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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-12-1-2021</article-id><title-group><article-title>Evaluating the dependence structure of compound precipitation and wind speed extremes</article-title><alt-title>Evaluating the dependence of compound extremes</alt-title>
      </title-group><?xmltex \runningtitle{Evaluating the dependence of compound extremes}?><?xmltex \runningauthor{J. Zscheischler et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2 aff3">
          <name><surname>Zscheischler</surname><given-names>Jakob</given-names></name>
          <email>jakob.zscheischler@ufz.de</email>
        <ext-link>https://orcid.org/0000-0001-6045-1629</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Naveau</surname><given-names>Philippe</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7231-6210</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff5 aff6">
          <name><surname>Martius</surname><given-names>Olivia</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8645-4702</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Engelke</surname><given-names>Sebastian</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Raible</surname><given-names>Christoph C.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Oeschger Centre for Climate Change Research, University of Bern, Bern, Switzerland</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Climate and Environmental Physics, University of Bern, Sidlerstrasse 5, 3012 Bern, Switzerland</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Computational Hydrosystems, <?xmltex \hack{\break}?>Helmholtz Centre for Environmental Research – UFZ, Leipzig, Germany</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Laboratoire des Sciences du Climat et de l’Environnement, Gif-sur-Yvette, France</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Institute of Geography,  University of Bern, Bern, Switzerland</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Mobiliar Lab for Natural Risks,  University of Bern, Bern, Switzerland</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Research Center for Statistics, University of Geneva, Geneva, Switzerland</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jakob Zscheischler (jakob.zscheischler@ufz.de)</corresp></author-notes><pub-date><day>6</day><month>January</month><year>2021</year></pub-date>
      
      <volume>12</volume>
      <issue>1</issue>
      <fpage>1</fpage><lpage>16</lpage>
      <history>
        <date date-type="received"><day>28</day><month>May</month><year>2020</year></date>
           <date date-type="rev-request"><day>4</day><month>June</month><year>2020</year></date>
           <date date-type="rev-recd"><day>27</day><month>October</month><year>2020</year></date>
           <date date-type="accepted"><day>9</day><month>November</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 </copyright-statement>
        <copyright-year>2021</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/.html">This article is available from https://esd.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e160">Estimating the likelihood of compound climate extremes such as concurrent drought and heatwaves or compound precipitation and wind speed extremes is important for assessing climate risks. Typically, simulations from climate models are used to assess future risks, but it is largely unknown how well the current generation of models represents compound extremes. Here, we introduce a new metric that measures whether the tails of bivariate distributions show a similar dependence structure across different datasets. We analyse compound precipitation and wind extremes in reanalysis data and different high-resolution simulations for central Europe. A state-of-the-art reanalysis dataset (ERA5) is compared to simulations with a weather model (Weather Research and Forecasting – WRF) either driven by observation-based boundary conditions or a global circulation model (Community Earth System Model – CESM) under present-day and future conditions with strong greenhouse gas forcing (Representative Concentration Pathway 8.5 – RCP8.5).
Over the historical period, the high-resolution WRF simulations capture precipitation and wind extremes as well as their response to orographic effects more realistically than ERA5. Thus, WRF simulations driven by observation-based boundary conditions are used as a benchmark for evaluating the dependence structure of wind and precipitation extremes.
Overall, boundary conditions in WRF appear to be the key factor in explaining differences in the dependence behaviour between strong wind and heavy precipitation between simulations. In comparison, external forcings (RCP8.5) are of second order.  Our approach offers new methodological tools to evaluate climate model simulations with respect to compound extremes.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <?pagebreak page2?><p id="d1e172">Compound climate extremes such as co-occurring drought and heat or compound precipitation and wind extremes can have a substantial impact on the natural environment and human systems that often exceeds the impact caused by a single extreme <xref ref-type="bibr" rid="bib1.bibx71 bib1.bibx53 bib1.bibx38 bib1.bibx57" id="paren.1"/>. Over recent years a number of compound extremes have been investigated. For instance, several studies have analysed the dependence between storm surge and heavy precipitation  <xref ref-type="bibr" rid="bib1.bibx64 bib1.bibx68 bib1.bibx3" id="paren.2"/> or extreme runoff <xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx25" id="paren.3"/> to estimate the risk of compound flooding in coastal areas. Compound droughts and heatwaves have been studied for different regions and varying temporal scales  <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx70 bib1.bibx36 bib1.bibx61 bib1.bibx69" id="paren.4"/>. The occurrence rate of compound precipitation and wind extremes has been estimated for the Mediterranean region <xref ref-type="bibr" rid="bib1.bibx53" id="paren.5"/>, Europe <xref ref-type="bibr" rid="bib1.bibx13" id="paren.6"/>, and at the global scale <xref ref-type="bibr" rid="bib1.bibx38" id="paren.7"/>. Other studies have investigated the co-occurrence of hot days and hot nights <xref ref-type="bibr" rid="bib1.bibx65" id="paren.8"/> or the co-occurrence rate of heavy precipitation and snowmelt to estimate the risk of rain-on-snow events <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx51" id="paren.9"/>.
Such a quantification of the occurrence rate of compound extremes is important for assessing the risk of associated impacts today and in the future. Most of the above studies identify compound extremes by thresholding the contributing variables to quantify the occurrence of compound extremes and changes associated with climate change.
However, the dependence structure in the tails is only rarely investigated.
Due to the rarity of compound extremes, a large number of samples is required to obtain robust estimates, making it difficult to rely solely on observational data <xref ref-type="bibr" rid="bib1.bibx54" id="paren.10"/>.</p>
      <p id="d1e206">Large ensemble simulations <xref ref-type="bibr" rid="bib1.bibx14" id="paren.11"/> offer an opportunity to estimate future changes in the occurrence of compound events without running into data limitations <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx6" id="paren.12"/>. However, such simulations need to be interpreted with care as it is often largely unknown how well the employed models represent observed compound events <xref ref-type="bibr" rid="bib1.bibx43" id="paren.13"/>, and differences might be large between models.
Climate models are regularly evaluated based on their ability to represent well-known processes in the climate system and predominantly univariate comparisons with key climate variables <xref ref-type="bibr" rid="bib1.bibx19" id="paren.14"/>, though some multivariate metrics have been explored <xref ref-type="bibr" rid="bib1.bibx56" id="paren.15"/>. Yet little is known about the ability of climate models to capture observed occurrence rates of compound extremes <xref ref-type="bibr" rid="bib1.bibx72" id="paren.16"/>, a challenging task for two primary reasons. First, due to their rarity, a robust quantification of the likelihood of compound extremes requires large amounts of data, thus making it difficult to establish a “ground truth” for many applications. Second, suitable metrics for evaluating multivariate extremes have not been widely tested and applied in a climate context. Such metrics, however, are essential to assess how well models represent compound events, in particular to assess future risks <xref ref-type="bibr" rid="bib1.bibx74" id="paren.17"/>.
When observational data are scarce, process-based model simulations <xref ref-type="bibr" rid="bib1.bibx10" id="paren.18"/> and reanalysis data <xref ref-type="bibr" rid="bib1.bibx38" id="paren.19"/> can be employed to extend or replace purely observational datasets.</p>
      <p id="d1e237">To date, model–data comparisons related to compound extremes have been conducted to a very limited extent, often relying on simplifying assumptions and typically confined to precipitation and temperature. For instance, a high likelihood of compound hot and dry summers has been linked to a strongly negative correlation between summer temperature and precipitation <xref ref-type="bibr" rid="bib1.bibx70" id="paren.20"/>. While there is generally good agreement with respect to this correlation between climate models and observation-based datasets in the Northern Hemisphere, there is strong disagreement in the Southern Hemisphere, for which the models show a much stronger dependence. This finding may suggest that climate models overestimate dependence between summer temperature and precipitation. However, this discrepancy may also be related to the way gridded observation-based datasets are assembled. In particular, for locations without an active measurement station nearby, the mean seasonal cycle is often used to fill gaps in the observational networks <xref ref-type="bibr" rid="bib1.bibx42" id="paren.21"><named-content content-type="pre">e.g.</named-content></xref>. This approach reduces the strength of co-variability between temperature and precipitation in poorly sampled regions, which are mostly in the Southern Hemisphere. Thus, assessing the ability of climate models to represent compound events may reveal underappreciated limitations in gridded observation-based datasets. We are not aware of studies so far that have evaluated the dependence between precipitation and wind speed.</p>
      <p id="d1e248">In this study we focus on compound precipitation and wind extremes, which can have severe socio-economic impacts including human fatalities, impaired critical infrastructure, and economical damage <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx35 bib1.bibx34 bib1.bibx53 bib1.bibx38" id="paren.22"/>.
We investigate differences in the occurrence of compound precipitation and wind extremes for different datasets over a region in central Europe including the Alps. To this end, we introduce a new measure that assesses dissimilarity between the tails of bivariate distributions.
We study an experimental design with two factors. The first factor is the type of boundary conditions in a high-resolution regional weather model, either from reanalysis or a global circulation model. The second factor corresponds to the effect of different climate forcing between today and the future under a high-emission scenario. Our object of study under this design is the dependence between heavy precipitation and strong wind in winter over central Europe. In addition, comparisons with a state-of-the-art reanalysis product are implemented.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
      <p id="d1e262">We use daily precipitation sums and daily maximum wind speed in the extended winter (November–March) from one reanalysis product and three model simulations over a period of 20 years.
The employed reanalysis product is ERA5  <xref ref-type="bibr" rid="bib1.bibx9" id="paren.23"/> from which we use data for the period 1980 to 1999 CE. This reanalysis is generated with an updated numerical weather prediction model and data assimilation system compared to the prior product ERA-Interim <xref ref-type="bibr" rid="bib1.bibx12" id="paren.24"/> and integrates additional data sources. The data are available at a resolution of roughly 30 km (spectral resolution of T639), with 137 vertical levels and hourly output.</p>
      <?pagebreak page3?><p id="d1e271">The three simulations are performed with the Weather Research and Forecasting (WRF) model <xref ref-type="bibr" rid="bib1.bibx58" id="paren.25"/> which is forced with boundary conditions from (i) ERA-Interim <xref ref-type="bibr" rid="bib1.bibx12" id="paren.26"/> (ERAI-WRF), (ii) a period of free-running global climate simulations for the present day (CESM-WRF), and (iii) a period covering the end of the 21st century under  Representative Concentration Pathway 8.5 (CESM-WRF-fut, a high-emission scenario). The global climate simulation is performed with the Community Earth System Model (CESM) <xref ref-type="bibr" rid="bib1.bibx27" id="paren.27"/> for the period 850 to 2100 CE. Details on the setting are described in <xref ref-type="bibr" rid="bib1.bibx33" id="text.28"/> and <xref ref-type="bibr" rid="bib1.bibx52" id="text.29"/>. In this study we use the period 1980 to 1999 CE as the present day and 2080 to 2099 CE as the future.</p>
      <p id="d1e289">The periods of the global simulations and the ERA-Interim period (1980 to 1999 CE) are dynamically downscaled with WRF in version 3.5. WRF is vertically discretized in 40 terrain-following <inline-formula><mml:math id="M1" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula>-coordinate levels. The horizontal resolutions of the four two-way nested domains (Fig. <xref ref-type="fig" rid="Ch1.F1"/>) are 54, 18, 6, and 2 km. The innermost domain covers the box <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mn mathvariant="normal">4.75</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mtext>E</mml:mtext><mml:mo>,</mml:mo><mml:mn mathvariant="normal">15.25</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mtext>E</mml:mtext><mml:mo>]</mml:mo><mml:mo>×</mml:mo><mml:mo>[</mml:mo><mml:mn mathvariant="normal">43.25</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mtext>N</mml:mtext><mml:mo>,</mml:mo><mml:mn mathvariant="normal">48.75</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mtext>N</mml:mtext><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> and is exclusively used in this study. The setup is described in more detail in <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx23" id="text.30"/> and <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx41" id="text.31"/>. Important for this a study is that the convection parameterization is disabled for the simulations at 6 and 2 km resolution; at these scales the model is convection-permitting. This is an important step in improving the simulation of precipitation, though some problems still remain <xref ref-type="bibr" rid="bib1.bibx1" id="paren.32"/>. For adequately simulating wind, the setting of the planetary boundary layer parameterization is key. We use a modified version of the fully non-local scheme developed by <xref ref-type="bibr" rid="bib1.bibx26" id="text.33"/>, which specifically treats effects of the unresolved orography <xref ref-type="bibr" rid="bib1.bibx29" id="paren.34"/>. For the ERAI-WRF simulation we allow analysis nudging of wind, temperature, and humidity above the planetary boundary layer in order to stay close to the large-scale behaviour of the reanalysis data <xref ref-type="bibr" rid="bib1.bibx22" id="paren.35"/>. For the two simulations driven by CESM, nudging is omitted to allow the regional model to correct potential systematic biases of the CESM (e.g. a zonal atmospheric circulation that is too strong in the mid-latitudes; <xref ref-type="bibr" rid="bib1.bibx4" id="altparen.36"/>). The WRF output is provided in hourly resolution.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e384">The four nested domains used in the dynamical downscaling.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f01.png"/>

      </fig>

      <p id="d1e393">We remap the original hourly data to a common regularly spaced grid with 0.25<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial resolution using conservative remapping and subsequently compute daily precipitation sums and daily wind speed maxima. The 0.25<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatial resolution was chosen as it is closest to the original resolution of the ERA5 reanalysis data. Note, however, that all WRF simulations are run at a much higher convection-resolving resolution. The explicit resolution of convection and a much higher resolution of the topography may result in a more accurate representation of the dependence between precipitation and wind extremes in the simulations than in ERA5.
We further note that mean wind speed in ERA5 generally decreases with elevation (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a), which is the opposite of the expected behaviour for the response of wind speed to elevation from observations <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx62" id="paren.37"/> and what is modelled by WRF (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b). The discrepancy in mountainous regions between reanalysis data and observations with respect to wind speed is also evident in other reanalysis datasets such as ERA-Interim <xref ref-type="bibr" rid="bib1.bibx30" id="paren.38"/>, which is the predecessor of ERA5. In contrast, WRF has been shown to also simulate wind speed reasonably well in mountainous terrain <xref ref-type="bibr" rid="bib1.bibx60" id="paren.39"/>. For these reasons – WRF better resolves cloud processes, topography, and wind speed, while ERA5 misrepresents the wind speed gradient with elevation – we use ERAI-WRF as the reference for all analyses.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e430">Relationship between mean winter wind speed and altitude for ERA5 <bold>(a)</bold> and the WRF model (ERAI-WRF simulation) <bold>(b)</bold>.</p></caption>
        <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <label>3</label><title>A measure for evaluating compound extremes</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Measuring tail dependence</title>
      <p id="d1e460">The extreme values of a univariate random variable can be analysed with tools from extreme value theory <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx7 bib1.bibx31 bib1.bibx45" id="paren.40"/>. For multivariate random vectors, the dependence between the largest values in the components becomes important <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx28 bib1.bibx16" id="paren.41"/>.</p>
      <?pagebreak page4?><p id="d1e469">We quickly review the concept of bivariate asymptotic tail dependence and independence <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx50" id="paren.42"/>. Two variables <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> with cumulative distribution functions <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, respectively, are  asymptotically dependent if
            <disp-formula id="Ch1.Ex1"><mml:math id="M9" display="block"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">lim⁡</mml:mo><mml:mrow><mml:mi>q</mml:mi><mml:mo>→</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munder><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>q</mml:mi><mml:mo>∣</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>∈</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>]</mml:mo></mml:mrow></mml:math></disp-formula>
          and asymptotically independent otherwise (i.e. if <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>). The coefficient <inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> is called extremal correlation and represents, after transforming <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to the uniform scale, the probability of one variable being extreme given that the other one is extreme. Note that two variables can be dependent at normal levels but asymptotically independent in the extremes, as in the case for a  bivariate Gaussian distribution <xref ref-type="bibr" rid="bib1.bibx55" id="paren.43"/>. To fine tune the rate of decay towards the asymptotically independent case (<inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>), the residual tail dependence coefficient <inline-formula><mml:math id="M15" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> contains additional information <xref ref-type="bibr" rid="bib1.bibx8" id="paren.44"/>:
            <disp-formula id="Ch1.Ex2"><mml:math id="M16" display="block"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:munder><mml:mo movablelimits="false">lim⁡</mml:mo><mml:mrow><mml:mi>q</mml:mi><mml:mo>→</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munder><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>log⁡</mml:mi><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>q</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mrow/><mml:mo>∈</mml:mo><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:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          <inline-formula><mml:math id="M17" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> is equal to 1 for asymptotically dependent variables, while for asymptotically independent variables <inline-formula><mml:math id="M18" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula>  indicates if <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are positively (<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>) or negatively (<inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>) associated in their extremes. Thus, the pair of coefficients <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> summarizes the tail dependence structure of <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e935">Because both coefficients <inline-formula><mml:math id="M26" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M27" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> are defined as a limit value, a usual way to analyse the behaviour of a bivariate tail dependence structure between two variables is to compute empirical estimates for varying threshold levels <inline-formula><mml:math id="M28" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> and then visually inspect their behaviour as <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>→</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>. We estimate <inline-formula><mml:math id="M30" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M31" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> with the function taildep from the R package extRemes <xref ref-type="bibr" rid="bib1.bibx21" id="paren.45"/>.</p>
      <p id="d1e995">To estimate <inline-formula><mml:math id="M32" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> empirically we use a high quantile for which a reasonably large number of data are available. For these reasons we generally estimate <inline-formula><mml:math id="M33" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> at <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>. Heavy precipitation events and extreme winds that lead to large damage can be linked through storms or föhn events across neighbouring locations with a lag of several days. To take this aspect into account, we estimate <inline-formula><mml:math id="M35" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> using a local block maxima approach, which is motivated by <xref ref-type="bibr" rid="bib1.bibx17" id="text.46"/>. We thus first compute the daily precipitation and wind speed maxima for varying block sizes ranging from 0.25<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (approximately 20–30 km) to 1.75<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (that is, a maximum of three grid points in any direction, or 100–200 km) and up to 5 d (i.e. maximum of 2 d before and after the day of interest).</p>
      <p id="d1e1054">We further assess whether estimates of <inline-formula><mml:math id="M38" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> are significantly different from 0. To this end, we bootstrap the data by randomly shuffling the temporal order of one variable to break the dependence structure. The coefficient <inline-formula><mml:math id="M39" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> is then estimated as above. Estimates of <inline-formula><mml:math id="M40" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> are considered significantly different from 0 if they are larger than 95 % of the bootstrapped estimates.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Measuring differences in bivariate extremal dependence structures</title>
      <p id="d1e1086">Classical tail coefficients like <inline-formula><mml:math id="M41" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> are informative summaries to assess the extremal dependence between two univariate random variables, say <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,  but they cannot quantify the difference in extremal dependence  between two bivariate random vectors, say <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>=</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>=</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>. For example, <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">χ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> can be computed  between heavy precipitation and strong winds computed from one dataset, e.g. ERA5, and compared to  a <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">χ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for a second dataset, e.g. ERAI-WRF.
But it would also be very convenient to have a single number to tell us if the extremal dependences between these two bivariate random vectors are different and, if so, by how much.
Recent work by
<xref ref-type="bibr" rid="bib1.bibx44" id="text.47"/>
showed that the well-known Kullback–Leibler (KL) divergence used in signal processing can be tailored  to the framework of  extreme value theory. The approach has been applied to cluster climate data according to their bivariate extremal behaviour <xref ref-type="bibr" rid="bib1.bibx63" id="paren.48"/>. However,
to our knowledge, multivariate  extremal divergence measures have never been applied to the analysis of compound weather and climate events.
By complementing  tail coefficients, this new tool could shed new light on  the  joint behaviour of  heavy precipitation and strong winds  across  our different datasets.</p>
      <p id="d1e1249">The KL divergence is defined on marginals which are normalized to standard Pareto distributions.
A risk function (<inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>:</mml:mo><mml:msup><mml:mi mathvariant="double-struck">R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>→</mml:mo><mml:mi mathvariant="double-struck">R</mml:mi></mml:mrow></mml:math></inline-formula>) is used to describe the extreme region in each of the bivariate distributions. There are different choices for the risk function. Taking the sum or the maximum gives similar results for asymptotically dependent data. In<?pagebreak page5?> addition, the minimum also covers asymptotic independence. The sum is defined as <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and the minimum as <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>min⁡</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, with <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. Hence, we consider those for which the sum (or minimum) of the components exceeds a given high quantile <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msubsup><mml:mi>q</mml:mi><mml:mi>u</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> of <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> corresponding to an exceedance probability <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>∈</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> to be extreme points. Varying the threshold <inline-formula><mml:math id="M56" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula> alters the extremal region of interest. For each of the two bivariate distributions, the set <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msup><mml:mi>A</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mi>r</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:msubsup><mml:mi>q</mml:mi><mml:mi>u</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> is partitioned into a fixed number <inline-formula><mml:math id="M59" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> of disjoint sets <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msubsup><mml:mi>A</mml:mi><mml:mi>W</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e1547">For two random samples (<inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">…</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>,</mml:mo><mml:msubsup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mi>n</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">…</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>,</mml:mo><mml:msubsup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mi>n</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) from the distributions <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, the empirical proportions of data points belonging to set <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mi>W</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> are computed as
            <disp-formula id="Ch1.Ex3"><mml:math id="M66" display="block"><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>w</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">#</mml:mi><mml:mfenced open="{" close="}"><mml:mrow><mml:mi>i</mml:mi><mml:mo>:</mml:mo><mml:msubsup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>∈</mml:mo><mml:msubsup><mml:mi>A</mml:mi><mml:mi>w</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mi mathvariant="italic">#</mml:mi><mml:mfenced open="{" close="}"><mml:mrow><mml:mi>i</mml:mi><mml:mo>:</mml:mo><mml:mi>r</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced><mml:mo>&gt;</mml:mo><mml:msubsup><mml:mi>q</mml:mi><mml:mi>u</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:mi>w</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi>W</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          The difference between the extremal behaviours of the two distributions can then be measured as the KL divergence between the two multinomial distributions defined through these proportions, i.e.
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M67" display="block"><mml:mtable columnspacing="1em" rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mn mathvariant="normal">12</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mi>D</mml:mi><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>w</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>W</mml:mi></mml:munderover><mml:mfenced close=")" open="("><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover><mml:mi>w</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>w</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced><mml:mi>log⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>w</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>/</mml:mo><mml:msubsup><mml:mover accent="true"><mml:mi>p</mml:mi><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover><mml:mi>w</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          Note that this divergence is symmetric and since it is a non-parametric statistic it does not require additional model assumptions. Equation (<xref ref-type="disp-formula" rid="Ch1.E1"/>) contrasts  differences among extremal dependence structures for both asymptotically dependent and asymptotically independent data.
The number of partitioning sets <inline-formula><mml:math id="M68" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> is a free parameter. If it is chosen too high, many sets will be empty, resulting in an undefined KL divergence. If it is too small, only a rough summary is computed but not really an estimate of tail dependence. We chose <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> in this study based on the simulation study shown in Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/>.
Under suitable assumptions the statistic  <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mn mathvariant="normal">12</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> follows a <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">χ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>(</mml:mo><mml:mi>W</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> distribution in the limit as the sample size goes to <inline-formula><mml:math id="M72" display="inline"><mml:mi mathvariant="normal">∞</mml:mi></mml:math></inline-formula>, which allows us to estimate whether distances are significantly different from 0.</p>
      <p id="d1e2005">The approach is illustrated in Figs. <xref ref-type="fig" rid="Ch1.F3"/> and <xref ref-type="fig" rid="Ch1.F4"/> with <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>. Figure <xref ref-type="fig" rid="Ch1.F3"/> shows daily precipitation sums and maximum wind speed at grid point 9<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 46.75<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N on the original scale (a, d) with margins normalized to the exponential scale (b, e) and to standard Pareto distributions (c, f) for ERAI-WRF (a–c) and CESM-WRF (d–f). The shown grid point reaches the highest tail dependence <inline-formula><mml:math id="M76" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> at <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula> in the ERAI-WRF simulation. The colours in all subpanels and the dashed lines in Fig. <xref ref-type="fig" rid="Ch1.F3"/>c and f highlight the three disjoint sets <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mrow><mml:mo>(</mml:mo><mml:mi>j</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> (see above).
At the exponential scale moderate and large extremes can be seen well, whereas at the Pareto scale only very extreme values can be easily visually identified.
Figure <xref ref-type="fig" rid="Ch1.F4"/> illustrates <inline-formula><mml:math id="M80" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> (a) and <inline-formula><mml:math id="M81" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> (c) for the distributions of the two simulations and the divergence based on Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) with “sum” (b) and “min” (d) as the risk function, including 95 % confidence intervals  of the empirical estimates. The estimates of <inline-formula><mml:math id="M82" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M83" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> start to diverge somewhat for <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>, suggesting different tail behaviour (uncertainty ranges are estimated based on the R function chiplot from the package evd; <xref ref-type="bibr" rid="bib1.bibx59" id="altparen.49"/>). This impression is confirmed by the estimates of the KL divergence: for most thresholds <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula> and for both choices of the risk function  the KL divergence is outside the
<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mn mathvariant="normal">95</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> quantile of the limiting <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">χ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>(</mml:mo><mml:mi>W</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> distribution of the statistic <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mn mathvariant="normal">12</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> under the null hypothesis of equal tail dependence structures.
This means that we can conclude that the two distributions have significantly different tail behaviour.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e2230">Scatterplots of daily precipitation and wind speed maxima in November–March (1980–1999) for the location with the highest tail dependence <inline-formula><mml:math id="M89" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>) in the ERAI-WRF simulations <bold>(a–c)</bold>. CESM-WRF simulations for the same location are shown in <bold>(d–f)</bold>. Shown are the original values <bold>(a, d)</bold>, values after transformation into exponential marginals <bold>(b, e)</bold>, and values after transformation into Pareto marginals <bold>(c, f)</bold>. The colours highlight the three separating sets <inline-formula><mml:math id="M91" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> to compute the KL divergence (see Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>) for a high threshold (see the main text). In <bold>(c)</bold> and <bold>(f)</bold>, the three sets are separated by dashed lines. Note that for the main analyses in the paper we use <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e2304">Illustration of the distance metrics between bivariate tails for the location with the highest estimated tail dependence <inline-formula><mml:math id="M93" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> at <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula> in ERAI-WRF.
<bold>(a, c)</bold> Tail dependence parameters <inline-formula><mml:math id="M95" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> <bold>(a)</bold> and <inline-formula><mml:math id="M96" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula> <bold>(c)</bold> for daily precipitation sums and daily maximum wind speed for different quantile-based thresholds <inline-formula><mml:math id="M97" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula>. Shading highlights the 95 % confidence intervals. Grey: ERAI-WRF. Red: CESM-WRF.
<bold>(b, d)</bold> Two different Kullback–Leibler (KL) divergences (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/> with <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>) for the tails of the bivariate precipitation–wind speed distribution between ERAI-WRF and CESM-WRF (solid lines). Dashed lines highlight the 95 % confidence interval of the null hypothesis assuming an equal dependence structure. <bold>(b)</bold> KL divergence based on the minimum (i.e. <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mo>min⁡</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>&gt;</mml:mo><mml:mi>u</mml:mi></mml:mrow></mml:math></inline-formula>). <bold>(d)</bold> KL divergence based on the sum (i.e. <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>&gt;</mml:mo><mml:mi>u</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f04.png"/>

        </fig>

      <p id="d1e2440">Note that in the bivariate case, a simple approach to quantify the difference in tail dependence would be the difference between <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">χ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">χ</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. However, for two distributions with the same <inline-formula><mml:math id="M103" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> coefficient but a different dependence structure, it is impossible to distinguish the two cases. In a way,  <inline-formula><mml:math id="M104" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> only focuses on the “diagonal”. Furthermore, while in this work we focus on the bivariate case, the KL divergence defined by Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) could easily be implemented with higher dimensions <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mo>,</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>,</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">…</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/></mml:mrow></mml:math></inline-formula>) because it is only based on counting points in different subsets. In contrast, using <inline-formula><mml:math id="M106" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula>, the number of pairs will increase rapidly with the dimension <inline-formula><mml:math id="M107" display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula>. In addition, <inline-formula><mml:math id="M108" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> coefficients will only capture pairwise dependencies.</p>
      <p id="d1e2537">We investigate how well different simulations represent the bivariate tail behaviour of daily precipitation sums and wind speed maxima in winter by comparing ERA5, CESM-WRF, and CESM-WRF-fut against ERAI-WRF with the divergence as defined in Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) based on the maxima over the spatio-temporal blocks that maximize tail dependence <inline-formula><mml:math id="M109" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> at <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>. Using local block maxima ensures that <inline-formula><mml:math id="M111" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M112" display="inline"><mml:mover accent="true"><mml:mi mathvariant="italic">χ</mml:mi><mml:mo mathvariant="normal">¯</mml:mo></mml:mover></mml:math></inline-formula>, and the KL divergence measure very extremal upper tail behaviour. Note, however, that this approach leads to different block sizes depending on the location, which makes a direct comparison in space difficult. For the computation of the KL divergence (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>) we use <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula> and  “sum” as the risk function. We further perform a sensitivity test using <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>∈</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.85</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>.  Furthermore, the marginals have been transformed into a Pareto scale through ranking. The choice of marginal transformation only has a minor influence on the KL divergence (see Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/>).</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
      <?pagebreak page6?><p id="d1e2632">We first present a simple correlation analysis based on the Spearman's rank correlation coefficient. Daily precipitation sums and maximum wind speed are generally strongly correlated in winter in most areas of the study domain except in the northwest of Italy (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). All model simulations show a relatively consistent pattern, whereas ERA5 shows negative correlations at the southern slopes of the Alps along the northwestern Italian border (Fig. <xref ref-type="fig" rid="Ch1.F5"/>b). Most correlations are significant (<inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d1e2651">When considering only the dependence in the tails based on <inline-formula><mml:math id="M116" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> and including a spatial and temporal neighbourhood, the spatial patterns look quite different (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). The WRF simulations  show a highly heterogeneous picture with strong local variations, generally strong dependence over most parts of the Alps and close to the Adriatic coast, and weak dependence otherwise (Fig. <xref ref-type="fig" rid="Ch1.F6"/>a, c, d). Overall, ERAI-WRF shows slightly higher tail dependence compared to the WRF simulations driven by CESM. In contrast to the WRF simulations, in ERA5 tail dependence varies rather smoothly in space, with higher values in northeastern Italy and along the eastern border of France (Fig. <xref ref-type="fig" rid="Ch1.F6"/>b).</p>

      <?xmltex \floatpos{p}?><?pagebreak page8?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e2669">Spearman's rank correlation between daily precipitation sums and maximum wind speed in the extended winter (November–March). <bold>(a)</bold> ERAI-WRF, <bold>(b)</bold> ERA5, <bold>(c)</bold> CESM-WRF, <bold>(d)</bold> CESM-WRF-fut. Non-significant correlations (<inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) are marked with a cross.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f05.png"/>

      </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e2705">Tail dependence (<inline-formula><mml:math id="M118" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> with <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>) between daily precipitation sums and maximum wind speed in the extended winter (November–March). Tail dependence was computed considering block maxima over a maximum range of 5 d temporally and 1.75<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> spatially. <bold>(a)</bold> ERAI-WRF, <bold>(b)</bold> ERA5, <bold>(c)</bold> CESM-WRF, <bold>(d)</bold> CESM-WRF-fut. Non-significant values based on bootstraps with the same maximum block size (<inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) are marked with a cross.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f06.png"/>

      </fig>

      <p id="d1e2767">The block sizes that attain the maximum tail dependence <inline-formula><mml:math id="M122" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> for precipitation and wind extremes for each pixel are shown in Fig. <xref ref-type="fig" rid="Ch1.F7"/>. On average for 75 % of the pixels, the maximum is attained with no temporal lag (blue in Fig. <xref ref-type="fig" rid="Ch1.F7"/>). In contrast, there seems to be a shift in space, as maxima tend to co-occur in neighbouring grid points: block sizes with larger than minimal (0.25<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) spatial extent occur on average in 60 % of all locations (lighter colours in Fig. <xref ref-type="fig" rid="Ch1.F7"/>). This means that extremes in daily precipitation sums and wind extremes tend to occur on the same day but potentially not at exactly the same location; they occur with some distance apart. In particular in the south of the Alps but also in some regions north of the Alps, this distance is 1.75<inline-formula><mml:math id="M124" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, or about 100–200 km (very light colours in Fig. <xref ref-type="fig" rid="Ch1.F7"/>).
The strongest agreement of the dependence patterns is between CESM-WRF and CESM-WRF-fut, which agree for half of the locations in the maximizing block size. In contrast, the agreement is 29 % between ERAI-WRF and ERA5 and 39 % between ERAI-WRF and CESM-WRF. Note that grid points at the boundaries cannot attain maxima with block sizes larger than one grid point as no data values are available outside the study domain.</p>
      <p id="d1e2804">The tails between winter daily precipitation sums and wind speed maxima show a significantly different dependence structure between ERAI-WRF and CESM-WRF in 46 % of all grid points, mostly in Switzerland and in the north of the study domain but also in many regions in northern Italy  (Fig. <xref ref-type="fig" rid="Ch1.F8"/>a). The percentage of grid points with significantly different tail behaviour is slightly higher for the comparison of ERAI-WRF and ERA5 (49 %), though in this case most of the differences occur in grid points located along a wide diagonal band from the southwest to the northeast through the entire study domain (Fig. <xref ref-type="fig" rid="Ch1.F8"/>b). Interestingly, the comparison of ERAI-WRF with CESM-WRF-fut results in only 36 % of pixels with significantly different tail behaviour (Fig. <xref ref-type="fig" rid="Ch1.F8"/>c). Thus, CESM-WRF-fut agrees better with ERAI-WRF with respect to the tail behaviour than CESM-WRF<?pagebreak page7?> and ERAI-WRF.
Finally, only 18 % of pixels show significantly different tail behaviour when comparing CESM-WRF and CESM-WRF-fut (Fig. <xref ref-type="fig" rid="Ch1.F8"/>d), indicating the pair with the largest number of grid points at which no significant difference in the tail behaviour could be found. The numbers of grid points with significantly different tail behaviour depend somewhat on the threshold <inline-formula><mml:math id="M125" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula> and generally decrease with increasing extremeness (that is, increasing <inline-formula><mml:math id="M126" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula>), but the differences between the different pairwise comparisons remain similar (Table <xref ref-type="table" rid="Ch1.T1"/>). In particular, the differences between ERAI-WRF and CESM-WRF and between ERAI-WRF and CESM-WRF-fut are generally larger than the differences between CESM-WRF and CESM-WRF-fut, indicating that the main finding, namely that boundary conditions in WRF appear to be the key factor in explaining differences in the dependence behaviour between wind and precipitation extremes, is robust for different parameter values of the difference measure.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e2835">Sensitivity analysis of KL divergence (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>). Reported is the fraction of grid points with a significantly different (<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) precipitation–wind speed dependence structure between two datasets for different thresholds <inline-formula><mml:math id="M128" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula> (with <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>). The case <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.90</mml:mn></mml:mrow></mml:math></inline-formula> is shown in Fig. <xref ref-type="fig" rid="Ch1.F8"/>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.80</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.85</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.90</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">ERAI-WRF vs. CESM-WRF</oasis:entry>
         <oasis:entry colname="col2">0.61</oasis:entry>
         <oasis:entry colname="col3">0.54</oasis:entry>
         <oasis:entry colname="col4">0.46</oasis:entry>
         <oasis:entry colname="col5">0.32</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ERAI-WRF vs. ERA5</oasis:entry>
         <oasis:entry colname="col2">0.59</oasis:entry>
         <oasis:entry colname="col3">0.53</oasis:entry>
         <oasis:entry colname="col4">0.49</oasis:entry>
         <oasis:entry colname="col5">0.40</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ERAI-WRF vs. CESM-WRF-fut</oasis:entry>
         <oasis:entry colname="col2">0.53</oasis:entry>
         <oasis:entry colname="col3">0.45</oasis:entry>
         <oasis:entry colname="col4">0.36</oasis:entry>
         <oasis:entry colname="col5">0.27</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CESM-WRF vs. CESM-WRF-fut</oasis:entry>
         <oasis:entry colname="col2">0.30</oasis:entry>
         <oasis:entry colname="col3">0.23</oasis:entry>
         <oasis:entry colname="col4">0.18</oasis:entry>
         <oasis:entry colname="col5">0.19</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><label>Figure 7</label><caption><p id="d1e3039">Blocks for which the maximum tail dependence (<inline-formula><mml:math id="M135" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> with <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>) between daily precipitation sums and maximum wind speed in the extended winter (November–March) is attained (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). Block sizes range from 0.25<inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and 1 d to 1.75<inline-formula><mml:math id="M138" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and 5 d. Blue, green, and orange refer to time lags of 1, 3, and 5 d, respectively. Darker shading illustrates higher spatial proximity. The colour bars next to the maps show the number of grid points of that colour in the corresponding map. <bold>(a)</bold> ERAI-WRF, <bold>(b)</bold> ERA5, <bold>(c)</bold> CESM-WRF, <bold>(d)</bold> CESM-WRF-fut. Grid points with non-significant tail dependence are marked with a cross (see Fig. <xref ref-type="fig" rid="Ch1.F6"/>). </p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f07.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><label>Figure 8</label><caption><p id="d1e3105">Locations for which the dependence between the tails of daily precipitation sums and wind speed maxima is significantly different based on the KL divergence according to Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) with <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> (dark grey, with <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). Dependence is assessed for the blocks that attain maximum tail dependence <inline-formula><mml:math id="M142" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> (at <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>) (see Fig. <xref ref-type="fig" rid="Ch1.F6"/>). Shown are comparisons between <bold>(a)</bold> ERAI-WRF and CESM-WRF, <bold>(b)</bold> ERAI-WRF and ERA5, <bold>(c)</bold> CESM-WRF and CESM-WRF-fut, and <bold>(d)</bold> ERAI-WRF and CESM-WRF-fut.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f08.png"/>

      </fig>

</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
      <p id="d1e3195">We have introduced a new metric for comparing tail dependence structures between wind and precipitation extremes in reanalysis data and weather model simulations.
In our WRF simulations, the type of  boundary conditions, either ERAI or CESM,  appears to have a stronger effect on the coupling between high wind and heavy precipitation  than the change in external forcing (present-day and future) in CESM
(Fig. <xref ref-type="fig" rid="Ch1.F8"/>). This suggests that the studied dependence structures between the tails of precipitation sums and wind speed maxima in winter are a rather robust feature of the combination of models (boundary conditions plus a high-resolution weather model) and thus also somewhat determined by the boundary conditions. In consequence this also means that here we are probably detecting rather stable dynamical features that are largely independent of strong external forcing such as (much) higher mean temperatures.
Because the model setting determines the dependence structure, sampling uncertainties in this dependence, for instance to robustly assess risks under future climate conditions, would require a range of different climate and weather model combinations.</p>
      <?pagebreak page9?><p id="d1e3200">The employed block maxima approach (Fig. <xref ref-type="fig" rid="Ch1.F6"/>) has the effect that precipitation and wind extremes are considered together even if they might occur some distance apart in either time or space. This is to ensure that extremes in wind and precipitation are considered together if they emerge from the same atmospheric processes (e.g. föhn). At the same time, the block maxima approach can help diagnose why datasets differ in their tail dependence structure of precipitation and wind extremes, for instance if the spatio-temporal blocks for which extremes are attained differ strongly.</p>
      <p id="d1e3205">Regarding the optimal spatial and temporal lags between wind and precipitation extremes there is generally good agreement that along the southern slopes of the Alps the dependence is maximized for precipitation and wind extremes occurring on the same day and up to 1.75<inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> apart (lightest blue in Fig. <xref ref-type="fig" rid="Ch1.F7"/>), which could be related to föhn events that lead to heavy precipitation north of the mountain range and extreme winds on the southern slopes or vice versa. Indeed, heavy precipitation events on the Alpine southern side are often related to high moisture transport ahead of cold fronts that is associated with moderate winds that are not as strong as potential föhn gusts on the Alpine northern side <xref ref-type="bibr" rid="bib1.bibx47" id="paren.50"/>.</p>
      <p id="d1e3222">Most heavy precipitation events in the investigation domain in winter are associated with extratropical cyclones. Within extratropical cyclones, wind speed maxima and precipitation maxima are often linked to fronts and conveyor belts <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx5 bib1.bibx49 bib1.bibx46" id="paren.51"/>, and this may result in co-located extremes. However, important modulations of both extreme wind and precipitation patterns by the local complex orography are to be expected <xref ref-type="bibr" rid="bib1.bibx67 bib1.bibx2" id="paren.52"/>,<?pagebreak page10?> and such local föhn effects, channelling effects, flow blocking, and many more might be captured by the high-resolution WRF simulations but not in ERA5.</p>
      <p id="d1e3232">Overall, ERA5 shows quite a different behaviour for the Spearman's rank correlation (Fig. <xref ref-type="fig" rid="Ch1.F5"/>) and simple tail dependence <inline-formula><mml:math id="M145" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> (Fig. <xref ref-type="fig" rid="Ch1.F6"/>) compared to the high-resolution weather model simulations. Spatial patterns are much smoother, probably related to the much coarser spatial resolution (30 km compared to the original 2 km in the WRF simulations). Furthermore, wind speeds over high mountains are unrealistic, as they decrease with height rather than increase (Fig. <xref ref-type="fig" rid="Ch1.F2"/>). These limitations render ERA5 unsuitable as a benchmark for the tail dependence between precipitation and wind extremes in the Alpine area with its complex orography.
Presently, homogenized gridded wind observations of good quality are not available for this region. Therefore, driving a well-calibrated high-resolution weather model with observation-based boundary conditions is currently the best benchmark to study compound wind and precipitation extremes.</p>
      <p id="d1e3248">We would like to note that in our setup ERAI-WRF is nudged to the driving reanalysis ERA-Interim. The reason for this is that the simulation should stay close to the large-scale behaviour of the reanalysis data. As mentioned in the Data section, we only use wind, temperature, and humidity above the planetary boundary layer and the nudging is not strong. Nevertheless, the behaviour of extremes might be changed due to the modification of the dynamical equations to some extent, but we think that this effect is minor. Furthermore, precipitation is not nudged.</p>
      <p id="d1e3251">Evaluating how well models represent tail dependencies may help select those models that are fit for purpose <xref ref-type="bibr" rid="bib1.bibx37" id="paren.53"/> regarding the analysis of compound events <xref ref-type="bibr" rid="bib1.bibx74" id="paren.54"/> for a range of different event types <xref ref-type="bibr" rid="bib1.bibx54" id="paren.55"/>. In particular, when the interest lies in the simulation of impacts, the approach may help decide when multivariate bias adjustment approaches would need to be employed <xref ref-type="bibr" rid="bib1.bibx20" id="paren.56"/>, as univariate bias adjustment might increase biases in impacts that depend on multiple correlated drivers <xref ref-type="bibr" rid="bib1.bibx73" id="paren.57"/>.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e3277">Evaluating the ability of climate models to represent the likelihood of compound climate extremes is important for well-informed climate risk assessments. In this study we investigated differences in the tail behaviour of precipitation and wind extremes in winter between different weather model simulations and a reanalysis dataset for a region in central Europe. Employing a new metric to measure differences in the tail behaviour of bivariate distributions, we found that simulations of the same model pair with different external forcing conditions (climate change conditions) differ less than simulations for present-day conditions with different<?pagebreak page11?> boundary data. Our results further suggest that reanalysis data are not suitable as a benchmark for the analysis of compound precipitation and wind extremes over complex terrain such as the Alps. Overall, differences between model simulations (different boundary conditions and weather and/or climate models) can be substantial. Our results suggest that climate impact modelling needs to take uncertainties related to the simulation of compound extremes  into account to provide robust risk assessments for today and the future.</p><?xmltex \hack{\clearpage}?>
</sec>

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

<?pagebreak page12?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><?xmltex \opttitle{Determining $W$}?><title>Determining <inline-formula><mml:math id="M146" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula></title>
      <p id="d1e3299">We simulated <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2000</mml:mn></mml:mrow></mml:math></inline-formula> samples of <inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in the outer power Clayton copula, which is in the domain of attraction of the logistic extreme value distribution. We chose the parameters such that the limiting <inline-formula><mml:math id="M150" display="inline"><mml:mi mathvariant="italic">χ</mml:mi></mml:math></inline-formula> coefficients are 0.4 and 0.55, which means one model with weaker and one with stronger dependence, respectively. Using the KL divergence for a probability threshold of <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula>, we compare the samples of <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">X</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for the dependence settings weak–weak, strong–strong, and weak–strong and plot in each case the probability of rejecting the null hypothesis of equal tail dependence structures. Note that the former two cases are in line with the null hypothesis, whereas the latter case does not satisfy the null hypothesis. We conduct the experiment for both known margins and empirically normalized margins, as well as for different numbers of sets <inline-formula><mml:math id="M154" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> in the KL divergence statistic.</p>
      <p id="d1e3405">Figures <xref ref-type="fig" rid="App1.Ch1.S1.F9"/> and <xref ref-type="fig" rid="App1.Ch1.S1.F10"/> show the Type I error of rejecting the null hypothesis in the case in which we have the same tail dependence based on 500 repetitions of the simulation based on empirical ranking of the marginals (Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F9"/>) and using the true marginals (Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F10"/>). For both normalizations the significance level of 5 % is in general well attained throughout all numbers of sets. The figures also contain the power of the test when the tail dependence structures are different. After <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> the power stabilizes and it seems to decrease slightly when the number of sets is chosen too large. We therefore use <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> throughout the paper. Note that this is only one particular simulation setup, and the results for the optimal number of sets can change depending on sample size and the strength of tail dependence.</p><?xmltex \hack{\newpage}?><?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F9"><?xmltex \currentcnt{A1}?><label>Figure A1</label><caption><p id="d1e3443">Simulation study using empirical margins.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f09.png"/>

      </fig>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F10"><?xmltex \currentcnt{A2}?><label>Figure A2</label><caption><p id="d1e3455">Simulation study using true margins.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://esd.copernicus.org/articles/12/1/2021/esd-12-1-2021-f10.png"/>

      </fig>

<?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e3470">ERA5 data are available from the ECMWF website: <uri>https://www.ecmwf.int/en/forecasts/datasets/reanalysis-datasets/era5</uri> <xref ref-type="bibr" rid="bib1.bibx9" id="paren.58"/>. The outputs from the WRF simulations are very large data files and are available from Christoph Raible (christoph.raible@climate.unibe.ch).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3482">JZ and PN conceived the idea and study design. PN and SE developed the code for the new metric. CCR provided the model simulations. OM helped with the interpretation of the results. JZ performed all analyses, created all figures, and wrote the first draft. All authors contributed substantially to the writing and revising of the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3488">The authors declare that they have no competing interests.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e3494">This article is part of the special issue “Understanding compound weather and climate events and related impacts (BG/ESD/HESS/NHESS inter-journal SI)”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3500">This research was supported by a Short-Term Scientific Mission from the European COST Action DAMOCLES (CA17109). We thank Martina Messmer for creating Fig. 1. The  CESM  and  WRF  simulations  were performed   on   the   supercomputing   architecture   of   the   Swiss National Supercomputing Centre (CSCS; Lugano, Switzerland). Part of Philippe Naveau's research was supported by the FRAISE-LEFE-MANU grant and  the French Agence National de la Recherche through ANR-Melody and ANR-TRex.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e3505">This research has been supported by the Swiss National Science Foundation (grant nos. 179876, 172745, and 178751), the Helmholtz Initiative and Networking Fund (Young Investigator
Group COMPOUNDX, grant agreement VH-NG-1537), and the European Cooperation in Science and Technology (grant no. CA17109).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3512">This paper was edited by Gabriele Messori and reviewed by Theophile Caby and two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><label>Ban et al.(2014)Ban, Schmidli, and Schaer</label><?label Ban2014?><mixed-citation>Ban, N., Schmidli, J., and Schaer, C.: Evaluation of the convection-resolving
regional climate modeling approach in decade-long simulations, J.
Geophys. Res.-Atmos., 119, 889–7907,
<ext-link xlink:href="https://doi.org/10.1002/2014JD021478" ext-link-type="DOI">10.1002/2014JD021478</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Barry(2008)</label><?label Barry2008?><mixed-citation>
Barry, R. G.: Mountain weather and climate, Cambridge University Press, Cambridge, UK,
2008.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Bevacqua et al.(2019)Bevacqua, Maraun, Vousdoukas, Voukouvalas, Vrac,
Mentaschi, and Widmann</label><?label Bevacqua2019?><mixed-citation>Bevacqua, E., Maraun, D., Vousdoukas, M. I., Voukouvalas, E., Vrac, M.,
Mentaschi, L., and Widmann, M.: Higher probability of compound flooding from
precipitation and storm surge in Europe under anthropogenic climate change,
Science Advances, 5, eaaw5531, <ext-link xlink:href="https://doi.org/10.1126/sciadv.aaw5531" ext-link-type="DOI">10.1126/sciadv.aaw5531</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Bracegirdle et al.(2013)Bracegirdle, Shuckburgh, Sallee, Wang,
Meijers, Bruneau, Phillips, and Wilcox</label><?label Bracegirdle2013?><mixed-citation>Bracegirdle, T. J., Shuckburgh, E., Sallee, J.-B., Wang, Z., Meijers, A. J. S.,
Bruneau, N., Phillips, T., and Wilcox, L. J.: Assessment of surface winds
over the Atlantic, Indian, and Pacific Ocean sectors of the Southern Ocean in
CMIP5 models: historical bias, forcing response, and state dependence,
J. Geophys. Res-Atmos., 118, 547–562,
<ext-link xlink:href="https://doi.org/10.1002/jgrd.50153" ext-link-type="DOI">10.1002/jgrd.50153</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Catto and Pfahl(2013)</label><?label Catto2013?><mixed-citation>Catto, J. L. and Pfahl, S.: The importance of fronts for extreme precipitation,
J. Geophys. Res-Atmos., 118, 10791–10801,
<ext-link xlink:href="https://doi.org/10.1002/jgrd.50852" ext-link-type="DOI">10.1002/jgrd.50852</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx6"><label>Champagne et al.(2020)Champagne, Leduc, Coulibaly, and
Arain</label><?label Champagne2020?><mixed-citation>Champagne, O., Leduc, M., Coulibaly, P., and Arain, M. A.: Winter hydrometeorological extreme events modulated by large-scale atmospheric circulation in southern Ontario, Earth Syst. Dynam., 11, 301–318, <ext-link xlink:href="https://doi.org/10.5194/esd-11-301-2020" ext-link-type="DOI">10.5194/esd-11-301-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>Coles(2001)</label><?label coles2001introduction?><mixed-citation>Coles, S.: An introduction to statistical modeling of extreme values, Springer, London, UK,
<ext-link xlink:href="https://doi.org/10.1007/978-1-4471-3675-0" ext-link-type="DOI">10.1007/978-1-4471-3675-0</ext-link>, 2001.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Coles et al.(1999)Coles, Heffernan, and Tawn</label><?label Coles1999?><mixed-citation>
Coles, S., Heffernan, J., and Tawn, J.: Dependence measures for extreme value
analyses, Extremes, 2, 339–365, 1999.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Copernicus Climate Change Service(2017)</label><?label era5?><mixed-citation>Copernicus Climate Change Service (C3S): ERA5: Fifth generation of ECMWF
atmospheric reanalyses of the global climate, <uri>https://www.ecmwf.int/en/forecasts/datasets/reanalysis-datasets/era5</uri> (last access: 28 May 2020), Copernicus Climate Change Service, Reading, UK, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Couasnon et al.(2020)Couasnon, Eilander, Muis, Veldkamp, Haigh, Wahl,
Winsemius, and Ward</label><?label Couasnon2020?><mixed-citation>Couasnon, A., Eilander, D., Muis, S., Veldkamp, T. I. E., Haigh, I. D., Wahl, T., Winsemius, H. C., and Ward, P. J.: Measuring compound flood potential from river discharge and storm surge extremes at the global scale, Nat. Hazards Earth Syst. Sci., 20, 489–504, <ext-link xlink:href="https://doi.org/10.5194/nhess-20-489-2020" ext-link-type="DOI">10.5194/nhess-20-489-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>Davison and Huser(2015)</label><?label Davison2015?><mixed-citation>
Davison, A. and Huser, R.: Statistics of Extremes, Annu. Rev. Stat.
Appl., 2, 203–235, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx12"><?xmltex \def\ref@label{{Dee et~al.(2011)Dee, Uppala, Simmons, Berrisford, Poli, Kobayashi,
Andrae, Balmaseda, Balsamo, Bauer, Bechtold, Beljaars, van~de Berg, Bidlot,
Bormann, Delsol, Dragani, Fuentes, Geer, Haimberger, Healy, Hersbach,
H{\'{o}}lm, Isaksen, K{\aa}llberg, K{\"{o}}hler, Matricardi, McNally, Monge-Sanz,
Morcrette, Park, Peubey, de~Rosnay, Tavolato, Th{\'{e}}paut, and
Vitart}}?><label>Dee et al.(2011)Dee, Uppala, Simmons, Berrisford, Poli, Kobayashi,
Andrae, Balmaseda, Balsamo, Bauer, Bechtold, Beljaars, van de Berg, Bidlot,
Bormann, Delsol, Dragani, Fuentes, Geer, Haimberger, Healy, Hersbach,
Hólm, Isaksen, Kållberg, Köhler, Matricardi, McNally, Monge-Sanz,
Morcrette, Park, Peubey, de Rosnay, Tavolato, Thépaut, and
Vitart</label><?label Dee2011?><mixed-citation>Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P., Kobayashi,
S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P., Bechtold, P.,
Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N., Delsol, C.,
Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy, S. B.,
Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M.,
Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park,
B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and
Vitart, F.: The ERA-Interim reanalysis: configuration and performance of the
data assimilation system, Q. J. Roy. Meteor.
Soc., 137, 553–597, <ext-link xlink:href="https://doi.org/10.1002/qj.828" ext-link-type="DOI">10.1002/qj.828</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>De Luca et al.(2020)De Luca, Messori, Pons, and Faranda</label><?label DeLuca2020?><mixed-citation>De Luca, P., Messori, G., Pons, F. M. E., and Faranda, D.: Dynamical systems
theory sheds new light on compound climate extremes in Europe and Eastern
North America, Q. J. Roy. Meteor. Soc.,  146, 1636–1650,
<ext-link xlink:href="https://doi.org/10.1002/qj.3757" ext-link-type="DOI">10.1002/qj.3757</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>Deser et al.(2020)Deser, Lehner, Rodgers, Ault, Delworth, DiNezio,
Fiore, Frankignoul, Fyfe, Horton, Kay, Knutti, Lovenduski, Marotzke,
McKinnon, Minobe, Randerson, Screen, Simpson, and Ting</label><?label Deser2020?><mixed-citation>Deser, C., Lehner, F., Rodgers, K. B., Ault, T., Delworth, T. L., DiNezio,
P. N., Fiore, A., Frankignoul, C., Fyfe, J. C., Horton, D. E., Kay, J. E.,
Knutti, R., Lovenduski, N. S., Marotzke, J., McKinnon, K. A., Minobe, S.,
Randerson, J., Screen, J. A., Simpson, I. R., and Ting, M.: Insights from
Earth system model initial-condition large ensembles and future prospects,
Nat. Clim. Change, 10, 1–10, <ext-link xlink:href="https://doi.org/10.1038/s41558-020-0731-2" ext-link-type="DOI">10.1038/s41558-020-0731-2</ext-link>, 2020.</mixed-citation></ref>
      <?pagebreak page14?><ref id="bib1.bibx15"><?xmltex \def\ref@label{{Embrechts et~al.(1997)Embrechts, Kl\"{u}ppelberg, and
Mikosch}}?><label>Embrechts et al.(1997)Embrechts, Klüppelberg, and
Mikosch</label><?label Embrechts1997?><mixed-citation>
Embrechts, P., Klüppelberg, C., and Mikosch, T.: Modelling Extremal Events:
for Insurance and Finance, Springer, London, UK, 1997.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Engelke and Ivanovs(2021)</label><?label Engelke2021?><mixed-citation>Engelke, S. and Ivanovs, J.: Sparse Structures for Multivariate Extremes,
Annu. Rev. Stat. Appl., 8, <ext-link xlink:href="https://doi.org/10.1146/annurev-statistics-040620-041554" ext-link-type="DOI">10.1146/annurev-statistics-040620-041554</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx17"><label>Ferreira and de Haan(2015)</label><?label Ferreira2015?><mixed-citation>
Ferreira, A. and de Haan, L.: On the block maxima method in extreme value
theory: PWM estimators, Ann. Stat., 43, 276–298, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx18"><?xmltex \def\ref@label{{Fink et~al.(2009)Fink, Br\"{u}cher, Ermert, Kr\"{u}ger, and
Pinto}}?><label>Fink et al.(2009)Fink, Brücher, Ermert, Krüger, and
Pinto</label><?label Fink2009?><mixed-citation>Fink, A. H., Brücher, T., Ermert, V., Krüger, A., and Pinto, J. G.: The European storm Kyrill in January 2007: synoptic evolution, meteorological impacts and some considerations with respect to climate change, Nat. Hazards Earth Syst. Sci., 9, 405–423, <ext-link xlink:href="https://doi.org/10.5194/nhess-9-405-2009" ext-link-type="DOI">10.5194/nhess-9-405-2009</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx19"><label>Flato et al.(2013)Flato, Marotzke, Abiodun, Braconnot, Chou, Collins,
Cox, Driouech, Emori, Eyring, Forest, Gleckler, Guilyardi, Jakob, Kattsov,
Reason, and Rummukainen</label><?label Flato2013?><mixed-citation>Flato, G., Marotzke, J., Abiodun, B., Braconnot, P., Chou, S., Collins, W.,
Cox, P., Driouech, F., Emori, S., Eyring, V., Forest, C., Gleckler, P.,
Guilyardi, E., Jakob, C., Kattsov, V., Reason, C., and Rummukainen, M.:
Evaluation of Climate Models, in: Climate Change 2013: The Physical
Science Basis, Contribution of Working Group I to the Fifth Assessment Report
of the Intergovernmental Panel on Climate Change, edited by: Stocker, T. F.,
Qin, D., Plattner, G.-K., Tignor, M., Allen, S. K., Boschung, J., Nauels, A.,
Xia, Y., Bex, V., and Midgley, P. M.,
Cambridge
University Press, Cambridge, United Kingdom and New York, USA,
741–866,
<ext-link xlink:href="https://doi.org/10.1017/CBO9781107415324.020" ext-link-type="DOI">10.1017/CBO9781107415324.020</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx20"><?xmltex \def\ref@label{{Fran\c{c}ois et~al.(2020)Fran\c{c}ois, Vrac, Cannon, Robin, and
Allard}}?><label>François et al.(2020)François, Vrac, Cannon, Robin, and
Allard</label><?label Francois2020?><mixed-citation>François, B., Vrac, M., Cannon, A. J., Robin, Y., and Allard, D.: Multivariate bias corrections of climate simulations: which benefits for which losses?, Earth Syst. Dynam., 11, 537–562, <ext-link xlink:href="https://doi.org/10.5194/esd-11-537-2020" ext-link-type="DOI">10.5194/esd-11-537-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx21"><label>Gilleland and Katz(2016)</label><?label Gilleland2016?><mixed-citation>Gilleland, E. and Katz, R. W.: extRemes 2.0: An Extreme Value Analysis
Package in R, J. Stat. Softw., 72, 1–39,
<ext-link xlink:href="https://doi.org/10.18637/jss.v072.i08" ext-link-type="DOI">10.18637/jss.v072.i08</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx22"><?xmltex \def\ref@label{{G\'{o}mez-Navarro et~al.({2015})G\'{o}mez-Navarro, Raible, and
Dierer}}?><label>Gómez-Navarro et al.(2015)Gómez-Navarro, Raible, and
Dierer</label><?label Gomez-Navarro2015?><mixed-citation>Gómez-Navarro, J. J., Raible, C. C., and Dierer, S.: Sensitivity of the WRF model to PBL parametrisations and nesting techniques: evaluation of wind storms over complex terrain, Geosci. Model Dev., 8, 3349–3363, <ext-link xlink:href="https://doi.org/10.5194/gmd-8-3349-2015" ext-link-type="DOI">10.5194/gmd-8-3349-2015</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx23"><?xmltex \def\ref@label{{G\'{o}mez-Navarro et~al.(2018)G\'{o}mez-Navarro, Raible, Bozhinova,
Martius, Garc\'{\i}a~Valero, and Mont\'{a}vez}}?><label>Gómez-Navarro et al.(2018)Gómez-Navarro, Raible, Bozhinova,
Martius, García Valero, and Montávez</label><?label Gomez-Navarro2018?><mixed-citation>Gómez-Navarro, J. J., Raible, C. C., Bozhinova, D., Martius, O., García Valero, J. A., and Montávez, J. P.: A new region-aware bias-correction method for simulated precipitation in areas of complex orography, Geosci. Model Dev., 11, 2231–2247, <ext-link xlink:href="https://doi.org/10.5194/gmd-11-2231-2018" ext-link-type="DOI">10.5194/gmd-11-2231-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx24"><label>Graf et al.(2019)Graf, Scherrer, Schwierz, Begert, Martius, Raible,
and Brönnimann</label><?label Graf2019?><mixed-citation>Graf, M., Scherrer, S. C., Schwierz, C., Begert, M., Martius, O., Raible,
C. C., and Brönnimann, S.: Near-surface mean wind in Switzerland:
Climatology, climate model evaluation and future scenarios, Int.
J. Climatol., 39, 4798–4810, <ext-link xlink:href="https://doi.org/10.1002/joc.6108" ext-link-type="DOI">10.1002/joc.6108</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx25"><label>Hendry et al.(2019)Hendry, Haigh, Nicholls, Winter, Neal, Wahl,
Joly-Laugel, and Darby</label><?label Hendry2019?><mixed-citation>Hendry, A., Haigh, I. D., Nicholls, R. J., Winter, H., Neal, R., Wahl, T., Joly-Laugel, A., and Darby, S. E.: Assessing the characteristics and drivers of compound flooding events around the UK coast, Hydrol. Earth Syst. Sci., 23, 3117–3139, <ext-link xlink:href="https://doi.org/10.5194/hess-23-3117-2019" ext-link-type="DOI">10.5194/hess-23-3117-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx26"><label>Hong and Lim(2020)</label><?label Hong2006?><mixed-citation>
Hong, S. and Lim, J.: The WRF single-moment 6-class micro-physics scheme
(WSM6), Journal of Korean Meteorology Society, 42, 129–151, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx27"><label>Hurrell et al.(2013)Hurrell, Holland, Gent, Ghan, Kay, Kushner,
Lamarque, Large, Lawrence, Lindsay, Lipscomb, Long, Mahowald, Marsh, Neale,
Rasch, Vavrus, Vertenstein, Bader, Collins, Hack, Kiehl, and
Marshall</label><?label Hurrell2013?><mixed-citation>Hurrell, J. W., Holland, M. M., Gent, P. R., Ghan, S., Kay, J. E., Kushner,
P. J., Lamarque, J. F., Large, W. G., Lawrence, D., Lindsay, K., Lipscomb,
W. H., Long, M. C., Mahowald, N., Marsh, D. R., Neale, R. B., Rasch, P.,
Vavrus, S., Vertenstein, M., Bader, D., Collins, W. D., Hack, J. J., Kiehl,
J., and Marshall, S.: The Community Earth System Model A Framework for
Collaborative Research, B. Am. Meteorol. Soc.,
94, 1339–1360, <ext-link xlink:href="https://doi.org/10.1175/BAMS-D-12-00121.1" ext-link-type="DOI">10.1175/BAMS-D-12-00121.1</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx28"><label>Huser and Wadsworth(2020)</label><?label Huser2020?><mixed-citation>Huser, R. and Wadsworth, J. L.: Advances in Statistical Modeling of Spatial
Extremes, WIREs Comput. Stat., e1537, <ext-link xlink:href="https://doi.org/10.1002/wics.1537" ext-link-type="DOI">10.1002/wics.1537</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx29"><label>Jimenez and Dudhia(2012)</label><?label Jimenez2012?><mixed-citation>Jimenez, P. A. and Dudhia, J.: Improving the Representation of Resolved and
Unresolved Topographic Effects on Surface Wind in the WRF Model, J.
Appl. Meteorol. Clim., 51, 300–316,
<ext-link xlink:href="https://doi.org/10.1175/JAMC-D-11-084.1" ext-link-type="DOI">10.1175/JAMC-D-11-084.1</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx30"><label>Jones et al.(2017)Jones, Harpham, Troccoli, Gschwind, Ranchin, Wald,
Goodess, and Dorling</label><?label Jones2017?><mixed-citation>Jones, P. D., Harpham, C., Troccoli, A., Gschwind, B., Ranchin, T., Wald, L., Goodess, C. M., and Dorling, S.: Using ERA-Interim reanalysis for creating datasets of energy-relevant climate variables, Earth Syst. Sci. Data, 9, 471–495, <ext-link xlink:href="https://doi.org/10.5194/essd-9-471-2017" ext-link-type="DOI">10.5194/essd-9-471-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx31"><label>Katz et al.(2002)Katz, Parlange, and Naveau</label><?label Katz2002?><mixed-citation>
Katz, R. W., Parlange, M. B., and Naveau, P.: Statistics of extremes in
hydrology, Adv. Water Resour., 25, 1287–1304, 2002.</mixed-citation></ref>
      <ref id="bib1.bibx32"><label>Ledford and Tawn(1997)</label><?label LedfordTawn1997?><mixed-citation>
Ledford, A. W. and Tawn, J. A.: Modelling dependence within joint tail regions,
J. R. Stat. Soc. Ser. B Stat. Methodol., 59, 475–499, 1997.</mixed-citation></ref>
      <ref id="bib1.bibx33"><label>Lehner et al.(2015)Lehner, Joos, Raible, Mignot, Born, Keller, and
Stocker</label><?label Lehner2015?><mixed-citation>Lehner, F., Joos, F., Raible, C. C., Mignot, J., Born, A., Keller, K. M., and Stocker, T. F.: Climate and carbon cycle dynamics in a CESM simulation from 850 to 2100 CE, Earth Syst. Dynam., 6, 411–434, <ext-link xlink:href="https://doi.org/10.5194/esd-6-411-2015" ext-link-type="DOI">10.5194/esd-6-411-2015</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx34"><label>Liberato(2014)</label><?label Liberato2014?><mixed-citation>Liberato, M. L.: The 19 January 2013 windstorm over the North Atlantic:
large-scale dynamics and impacts on Iberia, Weather and Climate Extremes,
5–6, 16–28, <ext-link xlink:href="https://doi.org/10.1016/j.wace.2014.06.002" ext-link-type="DOI">10.1016/j.wace.2014.06.002</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx35"><label>Lin et al.(2010)Lin, Emanuel, Smith, and Vanmarcke</label><?label Lin2010?><mixed-citation>Lin, N., Emanuel, K. A., Smith, J. A., and Vanmarcke, E.: Risk assessment of
hurricane storm surge for New York City, J. Geophys. Res.-Atmos., 115, D18121, <ext-link xlink:href="https://doi.org/10.1029/2009JD013630" ext-link-type="DOI">10.1029/2009JD013630</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx36"><label>Manning et al.(2019)Manning, Widmann, Bevacqua, Loon, Maraun, and
Vrac</label><?label Manning2019?><mixed-citation>Manning, C., Widmann, M., Bevacqua, E., Loon, A. F. V., Maraun, D., and Vrac,
M.: Increased probability of compound long-duration dry and hot events in
Europe during summer (1950–2013), Environ. Res.
Lett., 14, 094006, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ab23bf" ext-link-type="DOI">10.1088/1748-9326/ab23bf</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx37"><label>Maraun et al.(2017)Maraun, Shepherd, Widmann, Zappa, Walton,
Gutierrez, Hagemann, Richter, Soares, Hall, and Mearns</label><?label Maraun2017?><mixed-citation>Maraun, D., Shepherd, T. G., Widmann, M., Zappa, G., Walton, D., Gutierrez,
J. M., Hagemann, S., Richter, I., Soares, P. M. M., Hall, A., and Mearns,
L. O.: Towards process-informed bias correction of climate change
simulations, Nat. Clim. Change, 7, 764–773, <ext-link xlink:href="https://doi.org/10.1038/nclimate3418" ext-link-type="DOI">10.1038/nclimate3418</ext-link>,
2017.</mixed-citation></ref>
      <ref id="bib1.bibx38"><label>Martius et al.(2016)Martius, Pfahl, and
Chevalier</label><?label martius2016global?><mixed-citation>
Martius, O., Pfahl, S., and Chevalier, C.: A global quantification of compound
precipitation and wind extremes, Geophys. Res. Lett., 43,
7709–7717, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx39"><label>Mazdiyasni and AghaKouchak(2015)</label><?label Mazdiyasni2015?><mixed-citation>Mazdiyasni, O. and AghaKouchak, A.: Substantial increase in concurrent
droughts and heatwaves in the United States, P. Natl.
Acad. Sci. USA, 112, 11484–11489, <ext-link xlink:href="https://doi.org/10.1073/pnas.1422945112" ext-link-type="DOI">10.1073/pnas.1422945112</ext-link>,
2015.</mixed-citation></ref>
      <ref id="bib1.bibx40"><label>Messmer et al.(2017)</label><?label Messmer2017?><mixed-citation>Messmer, M., Gómez-Navarro, J. J., and Raible, C. C.: Sensitivity experiments on the response of Vb cyclones to sea surface temperature and soil moisture changes, Earth Syst. Dynam., 8, 477–493, <ext-link xlink:href="https://doi.org/10.5194/esd-8-477-2017" ext-link-type="DOI">10.5194/esd-8-477-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx41"><label>Messmer et al.(2020)</label><?label Messmer2020?><mixed-citation>Messmer, M., Raible, C. C., and Gómez-Navarro, J. J.: Impact of climate
change on the climatology of Vb cyclones, Tellus A, 72, 1–18, <ext-link xlink:href="https://doi.org/10.1080/16000870.2020.1724021" ext-link-type="DOI">10.1080/16000870.2020.1724021</ext-link>, 2020.</mixed-citation></ref>
      <?pagebreak page15?><ref id="bib1.bibx42"><label>Mitchell and Jones(2005)</label><?label Mitchell2005?><mixed-citation>Mitchell, T. D. and Jones, P. D.: An improved method of constructing a database
of monthly climate observations and associated high-resolution grids,
Int. J. Climatol., 25, 693–712, <ext-link xlink:href="https://doi.org/10.1002/joc.1181" ext-link-type="DOI">10.1002/joc.1181</ext-link>,
2005.</mixed-citation></ref>
      <ref id="bib1.bibx43"><label>Musselman et al.(2018)Musselman, Lehner, Ikeda, Clark, Prein, Liu,
Barlage, and Rasmussen</label><?label Musselman2018?><mixed-citation>Musselman, K., Lehner, F., Ikeda, K., Clark, M., Prein, A., Liu, C., Barlage,
M., and Rasmussen, R.: Projected increases and shifts in rain-on-snow flood
risk over western North America, Nat. Clim. Change, 8, 808–812,
<ext-link xlink:href="https://doi.org/10.1038/s41558-018-0236-4" ext-link-type="DOI">10.1038/s41558-018-0236-4</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx44"><label>Naveau et al.(2014)Naveau, Guillou, and Rietsch</label><?label Naveau2014?><mixed-citation>
Naveau, P., Guillou, A., and Rietsch, T.: A non-parametric entropy-based
approach to detect changes in climate extremes, J. Roy.
Stat. Soc. B, 76, 861–884, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx45"><label>Naveau et al.(2020)Naveau, Hannart, and Ribes</label><?label Naveau2020?><mixed-citation>Naveau, P., Hannart, A., and Ribes, A.: Statistical Methods for Extreme Event
Attribution in Climate Science, Annu. Rev. Stat.
Appl., 7, 89–110, <ext-link xlink:href="https://doi.org/10.1146/annurev-statistics-031219-041314" ext-link-type="DOI">10.1146/annurev-statistics-031219-041314</ext-link>,
2020.</mixed-citation></ref>
      <ref id="bib1.bibx46"><label>Pantillon et al.(2020)Pantillon, Adler, Corsmeier, Knippertz, Wieser,
and Hansen</label><?label Pantillon2020?><mixed-citation>Pantillon, F., Adler, B., Corsmeier, U., Knippertz, P., Wieser, A., and Hansen,
A.: Formation of Wind Gusts in an Extratropical Cyclone in Light of Doppler
Lidar Observations and Large-Eddy Simulations, Mon. Weather Rev., 148,
353–375, <ext-link xlink:href="https://doi.org/10.1175/Mwr-D-19-0241.1" ext-link-type="DOI">10.1175/Mwr-D-19-0241.1</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx47"><label>Panziera and Germann(2010)</label><?label Panziera2010?><mixed-citation>Panziera, L. and Germann, U.: The relation between airflow and orographic
precipitation on the southern side of the Alps as revealed by weather radar,
Q. J. Roy. Meteor. Soc., 136, 222–238,
<ext-link xlink:href="https://doi.org/10.1002/qj.544" ext-link-type="DOI">10.1002/qj.544</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx48"><label>Parton et al.(2010)Parton, Dore, and Vaughan</label><?label Parton2010?><mixed-citation>Parton, G., Dore, A., and Vaughan, G.: A climatology of mid-tropospheric
mesoscale strong wind events as observed by the MST radar, Aberystwyth,
Meteorol. Appl., 17, 340–354, <ext-link xlink:href="https://doi.org/10.1002/met.203" ext-link-type="DOI">10.1002/met.203</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx49"><label>Pfahl et al.(2014)Pfahl, Madonna, Boettcher, Joos, and
Wernli</label><?label Pfahl2014?><mixed-citation>Pfahl, S., Madonna, E., Boettcher, M., Joos, H., and Wernli, H.: Warm Conveyor
Belts in the ERA-Interim Dataset (1979–2010). Part II: Moisture Origin and
Relevance for Precipitation, J. Climate, 27, 27–40, <ext-link xlink:href="https://doi.org/10.1175/Jcli-D-13-00223.1" ext-link-type="DOI">10.1175/Jcli-D-13-00223.1</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx50"><label>Poon et al.(2003)Poon, Rockinger, and Tawn</label><?label poon2003extreme?><mixed-citation>
Poon, S.-H., Rockinger, M., and Tawn, J.: Extreme value dependence in financial
markets: Diagnostics, models, and financial implications, Rev. Financ. Stud., 17, 581–610, 2003.</mixed-citation></ref>
      <ref id="bib1.bibx51"><label>Poschlod et al.(2020)Poschlod, Zscheischler, Sillmann, Wood, and
Ludwig</label><?label Poschlod2020?><mixed-citation>Poschlod, B., Zscheischler, J., Sillmann, J., Wood, R. R., and Ludwig, R.:
Climate change effects on hydrometeorological compound events over southern
Norway, Weather and Climate Extremes, 28, 100253,
<ext-link xlink:href="https://doi.org/10.1016/j.wace.2020.100253" ext-link-type="DOI">10.1016/j.wace.2020.100253</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx52"><label>Raible et al.(2018)Raible, Messmer, Lehner, Stocker, and
Blender</label><?label Raible2018?><mixed-citation>Raible, C. C., Messmer, M., Lehner, F., Stocker, T. F., and Blender, R.: Extratropical cyclone statistics during the last millennium and the 21st century, Clim. Past, 14, 1499–1514, <ext-link xlink:href="https://doi.org/10.5194/cp-14-1499-2018" ext-link-type="DOI">10.5194/cp-14-1499-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx53"><label>Raveh-Rubin and Wernli(2015)</label><?label Raveh-Rubin2015?><mixed-citation>Raveh-Rubin, S. and Wernli, H.: Large-scale wind and precipitation extremes in
the Mediterranean: A climatological analysis for 1979–2012, Q.
J. Roy. Meteor. Soc., 141, 2404–2417,
<ext-link xlink:href="https://doi.org/10.1002/qj.2531" ext-link-type="DOI">10.1002/qj.2531</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx54"><label>Ridder et al.(2020)Ridder, Pitman, Westra, Ukkola, Do, Bador,
Hirsch, Evans, Luca, and Zscheischler</label><?label Ridder2020?><mixed-citation>Ridder, N., Pitman, A., Westra, S., Ukkola, A., Do, H., Bador, M., Hirsch, A.,
Evans, J., Luca, A. D., and Zscheischler, J.: Global hotspots for the
occurrence of compound events, Nat. Commun., 11, 5956, <ext-link xlink:href="https://doi.org/10.1038/s41467-020-19639-3" ext-link-type="DOI">10.1038/s41467-020-19639-3</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx55"><label>Sibuya(1960)</label><?label sibuya1960bivariate?><mixed-citation>
Sibuya, M.: Bivariate extreme statistics, Ann. I.
Stat. Math., 11, 195–210, 1960.</mixed-citation></ref>
      <ref id="bib1.bibx56"><label>Sippel et al.(2017)Sippel, Zscheischler, Mahecha, Orth, Reichstein,
Vogel, and Seneviratne</label><?label Sippel2017?><mixed-citation>Sippel, S., Zscheischler, J., Mahecha, M. D., Orth, R., Reichstein, M., Vogel, M., and Seneviratne, S. I.: Refining multi-model projections of temperature extremes by evaluation against land–atmosphere coupling diagnostics, Earth Syst. Dynam., 8, 387–403, <ext-link xlink:href="https://doi.org/10.5194/esd-8-387-2017" ext-link-type="DOI">10.5194/esd-8-387-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx57"><label>Sippel et al.(2018)Sippel, Reichstein, Ma, Mahecha, Lange, Flach, and
Frank</label><?label Sippel2018?><mixed-citation>Sippel, S., Reichstein, M., Ma, X., Mahecha, M. D., Lange, H., Flach, M., and
Frank, D.: Drought, Heat, and the Carbon Cycle: a Review, Current Climate
Change Reports, 4, 266–286, <ext-link xlink:href="https://doi.org/10.1007/s40641-018-0103-4" ext-link-type="DOI">10.1007/s40641-018-0103-4</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx58"><label>Skamarock et al.(2008)Skamarock, Klemp, Dudhia, Gill, Barker, Wang,
and Powers</label><?label Skamarock:2008?><mixed-citation>
Skamarock, W. C., Klemp, J. B., Dudhia, J., Gill, D. O., Barker, D. M., Wang,
W., and Powers, J. G.: A description of the advanced research WRF version 3,
Technical Report, TN-475+STR, National Center for Atmospheric Research, Boulder, CO, USA, 113 pp.,  2008.</mixed-citation></ref>
      <ref id="bib1.bibx59"><label>Stephenson(2002)</label><?label evd2002?><mixed-citation>Stephenson, A. G.: evd, Extreme Value Distributions, R News, 2.0, availabe at:
<uri>https://CRAN.R-project.org/doc/Rnews/</uri> (last access: 28 May 2020), 2002.</mixed-citation></ref>
      <ref id="bib1.bibx60"><label>Stucki et al.(2016)Stucki, Dierer, Welker, Gómez-Navarro, Raible,
Martius, and Brönnimann</label><?label Stucki2016?><mixed-citation>Stucki, P., Dierer, S., Welker, C., Gómez-Navarro, J. J., Raible, C. C.,
Martius, O., and Brönnimann, S.: Evaluation of downscaled wind speeds and
parameterised gusts for recent and historical windstorms in Switzerland,
Tellus A, 68, 31820,
<ext-link xlink:href="https://doi.org/10.3402/tellusa.v68.31820" ext-link-type="DOI">10.3402/tellusa.v68.31820</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx61"><label>Sutanto et al.(2020)Sutanto, Vitolo, Napoli, D’Andrea, and
Lanen</label><?label Sutanto2020?><mixed-citation>Sutanto, S. J., Vitolo, C., Napoli, C. D., D’Andrea, M., and Lanen, H. A. V.:
Heatwaves, droughts, and fires: Exploring compound and cascading dry hazards
at the pan-European scale, Environ. Int., 134, 105276,
<ext-link xlink:href="https://doi.org/10.1016/j.envint.2019.105276" ext-link-type="DOI">10.1016/j.envint.2019.105276</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx62"><label>Telesca et al.(2020)Telesca, Guignard, Laib, and
Kanevski</label><?label Telesca2020?><mixed-citation>Telesca, L., Guignard, F., Laib, M., and Kanevski, M.: Analysis of temporal
properties of extremes of wind measurements from 132 stations over
Switzerland, Renew. Energ., 145, 1091–1103,
<ext-link xlink:href="https://doi.org/10.1016/j.renene.2019.06.089" ext-link-type="DOI">10.1016/j.renene.2019.06.089</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx63"><label>Vignotto et al.(2020)Vignotto, Engelke, and
Zscheischler</label><?label Vignotto2020?><mixed-citation>
Vignotto, E., Engelke, S., and Zscheischler, J.: Clustering bivariate
dependences in the extremes of climate variables, Weather and Climate Extremes, in review, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx64"><label>Wahl et al.(2015)Wahl, Jain, Bender, Meyers, and Luther</label><?label Wahl2015?><mixed-citation>Wahl, T., Jain, S., Bender, J., Meyers, S. D., and Luther, M. E.: Increasing
risk of compound flooding from storm surge and rainfall for major US cities,
Nat. Clim. Change, 5, 1–6, <ext-link xlink:href="https://doi.org/10.1038/nclimate2736" ext-link-type="DOI">10.1038/nclimate2736</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx65"><label>Wang et al.(2020)Wang, Chen, Tett, Yan, Zhai, Feng, and
Xia</label><?label Wang2020?><mixed-citation>Wang, J., Chen, Y., Tett, S. F., Yan, Z., Zhai, P., Feng, J., and Xia, J.:
Anthropogenically-driven increases in the risks of summertime compound hot
extremes, Nat. Commun., 11, <ext-link xlink:href="https://doi.org/10.1038/s41467-019-14233-8" ext-link-type="DOI">10.1038/s41467-019-14233-8</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx66"><label>Ward et al.(2018)Ward, Couasnon, Eilander, Haigh, Hendry, Muis,
Veldkamp, Winsemius, and Wahl</label><?label ward2018dependence?><mixed-citation>Ward, P. J., Couasnon, A., Eilander, D., Haigh, I. D., Hendry, A., Muis, S.,
Veldkamp, T. I., Winsemius, H. C., and Wahl, T.: Dependence between high
sea-level and high river discharge increases flood hazard in global deltas
and estuaries, Environ. Res. Lett., 13, 084012, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/aad400" ext-link-type="DOI">10.1088/1748-9326/aad400</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx67"><label>Whiteman(2000)</label><?label Whiteman2000?><mixed-citation>
Whiteman, C. D.: Mountain meteorology fundamentals and applications, Oxford
University Press, New York, USA, 2000.</mixed-citation></ref>
      <ref id="bib1.bibx68"><label>Zheng et al.(2013)Zheng, Westra, and Sisson</label><?label zheng2013quantifying?><mixed-citation>
Zheng, F., Westra, S., and Sisson, S. A.: Quantifying the dependence between
extreme rainfall and storm surge in the coastal zone, J. Hydrol.,
505, 172–187, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx69"><label>Zscheischler and Fischer(2020)</label><?label Zscheischler2020b?><mixed-citation>Zscheischler, J. and Fischer, E.: The record-breaking compound hot and dry
2018 growing season in Germany, Weather and Climate Extremes, 19, 100270,
<ext-link xlink:href="https://doi.org/10.1007/s00484-020-01951-8" ext-link-type="DOI">10.1007/s00484-020-01951-8</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx70"><label>Zscheischler and Seneviratne(2017)</label><?label zscheischler2017dependence?><mixed-citation>Zscheischler, J. and Seneviratne, S. I.: Dependence of drivers affects risks
associated with compound events, Science Advances, 3, e1700263, <ext-link xlink:href="https://doi.org/10.1126/sciadv.1700263" ext-link-type="DOI">10.1126/sciadv.1700263</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx71"><label>Zscheischler et al.(2014)Zscheischler, Michalak, Schwalm, Mahecha,
Huntzinger, Reichstein, Berthier, Ciais, Cook, El-Masri, Huang, Ito, Jain,
King, Lei, Lu, Mao, Peng, Poulter, Ricciuto, Shi, Tao, Tian, Viovy, Wang,
Wei, Yang, and Zeng</label><?label Zscheischler2014?><mixed-citation>Zscheischler, J., Michalak, A. M., Schwalm, C., Mahecha, M. D., Huntzinger,
D. N., Reichstein, M., Berthier<?pagebreak page16?>, G., Ciais, P., Cook, R. B., El-Masri, B.,
Huang, M., Ito, A., Jain, A., King, A., Lei, H., Lu, C., Mao, J., Peng, S.,
Poulter, B., Ricciuto, D., Shi, X., Tao, B., Tian, H., Viovy, N., Wang, W.,
Wei, Y., Yang, J., and Zeng, N.: Impact of large-scale climate extremes on
biospheric carbon fluxes: An intercomparison based on MsTMIP data, Global
Biogeochem. Cy., 28, 585–600, <ext-link xlink:href="https://doi.org/10.1002/2014GB004826" ext-link-type="DOI">10.1002/2014GB004826</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx72"><label>Zscheischler et al.(2018)Zscheischler, Westra, Hurk, Seneviratne,
Ward, Pitman, AghaKouchak, Bresch, Leonard, Wahl, and
Zhang</label><?label zscheischler2018future?><mixed-citation>Zscheischler, J., Westra, S., Hurk, B. J., Seneviratne, S. I., Ward, P. J.,
Pitman, A., Agha Kouchak, A., Bresch, D. N., Leonard, M., Wahl, T., and Zhang,
X.: Future climate risk from compound events, Nat. Clim. Change, 8,
469–477, 2018.
 </mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bibx73"><label>Zscheischler et al.(2019)Zscheischler, Fischer, and
Lange</label><?label Zscheischler2019?><mixed-citation>Zscheischler, J., Fischer, E. M., and Lange, S.: The effect of univariate bias adjustment on multivariate hazard estimates, Earth Syst. Dynam., 10, 31–43, <ext-link xlink:href="https://doi.org/10.5194/esd-10-31-2019" ext-link-type="DOI">10.5194/esd-10-31-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx74"><?xmltex \def\ref@label{{Zscheischler et~al.(2020)Zscheischler, Martius, Westra, Bevacqua,
Raymond, Horton, van~den Hurk, AghaKouchak, J\'{e}z\'{e}quel, Mahecha,
Maraun, Ramos, Ridder, Thiery, and Vignotto}}?><label>Zscheischler et al.(2020)Zscheischler, Martius, Westra, Bevacqua,
Raymond, Horton, van den Hurk, AghaKouchak, Jézéquel, Mahecha,
Maraun, Ramos, Ridder, Thiery, and Vignotto</label><?label Zscheischler2020?><mixed-citation>Zscheischler, J., Martius, O., Westra, S., Bevacqua, E., Raymond, C., Horton,
R. M., van den Hurk, B., Agha Kouchak, A., Jézéquel, A., Mahecha,
M. D., Maraun, D., Ramos, A. M., Ridder, N., Thiery, W., and Vignotto, E.: A
typology of compound weather and climate events, Nature Reviews Earth and
Environment, 1, 333–347, <ext-link xlink:href="https://doi.org/10.1038/s43017-020-0060-z" ext-link-type="DOI">10.1038/s43017-020-0060-z</ext-link>, 2020.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Evaluating the dependence structure of compound precipitation and wind speed extremes</article-title-html>
<abstract-html><p>Estimating the likelihood of compound climate extremes such as concurrent drought and heatwaves or compound precipitation and wind speed extremes is important for assessing climate risks. Typically, simulations from climate models are used to assess future risks, but it is largely unknown how well the current generation of models represents compound extremes. Here, we introduce a new metric that measures whether the tails of bivariate distributions show a similar dependence structure across different datasets. We analyse compound precipitation and wind extremes in reanalysis data and different high-resolution simulations for central Europe. A state-of-the-art reanalysis dataset (ERA5) is compared to simulations with a weather model (Weather Research and Forecasting – WRF) either driven by observation-based boundary conditions or a global circulation model (Community Earth System Model – CESM) under present-day and future conditions with strong greenhouse gas forcing (Representative Concentration Pathway 8.5 – RCP8.5).
Over the historical period, the high-resolution WRF simulations capture precipitation and wind extremes as well as their response to orographic effects more realistically than ERA5. Thus, WRF simulations driven by observation-based boundary conditions are used as a benchmark for evaluating the dependence structure of wind and precipitation extremes.
Overall, boundary conditions in WRF appear to be the key factor in explaining differences in the dependence behaviour between strong wind and heavy precipitation between simulations. In comparison, external forcings (RCP8.5) are of second order.  Our approach offers new methodological tools to evaluate climate model simulations with respect to compound extremes.</p></abstract-html>
<ref-html id="bib1.bib1"><label>Ban et al.(2014)Ban, Schmidli, and Schaer</label><mixed-citation>
Ban, N., Schmidli, J., and Schaer, C.: Evaluation of the convection-resolving
regional climate modeling approach in decade-long simulations, J.
Geophys. Res.-Atmos., 119, 889–7907,
<a href="https://doi.org/10.1002/2014JD021478" target="_blank">https://doi.org/10.1002/2014JD021478</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Barry(2008)</label><mixed-citation>
Barry, R. G.: Mountain weather and climate, Cambridge University Press, Cambridge, UK,
2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Bevacqua et al.(2019)Bevacqua, Maraun, Vousdoukas, Voukouvalas, Vrac,
Mentaschi, and Widmann</label><mixed-citation>
Bevacqua, E., Maraun, D., Vousdoukas, M. I., Voukouvalas, E., Vrac, M.,
Mentaschi, L., and Widmann, M.: Higher probability of compound flooding from
precipitation and storm surge in Europe under anthropogenic climate change,
Science Advances, 5, eaaw5531, <a href="https://doi.org/10.1126/sciadv.aaw5531" target="_blank">https://doi.org/10.1126/sciadv.aaw5531</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Bracegirdle et al.(2013)Bracegirdle, Shuckburgh, Sallee, Wang,
Meijers, Bruneau, Phillips, and Wilcox</label><mixed-citation>
Bracegirdle, T. J., Shuckburgh, E., Sallee, J.-B., Wang, Z., Meijers, A. J. S.,
Bruneau, N., Phillips, T., and Wilcox, L. J.: Assessment of surface winds
over the Atlantic, Indian, and Pacific Ocean sectors of the Southern Ocean in
CMIP5 models: historical bias, forcing response, and state dependence,
J. Geophys. Res-Atmos., 118, 547–562,
<a href="https://doi.org/10.1002/jgrd.50153" target="_blank">https://doi.org/10.1002/jgrd.50153</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Catto and Pfahl(2013)</label><mixed-citation>
Catto, J. L. and Pfahl, S.: The importance of fronts for extreme precipitation,
J. Geophys. Res-Atmos., 118, 10791–10801,
<a href="https://doi.org/10.1002/jgrd.50852" target="_blank">https://doi.org/10.1002/jgrd.50852</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Champagne et al.(2020)Champagne, Leduc, Coulibaly, and
Arain</label><mixed-citation>
Champagne, O., Leduc, M., Coulibaly, P., and Arain, M. A.: Winter hydrometeorological extreme events modulated by large-scale atmospheric circulation in southern Ontario, Earth Syst. Dynam., 11, 301–318, <a href="https://doi.org/10.5194/esd-11-301-2020" target="_blank">https://doi.org/10.5194/esd-11-301-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Coles(2001)</label><mixed-citation>
Coles, S.: An introduction to statistical modeling of extreme values, Springer, London, UK,
<a href="https://doi.org/10.1007/978-1-4471-3675-0" target="_blank">https://doi.org/10.1007/978-1-4471-3675-0</a>, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Coles et al.(1999)Coles, Heffernan, and Tawn</label><mixed-citation>
Coles, S., Heffernan, J., and Tawn, J.: Dependence measures for extreme value
analyses, Extremes, 2, 339–365, 1999.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Copernicus Climate Change Service(2017)</label><mixed-citation>
Copernicus Climate Change Service (C3S): ERA5: Fifth generation of ECMWF
atmospheric reanalyses of the global climate, <a href="https://www.ecmwf.int/en/forecasts/datasets/reanalysis-datasets/era5" target="_blank"/> (last access: 28 May 2020), Copernicus Climate Change Service, Reading, UK, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Couasnon et al.(2020)Couasnon, Eilander, Muis, Veldkamp, Haigh, Wahl,
Winsemius, and Ward</label><mixed-citation>
Couasnon, A., Eilander, D., Muis, S., Veldkamp, T. I. E., Haigh, I. D., Wahl, T., Winsemius, H. C., and Ward, P. J.: Measuring compound flood potential from river discharge and storm surge extremes at the global scale, Nat. Hazards Earth Syst. Sci., 20, 489–504, <a href="https://doi.org/10.5194/nhess-20-489-2020" target="_blank">https://doi.org/10.5194/nhess-20-489-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Davison and Huser(2015)</label><mixed-citation>
Davison, A. and Huser, R.: Statistics of Extremes, Annu. Rev. Stat.
Appl., 2, 203–235, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Dee et al.(2011)Dee, Uppala, Simmons, Berrisford, Poli, Kobayashi,
Andrae, Balmaseda, Balsamo, Bauer, Bechtold, Beljaars, van de Berg, Bidlot,
Bormann, Delsol, Dragani, Fuentes, Geer, Haimberger, Healy, Hersbach,
Hólm, Isaksen, Kållberg, Köhler, Matricardi, McNally, Monge-Sanz,
Morcrette, Park, Peubey, de Rosnay, Tavolato, Thépaut, and
Vitart</label><mixed-citation>
Dee, D. P., Uppala, S. M., Simmons, A. J., Berrisford, P., Poli, P., Kobayashi,
S., Andrae, U., Balmaseda, M. A., Balsamo, G., Bauer, P., Bechtold, P.,
Beljaars, A. C. M., van de Berg, L., Bidlot, J., Bormann, N., Delsol, C.,
Dragani, R., Fuentes, M., Geer, A. J., Haimberger, L., Healy, S. B.,
Hersbach, H., Hólm, E. V., Isaksen, L., Kållberg, P., Köhler, M.,
Matricardi, M., McNally, A. P., Monge-Sanz, B. M., Morcrette, J.-J., Park,
B.-K., Peubey, C., de Rosnay, P., Tavolato, C., Thépaut, J.-N., and
Vitart, F.: The ERA-Interim reanalysis: configuration and performance of the
data assimilation system, Q. J. Roy. Meteor.
Soc., 137, 553–597, <a href="https://doi.org/10.1002/qj.828" target="_blank">https://doi.org/10.1002/qj.828</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>De Luca et al.(2020)De Luca, Messori, Pons, and Faranda</label><mixed-citation>
De Luca, P., Messori, G., Pons, F. M. E., and Faranda, D.: Dynamical systems
theory sheds new light on compound climate extremes in Europe and Eastern
North America, Q. J. Roy. Meteor. Soc.,  146, 1636–1650,
<a href="https://doi.org/10.1002/qj.3757" target="_blank">https://doi.org/10.1002/qj.3757</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Deser et al.(2020)Deser, Lehner, Rodgers, Ault, Delworth, DiNezio,
Fiore, Frankignoul, Fyfe, Horton, Kay, Knutti, Lovenduski, Marotzke,
McKinnon, Minobe, Randerson, Screen, Simpson, and Ting</label><mixed-citation>
Deser, C., Lehner, F., Rodgers, K. B., Ault, T., Delworth, T. L., DiNezio,
P. N., Fiore, A., Frankignoul, C., Fyfe, J. C., Horton, D. E., Kay, J. E.,
Knutti, R., Lovenduski, N. S., Marotzke, J., McKinnon, K. A., Minobe, S.,
Randerson, J., Screen, J. A., Simpson, I. R., and Ting, M.: Insights from
Earth system model initial-condition large ensembles and future prospects,
Nat. Clim. Change, 10, 1–10, <a href="https://doi.org/10.1038/s41558-020-0731-2" target="_blank">https://doi.org/10.1038/s41558-020-0731-2</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Embrechts et al.(1997)Embrechts, Klüppelberg, and
Mikosch</label><mixed-citation>
Embrechts, P., Klüppelberg, C., and Mikosch, T.: Modelling Extremal Events:
for Insurance and Finance, Springer, London, UK, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Engelke and Ivanovs(2021)</label><mixed-citation>
Engelke, S. and Ivanovs, J.: Sparse Structures for Multivariate Extremes,
Annu. Rev. Stat. Appl., 8, <a href="https://doi.org/10.1146/annurev-statistics-040620-041554" target="_blank">https://doi.org/10.1146/annurev-statistics-040620-041554</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Ferreira and de Haan(2015)</label><mixed-citation>
Ferreira, A. and de Haan, L.: On the block maxima method in extreme value
theory: PWM estimators, Ann. Stat., 43, 276–298, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Fink et al.(2009)Fink, Brücher, Ermert, Krüger, and
Pinto</label><mixed-citation>
Fink, A. H., Brücher, T., Ermert, V., Krüger, A., and Pinto, J. G.: The European storm Kyrill in January 2007: synoptic evolution, meteorological impacts and some considerations with respect to climate change, Nat. Hazards Earth Syst. Sci., 9, 405–423, <a href="https://doi.org/10.5194/nhess-9-405-2009" target="_blank">https://doi.org/10.5194/nhess-9-405-2009</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Flato et al.(2013)Flato, Marotzke, Abiodun, Braconnot, Chou, Collins,
Cox, Driouech, Emori, Eyring, Forest, Gleckler, Guilyardi, Jakob, Kattsov,
Reason, and Rummukainen</label><mixed-citation>
Flato, G., Marotzke, J., Abiodun, B., Braconnot, P., Chou, S., Collins, W.,
Cox, P., Driouech, F., Emori, S., Eyring, V., Forest, C., Gleckler, P.,
Guilyardi, E., Jakob, C., Kattsov, V., Reason, C., and Rummukainen, M.:
Evaluation of Climate Models, in: Climate Change 2013: The Physical
Science Basis, Contribution of Working Group I to the Fifth Assessment Report
of the Intergovernmental Panel on Climate Change, edited by: Stocker, T. F.,
Qin, D., Plattner, G.-K., Tignor, M., Allen, S. K., Boschung, J., Nauels, A.,
Xia, Y., Bex, V., and Midgley, P. M.,
Cambridge
University Press, Cambridge, United Kingdom and New York, USA,
741–866,
<a href="https://doi.org/10.1017/CBO9781107415324.020" target="_blank">https://doi.org/10.1017/CBO9781107415324.020</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>François et al.(2020)François, Vrac, Cannon, Robin, and
Allard</label><mixed-citation>
François, B., Vrac, M., Cannon, A. J., Robin, Y., and Allard, D.: Multivariate bias corrections of climate simulations: which benefits for which losses?, Earth Syst. Dynam., 11, 537–562, <a href="https://doi.org/10.5194/esd-11-537-2020" target="_blank">https://doi.org/10.5194/esd-11-537-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Gilleland and Katz(2016)</label><mixed-citation>
Gilleland, E. and Katz, R. W.: extRemes 2.0: An Extreme Value Analysis
Package in R, J. Stat. Softw., 72, 1–39,
<a href="https://doi.org/10.18637/jss.v072.i08" target="_blank">https://doi.org/10.18637/jss.v072.i08</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>Gómez-Navarro et al.(2015)Gómez-Navarro, Raible, and
Dierer</label><mixed-citation>
Gómez-Navarro, J. J., Raible, C. C., and Dierer, S.: Sensitivity of the WRF model to PBL parametrisations and nesting techniques: evaluation of wind storms over complex terrain, Geosci. Model Dev., 8, 3349–3363, <a href="https://doi.org/10.5194/gmd-8-3349-2015" target="_blank">https://doi.org/10.5194/gmd-8-3349-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>Gómez-Navarro et al.(2018)Gómez-Navarro, Raible, Bozhinova,
Martius, García Valero, and Montávez</label><mixed-citation>
Gómez-Navarro, J. J., Raible, C. C., Bozhinova, D., Martius, O., García Valero, J. A., and Montávez, J. P.: A new region-aware bias-correction method for simulated precipitation in areas of complex orography, Geosci. Model Dev., 11, 2231–2247, <a href="https://doi.org/10.5194/gmd-11-2231-2018" target="_blank">https://doi.org/10.5194/gmd-11-2231-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Graf et al.(2019)Graf, Scherrer, Schwierz, Begert, Martius, Raible,
and Brönnimann</label><mixed-citation>
Graf, M., Scherrer, S. C., Schwierz, C., Begert, M., Martius, O., Raible,
C. C., and Brönnimann, S.: Near-surface mean wind in Switzerland:
Climatology, climate model evaluation and future scenarios, Int.
J. Climatol., 39, 4798–4810, <a href="https://doi.org/10.1002/joc.6108" target="_blank">https://doi.org/10.1002/joc.6108</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Hendry et al.(2019)Hendry, Haigh, Nicholls, Winter, Neal, Wahl,
Joly-Laugel, and Darby</label><mixed-citation>
Hendry, A., Haigh, I. D., Nicholls, R. J., Winter, H., Neal, R., Wahl, T., Joly-Laugel, A., and Darby, S. E.: Assessing the characteristics and drivers of compound flooding events around the UK coast, Hydrol. Earth Syst. Sci., 23, 3117–3139, <a href="https://doi.org/10.5194/hess-23-3117-2019" target="_blank">https://doi.org/10.5194/hess-23-3117-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>Hong and Lim(2020)</label><mixed-citation>
Hong, S. and Lim, J.: The WRF single-moment 6-class micro-physics scheme
(WSM6), Journal of Korean Meteorology Society, 42, 129–151, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Hurrell et al.(2013)Hurrell, Holland, Gent, Ghan, Kay, Kushner,
Lamarque, Large, Lawrence, Lindsay, Lipscomb, Long, Mahowald, Marsh, Neale,
Rasch, Vavrus, Vertenstein, Bader, Collins, Hack, Kiehl, and
Marshall</label><mixed-citation>
Hurrell, J. W., Holland, M. M., Gent, P. R., Ghan, S., Kay, J. E., Kushner,
P. J., Lamarque, J. F., Large, W. G., Lawrence, D., Lindsay, K., Lipscomb,
W. H., Long, M. C., Mahowald, N., Marsh, D. R., Neale, R. B., Rasch, P.,
Vavrus, S., Vertenstein, M., Bader, D., Collins, W. D., Hack, J. J., Kiehl,
J., and Marshall, S.: The Community Earth System Model A Framework for
Collaborative Research, B. Am. Meteorol. Soc.,
94, 1339–1360, <a href="https://doi.org/10.1175/BAMS-D-12-00121.1" target="_blank">https://doi.org/10.1175/BAMS-D-12-00121.1</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>Huser and Wadsworth(2020)</label><mixed-citation>
Huser, R. and Wadsworth, J. L.: Advances in Statistical Modeling of Spatial
Extremes, WIREs Comput. Stat., e1537, <a href="https://doi.org/10.1002/wics.1537" target="_blank">https://doi.org/10.1002/wics.1537</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Jimenez and Dudhia(2012)</label><mixed-citation>
Jimenez, P. A. and Dudhia, J.: Improving the Representation of Resolved and
Unresolved Topographic Effects on Surface Wind in the WRF Model, J.
Appl. Meteorol. Clim., 51, 300–316,
<a href="https://doi.org/10.1175/JAMC-D-11-084.1" target="_blank">https://doi.org/10.1175/JAMC-D-11-084.1</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Jones et al.(2017)Jones, Harpham, Troccoli, Gschwind, Ranchin, Wald,
Goodess, and Dorling</label><mixed-citation>
Jones, P. D., Harpham, C., Troccoli, A., Gschwind, B., Ranchin, T., Wald, L., Goodess, C. M., and Dorling, S.: Using ERA-Interim reanalysis for creating datasets of energy-relevant climate variables, Earth Syst. Sci. Data, 9, 471–495, <a href="https://doi.org/10.5194/essd-9-471-2017" target="_blank">https://doi.org/10.5194/essd-9-471-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Katz et al.(2002)Katz, Parlange, and Naveau</label><mixed-citation>
Katz, R. W., Parlange, M. B., and Naveau, P.: Statistics of extremes in
hydrology, Adv. Water Resour., 25, 1287–1304, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>Ledford and Tawn(1997)</label><mixed-citation>
Ledford, A. W. and Tawn, J. A.: Modelling dependence within joint tail regions,
J. R. Stat. Soc. Ser. B Stat. Methodol., 59, 475–499, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Lehner et al.(2015)Lehner, Joos, Raible, Mignot, Born, Keller, and
Stocker</label><mixed-citation>
Lehner, F., Joos, F., Raible, C. C., Mignot, J., Born, A., Keller, K. M., and Stocker, T. F.: Climate and carbon cycle dynamics in a CESM simulation from 850 to 2100 CE, Earth Syst. Dynam., 6, 411–434, <a href="https://doi.org/10.5194/esd-6-411-2015" target="_blank">https://doi.org/10.5194/esd-6-411-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Liberato(2014)</label><mixed-citation>
Liberato, M. L.: The 19 January 2013 windstorm over the North Atlantic:
large-scale dynamics and impacts on Iberia, Weather and Climate Extremes,
5–6, 16–28, <a href="https://doi.org/10.1016/j.wace.2014.06.002" target="_blank">https://doi.org/10.1016/j.wace.2014.06.002</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Lin et al.(2010)Lin, Emanuel, Smith, and Vanmarcke</label><mixed-citation>
Lin, N., Emanuel, K. A., Smith, J. A., and Vanmarcke, E.: Risk assessment of
hurricane storm surge for New York City, J. Geophys. Res.-Atmos., 115, D18121, <a href="https://doi.org/10.1029/2009JD013630" target="_blank">https://doi.org/10.1029/2009JD013630</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Manning et al.(2019)Manning, Widmann, Bevacqua, Loon, Maraun, and
Vrac</label><mixed-citation>
Manning, C., Widmann, M., Bevacqua, E., Loon, A. F. V., Maraun, D., and Vrac,
M.: Increased probability of compound long-duration dry and hot events in
Europe during summer (1950–2013), Environ. Res.
Lett., 14, 094006, <a href="https://doi.org/10.1088/1748-9326/ab23bf" target="_blank">https://doi.org/10.1088/1748-9326/ab23bf</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Maraun et al.(2017)Maraun, Shepherd, Widmann, Zappa, Walton,
Gutierrez, Hagemann, Richter, Soares, Hall, and Mearns</label><mixed-citation>
Maraun, D., Shepherd, T. G., Widmann, M., Zappa, G., Walton, D., Gutierrez,
J. M., Hagemann, S., Richter, I., Soares, P. M. M., Hall, A., and Mearns,
L. O.: Towards process-informed bias correction of climate change
simulations, Nat. Clim. Change, 7, 764–773, <a href="https://doi.org/10.1038/nclimate3418" target="_blank">https://doi.org/10.1038/nclimate3418</a>,
2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>Martius et al.(2016)Martius, Pfahl, and
Chevalier</label><mixed-citation>
Martius, O., Pfahl, S., and Chevalier, C.: A global quantification of compound
precipitation and wind extremes, Geophys. Res. Lett., 43,
7709–7717, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Mazdiyasni and AghaKouchak(2015)</label><mixed-citation>
Mazdiyasni, O. and AghaKouchak, A.: Substantial increase in concurrent
droughts and heatwaves in the United States, P. Natl.
Acad. Sci. USA, 112, 11484–11489, <a href="https://doi.org/10.1073/pnas.1422945112" target="_blank">https://doi.org/10.1073/pnas.1422945112</a>,
2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Messmer et al.(2017)</label><mixed-citation>
Messmer, M., Gómez-Navarro, J. J., and Raible, C. C.: Sensitivity experiments on the response of Vb cyclones to sea surface temperature and soil moisture changes, Earth Syst. Dynam., 8, 477–493, <a href="https://doi.org/10.5194/esd-8-477-2017" target="_blank">https://doi.org/10.5194/esd-8-477-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Messmer et al.(2020)</label><mixed-citation>
Messmer, M., Raible, C. C., and Gómez-Navarro, J. J.: Impact of climate
change on the climatology of Vb cyclones, Tellus A, 72, 1–18, <a href="https://doi.org/10.1080/16000870.2020.1724021" target="_blank">https://doi.org/10.1080/16000870.2020.1724021</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>Mitchell and Jones(2005)</label><mixed-citation>
Mitchell, T. D. and Jones, P. D.: An improved method of constructing a database
of monthly climate observations and associated high-resolution grids,
Int. J. Climatol., 25, 693–712, <a href="https://doi.org/10.1002/joc.1181" target="_blank">https://doi.org/10.1002/joc.1181</a>,
2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Musselman et al.(2018)Musselman, Lehner, Ikeda, Clark, Prein, Liu,
Barlage, and Rasmussen</label><mixed-citation>
Musselman, K., Lehner, F., Ikeda, K., Clark, M., Prein, A., Liu, C., Barlage,
M., and Rasmussen, R.: Projected increases and shifts in rain-on-snow flood
risk over western North America, Nat. Clim. Change, 8, 808–812,
<a href="https://doi.org/10.1038/s41558-018-0236-4" target="_blank">https://doi.org/10.1038/s41558-018-0236-4</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Naveau et al.(2014)Naveau, Guillou, and Rietsch</label><mixed-citation>
Naveau, P., Guillou, A., and Rietsch, T.: A non-parametric entropy-based
approach to detect changes in climate extremes, J. Roy.
Stat. Soc. B, 76, 861–884, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Naveau et al.(2020)Naveau, Hannart, and Ribes</label><mixed-citation>
Naveau, P., Hannart, A., and Ribes, A.: Statistical Methods for Extreme Event
Attribution in Climate Science, Annu. Rev. Stat.
Appl., 7, 89–110, <a href="https://doi.org/10.1146/annurev-statistics-031219-041314" target="_blank">https://doi.org/10.1146/annurev-statistics-031219-041314</a>,
2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>Pantillon et al.(2020)Pantillon, Adler, Corsmeier, Knippertz, Wieser,
and Hansen</label><mixed-citation>
Pantillon, F., Adler, B., Corsmeier, U., Knippertz, P., Wieser, A., and Hansen,
A.: Formation of Wind Gusts in an Extratropical Cyclone in Light of Doppler
Lidar Observations and Large-Eddy Simulations, Mon. Weather Rev., 148,
353–375, <a href="https://doi.org/10.1175/Mwr-D-19-0241.1" target="_blank">https://doi.org/10.1175/Mwr-D-19-0241.1</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Panziera and Germann(2010)</label><mixed-citation>
Panziera, L. and Germann, U.: The relation between airflow and orographic
precipitation on the southern side of the Alps as revealed by weather radar,
Q. J. Roy. Meteor. Soc., 136, 222–238,
<a href="https://doi.org/10.1002/qj.544" target="_blank">https://doi.org/10.1002/qj.544</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Parton et al.(2010)Parton, Dore, and Vaughan</label><mixed-citation>
Parton, G., Dore, A., and Vaughan, G.: A climatology of mid-tropospheric
mesoscale strong wind events as observed by the MST radar, Aberystwyth,
Meteorol. Appl., 17, 340–354, <a href="https://doi.org/10.1002/met.203" target="_blank">https://doi.org/10.1002/met.203</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>Pfahl et al.(2014)Pfahl, Madonna, Boettcher, Joos, and
Wernli</label><mixed-citation>
Pfahl, S., Madonna, E., Boettcher, M., Joos, H., and Wernli, H.: Warm Conveyor
Belts in the ERA-Interim Dataset (1979–2010). Part II: Moisture Origin and
Relevance for Precipitation, J. Climate, 27, 27–40, <a href="https://doi.org/10.1175/Jcli-D-13-00223.1" target="_blank">https://doi.org/10.1175/Jcli-D-13-00223.1</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>Poon et al.(2003)Poon, Rockinger, and Tawn</label><mixed-citation>
Poon, S.-H., Rockinger, M., and Tawn, J.: Extreme value dependence in financial
markets: Diagnostics, models, and financial implications, Rev. Financ. Stud., 17, 581–610, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>Poschlod et al.(2020)Poschlod, Zscheischler, Sillmann, Wood, and
Ludwig</label><mixed-citation>
Poschlod, B., Zscheischler, J., Sillmann, J., Wood, R. R., and Ludwig, R.:
Climate change effects on hydrometeorological compound events over southern
Norway, Weather and Climate Extremes, 28, 100253,
<a href="https://doi.org/10.1016/j.wace.2020.100253" target="_blank">https://doi.org/10.1016/j.wace.2020.100253</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>Raible et al.(2018)Raible, Messmer, Lehner, Stocker, and
Blender</label><mixed-citation>
Raible, C. C., Messmer, M., Lehner, F., Stocker, T. F., and Blender, R.: Extratropical cyclone statistics during the last millennium and the 21st century, Clim. Past, 14, 1499–1514, <a href="https://doi.org/10.5194/cp-14-1499-2018" target="_blank">https://doi.org/10.5194/cp-14-1499-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>Raveh-Rubin and Wernli(2015)</label><mixed-citation>
Raveh-Rubin, S. and Wernli, H.: Large-scale wind and precipitation extremes in
the Mediterranean: A climatological analysis for 1979–2012, Q.
J. Roy. Meteor. Soc., 141, 2404–2417,
<a href="https://doi.org/10.1002/qj.2531" target="_blank">https://doi.org/10.1002/qj.2531</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>Ridder et al.(2020)Ridder, Pitman, Westra, Ukkola, Do, Bador,
Hirsch, Evans, Luca, and Zscheischler</label><mixed-citation>
Ridder, N., Pitman, A., Westra, S., Ukkola, A., Do, H., Bador, M., Hirsch, A.,
Evans, J., Luca, A. D., and Zscheischler, J.: Global hotspots for the
occurrence of compound events, Nat. Commun., 11, 5956, <a href="https://doi.org/10.1038/s41467-020-19639-3" target="_blank">https://doi.org/10.1038/s41467-020-19639-3</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>Sibuya(1960)</label><mixed-citation>
Sibuya, M.: Bivariate extreme statistics, Ann. I.
Stat. Math., 11, 195–210, 1960.
</mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>Sippel et al.(2017)Sippel, Zscheischler, Mahecha, Orth, Reichstein,
Vogel, and Seneviratne</label><mixed-citation>
Sippel, S., Zscheischler, J., Mahecha, M. D., Orth, R., Reichstein, M., Vogel, M., and Seneviratne, S. I.: Refining multi-model projections of temperature extremes by evaluation against land–atmosphere coupling diagnostics, Earth Syst. Dynam., 8, 387–403, <a href="https://doi.org/10.5194/esd-8-387-2017" target="_blank">https://doi.org/10.5194/esd-8-387-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>Sippel et al.(2018)Sippel, Reichstein, Ma, Mahecha, Lange, Flach, and
Frank</label><mixed-citation>
Sippel, S., Reichstein, M., Ma, X., Mahecha, M. D., Lange, H., Flach, M., and
Frank, D.: Drought, Heat, and the Carbon Cycle: a Review, Current Climate
Change Reports, 4, 266–286, <a href="https://doi.org/10.1007/s40641-018-0103-4" target="_blank">https://doi.org/10.1007/s40641-018-0103-4</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>Skamarock et al.(2008)Skamarock, Klemp, Dudhia, Gill, Barker, Wang,
and Powers</label><mixed-citation>
Skamarock, W. C., Klemp, J. B., Dudhia, J., Gill, D. O., Barker, D. M., Wang,
W., and Powers, J. G.: A description of the advanced research WRF version 3,
Technical Report, TN-475+STR, National Center for Atmospheric Research, Boulder, CO, USA, 113 pp.,  2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>Stephenson(2002)</label><mixed-citation>
Stephenson, A. G.: evd, Extreme Value Distributions, R News, 2.0, availabe at:
<a href="https://CRAN.R-project.org/doc/Rnews/" target="_blank"/> (last access: 28 May 2020), 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>Stucki et al.(2016)Stucki, Dierer, Welker, Gómez-Navarro, Raible,
Martius, and Brönnimann</label><mixed-citation>
Stucki, P., Dierer, S., Welker, C., Gómez-Navarro, J. J., Raible, C. C.,
Martius, O., and Brönnimann, S.: Evaluation of downscaled wind speeds and
parameterised gusts for recent and historical windstorms in Switzerland,
Tellus A, 68, 31820,
<a href="https://doi.org/10.3402/tellusa.v68.31820" target="_blank">https://doi.org/10.3402/tellusa.v68.31820</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>Sutanto et al.(2020)Sutanto, Vitolo, Napoli, D’Andrea, and
Lanen</label><mixed-citation>
Sutanto, S. J., Vitolo, C., Napoli, C. D., D’Andrea, M., and Lanen, H. A. V.:
Heatwaves, droughts, and fires: Exploring compound and cascading dry hazards
at the pan-European scale, Environ. Int., 134, 105276,
<a href="https://doi.org/10.1016/j.envint.2019.105276" target="_blank">https://doi.org/10.1016/j.envint.2019.105276</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib62"><label>Telesca et al.(2020)Telesca, Guignard, Laib, and
Kanevski</label><mixed-citation>
Telesca, L., Guignard, F., Laib, M., and Kanevski, M.: Analysis of temporal
properties of extremes of wind measurements from 132 stations over
Switzerland, Renew. Energ., 145, 1091–1103,
<a href="https://doi.org/10.1016/j.renene.2019.06.089" target="_blank">https://doi.org/10.1016/j.renene.2019.06.089</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib63"><label>Vignotto et al.(2020)Vignotto, Engelke, and
Zscheischler</label><mixed-citation>
Vignotto, E., Engelke, S., and Zscheischler, J.: Clustering bivariate
dependences in the extremes of climate variables, Weather and Climate Extremes, in review, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib64"><label>Wahl et al.(2015)Wahl, Jain, Bender, Meyers, and Luther</label><mixed-citation>
Wahl, T., Jain, S., Bender, J., Meyers, S. D., and Luther, M. E.: Increasing
risk of compound flooding from storm surge and rainfall for major US cities,
Nat. Clim. Change, 5, 1–6, <a href="https://doi.org/10.1038/nclimate2736" target="_blank">https://doi.org/10.1038/nclimate2736</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib65"><label>Wang et al.(2020)Wang, Chen, Tett, Yan, Zhai, Feng, and
Xia</label><mixed-citation>
Wang, J., Chen, Y., Tett, S. F., Yan, Z., Zhai, P., Feng, J., and Xia, J.:
Anthropogenically-driven increases in the risks of summertime compound hot
extremes, Nat. Commun., 11, <a href="https://doi.org/10.1038/s41467-019-14233-8" target="_blank">https://doi.org/10.1038/s41467-019-14233-8</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib66"><label>Ward et al.(2018)Ward, Couasnon, Eilander, Haigh, Hendry, Muis,
Veldkamp, Winsemius, and Wahl</label><mixed-citation>
Ward, P. J., Couasnon, A., Eilander, D., Haigh, I. D., Hendry, A., Muis, S.,
Veldkamp, T. I., Winsemius, H. C., and Wahl, T.: Dependence between high
sea-level and high river discharge increases flood hazard in global deltas
and estuaries, Environ. Res. Lett., 13, 084012, <a href="https://doi.org/10.1088/1748-9326/aad400" target="_blank">https://doi.org/10.1088/1748-9326/aad400</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib67"><label>Whiteman(2000)</label><mixed-citation>
Whiteman, C. D.: Mountain meteorology fundamentals and applications, Oxford
University Press, New York, USA, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib68"><label>Zheng et al.(2013)Zheng, Westra, and Sisson</label><mixed-citation>
Zheng, F., Westra, S., and Sisson, S. A.: Quantifying the dependence between
extreme rainfall and storm surge in the coastal zone, J. Hydrol.,
505, 172–187, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib69"><label>Zscheischler and Fischer(2020)</label><mixed-citation>
Zscheischler, J. and Fischer, E.: The record-breaking compound hot and dry
2018 growing season in Germany, Weather and Climate Extremes, 19, 100270,
<a href="https://doi.org/10.1007/s00484-020-01951-8" target="_blank">https://doi.org/10.1007/s00484-020-01951-8</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib70"><label>Zscheischler and Seneviratne(2017)</label><mixed-citation>
Zscheischler, J. and Seneviratne, S. I.: Dependence of drivers affects risks
associated with compound events, Science Advances, 3, e1700263, <a href="https://doi.org/10.1126/sciadv.1700263" target="_blank">https://doi.org/10.1126/sciadv.1700263</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib71"><label>Zscheischler et al.(2014)Zscheischler, Michalak, Schwalm, Mahecha,
Huntzinger, Reichstein, Berthier, Ciais, Cook, El-Masri, Huang, Ito, Jain,
King, Lei, Lu, Mao, Peng, Poulter, Ricciuto, Shi, Tao, Tian, Viovy, Wang,
Wei, Yang, and Zeng</label><mixed-citation>
Zscheischler, J., Michalak, A. M., Schwalm, C., Mahecha, M. D., Huntzinger,
D. N., Reichstein, M., Berthier, G., Ciais, P., Cook, R. B., El-Masri, B.,
Huang, M., Ito, A., Jain, A., King, A., Lei, H., Lu, C., Mao, J., Peng, S.,
Poulter, B., Ricciuto, D., Shi, X., Tao, B., Tian, H., Viovy, N., Wang, W.,
Wei, Y., Yang, J., and Zeng, N.: Impact of large-scale climate extremes on
biospheric carbon fluxes: An intercomparison based on MsTMIP data, Global
Biogeochem. Cy., 28, 585–600, <a href="https://doi.org/10.1002/2014GB004826" target="_blank">https://doi.org/10.1002/2014GB004826</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib72"><label>Zscheischler et al.(2018)Zscheischler, Westra, Hurk, Seneviratne,
Ward, Pitman, AghaKouchak, Bresch, Leonard, Wahl, and
Zhang</label><mixed-citation>
Zscheischler, J., Westra, S., Hurk, B. J., Seneviratne, S. I., Ward, P. J.,
Pitman, A., Agha Kouchak, A., Bresch, D. N., Leonard, M., Wahl, T., and Zhang,
X.: Future climate risk from compound events, Nat. Clim. Change, 8,
469–477, 2018.

</mixed-citation></ref-html>
<ref-html id="bib1.bib73"><label>Zscheischler et al.(2019)Zscheischler, Fischer, and
Lange</label><mixed-citation>
Zscheischler, J., Fischer, E. M., and Lange, S.: The effect of univariate bias adjustment on multivariate hazard estimates, Earth Syst. Dynam., 10, 31–43, <a href="https://doi.org/10.5194/esd-10-31-2019" target="_blank">https://doi.org/10.5194/esd-10-31-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib74"><label>Zscheischler et al.(2020)Zscheischler, Martius, Westra, Bevacqua,
Raymond, Horton, van den Hurk, AghaKouchak, Jézéquel, Mahecha,
Maraun, Ramos, Ridder, Thiery, and Vignotto</label><mixed-citation>
Zscheischler, J., Martius, O., Westra, S., Bevacqua, E., Raymond, C., Horton,
R. M., van den Hurk, B., Agha Kouchak, A., Jézéquel, A., Mahecha,
M. D., Maraun, D., Ramos, A. M., Ridder, N., Thiery, W., and Vignotto, E.: A
typology of compound weather and climate events, Nature Reviews Earth and
Environment, 1, 333–347, <a href="https://doi.org/10.1038/s43017-020-0060-z" target="_blank">https://doi.org/10.1038/s43017-020-0060-z</a>, 2020.
</mixed-citation></ref-html>--></article>
