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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESD</journal-id><journal-title-group>
    <journal-title>Earth System Dynamics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2190-4987</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/esd-17-929-2026</article-id><title-group><article-title>Strong intensification of extreme fire weather in Europe under 3 °C compared to 2 °C global warming</article-title><alt-title>Strong intensification of extreme fire weather in Europe</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff4">
          <name><surname>Bayar</surname><given-names>A. Serkan</given-names></name>
          <email>serkan.bayar@ufz.de</email>
        <ext-link>https://orcid.org/0000-0002-9663-2058</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Pinto</surname><given-names>Joaquim G.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8865-1769</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Gouveia</surname><given-names>Célia M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3147-5696</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Ramos</surname><given-names>Alexandre M.</given-names></name>
          <email>alexandre.ramos@kit.edu</email>
        <ext-link>https://orcid.org/0000-0003-3129-7233</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Institute of Meteorology and Climate Research – Troposphere Research (IMKTRO), Karlsruhe Institute of Technology (KIT), Karlsruhe, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>IDL-Instituto Dom Luíz, Faculdade de Ciências, Universidade de Lisboa, Lisboa, Portugal</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Instituto Português do Mar e da Atmosfera, Rua C do Aeroporto, Lisboa, Portugal</institution>
        </aff>
        <aff id="aff4"><label>a</label><institution>current address: Department of Compound Environmental Risks, Helmholtz Centre for Environmental Research – UFZ, Leipzig, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">A. Serkan Bayar (serkan.bayar@ufz.de) and Alexandre M. Ramos (alexandre.ramos@kit.edu)</corresp></author-notes><pub-date><day>1</day><month>July</month><year>2026</year></pub-date>
      
      <volume>17</volume>
      <issue>3</issue>
      <fpage>929</fpage><lpage>954</lpage>
      <history>
        <date date-type="received"><day>2</day><month>December</month><year>2025</year></date>
           <date date-type="rev-request"><day>8</day><month>December</month><year>2025</year></date>
           <date date-type="rev-recd"><day>1</day><month>June</month><year>2026</year></date>
           <date date-type="accepted"><day>4</day><month>June</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 A. Serkan Bayar 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://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026.html">This article is available from https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e133">The climate in Europe is warming faster than the global average, raising concerns about how climate change will affect extreme fire events. In this study, we use ERA5-Land reanalysis data and an ensemble of 33 high-resolution regional climate models (RCMs) from the EURO-CORDEX framework to compute the Canadian Forest Fire Weather Index (FWI) and investigate both recent and projected changes in atmospheric conditions favorable for wildfires across Europe. Historical trends (1950–2023) based on ERA5-Land data reveal statistically significant increases in the frequency and intensity of extreme fire weather in regions such as the Iberian Peninsula, Central Europe, and parts of Eastern Europe. All RCM input fields were bias-adjusted prior to FWI calculation using Quantile Delta Mapping, resulting in improved FWI representation relative to unadjusted simulations. Projections based on the bias-adjusted EURO-CORDEX ensemble indicate that future extreme fire weather will become more frequent, more intense, and more widespread across Europe as global warming progresses. The strongest signals are projected for southern Europe, with a northward expansion of fire-prone conditions under higher global warming levels (GWLs). At 3 °C GWL, the spatial extent of robust changes in extreme fire weather metrics nearly doubles compared to 2 °C, with one metric increasing fivefold. Relative increases in frequency-based metrics generally exceed those in magnitude-based metrics. These changes coincide with rising vapor pressure deficit, suggesting that thermodynamic processes play a key role through atmospheric drying. The projected intensification of extreme fire weather in Europe highlights the growing need for coordinated climate action along with proactive mitigation strategies.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e145">Wildfires have been part of Earth's history since the emergence of terrestrial plants more than 400 million years ago <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx92" id="paren.1"/>. They are an essential component of the Earth system, shaping the evolution and distribution of plant and animal life, as well as influencing key biogeochemical processes <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx49" id="paren.2"/>. Fires burn approximately 4 million km<sup>2</sup> area each year <xref ref-type="bibr" rid="bib1.bibx27" id="paren.3"/> and have significant direct and indirect impacts on both global and regional climate through the emission of greenhouse gases and aerosols. Despite considerable uncertainty, recent data indicate that global mean carbon emissions from anthropogenic and natural fires were estimated at 3.4 PgC yr<sup>−1</sup> during the period 2002–2022 <xref ref-type="bibr" rid="bib1.bibx104" id="paren.4"/>, which is approximately 30.6 % of the magnitude of global anthropogenic CO<sub>2</sub> emissions in 2022 <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx40" id="paren.5"/>.</p>
      <p id="d2e194">Satellite-derived data show a nearly 25 % decrease in global burned area between 1998 and 2015 <xref ref-type="bibr" rid="bib1.bibx6" id="paren.6"/>. This decline is primarily concentrated in tropical savannas and grasslands and is largely attributed to agricultural expansion and changes in land cover <xref ref-type="bibr" rid="bib1.bibx6" id="paren.7"/>. However, despite this decrease in global burned area, global fire emissions have remained relatively stable <xref ref-type="bibr" rid="bib1.bibx116" id="paren.8"/>, which is explained by an increase in forest fire emissions across North America and Eurasia where fires release more CO<sub>2</sub> per unit area burned <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx116" id="paren.9"/>. Moreover, the frequency and magnitude of extreme wildfires more than doubled between 2003 and 2023 <xref ref-type="bibr" rid="bib1.bibx31" id="paren.10"/>, and a significant proportion of extreme fire events occurred under extreme fire weather conditions <xref ref-type="bibr" rid="bib1.bibx15" id="paren.11"/>.</p>
      <p id="d2e225">Fire weather refers to atmospheric conditions that are conducive to triggering and propagating wildfires <xref ref-type="bibr" rid="bib1.bibx69" id="paren.12"/>. Numerous fire weather indices based on daily surface weather variables (e.g., temperature, precipitation, relative humidity, and wind) have been developed and applied across different regions <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx58" id="paren.13"/>. These indices reflect the effects of atmospheric conditions on fuel dryness and subsequent potential fire danger, and are strongly correlated with the magnitude and extent of wildfires, particularly in ecosystems with intermediate moisture availability <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx8 bib1.bibx23 bib1.bibx57 bib1.bibx58" id="paren.14"/>. In recent decades, increasing global trends have been observed both in the duration of the fire season and the frequency of these conditions <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx58" id="paren.15"/>. Under projected global warming, both the frequency and intensity of extreme fire weather are expected to further increase worldwide <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx15 bib1.bibx58 bib1.bibx69" id="paren.16"/>.</p>
      <p id="d2e243">Europe has warmed at twice the global average rate since the 1980s <xref ref-type="bibr" rid="bib1.bibx30" id="paren.17"/>. Moreover, approximately 70 %–90 % of the continent's land area is projected to shift into different climate zones by the end of the century under high-emission scenario simulations, with a notable tendency toward warmer and drier conditions in the southern and western regions <xref ref-type="bibr" rid="bib1.bibx7" id="paren.18"/>. Consistent with this tendency and the expected increase in compound hot and dry events <xref ref-type="bibr" rid="bib1.bibx69" id="paren.19"/>, extreme fire weather is also projected to increase across much of Europe <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx58" id="paren.20"/>, with particularly pronounced changes in the Mediterranean region <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx88" id="paren.21"/>. Growing concern also surrounds the impacts of climate change on extreme fire weather in central Europe, an area that is historically less prone to these events. <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx73 bib1.bibx76" id="paren.22"/></p>
      <p id="d2e265">In addition to global-scale studies that show a projected increase in fire weather extremes across the continent <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx58" id="paren.23"><named-content content-type="pre">e.g.,</named-content></xref>, two recent pan-European scale studies projected widespread increases in extreme fire weather under the impacts of climate change <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx50" id="paren.24"/>. Both studies relied on global climate model output from the sixth phase of the Climate Model Intercomparison Project (CMIP6) <xref ref-type="bibr" rid="bib1.bibx37" id="paren.25"/> and applied statistical downscaling techniques to reach the target resolution (<inline-formula><mml:math id="M5" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 31 km in <xref ref-type="bibr" rid="bib1.bibx35" id="altparen.26"/> and <inline-formula><mml:math id="M6" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 9 km in <xref ref-type="bibr" rid="bib1.bibx50" id="altparen.27"/>). However, since statistically downscaled fields still inherit the climate change signal from driving global climate models (GCMs) and do not incorporate fine-grid scale physical processes, they may not fully capture important regional scale phenomena, such as snow-albedo feedback in mountainous regions <xref ref-type="bibr" rid="bib1.bibx68" id="paren.28"/>, potentially leading to a loss of physical consistency and biased results. To address this limitation, dynamically downscaled regional climate models (RCMs) offer an alternative approach as they refine the large-scale circulation response obtained from GCMs to finer scales by explicitly simulating sub-GCM grid-scale processes <xref ref-type="bibr" rid="bib1.bibx43" id="paren.29"/>. Consistent with this, a recent study found that RCMs from the Coordinated Regional Climate Downscaling Experiment (CORDEX) reproduce historical fire weather trends more accurately than GCMs participating in CMIP5 and CMIP6 <xref ref-type="bibr" rid="bib1.bibx79" id="paren.30"/>.</p>
      <p id="d2e309">Many studies have used RCMs from the EURO-CORDEX domain <xref ref-type="bibr" rid="bib1.bibx54" id="paren.31"/> to project fire weather danger across Europe in a warming climate, but many of them relied on relatively small ensemble sizes <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx41" id="paren.32"><named-content content-type="pre">e.g.,</named-content></xref>, which limits the characterization of model uncertainty. Moreover, they were often limited to specific regions, such as Greece <xref ref-type="bibr" rid="bib1.bibx87" id="paren.33"/>, France <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx106" id="paren.34"/>, or the Iberian Peninsula <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx19" id="paren.35"/>. In addition to these limitations, simulations in the EURO-CORDEX framework have been found to exhibit systematic biases relative to observations and reanalysis, with an overall tendency to be too cold, too wet, and too windy <xref ref-type="bibr" rid="bib1.bibx109" id="paren.36"/>. Since extreme fire weather is a multivariate phenomenon driven by the combined effect of these fields, biases in them may compound and amplify the overall uncertainty in fire weather indices and associated outcomes. Accordingly, input fields for calculating the FWI need to be adjusted for biases to increase confidence in decision-making regarding the impacts of extreme fire weather in a warming climate.</p>
      <p id="d2e333">Despite the growing literature on projections of extreme fire weather in Europe, important gaps remain in terms of better representing regional details and uncertainty through the use of larger RCM ensembles, as well as increasing confidence in projections by bias-adjusting atmospheric fields. To address these research gaps, we use a relatively large ensemble from the EURO-CORDEX framework <xref ref-type="bibr" rid="bib1.bibx54" id="paren.37"/>, consisting of 33 GCM-RCM chains and aim to comprehensively assess projections of extreme fire weather danger at a pan-European scale in a warming climate. We focus on projected changes at 2  and 3 °C  global warming levels (GWLs) and rely on scenario simulations based on the Representative Concentration Pathway (RCP) 8.5. Fire weather is quantified using the Canadian Forest Fire Weather Index (FWI) System <xref ref-type="bibr" rid="bib1.bibx105" id="paren.38"/>, as it relies solely on daily meteorological input fields and has been shown to perform well in Europe, especially in the Mediterranean <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx58 bib1.bibx89 bib1.bibx110" id="paren.39"/>. Prior to calculating projected fire weather danger, model input fields are bias adjusted using quantile delta mapping (QDM) <xref ref-type="bibr" rid="bib1.bibx21" id="paren.40"/>, with ERA5-Land reanalysis data <xref ref-type="bibr" rid="bib1.bibx78" id="paren.41"/> serving as reference. We also use ERA5-Land reanalysis to estimate historical trends in FWI across Europe. Finally, we investigate subcomponents of the FWI system, individual meteorological fields, and vapor pressure deficit (VPD) to shed light on potential drivers of projected future changes in extreme fire weather. The main objectives of this study are as follows:</p>
      <p id="d2e351"><list list-type="bullet">
          <list-item>

      <p id="d2e356">Examine the observed climatology of extreme fire weather across Europe and its associated trends since 1950 based on ERA5-Land.</p>
          </list-item>
          <list-item>

      <p id="d2e362">Assess the added value of bias adjustment using QDM in terms of spatial patterns of bias in extreme FWI for the EURO-CORDEX multi-model ensemble median.</p>
          </list-item>
          <list-item>

      <p id="d2e368">Quantify changes in the frequency and intensity of extreme fire weather at 2 °C and 3 °C GWLs, and identify the potential drivers underlying these changes based on the bias-adjusted EURO-CORDEX multi-model ensemble.</p>
          </list-item>
        </list></p>
      <p id="d2e373">The study is structured as follows: Section 2 gives an overview of data and methods, Section 3 describes the results in detail, including the observed trends, the added value of bias adjustment, and projections of extreme fire weather across Europe in a warming climate. Section 4 summarizes the main results and provides a discussion.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Data</title>
<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><title>ERA5-Land Reanalysis</title>
      <p id="d2e398">In this study, hourly atmospheric fields, including 2-meter temperature, precipitation, 10 meter u (zonal) and v (meridional) components of wind speed and 2-meter dew point temperature were used from the European Centre for Medium-Range Weather Forecasts (ECMWF) ERA5-Land reanalysis <xref ref-type="bibr" rid="bib1.bibx78" id="paren.42"/>. The main advantage of ERA5-Land is its enhanced horizontal grid resolution of 9 km, compared to 31 km for ERA5 <xref ref-type="bibr" rid="bib1.bibx78" id="paren.43"/>. The dataset covers the period from 1950 to the present, with data up to 2023 used in this study. ERA5-Land reanalysis data were used for several purposes throughout the study, which can be summarized as follows: <list list-type="bullet"><list-item>
      <p id="d2e409">The hourly atmospheric fields were first used to calculate the original noon-time (12:00) FWI. These fields were then aggregated to the daily scale to estimate the most suitable proxy input variable combination to replace the original noon-time FWI calculation at the daily scale (see Table S1 in the Supplement for a complete list of variables used).</p></list-item><list-item>
      <p id="d2e413">The historical climatology of FWI metrics and the associated trends were calculated using the selected daily proxy input combination.</p></list-item><list-item>
      <p id="d2e417">The daily atmospheric fields derived from GCM-RCM chains were bias-adjusted using daily aggregated ERA5-Land values as a reference.</p></list-item></list></p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <label>2.1.2</label><title>EURO-CORDEX Simulations</title>
      <p id="d2e428">We considered a set of 33 GCM-RCM chains from the EURO-CORDEX framework <xref ref-type="bibr" rid="bib1.bibx54" id="paren.44"/> to quantify future changes in extreme fire weather in Europe (the largest ensemble available during the data curation phase of this study in December 2024 included 34 model chains, from which we removed one due to quality issues). The variables used include daily maximum temperature, accumulated precipitation, mean relative humidity, and maximum wind speed (for details on variable selection, see Sects. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS4"/> and <xref ref-type="sec" rid="Ch1.S3.SS1"/>). EURO-CORDEX simulations are dynamically downscaled from GCMs participating in CMIP5 <xref ref-type="bibr" rid="bib1.bibx97" id="paren.45"/> to provide high-resolution regional climate simulations across Europe. All models share a common horizontal grid spacing of <inline-formula><mml:math id="M7" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 12 km. Both historical simulations (covering the period from 1950 or 1970, depending on the model, to 2005) and scenario simulations (covering 2006 to 2100) were used. The scenario simulations follow the RCP8.5 scenario, which represents a high-end greenhouse gas emission scenario with a radiative forcing of 8.5 W m<sup>−2</sup> by the end of the century. We focused exclusively on the RCP8.5 scenario as all simulations reach both 2 °C and 3 °C GWL thresholds within the 21st century under this pathway, which allows for consistent ensemble sizes and a robust comparison across warming levels. A single model realization (r1i1p1) was used for each model. All simulations were regridded to the ERA5-Land grid resolution of 9 km using first-order conservative remapping <xref ref-type="bibr" rid="bib1.bibx60" id="paren.46"/>. The list of models used in this study is provided in Table <xref ref-type="table" rid="T1"/>.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e469">List of the 33 GCM-RCM chains used in this study. All scenario simulations follow RCP8.5, so that all models reach the 3 °C GWL during the 21st century. All models belong to the same ensemble member r1i1p1.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">GCM</oasis:entry>
         <oasis:entry colname="col2">RCM</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">CNRM-CERFACS-CNRM-CM5</oasis:entry>
         <oasis:entry colname="col2">DMI-HIRHAM5 <xref ref-type="bibr" rid="bib1.bibx13" id="paren.47"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                      <xref ref-type="bibr" rid="bib1.bibx111" id="paren.48"/>
                    </oasis:entry>
         <oasis:entry colname="col2">GERICS-REMO2015 <xref ref-type="bibr" rid="bib1.bibx53" id="paren.49"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">IPSL-WRF381P <xref ref-type="bibr" rid="bib1.bibx107" id="paren.50"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KNMI-RACMO22E <xref ref-type="bibr" rid="bib1.bibx72" id="paren.51"/></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SMHI-RCA4 <xref ref-type="bibr" rid="bib1.bibx63" id="paren.52"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ICHEC-EC-EARTH</oasis:entry>
         <oasis:entry colname="col2">CLMcom-ETH-COSMO-crCLIM-v1-1 <xref ref-type="bibr" rid="bib1.bibx96" id="paren.53"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                      <xref ref-type="bibr" rid="bib1.bibx47" id="paren.54"/>
                    </oasis:entry>
         <oasis:entry colname="col2">DMI-HIRHAM5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KNMI-RACMO22E</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SMHI-RCA4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">IPSL-IPSL-CM5A-MR</oasis:entry>
         <oasis:entry colname="col2">DMI-HIRHAM5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                      <xref ref-type="bibr" rid="bib1.bibx34" id="paren.55"/>
                    </oasis:entry>
         <oasis:entry colname="col2">GERICS-REMO2015</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">IPSL-WRF381P</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KNMI-RACMO22E</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SMHI-RCA4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MOHC-HadGEM2-ES</oasis:entry>
         <oasis:entry colname="col2">CLMcom-ETH-COSMO-crCLIM-v1-1</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                      <xref ref-type="bibr" rid="bib1.bibx29" id="paren.56"/>
                    </oasis:entry>
         <oasis:entry colname="col2">DMI-HIRHAM5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">IPSL-WRF381P</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KNMI-RACMO22E</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">MOHC-HadREM3-GA7-05 <xref ref-type="bibr" rid="bib1.bibx101" id="paren.57"/></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SMHI-RCA4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MPI-M-MPI-ESM-LR</oasis:entry>
         <oasis:entry colname="col2">CLMcom-ETH-COSMO-crCLIM-v1-1</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                      <xref ref-type="bibr" rid="bib1.bibx42" id="paren.58"/>
                    </oasis:entry>
         <oasis:entry colname="col2">DMI-HIRHAM5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">IPSL-WRF381P</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KNMI-RACMO22E</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">MOHC-HadREM3-GA7-05</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SMHI-RCA4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NCC-NorESM1-M</oasis:entry>
         <oasis:entry colname="col2">CLMcom-ETH-COSMO-crCLIM-v1-1</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">
                      <xref ref-type="bibr" rid="bib1.bibx10" id="paren.59"/>
                    </oasis:entry>
         <oasis:entry colname="col2">DMI-HIRHAM5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">GERICS-REMO2015</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">IPSL-WRF381P</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">KNMI-RACMO22E</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">MOHC-HadREM3-GA7-05</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SMHI-RCA4</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e809">In order to better understand regional differences in extreme fire weather behavior across Europe, these metrics have also been spatially aggregated and averaged over the PRUDENCE regions <xref ref-type="bibr" rid="bib1.bibx26" id="paren.60"/>. In addition to the eight regions that were previously defined, Turkey was included as an additional subregion (Fig. <xref ref-type="fig" rid="F1"/>a), as it has been shown to be particularly sensitive to extreme climate events <xref ref-type="bibr" rid="bib1.bibx44" id="paren.61"/>. We note that the eastern boundary of Turkey is not covered by the EURO-CORDEX domain and is therefore not included in this study.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS3">
  <label>2.1.3</label><title>Burned Area and Land Cover Data</title>
      <p id="d2e828">In order to provide a historical context for the projected changes in fire weather, we used burned area data from the fifth version of the Global Fire Emissions Database <xref ref-type="bibr" rid="bib1.bibx25" id="paren.62"><named-content content-type="pre">GFED5;</named-content></xref>. This dataset provides a monthly burned area record from 2002 to 2022 at a 0.25° grid resolution, and is derived from the Moderate Resolution Imaging Spectroradiometer (MODIS) MCD64A1 burned area product <xref ref-type="bibr" rid="bib1.bibx25" id="paren.63"/>. We used GFED5 burned area data to present the climatology of the total annual burned area fraction relative to the grid cell area across Europe (Fig. <xref ref-type="fig" rid="F1"/>b).</p>
      <p id="d2e841">We also obtained Global Land Cover data from Copernicus <xref ref-type="bibr" rid="bib1.bibx17" id="paren.64"/> for 2019 at a 100 m grid resolution to mask out regions that are considered unburnable. Similar to what was done for the EURO-CORDEX simulations, we first interpolated this field to the ERA5-Land grid resolution using first-order conservative remapping. Then, land areas classified as containing more than 80 % of urban/built-up, bare or sparse vegetation, snow and ice, or water were considered unburnable <xref ref-type="bibr" rid="bib1.bibx3" id="paren.65"/>. Finally, this interpolated unburnable land mask was applied to all fire weather-related analyses throughout the study.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e852"><bold>(a)</bold> PRUDENCE regions investigated in this study, based on the definitions of <xref ref-type="bibr" rid="bib1.bibx26" id="text.66"/> and shown with surface altitude data from COSMO-CLM in the EURO-CORDEX domain <xref ref-type="bibr" rid="bib1.bibx96" id="paren.67"/>. BI <inline-formula><mml:math id="M9" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> British Isles, SC <inline-formula><mml:math id="M10" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Scandinavia, FR <inline-formula><mml:math id="M11" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> France, ME <inline-formula><mml:math id="M12" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Mid-Europe, AL <inline-formula><mml:math id="M13" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Alps, EA <inline-formula><mml:math id="M14" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Eastern Europe, IP <inline-formula><mml:math id="M15" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Iberian Peninsula, MD <inline-formula><mml:math id="M16" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Mediterranean, TR <inline-formula><mml:math id="M17" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Turkey. Note that Turkey is included here in addition to the previously defined regions. <bold>(b)</bold> Climatology of the annual total burned area fraction relative to the grid cell area (% yr<sup>−1</sup>), calculated for the period 2002–2022 based on GFED5 <xref ref-type="bibr" rid="bib1.bibx25" id="paren.68"/>. The figure aims to provide a historical context to the projected changes in fire weather extremes from a burned area perspective.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f01.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Methods</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Global Warming Levels</title>
      <p id="d2e968">We use GWLs to quantify changes in extreme fire weather as many drivers of global and regional climate impacts are closely linked to GWLs <xref ref-type="bibr" rid="bib1.bibx69" id="paren.69"/>. GCMs have different climate sensitivities and each follows its own trajectory to reach a given GWL at a different time. Using the GWL approach enables the estimation of impacts independently of the specific scenario or timing at which a given GWL is reached. This study focuses on <inline-formula><mml:math id="M19" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2  and <inline-formula><mml:math id="M20" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWLs relative to the preindustrial reference period 1881–1910 following <xref ref-type="bibr" rid="bib1.bibx74" id="text.70"/> and <xref ref-type="bibr" rid="bib1.bibx52" id="text.71"/>. The methodology is based on the time sampling approach <xref ref-type="bibr" rid="bib1.bibx56" id="paren.72"/> as implemented by <xref ref-type="bibr" rid="bib1.bibx108" id="text.73"/> and <xref ref-type="bibr" rid="bib1.bibx98" id="text.74"/> for regional climate change signals in Europe.</p>
      <p id="d2e1004">First, the 30-year running average of the global mean temperature was calculated from the scenario simulations of the GCMs. The observed global warming from 1881–1910 to 1971–2000 was already estimated as 0.46 °C <xref ref-type="bibr" rid="bib1.bibx108" id="paren.75"/>. The average global mean temperature of the GCMs during 1971–2000 was then used as historical reference, so that an increase of 1.54 °C (2.54 °C) from that value corresponds to <inline-formula><mml:math id="M21" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C (<inline-formula><mml:math id="M22" display="inline"><mml:mo lspace="0mm">+</mml:mo></mml:math></inline-formula>3 °C) GWL relative to the preindustrial period. Next, 30-year time periods were identified based on when the relevant GWLs are reached for the first time in the running average (as listed in Table S2). We note that although the GWLs are defined relative to the preindustrial period, the change signals presented in this study are expressed relative to the historical reference period (1971–2000, <inline-formula><mml:math id="M23" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.46 °C). This is a deliberate choice, as RCM simulations from the EURO-CORDEX framework only begin after 1950.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Bias Adjustment of EURO-CORDEX Simulations</title>
      <p id="d2e1039">GCMs are known to have systematic biases due to various factors, such as discretization and spatial averaging within grid cells <xref ref-type="bibr" rid="bib1.bibx99" id="paren.76"/>, inadequate representation of thermodynamic processes <xref ref-type="bibr" rid="bib1.bibx112" id="paren.77"/>, or inaccuracies in simulating atmospheric dynamics <xref ref-type="bibr" rid="bib1.bibx95" id="paren.78"/>. Since the nested downscaled model is driven by imposed boundary conditions, RCMs also often inherit the biases of their driving GCMs, such as incorrect placement of storm tracks <xref ref-type="bibr" rid="bib1.bibx43" id="paren.79"/>, and can also introduce their own biases. Therefore, it is common practice to adjust biases in climate model output, particularly before using the results for impact modeling <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx33 bib1.bibx45 bib1.bibx77" id="paren.80"/>.</p>
      <p id="d2e1057">Here, we applied the QDM method <xref ref-type="bibr" rid="bib1.bibx21" id="paren.81"/> to adjust the biases in the input fields extracted from EURO-CORDEX simulations, which were subsequently used to calculate the FWI. It could be argued that adjusting the FWI itself might be a more direct and computationally cheaper approach than adjusting the input fields, especially if the sole objective is to increase confidence in the FWI projections. However, our aim is not only to enhance confidence in the FWI projections but also to understand the physical drivers of the expected changes in FWI by tracing changes in the underlying input fields. To avoid inconsistencies that might arise from adjusting only the FWI, each individual input field was adjusted via QDM.</p>
      <p id="d2e1063">In order to apply QDM, the non-exceedance probabilities of the simulations were first calculated over the projected time window:

              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M24" display="block"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msubsup><mml:mi>F</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">p</mml:mi></mml:mrow><mml:mi>d</mml:mi></mml:msubsup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>[</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">p</mml:mi></mml:mrow></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>]</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">p</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the projected simulation value of the variable of interest at time step <inline-formula><mml:math id="M26" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msubsup><mml:mi>F</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">p</mml:mi></mml:mrow><mml:mi>d</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> is the empirical cumulative distribution function (CDF) of the time series being corrected and <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the non-exceedance probability associated with time step t and has a range between 0 and 1.</p>
      <p id="d2e1178">Next, the relative change signal between the projected and historical simulations was calculated:

              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M29" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">p</mml:mi></mml:mrow></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msubsup><mml:mi>F</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">h</mml:mi></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>[</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>]</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the relative change signal at time step <inline-formula><mml:math id="M31" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msubsup><mml:mi>F</mml:mi><mml:mrow><mml:mi mathvariant="normal">s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">h</mml:mi></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> is the inverse CDF of the simulation during the calibration period.</p>
      <p id="d2e1290">Finally, the calculated climate change signal was multiplied by the corresponding reference observation value (from ERA5-Land) at the same quantile during the calibration period:

              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M33" display="block"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">ba</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msubsup><mml:mi>F</mml:mi><mml:mrow><mml:mi mathvariant="normal">r</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">h</mml:mi></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>[</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">ba</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the bias adjusted variable at time step t and <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msubsup><mml:mi>F</mml:mi><mml:mrow><mml:mi mathvariant="normal">r</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">h</mml:mi></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> is the inverse CDF of the reference data (ERA5-Land) during the calibration period (1971–2000).</p>
      <p id="d2e1389">We note that the described multiplicative approach was applied to precipitation, mean relative humidity, and maximum wind speed. An additive version of the same method was used for maximum temperature. For further details on the bias adjustment methodology, please see Section S1 in the Supplement.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>FWI Calculation</title>
      <p id="d2e1400">We employ the widely used Canadian Forest Fire Weather Index System <xref ref-type="bibr" rid="bib1.bibx105" id="paren.82"/> to calculate the historical and projected distribution of extreme fire weather throughout Europe. It consists of six components. The first three components are fuel moisture codes, namely, Fine Fuel Moisture Code (FFMC), Duff Moisture Code (DMC), and Drought Code (DC) and they represent the dryness of fuels in different layers of the Canadian forest floor <xref ref-type="bibr" rid="bib1.bibx114" id="paren.83"/>. The final three components of the FWI system represent fire behavior: Initial Spread Index (ISI) predicts the potential rate of fire spread based on wind speed and surface fuel dryness, BUI represents the total amount of fuel available for burning and FWI, which results from the combination of the previous two, is a numeric rating of the potential fire intensity <xref ref-type="bibr" rid="bib1.bibx114" id="paren.84"/>. Figure <xref ref-type="fig" rid="F2"/> provides a schematic overview of the calculation flow and the required atmospheric input fields.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e1416">Schematic representation of the Canadian Forest Fire Weather Index System, showing its input variables and six components, based on <xref ref-type="bibr" rid="bib1.bibx105" id="text.85"/>.</p></caption>
            <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f02.png"/>

          </fig>

      <p id="d2e1428">By definition, the FWI calculation requires temperature, relative humidity, and wind speed at local noon (12:00), as well as accumulated precipitation from the previous day's noon to the current day's noon. All input data required for the FWI calculation are directly available from the ERA5-Land reanalysis product, except for relative humidity. Therefore, relative humidity was calculated using the 2 m temperature and 2 m dewpoint temperature outputs from ERA5-Land, applying the Magnus formula <xref ref-type="bibr" rid="bib1.bibx5" id="paren.86"/>. FWI was then computed for the ERA5-Land reanalysis from 1950 to 2023 using these four atmospheric fields at noon as input.</p>
      <p id="d2e1435">To account for dry conditions outside the fire season (fall and winter), the overwintering approach was applied to the Drought Code (DC) <xref ref-type="bibr" rid="bib1.bibx71" id="paren.87"/>. The overwintering calculation requires a definition of the fire season, outside of which FWI is not calculated. The definition used here follows <xref ref-type="bibr" rid="bib1.bibx115" id="text.88"/>, where the fire season begins when the maximum temperature exceeds 12 °C for at least three consecutive days and ends when it drops below 5 °C for at least three consecutive days <xref ref-type="bibr" rid="bib1.bibx84" id="paren.89"/>. The purpose of overwintering the DC is to capture dry fall and winter conditions, which can lead to more severe fire weather conditions at the beginning of the fire season compared to the default DC value <xref ref-type="bibr" rid="bib1.bibx71" id="paren.90"/>.</p>
      <p id="d2e1450">We used four annual FWI metrics to analyze the extreme fire weather behavior at each grid cell for the reference period (1971–2000, <inline-formula><mml:math id="M36" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.46 °C) and at <inline-formula><mml:math id="M37" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 and <inline-formula><mml:math id="M38" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWLs, following the metrics used in <xref ref-type="bibr" rid="bib1.bibx57" id="text.91"/>, <xref ref-type="bibr" rid="bib1.bibx3" id="text.92"/> and <xref ref-type="bibr" rid="bib1.bibx84" id="text.93"/>: <list list-type="order"><list-item>
      <p id="d2e1486">Number of days exceeding the reference period (1971–2000) 95th percentile of FWI (FWI<sub>95 d</sub>), representing days with potentially high fire danger at the local scale</p></list-item><list-item>
      <p id="d2e1503">Number of days exceeding the mid-range FWI value (FWI<sub>fwsl</sub>), as an indicator of the duration of the fire season</p></list-item><list-item>
      <p id="d2e1516">30-year averaged annual maximum FWI (FWI<sub>max</sub>), as an indicator of the magnitude of the local extreme fire danger</p></list-item><list-item>
      <p id="d2e1529">30-year average of the annual peak 90 d mean FWI (FWI<sub>fs</sub>), representing the average fire weather conditions during the peak fire season.</p></list-item></list></p>
      <p id="d2e1541">The mid-range FWI value (FWI<sub>mid</sub>) is defined as the mean of the 30-year averaged annual minimum and maximum FWI during 1971–2000. It should be noted that despite the high spatial correlation among these metrics due to their dependence on the same climatic drivers, each of them captures a different dimension of fire weather danger from a process- and impact-based perspective.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS4">
  <label>2.2.4</label><title>Concatenation of the Reanalysis Data and Sensitivity Analysis</title>
      <p id="d2e1561">In order to account for the variation in local noon times across Europe, three different time zones were used to extract atmospheric fields at the corresponding local noon: UTC<inline-formula><mml:math id="M44" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1 for grids west of 0° longitude, UTC<inline-formula><mml:math id="M45" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 for those between 0  and 20° E longitudes and UTC+3 for grids east of 20° E longitude. These three regions were then concatenated into a single product to represent the original FWI calculation.</p>
      <p id="d2e1578">As many RCMs in the EURO-CORDEX framework do not provide sub-daily information, we searched for the best proxy input combination at daily resolution to approximate the typical noon-time FWI calculation. With this aim, hourly ERA5-Land data were first aggregated to daily resolution, including several combinations (a summary of the daily aggregated variable combinations tested in this study is provided in Table S1). Then, the FWI estimates derived from these combinations were compared with the original noon-time FWI calculation based on ERA5-Land. Specifically, the relative percentage bias in the 95th percentile of FWI was calculated at grid scale to evaluate the performance of each proxy input combination:

              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M46" display="block"><mml:mrow><mml:mi mathvariant="normal">Bias</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="normal">FWI</mml:mi><mml:mi mathvariant="normal">comb</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="normal">FWI</mml:mi><mml:mi mathvariant="normal">original</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi mathvariant="normal">FWI</mml:mi><mml:mi mathvariant="normal">original</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></disp-formula>

            where FWI<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">original</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> is the FWI 95th percentile value obtained from the original calculation scheme (noon-time variables), FWI<inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">comb</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> is the FWI 95th percentile value obtained using the input combination being tested. The time period covered is 1950 to 2023.</p>
      <p id="d2e1646">Finally, the combination resulting in the lowest absolute area-weighted average bias was selected (see Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/>). Since some daily resolution atmospheric fields may not be available for some models (e.g., minimum relative humidity), obtaining a sufficiently large model ensemble was also considered in the selection process.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS5">
  <label>2.2.5</label><title>Vapor Pressure Deficit</title>
      <p id="d2e1660">To shed light on the potential drivers of changes in extreme fire weather, we further investigated changes in VPD. VPD is defined as the difference between the saturation vapor pressure (<inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the actual vapor pressure (<inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and serves as an indicator of atmospheric aridity <xref ref-type="bibr" rid="bib1.bibx93" id="paren.94"/>. It is an essential metric for understanding how atmospheric conditions influence fuel dryness <xref ref-type="bibr" rid="bib1.bibx48" id="paren.95"/> and has been shown to be closely linked to wildfire activity, for example, in western U.S. forests <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx113" id="paren.96"/>. VPD can be calculated using temperature and relative humidity:

              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M51" display="block"><mml:mrow><mml:mi mathvariant="normal">VPD</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="normal">RH</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

            where RH is the relative humidity and <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the saturation vapor pressure as a function of the air temperature <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, calculated using the Clausius-Clapeyron equation:

              <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M54" display="block"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi>exp⁡</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><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:mi>T</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><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>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/></mml:mrow></mml:math></inline-formula>=<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mn mathvariant="normal">6.112</mml:mn></mml:mrow></mml:math></inline-formula> hPa is the saturation vapor pressure at the reference temperature <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mspace width="0.125em" linebreak="nobreak"/></mml:mrow></mml:math></inline-formula>=<inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">273.15</mml:mn></mml:mrow></mml:math></inline-formula> K, <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/></mml:mrow></mml:math></inline-formula>=<inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> J kg<sup>−1</sup> is the latent heat of vaporization for water and <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:msub><mml:mspace width="0.125em" linebreak="nobreak"/></mml:mrow></mml:math></inline-formula>=<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">461</mml:mn></mml:mrow></mml:math></inline-formula> J kg<sup>−1</sup> K<sup>−1</sup> is the specific gas constant for water vapor. We note that daily maximum temperature and mean relative humidity from the bias adjusted EURO-CORDEX simulations were used here to estimate projected changes in VPD, which leads to a possible overestimation <xref ref-type="bibr" rid="bib1.bibx48" id="paren.97"/>. However, the focus of this study is not on absolute VPD values, but rather on deviations from the baseline, which minimizes the implications of possible shortcomings.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS6">
  <label>2.2.6</label><title>Composite Analysis of Meteorological Conditions during Extreme Fire Weather Days</title>
      <p id="d2e1996">In order to characterize the average background conditions associated with the extreme fire weather days, we created composites of the meteorological conditions. To this end, we first calculated the 99th percentile of FWI for each grid cell and each warming level (reference period, <inline-formula><mml:math id="M66" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2  and <inline-formula><mml:math id="M67" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWLs) using the 30-year period corresponding to that climate state. Then, days exceeding this threshold during each warming level (FWI <inline-formula><mml:math id="M68" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> FWI<sup>99</sup>) were identified and used as a mask to extract the meteorological conditions that correspond to these extreme fire weather days. Finally, these meteorological fields were averaged over all exceedance days within each period and across the PRUDENCE regions for each model chain in the ensemble.</p>
      <p id="d2e2029">We created these composites for daily maximum temperature, 30 d accumulated antecedent precipitation, daily mean relative humidity, daily maximum wind speed, and VPD, as well as for FWI system sub-components (ISI and BUI), all of which are conditioned on days when FWI exceeds FWI<sup>99</sup>. Changes in these meteorological composites were then analyzed to diagnose the association between extreme fire weather and its drivers in a warming climate.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS7">
  <label>2.2.7</label><title>Significance and Robustness</title>
      <p id="d2e2049">To calculate trends in the historical period, the non-parametric Theil-Sen slope estimator was used, as it is relatively insensitive to outliers <xref ref-type="bibr" rid="bib1.bibx94 bib1.bibx100" id="paren.98"/>. The significance of these trends was tested using the non-parametric Mann-Kendall test <xref ref-type="bibr" rid="bib1.bibx62 bib1.bibx66" id="paren.99"/> at a significance level of <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e2070">To assess the robustness of the future climate change signal in the FWI indices, a criterion based on model agreement in both the significance and sign of the reported change was applied. Specifically, the climate change signal is considered robust only when at least 66 % of the models agree on both the sign and the statistical significance of the change <xref ref-type="bibr" rid="bib1.bibx54 bib1.bibx82" id="paren.100"/>. The significance of the simulated change was evaluated using a paired <inline-formula><mml:math id="M72" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>-test at a significance level of <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Sensitivity to Different Input Data</title>
      <p id="d2e2113">The typical FWI calculation is performed using the relevant atmospheric fields at local noon-time <xref ref-type="bibr" rid="bib1.bibx105" id="paren.101"/>. Since many RCMs do not provide subdaily scale information, daily fields need to be identified in such a way that they can replace the typical noon-time calculation with minimal bias. Figure <xref ref-type="fig" rid="F3"/> shows the distribution of the relative percentage bias in the 95th percentile of FWI calculated using the four different input combinations (given in Table S1) relative to the typical noon-time 95th percentile of FWI (FWI<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">original</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>) across Europe based on ERA5-Land reanalysis (note that the straight lines at 0  and 20° longitudes result from to the concatenation operation described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS4"/>). At the European scale, combinations that include mean relative humidity generally underestimate extreme fire weather danger (Fig. <xref ref-type="fig" rid="F3"/>a and  b), while those that include minimum relative humidity tend to overestimate it (Fig. <xref ref-type="fig" rid="F3"/>c and  d). Regarding the magnitude of the bias, using minimum relative humidity instead of mean relative humidity increases the absolute bias when the accompanying variable is maximum wind (Fig. <xref ref-type="fig" rid="F3"/>a and  c), whereas it decreases the bias when the accompanying variable is mean wind (Fig. <xref ref-type="fig" rid="F3"/>b and d).</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e2146">Relative percentage bias (%) of the 95th percentile of FWI calculated using the four daily input variable combinations <bold>(a)</bold> Comb-1, <bold>(b)</bold> Comb-2, <bold>(c)</bold> Comb-3, and <bold>(d)</bold> Comb-4, compared to the original noon-time FWI calculation based on ERA5-Land reanalysis data. Daily maximum temperature and daily accumulated precipitation are common to all combinations. The time period analyzed is 1950–2023. Areas classified as unburnable are shown in gray. Note that the artifacts near 0  and 20° longitudes result from the concatenation operation described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS4"/>. Details of the variables used in all combinations are given in Table S1.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f03.png"/>

        </fig>

      <p id="d2e2169">Since maximum temperature and daily precipitation are common in all combinations, using mean values for both relative humidity and wind leads to a substantial underestimation of FWI<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">original</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> with a mean absolute relative bias of 35.1 % (Fig. <xref ref-type="fig" rid="F3"/>b). In contrast, using daily extremes, i.e., minimum relative humidity and maximum wind speed, considerably overestimates FWI<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">original</mml:mi><mml:mn mathvariant="normal">95</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula>, resulting in a mean absolute relative bias of 43.9 % (Fig. <xref ref-type="fig" rid="F3"/>c). Thus, using the daily extreme for one variable and the mean for the other appears to offer a balanced compromise. The mean absolute biases for these combinations are similar: 21.2 % for Comb-1 and 20.8 % for Comb-4 (Fig. <xref ref-type="fig" rid="F3"/>a and d, respectively). Sensitivity tests show that this spatial pattern of bias between the different combinations does not depend on the 95th percentile threshold and is qualitatively similar across other parts of the distribution (Figs. S1–5 in the Supplement). Selecting Comb-4 would significantly reduce the number of models in the EURO-CORDEX ensemble, as minimum relative humidity is not an available output for most simulations. Therefore, Comb-1 is selected to calculate the FWI projections using the EURO-CORDEX ensemble, namely, daily maximum temperature, daily accumulated precipitation, mean relative humidity, and daily maximum wind speed. The remainder of the analysis in this study uses these atmospheric fields, for both ERA5-Land reanalysis and EURO-CORDEX models to ensure consistency.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Observed Climatology and Trends</title>
      <p id="d2e2211">To better understand the influence of ongoing climate change on fire danger in Europe, this section explores the climatology and trends of two FWI metrics, namely FWI<sub>mid</sub> and FWI<sub>95 d</sub>, for the period 1950–2023 based on ERA5-Land data. We begin with FWI<sub>mid</sub>, first presenting its climatology (Fig. <xref ref-type="fig" rid="F4"/>a), followed by the corresponding trends (Fig. <xref ref-type="fig" rid="F4"/>c). The FWI<sub>mid</sub> climatology displays a latitudinal gradient, with the highest values found around the Mediterranean Basin due to hot and dry summers, while the lower values are found in northern Europe (Fig. <xref ref-type="fig" rid="F4"/>a). The Iberian Peninsula and Turkey are mainly associated with FWI<sub>mid</sub> values in the range of moderate and high levels of fire risk according to the scale developed by <xref ref-type="bibr" rid="bib1.bibx89" id="text.102"/>. FWI<sub>mid</sub> shows a small but statistically significant positive trend in the central Iberian Peninsula, France, and Germany, with statistically significant trends observed in almost 30 % of the total burnable area across the study domain (Fig. <xref ref-type="fig" rid="F4"/>c). Most of Europe shows an increase in the intensity of fire weather conditions, but in eastern Europe and Scandinavia the trends are generally not statistically significant. It is also important to note that some of these regions are historically not prone to burning due to limiting factors such as climate or lack of ignition sources, as in parts of Norway (Fig. <xref ref-type="fig" rid="F1"/>b).</p>
      <p id="d2e2287">FWI<sup>95</sup> climatology (Fig. <xref ref-type="fig" rid="F4"/>b) displays the highest values in the Mediterranean Basin, with a latitudinal gradient across Europe except for lower values in mountainous regions. FWI<sup>95</sup> values above 38 indicate very high fire danger <xref ref-type="bibr" rid="bib1.bibx89" id="paren.103"/>, but this relationship varies regionally: higher values (<inline-formula><mml:math id="M85" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 50) usually signal extreme danger in warm and dry climates, while lower values (<inline-formula><mml:math id="M86" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 25) may indicate similar danger in cooler and moister climates <xref ref-type="bibr" rid="bib1.bibx65" id="paren.104"/>. Therefore, FWI<sub>mid</sub> and FWI<sup>95</sup> should be interpreted with caution, taking into account the local climate and biome.</p>
      <p id="d2e2350">Regarding the trends in FWI<sub>95 d</sub> (Fig. <xref ref-type="fig" rid="F4"/>d), more than 36 % of all burnable areas exhibit a significant trend, almost all of which indicate an increase. Notable positive trends were observed in the Iberian Peninsula, France, Germany and Ukraine, with trends exceeding 3 d decade<sup>−1</sup> in some areas, corresponding to more than 20 additional days of extreme fire weather over the 74-year study period. Some areas of the Iberian Peninsula show trends above 5 d decade<sup>−1</sup>, amounting to almost 40 additional days of high fire danger during the study period. In contrast, a small region in the eastern Mediterranean shows a statistically significant negative trend, while parts of Scandinavia and the United Kingdom show either no trend or negative but non-significant changes. Other fire-prone regions, including Italy, the Balkans, and the eastern Mediterranean, show mixed and generally non-significant trends, reflecting large interannual variability in extreme fire weather conditions. We note that an analysis focusing on more recent decades (e.g., 1980–2023) results in a much higher proportion of significant trends, with up to 61 % of the burnable land area exhibiting statistically significant trends (results not shown).</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e2395"><bold>(a)</bold> Observed climatology of the mid-range FWI (FWI<sub>mid</sub>) and <bold>(b)</bold> the 95th percentile FWI (FWI<sup>95</sup>) during the analysis period of 1950–2023 based on ERA5-Land reanalysis data. <bold>(c)</bold> Observed trends (decade<sup>−1</sup>) in FWI<sub>mid</sub> and <bold>(d)</bold> in the number of days per yr when FWI exceeds the 95th percentile (FWI<sub>95 d</sub>) relative to the reference period 1971–2000 (days decade<sup>−1</sup>) based on ERA5-Land reanalysis data. Trends are calculated using the Theil-Sen slope estimator. Areas without stippling indicate regions where the trend is statistically significant (<inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>), according to the Mann-Kendall test. The analysis covers the period 1950–2023. Areas classified as unburnable are shown in gray. Note that a single colorbar is used for both trend panels, although the units differ.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Evaluation of Model Performance after Bias Adjustment</title>
      <p id="d2e2500">GCMs are known to exhibit systematic biases for various reasons, and RCMS often inherit these biases because they use GCMs as boundary conditions for downscaling and may also introduce their own biases <xref ref-type="bibr" rid="bib1.bibx43" id="paren.105"/>. Figure <xref ref-type="fig" rid="F5"/> evaluates the bias in the 95th percentile of the FWI for the EURO-CORDEX ensemble median before and after bias adjustment, relative to the ERA5-Land reanalysis. It should be noted that the time period for the evaluation here is the same as the calibration period for bias adjustment (1971–2000). Although the performance of bias adjustment methods is typically evaluated using a separate validation period <xref ref-type="bibr" rid="bib1.bibx21" id="paren.106"><named-content content-type="pre">e.g.,</named-content></xref>, we focus on evaluating model performance during the calibration period as the historical simulations are not long enough to allocate a separate validation period for most of the EURO-CORDEX models, considering that 30 years of data have already been used for calibration. In addition, it is important to note that a cross-validation strategy may not always provide reliable results when evaluating the bias adjustment performance, as the internal variability of the climate system can dominate the differences between calibration and validation periods, potentially leading to misleading evaluations, particularly in mid-latitudes <xref ref-type="bibr" rid="bib1.bibx67" id="paren.107"/>.</p>
      <p id="d2e2516">Adjusting the biases of the individual model input fields prior to the calculation of the FWI results in a significant reduction in the bias of the FWI ensemble median (Fig. <xref ref-type="fig" rid="F5"/>). The spatial mean of the absolute relative percentage bias in the 95th percentile is 80 % before adjustment (Fig. <xref ref-type="fig" rid="F5"/>a), with particularly large biases found south of the 50° latitude. After bias adjustment, this spatial mean bias of the ensemble median is reduced to less than 9 % (Fig. <xref ref-type="fig" rid="F5"/>b), with significant improvements observed in regions where the raw ensemble median previously exhibited large biases. Sensitivity tests show that the observed spatial pattern of bias reduction is robust and largely independent of the choice of the 95th percentile threshold and exhibits qualitatively similar behavior across other parts of the distribution (Figs. S6–10). However, some small areas still exhibit high biases, especially mountainous regions, such as parts of the Alps, Carpathians, and Caucasus Mountains. However, it should be noted that the FWI values over the mountainous regions are already very low, so even large percentage biases are also usually low in terms of absolute values in these regions. For the purposes of this study, the substantial improvement in model performance by adjusting the input fields with the univariate QDM approach is considered sufficient; hence, the bias-adjusted ensemble is used for the rest of the study.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e2527">Relative percentage bias (%) in the 95th percentile of FWI for EURO-CORDEX ensemble median relative to ERA5-Land data during 1971–2000, based on <bold>(a)</bold> raw (unadjusted) and <bold>(b)</bold> bias-adjusted simulations. Areas classified as unburnable are shown in gray.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f05.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Projections of Extreme Fire Weather in Europe</title>
      <p id="d2e2550">As significant trends in extreme fire weather have been observed in many regions of Europe, and since all regions are projected to experience warmer summer climates, with a particular tendency towards increased drying in the southern and western regions <xref ref-type="bibr" rid="bib1.bibx7" id="paren.108"/>, it is reasonable to expect further changes in a warming climate. Figure <xref ref-type="fig" rid="F6"/> shows the patterns of the frequency-based FWI metrics (left panels for FWI<sub>fwsl</sub> and right panels for FWI<sub>95 d</sub>) over Europe during the reference period (1971–2000) and the changes relative to the reference period at 2 and 3 °C GWL based on the ensemble median of 33 bias-adjusted EURO-CORDEX models. The climatological patterns of FWI<sub>fwsl</sub> (Fig. <xref ref-type="fig" rid="F6"/>a) show longer fire seasons in southern Europe, particularly in the Iberian Peninsula, southern Italy, Greece and Turkey, with more than 60 d yr<sup>−1</sup>. In contrast, central and northern Europe experience shorter fire seasons. Since these values may seem lower than expected, it is important to distinguish between different methods for calculating the duration of the fire season. <xref ref-type="bibr" rid="bib1.bibx115" id="text.109"/> define the fire season based on a temperature threshold, and it is used for overwintering the DC <xref ref-type="bibr" rid="bib1.bibx71 bib1.bibx84" id="paren.110"/>. However, this definition may lead to an overestimation of fire season length, especially in southern Europe due to warmer temperatures throughout the yr. In contrast, <xref ref-type="bibr" rid="bib1.bibx57" id="text.111"/> define FWI<sub>fwsl</sub> as the number of days when FWI exceeds its mid-range value. Here, the definition of <xref ref-type="bibr" rid="bib1.bibx57" id="text.112"/> is followed for FWI<sub>fwsl</sub>, as in some other studies <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx58" id="paren.113"/>. However, this approach possibly underestimated the actual FWI<sub>fwsl</sub> in some regions, because overwintering the DC reduces the number of days with an available FWI value throughout the yr due to the condition of <xref ref-type="bibr" rid="bib1.bibx115" id="text.114"/>.</p>
      <p id="d2e2650">The projected changes in FWI<sub>fwsl</sub> at 2 °C and 3 °C GWLs relative to the reference period are shown in Fig. <xref ref-type="fig" rid="F6"/>c and  e, respectively. At 2 °C, robust increases in FWI<sub>fwsl</sub> are already evident in some regions, with a magnitude of up to 100 % in areas like parts of the Balkans, but the larger changes are mostly limited to regions with smaller climatological values. The increase in FWI<sub>fwsl</sub> becomes more widespread and intense at 3 °C, particularly in France and the Balkans, with a relative increase exceeding 150 %. Almost all regions show positive changes in FWI<sub>fwsl</sub> at both GWLs (except for a small area in northern Poland at 2 °C). The projected mean relative change in FWI<sub>fwsl</sub> for the grids where the models agree on both the sign and significance of the change almost doubles between the two GWLs: 52 % at 2 °C and 94 % at 3 °C. The signal is largely confined to regions south of 50° latitude, with a robust signal simulated in 25 % and 48 % of the burnable land area, at 2 °C and 3 °C, respectively.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e2703">Patterns of frequency-based extreme fire weather metrics and their projected relative changes in Europe based on the ensemble median of 33 bias-adjusted EURO-CORDEX models. The left panels show the fire weather season length (FWI<sub>fwsl</sub>) and the right panels show the number of days per yr exceeding the 95th percentile FWI (FWI<sub>95 d</sub>) relative to the reference period (1971–2000). <bold>a, b)</bold> Reference period patterns with a separate colorbar shown below, <bold>c, d)</bold> changes relative to the reference period at <inline-formula><mml:math id="M113" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C GWL and <bold>e, f)</bold> changes relative to the reference period at <inline-formula><mml:math id="M114" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWL. Note that the reference period is already 0.46 °C warmer than the preindustrial period. Areas without stippling indicate regions where at least 66 % of the models project statistically significant changes according to a <inline-formula><mml:math id="M115" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>-test (<inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and agree on the sign of change. Areas classified as unburnable are shown in gray. Absolute changes are shown in Fig. S11 to facilitate interpretation in regions where relative changes may be amplified by climatologically low baseline values.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f06.jpg"/>

        </fig>

      <p id="d2e2778">The right column of Fig. <xref ref-type="fig" rid="F6"/> shows the number of days per yr that exceed the 95th percentile FWI (FWI<sub>95 d</sub>) during the reference period (Fig. <xref ref-type="fig" rid="F6"/>b), along with the relative changes compared to the reference period at 2 °C (Fig. <xref ref-type="fig" rid="F6"/>d) and 3 °C (Fig.  <xref ref-type="fig" rid="F6"/>f) GWLs. Here, it is important to note that the spatial distribution of FWI<sub>95 d</sub> during the reference period would be nearly uniform with around 18 d yr<sup>−1</sup> across the domain if FWI was calculated continuously, since the 95th percentile is calculated locally for each grid. However, this is not the case here, as overwintering of the DC interrupts the continuous FWI calculation. Therefore, the latitudinal differences in FWI<sub>95 d</sub> are a natural consequence of this calculation. More days exceed the local 95th percentile at lower latitudes, primarily because the fire season is longer as defined by <xref ref-type="bibr" rid="bib1.bibx115" id="text.115"/>. In the Iberian Peninsula and some regions in southern Europe, there are about 18 d yr<sup>−1</sup> of FWI<sub>95 d</sub>, indicating that the fire season defined by the temperature threshold endures almost all yr.</p>
      <p id="d2e2869">The projected changes in FWI<sub>95 d</sub> relative to the reference period at 2 °C and 3 °C GWLs are shown in Fig. <xref ref-type="fig" rid="F6"/>d and  f. At 2 °C, the changes are mainly confined to southern Europe, with only 23 % of the total burnable land area in the domain exhibiting robust signals (Fig. <xref ref-type="fig" rid="F6"/>d). In contrast, at 3 °C, significant and robust signals are projected to extend into central Europe, covering 46 % of the total burnable area (Fig. <xref ref-type="fig" rid="F6"/>f). In addition, the strength of the signal becomes much more pronounced at 3 °C, with relative increases exceeding 150 % in many regions, such as the Iberian Peninsula, southern France, the Balkans, and Turkey. Even regions with historically low frequencies of extreme fire weather, such as northern Europe, show increases of up to 50 %. However, these increases are not statistically significant or model agreement is not established. In areas where the change signal is robust, the mean relative increase in FWI<sub>95 d</sub> is 97 % and 153 %, respectively, at 2 and 3 °C GWLs. Overall, a general increase in the frequency of fire weather conditions is projected across Europe, with the magnitude and spatial extent of the changes becoming much more pronounced at 3 °C compared to 2 °C. However, robust changes are still mainly limited to areas south of 50 °C latitude even at 3 °C.</p>
      <p id="d2e2904">In addition to projections of the frequency of extreme fire weather, it is also important to quantify the projected changes in the magnitude of extreme fire weather. Figure <xref ref-type="fig" rid="F7"/> shows the patterns of the magnitude-based FWI metrics (left panels for FWI<sub>fs</sub> and right panels for FWI<sub>max</sub>) over Europe during the reference period (1971–2000) and the changes relative to the reference period at 2 °C and 3 °C GWLs based on the ensemble median of 33 bias-adjusted EURO-CORDEX models. Similar to frequency metrics, a latitudinal gradient is apparent for FWI<sub>fs</sub>, with higher values concentrated mainly in southern Europe due to hot and dry summer conditions (Fig. <xref ref-type="fig" rid="F7"/>a). In regions such as the Iberian Peninsula, southern Italy, Greece, and Turkey FWI<sub>fs</sub> values exceed 30, approaching the very high fire danger threshold of 38, as accepted by <xref ref-type="bibr" rid="bib1.bibx89" id="text.116"/>.</p>
      <p id="d2e2951">The projections show a minor relative increase in FWI<sub>fs</sub> at 2 °C GWL across Europe, with the exception of regions such as Poland and northern Scandinavia (Fig. <xref ref-type="fig" rid="F7"/>c). However, many areas still lack robustness, with only 22 % of the burnable land area is projected to show robust signals. At <inline-formula><mml:math id="M130" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C, FWI<sub>fs</sub> is projected to become more widespread and intense, following the same pattern seen in frequency-based metrics (Fig. <xref ref-type="fig" rid="F7"/>e). It is projected to increase by more than 50 % (with robust signals) not only in southern and eastern Europe, but also in regions that historically exhibited lower fire danger, such as eastern France. The percentage of burnable land area with model agreement also increases to 41 % at 3 °C. The spatially averaged relative increase in FWI<sub>fs</sub> for regions with model agreement on robustness of the change signal is also projected to increase as the GWL increases: 25 % at 2 °C and 47 % at 3 °C.</p>
      <p id="d2e2993">The climatological distribution of FWI<sub>max</sub> displays higher values exceeding 40 in southern Europe and lower values, usually below 20 in central to northern Europe (Fig. <xref ref-type="fig" rid="F7"/>b). Mountainous regions, such as the Alps and Carpathians, exhibit very low FWI<sub>max</sub> values, reflecting their colder and moister climates compared to the surrounding areas. In southern Europe, regions like the Iberian Peninsula and Turkey have FWI<sub>max</sub> values greater than 50, indicating that these areas experience extreme fire weather conditions annually on average.</p>
      <p id="d2e3025">The projected changes in FWI<sub>max</sub> at 2 and 3 °C GWLs relative to the reference period are shown in Fig. <xref ref-type="fig" rid="F7"/>d and f, respectively. At 2 °C, the simulated positive changes are relatively small (around 10 %–20 %). Central and northern Europe show spatial variability, including negative changes in some regions (e.g., Poland), although these are not robust signals (Fig. <xref ref-type="fig" rid="F7"/>d). Only 8 % of the burnable land area shows model agreement on the direction and significance of the change at 2 °C, and these areas are mostly limited to regions with very low climatological FWI<sub>max</sub> values. In contrast, at 3 °C, the percentage of burnable land area where the majority of models project robust climate change signals increases sharply to 40 % (Fig. <xref ref-type="fig" rid="F7"/>f). However, areas with higher relative changes are still primarily the regions with low climatological values (e.g., mountainous regions), with the exception of some parts of Southern Europe, such as Italy and the Balkans, where projected increases range from 20 % to 40 %. Overall, in regions where change signal is robust, the simulated mean increase in FWI<sub>max</sub> is 26 % and 33 % relative to the reference period, respectively, at 2 and 3 °C.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e3065">Patterns of magnitude-based extreme fire weather metrics and their projected relative changes in Europe based on the ensemble median of 33 bias-adjusted EURO-CORDEX models. The left panels show the annual peak 90 d average FWI (FWI<sub>fs</sub>) and the right panels show the annual maximum FWI (FWI<sub>max</sub>). <bold>(a, b)</bold> Reference period (1971–2000) patterns with a separate colorbar shown below, <bold>(c, d)</bold> changes relative to the reference period at <inline-formula><mml:math id="M141" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C GWL and <bold>(e, f)</bold> changes relative to the reference period at <inline-formula><mml:math id="M142" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWL. Note that the reference period is already 0.46 °C warmer than the preindustrial period. Areas without stippling indicate regions where at least 66 % of the models project statistically significant changes according to a <inline-formula><mml:math id="M143" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>-test (<inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and agree on the sign of change. Areas classified as unburnable are shown in gray. Absolute changes are shown in Fig. S12 to facilitate interpretation in regions where relative changes may be amplified by climatologically low baseline values.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f07.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS5">
  <label>3.5</label><title>Sub-European Regions</title>
      <p id="d2e3144">In this section section, we show the same fire weather metrics analyzed throughout the study (FWI<sub>95 d</sub>, FWI<sub>fwsl</sub>, FWI<sub>max</sub>, FWI<sub>fs</sub>), but aggregate and average them over the PRUDENCE regions to highlight differences between the European subregions and show the spread across the model ensemble. Using the absolute values, we also aim to provide context for the relative changes presented in Sect. <xref ref-type="sec" rid="Ch1.S3.SS4"/>. The results are displayed as box plots for each PRUDENCE region for the reference period (1971-2000), and at 2  and 3 °C GWLs (Fig. <xref ref-type="fig" rid="F8"/>). The regions are ordered in a way that roughly corresponds to the latitude-longitude orientation (North-West to South-East) of the regions.</p>
      <p id="d2e3192">FWI<sub>95 d</sub> shows a quasi-uniform distribution across models in all PRUDENCE regions for the reference period, due to the definition of the metric and the bias adjustment of temperature, which effectively determines the start and end of the fire season based on the temperature-threshold used for overwintering DC (Fig. <xref ref-type="fig" rid="F8"/>a). Under both warming scenarios, the median FWI<sub>95 d</sub> is projected to increase across all regions with a stronger signal at 3 °C. In the Iberian Peninsula, for example, FWI<sub>95 d</sub> is projected to increase rapidly from a median of <inline-formula><mml:math id="M152" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 17 d yr<sup>−1</sup> during 1971–2000 to 31 d yr<sup>−1</sup> at 2 °C and to 46 d yr<sup>−1</sup> at 3 °C (Fig. <xref ref-type="fig" rid="F8"/>a). A similar trend is projected for France, with the median increasing from 14.5 d yr<sup>−1</sup> during 1971–2000 to more than 23 d yr<sup>−1</sup> at 2 °C and to 35 d yr<sup>−1</sup> at 3 °C. In some regions, such as Eastern Europe, the model spread is large, with some models projecting a negative change, and some projecting a very extreme positive change. The model agreement is stronger in southern European regions (IP, MD, TR), where all models project a positive trend under both 2 and 3 °C GWLs. In addition, the spread among models increases from 2 °C to 3 °C in all regions, indicating a growing uncertainty with higher levels of warming.</p>
      <p id="d2e3319">There is a clear regional separation in both the reference period and projected values of FWI<sub>fwsl</sub>, with southern European regions (IP, MD, TR) showing higher levels of fire danger than the rest of Europe (Fig. <xref ref-type="fig" rid="F8"/>b). However, a positive change signal is evident across almost all regions, especially at 3 °C GWL. In the Alps, a region historically characterized by shorter fire seasons, the median FWI<sub>fwsl</sub> is projected to more than double: from 14.4 d yr<sup>−1</sup> during 1971–2000, to almost 22 d yr<sup>−1</sup> at 2 °C, and to more than 31 d yr<sup>−1</sup> at 3 °C. The Iberian Peninsula is projected to experience the highest absolute increase in multi-model median FWI<sub>fwsl</sub>, rising from 43 d yr<sup>−1</sup> during 1971–2000 to a projected 64 d yr<sup>−1</sup> at 2 °C and almost 78 d yr<sup>−1</sup> at 3 °C.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e3427">Model spread of FWI metrics, spatially aggregated and averaged over the PRUDENCE regions, for the reference period (blue), <inline-formula><mml:math id="M168" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C GWL (orange), and <inline-formula><mml:math id="M169" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWL (red) based on the bias-adjusted EURO-CORDEX ensemble for <bold>a)</bold> FWI<sub>95 d</sub>, <bold>b)</bold> FWI<sub>fwsl</sub>, <bold>c)</bold> FWI<sub>max</sub>, <bold>d)</bold> FWI<sub>fs</sub>. Whiskers in the boxplots represent 1.5 times the inter-quartile range of the ensemble, with circles denoting outliers. BI <inline-formula><mml:math id="M174" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> British Isles, SC <inline-formula><mml:math id="M175" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Scandinavia, FR <inline-formula><mml:math id="M176" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> France, ME <inline-formula><mml:math id="M177" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula>  Mid-Europe, AL <inline-formula><mml:math id="M178" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Alps, EA <inline-formula><mml:math id="M179" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Eastern Europe, IP <inline-formula><mml:math id="M180" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Iberian Peninsula, MD <inline-formula><mml:math id="M181" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Mediterranean, TR <inline-formula><mml:math id="M182" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> Turkey.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f08.png"/>

        </fig>

      <p id="d2e3568">A clear latitudinal gradient is also observed in the magnitude of FWI<sub>max</sub> during the reference period and at both 2 °C and 3 °C GWLs with southern European regions exhibiting higher fire danger due to their warm and dry summer climates (Fig. <xref ref-type="fig" rid="F8"/>c). The main exception to this latitudinal pattern is the Alps, which exhibits lower values due to its colder and moister climate conditions. Overall, the median FWI<sub>max</sub> is projected to increase consistently across all regions as the GWL increases. However, the projected relative changes in FWI<sub>max</sub> (Fig. <xref ref-type="fig" rid="F8"/>c), a magnitude-based metric, are not as pronounced as those seen in frequency-based metrics (Fig. <xref ref-type="fig" rid="F8"/>a and  b). The Mediterranean, the Iberian Peninsula, and Turkey clearly stand out from other regions. For instance, Turkey shows a simulated median FWI<sub>max</sub> of 49 during 1971–2000, which is projected to increase to 54.6 at 2 °C and to 58 at 3 °C.</p>
      <p id="d2e3614">The FWI<sub>fs</sub> (Fig. <xref ref-type="fig" rid="F8"/>d) is also projected to follow a similar pattern to FWI<sub>max</sub>. However, the distribution ranges for FWI<sub>fs</sub> are narrower than those for FWI<sub>max</sub>, particularly in northern and central European regions due to the time averaging. The intensity of prolonged fire weather, as represented by FWI<sub>fs</sub>, is projected to increase in all regions. For example, the median FWI<sub>fs</sub> in the Mediterranean is projected to increase from 15 during 1971–2000 to 18 and 20 at 2 and 3 °C GWLs, respectively.</p>
      <p id="d2e3674">In summary, all four fire weather metrics are projected to increase in all regions with increasing temperature, and more pronounced changes are expected at 3 °C GWL compared to 2 °C. In general, southern European regions (IP, MED, TR) are projected to experience more intense and prolonged extreme fire weather conditions, consistent with their baseline climatologies of dry and warm summers. Overall, the relative change signals are stronger for the frequency-based metrics (FWI<sub>95 d</sub> and FWI<sub>fwsl</sub>) than for the magnitude-based metrics (FWI<sub>max</sub> and FWI<sub>fs</sub>). A clear latitudinal gradient is also observed, with southern European regions projected to experience more severe and frequent fire weather conditions. Furthermore, the ensemble spread increases from 2  to 3 °C GWL, particularly for the frequency-based metrics, indicating greater uncertainty at higher warming levels.</p>
</sec>
<sec id="Ch1.S3.SS6">
  <label>3.6</label><title>Evaluation of the Potential Drivers</title>
      <p id="d2e3725">Given the projected changes in extreme fire weather conditions across Europe, it is important to explain possible drivers. To provide insights into this question, we examine the two main subcomponents of FWI: BUI, which represents the effects of longer-term atmospheric conditions on fuel dryness, and ISI, which reflects the influence of short-term atmospheric conditions, namely the role of wind patterns and FFMC <xref ref-type="bibr" rid="bib1.bibx85" id="paren.117"/>. Figure <xref ref-type="fig" rid="F9"/> illustrates FWI as a function of ISI and BUI across PRUDENCE regions, based on spatially aggregated fields from the bias-adjusted EURO-CORDEX models. The ISI–BUI pairs correspond to the averaged values for the days when FWI exceeds its 99th percentile during the reference period (1971–2000), as well as at 2  and 3 °C GWLs for each model in the ensemble.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e3735">FWI as a function of ISI and BUI, with theoretical FWI contours overlaid for the PRUDENCE regions. ISI and BUI composite averages are shown for days when the FWI exceeds its 99th percentile. Blue squares denote the reference period (1971–2000), green triangles correspond to <inline-formula><mml:math id="M197" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C GWL, and red circles represent <inline-formula><mml:math id="M198" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWL. All values are spatially aggregated and area-weighted averaged over the PRUDENCE regions, namely: <bold>(a)</bold> British Isles, <bold>(b)</bold> Scandinavia, <bold>(c)</bold> France, <bold>(d)</bold> Mid-Europe, <bold>(e)</bold> Alps, <bold>(f)</bold> Eastern Europe, <bold>(g)</bold> Iberian Peninsula, <bold>(h)</bold> Mediterranean, and <bold>(i)</bold> Turkey. Each value corresponds to a bias adjusted EURO-CORDEX model; crosses indicate ensemble medians.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f09.png"/>

        </fig>

      <p id="d2e3786">As global warming increases, there is a projected shift in BUI towards higher values in all regions (Fig. <xref ref-type="fig" rid="F9"/>). However, the signals in BI and SC are mixed, with a slight tendency towards higher fire danger (Fig. <xref ref-type="fig" rid="F9"/>a and  b). In FR, ME, AL and EA regions, there is a notable shift in BUI, along with an increase in ISI, both of which contribute to the resulting increase FWI (Fig. <xref ref-type="fig" rid="F9"/>c–f). In particular in France, the median BUI is projected to increase by almost 50 % at 3 °C GWL relative to the reference period, while ISI is projected to increase only by around 25 %, which is an indication of the worsening of longer-term fuel drying. The increase in BUI is also apparent in the southern European regions (Fig. <xref ref-type="fig" rid="F9"/>g–i). However, this does not directly translate into a significant increase in FWI in these regions because the contribution of BUI to FWI saturates at higher BUI values, consistent with the principle that there is a limit to the amount of fuel that can be used in fires <xref ref-type="bibr" rid="bib1.bibx105" id="paren.118"/>. Instead, in these regions, the projected increase in FWI is driven by a projected increase in ISI values, which may result from an increased surface layer dryness (reflected by FFMC) or stronger winds.</p>
      <p id="d2e3801">To disentangle the contributions of wind speed and dryness conditions, Fig. <xref ref-type="fig" rid="F10"/> shows VPD plotted against maximum wind speed across PRUDENCE regions. The VPD-wind speed pairs correspond to the averaged values for the days when FWI exceeds its 99th percentile during the reference period (1971–2000), as well as at 2  and 3 °C GWLs for each model in the EURO-CORDEX ensemble. The medians of maximum wind speeds are projected to either decrease or remain largely unchanged across all PRUDENCE regions, except in southern Europe, where a very slight increase (less than 2 %) is projected, but likely not significant. In contrast, the median VPD, which reflects the thermodynamic effects of temperature and relative humidity through atmospheric drying, is projected to increase across all regions, with particularly strong increases in central and southern Europe. In southern European regions, the projected increase in the median VPD on days when FWI exceeds its 99th percentile at 3 °C GWL relative to the reference period is almost 40 %, with some models projecting changes greater than 70 % (Fig. <xref ref-type="fig" rid="F10"/>g–i).</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e3810">VPD (hPa) vs. maximum wind speed (km/h) composites for the PRUDENCE regions. VPD and maximum wind speed averages are shown for days when the FWI exceeds its 99th percentile. Blue squares denote the reference period (1971–2000), green triangles correspond to <inline-formula><mml:math id="M199" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C GWL, and red circles represent <inline-formula><mml:math id="M200" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWL. All values are spatially aggregated and area-weighted averaged over the PRUDENCE regions, namely <bold>(a)</bold> British Isles, <bold>(b)</bold> Scandinavia, <bold>(c)</bold> France, <bold>(d)</bold> Mid-Europe, <bold>(e)</bold> Alps, <bold>(f)</bold> Eastern Europe, <bold>(g)</bold> Iberian Peninsula, <bold>(h)</bold> Mediterranean, and <bold>(i)</bold> Turkey. Each value corresponds to a bias adjusted EURO-CORDEX model; crosses indicate ensemble medians. Note that the absolute VPD values are likely overestimated, as they are calculated using daily maximum temperature and daily mean relative humidity.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f10.png"/>

        </fig>

      <p id="d2e3861">To further analyze the key drivers responsible for changes in fire weather extremes, we calculate the simulated changes in 30 d accumulated antecedent precipitation conditioned on days with extreme FWI values (Fig. S13). There is a trend towards decreasing precipitation totals as GWL increases across regions for these conditional days in the ensemble median (except for Scandinavia). The decreasing precipitation totals seem more critical for regions such as France, in contrast to southern Europe, where the baseline climatology during extreme fire weather days is already very dry. Therefore, further drying in these regions might not increase fire weather danger as much as increases in temperature, as also reported in <xref ref-type="bibr" rid="bib1.bibx35" id="text.119"/>. However, to better discern the role of precipitation in intensifying fire weather extremes, a more targeted analysis is needed, as there is no model agreement in the change signal in many regions (e.g., Eastern Europe).</p>
      <p id="d2e3867">These results suggest that projected changes in FWI in southern Europe are primarily associated with an increase in fuel aridity due to amplified atmospheric moisture demand rather than changes in wind speeds. This may also indicate that the projected changes in ISI in southern Europe (Fig. <xref ref-type="fig" rid="F9"/>) are largely influenced by increased surface layer fuel dryness (FFMC), rather than wind speed. Precipitation is also an important contributor in regions such as France, but its role is more difficult to assess in many other regions due to the higher uncertainty.</p>
      <p id="d2e3872">In addition to the distribution of model statistics across the PRUDENCE regions, we also present the spatial pattern of the ensemble median changes in the composites of the variables of interest at 2  and 3 °C GWLs relative to the reference period conditioned on days when FWI exceeds its 99th percentile (Fig. <xref ref-type="fig" rid="F11"/>). The pattern of changes in extreme FWI (mean FWI on days when FWI <inline-formula><mml:math id="M201" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> FWI<sup>99</sup>) shows a high spatial correlation with changes in VPD on these days, higher than the individual correlations with maximum temperature and relative humidity. Specifically, the ensemble median field correlation between changes in VPD and FWI composites is 0.85 at 2 °C GWL and 0.87 at 3 °C GWL, with ensemble ranges of 0.51–0.91 and 0.71–0.91, respectively (at 2 °C, only two models show correlations below 0.67). The decline in 30 d accumulated precipitation is also evident in regions such as France and suggests that these events occur under drier antecedent conditions, especially at 3 °C GWL, but this is less relevant for southern regions. Changes in maximum wind speed are weak and spatially heterogeneous. Overall, the northward expansion of more extreme fire weather danger in a warming climate in Europe is associated with stronger atmospheric moisture demand through increasing VPD (i.e., increasing temperature and/or decreasing relative humidity), with compounding effects from declining precipitation in regions such as France. However, these relationships should be interpreted with caution, as they represent spatial co-variations rather than formal attribution statements.</p>

      <fig id="F11" specific-use="star"><label>Figure 11</label><caption><p id="d2e3896">Spatial patterns of the composites based on the ensemble median of 33 bias-adjusted EURO-CORDEX models, shown as changes relative to the reference period (1971–2000) at <inline-formula><mml:math id="M203" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 °C (left panels) and <inline-formula><mml:math id="M204" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>3 °C GWLs (right panels). Composites are created by averaging delta changes of <bold>(a, b)</bold> FWI, <bold>(c, d)</bold> VPD (hPa), <bold>(e, f)</bold> daily maximum temperature (°C), <bold>(g, h)</bold> daily mean relative humidity (%), <bold>(i, j)</bold> 30 d antecedent accumulated precipitation (mm), and <bold>(k, l)</bold> daily maximum wind speed (km h<sup>−1</sup>) on days when FWI exceeds its 99th percentile.</p></caption>
          <graphic xlink:href="https://esd.copernicus.org/articles/17/929/2026/esd-17-929-2026-f11.jpg"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Summary and Discussion</title>
      <p id="d2e3959">This study assesses how extreme fire weather in Europe is influenced by recent and future climate change. With this aim, it also evaluates the performance of EURO-CORDEX simulations in representing the extreme fire weather and the potential improvements offered by bias adjustment with QDM. The main results are as follows: <list list-type="order"><list-item>
      <p id="d2e3964">The most suitable combination of daily input variables to approximate typical noon-time FWI includes maximum temperature, accumulated precipitation, mean relative humidity, and maximum wind speed. These atmospheric fields were selected on the basis of their relatively lower bias in the resulting FWI calculations and broader model availability in the EURO-CORDEX ensemble.</p></list-item><list-item>
      <p id="d2e3968">An analysis of the historical period (1950–2023) based on ERA5-Land reanalysis data revealed a clear latitudinal gradient in extreme fire weather, with more severe conditions occurring in southern Europe. A positive trend in the frequency and magnitude of extreme fire weather has been observed since the 1950s across many regions, such that 30 % and 36 % of the burnable land area exhibited a significant trend in FWI<sub>mid</sub> and FWI<sub>95 d</sub>, respectively. The majority of the significant trends for both metrics were concentrated in the Iberian Peninsula, Central Europe, and Ukraine.</p></list-item><list-item>
      <p id="d2e3994">As the raw model outputs from the EURO-CORDEX framework have systematic biases <xref ref-type="bibr" rid="bib1.bibx109" id="paren.120"/>, the input fields were bias adjusted before calculating the FWI. The bias adjustment of the input fields with QDM significantly reduced the resulting FWI bias during the calibration period. Bias relative to the ERA5-Land for the 95th percentile of FWI in the EURO-CORDEX ensemble median is reduced from 80 % to below 9 %.</p></list-item><list-item>
      <p id="d2e4001">EURO-CORDEX future projections show that extreme fire weather in Europe is projected to become more widespread, more frequent, and more intense with increasing GWLs, consistent with previous assessments <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx35 bib1.bibx50 bib1.bibx58" id="paren.121"/>. Relative increases in frequency-based extreme fire weather metrics are larger than those for magnitude-based metrics. The spatial extent of robust signals is projected to nearly double at 3 °C GWL compared to 2 °C for three of the four metrics. For FWI<sub>max</sub>, the spatial extent at 3 °C is five times as large as that at 2 °C. It should be noted that extreme fire weather events may still occur even under a 2 °C GWL <xref ref-type="bibr" rid="bib1.bibx11" id="paren.122"/>.</p></list-item><list-item>
      <p id="d2e4020">A latitudinal gradient is also evident in the projected fire weather danger, where southern European regions (the Iberian Peninsula, the Mediterranean and Turkey) are expected to experience longer and more intense fire weather conditions. The frequency and magnitude of extreme fire weather are also projected to increase in regions such as France, the Alps, Eastern Europe, and Mid-Europe, particularly at 3 °C GWL.</p></list-item><list-item>
      <p id="d2e4024">The subcomponents of the FWI system, namely the BUI and the ISI are projected to increase in most regions, although with a relatively smaller increase for ISI. In regions such as France and Eastern Europe, contribution to the increase in FWI is shared between BUI and ISI. However, since the influence of BUI on FWI saturates beyond a certain threshold <xref ref-type="bibr" rid="bib1.bibx105" id="paren.123"/> and southern European regions already exhibit very high BUI values, changes in ISI emerge as the dominant driver of the increase in FWI in these regions.</p></list-item><list-item>
      <p id="d2e4031">The relevance of projected changes in wind speed is marginal, whereas VPD is projected to increase across all regions. This indicates that thermodynamic factors, through atmospheric drying, are the primary contributors to the projected changes in fire weather extremes in Europe. Declining antecedent precipitation totals during periods of extreme FWI are also projected for regions such as France. These findings align with a growing body of evidence indicating that increased fuel dryness is the key driver behind both observed and projected increases in fire weather in many regions worldwide <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx36 bib1.bibx55 bib1.bibx86 bib1.bibx113" id="paren.124"/>.</p></list-item></list></p>
      <p id="d2e4037">The proxy variable combination we selected to represent the original noon-time FWI calculation at daily resolution may have resulted in a possible underestimation of the baseline climatological values (as shown in Fig. <xref ref-type="fig" rid="F3"/>). However, a recent study found that all combinations at daily resolution overestimate the trend in FWI<sub>95 d</sub> relative to the original noon-time calculation <xref ref-type="bibr" rid="bib1.bibx70" id="paren.125"/>. We also calculated the difference between the trends from the original calculation and those from the proxy combination selected at daily resolution, and found that the daily combination overestimates the trend in FWI<sub>95 d</sub> by an area-weighted domain average of 17.7 %. This difference shows spatial heterogeneity across the domain, with the strongest signal concentrated in regions such as the Iberian Peninsula and western France (Fig. S14). Therefore, although our analysis revealed an underestimation of the extreme portion of the FWI distribution due to the use of mean relative humidity, it is still possible that the projected trends are overestimated. Similar to <xref ref-type="bibr" rid="bib1.bibx70" id="text.126"/>, we suggest that the next generation of climate model simulations should include more sub-daily output to better estimate risks associated with compound hazards in a warming climate.</p>
      <p id="d2e4074">The evaluation period used to assess bias-adjustment performance was the same as the calibration period (1971–2000), as it was important to use a longer period to reduce sampling uncertainty, and the historical time series from the EURO-CORDEX simulations are not long enough to allocate a separate validation period. Since uncertainty may also arise from the choice of bias adjustment methods, some studies have shown that the application of a multivariate bias adjustment method that not only adjusts the marginal distributions but also inter-variable dependencies can further improve the model performance in representing the multivariate hazard estimates <xref ref-type="bibr" rid="bib1.bibx20 bib1.bibx117" id="paren.127"/>. However, they usually come with greater computational cost  (e.g., <xref ref-type="bibr" rid="bib1.bibx20" id="text.128"/>). We suggest that there is still a need for further research on the performance of univariate and multivariate bias adjustment methods for the multivariate hazard estimates at a pan-European scale with a relatively large model ensemble.</p>
      <p id="d2e4083">Although extreme fire weather conditions, as represented by the FWI, are projected to intensify in terms of both frequency and magnitude, it is important to emphasize that the FWI is a fire weather rating metric and not a measure of fire occurrence. In fact, fire weather creates conditions that may enhance the susceptibility of landscapes to other key wildfire drivers, namely ignition, fuel dryness, and fuel continuity <xref ref-type="bibr" rid="bib1.bibx81" id="paren.129"/>. Burned area climatology from the past two decades (Fig. <xref ref-type="fig" rid="F1"/>b) reveals that fire occurrence has remained structurally limited in some regions, such as parts of Scandinavia, possibly due to a combination of bioclimatic and anthropogenic factors. However, it remains unclear whether these factors will remain unchanged in Europe in the future. In general, FWI provides the most meaningful danger information in regions where fire activity is limited by fuel dryness rather than by vegetation productivity <xref ref-type="bibr" rid="bib1.bibx58" id="paren.130"/>. The strongest relationships between FWI and burned area are observed in ecosystems with intermediate moisture availability <xref ref-type="bibr" rid="bib1.bibx58" id="paren.131"/>, including boreal and evergreen forests <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx8" id="paren.132"/>, as well as in Mediterranean Europe <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx23 bib1.bibx39 bib1.bibx58 bib1.bibx103" id="paren.133"/>. Furthermore, since the relationship between FWI and fire occurrence – and the thresholds for what constitutes extreme – varies regionally, it is important to incorporate regional climate and biome characteristics when interpreting FWI values for fire danger assessments to improve early warning systems and fire mitigation strategies in a changing climate <xref ref-type="bibr" rid="bib1.bibx65" id="paren.134"/>.</p>
      <p id="d2e4108">The ecosystem and socioeconomic impacts of a fire depend not only on fire weather, the availability of flammable vegetation, and ignition sources, but also on forest management practices prior to fire events and suppression efforts. For instance, the burned area in the Mediterranean has shown a declining trend since the 1980s, primarily due to enhanced suppression strategies <xref ref-type="bibr" rid="bib1.bibx102" id="paren.135"/>, despite increasing trends in fire weather. However, increasing pressure from climate change and more extreme fire weather may lead to conditions where high-intensity fires overwhelm the suppression capacity <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx83" id="paren.136"/>. In response to this growing challenge, international resource sharing has been recognized as both necessary and effective in Europe <xref ref-type="bibr" rid="bib1.bibx12" id="paren.137"/> and RescEU has been established as a collective response of European member states to this growing need by pooling resources <xref ref-type="bibr" rid="bib1.bibx51" id="paren.138"/>. However, it is also critical to recognize the so-called “fire-fighting trap” or the “suppression paradox”, where extinguishing all fires at any cost may lead to fires with greater severity in the following years under extreme fire weather conditions, due to fuel accumulation over time <xref ref-type="bibr" rid="bib1.bibx64 bib1.bibx75 bib1.bibx80" id="paren.139"/>. Given that the duration and intensity of extreme fire weather conditions are projected to increase with increasing greenhouse gas emissions, particularly in Mediterranean-type climates, a paradigm shift is advocated, emphasizing the importance of mitigation measures <xref ref-type="bibr" rid="bib1.bibx75" id="paren.140"/>. In this context, policy effectiveness should not be measured solely by the extent of the burned area, but rather by the degree to which socio-ecological damage is avoided <xref ref-type="bibr" rid="bib1.bibx75" id="paren.141"/>.</p>
      <p id="d2e4133">The next generation of simulations in the EURO-CORDEX framework, downscaled from CMIP6 GCMs, is currently underway <xref ref-type="bibr" rid="bib1.bibx61" id="paren.142"/>, with some outputs expected to become available soon. This new generation of simulations retains the same spatial resolution as their CMIP5 counterparts, but incorporates greenhouse gas forcing scenarios based on the state-of-the-art Shared Socioeconomic Pathways (SSPs) instead of RCPs, along with a consistent space- and time-varying aerosol forcing <xref ref-type="bibr" rid="bib1.bibx61" id="paren.143"/>. The latter may lead to a better representation of regional extreme fire weather conditions, considering that models that do not account for time-evolving aerosols underestimate the European summer warming <xref ref-type="bibr" rid="bib1.bibx90" id="paren.144"/>. In our analysis, we also found that the EURO-CORDEX ensemble median slightly underestimates the warming trend in the daily maximum temperature, as given in Fig. S15. In this sense, FWI-based analysis can serve as a useful framework to evaluate whether newer model generations improve the representation of complex multivariate weather hazards. Future studies should also employ these RCMs for further investigation while accounting for the “hot model problem” that was identified shortly after the release of the associated GCMs <xref ref-type="bibr" rid="bib1.bibx46" id="paren.145"/>. The present study can thus be seen as one more piece of the puzzle towards advancing our understanding of extreme fire weather in Europe in a warming climate, while emphasizing the need for measures to protect vulnerable regions.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d2e4153">The QDM implementation is based on the Python package cmethods <xref ref-type="bibr" rid="bib1.bibx91" id="paren.146"/>, available at <uri>https://python-cmethods.readthedocs.io/en/latest/</uri>, last access: 29 June 2026. Singularity Stochastic Removal, seasonal cycle correction, and relative change signal adjustment were implemented on top of this package by the authors of this study. FWI calculations were performed using a Python script provided by <xref ref-type="bibr" rid="bib1.bibx84" id="text.147"/> and available at <uri>https://github.com/yquilcaille/FWI_CMIP6</uri>, last access: 29 June 2026. All datasets used in this study are publicly available. ERA5-Land hourly reanalysis data are available at <uri>https://cds.climate.copernicus.eu/datasets/reanalysis-era5-land</uri>, last access: 30 December 2024. CMIP5 global climate model and EURO-CORDEX regional climate model data are available from the Earth System Grid Federation node at the German Climate Computing Center through <uri>https://esgf-metagrid.cloud.dkrz.de/search?project=CMIP5</uri>, last access: 30 December 2024 and <uri>https://esgf-metagrid.cloud.dkrz.de/search?project=CORDEX</uri>, last access: 30 December 2024. GFED5 monthly burned area data is accessible at <uri>https://www.globalfiredata.org/data.html</uri>, last access: 17 March 2026 and Copernicus land cover data is available at <uri>https://zenodo.org/records/3939050</uri> <xref ref-type="bibr" rid="bib1.bibx17" id="paren.148"/>.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d2e4189">The supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/esd-17-929-2026-supplement" xlink:title="pdf">https://doi.org/10.5194/esd-17-929-2026-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e4198">ASB: conceptualization, data curation, formal analysis, methodology, software, visualization, writing – original draft, writing – review and editing. JGP: conceptualization, methodology, resources, supervision, writing – review and editing. CMG: conceptualization, methodology, writing – review and editing. AMR: conceptualization, methodology, project administration, resources, supervision, writing – review and editing.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e4204">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="d2e4210">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="d2e4216">We acknowledge support by the KIT-Publication Fund of the Karlsruhe Institute of Technology. The authors thank the German Climate Computing Center (DKRZ) for providing computing resources. We also acknowledge the World Climate Research Program's Working Group on Coupled Modeling, which is responsible for CMIP, and the relevant climate modeling groups (listed in Table <xref ref-type="table" rid="T1"/>) for producing and making the CMIP5 output available. We also acknowledge the CORDEX community for producing the EURO-CORDEX simulations and making them available (listed in Table <xref ref-type="table" rid="T1"/>). AI-assisted tools (OpenAI ChatGPT, GPT-5 family models) were used for minor language editing of this manuscript. AMR was supported by the Helmholtz “Changing Earth – Sustaining our Future” program. JGP thanks the AXA Research Fund for support. The contribution of CMG was performed under the framework of the DHEFEUS project, funded by FCT (<ext-link xlink:href="https://doi.org/10.54499/2022.09185.PTDC" ext-link-type="DOI">10.54499/2022.09185.PTDC</ext-link>). The authors thank Hendrik Feldmann and Florian Ehmele (both IMKTRO, KIT) for discussions on EURO-CORDEX models and bias adjustment. The authors also thank Emanuele Bevacqua and Andreia F.S. Ribeiro (both UFZ, Germany) for helpful discussions after the revisions. Finally, we thank the editor and the two anonymous reviewers for their constructive feedback, which helped improve the manuscript.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e4228">The article processing charges for this open-access publication were covered by the Karlsruhe Institute  of Technology (KIT).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e4234">This paper was edited by Somnath Baidya Roy and reviewed by two anonymous referees.</p>
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