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  <front>
    <journal-meta><journal-id journal-id-type="publisher">BG</journal-id><journal-title-group>
    <journal-title>Biogeosciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">BG</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Biogeosciences</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1726-4189</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/bg-23-3407-2026</article-id><title-group><article-title><italic>Sphagnum</italic> and herbaceous net ecosystem exchanges in a Pyrenean peatland: a long-term study using the ISBA model</article-title><alt-title><italic>Sphagnum</italic> and herbaceous net ecosystem exchanges in a Pyrenean peatland</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Garisoain</surname><given-names>Raphael</given-names></name>
          <email>raphael.garisoain@univ-tlse3.fr</email>
        <ext-link>https://orcid.org/0000-0002-0489-1264</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Delire</surname><given-names>Christine</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6114-3211</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Decharme</surname><given-names>Bertrand</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8661-1464</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Gandois</surname><given-names>Laure</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Météo-France, CNRS, Univ. Toulouse, CNRM, Toulouse, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>CRBE, Universite de Toulouse, CNRS, Toulouse, France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Raphael Garisoain (raphael.garisoain@univ-tlse3.fr)</corresp></author-notes><pub-date><day>20</day><month>May</month><year>2026</year></pub-date>
      
      <volume>23</volume>
      <issue>10</issue>
      <fpage>3407</fpage><lpage>3431</lpage>
      <history>
        <date date-type="received"><day>23</day><month>October</month><year>2025</year></date>
           <date date-type="rev-request"><day>27</day><month>November</month><year>2025</year></date>
           <date date-type="rev-recd"><day>23</day><month>April</month><year>2026</year></date>
           <date date-type="accepted"><day>24</day><month>April</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Raphael Garisoain 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://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026.html">This article is available from https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026.html</self-uri><self-uri xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026.pdf">The full text article is available as a PDF file from https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e118">Peatlands play a crucial role in the global carbon cycle, acting as long-term carbon sinks. However, their stability is increasingly threatened by climate change, particularly through rising temperatures and the intensification of droughts. This study focuses on the Bernadouze peatland in the Pyrenees Mountains and aims to validate a newly implemented <italic>Sphagnum</italic> Plant Functional Type (PFT) in the ISBA land surface model, assess the temporal evolution of carbon fluxes over the past 64 years, and investigate the factors influencing carbon accumulation, with a particular emphasis on drought events.</p>

      <p id="d2e124">The model was validated using in situ data, demonstrating reasonable carbon flux estimations. Using this validated model, we reconstructed the net ecosystem exchange (NEE) dynamics of the Bernadouze peatland from 1959 to 2022. The results reveal significant interannual variability in NEE, largely driven by air temperature and water table depth. While the peatland has remained a carbon sink, extreme droughts such as those in 1989, 1994, 2003, and most recently 2022 have led to substantial <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions.</p>

      <p id="d2e138">Our findings suggest that although increasing temperatures have extended the growing season and enhanced gross primary productivity (GPP), the rising frequency and intensity of droughts pose a long-term risk to peatland carbon storage. The dryness index developed in this study appears to be a strong predictor of summer and annual NEE, offering a potential tool for estimating carbon fluxes in peatlands lacking direct measurements.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>Agence Nationale de la Recherche</funding-source>
<award-id>ANR-22-PEXF-0011</award-id>
<award-id>ANR-11-LABX0010</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="d2e150">Peatlands are vital to the global carbon cycle, serving as significant carbon reservoirs and actively exchanging <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and methane with the atmosphere <xref ref-type="bibr" rid="bib1.bibx26" id="paren.1"/>. However, the stability of these carbon stocks is increasingly threatened by global warming <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx7 bib1.bibx40" id="paren.2"/>, highlighting the need for precise models to predict their carbon balance. This concern is particularly relevant in mountainous regions, where climate change is expected to be more pronounced <xref ref-type="bibr" rid="bib1.bibx50" id="paren.3"/>, potentially affecting the functioning of mountain peatland ecosystems.</p>
      <p id="d2e173">Models have been developed to represent the biophysical and biogeochemical processes that occur in peatlands. <italic>Sphagnum</italic> mosses are considered the dominant vegetation in Northern peatlands <xref ref-type="bibr" rid="bib1.bibx56" id="paren.4"/> and function differently from vascular plants, lacking stomata to regulate their water content <xref ref-type="bibr" rid="bib1.bibx11" id="paren.5"/>. They acquire water either by absorbing atmospheric precipitation or through capillary action directly from the soil surface. Their presence is also crucial for the accumulation of organic carbon in peatlands, as they have a lower litter decomposition rate compared to vascular plants <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx38" id="paren.6"/>. As a result, various classes of models have been developed to account for the role of <italic>Sphagnum</italic> mosses, reflecting diverse approaches. Dynamic vegetation and ecosystem models, developed as offline tools without atmospheric, climate, or carbon feedbacks, have since incorporated these processes into their frameworks <xref ref-type="bibr" rid="bib1.bibx64 bib1.bibx18 bib1.bibx63 bib1.bibx25 bib1.bibx41" id="paren.7"/>. Furthermore, specific Continental Surface Models (CSMs) have been developed for the representation of peatlands <xref ref-type="bibr" rid="bib1.bibx55 bib1.bibx69 bib1.bibx70 bib1.bibx65 bib1.bibx45" id="paren.8"/>. There have also been ongoing efforts to improve the representation of <italic>Sphagnum</italic> mosses in Global Land Surface models, with varying degrees of complexity and scope <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx47 bib1.bibx16 bib1.bibx48 bib1.bibx52 bib1.bibx28 bib1.bibx53" id="paren.9"/>.</p>
      <p id="d2e204">Efforts to study peatland responses to drought episodes increasingly rely on field measurements and mesocosm experiments <xref ref-type="bibr" rid="bib1.bibx54 bib1.bibx49" id="paren.10"/>, though research in this area remains limited. A significant limitation of these methods is the scarcity of continuous field measurements capturing medium-term carbon fluxes over decades or longer. Such data would offer critical insights into the frequency and long-term effects of episodic drought events on carbon accumulation. Current carbon flux measurements are generally restricted to contemporary dynamics, which exhibit notable interannual variability, complicating efforts to extrapolate trends over medium or long-term timescales <xref ref-type="bibr" rid="bib1.bibx71" id="paren.11"/>. To explore long-term carbon accumulation dynamics, peat coring analyses provide a reliable means of determining the average LOng-term apparent Rates of C Accumulation (LORCA), offering insights into millennia of accumulation <xref ref-type="bibr" rid="bib1.bibx57" id="paren.12"/>. Additionally, based on the same methodology, the Actual Rate of Carbon Accumulation (ARCA) can be determined, theoretically enabling the observation of carbon accumulation over decades or centuries <xref ref-type="bibr" rid="bib1.bibx9" id="paren.13"/>. Interest in ARCA has grown recently, particularly as a means of assessing the effects of climate and environmental changes on carbon accumulation. However, its reliability has been questioned <xref ref-type="bibr" rid="bib1.bibx71 bib1.bibx19" id="paren.14"/>, as ARCA does not accurately reflect the net balance of organic carbon in peatlands. An alternative approach involves modeling exercises that combine peat core age data with empirical models of organic matter decomposition. This allows reconstruction of historical carbon fluxes, linking absorbed and released carbon to initial peatland carbon stock <xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx43 bib1.bibx18 bib1.bibx4 bib1.bibx39" id="paren.15"/>. In this study, we propose another complementary approach, leveraging a CSM that use atmospheric forcing data as input. Observationally-based atmospheric forcings, available with hourly resolution for some regions since the 1960s, provide a robust basis for modeling peatland evolution over the past several decades. Against the backdrop of Europe's severe drought in 2022 <xref ref-type="bibr" rid="bib1.bibx17" id="paren.16"/>, recent research on the Bernadouze peatland in the Pyrenees mountains identified a significant carbon release to the atmosphere during this event, supported by six years of field data <xref ref-type="bibr" rid="bib1.bibx22" id="paren.17"/>. This drought presents a compelling case within a 64 year record, raising questions about its severity as an isolated event versus its representation of a broader trend. Additionally, it prompts examination of whether the peatland's functioning during 2022 aligns with long-term behavior.</p>
      <p id="d2e232">To address these questions, this study pursues three key objectives: (1) Implementation and first-site evaluation of a new <italic>Sphagnum</italic> Plant Functional Type (PFT) within the ISBA land surface model; (2) Assessment of the temporal evolution of carbon fluxes from the Bernadouze peatland over the past 64 years; (3) Investigation of the factors influencing carbon accumulation, with a particular focus on drought episodes.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Materials and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Study site</title>
      <p id="d2e253">The Bernadouze peatland, located at an altitude of 1343 m in the eastern French Pyrenees (42.80273° N; 1.42361° E), covers roughly 4.7 ha and is part of a national biological reserve. Designated as a regional biological reserve since 1983 and a Natura 2000 site since 2007, it is one of the four sites of the French National Peatland Observatory Service SNO-Tourbieres. Characteristic of alpine and southwestern European mountainous peatlands, it is classified as a soligenous fen, continuously receiving water from precipitation and surface runoff. It has formed over the past 5000 years within a 1.4 km watershed with steep slopes averaging 50 %. A beech forest surrounds the fen, extending up to 1800 m. The peatland has an average peat depth of 2 m, reaching up to 6 m in some areas. The vegetation comprises species typical of both ombrotrophic areas, such as <italic>Sphagnum palustre</italic> and <italic>Sphagnum capillifolium</italic>, and minerotrophic areas, including <italic>Carex demissa</italic> and <italic>Equisetum fluviatile</italic> <xref ref-type="bibr" rid="bib1.bibx32" id="paren.18"/>. This distribution is illustrated in Fig. 1 of <xref ref-type="bibr" rid="bib1.bibx21" id="text.19"/>, which shows the spatial arrangement of vegetation types across the study site.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Environmental monitoring</title>
      <p id="d2e283">Piezometer wells are 50 mm diameter PVC tubes, distributed across the peatland to cover the full spatial extent of the site (Fig. 1 from  <xref ref-type="bibr" rid="bib1.bibx22" id="altparen.20"/>), and their placement corresponds to the locations where chamber measurements were conducted. Water table depth (WTD) data were recorded at 1 h intervals, and the mean value from the nine piezometers is used throughout the study. As in precedent studies of the same peatland <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx22" id="paren.21"/> we used the S2M reanalysis, which combines the French weather service SAFRAN meteorological reanalysis (8 km resolution) with the SURFEX/ISBA-Crocus snow cover model <xref ref-type="bibr" rid="bib1.bibx60" id="paren.22"/>. The S2M chain was applied in a local mode at the scale of the “Couserans” massif (a mountainous region in the central Pyrenees, southwestern France), assuming homogeneous weather conditions across the massif for equivalent altitudes but accounting for local topographic features in the calculation of shortwave radiation. The S2M model has a vertical resolution of 300 m and provides hourly outputs. The topographical features of the peatland, including altitude, slope, and aspect, were carefully accounted for to ensure that the atmospheric variables extracted for the site accurately represent local conditions.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Carbon fluxes</title>
      <p id="d2e304">Hourly validated time series of <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> fluxes (GPP, ER, and NEE) spanning 2017 to 2022 are available, as detailed by <xref ref-type="bibr" rid="bib1.bibx22" id="text.23"/>. These time series were derived from statistical models based on monthly <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> flux measurements using the static chamber technique. The use of the statistical model allows reconstruction of daily fluxes, enabling direct comparison with the ISBA model outputs at the same temporal resolution. The reconstructed fluxes are considered spatially representative of the peatland due to the coverage and replication of the chamber measurements. In the following sections, these reconstructed datasets are used as a reference for model validation, and readers should note that the validation is performed against the derived statistical model rather than the raw measurements.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Model development</title>
      <p id="d2e342">In the present study, we utilize the ISBA model, which is part of the SURFEX land surface modeling platform (Version 9) and serves as the land surface component of the global Earth System Model CNRM-ESM <xref ref-type="bibr" rid="bib1.bibx14" id="paren.24"/>. ISBA is widely employed to simulate surface processes, but it does not currently represent mosses or <italic>Sphagnum</italic>, which are essential components of ecosystems such as peatlands. To address this limitation, we introduce a new plant functional type (PFT) designed specifically for modeling mosses and <italic>Sphagnum</italic> within the ISBA framework. This work details the implementation of this novel PFT and the associated modifications to the model to better represent the dynamics of peatland ecosystems. The other PFTs, representing vegetation types such as herbaceous plants and trees, have been thoroughly described in the existing literature <xref ref-type="bibr" rid="bib1.bibx24" id="paren.25"/>.</p>
<sec id="Ch1.S2.SS4.SSS1">
  <label>2.4.1</label><title>Photosynthesis of <italic>Sphagnum</italic></title>
      <p id="d2e369">Plant photosynthesis is modeled according to the description by <xref ref-type="bibr" rid="bib1.bibx27" id="text.26"/> and <xref ref-type="bibr" rid="bib1.bibx33" id="text.27"/>, focusing on the equations involving the dependence on mesophyll conductance or <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>) and light dependency (Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>).

              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M6" display="block"><mml:mrow><mml:mtext>Am</mml:mtext><mml:mo>=</mml:mo><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mrow><mml:mo>-</mml:mo><mml:msup><mml:mtext>gm</mml:mtext><mml:mo>*</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

            Am is the assimilation rate under light-saturated conditions (<inline-formula><mml:math id="M7" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>  is the maximum assimilation rate (<inline-formula><mml:math id="M9" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msup><mml:mtext>gm</mml:mtext><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is the mesophyll conductance without water stress (<inline-formula><mml:math id="M11" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M13" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) is the internal mesophyll <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration (see Eq. 4) and <inline-formula><mml:math id="M15" display="inline"><mml:mi mathvariant="normal">Γ</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) is the <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> compensation point, meaning the <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration below which the plant no longer fixes <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.

              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M20" display="block"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mtext>Am</mml:mtext><mml:mo>+</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="italic">ϵ</mml:mi><mml:msub><mml:mi>I</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mtext>Am</mml:mtext><mml:mo>+</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:msup><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula>

            <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the net assimilation rate <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the “dark respiration” <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula> the light use efficiency <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">J</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the photosynthetically active radiation <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.

              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M29" display="block"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mtext>Am</mml:mtext><mml:mn mathvariant="normal">9</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the mitochondrial respiration, empirically fixed.</p>
      <p id="d2e868">In ISBA, <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msup><mml:mtext>gm</mml:mtext><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> depend on the PFT parameters and the leaf surface temperature following a <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> function, modified by <xref ref-type="bibr" rid="bib1.bibx12" id="text.28"/> to account for inhibitions <xref ref-type="bibr" rid="bib1.bibx34" id="paren.29"/>. Then, <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msup><mml:mtext>gm</mml:mtext><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is replaced by gm, which allows accounting for plant water stress conditions (see Table A1). Thus, the effect of stomatal closure on photosynthesis in ISBA is controlled by gm, not  by gs (the stomatal conductance), which is calculated as a function of <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and used solely to determine transpiration fluxes (see Eq. B5, Appendix B).</p>
      <p id="d2e933">To model the photosynthesis of <italic>Sphagnum</italic> mosses, only mesophyll conductance has been considered to contribute to photosynthesis, even though the transfer of <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> within the hyaline cells is still poorly understood <xref ref-type="bibr" rid="bib1.bibx66" id="paren.30"/>. Since <italic>Sphagnum</italic> mosses lack stomata, stomatal conductance is no longer defined for the <italic>Sphagnum</italic> PFT. Therefore, the relationship between <italic>Sphagnum</italic> moss photosynthesis and <italic>Sphagnum</italic> moss water content is accounted for through gm. <xref ref-type="bibr" rid="bib1.bibx53" id="text.31"/> and <xref ref-type="bibr" rid="bib1.bibx63" id="text.32"/> described <italic>Sphagnum</italic> moss photosynthesis using the concept of total <italic>Sphagnum</italic> moss <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> conductance, derived from measurements by <xref ref-type="bibr" rid="bib1.bibx67" id="text.33"/> relating <italic>Sphagnum</italic> moss water content to <italic>Sphagnum</italic> moss <inline-formula><mml:math id="M38" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> conductance. In our case, we relate <italic>Sphagnum</italic> moss mesophyll conductance and total <italic>Sphagnum</italic> moss <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> conductance. Although they are not the same physical quantity. In <xref ref-type="bibr" rid="bib1.bibx33" id="text.34"/> description, gm is the closest approximation to total <inline-formula><mml:math id="M40" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> conductance. Hence, the normalized total <italic>Sphagnum</italic> moss <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> conductance (<inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) was first defined following <xref ref-type="bibr" rid="bib1.bibx25" id="text.35"/> (Eq. <xref ref-type="disp-formula" rid="Ch1.E4"/> and Fig. A1). This variable was then used to parameterize the relationship between gm and <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> proposed by <xref ref-type="bibr" rid="bib1.bibx67" id="text.36"/> (Eq. <xref ref-type="disp-formula" rid="Ch1.E5"/>).

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M44" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E4"><mml:mtd><mml:mtext>4</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mfenced close="" open="{"><mml:mtable class="array" columnalign="center left"><mml:mtr><mml:mtd><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="italic">η</mml:mi><mml:mo>×</mml:mo><mml:msubsup><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn><mml:mo>×</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E5"><mml:mtd><mml:mtext>5</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mtext>gm</mml:mtext><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E6"><mml:mtd><mml:mtext>6</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="italic">η</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:msubsup><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E7"><mml:mtd><mml:mtext>7</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:mi mathvariant="italic">η</mml:mi></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            Where <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the water content of <italic>Sphagnum</italic> mosses (<inline-formula><mml:math id="M46" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the normalized total conductance, <inline-formula><mml:math id="M48" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M50" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> are coefficients given in Table A2, <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> respectively the maximum and minimum water content of <italic>Sphagnum</italic> mosses (<inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M55" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) is the water content of <italic>Sphagnum</italic> that maximizes <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M57" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M58" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) is a parametrized coefficient given in Table A2.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS2">
  <label>2.4.2</label><title>Leaf area index – Canopy scaling</title>
      <p id="d2e1505">The evolution of <italic>Sphagnum</italic> moss biomass results from the balance between carbon assimilation through photosynthesis and <italic>Sphagnum</italic> moss mortality, calculated according to Eq. (<xref ref-type="disp-formula" rid="Ch1.E8"/>):

              <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M59" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>B</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>exp⁡</mml:mi><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>-</mml:mo><mml:mi>t</mml:mi></mml:mrow><mml:mi mathvariant="italic">τ</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M60" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> is the active biomass of <italic>Sphagnum</italic> mosses in <inline-formula><mml:math id="M61" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>B</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>exp⁡</mml:mi><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mo>-</mml:mo><mml:mi>t</mml:mi></mml:mrow><mml:mi mathvariant="italic">τ</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:math></inline-formula> is the mortality of the <italic>Sphagnum</italic> moss biomass, <inline-formula><mml:math id="M63" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> is the characteristic mortality time, <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:math></inline-formula> is a timestep of 1 d, <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the net assimilation of the <italic>Sphagnum</italic> mosses canopy and <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the respiration of <italic>Sphagnum</italic> mosses canopy (<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mtext>LAI</mml:mtext><mml:mo>×</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mtext>LAI</mml:mtext><mml:mo>×</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d2e1719">The LAI is directly calculated from the leaf biomass reservoir <inline-formula><mml:math id="M69" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> according to:

              <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M70" display="block"><mml:mrow><mml:mtext>LAI</mml:mtext><mml:mo>=</mml:mo><mml:mi>B</mml:mi><mml:mo>×</mml:mo><mml:mtext>SLA</mml:mtext></mml:mrow></mml:math></disp-formula>

            where SLA (specific leaf area) is a foliar vegetation index representing the leaf area per unit of assimilated carbon (<inline-formula><mml:math id="M71" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>).

              <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M72" display="block"><mml:mrow><mml:mtext>SLA</mml:mtext><mml:mo>=</mml:mo><mml:mi>e</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:math></disp-formula>

            Here, <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the mass-based nitrogen concentration in the leaf <xref ref-type="bibr" rid="bib1.bibx5" id="paren.37"/>. The SLA is defined for each vegetation type.</p>
      <p id="d2e1812">Once net assimilation is calculated, multiplying by the LAI allows for scaling from the individual <italic>Sphagnum</italic> strand to the <italic>Sphagnum</italic> canopy. The ISBA model follows the assumption of maintaining constant temperature, humidity, and <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration throughout the canopy. Additionally, a radiative transfer model for photosynthetically active radiation was developed by <xref ref-type="bibr" rid="bib1.bibx6" id="text.38"/>, allowing for the representation of light diffusion within a canopy based on its LAI. This module accounts for the decrease in light radiation along the vertical profile of the canopy (with more light at the top of the canopy) as well as the diffusion of light towards the lower parts of the canopy. The attenuation of light within the canopy thus leads to a decreasing vertical profile of photosynthesis within the canopy. Leaf respiration, on the other hand, is assumed to be constant along the vertical profile of the canopy. Canopy respiration corresponds to the respiration calculated at the leaf level multiplied by the LAI.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS3">
  <label>2.4.3</label><title>Biomass pools</title>
      <p id="d2e1844">In the original ISBA model, vegetation is represented by up to six biomass reservoirs: leaves, stem, wood, fine and coarse roots, and a small storage pool corresponding to nonstructural carbohydrates <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx14" id="paren.39"/>. For grass/herbaceous PFTs', wood and coarse roots are excluded. Leaf biomass evolves based on photosynthetic carbon assimilation and is reduced by turnover, respiration, and allocation to other pools. Leaf area index (LAI) is derived from leaf biomass and specific leaf area, which depends on both PFT and nitrogen content. Mortality and turnover are PFT-dependent and climate-sensitive, especially for leaves. Photosynthesis and respiration are computed at sub-daily time steps, while the biomass pools evolve on a daily basis.</p>
      <p id="d2e1850">For <italic>Sphagnum</italic>, the structure was simplified to reflect its particular growth strategy and morphology. Only two biomass reservoirs are considered: <inline-formula><mml:math id="M75" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula>, representing the photosynthetically active green biomass, and <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>B</mml:mi><mml:mi mathvariant="normal">brown</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the dead biomass. The latter is fed by senescence from the green biomass and follows a similar formulation to the original model's decay processes, with an adjusted decay rate specific to <italic>Sphagnum</italic>. This minimalist representation captures the essential dynamics of <italic>Sphagnum</italic> growth and decomposition, consistent with its role in peat accumulation and its lack of differentiated organs like leaves or roots.</p>
      <p id="d2e1880">The brown <italic>Sphagnum</italic> mosses (<inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi>B</mml:mi><mml:mi mathvariant="normal">brown</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) are uniformly distributed over 10 cm of the soil profile, and this vertical distribution is maintained throughout the simulation.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS4">
  <label>2.4.4</label><title>Sphagnum water content</title>
      <p id="d2e1905">To model the evolution of the water content in <italic>Sphagnum</italic> mosses, we followed the work of <xref ref-type="bibr" rid="bib1.bibx55" id="text.40"/>, considering a linear relationship between the soil water content at 10 cm and the water content of <italic>Sphagnum</italic> mosses.

              <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M78" display="block"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>b</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">soil</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>c</mml:mi></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">Sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the water content of <italic>Sphagnum</italic> mosses in <inline-formula><mml:math id="M80" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">soil</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the soil water content at 10 cm in <inline-formula><mml:math id="M82" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. The empirical coefficients <inline-formula><mml:math id="M83" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M84" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula> are given in Table A2.</p>
      <p id="d2e2036">The precipitation interception reservoir is considered negligible. Consequently, <italic>Sphagnum</italic> mosses receive water primarily through capillary action from the soil within 10 cm of the surface. Although direct interception of rainfall also contributes in reality, this process is not explicitly modeled here. Instead, we account only for the effect of capillarity by relating the water content of <italic>Sphagnum</italic> to that of the upper 10 cm of soil. Precipitation that would otherwise be intercepted bypasses the moss canopy and infiltrates directly into the soil, thereby influencing both soil and <italic>Sphagnum</italic> water content.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS5">
  <label>2.4.5</label><title><italic>Sphagnum</italic> evaporation</title>
      <p id="d2e2059">Given that <italic>Sphagnum</italic> mosses do not possess stomata, we consider that the latent heat flux from the vegetation is solely due to the evaporation of water from the their epidermal cells. The plant transpiration phenomenon controlled by stomata is therefore eliminated here. Thus, we have: 

              <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M85" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">sp</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mtext>with </mml:mtext><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>H</mml:mi></mml:msub><mml:msub><mml:mi>V</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

            <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the latent heat flux from the vegetation (see Eq. B5, Appendix B) in <inline-formula><mml:math id="M87" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represent the air and <italic>Sphagnum</italic> canopy resistances, respectively. <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the fraction of vegetation, <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the specific humidity at saturation at temperature <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the surface temperature and <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the specific humidity of the air at reference altitude <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the air density at altitude <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>H</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the drag coefficient, and <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi>V</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the wind speed at <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e2364"><inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> has been modeled following the work of <xref ref-type="bibr" rid="bib1.bibx2" id="text.41"/> and <xref ref-type="bibr" rid="bib1.bibx25" id="text.42"/>, who experimentally established a relationship between the resistance of the <italic>Sphagnum</italic> canopy and the water content of the <italic>Sphagnum</italic> mosses. The <italic>Sphagnum</italic> moss resistance to water decreases towards low values when the water content of the <italic>Sphagnum</italic> mosses is high, leading to strong evaporation. Below a threshold value, as the <italic>Sphagnum</italic> mosses dry out, the resistance of the <italic>Sphagnum</italic> mosses increases linearly, allowing to retain a minimal threshold of water in the <italic>Sphagnum</italic> mosses. As such, we define:

              <disp-formula id="Ch1.E13" content-type="numbered"><label>13</label><mml:math id="M102" display="block"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">sp</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo movablelimits="false">max⁡</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mtext>SWI</mml:mtext><mml:mi mathvariant="normal">sp</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>d</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sp</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">min</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>

            with <inline-formula><mml:math id="M103" display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula> in <inline-formula><mml:math id="M104" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">s</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M105" display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sp</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">min</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> given in Table A2.</p>
      <p id="d2e2496">By choosing this approach, we diverge significantly from <xref ref-type="bibr" rid="bib1.bibx2" id="text.43"/> and <xref ref-type="bibr" rid="bib1.bibx25" id="text.44"/>, who link bulk resistivity to the water content of <italic>Sphagnum</italic> mosses. Here, we disregard the water content of <italic>Sphagnum</italic> mosses and instead directly use the soil water content at 10 cm depth through the <italic>Sphagnum</italic> Soil Wetness Index (<inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mtext>SWI</mml:mtext><mml:mi mathvariant="normal">sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). However, this new formulation remains consistent with previous ones when representing the <italic>Sphagnum</italic> canopy resistance (<inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) as a function of the water content of <italic>Sphagnum</italic> mosses (Fig. A2).</p>
      <p id="d2e2544">Following <xref ref-type="bibr" rid="bib1.bibx13" id="text.45"/> to account for soil water stress by using the Soil Wetness Index we define the <italic>Sphagnum</italic> Soil Wetness Index:

              <disp-formula id="Ch1.E14" content-type="numbered"><label>14</label><mml:math id="M109" display="block"><mml:mrow><mml:msub><mml:mtext mathvariant="normal">SWI</mml:mtext><mml:mi mathvariant="normal">sp</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>j</mml:mi></mml:munder><mml:msub><mml:mtext>sphafrac</mml:mtext><mml:mi>j</mml:mi></mml:msub><mml:mo movablelimits="false">max⁡</mml:mo><mml:mfenced close=")" open="("><mml:mrow><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:mo>,</mml:mo><mml:mo movablelimits="false">min⁡</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">soil</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">wilt</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">fc</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">wilt</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>

            Here, <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mtext>sphafrac</mml:mtext><mml:mi>j</mml:mi></mml:mrow></mml:math></inline-formula> is the proportion of brown <italic>Sphagnum</italic> in layer <inline-formula><mml:math id="M111" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">soil</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the soil water content of layer <inline-formula><mml:math id="M113" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">fc</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the soil water content at field capacity of layer <inline-formula><mml:math id="M115" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi mathvariant="normal">wilt</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the soil water content at wilting point of layer <inline-formula><mml:math id="M117" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, all in <inline-formula><mml:math id="M118" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e2759"><inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mtext>SWI</mml:mtext><mml:mi mathvariant="normal">sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> varies between <inline-formula><mml:math id="M120" display="inline"><mml:mrow><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> when the soil water content of the <italic>Sphagnum</italic> zone is less than or equal to the wilting point, and 1 when water is not a limiting factor. Beyond 10 cm depth where we assume there are no living <italic>Sphagnum</italic> anymore, <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mtext>SWI</mml:mtext><mml:mi mathvariant="normal">sp</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e2807">The resistance of <italic>Sphagnum</italic> mosses to water is inversely proportional to the availability of water in the surface layers of the soil. The more water there is in the surface layers, the lower the resistance, with a minimum value of <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>. The resistance then increases according to the inverse function as the water content of the soil decreases. The water evaporated by the <italic>Sphagnum</italic> mosses is then removed from the top 10 cm of soil, proportional to the layer depth from each layer concerned.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS6">
  <label>2.4.6</label><title>Soil physics</title>
      <p id="d2e2840">The ISBA model resolves soil heat and water exchanges using a 14-layer scheme over 12 m depth, minimizing numerical errors in diffusion equations. Thermal depth remains constant at 12 m, while hydrological depth varies with vegetation. The surface energy balance combines properties of snowpack and soil/vegetation. A 12-layer snow model by <xref ref-type="bibr" rid="bib1.bibx3" id="text.46"/> and improved by <xref ref-type="bibr" rid="bib1.bibx13" id="text.47"/> simulates snow properties like energy absorption, density, and melt processes, considering surface albedo and radiation absorption. Heat transfer in soil follows Fourier's law, accounting for soil water content, porosity, and conductivity. Water mass fluxes are described using the Richards equation, incorporating precipitation, snowmelt, freezing/thawing, and vapor transport. Soil hydraulic properties relate to water content and soil texture, with adjustments for ice presence.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS7">
  <label>2.4.7</label><title>Carbon pools in soil</title>
      <p id="d2e2857">The ISBA model balances plant debris decomposition and microbial activity to represent soil carbon stocks, based on the CENTURY model <xref ref-type="bibr" rid="bib1.bibx46" id="paren.48"/>. Plant debris, including leaves, stems, and roots, is divided into structural and metabolic litter reservoirs, above and belowground. These decompose into three types of soil carbon reservoirs: fast (less than a year), slow (about a decade), and passive (hundreds to thousands of years). This decomposition process drives soil heterotrophic respiration, releasing <inline-formula><mml:math id="M123" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx24" id="paren.49"/>.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS8">
  <label>2.4.8</label><title>Thermal and hydraulic properties of peat soils</title>
      <p id="d2e2885">ISBA calculates thermal and hydraulic properties of soil by combining mineral soil attributes with those of soil organic carbon (SOC), adjusted for the organic matter proportion in each layer. We keep the same method for peat soils. Peat organic matter density is defined using porosity and the density of pure organic matter (1300 <inline-formula><mml:math id="M124" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). In our simulations, the SOC fraction in each layer is fixed at 1, reflecting the assumption of a completely organic soil. Peat porosity ranges from 0.930 in surface fibric soil to 0.845 in deeper sapric soil, significantly affecting both the thermal conductivity and water retention capabilities of the soil. These variations influence organic matter density and overall soil properties, particularly in peat soils, ensuring accurate modeling of soil thermal and hydraulic dynamics <xref ref-type="bibr" rid="bib1.bibx13" id="paren.50"/>.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS9">
  <label>2.4.9</label><title>Biogeochemical processes in peat</title>
      <p id="d2e2917">The research conducted by <xref ref-type="bibr" rid="bib1.bibx42" id="text.51"/> has led to the development of a biogeochemical module capturing various physical and chemical processes occurring within peatlands. This module discretizes the soil into 14 layers, with soil physics resolved for each. It calculates the concentrations of <inline-formula><mml:math id="M125" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M126" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M127" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in each layer, enabling representation of biogeochemical processes across the entire vertical profile. Hence, processes such as methanogenesis in anaerobic conditions, methanotrophy (methane oxidation to <inline-formula><mml:math id="M128" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the presence of <inline-formula><mml:math id="M129" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), and heterotrophic respiration (production of <inline-formula><mml:math id="M130" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), are described within ISBA. Soil water level and thus <inline-formula><mml:math id="M131" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in peat regulate these chemical processes. Various equations account for the three different gas transport mechanisms in peat, including transport by plants, ebullition, and diffusion.</p>
      <p id="d2e3001">The carbon accumulation in the soil and its transfer between layers are represented by an advection term considered constant at 2 <inline-formula><mml:math id="M132" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx29" id="paren.52"/>. The phenomenon of cryoturbation, i.e., the mixing of surface peat layers due to freezing and thawing, is modeled using a diffusion equation following <xref ref-type="bibr" rid="bib1.bibx36" id="text.53"/>.</p>
</sec>
<sec id="Ch1.S2.SS4.SSS10">
  <label>2.4.10</label><title>Ecosystem respiration</title>
      <p id="d2e3035">Ecosystem respiration is defined here as the combination of heterotrophic respiration across the peat profile and autotrophic respiration from surface vegetation.</p>
      <p id="d2e3038">Heterotrophic respiration is calculated for each of the 14 soil layers, based on the <inline-formula><mml:math id="M133" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in each layer. Two sources of <inline-formula><mml:math id="M134" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are modeled for each layer: the production of <inline-formula><mml:math id="M135" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from organic matter decomposition (<inline-formula><mml:math id="M136" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">oxic</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) and the production of <inline-formula><mml:math id="M137" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> resulting from methane oxidation (<inline-formula><mml:math id="M138" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">methane</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>), indirectly linked to methane concentration in each layer and thus to methanogenesis.

              <disp-formula id="Ch1.E15" content-type="numbered"><label>15</label><mml:math id="M139" display="block"><mml:mrow><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msup><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">oxic</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi>i</mml:mi></mml:msup><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mtext>Tg</mml:mtext><mml:mo>)</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>×</mml:mo><mml:mo movablelimits="false">min⁡</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msub><mml:mo>∑</mml:mo><mml:mi>j</mml:mi></mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mtext>Tg</mml:mtext><mml:mo>)</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:math></disp-formula>

            Here, <inline-formula><mml:math id="M140" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M141" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> represent the types of carbon reservoirs (metabolic and structural litter, active C, slow C, passive C). <inline-formula><mml:math id="M142" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">oxic</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> production is determined by the organic matter decomposition rate (<inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mtext>Tg</mml:mtext><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, which initially depends on soil temperature and moisture content <xref ref-type="bibr" rid="bib1.bibx42" id="paren.54"/>. The function <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, varying between 0.05 (dry soil) and 1 (above field capacity), accounts for soil moisture impact on microbial activity. In this study, soil moisture did not appear to strongly constrain organic matter decomposition in near surface moss dominated layers as indicated by the closer agreement between ISBA and observed (statisticaly modelled) soil respiration when <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> was excluded (Fig. A4b and e). We nevertheless aimed to preserve contrasting drought responses across vegetation types. Therefore, <inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> was removed for <italic>Sphagnum</italic>, while it was retained for herbaceous to maintain drought sensitivity where moisture deficits are expected to constrain belowground carbon turnover. The decomposition rate (<inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mtext>Tg</mml:mtext><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) follows an Arrhenius-like equation (<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), accounting for increased decomposition with temperature rise. The last part of the equation considers oxygen availability with <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> representing the maximum carbon mass producible from available oxygen.</p>
      <p id="d2e3421">Methane oxidation <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>→</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> contributes to <inline-formula><mml:math id="M151" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> production, especially in deeper layers. For litter above ground, <inline-formula><mml:math id="M152" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is directly released to the atmosphere. In deeper layers, diffusion, plant-mediated transport (PMT), and evapotranspiration facilitate <inline-formula><mml:math id="M153" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> escape. Gas diffusion in soil layers leads to vertical gas movements based on concentration gradients. PMT depends on leaf area index (LAI), while evapotranspiration is influenced by PFT.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Water table depth diagnosis and dryness index development</title>
      <p id="d2e3509">First, based on the ISBA outputs, we derived Eq. (<xref ref-type="disp-formula" rid="Ch1.E16"/>), which relates, for each soil layer, the change in volumetric water content to the change in water equivalent height, assuming the layer is saturated.

            <disp-formula id="Ch1.E16" content-type="numbered"><label>16</label><mml:math id="M154" display="block"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">sat</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>h</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">soil</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

          with <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">sat</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> the volumetric water content of soil layer <inline-formula><mml:math id="M156" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> at saturation, <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the height of water in the layer <inline-formula><mml:math id="M158" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the vertical width of the layer <inline-formula><mml:math id="M160" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">soil</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> the volumetric water content of soil layer <inline-formula><mml:math id="M162" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>.</p>
      <p id="d2e3673">Then, we derived the ISBA-diagnosed WTD by summing over the soil layers down to 2 m depth, i.e. those where variations in water content are significant. This calculation assumes that the variation of <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with depth <inline-formula><mml:math id="M164" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> is negligible, allowing it to be factored out of the summation (see Fig. A3a):

            <disp-formula id="Ch1.E17" content-type="numbered"><label>17</label><mml:math id="M165" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">WTD</mml:mi><mml:mi mathvariant="normal">ISBA</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>j</mml:mi></mml:munder><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>h</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>j</mml:mi></mml:munder><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">soil</mml:mi></mml:mrow></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">sat</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>h</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>w</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">soil</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> represent the changes in water equivalent height and soil volumetric water content, respectively, calculated explicitly through the temporal discretization of Eq. (<xref ref-type="disp-formula" rid="Ch1.E16"/>).</p>
      <p id="d2e3793">The dryness index is based on the work of <xref ref-type="bibr" rid="bib1.bibx22" id="text.55"/> (see Fig. A3b). We first define the daily soil water deficit <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:mtext>dif</mml:mtext><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>:

            <disp-formula id="Ch1.E18" content-type="numbered"><label>18</label><mml:math id="M169" display="block"><mml:mrow><mml:mtext>dif</mml:mtext><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi>a</mml:mi><mml:mi>i</mml:mi><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">normalized</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mtext>WTD</mml:mtext><mml:mi mathvariant="normal">normalized</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

          We use the daily mean of <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mtext>WTD</mml:mtext><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> to calculate <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mtext>dif</mml:mtext><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. Normalization of each variable (<inline-formula><mml:math id="M173" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>) was done following <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">normalized</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">−</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mi mathvariant="normal">−</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></inline-formula>. A minimum WTD value of 1m was imposed to elevate the normalized WTD values, since the diagnosed WTD tends to produce water tables that do not drop sufficiently during droughts. This adjustment allows the normalized WTD to better discriminate drought periods, which would otherwise be overly smoothed by the index (see Fig. A3b).</p>
      <p id="d2e3953">To consider only periods of positive water deficit, we define the function <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> as:

            <disp-formula id="Ch1.E19" content-type="numbered"><label>19</label><mml:math id="M176" display="block"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable columnspacing="1em" rowspacing="0.2ex" class="cases" columnalign="left left" framespacing="0em"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">dif</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if </mml:mtext><mml:mi mathvariant="normal">dif</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mtext>otherwise</mml:mtext></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></disp-formula>

          The Dryness Index (DI) is then calculated by integrating <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> over the summer period:

            <disp-formula id="Ch1.E20" content-type="numbered"><label>20</label><mml:math id="M178" display="block"><mml:mrow><mml:mtext>DI</mml:mtext><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mi mathvariant="normal">july</mml:mi><mml:mi mathvariant="normal">august</mml:mi></mml:munderover><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:math></disp-formula>

          This formulation ensures that only days with a positive soil water deficit contribute to the DI, providing a simple and physically meaningful measure of summer dryness.</p>
</sec>
<sec id="Ch1.S2.SS6">
  <label>2.6</label><title>Statistical analyses</title>
      <p id="d2e4079">To compute Pearson correlation coefficients (<inline-formula><mml:math id="M179" 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>), root mean square errors (RMSE) trends and associated <inline-formula><mml:math id="M180" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values, we used the statsmodels Python library. In particular, the Ordinary Least Squares (OLS) (<uri>https://www.statsmodels.org/dev/generated/statsmodels.regression.linear_model.OLS.html</uri>, last access: 11 May 2026) regression function was employed to fit a linear model and perform an <inline-formula><mml:math id="M181" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>-test to assess the statistical significance of the relationship.</p>
      <p id="d2e4110">To assess the relative contribution of each season to interannual variability in net ecosystem exchange (NEE) (Fig. 6), we applied SHAP (SHapley Additive exPlanations), a game-theoretic approach widely used for interpreting machine learning models. Specifically, we trained an Ordinary least squares Linear Regression model from sklearn python library (<uri>https://scikit-learn.org/stable/modules/generated/sklearn.linear_model.LinearRegression.html</uri>, last access: 11 May 2026) to predict annual NEE from seasonal values (summer, autumn, spring, and winter). We then used SHAP values to estimate how much each seasonal predictor contributed to the model output. Rather than relying on model coefficients or explained variance, we computed the mean absolute SHAP values across all observations to quantify each season's average influence. These contributions were normalized to express their relative importance as percentages. This approach provides a robust and interpretable measure of feature relevance, even for collinear predictors. The SHAP methodology is described in detail at: <uri>https://shap.readthedocs.io/en/latest/index.html</uri> (last access: 11 May 2026).</p>
      <p id="d2e4119">A simple linear model using <inline-formula><mml:math id="M182" 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> or an <inline-formula><mml:math id="M183" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>-test tends to attribute explanatory power to the first variables entered into the model. When predictors are correlated as is the case here with seasonal NEE components (e.g., summer NEE , autumn NEE) this can lead to shared variance being unfairly credited to one variable over another. In contrast, SHAP values, based on Shapley values from cooperative game theory, average the contribution of each variable across all possible combinations of input features. This results in a fair and consistent allocation of importance, even when variables are highly interdependent or collinear.</p>
</sec>
<sec id="Ch1.S2.SS7">
  <label>2.7</label><title>Experimental protocol</title>
      <p id="d2e4148">At the Bernadouze site, we obtained a 64-year meteorological data series (1959–2022) from the S2M reanalysis, which was used as input for the ISBA land surface model. To establish a contemporary carbon balance for the various carbon compartments, we simulated a 7000-year spin-up to account for the peatland's age, repeating the 64 year atmospheric forcing. This approach ensured a realistic accumulation of carbon in the soil reservoirs. The model was run in a one-dimensional configuration, at a single grid point corresponding to the location of the Bernadouze peatland.</p>
      <p id="d2e4151">For model validation (Sect. 3), we constrast simulations with 100 % <italic>Sphagnum</italic> cover and 100 % herbaceous cover. Herbaceous cover was simulated with the use of the ISBA PFT boreal grassland (BOGD). For the remainder of the study (Sect. 4), the vegetation distribution is assumed to consist of 70 % herbaceous plants and 30 % <italic>Sphagnum</italic> mosses, based on the cartography provided by <xref ref-type="bibr" rid="bib1.bibx32" id="text.56"/>. Accordingly, the GPP, ER, and NEE values presented correspond to this vegetation mix. A subsection is dedicated to analyzing the sensitivity of carbon fluxes to vegetation composition.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e4165">Daily <bold>(a)</bold> gross primary productivity and <bold>(b)</bold> ecosystem respiration fluxes compared between statistical models (grey) <xref ref-type="bibr" rid="bib1.bibx22" id="paren.57"/> and ISBA over the 2017–2022 period for herbaceous (blue) and <italic>Sphagnum</italic> mosses (orange).</p></caption>
          <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f01.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Model validation over the 2017–2023 period</title>
<sec id="Ch1.S3.SSx1" specific-use="unnumbered">
  <title>Carbon fluxes</title>
      <p id="d2e4200">Figure 1 compares three time series from 2017 to 2023, illustrating Gross Primary Productivity (GPP), Ecosystem Respiration (ER) and Net Ecosystem Exchange (NEE) modeled by a statistical model (grey) and the ISBA model for <italic>Sphagnum</italic> (orange) and Herbaceous (blue). The top plot (a) shows GPP with <inline-formula><mml:math id="M184" 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 of 0.6 and 0.62 (RMSE of 1.9 and 1.6 <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, see Fig. A4a, b), indicating moderate agreement between the models. The middle plot (b) shows ER with  <inline-formula><mml:math id="M186" 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 of 0.82 and 0.44 (RMSE of 0.9 and 1.6 <inline-formula><mml:math id="M187" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, Fig. A4d, e), revealing stronger agreement for ER, particularly for <italic>Sphagnum</italic> respiration. The bottom plot, Fig. A4c, f, shows NEE with <inline-formula><mml:math id="M188" 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 of 0.1 and 0.2 (RMSE of 1.6 and 1.3 <inline-formula><mml:math id="M189" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">mol</mml:mi><mml:msup><mml:mo>.</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). Additional scatter plots for the mixed vegetation configuration (Fig. A4g–i) highlight contrasted performances across fluxes. For GPP, the mixed simulation shows a level of agreement comparable to that of herbaceous vegetation alone (<inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.62</mml:mn></mml:mrow></mml:math></inline-formula>, RMSE <inline-formula><mml:math id="M191" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.58 <inline-formula><mml:math id="M192" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). For ER, the mixed configuration exhibits an intermediate performance, but with a substantial improvement compared to herbaceous vegetation alone (<inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.60</mml:mn></mml:mrow></mml:math></inline-formula>, RMSE <inline-formula><mml:math id="M194" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.32 <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). For NEE, the mixed simulation yields higher skill scores (<inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.24</mml:mn></mml:mrow></mml:math></inline-formula>, RMSE <inline-formula><mml:math id="M197" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.17 <inline-formula><mml:math id="M198" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) than either vegetation type considered separately, although overall correlations remain low.</p>
      <p id="d2e4462">The ISBA model captures the interannual variability of GPP, ER and NEE effectively (Fig. A5), Consistently showing slightly higher values at the beginning of the growing season, much higher values at the end of the growing season, and stronger winter ecosystem respiration (ER) compared to the statistical model. Herbaceous vegetation is more sensitive to summer droughts than <italic>Sphagnum</italic>, leading to reduced GPP and ER in summer, especially during the 2022 drought, which caused a sharp decline in herbaceous GPP and ER.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e4470">Hourly in situ mean water table depth is shown in grey, with its standard deviation in shaded areas, compared to the hourly diagnosed water table depth of ISBA over the 2017–2022 period for two different types of vegetation herbaceous (blue) and Sphagnum mosses (orange).</p></caption>
          <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f02.png"/>

        </fig>

<sec id="Ch1.S3.SSx1.SSS1">
  <label>3.0.1</label><title>Water table depth</title>
      <p id="d2e4486">Figure 2 compares the mean water table depth (WTD) from in situ measurements (grey with shaded standard deviation) to the ISBA diagnosted WTD (orange for <italic>Sphagnum</italic> mosses and blue for herbaceous) over the period 2017–2022. The ISBA model generally follows the observed data, capturing the overall trends and seasonal variations (Fig. A5) in WTD although there are occasional deviations, particularly at the end of the growing season and during drought events where the observed data shows higher variability. Overall, the ISBA model demonstrates rather satisfactory performance in simulating WTD (<inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.47</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mtext>RMSE</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.09</mml:mn></mml:mrow></mml:math></inline-formula> m for herbaceous, <inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.33</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mtext>RMSE</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> m for <italic>Sphagnum</italic> and <inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:mtext>RMSE</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.09</mml:mn></mml:mrow></mml:math></inline-formula> m for the mixed vegetation, Fig. A6). The simulated WTD with herbaceous plants is consistently lower than with <italic>Sphagnum</italic> mosses.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e4582"><bold>(a)</bold> Mean and maximum annual air temperature (°C) and <bold>(b)</bold> annual cumulate precipitation mm yr<sup>−1</sup> both from the S2M reanalysis and <bold>(c)</bold> mean water table depth (m) diagnosed from ISBA outputs, along with their trends as red dashed lines and corresponding <inline-formula><mml:math id="M206" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values.</p></caption>
            <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f03.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results: Water and carbon balance of the peatland over the last 60 years</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Environmental variables</title>
      <p id="d2e4635">Figure 3 consists of three panels, labeled (a), (b), and (c), illustrating the evolution of mean and maximum annual temperature, annual cumulative precipitation, and annual mean water table depth (diagnosed from ISBA) from 1959 to 2022, along with their respective trends and <inline-formula><mml:math id="M207" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values. Annual mean temperature (a) shows a significant (<inline-formula><mml:math id="M208" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) increasing trend over the years. The annual mean temperature increases from approximately 7 °C in the early years to about 9 °C by 2022. Annual maximum temperature shows a similar evolution with an increase up to 8 °C from 1959 to 2022.</p>
      <p id="d2e4662">Annual cumulative precipitation (b) ranges from approximately 1000 to 2250 mm, while the Water Table Depth (WTD) (c) varies between <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.29</mml:mn></mml:mrow></mml:math></inline-formula> m over the whole period. A steady increase in the level of the water table is observed from 1967 to 1983, followed by a sharp decline, reaching its minimum in 1989. After this, the WTD rises again and stabilizes, although notable interannual fluctuations persist until the end of the period. Interestingly, the fluctuations in annual precipitation closely mirror those of the mean annual WTD, suggesting a strong correlation between these two variables. The trends of annual cumulative precipitation and annual mean WTD move in opposite directions, with precipitation increasing and the level of the water table decreasing. However, both trends are not significant (<inline-formula><mml:math id="M212" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>).</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Net ecosystem exchanges</title>
      <p id="d2e4710">This section analyzes long term NEE dynamics and their drivers using ISBA simulations forced by the S2M reanalysis. Unless stated otherwise, all simulations and analyses presented in this section use the site vegetation distribution derived from <xref ref-type="bibr" rid="bib1.bibx32" id="text.58"/>, i.e., 70 % herbaceous plants and 30 % <italic>Sphagnum</italic> mosses.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e4721"><bold>(a)</bold> Annual net ecosystem exchange (<inline-formula><mml:math id="M214" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">C</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">yr</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) from 1959 to 2022, as simulated by ISBA. <bold>(b)</bold> Hourly cumulated net ecosystem exchange (<inline-formula><mml:math id="M215" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">C</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) from 1959 to 2022, also from ISBA. The pannel additionally reports the linear trend (slope), its <inline-formula><mml:math id="M216" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value, and the standard deviation of annual NEE for three distinct periods: 1959–1980, 1980–2001, and 2001–2022.</p></caption>
          <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f04.png"/>

        </fig>

<sec id="Ch1.S4.SS2.SSS1">
  <label>4.2.1</label><title>An overall carbon sink despite strong inter-annual variability</title>
      <p id="d2e4796">Figure 4 illustrates (a) the annual Net Ecosystem Exchange (NEE) and (b) the cumulative NEE from 1959 to 2022. The lowest annual NEE is modelled in 2011 (<inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:mi mathvariant="normal">−</mml:mi><mml:mn mathvariant="normal">171</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M218" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">C</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), while the highest value occurs in 2022 (122 <inline-formula><mml:math id="M219" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">C</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>). Panel (b) shows a long-term decrease in cumulative NEE, indicating that the ecosystem acts as a net carbon sink over the entire study period. Piecewise linear trends computed for three successive 22 year periods (1959–1980, 1980–2001, and 2001–2022) reveal a progressive intensification of carbon uptake, as evidenced by increasingly negative slopes of cumulative NEE. The comparison of slopes between periods indicates that this intensification is not linear through time. The strongest increase in carbon sequestration occurs between the first and second periods, while the rate of intensification decreases after the early 2000s, suggesting a slowdown in the acceleration of the carbon sink despite continued strengthening.</p>
      <p id="d2e4867">Interannual variability, quantified by the standard deviation of annual NEE and reported as text annotations for each period, shows a marked temporal evolution. Variability is highest during the early period (1959–1980), decreases substantially during the phase of strongest sink intensification (1980–2001), and slightly increases again during the most recent period (2001–2022). This pattern suggests that the period of rapid carbon sink strengthening coincides with a more stable interannual behaviour, whereas recent decades combine sustained carbon uptake with a renewed increase in year-to-year variability.</p>
      <p id="d2e4870">Overall, despite substantial annual fluctuations, the long term signal remains robust and highlights a persistent accumulation of carbon by vegetation over the past six decades.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS2">
  <label>4.2.2</label><title>Seasonality of GPP, ER and NEE over the 1959–2022 period</title>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e4884">Seasonal evolution of cumulated <bold>(a)</bold> gross primary productivity (shown with negative sign by convention), <bold>(b)</bold> ecosystem respiration, <bold>(c)</bold> net ecosystem exchanges from ISBA over several time periods: 1959–1980 in blue, 1980–2001 in orange, 2001–2022 in green with interannual variability represented as a 90 % confidence interval. Superimposed, the 2022 NEE seasonality simulated by ISBA (red curve) and the statistical model (purple curve).</p></caption>
            <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f05.png"/>

          </fig>

      <p id="d2e4902">Figure 5 depicts the seasonal mean and interannual variability in gross primary production (a), ecosystem respiration (b), and net ecosystem exchange (c) over several time periods, specifically 1959–1980 (blue), 1980–2001 (orange), and 2001–2022 (green), with a focus on the year 2022 both from ISBA (red line) and the statistical model (purple line). Periods of approximately 22 years were chosen to ensure statistically robust trend estimates, following common climatological practice for analysing multi-decadal variability. Given the 64 year length of the record, three successive periods were defined with a slight overlap, allowing each period to be long enough for robust linear trends while maintaining three comparable intervals <xref ref-type="bibr" rid="bib1.bibx68" id="paren.59"/>. Each subplot shows cumulative values with their respective mean and interannual variability at 90 % confidence interval. In panel (a), GPP values are negative, indicating carbon uptake by vegetation, with more pronounced uptake during the growing season (April to September). Panel (b) shows ER values, which are positive, representing carbon release. Respiration increases during warmer months, with higher rates, suggesting intensified ecosystem respiration. Panel (c) combines GPP and ER to show NEE. The GPP intensifies over time and becomes increasingly pronounced  across the three periods. The same trend is observed for respiration. As a combination of these two variables, NEE exhibits greater seasonal variability, which is not necessarily easy to grasp from this graph but is more apparent in Fig. 6. The mean NEE values for the periods 1980–2001 and 2001–2022 show a similar trend, except during winter, when the NEE of the 2001–2022 period shifts towards positive values. Nonetheless, over the annual cycle, both of these periods display more negative NEE values compared to the 1959–1980 period.</p>
      <p id="d2e4908">The seasonality of GPP (a) and ER (b) has gradually intensified over time, as observed in the three periods. For NEE (c), the trend is less straightforward, but its seasonality has become increasingly pronounced. Additionally, the duration of the growing season has extended, as reflected by the earlier spring and later summer inflection points of cumulative NEE (solid blue, orange and green curves (panel c)).</p>
      <p id="d2e4912">Focusing on 2022, the NEE curve (red) deviates entirely from the interannual variability of the three periods combined, starting in July and continuing through November. Comparing this with the statistical model for 2022 (purple curve), we observe that despite differences in seasonality between ISBA and the statistical model, both agree in highlighting 2022 as a year significantly outside the confidence intervals. While GPP and ER for 2022 remain within the 2001–2022 interannual variability, the GPP is notably close to the lower limit (<inline-formula><mml:math id="M220" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula> GPP to the upper limit), underscoring the exceptional nature of this year in terms of carbon flux dynamics.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e4924"><bold>(a)</bold> Seasonal contributions to annual NEE across four time periods: 1959–1980 in blue, 1980–2001 in orange, 2001–2022 in green, 1959–2022 in grey. Each bar represents the relative importance of a season in explaining the total NEE, as determined by Shapley regression coefficients. Seasons are defined as winter (December–February), spring (March–June), summer (July–August), and autumn (September–November). <bold>(b)</bold> Distribution of SHAP values by season for 1959–2022. Positive or negative SHAP values indicate the direction of each season's contribution to annual NEE, showing whether a season increases or decreases the yearly flux.</p></caption>
            <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f06.png"/>

          </fig>

      <p id="d2e4938">Figure 6a shows that across all time periods, summer is the season contributing the most to annual NEE variability, accounting for approximately 39 % of the total contribution over the 1959–2022 period. Autumn and spring follow, alternating in second place depending on the period, with comparable contributions of around 23 %–25 %. Winter consistently exhibits the lowest contribution, around 11 % of the annual NEE variability. The distribution of signed SHAP values for the full period (Fig. 6b) further highlights the seasonal dynamics. Summer displays a wide variability, with the median and central 50 % of values slightly below zero, but with long positive tails reflecting years with strong <inline-formula><mml:math id="M221" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> release to the atmosphere. Autumn is generally shifted toward positive values, with extreme positive contributions in some years. Spring is centered slightly below zero, with extremes toward negative values. Winter shows relatively low variability, with a skewed distribution including many negative contributions but a long positive tail, indicating occasional meaningful contributions despite its overall smaller role. Overall, these results confirm that summer dominates the interannual variability of annual NEE, but also reveal that other seasons particularly autumn and spring can contribute substantially in certain years. This supports the focus on summer NEE drivers while recognizing the importance of seasonal context.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e4954"><bold>(a)</bold> Summer net ecosystem exchanges (in red) compared to annual (in blue) from 1959 to 2022, as simulated by ISBA. <bold>(b)</bold> Dryness index, derived from water table depth combining ISBA outputs and S2M reanalysis data, from 1959 to 2022 with its trend as red dashed line and associated <inline-formula><mml:math id="M222" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value.</p></caption>
            <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f07.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Joint Influence of Air Temperature and Water Table Depth on Summer NEE Variability</title>
      <p id="d2e4984">Panel (a) of Fig. 7 shows the evolution of cumulative summer NEE (red) compared to cumulative annual NEE (blue) from 1959 to 2022. The cumulative summer NEE tends to “drive” the cumulative annual NEE almost always sharing the same sign, except in years near equilibrium (cumulative annual NEE <inline-formula><mml:math id="M223" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0). This relationship is supported by a strong correlation between summer and annual cumulative NEE (<inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.71</mml:mn></mml:mrow></mml:math></inline-formula>, Fig. A7) and by the fact that summer NEE contributes approximately 40 % of the interannual variability of cumulative NEE (Fig. 6).</p>
      <p id="d2e5009">Panel (b) illustrates the evolution of the dryness index from 1959 to 2022. The trend shows an increasing pattern, with <inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.054</mml:mn></mml:mrow></mml:math></inline-formula>, which is slightly above the conventional significance threshold of 0.05. As the dryness index increases, the cumulative summer NEE also increases, showing a good correlation (<inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>, Fig. A8). The dryness index exceeded 6 in only one year from 1959 to 1980, in five years from 1980 to 2001, and in six years from 2001 to 2022. This suggests an increase in the frequency of high dryness index episodes, indicating a rising frequency of summer droughts. Four years also stand out with particularly high dryness index values: 1989, 1994, 2003, and 2022, all of which occurred after the 1980s.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e5041">Probability density function of annual cumulated net ecosystem exchange over 1959–2022. In black, the vegetation mix corresponds to 70 % herbaceous and 30 % <italic>Sphagnum</italic>. In orange a 100 % <italic>Sphagnum</italic> mix and in blue a 100 % herbaceous mix. In shaded areas, the 95 % confidence intervals corresponding to the variation of the vegetation mix in the form <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mtext>NEE</mml:mtext><mml:mi mathvariant="normal">Sphagnum</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mtext>NEE</mml:mtext><mml:mi mathvariant="normal">herbaceous</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M229" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> varying from 0 to 1 in steps of 0.01.</p></caption>
          <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f08.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS4">
  <label>4.4</label><title>Vegetation sensitivity</title>
      <p id="d2e5113">Figure 8 highlights the changes in the distribution of the annual cumulated Net Ecosystem Exchange (NEE) over 1959–2022. The black curve represents the probability density of NEE for a vegetation mix of 70 % herbaceous and 30 % <italic>Sphagnum</italic>, with shaded regions representing the 95 % confidence intervals accounting for variations in vegetation composition.</p>
      <p id="d2e5119">We observe that while the overall shape of the annual cumulative NEE probability density remains largely unchanged, significant differences arise depending on the vegetation type, particularly around the peak of the distributions. <italic>Sphagnum</italic> mosses amplify NEE extremes, either enhancing <inline-formula><mml:math id="M230" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> absorption by vegetation or increasing <inline-formula><mml:math id="M231" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> release to the atmosphere, resulting in a flatter distribution compared to herbaceous vegetation. In contrast, herbaceous plants have a buffering effect, with a distribution more concentrated around the main peak and a secondary, smaller peak slightly below <inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M233" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">C</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, resulting in a bimodal pattern. These findings highlight the importance of considering different vegetation types, as they respond differently to changing environmental conditions. For completeness, the corresponding figures for GPP and ER are provided in the Appendix (Fig. A10).</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussions</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Model validation and vegetation sensitivity</title>
      <p id="d2e5203">The primary objective of this study was to evaluate the newly implemented <italic>Sphagnum</italic> PFT in the ISBA land surface model. <italic>Sphagnum</italic> photosynthetic activity is linked to water content in the top 10 cm of soil. While the model reproduces site scale carbon fluxes reasonably well given observational constraints, a more detailed validation of the water cycle would require eddy covariance data and multi site evaluations to assess parameter transferability. The aim was not to optimize parameters, but to test whether realistic behavior could be reproduced at a well instrumented site using literature derived values.</p>
      <p id="d2e5212">The mixed representation, combining <italic>Sphagnum</italic> and herbaceous PFTs, accounts for contrasting responses to soil moisture. We removed the influence of soil moisture on respiration (<inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) for <italic>Sphagnum</italic>, allowing the moss layer to maintain microbial activity under dry conditions, while it was retained for herbaceous layers to preserve the soil moisture sensitivity of heterotrophic respiration. Although respiration from the herbaceous component alone is not improved, retaining <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is consistent with previous validations of the ISBA model for herbaceous vegetation, ensuring the parameterization remains grounded in established formulations <xref ref-type="bibr" rid="bib1.bibx24" id="paren.60"/>. Importantly, the combination of PFTs captures contrasting responses to soil moisture, introducing functional diversity that likely increases the robustness of ecosystem carbon fluxes. This mechanism is reflected in the observed modest improvement of NEE on the mixed vegetation dataset, even if GPP and respiration alone do not always show large gains. These results also highlight the broader uncertainty in representing heterotrophic respiration as a function of soil moisture: classical formulations derived from mineral soils may not adequately capture responses in organic soils, as noted in other peatland modeling studies <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx30" id="paren.61"/>, emphasizing the need for further research on moisture/respiration parameterizations.</p>
      <p id="d2e5257">By combining PFTs with contrasting functional responses, the model captures compensatory dynamics across vegetation types: herbaceous layers respond strongly to moisture deficits, while <italic>Sphagnum</italic> maintains near surface moisture and microbial activity. This functional diversity improves site scale carbon flux estimates and suggests increased model robustness under variable hydrological conditions, which could be further enhanced by including interactive dynamics between <italic>Sphagnum</italic> mosses and herbaceous following the work of <xref ref-type="bibr" rid="bib1.bibx35" id="text.62"/> but also competition and coupled carbon/water processes (Lippmann et al., 2023; Heijmans et al., 2008; Wu and Blodau, 2013a; Gong et al., 2020).</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>The key predictors of annual net ecosystem exchange (NEE)</title>
      <p id="d2e5277">The methodology developed in this study aimed to investigate the variability and evolution of carbon fluxes in the Bernadouze peatland from 1959 to 2022 using a CSM validated for the present period (2017–2022). This approach provides insight into the long-term functioning of the peatland on a century-scale timescale, which has been scarcely explored in the literature due to the lack of suitable tools. This novel methodology provides access to an unprecedented temporal scale, enabling current observations to be interpreted within a broader historical perspective.</p>
      <p id="d2e5280">Over the past 64 years, the Bernadouze peatland has shown marked variability in net ecosystem exchange (NEE), while overall maintaining its role as a carbon sink. This variability is strongly influenced by climatic and hydrological conditions, particularly precipitation, water table dynamics, and air temperature, as highlighted in previous research <xref ref-type="bibr" rid="bib1.bibx73 bib1.bibx37" id="paren.63"/>. The reconstruction of water table height, together with the development of a dryness index that integrates both air temperature and water table depth, offers a robust explanation for the observed fluctuations in carbon fluxes, as also supported by other studies <xref ref-type="bibr" rid="bib1.bibx31" id="paren.64"/>. Vapor Pressure Deficit (VPD) is generally an important factor to consider, particularly for vegetation development, as it influences both GPP and plant transpiration <xref ref-type="bibr" rid="bib1.bibx20" id="paren.65"/>. However, at the Bernadouze site, VPD is low and exhibits little variation (Figure A9 (a)), suggesting it has a limited effect on NEE. Furthermore, VPD is strongly correlated with temperature, which captures much of its potential influence. A recent study in Northern Hemisphere peatlands <xref ref-type="bibr" rid="bib1.bibx10" id="paren.66"/> also indicates that VPD has a neutral effect on vegetation and does not necessarily induce stomatal closure in vascular plants. The humid conditions at the site, along with the presence of bryophytes, help satisfy atmospheric water demand. Overall, air temperature and water table depth remain the primary drivers explaining NEE variability.</p>
      <p id="d2e5295">It is also observed that, in Bernadouze, summer NEE is the dominant contributor to the annual carbon balance, though the relative influence of other seasons varies across time periods. In recent decades, transitional seasons such as spring and autumn have become increasingly significant compared to earlier years. Understanding how climate change influences NEE seasonality offers key insight into the complex dynamics of carbon fluxes and the shifting balance between source and sink processes throughout the year, as also emphasized by <xref ref-type="bibr" rid="bib1.bibx31" id="text.67"/>. The dryness index developed in this study also appears to be a good proxy for summer NEE and, consequently, for annual NEE (Figs. A8 and A7). On other peatland sites where carbon flux measurements are not available, this index could potentially serve as a preliminary source of information to estimate the carbon balance of peatlands.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <label>5.3</label><title>Climate change and droughts episode</title>
      <p id="d2e5309">Over the past 64 years, the Bernadouze peatland has experienced an increasing frequency of severe droughts, as indicated by the calculated dryness index (Figs. 7b and A3b). These events have contributed to the destabilization of the NEE balance, particularly in 2022. Despite some differences in seasonal representation, both ISBA and the statistical model by <xref ref-type="bibr" rid="bib1.bibx22" id="text.68"/> agree that  from July to November 2022, conditions fell completely outside the range of interannual variability. Similar dry summers have occurred in the past, notably in 1989, 1994, and 2003, and have consistently led to significant <inline-formula><mml:math id="M236" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions into the atmosphere. The years 1989 and 2003 are recognized as having experienced different types of drought conditions in France, ranging from multi-year precipitation deficits (1989–1990) to short, hot, and dry periods (2003) <xref ref-type="bibr" rid="bib1.bibx62" id="paren.69"/>. Similarly, 1994 is also identified as a year with a hot summer, preceded by a winter precipitation deficit in Southern Europe <xref ref-type="bibr" rid="bib1.bibx59" id="paren.70"/>. The dryness index effectively captures these hot and dry summers, which impact vegetation, its development, and consequently, the NEE flux.</p>
      <p id="d2e5332">As the growing season lengthens and GPP increases due to rising air temperatures, a compensatory effect appears to be at play. The peatland's greening and higher summer GPP fluxes currently help mitigate the impact of droughts, allowing it to remain a carbon sink. Over the 2001–2022 period, spring and autumn have played a growing role in shaping annual NEE, suggesting that these transitional seasons, along with winter, may become increasingly influential in the future, potentially counterbalancing summer carbon losses. However, the longevity of this balance remains uncertain. Some years, in our data, show a partial imbalance, indicating that the compensatory effect may not always fully buffer extreme conditions. Similar patterns have been observed in European forest ecosystems <xref ref-type="bibr" rid="bib1.bibx58" id="paren.71"/>, where compensatory mechanisms were insufficient to maintain carbon balance; this provides a useful analogy for interpreting the partial signals we observe in our peatland data. While greening and seasonal compensation currently mitigate summer carbon losses, prolonged or intensified droughts in the future could challenge this balance and affect the peatland’s long term carbon sink function.</p>
      <p id="d2e5338">The significant increase in annual maximum temperatures about 8 °C over 64 years raises concerns about the vegetation's ability to withstand such extreme warming. Studies on potential shifts in plant composition under climate change could provide valuable insights into the future of these ecosystems <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx15" id="paren.72"/>. This further emphasizes the need to integrate a broader range of plant communities and their interactions into land surface models, to more accurately represent ecosystem dynamics and their role in the carbon cycle.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusion</title>
      <p id="d2e5353">This study highlights the importance of accurately representing <italic>Sphagnum</italic> mosses in land surface models to simulate peatland carbon dynamics under changing climatic conditions. Validation of the new <italic>Sphagnum</italic> PFT within the ISBA model showed its ability to reproduce observed carbon fluxes with reasonable agreement. Analysis of the Bernadouze peatland over the past 64 years revealed that while it has remained a net carbon sink, increasing drought frequency and severity, particularly exemplified by the 2022 event, are destabilizing its carbon balance. The findings emphasize the critical role of vegetation composition, hydrological conditions, and seasonal climate dynamics in modulating peatland carbon fluxes. They also suggest that although compensatory mechanisms currently maintain peatland sink function, future intensification of droughts driven by climate change could potentially shift these ecosystems from carbon sinks to carbon sources. This underscores the urgent need to integrate interactive vegetation dynamics and drought responses into land surface models to better project peatland contributions to the global carbon cycle under future climate scenarios.</p>
</sec>

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

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

      <fig id="FA1"><label>Figure A1</label><caption><p id="d2e5376">Normalised total Sphagnum conductance as a function of Sphagnum water content.</p></caption>
        
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f09.png"/>

      </fig>

      <fig id="FA2"><label>Figure A2</label><caption><p id="d2e5389">Sphagnum canopy water resistance as a function of Sphagnum water content.</p></caption>
        
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f10.png"/>

      </fig>

<fig id="FA3"><label>Figure A3</label><caption><p id="d2e5404"><bold>(a)</bold> Diagnosed water table depth (WTD) from 1959 to 2022 for the Sphagnum-herbaceous vegetation mix. <bold>(b)</bold> Light blue: normalized WTD, red: normalized air temperature (Tair), pink: normalized Tair minus normalized WTD, dark blue area under the curve represents the dryness index (DI). Normalization of each variable (<inline-formula><mml:math id="M237" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>) was done following <inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">normalized</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">−</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mi mathvariant="normal">−</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></inline-formula>. <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:msub><mml:mtext>WTD</mml:mtext><mml:mi mathvariant="normal">min</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> m is taken from observations and not the diagnosed one from ISBA.</p></caption>
        
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f11.png"/>

      </fig>

      <fig id="FA4"><label>Figure A4</label><caption><p id="d2e5482">Comparison of daily ecosystem photosynthesis, respiration and net ecosystem exhange from the statistical model with: <bold>(a)</bold> the new Sphagnum photosynthesis, <bold>(b)</bold> the new Sphagnum ecosystem respiration, <bold>(c)</bold> the new Sphagnum net ecosystem exchange, <bold>(d)</bold> the previous herbaceous photosynthesis, <bold>(e)</bold> the previous herbaceous ecosystem respiration, <bold>(f)</bold> the previous herbaceous net ecosystem exchange, <bold>(g)</bold> the mixed vegetation photosynthesis, <bold>(h)</bold> the mixed vegetation ecosystem respiration, <bold>(i)</bold> the mixed vegetation net ecosystem exchange.</p></caption>
        
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f12.png"/>

      </fig>

<fig id="FA5"><label>Figure A5</label><caption><p id="d2e5524">Daily annual cycle (2017–2022) of <bold>(a)</bold> Gross Primary Productivity, <bold>(b)</bold> Ecosystem Respiration, <bold>(c)</bold> Net Ecosystem Exchange, <bold>(d)</bold> Water Table Depth from the statistical model in black, the ISBA Sphagnum model in orange, the ISBA herbaceous model in blue, and the ISBA mixed vegetation in green.</p></caption>
        
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f13.png"/>

      </fig>

      <fig id="FA6"><label>Figure A6</label><caption><p id="d2e5549">Hourly ISBA-diagnosed water table depth (WTD) with herbaceous vegetation as the dominant cover is compared to hourly in situ WTD in the left panel, while the right panel presents ISBA-diagnosed WTD with Sphagnum as the dominant vegetation versus in situ WTD.</p></caption>
        
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f14.png"/>

      </fig>

<fig id="FA7"><label>Figure A7</label><caption><p id="d2e5564">Annual NEE versus Summer NEE for each year from 1959 to 2022.</p></caption>
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f15.png"/>

      </fig>

      <fig id="FA8"><label>Figure A8</label><caption><p id="d2e5575">Summer NEE versus Dryness Index for each year from 1959 to 2022.</p></caption>
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f16.png"/>

      </fig>

      <fig id="FA9"><label>Figure A9</label><caption><p id="d2e5586"><bold>(a)</bold> Annual mean of vapor pressure deficit (VPD) (Pa) and scatter plot between VPD and air temperature; <bold>(b)</bold> Annual mean of relative humidity (%) from 1959 to 2022 derived from the S2M reanalysis.</p></caption>
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f17.png"/>

      </fig>

      <fig id="FA10"><label>Figure A10</label><caption><p id="d2e5602">Probability density function of annual cumulated <bold>(a)</bold> GPP and <bold>(b)</bold> ER over 1959–2022. In black, the vegetation mix corre- sponds to 70 % herbaceous and 30 % Sphagnum. In orange a 100 % Sphagnum mix and in blue a 100 % herbaceous mix. In shaded areas, the 95 % confidence intervals corresponding to the variation of the vegetation mix in the form <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi mathvariant="normal">Sphagnum</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:mo>×</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi mathvariant="normal">herbaceous</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mi mathvariant="normal">−</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M242" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> varying from 0 to 1 in steps of 0.01 and <inline-formula><mml:math id="M243" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula> being GPP or ER.</p></caption>
        <graphic xlink:href="https://bg.copernicus.org/articles/23/3407/2026/bg-23-3407-2026-f18.png"/>

      </fig>

<table-wrap id="TA1"><label>Table A1</label><caption><p id="d2e5680">Changes between <italic>Sphagnum</italic> and C<sub>3</sub> herbaceous plant functional type in <italic>ISBA</italic>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="4cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="3cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">Parameters</oasis:entry>

         <oasis:entry colname="col2">Units</oasis:entry>

         <oasis:entry colname="col3" align="left">C<sub>3</sub> Herbaceous</oasis:entry>

         <oasis:entry colname="col4" align="left">Sphagnum</oasis:entry>

         <oasis:entry colname="col5" align="left">Comments</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">ppmv</oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M251" display="inline"><mml:mn mathvariant="normal">45</mml:mn></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M252" display="inline"><mml:mn mathvariant="normal">45</mml:mn></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5" align="left"/>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">kg<sub>CO<sub>2</sub></sub> J<sup>−1</sup> PAR</oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.017</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">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.017</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">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5" align="left"/>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">mg m<sup>−2</sup> s<sup>−1</sup></oasis:entry>

         <oasis:entry colname="col3" align="left">1.7</oasis:entry>

         <oasis:entry colname="col4" align="left">1.0</oasis:entry>

         <oasis:entry colname="col5" align="left">Jacob's hypothesis: <inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>V</mml:mi><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>.</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M262" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">(–)</oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mi>f</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M264" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mi>f</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M265" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> does not vary with air humidity</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">(–)</oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:msubsup><mml:mi>f</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mo>*</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5" align="left"/>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="2"><inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">m s<sup>−1</sup></oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M271" display="inline"><mml:mrow><mml:msubsup><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mn mathvariant="normal">2.381</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6103</mml:mn><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M272" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E5"/>)</oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:mtext>SWI</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M274" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mn mathvariant="normal">2.381</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6103</mml:mn><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M275" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E5"/>)</oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M276" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mtext>SWI</mml:mtext><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M277" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">minimum</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">tot</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E5"/>)</oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:mtext>SWI</mml:mtext><mml:mo>≤</mml:mo><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="2"><inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">kg<sub>H<sub>2</sub><italic>O</italic></sub> kg<inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">air</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M283" display="inline"><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.045</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left">Non used</oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M284" display="inline"><mml:mrow><mml:mtext>SWI</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M285" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mi>X</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mi>X</mml:mi></mml:msubsup><mml:mo>)</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mtext>SWI</mml:mtext><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left">Non used</oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M286" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mtext>SWI</mml:mtext><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M287" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mi>X</mml:mi></mml:msubsup><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>SWI</mml:mtext><mml:mrow><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left">Non used</oasis:entry>

         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:mtext>SWI</mml:mtext><mml:mo>≤</mml:mo><mml:msub><mml:mi mathvariant="normal">SWI</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"><inline-formula><mml:math id="M289" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col2">Days</oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M290" display="inline"><mml:mn mathvariant="normal">150</mml:mn></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M291" display="inline"><mml:mn mathvariant="normal">80</mml:mn></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5" align="left"/>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">SLA</oasis:entry>

         <oasis:entry colname="col2">m<sup>2</sup> kg<inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">DryMass</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mi>e</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.56</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M295" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">6.73</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:mi>e</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col5" align="left"/>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">Root zone</oasis:entry>

         <oasis:entry colname="col2">–</oasis:entry>

         <oasis:entry colname="col3" align="left">20 cm, exponential profile distribution</oasis:entry>

         <oasis:entry colname="col4" align="left">no roots</oasis:entry>

         <oasis:entry colname="col5" align="left">Uniform distribution of <italic>Sphagnum</italic> over the top 10 cm</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">Vegetation height</oasis:entry>

         <oasis:entry colname="col2">m</oasis:entry>

         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M300" display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>LAI</mml:mtext><mml:mn mathvariant="normal">6</mml:mn></mml:mfrac></mml:mstyle></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4" align="left">0.05</oasis:entry>

         <oasis:entry colname="col5" align="left">Impacts Drag coefficient (<inline-formula><mml:math id="M301" display="inline"><mml:mi>H</mml:mi></mml:math></inline-formula> and <italic>LE</italic> fluxes)</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d2e5698"><bold>Note 1</bold>: <inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:msubsup><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> are the same quantities as <inline-formula><mml:math id="M246" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> but without hydric stress. <bold>Note 2:</bold> <inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:msubsup><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi><mml:mi>X</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>: this is the maximum value of <inline-formula><mml:math id="M248" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p></table-wrap-foot></table-wrap>

<table-wrap id="TA2"><label>Table A2</label><caption><p id="d2e6886">Parameters used for the Sphagnum PFT and their associated equations.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Parameter</oasis:entry>
         <oasis:entry colname="col2">Value</oasis:entry>
         <oasis:entry colname="col3">Equation</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M302" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M303" display="inline"><mml:mn mathvariant="normal">0.0004</mml:mn></mml:math></inline-formula> (mol<sup>−1</sup> m<sup>3</sup>)</oasis:entry>
         <oasis:entry colname="col3">(<xref ref-type="disp-formula" rid="Ch1.E5"/>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M306" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">(4)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M308" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">0.5</oasis:entry>
         <oasis:entry colname="col3">(4)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M309" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.0416</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">(4)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M311" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M312" display="inline"><mml:mn mathvariant="normal">27.6</mml:mn></mml:math></inline-formula> (<inline-formula><mml:math id="M313" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(<xref ref-type="disp-formula" rid="Ch1.E11"/>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M314" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M315" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M316" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(<xref ref-type="disp-formula" rid="Ch1.E11"/>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M317" display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M318" display="inline"><mml:mn mathvariant="normal">1</mml:mn></mml:math></inline-formula> (<inline-formula><mml:math id="M319" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">s</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(<xref ref-type="disp-formula" rid="Ch1.E13"/>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">min</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M321" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi>e</mml:mi><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="M322" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">(<xref ref-type="disp-formula" rid="Ch1.E13"/>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mo>min⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">2.4 (<inline-formula><mml:math id="M324" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(4)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M325" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mo>max⁡</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">22 (<inline-formula><mml:math id="M326" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(4)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M327" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">6 (<inline-formula><mml:math id="M328" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">g</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(4)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>


</app>

<app id="App1.Ch1.S2">
  <label>Appendix B</label><title>ISBA equations</title>
      <p id="d2e7344"><disp-formula id="App1.Ch1.S2.E21" content-type="numbered"><label>B1</label><mml:math id="M329" display="block"><mml:mrow><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:msubsup><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>exp⁡</mml:mi><mml:mo>[</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>exp⁡</mml:mi><mml:mo>[</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>T</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo><mml:mo>]</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M330" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math id="M331" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at 25 °C, <inline-formula><mml:math id="M332" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is fixed at 2.0, <inline-formula><mml:math id="M333" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the skin temperature in °C and <inline-formula><mml:math id="M334" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>1 and <inline-formula><mml:math id="M335" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>2 are reference temperature values. gm in unstressed soil moisture conditions, <inline-formula><mml:math id="M336" display="inline"><mml:mrow><mml:msup><mml:mtext>gm</mml:mtext><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>, depends on temperature via the same <inline-formula><mml:math id="M337" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> function as <inline-formula><mml:math id="M338" display="inline"><mml:mrow><mml:msub><mml:mtext>Am</mml:mtext><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.

          <disp-formula id="App1.Ch1.S2.E22" content-type="numbered"><label>B2</label><mml:math id="M339" display="block"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:msubsup><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></disp-formula>

        <inline-formula><mml:math id="M340" display="inline"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">25</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math id="M341" display="inline"><mml:mi mathvariant="normal">Γ</mml:mi></mml:math></inline-formula> at 25 °C. Here <inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:msub><mml:mi>Q</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is fixed at 1.5.

          <disp-formula id="App1.Ch1.S2.E23" content-type="numbered"><label>B3</label><mml:math id="M343" display="block"><mml:mrow><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Γ</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="normal">Γ</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:math></disp-formula>

        <inline-formula><mml:math id="M344" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula> is the initial quantum use efficiency, where <inline-formula><mml:math id="M345" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the maximum quantum use efficiency.

          <disp-formula id="App1.Ch1.S2.E24" content-type="numbered"><label>B4</label><mml:math id="M346" display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>f</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

        The internal <inline-formula><mml:math id="M347" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration <inline-formula><mml:math id="M348" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, is directly derived from the <inline-formula><mml:math id="M349" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in the air <inline-formula><mml:math id="M350" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and from <inline-formula><mml:math id="M351" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> which is detailed in Table A1.

          <disp-formula id="App1.Ch1.S2.E25" content-type="numbered"><label>B5</label><mml:math id="M352" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:msub><mml:mi>C</mml:mi><mml:mi>H</mml:mi></mml:msub><mml:msub><mml:mi>V</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">δ</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

        The evaporation of the vegetated surface is the sum of the evaporation of the soil (<inline-formula><mml:math id="M353" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the evaporation of the vegetation (<inline-formula><mml:math id="M354" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>): <inline-formula><mml:math id="M355" display="inline"><mml:mrow><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The evaporation of the vegetation is itself distributed between the direct evaporation (<inline-formula><mml:math id="M356" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) due to the fraction of folliage covered by water intercepted and the transpiration (<inline-formula><mml:math id="M357" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>): <inline-formula><mml:math id="M358" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e8091"><inline-formula><mml:math id="M359" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">veg</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the fraction of vegetation, <inline-formula><mml:math id="M360" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> the fraction of folliage covered by intercepted water and <inline-formula><mml:math id="M361" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the canopy resistance taking into account the upscalling of the cuticular and stomatal resistance.</p>
      <p id="d2e8122">For the modelling of <italic>Sphagnum</italic>, <inline-formula><mml:math id="M362" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> is set to 0, and <inline-formula><mml:math id="M363" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is changed in <inline-formula><mml:math id="M364" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">sp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (in this context, historical transpiration effectively corresponds to the evaporation from <italic>Sphagnum</italic>).</p>
</app>
  </app-group><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d2e8164">The data presented in this study are available at <ext-link xlink:href="https://doi.org/10.5281/zenodo.16984992" ext-link-type="DOI">10.5281/zenodo.16984992</ext-link> <xref ref-type="bibr" rid="bib1.bibx23" id="paren.73"/>.</p>

      <p id="d2e8173">The S2M dataset is freely accessible via the AERIS data center at <ext-link xlink:href="https://doi.org/10.25326/37#v2020.2" ext-link-type="DOI">10.25326/37#v2020.2</ext-link> <xref ref-type="bibr" rid="bib1.bibx61" id="paren.74"/>. The S2M data are provided by Météo-France, CNRS, CNRM, and the Centre d'Études de la Neige through AERIS.</p>

      <p id="d2e8182">The model used in this study is open-source. The ISBA model, as implemented in this work, is part of SURFEX version 9 and can be downloaded from the SURFEX platform: <uri>http://www.umr-cnrm.fr/surfex/</uri> (last access: 11 May 2026).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e8192">RG, CD, BD and LG conceptualized and designed the study. RG modified and implemented the model, conducted formal analysis of the results, and led the writing of the original draft with contributions from all co-authors. All authors participated in reviewing, editing, and finalizing the manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e8198">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e8204">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e8210">The authors gratefully acknowledge Matthieu Lafaysse for providing the S2M data and for his valuable support.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e8216">This work is part of project PEACE of the exploratory research program FairCarboN and received government funding managed by the Agence Nationale de la Recherche under the France 2030 program, reference ANR-22-PEXF-0011. Observatoire Homme-Milieu Pyrenees Haut Vicdessos – LABEX DRIIHM ANR-11-LABX0010. The bernadouze site is part of the “Service National d'Observation des Tourbières” (SNO-French Peatland Observatory), part of the research infrastructure OZCAR, accredited by the INSU/CNRS.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e8222">This paper was edited by Petr Kuneš and reviewed by Katharina Jentzsch and one anonymous referee.</p>
  </notes><ref-list>
    <title>References</title>

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