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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ASCMO</journal-id><journal-title-group>
    <journal-title>Advances in Statistical Climatology, Meteorology and Oceanography</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ASCMO</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Adv. Stat. Clim. Meteorol. Oceanogr.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2364-3587</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/ascmo-12-87-2026</article-id><title-group><article-title>Selecting the best distribution for modeling trends in low, medium, and extreme daily precipitation under climate change</article-title><alt-title>Distribution selection for rainfall trends</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Haruna</surname><given-names>Abubakar</given-names></name>
          <email>abubakar.haruna@univ-grenoble-alpes.fr</email>
        <ext-link>https://orcid.org/0000-0002-0508-6734</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Blanchet</surname><given-names>Juliette</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8088-8895</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Evin</surname><given-names>Guillaume</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3456-9441</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Paquet</surname><given-names>Emmanuel</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Univ. Grenoble Alpes, CNRS, INRAE, IRD, Grenoble Institute of Engineering and Management, IGE, 38000 Grenoble, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>EDF-DTG, 38000 Grenoble, France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Abubakar Haruna (abubakar.haruna@univ-grenoble-alpes.fr)</corresp></author-notes><pub-date><day>24</day><month>March</month><year>2026</year></pub-date>
      
      <volume>12</volume>
      <issue>1</issue>
      <fpage>87</fpage><lpage>109</lpage>
      <history>
        <date date-type="received"><day>24</day><month>October</month><year>2025</year></date>
           <date date-type="rev-recd"><day>13</day><month>February</month><year>2026</year></date>
           <date date-type="accepted"><day>16</day><month>March</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Abubakar Haruna et al.</copyright-statement>
        <copyright-year>2026</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026.html">This article is available from https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026.html</self-uri><self-uri xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026.pdf">The full text article is available as a PDF file from https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e114">Changes in mean precipitation and the frequency and intensity of extreme precipitation represent one of the most consequential aspects of anthropogenic climate change. This study evaluates a set of statistical distributions for modeling trends across the full precipitation spectrum (low, medium, and extreme daily quantiles).  Modeling with a single flexible distribution ensures statistical consistency, thereby avoiding the artificial separation and discontinuity inherent in multi-model approaches. We used time as a covariate for dry-day frequency and sea surface temperature for the wet-day distribution parameters. We applied the methodology to a dense network of over 900 meteorological stations in France, offering a wide variety of climatic regimes, allowing for a robust conclusion. We employed a multi-criterion approach to select the best model, in the first step using the Akaike Information Criterion, and then based on their ability to flexibly capture trends across low, medium, and extreme precipitation quantiles. Our findings highlight that three-parameter distributions (generalized gamma and extended generalized Pareto distribution), particularly with evolving shape parameters, are essential for accurately capturing observed differential changes across the full precipitation spectrum, a flexibility that the two-parameter gamma distribution notably lacked. Although AIC generally favored generalized gamma, both generalized gamma and the extended generalized Pareto distribution demonstrated robust performance. This research underscores the critical need for a multi-criterion model identification framework in nonstationary trend analysis to provide reliable insights essential for hydrological and climate impact assessments.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>Agence Nationale de la Recherche</funding-source>
<award-id>France 2030 as part of the PEPR “Transformer la modélisation du climat pour les services climatiques” (TRACCS) program under grant number ANR-22-EXTR-0005</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e126">Changes in precipitation patterns, particularly in the frequency and intensity of both mean and extreme events, represent one of the most consequential aspects of anthropogenic climate change <xref ref-type="bibr" rid="bib1.bibx28" id="paren.1"/>. Detecting and modeling such changes are critical for improving hydrological forecasting, assessing flood and drought risks, and informing infrastructure planning and climate adaptation strategies.</p>
      <p id="d2e132">Accurately assessing these trends requires robust statistical models that can capture the complex behavior of daily precipitation. Daily precipitation poses well-known statistical challenges. It is non-negative, skewed, exhibits a discrete-continuous nature with periods of no rainfall (dry-days) interspersed with varying intensities of rainfall (wet-day), and often shows heavy tails <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx13" id="paren.2"/>. Traditional statistical approaches often simplify this complexity, either by focusing solely on trends in mean precipitation <xref ref-type="bibr" rid="bib1.bibx38" id="paren.3"><named-content content-type="pre">e.g.</named-content></xref>, or by treating only extreme events using nonparametric approaches <xref ref-type="bibr" rid="bib1.bibx5" id="paren.4"><named-content content-type="pre">e.g.</named-content></xref> or parametric techniques based on  Generalized Extreme Value (GEV) distribution <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx7" id="paren.5"><named-content content-type="pre">e.g.</named-content></xref>, or generalized Pareto (GPD) <xref ref-type="bibr" rid="bib1.bibx57" id="paren.6"><named-content content-type="pre">e.g.</named-content></xref>. However, in applications such as stochastic simulation,  where the marginal distribution of all the precipitation amounts is required, it is necessary to model the trends in the entire precipitation distribution.  Additionally, employing the entire precipitation data enables trend assessment within a single statistical framework. This ensures coherence by explicitly representing trends for all quantiles and provides robustness by leveraging the full long time series of daily observations. This constitutes an advantage over methods like the Theil-Sen slope estimator <xref ref-type="bibr" rid="bib1.bibx55 bib1.bibx51" id="paren.7"/> and the Mann-Kendall test <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx31" id="paren.8"/>, which separately estimate trends in mean (using only time series of means) and extremes (using only annual maxima series).</p>
      <p id="d2e165">Modeling the full spectrum of daily precipitation, accounting for its intermittency, can be achieved using a mixed-type distribution <xref ref-type="bibr" rid="bib1.bibx30" id="paren.9"/>, comprising a discrete component for dry-days and a continuous component for wet-day precipitation. The discrete component is represented by a probability mass concentrated at zero, while the continuous component is described by a parametric distribution function. Representing the marginal distribution of wet-day precipitation by a parametric distribution is essential for making extrapolations beyond the recorded values, for stochastic simulations in rainfall generators, or nonstationarity analysis. Conversely, an empirical function, based on plotting position formulas <xref ref-type="bibr" rid="bib1.bibx17" id="paren.10"><named-content content-type="pre">see</named-content></xref>, would suffice if the interest lies solely in the estimation of stationary quantiles within the bulk of the observed distribution, far from its tail.</p>
      <p id="d2e176">When modeling trends in whole daily precipitation distribution, choosing the right marginal distribution is crucial not only for fitting the data but also for accurately capturing its temporal evolution. An ideal distribution for this task must meet several conditions: (i) it needs to represent the positive and skewed nature of nonzero daily precipitation; (ii) it should be capable of modeling the entire range of nonzero precipitation, not just the upper tail; (iii) it needs to be flexible enough to handle different trend magnitudes and directions across the bulk and tail; and (iv) finally, it should achieve this with the fewest possible free parameters to minimize estimation uncertainties. The first condition excludes the commonly used Gaussian distribution due to its symmetry. The second condition rules out the classical extreme value theory distributions, such as the GEV and GPD, which are tailored to the tail of the distribution. The third condition excludes one-parameter distributions, such as the exponential distribution, because they lack the flexibility to model multiple trend directions in the distribution. The last condition finally excludes distributions with many parameters, such as kappa, leading to increased complexity and estimation uncertainty.</p>
      <p id="d2e180">Several parametric distributions could potentially satisfy these four conditions; however, considering them all would be impractical and computationally prohibitive. For this study, we consider three prominent candidate models with two or three parameters widely applied in hydro-climatological literature: gamma,  generalized gamma <xref ref-type="bibr" rid="bib1.bibx53" id="paren.11"/>, and the extended generalized Pareto distribution  <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx40" id="paren.12"/>. An additional advantage of selecting these distributions is their hierarchical nature, as many other commonly used distributions are special cases. For instance, the exponential distribution is a special case of both the gamma and the extended generalized Pareto, while, depending on the parametrization,   Weibull, gamma, exponential, and lognormal distributions can all be derived as special cases of the generalized gamma.</p>
      <p id="d2e189">The gamma (GA) distribution is a widely adopted choice for modeling precipitation due to its simplicity and flexibility, recognized as the most popular option in the literature <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx44 bib1.bibx59" id="paren.13"/>. As a two-parameter model belonging to the exponential family, its upper tail's behavior (exponential, slightly lighter, or heavier) depends on its shape parameter. However, numerous studies have shown that the upper tail of observed precipitation often exhibits heavier characteristics than GA model can adequately capture <xref ref-type="bibr" rid="bib1.bibx13" id="paren.14"/>,  leading to an underestimation of the magnitude and frequency of heavy precipitation events <xref ref-type="bibr" rid="bib1.bibx45" id="paren.15"/>. Nevertheless, GA remains a cornerstone within the hydro-climatological community, finding extensive applications in stochastic modeling <xref ref-type="bibr" rid="bib1.bibx50 bib1.bibx58 bib1.bibx4" id="paren.16"><named-content content-type="pre">e.g.</named-content></xref>, trend analysis <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx60" id="paren.17"><named-content content-type="pre">e.g.</named-content></xref>, and frequency analysis <xref ref-type="bibr" rid="bib1.bibx9" id="paren.18"><named-content content-type="pre">e.g.</named-content></xref>.</p>
      <p id="d2e217">The generalized gamma (GG) distribution is a three-parameter model that has also seen broad application in precipitation modeling <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx42 bib1.bibx59" id="paren.19"><named-content content-type="pre">e.g.</named-content></xref>. A comprehensive global analysis of over 15 000 daily precipitation datasets by <xref ref-type="bibr" rid="bib1.bibx45" id="text.20"/> found the GG distribution to flexibly model nonzero precipitation, leading the authors to recommend it as a primary choice for daily precipitation modeling. Unlike the two-parameter GA, the GG offers enhanced flexibility, capable of modeling heavy-tailed, light-tailed, or bounded distributions depending on the value of its shape parameter.</p>
      <p id="d2e228">The extended generalized Pareto distribution (EGPD) is a family of models that extends the classical GPD, which is typically tailored for extremes above a high threshold, to model the entire range of nonzero amounts. This extension ensures the EGPD remains consistent with extreme value theory  in its upper and lower tails while providing full-range applicability. Among the EGPD family, we consider the three-parameter model based on a power law that has been widely applied across various fields. Its utility has been demonstrated in modeling daily precipitation <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx49 bib1.bibx23 bib1.bibx37 bib1.bibx6" id="paren.21"><named-content content-type="pre">see</named-content></xref>, sub-daily precipitation <xref ref-type="bibr" rid="bib1.bibx22" id="paren.22"><named-content content-type="pre">e.g.</named-content></xref>, supra-daily precipitation <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx25" id="paren.23"><named-content content-type="pre">e.g.</named-content></xref>, sub-hourly precipitation <xref ref-type="bibr" rid="bib1.bibx24" id="paren.24"><named-content content-type="pre">e.g.</named-content></xref>, and even in diverse applications such as wave height modeling <xref ref-type="bibr" rid="bib1.bibx35" id="paren.25"/> and wildfire analysis using deep graphical regression <xref ref-type="bibr" rid="bib1.bibx15" id="paren.26"><named-content content-type="pre">e.g.</named-content></xref>. Furthermore, it has been successfully integrated into nonstationary frameworks <xref ref-type="bibr" rid="bib1.bibx41 bib1.bibx39 bib1.bibx26" id="paren.27"><named-content content-type="pre">e.g.</named-content></xref>. More recently, <xref ref-type="bibr" rid="bib1.bibx1" id="text.28"/> proposed a zero-inflated EGPD  model that unifies the modeling of dry days, low, moderate, and extreme rainfall within a single framework.</p>
      <p id="d2e268">The objective of this study, therefore, is to identify which of these candidate distributions most adequately models the observed trends across the entire range of daily precipitation, from its mean to its extremes. While comparisons of distributions for modeling daily precipitation have been conducted at both regional <xref ref-type="bibr" rid="bib1.bibx59" id="paren.29"><named-content content-type="pre">e.g.</named-content></xref> and global scales <xref ref-type="bibr" rid="bib1.bibx44" id="paren.30"><named-content content-type="pre">e.g.</named-content></xref>, these efforts have generally been confined to a stationary framework. Our study extends this crucial research by performing such comparisons within a nonstationary framework, explicitly addressing the temporal evolution of precipitation characteristics. Furthermore, our model selection methodology transcends typical goodness-of-fit criteria, incorporating a multi-criterion assessment of each model's flexibility in accurately capturing trends across low, medium, and extreme precipitation quantiles.</p>
      <p id="d2e281">We apply the framework to a dense network of meteorological stations in France. This region provides a suitable candidate given the wide variety of climatic regimes, ranging from mountainous, oceanic, continental, and Mediterranean. In addition, it also has a dense network of more than 900 stations, with an average of 70 years of data, enabling the conclusions drawn from this study to be considered broadly generic. The remainder of this article is organized as follows: Sect. <xref ref-type="sec" rid="Ch1.S2"/> presents the data and the study area. The methodology, model inference,  selection, as well as uncertainty analysis, are presented in Sect. <xref ref-type="sec" rid="Ch1.S3"/>. The results are presented in Sect. <xref ref-type="sec" rid="Ch1.S4"/> while discussion are done in Sect. <xref ref-type="sec" rid="Ch1.S5"/>. Finally, the conclusions and some relevant perspectives are given in Sect. <xref ref-type="sec" rid="Ch1.S6"/>.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
      <p id="d2e302">We have a daily precipitation dataset from a total of 934 rain gauges spread across metropolitan France, shown in Fig. <xref ref-type="fig" rid="F1"/>. The data is sourced from the Meteo-France networks and those of Électricité de France (EDF). From the Figure, the EDF stations are primarily situated in mountainous regions, including the Alps, Pyrenees, and Massif Central, for addressing the need of dam management. The data has been screened and homogenized  using an EDF-developed tool that combines Alexanderson's homogeneity test <xref ref-type="bibr" rid="bib1.bibx3" id="paren.31"/>, Bois Ellipse  <xref ref-type="bibr" rid="bib1.bibx12" id="paren.32"/>, and linear regression methods <xref ref-type="bibr" rid="bib1.bibx47" id="paren.33"/>. The length of the series ranges from 64 to 73 years from the period 1950 to 2022.   In this study, we consider only data coming from the autumn season, which we define as consisting of October, November, and December. Autumn is known to be the season when heavy precipitation is observed, particularly in the southern region <xref ref-type="bibr" rid="bib1.bibx8" id="paren.34"/> where the most intense extremes occur. To distinguish between dry and wet-day,  we use a threshold of 1 mm to reduce the uncertainty in the recording procedure.  This threshold of 1 mm is commonly used in the literature <xref ref-type="bibr" rid="bib1.bibx48" id="paren.35"><named-content content-type="pre">e.g.</named-content></xref>.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e327">Map of France showing the locations of 934 rain gauges, colored by network affiliation – Météo-France and Électricité de France (EDF). Some stations and locations cited in the article are also depicted. Black solid lines correspond to French borders and the contours around mountainous regions (400 and 800 m elevation).</p></caption>
        <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f01.png"/>

      </fig>

      <p id="d2e336">To explain the observed trends in wet-day precipitation, we incorporate Sea Surface Temperature (SST) anomaly as a covariate within our nonstationary models.  Warm  SST increases the turbulent near-surface heat fluxes that moisten and destabilize the atmosphere, thereby increasing evaporation and the intensity of convection and precipitation amounts <xref ref-type="bibr" rid="bib1.bibx20" id="paren.36"/>. SST has been widely used as a covariate to explain changes in precipitation <xref ref-type="bibr" rid="bib1.bibx52" id="paren.37"><named-content content-type="pre">e.g.</named-content></xref> and in the south of France by  <xref ref-type="bibr" rid="bib1.bibx57" id="text.38"/>. While other covariates have been used in the literature <xref ref-type="bibr" rid="bib1.bibx29" id="paren.39"><named-content content-type="pre">e.g. climatic covariates in </named-content></xref>, we consider their specific selection to be largely irrelevant for the comparative analysis presented in this study, as all models use the same SST series. In any case, SST provides a stable representation of the thermodynamic changes associated with global warming, allowing for a focused comparison of the internal flexibility of the candidate distributions without the confounding effects of model-selection uncertainty across multiple predictors. A more detailed analysis of covariate selection, including potential regional variations and alternative climate drivers, will form the subject of a future communication.</p>
      <p id="d2e356">The SST data we employ in the study was obtained from the NOAA-NCDC Extended Reconstructed Sea Surface Temperature Dataset Version 5 <xref ref-type="bibr" rid="bib1.bibx27" id="paren.40"/>. We spatially averaged the SST anomalies over the Mediterranean and the proximate Atlantic, specifically spanning longitude 28° W to 19° E and latitude 36 to 58° N (see Fig. <xref ref-type="fig" rid="F2"/>) . Given our focus on long-term trends, the annual SST values were smoothed using nonparametric locally weighted scatter plot smoothing (LOWESS), implemented via the <monospace>lowess</monospace> function in the  <inline-graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-g01.png"/>. Figure <xref ref-type="fig" rid="F2"/> illustrates both the raw and smoothed annual SST and the window over which we take the spatial average.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e376">Smoothed sea surface temperature (SST) used as a covariate in the trend analysis. The red box shows the area over which the spatial average was taken.</p></caption>
        <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methodology</title>
      <p id="d2e393">This section presents the statistical models that we use, the inference procedure, the comparison framework, as well as the method for uncertainty evaluations.</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Nonstationary models</title>
      <p id="d2e403">Let us define  <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as the random variable of daily precipitation recorded in autumn of a given year <inline-formula><mml:math id="M2" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can take either zero or positive values depending whether the day is dry or wet, respectively. As a result,  modeling daily precipitation,  <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, requires a mixed model for the discrete (dry-days) and continuous (wet-day intensity) components. Accordingly, the probability that <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> is <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, while the probability that <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> doesn't exceed a given nonzero  precipitation amount at a given location can be written as

            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M8" display="block"><mml:mrow><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where  <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the dry-day probability, and   <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the wet-day precipitation distribution.</p>
      <p id="d2e637">In this study, we employ the same model for the discrete part, which is obtained by fitting a logistic model to the empirical yearly proportion of dry-days in the data, using the year (<inline-formula><mml:math id="M11" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>) as the covariate. A preliminary analysis (see Fig. <xref ref-type="fig" rid="FA3"/>) revealed time as a better covariate in comparison with SST. The model for the dry-day probability is thus given by:

            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M12" display="block"><mml:mrow><mml:mi>log⁡</mml:mi><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>=</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:msub><mml:mi>t</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e709">In the case of the continuous part, the usual approach is to make a distributional assumption, where we assume that the marginal distribution of wet-day precipitation, <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> can be represented by a parametric distribution <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The subscript (<inline-formula><mml:math id="M15" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>) indicates that the parameters of the distribution change with time, based on a relationship with some temporal covariate, in our case SST. We will present the form of the relationship later.</p>
      <p id="d2e762">Given a specific form for <inline-formula><mml:math id="M16" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula>, the cumulative distribution function (CDF)  of <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can   be written as

            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M18" display="block"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi mathvariant="double-struck">P</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable columnspacing="1em" rowspacing="0.2ex" class="cases" columnalign="left left" framespacing="0em"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:msub><mml:mi>G</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mi>y</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>Statistics of interest</title>
      <p id="d2e912">From Eq. (<xref ref-type="disp-formula" rid="Ch1.E3"/>),  several statistics of interest can be derived, allowing us to analyze their evolution according to the covariates. We enumerate these key statistics below, as their temporal changes will be a focus of our subsequent analysis. <list list-type="order"><list-item>
      <p id="d2e919"><italic>Mean of wet-day distribution.</italic> (<inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). Knowing that <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the CDF for the wet-day precipitation, its mean, denoted as <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,  can be computed from the expectation of <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
<inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="double-struck">E</mml:mi><mml:mo>[</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>|</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>]</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula></p></list-item><list-item>
      <p id="d2e1005">Mean of all-day distribution (<inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>): The mean of all-day distribution (<inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) can be obtained by accounting for the dry-day probability:<disp-formula id="Ch1.Ex1"><mml:math id="M26" display="block"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="double-struck">E</mml:mi><mml:mo>[</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>]</mml:mo><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>where  <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the mean of the wet-day precipitation as defined above.</p></list-item><list-item>
      <p id="d2e1095"><italic>Quantiles of the wet-day distribution</italic> (<inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>). For a given probability  <inline-formula><mml:math id="M29" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>, the precipitation amount not exceeded in the  wet-day precipitation distribution (<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) is obtained from<disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M31" display="block"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>G</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p></list-item><list-item>
      <p id="d2e1170"><italic>Return levels</italic>. (<inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) If the interest is in a given return level, that is an amount that is exceeded, on average,  once every <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:math></inline-formula>years, then we have<disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M34" display="block"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>G</mml:mi><mml:mi>t</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mfenced open="[" close="]"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mi>T</mml:mi><mml:mo>×</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mi mathvariant="italic">δ</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>where <inline-formula><mml:math id="M35" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> is the number of days in the specified season (e.g. <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">92</mml:mn></mml:mrow></mml:math></inline-formula> in autumn).</p></list-item></list></p>
      <p id="d2e1284">Finally, we express the percent relative trend for these statistics as:

              <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M37" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mn mathvariant="normal">2022</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>v</mml:mi><mml:mn mathvariant="normal">1950</mml:mn></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>v</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where  <inline-formula><mml:math id="M38" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula> represents the statistic of interest for example, the mean or a given return level, and  <inline-formula><mml:math id="M39" display="inline"><mml:mover accent="true"><mml:mi>v</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> is the average value of that statistic over the entire period <inline-formula><mml:math id="M40" display="inline"><mml:mn mathvariant="normal">1950</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M41" display="inline"><mml:mn mathvariant="normal">2022</mml:mn></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>Candidates for  the marginal distribution of wet-day precipitation <inline-formula><mml:math id="M42" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula></title>
      <p id="d2e1365">The CDFs of the three distribution that we consider in this study are itemized below: <list list-type="order"><list-item>
      <p id="d2e1370"><italic>Gamma.</italic> The CDF of gamma with a location parameter <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and a scale parameter <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> is giving by<disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M45" display="block"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>y</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>where <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mo>(</mml:mo><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>(</mml:mo><mml:mo>.</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> are the ordinary gamma and incomplete gamma functions respectively. With this parameterization, the mean is given by <inline-formula><mml:math id="M48" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula>, while the <inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> represents the coefficient of variation, i.e  the ratio of the standard deviation to the mean of the distribution. Hence, <inline-formula><mml:math id="M50" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> controls the spread of the distribution. Under this parameterization, the distribution reduces to exponential when <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item>
      <p id="d2e1524"><italic>Generalized Gamma.</italic> Similar to gamma, the CDF of generalized gamma, as implemented in <monospace>gamlss</monospace> <xref ref-type="bibr" rid="bib1.bibx54" id="paren.41"/> is given as:<disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M52" display="block"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:msup></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mfenced close=")" open="("><mml:mi mathvariant="italic">β</mml:mi></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mstyle></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd/></mml:mtr><mml:mtr><mml:mtd><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:mi>y</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow></mml:mfenced><mml:mi mathvariant="italic">ν</mml:mi></mml:msup></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Γ</mml:mi><mml:mfenced open="(" close=")"><mml:mi mathvariant="italic">β</mml:mi></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mstyle></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>with <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mi mathvariant="italic">β</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mi mathvariant="italic">ν</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>.  The distribution has three parameters, <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mtext> and </mml:mtext><mml:mo>-</mml:mo><mml:mi mathvariant="normal">∞</mml:mi><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&lt;</mml:mo><mml:mi mathvariant="normal">∞</mml:mi></mml:mrow></mml:math></inline-formula>. <inline-formula><mml:math id="M57" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> is the location parameter (related to the mean), <inline-formula><mml:math id="M58" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> controls the spread, while <inline-formula><mml:math id="M59" display="inline"><mml:mi mathvariant="italic">ν</mml:mi></mml:math></inline-formula> controls the heaviness of the right tail, thereby affecting the magnitude and frequency of extreme events. The distribution is heavy-tailed when <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>,  reduces to gamma when <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, and  <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates a lighter than gamma-tailed model.</p></list-item><list-item>
      <p id="d2e1786"><italic>EGPD.</italic><disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M63" display="block"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mrow><mml:msup><mml:mfenced open="[" close="]"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>y</mml:mi><mml:mi mathvariant="italic">σ</mml:mi></mml:mfrac></mml:mstyle></mml:mstyle><mml:msubsup><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced><mml:mi mathvariant="italic">κ</mml:mi></mml:msup></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>≠</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd/></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>exp⁡</mml:mi><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mi>y</mml:mi><mml:mi mathvariant="italic">σ</mml:mi></mml:mfrac></mml:mstyle></mml:mstyle><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mi mathvariant="italic">κ</mml:mi></mml:msup></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext> if </mml:mtext><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>where <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mo>+</mml:mo></mml:msub><mml:mo>=</mml:mo><mml:mo>max⁡</mml:mo><mml:mo>(</mml:mo><mml:mi>a</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, the flexibility parameter <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> controls the lower tail, <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> is the scale parameter controlling the spread, and <inline-formula><mml:math id="M67" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> is the shape parameter that controls the upper tail of the distribution.  A positive <inline-formula><mml:math id="M68" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> indicates a heavy-tailed distribution, a negative <inline-formula><mml:math id="M69" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> indicates a bounded distribution, while <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> indicates a light-tailed distribution.</p></list-item></list></p>
</sec>
<sec id="Ch1.S3.SS1.SSS3">
  <label>3.1.3</label><title>Candidate nonstationary models</title>
      <p id="d2e1996">To account for the possibility of nonstationarity, we identify three cases of nonstationarity in the daily precipitation distribution.  They are mainly classified into the following: <list list-type="order"><list-item>
      <p id="d2e2001"><italic>Stationary case (No trend).</italic>  Both the dry and wet-day components remain constant over time, with no trend (Row 1 of Table <xref ref-type="table" rid="T1"/>).</p></list-item><list-item>
      <p id="d2e2009"><italic>Trend in dry-day frequency only.</italic> In this case, only the dry-day frequency exhibits a trend, while the distribution of wet-day precipitation remains stationary (Row 2 of Table <xref ref-type="table" rid="T1"/>).</p></list-item><list-item>
      <p id="d2e2017"><italic>Trend in wet-day distribution only.</italic> Here, the wet-day precipitation distribution shows a trend, but the dry-day frequency remains stationary (Row 3 of Table <xref ref-type="table" rid="T1"/>).</p></list-item><list-item>
      <p id="d2e2025"><italic>Trend in both dry-day frequency and wet-day distribution.</italic> Both the dry-day frequency and the wet-day precipitation distribution exhibit concurrent trends (Row 4 of Table <xref ref-type="table" rid="T1"/>).</p></list-item></list></p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e2035">Candidate models: The first column indicates the type of nonstationarity. The rest of the columns show the implementation based on the choice of the marginal distribution for the wet-day distribution. In each case, the parameter(s) in the subscript are those that are modeled with a trend component, while the number of parameters to be estimated is enclosed in brackets. <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> indicates a stationary model. </p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="2.5cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="2.5cm"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="3cm"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3" align="left">Gamma</oasis:entry>
         <oasis:entry colname="col4" align="left">Generalized</oasis:entry>
         <oasis:entry colname="col5" align="left">Extended Generalized</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3" align="left"/>
         <oasis:entry colname="col4" align="left">Gamma</oasis:entry>
         <oasis:entry colname="col5" align="left">Pareto</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">No trend</oasis:entry>
         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">Trend in dry-day frequency only</oasis:entry>
         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">Trend in wet-day precipitation only</oasis:entry>
         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mi mathvariant="italic">μ</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mi mathvariant="italic">μ</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mi mathvariant="italic">σ</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">Trend in both</oasis:entry>
         <oasis:entry colname="col3" align="left"><inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4" align="left"><inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">8</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5" align="left"><inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>  <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">8</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Number of candidate models</oasis:entry>
         <oasis:entry colname="col3" align="left">6</oasis:entry>
         <oasis:entry colname="col4" align="left">8</oasis:entry>
         <oasis:entry colname="col5" align="left">8</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e2696">Given the three candidate models for the wet-day distribution (GA, GG, and EGPD) presented in the preceding section, Table <xref ref-type="table" rid="T1"/> outlines the various forms of nonstationarity possible for each. This results in 6 variants for GA (ranging from 3 to 6 parameters), and 8 variants for both GG and EGPD (with parameters ranging from 4 to 8). It is worth noting that the standard practice in extreme value theory, particularly when employing GEV or GPD, often involves keeping the shape parameter <inline-formula><mml:math id="M94" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> stationary <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx11 bib1.bibx19" id="paren.42"/>. This approach is typically justified by concerns regarding parameter instability and estimation difficulties due to data limitations. However, in our study, data quantity is not a limitation as we utilize all nonzero daily observations in our inference procedure, allowing us to explore nonstationarity in the shape parameter.</p>
      <p id="d2e2712">Irrespective of the model, a linear relationship is assumed between the model parameter and SST according to

              <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M95" display="block"><mml:mrow><mml:mi mathvariant="italic">η</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SST</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M96" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> represents a given nonstationary parameter of GA, GG, or EGPD. <inline-formula><mml:math id="M97" display="inline"><mml:mi mathvariant="italic">η</mml:mi></mml:math></inline-formula> is a transformation applied to <inline-formula><mml:math id="M98" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, depending on its valid range; it is logarithmic for parameters defined on the positive real line  and identity otherwise.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Inference</title>
      <p id="d2e2783">We use the method of maximum likelihood estimation to infer the parameters of our models. The likelihood of the mixed distribution for a single year <inline-formula><mml:math id="M99" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, assuming independent observations, can be written as:

            <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M100" display="block"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">ψ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:munderover><mml:mo movablelimits="false">∏</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:munderover><mml:mo movablelimits="false">∏</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mfenced close=")" open="("><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where for year <inline-formula><mml:math id="M101" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>,   <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the <inline-formula><mml:math id="M103" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>th daily  precipitation,  <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the PDF of wet-day precipitation, <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">ψ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> is the vector of all model parameters, with <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">θ</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>  the vector of parameters of <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,  <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the total number of days , <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the number of dry days, and <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the number of wet days  in year <inline-formula><mml:math id="M111" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> such that <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d2e3061">The corresponding log-likelihood for a single year <inline-formula><mml:math id="M113" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> is then:

            <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M114" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="normal">ℓ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">ψ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>:</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:munder><mml:mi>log⁡</mml:mi><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d2e3199">For the total observation period across all <inline-formula><mml:math id="M115" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> years, the overall log-likelihood function to be maximized is:

            <disp-formula id="Ch1.E13" content-type="numbered"><label>13</label><mml:math id="M116" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">ℓ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">ψ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:msub><mml:mi mathvariant="normal">ℓ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">ψ</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:munderover><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi>s</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>w</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mi>log⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>:</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:munder><mml:mi>log⁡</mml:mi><mml:mo>[</mml:mo><mml:msub><mml:mi>g</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d2e3373">Here, <inline-formula><mml:math id="M117" display="inline"><mml:mi mathvariant="bold-italic">ψ</mml:mi></mml:math></inline-formula> contains all the parameters that define nonstationary relationships (e.g.  <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for dry-day and <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for wet-day parameters as introduced in Eqs. <xref ref-type="disp-formula" rid="Ch1.E2"/> and <xref ref-type="disp-formula" rid="Ch1.E10"/>).</p>
      <p id="d2e3441">To estimate <inline-formula><mml:math id="M122" display="inline"><mml:mi mathvariant="bold-italic">ψ</mml:mi></mml:math></inline-formula> by maximum likelihood, one can directly maximize the overall log-likelihood in Eq. (<xref ref-type="disp-formula" rid="Ch1.E13"/>). Alternatively, the parameters of the dry-day and wet-day precipitation components can be estimated separately by maximum likelihood. We have tried both and they yield similar estimates. For the remainder of this study, we adopt the second approach. The overall log-likelihood (Eq. <xref ref-type="disp-formula" rid="Ch1.E13"/>) is then calculated using the estimated parameters for subsequent model comparison.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Model selection</title>
<sec id="Ch1.S3.SS3.SSS1">
  <label>3.3.1</label><title>AIC</title>
      <p id="d2e3470">The model selection is through the use of the Akaike Information Criteria (AIC) <xref ref-type="bibr" rid="bib1.bibx2" id="paren.43"/> that rewards goodness-of-fit as measured by the likelihood as well as parsimony, in terms of the number of free parameters.  We adopt AIC because our primary objective is predictive performance rather than identifying a single true model of fixed dimension <xref ref-type="bibr" rid="bib1.bibx14" id="paren.44"><named-content content-type="pre">see</named-content></xref>, an assumption that is unlikely to hold for stochastic rainfall processes. AIC  has also been widely applied for model selection under nonstationarity <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx29" id="paren.45"><named-content content-type="pre">e.g.</named-content></xref>.  The criterion is computed from <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi mathvariant="normal">AIC</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>K</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="normal">ℓ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></inline-formula> where <inline-formula><mml:math id="M124" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> is the number of parameters of a given model (see Table <xref ref-type="table" rid="T1"/>) and <inline-formula><mml:math id="M125" display="inline"><mml:mi mathvariant="normal">ℓ</mml:mi></mml:math></inline-formula> is the log-likelihood from Eq. (<xref ref-type="disp-formula" rid="Ch1.E13"/>). The best model among candidate models is the one with the minimum value of AIC.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <label>3.3.2</label><title>Model Diagnostics</title>
      <p id="d2e3535">In addition to the AIC, we conduct a detailed diagnostic analysis to assess the performance of our candidate nonstationary models. Specifically, we evaluate how well each model captures relative trends <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi>v</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">%</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E6"/>) in key precipitation statistics, compared to those estimated using established benchmark approaches. We consider the four statistics introduced in  Sect. <xref ref-type="sec" rid="Ch1.S3.SS1.SSS1"/>. They are: (i) the mean of wet-day precipitation (<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), (ii) the mean of all-day precipitation (<inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), (iii) wet-day quantiles (<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>), and (iv) 10-year return level.</p>
      <p id="d2e3595">The benchmark methods we use as references are given below: <list list-type="order"><list-item>
      <p id="d2e3600">For the mean of wet-day precipitation (<inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and the mean of all-day precipitation (<inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), we use a  nonparametric approach based on the Theil-Sen slope estimator <xref ref-type="bibr" rid="bib1.bibx55 bib1.bibx51" id="paren.46"/>. This approach to trend estimation calculates the slopes between all possible pairs of data points in the time series and defines the overall trend as the median of all these slopes. Unlike Ordinary Least Squares (OLS), it is insensitive to outliers.</p></list-item><list-item>
      <p id="d2e3629">In the case of  wet-day quantiles (<inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>), we employ   a nonparametric quantile regression (QR) with total variation roughness penalties <xref ref-type="bibr" rid="bib1.bibx33" id="paren.47"/>. While standard regression models the trend in the mean, QR estimates the trend at specific quantiles  (e.g., the 0.5, 0.95, or 0.99). We use the <monospace>quantreg</monospace> R package to fit these trends, using the same SST covariate used in our parametric models.   To assess the performance of our candidate model in both low, medium, and high quantiles, we extract the trends at  <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>∈</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.8</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>,</mml:mo><mml:mtext>and </mml:mtext><mml:mn mathvariant="normal">0.98</mml:mn><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> and compare them to those obtained using QR.</p></list-item><list-item>
      <p id="d2e3711">For the 10-year return level,  we consider the estimated trends from a nonstationary GEV model  fitted to the seasonal block maxima.  At each station, we fit three versions of the NS-GEV and selected the one with the lowest AIC. The versions are: GEV-<inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mi mathvariant="italic">μ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, GEV-<inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mi mathvariant="italic">σ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and GEV-<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, where   <inline-formula><mml:math id="M137" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M138" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> are the GEV location and scale parameters. In each case, we use SST as the covariate, as is the case in our candidate models.</p></list-item></list></p>
      <p id="d2e3766">This process yields, for each model and each statistic, a set of 934 trend estimates, one per station, which are then compared directly to the 934 benchmark estimates for the same stations. A well-performing model is expected to closely match the benchmark trends across stations, both in direction and magnitude. To quantify the agreement, we utilize the Concordance Correlation Coefficient (CCC)

              <disp-formula id="Ch1.E14" content-type="numbered"><label>14</label><mml:math id="M139" display="block"><mml:mrow><mml:mi mathvariant="normal">CCC</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">ρ</mml:mi><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi>y</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M140" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> is the Pearson correlation.</p>
      <p id="d2e3839">This metric provides a comprehensive measure of the agreement in both the direction and magnitude of the trends.  Being a correlation measure, it takes values from <inline-formula><mml:math id="M141" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1 to 1, with 1 indicating perfect correlation. While classical correlation measures like Pearson's and Spearman's coefficients measure the linear or monotonic relationship, they are insensitive to bias or scale differences in the two variables. This is why we employ CCC, which measures the agreement, penalizing both scale and bias differences (the <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> term).</p>
</sec>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Trend significance and uncertainties</title>
      <p id="d2e3882">We assess the uncertainty and significance of a given trend through nonparametric bootstrap as done in <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx19" id="text.48"/>. To implement this, the trend for a given statistic of interest is re-estimated from bootstrap samples, which are generated by sampling with replacement from the original data. This resampling procedure is repeated 400 times, giving 400 sets of parameters. A trend is considered statistically significant if zero is not contained within the 2.5 % and 97.5 % empirical centiles of its bootstrap estimates. We comment here that the resampling is applied to the residuals of the original sample, rather than directly to the raw data. This approach ensures that the bootstrap samples are identically distributed. The residuals are obtained by applying the CDF of the given nonstationary model to the original sample. The bootstrap samples of residuals are then back-transformed using the quantile function of the nonstationary model to generate new precipitation series for trend estimation. For a more detailed exposition of this bootstrap procedure, readers are referred to Sect. 3.4 of <xref ref-type="bibr" rid="bib1.bibx26" id="text.49"/>.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Goodness-of-fit and model selection</title>
      <p id="d2e3907">This section presents a graphical diagnostic of the goodness-of-fit of some of the fitted models at some randomly selected stations. Next, we show the results of the model selection based on AIC.</p>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>Graphical diagnostics: Quantile-Quantile plots</title>
      <p id="d2e3917">We start with a diagnostic analysis to rigorously assess the goodness-of-fit of the models, utilizing graphical diagnostics, in this case, residual quantile–quantile (Q–Q) plots. Compared to classical Q–Q plots, residual Q–Q plots are relevant in the case of data that are not identically distributed <xref ref-type="bibr" rid="bib1.bibx16" id="paren.50"/>.  To produce the plots, we first transform the data for each year using the CDF derived from the fitted nonstationary model. When the model is correctly specified, this transformation yields uniformly distributed data within the interval (0, 1). Next, we transform this uniformly distributed data using the inverse CDF of the exponential distribution.  Consequently, the data become approximately identically distributed according to the exponential distribution. Using the exponential distribution facilitates the creation of effective Q–Q plots with a clearer visualization of the upper tail.  Figure <xref ref-type="fig" rid="F3"/> showcases the exponentiated quantile residual plots at some randomly selected stations. In each case, the points are colored according to the given distribution. Note that in the figure, the most flexible variant of each distribution  is considered; <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for GA, <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for GG and <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in the case of EGPD.  For a good model, the points should lie on the diagonal, here shown by the dashed line. In general, for all the cases shown here, all the points lie reasonably close to the diagonal, showcasing a good model fit. A few exceptions can be observed, with some deviations around the tail. Note that the Q–Q plots shown here are just for illustration of the model fit, rather than a comparison, due to the difference in the number of parameters of the models. A more flexible model is in general expected to perform better in comparison to a less flexible model. The next section uses AIC, which accounts for model complexity,  to compare and rank the models.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e4004">Illustration of model fits using exponentiated quantile residuals plots at some selected stations. The three models are gamma (GA-<inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>), generalized gamma (GG-<inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) and, extended generalized Pareto (EGPD-<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>).</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f03.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>AIC: Intramodel comparison</title>
      <p id="d2e4098">This section presents the model selection results based on AIC, applied separately to the variants of each candidate wet-day distribution (GA, GG and EGPD). Figure <xref ref-type="fig" rid="F4"/> illustrates these results for all three distributions. In each subplot of Fig. <xref ref-type="fig" rid="F4"/>, stationary models (indicating no trend) are represented by black-filled circles. Models incorporating a trend solely in the dry-day frequency are shown with yellow-filled circles. Models with trends exclusively within the wet-day distribution are depicted by square shapes, with varying shades of maroon. The darker the color, the higher the complexity of the model in terms of the number of parameters. Lastly, models featuring trends in both dry-day frequency and wet-day distribution are indicated by triangular shapes, with various shades of green. Across all three maps, there is a strong agreement in the spatial coherence of the selected model forms for nonstationarity, particularly evident between the two three-parameter distributions (GG and EGPD). Observing the regional patterns, especially in the northern and western parts of France (excluding areas along the Pyrenees), models with either a trend in dry-day frequency (yellow) or trends in both components (green triangular shapes) are consistently selected, regardless of the chosen wet-day distribution. A similar pattern emerges along the northern Alps and some locations along the southern part of the Massif Central, where models showing trends only in the wet-day distribution (maroon-colored square shapes) are favored. Finally, there is also notable agreement in locations where stationary models (black-colored circles) are selected, specifically at some stations along the Pyrenees and near the Mediterranean. Figure <xref ref-type="fig" rid="F5"/> further summarizes the number of stations corresponding to each form of nonstationarity across the three distributions, confirming the high degree of similarity, especially between the GG and EGPD.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e4109">Maps showing the model selection results based on AIC applied to the variants of each distribution separately. Each station is colored according to the best model. Stationary models (indicating no trend) are shown by black-filled circles. Models with trend in only the dry-day frequency are shown with yellow-filled circles. Models with trends in only the wet-day distribution are depicted by square shapes, with varying shades of maroon.  Lastly, models featuring trends in both dry-day frequency and wet-day distribution are indicated by triangular shapes, with various shades of green. The darker the color, the higher the complexity of the model in terms of the number of parameters.</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f04.png"/>

          </fig>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e4120">Number of stations with a given type of nonstationarity (horizontal axis) selected based on AIC. </p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f05.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <label>4.1.3</label><title>AIC: Intermodel comparison</title>
      <p id="d2e4137">We now proceed with the overall model selection based on AIC, irrespective of the initial distributional family. To achieve this, we compared the AIC of the best model (chosen in the preceding “Intramodel Comparison” section) from each of the three candidate distributions – GA, GG, and EGPD. The model with the lowest AIC value among these three is then selected as the overall best-performing model for that specific station. Figure <xref ref-type="fig" rid="F6"/> showcases the result of this selection. Each station is colored according to the best-performing distribution. In summary, the GG emerges as the preferred distribution in the majority of locations (68 %), followed by EGPD in 22 % of cases, and finally, GA in 10 %. There is no clear spatial pattern for the stations where the Gamma distribution is selected. For EGPD, however, the model appears to be favored in the region around the northeast of the Massif Central.</p>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e4144">Model selection result based on AIC  irrespective of the initial distributional family. Each station is colored according to the best-performing distribution, while shapes are used to illustrate the corresponding type of nonstationarity identified. </p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f06.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Model performance in capturing trends evolutions</title>
      <p id="d2e4162">While the AIC provides a solid theoretical justification for model selection by balancing goodness-of-fit and parsimony, we take a further step to evaluate the models based on their performance in reproducing relative trends (<inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi>v</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">%</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>). We compare our models' outputs against benchmark relative trends (<inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mi>v</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">%</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) obtained through nonparametric QR and nonstationary GEV models, as detailed in Sect. <xref ref-type="sec" rid="Ch1.S3.SS3.SSS2"/>. This  evaluation involves checking the trends in: (i) the mean of wet-day and all-day precipitation; (ii) low, medium, and high quantiles of the wet-day distribution; and (iii) extreme precipitation. The results are presented in the following subsections.</p>
<sec id="Ch1.S4.SS2.SSS1">
  <label>4.2.1</label><title>Trend  in wet-day quantiles</title>
      <p id="d2e4202">Given that a reliable model should accurately capture trends across the entire wet-day precipitation distribution, including low, medium, and high quantiles, we compare the performance of our candidate models using QR as a nonparametric benchmark. Figure <xref ref-type="fig" rid="F7"/>  shows the scatter plots (top row) of the nonzero precipitation (points) at three stations  (see locations in Fig. <xref ref-type="fig" rid="F1"/>), along with time-evolving wet-day quantiles (<inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) estimated with QR, for <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>∈</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0.8</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>,</mml:mo><mml:mn mathvariant="normal">0.98</mml:mn><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> (colored-lines). The three stations exhibit contrasting behaviors in terms of the trend direction.  Neuilly-sur-Marne has all the quantiles decreasing with time (unidirectional behavior), Amberieu has its low quantiles decreasing and the high quantiles increasing with time (bidirectional), while Paris-Montsouris has a negative trend in the lowest quantiles, transitioning to positive trends in the medium quantiles, and then reverting to negative in the highest quantiles (tridirectional).  A good model among our candidate models should be able to reproduce all this behavior.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e4264">Comparison of quantile trend evolutions for selected stations. The top row shows the time series plot of nonzero precipitation along with time-evolving quantiles predicted with nonparametric QR. The bottom row depicts the tile plots of relative trends (<inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:mi>v</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">%</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>), estimated with QR and the candidate model,  colored according to the trend direction (blue for positive trends, red for negative trends). The horizontal axis represents the quantile.</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f07.png"/>

          </fig>

      <p id="d2e4287">The second row presents the tile plots of relative trends (<inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mi>v</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">%</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) estimated with QR and the candidate models for the three stations,  colored according to the trend direction (blue for positive, red for negative). The quantiles are given on the horizontal axis, while the candidate models are depicted on the vertical axis, arranged from bottom to top,  in order of complexity (number  of  free parameters).  The models with the lowest flexibility, having only a single wet-day parameter varying with SST (GA-<inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, GG-<inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and EGPD-<inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>),  resulted in a single trend irrespective of the quantile and station. Notice in the case of Neuilly-sur-Marne  with unidirectional behavior,  although these models predicted a decreasing trend, the trends are independent of the quantile level.   The models with two wet-days parameters evolving with SST (GA-<inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, GG-<inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and EGPD-<inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) are able to show a bidirectional behavior, with negative trends for the smallest quantiles, and positive trends for the highest quantiles in the case of Amberieu which show a bidirectional behavior. The tridirectional behavior in the case of  Paris-Montsouris is only reproduced with the most flexible models  (GG-<inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and EGPD-<inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) as revealed by QR.</p>
      <p id="d2e4486">To generalize the result across all the stations, we use the  Concordance Correlation Coefficient (CCC) (detailed in Sect. <xref ref-type="sec" rid="Ch1.S3.SS3.SSS2"/>) to quantitatively assess the agreement between the relative trends (<inline-formula><mml:math id="M163" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula>(%)) from our models and those from QR.  For each quantile <inline-formula><mml:math id="M164" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>, we compute the CCC between the trends estimated with QR and each of the candidate models. The best model among the candidate models should have CCC = 1, signifying a perfect agreement with QR for that quantile level.  The results is presented in Fig. <xref ref-type="fig" rid="F8"/>. In the figure, GA models are depicted in shades of maroon, GG models in shades of green, and EGPD models in shades of blue; in each case, a darker shade denotes a more flexible model (i.e., more parameters changing with SST). Analyzing result,  the GG model <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> demonstrated the highest agreement with QR for virtually all quantiles. It is closely followed by the EGPD model <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>. The least flexible models, with only one parameter changing with SST, irrespective of the distribution, have the lowest correlation.  It is worth noting that, irrespective of the criterion, all the models have nearly similar performance within the bulk of the distribution (around <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>), but the disparity appears around the tails, especially the upper tail. The most flexible models GG model <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and the EGPD model <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in particular standout in their exclusive performance in the upper tail, where the other less flexible models have much lower performance. This strongly suggests that the increased flexibility of these models is indeed justified for accurately capturing the complex trend evolutions observed across the entire range of the precipitation dataset.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e4630">Comparison of model performance in reproducing relative trend in wet-day quantiles. The figure shows the Concordance Correlation Coefficient (CCC) computed between the relative trends estimated with QR  and each of the candidate models at all the stations. Gamma (GA) models are in shades of maroon, Generalized Gamma (GG) models in shades of green, and Extended Generalized Pareto Distribution (EGPD) models in shades of blue. Darker shades indicate more flexible models (more parameters evolving with SST).</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f08.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS2.SSS2">
  <label>4.2.2</label><title>Trend in  mean precipitation</title>
      <p id="d2e4647">The maps of the relative trends in mean wet-day precipitation (<inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) from our candidate models alongside a nonparametric benchmark based on Theil-Sen slope estimator are shown in Fig. <xref ref-type="fig" rid="F9"/>. The top row showcases trends predicted by the three GG model variants. The second row corresponds to the three EGPD model variants, while the first two maps in the bottom row represent the two GA model variants. The map on the bottom-right illustrates trends derived using the Theil-Sen slope estimator.  In general, all the models exhibit a similar spatial pattern in both the magnitude and direction of trends when compared to those obtained with the Theil-Sen slope method. This strong agreement is quantitatively confirmed by  a Concordance Correlation Coefficient (CCC)  close to one for all the models. While all models yield very satisfying results, GA-<inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> notably demonstrates the best performance. This can be attributed to its direct parametrization, where the evolving parameter <inline-formula><mml:math id="M172" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> is precisely the mean of the Gamma distribution itself.  For the case of the mean of all-day precipitation (<inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), the performance of the models is nearly indistinguishable. The maps of the trends for this statistic are provided in Fig. <xref ref-type="fig" rid="FA1"/>.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e4705">Maps of relative trends (%) in mean wet-day precipitation (<inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) for various nonstationary models and the Theil-Sen benchmark. Top row: GG models. Second row: EGPD models. Bottom row (first two maps): GA models. Bottom-right map: Trends obtained using the nonparametric Theil-Sen slope estimator (benchmark).</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f09.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS2.SSS3">
  <label>4.2.3</label><title>Trend in extreme precipitation</title>
      <p id="d2e4733">In this section, we compare the performance of the models in terms of the relative trends in extreme precipitation, specifically focusing on the 10-year return level (<inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>). To serve as a benchmark, we use a nonstationary GEV model (NS-GEV)  by parameterizing <inline-formula><mml:math id="M176" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> and/or <inline-formula><mml:math id="M177" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> as linear functions of SST to estimate these trends.  Figure <xref ref-type="fig" rid="F10"/> illustrates some return level plots at three stations (the same stations shown in Fig. <xref ref-type="fig" rid="F7"/>), comparing the trends obtained with GEV benchmark and the most flexible version of each of the three distributions (GA-<inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, GG-<inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and EGPD-<inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>).  For all the stations,  the least agreement is obtained with GA-<inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>. This is more apparent in the case of Paris-Montsouris, where the model predicts an opposing trend evolution compared to the other models, both for the 2-year and 10-year return level.</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e4873">Comparison of 2-year and 10-year return levels evolution for selected stations. Each panel displays return levels from the GEV benchmark (purple line) and the most flexible variant of each candidate distribution: GA-<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (orange line), GG-<inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (lime-green line), and EGPD-<inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (cyan line). The horizontal axis indicates the year, vertical axis is the precipitation amount.</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f10.png"/>

          </fig>

      <p id="d2e4938">Figure <xref ref-type="fig" rid="F11"/> shows the maps of the relative trends (%) in a 10-year return level estimated by our candidate models and the GEV over all the stations in the study area. Similar to Fig. <xref ref-type="fig" rid="F9"/>, the top rows show the trend predicted with the three GG models, the second row corresponds to the three EGPD models, while the first two maps in the bottom row correspond to the two GA models. The map on the bottom right corresponds to the trends obtained using the GEV. A first look at the spatial pattern reveals a column-wise similarity. The first column corresponds to models with only one nonstationary parameter. With these models, the trend is generally positive or close to zero in the north and the southwest. Negative trends are mainly observed near the Provence in the south and the northwest  of the Massif Central. The second column, which represents models with nonstationarity in two parameters, exhibits spatial patterns similar to those in the first column but with generally higher magnitudes of trends. A significant increase in the contrast of the spatial pattern of trends is observed in the last column, which corresponds to the most flexible models with three parameters (GG-<inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and EGPD-<inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>). This column reveals a distinct cluster of stations with negative trends around the Parisian area and the northeast, a pattern not as pronounced in less flexible variants. Furthermore, stronger negative trends are now evident in the southeastern and western sides of the Massif Central.  This pattern is in close agreement with the trends modeled using the GEV benchmark.</p>

      <fig id="F11" specific-use="star"><label>Figure 11</label><caption><p id="d2e5002">Maps of relative trends (%) in the 10-year return level (<inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) for various nonstationary models and the GEV benchmark. Top row: GG models. Second row: EGPD models. Bottom row (first two maps): GA models. Bottom-right map: Trends obtained using the nonstationary GEV model (benchmark).</p></caption>
            <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f11.png"/>

          </fig>

      <p id="d2e5027">Finally, to obtain a quantitative measure of the model's performance, we apply the Concordance Correlation Coefficient between the relative trend estimates obtain with the GEV and each of the candidate models. The results show that the  GG-<inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and EGPD-<inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> have the closest agreement with GEV (CCC = 0.8) compared to the other models with CC ranging from 0.4 to 0.55.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Observed trends and uncertainties with the best model</title>
      <p id="d2e5093">Our two complementary model comparison approaches, AIC-based selection and models' ability to capture trends, consistently point to similar conclusions regarding the most suitable distribution and its most effective nonstationary variant. The first approach, based on AIC, revealed GG as the favored distribution at 68 % of the stations compared to 22 % for the  EGPD and 20% for the  GA. The second approach, which rigorously assesses the models' ability and flexibility in capturing trends across the entire precipitation spectrum, also largely favored GG, and in particular the most flexible variant GG-<inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>. It is important to note that EGPD performed very similarly to GG in terms of trend reproduction. For instance, even when AIC more frequently selected GG variants, the spatial patterns of the best-performing variants for both GG and EGPD were strikingly similar (Figs. <xref ref-type="fig" rid="F4"/> and <xref ref-type="fig" rid="F5"/>). More interestingly,  both the GG-<inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and EGPD-<inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> models exhibited very similar, strong performances across the CCC, especially across wet-days quantiles and extreme preciptation. In contrast, the Gamma distribution, even its most flexible variant (GA-<inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>), consistently proved unable to adequately reproduce the observed complex trends.</p>

      <fig id="F12" specific-use="star"><label>Figure 12</label><caption><p id="d2e5207">Maps of relative trends and their significance for the selected best model (GG-<inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>). The top row shows trends in the mean of wet-day precipitation (<inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), the mean of all-day precipitation (<inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), and the 10-year return level (<inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>). Negative trends are shown in red, while positive trends are in blue. The bottom row shows the same maps, but only where the trends are  statistically significant based on the nonparametric bootstrap procedure (Sect. <xref ref-type="sec" rid="Ch1.S3.SS4"/>).</p></caption>
          <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f12.png"/>

        </fig>

      <p id="d2e5283">Based on the results, therefore, we consider GG as the best distribution and, in particular, the variant GG-<inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> to be a viable choice for modeling nonstationary daily precipitation in this region. The top row of Fig. <xref ref-type="fig" rid="F12"/> shows the relative trends obtained in the case of the mean of wet-day precipitation (<inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), the mean of all-day precipitation (<inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), and a 10-year return level <inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>. Negative trends are shown in red, while positive trends are shown in blue. The bottom row shows the same trends, but masking the nonsignificant trends based on the bootstrap procedure described in Sect. <xref ref-type="sec" rid="Ch1.S3.SS4"/>. The figure reveals a significant increase in the mean of wet-day precipitation, notably in the southeastern part. The mean of  all-day precipitation, on the other hand, shows a significant increase everywhere, except the southwestern region. In terms of extreme precipitation,  significant positive trends in the 10-year return level appear along the Rhone valley, the southeast, and some locations around Brittany. Significant negative trends are obtained at some locations in the northern Alps and the western side of the Massif Central.   While this illustrates the modeled trends, a more detailed spatial and seasonal analysis of these trends and a deeper investigation of covariate selection will be the subject of subsequent communications.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
      <p id="d2e5366">This study presents a comprehensive comparison framework for selecting the best nonstationary model of daily precipitation using a mixed discrete-continuous distribution, driven by SST and time as a key covariates. By evaluating various distributional families (GA, GG, EGPD) and their nonstationary variants, our approach moves beyond traditional stationary or simpler nonstationary methods to provide a more refined understanding of precipitation trends. We have chosen France as a case study due to its wide diversity of climates with different influences (Atlantic in the West, Mediterranean in the South, continental in the East) and a complex topography (Pyrenees, Massif Central, Alps). It also presents a dense network of long time series of observed precipitation, which enables the regional characterization of the trends. The multi-criteria model selection process, combining AIC with rigorous diagnostic comparisons of trend evolutions, has revealed critical insights into the best-performing models and the nature of precipitation nonstationarity across France.</p>
      <p id="d2e5369">A central finding of our AIC-based model selection is the evidence for nonstationarity in autumnal french daily precipitation (either in the dry-day frequency, wet-day distribution or both), with the stationary case being rarely selected (Fig. <xref ref-type="fig" rid="F4"/>). This shows the inadequacy of the stationary model and the need to incorporate evolving hydro-climatic conditions in climate impact studies and assessments. Furthermore, our intramodel comparisons revealed a strong spatial coherence in the form of nonstationarity, irrespective of the wet-day distribution assumed. The prevalence of trends in dry-day frequency (in isolation or alongside wet-day intensity trends) in northern and western France, contrasting with wet-day intensity-only trends in the southwest, suggests the possibility of geographically distinct climate drivers. This regional heterogeneity reinforces the need for localized nonstationary modeling rather than applying a single, uniform model across diverse climatic zones. For a regional study where continuous parameter maps are required, the most flexible model that accounts for all scenarios of nonstationarity, might be more appropriate.</p>
      <p id="d2e5374">The intermodel comparison conclusively demonstrated the superior performance of the GG distribution, which was selected by AIC at 68 % of stations. This widespread preference for GG can be attributed to its optimal balance of flexibility and parsimony. As a three-parameter distribution, GG offers greater adaptability to capture a wider range of shapes (e.g., varying skewness and kurtosis, inclusive of heavy tails) inherent in precipitation data compared to the two-parameter GA distribution. The absence of a clear spatial pattern for GA selections implies that where it is preferred, it likely reflects highly localized data characteristics that do not consistently align with broader geographical or climatic influences, rather than a systematic regional fit. This finding aligns with growing evidence in hydrological modeling that more flexible distributions, like the GG, are often better suited for complex environmental data <xref ref-type="bibr" rid="bib1.bibx45" id="paren.51"><named-content content-type="pre">e.g.,</named-content></xref>, especially precipitation with its high skewness.</p>
      <p id="d2e5382">While EGPD is also a three-parameter model designed for robust tail modeling (with <inline-formula><mml:math id="M202" display="inline"><mml:mi mathvariant="italic">κ</mml:mi></mml:math></inline-formula> controlling the lower tail, <inline-formula><mml:math id="M203" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> the spread, and <inline-formula><mml:math id="M204" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> the upper tail), its lower overall selection rate by AIC compared to GG, despite similar flexibility, suggests that the GG's family of shapes may better represent the overall characteristics of daily precipitation in most French regions. This is supported by Fig. <xref ref-type="fig" rid="F8"/> where the EGPD showed slightly lower performance compared to GG in the lower tails.  However, the concentrated selection of EGPD in specific areas like the northeast of the Massif Central indicates that its unique tail-capturing capabilities, particularly through its <inline-formula><mml:math id="M205" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> parameter, are indeed necessary for regions with distinct extreme precipitation characteristics. Figure <xref ref-type="fig" rid="FB1"/> highlight that precipitation in these regions is heavy-tailed, as measured by the shape parameters of stationary GG, EGPD, and GEV.</p>
      <p id="d2e5419">Beyond AIC, our diagnostic evaluations of trend reproduction further corroborated these findings. The ability of the most flexible GG-<inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and EGPD-<inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> variants to accurately reproduce the complex, often non-monotonic, trends in mean, quantile, and return level evolutions, especially in the tails, provides compelling empirical support for their increased flexibility. This was particularly evident in the tri-directional quantile trends observed at stations like Paris-Montsouris (Fig. <xref ref-type="fig" rid="F7"/>), which only the most flexible models could capture, while less flexible or simpler distributions like GA often exhibited significant biases. The strong agreement of these models with nonparametric QR and nonstationary GEV benchmarks underscores their robustness. This comprehensive validation addresses a crucial gap in many nonstationary studies that rely solely on information criteria for model selection.</p>
      <p id="d2e5478">It is pertinent to discuss our findings on parameter nonstationarity in the context of traditional extreme value theory applications. In many studies employing the GEV or GPD  for extreme precipitation analysis, trends are often modeled by allowing nonstationarity in only the location (<inline-formula><mml:math id="M208" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula>) or scale (<inline-formula><mml:math id="M209" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>) parameters, or both <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx11" id="paren.52"><named-content content-type="pre">e.g.,</named-content></xref>. The shape parameter (<inline-formula><mml:math id="M210" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula>) is frequently kept stationary, partly due to concerns about its estimation stability given limited extreme data points. However, in our mixed-distribution framework, the entire wet-day distribution is modeled, implying that the location and scale parameters (e.g., of the GG or EGPD) are heavily influenced by the bulk of the distribution, not just the extremes. Consequently, to adequately capture complex trends specifically in the extremes of the distribution, allowing for nonstationarity in the shape parameter (e.g., <inline-formula><mml:math id="M211" display="inline"><mml:mi mathvariant="italic">ν</mml:mi></mml:math></inline-formula> for GG, and particularly <inline-formula><mml:math id="M212" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> for EGPD) becomes crucial. Our results, particularly the superior performance of the most flexible models GG-<inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and EGPD-<inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in accurately reproducing trends in the upper quantiles and return levels, empirically support the necessity of this additional flexibility in the shape parameter to adequately characterize nonstationary in the upper tail of the precipitation distribution.</p>
      <p id="d2e5576">The observed trends with the best-performing GG-<inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> model reveal significant and spatially heterogeneous changes in daily precipitation characteristics across France. The widespread significant increase in wet-day frequency and mean all-day precipitation across most of the study area, coupled with a notable increase in wet-day intensity in the southeast, points towards a general moistening trend. However, the significant positive trends in the 10-year return levels in regions like the Rhône Valley and the southeast are particularly concerning. These findings indicate an intensification of extreme precipitation events, which carries substantial implications for flood risk management, agricultural planning, and water resource infrastructure in these vulnerable regions.</p>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d2e5614">Our study aimed to identify a suitable distribution that can flexibly model the observed trends in the entire range of daily precipitation distribution. Given the discrete-continuous nature of daily precipitation, resulting from the occurrence of dry and wet-day, we employ a mixed distribution of discrete type for the dry component, and continuous type for the nonzero component.  We identify three distributions commonly used in the literature for modeling nonzero precipitation: gamma, generalized gamma, and extended generalized Pareto (EGPD). Using these distributions, we form a number of nonstationary models, accounting for three main forms of nonstationarity: (i) Trend in only the dry-day frequency, (ii) Trend in only the wet-day distribution, and (iii) Trend in both the dry-day frequency and the wet-day distribution. Irrespective of the given distribution, we employ time as a covariate for the dry-day component, and sea surface temperature for parameters of the wet-day precipitation distribution.</p>
      <p id="d2e5617">We employ an approach based on information theory, utilizing AIC to select the best nonstationary model, complemented by an assessment of each model's capacity to flexibly capture trends across low, medium, and extreme quantiles of the precipitation distribution. As a case study, we consider autumnal daily precipitation in France at over 900 stations. The main findings of the study can be summaried below: <list list-type="order"><list-item>
      <p id="d2e5622">Irrespective of the chosen distribution, the resulting form of nonstationarity identified by AIC was regionally coherent, with the models involving a trend in the dry-day frequency selected in most of the study area.</p></list-item><list-item>
      <p id="d2e5626">The two-parameter gamma distribution, commonly employed,  lacked the flexibility to model the observed trends across the entire distribution, even when both parameters evolve with the covariates.</p></list-item><list-item>
      <p id="d2e5630">The three parameter models,  generalized gamma and EGPD, sufficiently capture the trends across the distribution, only after their shape parameters are allowed to evolve with the covariate.</p></list-item><list-item>
      <p id="d2e5634">AIC favored the generalized gamma, although both EGPD has similar performance at capturing the trends. This suggests both distributions offer robust alternatives to the simpler gamma, especially when nonstationary modeling is paramount.</p></list-item></list></p>
      <p id="d2e5637">These findings underscore the importance detailed and multi-criterion approach to model identification in trend analysis, particularly under changing climatic conditions, due to the resulting implications for both hydrological and climate impact assessments. Our study contributes to the critical challenge of flexibly modeling observed trends across the entire distribution of daily precipitation, a task complicated by its inherent discrete-continuous nature. With regards to stochastic weather generators, a major challenge is the seamless representation of both frequent low-intensity events and rare extremes. By using a single flexible distribution (like the EGPD or GG) that maintains statistical consistency across the full spectrum, these models avoid the artificial discontinuities often found in “split-model” generators (e.g., Gamma for the bulk and GPD for the tail). Because our model parameters are conditioned on covariates, these models are uniquely capable of generating non-stationary synthetic series. By forcing the models with GCM-derived SST or other relevant covariates projections, they can produce future stochastic rainfall realizations that account for thermodynamically and dynamically driven shifts in both mean and extreme intensities. Building on these results, the next phase of our research will involve a detailed trend analysis of French daily precipitation using the generalized gamma model. This will include comprehensive covariate selection, involving additional large-scale climate indices or local drivers,  and evaluation of regionally varying influences, ultimately contributing to more robust climate adaptation strategies for critical sectors such as water resource management, agriculture, and flood risk assessment.</p>
</sec>

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

<app id="App1.Ch1.S1">
  <label>Appendix A</label><title>Trends in some metrics</title>
      <p id="d2e5651">Figure <xref ref-type="fig" rid="FA1"/> shows the trends in mean of all-day precipitation from our candidate models alongside a nonparametric benchmark. The top row showcases trends predicted by the three GG model variants. The second row corresponds to the three EGPD model variants, while the first two maps in the bottom row represent the two GA model variants. The map on the bottom-right illustrates trends derived using the Theil-Sen slope estimator, which serves as our nonparametric benchmark for mean trends.</p>
      <p id="d2e5656">Figure <xref ref-type="fig" rid="FA2"/>  depicts the map of the dry-day component parameters. For interpretability, we show  <inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mn mathvariant="normal">950</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, the dry day frequency at the beginning of the period,  1950, instead of the intercept term <inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, which is the log-odds of a dry day in a year. The map shows that the probability of rain is lowest in the southeast region, particularly the Mediterranean area. The map of <inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, the change in the log-odds per year, shows that most of the region is experiencing a decrease in the log-odds of dry frequency, signifying an increase in the wet-day frequency.</p>

      <fig id="FA1"><label>Figure A1</label><caption><p id="d2e5710">Maps of relative trends (%) in mean all-day precipitation (<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for various nonstationary models and the Theil-Sen benchmark. Top row: GG models. Second row: EGPD models. Bottom row (first two maps): GA models. Bottom-right map: Trends obtained using the nonparametric Theil-Sen slope estimator (benchmark).</p></caption>
        
        <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f13.png"/>

      </fig>

<fig id="FA2"><label>Figure A2</label><caption><p id="d2e5736">Dry-day component parameters from the logit model.</p></caption>
        
        <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f14.png"/>

      </fig>

      <fig id="FA3"><label>Figure A3</label><caption><p id="d2e5749">Changes in Wet-day frequency (<inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) in autumn using Sen’s slope (reference, left), and two regression models with SST (center) and time (right) as covariates.</p></caption>
        
        <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f15.png"/>

      </fig>


</app>

<app id="App1.Ch1.S2">
  <label>Appendix B</label><title>Shape parameters</title>
      <p id="d2e5785">Figure <xref ref-type="fig" rid="FB1"/> shows the map of shape parameters obtained  with GEV and the nonstationary  EGPD and GG (<inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ν</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in EGPD-<inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and GG-<inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> respectively). In the case of GEV and EGPD, the tail is heavy when <inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, light when <inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and bounded when <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>. For GG,  the tail is heavy when <inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, gamma like when <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, and lighter than gamma when <inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>.</p>

      <fig id="FB1"><label>Figure B1</label><caption><p id="d2e5941">Map of upper tail shape parameters obtained with GEV and the nonstationary  EGPD and GG (<inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ν</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in EGPD-<inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ξ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and GG-<inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="script">M</mml:mi><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">ν</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> respectively). Red color shows locations with bounded tails, blue colors show heavy tails, while light tails are shown in white.</p></caption>
        
        <graphic xlink:href="https://ascmo.copernicus.org/articles/12/87/2026/ascmo-12-87-2026-f16.png"/>

      </fig>


</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e6034">The open data source from Meteo-France can be obtained from: <uri>https://www.data.gouv.fr/fr/organizations/meteo-france/</uri> (last access: 15 March 2024).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e6043">AH performed the numerical computations and prepared the paper.  EP prepared the datasets. All authors participated in the discussions, analysis of the results, and writing of the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e6049">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e6055">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e6061">Part of this study has received funding from the Agence Nationale de la Recherche – France 2030 as part of the PEPR “Transformer la modélisation du climat pour les services climatiques” (TRACCS) program under grant no. ANR-22-EXTR-0005, and by Électricité de France (EDF) in the framework of a collaboration with CNRS/IGE.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e6066">This research has been supported by the Agence Nationale de la Recherche (France 2030 as part of the PEPR “Transformer la modélisation du climat pour les services climatiques” (TRACCS) program under grant no. ANR-22-EXTR-0005).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e6073">This paper was edited by Mark Risser and reviewed by two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><label>Abbas et al.(2025)Abbas, Ahmad, and Ahmad</label><mixed-citation>Abbas, A., Ahmad, T., and Ahmad, I.: Modeling zero-inflated precipitation extremes, Commun. Stat., 1–17, <ext-link xlink:href="https://doi.org/10.1080/03610918.2025.2585398" ext-link-type="DOI">10.1080/03610918.2025.2585398</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Akaike(1974)</label><mixed-citation>Akaike, H.: A new look at the statistical model identification, IEEE T.  Automat. Contr., 19, 716–723, <ext-link xlink:href="https://doi.org/10.1109/TAC.1974.1100705" ext-link-type="DOI">10.1109/TAC.1974.1100705</ext-link>, 1974.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Alexandersson(1986)</label><mixed-citation>Alexandersson, H.: A homogeneity test applied to precipitation data, J. Climatol., 6, 661–675, <ext-link xlink:href="https://doi.org/10.1002/joc.3370060607" ext-link-type="DOI">10.1002/joc.3370060607</ext-link>, 1986.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Ayar et al.(2020)Ayar, Blanchet, Paquet, and Penot</label><mixed-citation>Ayar, P. V., Blanchet, J., Paquet, E., and Penot, D.: Space-time simulation of precipitation based on weather pattern sub-sampling and meta-Gaussian model, J. Hydrol., 581, 124451, <ext-link xlink:href="https://doi.org/10.1016/j.jhydrol.2019.124451" ext-link-type="DOI">10.1016/j.jhydrol.2019.124451</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Bauer and Scherrer(2024)</label><mixed-citation>Bauer, V. M. and Scherrer, S. C.: The observed evolution of sub‐daily to multi‐day heavy precipitation in Switzerland, Atmos. Sci. Lett., 25, e1240, <ext-link xlink:href="https://doi.org/10.1002/asl.1240" ext-link-type="DOI">10.1002/asl.1240</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx6"><label>Beneyto et al.(2024)Beneyto, Ángel Aranda, Salazar-Galán, Garcia-Bartual, Albentosa, and Francés</label><mixed-citation>Beneyto, C., Ángel Aranda, J., Salazar-Galán, S., Garcia-Bartual, R., Albentosa, E., and Francés, F.: Expanding information for flood frequency analysis using a weather generator: Application in a Spanish Mediterranean catchment, J. Hydrol., 53, 101826, <ext-link xlink:href="https://doi.org/10.1016/j.ejrh.2024.101826" ext-link-type="DOI">10.1016/j.ejrh.2024.101826</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>Blanchet and Creutin(2022)</label><mixed-citation>Blanchet, J. and Creutin, J.-D.: Instrumental agreement and retrospective analysis of trends in precipitation extremes in the French Mediterranean Region, Environ. Res. Lett., 17, 074011, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ac7734" ext-link-type="DOI">10.1088/1748-9326/ac7734</ext-link>,  2022.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Blanchet et al.(2018)Blanchet, Molinié, and Touati</label><mixed-citation>Blanchet, J., Molinié, G., and Touati, J.: Spatial analysis of trend in extreme daily rainfall in southern France, Clim. Dynam., 51, 799–812, <ext-link xlink:href="https://doi.org/10.1007/s00382-016-3122-7" ext-link-type="DOI">10.1007/s00382-016-3122-7</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Blanchet et al.(2019)Blanchet, Paquet, Vaittinada Ayar, and Penot</label><mixed-citation>Blanchet, J., Paquet, E., Vaittinada Ayar, P., and Penot, D.: Mapping rainfall hazard based on rain gauge data: an objective cross-validation framework for model selection, Hydrol. Earth Syst. Sci., 23, 829–849, <ext-link xlink:href="https://doi.org/10.5194/hess-23-829-2019" ext-link-type="DOI">10.5194/hess-23-829-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Blanchet et al.(2021a)Blanchet, Blanc, and Creutin</label><mixed-citation>Blanchet, J., Blanc, A., and Creutin, J.-D.: Explaining recent trends in extreme precipitation in the Southwestern Alps by changes in atmospheric influences, Weather and Climate Extremes, 33, 100356, <ext-link xlink:href="https://doi.org/10.1016/j.wace.2021.100356" ext-link-type="DOI">10.1016/j.wace.2021.100356</ext-link>, 2021a.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>Blanchet et al.(2021b)Blanchet, Creutin, and Blanc</label><mixed-citation>Blanchet, J., Creutin, J.-D., and Blanc, A.: Retreating winter and strengthening autumn Mediterranean influence on extreme precipitation in the Southwestern Alps over the last 60 years, Environ. Res. Lett., 16, 034056, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/abb5cd" ext-link-type="DOI">10.1088/1748-9326/abb5cd</ext-link>,  2021b.</mixed-citation></ref>
      <ref id="bib1.bibx12"><label>Bois(1986)</label><mixed-citation> Bois, P.: Contrôle de séries chronologiques corrélées par étude du cumul des résidus de la corrélation, Colloques et séminaires, 2èmes journées hydrologiques de l’ORSTOM, à Montpellier, 2, Montpellier (FRA), 16–17 September 1986, ISBN 2-7099-0865-4,1986.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>Cavanaugh et al.(2015)Cavanaugh, Gershunov, Panorska, and Kozubowski</label><mixed-citation>Cavanaugh, N. R., Gershunov, A., Panorska, A. K., and Kozubowski, T. J.: The probability distribution of intense daily precipitation, Geophys. Res. Lett., 42, 1560–1567, <ext-link xlink:href="https://doi.org/10.1002/2015GL063238" ext-link-type="DOI">10.1002/2015GL063238</ext-link>,  2015.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>Chakrabarti and Ghosh(2011)</label><mixed-citation>Chakrabarti, A. and Ghosh, J. K.: AIC, BIC and recent advances in model selection, Philosophy of Statistics, 583–605, <ext-link xlink:href="https://doi.org/10.1016/b978-0-444-51862-0.50018-6" ext-link-type="DOI">10.1016/b978-0-444-51862-0.50018-6</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx15"><label>Cisneros et al.(2024)Cisneros, Richards, Dahal, Lombardo, and Huser</label><mixed-citation>Cisneros, D., Richards, J., Dahal, A., Lombardo, L., and Huser, R.: Deep graphical regression for jointly moderate and extreme Australian wildfires, Spat. Stat.-Neth., 59, 100811, <ext-link xlink:href="https://doi.org/10.1016/j.spasta.2024.100811" ext-link-type="DOI">10.1016/j.spasta.2024.100811</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Coles et al.(2001)Coles, Bawa, Trenner, and Dorazio</label><mixed-citation>Coles, S., Bawa, J., Trenner, L., and Dorazio, P.: An introduction to statistical modeling of extreme values, Vol. 208, Springer, <ext-link xlink:href="https://doi.org/10.1007/978-1-4471-3675-0_2" ext-link-type="DOI">10.1007/978-1-4471-3675-0_2</ext-link>, 2001.</mixed-citation></ref>
      <ref id="bib1.bibx17"><label>Cunnane(1978)</label><mixed-citation>Cunnane, C.: Unbiased plotting positions – a review, J. Hydrol., 37, 205–222, <ext-link xlink:href="https://doi.org/10.1016/0022-1694(78)90017-3" ext-link-type="DOI">10.1016/0022-1694(78)90017-3</ext-link>, 1978.</mixed-citation></ref>
      <ref id="bib1.bibx18"><label>Evin et al.(2018)Evin, Favre, and Hingray</label><mixed-citation>Evin, G., Favre, A.-C., and Hingray, B.: Stochastic generation of multi-site daily precipitation focusing on extreme events, Hydrol. Earth Syst. Sci., 22, 655–672, <ext-link xlink:href="https://doi.org/10.5194/hess-22-655-2018" ext-link-type="DOI">10.5194/hess-22-655-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx19"><label>Evin et al.(2025)Evin, Le Roux, Kamir, and Morin</label><mixed-citation>Evin, G., Le Roux, E., Kamir, E., and Morin, S.: Estimating changes in extreme snow load in Europe as a function of global warming levels, Cold Reg. Sci. Technol., 231, 104424, <ext-link xlink:href="https://doi.org/10.1016/j.coldregions.2025.104424" ext-link-type="DOI">10.1016/j.coldregions.2025.104424</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx20"><label>Funatsu et al.(2009)Funatsu, Claud, and Chaboureau</label><mixed-citation>Funatsu, B. M., Claud, C., and Chaboureau, J.-P.: Comparison between the large-scale environments of moderate and intense precipitating systems in the Mediterranean region, Mon. Weather Rev., 137, 3933–3959, <ext-link xlink:href="https://doi.org/10.1175/2009mwr2922.1" ext-link-type="DOI">10.1175/2009mwr2922.1</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx21"><label>Groisman et al.(1999)Groisman, Karl, Easterling, Knight, Jamason, Hennessy, Suppiah, Page, Wibig, Fortuniak et al.</label><mixed-citation>Groisman, P. Y., Karl, T. R., Easterling, D. R., Knight, R. W., Jamason, P. F., Hennessy, K. J., Suppiah, R., Page, C. M., Wibig, J., Fortuniak, K., Razuvaev, V. N., Douglas, A., Førland, E., and  Zhai, P.-M.: Changes in the probability of heavy precipitation: important indicators of climatic change, Weather and Climate Extremes, 243–283, <ext-link xlink:href="https://doi.org/10.1023/a:1005432803188" ext-link-type="DOI">10.1023/a:1005432803188</ext-link>, 1999.</mixed-citation></ref>
      <ref id="bib1.bibx22"><label>Haruna(2024)</label><mixed-citation>Haruna, A.: Enhancing Precipitation Hazard Estimation through Intensity-Duration-Area-Frequency (IDAF) Relationships, Application to a Topographically Complex Area, PhD thesis, Université Grenoble Alpes, <uri>https://hal.science/tel-04632742</uri> (last access: 15 February 2026), 2024.</mixed-citation></ref>
      <ref id="bib1.bibx23"><label>Haruna et al.(2022)Haruna, Blanchet, and Favre</label><mixed-citation>Haruna, A., Blanchet, J., and Favre, A.-C.: Performance-based comparison of regionalization methods to improve the at-site estimates of daily precipitation, Hydrol. Earth Syst. Sci., 26, 2797–2811, <ext-link xlink:href="https://doi.org/10.5194/hess-26-2797-2022" ext-link-type="DOI">10.5194/hess-26-2797-2022</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx24"><label>Haruna et al.(2023)Haruna, Blanchet, and Favre</label><mixed-citation>Haruna, A., Blanchet, J., and Favre, A.-C.: Modeling Intensity-Duration-Frequency Curves for the Whole Range of Non-Zero Precipitation: A Comparison of Models, Water Resour. Res., 59, e2022WR033362, <ext-link xlink:href="https://doi.org/10.1029/2022WR033362" ext-link-type="DOI">10.1029/2022WR033362</ext-link>, 2023.</mixed-citation></ref>
      <ref id="bib1.bibx25"><label>Haruna et al.(2024)Haruna, Blanchet, and Favre</label><mixed-citation>Haruna, A., Blanchet, J., and Favre, A.-C.: Estimation of Intensity-Duration-Area-Frequency Relationships Based on the Full Range of Non-Zero Precipitation From Radar-Reanalysis Data, Water Resour. Res., 60, e2023WR035902, <ext-link xlink:href="https://doi.org/10.1029/2023WR035902" ext-link-type="DOI">10.1029/2023WR035902</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx26"><label>Haruna et al.(2025)Haruna, Blanchet, and Favre</label><mixed-citation>Haruna, A., Blanchet, J., and Favre, A.-C.: Joint estimation of trend in bulk and extreme daily precipitation in Switzerland, Weather and Climate Extremes, 48, 100769, <ext-link xlink:href="https://doi.org/10.1016/j.wace.2025.100769" ext-link-type="DOI">10.1016/j.wace.2025.100769</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx27"><label>Huang et al.(2017)Huang, Thorne, Banzon, Boyer, Chepurin, Lawrimore, Menne, Smith, Vose, and Zhang</label><mixed-citation>Huang, B., Thorne, P. W., Banzon, V. F., Boyer, T., Chepurin, G., Lawrimore, J. H., Menne, M. J., Smith, T. M., Vose, R. S., and Zhang, H.-M.: NOAA extended reconstructed sea surface temperature (ERSST), version 5, NOAA National Centers for Environmental Information [data set], <ext-link xlink:href="https://doi.org/10.7289/V5T72FNM" ext-link-type="DOI">10.7289/V5T72FNM</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx28"><label>IPCC(2023)</label><mixed-citation>IPCC: Climate Change 2023: Synthesis Report. Contribution of Working Groups I, II and III to the Sixth Assessment Report of the Intergovernmental Panel on Climate Change, 1st edn., edited by: Core Writing Team, Lee H., and Romero, J., IPCC, Geneva, Switzerland, Tech. rep., Intergovernmental Panel on Climate Change (IPCC), <ext-link xlink:href="https://doi.org/10.59327/IPCC/AR6-9789291691647" ext-link-type="DOI">10.59327/IPCC/AR6-9789291691647</ext-link>,  2023.</mixed-citation></ref>
      <ref id="bib1.bibx29"><label>Jayaweera et al.(2024)Jayaweera, Wasko, and Nathan</label><mixed-citation>Jayaweera, L., Wasko, C., and Nathan, R.: Modelling non-stationarity in extreme rainfall using large-scale climate drivers, J. Hydrol., 636, 131309, <ext-link xlink:href="https://doi.org/10.1016/j.jhydrol.2024.131309" ext-link-type="DOI">10.1016/j.jhydrol.2024.131309</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx30"><label>Kedem et al.(1990)Kedem, Chiu, and North</label><mixed-citation>Kedem, B., Chiu, L. S., and North, G. R.: Estimation of mean rain rate: Application to satellite observations, J. Geophys. Res.-Atmos., 95, 1965–1972, <ext-link xlink:href="https://doi.org/10.1029/jd095id02p01965" ext-link-type="DOI">10.1029/jd095id02p01965</ext-link>, 1990.</mixed-citation></ref>
      <ref id="bib1.bibx31"><label>Kendall(1975)</label><mixed-citation>Kendall, M. G.: Rank correlation methods, Griffin, <ext-link xlink:href="https://doi.org/10.2307/2333282" ext-link-type="DOI">10.2307/2333282</ext-link>, 1975.</mixed-citation></ref>
      <ref id="bib1.bibx32"><label>Kim et al.(2017)Kim, Kim, Shin, and Heo</label><mixed-citation>Kim, H., Kim, S., Shin, H., and Heo, J.-H.: Appropriate model selection methods for nonstationary generalized extreme value models, J. Hydrol., 547, 557–574, <ext-link xlink:href="https://doi.org/10.1016/j.jhydrol.2017.02.005" ext-link-type="DOI">10.1016/j.jhydrol.2017.02.005</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx33"><label>Koenker and Mizera(2004)</label><mixed-citation>Koenker, R. and Mizera, I.: Penalized triograms: Total variation regularization for bivariate smoothing, J. R. Stat. Soc. B, 66, 145–163, <ext-link xlink:href="https://doi.org/10.1111/j.1467-9868.2004.00437.x" ext-link-type="DOI">10.1111/j.1467-9868.2004.00437.x</ext-link>, 2004.</mixed-citation></ref>
      <ref id="bib1.bibx34"><label>Le Gall et al.(2022)Le Gall, Favre, Naveau, and Prieur</label><mixed-citation>Le Gall, P., Favre, A.-C., Naveau, P., and Prieur, C.: Improved regional frequency analysis of rainfall data, Weather and Climate Extremes, 36, 100456, <ext-link xlink:href="https://doi.org/10.1016/j.wace.2022.100456" ext-link-type="DOI">10.1016/j.wace.2022.100456</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx35"><label>Legrand et al.(2023)Legrand, Ailliot, Naveau, and Raillard</label><mixed-citation>Legrand, J., Ailliot, P., Naveau, P., and Raillard, N.: Joint stochastic simulation of extreme coastal and offshore significant wave heights, Ann. Appl. Stat., 17, 3363–3383, <ext-link xlink:href="https://doi.org/10.1214/23-aoas1766" ext-link-type="DOI">10.1214/23-aoas1766</ext-link>, 2023.</mixed-citation></ref>
      <ref id="bib1.bibx36"><label>Mann(1945)</label><mixed-citation>Mann, H. B.: Nonparametric tests against trend, Econometrica,  245–259, <ext-link xlink:href="https://doi.org/10.2307/1907187" ext-link-type="DOI">10.2307/1907187</ext-link>, 1945.</mixed-citation></ref>
      <ref id="bib1.bibx37"><label>Milojevic et al.(2023)Milojevic, Blanchet, and Lehning</label><mixed-citation>Milojevic, T., Blanchet, J., and Lehning, M.: Determining return levels of extreme daily precipitation, reservoir inflow, and dry spells, Frontiers in Water, 5, 1141786, <ext-link xlink:href="https://doi.org/10.3389/frwa.2023.1141786" ext-link-type="DOI">10.3389/frwa.2023.1141786</ext-link>, 2023.</mixed-citation></ref>
      <ref id="bib1.bibx38"><label>Ménégoz et al.(2020)Ménégoz, Valla, Jourdain, Blanchet, Beaumet, Wilhelm, Gallée, Fettweis, Morin, and Anquetin</label><mixed-citation>Ménégoz, M., Valla, E., Jourdain, N. C., Blanchet, J., Beaumet, J., Wilhelm, B., Gallée, H., Fettweis, X., Morin, S., and Anquetin, S.: Contrasting seasonal changes in total and intense precipitation in the European Alps from 1903 to 2010, Hydrol. Earth Syst. Sci., 24, 5355–5377, <ext-link xlink:href="https://doi.org/10.5194/hess-24-5355-2020" ext-link-type="DOI">10.5194/hess-24-5355-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx39"><label>Nanditha et al.(2025)Nanditha, Villarini, and Naveau</label><mixed-citation>Nanditha, J., Villarini, G., and Naveau, P.: Assessing future changes in daily precipitation extremes across the contiguous United States with the extended Generalized Pareto distribution, J. Hydrol., 659, 133212, <ext-link xlink:href="https://doi.org/10.2139/ssrn.5085534" ext-link-type="DOI">10.2139/ssrn.5085534</ext-link>, 2025.</mixed-citation></ref>
      <ref id="bib1.bibx40"><label>Naveau et al.(2016)Naveau, Huser, Ribereau, and Hannart</label><mixed-citation>Naveau, P., Huser, R., Ribereau, P., and Hannart, A.: Modeling jointly low, moderate, and heavy rainfall intensities without a threshold selection, Water Resour. Res., 52, 2753–2769, <ext-link xlink:href="https://doi.org/10.1002/2015WR018552" ext-link-type="DOI">10.1002/2015WR018552</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx41"><label>Nguyen et al.(2024)Nguyen, Vorogushyn, Nissen, Brunner, and Merz</label><mixed-citation>Nguyen, V. D., Vorogushyn, S., Nissen, K., Brunner, L., and Merz, B.: A non-stationary climate-informed weather generator for assessing future flood risks, Advances in Statistical Climatology, Meteorology and Oceanography, 10, 195–216, <ext-link xlink:href="https://doi.org/10.5194/ascmo-10-195-2024" ext-link-type="DOI">10.5194/ascmo-10-195-2024</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx42"><label>Papalexiou(2018)</label><mixed-citation>Papalexiou, S. M.: Unified theory for stochastic modelling of hydroclimatic processes: Preserving marginal distributions, correlation structures, and intermittency, Adv. Water Resour., 115, 234–252, <ext-link xlink:href="https://doi.org/10.1016/j.advwatres.2018.02.013" ext-link-type="DOI">10.1016/j.advwatres.2018.02.013</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx43"><label>Papalexiou and Koutsoyiannis(2012)</label><mixed-citation>Papalexiou, S. M. and Koutsoyiannis, D.: Entropy based derivation of probability distributions: A case study to daily rainfall, Adv. Water Resour., 45, 51–57, <ext-link xlink:href="https://doi.org/10.1016/j.advwatres.2011.11.007" ext-link-type="DOI">10.1016/j.advwatres.2011.11.007</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx44"><label>Papalexiou and Koutsoyiannis(2013)</label><mixed-citation>Papalexiou, S. M. and Koutsoyiannis, D.: Battle of extreme value distributions: A global survey on extreme daily rainfall, Water Resour. Res., 49, 187–201, <ext-link xlink:href="https://doi.org/10.1029/2012WR012557" ext-link-type="DOI">10.1029/2012WR012557</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx45"><label>Papalexiou and Koutsoyiannis(2016)</label><mixed-citation>Papalexiou, S. M. and Koutsoyiannis, D.: A global survey on the seasonal variation of the marginal distribution of daily precipitation, Adv. Water Resour., 94, 131–145, <ext-link xlink:href="https://doi.org/10.1016/j.advwatres.2016.05.005" ext-link-type="DOI">10.1016/j.advwatres.2016.05.005</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx46"><label>Papastathopoulos and Tawn(2013)</label><mixed-citation>Papastathopoulos, I. and Tawn, J. A.: Extended generalised Pareto models for tail estimation, J. Stat. Plan. Infer., 143, 131–143, <ext-link xlink:href="https://doi.org/10.1016/j.jspi.2012.07.001" ext-link-type="DOI">10.1016/j.jspi.2012.07.001</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx47"><label>Paquet(2024)</label><mixed-citation>Paquet, E.: A Detailed Stationarity Analysis and Trend Modelling of French Daily Precipitations, in: Proceedings of the International Meeting on Statistical Climatology (IMSC 2024), Meteo France, Toulouse, <ext-link xlink:href="https://doi.org/10.13140/RG.2.2.22302.34884" ext-link-type="DOI">10.13140/RG.2.2.22302.34884</ext-link>, 2024.</mixed-citation></ref>
      <ref id="bib1.bibx48"><label>Rivoire et al.(2021)Rivoire, Martius, and Naveau</label><mixed-citation>Rivoire, P., Martius, O., and Naveau, P.: A Comparison of Moderate and Extreme ERA-5 Daily Precipitation With Two Observational Data Sets, Earth and Space Science, 8, e2020EA001633, <ext-link xlink:href="https://doi.org/10.1029/2020EA001633" ext-link-type="DOI">10.1029/2020EA001633</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bibx49"><label>Rivoire et al.(2022)Rivoire, Le Gall, Favre, Naveau, and Martius</label><mixed-citation>Rivoire, P., Le Gall, P., Favre, A.-C., Naveau, P., and Martius, O.: High return level estimates of daily ERA-5 precipitation in Europe estimated using regionalized extreme value distributions, Weather and Climate Extremes, 38, 100500, <ext-link xlink:href="https://doi.org/10.1016/j.wace.2022.100500" ext-link-type="DOI">10.1016/j.wace.2022.100500</ext-link>, 2022.</mixed-citation></ref>
      <ref id="bib1.bibx50"><label>Schoof et al.(2010)Schoof, Pryor, and Surprenant</label><mixed-citation>Schoof, J. T., Pryor, S., and Surprenant, J.: Development of daily precipitation projections for the United States based on probabilistic downscaling, J. Geophys. Res.-Atmos., 115, <ext-link xlink:href="https://doi.org/10.1029/2009jd013030" ext-link-type="DOI">10.1029/2009jd013030</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx51"><label>Sen(1968)</label><mixed-citation>Sen, P. K.: Estimates of the regression coefficient based on Kendall's tau, J. Am. Stat. Assoc., 63, 1379–1389, <ext-link xlink:href="https://doi.org/10.1080/01621459.1968.10480934" ext-link-type="DOI">10.1080/01621459.1968.10480934</ext-link>, 1968.</mixed-citation></ref>
      <ref id="bib1.bibx52"><label>Senatore et al.(2020)Senatore, Furnari, and Mendicino</label><mixed-citation>Senatore, A., Furnari, L., and Mendicino, G.: Impact of high-resolution sea surface temperature representation on the forecast of small Mediterranean catchments' hydrological responses to heavy precipitation, Hydrol. Earth Syst. Sci., 24, 269–291, <ext-link xlink:href="https://doi.org/10.5194/hess-24-269-2020" ext-link-type="DOI">10.5194/hess-24-269-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bibx53"><label>Stacy(1962)</label><mixed-citation>Stacy, E. W.: A generalization of the gamma distribution, Ann. Math. Stat.,  1187–1192, <ext-link xlink:href="https://doi.org/10.1214/aoms/1177704481" ext-link-type="DOI">10.1214/aoms/1177704481</ext-link>, 1962.</mixed-citation></ref>
      <ref id="bib1.bibx54"><label>Stasinopoulos and Rigby(2008)</label><mixed-citation>Stasinopoulos, D. M. and Rigby, R. A.: Generalized additive models for location scale and shape (GAMLSS) in R, J. Stat.  Softw., 23, 1–46, <ext-link xlink:href="https://doi.org/10.32614/cran.package.gamlss" ext-link-type="DOI">10.32614/cran.package.gamlss</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx55"><label>Theil(1950)</label><mixed-citation>Theil, H.: A rank-invariant method of linear and polynomial regression analysis, Indagat. Math.-New Ser., 12, 173, <ext-link xlink:href="https://doi.org/10.1007/978-94-011-2546-8_20" ext-link-type="DOI">10.1007/978-94-011-2546-8_20</ext-link>,  1950.</mixed-citation></ref>
      <ref id="bib1.bibx56"><label>Tramblay et al.(2011)Tramblay, Neppel, and Carreau</label><mixed-citation>Tramblay, Y., Neppel, L., and Carreau, J.: Brief communication “Climatic covariates for the frequency analysis of heavy rainfall in the Mediterranean region”, Nat. Hazards Earth Syst. Sci., 11, 2463–2468, <ext-link xlink:href="https://doi.org/10.5194/nhess-11-2463-2011" ext-link-type="DOI">10.5194/nhess-11-2463-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx57"><label>Tramblay et al.(2013)Tramblay, Neppel, Carreau, and Najib</label><mixed-citation>Tramblay, Y., Neppel, L., Carreau, J., and Najib, K.: Non-stationary frequency analysis of heavy rainfall events in southern France, Hydrolog. Sci. J., 58, 280–294, <ext-link xlink:href="https://doi.org/10.1080/02626667.2012.754988" ext-link-type="DOI">10.1080/02626667.2012.754988</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx58"><label>Vaittinada Ayar et al.(2016)Vaittinada Ayar, Vrac, Bastin, Carreau, Déqué, and Gallardo</label><mixed-citation>Vaittinada Ayar, P., Vrac, M., Bastin, S., Carreau, J., Déqué, M., and Gallardo, C.: Intercomparison of statistical and dynamical downscaling models under the EURO-and MED-CORDEX initiative framework: present climate evaluations, Clim. Dynam., 46, 1301–1329, <ext-link xlink:href="https://doi.org/10.1023/a:1005432803188" ext-link-type="DOI">10.1023/a:1005432803188</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx59"><label>Ye et al.(2018)Ye, Hanson, Ding, Wang, and Vogel</label><mixed-citation>Ye, L., Hanson, L. S., Ding, P., Wang, D., and Vogel, R. M.: The probability distribution of daily precipitation at the point and catchment scales in the United States, Hydrol. Earth Syst. Sci., 22, 6519–6531, <ext-link xlink:href="https://doi.org/10.5194/hess-22-6519-2018" ext-link-type="DOI">10.5194/hess-22-6519-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx60"><label>Yoo et al.(2005)Yoo, Jung, and Kim</label><mixed-citation>Yoo, C., Jung, K.-S., and Kim, T.-W.: Rainfall frequency analysis using a mixed Gamma distribution: evaluation of the global warming effect on daily rainfall, Hydrol. Process., 19, 3851–3861, <ext-link xlink:href="https://doi.org/10.1002/hyp.5985" ext-link-type="DOI">10.1002/hyp.5985</ext-link>, 2005.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Selecting the best distribution for modeling trends in low, medium, and extreme daily precipitation under climate change</article-title-html>
<abstract-html/>
<ref-html id="bib1.bib1"><label>Abbas et al.(2025)Abbas, Ahmad, and Ahmad</label><mixed-citation>
      
Abbas, A., Ahmad, T., and Ahmad, I.: Modeling zero-inflated precipitation
extremes, Commun. Stat., 1–17,
<a href="https://doi.org/10.1080/03610918.2025.2585398" target="_blank">https://doi.org/10.1080/03610918.2025.2585398</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Akaike(1974)</label><mixed-citation>
      
Akaike, H.: A new look at the statistical model identification, IEEE
T.  Automat. Contr., 19, 716–723,
<a href="https://doi.org/10.1109/TAC.1974.1100705" target="_blank">https://doi.org/10.1109/TAC.1974.1100705</a>, 1974.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Alexandersson(1986)</label><mixed-citation>
      
Alexandersson, H.: A homogeneity test applied to precipitation data, J. Climatol., 6, 661–675, <a href="https://doi.org/10.1002/joc.3370060607" target="_blank">https://doi.org/10.1002/joc.3370060607</a>, 1986.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Ayar et al.(2020)Ayar, Blanchet, Paquet, and Penot</label><mixed-citation>
      
Ayar, P. V., Blanchet, J., Paquet, E., and Penot, D.: Space-time simulation of
precipitation based on weather pattern sub-sampling and meta-Gaussian model,
J. Hydrol., 581, 124451,
<a href="https://doi.org/10.1016/j.jhydrol.2019.124451" target="_blank">https://doi.org/10.1016/j.jhydrol.2019.124451</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Bauer and Scherrer(2024)</label><mixed-citation>
      
Bauer, V. M. and Scherrer, S. C.: The observed evolution of sub‐daily to
multi‐day heavy precipitation in Switzerland, Atmos. Sci.
Lett., 25, e1240, <a href="https://doi.org/10.1002/asl.1240" target="_blank">https://doi.org/10.1002/asl.1240</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Beneyto et al.(2024)Beneyto, Ángel Aranda, Salazar-Galán,
Garcia-Bartual, Albentosa, and Francés</label><mixed-citation>
      
Beneyto, C., Ángel Aranda, J., Salazar-Galán, S., Garcia-Bartual, R.,
Albentosa, E., and Francés, F.: Expanding information for flood frequency
analysis using a weather generator: Application in a Spanish Mediterranean
catchment, J. Hydrol., 53, 101826,
<a href="https://doi.org/10.1016/j.ejrh.2024.101826" target="_blank">https://doi.org/10.1016/j.ejrh.2024.101826</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Blanchet and Creutin(2022)</label><mixed-citation>
      
Blanchet, J. and Creutin, J.-D.: Instrumental agreement and retrospective
analysis of trends in precipitation extremes in the French Mediterranean
Region, Environ. Res. Lett., 17, 074011,
<a href="https://doi.org/10.1088/1748-9326/ac7734" target="_blank">https://doi.org/10.1088/1748-9326/ac7734</a>,  2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Blanchet et al.(2018)Blanchet, Molinié, and
Touati</label><mixed-citation>
      
Blanchet, J., Molinié, G., and Touati, J.: Spatial analysis of trend in
extreme daily rainfall in southern France, Clim. Dynam., 51, 799–812,
<a href="https://doi.org/10.1007/s00382-016-3122-7" target="_blank">https://doi.org/10.1007/s00382-016-3122-7</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Blanchet et al.(2019)Blanchet, Paquet, Vaittinada Ayar, and
Penot</label><mixed-citation>
      
Blanchet, J., Paquet, E., Vaittinada Ayar, P., and Penot, D.: Mapping rainfall hazard based on rain gauge data: an objective cross-validation framework for model selection, Hydrol. Earth Syst. Sci., 23, 829–849, <a href="https://doi.org/10.5194/hess-23-829-2019" target="_blank">https://doi.org/10.5194/hess-23-829-2019</a>, 2019.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Blanchet et al.(2021a)Blanchet, Blanc, and
Creutin</label><mixed-citation>
      
Blanchet, J., Blanc, A., and Creutin, J.-D.: Explaining recent trends in
extreme precipitation in the Southwestern Alps by changes in atmospheric
influences, Weather and Climate Extremes, 33, 100356,
<a href="https://doi.org/10.1016/j.wace.2021.100356" target="_blank">https://doi.org/10.1016/j.wace.2021.100356</a>, 2021a.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Blanchet et al.(2021b)Blanchet, Creutin, and
Blanc</label><mixed-citation>
      
Blanchet, J., Creutin, J.-D., and Blanc, A.: Retreating winter and
strengthening autumn Mediterranean influence on extreme precipitation in
the Southwestern Alps over the last 60 years, Environ. Res. Lett., 16, 034056, <a href="https://doi.org/10.1088/1748-9326/abb5cd" target="_blank">https://doi.org/10.1088/1748-9326/abb5cd</a>,  2021b.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Bois(1986)</label><mixed-citation>
      
Bois, P.: Contrôle de séries chronologiques corrélées par
étude du cumul des résidus de la corrélation, Colloques et
séminaires, 2èmes journées hydrologiques de l’ORSTOM, à
Montpellier, 2, Montpellier (FRA), 16–17 September 1986, ISBN
2-7099-0865-4,1986.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Cavanaugh et al.(2015)Cavanaugh, Gershunov, Panorska, and
Kozubowski</label><mixed-citation>
      
Cavanaugh, N. R., Gershunov, A., Panorska, A. K., and Kozubowski, T. J.: The
probability distribution of intense daily precipitation, Geophys. Res.
Lett., 42, 1560–1567, <a href="https://doi.org/10.1002/2015GL063238" target="_blank">https://doi.org/10.1002/2015GL063238</a>,  2015.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Chakrabarti and Ghosh(2011)</label><mixed-citation>
      
Chakrabarti, A. and Ghosh, J. K.: AIC, BIC and recent advances in model
selection, Philosophy of Statistics, 583–605,
<a href="https://doi.org/10.1016/b978-0-444-51862-0.50018-6" target="_blank">https://doi.org/10.1016/b978-0-444-51862-0.50018-6</a>, 2011.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Cisneros et al.(2024)Cisneros, Richards, Dahal, Lombardo, and
Huser</label><mixed-citation>
      
Cisneros, D., Richards, J., Dahal, A., Lombardo, L., and Huser, R.: Deep
graphical regression for jointly moderate and extreme Australian wildfires,
Spat. Stat.-Neth., 59, 100811,
<a href="https://doi.org/10.1016/j.spasta.2024.100811" target="_blank">https://doi.org/10.1016/j.spasta.2024.100811</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Coles et al.(2001)Coles, Bawa, Trenner, and
Dorazio</label><mixed-citation>
      
Coles, S., Bawa, J., Trenner, L., and Dorazio, P.: An introduction to
statistical modeling of extreme values, Vol. 208, Springer,
<a href="https://doi.org/10.1007/978-1-4471-3675-0_2" target="_blank">https://doi.org/10.1007/978-1-4471-3675-0_2</a>, 2001.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Cunnane(1978)</label><mixed-citation>
      
Cunnane, C.: Unbiased plotting positions – a review, J. Hydrol., 37,
205–222, <a href="https://doi.org/10.1016/0022-1694(78)90017-3" target="_blank">https://doi.org/10.1016/0022-1694(78)90017-3</a>, 1978.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Evin et al.(2018)Evin, Favre, and Hingray</label><mixed-citation>
      
Evin, G., Favre, A.-C., and Hingray, B.: Stochastic generation of multi-site daily precipitation focusing on extreme events, Hydrol. Earth Syst. Sci., 22, 655–672, <a href="https://doi.org/10.5194/hess-22-655-2018" target="_blank">https://doi.org/10.5194/hess-22-655-2018</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Evin et al.(2025)Evin, Le Roux, Kamir, and
Morin</label><mixed-citation>
      
Evin, G., Le Roux, E., Kamir, E., and Morin, S.: Estimating changes in extreme
snow load in Europe as a function of global warming levels, Cold Reg.
Sci. Technol., 231, 104424,
<a href="https://doi.org/10.1016/j.coldregions.2025.104424" target="_blank">https://doi.org/10.1016/j.coldregions.2025.104424</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>Funatsu et al.(2009)Funatsu, Claud, and
Chaboureau</label><mixed-citation>
      
Funatsu, B. M., Claud, C., and Chaboureau, J.-P.: Comparison between the
large-scale environments of moderate and intense precipitating systems in the
Mediterranean region, Mon. Weather Rev., 137, 3933–3959,
<a href="https://doi.org/10.1175/2009mwr2922.1" target="_blank">https://doi.org/10.1175/2009mwr2922.1</a>, 2009.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Groisman et al.(1999)Groisman, Karl, Easterling, Knight, Jamason,
Hennessy, Suppiah, Page, Wibig, Fortuniak et al.</label><mixed-citation>
      
Groisman, P. Y., Karl, T. R., Easterling, D. R., Knight, R. W., Jamason, P. F.,
Hennessy, K. J., Suppiah, R., Page, C. M., Wibig, J., Fortuniak, K., Razuvaev, V. N., Douglas, A., Førland, E., and  Zhai, P.-M.:
Changes in the probability of heavy precipitation: important indicators of
climatic change, Weather and Climate Extremes, 243–283,
<a href="https://doi.org/10.1023/a:1005432803188" target="_blank">https://doi.org/10.1023/a:1005432803188</a>, 1999.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>Haruna(2024)</label><mixed-citation>
      
Haruna, A.: Enhancing Precipitation Hazard Estimation through
Intensity-Duration-Area-Frequency (IDAF) Relationships, Application to a
Topographically Complex Area, PhD thesis, Université Grenoble Alpes, <a href="https://hal.science/tel-04632742" target="_blank"/> (last access: 15 February 2026), 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>Haruna et al.(2022)Haruna, Blanchet, and
Favre</label><mixed-citation>
      
Haruna, A., Blanchet, J., and Favre, A.-C.: Performance-based comparison of regionalization methods to improve the at-site estimates of daily precipitation, Hydrol. Earth Syst. Sci., 26, 2797–2811, <a href="https://doi.org/10.5194/hess-26-2797-2022" target="_blank">https://doi.org/10.5194/hess-26-2797-2022</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Haruna et al.(2023)Haruna, Blanchet, and
Favre</label><mixed-citation>
      
Haruna, A., Blanchet, J., and Favre, A.-C.: Modeling
Intensity-Duration-Frequency Curves for the Whole Range of
Non-Zero Precipitation: A Comparison of Models, Water Resour.
Res., 59, e2022WR033362, <a href="https://doi.org/10.1029/2022WR033362" target="_blank">https://doi.org/10.1029/2022WR033362</a>, 2023.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Haruna et al.(2024)Haruna, Blanchet, and
Favre</label><mixed-citation>
      
Haruna, A., Blanchet, J., and Favre, A.-C.: Estimation of
Intensity-Duration-Area-Frequency Relationships Based on the
Full Range of Non-Zero Precipitation From Radar-Reanalysis
Data, Water Resour. Res., 60, e2023WR035902,
<a href="https://doi.org/10.1029/2023WR035902" target="_blank">https://doi.org/10.1029/2023WR035902</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>Haruna et al.(2025)Haruna, Blanchet, and Favre</label><mixed-citation>
      
Haruna, A., Blanchet, J., and Favre, A.-C.: Joint estimation of trend in bulk
and extreme daily precipitation in Switzerland, Weather and Climate Extremes, 48,
100769, <a href="https://doi.org/10.1016/j.wace.2025.100769" target="_blank">https://doi.org/10.1016/j.wace.2025.100769</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Huang et al.(2017)Huang, Thorne, Banzon, Boyer, Chepurin, Lawrimore,
Menne, Smith, Vose, and Zhang</label><mixed-citation>
      
Huang, B., Thorne, P. W., Banzon, V. F., Boyer, T., Chepurin, G., Lawrimore,
J. H., Menne, M. J., Smith, T. M., Vose, R. S., and Zhang, H.-M.: NOAA
extended reconstructed sea surface temperature (ERSST), version 5, NOAA National Centers for Environmental Information [data set], <a href="https://doi.org/10.7289/V5T72FNM" target="_blank">https://doi.org/10.7289/V5T72FNM</a>, 2017.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>IPCC(2023)</label><mixed-citation>
      
IPCC: Climate Change 2023: Synthesis Report. Contribution of
Working Groups I, II and III to the Sixth Assessment Report
of the Intergovernmental Panel on Climate Change, 1st edn., edited by: Core Writing
Team, Lee H., and Romero, J., IPCC, Geneva,
Switzerland, Tech. rep., Intergovernmental Panel on Climate Change (IPCC),
<a href="https://doi.org/10.59327/IPCC/AR6-9789291691647" target="_blank">https://doi.org/10.59327/IPCC/AR6-9789291691647</a>,  2023.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Jayaweera et al.(2024)Jayaweera, Wasko, and
Nathan</label><mixed-citation>
      
Jayaweera, L., Wasko, C., and Nathan, R.: Modelling non-stationarity in extreme
rainfall using large-scale climate drivers, J. Hydrol., 636,
131309, <a href="https://doi.org/10.1016/j.jhydrol.2024.131309" target="_blank">https://doi.org/10.1016/j.jhydrol.2024.131309</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Kedem et al.(1990)Kedem, Chiu, and North</label><mixed-citation>
      
Kedem, B., Chiu, L. S., and North, G. R.: Estimation of mean rain rate:
Application to satellite observations, J. Geophys. Res.-Atmos., 95, 1965–1972, <a href="https://doi.org/10.1029/jd095id02p01965" target="_blank">https://doi.org/10.1029/jd095id02p01965</a>,
1990.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Kendall(1975)</label><mixed-citation>
      
Kendall, M. G.: Rank correlation methods, Griffin,
<a href="https://doi.org/10.2307/2333282" target="_blank">https://doi.org/10.2307/2333282</a>, 1975.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>Kim et al.(2017)Kim, Kim, Shin, and Heo</label><mixed-citation>
      
Kim, H., Kim, S., Shin, H., and Heo, J.-H.: Appropriate model selection methods
for nonstationary generalized extreme value models, J. Hydrol.,
547, 557–574, <a href="https://doi.org/10.1016/j.jhydrol.2017.02.005" target="_blank">https://doi.org/10.1016/j.jhydrol.2017.02.005</a>, 2017.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Koenker and Mizera(2004)</label><mixed-citation>
      
Koenker, R. and Mizera, I.: Penalized triograms: Total variation regularization
for bivariate smoothing, J. R. Stat. Soc. B, 66, 145–163,
<a href="https://doi.org/10.1111/j.1467-9868.2004.00437.x" target="_blank">https://doi.org/10.1111/j.1467-9868.2004.00437.x</a>, 2004.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Le Gall et al.(2022)Le Gall, Favre, Naveau, and
Prieur</label><mixed-citation>
      
Le Gall, P., Favre, A.-C., Naveau, P., and Prieur, C.: Improved regional
frequency analysis of rainfall data, Weather and Climate Extremes, 36,
100456, <a href="https://doi.org/10.1016/j.wace.2022.100456" target="_blank">https://doi.org/10.1016/j.wace.2022.100456</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Legrand et al.(2023)Legrand, Ailliot, Naveau, and
Raillard</label><mixed-citation>
      
Legrand, J., Ailliot, P., Naveau, P., and Raillard, N.: Joint stochastic
simulation of extreme coastal and offshore significant wave heights,
Ann. Appl. Stat., 17, 3363–3383,
<a href="https://doi.org/10.1214/23-aoas1766" target="_blank">https://doi.org/10.1214/23-aoas1766</a>, 2023.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Mann(1945)</label><mixed-citation>
      
Mann, H. B.: Nonparametric tests against trend, Econometrica,  245–259, <a href="https://doi.org/10.2307/1907187" target="_blank">https://doi.org/10.2307/1907187</a>,
1945.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Milojevic et al.(2023)Milojevic, Blanchet, and
Lehning</label><mixed-citation>
      
Milojevic, T., Blanchet, J., and Lehning, M.: Determining return levels of
extreme daily precipitation, reservoir inflow, and dry spells, Frontiers in
Water, 5, 1141786, <a href="https://doi.org/10.3389/frwa.2023.1141786" target="_blank">https://doi.org/10.3389/frwa.2023.1141786</a>, 2023.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>Ménégoz et al.(2020)Ménégoz, Valla, Jourdain, Blanchet, Beaumet,
Wilhelm, Gallée, Fettweis, Morin, and Anquetin</label><mixed-citation>
      
Ménégoz, M., Valla, E., Jourdain, N. C., Blanchet, J., Beaumet, J., Wilhelm, B., Gallée, H., Fettweis, X., Morin, S., and Anquetin, S.: Contrasting seasonal changes in total and intense precipitation in the European Alps from 1903 to 2010, Hydrol. Earth Syst. Sci., 24, 5355–5377, <a href="https://doi.org/10.5194/hess-24-5355-2020" target="_blank">https://doi.org/10.5194/hess-24-5355-2020</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Nanditha et al.(2025)Nanditha, Villarini, and
Naveau</label><mixed-citation>
      
Nanditha, J., Villarini, G., and Naveau, P.: Assessing future changes in daily
precipitation extremes across the contiguous United States with the extended
Generalized Pareto distribution, J. Hydrol., 659, 133212,
<a href="https://doi.org/10.2139/ssrn.5085534" target="_blank">https://doi.org/10.2139/ssrn.5085534</a>, 2025.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Naveau et al.(2016)Naveau, Huser, Ribereau, and
Hannart</label><mixed-citation>
      
Naveau, P., Huser, R., Ribereau, P., and Hannart, A.: Modeling jointly low,
moderate, and heavy rainfall intensities without a threshold selection, Water Resour. Res., 52, 2753–2769, <a href="https://doi.org/10.1002/2015WR018552" target="_blank">https://doi.org/10.1002/2015WR018552</a>, 2016.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Nguyen et al.(2024)Nguyen, Vorogushyn, Nissen, Brunner, and
Merz</label><mixed-citation>
      
Nguyen, V. D., Vorogushyn, S., Nissen, K., Brunner, L., and Merz, B.: A
non-stationary climate-informed weather generator for assessing future flood
risks, Advances in Statistical Climatology, Meteorology and Oceanography, 10,
195–216, <a href="https://doi.org/10.5194/ascmo-10-195-2024" target="_blank">https://doi.org/10.5194/ascmo-10-195-2024</a>, 2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>Papalexiou(2018)</label><mixed-citation>
      
Papalexiou, S. M.: Unified theory for stochastic modelling of hydroclimatic
processes: Preserving marginal distributions, correlation structures, and
intermittency, Adv. Water Resour., 115, 234–252,
<a href="https://doi.org/10.1016/j.advwatres.2018.02.013" target="_blank">https://doi.org/10.1016/j.advwatres.2018.02.013</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Papalexiou and Koutsoyiannis(2012)</label><mixed-citation>
      
Papalexiou, S. M. and Koutsoyiannis, D.: Entropy based derivation of
probability distributions: A case study to daily rainfall, Adv. Water Resour., 45, 51–57, <a href="https://doi.org/10.1016/j.advwatres.2011.11.007" target="_blank">https://doi.org/10.1016/j.advwatres.2011.11.007</a>, 2012.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Papalexiou and Koutsoyiannis(2013)</label><mixed-citation>
      
Papalexiou, S. M. and Koutsoyiannis, D.: Battle of extreme value distributions:
A global survey on extreme daily rainfall, Water Resour. Res., 49,
187–201, <a href="https://doi.org/10.1029/2012WR012557" target="_blank">https://doi.org/10.1029/2012WR012557</a>, 2013.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Papalexiou and Koutsoyiannis(2016)</label><mixed-citation>
      
Papalexiou, S. M. and Koutsoyiannis, D.: A global survey on the seasonal
variation of the marginal distribution of daily precipitation, Adv.
Water Resour., 94, 131–145,
<a href="https://doi.org/10.1016/j.advwatres.2016.05.005" target="_blank">https://doi.org/10.1016/j.advwatres.2016.05.005</a>, 2016.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>Papastathopoulos and Tawn(2013)</label><mixed-citation>
      
Papastathopoulos, I. and Tawn, J. A.: Extended generalised Pareto models for
tail estimation, J. Stat. Plan. Infer., 143,
131–143, <a href="https://doi.org/10.1016/j.jspi.2012.07.001" target="_blank">https://doi.org/10.1016/j.jspi.2012.07.001</a>, 2013.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Paquet(2024)</label><mixed-citation>
      
Paquet, E.: A Detailed Stationarity Analysis and Trend Modelling of French
Daily Precipitations, in: Proceedings of the International Meeting on
Statistical Climatology (IMSC 2024), Meteo France, Toulouse, <a href="https://doi.org/10.13140/RG.2.2.22302.34884" target="_blank">https://doi.org/10.13140/RG.2.2.22302.34884</a>,
2024.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Rivoire et al.(2021)Rivoire, Martius, and
Naveau</label><mixed-citation>
      
Rivoire, P., Martius, O., and Naveau, P.: A Comparison of Moderate and
Extreme ERA-5 Daily Precipitation With Two Observational Data
Sets, Earth and Space Science, 8, e2020EA001633,
<a href="https://doi.org/10.1029/2020EA001633" target="_blank">https://doi.org/10.1029/2020EA001633</a>, 2021.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>Rivoire et al.(2022)Rivoire, Le Gall, Favre, Naveau, and
Martius</label><mixed-citation>
      
Rivoire, P., Le Gall, P., Favre, A.-C., Naveau, P., and Martius, O.: High
return level estimates of daily ERA-5 precipitation in Europe estimated using
regionalized extreme value distributions, Weather and Climate Extremes, 38,
100500, <a href="https://doi.org/10.1016/j.wace.2022.100500" target="_blank">https://doi.org/10.1016/j.wace.2022.100500</a>, 2022.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>Schoof et al.(2010)Schoof, Pryor, and
Surprenant</label><mixed-citation>
      
Schoof, J. T., Pryor, S., and Surprenant, J.: Development of daily
precipitation projections for the United States based on probabilistic
downscaling, J. Geophys. Res.-Atmos., 115,
<a href="https://doi.org/10.1029/2009jd013030" target="_blank">https://doi.org/10.1029/2009jd013030</a>, 2010.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>Sen(1968)</label><mixed-citation>
      
Sen, P. K.: Estimates of the regression coefficient based on Kendall's tau,
J. Am. Stat. Assoc., 63, 1379–1389,
<a href="https://doi.org/10.1080/01621459.1968.10480934" target="_blank">https://doi.org/10.1080/01621459.1968.10480934</a>, 1968.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>Senatore et al.(2020)Senatore, Furnari, and
Mendicino</label><mixed-citation>
      
Senatore, A., Furnari, L., and Mendicino, G.: Impact of high-resolution sea surface temperature representation on the forecast of small Mediterranean catchments' hydrological responses to heavy precipitation, Hydrol. Earth Syst. Sci., 24, 269–291, <a href="https://doi.org/10.5194/hess-24-269-2020" target="_blank">https://doi.org/10.5194/hess-24-269-2020</a>, 2020.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>Stacy(1962)</label><mixed-citation>
      
Stacy, E. W.: A generalization of the gamma distribution, Ann. Math. Stat.,  1187–1192,
<a href="https://doi.org/10.1214/aoms/1177704481" target="_blank">https://doi.org/10.1214/aoms/1177704481</a>, 1962.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>Stasinopoulos and Rigby(2008)</label><mixed-citation>
      
Stasinopoulos, D. M. and Rigby, R. A.: Generalized additive models for location
scale and shape (GAMLSS) in R, J. Stat.  Softw., 23, 1–46,
<a href="https://doi.org/10.32614/cran.package.gamlss" target="_blank">https://doi.org/10.32614/cran.package.gamlss</a>, 2008.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>Theil(1950)</label><mixed-citation>
      
Theil, H.: A rank-invariant method of linear and polynomial regression
analysis, Indagat. Math.-New Ser., 12, 173,
<a href="https://doi.org/10.1007/978-94-011-2546-8_20" target="_blank">https://doi.org/10.1007/978-94-011-2546-8_20</a>,  1950.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>Tramblay et al.(2011)Tramblay, Neppel, and
Carreau</label><mixed-citation>
      
Tramblay, Y., Neppel, L., and Carreau, J.: Brief communication “Climatic covariates for the frequency analysis of heavy rainfall in the Mediterranean region”, Nat. Hazards Earth Syst. Sci., 11, 2463–2468, <a href="https://doi.org/10.5194/nhess-11-2463-2011" target="_blank">https://doi.org/10.5194/nhess-11-2463-2011</a>, 2011.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>Tramblay et al.(2013)Tramblay, Neppel, Carreau, and
Najib</label><mixed-citation>
      
Tramblay, Y., Neppel, L., Carreau, J., and Najib, K.: Non-stationary frequency
analysis of heavy rainfall events in southern France, Hydrolog. Sci.
J., 58, 280–294, <a href="https://doi.org/10.1080/02626667.2012.754988" target="_blank">https://doi.org/10.1080/02626667.2012.754988</a>, 2013.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>Vaittinada Ayar et al.(2016)Vaittinada Ayar, Vrac, Bastin, Carreau,
Déqué, and Gallardo</label><mixed-citation>
      
Vaittinada Ayar, P., Vrac, M., Bastin, S., Carreau, J., Déqué, M., and
Gallardo, C.: Intercomparison of statistical and dynamical downscaling models
under the EURO-and MED-CORDEX initiative framework: present climate
evaluations, Clim. Dynam., 46, 1301–1329,
<a href="https://doi.org/10.1023/a:1005432803188" target="_blank">https://doi.org/10.1023/a:1005432803188</a>, 2016.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>Ye et al.(2018)Ye, Hanson, Ding, Wang, and
Vogel</label><mixed-citation>
      
Ye, L., Hanson, L. S., Ding, P., Wang, D., and Vogel, R. M.: The probability distribution of daily precipitation at the point and catchment scales in the United States, Hydrol. Earth Syst. Sci., 22, 6519–6531, <a href="https://doi.org/10.5194/hess-22-6519-2018" target="_blank">https://doi.org/10.5194/hess-22-6519-2018</a>, 2018.

    </mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>Yoo et al.(2005)Yoo, Jung, and Kim</label><mixed-citation>
      
Yoo, C., Jung, K.-S., and Kim, T.-W.: Rainfall frequency analysis using a mixed
Gamma distribution: evaluation of the global warming effect on daily
rainfall, Hydrol. Process., 19, 3851–3861,
<a href="https://doi.org/10.1002/hyp.5985" target="_blank">https://doi.org/10.1002/hyp.5985</a>, 2005.

    </mixed-citation></ref-html>--></article>
