>Machine learning for snow depth estimation over the European Alps, using Sentinel-1 observations, meteorological  forcing data and process-based model simulations</article-title><alt-title>Machine learning for snow depth estimation over the European Alps</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Boeykens</surname><given-names>Lucas</given-names></name>
          <email>lucas.boeykens@ugent.be</email><email>lucas.boeykens@kuleuven.be</email>
        <ext-link>https://orcid.org/0009-0006-4365-4997</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Dunmire</surname><given-names>Devon</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-6299-9137</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Jans</surname><given-names>Jonas-Frederik</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8650-0377</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Waegeman</surname><given-names>Willem</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>De Lannoy</surname><given-names>Gabriëlle</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Beernaert</surname><given-names>Ezra</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0979-8998</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Verhoest</surname><given-names>Niko E. C.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4116-8881</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Lievens</surname><given-names>Hans</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6391-1691</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Hydro-Climate Extremes Lab, Ghent University, Coupure Links 653, 9000 Gent, Belgium</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth and Environmental sciences, KU Leuven, Celestijnenlaan 200E, 3001 Leuven, Belgium</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Data Analysis and Mathematical Modelling, Ghent University, Coupure Links 653, 9000 Gent, Belgium</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Lucas Boeykens (lucas.boeykens@ugent.be, lucas.boeykens@kuleuven.be)</corresp></author-notes><pub-date><day>29</day><month>May</month><year>2026</year></pub-date>
      
      <volume>20</volume>
      <issue>5</issue>
      <fpage>3187</fpage><lpage>3216</lpage>
      <history>
        <date date-type="received"><day>10</day><month>July</month><year>2025</year></date>
           <date date-type="rev-request"><day>30</day><month>July</month><year>2025</year></date>
           <date date-type="rev-recd"><day>16</day><month>April</month><year>2026</year></date>
           <date date-type="accepted"><day>16</day><month>April</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Lucas Boeykens et al.</copyright-statement>
        <copyright-year>2026</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://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026.html">This article is available from https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026.html</self-uri><self-uri xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026.pdf">The full text article is available as a PDF file from https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e159">Seasonal mountain snow is an indispensable resource, but accurate estimates of this water storage remain limited, even in the European Alps, where there is a dense network of in situ monitoring stations. In this study, we address Alpine snow depth estimation at a 100 m spatial resolution and sub-weekly temporal resolution over the 2015–2024 period using multiple input configurations within an extreme gradient boosting (XGBoost) machine learning (ML) model. We explore the potential of Sentinel-1 C-band dual-polarized synthetic aperture radar polarimetry (PolSAR) observations, and include either regionally downscaled meteorological forcing data or modeled snow depth as additional inputs to further explain interannual and spatial variability. A threefold nested cross-validation scheme is used to account for the spatio-temporal dependencies present in the snow depth data. XGBoost's internal booster and Shapley additive explanation (SHAP) values are used to relate the input features with the predictions for both dry and wet snow conditions. Our results indicate that the inclusion of PolSAR observations leads to modest improvements over a backscatter-intensity-based configuration, whereas the SHAP-based feature attribution reveals a high reliance of XGBoost on the polarimetric scattering angle and co-polarized (VV) backscatter intensity. Next, incorporating either meteorological forcing data or modeled snow depth substantially enhances predictive performance, particularly when spatially distributed training data, proven to be essential for capturing topographic controls on snow depth variability, are included. When supplemented with spatial training data and either meteorological forcing data or modeled snow depth estimates, XGBoost shows good agreement with nine snow surveys conducted in the Dischma valley (Switzerland), achieving correlation coefficients (<inline-formula><mml:math id="M1" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>) of 0.76 and 0.78 and mean biases of 0.07 and 0.17 m, respectively. When applied to unseen locations across the Alps, the performance remains high, with <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.80</mml:mn></mml:mrow></mml:math></inline-formula> and biases of <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.03</mml:mn></mml:mrow></mml:math></inline-formula> m, respectively.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>Belgian Federal Science Policy Office</funding-source>
<award-id>SR/00/407</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="d2e210">Globally, the spatial and temporal dynamics of seasonal snow have been changing over the last decades. <xref ref-type="bibr" rid="bib1.bibx65" id="text.1"/> and <xref ref-type="bibr" rid="bib1.bibx10" id="text.2"/> report a negative trend in global annual snow cover, while <xref ref-type="bibr" rid="bib1.bibx61" id="text.3"/> observed an overall decreasing trend in monthly mean snow depth (SD) for the months of November through May across the European Alps. These changes in seasonal snow dynamics have implications for society, ecosystems, and the climate system, given the critical role that snow plays in each of these domains. Snow namely serves as a natural water reservoir that contributes to river discharge, soil moisture and groundwater recharge <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx28" id="paren.4"/>, and moreover fuels water basins used for hydropower generation <xref ref-type="bibr" rid="bib1.bibx10" id="paren.5"/>. Snow also provides drinking water to over 1.2 billion people worldwide, supports agricultural irrigation through snowmelt-driven runoff, and exerts substantial socioeconomic impacts, for example through traffic delays and accidents and by sustaining a multi-billion-dollar winter recreation industry <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx4 bib1.bibx10 bib1.bibx72 bib1.bibx79 bib1.bibx17 bib1.bibx76 bib1.bibx67" id="paren.6"/>.</p>
      <p id="d2e232">The climatic significance of snow is arguably even greater, albeit harder to monetize <xref ref-type="bibr" rid="bib1.bibx79" id="paren.7"/>. The combination of the high albedo of snow, which reflects a large portion of the incoming solar radiation, with the vast area of the world covered yearly by snow, enhances global cooling, and thus influences the Earth's surface energy balance <xref ref-type="bibr" rid="bib1.bibx87 bib1.bibx39 bib1.bibx58" id="paren.8"/>. As a result of its importance, key snowpack properties such as SD and snow water equivalent (SWE), the latter relating to SD through snow bulk density, have been designated as essential climate variables <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx37" id="paren.9"/>, and various scientific institutions and international organizations have prioritized their enhanced observation and monitoring <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx89" id="paren.10"/>.</p>
      <p id="d2e247">To date, mountain SD and SWE have been observed and monitored using a wide range of measurement and modeling techniques, including manual and automated point measurements; airborne passive and active optical sensors; airborne and space-borne passive microwave radiometers; airborne and space-borne active microwave sensors, such as synthetic aperture radar (SAR); and process-based models. Manual and automated point measurements offer frequent data at many locations globally (e.g., <xref ref-type="bibr" rid="bib1.bibx35" id="altparen.11"/>, or <xref ref-type="bibr" rid="bib1.bibx61" id="altparen.12"/>), but fall short in capturing the snowpack’s spatial variability due to their relatively sparse and uneven spatial distribution within alpine regions <xref ref-type="bibr" rid="bib1.bibx64 bib1.bibx53" id="paren.13"/>. Moreover, this type of monitoring is often conducted at relatively flat and open sites, rarely covers the highest elevations, and can disturb the snowpack <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx25 bib1.bibx64" id="paren.14"/>. Snow measurements derived from airborne passive and active optical sensors, such as photogrammetry-based SD maps <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx59" id="paren.15"/> and lidar altimetry-derived SD and SWE products <xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx25" id="paren.16"/>, provide high-resolution, spatially distributed measurements within mountain ranges, yet their use is constrained by limited spatial coverage and sparse temporal sampling <xref ref-type="bibr" rid="bib1.bibx83 bib1.bibx28 bib1.bibx42" id="paren.17"/>. In contrast, space-borne passive microwave radiometers provide broad spatial coverage, but their effectiveness is reduced by a coarse spatial resolution (<inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> km) and signal saturation in deep (<inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> m) snowpacks <xref ref-type="bibr" rid="bib1.bibx80" id="paren.18"/>, limiting their applicability in mountainous regions. Alternatively, space-borne SAR has demonstrated potential for monitoring SD or SWE at finer spatial scales, particularly with Ku- and X-band observations <xref ref-type="bibr" rid="bib1.bibx83" id="paren.19"/>. Unfortunately, X-band observations are not publicly available, and no Ku-band satellite mission currently exists <xref ref-type="bibr" rid="bib1.bibx83" id="paren.20"/>, thereby constraining the development of such high-resolution SAR snow products over vast areas. Alternatively, multiple process-based snow models exist to estimate both SD and SWE at different spatial scales (e.g. Snowclim <xref ref-type="bibr" rid="bib1.bibx56" id="paren.21"/>; SNOWPACK <xref ref-type="bibr" rid="bib1.bibx5" id="paren.22"/>; SnowModel <xref ref-type="bibr" rid="bib1.bibx51" id="paren.23"/>; factorial snowpack model <xref ref-type="bibr" rid="bib1.bibx32" id="paren.24"/>). Such models use meteorological forcings – often reanalysis data – to simulate the snowpack as one or multiple layers; solving mass and energy balance equations and mathematically representing the physical processes occurring within the snowpack. However, due to uncertainties in the forcing data and/or limitations in model representation, the modeled snow properties may differ substantially compared to in situ measurements and among each other (e.g., <xref ref-type="bibr" rid="bib1.bibx81" id="altparen.25"/>, <xref ref-type="bibr" rid="bib1.bibx48" id="altparen.26"/>, and <xref ref-type="bibr" rid="bib1.bibx74" id="altparen.27"/>).</p>
      <p id="d2e324">Recently, SD retrieval algorithms have been developed that utilize Sentinel-1 (S1) active microwave observations at C-band (<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">5.4</mml:mn></mml:mrow></mml:math></inline-formula> GHz). For instance, <xref ref-type="bibr" rid="bib1.bibx50" id="text.28"/> use C-band co- (VV) and cross- (VH) polarized backscatter intensity observations in a conceptual change detection algorithm, which allows them to estimate SD across the European Alps at sub-kilometer spatial resolution. This algorithm was developed based on the results of <xref ref-type="bibr" rid="bib1.bibx49" id="text.29"/> and <xref ref-type="bibr" rid="bib1.bibx12" id="text.30"/>, who demonstrated the sensitivity of active microwave observations to snow at C-band. These previous studies have focused on C-band backscatter intensity in co- and cross-polarization, demonstrating that under dry snow conditions, an increasing snowpack depth leads to enhanced signal depolarization. This depolarization is thought to be related to snow volume scattering, (multiple) scattering on anisotropic snow crystals or clusters of crystals, and scattering at snow (or snow-ground) layer interfaces. As a result, mainly VH, or the ratio of VH to VV backscatter intensity is sensitive to an increasing SD <xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx83" id="paren.31"/>. <xref ref-type="bibr" rid="bib1.bibx45" id="text.32"/> further explored the sensitivity of S1 C-band backscatter intensity observations to seasonal patterns of SD and SWE across the European Alps. In addition, <xref ref-type="bibr" rid="bib1.bibx45" id="text.33"/> emphasize the potential of S1 C-band dual-polarized SAR polarimetry (PolSAR) for SD retrieval, through the use of derived PolSAR variables that inform about the dominant snow scattering mechanism (i.e., a polarimetric scattering angle that increases with a growing snowpack), or about the intensity of the total received backscatter (i.e., the first Stokes parameter). Previous work has explored PolSAR for wet snow or snow cover area detection <xref ref-type="bibr" rid="bib1.bibx82 bib1.bibx85" id="paren.34"/>, but no operational retrieval algorithms currently exist that utilize dual-polarized PolSAR observations for estimating mountain SD or SWE.</p>
      <p id="d2e360">Despite its ability to characterize mountain SD at high-resolution over vast areas, the algorithm of <xref ref-type="bibr" rid="bib1.bibx50" id="text.35"/> shows limited performance during periods of wet and shallow snow, in forested areas, or after frequent freeze-thaw events <xref ref-type="bibr" rid="bib1.bibx50 bib1.bibx12" id="paren.36"/>. To address some of these limitations, <xref ref-type="bibr" rid="bib1.bibx30" id="text.37"/> implemented machine learning (ML) to enhance S1-based SD estimates at a high spatial resolution (100 m). They utilized an extreme gradient boosting model <xref ref-type="bibr" rid="bib1.bibx20" id="paren.38"><named-content content-type="pre">XGBoost;</named-content></xref>, incorporating input features related to topography, land and snow cover, and S1 C-band backscatter intensity. For the latter, they focused on the same satellite observations used by <xref ref-type="bibr" rid="bib1.bibx50" id="text.39"/>, namely VV backscatter intensity, and the cross-polarization ratio, defined as the ratio of VH to VV backscatter intensity. Other studies have similarly explored the application of ML for estimating SD and SWE, both with and without integrating S1 C-band satellite observations <xref ref-type="bibr" rid="bib1.bibx91 bib1.bibx24 bib1.bibx13 bib1.bibx29" id="paren.40"/>. Similarly, multiple authors have explored the potential of ML in a hybrid physical/data-driven approach to enhance the outcomes of snow models (e.g., <xref ref-type="bibr" rid="bib1.bibx86" id="altparen.41"/>; <xref ref-type="bibr" rid="bib1.bibx70" id="altparen.42"/>). Thereby, additional information relevant to the snowpack can be incorporated, such as S1 C-band observations. A similar approach has been used by <xref ref-type="bibr" rid="bib1.bibx11" id="text.43"/>, <xref ref-type="bibr" rid="bib1.bibx26" id="text.44"/> and <xref ref-type="bibr" rid="bib1.bibx31" id="text.45"/> within a data-assimilation setup, which used S1 C-band snow retrievals to enhance modeled SD. Additionally, ML models can also be used as emulators, replacing physical models by directly estimating SD from meteorological forcings (e.g., <xref ref-type="bibr" rid="bib1.bibx19" id="altparen.46"/>). Nevertheless, few studies have investigated ML setups that directly integrate modeled SD with S1 C-band observations. Moreover, direct comparisons between SD ML configurations incorporating modeled SD and those using meteorological forcing data as emulator remain scarce, leaving unresolved whether meteorology-driven ML setups can achieve performance comparable to configurations that explicitly include modeled SD.</p>
      <p id="d2e403">In this manuscript, we further investigate the potential of ML with different input configurations to accurately estimate SD across the European Alps, essential for accurately quantifying the annual water stored as snow. To this end, we first conduct various experiments comparing the performance of S1 C-band backscatter intensity with PolSAR observations to quantify the added value of PolSAR observations relative to, and in combination with, backscatter intensity. To gain insights in when and where which type of satellite observations contribute to the SD predictions, we use feature importance (FI) analysis under both dry and wet snow conditions. We further evaluate the added value of incorporating meteorological forcing data and process-based snow model SD estimates as features in the ML model, to assess improvements in capturing interannual and site-specific variability, and to determine whether S1 observations remain influential. To validate our approach, we implement a threefold nested cross-validation (nested CV) framework, which masks subsets of the data during training and predicting (testing). This framework accounts for the spatial, temporal and spatio-temporal dependencies in the data, an essential consideration when validating ML models for spatio-temporal purposes <xref ref-type="bibr" rid="bib1.bibx63" id="paren.47"/>. Finally, to address the limitations of relying solely on point-based training data for spatial prediction and representing topographic effects on the estimates, we compare models trained with and without airborne snow survey data, and validate predictions against nine airborne photogrammetry surveys in the Dischma Valley, Switzerland.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
      <p id="d2e417">Various datasets were collected and reprojected (and/or resampled) to two geographic grids used in this study: the <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> m (<inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1008</mml:mn></mml:mrow></mml:math></inline-formula>°) resolution World Geodetic System 1984 (100 m WGS84) grid, used for fine-resolution datasets or to preserve more details in the target (SD) and auxiliary datasets, and the <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> m (<inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1008</mml:mn></mml:mrow></mml:math></inline-formula>°) WGS84 grid (500 m WGS84), used for the coarse-scale and satellite datasets. Table <xref ref-type="table" rid="T1"/> provides an overview of the data products and the grid to which each was aligned to be used within this study.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e469">Overview of the datasets and their associated targeted resolution. The 100 and 500 m resolutions refer to the spatial resolution of the WGS84 grid.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:colspec colnum="8" colname="col8" align="center"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Resolution</oasis:entry>
         <oasis:entry colname="col2">In situ SD</oasis:entry>
         <oasis:entry colname="col3">S1 C-band</oasis:entry>
         <oasis:entry colname="col4">Snow cover</oasis:entry>
         <oasis:entry colname="col5">Wet snow</oasis:entry>
         <oasis:entry colname="col6">Meteorological</oasis:entry>
         <oasis:entry colname="col7"><italic>Snowclim</italic></oasis:entry>
         <oasis:entry colname="col8">Auxiliary</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">WGS84</oasis:entry>
         <oasis:entry colname="col2">(incl. photogrammetry maps)</oasis:entry>
         <oasis:entry colname="col3">variables</oasis:entry>
         <oasis:entry colname="col4">data</oasis:entry>
         <oasis:entry colname="col5">mask</oasis:entry>
         <oasis:entry colname="col6">forcing data</oasis:entry>
         <oasis:entry colname="col7">SD</oasis:entry>
         <oasis:entry colname="col8">data</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">100 m</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M12" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M13" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M14" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">500 m</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M15" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M16" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M17" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M18" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>In situ SD measurements</title>
      <p id="d2e648">We compiled in situ SD data over the European Alps by combining stationary and point-based measurements with airborne photogrammetry snow surveys, sourced from multiple regional providers across the Alpine countries (Fig. <xref ref-type="fig" rid="F1"/>). Point-based measurements were collected for the time period 2015–2024, and include data from Austria (provided by Geosphere Austria, formerly ZAMG), France (from measurement stations operated by partners under agreement of MetéoFrance), Italy (collected in the autonomous regions of Valle d’Aosta, Trento and Alto-Adige, Piemonte, Lombardy and data provided by the International Center for Environmental Monitoring CIMA Research Foundation), and Switzerland (manual and automated point-based SD measurements collected and managed by the Swiss Federal Institute for Forest, Snow and Landscape Research (WSL) – Institute for Snow and Avalanche Research (SLF)). In addition, we augmented our SD dataset with measurement data sourced from the Synoptic Data platform and the National Oceanic and  Atmospheric Administration's Global Historical Climatology Network-Daily database (GHCNd, <xref ref-type="bibr" rid="bib1.bibx62" id="altparen.48"/>). With the addition of these data, our dataset also contained sites within Germany and Slovenia.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e658">Spatial distribution of (dots) static or point-based measurement sites colored by the number of available data in time, and (red box) airborne photogrammetry snow surveys conducted across the Dischma valley, used to train XGBoost and evaluate the SD predictions. The light gray area delineates the Alpine region as defined by the Alpine Convention <xref ref-type="bibr" rid="bib1.bibx2" id="paren.49"/>.</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f01.png"/>

        </fig>

      <p id="d2e670">Next, we collected spatial SD measurements, derived from airborne photogrammetry <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx16" id="paren.50"/> over the Dischma valley, Switzerland (Fig. <xref ref-type="fig" rid="F1"/>, red box). A total of nine photogrammetry SD surveys (snow surveys) were added to our dataset, with an original resolution of 0.5 m (6 maps, measured yearly near peak SD between 2017 and 2022) or 2 m (3 maps, collected on 3 distinct days in 2016). For both resolutions, we applied a linear averaging and reprojected all surveys to the target grid of our SD estimates, the 100 m WGS84 grid.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>S1 C-band PolSAR and backscatter intensity observations</title>
      <p id="d2e688">Within our research, we collected data from the European Space Agency (ESA) and Copernicus S1A and -B satellites, which operate at C-band and share the same orbital plane with a 180° orbital phasing difference. Both have a 12 d repeat cycle. Combined, they offer a repeat cycle of 6 d over the study area. S1B, however, has been out of operation since 24 December 2021, and thus does not cover the complete study period (2015–2024).</p>
      <p id="d2e691">S1 dual-polarized PolSAR observations were acquired from interferometric wide swath (IW) single look complex (SLC) data in dual-polarization (VV and VH) mode. The data were processed into two dual-polarized PolSAR variables: the polarimetric scattering angle (<inline-formula><mml:math id="M19" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>) and the first Stokes parameter (<inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), using the Sentinel application platform (SNAP) toolbox, version 9, with processing steps described in <xref ref-type="bibr" rid="bib1.bibx45" id="text.51"/>. These processing steps included applying precise orbit file corrections, radiometric calibration, debursting TOPSAR bursts, and merging sub-swaths into a single image. This was followed by the generation of the <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> covariance matrix (C2-matrix). The C2-matrix was then used as input for two distinct processing chains. The first one involved an eigenvector/value decomposition of the C2-matrix, followed by the H/<inline-formula><mml:math id="M22" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> decomposition <xref ref-type="bibr" rid="bib1.bibx21" id="paren.52"/>, from which <inline-formula><mml:math id="M23" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> was derived. The second processing chain utilized the compact-polarimetry Stokes parameter generation to derive <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from the C2-matrix. Next, both variables were multilooked to <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> m to reduce speckle and finally, a Range Doppler terrain correction was applied to both variables, reducing (geometric) distortions due to topographical variations in the scene. For the latter, the Copernicus 30 m global digital elevation model (GLO-30 DEM) was used.</p>
      <p id="d2e766">Next, co- (<inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>) and cross- (<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VH</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>) polarized backscatter intensity variables were retrieved from ground range detected (GRD) amplitude data. Processing steps, described in <xref ref-type="bibr" rid="bib1.bibx50" id="text.53"/> and <xref ref-type="bibr" rid="bib1.bibx45" id="text.54"/>, were applied, including precise orbit file application, GRD border and thermal noise removal, radiometric calibration, terrain flattening to backscatter as <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">γ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx77" id="paren.55"/> and finally a Range Doppler terrain correction. As for the PolSAR variables, the Copernicus GLO-30 DEM was used during the processing steps. Additionally, local incidence angle (LIA) information was preserved and the cross-polarization ratio (<inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>; calculated as the ratio between <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VH</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> in linear scale) was calculated.</p>
      <p id="d2e855">Finally, both the PolSAR and backscatter intensity observations were rescaled and summer-corrected, to reduce inter-orbital and interannual start-of-season differences, respectively. To this end, we first reprojected the satellite observations onto the 100 m WGS84 grid using linear averaging, and resampled to the 500 m WGS84 grid by taking the mean. Then, we performed a first and second-order moment scaling (to correct for differences in the mean and variance) between orbits. Finally, from each scaled time series for each snow season (September–June), we subtracted the mean summer value (July–September) of the summer preceding that snow season, thereby reducing interannual start-of-season differences that are not related to snow conditions (e.g., changing vegetation). To indicate that these variables have been rescaled, we further append a superscript “s” (<sup>s</sup>) to the satellite variable notation.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Snow cover data and wet snow mask</title>
      <p id="d2e875">Snow cover data were obtained from two sources: binary snow cover information from the interactive multisensor snow and ice mapping system (IMS; <xref ref-type="bibr" rid="bib1.bibx84" id="altparen.56"/>) at 1 km resolution, and fractional snow cover (FSC) information from the moderate resolution imaging spectroradiometer (MODIS; <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx41" id="altparen.57"/>) at 500 m resolution. For the latter, we collected cloud gap-filled FSC data separately from the Terra and Aqua satellites, which we both reprojected onto the 500 m WGS84 grid using linear averaging. Subsequently, we combined the individual products using a weighted average, which accounted for the quality flags of each product, the time lag between the last cloud-free FSC observation and the current date, and the time lag of the individual satellite observations relative to each other (Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/>). Next, a cutoff was set on the combined product, only allowing for FSC information less than 7 d before the current date. Finally, remaining gaps (3.95 % of the data points across the whole Alps and study period) were filled using IMS' binary snow cover information, reprojected to the same 500 m WGS84 grid using majority resampling. Hereby, a no-snow indication of IMS was set to an FSC value of 0 %, while an IMS snow covered pixel received a value of 100 %.</p>
      <p id="d2e886">Additionally, a wet snow mask was acquired to differentiate between dry and wet snow periods. This dataset, based on S1 C-band satellite observations and obtained from the Copernicus Land Monitoring Service (CLMS) High Resolution Snow and Ice Monitoring (HRSIM) SAR Wet Snow in high mountains (SWS) product <xref ref-type="bibr" rid="bib1.bibx22" id="paren.58"/>, provides a binary classification between wet snow conditions, and dry, patchy or snow-free conditions. The data, available at 60 m resolution from September 2016 onward, were first reprojected onto the 100 m WGS84 grid using majority resampling, whereby the most frequently occurring SWS value within each 100 m target pixel was selected while excluding any no-data values. Subsequently, all non-wet pixels were classified as dry, while quality flags were retained to identify locations and periods with no (reliable) classification.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Meteorological forcing data</title>
      <p id="d2e900">We downscaled 3-hourly meteorological forcing data over the European Alps to a 500 m spatial resolution, to serve as additional input to the ML model. To this end, we first collected coarse three-hourly meteorological forcing data with a 0.1° spatial resolution. Precipitation data were sourced from the multi-source weighted-ensemble precipitation (MSWEP, <xref ref-type="bibr" rid="bib1.bibx6" id="altparen.59"/>) dataset, which combines various state-of-the-art reanalysis products with gauge and satellite observations <xref ref-type="bibr" rid="bib1.bibx6" id="paren.60"/>. Other variables, including downward shortwave and longwave radiation, 2 m air temperature, wind speed, and 2 m relative humidity, were obtained from the multi-source weather (MSWX, <xref ref-type="bibr" rid="bib1.bibx7" id="altparen.61"/>) product. This dataset is derived from coarse-scale European centre for medium-range weather forecasts reanalysis version 5 (ERA5) data refined through bias correction and downscaling using monthly 0.1° reference climatologies <xref ref-type="bibr" rid="bib1.bibx7" id="paren.62"/>.</p>
      <p id="d2e915">Subsequently, we applied bilinear interpolation in combination with different downscaling techniques, explained below, to account for local terrain features. To this end, the Copernicus GLO-30 DEM was employed, linearly averaged to the 500 m WGS84 grid to match the target resolution for the meteorological forcings. First, coarse-scale precipitation (<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mtext>coarse</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>; [<inline-formula><mml:math id="M34" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> per 3 h]) was corrected as a function of elevation to account for orographic effects, using a rescaling function adapted from <xref ref-type="bibr" rid="bib1.bibx43" id="text.63"/>, who corrected in situ precipitation data for gauge undercatch in a glacier mass-balance study. Thus, for each location <inline-formula><mml:math id="M35" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> within the 500 m grid at time step <inline-formula><mml:math id="M36" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mtext>coarse</mml:mtext><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> was downscaled using the following equation:

                <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M38" display="block"><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>D</mml:mi><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mtext>coarse</mml:mtext><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mi>D</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mtext>coarse</mml:mtext><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:mo>⋅</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:mn mathvariant="normal">0.75</mml:mn><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>z</mml:mi><mml:mtext>min</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mtext>max</mml:mtext></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>z</mml:mi><mml:mtext>min</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mtext> with  </mml:mtext><mml:mi>D</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mtext>max</mml:mtext></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>z</mml:mi><mml:mtext>min</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mtext>dif</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>≤</mml:mo><mml:mi>D</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:math></disp-formula>

          with <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the elevation [m] of the 500 m Copernicus GLO-30 DEM, <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mtext>min</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mtext>max</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> the minimum and maximum elevation [m] within an interpolation window – centered on the location <inline-formula><mml:math id="M42" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and spanning an area roughly matching the original 0.1° grid size – and <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mtext>dif</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> a user defined difference in elevation, set to 250 m. The user defined difference was introduced to focus the corrections on the study area, with minor adjustments for areas with small elevation differences. Different from <xref ref-type="bibr" rid="bib1.bibx43" id="text.64"/>, Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) limits the downscaled precipitation values between 75 % and 125 % of the original <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mtext>coarse</mml:mtext><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> values.</p>
      <p id="d2e1209">The other forcings were adjusted as follows. The temperature was corrected using a seasonally varying lapse rate, following <xref ref-type="bibr" rid="bib1.bibx52" id="text.65"/>, to account for elevation-dependent temperature variations. For relative humidity, we first converted to dewpoint temperature, then applied a lapse rate correction similar as for the temperature, and finally converted the corrected dewpoint temperature back to relative humidity <xref ref-type="bibr" rid="bib1.bibx52" id="paren.66"/>. Downward shortwave radiation was adjusted following the method of <xref ref-type="bibr" rid="bib1.bibx34" id="text.67"/>, which involved partitioning the radiation data into direct and diffuse components, accounting for the elevation effect on the direct component, and applying a topographic correction to both components. In contrast, downward longwave radiation and wind speed were not adjusted after bilinear interpolation.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Process-based snow model <italic>Snowclim</italic></title>
      <p id="d2e1233">Modeled SD estimates were obtained using <italic>Snowclim</italic> <xref ref-type="bibr" rid="bib1.bibx56" id="paren.68"/>, a process-based enhanced single layer snow model utilizing a fully distributed energy and mass balance. We ran the model over the entire European Alps with the downscaled meteorological forcing data at a 500 m spatial and 3-hourly temporal resolution. To obtain daily values, the 3-hourly SD estimates were averaged to a daily time step. A description of the model's parameter settings, how they have been calibrated, and the model's performance when validated against in situ measurements, is provided in Appendix <xref ref-type="sec" rid="App1.Ch1.S2"/>.</p>
</sec>
<sec id="Ch1.S2.SS6">
  <label>2.6</label><title>Time-independent auxiliary data</title>
      <p id="d2e1252">In addition to time-dependent data, we employed time-independent auxiliary data, sourced from various providers. As with the other datasets (except the meteorological forcing and <italic>Snowclim</italic> data), these data were first projected onto the 100 m WGS84 grid, using linear averaging for continuous variables and majority resampling for categorical data. Forest cover fraction (FCF) data and land cover information, including a water mask, were acquired from the 2018 epoch of the 100 m Copernicus PROBA-V global land cover dataset <xref ref-type="bibr" rid="bib1.bibx14" id="paren.69"/>. Next, we used the Copernicus GLO-30 DEM to extract elevation and three topographic features: slope, aspect, and topographic position index (TPI), the latter quantifying the relative elevation of a grid cell concerning its surroundings within a predefined diameter. Slope and aspect were computed in MATLAB using the Geodetic <xref ref-type="bibr" rid="bib1.bibx23" id="paren.70"/> and TopoToolbox <xref ref-type="bibr" rid="bib1.bibx75" id="paren.71"/> toolboxes, while TPI was calculated following the methodologies of <xref ref-type="bibr" rid="bib1.bibx88" id="text.72"/> and <xref ref-type="bibr" rid="bib1.bibx55" id="text.73"/>. For this study, we computed the TPI using only the neighboring pixels of a specific grid cell, corresponding to a <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> grid window. Finally, we included a glacier mask, retrieved from the Randolph Glacier Inventory version 7.0 <xref ref-type="bibr" rid="bib1.bibx73" id="paren.74"/>, and collected the <xref ref-type="bibr" rid="bib1.bibx78" id="text.75"/> snow classes.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methods</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>XGBoost model selection</title>
      <p id="d2e1309">Within this study, we deployed XGBoost to estimate SD across the European Alps. XGBoost is a tree-based traditional ML algorithm that constructs multiple decision trees in a sequential order, to minimize a differentiable loss function <xref ref-type="bibr" rid="bib1.bibx20" id="paren.76"/>. Thereby, new trees are trained to fit the residual errors of the previously fitted trees, while incorporating regularization terms to reduce model complexity, and including additional mechanisms that contribute to its computational efficiency <xref ref-type="bibr" rid="bib1.bibx20" id="paren.77"/>. We chose this ML algorithm after comparative experiments with other tree-based methods (including Random Forest, LightGBM and CatBoost) in which XGBoost showed the best performance and computational efficiency, as well as its use in recent snow studies (e.g., <xref ref-type="bibr" rid="bib1.bibx30" id="altparen.78"/>, or <xref ref-type="bibr" rid="bib1.bibx38" id="altparen.79"/>).</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Dataset preparation</title>
      <p id="d2e1332">We trained, validated, and tested XGBoost with various configurations on a dataset containing input features associated with each SD measurement (predictor variable) from the in situ measurement sites and snow surveys. To construct this dataset, we first excluded those stationary measurement sites located within glaciated areas, as well as those with less than 5 % non-zero SD observations. Subsequently, we identified the unique locations of the stationary sites within the 100 m WGS84 grid, and averaged time series from sites within the same grid cell. Furthermore, we excluded SD measurements during the summer months July and August, and resampled the data with a 500 m spatial resolution to the 100 m WGS84 grid using value replication.</p>
      <p id="d2e1335">The S1 data spatially and temporally coinciding with available SD measurements on the 100 m WGS84 grid include both ascending and descending orbits. This allows a single location to have two S1 observation values for the same SD measurement on a given date. Importantly, we chose not to exclude satellite observations with high or low LIA, as we assumed that XGBoost could effectively learn the relationships between these satellite observations and the corresponding SD. For each location and date with an available satellite observation, we also selected the corresponding (nearest) time-dependent non-satellite data and time-independent auxiliary data. This resulted in a dataset comprising 1022 measurement sites, with the distributions of observed SD and selected auxiliary variables shown in Fig. <xref ref-type="fig" rid="FE1"/>.</p>
      <p id="d2e1340">A similar procedure was applied for the photogrammetry snow survey data: for each SD measurement, the nearest input feature values within the 100 m WGS84 grid were selected and compiled into a dataset, linking each SD observation with its corresponding input features. Since satellite acquisitions did not always coincide with the exact date of the snow surveys, we used the most recent S1 observation prior to the survey, with a maximum offset of two days. Lastly, to represent the temporal component of our datasets, we computed the day of the year (DOY) for each instance. To account for the cyclic nature of the calendar year and prevent discontinuity between 31 December and 1 January, we transformed the DOY into two separate features using sine (<inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mtext>DOY</mml:mtext><mml:mtext>sin</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) and cosine (<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mtext>DOY</mml:mtext><mml:mtext>cos</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) functions:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M48" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mtext>DOY</mml:mtext><mml:mtext>sin</mml:mtext></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:mtext>sin</mml:mtext><mml:mo mathsize="2.0em">(</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">π</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>DOY</mml:mtext></mml:mrow><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:mo mathsize="2.0em">)</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd><mml:mtext>3</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mtext>DOY</mml:mtext><mml:mtext>cos</mml:mtext></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:mtext>cos</mml:mtext><mml:mo mathsize="2.0em">(</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">π</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>DOY</mml:mtext></mml:mrow><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:mo mathsize="2.0em">)</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

          with <inline-formula><mml:math id="M49" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> the number of days in the corresponding year.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Feature configurations and SD prediction</title>
<sec id="Ch1.S3.SS3.SSS1">
  <label>3.3.1</label><title>S1 PolSAR vs. backscatter intensity observations</title>
      <p id="d2e1469">To assess the performance of ML setups using S1 PolSAR versus backscatter intensity observations, XGBoost was trained and validated under three distinct configurations (Table <xref ref-type="table" rid="T2"/>), without including meteorological forcing data or <italic>Snowclim</italic> SD estimates in these experiments. For each configuration, XGBoost incorporated the same time-independent auxiliary features: elevation, slope, aspect, TPI, and FCF. Next, DOY features, FSC data and LIA information were included, the latter to indirectly account for orbital differences. The first configuration, referred to as PolSAR<sub>ML</sub>, incorporated <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mi mathvariant="normal">s</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> next to the shared common input features. The second configuration, focusing on backscatter intensity observations (Backscatter<sub>ML</sub> configuration), included <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> as satellite input features. In addition, we combined the PolSAR and backscatter intensity satellite input features (Combination<sub>ML</sub> configuration), to identify the satellite variables most effectively used within XGBoost.</p>

<table-wrap id="T2" specific-use="star"><label>Table 2</label><caption><p id="d2e1540">Features included in the ML configurations tested in this study: polarimetric scattering angle (<inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>); first Stokes parameter (<inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mi mathvariant="normal">s</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>); cross-polarization ratio (<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>); co-polarized backscatter intensity (<inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>); cumulative snow precipitation and wind speed (<inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mtext>s,c</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mtext>Ua</mml:mtext><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, summed between 1 September of the corresponding snow year and the prediction date); cumulative shortwave radiation and melt days over the preceding 7 d (<inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mtext>SWd</mml:mtext><mml:mn mathvariant="normal">7</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mtext>MD</mml:mtext><mml:mn mathvariant="normal">7</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>); mean daily temperature on the prediction day (<inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>); and <italic>Snowclim</italic> SD estimates (<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mtext>SD</mml:mtext><mml:mtext>SC</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>). A cross (<inline-formula><mml:math id="M64" display="inline"><mml:mo lspace="0mm">×</mml:mo></mml:math></inline-formula>) denotes the presence of a feature in a given configuration. Additionally, all configurations include the following input features, indicated as <italic>common</italic> in the table: elevation, slope, aspect, topographic position index (TPI), forest cover fraction (FCF), fractional snow cover (FSC), sine and cosine values of the day of year (<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mtext>DOY</mml:mtext><mml:mtext>sin</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mtext>DOY</mml:mtext><mml:mtext>cos</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>), and the local incidence angle (LIA).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="18">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:colspec colnum="8" colname="col8" align="center"/>
     <oasis:colspec colnum="9" colname="col9" align="center"/>
     <oasis:colspec colnum="10" colname="col10" align="center"/>
     <oasis:colspec colnum="11" colname="col11" align="center"/>
     <oasis:colspec colnum="12" colname="col12" align="center"/>
     <oasis:colspec colnum="13" colname="col13" align="left"/>
     <oasis:colspec colnum="14" colname="col14" align="left"/>
     <oasis:colspec colnum="15" colname="col15" align="left"/>
     <oasis:colspec colnum="16" colname="col16" align="left"/>
     <oasis:colspec colnum="17" colname="col17" align="left"/>
     <oasis:colspec colnum="18" colname="col18" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">ML configuration</oasis:entry>
         <oasis:entry colname="col2"><italic>common</italic></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mi mathvariant="normal">s</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mtext>s,c</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mtext>Ua</mml:mtext><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col9"><inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mtext>SWd</mml:mtext><mml:mn mathvariant="normal">7</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col10"><inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mtext>MD</mml:mtext><mml:mn mathvariant="normal">7</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col11"><inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col12"><inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mtext>SD</mml:mtext><mml:mtext>SC</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col13"/>
         <oasis:entry colname="col14"/>
         <oasis:entry colname="col15"/>
         <oasis:entry colname="col16"/>
         <oasis:entry colname="col17"/>
         <oasis:entry colname="col18"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">PolSAR<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M77" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M78" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M79" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8"/>
         <oasis:entry colname="col9"/>
         <oasis:entry colname="col10"/>
         <oasis:entry colname="col11"/>
         <oasis:entry colname="col12"/>
         <oasis:entry colname="col13"/>
         <oasis:entry colname="col14"/>
         <oasis:entry colname="col15"/>
         <oasis:entry colname="col16"/>
         <oasis:entry colname="col17"/>
         <oasis:entry colname="col18"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Backscatter<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M80" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M81" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M82" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8"/>
         <oasis:entry colname="col9"/>
         <oasis:entry colname="col10"/>
         <oasis:entry colname="col11"/>
         <oasis:entry colname="col12"/>
         <oasis:entry colname="col13"/>
         <oasis:entry colname="col14"/>
         <oasis:entry colname="col15"/>
         <oasis:entry colname="col16"/>
         <oasis:entry colname="col17"/>
         <oasis:entry colname="col18"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Combination<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M83" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M84" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M85" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M86" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M87" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8"/>
         <oasis:entry colname="col9"/>
         <oasis:entry colname="col10"/>
         <oasis:entry colname="col11"/>
         <oasis:entry colname="col12"/>
         <oasis:entry colname="col13"/>
         <oasis:entry colname="col14"/>
         <oasis:entry colname="col15"/>
         <oasis:entry colname="col16"/>
         <oasis:entry colname="col17"/>
         <oasis:entry colname="col18"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Weather<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M88" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M89" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M90" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M91" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M92" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M93" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M94" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col9"><inline-formula><mml:math id="M95" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col10"><inline-formula><mml:math id="M96" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col11"><inline-formula><mml:math id="M97" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col12"/>
         <oasis:entry colname="col13"/>
         <oasis:entry colname="col14"/>
         <oasis:entry colname="col15"/>
         <oasis:entry colname="col16"/>
         <oasis:entry colname="col17"/>
         <oasis:entry colname="col18"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Snowclim</italic><sub>ML</sub></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M98" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M99" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M100" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M101" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M102" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8"/>
         <oasis:entry colname="col9"/>
         <oasis:entry colname="col10"/>
         <oasis:entry colname="col11"/>
         <oasis:entry colname="col12"><inline-formula><mml:math id="M103" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col13"/>
         <oasis:entry colname="col14"/>
         <oasis:entry colname="col15"/>
         <oasis:entry colname="col16"/>
         <oasis:entry colname="col17"/>
         <oasis:entry colname="col18"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <label>3.3.2</label><title>S1 observations plus meteorological forcing data or <italic>Snowclim</italic> SD estimates</title>
      <p id="d2e2297">The satellite observations were further complemented with either meteorological forcing data (Weather<sub>ML</sub> configuration) or <italic>Snowclim</italic> SD estimates (<italic>Snowclim</italic><sub>ML</sub> configuration) to better resolve interannual and in-between-site variability (Table <xref ref-type="table" rid="T2"/>). The Weather<sub>ML</sub> configuration was an extension of the Combination<sub>ML</sub> setup, now including cumulative snowfall, cumulative wind speed, cumulative shortwave radiation, a cumulative number of melt days, and the mean daily temperature (<inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). Cumulative snowfall (<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mtext>s,c</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) was estimated by first calculating the daily fraction of precipitation falling as snow, based on temperature, precipitation and relative humidity using the bivariate logistic regression model described by <xref ref-type="bibr" rid="bib1.bibx46" id="text.80"/>, and subsequently summing these fractions from 1 September of the corresponding snow year up to the prediction date. Similarly, the cumulative wind speed (<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mtext>Ua</mml:mtext><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) was derived as the sum of the daily wind speed from 1 September of the corresponding snow year up to the prediction date. Cumulative shortwave radiation (<inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mtext>SWd</mml:mtext><mml:mn mathvariant="normal">7</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), on the other hand, was summed over the seven days preceding the prediction date. Similarly, the cumulative number of melt days (<inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mtext>MD</mml:mtext><mml:mn mathvariant="normal">7</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) was defined as the number of days with a maximum temperature above 0 <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> within the 7 d preceding the prediction date. The <italic>Snowclim</italic><sub>ML</sub> configuration did not include meteorological forcing data as direct inputs, but instead makes use of modeled SD estimates from <italic>Snowclim</italic> (<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mtext>SD</mml:mtext><mml:mtext>SC</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>), which are driven by meteorological conditions.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS3">
  <label>3.3.3</label><title>XGBoost SD prediction procedure</title>
      <p id="d2e2416">Prior to being used in XGBoost for SD prediction, each feature was standardized individually, using the mean and standard deviation calculated from the training set values. This standardization was consistently applied to the validation and predicting (test) datasets as well, ensuring compatibility across all data splits. Since S1 observations are influenced by orbit-specific viewing geometries – potentially resulting in different SD estimates – input features from ascending and descending orbits were fed to XGBoost separately. In case a location had both an ascending and descending satellite observation on a given date, the mean of both XGBoost SD outputs was taken.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Spatio-temporal nested cross-validation and hyperparameter tuning</title>
      <p id="d2e2428">The concept of nested cross-validation (nested CV) has been extensively utilized in other studies <xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx1 bib1.bibx68" id="paren.81"/>, as it enables a correct characterization of the generalization error of an ML model <xref ref-type="bibr" rid="bib1.bibx8" id="paren.82"/>. Figure <xref ref-type="fig" rid="F2"/> illustrates that nested CV involves both inner and outer resampling to, respectively, train and tune the ML model (and its hyperparameters), and evaluate predictions on unseen and independent test data. Considering the susceptibility of SD measurements to spatial and temporal autocorrelation, we implemented the CV strategy described in <xref ref-type="bibr" rid="bib1.bibx47" id="text.83"/> within a threefold nested CV framework for the site data (excluding the snow surveys), in which subsets of the data are masked during training, validation and predicting (testing). To this end, the data of the site measurements were partitioned into spatial, temporal and spatio-temporal folds.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e2444">Principle of nested CV for <bold>(a)</bold> the spatio-temporal setup, <bold>(b)</bold> the spatial setup and <bold>(c)</bold> the temporal setup. The predicting (test) and training folds during outer resampling are colored in turquoise and light gray respectively. The validation and training folds during inner resampling are colored in dark and light blue. The striped boxes in <bold>(a)</bold> represent the excluded folds during training and testing within the spatio-temporal setup. During outer resampling, predictions are made with the trained ML model, with hyperparameters that are tuned during inner resampling. The numbers indicated in the arrows represent the amount of times outer and inner resampling are performed, respectively. For <bold>(a)</bold>, four iterations are shown, while for <bold>(b)</bold> and <bold>(c)</bold>, three iterations are displayed.</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f02.png"/>

        </fig>

      <p id="d2e2475">The spatial folds were constructed using a two-step approach: first, sites located within five km of one another were grouped into clusters, thereby preventing nearby sites with similar (climatic) characteristics and SD patterns from being split across training and test sets. Subsequently, these clusters were randomly assigned to five unique folds, ensuring that each fold contained a comparable amount of data and preserved a similar SD distribution. For the temporal folds, sites were not clustered; instead, all observations from a given snow season (September–June) and from across the study area were grouped into nine blocks (corresponding with the number of snow seasons for which SD data is available), which were then partitioned into five folds, again ensuring comparable fold sizes and a consistent SD distribution. Finally, by combining both fold-creation techniques, we constructed 25 unique spatio-temporal folds.</p>
      <p id="d2e2479">For each unique fold (five for spatial and temporal nested CV; 25 for spatio-temporal nested CV), we iteratively designated one fold as the test set during outer resampling, using the remaining folds for training and validation. To ensure independence of the test data, all data from the sites and/or years present in the test fold were excluded from the training and validation sets (Fig. <xref ref-type="fig" rid="F2"/>).</p>
      <p id="d2e2484">The same approach was applied during inner resampling, to split the training and validation data used for tuning XGBoost's hyperparameters. To tune the hyperparameters, we utilized Scikit-learn's <xref ref-type="bibr" rid="bib1.bibx69" id="paren.84"/> <italic>RandomizedSearchCV</italic> algorithm, employing the mean squared error (MSE) as loss function. A different random seed was set for each outer resampling loop, introducing variability in the selection of optimal hyperparameter combinations. During each loop, 150 hyperparameter combinations were chosen from a predefined tuning grid, based on the one provided in PyCaret <xref ref-type="bibr" rid="bib1.bibx71" id="paren.85"/>. The hyperparameters yielding the best mean MSE score across the validation folds were selected. This approach produced independent predictions for every instance in the dataset, enabling the calculation of performance metrics and the construction of FI scores.</p>
</sec>
<sec id="Ch1.S3.SS5">
  <label>3.5</label><title>Feature importance scores</title>
      <p id="d2e2505">We used both XGBoost's booster and Shapley additive explanations (SHAP; <xref ref-type="bibr" rid="bib1.bibx54" id="altparen.86"/>) values to assess the feature's impact on the SD estimates. For the booster, we selected the <italic>gain</italic> FI, which informs about the contribution of each input feature in minimizing the loss function during model training. As such, for every outer resampling loop within the nested CV framework, we computed the <italic>gain</italic> FI of the individual features during model training.</p>
      <p id="d2e2517">SHAP values, on the other hand, quantify the contribution of each input feature to an individual (SD) prediction, measured relative to an expected prediction (SD) value. Within the nested CV framework, SHAP values thus indicate how each feature influences the SD predictions made for the outer resampling predicting sets, relative to the average (SD) prediction computed from the training set. Consequently, SHAP values can be both positive and negative. To assess the overall global SHAP value FI during SD prediction, mean absolute SHAP values were computed for each input feature during every outer resampling loop. The latter were converted into relative contributions by normalizing them with the sum across all features.</p>
      <p id="d2e2520">We further used SHAP values to assess the contribution of the S1 PolSAR and backscatter intensity observations to the SD predictions throughout the seasonal evolution of the snowpack. To this end, for each site and snow season in the test sets, we first identified the periods during which a snowpack was present, based on the measured SD. The season start date was identified as the first date with <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mtext>SD</mml:mtext><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> cm, that was followed by nine consecutive days with <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mtext>SD</mml:mtext><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> cm. For low elevation sites with (very) shallow snowpacks, where this condition was not met for an entire snow season, the start of the snow season was marked by the first date with <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mtext>SD</mml:mtext><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> cm. Conversely, we defined the end of a site's snow season as the first day of a 10 d period with 0 cm SD, near the end of snowpack presence. In addition, we used the CLMS SWS product to distinguish, where possible, between dry and wet snow conditions. As this product is only available from September 2016 onward, the 2015–2016 snow season was omitted from the corresponding analyses.</p>
</sec>
<sec id="Ch1.S3.SS6">
  <label>3.6</label><title>Performance metrics</title>
      <p id="d2e2567">In addition to the FI and SHAP value analysis, several performance metrics were used to validate XGBoost SD predictions with measured SD. For each configuration and across all outer resampling predicting sets (thus the total dataset), we computed the spatio-temporal Pearson correlation coefficient (<inline-formula><mml:math id="M114" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>), mean absolute error (MAE), root mean squared error (RMSE) and bias between predicted and measured SD (all averaged over time and space). Since cross-validation is conducted in both space and time, the performance metrics reflect the ML model’s ability to generalize across purely spatial, purely temporal, and combined spatio-temporal domains. Additionally, certain metrics were calculated on a per-site basis, such as the MAE.</p>
      <p id="d2e2577">Next, we evaluated XGBoost’s capability to generate spatial SD predictions by comparing them with the photogrammetry snow surveys conducted in the Dischma Valley, Switzerland. For this case, we trained XGBoost exclusively on stationary and point-based measurements, excluding spatial data from the snow surveys. Model training and hyperparameter tuning were performed using fivefold spatial CV, as this approach best reflects the intended application of the ML model: predicting SD on unseen locations across the European Alps within the time period of our S1 data collection. After training, XGBoost was applied to predict SD for each of the nine snow surveys, and performance metrics were computed.</p>
      <p id="d2e2580">We then repeated this process, but now incorporating all snow survey data except those of the targeted date into the training dataset. This resulted in nine independently trained and tuned XGBoost models, each applied to predict SD for the corresponding unseen snow survey. In this approach, we also employed spatial CV for training and tuning, where every training snow survey was randomly assigned to one of the five folds. This ensured that the distribution of training and validation data remained consistent across folds.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results and discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Performance of ML configurations with S1 PolSAR and backscatter intensity variables</title>
      <p id="d2e2599">In general, all configurations (i.e., PolSAR<sub>ML</sub>, Backscatter<sub>ML</sub> and Combination<sub>ML</sub>) achieve best results within the temporal nested CV framework (Table <xref ref-type="table" rid="TE1"/>), and performance progressively deteriorates in the spatial and spatio-temporal frameworks (Table <xref ref-type="table" rid="T3"/>). This behavior is expected, as SD patterns within the same area (i.e., at the same sites) tend to recur across different years, such that SD prediction for an unseen snow season (i.e., the temporal framework) is inherently more favorable for XGBoost than prediction at unobserved locations (i.e., the spatial framework). Predicting at unobserved locations and during unseen snow seasons (i.e., the spatio-temporal framework), including times outside the study period is even more challenging, as XGBoost cannot exploit season-specific information from the training data nor rely on recurrent site-specific SD patterns. Consequently, because the intended application of XGBoost is to predict SD at previously unseen locations across the European Alps within the training dataset time period (e.g., Fig. <xref ref-type="fig" rid="F3"/>a), reliance on the temporal framework would lead to an overly optimistic evaluation of model performance, whereas the spatio-temporal framework would provide a more conservative assessment.</p>

<table-wrap id="T3" specific-use="star"><label>Table 3</label><caption><p id="d2e2621">Overall performance metrics for the PolSAR<sub>ML</sub>, Backscatter<sub>ML</sub> and Combination<sub>ML</sub> configurations for the spatial and spatio-temporal nested CV frameworks, when evaluated over all sites displayed in Fig. <xref ref-type="fig" rid="F1"/>. The values inside the brackets denote the metric values when zero-measured SD are included in the evaluation.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <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:colspec colnum="4" colname="col4" align="right" colsep="1"/>
     <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:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" namest="col2" nameend="col4" align="center" colsep="1">Spatial </oasis:entry>
         <oasis:entry rowsep="1" namest="col5" nameend="col7" align="center">Spatio-temporal </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Metric</oasis:entry>
         <oasis:entry colname="col2">PolSAR<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col3">Backscatter<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col4">Combination<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col5">PolSAR<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col6">Backscatter<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col7">Combination<sub>ML</sub></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M115" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> [–]</oasis:entry>
         <oasis:entry colname="col2">0.73 (0.81)</oasis:entry>
         <oasis:entry colname="col3">0.73 (0.81)</oasis:entry>
         <oasis:entry colname="col4">0.74 (0.82)</oasis:entry>
         <oasis:entry colname="col5">0.70 (0.79)</oasis:entry>
         <oasis:entry colname="col6">0.69 (0.79)</oasis:entry>
         <oasis:entry colname="col7">0.70 (0.79)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RMSE [m]</oasis:entry>
         <oasis:entry colname="col2">0.53 (0.41)</oasis:entry>
         <oasis:entry colname="col3">0.53 (0.42)</oasis:entry>
         <oasis:entry colname="col4">0.52 (0.41)</oasis:entry>
         <oasis:entry colname="col5">0.55 (0.43)</oasis:entry>
         <oasis:entry colname="col6">0.56 (0.44)</oasis:entry>
         <oasis:entry colname="col7">0.55 (0.43)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MAE [m]</oasis:entry>
         <oasis:entry colname="col2">0.35 (0.23)</oasis:entry>
         <oasis:entry colname="col3">0.35 (0.23)</oasis:entry>
         <oasis:entry colname="col4">0.35 (0.22)</oasis:entry>
         <oasis:entry colname="col5">0.37 (0.24)</oasis:entry>
         <oasis:entry colname="col6">0.37 (0.24)</oasis:entry>
         <oasis:entry colname="col7">0.37 (0.24)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">bias [m]</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (0.00)</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.00</mml:mn></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (0.00)</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (0.00)</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (0.00)</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (0.00)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e2881">Spatial SD estimate and underestimation of the Combination<sub>ML</sub> configuration. <bold>(a)</bold> Prediction on 18 January 2018 encompassing both an ascending and descending S1 observation, derived as the mean SD from the five XGBoost models trained within the spatial nested CV framework. Observations are indicated by dots and squares, with squares representing sites exhibiting a <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mtext>site-bias</mml:mtext><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m for this framework <bold>(</bold>displayed in <bold>b)</bold>. Estimates over Austria are highlighted to indicate an area of SD underestimation errors (yellow square) attributable to errors in the FSC input feature. <bold>(b)</bold> Measurement stations exhibiting a mean site <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mtext>bias</mml:mtext><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m within the spatial nested CV framework (zero-measured SD excluded). Sites with fewer than 10 observations are excluded. Colors indicate the configurations for which this underestimation occurs. Across the displayed sites, 23 % of the observed SD measurements <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> m, compared to only 2 % across the full training dataset.</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f03.jpg"/>

        </fig>

      <p id="d2e2945">The absolute improvements of using PolSAR observations, as a replacement for (or in combination with) backscatter intensities, are small within all nested CV frameworks, or even minimal within some CV frameworks. Within the spatial framework, the PolSAR<sub>ML</sub> and Backscatter<sub>ML</sub> configurations display marginal differences in overall performance metrics (Table <xref ref-type="table" rid="T3"/>), which likely stems from the similar relationship of the variables with SD, and the spatial noise present in both types of S1 variables. The Combination<sub>ML</sub> configuration also shows similar overall performance compared to the Backscatter<sub>ML</sub> configuration, yet the improvements in MAE, computed per site, are significant (<inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>≪</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>, 95 % confidence level), resulting in an overall MAE of 35 cm, a mean site-MAE of 29 cm, and a mean site-bias of <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">11</mml:mn></mml:mrow></mml:math></inline-formula> mm (excluding zero-measured SD). PolSAR observations moreover improve model performance for the spatio-temporal framework, with significant improvements in site-MAE for both the PolSAR<sub>ML</sub> and Combination<sub>ML</sub> configurations (<inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>≪</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>, 95 % confidence interval). This improvement suggests that PolSAR observations, alone or in combination with backscatter intensities, more effectively capture the seasonal evolution of SD, a conclusion that is further supported by statistically significant gains in site-MAE (<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>≪</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>, 95 % confidence level) observed in the temporal nested CV framework. Nonetheless, also here the overall improvements remain limited, and the increased computational cost of processing S1 SLC data into PolSAR variables relative to deriving backscatter intensity from GRD data must be considered. Indeed, besides requiring separate processing chains to retrieve <inline-formula><mml:math id="M130" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from the C2-matrix (Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>), handling SLC data is more demanding, with raw images (<inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> Gb) substantially larger than GRD products (<inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> Gb).</p>
      <p id="d2e3056">Additionally, all three configurations exhibit difficulties in predicting high SD values at unobserved sites (Fig. <xref ref-type="fig" rid="F3"/>), which likely arises from the scarcity of high SD observations in the training dataset (Fig. <xref ref-type="fig" rid="FE1"/>a). For the spatial nested CV framework, the PolSAR<sub>ML</sub>, Backscatter<sub>ML</sub> and Combination<sub>ML</sub> configurations exhibit a bias of <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.46</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.51</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.48</mml:mn></mml:mrow></mml:math></inline-formula> m for observed <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mtext>SD</mml:mtext><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> m, which further deteriorates in the spatio-temporal framework. This is also visible in Fig. <xref ref-type="fig" rid="F3"/>a, when comparing the observations (squares) with the SD prediction, and in Fig. <xref ref-type="fig" rid="F3"/>b, that displays sites with a <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mtext>bias</mml:mtext><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m for the different configurations within the spatial nested CV framework (zero-measured SD excluded). Interestingly, many of the sites displayed in Fig. <xref ref-type="fig" rid="F3"/>b also appear to have strong negative biases in Fig. 2a of <xref ref-type="bibr" rid="bib1.bibx30" id="text.87"/>. Consequently, the reduced ability of XGBoost models, trained with S1 variables to explain interannual and site-specific variability, to predict high SD values must be taken into account when deploying the model across the European Alps, particularly when applying it beyond the temporal range covered by the training data.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Feature importance for ML configurations with S1 PolSAR and backscatter intensity variables</title>
      <p id="d2e3147">Across the configurations and nested CV frameworks, FSC and elevation consistently emerge as the most important features, similar to what has been reported by <xref ref-type="bibr" rid="bib1.bibx30" id="text.88"/>, indicated by both XGBoost’s internal <italic>gain</italic> metric and SHAP values (Fig. <xref ref-type="fig" rid="F4"/>a and b). FSC is particularly important, which makes the predictions prone to potential errors in this input feature (e.g., the high-alpine area in the yellow box in Fig. <xref ref-type="fig" rid="F3"/>a, where erroneously low FSC-values led to SD underestimation). The <italic>gain</italic> FI (Fig. <xref ref-type="fig" rid="F4"/>a) moreover indicates an increasing FSC importance when transitioning from temporal to spatio-temporal nested CV frameworks (<inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula> % to <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> %), with an opposite trend for elevation (<inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> % to <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> %). When predicting at unseen locations, XGBoost seems to rely more heavily on FSC to distinguish snow-covered periods, and cannot rely as much on recurring SD patterns that display a strong relationship with elevation. Finally, the DOY features, which help capturing the seasonal variations in the estimates, also emerge as important inputs, as reflected across the configurations in both Fig. <xref ref-type="fig" rid="F4"/>a and b.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e3210">Feature importance for the PolSAR<sub>ML</sub>, Backscatter<sub>ML</sub> and Combination<sub>ML</sub> configurations, indicating the strong influence of FSC, elevation and DOY on the model outcome <bold>(a, b)</bold>, the elevated usage of <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> during SD prediction <bold>(b)</bold>, and the preference of the Combination<sub>ML</sub> configuration for <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> over <inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> <bold>(a, b)</bold>. Upper row <bold>(a)</bold>: Relative gain-based FI. Bars represent the mean FI across the XGBoost models trained during inner resampling, with colors indicating the type of nested CV framework. Lower row <bold>(b)</bold>: Similar to <bold>(a)</bold>, but here FI is quantified as the mean absolute SHAP value per feature (relative values), computed separately for each test fold during outer resampling. The black lines in the bars denote the 95 % confidence interval.</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f04.png"/>

        </fig>

      <p id="d2e3299">When used in the separate configurations, the S1 PolSAR and backscatter intensity features are similarly used during model training (Fig. <xref ref-type="fig" rid="F4"/>a). However, the <italic>gain</italic> FI indicates a stronger importance of <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> within the PolSAR<sub>ML</sub> configuration over <inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> in the Backscatter<sub>ML</sub> one. This observation is further confirmed in Fig. <xref ref-type="fig" rid="F4"/>b across all nested CV frameworks, indicating that XGBoost seems to effectively extract more information from <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> during model training and SD prediction. Consistent with this finding, the Combination<sub>ML</sub> configuration also exhibits a clear preference of <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> over <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>. In addition, both the <italic>gain</italic>-based and SHAP value FI analyses reveal a less distinct separation between the S1 input features in the Backscatter<sub>ML</sub> configuration, with the SHAP values even suggesting that <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> contributes as much as, or slightly more than, <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> during SD prediction at unseen locations and/or time periods.</p>
<sec id="Ch1.S4.SS2.SSSx1" specific-use="unnumbered">
  <title>SHAP value analysis during snowpack presence</title>
      <p id="d2e3417">The SHAP value FI of the S1 variables (Fig. <xref ref-type="fig" rid="F4"/>b) were further evaluated during snow-covered periods – encompassing both wet and dry snow periods – within the spatial nested CV framework, as this framework matches best with the objective of the study: SD prediction across the Alps using the available S1 archive. Figure <xref ref-type="fig" rid="F5"/>a presents the FI for both the full set of predictions (fully colored bars), and the subset remaining after excluding the non-valid areas masked within the wet snow product (dark gray lines). Excluding the non-valid areas increases the overall and dry-period FI for both <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> within the PolSAR<sub>ML</sub> and Backscatter<sub>ML</sub> configuration, respectively. As these non-valid areas include low-elevation areas (i.e., valleys) and densely-forested regions, locations where typically low SD values are observed, these results suggests that XGBoost places relatively more importance on these S1 variables at bare, higher-elevation locations that are often characterized by deeper snowpacks. Conversely, the decrease in SHAP value FI when including these non-valid areas indicates the limited added value of the S1 variables to predict SD at low-elevation and/or densely-forested sites. Although no valid wet-snow classification is available for such areas (e.g., Fig. <xref ref-type="fig" rid="F5"/>d where only low FCF values appear for the wet-snow subplot) and more advanced classification approaches incorporating meteorological data could enable a more accurate separation of dry and wet snow periods, we argue that the current analysis is sufficient given the limited contribution of S1 variables in these environments. This marginal contribution was also reported by <xref ref-type="bibr" rid="bib1.bibx30" id="text.89"/> and is further evident in Fig. <xref ref-type="fig" rid="FC1"/>d. As this limitation arises from the raw S1 observations rather than the type of processed S1 observations (i.e., PolSAR vs. backscatter intensities), this limitation should be addressed by incorporating additional input features (e.g., Fig. <xref ref-type="fig" rid="FC2"/>).</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e3466">SHAP value analysis for the spatial nested CV framework during snow presence, indicating XGBoost's stronger reliance of, and preference for, <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> compared to <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>, and the notable use of <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> during wet snow periods. <bold>(a)</bold> Relative SHAP value FI of the satellite input features for the PolSAR<sub>ML</sub>, Backscatter<sub>ML</sub> and Combination<sub>ML</sub> configurations. The dark gray lines represent the FI after masking out non-valid dry snow classifications. <bold>(b)</bold> Scatter plot of mean <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> values and corresponding SHAP values for the PolSAR<sub>ML</sub> configuration, taken as the mean per site and snow season during dry and wet snow conditions (only valid classifications). The dots are colored according to the mean predicted SD (SD<sub>pred</sub>). <bold>(c)</bold> Same as <bold>(b)</bold>, but for <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> within the Backscatter<sub>ML</sub> configuration.  <bold>(d)</bold> Same as  <bold>(c)</bold> for <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>, but colorized to the site FCF, indicating that the classification primarily targets higher-elevation non-forested areas.</p></caption>
            <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f05.png"/>

          </fig>

      <p id="d2e3594">Figure <xref ref-type="fig" rid="F5"/>a also explains the more pronounced difference in SHAP value FI between the PolSAR variables, as XGBoost relies more heavily on <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> than on <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mi mathvariant="normal">s</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> across all snow conditions. In contrast, the Backscatter<sub>ML</sub> configuration places greater emphasis on <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> than on <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> during wet snow conditions, which accounts for their nearly equivalent overall SHAP value FI (Fig. <xref ref-type="fig" rid="F4"/>). In addition, the FI patterns observed in the Combination<sub>ML</sub> configuration closely resemble those of the PolSAR<sub>ML</sub> and Backscatter<sub>ML</sub> configurations, with the notable exception of <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>. Here, XGBoost seems to rely more heavily on <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> at the expense of <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>, which was also evident from Fig. <xref ref-type="fig" rid="F4"/>, and is also observed at a measurement site located near Prato, Switzerland (46.47° N, 8.72° E; Fig. <xref ref-type="fig" rid="FC1"/>c). Similar observations were made by <xref ref-type="bibr" rid="bib1.bibx45" id="text.90"/>, who reported stronger correlations between <inline-formula><mml:math id="M170" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and modeled SD during the accumulation (dry snow) period at most locations in their study area than between modeled SD and <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>. In addition, <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> shows a similar SHAP value FI importance as <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> during dry snow conditions (Fig. <xref ref-type="fig" rid="F5"/>a, Combination<sub>ML</sub> configuration), and is even more important at bare high-elevation sites (dark gray lines), further confirming the findings of <xref ref-type="bibr" rid="bib1.bibx45" id="text.91"/>. In contrast, <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is more extensively used during wet snow conditions, resulting in the slightly higher observed overall FI for this S1 variable.</p>
      <p id="d2e3772">Within the PolSAR<sub>ML</sub> configuration (Fig. <xref ref-type="fig" rid="F5"/>b), XGBoost has learned a positive relationship between <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and its contribution to the SD estimates, consistent with the findings of <xref ref-type="bibr" rid="bib1.bibx45" id="text.92"/>, who reported increasing <inline-formula><mml:math id="M176" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-values with dry snowpack accumulation at sites where the S1 signal penetrates the snowpack at oblique incidence angles (medium to high LIA). However, at certain medium–high elevation sites (1500–2500 m; e.g., Fig. <xref ref-type="fig" rid="FC1"/>b), both <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and its SHAP value contributions remain low or even negative (Fig. <xref ref-type="fig" rid="FC1"/>b) despite relatively high predicted and observed SD. Instead, increases in <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:msubsup><mml:mi>S</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mi mathvariant="normal">s</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> are observed, a pattern shown to be more prevalent at sites with low-LIA satellite overpasses <xref ref-type="bibr" rid="bib1.bibx45" id="paren.93"/> where the S1 signal penetrates the snowpack more vertically and decreasing <inline-formula><mml:math id="M180" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-values are observed. Nevertheless, these patterns may also occur at locations with medium-LIA S1 observations (e.g., the site in Fig. <xref ref-type="fig" rid="FC1"/>b that shows increasing <inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>-values) and further research is required to understand their origin. In addition, these patterns help explain the dual relationship observed for <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> in Fig. <xref ref-type="fig" rid="F5"/>c: at certain locations, a limited positive contribution is found, whereas at the majority of sites, a strong inverse relationship emerges during wet snow conditions, when a decrease in this S1 variable is typically observed (e.g., Fig. <xref ref-type="fig" rid="FC1"/>a). Finally, Fig. <xref ref-type="fig" rid="F5"/>b and d illustrate that under wet snow conditions, <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> remains more elevated compared to <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>, leading to higher associated <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> SHAP values in the PolSAR<sub>ML</sub> configuration than the corresponding <inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> SHAP values in the Backscatter<sub>ML</sub> configuration. This suggests that SD estimation based on <inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> might be less sensitive to the presence of liquid water than SD estimation based on <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Added value of meteorological forcings and <italic>Snowclim</italic> SD estimates</title>
      <p id="d2e3981">Figure <xref ref-type="fig" rid="F6"/> illustrates the improvements when incorporating either regionally downscaled meteorological forcing data or <italic>Snowclim</italic> SD estimates (Table <xref ref-type="table" rid="T2"/>; Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations) when predicting at unseen locations (and time periods; Fig. <xref ref-type="fig" rid="F6"/>a and b), with the most important improvements for high SD observations (<inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> m). The bias for observations <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> m improves by 28 cm when comparing the Weather<sub>ML</sub> to the Combination<sub>ML</sub> configuration within the spatial nested CV framework (Fig. <xref ref-type="fig" rid="F6"/>a), decreasing from <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.48</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.20</mml:mn></mml:mrow></mml:math></inline-formula> m. Incorporating <italic>Snowclim</italic> SD estimates further reduces this bias to <inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.12</mml:mn></mml:mrow></mml:math></inline-formula> m, likely reflecting a stronger correspondence between the <italic>Snowclim</italic> estimates and high SD observations than what is captured through derived meteorological variables. Despite these gains, the number of sites with a mean bias <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m remains similar in both the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations – with most of these sites again located in Switzerland (Fig. <xref ref-type="fig" rid="FE2"/>) – reflecting the need for expanded high SD data collection. Furthermore, while the inclusion of meteorological forcing data or modeled SD estimates reduces the relative SHAP value FI of the S1 input features, these features continue to influence SD predictions (Fig. <xref ref-type="fig" rid="F6"/>d), accounting in total for approximately 9 % and 7 % of the SHAP value FI in the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations, respectively, when predicting at unseen locations.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e4103">Improvements brought by additional input of meteorological forcing data or <italic>Snowclim</italic> SD estimates when predicting at unseen locations and time periods. <bold>(a)</bold> 2D histograms of measured vs. predicted SD for the Combination<sub>ML</sub>, Weather<sub>ML</sub>, and <italic>Snowclim</italic><sub>ML</sub> configurations for the spatial nested CV framework. Performance metrics are computed with exclusion of zero-measured SD. <bold>(b)</bold> Same as <bold>(a)</bold>, but for the spatio-temporal framework.  <bold>(c)</bold> 7 d mean bias (including zero-measured SD) over the course of a general snow season, for different elevation classes.  <bold>(d)</bold> Relative SHAP value FI for the different configurations for the spatial (full colored bars) and the spatio-temporal nested CV framework (gray line).</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f06.png"/>

        </fig>

      <p id="d2e4142">Overall, the <italic>Snowclim</italic><sub>ML</sub> configuration yields the best performance (Fig. <xref ref-type="fig" rid="F6"/>a and b). Under the spatio-temporal nested CV framework, site-MAE during snow-covered periods decreases by at least 2.5 cm at 55 % of sites, while only 16 % exhibit an increase of 2.5 cm or more, relative to the Combination<sub>ML</sub> configuration. Compared to the Weather<sub>ML</sub> configuration, the difference in site-MAE is minimal, and only significant for the spatio-temporal framework. However, the <italic>Snowclim</italic> SD estimates appear to more accurately represent conditions at low-elevation sites (<inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula> m) during the early snow season (Fig. <xref ref-type="fig" rid="F6"/>c), highlighting the importance of reliable FSC information to correctly indicate snow-free conditions when relying solely on meteorological forcing data. In addition, while the Weather<sub>ML</sub> configuration displays the lowest bias of the three configurations at medium-elevation (1000–2500 m) sites (Fig. <xref ref-type="fig" rid="F6"/>c), the <italic>Snowclim</italic><sub>ML</sub> configuration still performs best at high-elevation sites (<inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">2500</mml:mn></mml:mrow></mml:math></inline-formula> m) during peak SD and the ablation period. Nonetheless, both the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations seem to underestimate SD near March–May, with the differences being less pronounced for the 1500–2500 m elevation class. As such, the results indicate that directly using meteorological forcings can achieve comparable predictive performance within the applied XGBoost setup. This would eliminate the need to run a snow model, which reduces both computational cost and model complexity.</p>
</sec>
<sec id="Ch1.S4.SS4">
  <label>4.4</label><title>Spatial SD prediction</title>
      <p id="d2e4211">To address the findings of <xref ref-type="bibr" rid="bib1.bibx53" id="text.94"/> and <xref ref-type="bibr" rid="bib1.bibx64" id="text.95"/>, who emphasized that stationary and point-based SD measurements inadequately capture spatial snowpack variability, we trained the Combination<sub>ML</sub>, Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations with additional spatially distributed SD training (survey) data, and compared its impact over the Dischma valley. Figure <xref ref-type="fig" rid="F7"/>a–c display the results of the 16 March 2017 snow survey (Fig. <xref ref-type="fig" rid="F7"/>d), in which mountain ridges appear more distinctly in the predictions, and high SD estimates at steep locations and near ridges are more accurately corrected compared to Fig. <xref ref-type="fig" rid="FE3"/>a–e, which depict results obtained without spatial training data. Negative adjustments can be observed at high-elevation areas with (relatively) steep slopes for all configurations, but is most pronounced for the Combination<sub>ML</sub> configuration (Appendix <xref ref-type="sec" rid="App1.Ch1.S4"/>). For the latter, the negative corrections are reflected in a reduced SHAP value FI of the topographic inputs (Fig. <xref ref-type="fig" rid="F7"/>h, survey data; Appendix <xref ref-type="sec" rid="App1.Ch1.S4"/>). In contrast, the SHAP value FI of the topographic inputs increases in the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations (Fig. <xref ref-type="fig" rid="F7"/>i and j). Here, the topographic features contributed less when the models were trained solely on point-based measurements but become increasingly influential once spatial training data are included, enabling improved representation of topographic controls on the SD estimates. Notably, <inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> remains among the more influential features for these configurations, indicating that despite its reduced relative importance, the inclusion of this S1 variable (and potentially other S1 variables) continues to affect the final SD predictions.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e4271">Improvements obtained by incorporating spatially distributed SD training data when predicting across the Dischma Valley (Switzerland), including their impact on SHAP-based FI. The first column <bold>(a, e, h)</bold> represents the results for the Combination<sub>ML</sub> configuration, while the second <bold>(b, f, i)</bold> and third column <bold>(c, g, j)</bold> show the results for the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations, respectively. <bold>(a)</bold>, <bold>(b)</bold> and <bold>(c)</bold> display the spatial predictions for the 16 March 2017 snow survey, with <bold>(d)</bold> representing the measured SD.  <bold>(e)</bold>, <bold>(f)</bold> and  <bold>(g)</bold> show 2D histograms and performance metrics across all nine conducted snow surveys. Finally,  <bold>(h)</bold>,  <bold>(i)</bold> and  <bold>(j)</bold> display relative SHAP value FI, both when trained with or without spatial SD (survey) data. The 95 % confidence interval is indicated with a red bar.</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f07.jpg"/>

        </fig>

      <p id="d2e4332">Despite the improvements, SD remains overestimated for the 16 March 2017 snow survey across all configurations. This overestimation is most pronounced for the Combination<sub>ML</sub> configuration and exceeds the bias reported by <xref ref-type="bibr" rid="bib1.bibx30" id="text.96"/>. Although it is not the objective of this study to perform a direct comparison, the persistence of the Combination<sub>ML</sub> bias indicates potential limitations in the current feature selection or training dataset. Nonetheless, both the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations outperform the results reported by <xref ref-type="bibr" rid="bib1.bibx30" id="text.97"/>. For the 9 March 2016 and 16 March 2017 snow surveys used by <xref ref-type="bibr" rid="bib1.bibx30" id="text.98"/> for model validation, the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations achieve higher correlation coefficients (0.68 and 0.64) and lower mean absolute errors (31 and 36 cm, respectively) than those reported by <xref ref-type="bibr" rid="bib1.bibx30" id="text.99"/> (0.56 and 41 cm). For the 16 March 2017 survey specifically, <xref ref-type="bibr" rid="bib1.bibx30" id="text.100"/> reported a mean SD difference (predicted minus observed) of 16 cm, whereas the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations exhibit differences of <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> and 15 cm, respectively. Thereby, the more pronounced overestimation of the <italic>Snowclim</italic><sub>ML</sub> configuration likely results from the systematic overestimation in the <italic>Snowclim</italic> SD estimates for this survey (Fig. <xref ref-type="fig" rid="FD2"/>d), which may also explain the 6 cm higher MAE compared to the Weather<sub>ML</sub> configuration (Fig. <xref ref-type="fig" rid="F7"/>b and c).</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e4411">Improved representation of topographical controls on SD estimates for the Weather<sub>ML</sub> configuration on 29 January 2018 over the Ötztal, Austria (top row) and the Lötschental, Switzerland (bottom row). <bold>(a, e)</bold> Mean SD estimates predicted with the nine separately trained XGBoost models utilizing no spatial (No survey) training data. <bold>(b, f)</bold> Same as <bold>(a, e)</bold>, but with inclusion of spatial SD training data (Survey).  <bold>(c, g)</bold> Difference maps between the mean SD predictions, trained with and without spatial SD training data.  <bold>(d, h)</bold> Scatter plots of TPI and SD differences, colored according to slope. Observed SD at the stationary sites are displayed in <bold>(a)</bold>,  <bold>(b)</bold>,  <bold>(e)</bold> and  <bold>(f)</bold> as dots. Glaciers and lakes located within the valleys are colored in white and dark gray, respectively, and are excluded from the analyses.</p></caption>
          <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f08.jpg"/>

        </fig>

      <p id="d2e4451">Across the nine snow surveys, the inclusion of spatially distributed SD training data primarily improves predictions for lower observed SD values (Fig. <xref ref-type="fig" rid="F7"/> and <xref ref-type="fig" rid="FE3"/>e–g), whereas differences for higher SD observations (<inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> m) remain less pronounced, albeit best captured by the <italic>Snowclim</italic><sub>ML</sub> configuration. Despite a persistent positive bias across all configurations, the Weather<sub>ML</sub> configuration exhibits a bias reduction of approximately 10 cm relative to the <italic>Snowclim</italic><sub>ML</sub> configuration, suggesting that explicitly running <italic>Snowclim</italic> may not be required when the primary objective is to obtain accurate SD estimates across the European Alps. Indeed, XGBoost effectively learns the relationship between the meteorological forcing data and observed SD, without explicitly representing the physical processes governing snowpack evolution. For the <italic>Snowclim</italic><sub>ML</sub> configuration, the remaining overestimation largely originates from biases in the <italic>Snowclim</italic> SD estimates themselves (Figs. <xref ref-type="fig" rid="FB1"/>b and <xref ref-type="fig" rid="FD2"/>d). In contrast, the origin of the positive bias in the Weather<sub>ML</sub> configuration is less straightforward and may reflect either an overestimation of cumulative snowfall (<inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mtext>s,c</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) or limitations in XGBoost’s ability to implicitly represent variations in snow bulk density. In the latter case, even accurate snowfall forcing may still result in SD overestimation due to an implicit underrepresentation of snow densification processes. Further research should attempt to include factors or use ML models that govern variations in snow density, especially to enhance the potential of predicting short-term variations in SD. Finally, elevation mismatches within the relatively coarse 500 m meteorological forcing data may introduce temperature biases, thereby affecting snowfall estimates and the inferred number of melt days.</p>
      <p id="d2e4512">Figure <xref ref-type="fig" rid="F8"/> further illustrates the impact of the spatial training data outside the Dischma valley. The top row displays the SD estimates across the Ötztal region (Austria) on 29 January 2018, while the bottom row showcases the results for the Lötschental region (Switzerland), on the same date. For both valleys, the inclusion of spatial training data improved the spatial patterns, manifested by the appearance of mountain ridges and local depressions (Fig. <xref ref-type="fig" rid="F8"/>b and f). These patterns also appear in the difference maps (Fig. <xref ref-type="fig" rid="F8"/>c and g), and seem to be related to the TPI (Fig. <xref ref-type="fig" rid="F8"/>d and h). Specifically, Fig. <xref ref-type="fig" rid="F8"/>d and h indicate that SD estimates at areas situated below their surroundings (negative TPI) are positively corrected, whereas the opposite is true near mountain ridges. Figure <xref ref-type="fig" rid="F8"/>d and h moreover indicate a dependency with the slope of the area, with steeper areas exhibiting more pronounced negative corrections, while flatter regions show the opposite tendency. The relationship with the other topographic features (e.g., aspect), however, is less clear.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d2e4538">An extreme gradient boosting model (XGBoost) was applied to assess whether the integration of Sentinel-1 (S1) C-band synthetic aperture radar (SAR) dual-polarized polarimetric (PolSAR) observations – either as a replacement for, or in combination with S1 backscatter intensity observations – improves SD predictions across the European Alps relative to a backscatter-intensity-based configuration. In addition, two extended configurations were evaluated in which the S1 observations were supplemented with either meteorological forcing data or SD estimates from the process-based <italic>Snowclim</italic> model, to assess both the associated performance gains and the continued contribution of S1 observations to SD prediction. Results were evaluated at locations and/or during time periods not covered by the training data using a threefold nested cross-validation (nested CV) scheme, while feature importance analysis was employed to assess the contribution of the different input variables during both dry and wet snow periods. In addition, nine photogrammetry snow surveys were used to validate the spatial prediction capacity of the configurations.</p>
      <p id="d2e4544">Our results show modest improvements in estimated SD with the inclusion of S1 C-band PolSAR observations, with gains primarily observed in site-level performance under spatio-temporal generalization, whereas no significant improvements are found in these metrics under spatial generalization alone. However, feature importance analysis indicates a stronger reliance on the polarimetric scattering angle (<inline-formula><mml:math id="M201" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>) than the cross-polarization ratio (<inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>), during both dry and wet snow periods, while the drop in co-polarized (VV) backscatter intensity (<inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>vv</mml:mtext><mml:mn mathvariant="normal">0</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>) seems to be actively used during the ablation period. Incorporating meteorological forcing data or <italic>Snowclim</italic> SD estimates further improved XGBoost's performance substantially, while the model continued to make use of information from the S1 observations, particularly <inline-formula><mml:math id="M204" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>. Nonetheless, high SD observations remain systematically underestimated, primarily due to their limited representation in the training dataset. Finally, our results depict the importance of spatially distributed SD training data to capture topographic variability, reflected through a negative relationship between topographic position index (TPI) and adjustments in SD estimates relative to predictions from XGBoost trained without spatial training data.</p>
      <p id="d2e4590">Despite these advances, SD values above approximately 2.5 m remain underestimated, emphasizing the need for more extensive snow monitoring and additional spatial snow surveys within the European Alps. Furthermore, XGBoost operates at the pixel level and cannot inherently capture dependencies between adjacent pixels; instead, spatial context must be explicitly incorporated through engineered features. Finally, while improving SD estimates is a step toward addressing snow mass knowledge gaps, future research should focus on direct snow mass estimation and integrating spatial dependencies through methods that incorporate information from adjacent pixels.</p>
</sec>

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

<app id="App1.Ch1.S1">
  <label>Appendix A</label><title>Combining Terra and Aqua fractional snow cover data</title>
      <p id="d2e4604">To generate a combined daily fractional snow cover (FSC) product from the MODIS Terra and Aqua satellites, we applied a weighted averaging approach to merge the individual satellite observations. As such, we calculated for each location <inline-formula><mml:math id="M205" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and day <inline-formula><mml:math id="M206" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> the weights of the individual FSC data (<inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi>W</mml:mi><mml:mrow><mml:msub><mml:mtext>sat</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) using the following formula:

              <disp-formula id="App1.Ch1.S1.E4" content-type="numbered"><label>A1</label><mml:math id="M208" display="block"><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>W</mml:mi><mml:mrow><mml:msub><mml:mtext>sat</mml:mtext><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mi>W</mml:mi><mml:mtext>QA</mml:mtext></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mi>W</mml:mi><mml:mtext>CP</mml:mtext></mml:msub><mml:mo>⋅</mml:mo><mml:msub><mml:mi>W</mml:mi><mml:mtext>DD</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

        
        in which <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:msub><mml:mi>W</mml:mi><mml:mtext>QA</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the weight associated with the quality flag (QA, that ranges between 0 and 2 with 0 indicating the highest quality) of the satellite data; <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:msub><mml:mi>W</mml:mi><mml:mtext>CP</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the weight based on the number of days since the last cloud-free observation (CP; values between 0 and <inline-formula><mml:math id="M211" display="inline"><mml:mi mathvariant="normal">∞</mml:mi></mml:math></inline-formula>); and <inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:msub><mml:mi>W</mml:mi><mml:mtext>DD</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the weight accounting for the difference in days between the most recent cloud-free Terra and Aqua observations (DD; values between 0 and <inline-formula><mml:math id="M213" display="inline"><mml:mi mathvariant="normal">∞</mml:mi></mml:math></inline-formula>, where 0 corresponds to the satellite with the most recent cloud-free data). The individual weights were computed using the following formulations, which were designed to ensure that none of the weights attain zero:

              <disp-formula specific-use="align" content-type="numbered"><mml:math id="M214" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="App1.Ch1.S1.E5"><mml:mtd><mml:mtext>A2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>W</mml:mi><mml:mtext>QA</mml:mtext></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mtext>QA</mml:mtext><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo><mml:mtext>QA</mml:mtext><mml:mo>)</mml:mo></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="App1.Ch1.S1.E6"><mml:mtd><mml:mtext>A3</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>W</mml:mi><mml:mtext>CP</mml:mtext></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mtext>CP</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><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:mlabeledtr><mml:mlabeledtr id="App1.Ch1.S1.E7"><mml:mtd><mml:mtext>A4</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>W</mml:mi><mml:mtext>DD</mml:mtext></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mtext>DD</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula></p>
</app>

<app id="App1.Ch1.S2">
  <label>Appendix B</label><title><italic>Snowclim</italic> parameter settings and performance</title>
      <p id="d2e4865"><italic>Snowclim</italic> model parameters were calibrated with a two-step approach, involving a subset of the snow dataset. First, we identified the best working downscaling techniques – multiple options were assessed to downscale temperature, precipitation, relative humidity, and downward shortwave radiation – by comparing model performance with measured SD using the standard parameter set used by <xref ref-type="bibr" rid="bib1.bibx56" id="text.101"/> (Table 2, superscript <sup>c</sup>) in their full model run. Next, we used the downscaled forcing data to select the optimal parameters out of 1276 tested combinations, by applying a similar approach as described in <xref ref-type="bibr" rid="bib1.bibx56" id="text.102"/>. A list of the final calibrated parameters is provided in Table <xref ref-type="table" rid="TB1"/>.</p>

<table-wrap id="TB1" specific-use="star"><label>Table B1</label><caption><p id="d2e4884">Parameter settings used to generate SD estimates across the European Alps. For the detailed description of the separate parameters, we refer to <xref ref-type="bibr" rid="bib1.bibx56" id="text.103"/>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Parameter</oasis:entry>
         <oasis:entry colname="col2">Abbreviated name</oasis:entry>
         <oasis:entry colname="col3">Calibrated values/methods</oasis:entry>
         <oasis:entry colname="col4">Units</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Albedo algorithm</oasis:entry>
         <oasis:entry colname="col2"><italic>albedo_opt</italic></oasis:entry>
         <oasis:entry colname="col3">Essery<sup>*</sup></oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Momentum roughness length</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">m</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Heat and vapor roughness length</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">m</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Maximum albedo</oasis:entry>
         <oasis:entry colname="col2"><italic>albedo_max</italic></oasis:entry>
         <oasis:entry colname="col3">0.90</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Maximum liquid water fraction</oasis:entry>
         <oasis:entry colname="col2"><italic>lw_max</italic></oasis:entry>
         <oasis:entry colname="col3">0.1</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Windless heat exchange coefficient</oasis:entry>
         <oasis:entry colname="col2"><italic>E0</italic></oasis:entry>
         <oasis:entry colname="col3">1</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M219" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">Wm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">K</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Windless heat exchange coefficient flux application</oasis:entry>
         <oasis:entry colname="col2"><italic>E0_app</italic></oasis:entry>
         <oasis:entry colname="col3">1</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Windless heat exchange coefficient stability condition</oasis:entry>
         <oasis:entry colname="col2"><italic>E0_stability</italic></oasis:entry>
         <oasis:entry colname="col3">2</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cold content threshold at which to start energy tax</oasis:entry>
         <oasis:entry colname="col2">cc<sub>0</sub></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5000</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M222" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cold content range to tax</oasis:entry>
         <oasis:entry colname="col2">cc<sub>1</sub></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5000</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M225" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Maximum tax to apply to snow cover energy</oasis:entry>
         <oasis:entry colname="col2">maxtax</oasis:entry>
         <oasis:entry colname="col3">0.9</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Snow cover energy flux smoothing window</oasis:entry>
         <oasis:entry colname="col2"><italic>smooth_hrs</italic></oasis:entry>
         <oasis:entry colname="col3">24</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M226" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Snow surface temperature augmentation</oasis:entry>
         <oasis:entry colname="col2"><italic>T</italic><sub>add</sub></oasis:entry>
         <oasis:entry colname="col3">2</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M227" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d2e4891"><sup>*</sup> <xref ref-type="bibr" rid="bib1.bibx33" id="text.104"/>.</p></table-wrap-foot></table-wrap>

      <p id="d2e5283">Figure <xref ref-type="fig" rid="FB1"/> shows the performance across the SD dataset, for (a) data from the stationary and point-based measurements, and (b) the Dischma valley photogrammetry snow surveys. Performance metrics are computed excluding zero-measured SD. When zero values and both stationary site and survey data are included, the Pearson correlation coefficient is 0.84, while the RMSE and MAE display values of 0.64 and 0.40 m, respectively. Compared to the stationary sites alone, the <italic>Snowclim</italic> SD estimates show higher accuracy, with an MAE of 0.40 m (excluding zero-measured SD). In contrast, when only the nine photogrammetry snow surveys are compared with the corresponding <italic>Snowclim</italic> estimates, the MAE deteriorates to 0.80 m.</p>

      <fig id="FB1"><label>Figure B1</label><caption><p id="d2e5297">Performance of the process-based model <italic>Snowclim</italic> for the snow measurements dataset, indicating a general overestimation, particularly for the Dischma valley snow surveys. <bold>(a)</bold> 2D histogram comparing measured SD at the stationary sites with the <italic>Snowclim</italic> SD estimates. <bold>(b)</bold> Same as <bold>(a)</bold>, but for the nine Dischma valley snow surveys. Displayed performance metrics do not incorporate zero-measured SD.</p></caption>
        
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f09.png"/>

      </fig>


</app>

<app id="App1.Ch1.S3">
  <label>Appendix C</label><title>Time series of SD and SHAP values</title>
      <p id="d2e5333">The SHAP value contributions of the S1 variables within the Combination<sub>ML</sub> configuration were assessed during the 2017–2018 and 2018–2019 snow seasons at four distinct sites in Switzerland (Fig. <xref ref-type="fig" rid="FC1"/>). All sites are operated by the Swiss Institute for Snow and Avalanche Research (SLF; Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/>), and the results shown correspond to the spatial nested CV framework. Figure <xref ref-type="fig" rid="FC1"/>a shows the time series for a measurement site near Arolla, Valais (46.41° N, 8.92° E), located in a bare rock area with a 0 % FCF and surrounded by mountains to the east, north, and west. At this high-elevation and bare site, the added value of <inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> under dry snow conditions and <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> under wet snow conditions becomes clear. During the 2017–2018 snow season, namely, a clear increase in <inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> is observed during the accumulation phase. After reaching peak values around late January, associated with a large snowfall event, <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and its associated SHAP values remain elevated until the snowpack starts to wet near the end of March. However, the peak occurs before the maximum measured SD in early April, a phenomenon not unique to this site and also reported by <xref ref-type="bibr" rid="bib1.bibx45" id="text.105"/>, who found an average lag of around 60 d between peak <inline-formula><mml:math id="M232" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and peak SD in their study area. In contrast, the observed <inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> values do not increase during the accumulation phase, consistent with the findings of <xref ref-type="bibr" rid="bib1.bibx49" id="text.106"/>, and contribute minimally to the SD predictions. At certain sites – usually with low-LIA satellite overpasses – however, <inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> and it's SHAP values do increase during the accumulation period (e.g., a site near Grindelwand shown in Fig. <xref ref-type="fig" rid="FC1"/>b). As such, depending on the LIA, <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> might contribute more or less to the predictions during dry snow conditions.</p>
      <p id="d2e5458">During the ablation phase, marked by a decline in <inline-formula><mml:math id="M237" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> in early April, the contribution of <inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> drops sharply, in line with decreasing observed values. In contrast, <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> emerges as the most informative S1 feature under these wet snow conditions, with positive SHAP values peaking near its lowest observed backscatter intensities. Beyond this point, as <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> increases due to the growing influence of superficial scattering processes <xref ref-type="bibr" rid="bib1.bibx57" id="paren.107"/>, the contribution gradually declines. Similar patterns have been observed at other sites (e.g., 46.42° N, 8.23° E and 46.39° N, 7.97° E) and is also evident from Fig. <xref ref-type="fig" rid="F5"/>c. In contrast, the behavior of <inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and its contribution to the SD estimates during the ablation period is less consistent. At some sites (e.g., 46.08° N, 7.92° E), the drop in <inline-formula><mml:math id="M242" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> coincides with a sudden increase in <inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>, whereas at other sites, no such increase is observed or an increase is linked to late-season snowfall events. Further research is required to better understand the interaction between wet snow and <inline-formula><mml:math id="M244" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, though this is beyond the scope of this study.</p>
      <p id="d2e5559">The Arolla site (Fig. <xref ref-type="fig" rid="FC1"/>a) shows a similar seasonal evolution of <inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> in 2018–2019 as in 2017–2018, further supporting the findings of Fig. <xref ref-type="fig" rid="F5"/> on the role of this S1 feature under different snow conditions. In contrast, although <inline-formula><mml:math id="M246" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> increases slightly in mid-March, it begins to decline as early as late February, whereas no corresponding sharp decrease is observed in <inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula>. While difficult to confirm, this may be related to melt-freeze events and/or metamorphism processes happening in the snowpack starting in early March. Nevertheless, <inline-formula><mml:math id="M248" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> also here strongly contributes during snow accumulation, when it is most informative.</p>
      <p id="d2e5615">The potentially added value of <inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> to the SD predictions at higher-elevated, bare locations is further supported by Fig. <xref ref-type="fig" rid="FC1"/>c, that displays the time series at a measurement site located near Prato, Ticino (46.47° N, 8.72° E), with a similar 0 % FCF but lower elevation (2222 m above sea level (m a.s.l.)). Unlike the Arolla site, however, <inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> is not only mainly informative during snow accumulation, but remains relatively elevated throughout February and March for both snow seasons, when the snowpack exceeds 2 m of snow. Nonetheless, the SD predictions appear to level off with only a limited response to new snowfall events, which is observed at the Arolla site during the 2017–2018 snow season as well. One explanation lies in the limited number of high SD observations used to train XGBoost (Fig. <xref ref-type="fig" rid="FE1"/>a), which constrains the model’s ability to represent higher SD values and results in a flattening of the predicted SD range (Fig. <xref ref-type="fig" rid="F6"/>a). Differently, there might be a saturation, or even already a decrease, in the S1 variables that respond to increasing SD at the beginning of the snow season, so that XGBoost cannot rely on these features to account for new snow events. This leveling-off should be taken into account when deploying XGBoost to predict SD across the Alps, especially when relying solely on S1 variables and FSC to explain interannual variability. Additionally, Fig. <xref ref-type="fig" rid="FC1"/>c helps to explain the relative SHAP value FI of <inline-formula><mml:math id="M251" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> in the bottom panel of Fig. <xref ref-type="fig" rid="F5"/>a. Although XGBoost captures the increase in <inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> during the accumulation period to contribute positively to the predicted SD, the SHAP value contribution is way smaller compared to <inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>, indicating a preference for <inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> over <inline-formula><mml:math id="M255" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> by XGBoost.</p>
      <p id="d2e5714">Finally, the bottom time series (Fig. <xref ref-type="fig" rid="FC1"/>d) corresponds to a forested (63 % FCF, 1868 m a.s.l.) site in Sobrio, Ticino (46.41° N, 8.92° E). Despite being consistently classified as dry snow in the time series, this area is actually masked as forest in the CLMS SWS wet snow product. This site was also analyzed by <xref ref-type="bibr" rid="bib1.bibx30" id="text.108"/>, who concluded that, given the low FI of <inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>CR</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> in their study, S1 satellite observations should not be used for this location. Our findings support the limited contribution of the S1 features at similar lower and/or forested areas, as we observe minimal added value from both <inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M259" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mtext>VV</mml:mtext><mml:mtext>0,s</mml:mtext></mml:msubsup></mml:mrow></mml:math></inline-formula> at this site. Within such sites, the predictions from XGBoost trained without satellite observations (No S1) are similar to, or even outperform, those based on satellite inputs (Fig. <xref ref-type="fig" rid="FC2"/>). Differently, additional inputs such as meteorological forcings can also improve the results (Fig. <xref ref-type="fig" rid="FC2"/>).</p>

      <fig id="FC1" specific-use="star"><label>Figure C1</label><caption><p id="d2e5779">SD predictions (spatial nested CV framework) and associated contribution of various S1 input features for the 2017–2018 and 2018–2019 snow seasons, at four SLF sites within Switzerland: <bold>(a)</bold> Arolla: 46.41° N, 8.92° E, <bold>(b)</bold> Grindelwand: 46.67° N, 8.06° E,  <bold>(c)</bold> Prato: 46.47° N, 8.72° E, and  <bold>(d)</bold> Sobrio: 46.41° N, 8.92° E. Measured SD is shown in gray, while predictions are denoted by light blue crosses. SHAP values for two S1 variables, representing their contribution in time, are plotted as well, and colored according to their input value in XGBoost. The stripes below the time series indicate dry (light gray) or wet (dark blue) snow conditions according to CLMS SWS wet snow product.</p></caption>
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f10.jpg"/>

      </fig>

      <fig id="FC2" specific-use="star"><label>Figure C2</label><caption><p id="d2e5802">Time series for the spatial nested CV framework at an SLF site near Prato, Ticino in Switzerland (46.41° N, 8.92 E), displaying the added value of meteorological forcings, and the performance without inclusion of S1 variables. The time series display measured (gray) and predicted (crosses) SD for the 2017–2018 and 2018–2019 snow seasons. The colors indicate the configuration used: Combination<sub>ML</sub> (blue), Weather<sub>ML</sub> (purple) and a configuration using no S1 variables, nor meteorological forcings or <italic>Snowclim</italic> SD estimates (No S1; yellow).</p></caption>
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f11.png"/>

      </fig>


</app>

<app id="App1.Ch1.S4">
  <label>Appendix D</label><title>16 March 2017 Dischma valley snow survey SD estimates</title>
      <p id="d2e5834">Figure <xref ref-type="fig" rid="FD1"/> illustrates differences in predicted SD values for the Combination<sub>ML</sub> configuration trained without (No survey; b) and with (Survey; c) spatially distributed SD training data. Although substantial overestimation persists after incorporating spatial SD training data, excessively high SD predictions at steep slopes and near mountain ridges are more effectively corrected. Two regions exhibiting pronounced corrections are highlighted in Fig. <xref ref-type="fig" rid="FD1"/>a and e. Figure <xref ref-type="fig" rid="FD1"/>a shows the difference between panels (b) and (c), together with the associated slope values, and the corresponding slope SHAP values for the configuration trained without spatially distributed SD data. Areas characterized by relatively steep slopes exhibit strong positive SHAP values, indicating that XGBoost previously learned an erroneous relationship between increasing slope and positive contributions to SD estimates, leading to inflated SD predictions at this high-elevation area with steep terrain. Such regions are negatively adjusted in Fig. <xref ref-type="fig" rid="FD1"/>c, as evident in both zoomed-in areas. Figure <xref ref-type="fig" rid="FD1"/>e, however, further highlights the influence of the TPI, in addition to the slope. Comparison of the central and right panels of Fig. <xref ref-type="fig" rid="FD1"/>e shows that areas characterized by strongly positive TPI values are also substantially negatively adjusted. Conversely, SD estimates are substantially positively adjusted in regions characterized by lower slope values following the inclusion of spatially distributed SD training data.</p>
      <p id="d2e5853">Including meteorological forcing data or <italic>Snowclim</italic> SD estimates further improves SD predictions for the 16 March 2017 snow survey, as shown in Fig. <xref ref-type="fig" rid="F7"/>b and c, and is reflected in Fig. <xref ref-type="fig" rid="FD2"/>a. Without spatially distributed SD training data (No survey), both the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations generally overestimate SD values, except at the lowest elevations (<inline-formula><mml:math id="M260" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1500</mml:mn></mml:mrow></mml:math></inline-formula> m). Here, an underestimation is observed for both configurations (Fig. <xref ref-type="fig" rid="FD2"/>a), particularly for the Ephemeral snow class (Fig. <xref ref-type="fig" rid="FD2"/>b). Also the <italic>Snowclim</italic> estimates reveal an underestimation in these areas (Fig. <xref ref-type="fig" rid="FD2"/>d), whereas the meteorological forcings may display overly warm temperature estimates or an undercatch of preceding snowfall events.</p>
      <p id="d2e5892">For the mid-elevation regions between 1500 and 2500 m the Weather<sub>ML</sub> configuration shows an approximately zero bias, whereas the <italic>Snowclim</italic><sub>ML</sub> configuration retains a persistent overestimation of about 17 cm. These areas are dominated by the Prairie, Montane Forest, and Maritime snow classes (Fig. <xref ref-type="fig" rid="FD2"/>c), which explains the biases observed for the Montane Forest and Priarie snow classes in Fig. <xref ref-type="fig" rid="FD2"/>b. At the highest elevations, dominated by the Tundra snow class with only a few Ice-class locations, the <italic>Snowclim</italic><sub>ML</sub> configuration continues to overestimate SD, while the Weather<sub>ML</sub> configuration again exhibits a slight underestimation, as reflected in Fig. <xref ref-type="fig" rid="FD2"/>b. Nonetheless, both configurations underestimate high (<inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:math></inline-formula> m) SD observations, resulting in an underestimation of <inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.34</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.16</mml:mn></mml:mrow></mml:math></inline-formula> m for the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations.</p>

      <fig id="FD1"><label>Figure D1</label><caption><p id="d2e5960">Improvements obtained by adding spatially distributed SD training data (Survey) within the Combination<sub>ML</sub> configuration for the 16 March 2017 Dischma valley snow survey. <bold>(a)</bold> Zoom-in of the difference map (Survey <bold>(b)</bold> – No survey <bold>(c)</bold> SD estimates), with corresponding slope and slope SHAP values. The slope SHAP values correspond with the No survey SD estimates. <bold>(b)</bold> SD estimates from the Combination<sub>ML</sub> configuration when no spatially distributed SD data is used during training.  <bold>(c)</bold> Same as <bold>(b)</bold>, but with inclusion of spatial SD training data.  <bold>(d)</bold> Difference map of predicted SD between <bold>(b)</bold> and <bold>(c)</bold>.  <bold>(e)</bold> Zoom-in of <bold>(d)</bold>, with corresponding slope and TPI values for the area.</p></caption>
        
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f12.jpg"/>

      </fig>

<fig id="FD2"><label>Figure D2</label><caption><p id="d2e6015">Improvement brought by adding spatially distributed SD training data (Survey) within the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations for the 16 March 2017 Dischma valley snow survey. <bold>(a)</bold> Bias for the two configurations within elevation bins of 50 m, trained without (No survey) and with (Survey) spatial SD training data. The black curve displays the amount of observations per elevation bin. <bold>(b)</bold> Bias displayed per <xref ref-type="bibr" rid="bib1.bibx78" id="text.109"/> snow class.  <bold>(c)</bold> Spatial distribution of the snow classes within different elevation areas.  <bold>(d)</bold> Difference map between <italic>Snowclim</italic> SD estimates and measured SD. The black lines in <bold>(c)</bold> and  <bold>(d)</bold> denote the contour line of 1500 m elevation.</p></caption>
        
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f13.jpg"/>

      </fig>

</app>

<app id="App1.Ch1.S5">
  <label>Appendix E</label><title>Additional tables and figures</title>

      <fig id="FE1"><label>Figure E1</label><caption><p id="d2e6069">Distributions of measured SD and static features of the in situ measurement sites used to train, validate and test XGBoost. <bold>(a)</bold> Distribution of measured SD. <bold>(b)</bold> Distribution of forest cover fraction of the unique measurement sites.  <bold>(c–f)</bold> Same as <bold>(b)</bold>, but for the snow classes described in <xref ref-type="bibr" rid="bib1.bibx78" id="text.110"/>, elevation, aspect and slope, respectively.</p></caption>
        
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f14.png"/>

      </fig>

<table-wrap id="TE1"><label>Table E1</label><caption><p id="d2e6100">Overall performance metrics for the PolSAR<sub>ML</sub>, Backscatter<sub>ML</sub> and Combination<sub>ML</sub> configurations for the temporal nested CV framework. The values inside the brackets denote the metric values when zero-measured SD are included in the evaluation.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:colspec colnum="4" colname="col4" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Metric</oasis:entry>
         <oasis:entry colname="col2">PolSAR<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col3">Backscatter<sub>ML</sub></oasis:entry>
         <oasis:entry colname="col4">Combination<sub>ML</sub></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M264" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> [–]</oasis:entry>
         <oasis:entry colname="col2">0.83 (0.88)</oasis:entry>
         <oasis:entry colname="col3">0.83 (0.88)</oasis:entry>
         <oasis:entry colname="col4">0.84 (0.89)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MAE [m]</oasis:entry>
         <oasis:entry colname="col2">0.30 (0.19)</oasis:entry>
         <oasis:entry colname="col3">0.30 (0.19)</oasis:entry>
         <oasis:entry colname="col4">0.29 (0.18)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RMSE [m]</oasis:entry>
         <oasis:entry colname="col2">0.43 (0.33)</oasis:entry>
         <oasis:entry colname="col3">0.44 (0.34)</oasis:entry>
         <oasis:entry colname="col4">0.42 (0.33)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bias [m]</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula> (0.01)</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula> (0.01)</oasis:entry>
         <oasis:entry colname="col4">0.02 (0.01)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <fig id="FE2"><label>Figure E2</label><caption><p id="d2e6240">Measurement stations exhibiting a mean site <inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:mtext>bias</mml:mtext><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m within the spatial nested CV framework for the Weather<sub>ML</sub> and <italic>Snowclim</italic><sub>ML</sub> configurations. Sites with fewer than 10 observations are excluded. Colors indicate for which configurations a mean site <inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:mtext>bias</mml:mtext><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> m is observed.</p></caption>
        
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f15.png"/>

      </fig>

      <fig id="FE3"><label>Figure E3</label><caption><p id="d2e6289">XGBoost spatial prediction performance for the Dischma valley snow surveys with no spatial data included during model training and tuning. The first column <bold>(a, e)</bold> represents the Combination<sub>ML</sub> configuration, while the second and third column show the results for the Weather<sub>ML</sub> <bold>(b, f)</bold> and <italic>Snowclim</italic><sub>ML</sub> <bold>(c, g)</bold> configurations, respectively. <bold>(a)</bold>, <bold>(b)</bold>, and <bold>(c)</bold> display the spatial predictions for the 16 March 2017 snow survey, with <bold>(d)</bold> representing the measured SD. <bold>(e)</bold>, <bold>(f)</bold>, and <bold>(g)</bold> show 2D histograms and performance metrics across all nine conducted snow surveys.</p></caption>
        
        <graphic xlink:href="https://tc.copernicus.org/articles/20/3187/2026/tc-20-3187-2026-f16.png"/>

      </fig>


</app>
  </app-group><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d2e6349">The datasets with the ML experiments, and all code used for visualization and data analysis, can be retrieved from: <ext-link xlink:href="https://doi.org/10.5281/zenodo.19697176" ext-link-type="DOI">10.5281/zenodo.19697176</ext-link> <xref ref-type="bibr" rid="bib1.bibx9" id="paren.111"/>.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e6361">The Sentinel-1 data is freely available on the Alaska Satellite Facility’s Vertex data portal (<uri>https://search.asf.alaska.edu</uri>, last access: 19 May 2026). IMS and MODIS snow cover data can be downloaded at <uri>https://cmr.earthdata.nasa.gov/search/concepts/C1386246258-NSIDCV0.html</uri> (last access: 19 May 2026) and by using the earthaccess Python package (“MOD10A1F” and “MYD10A1F” collections), respectively. The SAR Wet Snow product can be sourced from <ext-link xlink:href="https://doi.org/10.2909/cd23c4bb-b3cb-4331-bb89-93321b46f8ed" ext-link-type="DOI">10.2909/cd23c4bb-b3cb-4331-bb89-93321b46f8ed</ext-link> <xref ref-type="bibr" rid="bib1.bibx22" id="paren.112"/>. Instructions to download the MSWX and MSWEP meteorological data can be found at <uri>https://www.gloh2o.org/</uri> (last access: 19 May 2026). The Copernicus 30 m digital elevation model can be retrieved from the Copernicus data space ecosystem: <ext-link xlink:href="https://doi.org/10.5270/ESA-c5d3d65" ext-link-type="DOI">10.5270/ESA-c5d3d65</ext-link> <xref ref-type="bibr" rid="bib1.bibx18" id="paren.113"/>. Finally, land cover data can be sourced from the Copernicus Land Monitoring Service via: <ext-link xlink:href="https://land.copernicus.eu/en/products/global-dynamic-land-cover/copernicus-global-land-service-land-cover-100m-collection-3-epoch-2015-2019-globe">https://land.copernicus.eu/en/products/global-dynamic-land-cover/copernicus-global-land-service-land-cover-100m-collection-3-epoch-2015-2019-globe</ext-link> (last access: 19 May 2026).</p>

      <p id="d2e6389">The majority of the in situ snow depth measurements can be freely downloaded from the various providers across the European Alps: <list list-type="bullet"><list-item>
      <p id="d2e6394">IMIS measuring network; Switzerland (<ext-link xlink:href="https://doi.org/10.16904/envidat.406" ext-link-type="DOI">10.16904/envidat.406</ext-link>, <xref ref-type="bibr" rid="bib1.bibx44" id="altparen.114"/>)</p></list-item><list-item>
      <p id="d2e6404">Manual measuring network; Switzerland (<ext-link xlink:href="https://doi.org/10.16904/envidat.408" ext-link-type="DOI">10.16904/envidat.408</ext-link>, <xref ref-type="bibr" rid="bib1.bibx90" id="altparen.115"/>)</p></list-item><list-item>
      <p id="d2e6414">Arpa Piemonte; Italy (<ext-link xlink:href="https://www.arpa.piemonte.it/rischi_naturali/snippets_arpa_graphs/map_meteoweb/?rete=stazione_meteorologica">https://www.arpa.piemonte.it/rischi_</ext-link>
<ext-link xlink:href="https://www.arpa.piemonte.it/rischi_naturali/snippets_arpa_graphs/map_meteoweb/?rete=stazione_meteorologica">naturali/snippets_arpa_graphs/map_meteoweb/?rete=stazione</ext-link>
<ext-link xlink:href="https://www.arpa.piemonte.it/rischi_naturali/snippets_arpa_graphs/map_meteoweb/?rete=stazione_meteorologica">_meteorologica</ext-link>, last access: 19 May 2026)</p></list-item><list-item>
      <p id="d2e6428">Airplane photogrammetry SD maps; Switzerland (<ext-link xlink:href="https://doi.org/10.16904/envidat.418" ext-link-type="DOI">10.16904/envidat.418</ext-link>, <xref ref-type="bibr" rid="bib1.bibx15" id="altparen.116"/>)</p></list-item><list-item>
      <p id="d2e6438">Digital photogrammetry SD maps; Switzerland (<ext-link xlink:href="https://doi.org/10.16904/envidat.62" ext-link-type="DOI">10.16904/envidat.62</ext-link>, <xref ref-type="bibr" rid="bib1.bibx60" id="altparen.117"/>)</p></list-item><list-item>
      <p id="d2e6448">METEO FRANCE; France (<uri>https://donneespubliques.meteofrance.fr/?fond=recherche</uri>, last access: 19 May 2026)</p></list-item><list-item>
      <p id="d2e6455">MeteoTrentino – open data; Italy (<uri>https://www.meteotrentino.it/dati/neve/</uri>, last access: 19 May 2026)</p></list-item><list-item>
      <p id="d2e6462">MeteoTrentino – data upon request; Italy (<uri>https://contenuti.meteotrentino.it/dati-meteo/modulo.pdf</uri>, last access: 19 May 2026)</p></list-item><list-item>
      <p id="d2e6469">Open Meteo Data V1; Italy (<uri>https://data.civis.bz.it//dataset/1512fa49-3e97-40d7-9bdb-2fc76c9efe3c/resource/9ca68cd2-2060-4a02-8a04-09b9d4acac40/download/dokumentationopendatameteode.pdf</uri>, last access: 19 May 2026) </p></list-item><list-item>
      <p id="d2e6477">GeoSphere Austria; Austria (<uri>https://dataset.api.hub.geosphere.at/app/frontend/station/historical/klima-v2-1d</uri>, last access: 19 May 2026)</p></list-item><list-item>
      <p id="d2e6484">Global Historical Climatology Network-Daily database; Germany, Slovenia … (<uri>https://www.ncei.noaa.gov/cdo-web/search?datasetid=GHCND</uri>, last access: 19 May 2026)</p></list-item></list> We further collected snow depth measurements from Valle d'Aosta through personal communication (arpavda@cert.legalmail.it). In addition, Italian snow depth data was obtained from the Italian Department of Civil Protection and processed by the Centro Internazionale in Monitoraggio Ambientale (CIMA).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e6494">LB, HL, DD, WW and GDL designed the study. LB and EB worked on the data preparation, and LB conducted the experiments discussed in the manuscript. The analyses, original draft preparation and visualization was performed by LB. All other authors reviewed and edited the manuscript before first submission.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e6500">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="d2e6506">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e6512">The Flemish Supercomputer Center, funded by Research Fund – Flanders (FWO) and the Flemish Government, was used for computational resources and services. Next, the authors employed chatGPT to further improve the readability and language of the manuscript. Before submission, the authors edited and reviewed the manuscript, and take full responsibility for its content.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e6517">This work was funded by the SNOWTRANE project (SR/00/407) of the Belgian Science Policy Office (BELSPO).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e6523">This paper was edited by Francesco Avanzi and reviewed by three anonymous referees.</p>
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