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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESSD</journal-id><journal-title-group>
    <journal-title>Earth System Science Data</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESSD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Sci. Data</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1866-3516</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/essd-18-3507-2026</article-id><title-group><article-title>Machine-learning-based estimates of global natural vegetated wetland methane emissions (2000–2025)</article-title><alt-title>Global natural vegetated wetland methane emissions</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Li</surname><given-names>Mengze</given-names></name>
          <email>mengze@nus.edu.sg</email>
        <ext-link>https://orcid.org/0000-0003-0620-6301</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Jackson</surname><given-names>Robert B.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8846-7147</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Saunois</surname><given-names>Marielle</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Ciais</surname><given-names>Philippe</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8560-4943</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Poulter</surname><given-names>Ben</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9493-8600</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Canadell</surname><given-names>Josep G.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8788-3218</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7 aff8">
          <name><surname>Patra</surname><given-names>Prabir K.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5700-9389</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9 aff10">
          <name><surname>Tian</surname><given-names>Hanqin</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1806-4091</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff11">
          <name><surname>Zhang</surname><given-names>Zhen</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0899-1139</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12">
          <name><surname>Fluet-Chouinard</surname><given-names>Etienne</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff13">
          <name><surname>Ouyang</surname><given-names>Zutao</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhang</surname><given-names>Ting</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff14">
          <name><surname>Beerling</surname><given-names>David J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15">
          <name><surname>Belikov</surname><given-names>Dmitry A.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2114-7250</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Bousquet</surname><given-names>Philippe</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Custodio</surname><given-names>Danilo</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Chandra</surname><given-names>Naveen</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5357-7757</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Dou</surname><given-names>Xinyu</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7783-6971</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff16">
          <name><surname>Gedney</surname><given-names>Nicola</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2165-5239</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff17">
          <name><surname>Hopcroft</surname><given-names>Peter O.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3694-9181</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Hoyt</surname><given-names>Alison M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15 aff18">
          <name><surname>Ichii</surname><given-names>Kazuhito</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff19">
          <name><surname>Ito</surname><given-names>Akihito</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5265-0791</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff20">
          <name><surname>Jain</surname><given-names>Atul K.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4051-3228</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff21">
          <name><surname>Jensen</surname><given-names>Katherine</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff22">
          <name><surname>Joos</surname><given-names>Fortunat</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9483-6030</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff23">
          <name><surname>Kleinen</surname><given-names>Thomas</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9550-5164</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8 aff24 aff25 aff26 aff27 aff28">
          <name><surname>Kondo</surname><given-names>Masayuki</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5466-4847</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff29 aff2">
          <name><surname>Li</surname><given-names>Fa</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff30">
          <name><surname>Li</surname><given-names>Tingting</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff31">
          <name><surname>Liu</surname><given-names>Xiangyu</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4676-6362</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff32">
          <name><surname>Maksyutov</surname><given-names>Shamil</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1200-9577</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff33">
          <name><surname>Malhotra</surname><given-names>Avni</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7850-6402</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Martinez</surname><given-names>Adrien</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8508-9005</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff21">
          <name><surname>McDonald</surname><given-names>Kyle</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff34">
          <name><surname>Melton</surname><given-names>Joe R.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9414-064X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff22">
          <name><surname>Müller</surname><given-names>Jurek</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff32">
          <name><surname>Niwa</surname><given-names>Yosuke</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7600-9816</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff35 aff9">
          <name><surname>Pan</surname><given-names>Shufen</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff36">
          <name><surname>Peng</surname><given-names>Shushi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5098-726X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff37 aff38">
          <name><surname>Peng</surname><given-names>Changhui</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff39">
          <name><surname>Qin</surname><given-names>Zhangcai</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9414-4854</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff40">
          <name><surname>Raymond</surname><given-names>Peter</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8564-7860</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff41">
          <name><surname>Riley</surname><given-names>William</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4615-2304</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff42">
          <name><surname>Segers</surname><given-names>Arjo</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1319-0195</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff16">
          <name><surname>Thompson</surname><given-names>Rona L.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9485-7176</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff43">
          <name><surname>Tsuruta</surname><given-names>Aki</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9197-3005</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Xi</surname><given-names>Yi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2654-4615</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff44">
          <name><surname>Yuan</surname><given-names>Kunxiaojia</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff45 aff46">
          <name><surname>Zhang</surname><given-names>Wenxin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff47 aff48">
          <name><surname>Zheng</surname><given-names>Bo</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8344-3445</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff41">
          <name><surname>Zhu</surname><given-names>Qing</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff49">
          <name><surname>Zhu</surname><given-names>Qiuan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff31">
          <name><surname>Zhuang</surname><given-names>Qianlai</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4536-9851</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Geography, National University of Singapore, Singapore</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth System Science, Stanford Doerr School of Sustainability, Stanford, CA, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Woods Institute for the Environment and Precourt Institute for Energy, Stanford University, Stanford, CA, USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Laboratoire des Sciences du Climat et de l'Environnement (LSCE), CEA, CNRS, UVSQ,  Université Paris Saclay, Gif-sur-Yvette, France</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Spark Climate Solutions, San Francisco, CA, USA</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Global Carbon Project, CSIRO Environment, Canberra, ACT 2601, Australia</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Research Institute for Global Change, JAMSTEC, 3173-25 Showa-machi,  Kanazawa, Yokohama, 236-0001, Japan</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>Seto Inland Sea Carbon Neutral Research Center (S-CNC), Hiroshima University,  Higashi-Hiroshima, Hiroshima 739-8529, Japan</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>Center for Earth System Science and Global Sustainability, Boston College, Chestnut Hill, MA, USA</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>Department of Earth and Environmental Sciences, Boston College, Chestnut Hill, MA, USA</institution>
        </aff>
        <aff id="aff11"><label>11</label><institution>State Key Laboratory of Tibetan Plateau Earth System, Environment and Resources, and Institute of Tibetan Plateau Research, Chinese Academy of Sciences, Beijing, China</institution>
        </aff>
        <aff id="aff12"><label>12</label><institution>Earth System Science Division, Pacific Northwest National Laboratory, Richland, WA, USA</institution>
        </aff>
        <aff id="aff13"><label>13</label><institution>College of Forestry, Wildlife and Environment, Auburn University, Auburn, AL, USA</institution>
        </aff>
        <aff id="aff14"><label>14</label><institution>School of Biosciences, University of Sheffield, Sheffield, UK</institution>
        </aff>
        <aff id="aff15"><label>15</label><institution>Center for Environmental Remote Sensing, Chiba University, Chiba, Japan</institution>
        </aff>
        <aff id="aff16"><label>16</label><institution>Met Office Hadley Centre, Joint Centre for Hydrometeorological Research, Wallingford, UK</institution>
        </aff>
        <aff id="aff17"><label>17</label><institution>School of Geography, Earth &amp; Environmental Sciences, University of Birmingham, Birmingham, UK</institution>
        </aff>
        <aff id="aff18"><label>18</label><institution>Graduate School of Science and Engineering, Chiba University, 1-33, Yayoi-cho, Inage-ku, Japan</institution>
        </aff>
        <aff id="aff19"><label>19</label><institution>Graduate School of Agricultural and Life Sciences, The University of Tokyo, Tokyo, Japan</institution>
        </aff>
        <aff id="aff20"><label>20</label><institution>Department of Climate, Meteorology, and Atmospheric Sciences,   University of Illinois at Urbana-Champaign, Urbana, IL, USA</institution>
        </aff>
        <aff id="aff21"><label>21</label><institution>Department of Earth and Atmospheric Sciences, City University of New York, New York, NY, USA</institution>
        </aff>
        <aff id="aff22"><label>22</label><institution>Climate and Environmental Physics, Physics Institute and Oeschger Centre for Climate Change Research, University of Bern, Bern, Switzerland</institution>
        </aff>
        <aff id="aff23"><label>23</label><institution>Max Planck Institute for Meteorology, Hamburg, Germany</institution>
        </aff>
        <aff id="aff24"><label>24</label><institution>The IDEC Institute – Center for Peaceful and Sustainable Futures (CEPEAS), Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8529, Japan</institution>
        </aff>
        <aff id="aff25"><label>25</label><institution>Network for Education and Research on Peace and Sustainability (NERPS), Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8529, Japan</institution>
        </aff>
        <aff id="aff26"><label>26</label><institution>Graduate School of Humanities and Social Sciences International Economic Development Program (IEDP), Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8529, Japan</institution>
        </aff>
        <aff id="aff27"><label>27</label><institution>Graduate School of Innovation and Practice for Smart Society (SmaSo), Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8529, Japan</institution>
        </aff>
        <aff id="aff28"><label>28</label><institution>Town &amp; Gown Institute for Innovation for the Future (TGIF), Hiroshima University,  Higashi-Hiroshima, Hiroshima 739-8529, Japan</institution>
        </aff>
        <aff id="aff29"><label>29</label><institution>Department of Earth and Planetary Sciences, Jackson School of Geosciences,  The University of Texas at Austin, Austin, TX, USA</institution>
        </aff>
        <aff id="aff30"><label>30</label><institution>Key Laboratory of Atmospheric Environment and Extreme Meteorology, Institute of Atmospheric Physics, Chinese Academy of Sciences, Beijing, China</institution>
        </aff>
        <aff id="aff31"><label>31</label><institution>Department of Earth, Atmospheric, and Planetary Sciences,  Purdue University, West Lafayette, IN, USA</institution>
        </aff>
        <aff id="aff32"><label>32</label><institution>Earth System Division, National Institute for Environmental Studies, Tsukuba, Ibaraki, Japan</institution>
        </aff>
        <aff id="aff33"><label>33</label><institution>Biological Sciences Division, Pacific Northwest National Laboratory, Richland, WA, USA</institution>
        </aff>
        <aff id="aff34"><label>34</label><institution>Climate Research Division, Environment and Climate Change Canada, Victoria, BC, Canada</institution>
        </aff>
        <aff id="aff35"><label>35</label><institution>Department of Engineering, Boston College, Chestnut Hill, MA, USA</institution>
        </aff>
        <aff id="aff36"><label>36</label><institution>Sino-French Institute for Earth System Science, College of Urban and Environmental Sciences,   Peking University, Beijing 100871, China</institution>
        </aff>
        <aff id="aff37"><label>37</label><institution>Department of Biology Sciences, University of Quebec at Montreal, C.P. 8888,   Succ. Centre-Ville, Montreal, QC H3C 3P8, Canada</institution>
        </aff>
        <aff id="aff38"><label>38</label><institution>College of Geographic Science, Hunan Normal University, Changsha 410081, China</institution>
        </aff>
        <aff id="aff39"><label>39</label><institution>School of Atmospheric Sciences, Sun Yat-sen University, and Southern Marine Science and Engineering Guangdong Laboratory (Zhuhai), Zhuhai 519000, China</institution>
        </aff>
        <aff id="aff40"><label>40</label><institution>School of the Environment, Yale University, New Haven, CT, USA</institution>
        </aff>
        <aff id="aff41"><label>41</label><institution>Climate and Ecosystem Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA</institution>
        </aff>
        <aff id="aff42"><label>42</label><institution>TNO, Department of Climate Air &amp; Sustainability, P.O. Box 80015, 3508-TA, Utrecht, the Netherlands</institution>
        </aff>
        <aff id="aff43"><label>43</label><institution>Finnish Meteorological Institute, P.O. Box 503, 00101, Helsinki, Finland</institution>
        </aff>
        <aff id="aff44"><label>44</label><institution>Department of Earth and Atmospheric Sciences, University of Houston, Houston, TX, USA</institution>
        </aff>
        <aff id="aff45"><label>45</label><institution>School of Geographical &amp; Earth Sciences, University of Glasgow, Glasgow, UK</institution>
        </aff>
        <aff id="aff46"><label>46</label><institution>Department of Earth and Environmental Sciences, Lund University, Lund, Sweden</institution>
        </aff>
        <aff id="aff47"><label>47</label><institution>Institute of Environment and Ecology, Tsinghua Shenzhen International Graduate School,   Tsinghua University, Shenzhen 518055, China</institution>
        </aff>
        <aff id="aff48"><label>48</label><institution>State Environmental Protection Key Laboratory of Sources and Control of Air Pollution Complex,   Beijing 100084, China</institution>
        </aff>
        <aff id="aff49"><label>49</label><institution>College of Hydrology and Water Resources, Hohai University, Nanjing 210098, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Mengze Li (mengze@nus.edu.sg)</corresp></author-notes><pub-date><day>22</day><month>May</month><year>2026</year></pub-date>
      
      <volume>18</volume>
      <issue>5</issue>
      <fpage>3507</fpage><lpage>3524</lpage>
      <history>
        <date date-type="received"><day>5</day><month>March</month><year>2026</year></date>
           <date date-type="rev-request"><day>12</day><month>March</month><year>2026</year></date>
           <date date-type="rev-recd"><day>21</day><month>April</month><year>2026</year></date>
           <date date-type="accepted"><day>27</day><month>April</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Mengze Li 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://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026.html">This article is available from https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026.html</self-uri><self-uri xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026.pdf">The full text article is available as a PDF file from https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e927">Wetlands are the largest natural source of atmospheric methane (CH<sub>4</sub>), yet comprehensive global budgets are typically delayed by years, preventing a timely understanding of CH<sub>4</sub> sources, sinks, and trends. To reduce this delay, we present a model emulator-driven framework and accompanying workflow that enable timely, continuous emission updates using a machine-learning emulator to reconstruct spatially explicit monthly emission fields at 1° <inline-formula><mml:math id="M3" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1° resolution. We apply this framework to a global dataset of natural vegetated wetland CH<sub>4</sub> emissions to extend the most recent Global Methane Budget (GMB; Saunois et al., 2025) record that covers the 2000–2020 emissions through 2025. In the test data (<inline-formula><mml:math id="M5" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 30 % of the total dataset), the emulator achieved a global <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.65 <inline-formula><mml:math id="M7" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.003 (mean <inline-formula><mml:math id="M8" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 95 % CI, hereafter) and an RMSE of <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.49</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.12</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> Tg CH<sub>4</sub> yr<sup>−1</sup>. The emulator is trained on 35 GMB model estimates, including 22 process-based models and 13 atmospheric inversions, paired with 10 ensemble realizations of 11 gridded climate predictor variables from atmospheric reanalyses. Our results show that the global mean predicted wetland CH<sub>4</sub> emissions for 2021–2025 (157.8 <inline-formula><mml:math id="M13" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.4 Tg CH<sub>4</sub> yr<sup>−1</sup>) are not significantly higher (<inline-formula><mml:math id="M16" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 0.05 Tg CH<sub>4</sub> yr<sup>−1</sup>) than the 2000–2020 baseline. However, this stability masks a significant hemispheric redistribution of emissions. We detect an increase in Northern Hemisphere (NH) emissions in 2021–2025, with mid- and high-latitudes increasing by 0.76 <inline-formula><mml:math id="M19" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07 and 0.35 <inline-formula><mml:math id="M20" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.03 Tg CH<sub>4</sub> yr<sup>−1</sup>, respectively, while the tropics and Southern Hemisphere (SH) extratropics show offsetting negative trends (<inline-formula><mml:math id="M23" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.95 <inline-formula><mml:math id="M24" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.19 and <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula> Tg CH<sub>4</sub> yr<sup>−1</sup>, respectively). The predicted emissions are able to capture the low emissions in 2023 in South America linked to El Niño-related drought, as reported by recent studies (Ciais et al., 2026; Quinn et al., 2025). Furthermore, we identify a distinct seasonal amplification of global emission trends that peaks in late boreal summer. This new modeled dataset and operational framework bridge the gap between the latest updated budgets and low-latency monitoring, providing a scalable capacity to frequently update global emission estimates and critical early warnings of regional wetland feedback loops. The data are publicly available at <ext-link xlink:href="https://doi.org/10.5281/zenodo.18870108" ext-link-type="DOI">10.5281/zenodo.18870108</ext-link> (Li et al., 2026).</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National University of Singapore</funding-source>
<award-id>Start-Up grant</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="d2e1204">Wetlands are the largest natural source of methane (CH<inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, a potent greenhouse gas, yet they remain one of the most uncertain components of the global CH<sub>4</sub> budget (Saunois et al., 2025; Zhu et al., 2025). They account for 25 %–30 % of global CH<sub>4</sub> emissions and strongly influence the global carbon cycle (Jackson et al., 2024; Li et al., 2026b; Peng et al., 2022; Saunois et al., 2025; Zhang et al., 2023). Quantifying how wetland CH<sub>4</sub> emissions respond to climate variability is essential for interpreting interannual variability in the global CH<sub>4</sub> budget and for understanding recent atmospheric CH<sub>4</sub> changes (Ciais et al., 2026; Gedney et al., 2019a; Parker et al., 2018; Stavert et al., 2022). Community efforts such as the Global Methane Budget (GMB) synthesize process-based “bottom-up” (BU) models and atmospheric “top-down” (TD) inversions to estimate all CH<sub>4</sub> emission sources and sinks (Saunois et al., 2020, 2025). However, the substantial effort required to assemble these products into a reliable ensemble typically leads to lags of multiple years. For instance, the most recent GMB published in 2025 (Saunois et al., 2025) covered the period 2000–2020. Although low-latency estimates exist for some individual models (Quinn et al., 2025), accelerating the assembly of a trustworthy multi-model synthesis would better support timely emission monitoring and evidence-based assessment of mitigation progress.</p>
      <p id="d2e1274">Wetland CH<sub>4</sub> emissions combine biogeochemical and hydrometeorological controls that regulate CH<sub>4</sub> production with oxidation processes within sediments and the water column. Temperature exerts a strong influence on microbial methanogenesis and ecosystem respiration (Knox et al.,  2019; Bansal et al., 2023; Li et al., 2025; Yvon-Durocher et al., 2014), whereas soil thermal and freeze-thaw conditions can modulate growing-season length and cold-season CH<sub>4</sub> dynamics (Hyvärinen et al., 2025; Zona et al., 2016). Hydrology, often summarized by water table depth, soil moisture content, and inundation extent, controls oxygen availability and redox conditions and influences wetland CH<sub>4</sub> production and oxidation (Cui et al., 2024; He et al., 2025; Knox et al., 2021). Precipitation, lateral water transport, and surface energy fluxes jointly constrain water balance through inputs and evapotranspiration (Aalto et al., 2025; Helbig et al., 2020; Tyystjärvi et al., 2024). Furthermore, radiation and vegetation state provide proxies of substrate supply and plant-mediated transport pathways that connect below-ground CH<sub>4</sub> production to the atmosphere (Helfter et al., 2022; McNicol et al., 2023).</p>
      <p id="d2e1322">Currently, global wetland CH<sub>4</sub> emissions are primarily estimated using two approaches: BU and TD models. Process-based BU models explicitly simulate the complex biogeochemical mechanisms driven by environmental conditions (Zhang et al., 2025). TD atmospheric inversions estimate surface fluxes by optimising prior emission inventories to match observed atmospheric CH<sub>4</sub> concentrations (Patra et al., 2018). Recent studies have increasingly turned to data-driven machine-learning models. For instance, McNicol et al. (2023) upscaled eddy covariance CH<sub>4</sub> fluxes globally using random forest algorithms; Bernard et al. (2025) introduced a satellite observation-based model to simulate temporal emission variability. These machine-learning approaches offer some advantages, including rapid operational speeds and lower computational costs. However, they are constrained by the sparsity of training data, particularly in the tropics and high latitudes.</p>
      <p id="d2e1352">Building on these well-established controls and the advancements in data-driven modeling, we provide a low-latency continuation of the GMB gridded wetland CH<sub>4</sub> emissions by extending monthly emissions from 2000–2020 through 2025 at 1° <inline-formula><mml:math id="M44" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1° resolution. Our approach is supported by the fact that many key climate, hydrometeorological and vegetation drivers are routinely updated as global gridded datasets, enabling a practical emulator-based pathway for timely wetland CH<sub>4</sub> emission estimates. In this study, wetlands are defined following the GMB natural vegetated wetland category, excluding lakes, rivers, reservoirs, coastal waters and managed sources (Saunois et al., 2025). We emulate each BU and TD ensemble member from GMB using machine-learning models trained on the 2000–2020 GMB wetland emission fields and climate predictor variables (e.g., soil temperature and precipitation) from ERA5 reanalysis to yield spatially explicit monthly emissions for 2000–2025 with uncertainty derived from both GMB ensemble spread (35 runs) and ERA5 monthly reanalysis (10 ensemble members). Using the resulting 2000–2025 wetland CH<sub>4</sub> emission data, we then quantify recent emission changes in 2021–2025 relative to 2000–2020, characterize interannual variability in annual regional and latitudinal emission time series, and diagnose long-term growth rates and their seasonality.</p>
      <p id="d2e1390">Our proposed framework and dataset provide a lower-latency, scalable tool for spatially explicit wetland CH<sub>4</sub> emission estimates. They provide support for early-warning diagnostics, attribution of recent atmospheric CH<sub>4</sub> anomalies, and provision of timely priors for atmospheric inversions.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Input datasets</title>
<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><title>Wetland CH<sub>4</sub> flux data</title>
      <p id="d2e1443">We used monthly net CH<sub>4</sub> flux estimates for natural vegetated wetlands from the most recent Global Methane Budget (GMB) synthesis for 2000–2020, including both process-based BU models and atmospheric TD inversions (Saunois et al., 2025; Zhang et al., 2025). In this study, the natural vegetated wetland definition excludes lakes, rivers, reservoirs, coastal waters, and managed sources, following the underlying GMB definition (Saunois et al., 2025). Detailed descriptions of each model and inversion framework are provided in the cited GMB publications; here we summarize the key elements relevant to this study.</p>
      <p id="d2e1455">The BU wetland biogeochemical models (22 estimates, Table S1 in the Supplement) included in the analysis are from 11 models: CLASSIC (Arora et al., 2018; Melton and Arora, 2016), ELM-ECA (Riley et al., 2011), ISAM (Shu et al., 2020; Xu et al., 2021), JSBACH (Kleinen et al., 2020, 2021, 2023), JULES (Gedney et al., 2019b), LPJ-MPI (Kleinen et al., 2012), LPJ-WSL (Zhang et al., 2016), LPX-Bern (Spahni et al., 2011; Stocker et al., 2014), ORCHIDEE (Ringeval et al., 2011), SDGVM (Beerling and Woodward, 2001; Hopcroft et al., 2011, 2020), and VISIT (Ito and Inatomi, 2012). Each model was run under two global climate forcings (CRU and GSWP3-W5E5). All BU simulations are prognostic, i.e. each model computes wetland extent internally rather than relying on a shared wetland extent dataset. Differences in simulated wetland extent therefore contribute to inter-model spread in CH<sub>4</sub> emissions and may explain a substantial fraction of discrepancies across regions.</p>
      <p id="d2e1467">The TD inversion products (13 estimates, Table S2) were constrained by surface or satellite observations over the 2000–2020 period and they are from six systems: CarbonTracker Europe-CH<sub>4</sub> (Tsuruta et al., 2017), LMDz-CIF (Thanwerdas et al., 2022), LMDz-PYVAR (Zheng et al., 2018a, b, 2019), MIROC4-ACTM (Chandra et al., 2021; Patra et al., 2018), NISMON-CH<sub>4</sub> (Niwa et al., 2022, 2025), and NIES-TM-FLEXPART (NFVAR) (Maksyutov et al., 2021; Wang et al., 2019). Two alternative anthropogenic prior inventories, EDGAR v6 (Crippa et al., 2021) and GAINS (Höglund-Isaksson et al., 2020), were used to represent anthropogenic emissions. Wetland and inland freshwater emissions were prescribed as separate prior fluxes in the inversion framework. Wetland priors were derived from the ensemble mean of dynamic process-based BU wetland models used in the GMB estimates, whereas inland freshwater emissions were based on independent BU estimates. We used posterior flux estimates throughout this study.</p>
      <p id="d2e1489">All BU and TD outputs provide monthly wetland CH<sub>4</sub> flux as emission per grid cell area, typically at 1° <inline-formula><mml:math id="M55" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1° resolution in the regridded GMB output products. Coarser products (CLASSIC models at 1.85° and JSBACH models at 2.8°) were remapped to a 1° <inline-formula><mml:math id="M56" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1° grid for spatial consistency across datasets. In total, we included 22 BU estimates and 13 TD estimates (35 estimates overall). Tables S1 and S2 summarize the BU and TD estimates.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <label>2.1.2</label><title>Predictor variables from ERA5 reanalysis</title>
      <p id="d2e1523">We assembled 10 ensemble members of global ERA5 monthly averaged data at 0.5° <inline-formula><mml:math id="M57" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.5° spatial resolution (Hersbach et al., 2023) for 11 climate predictor variables: t2m (near-surface air temperature), tp (total precipitation), ssrd (downward shortwave radiation at surface), slhf (surface latent heat flux), sshf (surface sensible heat flux), swvl1 (volumetric soil water in layers 1, 0–7 cm below surface), swvl2 (volumetric soil water in layers 2, 7–28 cm below surface), stl1 (soil temperature in layer 1, 0–7 cm below surface), stl2 (soil temperature in layer 2, 7–28 cm below surface), lai_hv (high-vegetation leaf area index), and lai_lv (low-vegetation leaf area index). LAI (leaf area index) from ERA5 is prescribed in the ECMWF land-surface model as a seasonally varying, monthly climatology derived from satellite LAI (Roberts et al., 2018). We chose ERA5 data in part because it is operationally updated regularly, which enables continuous extension of predictor fields and low-latency updating of emission reconstructions as new months become available. ERA5 data has also undergone extensive evaluation and is widely used due to its high spatiotemporal consistency and generally strong performance (Hersbach et al., 2020), but notably regional biases remain, for example, a weaker performance in parts of Asia/Africa for hydrology (Gebrechorkos et al., 2024) and temperature in the Arctic (Tian et al., 2024). The 10 ensemble members correspond to the ERA5 Ensemble of Data Assimilations, which provides multiple physically consistent realizations of the reanalysis by perturbing the data assimilation system to sample uncertainty in atmospheric and land-surface states. The ensemble spread can be interpreted as an indicator of reanalysis uncertainty.</p>
      <p id="d2e1533">The 11 variables included in this analysis represent first-order climatic and biophysical controls on wetland CH<sub>4</sub> production, oxidation, and transport. Their relevance to wetland CH<sub>4</sub> emissions is well established in the literature (Knox et al., 2021; Li et al., 2024, 2025; McNicol et al., 2023; Pu et al., 2024; Toet et al., 2011; Yuan et al., 2022, 2024; Zhang et al., 2025). To represent the ecosystem memory effect in response to environmental conditions (Chen et al., 2025), we also included 1-month and 2-month lagged versions of each variable. While introducing short lags would increase collinearity in the machine-learning model, the risk of overfitting is reduced by our model architecture (Sect. 2.2.2, including feature screening, regularization, subsampling, and early stopping). The data are regridded using bilinear interpolation to 1° <inline-formula><mml:math id="M60" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1° resolution to match the wetland CH<sub>4</sub> flux data from the regridded GMB models for further machine-learning modeling.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>XGBoost model</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Data assembly and filtering</title>
      <p id="d2e1586">For each of 350 model-ensemble pairs (35 GMB model estimates <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mo>×</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> ERA5 ensemble members), we constructed gridded monthly time series pairing GMB data with a set of 35 predictor variables: 11 contemporaneous ERA5 variables, 22 lagged variables (1- and 2-month lags for each of the 11 ERA5 variables), and two seasonal encoding terms:

              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M63" display="block"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi mathvariant="normal">sin</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">sin</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">12</mml:mn><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>m</mml:mi><mml:mi mathvariant="normal">cos</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">cos</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">12</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

            Where: <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> month of year (1–12, 1 <inline-formula><mml:math id="M65" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> January and 12 <inline-formula><mml:math id="M66" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> December); <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mi mathvariant="italic">π</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> the constant pi; <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi mathvariant="normal">sin</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi mathvariant="normal">cos</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the sine/cosine transforms of <inline-formula><mml:math id="M70" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> and represent seasonality.</p>
      <p id="d2e1718">We optimised our analyses to reduce noise and computational burden by retaining only grid cells with substantial wetland emissions, defined as those maintaining a mean flux of <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> kg CH<sub>4</sub> m<sup>−2</sup> s<sup>−1</sup> across all GMB model estimates over 2000–2020 (30 000 times lower than the global mean flux).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Model architecture</title>
      <p id="d2e1778">To systematically reconstruct wetland CH<sub>4</sub> fluxes, we developed a machine-learning pipeline, training independent Extreme Gradient Boosting (XGBoost) models (Chen and Guestrin, 2016) for each grid cell and model-ensemble pair. XGBoost has been applied as a surrogate model for ensemble estimates of GMB BU models with high performance (Zhu et al., 2024). The overall modeling workflow consisted of four stages: (1) data splitting, (2) feature screening, (3) hyperparameter tuning, and (4) final model fitting and prediction. Each stage is introduced as follows.</p>
      <p id="d2e1790">Each model-ensemble pair dataset was temporally split into a training set and two testing sets to assess reconstruction capability across different climatic periods at monthly scale. The training data covers January 2003 to December 2017. The testing data covers two periods: January 2000–December 2002 and January 2018–December 2020. Two test windows were used only for out-of-sample evaluation and were not seen during fitting or tuning. The final 24 months of the training period (January 2016 to December 2017) were reserved as a validation set for early stopping and hyperparameter selection. This splitting strategy is to test the model's ability to capture long-term climate variabilities in early/late periods and reduce overfitting.</p>
      <p id="d2e1793">Prior to XGBoost training, we applied Boruta feature screening (Kursa and Rudnicki, 2010) on the training subset to reduce the effective dimensionality of the predictor set and mitigate overfitting risk arising from the relatively large number of candidate predictors. Boruta augments the predictor matrix with “shadow” features formed by randomly permuting each predictor across samples, thereby preserving each predictor's marginal distribution while separating its association with CH<sub>4</sub> flux. A random forest regressor is fit to the combined real/shadow feature set and feature importances are compared. Predictor variables were retained if their random forest importance exceeded the maximum shadow-feature importance in more than 20 % of 10 iterations (Boruta-style screening), while seasonal terms were always retained. The resulting per-grid cell feature subset was then used for both XGBoost fitting and subsequent reconstructions, ensuring that training and prediction used an identical, cell-specific predictor variable set.</p>
      <p id="d2e1805">After the feature screening, we performed a grid search over six hyperparameter configurations (learning rate, maximum tree depth, minimum child weight, subsampling ratio, column subsampling per tree, and L2 regularization) (Table S3). For each configuration, training stopped if the validation Root Mean Squared Error (RMSE) did not improve for 50 consecutive boosting rounds. Once the optimal hyperparameter set was identified for a grid cell, the model was refitted on the full training data using the optimal number of boosting iterations selected during early stopping.</p>
      <p id="d2e1809">After that, the saved booster was then applied to predict wetland CH<sub>4</sub> flux 2000–2025 (including 2021–2025, which extends beyond the most recent GMB estimates period). All the predicted wetland fluxes (unit of kg CH<sub>4</sub> m<sup>−2</sup> s<sup>−1</sup>) were converted to emissions (Tg CH<sub>4</sub> per month) by multiplying the fluxes by grid-cell area (m<sup>2</sup>) and total number of seconds (s) in each month.</p>
      <p id="d2e1873">We recognize that many of these variables are multicollinear, an issue that XGBoost is considered robust against. Nevertheless, we minimized overfitting by constraining model complexity (feature screening, regularized trees with subsampling), using a held-out validation window with early stopping to select the optimal number of boosting iterations, and evaluating performance on temporally separated test periods (2000–2002, 2018–2020) not seen during training. In addition, using the 10 ERA5 ensemble members allows us to propagate reanalysis uncertainty in the predictor fields through the reconstruction.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Model evaluation</title>
      <p id="d2e1884">Model performance was evaluated for each grid cell per model-ensemble pair by computing the <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, RMSE, and NRMSE (normalised RMSE, computed by dividing the RMSE by the standard deviation of emissions) values on the withheld test periods. The mean <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, RMSE and NRMSE of pairs per grid cell are applied to evaluate model performance at the grid cell level (Fig. 1). To assess the model reconstruction skills for grid cells with different emission magnitudes, we grouped grid cells into (1) emission percentile bins based on their total wetland CH<sub>4</sub> emissions during 2000–2020 from GMB estimates, (2) 18 geographical regions defined in Saunois et al. (2025) (they are USA, Canada, Central America, Northern South America, Brazil, Southwest South America, Europe, Northern Africa, Equatorial Africa, Southern Africa, Russia, Central Asia, Middle East, China, Korea-Japan, South Asia, Southeast Asia, and Australasia), and (3) five latitude bands: global, Northern Hemisphere (NH) high-latitudes (60–90° N), NH mid-latitudes (30–60° N), tropics (30° N–30° S), and Southern Hemisphere (SH) extratropics (30–90° S). We then compared the mean <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and RMSE values of each emission bin (0 %–10 % denotes the highest emitting grid cells) and 18 geographical regions (Figs. S1, S2). Monthly mean <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and RMSE at five latitude bands over test periods are presented to study the temporal variation of model performance (Figs. S3, S4). Detrended monthly global emissions from GMB and predictions were compared to assess the model performance in capturing interannual variability (Fig. S5). Detrended anomalies were calculated by fitting a linear least-squares trend to each monthly time series over 2000–2020 and subtracting the corresponding best-fit linear trend from the original series. We generated out-of-sample wetland CH<sub>4</sub> emission predictions (CH<sub>4</sub>_pred) for the test periods to compare with the emissions from GMB models (CH<sub>4</sub>_GMB) (Fig. 2). This ensured that the model predicted CH<sub>4</sub>_pred based on the trained model without having seen the CH<sub>4</sub>_GMB in the test data.</p>

      <fig id="F1"><label>Figure 1</label><caption><p id="d2e1988">Predictive skill of the XGBoost wetland CH<sub>4</sub> model (per-grid-cell <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, RMSE, and NRMSE over the test periods). Insets indicate the zonal mean <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, RMSE and NRMSE in 2° latitude bands.</p></caption>
            <graphic xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026-f01.jpg"/>

          </fig>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e2030">Wetland CH<sub>4</sub> emissions (per 1° <inline-formula><mml:math id="M97" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1° grid cell) from GMB models and XGBoost predictions for two test periods combined. <bold>(a)</bold> Mean CH<sub>4</sub>_GMB (GMB emissions) over all test months. <bold>(b)</bold> Mean CH<sub>4</sub>_pred (XGBoost prediction) over all test months. <bold>(c)</bold> Differences in mean CH<sub>4</sub>_GMB and mean CH<sub>4</sub>_pred. <bold>(d)</bold> Percent emission difference between mean CH<sub>4</sub>_GMB and mean CH<sub>4</sub>_pred. Reds in <bold>(c)</bold> and <bold>(d)</bold> indicate higher emissions in CH<sub>4</sub>_pred, blues lower emissions.</p></caption>
            <graphic xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026-f02.jpg"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Emission trend analyses</title>
      <p id="d2e2147">We quantified spatial patterns, regional aggregates and temporal emission trends in reconstructed wetland CH<sub>4</sub> emissions for 2000–2025, and compared them with corresponding GMB estimates over 2000–2020. We performed analyses for 18 geographic regions and for five latitude bands.</p>
      <p id="d2e2159">We analyzed recent emission changes by comparing 2021–2025 against 2000–2020 baseline at both grid-cell and regional scales (Figs. 3, 4). For Fig. 3, gridded monthly emissions were aggregated to per-grid mean emissions for each period (2021–2025 and 2000–2020). Emissions presented in Fig. 4 were summed across grid cells within each region. Emission changes between the two periods were calculated as paired differences for each grid cell and model–ensemble pair. Therefore, the reported mean and 95 % confidence interval for emission changes reflect the uncertainty of the paired differences themselves. We examined interannual variability and long-term annual emission changes by aggregating monthly emissions to annual totals for both the latitude bands and 18 geographic regions (Figs. 5, S6, S8). Ordinary least squares regression was applied to monthly emissions over 2000–2025 to estimate emission trends (Fig. 6).</p>

      <fig id="F3"><label>Figure 3</label><caption><p id="d2e2164"><bold>(a)</bold> Mean XGBoost model predicted wetland CH<sub>4</sub> emissions for 2021–2025. <bold>(b)</bold> Difference between mean emissions in 2021–2025 and 2000–2020. Reds indicate higher emissions in 2021–2025, blues lower. Insets indicate the zonal mean in 2° latitude bands.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026-f03.jpg"/>

        </fig>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e2190"><bold>(a)</bold> Spatial distribution of the 18 regions; <bold>(b)</bold> Regional wetland CH<sub>4</sub> emission changes during 2021–2025 relative to 2000–2020 across 18 regions using XGBoost modeled emissions. Bars show regional mean emission changes (annual mean in 2021–2025 minus that in 2000–2020). Error bars indicate 95 % CI. A two-sided paired test was applied for each region to assess whether the 2021–2025 mean emission differs from the 2000–2020 mean. Regions with <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> are labelled “ns”. Asterisks above bars denote significance: *** for <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.001</mml:mn></mml:mrow></mml:math></inline-formula>, ** for <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>, * for <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026-f04.png"/>

        </fig>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e2264">Annual wetland CH<sub>4</sub> emissions for the six top-emitting regions. Solid lines show model predictions of annual mean emissions, and shaded areas indicate 95 % CI. Dashed lines show GMB emission estimates (mean). Panel titles indicate the region code and region name, which correspond to the region definitions shown in Fig. 4.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026-f05.png"/>

        </fig>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e2284">Regional and seasonal trends (TgCH<sub>4</sub> yr<sup>−1</sup>) in predicted wetland CH<sub>4</sub> emissions. <bold>(a)</bold> Trends across five latitude bands across three time periods (2000–2025, 2021–2025, and 2000–2020). <bold>(b)</bold> Trends for each calendar month over 2000–2025. Positive trends indicate an increase in CH<sub>4</sub> emissions, while negative values indicate a decrease. Error bars indicate 95 % CI.</p></caption>
          <graphic xlink:href="https://essd.copernicus.org/articles/18/3507/2026/essd-18-3507-2026-f06.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Uncertainty analysis</title>
      <p id="d2e2347">Emulator skill uncertainty was evaluated using held-out test period <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, RMSE, NRMSE and prediction residuals relative to the GMB fields (Sects. 2.2.3 and 3.1). Uncertainty in reconstructed wetland CH<sub>4</sub> emissions was estimated from the ensemble spread across all reconstructions generated from the 35 GMB estimates and 10 ERA5 ensemble members. This propagated two sources of uncertainty through the framework: (i) spread in the underlying GMB estimates and (ii) uncertainty in the predictors represented by the ERA5 ensemble. We use 95 % confidence interval (CI) to represent this emission uncertainty.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and Discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Model performance evaluation</title>
      <p id="d2e2386">We begin by evaluating model performance at the spatial scales most relevant to CH<sub>4</sub> budgeting. Aggregated annual wetland CH<sub>4</sub> emissions at the global and latitudinal-band scales show that the emulator reproduces the overall magnitude, temporal variability, and broad zonal structure of the GMB estimates over 2000–2020 (Fig. S6), providing a large-scale context for the finer grid-cell evaluation presented below.</p>
      <p id="d2e2407">Across the two test windows (2000–2002 and 2018–2020), the XGBoost model reproduces monthly wetland CH<sub>4</sub> emissions well. Globally, the coefficient of determination was <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.65 <inline-formula><mml:math id="M123" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.003 (mean <inline-formula><mml:math id="M124" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 95 % CI, hereafter; Fig. 1a), which refers to the mean grid-cell <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> across all global land cells over the two test periods, with the 95 % confidence interval calculated across grid cells. This reported reconstructive skill indicates strong predictability from predictor variables. However, the model performance varies geographically. Mean <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> is higher in the Southern Hemisphere (SH) than in the Northern Hemisphere (NH) (0.77 <inline-formula><mml:math id="M127" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.006 compared with 0.62 <inline-formula><mml:math id="M128" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004, respectively), and higher in the tropics than in the extratropics (<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.78</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.004</mml:mn></mml:mrow></mml:math></inline-formula> and 0.58 <inline-formula><mml:math id="M130" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.004, respectively). In the top emitting regions, mean <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values are generally higher than in regions with lower emissions (Fig. S1a). Global RMSE over test periods is <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.49</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.12</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup> (Fig. 1b). RMSE for the tropics is about twice that of the RMSE for the extratropics (9.37 <inline-formula><mml:math id="M135" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.27 <inline-formula><mml:math id="M136" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<sup>−3</sup> and 3.35 <inline-formula><mml:math id="M138" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.08 <inline-formula><mml:math id="M139" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<sup>−3</sup> Tg CH<sub>4</sub> yr<sup>−1</sup>, respectively). Top emitting regions exhibit higher RMSE, e.g., RMSE doubled for top 10 % emitting regions compared with top 10 %–20 % emitting regions (Fig. S1b). Regionally, mean <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values are highest in Southeast Asia and Korea-Japan (<inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>), and lowest in Russia and Canada (<inline-formula><mml:math id="M145" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 0.5) (Fig. S2a). Mean RMSE is highest in the Americas (Northern South America and Central America), and lowest in the Middle East and Central Asia. Generally, NRMSE is inversely correlated to <inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, indicating a better performance of our model in top emitting regions (Fig. 1c). Temporal variation of model performance reveals the lowest <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> in January/February in NH high latitudes (Fig. S3), and the highest RMSE in July–September in the tropics (Fig. S4). We further evaluate how these spatial and temporal differences in model skill influence long-term variability in annual emissions in Sect. 3.3.</p>
      <p id="d2e2680">To examine predictive uncertainty, we compare wetland CH<sub>4</sub> emissions from the GMB models (CH<sub>4</sub>_GMB; Fig. 2a) with XGBoost predictions (CH<sub>4</sub>_pred; Fig. 2b) over the two test periods. Globally, CH<sub>4</sub>_pred reproduces both the magnitude and spatial pattern of CH<sub>4</sub>_GMB, including the major hotspots concentrated in the tropics, such as Amazon Basin (central-western Amazon floodplains, Pantanal and Moxos plains), Congo Basin, the Sudd wetlands in South Sudan, and Southeast Asia (Sumatra, Borneo, Peninsular Malaysia, and New Guinea), with additional hotspots in NH high latitudes, such as West Siberian Plain and Hudson/James Bay Lowlands.</p>
      <p id="d2e2728">The differences in emissions (Fig. 2c) and the corresponding percent emission differences (Fig. 2d) between CH<sub>4</sub>_GMB and CH<sub>4</sub>_pred highlight spatial biases. During the test periods, the global mean predicted wetland CH<sub>4</sub> emission is <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mn mathvariant="normal">158.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.1</mml:mn></mml:mrow></mml:math></inline-formula> Tg CH<sub>4</sub> yr<sup>−1</sup>, which is 2.3 Tg CH<sub>4</sub> yr<sup>−1</sup> lower than the global mean of CH<sub>4</sub>_GMB (160.7 <inline-formula><mml:math id="M162" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.2 Tg CH<sub>4</sub> yr<sup>−1</sup>), corresponding to a 1.4 % underestimation (Fig. 2c). This difference is within the estimated uncertainty range of the two global means. Underestimation is strongest over high-emission systems, such as the central-western Amazon Basin, Southeast Asia, Congo Basin and West Siberian Plain (Fig. 2c), where our model predicted emissions are lower than GMB estimates, but percent differences are smaller because the denominator (CH<sub>4</sub>_GMB) is large. For example, in Southeast Asia, the mean bias is <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.44</mml:mn></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup>, yet the relative bias is only <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.7</mml:mn></mml:mrow></mml:math></inline-formula> % given a high regional mean emission (CH<sub>4</sub>_GMB of 25.2 Tg CH<sub>4</sub> yr<sup>−1</sup>). Monthly anomalies in global emissions reveal small disagreements between the predictions and GMB estimates (<inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>±</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> Tg CH<sub>4</sub> yr<sup>−1</sup>) (Fig. S5). Largest discrepancies occur in July/August 2020 (underestimation of 15 Tg CH<sub>4</sub> yr<sup>−1</sup>).</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Emission trends and predicted anomalies in recent years (2021–2025)</title>
      <p id="d2e2995">Figure 3 shows spatial maps of global predicted mean wetland CH<sub>4</sub> emissions for 2021–2025 (Fig. 3a) and emission differences between 2021–2025 and 2000–2020. The 2021–2025 mean emission is 157.8 <inline-formula><mml:math id="M179" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.4 TgCH<sub>4</sub> yr<sup>−1</sup> (<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3.72</mml:mn></mml:mrow></mml:math></inline-formula>, with the <inline-formula><mml:math id="M183" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula>-score indicating how far each region's mean emission estimate deviates from the cross-region mean, measured in standard deviation units), representing a non-significant increase of 0.05 Tg CH<sub>4</sub> yr<sup>−1</sup> relative to the 2000–2020 mean. However, changes are more pronounced across latitudes. NH mid- and high-latitude wetland emissions increase during 2021–2025 by 0.76 <inline-formula><mml:math id="M186" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07 (from 29.9 <inline-formula><mml:math id="M187" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.1 in 2000–2020 to 30.7 <inline-formula><mml:math id="M188" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.2 in 2021–2025, <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.21</mml:mn></mml:mrow></mml:math></inline-formula>) and 0.35 <inline-formula><mml:math id="M190" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.03 (from 11.0 <inline-formula><mml:math id="M191" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.7 to <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mn mathvariant="normal">11.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup>, <inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.01</mml:mn></mml:mrow></mml:math></inline-formula>), respectively, compared with 2000–2020 emissions. These changes correspond to <inline-formula><mml:math id="M196" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2.5 % and <inline-formula><mml:math id="M197" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 3.2 % increase. The continued growth in these regions in 2021–2025 (relative to 2000–2020), together with increases reported for 2010–2018 relative to 1981–1989 (Feron et al., 2024), suggests an increasing role of boreal and temperate wetlands in recent decades of global warming. In contrast, emissions decrease in the tropics and SH extratropics during 2021–2025. The tropics exhibit a 0.95 <inline-formula><mml:math id="M198" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.19 TgCH<sub>4</sub> yr<sup>−1</sup> emission decrease (<inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.81</mml:mn></mml:mrow></mml:math></inline-formula>), from 113.9 <inline-formula><mml:math id="M202" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.5 (2000–2020) to 112.9 <inline-formula><mml:math id="M203" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.5 TgCH<sub>4</sub> yr<sup>−1</sup> (2021–2025), while SH extratropics emissions decline by 3.5 % (<inline-formula><mml:math id="M206" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.11 <inline-formula><mml:math id="M207" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.02 TgCH<sub>4</sub> yr<sup>−1</sup>, <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.34</mml:mn></mml:mrow></mml:math></inline-formula>)  from 3.1 <inline-formula><mml:math id="M211" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.1 (2000–2020) to 3.0 <inline-formula><mml:math id="M212" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.1 TgCH<sub>4</sub> yr<sup>−1</sup> (2021–2025).</p>
      <p id="d2e3348">We further assess regional wetland CH<sub>4</sub> emission changes in 2021–2025 compared with 2000–2020 across 18 regions using XGBoost predictions (Fig. 4). Four regions show no significant change (<inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> from two-sided paired significance test, labelled “ns”). Among the 14 regions with significant changes, nine regions show increases and five show decreases (Northern South America, Brazil, Southwest South America, Northern Africa, and Equatorial Africa). Notably, all regions with decreases are located in South America and Africa. The largest emission changes (2021–2025 relative to 2000–2020) occur in Brazil (<inline-formula><mml:math id="M217" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.59 <inline-formula><mml:math id="M218" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09 TgCH<sub>4</sub> yr<sup>−1</sup>), Canada (<inline-formula><mml:math id="M221" display="inline"><mml:mo lspace="0mm">+</mml:mo></mml:math></inline-formula>0.46 <inline-formula><mml:math id="M222" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.05 TgCH<sub>4</sub> yr<sup>−1</sup>), Southwest South America (<inline-formula><mml:math id="M225" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.43 <inline-formula><mml:math id="M226" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07 TgCH<sub>4</sub> yr<sup>−1</sup>), Russia (<inline-formula><mml:math id="M229" display="inline"><mml:mo lspace="0mm">+</mml:mo></mml:math></inline-formula>0.31 <inline-formula><mml:math id="M230" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.03 TgCH<sub>4</sub> yr<sup>−1</sup>), Southeast Asia (<inline-formula><mml:math id="M233" display="inline"><mml:mo lspace="0mm">+</mml:mo></mml:math></inline-formula>0.22 <inline-formula><mml:math id="M234" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.03 TgCH<sub>4</sub> yr<sup>−1</sup>) and Equatorial Africa (<inline-formula><mml:math id="M237" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.21 <inline-formula><mml:math id="M238" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.04 TgCH<sub>4</sub> yr<sup>−1</sup>). The pronounced decline over Brazil possibly reflects the exceptional drought conditions in the Amazon basin during 2022–2024, including record-low river levels and anomalously warm, dry conditions (Espinoza et al., 2024). Such hydroclimatic drying reduces floodplain inundation and lowers water tables, which suppresses anaerobic conditions and thereby limits wetland methane production and emissions (Cui et al., 2024).</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>26-year emission trends and anomalies (2000–2025)</title>
      <p id="d2e3594">The emission predictions enable an assessment of long-term trends and interannual variability in wetland emissions over 2000–2025. Annual emission time series show pronounced peaks in 2011 and 2016/2017 in the tropics, NH mid-latitudes, and globally (Fig. S6). Monthly emission anomalies in these regions (Fig. S7) indicate that the annual maxima are driven by sustained positive anomalies during August 2010–May 2011 and August 2016–December 2017, which coincide with La Niña conditions. This alignment is consistent with prior studies reporting La Niña-driven wetting and expanded inundation that enhance tropical wetland CH<sub>4</sub> emissions (Hodson et al., 2011; Hasan et al., 2022; Nisbet et al., 2023; Lin et al., 2024; Murguia-Flores et al., 2023; Zhang et al., 2020, 2018; Zhu et al., 2017), and with the broader evidence that CH<sub>4</sub> growth in 2020–2022 coincided with an unusual persistent La Niña event.</p>
      <p id="d2e3615">In the 2020s, global and tropical annual emissions reach a minimum in 2023 (Figs. S6, S7), coincident with a strong El Niño event. This is supported by two recent studies reporting a sharp decline in wetland emissions in South America (Ciais et al., 2026) and Amazonia (Quinn et al., 2025) in 2023 linked to El Niño-related drought. Our results further suggest that Brazil and Southwest South America are the key contributors, and both rank among the top six emitting regions globally (Fig. 5). Annual emissions in Brazil decline steadily across the study period, from <inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mn mathvariant="normal">24.8</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup> in 2000 to 23.3 <inline-formula><mml:math id="M246" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 TgCH<sub>4</sub> yr<sup>−1</sup> in 2025, with the lowest emission in 2024 (22.8 <inline-formula><mml:math id="M249" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 TgCH<sub>4</sub> yr<sup>−1</sup>) (Fig. 5). Emissions in Southwest South America are relatively stable during 2000–2014, decrease markedly during 2014–2023 (from 17.2 <inline-formula><mml:math id="M252" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.6 to <inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mn mathvariant="normal">15.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup>), and show a modest recovery in 2024/2025 (Fig. 5).</p>
      <p id="d2e3749">The remaining four top emitting regions show contrasting behavior. Since 2019, Southeast Asia, Canada and Russia show increasing emissions, whereas Equatorial Africa emissions decrease slightly (Fig. 5). Southeast Asian emissions fluctuate around 24.7 <inline-formula><mml:math id="M256" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.5 TgCH<sub>4</sub> yr<sup>−1</sup> over 2000–2025, with a minimum in 2015 (23.8 <inline-formula><mml:math id="M259" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.7 TgCH<sub>4</sub> yr<sup>−1</sup>) and a maximum in 2017 (25.6 <inline-formula><mml:math id="M262" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.7 TgCH<sub>4</sub> yr<sup>−1</sup>). Emissions in Canada are comparatively stable during 2005–2015, while variability is larger before 2005 and after 2015: the amplitude reaches <inline-formula><mml:math id="M265" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1.5 TgCH<sub>4</sub> yr<sup>−1</sup> in these periods, approximately double that during 2005–2015 (<inline-formula><mml:math id="M268" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 0.8 TgCH<sub>4</sub> yr<sup>−1</sup>). Equatorial African emissions remain 17.0 <inline-formula><mml:math id="M271" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 TgCH<sub>4</sub> yr<sup>−1</sup> during 2000–2025, despite two notable declines during 2002–2005 (<inline-formula><mml:math id="M274" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.5 TgCH<sub>4</sub> yr<sup>−1</sup>) and 2019–2025 (<inline-formula><mml:math id="M277" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.6 TgCH<sub>4</sub> yr<sup>−1</sup>).</p>
      <p id="d2e3980">For regions showing increasing emissions in our XGBoost predictions (e.g., Southeast Asia, Canada, and Russia), these changes are likely driven by wetter and/or warmer conditions that enhance inundation, substrate supply, and CH<sub>4</sub> production. For instance, observed increases in Boreal-Arctic wetland CH<sub>4</sub> emissions have been linked to warming and enhanced ecosystem productivity (Yuan et al., 2024), while inversion-based studies highlight the role of La Niña-driven inundation in enhancing emissions from Equatorial Asia (Qu et al., 2024; Lin et al., 2024; Feng et al., 2022). However, our emulator predictions diverge from recent atmospheric inversion literature regarding African wetland emissions. Multiple top-down studies indicate that enhanced emissions from tropical Africa contributed substantially to the global CH<sub>4</sub> surge during 2020–2024 (Balasus et al., 2026; Qu et al., 2024). In contrast, our climate-driven emulator predicts that emissions across Northern, Equatorial, and Southern Africa remained relatively stable or slightly decreased during similar time periods (Figs. 4, 5, S8). We attribute this discrepancy to weaker performance and regional precipitation biases of ERA5 data over parts of Africa in capturing complex African hydrological dynamics (Gebrechorkos et al., 2024).</p>
      <p id="d2e4011">Regional emission time series (Figs. 5, S8) help explain the pronounced disagreement in 2019–2020 for global and tropical emissions, where predictions are substantially lower than the GMB estimates (Fig. S6). For 2019, the prediction mean emissions are 5.5 TgCH<sub>4</sub> yr<sup>−1</sup> below the GMB estimates for global emissions (<inline-formula><mml:math id="M285" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 3.5 % underestimation), while emission changes in Equatorial Africa, Brazil, USA, Southern Africa, and Southwest South America jointly account for 4.3 TgCH<sub>4</sub> yr<sup>−1</sup> of this discrepancy. In 2020, the modeled mean global emissions are 9.8 TgCH<sub>4</sub> yr<sup>−1</sup> lower than GMB (<inline-formula><mml:math id="M290" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 6 % underestimation). The discrepancies in the tropics explain 9.2 TgCH<sub>4</sub> yr<sup>−1</sup> of the underestimation, including major regions such as Eastern Africa, Southwest South America, Southeast Asia, Brazil, and Northern Africa. Notably, this disagreement in 2019–2020 is not evident in other latitude bands and does not persist outside these years. We cautiously interpret this mismatch as the limitations of the emulator and uncertainty in the underlying GMB ensemble. The climate predictors used in this study can only indirectly capture ENSO (El Niño-Southern Oscillation) effects. Although the training period includes several ENSO events, the unusual persistence of the 2020–2023 triple-dip La Niña may still be underrepresented. In addition, most TD estimates from GMB use a similar prescribed OH (hydroxyl radical) distribution, possibly causing OH-related uncertainty to be underrepresented, particularly during anomalous periods such as COVID.</p>
      <p id="d2e4113">Finally, we examine trends in predicted monthly wetland CH<sub>4</sub> emissions across five latitude bands (Fig. 6a) and 12 calendar-month categories (Fig. 6b). Figure 6a compares these trends across three time periods (2000–2025, 2021–2025, and 2000–2020). Figure 6b shows the trends by 12 calendar-month categories for the 2000–2025 period. We summed predicted monthly emissions across all grid cells within each latitude band to form regional monthly time series, then computed monthly emission anomalies by subtracting the 2000–2025 climatological mean. We then estimated trends (Tg CH<sub>4</sub> yr<sup>−1</sup>) using ordinary least squares linear regression of the anomaly time series. We calculated a <inline-formula><mml:math id="M296" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula>-score for each region and period by dividing the estimated trend by its standard error to assess the statistical significance of the trends.</p>
      <p id="d2e4153">The global wetland CH<sub>4</sub> emission trend is three times lower in 2021–2025 compared with the 2000–2020 period (0.05 <inline-formula><mml:math id="M298" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.28 and 0.15 <inline-formula><mml:math id="M299" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.05 Tg CH<sub>4</sub> yr<sup>−1</sup>, respectively) (Fig. 6a). However, the magnitude of changes in emission trends in NH mid-latitudes, the tropics and SH extratropics is greater in 2021–2025 than 2000–2020 level. Emission trends in NH mid-latitudes increased three times from 0.05 <inline-formula><mml:math id="M302" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.02 TgCH<sub>4</sub> yr<sup>−1</sup> (<inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4.94</mml:mn></mml:mrow></mml:math></inline-formula>) in 2000–2020 to <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.16</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.12</mml:mn></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup> (<inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.49</mml:mn></mml:mrow></mml:math></inline-formula>) during 2021–2025. The tropics exhibit a reversal of their emission trends from positive in 2000–2020 (0.07 <inline-formula><mml:math id="M310" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.03 Tg CH<sub>4</sub> yr<sup>−1</sup>, <inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3.95</mml:mn></mml:mrow></mml:math></inline-formula>) to negative in 2021–2025 (<inline-formula><mml:math id="M314" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.18 <inline-formula><mml:math id="M315" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.24 Tg CH<sub>4</sub> yr<sup>−1</sup>, <inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.45</mml:mn></mml:mrow></mml:math></inline-formula>). Emission trends in SH extratropics increased from nearly zero in 2000–2020 (<inline-formula><mml:math id="M319" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8.74</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5.18</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> TgCH<sub>4</sub> yr<sup>−1</sup>, <inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.33</mml:mn></mml:mrow></mml:math></inline-formula>) to higher than the global average in 2021-2025 (0.04 <inline-formula><mml:math id="M324" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.02 TgCH<sub>4</sub> yr<sup>−1</sup>, <inline-formula><mml:math id="M327" display="inline"><mml:mrow><mml:mi>z</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3.30</mml:mn></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d2e4494">Evaluating emission trends over individual months (Fig. 6b), we find that the global trend peaks in late boreal summer, with the largest increases in August and September (0.15 <inline-formula><mml:math id="M328" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.18 and 0.21 <inline-formula><mml:math id="M329" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13 TgCH<sub>4</sub> yr<sup>−1</sup>, respectively). The strongest seasonal intensification occurs in NH mid-latitudes during June–September (0.09–0.12 Tg CH<sub>4</sub> yr<sup>−1</sup>), consistent with the dominant contribution from boreal growing-season emissions. For both NH mid- and high-latitudes, growth rates are systematically higher during May–October (growing season) than during November–April. In the tropics, monthly growth reaches its highest in October–December and lowest in June–August (negative growth). SH extratropics show near-zero growth throughout the year (slightly negative).</p>
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<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Limitations</title>
      <p id="d2e4562">A limitation concerns source attribution in the TD estimates used for training. Although the TD inversions adopted BU wetland priors that exclude inland freshwater systems, the coarse spatial resolution of TD inversions can still limit the separation of natural vegetated wetland emissions from nearby open-water or inland-freshwater emissions in mixed floodplain environments. This uncertainty cannot be quantified explicitly in the present framework because no independent source-resolved posterior diagnostic is available. Future progress is likely to come from higher-resolution atmospheric inverse frameworks. Two recent studies performed 25 km resolution atmospheric inversions using satellite observations in regional and global applications and improved spatial attribution (East et al., 2025; Hancock et al., 2025).</p>
      <p id="d2e4565">Another limitation is that our framework predicts wetland emissions from climate predictors only. ENSO-related impacts can be captured only indirectly, while dynamic inundation and atmospheric chemistry perturbations are outside the predictor space of the model.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Data availability</title>
      <p id="d2e4577">ERA5 monthly averaged data are available at Copernicus Climate Change Service Climate Data Store at <uri>https://cds.climate.copernicus.eu/datasets/reanalysis-era5-single-levels-monthly-means?tab=overview</uri> (last access: 22 January 2026) (<ext-link xlink:href="https://doi.org/10.24381/cds.f17050d7" ext-link-type="DOI">10.24381/cds.f17050d7</ext-link>) (Copernicus Climate Change Service, 2023). The global natural wetland methane emission dataset generated from this study is publicly available at <ext-link xlink:href="https://doi.org/10.5281/zenodo.18870108" ext-link-type="DOI">10.5281/zenodo.18870108</ext-link> (Li et al., 2026).</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d2e4598">This study presents a framework to extend global natural wetland CH<sub>4</sub> emissions from 2000 through 2025 by applying a machine-learning emulator to provide a lower-latency release of GMB estimates to estimate wetland emissions and is intended for routine updates. The framework reproduces both spatial patterns and interannual variability of the GMB estimates. The extended wetland CH<sub>4</sub> emission record shows that the magnitude of emission changes in 2021–2025 is substantially larger than the long-term trend over 2000–2020, even though the global mean emission change is relatively small.</p>
      <p id="d2e4619">A key emerging feature is accelerated emissions estimated in the NH mid-latitudes and high-latitudes. Seasonal trend analyses indicate that these increases are concentrated in the warm season (May–October), consistent with an amplification of the seasonal cycle and a strengthening of late-summer growth, highlighting Northern mid- and high-latitude wetlands as regions where intensifying trends are most evident in recent years.</p>
      <p id="d2e4622">In contrast, the tropics show a reversal in emission trend in the post-2020s, from an emission increase during 2000–2020 to a decline in 2021–2025. Nevertheless, the tropics still dominate interannual variability of global wetland emissions and can strongly influence the global CH<sub>4</sub> budget through episodic hydroclimate extremes.</p>
      <p id="d2e4634">More broadly, this emulator framework may also apply to other low-latency Earth system applications beyond wetland CH<sub>4</sub> emissions, particularly for environments and pollutants that can be constrained by routinely updated predictor fields. At the same time, the present results point to several opportunities for improvement, including better representation of dynamic inundation and improved separation of wetland and inland-freshwater emissions.</p>
      <p id="d2e4647">Overall, this work proposes an operational, low-latency emulator framework that provides a scalable pathway to track wetland CH<sub>4</sub> emissions in response to climate anomalies by leveraging routinely updated Earth observation reanalysis data.</p>
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    <back><app-group>
        <supplementary-material position="anchor"><p id="d2e4658">The supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/essd-18-3507-2026-supplement" xlink:title="pdf">https://doi.org/10.5194/essd-18-3507-2026-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e4669">M.L.: conceptualization, methodology, workflow development, formal analysis, visualization, writing – original draft, supervision, funding acquisition. R.B.J.: conceptualization, methodology, data curation, supervision, funding acquisition. M.S.: conceptualization, methodology, data curation. P.C.: conceptualization, methodology. B.P.: conceptualization, methodology, data curation. J.G.C.: conceptualization, methodology, data curation. P.K.P.: conceptualization, methodology, data curation. H.T.: conceptualization, methodology, data curation. Z.Z.: methodology, data curation. E.F.-C.: methodology, data curation. Z.O.: methodology, data curation. T.Z.: visualization. D.J.B.: data curation. D.A.B.: data curation. P.B.: data curation. D.C.: data curation. N.C.: data curation. N.G.: data curation. P.O.H.: data curation. K.I.: data curation. A.I.: data curation. A.K.J.: data curation. K.J.: data curation. F.J.: data curation. T.K.: data curation. M.K.: data curation. T.L.: data curation. X.L.: data curation. S.M.: data curation. A.M.: data curation. A.M.H.: data curation. K.M.: data curation. J.R.M.: data curation. J.M.: data curation. Y.N.: data curation. S.Pan.: data curation. S.Peng: data curation. C.P.: data curation. Z.Q.: data curation. P.R.: data curation. W.R.: data curation. A.S.: data curation. R.L.T.: data curation. A.T.: data curation. X.Y.: data curation. W.Z.: data curation. B.Z.: data curation. Q.Zhu: data curation. Q.Zhuang: data curation. All authors contributed to writing – review &amp; editing of the manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e4675">At least one of the (co-)authors is a member of the editorial board of <italic>Earth System Science Data</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="d2e4684">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><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e4690">This research is supported by the National University of Singapore (NUS) (Start-Up grant). R.J. received support from the Gordon and Betty Moore Foundation (grant no. GBMF11519 to Stanford University), the Global Methane Office at the Stanford Doerr School of Sustainability, and the John Wesley Powell Center for Analysis and Synthesis of the U.S. Geological Survey (“Scaling tropical wetland methane fluxes regionally and globally” working group). D.B. and P.K. were supported by the Environment Research and Technology Development Fund (grant no. JPMEERF24S12205) of the Environmental Restoration and Conservation Agency of Japan. F.L. received support from startup funds provided by The University of Texas at Austin. A.M. was supported by an Early Career Award by the U.S. Department of Energy. A.M.H. received support from the National Science Foundation award 2406964. F.J. and J.M. received funding from the Swiss National Science Foundation (No. 200020_200511). N.G was funded by the Met Office Climate Science for Service Partnership (CSSP) Brazil project which is supported by the Department for Science, Innovation &amp; Technology (DSIT). C.P. was supported by the Joint Fund for Regional Innovation and Development of the National Science Foundation (U22A20570). K.Y. was supported by UH Energy. This paper is a contribution to the League of geophysical research eXcellences for tropical Asia (LeXtra).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e4696">This paper was edited by Yuqiang Zhang and reviewed by three anonymous referees.</p>
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