<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article"><?xmltex \bartext{Model evaluation paper}?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">GMD</journal-id><journal-title-group>
    <journal-title>Geoscientific Model Development</journal-title>
    <abbrev-journal-title abbrev-type="publisher">GMD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Geosci. Model Dev.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1991-9603</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/gmd-15-4941-2022</article-id><title-group><article-title>Assessment of stochastic weather forecast of precipitation near European cities, based on analogs of circulation</article-title><alt-title>Stochastic forecast of precipitation with analogs</alt-title>
      </title-group><?xmltex \runningtitle{Stochastic forecast of precipitation with analogs}?><?xmltex \runningauthor{M. Krouma et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Krouma</surname><given-names>Meriem</given-names></name>
          <email>meriem.krouma@lsce.ipsl.fr</email>
        <ext-link>https://orcid.org/0000-0003-0617-9956</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Yiou</surname><given-names>Pascal</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8534-5355</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Déandreis</surname><given-names>Céline</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Thao</surname><given-names>Soulivanh</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>ARIA Technologies, 8 Rue de la Ferme, 92100 Boulogne-Billancourt, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Laboratoire des Sciences du Climat et de l’Environnement, UMR 8212 CEA-CNRS-UVSQ,<?xmltex \hack{\break}?> IPSL &amp; Université Paris-Saclay, 91191 Gif-sur-Yvette, France</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Meriem Krouma (meriem.krouma@lsce.ipsl.fr)</corresp></author-notes><pub-date><day>28</day><month>June</month><year>2022</year></pub-date>
      
      <volume>15</volume>
      <issue>12</issue>
      <fpage>4941</fpage><lpage>4958</lpage>
      <history>
        <date date-type="received"><day>9</day><month>February</month><year>2021</year></date>
           <date date-type="rev-request"><day>24</day><month>March</month><year>2021</year></date>
           <date date-type="rev-recd"><day>13</day><month>May</month><year>2022</year></date>
           <date date-type="accepted"><day>20</day><month>May</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Meriem Krouma et al.</copyright-statement>
        <copyright-year>2022</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://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022.html">This article is available from https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022.html</self-uri><self-uri xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e117">In this study, we assess the skill of a stochastic weather generator (SWG) to forecast precipitation in several cities in western Europe. The SWG is based on a random sampling of analogs of the geopotential height at 500 hPa (<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula>). The SWG is evaluated for two reanalyses (NCEP and ERA5).
We simulate 100-member ensemble forecasts on a daily time increment. We evaluate the performance of SWG with forecast skill scores and we compare it to ECMWF forecasts.</p>

      <p id="d1e130">Results show significant positive skill score (continuous rank probability skill score and correlation) compared with persistence and climatology forecasts for lead times of 5 and 10 d  for different areas in Europe. We find that the low predictability episodes of our model are related to specific weather regimes, depending on the European region. Comparing the SWG forecasts to ECMWF forecasts, we find that the SWG shows a good performance for 5 d. This performance varies from one region to another. This paper is a proof of concept for a stochastic regional ensemble precipitation forecast. Its parameters (e.g., region for analogs) must be tuned for each region in order to optimize its performance.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e142">Ensemble weather forecasts were designed to overcome the issues of meteorological chaos, from which small uncertainties in initial conditions can lead to a wide range of possible trajectories <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx26" id="paren.1"/>. Hence, from a sufficiently large ensemble of initial conditions, it is in principle possible to sample the probability distribution of future states of the system.</p>
      <p id="d1e148">Forecasts issued by meteorological centers are obtained by computing several simulations with perturbed initial conditions, in order to sample uncertainties. Those experiments are rather costly in terms of computing resources and are generally limited to a few tens of members <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx36" id="paren.2"/>, which can hinder a proper estimate of probability distributions of trajectories. Moreover, obtaining information at local spatial scales can be difficult because the horizontal resolution of the atmospheric models is around 18 km, e.g., for the European Centre for Medium-Range Weather Forecasts (ECMWF) ensemble forecast system.</p>
      <p id="d1e154">From a mathematical point of view, computing the probability distribution of the trajectories of a (deterministic) system makes the underlying assumption that the system behaves like a stochastic process, for which statistical properties are defined naturally <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx6" id="paren.3"/>. This has justified the development of stochastic weather generators (SWG), which are stochastic processes that emulate the behavior of key climate variables <xref ref-type="bibr" rid="bib1.bibx1" id="paren.4"/>. The advantages of stochastic models are a relative simplicity of implementation and a low computing cost. The challenge of their development is to verify that the behavior of the simulations is realistic, according to well-defined criteria <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx17" id="paren.5"/>.</p>
      <p id="d1e166">The first stochastic weather generators were devised to simulate rainfall occurrence <xref ref-type="bibr" rid="bib1.bibx10" id="paren.6"/>
and to simulate rainfall amounts <xref ref-type="bibr" rid="bib1.bibx34" id="paren.7"/>.
SWGs were developed and used to estimate the probability distributions of climate variables such as temperature, solar radiation, and precipitation through extensive simulations <xref ref-type="bibr" rid="bib1.bibx30" id="paren.8"/>.</p>
      <p id="d1e179">Stochastic weather generators can be useful complements to atmospheric circulation models, in order to simulate large ensembles of local variables,
as they can be calibrated for small spatial scales compared with numerical models <xref ref-type="bibr" rid="bib1.bibx1" id="paren.9"/>. This explains their wide applications in impact studies.</p>
      <p id="d1e185">A successful simulation with a SWG relies on the choice of inputs. The atmospheric circulation can be chosen a predictor for other local variables. The (loose) rationale for this choice is that the circulation is modeled by prognostic equations <xref ref-type="bibr" rid="bib1.bibx28" id="paren.10"/>, which drive the other physical variables. Therefore, the primitive equations of the atmosphere (<xref ref-type="bibr" rid="bib1.bibx28" id="altparen.11"/>, Chap. 3) suggest that reproducing temporal variability on daily time scales requires considering circulation variables. The influence of large-scale circulation on local climate variables has been proven in previous studies such as the influence of atmospheric circulation on the Mediterranean Basin <xref ref-type="bibr" rid="bib1.bibx24" id="paren.12"/> and Greece's precipitation <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx37" id="paren.13"/>. Similar influences have been found on precipitation and temperature over the North Atlantic region <xref ref-type="bibr" rid="bib1.bibx18" id="paren.14"/>.</p>
      <p id="d1e203">Analogs of circulation were initially designed to provide “model-free” forecasts by assuming that similar situations in atmospheric circulation may lead to similar local weather conditions <xref ref-type="bibr" rid="bib1.bibx23" id="paren.15"/>. The potential to simulate large ensembles of forecast temperature with circulation analogs was explored by <xref ref-type="bibr" rid="bib1.bibx44" id="text.16"/> by considering random resamplings of <inline-formula><mml:math id="M2" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> best analogs (rather than only considering the best analog). This has led to the development of an SWG in “predictive” mode, which uses updates of reanalysis datasets as input.</p>
      <p id="d1e219">Alternative systems of analogs to forecast precipitation have been proposed by <xref ref-type="bibr" rid="bib1.bibx3" id="text.17"/>. Those systems are based on analogs of precipitation itself. Such systems are very efficient for nowcasting, i.e., forecasting precipitation within the next few hours. Considering the atmospheric circulation analogs allows focusing on longer time scales.</p>
      <p id="d1e225"><xref ref-type="bibr" rid="bib1.bibx44" id="text.18"/> evaluated ensemble forecasts of the analog SWG for temperature and the NAO index with classical probability scores against climatology and persistence. Reasonable scores were obtained up to 20 d. Through this study, we aim to assess the skill of this SWG to forecast precipitation in different areas of Europe and for different lead times.
The previous study on this forecasting tool was a proof of concept for temperature. In this study, we will adapt the parameters of the analog SWG to optimize the simulation of European precipitations. We then analyze the performance of this SWG for lead times of 5–20 d, with the forecast skill scores used by <xref ref-type="bibr" rid="bib1.bibx44" id="text.19"/>.</p>
      <p id="d1e233">We will evaluate the seasonal dependence of the forecast skills of precipitation and the conditional dependence on weather regimes. Finally, comparisons with medium-range precipitation forecasts from the ECMWF will be performed.</p>
      <p id="d1e237">The paper is divided as follows: Section <xref ref-type="sec" rid="Ch1.S2"/> is dedicated to describing the data used for the experiments. Section <xref ref-type="sec" rid="Ch1.S3"/> explains the methodology (analogs, stochastic weather generator, and forecast skill scores). Section <xref ref-type="sec" rid="Ch1.S4"/> details the experimental setup and justifies the choice of parameters that we made for the forecast parameters. Section <xref ref-type="sec" rid="Ch1.S5"/> details the results of simulations and the evaluation of the ensemble forecast. Section <xref ref-type="sec" rid="Ch1.S6"/> contains the main conclusions of the analyses.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
      <p id="d1e258">Daily precipitation data were obtained from the European Climate Assessment and Data (ECAD) project <xref ref-type="bibr" rid="bib1.bibx21" id="paren.20"/> for four locations in western Europe (Berlin, Madrid, Orly, and Toulouse), which are subject to contrasted meteorological influences (Fig. <xref ref-type="fig" rid="Ch1.F1"/>). The ECAD provides station data that are available at a daily time step from 1948 to 2019. The choice of those stations was based on the availability of a large and common period of observations with a low rate of missing data (less than 10 %). For verification purposes, we used also the E-Obs data <xref ref-type="bibr" rid="bib1.bibx13" id="paren.21"/>, which are a daily gridded data available from 1979 to the present
with a horizontal resolution of 0.25<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M4" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.25<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. E-Obs data are spatial interpolations of ECAD data.</p>
      <p id="d1e295">We recovered the geopotential height at 500 hPa (<inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula>) and sea level pressure (SLP) fields from the reanalysis of the National Centers for Environmental Prediction (NCEP: <xref ref-type="bibr" rid="bib1.bibx20" id="altparen.22"/>) with a spatial resolution of 2.5<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M8" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> from 1 January 1948 to 31 December 2019.</p>
      <p id="d1e336">We also used the atmospheric reanalysis (version 5) of the European Centre for Medium-Range Weather Forecasts (ECMWF) (ERA5; <xref ref-type="bibr" rid="bib1.bibx16" id="altparen.23"/>). ERA5 data are available from 1950 to the present with a horizontal resolution of 0.25<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M11" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.25<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The two reanalyses have fundamental differences in terms of atmospheric models, assimilated data, and assimilation scheme.</p>
      <p id="d1e367">We considered the daily averages of <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> from NCEP and ERA5, over the region covering 30<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 40–60<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, to compute circulation analogs. Daily averages of SLP were used over the region covering 80<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 30–70<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N to define weather regimes.</p>
      <p id="d1e436">In order to assess the predictive skill of our precipitation forecast model, a comparison with another forecast was made. Many available datasets can be used for deriving this information. We considered the ECMWF ensemble forecast dataset system 5 <xref ref-type="bibr" rid="bib1.bibx40" id="paren.24"/>. It is a daily gridded dataset interpolated over Europe that provides information covering all the domains. Data are available through the Copernicus Climate Data Store. They include forecasts created in real time (since 2017) and hindcast forecasts from 1993 to 2019 <xref ref-type="bibr" rid="bib1.bibx40" id="paren.25"/>. The data are provided at an hourly time step with a horizontal resolution of 0.25<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M21" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.25<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. We considered the grid points that include Berlin, Madrid, Orly, and Toulouse, which were identified in the ECAD database.</p>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methodology</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Analogs</title>
      <p id="d1e485">The first step is to build a database of analogs of the atmospheric circulation. We outline the procedure of <xref ref-type="bibr" rid="bib1.bibx44" id="text.26"/>, summarized in Fig. <xref ref-type="fig" rid="Ch1.F1"/>a.
For a given day <inline-formula><mml:math id="M23" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, we determine the similarity of <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> for all days <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> that are within 30 calendar days of <inline-formula><mml:math id="M26" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> but in a different year from <inline-formula><mml:math id="M27" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>. The similarity is quantified by a Euclidean distance (or root mean square error) between the daily <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> maps. Other types of similarity measures are possible <xref ref-type="bibr" rid="bib1.bibx4" id="paren.27"/>, but the expected impact on the results is often marginal <xref ref-type="bibr" rid="bib1.bibx35" id="paren.28"/>. We believe that the simplicity of the Euclidean distance makes it more robust to changes in horizontal resolution (e.g., from NCEP to ERA5), compared with more sophisticated distances that include local spatial gradients, which would require adjustments and additional tuning. This choice can be left open for future fine-tuning, depending on the region.</p>
      <p id="d1e552">For each day <inline-formula><mml:math id="M29" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, we consider the <inline-formula><mml:math id="M30" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> best analogs, i.e., for which the distances are the smallest. We compute the spatial rank correlation between the <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> best analogs and the <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> at time <inline-formula><mml:math id="M33" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> for posterior verification purposes.</p>
      <p id="d1e596">As a refinement over the study of <xref ref-type="bibr" rid="bib1.bibx44" id="text.29"/>, a time embedding of <inline-formula><mml:math id="M34" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> days was used for the search of the analogs dates. This means that the field <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for which we compute analogs is <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. This ensures that temporal derivatives of the atmospheric field are preserved <xref ref-type="bibr" rid="bib1.bibx46" id="paren.30"/>. Hence, the distance that is optimized to find analogs of the <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> field is
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M38" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{8.9}{8.9}\selectfont$\displaystyle}?><mml:mi>D</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi>t</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>x</mml:mi></mml:munder><mml:mfenced close=")" open="("><mml:mrow><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow><mml:mi mathvariant="italic">τ</mml:mi></mml:munderover><mml:msup><mml:mfenced open="|" close="|"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi>t</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:msup><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M39" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> is a spatial index and <inline-formula><mml:math id="M40" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> is the embedding time.</p>
      <p id="d1e831">We consider different geographic domains as shown in Fig. <xref ref-type="fig" rid="Ch1.F1"/> for the computation of analogs and weather regimes. The computation of circulation analogs was performed with the “blackswan” Web Processing Service (WPS; <xref ref-type="bibr" rid="bib1.bibx14" id="altparen.31"/>). The “blackswan” WPS is an online tool that helps compute circulation analogs on various datasets (e.g., reanalyses and climate model simulations) with a user-friendly interface.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e842">Parameters of the analog computation. <bold>(a)</bold> For each day <inline-formula><mml:math id="M41" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> in year <inline-formula><mml:math id="M42" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>, we chose an analog day <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msup><mml:mi>t</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> with a similar sequence of <inline-formula><mml:math id="M44" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> consecutive day <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> patterns. <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is selected within 30 calendar days of <inline-formula><mml:math id="M47" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> and in a year <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msup><mml:mi>y</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>≠</mml:mo><mml:mi>y</mml:mi></mml:mrow></mml:math></inline-formula>. <bold>(b)</bold> Domains of computation of analogs. We computed analogs over different domains, each one including a part of the Atlantic and focusing on a part of western Europe, in order to test the sensitivity of our model to different geographic areas. The optimizing area was [30<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N], indicated by the red rectangle.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f01.png"/>

        </fig>

<?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Configuration of stochastic weather generator</title>
      <p id="d1e971">We use a stochastic weather generator (SWG) based on a random sampling of the circulation analogs. The operation of the SWG and its design are detailed by <xref ref-type="bibr" rid="bib1.bibx44" id="text.32"/>. The aim is to generate random trajectories from the previously computed analogs. Therefore, to generate a trajectory, we proceed as follows: for a given day <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in year <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, we generate a set of <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> simulations until a time <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>, with a lead time <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>∈</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">20</mml:mn><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> d.
We start at day <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and randomly select an analog (out of <inline-formula><mml:math id="M58" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> analogs) of day <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>. The random selection of analogs of the day <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> is performed with weights that are proportional to the calendar difference between <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and analog dates, to ensure that time goes forward. We also exclude analog dates with years that are equal to <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. This rule is important for the next iterations. We then replace <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> by the selected analog of <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> and repeat the operation <inline-formula><mml:math id="M65" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> times. Excluding analogs in year <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from the selection ensures that we do not use information from the <inline-formula><mml:math id="M67" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> days that follow <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Hence, we obtain a hindcast trajectory between <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e1211">The procedure presented above is repeated <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> times to simulate <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> trajectories from <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. The daily precipitation of each trajectory is time averaged between <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>. Hence, we obtain an ensemble of <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> forecasts of the average precipitation for day <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and lead time <inline-formula><mml:math id="M79" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>.</p>
      <p id="d1e1324">Then <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is shifted by <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> d, and the ensemble simulation procedure is repeated. This provides a set of ensemble forecasts with analogs.</p>
      <p id="d1e1352">We made a hindcast exercise, where the forecasts of precipitations based on analogs of atmospheric circulation (<inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula>), are started every <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>≈</mml:mo></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> d between 1 January 1948 and 31 December 2019. This yields a stochastic ensemble hindcast of precipitation and atmospheric circulation (<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula>). In this paper, therefore, we analyze the properties of an ensemble forecast of mean precipitation between <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>. To evaluate our forecasts, the predictions made with the SWG are compared with the persistence and climatological forecasts. The persistence forecast consists of using the average value between <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for a given year. The climatological forecast takes the climatological mean between <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>. The two “reference” forecasts are randomized by adding a small Gaussian noise, whose standard deviation is estimated by bootstrapping over <inline-formula><mml:math id="M92" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> long intervals. We thus generate sets of persistence forecasts and climatological forecasts that are consistent with the observations <xref ref-type="bibr" rid="bib1.bibx44" id="paren.33"/>.</p>
      <p id="d1e1490">The simulations of this stochastic model will be called “SWG forecasts”, as opposed to ECMWF forecasts.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Forecast verification</title>
      <p id="d1e1501">Forecast verification is the process of determining the statistical quality of forecasts. A wide variety of ensemble forecast verification procedures exists <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx42" id="paren.34"/>​​​​​​​. They involve measures of the relationship between a set of forecasts and corresponding observations. To assess the quality of precipitation forecasts, we compute indicators such as the correlation and continuous rank probability skill score (CRPSS) for each lead time <inline-formula><mml:math id="M93" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>, for different seasons and months.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1516">Weather regimes over Europe from SLP fields. Upper panels <bold>(a)</bold>–<bold>(d)</bold> contain winter (December–January–February: DJF) regimes: negative phase of the North Atlantic oscillation (NAO<inline-formula><mml:math id="M94" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>), Atlantic Ridge (AR), Scandinavian blocking (BLO), and Zonal regime (ZO). Lower panels <bold>(e)</bold>–<bold>(h)</bold> contain summer (June–July–August: JJA) weather regimes: negative phase of the North Atlantic oscillation (NAO<inline-formula><mml:math id="M95" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>), Zonal (ZO), Scandinavian blocking (BLO) and Atlantic low (AL).
The isolines show seasonal anomalies with respect to a DJF and JJA, in hPa with 2 hPa increments.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f02.png"/>

        </fig>

      <p id="d1e1552">The temporal rank correlation (referred to as correlation skill) is calculated between the precipitation observations and the median of 100 simulations. This simple diagnostic is often used to assess forecast skills of indices <xref ref-type="bibr" rid="bib1.bibx32" id="paren.35"/>.</p>
      <p id="d1e1559">The continuous ranked probability score (CRPS) is widely used for probabilistic forecast verification <xref ref-type="bibr" rid="bib1.bibx9" id="paren.36"/>. It is sensitive to the distance between forecast and observation probability distributions.</p>
      <p id="d1e1565">If the ensemble forecast <inline-formula><mml:math id="M96" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> yields a probability distribution <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for a value <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the CRPS measures how the probability distribution of <inline-formula><mml:math id="M99" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> compares with <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx15" id="paren.37"/>.</p>
      <p id="d1e1622">The CRPS is computed as
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M101" display="block"><mml:mrow><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mo>(</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">∞</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo><mml:mi mathvariant="normal">∞</mml:mi></mml:mrow></mml:munderover><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>P</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="script">H</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the observation and <inline-formula><mml:math id="M103" display="inline"><mml:mi mathvariant="script">H</mml:mi></mml:math></inline-formula> is the Heaviside function of the occurrence of <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mi mathvariant="script">H</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> if <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mi>y</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi mathvariant="script">H</mml:mi><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> otherwise).
The decomposition and properties of the CRPS have been investigated by <xref ref-type="bibr" rid="bib1.bibx9" id="text.38"/>, <xref ref-type="bibr" rid="bib1.bibx15" id="text.39"/>, and <xref ref-type="bibr" rid="bib1.bibx47" id="text.40"/>. A perfect forecast would have a CRPS equal to 0, but the CRPS value obviously depends on the units of the variable to forecast, so quantifying what is a “good” forecast requires a normalization. It is hence difficult to compare CRPS values for temperature and precipitation, within the same ensemble forecast. This issue is also acute for non-Gaussian variables with heavy tails <xref ref-type="bibr" rid="bib1.bibx47" id="paren.41"/> so that the interpretation of a given CRPS value might not be informative.</p>
      <p id="d1e1788">One way of circumventing this difficulty is to compare CRPS values to reference forecasts, such as persistence or climatology. The continuous rank probability skill score (CRPSS) is a normalization of Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) with respect to such a reference.</p>
      <p id="d1e1793">The CRPSS is hence computed by
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M108" display="block"><mml:mrow><mml:mi mathvariant="normal">CRPSS</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mover accent="true"><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M109" display="inline"><mml:mover accent="true"><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> is the time average of the <inline-formula><mml:math id="M110" display="inline"><mml:mi mathvariant="normal">CRPS</mml:mi></mml:math></inline-formula> of the SWG forecast and <inline-formula><mml:math id="M111" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ref</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> is the time average of the <inline-formula><mml:math id="M112" display="inline"><mml:mi mathvariant="normal">CRPS</mml:mi></mml:math></inline-formula> of the reference (either climatology or persistence). The CRPSS is interpreted as a fraction of improvement over a reference forecast.</p>
      <p id="d1e1866">The values of the CRPSS vary between <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">∞</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M114" display="inline"><mml:mn mathvariant="normal">1</mml:mn></mml:math></inline-formula>. The forecast is considered to be an improvement over the reference when the CRPSS value is positive. Values of CRPSS equal to 0 indicate no improvement over the reference. Values inferior to 0 mean that the forecast is worse than the reference.</p>
      <p id="d1e1887">We use the CRPSS values to determine the maximum lead time <inline-formula><mml:math id="M115" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> for which the SWG forecast is better than references. Then the SWG assessments will use the CRPS and directly compare the probability distributions of precipitation ensemble forecasts.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Dependence of forecast on weather regimes</title>
      <p id="d1e1905">We investigated the role of North Atlantic weather patterns on the forecast quality by attributing CRPS values of the SWG precipitation simulations to weather regimes.
Weather regimes are defined as large-scale quasi-stationary atmospheric states. They are characterized by their recurrence, persistence, and stationarity <xref ref-type="bibr" rid="bib1.bibx25" id="paren.42"/>. They help in describing the features of the atmospheric circulation. Surface variables like temperature and precipitation are largely correlated with weather regimes <xref ref-type="bibr" rid="bib1.bibx39" id="paren.43"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1916">Time series of analog ensemble forecasts for 2002, for lead times of 5 d <bold>(a, b)</bold> and 10 d <bold>(c, d)</bold>​​​​​​​ for summer (June to
August) <bold>(a)</bold> and <bold>(c)</bold> and winter (December to February) <bold>(b)</bold> and <bold>(d)</bold> for Orly. The median of 100 simulations is represented by the red line. The black line represents observation values. Dashed lines represent the 5th and 95th quantiles. The blue line represents the persistence forecasts and the orange line represents the climatology forecasts. The <inline-formula><mml:math id="M116" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>-axis represents the average precipitation over <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>, 10 d.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f03.png"/>

        </fig>

      <p id="d1e1963">The North Atlantic weather regimes were computed with the procedure of <xref ref-type="bibr" rid="bib1.bibx45" id="text.44"/>, with the NCEP reanalysis. The first 10 principal components of SLP (large region in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b) were classified with a <inline-formula><mml:math id="M118" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means algorithm onto four classes over a reference period between 1970 and 2010. The procedure was repeated 100 times with random <inline-formula><mml:math id="M119" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means initialization. Then we classified the resulting <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M121" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-means weather regimes in order to determine the most probable classification. This heuristic procedure increases the robustness of the obtained weather regimes.
Figure <xref ref-type="fig" rid="Ch1.F2"/> shows four weather regimes for each season (winter and summer) that are coherent with the literature <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx11 bib1.bibx19 bib1.bibx25" id="paren.45"/>.</p>
      <p id="d1e2011">The winter weather regimes are the negative phase of the North Atlantic oscillation (NAO<inline-formula><mml:math id="M122" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>), Atlantic Ridge (AR), Scandinavian blocking (BLO), and Zonal (ZO). The summer weather regimes are the negative phase of the NAO (NAO<inline-formula><mml:math id="M123" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>), Zonal (ZO), Scandinavian blocking (BLO), and Atlantic low (AL). The regimes are not the same in both seasons due to the seasonality of the large-scale atmospheric circulation.</p>
      <p id="d1e2028">For each day (in winter and summer) between 1948 and 2019, we classified the SLP by minimizing the root mean square to four reference (1970–2010) weather regimes.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e2033">Skill scores for the precipitation of Orly, Madrid, Berlin, and Toulouse for lead times of 5, 10, 20 d for January (blue) and July (red) for analogs computed from reanalyses of NCEP. Squares indicate CRPSS where the persistence is the baseline, triangles indicate CRPSS where the climatology is the reference, and boxplots indicate the probability distribution of correlation between observation and the median of 100 simulations for all days.
The boxplot upper whisker is: <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mo>min⁡</mml:mo><mml:mfenced close="}" open="{"><mml:mrow><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:mo>max⁡</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">CRPSS</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>.
The boxplot lower whisker is: <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mo>max⁡</mml:mo><mml:mfenced close="}" open="{"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mo>min⁡</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">CRPSS</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f04.png"/>

        </fig>

      <p id="d1e2134">For each day <inline-formula><mml:math id="M126" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> (within a given season), we considered the analog dates of all <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> simulations between <inline-formula><mml:math id="M128" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula> and the corresponding classification into weather regimes. Then we determined the most frequent weather regime
of the <inline-formula><mml:math id="M130" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> member ensemble forecast between <inline-formula><mml:math id="M131" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>. We hence obtained time series on the most likely weather pattern that dominates in the ensemble forecast between <inline-formula><mml:math id="M133" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e2221">We evaluated the influence of the dominating weather regimes on the SWG forecast quality by plotting the probability distribution of CRPS values <italic>conditioned</italic> on the weather regimes. This is done separately for “good” forecasts (low CRPS values) and “poor” forecasts (high CRPS values).</p>
      <p id="d1e2228">We identified two classes of predictability from CRPS values:
<list list-type="bullet"><list-item>
      <p id="d1e2233">Low predictability is related to high values of CRPS that exceed the 75th quantile.</p></list-item><list-item>
      <p id="d1e2237">High predictability is linked to low values of CRPS, below the 25th quantile.</p></list-item></list>
Then we associated the dominating weather regimes computed above with classes of high or low predictability.
This procedure helps in identifying atmospheric patterns that could lead to low or high predictability with the SWG model.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Stochastic weather generator parameter optimization</title>
      <p id="d1e2250">We started by verifying the relationship between <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> over the Euro-Atlantic region and the precipitation in the four studied areas to ensure that <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> analogs would be reasonable predictors of precipitation. We show the maps of the temporal rank correlation between the daily average of <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> and the precipitation in Appendix <xref ref-type="fig" rid="App1.Ch1.S2.F9"/>. We found a significant negative correlation between <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> and the precipitation with <inline-formula><mml:math id="M139" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e2313">Then we empirically adjusted the parameters of the SWG simulations to optimize the forecast scores. The first parameter is the geographic area. We computed sample trajectories of the SWG for the four domains outlined in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b. We used different domains in order to find an optimal region that allows verifying the relationship between precipitation and <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> for the four studied areas. Each domain included a part of the Atlantic and a part of western Europe. We chose the widest domain with the coordinates 80<inline-formula><mml:math id="M142" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 30–70<inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in order to catch the variability in the whole Euro-Atlantic region; however, this large domain gave the poorest skill scores for precipitation forecasting for the studied areas as shown in Table <xref ref-type="table" rid="Ch1.T1"/>. Then we focused on two smaller domains (outlined in blue in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b): one centered over northern Europe and the other centered over southern Europe. We found better forecast skills for specific locations. The same level of performance was found for the domain (outlined in red in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b) with coordinates 30<inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 40–60<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.
Therefore, we kept this domain for the subsequent analyses, because it allows optimizing the correlations between <inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> and precipitation for the four studied areas and the time of computation of analogs at the same time.
We compared the skill scores over the geographic domain with the coordinates [80<inline-formula><mml:math id="M149" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M150" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 30–70<inline-formula><mml:math id="M151" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] and [30<inline-formula><mml:math id="M152" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M153" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M154" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N]. We determined that the SWG simulations showed a better skill for the geographic domain (outlined in red in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b) and the skill scores remained the highest ones as represented in Table <xref ref-type="table" rid="Ch1.T1"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e2462">Correlation between observations and the median of 100 simulations for the winter (DJF) for the different studied domains represented in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b, with the coordinates [80<inline-formula><mml:math id="M155" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 30–70<inline-formula><mml:math id="M157" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] for the largest one (blue) and [30<inline-formula><mml:math id="M158" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M159" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40<inline-formula><mml:math id="M160" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>–60<inline-formula><mml:math id="M161" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] for the red rectangle for a lead time of 5 d.</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="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="1">Location</oasis:entry>

         <oasis:entry rowsep="1" namest="col2" nameend="col3">[80<inline-formula><mml:math id="M162" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 30–70<inline-formula><mml:math id="M164" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] domain </oasis:entry>

         <oasis:entry rowsep="1" namest="col4" nameend="col5">[30<inline-formula><mml:math id="M165" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M166" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M167" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] domain </oasis:entry>

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

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

         <oasis:entry colname="col3">95 % confidence interval</oasis:entry>

         <oasis:entry colname="col4">Correlation</oasis:entry>

         <oasis:entry colname="col5">95 % confidence interval</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

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

         <oasis:entry colname="col2">0.32</oasis:entry>

         <oasis:entry colname="col3">0.30–0.35</oasis:entry>

         <oasis:entry colname="col4">0.50</oasis:entry>

         <oasis:entry colname="col5">0.48–0.56</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.35</oasis:entry>

         <oasis:entry colname="col3">0.33–0.39</oasis:entry>

         <oasis:entry colname="col4">0.53</oasis:entry>

         <oasis:entry colname="col5">0.51–0.55</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.39</oasis:entry>

         <oasis:entry colname="col3">0.37–0.41</oasis:entry>

         <oasis:entry colname="col4">0.58</oasis:entry>

         <oasis:entry colname="col5">0.56–0.59</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.34</oasis:entry>

         <oasis:entry colname="col3">0.31–0.36</oasis:entry>

         <oasis:entry colname="col4">0.40</oasis:entry>

         <oasis:entry colname="col5">0.39–0.44</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2707">The second parameter is the number <inline-formula><mml:math id="M168" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> of the best analogs that we use to simulate the precipitation. Our choice was based on numerical experiments. We performed different SWG simulations where we varied the number of analogs (<inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>, 10, 20). We noticed an improvement in the skill scores by increasing the number of analogs as shown in Table <xref ref-type="table" rid="Ch1.T2"/>. Therefore, we
considered <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> analogs to ensure that we had enough analog dates for the simulations. It appears that the Euclidean distance of analogs grows rather slowly after <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula>.
Our choice was also supported by a theoretical study by <xref ref-type="bibr" rid="bib1.bibx29" id="paren.46"/> who showed that, for complex systems, the use of a large
number of analogs (<inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> analogs) does not change the prediction properties with analogs. Thus, we kept <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> best analogs for the rest of the analyses.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e2786">CRPSS versus persistence and climatology for SWG simulations with 5, 10, and 20 analogs for the [30<inline-formula><mml:math id="M174" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M175" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] domain and for a lead time of 5 d.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="1">Location</oasis:entry>

         <oasis:entry rowsep="1" namest="col2" nameend="col3"><inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> analogs  </oasis:entry>

         <oasis:entry rowsep="1" namest="col4" nameend="col5"><inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> analogs </oasis:entry>

         <oasis:entry rowsep="1" namest="col6" nameend="col7"><inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> analogs </oasis:entry>

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

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

         <oasis:entry colname="col3">Climatology</oasis:entry>

         <oasis:entry colname="col4">Persistence</oasis:entry>

         <oasis:entry colname="col5">Climatology</oasis:entry>

         <oasis:entry colname="col6">Persistence</oasis:entry>

         <oasis:entry colname="col7">Climatology</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

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

         <oasis:entry colname="col2">0.29</oasis:entry>

         <oasis:entry colname="col3">0.20</oasis:entry>

         <oasis:entry colname="col4">0.39</oasis:entry>

         <oasis:entry colname="col5">0.31</oasis:entry>

         <oasis:entry colname="col6">0.56</oasis:entry>

         <oasis:entry colname="col7">0.50</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.32</oasis:entry>

         <oasis:entry colname="col3">0.31</oasis:entry>

         <oasis:entry colname="col4">0. 40</oasis:entry>

         <oasis:entry colname="col5">0.39</oasis:entry>

         <oasis:entry colname="col6">0.57</oasis:entry>

         <oasis:entry colname="col7">0.57</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.34</oasis:entry>

         <oasis:entry colname="col3">0.12</oasis:entry>

         <oasis:entry colname="col4">0. 40</oasis:entry>

         <oasis:entry colname="col5">0.23</oasis:entry>

         <oasis:entry colname="col6">0.60</oasis:entry>

         <oasis:entry colname="col7">0.53</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.34</oasis:entry>

         <oasis:entry colname="col3">0.24</oasis:entry>

         <oasis:entry colname="col4">0.38</oasis:entry>

         <oasis:entry colname="col5">0.45</oasis:entry>

         <oasis:entry colname="col6">0.41</oasis:entry>

         <oasis:entry colname="col7">0.48</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e3012">We quantified the dependence of the forecast on the time embedding for the analogs <inline-formula><mml:math id="M180" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> by calculating the analogs based on different embedding values from <inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>– 4 d. We found that an embedding of 4 d helped to better catch the persistence and improve the skill scores for the forecast compared with 1 d, as shown in Table <xref ref-type="table" rid="Ch1.T3"/>. Therefore, we kept the forecast based on a 4 d embedding.
This choice was based on the numerical experiments performed for the studied locations. This is also supported by the study of <xref ref-type="bibr" rid="bib1.bibx46" id="text.47"/>, where the analog computation with time embedding was argued to improve the temporal smoothness of simulations. With such an embedding, forecasts for lead times of <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d yield at least two time increments.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e3054">Correlation between observations and the median of 100 simulations for the winter (DJF) based on analogs computed with an embedding of 1 and 4 d for the geographic domain with the coordinates [30<inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M184" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M185" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] for a lead time of 5 d.</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="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:thead>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="1">Location</oasis:entry>

         <oasis:entry rowsep="1" namest="col2" nameend="col3" colsep="1"><inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> d time embedding </oasis:entry>

         <oasis:entry rowsep="1" namest="col4" nameend="col5"><inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> d time embedding </oasis:entry>

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

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

         <oasis:entry colname="col3">95 % confidence interval</oasis:entry>

         <oasis:entry colname="col4">Correlation</oasis:entry>

         <oasis:entry colname="col5">95 % confidence interval</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

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

         <oasis:entry colname="col2">0.39</oasis:entry>

         <oasis:entry colname="col3">0.37–0.43</oasis:entry>

         <oasis:entry colname="col4">0.50</oasis:entry>

         <oasis:entry colname="col5">0.48–0.56</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.40</oasis:entry>

         <oasis:entry colname="col3">0.38–0.42</oasis:entry>

         <oasis:entry colname="col4">0.53</oasis:entry>

         <oasis:entry colname="col5">0.51–0.55</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.42</oasis:entry>

         <oasis:entry colname="col3">0.39–0.45</oasis:entry>

         <oasis:entry colname="col4">0.58</oasis:entry>

         <oasis:entry colname="col5">0.56–0.59</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">0.35</oasis:entry>

         <oasis:entry colname="col3">0.34–0.37</oasis:entry>

         <oasis:entry colname="col4">0.40</oasis:entry>

         <oasis:entry colname="col5">0.39–0.44</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e3227">For comparison purposes, SWG simulations are obtained using analogs computed from reanalyses on the NCEP and ERA5 reanalyses.
By comparing their skill scores, we found that CRPSS and correlations between observations and simulations are positive in both cases, and show positive improvement compared with persistence and climatology forecasts. The CRPSS and correlation for simulations with analogs of NCEP are almost identical to those with ERA5, as shown in Table <xref ref-type="table" rid="Ch1.T4"/>. Therefore, we focused on SWG simulations with analogs from the NCEP reanalysis in the sequel as both NCEP and ERA5 (1950–2019) have the same skill, as shown in Table <xref ref-type="table" rid="Ch1.T4"/>, and because NCEP is easier to handle due to its lower horizontal resolution.
The computations were made using observations of precipitation from the ECAD <xref ref-type="bibr" rid="bib1.bibx21" id="paren.48"/> and E-Obs <xref ref-type="bibr" rid="bib1.bibx13" id="paren.49"/> databases. We found the same results because the ECAD and E-Obs are highly correlated (by the construction of E-Obs).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><?xmltex \currentcnt{4}?><label>Table 4</label><caption><p id="d1e3244">Comparison between the values of the CRPSS of SWG computed using different reanalysis datasets for NCEP and ERA5 from 1979 to 2019 for a lead time of <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d for winter (DJF).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Location</oasis:entry>
         <oasis:entry colname="col2">CRPSS DJF (ERA5)</oasis:entry>
         <oasis:entry colname="col3">CRPSS DJF (NCEP)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Berlin</oasis:entry>
         <oasis:entry colname="col2">0.50</oasis:entry>
         <oasis:entry colname="col3">0.50</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Madrid</oasis:entry>
         <oasis:entry colname="col2">0.55</oasis:entry>
         <oasis:entry colname="col3">0.57</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Orly</oasis:entry>
         <oasis:entry colname="col2">0.53</oasis:entry>
         <oasis:entry colname="col3">0.53</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Toulouse</oasis:entry>
         <oasis:entry colname="col2">0.41</oasis:entry>
         <oasis:entry colname="col3">0.41</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e3336">In summary, we made the forecast of the precipitation using <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> analogs computed from <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> over the [30<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M193" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] domain (red rectangle in Fig. <xref ref-type="fig" rid="Ch1.F1"/>b). To compute analogs, we used NCEP reanalyses and an embedding of <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> d. The computations were based on ECAD observations <xref ref-type="bibr" rid="bib1.bibx21" id="paren.50"/>.</p>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Results</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Sample forecast</title>
      <p id="d1e3422">As an example, we illustrate the behavior of the trajectories in Orly for the summer and winter of 2002. Figure <xref ref-type="fig" rid="Ch1.F3"/> shows the observed and simulated values of precipitation for lead times of 5 and 10 d for summer (June–July–August: JJA) and winter (December–January–February: DJF), for Orly precipitation data. We observe significantly positive correlations between observed values and the median of the forecasts for the four data sets as represented in Table <xref ref-type="table" rid="Ch1.T5"/>. The correlation is generally smaller in the summer than in the winter.
The correlation skill is low for some extreme values of precipitation.
For a lead time of 10 d, SWG simulation still shows a capacity to predict precipitation, in particular for winter with a correlation equal to 0.23 (Orly), 0.30 (Berlin), 0.43 (Madrid), and 0.31 (Toulouse).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><?xmltex \currentcnt{5}?><label>Table 5</label><caption><p id="d1e3432">Correlation between observations and the median of 100 simulations for both seasons, winter (DJF) and summer (JJA), for a lead time of 5 d.</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="center"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Location</oasis:entry>
         <oasis:entry colname="col2">Correlation DJF</oasis:entry>
         <oasis:entry colname="col3">95 % confidence interval</oasis:entry>
         <oasis:entry colname="col4">Correlation JJA</oasis:entry>
         <oasis:entry colname="col5">95 % confidence interval</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Berlin</oasis:entry>
         <oasis:entry colname="col2">0.50</oasis:entry>
         <oasis:entry colname="col3">0.48–0.56</oasis:entry>
         <oasis:entry colname="col4">0.22</oasis:entry>
         <oasis:entry colname="col5">0.21–0.23</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Madrid</oasis:entry>
         <oasis:entry colname="col2">0.53</oasis:entry>
         <oasis:entry colname="col3">0.51–0.55</oasis:entry>
         <oasis:entry colname="col4">0.29</oasis:entry>
         <oasis:entry colname="col5">0.27–0.30</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Orly</oasis:entry>
         <oasis:entry colname="col2">0.58</oasis:entry>
         <oasis:entry colname="col3">0.56–0.59</oasis:entry>
         <oasis:entry colname="col4">0.23</oasis:entry>
         <oasis:entry colname="col5">0.20–0.24</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Toulouse</oasis:entry>
         <oasis:entry colname="col2">0.40</oasis:entry>
         <oasis:entry colname="col3">0.39–0.44</oasis:entry>
         <oasis:entry colname="col4">0.18</oasis:entry>
         <oasis:entry colname="col5">0.15–0.19</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e3547">We observe that the 5th and 95th quantiles of the simulations include the different values of observations. This heuristically confirms the good skill of SWG to forecast precipitation from <inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> for various seasons (winter and summer) in several locations for <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> d lead times.</p>
      <p id="d1e3585">The difference in the forecast correlation skills between the four studied locations may be related to the variation of the local climate from one region to another. The studied areas are in different climate types according to the Köppen–Geiger climate classification <xref ref-type="bibr" rid="bib1.bibx27" id="paren.51"/>. From the southwestern side of Europe, Madrid is in the arid zone of the classification <xref ref-type="bibr" rid="bib1.bibx27" id="paren.52"/>, which indicates that convective rains are less frequent, and the origin of precipitation might be the result of humidity coming from the Atlantic. Conversely, Berlin is located in a cold zone characterized by warm summer and the absence of a dry season <xref ref-type="bibr" rid="bib1.bibx27" id="paren.53"/>; the precipitation could be the result of both, convective rains and Atlantic humidity.</p>
      <p id="d1e3597">In this paper, we decided (for simplicity) to use the same analogs to forecast precipitation for those four stations as discussed in Sect. <xref ref-type="sec" rid="Ch1.S4"/>. A refinement of the analog regions would be necessary when focusing on Madrid vs. Berlin.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Forecast probability skill</title>
      <p id="d1e3610">The CRPSS and correlation skill scores are computed for the four studied stations (Berlin, Madrid, Orly, and Toulouse), as shown in Fig. <xref ref-type="fig" rid="Ch1.F4"/> and for lead times from 5 to 20 d.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e3617">Percentage of each weather regime for observations dates (Obs) and the most frequent weather regime from SWG simulations between <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d (Analog) over the period from 1948 to 2019 for summer (JJA: <bold>a</bold>) and winter (DJF: <bold>b</bold>). The percentage of weather regime is the same in Obs and Analog.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f05.png"/>

        </fig>

      <p id="d1e3662">In this paper, we chose to present the results for summer and winter to highlight the capacity of the SWG to forecast the precipitation in extreme seasons. We focus on January and July in order to show the skill of the SWG in predicting precipitation in different conditions.</p>
      <p id="d1e3666">The CRPSS against the persistence and climatology references show positive values for lead times of up to 20 d (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). The values of CRPSS against the persistence reference (represented by squares) decrease with lead times in winter for the different studied areas, showing high values over 5 d. However, for summer, we notice that the values of CRPSS against persistence increase with lead time, with high values over 20 d except for Berlin. This indicates that the SWG forecast is still better than the persistence forecast (the average of the CRPS of SWG is smaller than the average of the CRPS of the persistence) for lead times of 20 d in the summer.
This could be explained by the fact that summer precipitation in Orly (51 % of the time, on average) comes in clusters contrary to precipitation in Berlin. Indeed, we computed the seasonal frequency of precipitation (defined as the number of days when precipitation exceeds 0.5 mm d<inline-formula><mml:math id="M200" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). We found that for Berlin, precipitation exceeding 0.5 mm d<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> is more frequent than in the other stations (close to 50 % of the time for both seasons).</p>
      <p id="d1e3695">This means that a persistence forecast for Orly is likely to be skillful, even for longer lead times, especially in the summer. Therefore, the trends in CRPSS values for different lead times are probably due to the intrinsic time persistence of local precipitation.</p>
      <p id="d1e3698">The CRPSS against the climatology reference (triangles in Fig. <xref ref-type="fig" rid="Ch1.F4"/>) shows lower values compared with the CRPSS against persistence reference, although they are positive for all lead times and for both seasons. However, we notice that for a short lead time the SWG is better than the climatology.</p>
      <p id="d1e3703">The correlation skill is positive for both seasons but higher in winter (January) than in summer (July). For a lead time of 5 d, the correlation is equal to 0.59 for Madrid, 0.50 for Berlin, and 0.40 for Toulouse. For a lead time of 10 d, it is equal to 0.42 for Madrid, 0.30 for Berlin, and 0.41 for Toulouse.</p>
      <p id="d1e3706">The SWG was tested by <xref ref-type="bibr" rid="bib1.bibx44" id="text.54"/> to forecast temperature in western Europe. Comparing the performance of the SWG to forecast those different meteorologic variables, we noticed that the model shows good performance to forecast the temperature in the winter; also the best performance of the model is at a lead time of 5 d. We find that the skill scores (CRPSS and correlation) decrease with lead times. The forecast skill of the SWG shows variability from one location to another. However, the model was able to forecast temperature until 40 d in Berlin, Orly, and Toulouse with positive skill scores.</p>
      <p id="d1e3712">From a visual inspection of the CRPSS and correlations, we chose to focus on lead times of <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d, for which the correlation exceeds 0.5 in the winter. It is rather low in the summer, due to convective events leading to a high precipitation variability (from no rain to very high values). Correlation scores become barely significant for lead times of 20 d, so that, like temperature, the SWG should not be used beyond that horizon.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <label>5.3</label><title>Relation between weather regimes and CRPS</title>
      <p id="d1e3735">We investigated the role of North Atlantic weather patterns defined in Sect. <xref ref-type="sec" rid="Ch1.S3.SS4"/> (Fig. <xref ref-type="fig" rid="Ch1.F2"/>) on the forecast skill of the SWG precipitation simulations.</p>
      <p id="d1e3742">We started by comparing the frequencies of the weather regimes from the observations and the most frequent weather regime found in SWG simulations for a given lead time <inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d. We found that the percentages are very similar (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). This means that the weather regimes of the simulated trajectories do not yield major biases for the summer or winter seasons.</p>
      <p id="d1e3759">Then we looked at the relation between weather regimes and CRPS values by using the most frequent weather regime within <inline-formula><mml:math id="M204" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> days and the two classes of quantiles of the CRPS that related to good quality of forecast (attributed to low values of CRPS <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mo>≤</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">25</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and poor quality of forecast (attributed to high values of CRPS <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mo>≥</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). This relation is represented in Fig. <xref ref-type="fig" rid="Ch1.F6"/> for Orly and for the rest of the studied stations in Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F8"/>. We found a small influence of specific weather regimes on the CRPS distribution for summer.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e3802">Relation between CRPS and weather regimes for Orly, for SWG forecasts with lead time <inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d. Panels <bold>(a)</bold> and <bold>(b)</bold> show CRPS value distribution conditioned on four weather regimes, when CRPS is lower than <inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">25</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Panels <bold>(c)</bold> and <bold>(d)</bold> show that CRPS is higher than <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. The boxplots indicate the median (<inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) of the distribution (thick bar). The 25th (<inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">25</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and 75th (<inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) quartiles (lower and upper segments of each boxplot). The boxplot upper whisker is <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mo>min⁡</mml:mo><mml:mfenced close="}" open="{"><mml:mrow><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:mo>max⁡</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>. The boxplot lower whisker is <inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:mo>max⁡</mml:mo><mml:mfenced close="}" open="{"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mo>min⁡</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f06.png"/>

        </fig>

      <p id="d1e3984">The weather regime signal for “good” forecasts depends on the season and the considered station.
When the forecast has a low CRPS value (for Orly), we find that the Scandinavian blocking regime slightly dominates (green bar in Fig. <xref ref-type="fig" rid="Ch1.F6"/>a, b). This is also the case for Berlin (in winter) and Toulouse (Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F8"/>b, j). The low CRPS values in Madrid are obtained for the Atlantic Ridge regime (Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F8"/>f).</p>
      <p id="d1e3993">The weather regime signal for “poor” forecasts also yields a dependence on the season and station.
Higher CRPS values are obtained with the Zonal regime in the summer for Orly (red line in Fig. <xref ref-type="fig" rid="Ch1.F6"/>c) and Toulouse. The Atlantic Ridge regime favors high CRPS values (i.e., poor forecasts) for Madrid in winter Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F8"/>h. The Scandinavian blocking favors high CRPS values for Berlin in winter and summer (green line in Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F8"/>c and d). The different impacts of the weather regimes on the studied areas are related to the position of the high- and low-pressure regions of each weather regime in the studied areas.</p>
      <p id="d1e4002">This relation between predictability (or the CRPS distribution) and weather regimes, albeit weak, is consistent with previous work of <xref ref-type="bibr" rid="bib1.bibx8" id="text.55"/>. Similar relations were found between weather regimes over Europe and the temperature in a recent study by <xref ref-type="bibr" rid="bib1.bibx2" id="text.56"/>. We found that the sensitivity of the forecast to weather regime is larger for low values of CRPS and in winter. The sensitivity of forecast skill to weather regimes is rather small on average, even for small lead times (<inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d).</p>
</sec>
<sec id="Ch1.S5.SS4">
  <label>5.4</label><title>Comparison with ECMWF forecast</title>
      <p id="d1e4031">We first compared the CRPSS of SWG forecasts for winter and summer with the CRPSS of ECMWF forecasts.</p>
      <p id="d1e4034">The CRPSS of the ECMWF forecast is
computed for different lead times going from 1 to 10 d for precipitation <xref ref-type="bibr" rid="bib1.bibx12" id="paren.57"/> over the region 12.5<inline-formula><mml:math id="M216" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–42.5<inline-formula><mml:math id="M217" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 35.0–75.0<inline-formula><mml:math id="M218" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N <xref ref-type="bibr" rid="bib1.bibx7" id="paren.58"/>. It uses the climatology as a reference <xref ref-type="bibr" rid="bib1.bibx12" id="paren.59"/>. The values of CRPSS for Europe for 2020 decrease in accordance with lead times <xref ref-type="bibr" rid="bib1.bibx12" id="paren.60"/>. The CRPSS of ECMWF is about 0.16 in summer (JJA) and 0.25 in winter (DJF) for a lead time of <inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d <xref ref-type="bibr" rid="bib1.bibx7" id="paren.61"/>.
The CRPSS of SWG simulations for a lead time of <inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d is shown in Table <xref ref-type="table" rid="Ch1.T4"/>. The values suggest that the predictive skill of SWG is qualitatively promising for short lead times, compared with ECMWF forecasts. However, we have to mention that the values of CRPSS for ECMWF are computed over all of Europe for both seasons <xref ref-type="bibr" rid="bib1.bibx12" id="paren.62"/>, while with the SWG we are doing a forecast for local stations.</p>
      <p id="d1e4110">We made a quantitative comparison between the two forecasts for the different lead times. We computed the CRPS for the ECMWF forecast. Then we used the Kolmogorov–Smirnov (KS) test (<xref ref-type="bibr" rid="bib1.bibx41" id="altparen.63"/>, chap. 1) to compare the probability distributions of the CRPS of SWG and ECMWF forecasts. The null hypothesis supposes that the CRPS of ECMWF and SWG forecasts have the same distribution. The null hypothesis of the KS test was rejected; this means that the two time series do not have the same distribution, with a <inline-formula><mml:math id="M221" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn></mml:mrow></mml:math></inline-formula>. A similar result was found by <xref ref-type="bibr" rid="bib1.bibx2" id="text.64"/>, where they compared the efficiency between ECMWF and CNRM forecasts.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e4139">Empirical cumulative distribution function of the CRPS of ECMWF (blue) and SWG (red) forecasts for 5 d, for Orly <bold>(a)</bold>, Berlin <bold>(b)</bold>, Madrid <bold>(c)</bold>, and Toulouse <bold>(d)</bold>. <inline-formula><mml:math id="M223" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> is the maximum distance between both ECDFs (value of Kolmogorov–Smirnov test). <inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> is the value of the time average of CRPS of SWG and <inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> is the value of the time average of CRPS of ECMWF. The dashed vertical lines represent the median of CRPS of ECMWF (blue) and SWG (red).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f07.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T6" specific-use="star"><?xmltex \currentcnt{6}?><label>Table 6</label><caption><p id="d1e4191">CRPSS of ECMWF forecasts using as a reference the CRPS of SWG, for lead times of <inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>, 10, and 20 d. The forecasts show that the
SWG has a positive improvement compared with the ECMWF forecast as the CRPSS scores are above zero, except for that of Toulouse.</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="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Location</oasis:entry>
         <oasis:entry colname="col2">Orly</oasis:entry>
         <oasis:entry colname="col3">Berlin</oasis:entry>
         <oasis:entry colname="col4">Madrid</oasis:entry>
         <oasis:entry colname="col5">Toulouse</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">CRPSS <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M228" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.09</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M229" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.02</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M230" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.2</oasis:entry>
         <oasis:entry colname="col5">0.25</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CRPSS <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> d</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M232" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.17</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M233" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.54</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M234" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.33</oasis:entry>
         <oasis:entry colname="col5">0.23</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CRPSS <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> d</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M236" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.50</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M237" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.36</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M238" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.1</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M239" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.08</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e4396">We found that 80 %, 39 %, 50 %, and 40 % of the CRPS of SWG forecast are equal to zero for, respectively, Orly, Berlin, Madrid, and Toulouse, for a lead time of <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d Fig. <xref ref-type="fig" rid="Ch1.F7"/>, which shows the capacity of the SWG to simulate rain events well.
One notable difference between SWG and ECMWF forecasts is that although the proportion of CRPS values close to zero is higher for ECMWF, the CRPS for the worst forecasts is much higher than those of SWG. Indeed, we noticed that the time average of CRPS of ECMWF (vertical blue lines) and SWG (red vertical lines) for <inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d are close, with higher values for ECMWF (Fig. <xref ref-type="fig" rid="Ch1.F7"/>). However, the median CRPS of ECMWF is smaller compared with the SWG (dashed vertical lines in Fig. <xref ref-type="fig" rid="Ch1.F7"/>).
Finally, we computed the CRPSS for ECMWF forecasts taking as a reference the CRPS of SWG (Table <xref ref-type="table" rid="Ch1.T6"/>). We hence computed the CRPSS of ECMWF forecast by normalizing the CRPS by the CRPS of the SWG forecast in Eq. (<xref ref-type="disp-formula" rid="App1.Ch1.S3.E4"/>).</p>
      <p id="d1e4434"><?xmltex \hack{\newpage}?>This new ECMWF CRPSS evaluates the added value of the ECMWF forecast over the SWG forecast. We found that the ECMWF forecast has no improvement over the SWG forecast for the different lead times because the CRPSS values are negative. At <inline-formula><mml:math id="M242" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d, we noticed that the improvement is negligible for Orly and Berlin, while it is much better for Madrid. However, for Toulouse, the ECMWF forecast still has better skills for lead times of <inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> and 10 d. For a lead time of <inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> d, the improvement of the SWG forecast over the ECMWF is significant, particularly for Berlin and Madrid. There is a major improvement for a lead time of <inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> d for Orly and Berlin.</p>
      <p id="d1e4486">This confirms the relatively good skill of the SWG to forecast precipitation, compared with ECMWF. This could be explained by the difference in the average of the CRPS of the two forecasts. Indeed, as we mentioned before, the ECMWF forecast yields the best skill scores for small values of precipitations (<inline-formula><mml:math id="M246" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> mm d<inline-formula><mml:math id="M247" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). We further illustrate those comparisons in Fig. <xref ref-type="fig" rid="App1.Ch1.S3.F10"/> and Table <xref ref-type="table" rid="App1.Ch1.S3.T7"/>.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e4524">In this work, we have shown the performance of a stochastic weather generator (SWG) to simulate precipitation over different locations in western Europe and for various time scales from 5 to 20 d. The input of our model was analogs of geopotential heights at 500 hPa (<inline-formula><mml:math id="M248" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula>). The choice of such input was made in order to evaluate the impact of large-scale circulation on local weather variables. The SWG showed a good skill in predicting precipitation for a lead time of 5 and 10 d from analogs of <inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e4547">This study of precipitation forecast complements the work of <xref ref-type="bibr" rid="bib1.bibx44" id="text.65"/> initially made to forecast temperature and the NAO index.
We explored the sensitivity of the SWG model on analogs computed from different geographic areas and from different reanalyses (ERA5 and NCEP). We found that both NCEP and ERA5 reanalyses perform well for simulations.</p>
      <p id="d1e4553">We evaluated the relation between the quality of the forecast and weather regimes over Europe. We found that low and high predictability were related to specific weather regimes. This dependence is more significant in winter than in summer. We found that good predictability is mainly related to blocking.</p>
      <p id="d1e4556"><?xmltex \hack{\newpage}?>A comparison with the ECMWF forecast system over western Europe confirmed quantitatively and qualitatively the skill forecast of the SWG , for lead times of <inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> d. Of course, the SWG model cannot replace a numerical weather prediction, as the SWG parameters (e.g., region of analogs) need to be tuned to local variables and rely on the existence of a fairly large database to compute analogs. Here we used the same domain of circulation analogs for stations from Madrid to Berlin. Obviously, this region should be optimized for each individual station. Therefore, the main utility of the SWG forecast system is to make local ensemble simulations, where its performances can challenge a numerical weather prediction if the parameters are well tuned.</p>
      <p id="d1e4573"><?xmltex \hack{\newpage}?>This paper hence confirms the proof of concept to generate ensembles of (local) precipitation forecasts from analogs of circulation. The SWG ensemble forecast performance relies on the relation between precipitation and the synoptic atmospheric circulation, which is verified for western Europe. Transposing this SWG to other regions of the globe requires observations covering several decades. Numerical weather models obviously do not yield this constraint.</p><?xmltex \hack{\clearpage}?>
</sec>

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

<app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title>CRPS and weather regimes</title>
      <p id="d1e4589">To avoid a tedious redundancy we deferred the figures of evaluation of the forecast quality by weather regimes to this appendix section.</p>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F8"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Figure}?><label>Figure A1</label><caption><p id="d1e4594">Relation between CRPS and weather regimes for Berlin <bold>(a–d)</bold>, Madrid <bold>(e–h)</bold>, and Toulouse <bold>(i–l)</bold>, for SWG forecasts with lead time <inline-formula><mml:math id="M251" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> d. Panels <bold>(a)</bold>, <bold>(b)</bold>, <bold>(e)</bold>, <bold>(f)</bold>, <bold>(i)</bold>, and <bold>(j)</bold> correspond to CRPS value distribution conditioned on four weather regimes, when CRPS is lower than <inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">25</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Panels <bold>(c)</bold>, <bold>(d)</bold>, <bold>(g)</bold>, <bold>(h)</bold>, <bold>(k)</bold>, and <bold>(l)</bold> correspond to a higher CRPS value (<inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mo>≥</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). The boxplots indicate the median (<inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) of the distribution (thick bar).</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=284.527559pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f08.png"/>

      </fig>

<?xmltex \hack{\clearpage}?>
</app>

<app id="App1.Ch1.S2">
  <?xmltex \currentcnt{B}?><label>Appendix B</label><?xmltex \opttitle{Relation between $Z500$ and precipitation}?><title>Relation between <inline-formula><mml:math id="M255" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> and precipitation</title>
      <p id="d1e4723">In order to justify the use of the <inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> as a driver of precipitation, we computed the rank spatial correlation between the daily average of <inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> over the Euro-Atlantic region and the precipitation in each studied station (Berlin, Madrid, Orly, and Toulouse). We did the analysis for different seasons (DJF and JJA).
We found a maximum correlation amplitude of <inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> for Madrid and Orly, and a correlation of <inline-formula><mml:math id="M259" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M260" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>, respectively, for Toulouse and Berlin. The correlation is significant as we have a <inline-formula><mml:math id="M261" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value <inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> for the different grid points. This indicates the relation between <inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> patterns and precipitation, in particular in western Europe, and that a decrease in <inline-formula><mml:math id="M264" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> is linked with precipitation.</p>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S2.F9"><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Figure}?><label>Figure B1</label><caption><p id="d1e4816">Maps of correlation between <inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> and precipitation in Berlin, Madrid, Orly, and Toulouse for the period from 1948 to 2019 over the Euro-Atlantic region. The rectangles represent the domains of computation of analogs. The optimized area [30<inline-formula><mml:math id="M266" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–20<inline-formula><mml:math id="M267" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 40–60<inline-formula><mml:math id="M268" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N] is highlighted by the red rectangle.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f09.png"/>

      </fig>

</app>

<app id="App1.Ch1.S3">
  <?xmltex \currentcnt{C}?><label>Appendix C</label><title>CRPSS of ECMWF vs. SWG</title>
      <p id="d1e4872">We explain further the comparison that we made between the ECMWF forecast and the SWG forecast. As mentioned we found that the SWG has improved compared with the ECMWF forecast. This is related to the difference in the time average of the CRPS of the two forecasts.
We computed the CRPSS as follows:
          <disp-formula id="App1.Ch1.S3.E4" content-type="numbered"><label>C1</label><mml:math id="M269" display="block"><mml:mrow><mml:mi mathvariant="normal">CRPSS</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ECMWF</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">SWG</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M270" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ECMWF</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> is the time average of the <inline-formula><mml:math id="M271" display="inline"><mml:mi mathvariant="normal">CRPS</mml:mi></mml:math></inline-formula> of the ECMWF forecast and <inline-formula><mml:math id="M272" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">SWG</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> is the time average of the <inline-formula><mml:math id="M273" display="inline"><mml:mi mathvariant="normal">CRPS</mml:mi></mml:math></inline-formula> of the SWG.</p><?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S3.T7"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{C1}?><label>Table C1</label><caption><p id="d1e4957">Average and median values of CRPS, average CRPSS (in bold) of the ECMWF and SWG forecasts for lead times of <inline-formula><mml:math id="M274" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>, 10, and 20 d. The table shows that the CRPS of the SWG forecast has a smaller average than the CRPS of the ECMWF forecast, which explains the values of CRPSS for the different studied areas and the positive improvement of the SWG compared with the ECMWF.​​​​​​​</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Location</oasis:entry>
         <oasis:entry colname="col2">Orly</oasis:entry>
         <oasis:entry colname="col3">Berlin</oasis:entry>
         <oasis:entry colname="col4">Madrid</oasis:entry>
         <oasis:entry colname="col5">Toulouse</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M275" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ECMWF</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>; median</oasis:entry>
         <oasis:entry colname="col2">1.87; 0.04</oasis:entry>
         <oasis:entry colname="col3">16.56; 0.05</oasis:entry>
         <oasis:entry colname="col4">18.73; 0.003</oasis:entry>
         <oasis:entry colname="col5">12.76; 0.01</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M276" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">SWG</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>; median</oasis:entry>
         <oasis:entry colname="col2">1.70; 0.67</oasis:entry>
         <oasis:entry colname="col3">16.10; 10.37</oasis:entry>
         <oasis:entry colname="col4">15.49; 5.45</oasis:entry>
         <oasis:entry colname="col5">17.16; 8.39</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M277" display="inline"><mml:mi mathvariant="bold">CRPSS</mml:mi></mml:math></inline-formula> for <inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="bold">5</mml:mn></mml:mrow></mml:math></inline-formula> <bold>d</bold>​​​​​​​</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.09</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M281" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M282" display="inline"><mml:mn mathvariant="bold">0.25</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M283" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ECMWF</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">1.70; 0.05</oasis:entry>
         <oasis:entry colname="col3">18.1; 0.06</oasis:entry>
         <oasis:entry colname="col4">20.03; 0.1</oasis:entry>
         <oasis:entry colname="col5">14.87; 0.09</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M284" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">SWG</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">1.44; 0.78</oasis:entry>
         <oasis:entry colname="col3">11.67; 5.45</oasis:entry>
         <oasis:entry colname="col4">15.04; 6.13</oasis:entry>
         <oasis:entry colname="col5">19.45; 7.89</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M285" display="inline"><mml:mi mathvariant="bold">CRPSS</mml:mi></mml:math></inline-formula> for <inline-formula><mml:math id="M286" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="bold">10</mml:mn></mml:mrow></mml:math></inline-formula> <bold>d</bold></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M287" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.17</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.54</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.33</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M290" display="inline"><mml:mn mathvariant="bold">0.23</mml:mn></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M291" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">ECMWF</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">1.67; 0.1</oasis:entry>
         <oasis:entry colname="col3">13.54; 0.09</oasis:entry>
         <oasis:entry colname="col4">17.89; 0.1</oasis:entry>
         <oasis:entry colname="col5">17.8; 0.08</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M292" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="normal">CRPS</mml:mi><mml:mi mathvariant="normal">SWG</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">1.11; 0.9</oasis:entry>
         <oasis:entry colname="col3">9.91; 6.3</oasis:entry>
         <oasis:entry colname="col4">16.23; 5.89</oasis:entry>
         <oasis:entry colname="col5">16.41; 8.34</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M293" display="inline"><mml:mi mathvariant="bold">CRPSS</mml:mi></mml:math></inline-formula> for <inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="bold">20</mml:mn></mml:mrow></mml:math></inline-formula> <bold>d</bold></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M295" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.50</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.36</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="bold">0.08</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S3.F10"><?xmltex \currentcnt{C1}?><?xmltex \def\figurename{Figure}?><label>Figure C1</label><caption><p id="d1e5402">Boxplots of CRPS of ECMWF and CRPS of SWG for Orly, with lead time <inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>, 10, and 20 d. The boxplots indicate the median
(<inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>​​​​​​​) of the distribution (thick blue bar for ECMWF and red for SWG). The 25th (<inline-formula><mml:math id="M301" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">25</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>​​​​​​​) and 75th (<inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) quartiles are, respectively, the lower and upper segments of each boxes.
The upper whisker is <inline-formula><mml:math id="M303" display="inline"><mml:mrow><mml:mo>min⁡</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mo>max⁡</mml:mo><mml:mo>(</mml:mo><mml:mi>X</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">50</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>(</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">75</mml:mn></mml:msub><mml:mi mathvariant="normal">−</mml:mi><mml:msub><mml:mi>q</mml:mi><mml:mn mathvariant="normal">25</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>​​​​​​​. The average CRPS of the ECMWF and SWG forecasts are indicated with
dashed horizontal lines. Note that the distribution is asymmetric as the median and the average are unequal. The average
CRPS for the SWG forecast is lower than the average CRPS for the ECMWF forecast. The outliers that are above the upper whiskers are not shown.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/4941/2022/gmd-15-4941-2022-f10.png"/>

      </fig>

</app>
  </app-group><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e5510">The code and data files are available at <ext-link xlink:href="https://doi.org/10.5281/zenodo.4524562" ext-link-type="DOI">10.5281/zenodo.4524562</ext-link> <xref ref-type="bibr" rid="bib1.bibx22" id="paren.66"/>.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e5522">MK performed the analyses. PY co-designed the analyses. CD and ST participated in the manuscript preparation.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e5528">The contact author has declared that neither they nor their co-authors have any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e5534">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><?xmltex \hack{\vspace*{15.9cm}}?><ack><title>Acknowledgements</title><p id="d1e5541">This work is part of the EU International Training Network (ITN) Climate Advanced Forecasting of subseasonal Extremes (CAFE). We thank Linus Magnusson and Florian Pappenberger​​​​​​​ for helpful discussions on the ECMWF data.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e5547">This work is part of the EU International
Training Network (ITN) “Climate Advanced Forecasting of subseasonal
Extremes” (CAFE). The project receives funding from the European
Union's Horizon 2020 research and innovation program under
the Marie Skłodowska-Curie Grant (agreement no. 813844).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e5553">This paper was edited by Chiel van Heerwaarden and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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