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<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">
  <front>
    <journal-meta><journal-id journal-id-type="publisher">ESD</journal-id><journal-title-group>
    <journal-title>Earth System Dynamics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ESD</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Earth Syst. Dynam.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2190-4987</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/esd-10-189-2019</article-id><title-group><article-title><?xmltex \hack{\vspace*{3mm}}?> September Arctic sea ice minimum prediction <?xmltex \hack{\break}?> – a skillful new statistical approach</article-title><alt-title>September Arctic sea ice minimum prediction – a new skillful statistical approach</alt-title>
      </title-group><?xmltex \runningtitle{September Arctic sea ice minimum prediction -- a new skillful statistical approach}?><?xmltex \runningauthor{M.~Ionita et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Ionita</surname><given-names>Monica</given-names></name>
          <email>monica.ionita@awi.de</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Grosfeld</surname><given-names>Klaus</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Scholz</surname><given-names>Patrick</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2692-7624</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Treffeisen</surname><given-names>Renate</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Lohmann</surname><given-names>Gerrit</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2089-733X</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Alfred Wegener Institute, Helmholtz Centre for Polar and Marine Research, Bremerhaven, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>MARUM – Center for Marine Environmental Sciences, University of Bremen, Bremen, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Monica Ionita (monica.ionita@awi.de)</corresp></author-notes><pub-date><day>21</day><month>March</month><year>2019</year></pub-date>
      
      <volume>10</volume>
      <issue>1</issue>
      <fpage>189</fpage><lpage>203</lpage>
      <history>
        <date date-type="received"><day>16</day><month>August</month><year>2018</year></date>
           <date date-type="rev-request"><day>20</day><month>September</month><year>2018</year></date>
           <date date-type="rev-recd"><day>27</day><month>February</month><year>2019</year></date>
           <date date-type="accepted"><day>8</day><month>March</month><year>2019</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2019 Monica Ionita et al.</copyright-statement>
        <copyright-year>2019</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019.html">This article is available from https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019.html</self-uri><self-uri xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019.pdf">The full text article is available as a PDF file from https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e126">Sea ice in both polar regions is an important indicator of the
expression of global climate change and its polar amplification.
Consequently, broad interest exists on sea ice coverage, variability and
long-term change. However, its predictability is complex and it depends
strongly on different atmospheric and oceanic parameters. In order to
provide insights into the potential development of a monthly/seasonal signal
of sea ice evolution, we applied a robust statistical model based on
different oceanic and atmospheric parameters to calculate an estimate of the
September sea ice extent (SSIE) on a monthly timescale. Although previous
statistical attempts of monthly/seasonal SSIE forecasts show a relatively
reduced skill, when the trend is removed, we show here that the September
sea ice extent has a high predictive skill, up to 4 months ahead, based on
previous months' oceanic and atmospheric conditions. Our statistical model
skillfully captures the interannual variability of the SSIE and could
provide a valuable tool for identifying relevant regions and oceanic and
atmospheric parameters that are important for the sea ice development in the
Arctic and for detecting sensitive/critical regions in global coupled
climate models with a focus on sea ice formation.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e136">Arctic sea ice plays an important role in modulating the global climate
system by influencing the atmospheric and oceanic circulation in polar
regions. Moreover, it has a strong impact also on the global economic system
through changes in marine and natural resources development. The sea ice
extent over the Arctic region has undergone an extraordinary decline during
the last decades that can be linked to climate change (Allison et al., 2009;
Kay et al., 2011; Notz and Marotzke, 2012; Stroeve and Notz, 2018). The
trends in the Arctic sea ice extent are negative for all months, with the
largest trend recorded at the end of the melt season in September (Serreze
et al., 2007), with an average decline of 12.9 % per decade relative to
the long-term mean of 1981–2010 September average (Cavalieri and Parkinson,
2012; Comiso et al., 2017). These negative trends, with their environmental
and economic implications as well as its impacts on human society, have led
to a rising demand for accurate sea ice predictions at monthly, seasonal and up
to decadal timescales, which in turn will be able to address the growing
demands from different stakeholders and the scientific community (Meier et
al., 2014). As such, an accurate sea ice prediction plays a crucial role for
ecosystems, coastal communities, planning for new shipping ports, oil and
gas exploration and marine transportation. The 10 lowest September sea ice
extents all occurred in the past 10 years, and climate projections indicate
that the Arctic Ocean could be ice free (sea ice less than <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>
for at least 5 consecutive years) in September in the
second half of the 21st century (IPCC, 2013). As a result, the ship
traffic and Arctic resources extraction have already increased (Pizzolato et
al., 2014). For example, the exploitation of shipping via the Northwest
Passage or Northeast Passage could reduce the navigational distance between
Europe and Asia by <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> % compared to the route via the Suez
Canal (Schøyen and Bråthen, 2011). The reduction in distance compared
to the Suez and/or Panama Canal routes could result in large cost savings due
to reduced<?pagebreak page190?> fuel consumption and an increase in the number of ships (Lassere,
2015). Melia et al. (2016) have shown that by mid-century, the frequency of
navigable period will double and the routes across the central Arctic will
become available. For example, for a high-emission scenario, they have shown
that by the late 21st century  trans-Arctic shipping might become commonplace, with
the shipping season ranging from 4 to 8 months. Overall, the
summertime use of these routes by different vessels (i.e., cargo ship and
tanks) has increased (Eguíluz et al., 2016); thus, the need for a proper
forecast for the Arctic sea ice conditions has become imperative. Currently,
forecasting the open water route through the Arctic basin is accurate within
200 km when the predictions are initialized in July (Melia et al., 2016). As
such, early knowledge on the potential opening of the maritime Arctic
routes could allow a better management for the shipping companies to
optimize (in terms of time and costs) shipping routes between the Atlantic
and the Pacific Oceans (Hassol, 2004; Smith and Stephenson, 2013). However,
the opening of the Northeast and Northwest passages does not guarantee
ice-free transects along the passages at all times and can always include the
possibility of drifting ice flows, which pose high
risks and potential environmental danger for conventional ships  when they are damaged in case of
accidents. Pizzolato et al. (2016) have shown that, despite the persistence
of low sea ice conditions since 2007, very few shipping activities have
been recorded within the northern route of the Northwest Passage. This might
be attributed to the multiyear ice concentrations in the Canadian Arctic
waters, which strongly influences the shipping activity. Hence, a proper
forecast does not imply a danger-free transect as long as the Arctic
Ocean is ice covered with thick multiyear ice for its larger parts over the
significant times of the year.</p>
      <p id="d1e173">Although the evolution of Arctic sea ice physical properties has been
extensively studied, the prediction of detrended Arctic sea ice extent, with
lead times of 3 months and longer, has not been very promising (Lindsay et
al., 2008; Blanchard-Wrigglesworth et al., 2011). From a forecasting point
of view, the evolution of autumn Arctic sea ice is closely associated with
initial conditions in the previous winter and spring. Different studies have
emphasized that some parameters contribute significantly to the improvement
of the seasonal sea ice forecast skill at different time lags (Holland and
Stroeve, 2011; Lindsay et al., 2008). For example, sea surface temperature
and sea ice concentration in spring are highly relevant predictors for the
minimum Arctic sea ice extent (Drobot et al., 2006). Some studies suggested
that accurate sea ice thickness could increase the forecast skill 2 months
ahead (Day et al., 2014; Dirkson et al., 2017). Also, the spring melt pond
fraction has been employed to improve the forecast skill of the Arctic
minimum sea ice extent (Schröder et al., 2014).</p>
      <p id="d1e176">Currently, there are different approaches used to make sea ice forecasts:
ice–ocean–atmosphere coupled models, statistical models, best-guess models
and mixed models (Stroeve et al., 2014; Hamilton and Stroeve, 2016). From a
statistical point of view, Drobot et al. (2006) showed that 46 % of the
pan-Arctic minimum sea ice extent would be predictable as early as February
based on monthly sea ice concentration, surface albedo, downwelling
longwave radiation and surface skin temperature. Lindsay et al. (2008) have
shown that their statistical model based on a wide range of predictors
(e.g., atmospheric circulation indices, sea ice extent and sea ice
concentration, ocean temperature at different levels) exhibited a greater
skill in predicting the September sea ice extent (SSIE) than those by Drobot
et al. (2006). The forecasts based on the state-of-the-art coupled
atmosphere–ocean sea ice models (Chevallier et al., 2013; Sigmond et al.,
2013) do not show better results when compared with the statistical models
(Kapsch et al., 2014; Schröder et al., 2014; Zhan and Davies, 2017).
These caveats indicate that our understanding regarding the controlling
factors of Arctic sea ice may still be insufficient. Overall, skillful
forecasts extend only 2 to 5 months ahead, for the summer months
(Stroeve et al., 2015; Schröder et al., 2014), regardless of the type of
the model used for the forecast (dynamical or statistical). The results and
error margins based on these different approaches have highlighted how
difficult it is to make skillful prediction for the SSIE. This is particular
true for the years with extreme low September sea ice concentrations (e.g.,
2012 or 2007), with both the dynamical and the statistical models showing
similar limitations (Stroeve et al., 2014, 2015; Schröder et al., 2014;
Hamilton and Stroeve, 2016). Stroeve et al. (2014)
have shown that seasonal predictions of the SSIE are most accurate in years
when the sea ice extent is near the long-term trend, but skillful sea ice
extent prediction appears challenging in years when the weather plays a
larger role (Hamilton and Stroeve, 2016).</p>
      <p id="d1e179">In order to improve the monthly/seasonal prediction skill of the sea ice
extent, one possibility would be to identify stable predictors (the
correlation coefficient between the predictor and the predictand does not
change in time) and to develop a statistical forecast model based on these
predictors. Following this idea, here we analyze the oceanic and atmospheric
conditions associated with the SSIE in order to identify potential predictors
based on a simple statistical methodology and place them in a longer
temporal context. Our statistical model takes into account different
atmospheric and oceanic variables following the approach in Ionita et
al. (2008, 2014, 2018) and Ionita (2017). These parameters are sea level pressure (SLP),
air temperature (TT), precipitable water content (PWC), surface zonal wind (USURF),
surface meridional wind (VSURF), the ocean heat content integrated
over the first 700 m (OHC), sea surface temperature (SST) and water
temperature integrated over the first 100 m (OT100), and they are used in order to calculate an
estimate of SSIE. The paper is structured as follows: the data and methods
used in this study are presented in Sect. 2, while the main results of our
analysis are shown in Sect. 3. The<?pagebreak page191?> discussion and concluding remarks are
presented in Sects. 4 and 5.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><label>Table 1</label><caption><p id="d1e186">Name, abbreviation, source, spatial and temporal resolution of the data
sets used in this study.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.89}[.89]?><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Name</oasis:entry>
         <oasis:entry colname="col2">Source</oasis:entry>
         <oasis:entry colname="col3">Temporal</oasis:entry>
         <oasis:entry colname="col4">Spatial</oasis:entry>
         <oasis:entry colname="col5">Reference</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">resolution</oasis:entry>
         <oasis:entry colname="col4">resolution</oasis:entry>
         <oasis:entry colname="col5"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Arctic sea ice extent</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://sidads.colorado.edu/DATASETS/NOAA/G02135/north/monthly/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">Fetterer et al. (2016)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(last access: 10 May 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">AMO index</oasis:entry>
         <oasis:entry colname="col2"><uri>https://climexp.knmi.nl/data/iamo_ersst.dat</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">Huang et al. (2014)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(last access: 10 May 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Mean air temperature at</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.cdc.noaa.gov/Datasets/ncep.reanalysis.derived/surface_gauss/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M5" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Kalnay et al. (1996)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">2 m (TT)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Downward longwave</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.cdc.noaa.gov/Datasets/ncep.reanalysis.derived/surface_gauss/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M8" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Kalnay et al. (1996)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">radiation (DLR)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Zonal surface wind</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.cdc.noaa.gov/Datasets/ncep.reanalysis.derived/surface/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M11" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Kalnay et al. (1996)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">(USURF)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Meridional surface wind</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.cdc.noaa.gov/Datasets/ncep.reanalysis.derived/surface/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M14" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Kalnay et al. (1996)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">(VSURF)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Precipitable water</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.cdc.noaa.gov/Datasets/ncep.reanalysis.derived/surface/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M17" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Kalnay et al. (1996)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">content (PWC)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sea level pressure (SLP)</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.cdc.noaa.gov/Datasets/ncep.reanalysis.derived/surface/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M20" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Kalnay et al. (1996)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sea surface temperature</oasis:entry>
         <oasis:entry colname="col2"><uri>ftp://ftp.ncdc.noaa.gov/pub/data/cmb/ersst/v5/netcdf/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.0<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M23" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.0<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Huang et al. (2014)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">(ERSSTv5)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ocean heat content in</oasis:entry>
         <oasis:entry colname="col2"><uri>https://www.nodc.noaa.gov/OC5/3M_HEAT_CONTENT/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M26" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Levitus et al. (2012)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">the first 700 m (OHC)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">Boyer et al. (2013)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ocean temperature in the</oasis:entry>
         <oasis:entry colname="col2"><uri>https://www.nodc.noaa.gov/OC5/3M_HEAT_CONTENT/</uri></oasis:entry>
         <oasis:entry colname="col3">1979–2017</oasis:entry>
         <oasis:entry colname="col4">2.5<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M29" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Levitus et al. (2012)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">first 100 m (OT100)</oasis:entry>
         <oasis:entry colname="col2">(last access: 6 June 2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">Boyer et al. (2013)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2">
  <title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Data</title>
      <p id="d1e845">The monthly sea ice extent has been extracted from the National Snow and Ice
Data Center ftp server (<uri>ftp://sidads.colorado.edu/DATASETS/NOAA/G02135/north/</uri>,
last access: 10 May 2018) (Fetterer et al., 2016).</p>
      <p id="d1e851">For the Northern Hemisphere temperature and atmospheric circulation, we use
the monthly means of air temperature at 2 m (TT), downward longwave radiation
flux (DW), zonal wind (USURF), meridional wind (VSURF), precipitable water
content (PWC) and the mean sea level pressure (SLP) from the NCEP/NCAR
40-year reanalysis project (Kalnay et al., 1996) on a
2.5<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M32" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid. Global sea surface
temperature (SST) is extracted from the Extended Reconstructed Sea Surface
Temperature data (ERSSTv5) (Huang et al., 2014). This data set covers the
period 1854–present and has a spatial resolution of 2<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M35" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.
The global heat content data in the first 700 m (OHC) and the
ocean temperature integrated over the first 100 m (OT100) are extracted from
the Global Ocean Heat and Salt Content database (Levitus et al., 2012; Boyer
et al., 2013).</p>
      <p id="d1e905">The monthly Atlantic Multidecadal Oscillation (AMO) index has
been calculated as the average of monthly SST anomalies with respect to the
mean over the North Atlantic north of 25<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N (25–60<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 75–7<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W). For the
AMO index computation, we used the RRSSTv5 data set (Huang et al., 2014). In
this study, we use the yearly mean of AMO index. Table 1 gives an overview
of all the data sets included in the study. All used data sets have been
detrended before the analysis by computing the linear trend for the entire
time series/gridded fields in question. This trend was then subtracted from
the initial time series/gridded data set. The linear trend was estimated
using a least-squares linear regression.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><label>Table 2</label><caption><p id="d1e938">Time lags used for the forecast of SSIE. Seasonal averages are
indicated as winter (December/January/February – DJF), spring (March/April/May – MAM),
summer (JJA – June/July/August) and autumn (September/October/December – SON).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Variable</oasis:entry>
         <oasis:entry colname="col2">Time lag</oasis:entry>
         <oasis:entry colname="col3">Month</oasis:entry>
         <oasis:entry colname="col4">Season</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">TT, DLR, USURF, VSURF, PWC, SLP</oasis:entry>
         <oasis:entry colname="col2">1–7 months, 1–2 seasons</oasis:entry>
         <oasis:entry colname="col3">January–July</oasis:entry>
         <oasis:entry colname="col4">DJF, MAM</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ERSSTv5</oasis:entry>
         <oasis:entry colname="col2">1–7 months, 1–2 seasons</oasis:entry>
         <oasis:entry colname="col3">January–July</oasis:entry>
         <oasis:entry colname="col4">DJF, MAM</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">OHC, OT100</oasis:entry>
         <oasis:entry colname="col2">1–4 seasons, 1–4 years</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">Annual, DJF, MAM, JJA, SON</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">AMO index</oasis:entry>
         <oasis:entry colname="col2">1–4 years</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">Annual mean</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><label>Figure 1</label><caption><p id="d1e1037">Stability map of the correlation between September sea ice extent
and <bold>(a)</bold> OHC SON, <bold>(b)</bold> SST MAM, <bold>(c)</bold> SLP May,
<bold>(d)</bold> PWC Apr and <bold>(e)</bold> VSURF MAM. Regions where the
correlation is stable, positive and significant for at least 80 % of the
21-year windows are shaded with dark red (95 %), red (90 %), orange
(85 %) and yellow (80 %). The corresponding regions where the correlation
is stable, but negative, are shaded with dark blue (95 %), blue (90 %),
green (85 %) and light green (80 %). The black boxes indicate the regions
used for the September sea ice extent at the end of May.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f01.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <title>Stability maps</title>
      <p id="d1e1067">The statistical model used in this study for the estimation of SSIE is based
on a methodology successfully used to make monthly/seasonal streamflow
predictions for the central European rivers (e.g., Elbe river, Rhine river,
Danube river, Ionita et al., 2008, 2014, 2018; Ionita, 2017; Meißner et al.,
2017). Furthermore, they were used for identifying the drivers of the Antarctic sea ice
variability (Ionita et al., 2018). The basic idea of this method is to
identify regions where the spatiotemporal distribution of the predictors is
stable when  correlated with the pan-Arctic SSIE. The SSIE has been correlated
with the potential predictors from previous months (Table 2) in a moving
window of 21 years, and the statistical significance of the correlation
coefficient was tested using a two-sided Student's  <inline-formula><mml:math id="M40" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> test. The correlation is considered
stable for those grid points where SSIE and the large-scale predictors (e.g., OHC,
OT100, SST, SLP, TT, PWC, DW, USURF and VSURF) are significantly correlated
at 95 %, 90 %, 85 % and 80 % significance levels for more than 80 %
of the 21-year windows, covering the period 1979–2007. We choose the
period 1979–2007 as  the calibration period, as both extreme years of sea ice extent,
namely 1996 and 2007, were included and it provides a climate-relevant
period of nearly 30 years. The areas where the correlation coefficient is
stable and positive are represented as dark red (95 %), red (90 %),
orange (85 %) and yellow (80 %), while the regions where the correlation
coefficient is stable and negative are represented as dark blue (95 %),
blue (90 %), green (85 %) and light green (80 %). Such maps are
referred to in our study as stability maps, and their spatial structures remain qualitatively
the same if the significance levels that define the stability of the
correlation vary within reasonable limits and if the length of the moving
window varies between 15 and 25 years. The optimal predictors are defined as
the average values over the stable regions for each gridded parameter. For
the current analysis, only regions where the correlation is above 90 %
significance level are retained for further analysis (Fig. 1). The raw
stability maps between SSIE (pan-Arctic and regional) and the potential
predictors are shown in Figs. S3–S15. Although the length of our time
series is relatively short (40 years), the methodology proved to work also in
cases of time series <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula> years (Ionita et al., 2018). Moreover, we
use the same methodology, with the same number of years (40 years), for the
prediction of September Arctic and Antarctic sea ice (<uri>https://www.arcus.org/sipn/sea-ice-outlook/2017/post-season</uri>, last access: 10 May 2018).</p>
      <p id="d1e1090">As a further main contributor to our forecast model, we use persistence,
defined here as the sea ice extent from previous months (e.g., January,
February and up to August). Persistence of sea ice anomalies stands as the first
source of predictability for sea ice (Guemas et al., 2016; Walsh and Johnson,
1979; Blanchard-Wrigglesworth et al., 2011).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Multiple linear regression</title>
      <?pagebreak page192?><p id="d1e1099">For the forecast, all data sets were separated into two parts: (1) the
calibration period (1979–2007) and (2) the validation period (2008–2017).
The optimal predictors are identified by employing stepwise multiple
regression analysis (e.g., Von Storch and Zwiers, 1999). Although the
“stability maps” methodology (Fig. 1) identifies multiple stable regions for each
atmospheric/oceanic parameter (Figs. S3–S15), after applying the
stepwise multiple regression, the optimal/final prediction model is based
just on the regions shown in Figs. 1–3 and 5–7. To forecast the
September sea ice extent, we have used a multiple linear regression model
with the regression equation
<?xmltex \hack{\newpage}?><?xmltex \hack{\vspace*{-6mm}}?>

                <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M42" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>Y</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:msub><mml:mi>x</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ε</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M43" display="inline"><mml:mi>Y</mml:mi></mml:math></inline-formula> represents the SSIE, <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>o</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, … <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
are constants determined by the least-squares
procedure, <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, … <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the predictors used (e.g., OHC, OT100,
etc.), and <inline-formula><mml:math id="M51" display="inline"><mml:mi mathvariant="italic">ε</mml:mi></mml:math></inline-formula> is the error.</p>
      <p id="d1e1261">In this study, we choose stepwise regression. Thus, each predictor was
prioritized based on its correlation coefficient with the SSIE and was added
to the model in that order. As we added more predictors to the model, the
<inline-formula><mml:math id="M52" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> statistic was used to determine whether the added predictors were
significant in the regression equation. Entrance and exit criteria for the
<inline-formula><mml:math id="M53" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> statistic were set to 0.05 and 0.1, respectively. Stepwise regression was
used because it prioritizes predictors based on the partial correlation and
it is likely that high and significant correlations will reflect underlying
physical processes. In order to estimate possible overfitting, we make use
of the Akaike information criterion (AIC) (Von Storch and Zwiers,
1999), the explained variance, <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> and the residual standard error. A
workflow of the selection of the optimal model for the SSIE prediction is
shown in the Supplement and Fig. S2.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>Pan-Arctic September sea ice prediction</title>
      <p id="d1e1301">The skill of a long-range forecast for the Arctic SSIE is associated with
the predictors that represent the slow varying components of the climate
system that are able to integrate the climate information such as ocean heat
content and SST (Guemas et al., 2016; Lindsay et al., 2008). These variables
can be used as potential predictors for months and even<?pagebreak page193?> seasons in advance
due to their long-term memory. Thus, here we investigate the potential link
between the Arctic SSIE (Fetterer et al., 2016) and OHC, OT100 (Levitus et
al., 2012; Boyer et al., 2013) and SST (Huang et al., 2014) as
long-term predictors (lags <inline-formula><mml:math id="M55" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 4 years (AMO index) up to
2 months in advance; see Table 2 for a detailed description of all the lags
used in the study). On shorter timescales (2–4 months), the atmospheric
circulation, especially during the summer months, plays a major role in
driving the Arctic sea ice variability (Guemas et al., 2016). The
atmospheric circulation can substantially contribute to the skill of the sea
ice predictions. As such, for the SSIE prediction, we have also tested the
skill of atmospheric variables (up to 4 months in advance), e.g., SLP, TT,
PWC, USURF and VSURF (Kalnay et al., 1996). Atmospheric moisture content
(e.g., clouds, water vapor content) has an impact on the net surface
radiation balance and hence also on the SSIE (Kapsch et al., 2013, 2014). As
a measure for this impact, we use the precipitable water content (PWC) as an
additional predictor.</p>
      <?pagebreak page194?><p id="d1e1311">For the final forecast, based on data available at the end of May (4 months
ahead of forecast), we have retained all identified stable regions shown as
black boxes in Fig. 1. For the forecast based on June data, we have
included also the stable regions based on all June stability maps (Fig. 2).
We have applied the same technique for the July data (Fig. 3). For
SSIE prediction based on the end-of-May data, the optimal model is based on
a combination of OHC SON, SST MAM, PWC Apr, VSURF MAM and SLP May
(Table 3). Together with these identified stable regions, the optimal model
includes also the persistence of sea ice extent, here the sea ice extent
from the previous March (SIE Mar), as well as the annual Atlantic Multidecadal
Oscillation index, with a lag of 4 years (AMO L4). The highest correlation
between SSIE and the annual AMO index was found at a time lag of 4 years
(AMO leads SSIE). The time lag identified in our analysis is in line with
previous studies (Day et al., 2012; Mahajan et al., 2011). The observed and
forecasted values based on the May data are shown in Fig. 4a. The
explained variance of the model, over the calibration (validation) period, is 81 %
(71 %), and the correlation coefficient between the observed and forecasted SSIE
is <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.90</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M57" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M58" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 84) (99.9 % significance level). To better assess the
skill of the SSIE prediction, the root mean square error (RMSE), the
Nash–Sutcliffe efficiency (NSE) and the index of agreement (<inline-formula><mml:math id="M59" display="inline"><mml:mi>d</mml:mi></mml:math></inline-formula>) are
calculated, among other statistical tests (see Table S1 in the Supplement and
the Supplement file for a definition of all the metrics used to test the skill of the
model). The forecasted model based on May data shows very good skill
(Table S1): NSE <inline-formula><mml:math id="M60" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.82 (0.68) (NSE <inline-formula><mml:math id="M61" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1 indicates a perfect model) and <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>
(0.88) (<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates a perfect match between the observed and forecasted
values; <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> indicates no agreement at all).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><label>Figure 2</label><caption><p id="d1e1400">Stability map of the correlation between September sea ice extent
and <bold>(a)</bold> TT Jun, <bold>(b)</bold> USURF Jun and <bold>(c)</bold> VSURF Jun.
Regions where the correlation is stable, positive and significant for at
least 80 % of the 21-year windows are shaded with dark red (95 %), red
(90 %), orange (85 %) and yellow (80 %). The corresponding regions
where the correlation is stable, but negative, are shaded with dark blue
(95 %), blue (90 %), green (85 %) and light green (80 %). The black
boxes indicate the regions used for the September sea ice extent at the end
of June in addition to the variables of May.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f02.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><label>Figure 3</label><caption><p id="d1e1421">Stability map of the correlation between September sea ice extent
and <bold>(a)</bold> SLP Jul, <bold>(b)</bold> PWC Jul, <bold>(c)</bold> TT Jul and
<bold>(d)</bold> USURF Jul. Regions where the correlation is stable, positive and
significant for at least 80% of the 21-year windows are shaded with dark
red (95 %), red (90 %), orange (85 %) and yellow (80 %). The
corresponding regions where the correlation is stable, but negative, are
shaded with dark blue (95 %), blue (90 %), green (85 %) and light green
(80 %). The black boxes indicate the regions used for the September sea ice
extent at the end of July in addition to the variables of May and June.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f03.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><label>Table 3</label><caption><p id="d1e1445">Variables retained for the September pan-Arctic sea ice extent forecast
(black boxes in Figs. 1–3). Single months are abbreviated with the first three
letters of the month.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">May data</oasis:entry>

         <oasis:entry colname="col3">June data</oasis:entry>

         <oasis:entry colname="col4">July data</oasis:entry>

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

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

         <oasis:entry colname="col2">SIE Mar</oasis:entry>

         <oasis:entry colname="col3">SIE Mar</oasis:entry>

         <oasis:entry colname="col4">SIE Mar</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="2">Ocean variables</oasis:entry>

         <oasis:entry colname="col2">OHC SON</oasis:entry>

         <oasis:entry colname="col3">OHC SON</oasis:entry>

         <oasis:entry colname="col4">OHC SON</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">SST MAM</oasis:entry>

         <oasis:entry colname="col3">SST MAM</oasis:entry>

         <oasis:entry colname="col4">SST MAM</oasis:entry>

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

         <oasis:entry colname="col2">AMO – L4</oasis:entry>

         <oasis:entry colname="col3">AMO – L4</oasis:entry>

         <oasis:entry colname="col4">AMO – L4</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="9">Atmospheric variables</oasis:entry>

         <oasis:entry colname="col2">SLP May</oasis:entry>

         <oasis:entry colname="col3">SLP May</oasis:entry>

         <oasis:entry colname="col4">SLP May</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">SLP Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">VSURF MAM</oasis:entry>

         <oasis:entry colname="col3">VSURF MAM</oasis:entry>

         <oasis:entry colname="col4">VSURF MAM</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3">VSURF Jun</oasis:entry>

         <oasis:entry colname="col4">VSURF Jun</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3">USURF Jun</oasis:entry>

         <oasis:entry colname="col4">USURF Jun</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">USURF Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">PWC Apr</oasis:entry>

         <oasis:entry colname="col3">PWC Apr</oasis:entry>

         <oasis:entry colname="col4">PWC Apr</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">PWC Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3">TT Jun</oasis:entry>

         <oasis:entry colname="col4">TT Jun</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">TT Jul</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup>

</oasis:table><?xmltex \hack{\vspace*{3mm}}?></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><label>Figure 4</label><caption><p id="d1e1653">Observed (black) and predicted (red) September sea ice extent
detrended anomalies over the period 1979–2017 based on <bold>(a)</bold> May,
<bold>(b)</bold> June and <bold>(c)</bold> July predictors from the stable regions.
The shaded area represents the 95 % uncertainty bounds.</p></caption>
          <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f04.jpg"/>

          <?xmltex \hack{\vspace*{3mm}}?>
        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><label>Figure 5</label><caption><p id="d1e1675">Stability map of the correlation between East Siberian September sea
ice extent and <bold>(a)</bold> OT100 annual (L4), <bold>(b)</bold> OT100
annual (L1), <bold>(c)</bold> SST MAM, <bold>(d)</bold> TT May, <bold>(e)</bold> DW MAM,
<bold>(f)</bold> PWC May, <bold>(g)</bold> SLP Jan and <bold>(h)</bold> VSURF MAM.
Regions where the correlation is stable, positive and significant for at
least 80 % of the 21-year windows are shaded with dark red (95 %), red
(90 %), orange (85 %) and yellow (80 %). The corresponding regions
where the correlation is stable, but negative, are shaded with dark blue
(95 %), blue (90 %), green (85 %) and light green (80 %). The black
boxes indicate the regions used for the September sea ice extent at the end of May.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f05.jpg"/>

        </fig>

      <p id="d1e1710">Following the same steps as in the case of May data, for the model based on
June data, the parameters contributing to the optimal forecast model are
shown in Fig. 2. As additional predictors, on top of those for May (Fig. 1),
we have VSURF Jun, USURF Jun and TT Jun (Table 3). The observed and
forecasted values of SSIE based on June data are shown in Fig. 4b. The
overall explained variance of the June-based model, over the calibration
(validation) period, is 85 % (79 %), and the correlation coefficient between the observed
and forecasted SSIE values is <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.92</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M66" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M67" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.89) (99.9 % significance
level). The June-based model exhibits also very good skill and shows
slight improvements compared to the May-based model: NSE <inline-formula><mml:math id="M68" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.85
(0.78) and <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.96</mml:mn></mml:mrow></mml:math></inline-formula> (0.93). For the model based on July data, the parameters
contributing to the optimal forecast model, on top of those based on May
(Fig. 1) and June (Fig. 2), are shown in Fig. 3 and Table 3. The
observed and predicted values of SSIE based on July data are shown in
Fig. 4c. The overall explained variance of the June-based model, over the
calibration (validation) period, is 86 % (81 %), and the correlation coefficient between
the observed and forecasted SSIE values is <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.93</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M71" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M72" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.90) (99.9 %
significance level). The July-based model exhibits also very good skill
and shows also slight improvements compared to the May- and June-based
models: NSE <inline-formula><mml:math id="M73" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.86 (0.80) and <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.96</mml:mn></mml:mrow></mml:math></inline-formula> (0.94).</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Application of the methodology for regional SSIE prediction</title>
      <p id="d1e1810">To test the robustness of our statistical model and to move towards
stakeholder-relevant regions, in this study, we are investigating also the
skill of our model at regional scale. Thus, we have repeated the same
analysis as in the previous section but for the sea ice extent averaged over
the East Siberian Sea (ESS) (Fig. S1 in the Supplement). In this study, we focus on the ESS
because in September 2007 and 2012, negative ice concentration anomalies
were particularly pronounced over this region of the Arctic Ocean
(Fig. S1a and b, respectively) and the highest variability of the SSIE is
recorded here (Fig. S1c). In addition, since 2011, the eastern ESS has been
nearly ice free (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> % SSIE) at the end of summer (Polyakov et
al., 2017). Moreover, when looking at the correlation coefficients between
the pan-Arctic SSIE and regional September SIE, the highest correlation, at
lag 0, is found with ESS SSIE (<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.72</mml:mn></mml:mrow></mml:math></inline-formula>, Table 4).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><label>Figure 6</label><caption><p id="d1e1837">Stability map of the correlation between East Siberian September sea
ice extent and TT Jun. Regions where the correlation is stable, positive and
significant for at least 80 % of the 21-year windows are shaded with dark
red (95 %), red (90 %), orange (85 %) and yellow (80 %). The
corresponding regions where the correlation is stable, but negative, are
shaded with dark blue (95 %), blue (90 %), green (85 %) and light green
(80 %). The black boxes indicate the regions used for the September sea ice
extent at the end of June in addition to the variables of May.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f06.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><label>Figure 7</label><caption><p id="d1e1848">Stability map of the correlation between East Siberian September sea
ice extent and <bold>(a)</bold> SST Jul, <bold>(b)</bold> TT Jul,
<bold>(c)</bold> PWC Jul and <bold>(d)</bold> VSURF Jul. Regions where the
correlation is stable, positive and significant for at least 80 % of the
21-year windows are shaded with dark red (95 %), red (90 %), orange
(85 %) and yellow (80 %). The corresponding regions where the correlation
is stable, but negative, are shaded with dark blue (95 %), blue (90 %),
green (85 %) and light green (80 %). The black boxes indicate the regions
used for the September sea ice extent at the end of July in addition to the
variables of May and June.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f07.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><label>Table 4</label><caption><p id="d1e1873">The correlation coefficients between the detrended pan-Arctic September
sea ice extent and the regional September sea ice extent. A detailed description
regarding the definition of each region is given here: <uri>ftp://sidads.colorado.edu/DATASETS/NOAA/G02135/seaice_analysis/</uri>
(last access: 10 May 2018).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Lag 4</oasis:entry>
         <oasis:entry colname="col3">Lag 3</oasis:entry>
         <oasis:entry colname="col4">Lag 2</oasis:entry>
         <oasis:entry colname="col5">Lag 1</oasis:entry>
         <oasis:entry colname="col6">Lag 0</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Baffin</oasis:entry>
         <oasis:entry colname="col2">0.07</oasis:entry>
         <oasis:entry colname="col3">0.09</oasis:entry>
         <oasis:entry colname="col4">0.34</oasis:entry>
         <oasis:entry colname="col5">0.40</oasis:entry>
         <oasis:entry colname="col6">0.39</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Barents</oasis:entry>
         <oasis:entry colname="col2">0.20</oasis:entry>
         <oasis:entry colname="col3">0.16</oasis:entry>
         <oasis:entry colname="col4">0.27</oasis:entry>
         <oasis:entry colname="col5">0.13</oasis:entry>
         <oasis:entry colname="col6">0.14</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Beaufort</oasis:entry>
         <oasis:entry colname="col2">0.15</oasis:entry>
         <oasis:entry colname="col3">0.24</oasis:entry>
         <oasis:entry colname="col4">0.37</oasis:entry>
         <oasis:entry colname="col5">0.51</oasis:entry>
         <oasis:entry colname="col6">0.60</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bering</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">0.14</oasis:entry>
         <oasis:entry colname="col5">0.00</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Canadian</oasis:entry>
         <oasis:entry colname="col2">0.07</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">0.01</oasis:entry>
         <oasis:entry colname="col5">0.52</oasis:entry>
         <oasis:entry colname="col6">0.49</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Chukchi</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.26</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">0.03</oasis:entry>
         <oasis:entry colname="col4">0.09</oasis:entry>
         <oasis:entry colname="col5">0.53</oasis:entry>
         <oasis:entry colname="col6">0.60</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">East Siberian</oasis:entry>
         <oasis:entry colname="col2">0.19</oasis:entry>
         <oasis:entry colname="col3">0.24</oasis:entry>
         <oasis:entry colname="col4">0.39</oasis:entry>
         <oasis:entry colname="col5">0.61</oasis:entry>
         <oasis:entry colname="col6">0.72</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Greenland</oasis:entry>
         <oasis:entry colname="col2">0.04</oasis:entry>
         <oasis:entry colname="col3">0.06</oasis:entry>
         <oasis:entry colname="col4">0.22</oasis:entry>
         <oasis:entry colname="col5">0.16</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hudson</oasis:entry>
         <oasis:entry colname="col2">0.44</oasis:entry>
         <oasis:entry colname="col3">0.51</oasis:entry>
         <oasis:entry colname="col4">0.46</oasis:entry>
         <oasis:entry colname="col5">0.38</oasis:entry>
         <oasis:entry colname="col6">0.47</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kara</oasis:entry>
         <oasis:entry colname="col2">0.09</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.03</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">0.05</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Laptev</oasis:entry>
         <oasis:entry colname="col2">0.34</oasis:entry>
         <oasis:entry colname="col3">0.32</oasis:entry>
         <oasis:entry colname="col4">0.40</oasis:entry>
         <oasis:entry colname="col5">0.37</oasis:entry>
         <oasis:entry colname="col6">0.53</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2239">The stability maps between the detrended ESS SSIE and the large-scale
oceanic and atmospheric fields are shown in Fig. 5 (stability maps based
on May and previous months' data), Fig. 6 (stability maps based on June and
previous months' data) and Fig. 7 (stability maps based on July and
previous months' data), respectively. For ESS SSIE prediction based on the
end-of-May data, the optimal model is based on a combination of annual
OT100, SST MAM, SLP Jan, VSURF MAM, PWC May, TT May and DW MAM (Table 5).
The observed and forecasted values based on the May data are shown in
Fig. 8a. The explained variance of the model, over the calibration (validation) period, is
88 % (58 %), and the correlation coefficient between the observed and
forecasted ESS SSIE is <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.94</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M87" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M88" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.77) (99.9 % significance level). The
forecasted model based on the May shows very good skill (Table S2):
NSE <inline-formula><mml:math id="M89" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.88 (0.57) (NSE <inline-formula><mml:math id="M90" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1 indicates a perfect model) and <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.97</mml:mn></mml:mrow></mml:math></inline-formula>(0.86) (<inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates
a perfect match between the observed and forecasted values; <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>
indicates no agreement at all).</p>
      <p id="d1e2319">For the model based on June data, the parameters contributing to the optimal
forecast model in addition to the May variables are shown in Fig. 6 and
Table 5. As additional predictors, on top of May data (Fig. 5), we have
SIE Jun and TT Jun (Table 5). The observed and forecasted values of
ESS SSIE based on June data are shown in Fig. 8b. The overall explained
variance of the June-based model, over the calibration (validation) period, is 91 %
(71 %), and the correlation coefficient between the observed and forecasted SSIE
values is <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M95" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M96" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.84) (99.9 % significance level). The June-based
model exhibits also very good skill and shows slight improvements compared
to the May-based model: NSE <inline-formula><mml:math id="M97" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.91 (0.69) and <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.98</mml:mn></mml:mrow></mml:math></inline-formula> (0.91). For the model
based on July data, the parameters contributing to the optimal forecast
model, on top of May data (Fig. 5) and June data (Fig. 6), are shown in
Fig. 7 and Table 5. The observed and predicted values of SSIE based on
July data are shown in Fig. 8c. The overall explained variance of the
July-based model, over the calibration (validation) period, is 94 % (81 %), and the
correlation coefficient between the observed and forecasted SSIE values is
<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.97</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M100" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M101" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.90) (99.9 % significance level). The July-based model exhibits
also very good skill and shows slight improvements compared to the May- and
June-based models: NSE <inline-formula><mml:math id="M102" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.94 (0.78) and <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.98</mml:mn></mml:mrow></mml:math></inline-formula> (0.93).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><label>Figure 8</label><caption><p id="d1e2415">Observed (black) and predicted (red) East Siberian sea ice extent
detrended anomalies over the period 1979–2017 based on <bold>(a)</bold> May,
<bold>(b)</bold> June and <bold>(c)</bold> July predictors from the stable regions.
The shaded area represents the 95 % uncertainty bounds.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://esd.copernicus.org/articles/10/189/2019/esd-10-189-2019-f08.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><label>Table 5</label><caption><p id="d1e2436">Variables retained for the September East Siberian sea (ESS) ice extent
forecast (black boxes in Figs. 5–7). Seasonal averages are indicated as spring
MAM (March, April, May); single months are abbreviated with the first three
letters of the month.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2">May data</oasis:entry>

         <oasis:entry colname="col3">June data</oasis:entry>

         <oasis:entry colname="col4">July data</oasis:entry>

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

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

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3">SIE Jun</oasis:entry>

         <oasis:entry colname="col4">SIE Jun</oasis:entry>

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

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">SIE Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

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

         <oasis:entry colname="col2">OT100 – L4, L1</oasis:entry>

         <oasis:entry colname="col3">OT100 – L4, L1</oasis:entry>

         <oasis:entry colname="col4">OT100 – L4, L1</oasis:entry>

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

         <oasis:entry colname="col2">SST MAM</oasis:entry>

         <oasis:entry colname="col3">SST MAM</oasis:entry>

         <oasis:entry colname="col4">SST MAM</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="8">Atmospheric variables</oasis:entry>

         <oasis:entry colname="col2">SLP Jan</oasis:entry>

         <oasis:entry colname="col3">SLP Jan</oasis:entry>

         <oasis:entry colname="col4">SLP Jan</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">VSURF MAM</oasis:entry>

         <oasis:entry colname="col3">VSURF MAM</oasis:entry>

         <oasis:entry colname="col4">VSURF MAM</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">VSURF Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">PWC May</oasis:entry>

         <oasis:entry colname="col3">PWC May</oasis:entry>

         <oasis:entry colname="col4">PWC May</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">PWC Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">TT May</oasis:entry>

         <oasis:entry colname="col3">TT May</oasis:entry>

         <oasis:entry colname="col4">TT May</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3">TT Jun</oasis:entry>

         <oasis:entry colname="col4">TT Jun</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">TT Jul</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">DW MAM</oasis:entry>

         <oasis:entry colname="col3">DW MAM</oasis:entry>

         <oasis:entry colname="col4">DW MAM</oasis:entry>

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

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
      <p id="d1e2637">The results of this study demonstrate that statistically based models are
able to predict SSIE with high skill, if the accurate drivers and their
regional localizations (herein stable regions) are identified via various
statistical techniques. In this paper, our analysis was focused on a single
month (September), but the same methodology has been be successfully applied
also for other months/seasons and also for the Antarctic region (Ionita et al., 2018).</p>
      <?pagebreak page199?><p id="d1e2640">Our results highlight the potential for skillful prediction of SSIE, both at
pan-Arctic level as well as for ESS, based on large-scale drivers from
stable regions. The ocean drivers (OHC, TT100 and SST) from the identified
stable regions are strongly related to the Atlantic inflow or to the SST
variability over regions strongly influenced by decadal modes of variability
(e.g., Pacific Decadal Oscillation – PDO – in the central and north Pacific)
to multidecadal modes of variability (e.g., Atlantic Multidecadal
Oscillation – AMO – in the Atlantic Ocean region). The Atlantic inflow, AMO
and PDO play a significant role in driving the Arctic sea ice variability
(Polyakov et al., 2017; Miles et al., 2014; Ionita et al., 2016; Screen and
Francis, 2016). For example, the North Atlantic might act as a source for the
OHC anomaly identified over the Kara Sea, Laptev Sea and ESS (Figs. 1
and 5), thus contributing to the skill of our forecast. The OHC anomalies
form the North Atlantic flow into the Arctic basin, via advection, and affect
the sea ice distribution (Polyakov et al., 2017; Ono et al., 2018). In a
recent study, Yu et al. (2017) have shown that the leading mode of
variability of global sea ice concentration is positively correlated with
the AMO and negatively correlated with the PDO. Furthermore, two-thirds of
the total global sea ice trend can be explained by a combination of these
two modes of variability. Superimposed on the interannual variability, the
temperature and salinity of the Atlantic inflows to the Arctic Ocean show
also pronounced decadal to multidecadal variability (Zhang, 2015). This
aligns with the concept of different previous studies, which suggest that
the decreasing trend in the Arctic sea ice is partially driven by AMO (Park
and Latif, 2008; Lindsay et al., 2005; Ding et al., 2014; Yu et al., 2017).
Moreover, starting at the beginning of 1990s, the AMO switched to a
positive phase, at the same time when the Arctic sea ice extent started its
abrupt decline. Thus, in this study, we have tested previous years' AMO index
as a potential driver of the Arctic sea ice extent.</p>
      <p id="d1e2643">The stability maps based on the predictors related to the atmospheric
variables (Figs. 1–3) show significant and stable correlations with
regions restricted to the Arctic basin, indicating a very regional connection
between the September sea ice variability and large-scale atmospheric
circulation. The state of the Arctic SSIE depends both on the state of the
ice in spring and on the atmospheric condition during summer (Ding et
al., 2017). In this respect, the precipitable water content and air
temperature in spring and early summer were found to show significant
predictive skill for the SSIE both at pan-Arctic as well as regional levels.
This is also in agreement with previous studies (Kapsch et al., 2013, 2014)
which have shown a significantly increased cloudiness and humidity over the
Arctic region in spring, thus accelerating the sea ice retreat in the
upcoming summer, via enhanced longwave radiation.</p>
      <p id="d1e2646">Overall, such a methodology can be valuable also for the modeling
community. If the coupled models, used for forecasting purposes, face
problems to simulate the ocean and/or the climate background over the areas
that play a significant role in driving the SSIE variability (stable
regions), one expects a relatively small forecast skill. The opposite case
is also valid: a good representation of the key regions that drive SSIE
could imply a good forecast skill. For example, Parkinson et al. (2006)
determined that many climate models tend to simulate more winter sea ice in
the Barents Sea compared to observations. One hypothesis for this
overestimation is that the models underestimate the heat content in the
Atlantic basin (which has proven to be one of the main contributors for a
skillful prediction for SSIE in our model). By using a simple and
computationally inexpensive statistical approach, one can anticipate more
than 80 % of SSIE up to 4 months in advance, based on the antecedent
atmospheric and oceanic conditions over stable regions. Moreover, our
statistical model is able to properly reproduce the years with extreme low/high
sea ice extent, both at pan-Arctic level as well as at regional scale
(e.g., 2007 and 2012 – low SSIE, and 1996 – high SSIE; see Figs. 4 and 8).
The predictability of these extreme years poses big challenges
for the sea ice prediction community (Hamilton and Stroeve, 2016).</p>
      <p id="d1e2650">For example, one of the most unpredictable years was 2012. Most of the
models (statistical and dynamical) were unable to properly forecast the
extremely low value of the sea ice extent in September 2012 (Stroeve et al.,
2014). Overall, the statistical predictions came closer to the unexpected
low sea ice extent in September 2012 than the dynamical-based predictions.
In this respect, our statistical model was able to capture the overall
decline in the SSIE and we forecasted the lowest sea ice extent since the
observational period (Fig. 4). Nevertheless, in terms of amplitude, our
forecast has underestimated the observed values (Fig. 4). One of the
reasons for this underestimation could come from the fact that in August 2012
a strong storm prevailed over the Arctic basin, which triggered extreme
sea ice melt by bringing heat and moisture from the south towards the
central Arctic (Parkinson and Comiso, 2013). Another potential trigger of the
extreme sea ice melt in 2012 might be a combination of extremely thin sea
ice pack and increased upward ocean heat transport, which created conditions
that made the sea ice particularly vulnerable to storms (Zhang et al.,
2013). The storm in August 2012 allowed a large amount of oceanic heat to be
mixed up to the surface, thus enhancing the sea ice melt. Because the
atmosphere is mostly unpredictable beyond 1 or 2 weeks, we were not able to
accurately predict, in terms of amplitude, the sea ice conditions that
developed because of the Arctic storm in August 2012.</p>
      <p id="d1e2653">Another challenge for the sea ice community was the predictability of SSIE
in 2013. Sea ice extent in September 2013 was characterized by a revival
compared to the low values recorded in September 2012 (SSIE in 2013 was
1.69 million km<inline-formula><mml:math id="M104" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> above the record minimum extent in September 2012).
Most of the models, involved in the Sea Ice Prediction Network (SIPN), have underestimated the
September 2013 sea ice extent,  despite the fact that this was not an extreme
low sea ice year like 2012. The observed September 2013 sea ice extent lied
outside the intervals given with 13 out of 16 predictions, but the modeling
methods performed better than the statistical ones (Stroeve et al., 2014).
For September 2013, our statistical model performed almost<?pagebreak page200?> perfectly, giving
one of the best predictions (in terms of amplitude) over the validation
period. The revival of the sea ice extent in 2013 was due to a combination
of different factors: a colder summer over the Arctic basin, compared to 2012,
and no storms prevailing throughout the summer months; less winter
clouds in January–February 2013, which resulted in more strongly negative
surface radiation budget (Liu and Key, 2014); later melt onset, intermittent
freezing events and an earlier fall freeze-up (Wang et al., 2016), among
others. Summer 2013 was characterized by an unusual low pressure system over
much of the Arctic Ocean, which acted as a limiting factor for the heat
transport from the south. Both the SLP and air temperature over the Arctic
basin were part of our final predictors for the sea ice extent in 2013
(Figs. 2 and 3). As such, the accurate predictions based on our
statistical model for 2013 may arise from the fact that no extreme weather
events were occurring throughout the summer months over the Arctic region.
In addition, we had persistent negative temperature anomalies and a
long-lasting low pressure system prevailing in June and July over the Arctic
basin, variables which were used in our forecast model. A high/low skill in
the predictability of extreme September sea ice can be the result of
extreme spring preconditioning (e.g., very low ice thickness) and/or the
results of extremely anomalous summer weather systems, independent of the
spring preconditioning. In observation, not all extremes are the results of
the same forcing, thus implying that different extreme events will have a
different level of predictability.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e2672">In this study, we have developed a statistical method based on different
oceanic and atmospheric variables to estimate the monthly signal and
variability of the Arctic sea ice extent. Based on stepwise multiregression
analysis, optimal predictors are identified in terms of stability maps to
forecast SSIE on a pan-Arctic or regional scale. We have demonstrated that our
well-established statistical approach can be used as a promising tool to
improve the skill of sea ice extent prediction. In the future, the same
methodology will be applied to test the potential predictability, up to 2
years ahead, by taking into account variables with long-term memory (e.g.,
heat content and water temperature integrated over different depths) for the
whole Arctic. For other regions prone to extreme decrease in the sea ice
extent (e.g., Chukchi Sea, Beaufort Sea, Barents Sea), as well as for
Antarctica, the method will also be adopted. Finally, since the concept can
be used as an early warning system for September sea ice extent, both at
pan-Arctic level as well as regionally, the potential environmental and
economic benefits can be very high.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e2679">All the data sets used in our study are publicly available
(see Tables 1 and 4).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2682">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/esd-10-189-2019-supplement" xlink:title="pdf">https://doi.org/10.5194/esd-10-189-2019-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2691">MI designed the study and wrote the paper. PS wrote the code
for the data analysis. KG, PS, RT and GL helped write the paper and interpret the results.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2697">The authors declare that they have no conflict of interest.</p>
  </notes><?xmltex \hack{\newpage}?><ack><title>Acknowledgements</title><p id="d1e2704">This study was promoted by Helmholtz funding through the Polar Regions and
Coasts in the Changing Earth System (PACES) program of the AWI. Funding by
the Helmholtz Climate Initiative REKLIM is gratefully acknowledged.
Patrick Scholz has been funded by the Collaborative Research Centre TRR 181
“Energy Transfer in Atmosphere and Ocean”.  <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
The article processing charges for this open-access <?xmltex \hack{\newline}?> publication
were covered by a Research <?xmltex \hack{\newline}?> Centre of the Helmholtz Association.</p></ack><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2716">This paper was edited by Christian Franzke and reviewed by three anonymous referees.</p>
  </notes><ref-list>
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    <!--<article-title-html> September Arctic sea ice minimum prediction  – a skillful new statistical approach</article-title-html>
<abstract-html><p>Sea ice in both polar regions is an important indicator of the
expression of global climate change and its polar amplification.
Consequently, broad interest exists on sea ice coverage, variability and
long-term change. However, its predictability is complex and it depends
strongly on different atmospheric and oceanic parameters. In order to
provide insights into the potential development of a monthly/seasonal signal
of sea ice evolution, we applied a robust statistical model based on
different oceanic and atmospheric parameters to calculate an estimate of the
September sea ice extent (SSIE) on a monthly timescale. Although previous
statistical attempts of monthly/seasonal SSIE forecasts show a relatively
reduced skill, when the trend is removed, we show here that the September
sea ice extent has a high predictive skill, up to 4 months ahead, based on
previous months' oceanic and atmospheric conditions. Our statistical model
skillfully captures the interannual variability of the SSIE and could
provide a valuable tool for identifying relevant regions and oceanic and
atmospheric parameters that are important for the sea ice development in the
Arctic and for detecting sensitive/critical regions in global coupled
climate models with a focus on sea ice formation.</p></abstract-html>
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