<?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">
  <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-15-1841-2022</article-id><title-group><article-title>Extreme events representation in CMCC-CM2 standard and<?xmltex \hack{\break}?> high-resolution
general circulation models</article-title><alt-title>Extreme events representation in CMCC-CM2</alt-title>
      </title-group><?xmltex \runningtitle{Extreme events representation in CMCC-CM2}?><?xmltex \runningauthor{E. Scoccimarro et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Scoccimarro</surname><given-names>Enrico</given-names></name>
          <email>enrico.scoccimarro@cmcc.it</email>
        <ext-link>https://orcid.org/0000-0001-7987-4744</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Peano</surname><given-names>Daniele</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6975-4447</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Gualdi</surname><given-names>Silvio</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7777-8935</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Bellucci</surname><given-names>Alessio</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Lovato</surname><given-names>Tomas</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Fogli</surname><given-names>Pier Giuseppe</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7997-6273</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Navarra</surname><given-names>Antonio</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Fondazione Centro Euro-Mediterraneo sui Cambiamenti Climatici,
Bologna, Italy</institution>
        </aff>
        <aff id="aff2"><label>a</label><institution>currently at: Consiglio Nazionale delle Ricerche, Istituto di
Scienze dell'Atmosfera e del Clima, Bologna, Italy​​​​​​​</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Enrico Scoccimarro (enrico.scoccimarro@cmcc.it)</corresp></author-notes><pub-date><day>3</day><month>March</month><year>2022</year></pub-date>
      
      <volume>15</volume>
      <issue>4</issue>
      <fpage>1841</fpage><lpage>1854</lpage>
      <history>
        <date date-type="received"><day>25</day><month>August</month><year>2021</year></date>
           <date date-type="rev-request"><day>15</day><month>September</month><year>2021</year></date>
           <date date-type="rev-recd"><day>26</day><month>January</month><year>2022</year></date>
           <date date-type="accepted"><day>27</day><month>January</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Enrico Scoccimarro 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/15/1841/2022/gmd-15-1841-2022.html">This article is available from https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022.html</self-uri><self-uri xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022.pdf">The full text article is available as a PDF file from https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e144">The recent advancements in climate modeling partially
build on the improvement of horizontal resolution in different components of
the simulating system. A higher resolution is expected to provide a better
representation of the climate variability, and in this work we are
particularly interested in the potential improvements in representing
extreme events of high temperature and precipitation. The two versions of
the Centro Euro-Mediterraneo sui Cambiamenti Climatici (CMCC-CM2) model used here adopt the highest horizontal resolutions
available within the last family of the global coupled climate models
developed at CMCC to participate in the Coupled Model Intercomparison Projects, Phase 6 (CMIP6) effort.</p>

      <p id="d1e147">The main aim of this study is to document the ability of the CMCC-CM2 models
to represent the spatial distribution of extreme events of temperature
and precipitation, under the historical period, comparing model results to
observations, the European Centre for Medium-Range Weather Forecasts (ECMWF) reanalysis (ERA5), multi-source weighted-ensemble precipitation (MSWEP) and Climate Hazards Group infrared precipitation with station data (CHIRPS) observations. For a more
detailed evaluation we use both 6-hourly and daily time series, to compute
indices representative of intense and extreme conditions.</p>

      <p id="d1e150">In terms of mean climate, the two models are able to realistically reproduce
the main patterns of temperature and precipitation. The high resolution
version (<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> horizontal resolution) of the atmospheric
model provides better results than the standard resolution one (1°),
not only in terms of means but also in terms of intense and extreme events
of temperature defined at daily and 6-hourly frequencies. This is also the
case of average and intense precipitation. On the other hand the extreme
precipitation is not improved by the adoption of a higher horizontal
resolution.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e182">An extreme climate event can have an impact on human activities, either as
direct and indirect damages and, unfortunately also as loss of human life.
For this reason it is very relevant to investigate the ability of general circulation models (GCMs) to simulate extreme events and to understand how the
changing climate is influencing their distribution, frequency and location.
Simulations of GCMs under the historical climate radiative forcing have been
assessed in previous generations of the Coupled Model Intercomparison
Projects (CMIP; Flato et al., 2013) and, more recently for CMIP6 (Eyring et
al., 2016). Within CMIP6 the High Resolution Model Intercomparison Project
protocol (HighResMIP, Haarsma et al., 2016) was designed to understand the
role of the horizontal resolution in improved process representation in all
components of the climate system. In this paper, we present an analysis
based on two versions of the GCM developed at the Centro Euro-Mediterraneo sui Cambiamenti Climatici (CMCC-CM, Cherchi et al.,
2019) that we use for two simulations of the historical climate (1950–2014)
differing only in their atmospheric horizontal resolution: HR with a
horizontal resolution of 1<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and VHR with a resolution of
<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> of a degree. The two models are described in detail in the
next section.</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="d1e208">Winter (December, January, February, DJF) extreme temperature (99th percentile, 99p) computed
at the daily frequency. Upper panel shows ERA5 results. Central panels show
model results (HR on the left and VHR on the right) and lower panels show
the relative model bias. Units are [<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C]. Vertical color bar refers to
the three upper panels, while the horizontal color bar refers to the two
bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f01.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e228">Summer (June, July, August, JJA) extreme temperature (99th percentile, 99p) computed
at the daily frequency. Upper panel shows ERA5 results. Central panels show
model results (HR on the left and VHR on the right) and lower panels show
the relative model bias. Units are [<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C]. Vertical color bar refers to
the three upper panels, while the horizontal color bar refers to the two
bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f02.png"/>

      </fig>

      <p id="d1e247"><?xmltex \hack{\newpage}?>The difference between the results obtained with the two versions of the
model allows us to evaluate the impact of the model HR on
the temporal distribution of temperature and precipitation events compared
to observations. It has been shown that the HR can affect
the representation of extreme events in state-of-the-art climate models (Van
Haren et al., 2015; Iles et al., 2020). Furthermore, Demory et al. (2020) have
shown that high-resolution models, when implemented with a resolution
similar to VHR, achieve SKILLS comparable to state-of-the-art regional
climate models in reproducing precipitation distributions over Europe.
However, most of the analyses on extreme events employ relatively low frequency
data (typically daily), and short-duration high-intensity precipitation
events can easily escape detection if high-frequency data are not used
(Meredith et al., 2020; Scoccimarro et al., 2015).</p>
      <p id="d1e251">Regarding the extremely high temperature representation, based on data at
the daily frequency it has been shown that GCMs tend to have warm bias over
most land areas (Li et al., 2021) and the HR plays a
minor role in affecting the bias, with respect to the role played in the
extreme precipitation representation (Kharin et al., 2013; Wei et al., 2019).</p>
      <p id="d1e254">Regarding the extreme precipitation representation in GCMs, based on
simulations from a single model, some improvement in SKILL at higher
resolution for some measures of extreme precipitation over certain regions
of the globe have been found in the past (Wehner et al., 2014; Kopparla et
al., 2013). Only recently, multi-model assessments on this topic have been
done, confirming that increasing the horizontal resolution to
<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> of a degree (the highest adopted by the model object of this
study), the magnitude of simulated daily (Bador et al., 2020) and sub-daily
precipitation (Wehner et al., 2021) extremes is increased. On the other hand
this is not associated with a systematic improvement in the simulation of
precipitation extremes when compared to observations and, quantitatively, at
the global scale the intensification of precipitation extremes at increased
resolution varies substantially from model to model (Bador et al., 2020).
Also, for grid point GCMs (as opposed to spectral GCMs), the fraction of
land precipitation increases, largely due to better resolution of orography
(Vannière et al., 2019; Terai et al., 2018; Demory et al., 2014).</p>
      <p id="d1e269">In this paper we present both a daily and a high-frequency analysis using
6-hourly data from the experiments, comparing model results to data from a
reanalysis dataset with comparable horizontal resolution (ERA5, Hersbach et
al., 2020) and two observational precipitation datasets, such as multi-source weighted-ensemble precipitation (MSWEP) (Beck
et al., 2019) and Climate Hazards Group infrared precipitation with station data (CHIRPS) (Funk et al., 2015). The importance of evaluating
extreme events at the sub-daily scale resides in the importance of such
events on human health and over both urban and rural environments (Wehner et
al., 2021).</p>
      <p id="d1e272">The work is organized as follows: Sect. 2 describes the data and the
methodology adopted, Sects. 3 and 4 describe the evaluation of model
ability in representing the distribution of temperature and precipitation
events, respectively, and Sect. 5 summarizes and concludes the work.</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="d1e278">Winter (DJF) extreme temperature (99th percentile, 99p) computed
at the 6-hourly frequency. Upper panel shows ERA5 results. Central panels
show model results (HR on the left and VHR on the right) and lower panels
show the relative model bias. Units are [<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C]. Vertical color bar refers
to the three upper panels, while the horizontal color bar refers to the two
bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f03.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e298">Summer (JJA) extreme temperature (99th percentile, 99p) computed
at the 6-hourly frequency. Upper panel shows ERA5 results. Central panels
show model results (HR on the left and VHR on the right) and lower panels
show the relative model bias. Units are [<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C]. Vertical color bar refers
to the three upper panels, while the horizontal color bar refers to the two
bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f04.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e318">Winter (DJF) extreme precipitation (99th percentile, 99p) computed
at the daily frequency. Upper panel shows MSWEP observational results.
Central panels show model results (HR on the left and VHR on the right) and
lower panels show the relative model bias. Units are [mm d<inline-formula><mml:math id="M10" 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>]. Vertical
color bar refers to the three upper panels, while the horizontal color bar
refers to the two bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f05.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e341">Summer (JJA) extreme precipitation (99th percentile, 99p) computed
at the daily frequency. Upper panel shows MSWEP observational results.
Central panels show model results (HR on the left and VHR on the right) and
lower panels show the relative model bias. Units are [mm d<inline-formula><mml:math id="M11" 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>]. Vertical
color bar refers to the three upper panels, while the horizontal color bar
refers to the two bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f06.png"/>

      </fig>

</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methodology</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Numerical experiments</title>
      <p id="d1e377">The CMCC general circulation model has been developed in several
configurations (Cherchi et al., 2019). The model uses as atmospheric module
the community atmosphere model (CAM) atmospheric component (CAM4, Neale et al., 2010) in its grid point
configuration. We will not go in a detailed description here, but since it
is worthwhile to mention for our discussion on precipitation biases, the
deep convection scheme is the one developed by Zhang and McFarlane (1995),
modified following Richter and Rasch (2008) and Raymond and Blith (1986,
1992). The scheme is based on a plume ensemble approach where it is assumed
that an ensemble of convective scale updrafts may exist whenever the
atmosphere is conditionally unstable in the lower troposphere. Moist
convection occurs only when there is convective available potential energy
(CAPE) for which parcel ascent from the sub-cloud layer acts to destroy the
CAPE at an exponential rate using a specified adjustment time scale. In
other words the deep convection scheme is triggered based on a minimum
positive threshold of CAPE,the  same as in the standard version of the CAM5
model (Wang and Zhang, 2013). The two models that are the object of this study differ
only in the horizontal resolution of their atmospheric component (CAM4) that
is one degree in HR, the standard resolution one, and <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in VHR, the high resolution one. The ocean and sea-ice components
are the same in HR and VHR models: a <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> HR version for both ocean (NEMO3.6, Madec and the NEMO team, 2016)
and sea-ice (CICE4, Hunke and Lipscomb, 2008). The land model (CLM4.5,
Oleson et al., 2013) is implemented with the atmospheric model grid. The
basis of the coupling between the different components is described in Fogli
and Iovino (2014). The single components of the coupled model are described
in detail in Cherchi et al. (2019); additional studies based on last
generation CMCC GCMs can be found in Scoccimarro et al. (2017a, 2020), Bellucci et al. (2021). No changes are applied in terms of
parameterization choices and relative tuning parameters moving from HR
to VHR to be compliant with the HighResMIP protocol. Also, the two model
versions use the same number of vertical levels in both atmosphere (26) and
ocean (50) components. The complete set of experiments run with these two
models is described in Haarsma et al. (2016). In the current analysis we
investigate the hist-1950 HighResMIP experiment as described in Sect. 2.3.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Reanalyses and observations for comparison</title>
      <p id="d1e428">The model performance in representing the temperature distribution is
evaluated by comparing results to the European Centre for Medium Range
Weather Forecasts (ECMWF) reanalyses (ERA5, Hersbach et al., 2020; Andersson
and Thepaut, 2008), with 137 hybrid sigma/pressure (model) levels in the
vertical, and the top level at 0.01 hPa. The temperature data used in the
paper (2m temperature, hereafter “temperature”) can be obtained
from the Copernicus Data Store (CDS) at <uri>https://cds.climate.copernicus.eu</uri> (last access: 15 July <?xmltex \hack{\mbox\bgroup}?>2021​​​​​​​)<?xmltex \hack{\egroup}?> up to hourly frequency. The HR in ERA5 is about 0.28<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, close to the one of the higher
(VHR) resolution model employed here (<inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>). It is important to note
that the improvement of ERA5 with respect to the previous
ERA-Interim (Dee et al., 2011) product is due not only to the increased
resolution but also to the addition of new integrated observation and
aircraft data covering the recent decades, assimilated by the 4D-Var
algorithm. Since there are many known issues with ERA5 precipitation
(Rivoire et al., 2021; Hu and Franzke, 2020; Crosset et al., 2020), for the
evaluation of the model performance in representing the precipitation
distribution, we build on MSWEP version 2 observational dataset (Beck et al., 2019): The MSWEP global
precipitation dataset is available at a 3-hourly temporal resolution,
covering the period from 1979 to the near present, with a horizontal
resolution of 0.1<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The dataset takes advantage of the complementary
strengths of gauge-based, satellite-based, and reanalysis-based data to provide
reliable precipitation estimates over the globe.</p>
      <p id="d1e477">Since we aim to characterize different types of extreme events, we consider
both 6-hourly and daily time series for the computation of the percentiles
(see Sect. 2.3) for the chosen climate parameters.</p>
      <p id="d1e480">For a more exhaustive evaluation of the precipitation distribution, we also
take advantage of the CHIRPS daily observational dataset. The version 2.0 of the CHIRPS
database comprises a quasi-global (50<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–50<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
180<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E–180<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) domain, at <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
resolution, and 1981 to near present gridded precipitation daily time
series. This dataset merges three types of information: global climatology,
satellite estimates, and in situ observations (Funk et al., 2015).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Methodology</title>
      <p id="d1e547">The period used to compare the simulated temperature (tas <inline-formula><mml:math id="M26" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> temperature of the air at the surface) distribution to
the observations is 1950–2014. On the other hand, due to the shorter period
available for the MSWEP and CHIRPS datasets, the precipitation (pr)
distribution is evaluated over the common period between the observations
and the historical model run 1981–2014. This time period is sufficiently
long to capture the temporal variability at the global scale (Schindler et
al., 2015). Typically, the warm extremes are computed based on maximum daily
temperatures, but in this work we want to verify the potential improvements
induced by the increased resolution in the representation of extreme
temperature events defined at two different time frequencies (daily and
6-hourly). For this reason we investigate the distribution of daily and
6-hourly average temperature (tas), instead of maximum daily temperature.</p>
      <p id="d1e557">Model averages and 99th/90th​​​​​​​ percentile (99p/90p hereafter) are
computed on the native grid and then the results are compared to ERA5 or
observational datasets, linearly interpolating the reanalysis (or
observations) on the model grid. The kind of interpolation introduces very
little differences in the fields (not shown). We denote events belonging to
the 99p as “extreme events” and the ones belonging to the 90p as “intense
events” (Scoccimarro et al., 2016). Two seasons are considered, December to
February (DJF) and June to August (JJA) representative
of the boreal winter and summer, respectively.</p>
      <p id="d1e560">Temperature percentiles computed at the daily time frequency are obtained
based on a sample of 5850 (90 d <inline-formula><mml:math id="M27" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 65 years) events, while the percentiles computed at the
6-hourly time frequency are obtained based on a sample of 23 400 (90 d <inline-formula><mml:math id="M28" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 65 years <inline-formula><mml:math id="M29" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 4; 6-hourly data in a day) events.
Precipitation percentiles computed at the daily time frequency are obtained
based on a sample of 3060 (90 d <inline-formula><mml:math id="M30" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 34 years) events, while the percentiles computed at the
6-hourly time frequency are obtained based on a sample of 12 240 (90 d <inline-formula><mml:math id="M31" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 34 years <inline-formula><mml:math id="M32" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 4; 6-hourly data in a day) events.</p>
      <p id="d1e606">Temperature related parameters are expressed in degrees Celsius [<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C],
and precipitation related parameters in [mm d<inline-formula><mml:math id="M34" 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>]. When expressed as %
fraction (Fig. S17 only) the precipitation is shown only for regions where
the seasonal average of precipitation is higher than 0.5 mm d<inline-formula><mml:math id="M35" 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> to avoid
misleading percentual differences over dry domains (Scoccimarro et al., 2013). The comparison with CHIRPS precipitation data is performed at the
daily frequency only.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Representation of extreme events of temperature</title>
      <p id="d1e651">In this section modeled extreme temperature is compared to the ERA5
reanalysis. Figure 1 shows the DJF 99th percentile of ERA5 temperature
time series (upper panel) at the daily frequency, together with model
results (central panels), and relative biases (lower panels). Figure 2 shows
the JJA season results following the same structure while Figs. 3 and 4 refer to 6-hourly statistics. Higher values for extreme events
appear when focusing on the 6-hourly results, with maximum differences (up
to 5 <inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) along the Tropics and in particular over Central America,
western India and Equatorial Africa during DJF (Fig. 1 compared to Fig. 3, upper panels) and over northern Africa, Saudi Arabia and western USA during JJA (Fig. 2 compared to Fig. 4, upper panels).</p>
      <p id="d1e663">The daily based extreme temperature bias is shown in Figs. 1 (for DJF) and 2 (for JJA) for the HR and VHR models in the lower panels. The large
positive DJF bias shown by the HR model at the high latitudes in the
Northern Hemisphere, reaching 9 <inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C over Alaska, northern Canada and
eastern Siberia (Fig. 1 lower left panel), is significantly reduced in
the VHR model (Fig. 1, lower right panel). Also the positive HR bias in DJF
over eastern Europe is more than halved in VHR, while the DJF negative
biases over northern Africa and the Tibetan Plateau worsen moving to the higher
resolution. The positive extreme temperature bias between 30 and
60<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N shown by the HR model during JJA (Fig. 2 lower left panel) is
partially reduced in VHR especially over Europe and Asia. Similarly, the 5
to 7 <inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C positive JJA bias over the western coast of South America in HR is halved in VHR. On the other hand, the negative JJA bias of about
<inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C over northeast Canada shown by the HR model is even worse in the
VHR version, where a larger portion of the domain is subject to a bias of
about <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. This negative bias is also consistent with the tendency of
the two versions of the CMCC-CM2 model to overestimate the sea-ice cover
during summer over the Northern Hemisphere (not shown).</p>
      <p id="d1e730">Moving to the 6-hourly based extreme events, the fraction of land affected
by a positive bias higher than 5 <inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C is more pronounced compared to the
daily statistics, especially for the HR model during JJA (Fig. 4). The
positive bias over the northwestern part of South America, during JJA,
reaches 9 <inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in HR and is only partially reduced in VHR; during the same
season the positive bias of the same order of magnitude over central and
eastern USA is not improved by the increased resolution. Similar
patterns, but less pronounced, are reflected on the average temperature, as
shown in Supplement Figs. S1–S2, and intense events representation
(Figs. S7–S10).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e754">Winter (DJF) extreme precipitation (99th percentile, 99p) computed
at the 6-hourly frequency. Upper panel shows MSWEP observational results.
Central panels show model results (HR on the left and VHR on the right) and
lower panels show the relative model bias. Units are [mm d<inline-formula><mml:math id="M46" 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>]. Vertical
color bar refers to the three upper panels, while the horizontal color bar
refers to the two bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f07.png"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Representation of extreme events of precipitation</title>
      <p id="d1e783">Following the same structure as in the previous section, the model extreme
precipitation is here compared to the MSWEP observations (from Figs. 5 to 8) for both daily and 6-hourly statistics, and then to the CHIRPS
dataset (Figs. 9 and 10) for daily statistics only. Figure 5 shows the
MSWEP DJF seasonal extreme precipitation (upper panel) during the historical
period and the modeled results (central panels) together with the relative
biases (lower panels). Figure 6 shows the same 99p parameter but for JJA,
computed based on daily time series. Figures 7 (for DJF) and 8 (for JJA),
instead, show the 99p computed based on 6-hourly time series. The higher
extreme events magnitude associated with the 6-hourly results (Figs. 7 and
8, upper panel) compared to the daily statistics (Figs. 5 and 6, upper
panel) is visible almost everywhere, but it is more pronounced over the
Tropics. In fact this is where convective processes are expected, and it is
well known that convective precipitation tends to be short-lived, while
long duration intense events (from 12 h to 3 d) are often associated
with synoptic weather systems and tend to have larger spatial scales (Chan et
al., 2014; Scoccimarro et al., 2015).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e788">Summer (JJA) extreme precipitation (99th percentile, 99p) computed
at the 6-hourly frequency. Upper panel shows MSWEP observational results.
Central panels show model results (HR on the left and VHR on the right) and
lower panels show the relative model bias. Units are [mm d<inline-formula><mml:math id="M47" 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>]. Vertical
color bar refers to the three upper panels, while the horizontal color bar
refers to the two bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f08.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e811">Same as Fig. 5 but based on CHIRPS observations. Winter (DJF)
extreme precipitation (99th percentile, 99p) computed at the daily
frequency. Upper panel shows CHIRPS observational results. Central panels
show model results (HR on the left and VHR on the right) and lower panels
show the relative model bias. Units are [mm d<inline-formula><mml:math id="M48" 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>]. Vertical color bar refers to
the three upper panels, while the horizontal color bar refers to the two
bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f09.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e835">Same as Fig. 6 but based on CHIRPS observation. Summer (JJA)
extreme precipitation (99th percentile, 99p) computed at the daily
frequency. Upper panel shows CHIRPS observational results. Central panels
show model results (HR on the left and VHR on the right) and lower panels
show the relative model bias. Units are [mm d<inline-formula><mml:math id="M49" 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>]. Vertical color bar refers to
the three upper panels, while the horizontal color bar refers to the two
bottom panels.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://gmd.copernicus.org/articles/15/1841/2022/gmd-15-1841-2022-f10.png"/>

      </fig>

      <p id="d1e856">In terms of average precipitation the VHR model shows less pronounced biases
with respect to the HR model (Figs. S3 and S4 for DJF and JJA, respectively
based on MSWEP and Figs. S5 and S6 for the same seasons based on CHIRPS).
In particular, during DJF, the negative bias over the northern part of South
America is reduced from about 4 to 2 mm d<inline-formula><mml:math id="M50" 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>, while the positive bias over
western USA, South Africa and Australia is almost halved. During
JJA, the bias tends to be less pronounced in both models, and the
differences between the two are mainly located over Peru, Bolivia and Brazil
ranging from about <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> mm d<inline-formula><mml:math id="M52" 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> of the HR model to values closer to zero, even
positive, over a small portion of the domain in the VHR model.</p>
      <p id="d1e893">A different behavior is found focusing on daily extreme precipitation
events. No particular differences between high and low resolution biases are
found north of 30<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N during winter (Fig. 5), while the VHR model tends
to overestimate the 99th percentile of daily precipitation distribution
in both seasons within the Tropics (Figs. 5 and 6). Similar patterns
emerge for the 6-hourly based extreme precipitation (Fig. 6), but with a
less pronounced overestimate in VHR over the Tropics, compared to the HR
results. The intense events are better represented by the VHR model compared
to the HR one, especially during winter in the Southern Hemisphere (Fig. S11, lower panels), where the 8 mm d<inline-formula><mml:math id="M54" 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> HR positive bias over Australia and
South Africa is halved in VHR. This is consistent with the better
representation of the DJF average precipitation in the VHR model (Fig. S3), suggesting that the bad representation of DJF extreme precipitation in
VHR (Fig. 5) is mainly due to a much too pronounced stretching of the
right part of the precipitation distribution.</p>
      <p id="d1e917">To corroborate our results in terms of precipitation biases, we computed the
same statistics obtained from MSWEP, using the CHIRPS observational daily
dataset for averages (Figs. S5 and S6) and extreme events (Figs. 9 and
10). The biases computed with respect to the CHIRPS dataset are very similar
to what we already described based on MSWEP, but with a slightly increased
magnitude (Fig. 9 compared to Fig. 5) for extreme events in both models,
especially during DJF, along the Tropics.</p>
      <p id="d1e920">The worsening of the extreme precipitation bias moving from the HR to the
VHR model along the Tropics, especially in the Southern Hemisphere during
JJA, is also associated with a deterioration of the representation of the
fraction of precipitation associated with extreme events with respect to the
total precipitation: this metric is obtained by accumulating the water of all
the events more intense than the 99p, and normalizing it by the total amount
of precipitation in the considered period (season by season). Figure S17
shows that both models capture this metric reasonably well in both seasons
compared to MSWEP, but the VHR model tends to overestimate such amounts over
the Southern Hemisphere, except for the Australian domain. In particular,
the strong positive bias of DJF average precipitation over Australia (up to
4 mm d<inline-formula><mml:math id="M55" 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>, Fig. S3, lower panels) cannot be attributed to the positive (higher
than 15 mm d<inline-formula><mml:math id="M56" 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>, Fig. 5 lower panels) bias found for extreme events, but must
be associated with a right shift of the remaining part of the precipitation
distribution, more pronounced for the non-extreme events as partially
confirmed by the positive bias in the 90p metric over the same season
(Fig. S11).</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Summary and conclusions</title>
      <p id="d1e956">The CMCC-CM2-HR4 and CMCC-CM2-VHR4 models are state-of-the-art fully coupled
climate models, participating in different Model Intercomparison Projects
within the 6th Coupled Model Intercomparison Project (CMIP6). The CMCC-CM2-HR4
presents a horizontal resolution typical of most of the models involved in CMIP6
, while CMCC-CM2-VHR4 has a horizontal resolution standard for the
models involved in the High-Resolution Model Intercomparison Project
(HighResMIP). In this paper we highlight the ability of the two models to
represent extreme climate conditions, based on daily and 6-hourly time
series, comparing temperature and precipitation modeled distributions to
the observed ones. In order to have a gridded dataset representative of the
observed climate at the daily and 6-hourly time frequencies, we used ERA5
reanalysis for temperature and MSWEP observations for precipitation. For the
precipitation analysis we also reinforce our investigation on the basis of
the CHIRPS daily observations.</p>
      <p id="d1e959">It is well known that the representation of extreme precipitation indices is
more dependent on the horizontal resolution than what we would expect for
extreme temperature indices (Wei et al., 2019). On average, the
highest resolution CMCC model (VHR) is better than the lower resolution
model (HR) in representing average, intense (90p) and extreme (99p) events
of temperature both in terms of patterns and magnitude. This is true for
daily and 6-hourly based statistics. Also VHR results are quite in agreement
with CMIP6 multi-member average of daily intense and extreme temperature
indices (Scoccimarro and Navarra, 2021). The described differences between
the computed daily and 6-hourly biases in temperature statistics are very
similar for HR and VHR models. This result suggests that a higher horizontal
resolution is not sufficient to improve the representation of extreme
temperature events at the highest time frequency considered. Consequently,
the worsening of model biases in high frequency (6-hourly) temperature
statistics is derived from deficiencies of the current version of model
components and parameterizations in representing high-frequency processes.</p>
      <p id="d1e962">Regarding the precipitation distribution, the VHR model performs better in
representing averages and intense events, but more pronounced biases appear
in VHR compared to HR when focusing on extreme events, with a more evident
degradation in the daily compared to the 6-hourly statistics. This latter
result reduces the confidence usually attributed to the highest horizontal
resolution in modeling extreme precipitation, and is consistent with single
model analysis based on the CAM5.1 atmospheric model (Wehner et al., 2014)
suggesting a positive bias over most of the globe in the representation of
extreme events at <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> horizontal resolution. This is also
in agreement with recent findings (Bador et al., 2020) suggesting that
highest resolution models tend to produce more pronounced extremes than
lower resolution ones. In addition many of them show lower SKILL in
representing observed patterns, both in terms of intensity and spatial
distribution, at the higher resolution, compared to the corresponding
lower resolution version.</p>
      <p id="d1e985">This emphasizes the need to focus not only on the horizontal resolution to
improve the model ability in representing the climate system, but also on
physics and tuning. It is important to note that in the model object of this
analysis the tuning parameters were kept constant, moving from the HR to the
VHR version, in order to be compliant with the HigResMIP protocol.</p>
      <p id="d1e989">The different biases, obtained based on daily and 6-hourly time frequencies,
also suggest that for the set-up of model physics and tuning we need to
consider the event distributions at different time frequencies, to take into
account the representation of the different processes responsible for the
extreme conditions emerging at the different frequencies (Scoccimarro et al., 2015).</p>
      <p id="d1e992">The poor performance of climate models in representing extreme precipitation
was not improved in the last CMIP6 generation models, compared to the
previous CMIP5 generation (Scoccimarro and Gualdi, 2020). In the present work we
have shown that this lack is even more evident when moving to the highest
resolution version of the CMCC-CM2 model adopted for HighResMIP,
consistent with multi-model analyses performed at the same horizontal
resolution (Bador et al., 2020): GCMs whose parameterizations were not
retuned at higher resolution lead to worse results. The high-resolution
version of the model tends to overestimate extreme precipitation in the wet
and warm regions, consistent with findings based on experiments carried
out with the CAM5 atmospheric model at the same resolutions (Wehner et al.,
2014), highlighting once again the importance of an extensive model tuning
at high resolution. In addition it is important to note that moving from
the standard to the high resolution of CMCC-CM2, the model behaves
consistently with the models participating to the HighResMIP project: a
tendency to an increased fraction of land precipitation in the highest
resolution, and the same tendency for the fraction of land precipitation
caused by moisture convergence (Vennière et al., 2019). Also, in the CMCC-CM2
model, the orographic precipitation captures most of the change of
precipitation due to resolution, consistent with most of the HighResMIP models
(Vennière et al., 2019).</p>
      <p id="d1e995">In principle, the horizontal resolution increase should improve the
representation of extreme storms, such as tropical cyclones (Scoccimarro  and Gualdi, 2020) and for this reason also the representation of the associated
short-term extreme precipitation should improve, but this is not the case
for the model object of this study, and it is also confirmed by recent
analysis on the same topic (Wehner et al., 2021).</p>
</sec>

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

      <p id="d1e1002">The code relative to the CMCC-CM2-HR4 and the CMCC-CM2-VHR4 climate models
are available on the Zenodo repository (​​​​​​DOI: <uri>https://doi.org/10.5281/zenodo.5499856</uri>, Scoccimarro et al., 2021). The data relative to the two models are
available through the Earth System Grid Federation (ESGF) data portal (<uri>https:// doi.org/10.22033/ESGF/CMIP6.1359</uri>, Scoccimarro et al., 2017b and <uri>https://doi.org/10.22033/ESGF/CMIP6.1367</uri> Scoccimarro et al., 2017c, respectively). The ERA5 results are available
through the Copernicus data portal (<uri>https://climate.copernicus.eu</uri>, last access: 15 July 2021, Hersbach, <?xmltex \hack{\mbox\bgroup}?>2020​​​​​​​)<?xmltex \hack{\egroup}?>. The CHIRPS observational dataset is available
through the data storage of the University of California in Santa Barbara
(<uri>https://doi.org/10.15780/G2RP4Q</uri>, Funk, 2015).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e1025">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/gmd-15-1841-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/gmd-15-1841-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1034">ES, AB and DP implemented the two model versions and ran the simulations.
PGF supported the implementation of the Aerosol input management routines. TL
prepared the radiative forcing files and supported the model output
postprocessing. SG and AN supported the CMCC-CM2 model implementation phase. ES prepared the article with contributions from all
co-authors.​​​​​​​</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1040">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="d1e1046">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1052">This paper was edited by Sophie Valcke and reviewed by two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><?label 1?><mixed-citation>
Andersson E. and Thépaut, J. N.: ECMWF's 4D-Var data assimilation system –
the genesis and ten years in operations, ECMWF Newsl., 115, 8–12, 2008.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><?label 1?><mixed-citation>Bador, M., Boé, J., Terray, L., Alexander, L. V., Bellucci, A., Haarsma,
R., Koenigk, T., Moine, M.-P., Lohmann, K., Putrasahan, D. A., Roberts, C.,
Roberts, M., Scoccimarro, E., Schiemann, R., Seddon, J., Senan, R., Valcke,
S., and Vanniere, B.: Impact of higher spatial atmospheric resolution on
precipitation extremes over land in global climate models, J.
Geophys. Res.-Atmos, 125, e2019JD032184, <ext-link xlink:href="https://doi.org/10.1029/2019JD032184" ext-link-type="DOI">10.1029/2019JD032184</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><?label 1?><mixed-citation>Beck, H. E., Wood, E. F., Pan, M., Fisher, C. K., Miralles, D. G., van Dijk,
A. I. J. M., McVicar, T. R., and Adler, R. F.: MSWEP V2 Global 3-Hourly
0.1<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> Precipitation: Methodology and Quantitative Assessment,
B. Am. Meteorol. Soc., 100, 473–500, 2019.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><?label 1?><mixed-citation>Bellucci, A.,  Athanasiadis, P. J.,  Scoccimarro, E.,  Ruggieri, P.,  Gualdi, S.,  Fedele, G.,  Haarsma, R. J.,  Garcia-Serrano, J.,  Castrillo, M.,  Putrahasan, D.,  Sanchez-Gomez, E.,  Moine, M.-P.,  Roberts, C. D.,  Roberts, M. J.,  Seddon, J., and  Vidale, P. L.​​​​​​​: Air-Sea interaction over
the Gulf Stream in an ensemble of HighResMIP present climate simulations,
Clim. Dynam., 56, 2093–2111, <ext-link xlink:href="https://doi.org/10.1007/s00382-020-05573-z" ext-link-type="DOI">10.1007/s00382-020-05573-z</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><?label 1?><mixed-citation>Chan, S. C., Kendon, E. J., Fowler, H. J., Blenkinsop, S., Roberts, N. M., and
Ferro, C. A. T.: The Value of High-Resolution Met Office Regional Climate
Models in the Simulation of Multihourly Precipitation Extremes, J. Climate, 27, 6155–6174​​​​​​​, 2014.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><?label 1?><mixed-citation>Cherchi, A.,  Lovato, T.,  Fogli, P. G.,  Peano, D.,  Gualdi, S., Masina, S., Scoccimarro, E.,  Materia, S.,  Iovino, D., and  Navarra, A.: Global mean climate and
main patterns of variability in the CMCC-CM2 coupled model, J.
Adv. Model. Earth Sy., 11, 185–209, <ext-link xlink:href="https://doi.org/10.1029/2018MS001369" ext-link-type="DOI">10.1029/2018MS001369</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><?label 1?><mixed-citation>Crossett, C. C.,  Betts, A. K.,  Dupigny-Giroux, L. A. L., and  Bomblies, A.​​​​​​​: Evaluation of Daily Precipitation from the ERA5 Global
Reanalysis against GHCN Observations in the Northeastern United States,
Climate, 8, 148​​​​​​​, <ext-link xlink:href="https://doi.org/10.3390/cli8120148" ext-link-type="DOI">10.3390/cli8120148</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><?label 1?><mixed-citation> Dee, D. P.,  Uppala, S. M.,  Simmons, A. J.,  Berrisford, P.,  Poli, P.,  Kobayashi, S.,  Andrae, U.,  Balmaseda, M. A.,  Balsamo, G., Bauer, P.,  Bechtold, P.,  Beljaars, A. C. M.,  van de Berg, L.,  Bidlot, J.,  Bormann, N.,  Delsol, C.,  Dragani, R.,  Fuentes, M.,  Geer, A. J., Haimberger, L.,  Healy, S. B.,  Hersbach, H.,  Hólm, E. V.,  Isaksen, L., Kållberg, P.,  Köhler, M.,  Matricardi, M.,  McNally, A. P.,  Monge-Sanz, B. M.,  Morcrette, J.-J.,  Park, B.-K.,  Peubey, C.,  de Rosnay, P.,  Tavolato, C.,  Thépaut, J.-N., and Vitart, F.​​​​​​​: The ERA-Interim reanalysis: configuration and performance of
the data assimilation system, Q. J. Roy. Meteor. Soc., 137, 553–597, 2011.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><?label 1?><mixed-citation>Demory, M.-E., Vidale, P. L., Roberts, M. J., Berrisford, P., Strachan, J.,
Schiemann, R., and Mizielinski, M. S.: The role of horizontal resolution in
simulating drivers of the global hydrological cycle, Clim. Dynam., 42,
2201–2225, <ext-link xlink:href="https://doi.org/10.1007/s00382-013-1924-4" ext-link-type="DOI">10.1007/s00382-013-1924-4</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><?label 1?><mixed-citation>Demory, M.-E., Berthou, S., Fernández, J., Sørland, S. L., Brogli, R., Roberts, M. J., Beyerle, U., Seddon, J., Haarsma, R., Schär, C., Buonomo, E., Christensen, O. B., Ciarlò, J. M., Fealy, R., Nikulin, G., Peano, D., Putrasahan, D., Roberts, C. D., Senan, R., Steger, C., Teichmann, C., and Vautard, R.: European daily precipitation according to EURO-CORDEX regional climate models (RCMs) and high-resolution global climate models (GCMs) from the High-Resolution Model Intercomparison Project (HighResMIP), Geosci. Model Dev., 13, 5485–5506, <ext-link xlink:href="https://doi.org/10.5194/gmd-13-5485-2020" ext-link-type="DOI">10.5194/gmd-13-5485-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><?label 1?><mixed-citation>Eyring, V., Bony, S., Meehl, G. A., Senior, C. A., Stevens, B., Stouffer, R. J., and Taylor, K. E.: Overview of the Coupled Model Intercomparison Project Phase 6 (CMIP6) experimental design and organization, Geosci. Model Dev., 9, 1937–1958, <ext-link xlink:href="https://doi.org/10.5194/gmd-9-1937-2016" ext-link-type="DOI">10.5194/gmd-9-1937-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><?label 1?><mixed-citation>Flato, G., Marotzke, J., Abiodun, B., Braconnot, P., Chou, S. C., Collins, W. J., Cox, P., Driouech, F., Emori, S., Eyring, V., and Forest, C.​​​​​​​: Evaluation of climate models. Climate change 2013: The physical
science basis, Contribution of Working Group I to the Fifth Assessment
Report of the Intergovernmental Panel on Climate Change, 5,  741–866, 2013.</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><?label 1?><mixed-citation>Fogli, P. G. and Iovino, D.: CMCC-CESM-NEMO: toward the new CMCC Earth System
Model, CMCC Research Papers, RP0248, 15 pp., <uri>https://papers.ssrn.com/sol3/papers.cfm?abstract_id=2603176</uri> (last access: 15 July 2021​​​​​​​),  2014.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><?label 1?><mixed-citation>Funk, C.: Climate Hazards Group, Climate Hazards Center [data set], <ext-link xlink:href="https://doi.org/10.15780/G2RP4Q" ext-link-type="DOI">10.15780/G2RP4Q</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><?label 1?><mixed-citation>Funk, C., Peterson P., Landsfeld M., Pedreros D., Verdin J., Shukla S., Husak G., Rowland J., Harrison L., Hoell A., and Michaelsen J.​​​​​​​: The climate hazards infrared
precipitation with stations – a new environmental record for monitoring
extremes, Sci. Data, 2, 150066, <ext-link xlink:href="https://doi.org/10.1038/sdata.2015.66" ext-link-type="DOI">10.1038/sdata.2015.66</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><?label 1?><mixed-citation>Haarsma, R. J., Roberts, M. J., Vidale, P. L., Senior, C. A., Bellucci, A., Bao, Q., Chang, P., Corti, S., Fučkar, N. S., Guemas, V., von Hardenberg, J., Hazeleger, W., Kodama, C., Koenigk, T., Leung, L. R., Lu, J., Luo, J.-J., Mao, J., Mizielinski, M. S., Mizuta, R., Nobre, P., Satoh, M., Scoccimarro, E., Semmler, T., Small, J., and von Storch, J.-S.: High Resolution Model Intercomparison Project (HighResMIP v1.0) for CMIP6, Geosci. Model Dev., 9, 4185–4208, <ext-link xlink:href="https://doi.org/10.5194/gmd-9-4185-2016" ext-link-type="DOI">10.5194/gmd-9-4185-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><?label 1?><mixed-citation>Hersbach, H., Bell, B., Berrisford, P., Hirahara, S., Horányi, A., Muñoz-Sabater, J., Nicolas, J., Peubey, C., Radu, R., Schepers, D., Simmons, A., Soci, C., Abdalla, S., Abellan, X., Balsamo, G., Bechtold, P., Biavati, G., Bidlot, J., Bonavita, M., Chiara, G., Dahlgren, P., Dee, D., Diamantakis, M., Dragani, R., Flemming, J., Forbes, R., Fuentes, M., Geer, A., Haimberger, L., Healy, S., Hogan, R. J., Hólm, E., Janisková, M., Keeley, S., Laloyaux, P., Lopez, P., Lupu, C., Radnoti, G., Rosnay, P., Rozum, I., Vamborg, F., Villaume, S., Thepaut, J.-N.​​​​​​​: The ERA5 global reanalysis, Q. J. Roy. Meteor. Soc., 146, 1999–2049, <ext-link xlink:href="https://doi.org/10.1002/qj.3803" ext-link-type="DOI">10.1002/qj.3803</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib18"><label>18</label><?label 1?><mixed-citation>Hu, G. and Franzke, C. L. E.: Evaluation of daily precipitation extremes in
reanalysis and gridded observation based data sets over Germany, Geophys.
Res. Lett., 47, e2020GL089624, <ext-link xlink:href="https://doi.org/10.1029/2020GL089624" ext-link-type="DOI">10.1029/2020GL089624</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><?label 1?><mixed-citation>Hunke, E. and Lipscomb, W.: CICE: The Los Alamos sea ice model,
documentation and software, version 4.0, Los Alamos National Laboratory,
Technical Report, Los Alamos NM, LA-CC-06-012, 76, 2008.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><?label 1?><mixed-citation>Iles, C. E., Vautard, R., Strachan, J., Joussaume, S., Eggen, B. R., and Hewitt, C. D.: The benefits of increasing resolution in global and regional climate simulations for European climate extremes, Geosci. Model Dev., 13, 5583–5607, <ext-link xlink:href="https://doi.org/10.5194/gmd-13-5583-2020" ext-link-type="DOI">10.5194/gmd-13-5583-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><?label 1?><mixed-citation>Kharin, V. V., Zwiers, F. W., Zhang, X., and Wehner, M.​​​​​​​: Changes in temperature and
precipitation extremes in the CMIP5 ensemble, Climatic Change, 119, 345–357,
<ext-link xlink:href="https://doi.org/10.1007/s10584-013-0705-8" ext-link-type="DOI">10.1007/s10584-013-0705-8</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib22"><label>22</label><?label 1?><mixed-citation>Kopparla, P., Fischer, E. M., Hannay, C., and Knutti, R.: Improved
simulation of extreme precipitation in a high-resolution atmosphere model,
Geophys. Res. Lett., 40, 5803–5808,
<ext-link xlink:href="https://doi.org/10.1002/2013GL057866" ext-link-type="DOI">10.1002/2013GL057866</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><?label 1?><mixed-citation>Li, C., Zwiers, F., Zhang, X., Li, G., Sun, Y., and Wehner, M.: Changes in
Annual Extremes of Daily Temperature and Precipitation in CMIP6 Models,
J. Climate, 34, 3441–3460, 2021.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><?label 1?><mixed-citation>Madec, G. and the NEMO team: NEMO ocean engine – Version 3.6, Tech. Rep., no. 27 Pôle de Modélisation, Institut Pierre-Simon
Laplace (IPSL), France, NEMO ocean engine, NEMO System Team, Scientific Notes of Climate Modelling Center, 27, Institut Pierre-Simon Laplace (IPSL), ISSN 1288-1619, <ext-link xlink:href="https://doi.org/10.5281/zenodo.1464816" ext-link-type="DOI">10.5281/zenodo.1464816</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><?label 1?><mixed-citation>Meredith, E. P., Ulbrich, U., and Rust, H. W.​​​​​​​: Subhourly rainfall in a convection-permitting model,
Environ. Res. Lett., 15, 034031, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/ab6787" ext-link-type="DOI">10.1088/1748-9326/ab6787</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><?label 1?><mixed-citation>Neale, R. B. , Richter, J. H., Conley, A. J., Park, S., Lauritzen, P. H., Gettelman, A., Williamson, D. L., Rasch, P. J., Vavrus, S. J., Taylor, M. A., Collins, W. D., Zhang, M., and Lin, S.​​​​​​​: Description of the NCAR Community Atmosphere
Model (CAM4.0), NCAR Tech. Note, NCAR/TN-4851STR, 212 pp., 2010.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><?label 1?><mixed-citation>Oleson, K. W., Lawrence, D. M., Bonan, G. B., Drewniak, B., Huang, M.,
Koven, C. D., Levis, S., Li, F., Riley, W. J.,  Subin, Z. M.,  Swenson, S. C., and Thornton, P. E.​​​​​​​: Technical description of version 4.5 of the Community
Land Model (CLM), NCAR Technical Note, NCAR/TN-503+STR, 2013.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><?label 1?><mixed-citation>Raymond, D. J. and  Blyth, A. M.: A stochastic mixing model for
non-precipitating cumulus clouds, J. Atmos. Sci., 43, 2708–2718, 1986.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><?label 1?><mixed-citation>Raymond, D. J. and  Blyth, A. M.: Extension of the stochastic mixing model to
cumulonimbus clouds, J. Atmos. Sci., 49, 1968–1983, 1992.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><?label 1?><mixed-citation>Richter, J. H. and  Rasch, P. J.: Effects of convective momentum transport on
the atmospheric circulation in the community atmosphere model, version 3, J.
Climate, 21, 1487–1499, 2008.</mixed-citation></ref>
      <ref id="bib1.bib31"><label>31</label><?label 1?><mixed-citation>Rivoire, P., Martius, O., and Naveau, P.: A comparison of moderate and
extreme ERA-5 daily precipitation with two observational data sets, Earth
and Space Science, 8, e2020EA001633, <ext-link xlink:href="https://doi.org/10.1029/2020EA001633" ext-link-type="DOI">10.1029/2020EA001633</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bib32"><label>32</label><?label 1?><mixed-citation>Schindler A.,  Toreti, A.,  Zampieri, M.,  Scoccimarro, E.,  Gualdi, S.,  Fukutome, S., Xoplaki, E., and Luterbacher, J.: On the internal variability of simulated daily
precipitation, J. Climate, 28, 3624–3630, <ext-link xlink:href="https://doi.org/10.1175/JCLI-D-14-00745.1" ext-link-type="DOI">10.1175/JCLI-D-14-00745.1</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><?label 1?><mixed-citation>Scoccimarro, E. and Gualdi, S.: Heavy Daily Precipitation Events in the CMIP6
Worst-Case Scenario: Projected Twenty-First-Century Changes, J.
Climate, 33, 7631–7642, <ext-link xlink:href="https://doi.org/10.1175/JCLI-D-19-0940.1" ext-link-type="DOI">10.1175/JCLI-D-19-0940.1</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib34"><label>34</label><?label 1?><mixed-citation>Scoccimarro, E. and Navarra, A.: Precipitation and temperature extremes in a
changing climate, in: Hydrometeorological Extreme Events and
Public Health, 1st edn., chap. 2, edited by: Matthies, F., Wiley book, 320 pp., ISBN 978-1-119-25930-5, 2021.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><?label 1?><mixed-citation>Scoccimarro, E.,  Gualdi, S.,  Bellucci, A.,  Zampieri, M., and  Navarra, A.: Heavy
precipitation events in a warmer climate: results from CMIP5 models, J.
Climate, 26, 7902–7911, <ext-link xlink:href="https://doi.org/10.1175/JCLI-D-12-00850.1" ext-link-type="DOI">10.1175/JCLI-D-12-00850.1</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><?label 1?><mixed-citation>Scoccimarro, E.,  Villarini, G., Vichi, M.,  Zampieri, M., Fogli,  P. G., Bellucci, A., and Gualdi, S.: Projected changes in intense precipitation over Europe at the
daily and sub-daily time scales, J. Climate, 28,  6193–6203, <ext-link xlink:href="https://doi.org/10.1175/JCLI-D-14-00779.1" ext-link-type="DOI">10.1175/JCLI-D-14-00779.1</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><?label 1?><mixed-citation>Scoccimarro, E.,  Gualdi, S.,  Bellucci, A.,  Zampieri, M., and Navarra, A.: Heavy
precipitation events over the Euro-Mediterranean region in a warmer climate:
results from CMIP5 models, Reg. Environ. Change, 16, 595–602, <ext-link xlink:href="https://doi.org/10.1007/s10113-014-0712-y" ext-link-type="DOI">10.1007/s10113-014-0712-y</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><?label 1?><mixed-citation>Scoccimarro, E.,  Fogli, P. G.,  Reed, K.,  Gualdi, S., Masina, S., and Navarra, A.:
Tropical cyclone interaction with the ocean: the role of high frequency
(sub-daily) coupled processes, J. Climate, 30,  145–162, <ext-link xlink:href="https://doi.org/10.1175/JCLI-D-16-0292.1" ext-link-type="DOI">10.1175/JCLI-D-16-0292.1</ext-link>, 2017a.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><?label 1?><mixed-citation>Scoccimarro, E., Bellucci, A., and Peano, D.: CMCC CMCC-CM2-HR4 model output
prepared for CMIP6 HighResMIP hist-1950, Earth System Grid Federation [data set],
<ext-link xlink:href="https://doi.org/10.22033/ESGF/CMIP6.1359" ext-link-type="DOI">10.22033/ESGF/CMIP6.1359</ext-link>, 2017b.</mixed-citation></ref>
      <ref id="bib1.bib40"><label>40</label><?label 1?><mixed-citation>Scoccimarro, E.,  Bellucci, A., and Peano, D.: CMCC CMCC-CM2-VHR4 model output
prepared for CMIP6 HighResMIP, Earth System Grid Federation [data set],
<ext-link xlink:href="https://doi.org/10.22033/ESGF/CMIP6.1367" ext-link-type="DOI">10.22033/ESGF/CMIP6.1367</ext-link>, 2017c.</mixed-citation></ref>
      <ref id="bib1.bib41"><label>41</label><?label 1?><mixed-citation>Scoccimarro, E., Gualdi, S., Bellucci, A., Peano, D.,
Cherchi, A., Vecchi, G. A., and Navarra, A.: The
typhoon-induced drying of the Maritime Continent, PNAS, 117, 3983–3988, <ext-link xlink:href="https://doi.org/10.1073/pnas.1915364117" ext-link-type="DOI">10.1073/pnas.1915364117</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib42"><label>42</label><?label 1?><mixed-citation>Scoccimarro, E., Peano, D., Gualdi, S., Bellucci, A., Lovato, T., Fogli, P. G., and Navarra, A.: CMCC-Foundation/CMCC-CM2-HighResMIP: CMCC-CM2-HighResMIP code for CMIP6 (cmip6-code), Zenodo [data set], <ext-link xlink:href="https://doi.org/10.5281/zenodo.5499856" ext-link-type="DOI">10.5281/zenodo.5499856</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bib43"><label>43</label><?label 1?><mixed-citation>Terai, C. R., Caldwell, P. M., Klein, S. A. Tang, Q., and Branstetter, M.
L.: The atmospheric hydrologic cycle in the ACME v0.3 model, Clim. Dynam.,
50, 3251–3279, <ext-link xlink:href="https://doi.org/10.1007/s00382-017-3803-x" ext-link-type="DOI">10.1007/s00382-017-3803-x</ext-link>,
2018.</mixed-citation></ref>
      <ref id="bib1.bib44"><label>44</label><?label 1?><mixed-citation>Van Haren, R., Haarsma, R. J., de Vries, H., van Oldenborgh, G. J., and
Hazeleger, W.: Resolution dependence of circulation forcedfuture central
European summer drying, Environ. Res. Lett., 10, 055002,
<ext-link xlink:href="https://doi.org/10.1088/1748-9326/10/5/055002" ext-link-type="DOI">10.1088/1748-9326/10/5/055002</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib45"><label>45</label><?label 1?><mixed-citation>Vannière, B., Vidale, P. L., Demory, M.-E., Schiemann, R., Roberts, M. J.,
Roberts, C. D., Matsueda, M., Terray, L., Koenigk, T., and Senan, R.:
Multi-model evaluation of the sensitivity of the global energy budget and
hydrological cycle to resolution, Clim. Dynam., 52, 6817–6846, <ext-link xlink:href="https://doi.org/10.1007/s00382-018-4547-y" ext-link-type="DOI">10.1007/s00382-018-4547-y</ext-link>, 2019.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib46"><label>46</label><?label 1?><mixed-citation>Wang, X. and Zhang, M.: An analysis of parameterization interactions and
sensitivity of single-column model simulations to convection schemes in CAM4
and CAM5, J. Geophys. Res.-Atmos., 118, 8869–8880, <ext-link xlink:href="https://doi.org/10.1002/jgrd.50690" ext-link-type="DOI">10.1002/jgrd.50690</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib47"><label>47</label><?label 1?><mixed-citation>Wehner, M. F., Reed, K. A., Li, F., Bacmeister, P. J., Chen, C. T., Paciorek, C., Gleckler, P. J., Sperber, K. R., Collins, W. D., Gettelman, A., and Jablonowski, C.​​​​​​​: The effect of horizontal resolution on simulation
quality in the Community Atmospheric Model, CAM5.1, J. Adv. Model. Earth
Sy., 6, 980–997, <ext-link xlink:href="https://doi.org/10.1002/2013MS000276" ext-link-type="DOI">10.1002/2013MS000276</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib48"><label>48</label><?label 1?><mixed-citation>Wehner, M., Lee, J., Risser, M., Ullrich, P., Gleckler, P., and Collins, W. D.:
Evaluation of extreme sub-daily precipitation in high-resolution global
climate model simulations, Philos. Tr. R. Soc. A., 379,
20190545, <ext-link xlink:href="https://doi.org/10.1098/rsta.2019.0545" ext-link-type="DOI">10.1098/rsta.2019.0545</ext-link>, 2021.</mixed-citation></ref>
      <ref id="bib1.bib49"><label>49</label><?label 1?><mixed-citation>Wei, L.,  Xin, X.,  Xiao, C., Li, Y., Wu, Y., and Tang, H.​​​​​​​: Performance of BCC-CSM Models with
Different Horizontal Resolutions in Simulating Extreme Climate Events in
China, J. Meteor. Res., 33, 720–733, <ext-link xlink:href="https://doi.org/10.1007/s13351-019-8159-1" ext-link-type="DOI">10.1007/s13351-019-8159-1</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib50"><label>50</label><?label 1?><mixed-citation>Zhang, G. J. and  McFarlane, N. A.: Sensitivity of climate simulations to the
parameterization of cumulus convection in the Canadian Climate Centre
general circulation model, Atmos. Ocean, 33, 407–446, 1995.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Extreme events representation in CMCC-CM2 standard and high-resolution general circulation models</article-title-html>
<abstract-html/>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Andersson E. and Thépaut, J. N.: ECMWF's 4D-Var data assimilation system –
the genesis and ten years in operations, ECMWF Newsl., 115, 8–12, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>Bador, M., Boé, J., Terray, L., Alexander, L. V., Bellucci, A., Haarsma,
R., Koenigk, T., Moine, M.-P., Lohmann, K., Putrasahan, D. A., Roberts, C.,
Roberts, M., Scoccimarro, E., Schiemann, R., Seddon, J., Senan, R., Valcke,
S., and Vanniere, B.: Impact of higher spatial atmospheric resolution on
precipitation extremes over land in global climate models, J.
Geophys. Res.-Atmos, 125, e2019JD032184, <a href="https://doi.org/10.1029/2019JD032184" target="_blank">https://doi.org/10.1029/2019JD032184</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>Beck, H. E., Wood, E. F., Pan, M., Fisher, C. K., Miralles, D. G., van Dijk,
A. I. J. M., McVicar, T. R., and Adler, R. F.: MSWEP V2 Global 3-Hourly
0.1° Precipitation: Methodology and Quantitative Assessment,
B. Am. Meteorol. Soc., 100, 473–500, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>Bellucci, A.,  Athanasiadis, P. J.,  Scoccimarro, E.,  Ruggieri, P.,  Gualdi, S.,  Fedele, G.,  Haarsma, R. J.,  Garcia-Serrano, J.,  Castrillo, M.,  Putrahasan, D.,  Sanchez-Gomez, E.,  Moine, M.-P.,  Roberts, C. D.,  Roberts, M. J.,  Seddon, J., and  Vidale, P. L.​​​​​​​: Air-Sea interaction over
the Gulf Stream in an ensemble of HighResMIP present climate simulations,
Clim. Dynam., 56, 2093–2111, <a href="https://doi.org/10.1007/s00382-020-05573-z" target="_blank">https://doi.org/10.1007/s00382-020-05573-z</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>Chan, S. C., Kendon, E. J., Fowler, H. J., Blenkinsop, S., Roberts, N. M., and
Ferro, C. A. T.: The Value of High-Resolution Met Office Regional Climate
Models in the Simulation of Multihourly Precipitation Extremes, J. Climate, 27, 6155–6174​​​​​​​, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>Cherchi, A.,  Lovato, T.,  Fogli, P. G.,  Peano, D.,  Gualdi, S., Masina, S., Scoccimarro, E.,  Materia, S.,  Iovino, D., and  Navarra, A.: Global mean climate and
main patterns of variability in the CMCC-CM2 coupled model, J.
Adv. Model. Earth Sy., 11, 185–209, <a href="https://doi.org/10.1029/2018MS001369" target="_blank">https://doi.org/10.1029/2018MS001369</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>Crossett, C. C.,  Betts, A. K.,  Dupigny-Giroux, L. A. L., and  Bomblies, A.​​​​​​​: Evaluation of Daily Precipitation from the ERA5 Global
Reanalysis against GHCN Observations in the Northeastern United States,
Climate, 8, 148​​​​​​​, <a href="https://doi.org/10.3390/cli8120148" target="_blank">https://doi.org/10.3390/cli8120148</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation> Dee, D. P.,  Uppala, S. M.,  Simmons, A. J.,  Berrisford, P.,  Poli, P.,  Kobayashi, S.,  Andrae, U.,  Balmaseda, M. A.,  Balsamo, G., Bauer, P.,  Bechtold, P.,  Beljaars, A. C. M.,  van de Berg, L.,  Bidlot, J.,  Bormann, N.,  Delsol, C.,  Dragani, R.,  Fuentes, M.,  Geer, A. J., Haimberger, L.,  Healy, S. B.,  Hersbach, H.,  Hólm, E. V.,  Isaksen, L., Kållberg, P.,  Köhler, M.,  Matricardi, M.,  McNally, A. P.,  Monge-Sanz, B. M.,  Morcrette, J.-J.,  Park, B.-K.,  Peubey, C.,  de Rosnay, P.,  Tavolato, C.,  Thépaut, J.-N., and Vitart, F.​​​​​​​: The ERA-Interim reanalysis: configuration and performance of
the data assimilation system, Q. J. Roy. Meteor. Soc., 137, 553–597, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>Demory, M.-E., Vidale, P. L., Roberts, M. J., Berrisford, P., Strachan, J.,
Schiemann, R., and Mizielinski, M. S.: The role of horizontal resolution in
simulating drivers of the global hydrological cycle, Clim. Dynam., 42,
2201–2225, <a href="https://doi.org/10.1007/s00382-013-1924-4" target="_blank">https://doi.org/10.1007/s00382-013-1924-4</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>Demory, M.-E., Berthou, S., Fernández, J., Sørland, S. L., Brogli, R., Roberts, M. J., Beyerle, U., Seddon, J., Haarsma, R., Schär, C., Buonomo, E., Christensen, O. B., Ciarlò, J. M., Fealy, R., Nikulin, G., Peano, D., Putrasahan, D., Roberts, C. D., Senan, R., Steger, C., Teichmann, C., and Vautard, R.: European daily precipitation according to EURO-CORDEX regional climate models (RCMs) and high-resolution global climate models (GCMs) from the High-Resolution Model Intercomparison Project (HighResMIP), Geosci. Model Dev., 13, 5485–5506, <a href="https://doi.org/10.5194/gmd-13-5485-2020" target="_blank">https://doi.org/10.5194/gmd-13-5485-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>Eyring, V., Bony, S., Meehl, G. A., Senior, C. A., Stevens, B., Stouffer, R. J., and Taylor, K. E.: Overview of the Coupled Model Intercomparison Project Phase 6 (CMIP6) experimental design and organization, Geosci. Model Dev., 9, 1937–1958, <a href="https://doi.org/10.5194/gmd-9-1937-2016" target="_blank">https://doi.org/10.5194/gmd-9-1937-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>Flato, G., Marotzke, J., Abiodun, B., Braconnot, P., Chou, S. C., Collins, W. J., Cox, P., Driouech, F., Emori, S., Eyring, V., and Forest, C.​​​​​​​: Evaluation of climate models. Climate change 2013: The physical
science basis, Contribution of Working Group I to the Fifth Assessment
Report of the Intergovernmental Panel on Climate Change, 5,  741–866, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>Fogli, P. G. and Iovino, D.: CMCC-CESM-NEMO: toward the new CMCC Earth System
Model, CMCC Research Papers, RP0248, 15 pp., <a href="https://papers.ssrn.com/sol3/papers.cfm?abstract_id=2603176" target="_blank"/> (last access: 15 July 2021​​​​​​​),  2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>Funk, C.: Climate Hazards Group, Climate Hazards Center [data set], <a href="https://doi.org/10.15780/G2RP4Q" target="_blank">https://doi.org/10.15780/G2RP4Q</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>Funk, C., Peterson P., Landsfeld M., Pedreros D., Verdin J., Shukla S., Husak G., Rowland J., Harrison L., Hoell A., and Michaelsen J.​​​​​​​: The climate hazards infrared
precipitation with stations – a new environmental record for monitoring
extremes, Sci. Data, 2, 150066, <a href="https://doi.org/10.1038/sdata.2015.66" target="_blank">https://doi.org/10.1038/sdata.2015.66</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>Haarsma, R. J., Roberts, M. J., Vidale, P. L., Senior, C. A., Bellucci, A., Bao, Q., Chang, P., Corti, S., Fučkar, N. S., Guemas, V., von Hardenberg, J., Hazeleger, W., Kodama, C., Koenigk, T., Leung, L. R., Lu, J., Luo, J.-J., Mao, J., Mizielinski, M. S., Mizuta, R., Nobre, P., Satoh, M., Scoccimarro, E., Semmler, T., Small, J., and von Storch, J.-S.: High Resolution Model Intercomparison Project (HighResMIP v1.0) for CMIP6, Geosci. Model Dev., 9, 4185–4208, <a href="https://doi.org/10.5194/gmd-9-4185-2016" target="_blank">https://doi.org/10.5194/gmd-9-4185-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>Hersbach, H., Bell, B., Berrisford, P., Hirahara, S., Horányi, A., Muñoz-Sabater, J., Nicolas, J., Peubey, C., Radu, R., Schepers, D., Simmons, A., Soci, C., Abdalla, S., Abellan, X., Balsamo, G., Bechtold, P., Biavati, G., Bidlot, J., Bonavita, M., Chiara, G., Dahlgren, P., Dee, D., Diamantakis, M., Dragani, R., Flemming, J., Forbes, R., Fuentes, M., Geer, A., Haimberger, L., Healy, S., Hogan, R. J., Hólm, E., Janisková, M., Keeley, S., Laloyaux, P., Lopez, P., Lupu, C., Radnoti, G., Rosnay, P., Rozum, I., Vamborg, F., Villaume, S., Thepaut, J.-N.​​​​​​​: The ERA5 global reanalysis, Q. J. Roy. Meteor. Soc., 146, 1999–2049, <a href="https://doi.org/10.1002/qj.3803" target="_blank">https://doi.org/10.1002/qj.3803</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation>Hu, G. and Franzke, C. L. E.: Evaluation of daily precipitation extremes in
reanalysis and gridded observation based data sets over Germany, Geophys.
Res. Lett., 47, e2020GL089624, <a href="https://doi.org/10.1029/2020GL089624" target="_blank">https://doi.org/10.1029/2020GL089624</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation>Hunke, E. and Lipscomb, W.: CICE: The Los Alamos sea ice model,
documentation and software, version 4.0, Los Alamos National Laboratory,
Technical Report, Los Alamos NM, LA-CC-06-012, 76, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation>Iles, C. E., Vautard, R., Strachan, J., Joussaume, S., Eggen, B. R., and Hewitt, C. D.: The benefits of increasing resolution in global and regional climate simulations for European climate extremes, Geosci. Model Dev., 13, 5583–5607, <a href="https://doi.org/10.5194/gmd-13-5583-2020" target="_blank">https://doi.org/10.5194/gmd-13-5583-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation>Kharin, V. V., Zwiers, F. W., Zhang, X., and Wehner, M.​​​​​​​: Changes in temperature and
precipitation extremes in the CMIP5 ensemble, Climatic Change, 119, 345–357,
<a href="https://doi.org/10.1007/s10584-013-0705-8" target="_blank">https://doi.org/10.1007/s10584-013-0705-8</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation>Kopparla, P., Fischer, E. M., Hannay, C., and Knutti, R.: Improved
simulation of extreme precipitation in a high-resolution atmosphere model,
Geophys. Res. Lett., 40, 5803–5808,
<a href="https://doi.org/10.1002/2013GL057866" target="_blank">https://doi.org/10.1002/2013GL057866</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation>Li, C., Zwiers, F., Zhang, X., Li, G., Sun, Y., and Wehner, M.: Changes in
Annual Extremes of Daily Temperature and Precipitation in CMIP6 Models,
J. Climate, 34, 3441–3460, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation>Madec, G. and the NEMO team: NEMO ocean engine – Version 3.6, Tech. Rep., no. 27 Pôle de Modélisation, Institut Pierre-Simon
Laplace (IPSL), France, NEMO ocean engine, NEMO System Team, Scientific Notes of Climate Modelling Center, 27, Institut Pierre-Simon Laplace (IPSL), ISSN 1288-1619, <a href="https://doi.org/10.5281/zenodo.1464816" target="_blank">https://doi.org/10.5281/zenodo.1464816</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation>Meredith, E. P., Ulbrich, U., and Rust, H. W.​​​​​​​: Subhourly rainfall in a convection-permitting model,
Environ. Res. Lett., 15, 034031, <a href="https://doi.org/10.1088/1748-9326/ab6787" target="_blank">https://doi.org/10.1088/1748-9326/ab6787</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>Neale, R. B. , Richter, J. H., Conley, A. J., Park, S., Lauritzen, P. H., Gettelman, A., Williamson, D. L., Rasch, P. J., Vavrus, S. J., Taylor, M. A., Collins, W. D., Zhang, M., and Lin, S.​​​​​​​: Description of the NCAR Community Atmosphere
Model (CAM4.0), NCAR Tech. Note, NCAR/TN-4851STR, 212 pp., 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation>Oleson, K. W., Lawrence, D. M., Bonan, G. B., Drewniak, B., Huang, M.,
Koven, C. D., Levis, S., Li, F., Riley, W. J.,  Subin, Z. M.,  Swenson, S. C., and Thornton, P. E.​​​​​​​: Technical description of version 4.5 of the Community
Land Model (CLM), NCAR Technical Note, NCAR/TN-503+STR, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation>Raymond, D. J. and  Blyth, A. M.: A stochastic mixing model for
non-precipitating cumulus clouds, J. Atmos. Sci., 43, 2708–2718, 1986.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation>Raymond, D. J. and  Blyth, A. M.: Extension of the stochastic mixing model to
cumulonimbus clouds, J. Atmos. Sci., 49, 1968–1983, 1992.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation>Richter, J. H. and  Rasch, P. J.: Effects of convective momentum transport on
the atmospheric circulation in the community atmosphere model, version 3, J.
Climate, 21, 1487–1499, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation>Rivoire, P., Martius, O., and Naveau, P.: A comparison of moderate and
extreme ERA-5 daily precipitation with two observational data sets, Earth
and Space Science, 8, e2020EA001633, <a href="https://doi.org/10.1029/2020EA001633" target="_blank">https://doi.org/10.1029/2020EA001633</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation>Schindler A.,  Toreti, A.,  Zampieri, M.,  Scoccimarro, E.,  Gualdi, S.,  Fukutome, S., Xoplaki, E., and Luterbacher, J.: On the internal variability of simulated daily
precipitation, J. Climate, 28, 3624–3630, <a href="https://doi.org/10.1175/JCLI-D-14-00745.1" target="_blank">https://doi.org/10.1175/JCLI-D-14-00745.1</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation>Scoccimarro, E. and Gualdi, S.: Heavy Daily Precipitation Events in the CMIP6
Worst-Case Scenario: Projected Twenty-First-Century Changes, J.
Climate, 33, 7631–7642, <a href="https://doi.org/10.1175/JCLI-D-19-0940.1" target="_blank">https://doi.org/10.1175/JCLI-D-19-0940.1</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation>Scoccimarro, E. and Navarra, A.: Precipitation and temperature extremes in a
changing climate, in: Hydrometeorological Extreme Events and
Public Health, 1st edn., chap. 2, edited by: Matthies, F., Wiley book, 320 pp., ISBN 978-1-119-25930-5, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation>Scoccimarro, E.,  Gualdi, S.,  Bellucci, A.,  Zampieri, M., and  Navarra, A.: Heavy
precipitation events in a warmer climate: results from CMIP5 models, J.
Climate, 26, 7902–7911, <a href="https://doi.org/10.1175/JCLI-D-12-00850.1" target="_blank">https://doi.org/10.1175/JCLI-D-12-00850.1</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation>Scoccimarro, E.,  Villarini, G., Vichi, M.,  Zampieri, M., Fogli,  P. G., Bellucci, A., and Gualdi, S.: Projected changes in intense precipitation over Europe at the
daily and sub-daily time scales, J. Climate, 28,  6193–6203, <a href="https://doi.org/10.1175/JCLI-D-14-00779.1" target="_blank">https://doi.org/10.1175/JCLI-D-14-00779.1</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation>Scoccimarro, E.,  Gualdi, S.,  Bellucci, A.,  Zampieri, M., and Navarra, A.: Heavy
precipitation events over the Euro-Mediterranean region in a warmer climate:
results from CMIP5 models, Reg. Environ. Change, 16, 595–602, <a href="https://doi.org/10.1007/s10113-014-0712-y" target="_blank">https://doi.org/10.1007/s10113-014-0712-y</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>Scoccimarro, E.,  Fogli, P. G.,  Reed, K.,  Gualdi, S., Masina, S., and Navarra, A.:
Tropical cyclone interaction with the ocean: the role of high frequency
(sub-daily) coupled processes, J. Climate, 30,  145–162, <a href="https://doi.org/10.1175/JCLI-D-16-0292.1" target="_blank">https://doi.org/10.1175/JCLI-D-16-0292.1</a>, 2017a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>Scoccimarro, E., Bellucci, A., and Peano, D.: CMCC CMCC-CM2-HR4 model output
prepared for CMIP6 HighResMIP hist-1950, Earth System Grid Federation [data set],
<a href="https://doi.org/10.22033/ESGF/CMIP6.1359" target="_blank">https://doi.org/10.22033/ESGF/CMIP6.1359</a>, 2017b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>40</label><mixed-citation>Scoccimarro, E.,  Bellucci, A., and Peano, D.: CMCC CMCC-CM2-VHR4 model output
prepared for CMIP6 HighResMIP, Earth System Grid Federation [data set],
<a href="https://doi.org/10.22033/ESGF/CMIP6.1367" target="_blank">https://doi.org/10.22033/ESGF/CMIP6.1367</a>, 2017c.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>41</label><mixed-citation>Scoccimarro, E., Gualdi, S., Bellucci, A., Peano, D.,
Cherchi, A., Vecchi, G. A., and Navarra, A.: The
typhoon-induced drying of the Maritime Continent, PNAS, 117, 3983–3988, <a href="https://doi.org/10.1073/pnas.1915364117" target="_blank">https://doi.org/10.1073/pnas.1915364117</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>42</label><mixed-citation>Scoccimarro, E., Peano, D., Gualdi, S., Bellucci, A., Lovato, T., Fogli, P. G., and Navarra, A.: CMCC-Foundation/CMCC-CM2-HighResMIP: CMCC-CM2-HighResMIP code for CMIP6 (cmip6-code), Zenodo [data set], <a href="https://doi.org/10.5281/zenodo.5499856" target="_blank">https://doi.org/10.5281/zenodo.5499856</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>43</label><mixed-citation>Terai, C. R., Caldwell, P. M., Klein, S. A. Tang, Q., and Branstetter, M.
L.: The atmospheric hydrologic cycle in the ACME v0.3 model, Clim. Dynam.,
50, 3251–3279, <a href="https://doi.org/10.1007/s00382-017-3803-x" target="_blank">https://doi.org/10.1007/s00382-017-3803-x</a>,
2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>44</label><mixed-citation>Van Haren, R., Haarsma, R. J., de Vries, H., van Oldenborgh, G. J., and
Hazeleger, W.: Resolution dependence of circulation forcedfuture central
European summer drying, Environ. Res. Lett., 10, 055002,
<a href="https://doi.org/10.1088/1748-9326/10/5/055002" target="_blank">https://doi.org/10.1088/1748-9326/10/5/055002</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>45</label><mixed-citation>Vannière, B., Vidale, P. L., Demory, M.-E., Schiemann, R., Roberts, M. J.,
Roberts, C. D., Matsueda, M., Terray, L., Koenigk, T., and Senan, R.:
Multi-model evaluation of the sensitivity of the global energy budget and
hydrological cycle to resolution, Clim. Dynam., 52, 6817–6846, <a href="https://doi.org/10.1007/s00382-018-4547-y" target="_blank">https://doi.org/10.1007/s00382-018-4547-y</a>, 2019.

</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>46</label><mixed-citation>Wang, X. and Zhang, M.: An analysis of parameterization interactions and
sensitivity of single-column model simulations to convection schemes in CAM4
and CAM5, J. Geophys. Res.-Atmos., 118, 8869–8880, <a href="https://doi.org/10.1002/jgrd.50690" target="_blank">https://doi.org/10.1002/jgrd.50690</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>47</label><mixed-citation>Wehner, M. F., Reed, K. A., Li, F., Bacmeister, P. J., Chen, C. T., Paciorek, C., Gleckler, P. J., Sperber, K. R., Collins, W. D., Gettelman, A., and Jablonowski, C.​​​​​​​: The effect of horizontal resolution on simulation
quality in the Community Atmospheric Model, CAM5.1, J. Adv. Model. Earth
Sy., 6, 980–997, <a href="https://doi.org/10.1002/2013MS000276" target="_blank">https://doi.org/10.1002/2013MS000276</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>48</label><mixed-citation>Wehner, M., Lee, J., Risser, M., Ullrich, P., Gleckler, P., and Collins, W. D.:
Evaluation of extreme sub-daily precipitation in high-resolution global
climate model simulations, Philos. Tr. R. Soc. A., 379,
20190545, <a href="https://doi.org/10.1098/rsta.2019.0545" target="_blank">https://doi.org/10.1098/rsta.2019.0545</a>, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>49</label><mixed-citation>Wei, L.,  Xin, X.,  Xiao, C., Li, Y., Wu, Y., and Tang, H.​​​​​​​: Performance of BCC-CSM Models with
Different Horizontal Resolutions in Simulating Extreme Climate Events in
China, J. Meteor. Res., 33, 720–733, <a href="https://doi.org/10.1007/s13351-019-8159-1" target="_blank">https://doi.org/10.1007/s13351-019-8159-1</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>50</label><mixed-citation>Zhang, G. J. and  McFarlane, N. A.: Sensitivity of climate simulations to the
parameterization of cumulus convection in the Canadian Climate Centre
general circulation model, Atmos. Ocean, 33, 407–446, 1995.
</mixed-citation></ref-html>--></article>
