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  <front>
    <journal-meta><journal-id journal-id-type="publisher">NHESS</journal-id><journal-title-group>
    <journal-title>Natural Hazards and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1684-9981</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/nhess-26-2637-2026</article-id><title-group><article-title>Quantifying the current and future likelihood of the 2022 extreme wildfire weather conditions in France with anthropogenic climate change</article-title><alt-title>Climate change and 2022 wildfire weather in France</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Zhu</surname><given-names>Shengling</given-names></name>
          <email>shengling.zhu@inrae.fr</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Barbero</surname><given-names>Renaud</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8610-0018</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Pimont</surname><given-names>François</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Renard</surname><given-names>Benjamin</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8447-5430</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>INRAE, Aix-Marseille University, RECOVER, Aix-en-Provence, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>INRAE, URFM, Avignon, France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Shengling Zhu (shengling.zhu@inrae.fr)</corresp></author-notes><pub-date><day>5</day><month>June</month><year>2026</year></pub-date>
      
      <volume>26</volume>
      <issue>6</issue>
      <fpage>2637</fpage><lpage>2652</lpage>
      <history>
        <date date-type="received"><day>9</day><month>January</month><year>2026</year></date>
           <date date-type="rev-request"><day>22</day><month>January</month><year>2026</year></date>
           <date date-type="rev-recd"><day>19</day><month>May</month><year>2026</year></date>
           <date date-type="accepted"><day>19</day><month>May</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Shengling Zhu 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://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026.html">This article is available from https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e117">In 2022, southwestern France experienced an exceptional wildfire season, recording a burned area 14 times higher than the 2006–2023 average. Here, we assess the rarity (return period) of the fire weather conditions observed in 2022 and how anthropogenic climate change (ACC) has already altered and will continue to alter the probability of fire weather conditions associated with the three largest wildfires (Landiras-1: 12 552 ha; Landiras-2: 7124 ha; La Teste-de-Buch: 5709 ha). Drawing from the daily Fire Weather Index (FWI) computed from two reanalysis datasets (1959–2023) and a nationwide wildfire record dataset (2006–2023), we first sought to quantify the rarity of those conditions across a range of spatial (local vs. regional) and temporal (fire duration vs. 30 d window) scales. Our results demonstrate that the rarity of FWI conditions is generally the highest at local and fire duration scales with the associated return periods increasing from 6 to 34 <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula>, from 22 to 38 <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula>, and from 6 to 101 <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> when moving from the coarsest to the finest spatiotemporal scale for the Landiras-1, Landiras-2, and La Teste-de-Buch wildfires, respectively. Using climate simulations from the Coupled Model Intercomparison Project Phase 6 (CMIP6), we examined how ACC has modified and will modify the probability of such fire weather conditions over the period 1950–2100. The multi-model median suggests that, in 2022, FWI conditions of the same exceedance probability as the 2022 wildfire-related conditions were approximately 2–10 times more likely under anthropogenic and natural forcings combined than under the natural-forcing-only climate, depending on the spatiotemporal scale, with considerable inter-model spread. By the end of the century under the Shared Socioeconomic Pathway 2-4.5 (SSP2-4.5), these FWI conditions are projected to become roughly 1 to 2 orders of magnitude more probable, with still large inter-model uncertainty. Our study underlines the growing influence of ACC on the risk of extreme wildfires in France across a range of scales.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e153">The past decade has witnessed a number of unprecedented extreme wildfires across parts of the world (e.g. Australia in 2019–2020, Canada in 2023, or California in 2020 and 2025), causing widespread impacts on societies, ecological environments, and human life. In 2022, southwestern Europe also faced an extreme fire season due to a persistent anticyclonic anomaly <xref ref-type="bibr" rid="bib1.bibx18" id="paren.1"/> causing widespread soil moisture deficit <xref ref-type="bibr" rid="bib1.bibx8" id="paren.2"/>, and record burned area in some regions <xref ref-type="bibr" rid="bib1.bibx51" id="paren.3"/> including parts of France. At the national level, more than 55 000 ha of forests and other natural vegetation were burned <xref ref-type="bibr" rid="bib1.bibx28" id="paren.4"/> – an area 6–7 times larger than the average over the preceding decade. In southwestern (SW) France specifically, the burned area was even more than 14 times larger than the regional average (Fig. <xref ref-type="fig" rid="F1"/>b). This extensive burned area resulted in substantial biomass losses in Atlantic pine forests <xref ref-type="bibr" rid="bib1.bibx60" id="paren.5"/> and was largely driven by a small number of large wildfires. In particular, three events alone accounted for more than 45 % of the total annual burned area in France in 2022 and over 80 % of that in SW France. On 12 July 2022, two wildfires started simultaneously within the Gironde department: La Teste-de-Buch wildfire burned approximately 5709 ha over 12 <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula>, while the second one in Landiras burned 12 552 ha over 14 <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula>, due to frequent wind shifts causing spread in multiple directions (Office National des Forêts, personal communication, October 2025). After this wildfire (hereafter Landiras-1) was brought under control, it reignited 15 <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula> later, on 9 August 2022 (hereafter Landiras-2), and spread over six days, driven by northerly winds. When combined, the Landiras-1<inline-formula><mml:math id="M7" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2 wildfire burned over 19 676 ha, which makes it the largest wildfire in France since the Landes forest fire of August 1949 <xref ref-type="bibr" rid="bib1.bibx54" id="paren.6"/>.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e210"><bold>(a)</bold> Wildfires <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> ha recorded in the BDIFF database from 2006 to 2023. Color denotes burned area (BA) classes and the black box delineates the southwestern France region (<inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">4.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">4</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>). <bold>(b)</bold> Total burned area during the warm season (May–September) for France (orange line) and the southwestern region (black line).</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f01.png"/>

      </fig>

      <p id="d2e262">Those wildfires in SW France provided a glimpse of future projections across the region, featuring a spatial expansion of the potential fire niche with climate change towards western and northern latitudes <xref ref-type="bibr" rid="bib1.bibx19" id="paren.7"/>, a fire niche historically limited to the southeastern Mediterranean region. The 2022 fire season was indeed concomitant with a broader context of global and regional climate warming. Copernicus data indicated that July 2022 was among the three warmest Julys recorded globally, exceeding the 1991–2020 average by about 0.38 <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>. In France, Météo-France recorded an average annual temperature of 14.5 <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>, approximately 2.9 <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">°</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> higher than the 1959–2000 baseline. This warmer atmosphere and elevated atmospheric aridity have contributed to a reduced fuel moisture content, thereby increasing landscape flammability.</p>
      <p id="d2e299">Attribution analysis is essential to better understand how global warming is currently altering the likelihood of extreme events  and associated impacts <xref ref-type="bibr" rid="bib1.bibx42" id="paren.8"/>. Quantifying the likelihood of such impacts may enhance awareness and encourage adaptation efforts. Attribution studies employ both observational and simulated climate datasets to quantify the extent to which human emissions alter the probability of a given extreme weather event. So far, most of those studies have typically focused on meteorological events such as heatwaves <xref ref-type="bibr" rid="bib1.bibx41 bib1.bibx63" id="paren.9"/>, droughts <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx25" id="paren.10"/>, or extreme rainfall <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx67" id="paren.11"/>. However, fire weather conditions (combining multiple meteorological variables) have received less attention, although a number of efforts have been made in the western US <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx69 bib1.bibx10" id="paren.12"/>, Canada <xref ref-type="bibr" rid="bib1.bibx31" id="paren.13"/>, Australia <xref ref-type="bibr" rid="bib1.bibx61" id="paren.14"/>, and France <xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx34" id="paren.15"/>. Recently, <xref ref-type="bibr" rid="bib1.bibx34" id="text.16"/> conducted an attribution study of the 2022 fire season in SW France using multiple standardized climate indices. Their findings suggest that climate change doubled the likelihood of the climate conditions observed during the month of July. However, the analysis was performed over relatively broad spatial (the entire SW region of France) and temporal (the whole month of July) scales,  while attribution scores have been shown to be sensitive to the selection of spatial and temporal scales <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx32 bib1.bibx35" id="paren.17"/>. Finally, the attribution scores were limited to the year 2022, with no projections on how those conditions might change in the future. Such projections may help plan adaptation strategies.</p>
      <p id="d2e333">Building on prior attribution studies, we use here a complementary multi-scale framework to (i) provide a broader context of the spatiotemporal variability of fire weather conditions across France over the whole observational period from 1959 to 2023, (ii) quantify fire weather anomalies conducive to the 2022 wildfires, (iii) estimate return periods (RPs) of fire weather conditions associated with the three largest wildfires, considering a combination of different and complementary spatial and temporal scales, and (iv) estimate the extent to which those fire weather conditions have become, in 2022, more or less likely under anthropogenic-plus-natural forcings than under the natural-forcing-only climate, and how this contrast is likely to further increase in the future.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Wildfire data</title>
      <p id="d2e351">We used the BDIFF (Base de Données sur les Incendies de Forêts en France, <xref ref-type="bibr" rid="bib1.bibx28" id="altparen.18"/>) dataset, a forest-fire record for France (2006–2023), providing date, location, and burned area (BA; ha). Despite some consistency issues in low fire activity regions <xref ref-type="bibr" rid="bib1.bibx45" id="paren.19"/>, BDIFF has been shown to be reliable for estimating regional total BA, including SW France, and has been used in previous studies <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx46" id="paren.20"/>. We selected wildfires <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> ha occurring during the warm season (May to September, see Fig. <xref ref-type="fig" rid="F1"/>a) following <xref ref-type="bibr" rid="bib1.bibx44" id="text.21"/>.  We also classified wildfires into three size classes (small: 1–10 ha; medium: 10–100 ha; large: <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> ha) as shown in Fig. <xref ref-type="fig" rid="F1"/>a. Note that large wildfires were mostly concentrated in southern France, in particular along the Mediterranean coast and SW France (Fig. <xref ref-type="fig" rid="F1"/>a). In 2022, national BA reached approximately 55 000 ha, with the SW region accounting for over half of this total (Fig. <xref ref-type="fig" rid="F1"/>b) due to three major wildfires. Table <xref ref-type="table" rid="T1"/> provides the name, starting and ending dates as well as the extent of each of those wildfires.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e400">The three largest wildfires in southwestern France in 2022. The last column indicates their respective contribution to total burned area in southwestern France in 2022.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Fire name</oasis:entry>
         <oasis:entry colname="col2">Burning period</oasis:entry>
         <oasis:entry colname="col3">Burned area <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:mo>(</mml:mo><mml:mi mathvariant="normal">ha</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">Contribution <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="unit"><mml:mo>(</mml:mo><mml:mi mathvariant="normal">%</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Landiras-1</oasis:entry>
         <oasis:entry colname="col2">12–25 July 2022</oasis:entry>
         <oasis:entry colname="col3">12 552</oasis:entry>
         <oasis:entry colname="col4">40</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Landiras-2</oasis:entry>
         <oasis:entry colname="col2">9–14 August 2022</oasis:entry>
         <oasis:entry colname="col3">7124</oasis:entry>
         <oasis:entry colname="col4">22</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">La Teste-de-Buch</oasis:entry>
         <oasis:entry colname="col2">12–23 July 2022</oasis:entry>
         <oasis:entry colname="col3">5709</oasis:entry>
         <oasis:entry colname="col4">19</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Fire weather observations</title>
      <p id="d2e513">Fire weather conditions were estimated with the Fire Weather Index (FWI), a composite index based on four daily meteorological observations – maximum air temperature, relative humidity, wind speed, and precipitation. Originally developed in Canada by <xref ref-type="bibr" rid="bib1.bibx62" id="text.22"/> for northern boreal forest conditions, the FWI has been used across various countries and climatic regions to track wildfire activity, including in Europe <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx26" id="paren.23"/> and in France <xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx45 bib1.bibx46" id="paren.24"/>. Daily meteorological variables used to calculate the FWI were obtained from SAFRAN (Système d'Analyse Fournissant des Renseignements Atmosphériques à la Neige), a French reanalysis product available at a daily resolution on an 8 <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> grid from 1959 to 2023 <xref ref-type="bibr" rid="bib1.bibx64" id="paren.25"/>. The analyses were repeated using ERA5 reanalysis at a slightly coarser resolution of 25 <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>. The results were similar for both datasets (see Figs. S1–S3 in the Supplement). The FWI was calculated using the <monospace>cffdrs</monospace> package in R <xref ref-type="bibr" rid="bib1.bibx68" id="paren.26"/>.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Spatiotemporal variability of fire weather</title>
      <p id="d2e559">In climate sciences, empirical orthogonal function (EOF) is often employed to examine large spatiotemporal datasets and identify the main modes of climate variability. In this study, an EOF was applied to a matrix with seasonal FWI values (averaged from May to September, corresponding to the traditional wildfire season) for each grid cell across France, structured as an <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mtext>year</mml:mtext></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>n</mml:mi><mml:mtext>grid</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> matrix, where <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mtext>year</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is the number of years and <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mtext>grid</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> the number of grid cells. After data normalization and eigenvalue decomposition, the matrix was decomposed into a few dominant spatial modes (EOFs), together with their corresponding time-varying coefficients, known as principal components (PCs). Each PC constitutes a time series that illustrates the interannual variability of its corresponding EOF <xref ref-type="bibr" rid="bib1.bibx65" id="paren.27"/>.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Fire weather conducive to wildfires in SW France</title>
      <p id="d2e613">To quantify the relationship between local FWI conditions and wildfire events, we extracted for each wildfire the daily FWI time series from the nearest SAFRAN grid cell, over a window extending from 90 <inline-formula><mml:math id="M23" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula> before to 90 <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula> after the wildfire start. Note that BDIFF does not provide the wildfire perimeter and that multiple grid cells may potentially intersect with the actual wildfire perimeter. However, this effect should be limited given the size of the SAFRAN grid cell (<inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mn mathvariant="normal">64</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula>) and the inherent spatial autocorrelation of FWI. To quantify the departure from the FWI climatology (i.e. normal conditions), we removed the seasonality by computing deviations from the local mean seasonal cycle and expressed them as percentage anomalies. Finally, we stratified the sample by wildfire size and averaged FWI within predefined wildfire extent classes (small, medium, large) to relate the amplitude of FWI anomalies to wildfire size. In addition, analyses were performed on all years (2006–2023) and then on the year 2022 only.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Fire weather simulations</title>
      <p id="d2e656">The Coupled Model Intercomparison Project Phase 6 (CMIP6) provides a comprehensive and standardized ensemble of multi-model climate simulations, enabling improved understanding of climate change driven by natural internal variability and external radiative forcings under various past, present, and future scenarios <xref ref-type="bibr" rid="bib1.bibx17" id="paren.28"/>. Here, we used simulations from the Detection and Attribution Model Intercomparison Project (DAMIP) and the Scenario Model Intercomparison Project (ScenarioMIP) <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx39" id="paren.29"/>, a sub-project of CMIP6. DAMIP provides simulations for historical periods (up to 2014, with extensions to 2020 in some cases) under anthropogenic and natural forcing scenarios <xref ref-type="bibr" rid="bib1.bibx24" id="paren.30"/>. ScenarioMIP provides climate projections informed by future emissions and land-use scenarios, primarily driven by Shared Socioeconomic Pathways (SSPs) <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx48" id="paren.31"/>. For historical simulations, we used the “historical” and the DAMIP “hist-nat” experiments. The “historical” experiment covers 1850–2014 and includes all observed external forcings – greenhouse gases, aerosols, solar variability, and volcanic eruptions. In contrast, the “hist-nat” experiment includes only natural external forcings (total solar irradiance and volcanic stratospheric aerosol injections) over 1850–2020. For future climate projections, we used the “ssp245” experiment, representing a medium mitigation scenario, and the “ssp245-nat” experiment. Similar to their historical counterparts, the “ssp245” experiment includes both anthropogenic and natural forcings, whereas the “ssp245-nat” experiment includes only natural forcings. Not all CMIP6 models provide all the meteorological outputs needed to compute the FWI (see Sect. 2.2). Hence, we used the following models: IPSL-CM6A-LR, CanESM5, MIROC6, and NorESM2-LM. Each CMIP6 model is analyzed at its native spatial resolution. For each model, we used a single member (r1i1p1f1) in both the ALL and NAT experiments. This choice was primarily motivated by data availability: for NorESM2-LM, only one realization was publicly available for the ssp245-nat experiment in the CMIP6 archive. For consistency, we used a single member for all four models.</p>
</sec>
<sec id="Ch1.S2.SS6">
  <label>2.6</label><title>Probability of exceedance of 2022 extreme wildfires across spatial and temporal scales</title>
      <p id="d2e679">We quantified the expected return periods of fire weather conditions associated with the three largest fires in 2022 to assess the rarity of these conditions. This estimation requires three steps: (1) characterizing fire weather conditions associated with each wildfire across spatial and temporal scales; (2) fitting an appropriate statistical distribution; (3) calculating the exceedance probability (or return period) of the fire weather conditions defined in step 1 based on the distribution fitted in step 2.</p>
      <p id="d2e682">The choice of temporal and spatial scales is the most critical step due to their impact on attribution scores <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx32" id="paren.32"/>. Moreover, refining or broadening scales may provide different and complementary insights for wildfire managers. In the temporal dimension, we may either opt for a 30 d window centered on the fire occurrence as in <xref ref-type="bibr" rid="bib1.bibx34" id="text.33"/> or focus on fire duration from ignition to suppression, a period more representative of the burning conditions. In the spatial dimension, we may either select a single grid cell (8 km with SAFRAN or 25 km with ERA5) co-located with the wildfire location or consider a broader regional bounding box as done in <xref ref-type="bibr" rid="bib1.bibx34" id="text.34"/> to improve the signal-to-noise ratio. Here, in order to analyze the sensitivity of the results to these assumptions, we used the four possible combinations of these different resolutions. For each wildfire, we derived the daily FWI time series corresponding to both spatial resolutions over the full period (1 January 1959–31 December 2023). We then applied a moving average (MA) to each time series, using both a 30 d window and a <inline-formula><mml:math id="M26" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula>-day window – where <inline-formula><mml:math id="M27" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> equals the fire duration (Landiras-1: 14 <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula>; Landiras-2: 6 <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula>; La Teste-de-Buch: 12 <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula>). The annual maxima of these MA time series were then extracted to fit the historical distribution using the generalized extreme value (GEV) theory. Finally, based on the fitted distributions, we calculated the exceedance probabilities and corresponding return periods of the observed FWI during the three largest wildfires in 2022 according to each spatiotemporal scale. Note that the annual maxima of the MA-FWI time series were used only as annual extreme inputs for fitting the GEV distribution, and do not represent the fire weather conditions of any individual wildfire. The FWI level observed during each wildfire is therefore distinct from the annual maxima used in the GEV fitting.</p>
</sec>
<sec id="Ch1.S2.SS7">
  <label>2.7</label><title>The contribution of anthropogenic climate change</title>
      <p id="d2e741">To quantify the impact of anthropogenic climate change (ACC), we employed a commonly used approach to calculate the exceedance probability of each wildfire-related FWI  <xref ref-type="bibr" rid="bib1.bibx6" id="paren.35"/>, following the procedure applied in the previous section to the 1959–2023 SAFRAN observations. Here, SAFRAN is used only to estimate the exceedance probability of the observed event (<inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>OBS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>). We then compared the exceedance probabilities under two scenarios: (i) the ALL scenario, including all anthropogenic and natural forcings (hereafter <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>), and (ii) the NAT scenario, which includes only natural forcings (hereafter <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>). For the GEV distribution fitted to the ALL-scenario simulated annual maxima of the MA-FWI time series, we inverted its cumulative distribution function (CDF), <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, to find for each year, the FWI level in the ALL scenario such that <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mtext>OBS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>. We then applied this year-specific <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> threshold to the GEV distribution fitted to the NAT-scenario simulated annual maxima of the MA-FWI time series – using its CDF <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> – to compute <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. Note that <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is year-dependent and represents the FWI level in the ALL climate with the same exceedance probability as the observed 2022 wildfire-related FWI; the analysis is thus probability-based rather than based on a fixed absolute FWI threshold. Because the attribution metric relies on the within-model ratio between <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, no spatial downscaling was required.</p>
      <p id="d2e922">As the FWI is assumed to be non-stationary with global warming, we used here a non-stationary GEV model where the location and scale parameters may vary with year according to a GAMLSS framework (Generalized Additive Models for Location, Scale and Shape), to capture smooth nonlinear relationships <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx50" id="paren.36"/>. The covariate effects on the location and log-scale parameters are represented using penalized cubic regression splines in the <monospace>evgam</monospace> package, with at most five basis functions for each smooth term, and smoothing parameters selected by restricted maximum likelihood (REML; <xref ref-type="bibr" rid="bib1.bibx70" id="altparen.37"/>). As opposed to what has been done previously in Sect. 2.6 where we sought to estimate the probability of exceedance over the full observational period available without any assumptions, we did use here a non-stationary GEV to make the return periods explicitly time-dependent. Based on the GAMLSS fits, we estimated for each year the GEV distribution of annual maxima FWI under the ALL and NAT scenarios and computed the ratio <inline-formula><mml:math id="M42" display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:math></inline-formula>, commonly referred to as the risk ratio (RR). This metric has been widely used in event-attribution studies to quantify how many times as likely an extreme event is to occur under the ALL scenario compared to the NAT scenario <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx40" id="paren.38"/>. Additionally, we employed the fraction of attributable risk (<inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mtext>FAR</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mtext>RR</mml:mtext></mml:mrow></mml:math></inline-formula>), which reflects, when positive, the proportion of risk attributable to ACC <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx37 bib1.bibx7" id="paren.39"/>.</p>
      <p id="d2e980">To quantify the sampling uncertainty surrounding RR and FAR, a parametric bootstrap approach was implemented as follows: <list list-type="order"><list-item>
      <p id="d2e985">Generate new samples of ALL and NAT scenarios from the estimated non-stationary GEVs.</p></list-item><list-item>
      <p id="d2e989">Re-estimate the non-stationary GEVs based on these new samples and compute the RR and the FAR.</p></list-item><list-item>
      <p id="d2e993">Repeat steps 1–2 100 times to derive model-specific parametric confidence intervals.</p></list-item></list></p>
      <p id="d2e996">Finally, attribution scores (RR and FAR) from individual models were aggregated across models using a multi-model median. In that case, we pooled together the 100 bootstrap replicates from each of the four models. This pooled ensemble range is intended to reflect both within-model sampling uncertainty and the spread across models. The full computation workflow – from the CMIP6 annual maxima MA-FWI to the RR/FAR calculation – is summarized in Fig. <xref ref-type="fig" rid="F2"/>.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e1004">Schematic workflow used to estimate exceedance probabilities (denoted by <inline-formula><mml:math id="M44" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>) under ALL and NAT forcings from CMIP6 annual maxima moving-average FWI (MA-FWI):  a non-stationary GEV fit provides the cumulative distribution functions (CDFs) <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> (where <inline-formula><mml:math id="M47" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> denotes the fitted GEV CDF); <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is obtained by inverting <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> such that <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mtext>OBS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is then computed as <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mtext>FWI</mml:mtext><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>.</p></caption>
          <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f02.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
      <p id="d2e1159">Figure <xref ref-type="fig" rid="F3"/> illustrates the first two dominant modes of May–September FWI variability over the 1959–2023 period, with the EOF loadings (left panels) and their corresponding PCs (right panels). The loadings characterize the spatial structure of a given mode, identifying regions where FWI anomalies vary either in phase (same sign) or in opposition. The PCs reflect the temporal evolution of each mode, highlighting years during which the associated spatial structure is either amplified or dampened. In other words, the initial FWI time series in a specific grid cell featuring a high positive loading will strongly look like the associated PC. A negative loading will in turn indicate that the FWI time series varies in opposition to the PC. Together, the first two modes explain about 75 % of the total variance (61.69 % and 12.75 % for EOF-1 and EOF-2, respectively). EOF-1 exhibits positive loadings throughout France, albeit with smaller coefficients along the Mediterranean (Fig. <xref ref-type="fig" rid="F3"/>a). This mode presents  a strong interannual variability with an upward underlying trend, featuring an increasing frequency of higher FWI years in recent decades with global warming (Fig. <xref ref-type="fig" rid="F3"/>b). We found that PC-1 was strongly correlated with both temperature and rainfall anomalies over a large portion of western Europe (see Fig. S4). Note that the highest amplitude is seen in 2022, followed by 1976, a notoriously warm and dry year in France. By contrast, after removing the influence of PC-1, EOF-2 shows a slightly unbalanced north–south dipole, with a near-zero band straddling central France. In other words, when positive FWI anomalies occur preferentially in the south, negative anomalies are seen in the north and vice versa. This mode of variability correlates with a larger continental-scale dipole in rainfall anomalies, as well as with temperature anomalies south of <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mn mathvariant="normal">45</mml:mn><mml:mi mathvariant="italic">°</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> (see Fig. S5). Like the first mode, the second mode presents a long-term trend (Fig. <xref ref-type="fig" rid="F3"/>d), reflecting an increasing occurrence of years with higher FWI in southern France and lower FWI in northern France. Note that the following modes were not analyzed due to their little variance explained and their lack of consistency across space.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e1185">Leading two modes of mean May–September Fire Weather Index (FWI) over France from 1959 to 2023. <bold>(a)</bold> First empirical orthogonal function (EOF) (variance explained <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mn mathvariant="normal">61.69</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>) with <bold>(b)</bold> its corresponding principal component (PC-1) time series. <bold>(c)</bold> Second EOF (variance explained <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mn mathvariant="normal">12.75</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>) with <bold>(d)</bold> its corresponding PC-2 time series.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f03.png"/>

      </fig>

      <p id="d2e1229">We then restricted our attention to local FWI conditions associated with actual wildfires across SW France. Figure <xref ref-type="fig" rid="F4"/>a shows that, on average, FWI increases until the wildfire day and decreases in the following days, with higher FWI values for larger wildfires. Figure <xref ref-type="fig" rid="F4"/>c shows positive anomalies three months before wildfires (note that <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> indicates that FWI was twice as high as expected from average local conditions), reaching 71 %, 106 %, and 155 % for small, medium, and large fires, respectively. These persistent pre-wildfire positive anomalies may reflect not only prolonged antecedent hot and dry conditions, but also, to some extent, an earlier seasonal onset of the fire weather season. A similar signal was observed in 2022 (Fig. <xref ref-type="fig" rid="F4"/>b and d), but FWI anomalies were that time higher during the previous months and were 119 %, 137 %, and 180 % higher than mean conditions on the starting days of small, medium and large wildfires, respectively (Fig. <xref ref-type="fig" rid="F4"/>d).</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e1254">Lead–lag time series of FWI <bold>(a, b)</bold> and percent anomalies <bold>(c, d)</bold> relative to wildfire dates for three fire size classes over 2006–2023 <bold>(a, c)</bold> and 2022 only <bold>(b, d)</bold> in SW France. Anomalies were computed relative to the long-term (1959–2023) mean local seasonal cycle. Curves denote the three burned-area classes: BA <inline-formula><mml:math id="M57" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1–10 ha, BA <inline-formula><mml:math id="M58" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 10–100 ha, and BA <inline-formula><mml:math id="M59" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 100 ha, as indicated in the legend. Shaded bands indicate 95 % bootstrap confidence intervals. The <inline-formula><mml:math id="M60" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis shows lead/lag days from <inline-formula><mml:math id="M61" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>90 to <inline-formula><mml:math id="M62" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>90 relative to the wildfire starting day (day 0; vertical dashed line).</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f04.png"/>

      </fig>

      <p id="d2e1318">We then examined the return periods (RPs) of the three largest wildfires of 2022. Figure <xref ref-type="fig" rid="F5"/> (left panels) indicates that the annual maxima of the moving-average (MA) FWI are consistently highest when computed at the finest spatiotemporal resolution (i.e. the fire-duration window at the 64 <inline-formula><mml:math id="M63" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> SAFRAN grid cell fire level). These annual maxima decrease when the temporal window is lengthened to 30 <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">d</mml:mi></mml:mrow></mml:math></inline-formula> or when FWI conditions are spatially averaged over SW France region (<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">4.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">4</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>). This pattern holds for all three wildfires (Fig. <xref ref-type="fig" rid="F5"/>, left panels). In every case, the absolute maximum occurs in 2022, underscoring the exceptional FWI conditions during that year. Overall, the rarity of those conditions also increases with the resolution (Fig. <xref ref-type="fig" rid="F5"/>, right panels), with the best-estimate RPs increasing from <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">34</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M69" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula>, from <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">22</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">38</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M72" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula>, and from <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">101</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> when moving from the coarsest to the finest spatiotemporal scale for Landiras-1 (Fig. <xref ref-type="fig" rid="F5"/>b), Landiras-2 (Fig. <xref ref-type="fig" rid="F5"/>d), and La Teste-de-Buch (Fig. <xref ref-type="fig" rid="F5"/>f) wildfires, respectively, illustrating how sensitive the RPs are to the chosen scales.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e1469">Annual maxima of moving-averaged FWI at multiple spatiotemporal scales (left) and return-levels (right) associated with Landiras-1 <bold>(a, b)</bold>, Landiras-2 <bold>(c, d)</bold>, and La Teste-de-Buch <bold>(e, f)</bold>. Return levels on the right (logarithmic <inline-formula><mml:math id="M76" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis from 1 to <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> years) were estimated by fitting a GEV distribution to the annual-maximum moving-averaged FWI. Shaded envelopes indicate 80 % parametric-bootstrap confidence intervals. Dashed lines indicate the estimated return periods of the FWI level observed for each wildfire according to the chosen scale.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f05.png"/>

      </fig>

      <p id="d2e1505">Finally, we examined how ACC altered the probability of those FWI conditions. Figure <xref ref-type="fig" rid="F6"/> illustrates, for one model (NorESM2-LM, r1i1p1f1) and one spatiotemporal set-up (local and fire duration), how <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> varies relative to the reference probability <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mtext>OBS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> by construction). In this spatiotemporal set-up, <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> slightly exceeds <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> until the 1970s although <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> remains within the bootstrapping confidence interval. After the 1970s, <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> becomes systematically lower than <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> and tends toward zero after the 2040s, reflecting the growing inability of the NAT climate to produce FWI conditions that remain at the same extreme quantile in the warming ALL climate. We then computed the risk ratio (RR) for the Landiras-1 wildfire (Fig. <xref ref-type="fig" rid="F7"/>) using all models. The RR exhibits a consistent increase from the late 20th century for each model and across all temporal and spatial scales. The multi-model ensembles exceed the reference line <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mtext>RR</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (indicating that <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>) around 1970–1980, with earlier emergences for finer resolutions (Fig. <xref ref-type="fig" rid="F7"/>d). In 2022, three of the four models yield best-estimated <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:mtext>RR</mml:mtext><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> across spatiotemporal scales: IPSL-CM6A-LR <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn></mml:mrow></mml:math></inline-formula>–3, CanESM5 <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula>–20, and NorESM2-LM <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>–130; by contrast, MIROC6 presents an <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mtext>RR</mml:mtext><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>–0.6). The multi-model median RR lies between <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> and 10 in 2022 across the four scales. In the latter half of the century, this ratio increases by 1 to 2 orders of magnitude. Note the large confidence intervals within and across models and scales, reflecting the strong sensitivity to internal variability, parameter uncertainty and model uncertainty. Also, RR scores may sometimes exceed 10 000 as from the mid-to-late 21st century due to very low <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> approaching zero as shown in Fig. <xref ref-type="fig" rid="F6"/>.</p>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e1726">Example of the NAT-only exceedance probability for the Landiras-1 wildfire weather conditions  (local and fire-duration set-up) using NorESM2-LM (r1i1p1f1): the NAT-only exceedance probability <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>NAT</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> (black; median) is shown relative to the reference probability <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mtext>ALL</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mtext>OBS</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> (blue) that does not change with time. Shaded envelope indicates the 80 % parametric-bootstrap confidence interval.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f06.png"/>

      </fig>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e1767">Risk ratio (RR) of FWI conditions of the same exceedance probability as those associated with the Landiras-1 wildfire, from four CMIP6 models (IPSL-CM6A-LR, CanESM5, MIROC6, NorESM2-LM) and the multi-model median (black) across different scales: <bold>(a)</bold> regional over 30 d window; <bold>(b)</bold> regional over 14 d event duration; <bold>(c)</bold> local over 30 d window; <bold>(d)</bold> local over 14 d event duration. Shaded envelopes denote 90 % parametric-bootstrap confidence intervals for individual models. All panels use a logarithmic <inline-formula><mml:math id="M98" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis. The horizontal dashed line indicates RR <inline-formula><mml:math id="M99" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1 (no anthropogenic influence).</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f07.png"/>

      </fig>

      <p id="d2e1803">Using the finest spatiotemporal set-up (local over fire duration), we found that ACC contributed approximately 78 %, 73 %, and 79 % to the FWI conditions associated with Landiras-1, Landiras-2 and La Teste-de-Buch wildfires respectively, and will approach 100 % by mid-21st century (Fig. <xref ref-type="fig" rid="F8"/>) with very large uncertainty until 2070s. Note that the signals for Landiras-1 and La Teste-de-Buch are very similar, as the two events occurred approximately over the same period.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e1810">Fraction of attributable risk (FAR, <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mtext>RR</mml:mtext></mml:mrow></mml:math></inline-formula>) using the local FWI over the event-duration window for <bold>(a)</bold> Landiras-1 (14 d), <bold>(b)</bold> Landiras-2 (6 d), and <bold>(c)</bold> La Teste-de-Buch (12 d). The black curve shows the multi-model median across models. The <inline-formula><mml:math id="M101" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis is truncated to <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>; horizontal dashed lines indicate FAR <inline-formula><mml:math id="M103" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0 (no anthropogenic contribution) and FAR <inline-formula><mml:math id="M104" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1 (fully attributable). The shaded envelope indicates the 90 % pooled ensemble uncertainty range for the multi-model median, obtained by pooling the bootstrap replicates from the four models and taking the 5th and 95th percentiles of the pooled distribution. This approach captures both within-model sampling uncertainty and inter-model spread.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/2637/2026/nhess-26-2637-2026-f08.png"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
      <p id="d2e1892">The spatiotemporal variability of the observed warm-season (May–September) FWI during 1959–2023 has been synthesized into two leading modes. The first mode (<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">61.69</mml:mn></mml:mrow></mml:math></inline-formula> % of variance explained) shows strong interannual variability due to an alternation between warmer/drier and cooler/wetter years throughout France. This mode also features an increased frequency of years with positive FWI anomalies over time. This evolution is consistent with the long-term trend in temperature <xref ref-type="bibr" rid="bib1.bibx49" id="paren.40"/> and drought <xref ref-type="bibr" rid="bib1.bibx8" id="paren.41"/> in France, collectively contributing to increased fire weather conditions as observed more broadly in the Mediterranean region <xref ref-type="bibr" rid="bib1.bibx53 bib1.bibx26" id="paren.42"/>, Europe <xref ref-type="bibr" rid="bib1.bibx23" id="paren.43"/>, and globally <xref ref-type="bibr" rid="bib1.bibx29" id="paren.44"/>. The second mode (accounting for <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">12.75</mml:mn></mml:mrow></mml:math></inline-formula> % of variance) reveals a north–south dipole. This north–south contrast in climate anomalies probably relates to the summer North Atlantic Oscillation, which is, during negative phases, generally associated with blocking events producing cooler/wetter conditions in northern Europe and warmer/drier conditions in the south <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx66 bib1.bibx36" id="paren.45"/>. An underlying long-term trend with more frequent warmer/drier years in the south in recent years was also evident, in agreement with precipitation decreases in southern Europe and slightly wetter conditions in the north as documented in observations <xref ref-type="bibr" rid="bib1.bibx52 bib1.bibx8 bib1.bibx59" id="paren.46"/> as well as in future simulations <xref ref-type="bibr" rid="bib1.bibx23" id="paren.47"/>. Interestingly, both PC-1 and PC-2 scores indicate that the year 2022 represented a combination of these two leading modes, with unprecedented FWI anomalies over a large portion of France and, orthogonal to that mode, a latitudinal dipole with higher (lower) FWI in the southern (northern) half of the country.</p>
      <p id="d2e1940">The exceptionally high FWI values observed in 2022 in SW France, whether sampled locally or regionally, were conducive to a series of wildfires, with larger wildfires associated with larger FWI anomalies. We found that FWI levels reached their highest amplitude on the day of ignition (or the week surrounding it), boosted by either synoptic-scale heat waves or local wind bursts, as shown in previous studies over southern Europe <xref ref-type="bibr" rid="bib1.bibx53" id="paren.48"/> and France <xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx44" id="paren.49"/>. We estimated that the conditions observed locally during the three largest wildfires were expected, on average, to occur once every 34, 38, and 101 <inline-formula><mml:math id="M107" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> for the Landiras-1, Landiras-2, and La Teste-de-Buch wildfires, respectively. The last estimate, relying on extrapolation beyond the observational record, naturally involves substantial uncertainty.</p>
      <p id="d2e1957">Across spatial scales, Landiras-1 and La Teste-de-Buch wildfires exhibited higher RPs at the local scale than at the regional scale, reflecting the well-known effect of spatial averaging on dampening extremes <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx4 bib1.bibx32" id="paren.50"/>. We note that the region is flat, suggesting that those spatial differences cannot be attributed to terrain-related factors. However, Landiras-2 displayed the opposite pattern, with regional RPs exceeding local RPs. This inversion may be due to the fact that Landiras-2 was a rekindling of the Landiras-1 wildfire and was driven mainly by smoldering peat rather than by fire weather conditions. Also, we noticed that some precipitation occurred locally on 13–14 August, depressing the local FWI during the 9–14 August interval. Furthermore, even though the regional-scale FWI had a longer return period, the FWI associated with Landiras-2 was still higher in absolute terms at the local scale. Across temporal scales, all three wildfires exhibited higher RPs during the fire-duration window than during the 30 d window, indicating that short-duration, but more acute FWI driven by daily or synoptic meteorological variations also contributed strongly to these wildfires. Note that the wide confidence intervals around the RPs illustrate the uncertainty inherent in GEV fits with limited sample sizes.</p>
      <p id="d2e1963">Our results indicated that anthropogenic warming has, since the early twenty-first century, markedly increased the probability of occurrence of FWI conditions associated with those wildfires. This is consistent with a growing body of fire-attribution research at the global scale <xref ref-type="bibr" rid="bib1.bibx30 bib1.bibx3" id="paren.51"/> and at regional scales across parts of the US <xref ref-type="bibr" rid="bib1.bibx47 bib1.bibx10 bib1.bibx69" id="paren.52"/>, Canada <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx33" id="paren.53"/>, Australia <xref ref-type="bibr" rid="bib1.bibx61" id="paren.54"/>, the Arctic <xref ref-type="bibr" rid="bib1.bibx16" id="paren.55"/>, Portugal <xref ref-type="bibr" rid="bib1.bibx55" id="paren.56"/>, and France <xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx34" id="paren.57"/>. This increase is evident across temporal and spatial scales in the multi-model median, although its magnitude and timing differ substantially among models. Likewise, the timing at which the RR exceeds 1 and remains above that threshold is broadly consistent with the emergence of anthropogenic signals in simulated fire weather indices since the late twentieth century in southern Europe <xref ref-type="bibr" rid="bib1.bibx2" id="paren.58"/>. Our study suggests that the multi-model median probability of such conditions increased by approximately 2–10 times in 2022 and is projected to increase by roughly 1 to 2 orders of magnitude by the end of the twenty-first century under a medium-level radiative forcing scenario. However, the pooled ensemble uncertainty range indicates substantial uncertainty across and within models (see Fig. S6). This validates, across different metrics, fire weather indices, and spatiotemporal scales, the results obtained by <xref ref-type="bibr" rid="bib1.bibx34" id="text.59"/> using a soil-moisture index. Interestingly, despite the large spread in RPs across scales, the attribution scores were not found to change substantially across regional and local scales, suggesting that the rarity of FWI conditions does not necessarily relate to the magnitude of the anthropogenic forcing <xref ref-type="bibr" rid="bib1.bibx12" id="paren.60"/>. Although inter-model differences were evident in terms of amplitude and timing (i.e. the date at which the RR emerges above 1), due to model sensitivity to greenhouse gas emissions, all models point to a substantial increase in 2022-like conditions in future decades, consistent with previous projections of FWI <xref ref-type="bibr" rid="bib1.bibx19" id="paren.61"/> or FWI-derived fire activity <xref ref-type="bibr" rid="bib1.bibx46" id="paren.62"/> in France. Also, MIROC6 was found to cross the <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mtext>RR</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line later than other models, supporting the findings of <xref ref-type="bibr" rid="bib1.bibx34" id="text.63"/> who detected a lower climate change signal in MIROC6. This probably relates to the lower climate sensitivity of MIROC6 <xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx20" id="paren.64"/> due to the radiative forcing of aerosols <xref ref-type="bibr" rid="bib1.bibx56" id="paren.65"/> and cloud feedback <xref ref-type="bibr" rid="bib1.bibx27" id="paren.66"/>. Finally, our study shows that approximately 70 % of the risk that fire weather conditions reach the levels observed during those wildfires can be attributed to ACC (more than the 49 % found in <xref ref-type="bibr" rid="bib1.bibx34" id="text.67"/> over broader spatial and temporal scales, and the nearly half contribution reported by <xref ref-type="bibr" rid="bib1.bibx6" id="text.68"/> at a multi-decadal scale for Mediterranean France) and that this estimate will reach 100 % by the 2050s. These conclusions apply to other large wildfires (Landiras-2 and La Teste-de-Buch) as well.</p>
      <p id="d2e2036">We note that the methodology developed here has some limitations. First, our analysis was based solely on meteorological forcing and therefore lacks information on fuels (e.g. forest cover, fuel breaks, and horizontal/vertical continuity). The use of a statistical model that accounts for some of these features (e.g. Firelihood; <xref ref-type="bibr" rid="bib1.bibx44" id="altparen.69"/>) would produce more realistic estimates. Previous studies have also shown that some wildfires are driven primarily by wind, whereas others are driven by the dryness of climate conditions <xref ref-type="bibr" rid="bib1.bibx53" id="paren.70"/>. Further efforts are thus needed to resolve the respective contributions of fuel moisture and wind forcing, based, for instance, on sub-indices of the FWI (e.g. Fine Fuel Moisture Code (FFMC), Duff Moisture Code (DMC), and Drought Code (DC)) and complementary atmospheric drivers such as the vapor pressure deficit (VPD) and wind speed, as recently implemented in a probabilistic framework <xref ref-type="bibr" rid="bib1.bibx11" id="paren.71"/>. Second, our analysis does not explicitly consider ignition sources and their spatiotemporal variability. In France, approximately 95 % of ignitions are related to human activities <xref ref-type="bibr" rid="bib1.bibx22" id="paren.72"/>, and the realized fire activity therefore reflects the interplay between human pressure and fire weather conditions. As a simple approximation, the “fire start probability” could be expressed as a monotonically increasing function of the FWI (i.e. an ignition probability conditional on fire weather) using a probabilistic framework such as the Firelihood model <xref ref-type="bibr" rid="bib1.bibx44" id="paren.73"/> combining FWI with land use and land cover information. Also, our event-attribution analysis was based on three large wildfires in southwestern France. Extending the analysis to the French Mediterranean, which recently experienced the second largest wildfire in France since 1949 (early August 2025; approximately 17 000 ha burned at Ribaute), would be of interest. Although the spread of this wildfire was facilitated by hot and dry conditions alongside strong winds, wildfires in that region are generally associated with higher FWI levels that are expected, on average, once every year or so. Regarding climate simulations, we note that only a single ensemble member (r1i1p1f1) was used for each model. Using additional members would obviously reduce internal variability. Further work is also needed to improve the multi-model averaging by introducing weights based on each model's skill over the historical period <xref ref-type="bibr" rid="bib1.bibx21" id="paren.74"/>. Finally, we used the SSP2-4.5 scenario in CMIP6, corresponding to a medium level of radiative forcing. Using higher-forcing scenarios (e.g. SSP5-8.5) would yield much higher RR in the future.</p>
      <p id="d2e2058">The three wildfires examined here burned over multiple days, each undergoing several complete nocturnal cycles. Overnight burning is relatively new in France, where the vast majority of wildfires were historically extinguished within a single day. Further research is thus needed to elucidate (i) the role of nighttime conditions in overnight burning and the extent to which the so-called nighttime barrier is likely to weaken under ACC <xref ref-type="bibr" rid="bib1.bibx5" id="paren.75"/>, and (ii) the relative contributions of nighttime aridity vs. seasonal drought <xref ref-type="bibr" rid="bib1.bibx38" id="paren.76"/>, as well as the potential role of other meteorological variables such as wind speed <xref ref-type="bibr" rid="bib1.bibx14" id="paren.77"/>. Such analyses may complement the information provided by traditional daytime-based indicators (e.g. FWI) used in climate–fire or attribution studies.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d2e2079">This study aimed at quantifying how ACC has already, and will further, alter the probability of fire weather conditions associated with the three largest wildfires of 2022 across France (Landiras-1, Landiras-2, La Teste-de-Buch). First, we found that warm-season (May–September) FWI gradually intensified over 1959–2023, especially in southern France, making the landscape more and more flammable. Second, we found that return periods of FWI associated with extreme wildfires observed in 2022 were scale-dependent and may range for instance from about 6 (at monthly and regional scales) to more than 101 <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">years</mml:mi></mml:mrow></mml:math></inline-formula> (at fire-duration and local scales) for La Teste-de-Buch wildfire. Finally, attribution metrics indicated that FWI conditions of comparable rarity to those observed during the wildfires were substantially less likely under the natural-forcing-only climate, and that anthropogenic climate change made those conditions approximately 2–10 times more likely in 2022. Under a moderate-emissions pathway, those FWI conditions are projected to become roughly 1 to 2 orders of magnitude more probable by the end of the century, although substantial uncertainty remains across and within models.</p>
</sec>

      
      </body>
    <back><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d2e2094">The code used in this study is available from the first author upon reasonable request.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e2100">Wildfire records were obtained from the <italic>Base de Données sur les Incendies de Forêts en France</italic> (BDIFF) at  <uri>https://www.data.gouv.fr/en/datasets/base-de-donnees-sur-les-incendies-de-forets-en-france-bdiff/</uri> <xref ref-type="bibr" rid="bib1.bibx28" id="paren.78"/>. Daily meteorological variables from the SAFRAN atmospheric reanalysis over France <xref ref-type="bibr" rid="bib1.bibx64" id="paren.79"/> were retrieved from the Météo-France open-data services (<uri>https://meteo.data.gouv.fr</uri>,  last access: 30 May 2026). ERA5 reanalysis fields were downloaded from the Copernicus Climate Data Store (CDS). For reproducibility, we cite the CDS dataset used in this study: <italic>ERA5 hourly data on single levels from 1940 to present</italic> <xref ref-type="bibr" rid="bib1.bibx15" id="paren.80"/> (<ext-link xlink:href="https://doi.org/10.24381/cds.adbb2d47" ext-link-type="DOI">10.24381/cds.adbb2d47</ext-link>). CMIP6 simulations (historical, DAMIP, and ScenarioMIP) were obtained from the Earth System Grid Federation (ESGF) archive (<uri>https://esgf-node.llnl.gov/search/cmip6/</uri>, last access: 30 May 2026), following the CMIP6 and MIP design descriptions <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx24 bib1.bibx39" id="paren.81"/>.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d2e2134">The supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/nhess-26-2637-2026-supplement" xlink:title="pdf">https://doi.org/10.5194/nhess-26-2637-2026-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e2143">SZ performed all analyses and wrote the first draft of the manuscript. SZ, RB, FP, and BR jointly contributed to the study design, the interpretation of the results, and the writing and revision of the manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e2149">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="d2e2155">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="d2e2161">SZ gratefully acknowledges the support of the Sud Provence-Alpes-Côte d'Azur (PACA) region and the Société du Canal de Provence (SCP) for his doctoral project.</p></ack><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e2166">This paper was edited by Jean-Baptiste Filippi and reviewed by Thomas Janssen and one anonymous referee.</p>
  </notes><ref-list>
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