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  <front>
    <journal-meta><journal-id journal-id-type="publisher">AMT</journal-id><journal-title-group>
    <journal-title>Atmospheric Measurement Techniques</journal-title>
    <abbrev-journal-title abbrev-type="publisher">AMT</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Meas. Tech.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1867-8548</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/amt-19-2407-2026</article-id><title-group><article-title>TROPOMI/WFMD v2.0: Improved retrievals of <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> with XGBoost-based quality filtering</article-title><alt-title>TROPOMI/WFMD v2.0: Improved retrievals of <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula></alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Schneising</surname><given-names>Oliver</given-names></name>
          <email>oliver.schneising@iup.physik.uni-bremen.de</email>
        <ext-link>https://orcid.org/0000-0003-1725-8246</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Bovensmann</surname><given-names>Heinrich</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Buchwitz</surname><given-names>Michael</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7616-1837</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Buschmann</surname><given-names>Matthias</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5077-9524</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Deutscher</surname><given-names>Nicholas M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2906-2577</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Griffith</surname><given-names>David W. T.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7986-1924</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Hachmeister</surname><given-names>Jonas</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5700-4502</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Hase</surname><given-names>Frank</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Iraci</surname><given-names>Laura T.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2859-5259</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Kivi</surname><given-names>Rigel</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8828-2759</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Morino</surname><given-names>Isamu</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2720-1569</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Ohyama</surname><given-names>Hirofumi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2109-9874</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Petri</surname><given-names>Christof</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7010-5532</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Reuter</surname><given-names>Maximilian</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9141-3895</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Robinson</surname><given-names>John</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Roehl</surname><given-names>Coleen</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9">
          <name><surname>Sha</surname><given-names>Mahesh Kumar</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1440-1529</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff10">
          <name><surname>Shiomi</surname><given-names>Kei</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1206-8614</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff11">
          <name><surname>Strong</surname><given-names>Kimberly</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12">
          <name><surname>Sussmann</surname><given-names>Ralf</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1970-7538</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff13">
          <name><surname>Té</surname><given-names>Yao</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-6405-8074</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff14">
          <name><surname>Velazco</surname><given-names>Voltaire A.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1376-438X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15 aff1 aff16">
          <name><surname>Vrekoussis</surname><given-names>Mihalis</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8292-8352</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff17">
          <name><surname>Wang</surname><given-names>Wei</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Warneke</surname><given-names>Thorsten</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff18">
          <name><surname>Weidmann</surname><given-names>Damien</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0178-7904</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff11">
          <name><surname>Wunch</surname><given-names>Debra</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4924-0377</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff19">
          <name><surname>Zhou</surname><given-names>Minqiang</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3427-5873</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Bösch</surname><given-names>Hartmut</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3944-9879</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Institute of Environmental Physics (IUP), University of Bremen, Bremen, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Environmental Futures, School of Science, University of Wollongong, Wollongong, NSW, Australia</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Karlsruhe Institute of Technology (KIT), IMKASF, Karlsruhe, Germany</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Earth Science Division, NASA Ames Research Center, Moffett Field, CA, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Space and Earth Observation Centre, Finnish Meteorological Institute, Sodankylä, Finland</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Satellite Remote Sensing Section and Satellite Observation Center, Earth System Division,  National Institute for Environmental Studies (NIES), Tsukuba, Ibaraki, Japan</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Earth Sciences New Zealand, Omakau, New Zealand</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>California Institute of Technology, Pasadena, CA, USA</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>Royal Belgian Institute for Space Aeronomy (BIRA-IASB), Brussels, Belgium</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>Earth Observation Research Center (EORC), Japan Aerospace Exploration Agency (JAXA), Tsukuba, Ibaraki, Japan</institution>
        </aff>
        <aff id="aff11"><label>11</label><institution>Department of Physics, University of Toronto, Toronto, Ontario, Canada</institution>
        </aff>
        <aff id="aff12"><label>12</label><institution>Karlsruhe Institute of Technology (KIT), IMKIFU, Garmisch-Partenkirchen, Germany</institution>
        </aff>
        <aff id="aff13"><label>13</label><institution>Sorbonne Université, CNRS, MONARIS, UMR8233, Paris, France</institution>
        </aff>
        <aff id="aff14"><label>14</label><institution>Deutscher Wetterdienst (DWD), Meteorological Observatory Hohenpeissenberg, Hohenpeissenberg, Germany</institution>
        </aff>
        <aff id="aff15"><label>15</label><institution>Climate and Atmosphere Research Centre (CARE-C), The Cyprus Institute, Nicosia, Cyprus</institution>
        </aff>
        <aff id="aff16"><label>16</label><institution>Center of Marine Environmental Sciences (MARUM), University of Bremen, Bremen, Germany</institution>
        </aff>
        <aff id="aff17"><label>17</label><institution>Key Laboratory of Environmental Optics and Technology, Anhui Institute of Optics and Fine Mechanics,   Chinese Academy of Sciences, Hefei, China</institution>
        </aff>
        <aff id="aff18"><label>18</label><institution>STFC Rutherford Appleton Laboratory, Space Science and Technology Department, Harwell Campus, Didcot, UK</institution>
        </aff>
        <aff id="aff19"><label>19</label><institution>State Key Laboratory of Atmospheric Environment and Extreme Meteorology, Institute of Atmospheric Physics,   Chinese Academy of Sciences, Beijing, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Oliver Schneising (oliver.schneising@iup.physik.uni-bremen.de)</corresp></author-notes><pub-date><day>14</day><month>April</month><year>2026</year></pub-date>
      
      <volume>19</volume>
      <issue>7</issue>
      <fpage>2407</fpage><lpage>2435</lpage>
      <history>
        <date date-type="received"><day>2</day><month>November</month><year>2025</year></date>
           <date date-type="rev-request"><day>13</day><month>November</month><year>2025</year></date>
           <date date-type="rev-recd"><day>26</day><month>March</month><year>2026</year></date>
           <date date-type="accepted"><day>29</day><month>March</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Oliver Schneising 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://amt.copernicus.org/articles/amt-19-2407-2026.html">This article is available from https://amt.copernicus.org/articles/amt-19-2407-2026.html</self-uri><self-uri xlink:href="https://amt.copernicus.org/articles/amt-19-2407-2026.pdf">The full text article is available as a PDF file from https://amt.copernicus.org/articles/amt-19-2407-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e506">The TROPOspheric Monitoring Instrument (TROPOMI) on board the Sentinel-5 Precursor satellite provides daily global observations of atmospheric methane (<inline-formula><mml:math id="M5" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and carbon monoxide (<inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>) at relatively high spatial resolution. The dense spatial and temporal coverage is achieved by the instrument's wide swath, which permits detailed mapping of the worldwide distribution of these important atmospheric constituents. The adaptation and optimisation of the Weighting Function Modified Differential Optical Absorption Spectroscopy (WFMD) algorithm for the simultaneous retrieval of the column-averaged dry-air mole fractions <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M8" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> from TROPOMI's shortwave infrared (SWIR) radiance measurements has proven to be a valuable complement and alternative to the operational TROPOMI products.</p>

      <p id="d2e560">The latest release of the TROPOMI/WFMD product (version 2.0) includes several improvements expanding its suitability for a wider range of scientific applications. Data yield at mid and high latitudes has increased, accompanied by improved accuracy and precision according to the validation with the ground-based Total Carbon Column Observing Network (TCCON). These advancements are primarily due to more refined quality filtering that has been accomplished by replacing the previous Random Forest Classifier with the more efficient and potentially higher performing Extreme Gradient Boosting (XGBoost) algorithm in conjunction with improved training data incorporating an updated cloud product from the Visible Infrared Imaging Radiometer Suite (VIIRS) and the TROPOMI Aerosol Index. This enhanced training data set enables more reliable identification of cloudy scenes and mitigates issues related to specific aerosol events over bright surfaces. Importantly, as with previous product versions, the actual quality classification does not depend on the real-time availability of these external data products, which are only required during the training phase.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>European Space Agency</funding-source>
<award-id>4000126450/19/I-NB</award-id>
<award-id>4000142730/23/I-NS</award-id>
</award-group>
<award-group id="gs2">
<funding-source>Bundesministerium für Forschung, Technologie und Raumfahrt</funding-source>
<award-id>01 LK2103A</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="d2e592">Methane (<inline-formula><mml:math id="M9" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) is the second most important anthropogenic greenhouse gas in terms of radiative forcing following carbon dioxide (<inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). While it is less abundant in the atmosphere, the global warming potential of <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> by mass unit is significantly greater than that of <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx43" id="paren.1"/>. However, thanks to its much shorter atmospheric lifetime of around a decade <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx37" id="paren.2"/>, reducing <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions will have a decisive impact on climate on a short timescale, so that rapid action can support measures to limit global warming to well below <inline-formula><mml:math id="M14" display="inline"><mml:mn mathvariant="normal">2</mml:mn></mml:math></inline-formula> °C above pre-industrial levels. Carbon monoxide (<inline-formula><mml:math id="M15" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>) is a reactive gas that is formed as a by-product during incomplete combustion and oxidation of hydrocarbons, including emissions from wildfires as a natural source. It contributes indirectly to climate change by depleting hydroxyl radicals (<inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:math></inline-formula>), which are critical for removing other gases that contribute to global warming, such as <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. At the same time, the oxidation of <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> produces <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Under certain conditions, <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> also participates in photochemical reactions forming tropospheric ozone, which is itself a greenhouse gas. With a typical lifetime of 1 to 2 months, <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> is a useful tracer for atmospheric air masses of anthropogenic origin. For sources that emit both <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M23" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> simultaneously, it is feasible to use <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> as a proxy for <inline-formula><mml:math id="M25" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions by using emission factors <xref ref-type="bibr" rid="bib1.bibx70 bib1.bibx88 bib1.bibx65" id="paren.3"/>. Because of these reasons, monitoring both gases helps to better understand atmospheric chemistry and guide efforts to mitigate climate change.</p>
      <p id="d2e769">Satellite remote sensing has emerged as a useful method for tracking global distributions of <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>. It thus offers unique insights into the underlying sources, sinks, and atmospheric transport processes. In particular, measuring upwelling shortwave infrared (SWIR) radiances is especially useful because of the sensitivity to changes in trace gas abundance throughout the entire atmospheric column. Instruments such as MOPITT (Terra) <xref ref-type="bibr" rid="bib1.bibx18" id="paren.4"/>, SCIAMACHY (ENVISAT) <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx8" id="paren.5"/>, and TANSO-FTS (GOSAT, GOSAT-2) <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx73" id="paren.6"/> have contributed important data on <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>, or both, depending on which spectral range each sensor covers.</p>
      <p id="d2e845">Launched on 13 October 2017, TROPOMI on board ESA's Sentinel-5 Precursor satellite measures radiances across eight spectral bands from the ultraviolet (UV) to the SWIR <xref ref-type="bibr" rid="bib1.bibx77" id="paren.7"/> with daily global coverage and relatively high spatial resolution (<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.5</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula> km<sup>2</sup> at nadir in the SWIR bands, after August 2019). The unique capabilities of TROPOMI enable unprecedented mapping of <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> distributions, supporting the detection of large-scale patterns as well as localised emission sources in a single satellite overpass. The data can be combined with targeted high-resolution airborne or satellite-based measurements with limited coverage (e.g., from GHGSat <xref ref-type="bibr" rid="bib1.bibx28" id="paren.8"/>) in a tip and cue approach to zoom in on and quantify individual point sources detected by TROPOMI
<xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx66" id="paren.9"/>. In addition to the operational TROPOMI products for <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx25 bib1.bibx23" id="paren.10"/> and <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx34" id="paren.11"/>, the TROPOMI/WFMD product, which retrieves both gases simultaneously from a common spectral window <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx64" id="paren.12"/>, has proven valuable as an independent data set in geophysical applications and in sensitivity studies to assess the robustness of findings with respect to the specific selection of the underlying data product <xref ref-type="bibr" rid="bib1.bibx78 bib1.bibx50 bib1.bibx38" id="paren.13"/>.</p>
      <p id="d2e960">A non-linear machine learning quality screening algorithm based on a Random Forest Classifier was implemented for the first time in the original TROPOMI/WFMD combined <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> retrieval to exclude measurements that are insufficiently characterised by the tabulated forward model, which assumes rather simple physical conditions (e.g., cloud-free scenes) for fast processing <xref ref-type="bibr" rid="bib1.bibx63" id="paren.14"/>. Similar machine learning-based filtering techniques are now widely used in greenhouse gas retrievals from multiple satellite instruments <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx7 bib1.bibx4" id="paren.15"/>, reflecting a broader shift towards data-driven quality control in this field of remote sensing.</p>
      <p id="d2e994">In this article, we present the recent updates that have been incorporated into the latest version of the TROPOMI/WFMD product (version 2.0). In particular, the Random Forest Classifier previously used for quality filtering has been replaced with the more efficient high-performance XGBoost algorithm, and the training data have been improved. The following sections provide a detailed account of these modifications, a comprehensive validation of the resulting data products, and demonstrate the consequential enhancements in data quality relative to the previous product version.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>TROPOMI/WFMD algorithm improvements</title>
      <p id="d2e1009">The Weighting Function Modified DOAS (WFMD) algorithm retrieves column-averaged dry-air mole fractions of methane (<inline-formula><mml:math id="M38" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and carbon monoxide (<inline-formula><mml:math id="M39" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>) from SWIR radiances in the <inline-formula><mml:math id="M40" display="inline"><mml:mn mathvariant="normal">2.3</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> spectral range measured by TROPOMI and is described in detail in <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx64" id="text.16"/>. Therefore, only the main aspects are briefly summarised here. WFMD uses a least-squares approach to scale pre-defined vertical profiles and fits a linearised radiative transfer model based on SCIATRAN <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx60" id="paren.17"/> to the logarithm of the sun-normalised radiance. A look-up table enables efficient retrievals of the vertical columns of the targeted species by covering various atmospheric conditions. The retrieved columns are converted to <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M43" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> using dry air columns from the European Centre for Medium-Range Weather Forecasts (ECMWF) adjusted for the higher resolved actual surface elevation of the individual satellite scenes. A machine learning-based classifier filters low-quality scenes using cloud data from the Visible Infrared Imaging Radiometer Suite (VIIRS) onboard Suomi NPP <xref ref-type="bibr" rid="bib1.bibx26" id="paren.18"/> in the training phase. To mitigate residual albedo-related biases in <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, a random forest regressor with shallow decision trees (leaf nodes <inline-formula><mml:math id="M45" display="inline"><mml:mo>≪</mml:mo></mml:math></inline-formula> training scenes <inline-formula><mml:math id="M46" display="inline"><mml:mo>≪</mml:mo></mml:math></inline-formula> all scenes) is trained on a small spatio-temporally constrained subset using a small number of features and the SLIMCH4 climatology <xref ref-type="bibr" rid="bib1.bibx48" id="paren.19"/> as a low-resolution reference. This post-processing correction method is statistically robust and generalises effectively to unseen data <xref ref-type="bibr" rid="bib1.bibx64" id="paren.20"/>. No similar correction is required for <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> due to its larger natural variability and relaxed quality requirements.</p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>General processing improvements</title>
      <p id="d2e1133">TROPOMI/WFMD v2.0 introduces several improvements aimed at enabling more robust results in scientific applications. It consistently uses TROPOMI Level 1b V02.01.XX files as input, ensuring the inclusion of the latest instrument calibration. The first part of the split spectral fitting window described in <xref ref-type="bibr" rid="bib1.bibx63" id="text.21"/> contains a continuum-like region (with virtually no absorption by atmospheric constituents), which serves to determine the apparent albedo in the preprocessing step in order to disentangle surface reflection and molecular abundances in the actual fitting procedure. In v2.0, the first part of the retrieval window has been slightly extended by <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.4</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> at the long-wavelength end and now covers the spectral range from <inline-formula><mml:math id="M49" display="inline"><mml:mn mathvariant="normal">2311</mml:mn></mml:math></inline-formula>–<inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mn mathvariant="normal">2315.9</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>, while the enclosed near-continuum itself remains unchanged. The extension aims at improving the transition to the region with stronger molecular absorption features captured in the second part of the fitting window (<inline-formula><mml:math id="M51" display="inline"><mml:mn mathvariant="normal">2320</mml:mn></mml:math></inline-formula>–<inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mn mathvariant="normal">2338</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>) and may enhance the signal-to-noise ratio and baseline fitting, thereby supporting more stable and precise retrievals. The position of the fitting window and the continuum-like interval it contains is shown together with the corresponding molecular absorption features in Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/> in an example spectral fit.</p>
      <p id="d2e1199">Another update in v2.0 is the usage of a hybrid sigma-pressure vertical coordinate system consisting of <inline-formula><mml:math id="M53" display="inline"><mml:mn mathvariant="normal">31</mml:mn></mml:math></inline-formula> layers to provide the prior profiles and averaging kernels, replacing the previous pure sigma coordinate system with <inline-formula><mml:math id="M54" display="inline"><mml:mn mathvariant="normal">20</mml:mn></mml:math></inline-formula> layers, in which each layer represented an equal fraction of the total surface pressure. Figure <xref ref-type="fig" rid="F1"/> compares the two vertical discretisations using an example of surface elevation variation. The new hybrid layering combines terrain-following characteristics near the surface with enhanced vertical resolution in the lower atmosphere and fixed reference levels in the upper atmosphere. The increased near-surface vertical detail in the prior and averaging kernel information supports the consideration of surface pressure mismatches during comparison with other measurements (e.g., for validation) or during assimilation in inverse modelling frameworks. Such mismatches can occur due to local horizontal displacement relative to comparison measurements or from the coarse horizontal resolution of models. The enhanced vertical representation may therefore facilitate better harmonisation of these inherent differences, especially over complex terrain.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e1220">Comparison of <bold>(a)</bold> the 31-layer hybrid sigma-pressure vertical coordinate system used in TROPOMI/WFMD v2.0 with <bold>(b)</bold> the previous 20-layer pure sigma coordinate system. The dark grey area illustrates exemplary surface elevation variation in <inline-formula><mml:math id="M55" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>-direction. The associated pressure layer thicknesses are colour-coded. The perceptual uniform colormap used here and in many other figures is described in Appendix <xref ref-type="sec" rid="App1.Ch1.S2"/>.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>XGBoost-based quality filtering</title>
      <p id="d2e1257">In earlier versions of the product, quality filtering was accomplished using a Random Forest classifier <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx64" id="paren.22"/>, since it delivers robust results that are largely insensitive to fine-tuning of the hyperparameters <xref ref-type="bibr" rid="bib1.bibx74" id="paren.23"/>. Random Forest is a bagging-based ensemble learning method that trains the involved decision trees in parallel. In the standard implementation, these trees are deep and unpruned. All trees train independently on bootstrapped subsets of the training data, with a random subset of features made available at each split <xref ref-type="bibr" rid="bib1.bibx9" id="paren.24"/>. This double randomisation of the training process implies that each tree is created from a different subset of data and features, which decorrelates the individual trees from each other and reduces overfitting by means of the imposed diversity within the ensemble. The final predictions are made by majority voting among the trees, which reduces variance, as the collective decision-making process aggregates the results of the heterogeneous ensemble members. For a global quality filtering task that spans a wide range of surface types, atmospheric states, and illumination conditions, achieving sufficient ensemble diversity quickly drives up model size and memory demands, which limits extensibility to additional effects. In particular, infrequent but physically consistent quality-degrading conditions, such as specific aerosol events over bright surfaces targeted in the updated product version, may not be optimally captured by a Random Forest classifier, as its ensemble-averaging strategy risks diluting such sporadic signals.</p>
      <p id="d2e1269">To address this limitation, the latest product TROPOMI/WFMD v2.0 uses Extreme Gradient Boosting (XGBoost) <xref ref-type="bibr" rid="bib1.bibx12" id="paren.25"/>, providing a more compact and computationally efficient framework for comprehensive quality filtering. XGBoost builds trees sequentially, with each new tree aiming to correct the residual errors of the preceding ensemble. To achieve this, the respective new tree is trained to predict the negative gradient of the current loss function in order to determine the direction and magnitude of the required correction. By iteratively adding these correction trees, XGBoost reduces bias and variance, often surpassing the predictive performance of bagging-based models. The one-time training process is slower due to its sequential nature, but the resulting model tends to be shallower and more optimised, which is beneficial when used in resource-constrained environments. Unlike Random Forest, which usually performs well with default settings, XGBoost is more sensitive to hyperparameter optimisation due to the complex way its tuning parameters interact with each other. For the TROPOMI/WFMD v2.0 quality filter, the Python package <italic>xgboost</italic> is used, and tuning efforts focussed on balancing model simplicity with generalisation ability, resulting in the following parameter values, which demonstrate the importance of carefully tuning XGBoost to create a maximally robust and generalisable model.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Model training and internal evaluation</title>
      <p id="d2e1314">To prevent overfitting, a conservative <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi mathvariant="monospace">learning</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">rate</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.03</mml:mn></mml:mrow></mml:math></inline-formula> was chosen to shrink the weights for the corrections by new trees, with the trade-off that more boosting rounds are required to compensate for the slower (but more accurate) learning. The complexity of the individual trees was constrained with <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mi mathvariant="monospace">max</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">depth</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mi mathvariant="monospace">min</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">child</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">weight</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> in order to obtain suitable pruning without uncontrolled growth. An increase in the generalisation capability to unseen data was achieved by adding a random component to the training process via <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi mathvariant="monospace">subsample</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mi mathvariant="monospace">colsample</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">bytree</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>. This means that each tree of the model is trained on randomly selected <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mn mathvariant="normal">70</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the training data using <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mn mathvariant="normal">70</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the available features, which makes the model less likely to fit to noise or irrelevant patterns in the training data. Besides the tree construction and sampling parameters, there are also other regularisation parameters in addition to the already discussed learning rate: <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mi mathvariant="monospace">gamma</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> requires that nodes in a single tree are only added if the associated loss reduction is large enough, thus impeding unnecessary splits; <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi mathvariant="monospace">lambda</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> controls the L2 regularisation of the leaf weights by encouraging the model to find a simpler solution that generalises better to unseen data. While <inline-formula><mml:math id="M65" display="inline"><mml:mi mathvariant="monospace">lambda</mml:mi></mml:math></inline-formula> is applied during tree creation, <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mi mathvariant="monospace">learning</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">rate</mml:mi></mml:mrow></mml:math></inline-formula> scales down the final tree weights at the moment it is added to the ensemble.</p>
      <p id="d2e1463">The XGBoost classifier was trained using data from 38 randomly selected days distributed across 2020 and 2021, with the additional requirement that all seasons are adequately represented. This sampling strategy covers all physically observable combinations of latitude and solar zenith angle and captures a broad range of atmospheric conditions, while keeping the overall data set size manageable. The training truth for the quality filter was informed by an updated cloud product from the Visible Infrared Imaging Radiometer Suite (VIIRS; S5P S-NPP Cloud processor version V01.03.00 based on the VIIRS Enterprise Cloud Mask) and the TROPOMI Aerosol Index (V02.04.00), aiming at improved identification of cloudy scenes and mitigation of issues arising from specific aerosol events over bright surfaces. The classification task involves a clear class imbalance, with good quality observations (class <inline-formula><mml:math id="M67" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula>) representing a minority (<inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.151</mml:mn></mml:mrow></mml:math></inline-formula>). The set of <inline-formula><mml:math id="M69" display="inline"><mml:mn mathvariant="normal">26</mml:mn></mml:math></inline-formula> features used in XGBoost (listed in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS2"/>) remains identical to the quality filter of v1.8 <xref ref-type="bibr" rid="bib1.bibx64" id="paren.26"/> and comprises only intrinsic parameters available from preceding processing. This means that the quality filter remains independent of real-time availability of external cloud and aerosol information during the actual quality prediction.</p>

      <fig id="F2"><label>Figure 2</label><caption><p id="d2e1517">Training and validation performance, measured by <bold>(a)</bold> Logloss and <bold>(b)</bold> the Area Under the Precision-Recall Curve (AUPRC, see main text for details) for class <inline-formula><mml:math id="M70" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> (good quality), as a function of boosting rounds, illustrating stable convergence without notable overfitting. The relative gap metric <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> quantifies how large the final training-validation gap is relative to the achieved gain on the validation set over the baseline. A small value of <inline-formula><mml:math id="M72" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> indicates that the fitted model generalises effectively to unseen data.</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f02.png"/>

          </fig>

      <p id="d2e1554">Model performance was assessed using completely independent data from 2022, a year that was not involved at all in the training process. To monitor and prevent overfitting, <italic>early stopping</italic> was applied during training (<inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi mathvariant="monospace">early</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">stopping</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">rounds</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula>) using the <italic>Logloss</italic> metric for progress tracking. Logloss was chosen because it corresponds directly to the objective function that is minimised in XGBoost training, thus ensuring consistency of the evaluation step with the underlying optimisation process. As a performance measure, Logloss evaluates the calibration quality of predicted probabilities across all classes. Early stopping intervened after <inline-formula><mml:math id="M74" display="inline"><mml:mn mathvariant="normal">8000</mml:mn></mml:math></inline-formula> boosting rounds (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mi mathvariant="monospace">n</mml:mi><mml:mi mathvariant="monospace">_</mml:mi><mml:mi mathvariant="monospace">estimators</mml:mi></mml:mrow></mml:math></inline-formula>) because the Logloss on the validation set had not improved in <inline-formula><mml:math id="M76" display="inline"><mml:mn mathvariant="normal">25</mml:mn></mml:math></inline-formula> consecutive rounds, revealing that the learning progress had already levelled off significantly. According to Fig. <xref ref-type="fig" rid="F2"/>, the corresponding validation Logloss curve decreases monotonically during the <inline-formula><mml:math id="M77" display="inline"><mml:mn mathvariant="normal">8000</mml:mn></mml:math></inline-formula> boosting rounds to values substantially below the baseline entropy of <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.424</mml:mn></mml:mrow></mml:math></inline-formula> expected under the prevalence <inline-formula><mml:math id="M79" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> of class <inline-formula><mml:math id="M80" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula>.</p>

      <fig id="F3"><label>Figure 3</label><caption><p id="d2e1691">Final precision-recall curve of the XGBoost classifier for class <inline-formula><mml:math id="M81" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> (good quality) evaluated on the validation set compared to a respective curve for an early boosting round. The curves are colour-coded according to the corresponding decision threshold <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, illustrating how model performance changes as the threshold varies. The circles represent the standard threshold <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> used for assigning the class label <inline-formula><mml:math id="M84" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> in the TROPOMI/WFMD v2.0 quality filter.</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f03.png"/>

          </fig>

      <p id="d2e1749">To interpret the magnitude of potential overfitting, we quantify the achieved gain on the validation set as the decrease in Logloss relative to the baseline entropy and define the relative gap metric <inline-formula><mml:math id="M85" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> to be the ratio of the final training-validation gap to this gain. This metric offers an intuitive way to assess overfitting and how well a model generalises to unknown data that was not used in training. In the present case, <inline-formula><mml:math id="M86" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> is only about <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mn mathvariant="normal">8</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, demonstrating that the final training-validation gap is negligible relative to the validation improvement and that the vast majority of the model's fitted relationships generalise effectively, with overfitting being negligible when assessed in terms of Logloss.</p>
      <p id="d2e1777">In addition to the previous assessment, potential overfitting was further evaluated using the <italic>Area Under the Precision-Recall Curve (AUPRC)</italic>, which is particularly suitable for the present application due to the considerable class imbalance. The AUPRC is specifically meaningful under these conditions as it captures the trade-off between recall (coverage of actual positives) and precision (correctness of positive predictions). It penalises false positives more than other metrics such as the Area Under the Receiver Operating Characteristic Curve (AUROC). This emphasis is in line with practical considerations in quality filtering, where false positives (e.g., cloudy scenes that incorrectly pass the quality filter) can introduce systematic retrieval biases, as such scenes are typically not well characterised by the tabulated forward model.</p>
      <p id="d2e1783">Since a random classifier would produce an AUPRC close to the prevalence <inline-formula><mml:math id="M88" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>, any substantial improvement over this baseline clearly signals successful distinction between classes. Analogous to the Logloss evaluation, the relative gap metric <inline-formula><mml:math id="M89" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> is defined as the ratio of the final training-validation gap to the gain achieved and quantifies potential overfitting in terms of AUPRC. As shown in Fig. <xref ref-type="fig" rid="F2"/>, the AUPRC curve of the validation data set rises monotonically to high values close to the theoretical maximum of <inline-formula><mml:math id="M90" display="inline"><mml:mn mathvariant="normal">1.0</mml:mn></mml:math></inline-formula> and reaches approximately <inline-formula><mml:math id="M91" display="inline"><mml:mn mathvariant="normal">0.92</mml:mn></mml:math></inline-formula> after the completed <inline-formula><mml:math id="M92" display="inline"><mml:mn mathvariant="normal">8000</mml:mn></mml:math></inline-formula> boosting rounds, which is about six times the prevalence baseline. The corresponding <inline-formula><mml:math id="M93" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> is a mere <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, showing that the final difference between the training and validation curves is negligible compared to the improvement achieved on the validation set, which is consistent with the conclusions from the Logloss analysis. Overall, the consistent performance across the complementary evaluation metrics Logloss and AUPRC shows that the implemented XGBoost model validly distinguishes between classes under imbalanced conditions, without showing appreciable signs of overfitting.</p>
      <p id="d2e1847">The resulting precision-recall curve is shown in Fig. <xref ref-type="fig" rid="F3"/> with colour-coded decision threshold <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, which is the minimum level of prediction probability for assigning an instance to class <inline-formula><mml:math id="M96" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> (good quality). The graph illustrates the classifier performance trend when varying the threshold, supporting a more reasonable choice of <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> based on the required balance between precision and recall. In the context of a quality filter, it is helpful to recognise that recall and data yield are positively correlated. Increasing the threshold results in higher precision (reducing the number of false positives) but at the expense of lower recall, meaning that more true positives are missed. Conversely, a lower threshold raises recall, but it also leads to more false positives. For the TROPOMI/WFMD v2.0 quality filter, the standard threshold <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> is used to assign class labels because it is a transparent default that is easy to interpret. This value reflects the point at which the model is equally confident in assigning either class, which is commonly chosen when there is no strong preference for favouring precision over recall. In the current product, this threshold is fixed by design and only the resulting binary quality flag is provided, prioritising simplicity and consistent data quality over enabling user-controlled adjustment of the decision threshold.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Feature importance</title>
      <p id="d2e1909">The XGBoost quality filter is trained on a set of 26 input features, identical to those used in the Random Forest classifier of v1.8 <xref ref-type="bibr" rid="bib1.bibx64" id="paren.27"/>. For transparency and reproducibility, all variables are listed in Table <xref ref-type="table" rid="T1"/>. The features are divided into the following groups according to their functional role: cloud proxies, surface properties, viewing geometry, atmospheric state, retrieval diagnostics, and geospatial context. This categorisation enables a process-oriented interpretation of model behaviour extending beyond the influence of individual variables.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e1920">Input features used by the quality filter, ordered by decreasing mean absolute SHAP importance.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Feature</oasis:entry>
         <oasis:entry colname="col2">Description</oasis:entry>
         <oasis:entry colname="col3">Category</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Difference between ECMWF and retrieved <inline-formula><mml:math id="M100" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> column</oasis:entry>
         <oasis:entry colname="col3">Cloud proxy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">cloud</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Cloud parameter</oasis:entry>
         <oasis:entry colname="col3">Cloud proxy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msubsup><mml:mi>L</mml:mi><mml:mi mathvariant="normal">cloud</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>/</mml:mo><mml:msubsup><mml:mi>L</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Radiance ratio of strong <inline-formula><mml:math id="M103" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> absorption to continuum</oasis:entry>
         <oasis:entry colname="col3">Cloud proxy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msubsup><mml:mi>L</mml:mi><mml:mi mathvariant="normal">cloud</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Radiance in strong <inline-formula><mml:math id="M105" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> absorption lines</oasis:entry>
         <oasis:entry colname="col3">Cloud proxy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Difference between ECMWF and retrieved pressure</oasis:entry>
         <oasis:entry colname="col3">Cloud proxy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Linear polynomial coefficient of spectral fit</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M109" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> retrieval fit error</oasis:entry>
         <oasis:entry colname="col3">Retrieval diagnostics</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Retrieved <inline-formula><mml:math id="M111" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> column</oasis:entry>
         <oasis:entry colname="col3">Atmospheric state</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi mathvariant="normal">type</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Simplified surface type class (water, coastal, land, desert, ice)</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M113" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Retrieved atmospheric temperature</oasis:entry>
         <oasis:entry colname="col3">Atmospheric state</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M114" display="inline"><mml:mi mathvariant="italic">φ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Latitude</oasis:entry>
         <oasis:entry colname="col3">Geospatial context</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M115" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">α</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Retrieved apparent surface albedo</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi mathvariant="normal">RMS</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Root-mean-square of spectral fit residual</oasis:entry>
         <oasis:entry colname="col3">Retrieval diagnostics</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M117" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Across-track dimension index</oasis:entry>
         <oasis:entry colname="col3">Viewing geometry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msubsup><mml:mi>L</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Radiance in continuum-like interval</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mi mathvariant="normal">dry</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Dry air column based on ECMWF</oasis:entry>
         <oasis:entry colname="col3">Atmospheric state</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Difference between ECMWF and retrieved temperature</oasis:entry>
         <oasis:entry colname="col3">Cloud proxy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M121" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Longitude</oasis:entry>
         <oasis:entry colname="col3">Geospatial context</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Solar zenith angle</oasis:entry>
         <oasis:entry colname="col3">Viewing geometry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M124" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> retrieval fit error</oasis:entry>
         <oasis:entry colname="col3">Retrieval diagnostics</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M125" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Surface elevation</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">ϕ</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Relative azimuth angle</oasis:entry>
         <oasis:entry colname="col3">Viewing geometry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>h</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Surface roughness</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Pressure retrieval fit error</oasis:entry>
         <oasis:entry colname="col3">Retrieval diagnostics</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M129" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Retrieved pressure</oasis:entry>
         <oasis:entry colname="col3">Atmospheric state</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Cubic polynomial coefficient of spectral fit</oasis:entry>
         <oasis:entry colname="col3">Surface properties</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e2586">Several of these features provide clear indications of cloud cover. A prime example is the cloud parameter <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">cloud</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, which relates the measured radiances in strong <inline-formula><mml:math id="M132" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> absorption bands to reference radiances for cloud-free conditions <xref ref-type="bibr" rid="bib1.bibx24" id="paren.28"/>. The feature set also includes related radiance-based indicators, which respond in a similar way when clouds are present. Another, conceptually different approach compares ECMWF reanalysis fields with the corresponding retrieved state variables, on the assumption that systematic deviations may occur when clouds interfere with the measurements. High positive values of <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula>, for example, are a typical signature of optically thick clouds that mask part of the atmospheric column. The sign of <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>, on the other hand, is less consistent in cloudy conditions and does not provide an equally clear diagnostic.</p>
      <p id="d2e2654">The interpretability of the model and the importance of the included features are assessed using SHAP (SHapley Additive exPlanations) <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx41" id="paren.29"/>. SHAP values decompose individual predictions into additive contributions from each input feature, allowing both global ranking of feature importance and local interpretation of specific decisions. Figure <xref ref-type="fig" rid="F4"/> summarises the SHAP analysis for the validation data set. Features are ordered by their mean absolute SHAP values, while violin plots illustrate the full distribution and direction of their contributions. Positive SHAP values shift predictions towards the “bad” quality class. The five most influential features are all cloud proxies. In line with physical expectations, high values of these variables correspond to positive SHAP contributions and therefore to rejection by the quality filter. This behaviour reflects either direct shielding of the atmospheric water vapour column by clouds or enhanced radiance in strong <inline-formula><mml:math id="M136" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> absorption bands, which would remain low under clear-sky conditions due to near-saturation of the relevant spectral lines.</p>

      <fig id="F4"><label>Figure 4</label><caption><p id="d2e2677">SHAP-based feature analysis for the XGBoost classifier evaluated on the validation data set. Mean absolute SHAP values (shown in brackets next to each feature) and the corresponding grey bars summarise global feature importance. Violin plots illustrate the distribution and sign of feature contributions, coloured by feature value. The stacked bar shows the relative contribution of the different feature categories to the total mean absolute SHAP.</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f04.png"/>

          </fig>

      <p id="d2e2686">Totalling the SHAP scores by feature category offers a nuanced view of the broader factors that shape the classifier's decisions. Cloud proxies have the greatest impact, accounting for <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mn mathvariant="normal">51</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the total mean absolute SHAP value. Next come surface properties at <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mn mathvariant="normal">17</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, followed by atmospheric state variables (<inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mn mathvariant="normal">11</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>), retrieval diagnostics (<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>), geographical context (<inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mn mathvariant="normal">6</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>), and viewing geometry (<inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>). The weighting of these factors reveals a defined hierarchy in the classification process: the model is primarily based on physically motivated cloud indicators, while the other feature groups provide contextual assistance that refines the interpretation. The relatively modest influence of geographical context demonstrates that latitude and longitude serve as secondary decision modifiers rather than directly driving climatological filtering.</p>

      <fig id="F5"><label>Figure 5</label><caption><p id="d2e2758">Spatial distribution of changes in the number of scenes passing the quality filter <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>N</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, resulting from the inclusion of latitude and longitude as input features. The analysis is based on the validation data set and evaluated on a <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grid. Spatially connected clusters of grid cells in the upper and lower tails of the <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>N</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> distribution are marked as Regions of High Impact (RHI <inline-formula><mml:math id="M146" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> RHI<inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup><mml:mo>∪</mml:mo></mml:mrow></mml:math></inline-formula> RHI<sup>−</sup>), identifying areas where geospatial context leads to the largest net increase or decrease in accepted scenes.</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f05.png"/>

          </fig>

      <p id="d2e2840">To further substantiate this interpretation, a dedicated sensitivity experiment was performed in which geographical features (latitude and longitude) were excluded from model training. All other aspects, including the validation data set used for performance evaluation, were kept unchanged. Comparing the resulting performance with the reference configuration reveals that the inclusion of geospatial context improves global performance, increasing the precision and recall of accepted good-quality scenes by approximately <inline-formula><mml:math id="M149" display="inline"><mml:mn mathvariant="normal">0.8</mml:mn></mml:math></inline-formula> and <inline-formula><mml:math id="M150" display="inline"><mml:mn mathvariant="normal">0.4</mml:mn></mml:math></inline-formula> percentage points, respectively.</p>
      <p id="d2e2858">To localise the impact of geospatial context, Regions of High Impact (RHI) are defined based on changes in the number of scenes passing the quality filter when latitude and longitude are included. These changes are aggregated on a <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grid (Fig. <xref ref-type="fig" rid="F5"/>). Spatially connected clusters of grid cells in the upper and lower tails of the sample-weighted distribution of acceptance changes are labelled RHI<sup>+</sup> and RHI<sup>−</sup>, denoting regions with the largest net increase or decrease in accepted scenes. Their union constitutes the RHI subset, accounting for about <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of all scenes. The improvements in performance are most evident in the RHI. Here, precision and recall increase by about <inline-formula><mml:math id="M155" display="inline"><mml:mn mathvariant="normal">1.7</mml:mn></mml:math></inline-formula> and <inline-formula><mml:math id="M156" display="inline"><mml:mn mathvariant="normal">2.6</mml:mn></mml:math></inline-formula> percentage points, respectively, which is well above the global averages. Furthermore, the inclusion of geolocation features significantly narrows the precision gap for class 0 between RHI<sup>+</sup> and RHI<sup>−</sup> by <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mn mathvariant="normal">66</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, yielding more consistent data quality across regions. Even so, SHAP analysis of the RHI subset shows that cloud proxies remain the primary drivers of the classification (<inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:mn mathvariant="normal">45</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>), with geographic context still playing a comparatively minor role (<inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mn mathvariant="normal">6</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d2e2977">As illustrated in Fig. <xref ref-type="fig" rid="F5"/>, the RHI are not collocated with climatologically cloudy areas. Instead, their defining characteristics are above-average surface brightness and below-average cloudiness. In such regimes, radiance-based indicators become less informative, as optically thick clouds are also linked to increased brightness levels. This reduction in discriminatory ability is likely further intensified by aerosol scattering. Geographic information helps to resolve such ambiguities in quality prediction. When combined with physically based cloud indicators, it provides additional context and supports the exploitation of other feature categories. This means that, in this filtering approach, geolocation is not a shortcut for climatological cloud masking, but rather a supplementary guide for fine-tuning individual decisions.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Post-processing quality control</title>
      <p id="d2e2991">To further maximise the quality of the final data product, we refined the supplementary residual-based and spatial consistency filtering from <xref ref-type="bibr" rid="bib1.bibx64" id="text.30"/>, which is applied after the machine learning quality prediction. This extra step in quality control has two key components: (1) Filtering based on the root mean square of the fit residuals <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mtext>RMS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> as a function of the sun-normalised continuum radiance <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mtext>con</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> (see Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/> for a definition of fit residual and <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mtext>con</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>). Measurements with <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mtext>RMS</mml:mtext></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.03</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mtext>RMS</mml:mtext></mml:msub><mml:mo>&gt;</mml:mo><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>I</mml:mi><mml:mtext>con</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:mi>b</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>+</mml:mo><mml:mi>c</mml:mi></mml:mrow></mml:math></inline-formula> are flagged as bad quality, where the parameters <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mi>a</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0015</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mi>c</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.011</mml:mn></mml:mrow></mml:math></inline-formula> were determined empirically to separate typical values of <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mtext>RMS</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>I</mml:mi><mml:mtext>con</mml:mtext></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> from outliers. The purpose of this filter is to remove specific scenes where the fit quality is worse than for other scenes with similar radiance. Such anomalies can arise, for example, from high aerosol concentrations or other unusual atmospheric conditions. (2) Downward outlier detection in three-dimensional (latitude, longitude, <inline-formula><mml:math id="M171" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)-space on a daily basis with the Density-Based Spatial Clustering of Applications with Noise (DBSCAN) <xref ref-type="bibr" rid="bib1.bibx19" id="paren.31"/>. This clustering algorithm groups spatially dense points and marks points in low-density regions as outliers. It is utilised instead of the previously used Local Outlier Factor (LOF) as it tends to be more robust in areas where data points are distributed more sparsely. Together, these two filtering steps remove roughly <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.5</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the data that initially passed the machine learning quality screening; about <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.2</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> are rejected by the <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mtext>RMS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> filter and about <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.3</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> by DBSCAN's outlier detection. The overall removal rate corresponds almost exactly to that of the previous method.</p>
      <p id="d2e3212">As a follow-up to the performance evaluation of the XGBoost-based quality filter with unseen data, the precision in identifying cloud-free retrievals is analysed in the subsequent statistical analysis. To this end, Fig. <xref ref-type="fig" rid="F6"/> compares the percentage of actually cloud-free scenes (<italic>confidently cloudy</italic> sub-scene fraction below <inline-formula><mml:math id="M176" display="inline"><mml:mn mathvariant="normal">0.1</mml:mn></mml:math></inline-formula> according to VIIRS) among all scenes that pass the quality filter for v2.0 and v1.8. At all latitude bands considered, v2.0 consistently achieves better precision than v1.8, reflecting an improvement in the reliability of cloud filtering as there is less misclassified data falsely passing quality screening. Nevertheless, the data yield is generally increasing at the same time, especially in the mid and high latitudes, as the brown bars in the figure indicate. The only exception is the band closer to the equator, which also includes regions with frequent aerosol exposure like the Sahara Desert; there is a small decline in scenes classified as good, contrary to the general trend. This decrease suggests that certain aerosol-affected scenes are better removed, which was intended by including the TROPOMI Aerosol Index in the training of the quality filter.</p>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e3241">Precision of the quality filter concerning identification of cloud-free scenes in versions 1.8 and 2.0, shown for selected latitude ranges. Precision is defined as the percentage of actually cloud-free scenes according to VIIRS among those passing the quality filter. The brown bars highlight the change in the absolute number of good quality scenes (v2.0 relative to v1.8).</p></caption>
            <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f06.png"/>

          </fig>

      <p id="d2e3255">Overall, these results suggest that version 2.0 delivers both improved data quality and increased data yield, except under certain challenging conditions, such as those involving desert aerosols, where somewhat more data is filtered out. However, this observation still needs to be confirmed by validation with independent reference data (see Sect. <xref ref-type="sec" rid="Ch1.S3"/>) and a detailed analysis of the regional patterns of the satellite data (see Sect. <xref ref-type="sec" rid="Ch1.S4"/>). It needs to be emphasised that the subsequent shallow machine learning calibration, based on a Random Forest Regressor, to reduce the remaining systematic errors in the <inline-formula><mml:math id="M177" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> data remains the same as in v1.8. Specifically, the training regions, the maximum tree growth limit, and the small set of input features, mainly related to albedo, have not been changed. Even though the settings remain identical, this post-processing correction might perform better with the current version as the improved quality filter produces more consistent data, helping the regressor model to learn the core relationships more effectively.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Validation</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Random and spatial systematic errors</title>
      <p id="d2e3290">TCCON is a global network of ground-based Fourier-transform spectrometers that measure direct solar radiation in the near- and shortwave-infrared spectral region to retrieve precise column-averaged abundances of trace gases such as <inline-formula><mml:math id="M178" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M179" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>, serving as a benchmark for satellite data validation <xref ref-type="bibr" rid="bib1.bibx89" id="paren.32"/>. All sites operate similar instrumentation (Bruker IFS 125HR) and use a standardised retrieval algorithm. Data are tied to the WMO trace gas scale using airborne in-situ measurements with species-specific scaling factors, yielding estimated accuracies of about <inline-formula><mml:math id="M180" display="inline"><mml:mn mathvariant="normal">4</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M181" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M182" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M183" display="inline"><mml:mn mathvariant="normal">2</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M184" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> in the GGG2020 version used here <xref ref-type="bibr" rid="bib1.bibx35" id="paren.33"/>.</p>
      <p id="d2e3368">To enable a quantitative comparison with satellite data, the differences in instrument sensitivity and prior profiles must be taken into account. This involves adjusting the measurements for the influence of their native prior profiles using a common prior <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx17 bib1.bibx63" id="paren.34"/>, here taken from the TCCON:

            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M186" display="block"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi mathvariant="normal">adj</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><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>m</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>l</mml:mi></mml:munder><mml:msub><mml:mi>m</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">a</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow><mml:mi>l</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>x</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mi>l</mml:mi></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M187" display="inline"><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula> is the original TROPOMI retrieval, <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the satellite averaging kernel, <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mrow><mml:mi mathvariant="normal">a</mml:mi><mml:mo>,</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> the TROPOMI and TCCON prior profiles, respectively. <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> denotes the dry air mass in layer <inline-formula><mml:math id="M192" display="inline"><mml:mi>l</mml:mi></mml:math></inline-formula> from pressure differences corrected for water vapour, and <inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the total dry air mass. The averaging kernels of the satellite data product are illustrated in Fig. <xref ref-type="fig" rid="F7"/>, demonstrating that the retrievals are sensitive to all atmospheric layers.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e3546">Averaging kernels of the TROPOMI/WFMD v2.0 satellite data product used in the prior profile adjustment of Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>). Shown are the averaging kernels of all measurements from every second day of a given year for <bold>(a)</bold> <inline-formula><mml:math id="M194" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>, illustrating the vertical sensitivities of the satellite retrievals.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f07.png"/>

        </fig>

      <p id="d2e3588">Theoretically, smoothing errors can be further reduced by adjusting the TCCON results <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> before the comparison with <inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi mathvariant="normal">adj</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> using the retrieved TCCON profile scaling factors in conjunction with the satellite averaging kernels <xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx90 bib1.bibx63" id="paren.35"/>. However, this second correction step is omitted in the present analysis for the sake of simplicity, as it became apparent in the past that this adjustment is negligible in the validation of TROPOMI/WFMD. Since the satellite averaging kernels in the lower atmosphere are sufficiently close to <inline-formula><mml:math id="M198" display="inline"><mml:mn mathvariant="normal">1.0</mml:mn></mml:math></inline-formula>, the resulting correction would be in the sub-ppb range, which is significantly smaller than the systematic errors associated with the TROPOMI and TCCON retrievals.</p>
      <p id="d2e3634">To account for surface elevation differences between TROPOMI observations and TCCON measurements, a height correction is applied to the retrieved column-averaged dry-air mole fractions <inline-formula><mml:math id="M199" display="inline"><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula>, such that the collocated data pairs are referenced to a common surface pressure <xref ref-type="bibr" rid="bib1.bibx67" id="paren.36"/>. Specifically, this height correction estimates the mole fraction that would be retrieved by the satellite measurement, had the retrieval been performed at the surface pressure, <inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, of the TCCON station, rather than at the original TROPOMI surface pressure, <inline-formula><mml:math id="M201" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>. This adjustment incorporates the retrieved TROPOMI profile scaling factor <inline-formula><mml:math id="M202" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">γ</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover></mml:math></inline-formula>, assuming that the scaling factor does not change but the associated profile <inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is suitably extended or truncated consistent with the updated surface pressure. The complete height-correction is given by

            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M204" display="block"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mrow><mml:mi>P</mml:mi><mml:mo>→</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mover accent="true"><mml:mi>c</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mo>⋅</mml:mo><mml:mi>P</mml:mi><mml:mo>+</mml:mo><mml:mover accent="true"><mml:mi mathvariant="italic">γ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">d</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:mfenced><mml:msubsup><mml:mi>P</mml:mi><mml:mi>T</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></disp-formula>

          where the integral accounts for the additional or missing air mass resulting from the difference in surface pressure. The generic prior <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is available across all realistic pressures and can therefore be applied when <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>T</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula> as well. The integral inherently yields the correct sign depending on whether <inline-formula><mml:math id="M207" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> or <inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is greater.</p>
      <p id="d2e3823">The validation is performed using the latest TCCON data version GGG2020 <xref ref-type="bibr" rid="bib1.bibx35" id="paren.37"/> and the <inline-formula><mml:math id="M209" display="inline"><mml:mn mathvariant="normal">26</mml:mn></mml:math></inline-formula> sites listed in Table <xref ref-type="table" rid="TC1"/>. The used collocation criteria balance representativity and statistical robustness: Satellite data must be within <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> horizontally and <inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:mn mathvariant="normal">500</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> vertically of the TCCON site, with a maximum time difference of <inline-formula><mml:math id="M212" display="inline"><mml:mn mathvariant="normal">2</mml:mn></mml:math></inline-formula> h between observations. Since sources in the vicinity of Edwards and Xianghe limit the representability, the collocation radius for these two locations is reduced to <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mn mathvariant="normal">50</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>
<xref ref-type="bibr" rid="bib1.bibx63" id="paren.38"/>.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e3887">Comparison of the TROPOMI/WFMD v2.0 <inline-formula><mml:math id="M214" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> time series (green) with ground based measurements from the TCCON (red). For each site, <inline-formula><mml:math id="M215" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> is the number of collocations, <inline-formula><mml:math id="M216" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> corresponds to the mean local bias and <inline-formula><mml:math id="M217" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> to the scatter of the satellite data relative to TCCON in ppb.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f08.jpg"/>

        </fig>

      <p id="d2e3933">The validation results are summarised in Figs. <xref ref-type="fig" rid="F8"/> and <xref ref-type="fig" rid="F9"/> including the mean local offsets <inline-formula><mml:math id="M218" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> and the scatter <inline-formula><mml:math id="M219" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> relative to the TCCON for each site. The results for the individual sites are condensed to the following figures of merit for the overall quality assessment of the satellite data: the global offset <inline-formula><mml:math id="M220" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> is defined as the mean of the local biases at the individual sites, the random error <inline-formula><mml:math id="M221" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">σ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> is the site-wise mean scatter relative to the TCCON, and the spatial systematic error <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the standard deviation of the local offsets relative to the TCCON at the individual sites as a measure of the station-to-station biases. For <inline-formula><mml:math id="M223" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the global offset amounts to <inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.65</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M225" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula>, the random error is <inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">σ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mn mathvariant="normal">13.35</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M227" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula>, and the spatial systematic error is given by <inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4.46</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M229" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula>. For <inline-formula><mml:math id="M230" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>, the corresponding values are <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.44</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M232" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">σ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.55</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M234" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.67</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M236" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula>. Thus, the estimated spatial systematic errors for both species are on the order of the estimated (station-to-station) accuracy of the TCCON. In the case of <inline-formula><mml:math id="M237" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the largest scatter <inline-formula><mml:math id="M238" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> relative to TCCON is observed at high northern latitude sites, with the largest local offset <inline-formula><mml:math id="M239" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> at Eureka. These features are attributed to the influence of the polar vortex, which can introduce representation errors when the vortex boundary lies between the TCCON site and individual satellite measurements, leading to genuine differences in <inline-formula><mml:math id="M240" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> between the two data sets <xref ref-type="bibr" rid="bib1.bibx21" id="paren.39"/>.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e4199">As Fig. <xref ref-type="fig" rid="F8"/> but for <inline-formula><mml:math id="M241" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>. Individual collocated pairs with lower agreement are typically associated with wildfire events, e.g., when there is a true <inline-formula><mml:math id="M242" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> enhancement in a distant satellite scene but not directly at the TCCON site or vice versa (representation error).</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f09.jpg"/>

        </fig>

      <p id="d2e4226">Figure <xref ref-type="fig" rid="F10"/> shows how the validation results compare to the previous version 1.8. Overall, the number of collocations has increased by about <inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> in version 2.0, thanks to better data coverage. In the Arctic in particular, coverage improved by roughly <inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:mn mathvariant="normal">40</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, which reflects the enhanced data yield under challenging conditions, such as high solar zenith angles and low surface reflectivity. Even though the number of collocations <inline-formula><mml:math id="M245" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> is larger, which often introduces more variability, both the random and systematic errors have actually improved in v2.0, indicating more consistent and reliable retrievals. The only exception is the spatial systematic <inline-formula><mml:math id="M246" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> error, which remains mostly unchanged. Furthermore, the global offset <inline-formula><mml:math id="M247" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> of <inline-formula><mml:math id="M248" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> relative to the TCCON has been significantly reduced and is now nearly zero. While this former global offset was not a critical quality issue since it could be easily corrected with a dedicated bias correction, the fact that it is improved aligns well with the better accuracy of the new v2.0 data product.</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e4292">Comparison of the retrieval results for TROPOMI/WFMD v1.8 and v2.0. The comparison was limited to the period during which both product versions were available (May 2018–June 2024). As a result, the numbers differ slightly from those in the full validation of v2.0.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f10.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Seasonal biases</title>
      <p id="d2e4313">In order to further analyse the intra-annual variability of the discrepancies between the collocated TROPOMI and TCCON data, the site-specific mean offsets <inline-formula><mml:math id="M249" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> are first subtracted from the differences of the individual data pairs to remove the already discussed spatial bias component. The resulting anomalies are then grouped by season and categorised as January–March (JFM), April–June (AMJ), July–September (JAS), and October–December (OND). To summarise joint seasonal characteristics, the sites are additionally divided into broad latitudinal bands, namely Arctic (<inline-formula><mml:math id="M250" display="inline"><mml:mn mathvariant="normal">90</mml:mn></mml:math></inline-formula>–<inline-formula><mml:math id="M251" display="inline"><mml:mn mathvariant="normal">66.5</mml:mn></mml:math></inline-formula>° N), Northern mid-latitudes (<inline-formula><mml:math id="M252" display="inline"><mml:mn mathvariant="normal">66.5</mml:mn></mml:math></inline-formula>–<inline-formula><mml:math id="M253" display="inline"><mml:mn mathvariant="normal">23.5</mml:mn></mml:math></inline-formula>° N), Tropics (<inline-formula><mml:math id="M254" display="inline"><mml:mn mathvariant="normal">23.5</mml:mn></mml:math></inline-formula>–<inline-formula><mml:math id="M255" display="inline"><mml:mn mathvariant="normal">23.5</mml:mn></mml:math></inline-formula>° S), and Southern mid-latitudes (<inline-formula><mml:math id="M256" display="inline"><mml:mn mathvariant="normal">23.5</mml:mn></mml:math></inline-formula>–<inline-formula><mml:math id="M257" display="inline"><mml:mn mathvariant="normal">66.5</mml:mn></mml:math></inline-formula>° S). Since there are many TCCON sites in the Northern Hemisphere's mid-latitudes, this band is further separated into smaller sub-regions based on longitude (North America, Europe, and Asia). The associated spatio-temporal averages are only included in the analysis for those combinations of region and season that contain data from at least three different years for more than one calendar month of the respective season in order to ensure statistical robustness.</p>

      <fig id="F11" specific-use="star"><label>Figure 11</label><caption><p id="d2e4386">Seasonal mean biases for <bold>(a)</bold> <inline-formula><mml:math id="M258" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M259" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> relative to the TCCON for the analysed regions. Masked cells indicate insufficient coverage (see main text for details). Row and column averages further summarise the overarching regional and seasonal variability. The standard deviation of the seasonal biases across all regions is interpreted as the overall seasonal bias and indicated in the bottom-right corner. <bold>(c)</bold> Number of collocations <inline-formula><mml:math id="M260" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> for the different combinations of region and season. The number of contributing years <inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">y</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is shown in the top-left corner of each cell; the number of calendar months <inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> contributing data to the corresponding 3-month season is displayed in the bottom-right corner of each cell, only if it is smaller than the maximum value of 3.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f11.png"/>

        </fig>

      <p id="d2e4453">The results are displayed as heat maps in Fig. <xref ref-type="fig" rid="F11"/>, where the average bias values are annotated on the corresponding cells and entries with insufficient sampling are masked. In addition, the row and column mean values provide an average overview of regional and seasonal variations, respectively. The total seasonal bias relative to the TCCON is then calculated as the standard deviation of the individual biases across all regions and seasons, resulting in <inline-formula><mml:math id="M263" display="inline"><mml:mn mathvariant="normal">1.92</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M264" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M265" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M266" display="inline"><mml:mn mathvariant="normal">1.10</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M267" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M268" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Uncertainties</title>
      <p id="d2e4516">The individual uncertainties of the TROPOMI/WFMD measurements are provisionally estimated during the inversion process by error propagation based on the uncorrelated spectral errors provided in the TROPOMI Level 1 files. However, this estimate does not take into account pseudo-noise components that may arise from specific atmospheric conditions or instrumental characteristics, nor systematic uncertainties associated with spectroscopic parameters. For this reason, the initial uncertainty estimates tend to underestimate the actual measurement error and are therefore inflated by a simple linear adjustment to provide more realistic values <xref ref-type="bibr" rid="bib1.bibx61" id="paren.40"/>.</p>
      <p id="d2e4530">The resulting final uncertainties <inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>unc</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> reported in the TROPOMI/WFMD v2.0 product are checked by comparison with the actual measured scatter relative to the TCCON. To this end, a data-driven adaptive binning approach based on <inline-formula><mml:math id="M270" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means<inline-formula><mml:math id="M271" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula> clustering <xref ref-type="bibr" rid="bib1.bibx2" id="paren.41"/> is applied as a preparatory step. This approach divides the data into discrete bins of similar uncertainty by minimising the within-cluster variance. For each of these bins, the mean reported uncertainty is calculated and compared to the actual observed scatter of the differences relative to the TCCON. The results presented in Fig. 10 demonstrate that the uncertainty estimates provided are generally realistic, as evidenced by the fact that the mean uncertainty ratio <inline-formula><mml:math id="M272" display="inline"><mml:mover accent="true"><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula>, defined as the reported uncertainty divided by the measured scatter, is close to <inline-formula><mml:math id="M273" display="inline"><mml:mn mathvariant="normal">1.0</mml:mn></mml:math></inline-formula> (<inline-formula><mml:math id="M274" display="inline"><mml:mn mathvariant="normal">1.03</mml:mn></mml:math></inline-formula> for <inline-formula><mml:math id="M275" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M276" display="inline"><mml:mn mathvariant="normal">1.01</mml:mn></mml:math></inline-formula> for <inline-formula><mml:math id="M277" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>), which is what one would expect from a reliable, high-quality uncertainty estimate. There is a slight overall tendency to overestimate the uncertainties on average (<inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>), with the exception of the rather rare cases of poor <inline-formula><mml:math id="M279" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> precision, where the reported uncertainties of the satellite data appear to be somewhat underestimated.</p>

      <fig id="F12" specific-use="star"><label>Figure 12</label><caption><p id="d2e4645">Comparison of reported uncertainties in the TROPOMI/WFMD v2.0 product with the measured scatter relative to the TCCON for <bold>(a)</bold> <inline-formula><mml:math id="M280" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M281" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>. In the blue-shaded areas, reported uncertainties exceed the observed scatter (overestimation), whereas in the yellow-shaded areas, they fall below it (underestimation).</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f12.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Surface albedo sensitivity</title>
      <p id="d2e4692">To investigate possible albedo-related biases in the TROPOMI/WFMD product, the sensitivity of TROPOMI to TCCON discrepancies with respect to surface albedo variability is examined on a daily basis, taking into account site-specific offsets that could complicate the determination of such a relationship. Although the local offsets determined during the validation are probably largely independent of albedo, it cannot be entirely excluded that albedo also contributes to some extent to the site-specific biases. To rigorously account for this by disentangling these components, a joint hierarchical Bayesian linear regression model from the probabilistic programming library <italic>PyMC</italic> <xref ref-type="bibr" rid="bib1.bibx1" id="paren.42"/> is applied, which allows comprehensive uncertainty quantification and propagation, enabling a fully probabilistic characterisation of albedo sensitivity. In this framework, site-specific offsets are modelled as random intercepts informed by the previous validation results, while the relationship between surface albedo and the difference to the TCCON is represented by a global fixed regression slope <inline-formula><mml:math id="M282" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> across all sites. Consequently, the hierarchical approach leaves the model free to attribute parts of the estimated local biases to albedo, thus yielding a more realistic estimate of <inline-formula><mml:math id="M283" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>.</p>
      <p id="d2e4724">The model inference is performed by Markov Chain Monte Carlo sampling using the No-U-Turn Sampler (NUTS), an adaptive Hamiltonian Monte Carlo algorithm that efficiently explores high-dimensional posterior distributions, even in the presence of complex hierarchical structures. In the specific case presented here, six independent chains are run in parallel and their convergence to a common posterior distribution is evaluated using the potential scale reduction factor <inline-formula><mml:math id="M284" display="inline"><mml:mover accent="true"><mml:mi>R</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula>
<xref ref-type="bibr" rid="bib1.bibx79" id="paren.43"/>, which compares the variance between multiple chains to the within-chain variance. Values of <inline-formula><mml:math id="M285" display="inline"><mml:mover accent="true"><mml:mi>R</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula> close to <inline-formula><mml:math id="M286" display="inline"><mml:mn mathvariant="normal">1.0</mml:mn></mml:math></inline-formula> indicate that the chains have mixed well, i.e., they have sufficiently explored the parameter space and converged to virtually the same posterior distribution.</p>
      <p id="d2e4757">To inform plausible data-driven values for the slope parameter <inline-formula><mml:math id="M287" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>, the observed albedo range is divided into bins of fixed width. Within each bin, the median values of albedo, <inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (satellite minus collocated TCCON measurements) are calculated, and the respective slopes for all possible pairs of bins are computed to obtain an empirical distribution that reflects the variability over the entire domain. The median absolute deviation (MAD) of these pairwise slopes is then used to conservatively estimate the variability <inline-formula><mml:math id="M290" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">β</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. Assuming a normal prior centered at zero, this defines a weakly informative normal prior for the slope parameter <inline-formula><mml:math id="M291" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>.</p>
      <p id="d2e4810">With <inline-formula><mml:math id="M292" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> denoting individual daily averaged observations and <inline-formula><mml:math id="M293" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> indexing TCCON sites, the complete hierarchical model includes hyperpriors on site-level intercepts, additional informative validation-based anchor data, a linear predictor combining site biases and albedo dependence, and a likelihood assuming normally distributed observational uncertainties:

            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M294" display="block"><mml:mrow><mml:mtable class="array" rowspacing="0.2ex 14.226378pt 0.2ex 14.226378pt 14.226378pt 0.2ex" columnalign="left left left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>∼</mml:mo><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mtext>with</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mo>∼</mml:mo><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mo>∼</mml:mo><mml:mi mathvariant="script">H</mml:mi><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>a</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub><mml:mo>∼</mml:mo><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>eff</mml:mtext><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mtext>with</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>eff</mml:mtext><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:msqrt><mml:mrow><mml:mi>f</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi>N</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:msqrt></mml:mfrac></mml:mstyle></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd/><mml:mtd><mml:mrow><mml:mi>f</mml:mi><mml:mo>∼</mml:mo><mml:mi mathvariant="script">B</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mtext>with</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>∼</mml:mo><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">β</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>∼</mml:mo><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>obs</mml:mtext><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mtext>with</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>obs</mml:mtext><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>unc</mml:mtext><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>res</mml:mtext><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>]</mml:mo></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>res</mml:mtext><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:msub><mml:mo>∼</mml:mo><mml:mi mathvariant="script">H</mml:mi><mml:mi mathvariant="script">N</mml:mi><mml:mo>(</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mstyle><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">σ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mtext>unc</mml:mtext></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M295" display="inline"><mml:mi mathvariant="script">N</mml:mi></mml:math></inline-formula> denotes a normal distribution, <inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:mi mathvariant="script">H</mml:mi><mml:mi mathvariant="script">N</mml:mi></mml:mrow></mml:math></inline-formula> denotes a half-normal distribution, and <inline-formula><mml:math id="M297" display="inline"><mml:mi mathvariant="script">B</mml:mi></mml:math></inline-formula> a Beta distribution. The systematic errors <inline-formula><mml:math id="M298" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> and <inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> estimated from the preceding validation are used to construct the prior for <inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, which describes the site-specific bias for site <inline-formula><mml:math id="M301" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>. The local biases are further informed by observed validation-based estimates <inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>a</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, which are treated as noisy measurements with effective standard errors <inline-formula><mml:math id="M303" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>eff</mml:mtext><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> reflecting the corresponding uncertainties of the previously obtained local offset estimates <inline-formula><mml:math id="M304" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from validation. Thereby, the co-fitted factor <inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>∈</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> shrinks the collocation sample size <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in computing the standard error from the scatter <inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> relative to the TCCON. The parameters <inline-formula><mml:math id="M308" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are defined as in Figs. <xref ref-type="fig" rid="F8"/> and <xref ref-type="fig" rid="F9"/> but for daily averages. The quantity <inline-formula><mml:math id="M311" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the mean response predicted by the model for observation <inline-formula><mml:math id="M312" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (where <inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:mi>j</mml:mi><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> refers to the site associated with <inline-formula><mml:math id="M314" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>), <inline-formula><mml:math id="M315" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> denotes the associated surface albedo, and <inline-formula><mml:math id="M316" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the observed differences to TCCON, incorporating both the daily averaged reported observational uncertainty <inline-formula><mml:math id="M317" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>unc</mml:mtext><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (see previous subsection) and site-level residual variability <inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mtext>res</mml:mtext><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>[</mml:mo><mml:mi>i</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>. The additional <inline-formula><mml:math id="M319" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>res</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> may be elevated at specific sites, for example due to representation errors during wildfire events, when for some <inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the two involved data sets are differently affected by corresponding <inline-formula><mml:math id="M321" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> enhancements as a result of spatial separation.</p>
      <p id="d2e5524">In Fig. <xref ref-type="fig" rid="F13"/>, the posterior mean values of the site-specific intercepts <inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> have been subtracted from the observed <inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M324" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values to focus on their dependence on surface albedo. The resulting residuals are free of site-to-site biases and are thus ideally suited to analyse the pure albedo sensitivity <inline-formula><mml:math id="M325" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> of the data. The arising marginal posterior distributions of the albedo sensitivity parameter are shown as insets in the figure together with the results of the individual Markov Chains. The excellent agreement between the individual resulting distributions, with an associated potential scale reduction factor <inline-formula><mml:math id="M326" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>R</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi mathvariant="italic">β</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> close to <inline-formula><mml:math id="M327" display="inline"><mml:mn mathvariant="normal">1.0</mml:mn></mml:math></inline-formula> in both cases, demonstrates that the sampling chains have reliably converged to a common posterior distribution.</p>

      <fig id="F13" specific-use="star"><label>Figure 13</label><caption><p id="d2e5596">Assessment of the surface albedo sensitivity of TROPOMI/WFMD v2.0 <bold>(a)</bold>
<inline-formula><mml:math id="M328" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M329" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> based on daily means. Residual <inline-formula><mml:math id="M330" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M331" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> were obtained by subtracting the posterior mean site-specific intercepts from the observed differences to remove site-to-site biases. The fitted slope <inline-formula><mml:math id="M332" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> and its <inline-formula><mml:math id="M333" display="inline"><mml:mrow><mml:mn mathvariant="normal">95</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> credible band are overlaid illustrating the inferred sensitivity to surface albedo for each trace gas. The insets show the respective marginal posterior distribution of the albedo sensitivity parameter <inline-formula><mml:math id="M334" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> from the hierarchical model. The width of the distribution reflects the inferred uncertainty in the slope, with the peak indicating the most probable value.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f13.png"/>

        </fig>

      <p id="d2e5685">The found surface albedo sensitivity in the case of <inline-formula><mml:math id="M335" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math id="M336" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M337" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> for a unit increase in albedo (<inline-formula><mml:math id="M338" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>), with a coefficient of determination <inline-formula><mml:math id="M339" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0002</mml:mn></mml:mrow></mml:math></inline-formula>. This means that there is a statistically significant positive relationship between surface albedo and <inline-formula><mml:math id="M340" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>, but albedo explains only a marginal fraction of the overall variance. Some additional uncertainty arises from the fact that the TCCON collocations may not fully represent the entire range of naturally occurring surface albedos. For <inline-formula><mml:math id="M341" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the estimated sensitivity is <inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M343" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> per unit albedo, with <inline-formula><mml:math id="M344" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0001</mml:mn></mml:mrow></mml:math></inline-formula> suggesting that there is no significant bias due to surface albedo. If we consider only the two neighbouring sites, Edwards and Caltech, whose combined albedo range already extends from <inline-formula><mml:math id="M345" display="inline"><mml:mn mathvariant="normal">0.1</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M346" display="inline"><mml:mn mathvariant="normal">0.4</mml:mn></mml:math></inline-formula>, the sensitivities for both gases are very similar to those obtained in the full analysis, albeit with increased uncertainty. Since albedo is a dimensionless quantity with values ranging from <inline-formula><mml:math id="M347" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M348" display="inline"><mml:mn mathvariant="normal">1</mml:mn></mml:math></inline-formula>, and typical observed albedo values cover a considerably narrower subrange, the practical influence of surface albedo on <inline-formula><mml:math id="M349" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M350" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is correspondingly even smaller. Thus, the albedo-induced bias under typical conditions is limited to the sub-ppb range. These results imply that surface albedo has a minor impact on the <inline-formula><mml:math id="M351" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> retrievals and a negligible effect on <inline-formula><mml:math id="M352" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in terms of retrieval biases.</p>
      <p id="d2e5881">Because the albedo range covered by the TCCON comparison is limited (<inline-formula><mml:math id="M353" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>≲</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>), an additional analysis independent of the TCCON is performed to further assess albedo sensitivity. In the absence of a reference data set to serve as ground truth, a region with negligible methane emissions has to be selected. For this reason, the Sahara is used here (see Fig. <xref ref-type="fig" rid="F14"/>), which also has high albedo variability and is therefore well-suited for this analysis. To remove the influence of the seasonal cycle and the long-term methane increase, the seasonal and level components of a Dynamic Linear Model (DLM) <xref ref-type="bibr" rid="bib1.bibx20" id="paren.44"/> based on daily data are subtracted from the time series of individual satellite observations, yielding an anomaly <inline-formula><mml:math id="M354" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">gas</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for each measurement. The albedo sensitivity  is then estimated as the slope parameter <inline-formula><mml:math id="M355" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> of a linear regression fit between these anomalies and surface albedo. To assess uncertainty, we use a subsampling bootstrap technique, in which random subsets of <inline-formula><mml:math id="M356" display="inline"><mml:mn mathvariant="normal">1000</mml:mn></mml:math></inline-formula> data points are repeatedly drawn from the complete data set and linear regression is re-performed on each subset. This yields empirical distributions of the regression parameters, from which uncertainties are quantified using the corresponding <inline-formula><mml:math id="M357" display="inline"><mml:mrow><mml:mn mathvariant="normal">95</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> credible bands.</p>

      <fig id="F14" specific-use="star"><label>Figure 14</label><caption><p id="d2e5942">Assessment of the surface albedo sensitivity of TROPOMI/WFMD v2.0 over the Sahara (white region) for <bold>(a)</bold> <inline-formula><mml:math id="M358" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M359" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> after subtracting the seasonal and level components of a fitted Dynamic Linear Model (DLM). The fitted slope <inline-formula><mml:math id="M360" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> and its <inline-formula><mml:math id="M361" display="inline"><mml:mrow><mml:mn mathvariant="normal">95</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> credible band are overlaid illustrating the inferred sensitivity to surface albedo for each trace gas.</p></caption>
          <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f14.png"/>

        </fig>

      <p id="d2e6000">The findings align with the TCCON-based results and show that there is no evidence of critical albedo-related biases in the TROPOMI/WFMD data. In fact, the estimated surface albedo sensitivities <inline-formula><mml:math id="M362" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> are of the same order of magnitude as in the TCCON assessment and do not differ significantly from zero. The magnitude of the uncertainty estimates is about four times greater than that of the TCCON analysis. Specifically, the sensitivities are <inline-formula><mml:math id="M363" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">6.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M364" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> per unit albedo for <inline-formula><mml:math id="M365" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M366" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3.2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M367" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M368" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>, with a coefficient of determination of <inline-formula><mml:math id="M369" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.002</mml:mn></mml:mrow></mml:math></inline-formula> in both cases.</p>
</sec>
<sec id="Ch1.S3.SS5">
  <label>3.5</label><title>Summary of validation results</title>
      <p id="d2e6106">Independent ground-based measurements from the TCCON confirmed that the updated TROPOMI/WFMD v2.0 <inline-formula><mml:math id="M370" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M371" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> products have higher quality than the previous version. The refined retrievals are not only more accurate and precise, but also provide increased data yield at mid and high latitudes, including observationally challenging regions such as the Arctic. The broader coverage of v2.0 is beneficial for all types of applications, whether at the regional level, such as quantifying local hotspot emissions, or on a larger scale, like analysing growth rates of latitude bands. According to the review of the uncertainties reported for each measurement, the estimates are reasonable and realistic. Furthermore, the analysis showed that surface albedo does not introduce any relevant biases into the data products. This is an important finding as albedo-related biases are often a concern in the application of TROPOMI methane retrievals <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx3" id="paren.45"/>.</p>
      <p id="d2e6144">The improved performance relative to the previous version is driven primarily by the updated quality filtering, whereas the additional processing changes have only a minor effect in comparison. The quality assessment results are summarised in Table <xref ref-type="table" rid="T2"/>, including metrics that measure both random and systematic errors of the data product. These figures of merit give a clear overview of how well the TROPOMI/WFMD v2.0 products perform and are helpful benchmarks for users intending to use the data in scientific research. The reported values should be interpreted as upper limits, reflecting uncertainties in the TCCON reference as well as potential representation errors arising from the non-zero collocation radius, particularly when one instrument is affected by local events such as wildfires or the polar vortex and the other is not.</p>

<table-wrap id="T2"><label>Table 2</label><caption><p id="d2e6156">Figures of merit from the quality assessment of TROPOMI/WFMD v2.0 using TCCON GGG2020. The total systematic error is defined as the root-sum-square of the spatial and seasonal systematic errors. Also shown is the derived albedo sensitivity from the TCCON-independent time series analysis over the Sahara in italics.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M372" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M373" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Random Error <inline-formula><mml:math id="M374" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">σ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> (ppb)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M375" display="inline"><mml:mn mathvariant="normal">13.35</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M376" display="inline"><mml:mn mathvariant="normal">5.55</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Global Offset <inline-formula><mml:math id="M377" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">μ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> (ppb)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M378" display="inline"><mml:mn mathvariant="normal">0.65</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M379" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.44</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spatial Systematic Error <inline-formula><mml:math id="M380" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> (ppb)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M381" display="inline"><mml:mn mathvariant="normal">4.46</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M382" display="inline"><mml:mn mathvariant="normal">2.67</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Seasonal Systematic Error (ppb)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M383" display="inline"><mml:mn mathvariant="normal">1.92</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M384" display="inline"><mml:mn mathvariant="normal">1.10</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total Systematic Error (ppb)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M385" display="inline"><mml:mn mathvariant="normal">4.86</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M386" display="inline"><mml:mn mathvariant="normal">2.89</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Uncertainty Ratio <inline-formula><mml:math id="M387" display="inline"><mml:mover accent="true"><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M388" display="inline"><mml:mn mathvariant="normal">1.03</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M389" display="inline"><mml:mn mathvariant="normal">1.01</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">[reported/measured] (–)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Albedo sensitivity (ppb)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M390" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M391" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Albedo sensitivity [Sahara] (ppb)</italic></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M392" display="inline"><mml:mrow><mml:mn mathvariant="italic">4.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="italic">6.5</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M393" display="inline"><mml:mrow><mml:mn mathvariant="italic">2.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="italic">3.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e6463">Overall, the TROPOMI/WFMD v2.0 product performs reliably in retrieving <inline-formula><mml:math id="M394" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M395" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> from actual TROPOMI data, achieving accuracy and precision levels well within the mission requirements after appropriate quality filtering. In concrete terms, this means that the products meet the strict limits of less than <inline-formula><mml:math id="M396" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.5</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> bias and <inline-formula><mml:math id="M397" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.0</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> random error for <inline-formula><mml:math id="M398" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, as well as less than <inline-formula><mml:math id="M399" display="inline"><mml:mrow><mml:mn mathvariant="normal">15</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> bias and <inline-formula><mml:math id="M400" display="inline"><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> random error for <inline-formula><mml:math id="M401" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>, confirming the suitability of the algorithm for quasi-operational processing of TROPOMI measurements.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Regional assessments</title>
      <p id="d2e6566">To elucidate how the improvements in TROPOMI/WFMD v2.0 manifest in the retrieval results, this section examines regional patterns in the data products. While previous sections focussed on evaluating the trained quality filter using unseen data and validation with independent reference measurements from the TCCON, the spatially resolved assessment here reveals how these refinements translate specifically into increased regional coverage. While this section mainly discusses <inline-formula><mml:math id="M402" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> because of its stricter quality requirements, it is worth noting that the data coverage for <inline-formula><mml:math id="M403" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> is exactly the same across all cases. Depending on the intended application, this assessment is carried out by means of selected examples based on temporal averaging on a <inline-formula><mml:math id="M404" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">0.1</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">0.1</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grid or daily swath data.</p>
      <p id="d2e6615">As a first step, Fig. <xref ref-type="fig" rid="F15"/> presents the global distribution of the retrieved <inline-formula><mml:math id="M405" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M406" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> mole fractions for the years 2022 and 2023. There are clear differences between the hemispheres with higher values in the Northern Hemisphere, where most emission sources are concentrated. This gradient is further modified by additional increases over key regions, such as China, India, and Southeast Asia, which are caused by the many anthropogenic sources located there. For <inline-formula><mml:math id="M407" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, elevated abundances are also observed over tropical wetlands and specific hotspots, such as California's Central Valley and the Po Valley in northern Italy. For <inline-formula><mml:math id="M408" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>, additional enhanced values are primarily associated with biomass burning in Africa and South America, as well as with major urban agglomerations including Mexico City and Tehran. The coverage over land is generally high, although persistent cloud cover and low surface reflectivity result in some data gaps near the equator. Coverage over oceans and inland waters is more limited, as good measurements mainly occur under favourable observational conditions, such as sun-glint geometries or certain sea ice scenarios.</p>

      <fig id="F15"><label>Figure 15</label><caption><p id="d2e6660">Biennial mean (2022/2023) of retrieved TROPOMI/WFMD v2.0 <bold>(a)</bold> <inline-formula><mml:math id="M409" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M410" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f15.jpg"/>

      </fig>

      <p id="d2e6700">To further assess the performance of the updated quality filter, regional coverage and temporal variability are analysed using monthly data. Figures <xref ref-type="fig" rid="F16"/> and <xref ref-type="fig" rid="F17"/> present the differences between v1.8 and v2.0 for February and October 2023. An obvious change in v2.0 is the slight decrease in coverage over the Sahara, attributable to stricter aerosol filtering. Conversely, coverage at higher latitudes has improved, in line with the results of Sect. <xref ref-type="sec" rid="Ch1.S3"/>. For a given grid cell, v2.0 shows less variation within a month, especially in desert and mountain areas, which is reflected in reduced scatter <inline-formula><mml:math id="M411" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>. While the standard deviation for each grid cell partly captures natural changes, the overall reduction indicates that more low-quality observations have been filtered out.</p>

      <fig id="F16" specific-use="star"><label>Figure 16</label><caption><p id="d2e6718">Comparison of monthly averages for <bold>(a)</bold> TROPOMI/WFMD v1.8 and <bold>(b)</bold> v2.0 using the example of February 2023. The top row shows the <inline-formula><mml:math id="M412" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the middle row the number of days that contribute to the monthly average as a percentage (<inline-formula><mml:math id="M413" display="inline"><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> corresponds to 28 d in this example), and the bottom row the standard deviation of <inline-formula><mml:math id="M414" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> per grid cell. As at least two values are required to calculate a meaningful standard deviation, only grid cells with two or more measurements are shown in the bottom row.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f16.jpg"/>

      </fig>

      <fig id="F17" specific-use="star"><label>Figure 17</label><caption><p id="d2e6773">As Fig. <xref ref-type="fig" rid="F16"/> but for October 2023.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f17.jpg"/>

      </fig>

      <fig id="F18" specific-use="star"><label>Figure 18</label><caption><p id="d2e6786">Comparison of <bold>(a)</bold> TROPOMI/WFMD v1.8 and <bold>(b)</bold> v2.0 <inline-formula><mml:math id="M415" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for two example days (columns) over the Sahara demonstrating the improved filtering of spurious high values associated with individual aerosol events or cloud edges in v2.0.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f18.jpg"/>

      </fig>

      <fig id="F19" specific-use="star"><label>Figure 19</label><caption><p id="d2e6819">Comparison of <bold>(a)</bold> TROPOMI/WFMD v1.8 and <bold>(b)</bold> v2.0 <inline-formula><mml:math id="M416" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> over Central Europe for example satellite overpasses demonstrating the improved cloud screening in v2.0. The background shows the corresponding Suomi NPP/VIIRS True Colour image (bands I1-M4-M3) to highlight the position of the clouds. Elevated methane abundances associated with emissions from the Upper Silesian Coal Basin in Poland are clearly visible on both days.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f19.jpg"/>

      </fig>

      <p id="d2e6853">In addition to temporally averaged products, individual Level 2 swath data help evaluate how the updated quality filter performs under specific atmospheric conditions, such as dust storm events over the Sahara. Figure <xref ref-type="fig" rid="F18"/> shows two example days where the v2.0 filter more effectively removes aerosol-contaminated observations than v1.8. In these cases, the number of retained observations in v2.0 is reduced by <inline-formula><mml:math id="M417" display="inline"><mml:mrow><mml:mn mathvariant="normal">19</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M418" display="inline"><mml:mrow><mml:mn mathvariant="normal">12</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, respectively. In particular, spurious high values linked to elevated aerosol loading or cloud edges are removed more reliably, e.g., those from dust plumes originating from the Bodélé Depression in Chad. The result is a much more spatially homogeneous methane distribution in v2.0 compared to v1.8.</p>

      <fig id="F20" specific-use="star"><label>Figure 20</label><caption><p id="d2e6882">Similar to Fig. <xref ref-type="fig" rid="F19"/> but showing <inline-formula><mml:math id="M419" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> and different satellite overpasses. Distinct enhancements are evident over major Central European steelworks including those located in Duisburg and Dillingen, Germany.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f20.jpg"/>

      </fig>

      <fig id="F21" specific-use="star"><label>Figure 21</label><caption><p id="d2e6903">Comparison of <bold>(a)</bold> TROPOMI/WFMD v1.8 and <bold>(b)</bold> v2.0 <inline-formula><mml:math id="M420" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> over Siberia for example satellite overpasses demonstrating the improved cloud screening in v2.0. The background shows a specific Suomi NPP/VIIRS false-colour composite (bands M3-I3-M11), which is capable of distinguishing clouds (warm off-white) from snow/ice (bright red). In a true colour image both would appear white and would be indistinguishable. The observed elevated methane abundances are attributed to leakage from oil and gas facilities.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f21.jpg"/>

      </fig>

      <p id="d2e6937">The v2.0 quality filter also improves cloud screening and increases data coverage at mid- and high latitudes. Figures <xref ref-type="fig" rid="F19"/>–<xref ref-type="fig" rid="F21"/> show example satellite overpasses over Central Europe and Siberia for both <inline-formula><mml:math id="M421" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M422" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula>. While both versions correlate well and effectively remove cloudy scenes, v2.0 allows more valid observations under cloud-free conditions, thereby boosting the data yield. In these examples, the number of soundings passing the filter increases by about <inline-formula><mml:math id="M423" display="inline"><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M424" display="inline"><mml:mrow><mml:mn mathvariant="normal">20</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> over Central Europe, and by <inline-formula><mml:math id="M425" display="inline"><mml:mrow><mml:mn mathvariant="normal">60</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M426" display="inline"><mml:mrow><mml:mn mathvariant="normal">15</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> for the two example overpasses in Siberia. Better coverage also enables improved estimation of emissions sources, some examples of which are easily identifiable in the presented images. In Fig. <xref ref-type="fig" rid="F19"/>, methane emissions from the Upper Silesian Coal Basin in Poland are evident on both observation days, while the Siberian enhancements in Fig. <xref ref-type="fig" rid="F21"/> are associated with methane leakage from oil and gas infrastructure. Figure <xref ref-type="fig" rid="F20"/> displays major carbon monoxide emissions from steel production plants in Central Europe, particularly in Germany, Poland, Slovakia, and the Czech Republic <xref ref-type="bibr" rid="bib1.bibx65 bib1.bibx36" id="paren.46"/>.</p>
      <p id="d2e7019">These figures use various Suomi NPP/VIIRS band combinations to highlight cloud cover, which helps to visually identify observations that should be excluded. In the examples for Central Europe, the background image displays a True Colour composite (bands I1-M4-M3), which closely resembles the natural appearance of land, ocean, and atmospheric features as perceived by the human eye. In this representation, the clouds appear white due to the approximately equal scattering of light across the visible bands used.</p>
      <p id="d2e7026">For the Siberian case, a false-colour composite (bands M3-I3-M11) is used instead, because it more effectively distinguishes clouds from snow and ice, which look similar in standard true-colour images. In this representation, snow and ice appear bright red because they strongly reflect visible light (band M3, centered at <inline-formula><mml:math id="M427" display="inline"><mml:mn mathvariant="normal">0.49</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M428" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>), while they strongly absorb in the shortwave infrared (SWIR) range (band I3: <inline-formula><mml:math id="M429" display="inline"><mml:mn mathvariant="normal">1.61</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M430" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>; band M11: <inline-formula><mml:math id="M431" display="inline"><mml:mn mathvariant="normal">2.25</mml:mn></mml:math></inline-formula> <inline-formula><mml:math id="M432" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>). Vegetation appears green as it reflects strongly in band I3 but much less in the other two bands. Water clouds are warm off-white with a pale orange or beige tint, while high cirrus clouds appear pastel pink as a result of scattering by small ice crystals.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d2e7090">The TROPOMI/WFMD v2.0 product represents a substantial advance in the remote sensing of atmospheric <inline-formula><mml:math id="M433" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">XCH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M434" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">XCO</mml:mi></mml:mrow></mml:math></inline-formula> from space. This improvement is mainly the result of implementing refined quality filtering based on Extreme Gradient Boosting (XGBoost) in order to address the increasing demands for enhanced retrieval accuracy and computational efficiency. Thorough quality assessments have shown that the updated algorithm delivers higher data yield with better precision and accuracy, as well as robust estimates of uncertainty. In particular, dedicated analyses have confirmed that there are no critical biases related to albedo in the TROPOMI/WFMD data product. This finding helps to defuse a frequent concern associated with using TROPOMI methane observations for certain applications. The demonstrated quality of this data product broadens its suitability for a more extensive range of scientific investigations.</p>
      <p id="d2e7128">With a steadily growing data record of currently seven years, the advanced TROPOMI/WFMD v2.0 product is well-positioned for integration into comprehensive monitoring systems that combine complementary information from accurate local in-situ measurements and global satellite observations within an inverse modelling framework. The proven performance of the data product also supports important applications, such as the quantification of emission sources. The expertise in applying machine learning techniques in the field of satellite retrievals, which was gained during the development of the TROPOMI/WFMD algorithm, establishes a sound basis for similar approaches in future missions, including the Sentinel-5 satellites.</p>
</sec>

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

<app id="App1.Ch1.S1">
  <label>Appendix A</label><title>Spectral fit example</title>
      <p id="d2e7154">The spectral fitting window of TROPOMI/WFMD v2.0 can be seen in the example fit shown in Fig. <xref ref-type="fig" rid="FA1"/>. The strong methane band around <inline-formula><mml:math id="M435" display="inline"><mml:mrow><mml:mn mathvariant="normal">2317</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> is generally excluded to retrieve <inline-formula><mml:math id="M436" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M437" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> simultaneously as accurately as possible <xref ref-type="bibr" rid="bib1.bibx63" id="paren.47"/>. The apparent albedo is retrieved in the preprocessing from the measured mean radiance <inline-formula><mml:math id="M438" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mtext>con</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> in the continuum interval and is then prescribed in the actual fitting procedure. The relative fit residual <inline-formula><mml:math id="M439" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula> is defined as <inline-formula><mml:math id="M440" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mtext>Model</mml:mtext><mml:mo>-</mml:mo><mml:mtext>TROPOMI</mml:mtext></mml:mrow><mml:mrow><mml:mtext>Model</mml:mtext><mml:mo>+</mml:mo><mml:mtext>TROPOMI</mml:mtext></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></inline-formula>.</p>

      <fig id="FA1"><label>Figure A1</label><caption><p id="d2e7240">Spectral fit for a sample scene in Bavaria, Germany. <bold>(a)</bold> The TROPOMI spectral measurements (red circles) are shown together with the fitted radiative transfer model (black line) and the resulting (relative) fit residual <inline-formula><mml:math id="M441" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula> below. The grey dashed line highlights the baseline of the model, i.e., the fitted polynomial without absorption. The difference between the baseline relative to the model or measurement gives a sense of the depth of the individual absorption lines. The blue-shaded interval indicates the virtually absorption-free continuum-like portion used to determine the apparent albedo, which is important to disentangle surface reflection and molecular abundances in the fitting procedure. <bold>(b)</bold> Weighting functions with respect to the fitted gases <inline-formula><mml:math id="M442" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> scaled with the respective retrieved columns <inline-formula><mml:math id="M443" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>v</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, breaking down which of the measured features are attributable to which absorber. This representation also explicitly reconfirms that none of the gases has any significant absorption in the continuum-like interval used.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f22.png"/>

      </fig>


</app>

<app id="App1.Ch1.S2">
  <label>Appendix B</label><title>Perceptual uniform colormap vivian</title>
      <p id="d2e7293">It is increasingly recognised that scientific visualisation benefits from perceptually uniform colormaps, which enable accurate and accessible interpretation of data. Non-uniform changes in brightness or hue can distort the perception of quantitative values. Many conventional colour scales remain difficult to interpret, especially for viewers with colour vision deficiencies.</p>
      <p id="d2e7296">The <italic>vivian</italic> colormap, which is available in the Python package <italic>cmuseo</italic>, is designed to be perceptually uniform and accessible to people with colour vision deficiencies. Like the widely used <italic>viridis</italic> colormap, <italic>vivian</italic> targets the needs of scientific visualisation, but is intended to achieve a wider perceptual range. The perceptual gradient curve, used to assess the quality of colormaps, is generated by calculating the colour differences <inline-formula><mml:math id="M444" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>E</mml:mi></mml:mrow></mml:math></inline-formula> between adjacent colours using Euclidean distance in  CAM02-UCS space, which closely models the human perception of colour. If the <inline-formula><mml:math id="M445" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>E</mml:mi></mml:mrow></mml:math></inline-formula> curve remains flat, this means that equal changes in the data translate into equal perceived differences, helping to preserve gradients and fine structures without introducing visual artefacts. We measure this flatness with the normalised root mean square (RMS) deviation <inline-formula><mml:math id="M446" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="normal">RMS</mml:mi><mml:mi mathvariant="italic">%</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>, which is reported as a percentage of the average <inline-formula><mml:math id="M447" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>E</mml:mi></mml:mrow></mml:math></inline-formula>. The total perceptual arc length <inline-formula><mml:math id="M448" display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mo>∫</mml:mo><mml:mi mathvariant="script">C</mml:mi></mml:msub><mml:mi>d</mml:mi><mml:mi>E</mml:mi></mml:mrow></mml:math></inline-formula> of the colormap's trajectory <inline-formula><mml:math id="M449" display="inline"><mml:mi mathvariant="script">C</mml:mi></mml:math></inline-formula> in the CAM02-UCS space reflects how large the perceptual range is that the colormap can cover, with larger <inline-formula><mml:math id="M450" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> values indicating a better ability to reproduce fine details. In addition to ensuring the perceptual uniformity of the original colour information, it is also important that changes in brightness, calculated as <inline-formula><mml:math id="M451" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mi>J</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>J</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, are likewise uniform and monotonic in order to guarantee flawless greyscale representation and better accessibility for viewers with limited colour perception.</p>
      <p id="d2e7435">Figure <xref ref-type="fig" rid="FB1"/> shows that <italic>vivian</italic> is perfectly perceptually uniform, both in original colour representation and also when converted to greyscale, and is thus a reliable choice for accurate and accessible data visualisation in science. In line with the intended objective, the colormap offers a slightly larger perceptual range than <italic>viridis</italic> (<inline-formula><mml:math id="M452" display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">145.0</mml:mn></mml:mrow></mml:math></inline-formula> versus <inline-formula><mml:math id="M453" display="inline"><mml:mn mathvariant="normal">123.9</mml:mn></mml:math></inline-formula>).</p>

      <fig id="FB1"><label>Figure B1</label><caption><p id="d2e7468">Perceptual analysis of the <italic>vivian</italic> colormap. Shown are perceptual differences along the colormap (top left) and corresponding lightness differences (top right) in CAM02-UCS space. The bottom panel shows the 3D-trajectory of <italic>vivian</italic> and an example figure.</p></caption>
        <graphic xlink:href="https://amt.copernicus.org/articles/19/2407/2026/amt-19-2407-2026-f23.png"/>

      </fig>


</app>

<app id="App1.Ch1.S3">
  <label>Appendix C</label><title>List of TCCON sites</title>

<table-wrap id="TC1"><label>Table C1</label><caption><p id="d2e7501"> TCCON sites used in the validation sorted according to latitude from north to south.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <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:colspec colnum="5" colname="col5" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Site</oasis:entry>
         <oasis:entry colname="col2">Latitude</oasis:entry>
         <oasis:entry colname="col3">Longitude</oasis:entry>
         <oasis:entry colname="col4">Altitude</oasis:entry>
         <oasis:entry colname="col5">Reference</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(°)</oasis:entry>
         <oasis:entry colname="col3">(°)</oasis:entry>
         <oasis:entry colname="col4">(km)</oasis:entry>
         <oasis:entry colname="col5"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Eureka</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M454" display="inline"><mml:mn mathvariant="normal">80.05</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M455" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">86.42</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M456" display="inline"><mml:mn mathvariant="normal">0.61</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx71" id="text.48"/>, <xref ref-type="bibr" rid="bib1.bibx6" id="text.49"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ny-Ålesund</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M457" display="inline"><mml:mn mathvariant="normal">78.92</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M458" display="inline"><mml:mn mathvariant="normal">11.92</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M459" display="inline"><mml:mn mathvariant="normal">0.02</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx11" id="text.50"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sodankylä</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M460" display="inline"><mml:mn mathvariant="normal">67.37</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M461" display="inline"><mml:mn mathvariant="normal">26.63</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M462" display="inline"><mml:mn mathvariant="normal">0.19</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx31" id="text.51"/>, <xref ref-type="bibr" rid="bib1.bibx30" id="text.52"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">East Trout Lake</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M463" display="inline"><mml:mn mathvariant="normal">54.35</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M464" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">104.99</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M465" display="inline"><mml:mn mathvariant="normal">0.50</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx91" id="text.53"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Białystok</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M466" display="inline"><mml:mn mathvariant="normal">53.23</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M467" display="inline"><mml:mn mathvariant="normal">23.03</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M468" display="inline"><mml:mn mathvariant="normal">0.19</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx52" id="text.54"/>, <xref ref-type="bibr" rid="bib1.bibx44" id="text.55"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bremen</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M469" display="inline"><mml:mn mathvariant="normal">53.10</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M470" display="inline"><mml:mn mathvariant="normal">8.85</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M471" display="inline"><mml:mn mathvariant="normal">0.03</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx49" id="text.56"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Harwell</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M472" display="inline"><mml:mn mathvariant="normal">51.57</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M473" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.32</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M474" display="inline"><mml:mn mathvariant="normal">0.14</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx83" id="text.57"/>, <xref ref-type="bibr" rid="bib1.bibx84" id="text.58"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Karlsruhe</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M475" display="inline"><mml:mn mathvariant="normal">49.10</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M476" display="inline"><mml:mn mathvariant="normal">8.44</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M477" display="inline"><mml:mn mathvariant="normal">0.11</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx22" id="text.59"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Paris</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M478" display="inline"><mml:mn mathvariant="normal">48.85</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M479" display="inline"><mml:mn mathvariant="normal">2.36</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M480" display="inline"><mml:mn mathvariant="normal">0.06</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx75" id="text.60"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Orléans</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M481" display="inline"><mml:mn mathvariant="normal">47.97</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M482" display="inline"><mml:mn mathvariant="normal">2.11</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M483" display="inline"><mml:mn mathvariant="normal">0.13</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx82" id="text.61"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Garmisch</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M484" display="inline"><mml:mn mathvariant="normal">47.48</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M485" display="inline"><mml:mn mathvariant="normal">11.06</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M486" display="inline"><mml:mn mathvariant="normal">0.75</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx72" id="text.62"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Park Falls</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M487" display="inline"><mml:mn mathvariant="normal">45.94</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M488" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">90.27</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M489" display="inline"><mml:mn mathvariant="normal">0.44</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx86" id="text.63"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Rikubetsu</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M490" display="inline"><mml:mn mathvariant="normal">43.46</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M491" display="inline"><mml:mn mathvariant="normal">143.77</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M492" display="inline"><mml:mn mathvariant="normal">0.38</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx45" id="text.64"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Xianghe</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M493" display="inline"><mml:mn mathvariant="normal">39.80</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M494" display="inline"><mml:mn mathvariant="normal">116.96</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M495" display="inline"><mml:mn mathvariant="normal">0.04</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx93" id="text.65"/>, <xref ref-type="bibr" rid="bib1.bibx92" id="text.66"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Lamont</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M496" display="inline"><mml:mn mathvariant="normal">36.60</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M497" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">97.49</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M498" display="inline"><mml:mn mathvariant="normal">0.32</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx87" id="text.67"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Tsukuba</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M499" display="inline"><mml:mn mathvariant="normal">36.05</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M500" display="inline"><mml:mn mathvariant="normal">140.12</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M501" display="inline"><mml:mn mathvariant="normal">0.03</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx46" id="text.68"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Nicosia</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M502" display="inline"><mml:mn mathvariant="normal">35.14</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M503" display="inline"><mml:mn mathvariant="normal">33.38</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M504" display="inline"><mml:mn mathvariant="normal">0.19</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx53" id="text.69"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Edwards</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M505" display="inline"><mml:mn mathvariant="normal">34.96</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M506" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">117.88</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M507" display="inline"><mml:mn mathvariant="normal">0.70</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx27" id="text.70"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Caltech</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M508" display="inline"><mml:mn mathvariant="normal">34.14</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M509" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">118.13</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M510" display="inline"><mml:mn mathvariant="normal">0.24</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx85" id="text.71"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Saga</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M511" display="inline"><mml:mn mathvariant="normal">33.24</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M512" display="inline"><mml:mn mathvariant="normal">130.29</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M513" display="inline"><mml:mn mathvariant="normal">0.01</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx69" id="text.72"/>, <xref ref-type="bibr" rid="bib1.bibx51" id="text.73"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hefei</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M514" display="inline"><mml:mn mathvariant="normal">31.90</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M515" display="inline"><mml:mn mathvariant="normal">119.17</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M516" display="inline"><mml:mn mathvariant="normal">0.04</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx39" id="text.74"/>, <xref ref-type="bibr" rid="bib1.bibx81" id="text.75"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Burgos</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M517" display="inline"><mml:mn mathvariant="normal">18.53</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M518" display="inline"><mml:mn mathvariant="normal">120.65</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M519" display="inline"><mml:mn mathvariant="normal">0.04</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx47" id="text.76"/>, <xref ref-type="bibr" rid="bib1.bibx80" id="text.77"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Darwin</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M520" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">12.46</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M521" display="inline"><mml:mn mathvariant="normal">130.93</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M522" display="inline"><mml:mn mathvariant="normal">0.04</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx16" id="text.78"/>, <xref ref-type="bibr" rid="bib1.bibx14" id="text.79"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Réunion</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M523" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">20.90</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M524" display="inline"><mml:mn mathvariant="normal">55.49</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M525" display="inline"><mml:mn mathvariant="normal">0.09</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx13" id="text.80"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Wollongong</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M526" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">34.41</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M527" display="inline"><mml:mn mathvariant="normal">150.88</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M528" display="inline"><mml:mn mathvariant="normal">0.03</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">
                  <xref ref-type="bibr" rid="bib1.bibx15" id="text.81"/>
                </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Lauder</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M529" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">45.04</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M530" display="inline"><mml:mn mathvariant="normal">169.68</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M531" display="inline"><mml:mn mathvariant="normal">0.37</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><xref ref-type="bibr" rid="bib1.bibx68" id="text.82"/>, <xref ref-type="bibr" rid="bib1.bibx55" id="text.83"/>, <xref ref-type="bibr" rid="bib1.bibx54" id="text.84"/></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e8550">The methane and carbon monoxide data products presented in this publication are available at <uri>https://www.iup.uni-bremen.de/carbon_ghg/products/tropomi_wfmd/</uri> (<xref ref-type="bibr" rid="bib1.bibx62" id="altparen.85"/>). The Total Carbon Column Observing Network data are available in the TCCON data archive hosted by CaltechDATA at <uri>https://tccondata.org</uri> (last access: 2 November 2025).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e8565">OS designed and operated the TROPOMI/WFMD satellite retrievals, set up and optimised the machine learning environment, performed the data analysis, and wrote the paper. MiB, JH, MR, HeB, and HaB contributed significantly to the conceptual design of the retrievals and the development of the analysis strategy. MaB, NMD, DWTG, FH, LTI, RK, IM, HO, CP, JR, CR, MKS, KeS, KiS, RS, YT, VAV, MV, WW, TW, DaW, DeW, MZ operated the TCCON retrievals for the various sites and provided support in using the data and interpreting the outcomes. All authors discussed the results and improved the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e8574">At least one of the (co-)authors is a member of the editorial board of <italic>Atmospheric Measurement Techniques</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e8583">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="d2e8589">This publication contains modified Copernicus Sentinel data (2018–2024). Sentinel-5 Precursor is an ESA mission implemented on behalf of the European Commission. The TROPOMI payload is a joint development by ESA and the Netherlands Space Office (NSO). The Sentinel-5 Precursor ground-segment development has been funded by ESA and with national contributions from The Netherlands, Germany, and Belgium.</p><p id="d2e8603">We acknowledge the use of VIIRS imagery from the NASA Worldview application (<uri>https://worldview.earthdata.nasa.gov/</uri>, last access: 2 November 2025) operated by the NASA/Goddard Space Flight Center Earth Science Data and Information System (ESDIS) project and thank the European Centre for Medium-Range Weather Forecasts (ECMWF) for providing the ERA5 reanalysis.</p><p id="d2e8608">The colormap <italic>vivian</italic> used in many figures is part of the Python package cmuseo (<uri>https://pypi.org/project/cmuseo/</uri>, last access: 2 November 2025). Parts of the results in this work make use of colormaps in the CMasher package <xref ref-type="bibr" rid="bib1.bibx76" id="paren.86"/>.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e8623">The research leading to the presented results received funding from the European Space Agency (ESA) via the projects GHG-CCI+ and SMART-CH4 (ESA contract nos. 4000126450/19/I-NB and 4000142730/23/I-NS) and from the German Federal Ministry of Research, Technology and Space (BMFTR) within its project ITMS via grant 01 LK2103A. The TROPOMI/WFMD retrievals presented here were performed on HPC facilities of the IUP, University of Bremen, funded under DFG/FUGG grant nos. INST 144/379-1 and INST 144/493-1.</p>

      <p id="d2e8630">The TCCON sites at Rikubetsu, Tsukuba, and Burgos are supported in part by the GOSAT series project. Local support for Burgos is provided by the Energy Development Corporation (EDC, the Philippines). The TCCON site at Réunion Island has been operated by the Royal Belgian Institute for Space Aeronomy with financial support since 2014 by the EU project ICOS-Inwire (Grant agreement ID 313169), the ministerial decree for ICOS (FR/35/IC1 to FR/35/C6), ESFRI-FED ICOS-BE project (EF/211/ICOS-BE) and local activities supported by LACy/UMR8105 and by OSU-R/UMS3365 – Université de La Réunion. The Paris TCCON site has received funding from Sorbonne Université, the French research center CNRS, and the French space agency CNES. The Nicosia TCCON site received financial support from the European Union's Horizon 2020 research and innovation programme under Grant agreement no. 856612 (EMME-CARE) and the Cyprus Government. The Garmisch TCCON site is supported by funding from the Helmholtz Research Program Changing Earth – Sustaining our Future within the Helmholtz research field Earth and Environment.</p>

      <p id="d2e8633">The article processing charges for this open-access publication were covered by the University of Bremen.The article processing charges for this open-access publication were covered by the University of Bremen.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e8644">This paper was edited by Zhao-Cheng Zeng and reviewed by two anonymous referees.</p>
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