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  <front>
    <journal-meta><journal-id journal-id-type="publisher">CP</journal-id><journal-title-group>
    <journal-title>Climate of the Past</journal-title>
    <abbrev-journal-title abbrev-type="publisher">CP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Clim. Past</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1814-9332</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/cp-18-1709-2022</article-id><title-group><article-title>Regional validation of the use of diatoms in ice cores from <?xmltex \hack{\break}?> the Antarctic Peninsula as a Southern Hemisphere<?xmltex \hack{\break}?> westerly wind proxy</article-title><alt-title>Diatoms as a Southern Hemisphere westerly wind proxy</alt-title>
      </title-group><?xmltex \runningtitle{Diatoms as a Southern Hemisphere westerly wind proxy}?><?xmltex \runningauthor{D. R. Tetzner et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Tetzner</surname><given-names>Dieter R.</given-names></name>
          <email>dietet95@bas.ac.uk</email>
        <ext-link>https://orcid.org/0000-0001-7659-8799</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Thomas</surname><given-names>Elizabeth R.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3010-6493</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Allen</surname><given-names>Claire S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0938-0551</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Grieman</surname><given-names>Mackenzie M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9610-7141</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>British Antarctic Survey, Ice Dynamics and Paleoclimate, Cambridge,
CB3 0ET, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth Sciences, University of Cambridge, Cambridge, CB2 3EQ, UK</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Dieter R. Tetzner (dietet95@bas.ac.uk)</corresp></author-notes><pub-date><day>21</day><month>July</month><year>2022</year></pub-date>
      
      <volume>18</volume>
      <issue>7</issue>
      <fpage>1709</fpage><lpage>1727</lpage>
      <history>
        <date date-type="received"><day>9</day><month>July</month><year>2021</year></date>
           <date date-type="rev-request"><day>22</day><month>July</month><year>2021</year></date>
           <date date-type="rev-recd"><day>8</day><month>April</month><year>2022</year></date>
           <date date-type="accepted"><day>15</day><month>April</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 </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://cp.copernicus.org/articles/.html">This article is available from https://cp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://cp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://cp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e118">The Southern Hemisphere westerly winds are among the most
important drivers of recently observed environmental changes in West
Antarctica. However, the lack of long-term wind records in this region
hinders our ability to assess the long-term context of these variations. Ice
core proxy records yield valuable information about past environmental
changes, although current proxies present limitations when aiming to
reconstruct past winds. Here we present the first regional wind study based
on the novel use of diatoms preserved in Antarctic ice cores. We assess the
temporal variability in diatom abundance and its relation to regional
environmental parameters spanning a 20-year period across three sites in the
southern Antarctic Peninsula and Ellsworth Land, Antarctica. Correlation
analyses reveal that the temporal variability of diatom abundance from high-elevation ice core sites is driven by changes in wind strength over the core
of the Southern Hemisphere westerly wind belt, validating the use of diatoms
preserved in ice cores from high-elevation inland sites in the southern
Antarctic Peninsula and Ellsworth Land as a proxy for reconstructing past
variations in wind strength over the Pacific sector of the Southern
Hemisphere westerly wind belt.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e130">Winds over the Southern Ocean (circumpolar westerlies) play a key role in
driving the exchange of heat and carbon dioxide between the ocean and
atmosphere (Russell et al., 2006; Quéré et al., 2007; Hodgson and
Sime, 2010; Landschutzer et al., 2015). In recent decades, the circumpolar
wind belt has increased in strength and has shifted towards the Antarctic
continent, constituting one of the strongest climatic trends in the Southern
Hemisphere (Thompson and Solomon, 2002; Gille et al., 2008; Young et al., 2011). These atmospheric changes have been linked as drivers of the
widespread warming observed in the Antarctic Peninsula (AP) (Orr et al., 2004; Van Den Broeke and Van Lipzig, 2004; Marshall et al., 2006; Thomas et al., 2009; Thomas and Tetzner, 2018; Turner et al., 2020) and West
Antarctica (WA) (Thomas et al., 2013) and as the mechanism behind the
enhanced upwelling of deep and relatively warm, CO<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>-rich oceanic water
(Nakayama et al., 2018). The upwelling of circumpolar deep water has been
shown to promote accelerated melting and thinning at the base of the ice
shelves (Thoma et al., 2008; Jacobs et al., 2011; Pritchard et al., 2012;
Steig et al., 2012; Wåhlin et al., 2013; Dutrieux et al., 2014; Favier
et al., 2014; Gille et al., 2014; Joughin et al., 2014; Paolo et al., 2015;
Holland et al., 2019), thus threatening the stability of floating ice
shelves along the coastline of the Amundsen–Bellingshausen seas and
ultimately contributing to global sea level rise (Pritchard et al., 2012).
Changes in the circumpolar westerlies have also been linked to an observed
pattern of increased snow accumulation in Antarctica over the 20th century, which has mitigated global mean sea level rise (Medley and Thomas, 2019). To assess the context of these recent wind changes, an extended record of wind strength is needed.</p>
      <p id="d1e142">Direct meteorological observations in the AP region are sparse, relatively
short-term and mostly constrained to coastal regions (Lazzara et al., 2012;
Oliva et al., 2017; Thomas and Tetzner, 2018; Turner et al., 2020). The
scarcity of continuous long-term data can be partly addressed by using
climate reanalyses datasets. These datasets comprise model outputs from
simulations that are used to interpolate measured climate variables,
providing accurate meteorological data in this region for the satellite era
(1979–present) (Tetzner et al., 2019; Dong et al., 2020; Zhu et al., 2021),
but are not viable for studying pre-satellite regional climate variability.
Climate models can be used to extend the record back in time; however, model
simulations from the Fifth Coupled Model Intercomparison Project (CMIP5)
exhibit strong biases over the Southern Ocean compared with observations
(Bracegirdle et al., 2013). Overall, the lack of long-term wind records in
the region hinders the possibility to assess the long-term context of the
recently observed changes.</p>
      <p id="d1e145">Ice cores provide valuable climatic information over a range of timescales
(Legrand and Mayewski, 1997). Insoluble mineral dust concentrations in
Antarctic ice cores have been widely used to infer past variability in
regional-to-hemispheric atmospheric circulation (Röthlisberger et al., 2002; Lambert et al., 2008; Koffman et al., 2014; Delmonte et al., 2020;
Laluraj et al., 2020). Geochemical tracers of mineral dust, such as the
non-sea-salt component of soluble calcium (nssCa<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>) or potassium
(nssK<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>), have been used to track changes in the strength and position
of the Southern Hemisphere westerly wind (SHWW) belt (Dixon et al., 2012;
Mayewski et al., 2013). However, these traditional proxies typically
originate from South America, Australia and New Zealand, and local Antarctic
ice-free areas and are therefore potentially influenced by environmental
changes in these distal source regions (McConnell et al., 2007; Lambert et
al., 2008; Li et al., 2010; Wolff et al., 2010; Bullard et al., 2016;
Delmonte et al., 2017). Sea salt sodium (ssNa<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>) has been previously
interpreted as a proxy for increased meridional transport from the Southern
Ocean to ice core sites in Antarctica (Kreutz et al., 2000; Goodwin et al., 2004; Kaspari et al., 2005; Mayewski et al., 2013; Vance et al., 2013).
However, the ssNa<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> signal is potentially influenced by inputs from
blowing snow above sea ice (Frey et al., 2020) and by the production of
ssNa<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> in “frost flowers”, as well as by inputs from the open ocean
(Huang and Jaeglé, 2017). As frost flowers are precipitated from the
surface of freshly formed sea ice (Wagenbach et al., 1998; Rankin et al., 2000) and all these sources are affected by sea ice extent, some studies
have reflected on the potential of the ssNa<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> ice core record from
Antarctic coastal sites as a proxy for seasonal sea ice extension (Rankin et
al., 2002; Wolff et al., 2003, 2006). These conflicting
sources of ssNa<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> suggest that the variability of the ssNa<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> record
is not entirely driven by changes in winds or atmospheric circulation. The
current limitations identified in conventional ice core wind and atmospheric
circulation proxies highlight the need to explore new species to reconstruct
wind strength.</p>
      <p id="d1e224">Diatoms entrained in Antarctic snow and ice have recently been proposed as
an alternative source of information about winds (Allen et al., 2020).
Diatoms are unicellular algae with siliceous cell walls that inhabit marine,
brackish and freshwater environments throughout the world (Smol and
Stoermer, 2010). Despite their aquatic habitats, several studies support
the idea that they can be airborne (Chalmers et al., 1996; Gayley et al., 1989;
Lichti-Federovich, 1984; McKay et al., 2008; Wang et al., 2008; Harper and
Mackay, 2010; Spaulding et al., 2010; Hausmann et al., 2011; Budgeon et al., 2012; Papina et al., 2013; Fritz et al., 2015). Airborne diatoms can be
sourced from both exposed diatom-bearing sediments and modern water bodies
(e.g. oceans, streams, lakes) (Harper and McKay, 2010). Marine diatoms can
be effectively lifted from the sea surface microlayer into the atmosphere by
wind-induced bubble-bursting and wave-breaking processes (Cipriano and
Blanchard, 1981; Farmer et al., 1993). Once in the atmosphere, they can be
transported by winds over long distances (Chalmers et al., 1996; Elster et al., 2007; Harper and McKay, 2010; Budgeon et al., 2012; Marks et al., 2019;
Allen et al., 2020). Diatom records have been evaluated at multiple ice core
sites in the AP and Ellsworth Land (EL) regions (Tetzner et al., 2022a) to
reveal consistent spatial variations and increases in the diatom
concentration during the past 3 decades. Despite the potential the
diatom record has shown to reconstruct past wind strength, this proxy
requires evaluation against more established ice core wind and atmospheric
circulation proxies.</p>
      <p id="d1e228">In this study, we evaluate the potential for diatoms to reconstruct regional
wind strength using an array of three shallow-depth ice cores drilled in the
AP and EL regions. We investigate the relationship between diatom abundance
and changes in environmental parameters to assess the regional consistency
of the diatom-based wind proxy. We expand these analyses by comparing the
diatom record to traditional ice core wind and atmospheric circulation
proxies based on major ions and dust.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Ice core records and age scales</title>
      <p id="d1e246">Three ice cores and firn cores from the southern AP and EL were included in
this study (Fig. 1, Table 1). The Jurassic ice core (JUR, 140 m) was
drilled in the vicinity of Jurassic Nunatak using the BAS electromechanical
drill during the austral summer 2012–2013. The Sky-Blu firn core (SKBL, 21.8 m) from the vicinity of Sky-Blu Field Station, southern AP, and the Sherman Island firn core (SHIC, 21.3 m) from Eights Coast were drilled using a
Kovacs hand auger during the austral summer 2019–2020; hereafter, for
practical reasons, firn cores will be referred to as ice cores. For JUR,
SKBL and SHIC, an ice core chronology was established (Tetzner et al., 2022a) based on their hydrogen peroxide (H<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O<inline-formula><mml:math id="M11" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>) annual cycle that
is assumed to peak during the austral summer solstice and to exhibit its
minimum during the austral winter (Frey et al., 2006; Thomas et al., 2008).
Ice core chronologies were corroborated using the annual cycle of the
non-sea-salt component of major ions, such as non-sea-salt sulfate
(nssSO<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) (Piel et al., 2006), that is assumed to peak between
November and January in this region (Pasteris et al., 2014; Thoen et al., 2018). Ice core chronologies were corroborated with the presence of volcanic tephra in the 2001 CE ice core layer (Tetzner et al., 2021b). The top 15 m of SKBL included in this work and the full SHIC core were dated back to 1999 CE, and the top 36.90 m of JUR included in this work dated back to 1992 CE. The estimated dating error is <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> months for each year with no accumulated error.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e294">Map showing the location of the ice core sites and main oceanographic features considered in this study. The red circles show the locations of the three ice core sites. The pale green line shows the median September sea ice extension between 1980 and 2010 CE, and the pale green area represents the seasonal sea ice zone (SSIZ). The red line shows the median February sea ice extension between 1980 and 2010 CE, and the pale red area represents the perennial sea ice zone (PSIZ). SAF: Sub-Antarctic Front.
APF: Antarctic Polar Front. CP: coastal polynya. EI-C: Eights Coast. BC: Bryan Coast. ASE: Amundsen Sea Embayment. PAL: Palmer ice core site. FER: Ferrigno ice core site. AP: Antarctic Peninsula.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/1709/2022/cp-18-1709-2022-f01.jpg"/>

        </fig>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e306">Summary of each ice core geographical location and main features
analysed in this study. SIE: sea ice edge (<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula>) – the distance from SIE reported corresponds to the median for years covering the data interval.
September SIE values used for calculations were obtained as the distance between
the ice core site and the closest point in the northern limit of 15 % sea
ice cover. February SIE values used for calculations were obtained as the
distance between the ice core site and the closest sea-ice-free region.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:colspec colnum="7" colname="col7" align="center"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="center"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Core</oasis:entry>
         <oasis:entry colname="col2">Long</oasis:entry>
         <oasis:entry colname="col3">Lat</oasis:entry>
         <oasis:entry colname="col4">Elevation</oasis:entry>
         <oasis:entry namest="col5" nameend="col6">Annual record </oasis:entry>
         <oasis:entry colname="col7">Total depth</oasis:entry>
         <oasis:entry namest="col8" nameend="col9" align="center">Distance from </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">name</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">(m a.s.l.)</oasis:entry>
         <oasis:entry rowsep="1" namest="col5" nameend="col6"/>
         <oasis:entry colname="col7">used (m)</oasis:entry>
         <oasis:entry rowsep="1" namest="col8" nameend="col9" align="center">SIE (km)<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:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">Years (CE)</oasis:entry>
         <oasis:entry colname="col6">No. samples</oasis:entry>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8">September</oasis:entry>
         <oasis:entry colname="col9">February</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">JUR</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">73.06</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">74.33</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">1139</oasis:entry>
         <oasis:entry colname="col5">1992–2012</oasis:entry>
         <oasis:entry colname="col6">20</oasis:entry>
         <oasis:entry colname="col7">36.9</oasis:entry>
         <oasis:entry colname="col8">1045</oasis:entry>
         <oasis:entry colname="col9">140</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SKBL</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">71.59</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">74.85</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">1419</oasis:entry>
         <oasis:entry colname="col5">1999–2019</oasis:entry>
         <oasis:entry colname="col6">20</oasis:entry>
         <oasis:entry colname="col7">15.0</oasis:entry>
         <oasis:entry colname="col8">1148</oasis:entry>
         <oasis:entry colname="col9">200</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SHIC</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M20" display="inline"><mml:mn mathvariant="normal">99.63</mml:mn></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">72.67</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">474</oasis:entry>
         <oasis:entry colname="col5">1999–2019</oasis:entry>
         <oasis:entry colname="col6">20</oasis:entry>
         <oasis:entry colname="col7">21.3</oasis:entry>
         <oasis:entry colname="col8">753</oasis:entry>
         <oasis:entry colname="col9">130</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Sample preparation and analyses</title>
      <p id="d1e576">All ice cores included in this study were cut using a bandsaw with a steel
blade. Discrete ice core samples were cut at 5 cm resolution for ion
chromatographic analyses using reagent-free Dionex ICS-2500 anion and IC 2000 cation systems in a class-100 clean room. Major ion concentrations were
used to calculate the ionic contributions from marine and continental
sources. The marine sea salt fraction of sodium (ssNa<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>) and the non-sea-salt fraction of calcium (nssCa<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>) were calculated using Eqs. (1)
and (2):

                <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M24" display="block"><mml:mtable rowspacing="4.267913pt" displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">ssNa</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">Na</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>-</mml:mo><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">nssCa</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">crust</mml:mi></mml:msub><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">nssCa</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">Ca</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>-</mml:mo><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">ssNa</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>×</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sea</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">water</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">crust</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sea</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">water</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are the mean ratios (weight
by weight – <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mi>w</mml:mi><mml:mo>/</mml:mo><mml:mi>w</mml:mi></mml:mrow></mml:math></inline-formula>) of <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:math></inline-formula> in the Earth's crust (<inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">crust</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.78</mml:mn></mml:mrow></mml:math></inline-formula>) and in bulk seawater (<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sea</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">water</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.038</mml:mn></mml:mrow></mml:math></inline-formula>), respectively (Bowen, 1979). The non-sea-salt fraction of potassium (nssK<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>) was calculated using Eq. (3):
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M32" display="block"><mml:mrow><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">nssK</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">K</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>-</mml:mo><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msup><mml:mi mathvariant="normal">ssNa</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo>]</mml:mo></mml:mrow><mml:mo>×</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sea</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">water</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">K</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sea</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">water</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">K</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the mean ratio (weight by weight – <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mi>w</mml:mi><mml:mo>/</mml:mo><mml:mi>w</mml:mi></mml:mrow></mml:math></inline-formula>) of <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">K</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:math></inline-formula> in bulk seawater (<inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">sea</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">water</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">K</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.036</mml:mn></mml:mrow></mml:math></inline-formula>) (Piel et al., 2006).</p>
      <p id="d1e978">Microparticle concentration (MPC) was measured on each ice core using a
flow-through Klotz Abakus laser particle counter connected to a continuous
ice core melter system at the British Antarctic Survey (Grieman et al., 2021).</p>
      <p id="d1e981">Diatom samples from each ice core site were previously analysed and reported
by Tetzner et al. (2022a). All diatom samples were extracted by filtration.
Ice core meltwater was filtered through polycarbonate membrane filters (pore
diameter 1.0 <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) and subsequently scanned in a scanning electron
microscope (SEM) following the method presented in Tetzner et al. (2021a).
Observations of diatom preservation were based on the visual identification
of characteristic frustule dissolution features and degradation described in
Warnock and Scherer (2015). Diatom frustules and fragments less than 5 <inline-formula><mml:math id="M38" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> were excluded from counting and identification. Diatom counts per sample (<inline-formula><mml:math id="M39" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>) included all diatom valves, partially obscured diatom valves and
diatom fragments identified in each sample. After processing, diatom counts
per sample (<inline-formula><mml:math id="M40" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>) were represented as their temporal equivalent, diatom
abundance (<inline-formula><mml:math id="M41" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> per year). The diatom abundance parameter includes all diatoms
and diatom remains identified on each sample, regardless of their potential
source. As reported by Tetzner et al. (2022a), the diatom assemblages at all
ice core sites presented in this study are primarily comprised of
<italic>Fragilariopsis cylindrus</italic>, <italic>Fragilariopsis pseudonana</italic>, <italic>Pseudonitzschia</italic> spp., <italic>Shionodiscus gracilis</italic> and <italic>Cyclotella</italic> group., with the exclusive presence of other diatom species at each site (Appendix A – Table A1).</p>
      <p id="d1e1041">All correlations are based on linearly detrended data and calculated using
the Pearson's linear correlation (<inline-formula><mml:math id="M42" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>). Time series linear correlations were
calculated over a 20-year period (1992–2012 CE for JUR and 1999–2019 CE for SHIC and SKBL). Seasons are reported as austral summer (December to
February, DJF), autumn (March to May, MAM), winter (June to August, JJA) and
spring (September to November, SON).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Climate reanalyses and sea ice extension data</title>
      <p id="d1e1059">Monthly reanalysis fields from the fifth generation of the European Centre
for Medium-Range Weather Forecasts (ECMWF), ERA5 (Hersbach and Dee, 2016),
were used to obtain spatial correlations between ice core records and
environmental parameters. Three fields were used to perform spatial
correlation analyses: wind speed (10 m wind speed), precipitation and sea
ice cover. ERA5 datasets provide hourly data available at 0.25<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
resolution (<inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">31</mml:mn></mml:mrow></mml:math></inline-formula> km) since 1979 CE.</p>
      <p id="d1e1081">Sea ice extension data were obtained from the Sea Ice Index version 3
dataset (Fetterer et al., 2017) from the National Snow and Ice Data Centre
(NSIDC), providing monthly sea ice concentrations at 25 km resolution from
1979 to 2021 CE. September sea ice limits (defined as the median northerly
extent of 15 % sea ice cover) were considered the annual sea ice maximum
and February sea ice limits (defined as the median northerly extent of
15 % sea ice cover) were considered the annual sea ice minimum (Thomas et
al., 2019).</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Statistical analyses</title>
      <p id="d1e1092">For each ice core site, the diatom abundance was compared to conventional
ice core wind and atmospheric circulation proxies (ssNa<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, nssCa<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>,
nssK<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> and MPC) and to records of methane sulfonic acid (MSA), a
traditional sea ice proxy. All correlations were based on annual averages
(winter-to-winter). The correlation of chemical, MPC and diatom abundance
records across all ice core sites was carried out using the flux parameter
(except for diatom abundance). Annual fluxes were calculated after
multiplying the annual mean concentration by the estimated annual snow
accumulation (mm of water equivalent). Spatial correlations were calculated
using chemical and MPC mean annual concentrations and diatom abundance.
Spatial correlations were generated using the field correlation tool from
the Royal Netherlands Meteorological Institute (KNMI) Climate Explorer
(<uri>https://climexp.knmi.nl/start.cgi</uri>, last access: 1 July 2021). Spatial correlations were based on linearly detrended data and calculated using the Pearson's linear
correlation (<inline-formula><mml:math id="M48" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>) over the South Pacific sector from 180 to
60<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W and 40 to 90<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, which was selected based on
air mass pathways reaching the ice core sites (Thomas and Bracegirdle,
2015). Based on the records of September sea ice cover between 1992 and 2020 CE (Fetterer et al., 2017), spatial correlations for sea ice cover were
calculated over a reduced region (between 180 to 60<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W and 55 to 90<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S). All linear correlations were calculated over a 20-year period (1992–2012 CE for JUR and 1999–2019 CE for SHIC and SKBL). The MPC record from JUR covers the interval 1992–2011 CE; therefore, correlations calculated using this parameter at JUR are calculated over a 19-year period. Since diatom concentrations at SHIC peak during the austral summer (Tetzner et al., 2022a), spatial correlations for the SHIC diatom record were also calculated over a 6-month period covering the austral spring and summer season (September–February).</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Jurassic ice core (JUR)</title>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>Chemistry, MPC and diatom abundance annual records</title>
      <p id="d1e1195">The JUR chemical fluxes, MPC flux and diatom abundance records are
characterized by positive trends during the 1992-2012 CE period, with the
exception of the MSA flux, which exhibits a negative trend (Fig. 2, Table S1 in the Supplement). Of them, only the nssCa<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> flux and nssK<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> fluxes were statistically significant (<inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (Table S1). The nssCa<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> flux shows a steady increase, reaching a maximum between 2010 and 2011 CE. The nssK<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux shows a similar pattern with values increasing steadily after 2002 CE. The ssNa<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux is moderately variable from 1992 to 2012 CE, with an overall increase between 2000 and 2002 CE. The MSA flux displays an overall decrease between 1992 and 2003 CE, followed by a general increase during 2003 and 2012 CE. Similarly, the MPC exhibits an increase during 1992–2012 CE with its lowest values during 1998 CE. The diatom abundance is moderately variable between 1992 and 2004 CE, followed by a marked increase after 2004 CE, reaching its highest value during 2009–2010 CE (Fig. 2). Similar features were present in the JUR chemical and MPC concentration records (Table S2 and Fig. S1 in the Supplement).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1264">Time series of chemical species fluxes, MPC flux and diatom abundance for each ice core site. Data points represent the annual austral winter-to-winter average and were plotted over the correspondent austral summer. Colour-coded dashed lines show statistically significant linear trends (<inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). The MPC flux record from JUR covers the interval 1992–2011 CE. Data presented in panel <bold>(a)</bold> were previously presented by Tetzner et al. (2022a).</p></caption>
            <?xmltex \igopts{width=327.206693pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/1709/2022/cp-18-1709-2022-f02.png"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>Environmental correlations</title>
      <p id="d1e1296">All records (excluding MSA) presented strong and significant correlations
with wind strength (<inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>; Appendix B – Fig. B1). Diatom abundance is positively correlated with wind
strength (<inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.67</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) over a latitudinal band at
the northern limit of the Amundsen Sea (<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) and negatively correlated with the sea ice cover north of the SHIC ice core
drilling site (<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≥</mml:mo><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.69</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 3). The MPC
is positively correlated with wind strength over the east coast of Argentina
(<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.73</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). The nssCa<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> exhibits a positive correlation with wind strength (<inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.62</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and with precipitation (<inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.77</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) off the western coast of southern South America. The nssK<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> shows a positive correlation with wind strength (<inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.66</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) over the Amundsen Sea. The ssNa<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> is positively correlated with wind strength over the Drake Passage (<inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and over Ellsworth Land (<inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.63</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). No significant correlations were identified with wind strength or precipitation at or near the JUR ice core drilling site. No strong correlations (<inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) between the MSA record and sea ice cover were identified in the region.</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="d1e1645">Regional maps showing spatial correlations between environmental
parameters and diatom abundance. Colour-coded polygons in the maps indicate
highly correlated regions (<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn></mml:mrow></mml:math></inline-formula>). All polygons
plotted are statistically significant (<inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). The pale grey latitudinal band indicates the core of the Southern Hemisphere westerly wind (SHWW) belt. Pale blue polygons indicate the region covered by seasonal sea ice. Pale orange polygons indicate the region covered by perennial sea ice. Black squares represent a <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> quadrant around the point of highest correlation (QHC) between wind strength and diatom abundance. Regional maps only present areas of spatial correlation larger than <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>. Degrees of freedom (DF) for each spatial
correlation can be obtained using the following expression dependent on the
sample size (<inline-formula><mml:math id="M91" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>): DF <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/1709/2022/cp-18-1709-2022-f03.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Sky-Blu ice core (SKBL)</title>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Chemistry, MPC and diatom abundance annual records</title>
      <p id="d1e1770">The SKBL chemical fluxes, MPC flux and diatom abundance records are
characterized by negative trends during the 1999–2019 CE period (Fig. 2)
(Table S1). Among these trends, only MPC, nssCa<inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and nssK<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> fluxes exhibited linear trends that were statistically significant (<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). The diatom abundance is characterized by moderate interannual variability and single major increases during 1999–2000, 2002–2003 and 2009–2010 CE, with the latter presenting the absolute highest value (77 <inline-formula><mml:math id="M96" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> yr<inline-formula><mml:math id="M97" 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>). A major increase in MSA flux was also registered during 2003 CE (Fig. 2). Similar features were present in the SKBL chemical concentration and MPC records (Table S2, Fig. S1).</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Environmental correlations</title>
      <p id="d1e1833">The diatom abundance, chemical and MPC records from SKBL were compared to
environmental parameters over the 1999–2019 CE period (Appendix B – Fig. B1). Two records are highly correlated with wind strength: the diatom
abundance and ssNa<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>. Diatom abundance exhibits a positive correlation
with wind strength (<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.78</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) over a latitudinal band (<inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) extending from the Ross Sea to the Amundsen Sea and a negative correlation with the sea ice cover (<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≥</mml:mo><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.71</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) over the Amundsen Sea Embayment (Fig. 3). The ssNa<inline-formula><mml:math id="M105" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> is positively correlated with wind strength (<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.75</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) off the west coast of South America at <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">45</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. No correlations were identified between the ice core records and wind strength or precipitation over the SKBL ice core drilling site. No strong correlations (<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) between the MSA record and sea ice cover were identified in the region.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Sherman Island ice core (SHIC)</title>
<sec id="Ch1.S3.SS3.SSS1">
  <label>3.3.1</label><title>Chemistry, MPC and diatom abundance annual records</title>
      <p id="d1e2022">The SHIC chemical fluxes, MPC flux and diatom abundance records present
contrasting features over the 1999–2019 CE period (Fig. 2, Table S1). Negative linear trends are observed in nssCa<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> flux, nssK<inline-formula><mml:math id="M113" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux and MSA flux. The ssNa<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux exhibits a positive trend with values reaching an absolute maximum during 2015 CE. The MSA flux was relatively constant over the 1999–2014 CE period. After 2014 CE, MSA flux decreases, reaching its absolute minimum between 2018 and 2019 CE. The MPC flux shows a steady increase after 2008–2009 CE, reaching its highest value in 2018–2019 CE. The diatom abundance exhibits a positive trend (2.16 <inline-formula><mml:math id="M115" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> yr<inline-formula><mml:math id="M116" 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>, <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) with a strong interannual variability which describes a semi-periodic 3-year pattern (Fig. 2). Similar features were present in the SHIC chemical concentration and MPC records (Table S2, Fig. S1).</p>
</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <label>3.3.2</label><title>Environmental correlations</title>
      <p id="d1e2095">The diatom abundance, chemical and MPC records from SHIC were compared to
environmental parameters over the 1999–2019 CE period (Appendix B – Fig. B1). Diatom abundance, MPC and ssNa<inline-formula><mml:math id="M118" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> are highly correlated with wind strength over the 1999–2019 CE period. Annual diatom abundance is positively correlated with wind strength (<inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.61</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) over the Bryan Coast sector (Fig. 3). The spring–summer diatom abundance is
positively correlated with wind strength over a latitudinal band at the
northern limit of the Bellingshausen Sea (<inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) (<inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.64</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>), over the Bryan Coast (<inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.64</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and over the Amundsen Sea Embayment (<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.71</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 3). In parallel, the spring–summer diatom abundance is positively correlated with the sea ice cover over the Amundsen Sea (<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.81</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 3). MPC is positively correlated with precipitation (<inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.66</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) over the SHIC drilling site. Conversely, MPC is negatively correlated with precipitation off the southern coast of South America (<inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≥</mml:mo><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.65</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). The ssNa<inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> is positively correlated with sea ice (<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) to the west and north-west of the SHIC drilling site. No clear correlations were identified with the nssCa<inline-formula><mml:math id="M138" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and nssK<inline-formula><mml:math id="M139" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> records. No strong correlations (<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) between the MSA record and sea ice cover were identified for the SHIC site.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Correlation of ice core records</title>
      <p id="d1e2421">Linear correlations were calculated between the annual chemical and MPC
fluxes, as well as diatom abundance records across all ice core sites
(Table S3). Strong positive and statistically significant (<inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) correlations were identified between nssCa<inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> flux and nssK<inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux in SHIC, JUR and SKBL (<inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.48</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.82</mml:mn></mml:mrow></mml:math></inline-formula>, respectively) and between ssNa<inline-formula><mml:math id="M148" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux and MSA flux in SHIC, JUR and SKBL (<inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.63</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.52</mml:mn></mml:mrow></mml:math></inline-formula>, respectively). Diatom abundance and ssNa<inline-formula><mml:math id="M152" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux exhibited strong and significant correlations (<inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) across all the ice core sites (<inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.47</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.46</mml:mn></mml:mrow></mml:math></inline-formula>, for SHIC, JUR and SKBL, respectively). The only statistically significant correlation in the same proxy across the sites was between diatom abundance in the JUR and SKBL cores (<inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.84</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). No clear or consistent pattern was identified when comparing chemical proxies from different ice core sites.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Temporal variability of the diatom record</title>
      <p id="d1e2639">The diatom abundance preserved in ice cores reveals a strong interannual
variability across the AP and EL regions from 1992 to 2019 CE. The relationships between diatom abundance and environmental parameters at the ice core drilling sites are weak and not statistically significant, indicating that conditions at the ice core site are not drivers of the diatom temporal
variability, in agreement with previous studies concluding that ice core
diatom records are not dependent on annual snow accumulation or local wind
conditions (Allen et al., 2020; Tetzner et al., 2022a).</p>
      <p id="d1e2642">Spatial correlations of annual wind strength and the annual diatom abundance
preserved in ice cores reveal regions of significant positive correlations
(<inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.78</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 3). These regions match the oceanographic zones indicated by the ecology of the dominant marine diatom taxa well (Tetzner et al., 2022a). Furthermore, the neighbouring ice core sites of JUR and SKBL share similar regions of spatial correlation
(<inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.78</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 3). Numerous studies have highlighted the relationship between wind strength and sea spray production (Blanchard, 1963; Schlichting, 1974; Monahan et al., 1983; Callaghan et al., 2008; Löndahl, 2014; Tesson et al., 2016; Wiśniewska et al.,  2019;
Marks et al., 2019). Stronger winds have been shown to enhance the
production of sea spray aerosols, including microalgae, which implies an
increased transfer of diatoms from the sea surface microlayer into the
atmosphere (Marks et al., 2019). Studies on regional atmospheric circulation
confirm that air masses from these regions are effectively transported to
ice core sites (Thomas and Bracegirdle, 2009; Abram et al., 2010; Thomas and
Bracegirdle, 2015; Allen et al., 2020), therefore establishing an efficient
transport pathway from the identified source regions to the ice core sites.</p>
      <p id="d1e2701">Two oceanographic zones were highlighted in the spatial correlation analyses
for their strong link between changes in wind strength and changes in diatom
abundance: the seasonal sea ice zone (SSIZ) and permanently open ocean zone
(POOZ). The JUR and SKBL diatom records were correlated exclusively with
winds in the POOZ (northern Amundsen Sea), and the SHIC spring–summer diatom
record was correlated with regions from both the SSIZ (Bryan Coast sector
and Amundsen Sea Embayment) and POOZ (northern Bellingshausen Sea) (Fig. 3). It is important to note that these regions of spatial correlation agree
with the oceanographic affiliations of the diatom assemblages for the
respective ice cores (coastal vs. inland sites) reported by Tetzner et al. (2022a). Despite the correlation between the SHIC spring–summer diatom
record and winds in the POOZ, the diatom assemblages for SHIC support a
stronger link with the SSIZ (Tetzner et al., 2022a). Therefore, discussion
for the SHIC diatom record will be focused on environmental changes within
the SSIZ. The correlation between the SHIC summer–spring diatom record and
winds in the POOZ (Fig. 3) is likely explained by the close association
between regional atmospheric circulation (SHWW), sea ice dynamics and
primary productivity in the Amundsen–Bellingshausen seas (Arrigo et al., 2008; Soppa et al., 2016).</p>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>SSIZ controls on diatom variability at a coastal site (SHIC)</title>
      <p id="d1e2711">The SSIZ is identified as the dominant source region by both the spatial
correlation analyses and the ecological associations of the SHIC diatom
record (Tetzner et al., 2022a). Wind strength and sea ice dynamics play an
important role in driving the primary productivity in diatom source regions
within the SSIZ (Arrigo et al., 2008, 2012). In the Bryan Coast and Amundsen Sea Embayment, winds drive sea ice northward, producing large ice-free areas (polynyas) near the coast (Arrigo et al., 2012; Holland
and Kwok, 2012). These coastal polynyas have been identified as among the
most productive regions in the Southern Ocean (Arrigo et al., 2008; Soppa et
al., 2016). The stronger link to wind strength during the austral spring and
summer (Fig. 3) and strong seasonality identified in the sub-annual diatom record reflect the enhanced austral spring–summer primary productivity in these regions (Arrigo et al., 2008; Soppa et al., 2016; Tetzner et al., 2022a). This suggests that the interannual diatom
variability at this site is not exclusively driven by wind strength, but is
also dependent on sea ice dynamics and/or primary productivity. Previous
studies have identified recent reductions in the ice-covered days (sea ice
concentration) during the austral summer (Stammerjohn et al., 2012) and the
development of coastal polynyas (Eltanin Polynya, Pine Island Polynya and
Amundsen Sea Polynya) within the coastal regions identified as the SHIC
diatom sources (Arrigo and van Dijken, 2003; Arrigo et al., 2012). Both lead
to prolonged and increased biogenic primary productivity near the ice core
site. Greater sea ice breakup and more open water in summer often result in
larger phytoplankton blooms (Soppa et al., 2016). A prolonged ice-free
diatom source and/or recently enhanced primary productivity will increase
the availability of diatoms on the ocean surface, favouring potentially
larger entrainments of diatoms by strong winds. This is consistent with the
recent large decadal increases seen in the SHIC diatom concentration
(Tetzner et al., 2022a).</p>
      <p id="d1e2714">The clear link identified between the seasonality of the diatom record and
sea ice primary productivity is complemented by the strong relationship
between the austral spring–summer diatom abundance and sea ice cover over
the Amundsen Sea. However, no direct relationship was observed between the
diatom abundance and the sea ice cover directly in the vicinities of SHIC
(Fig. 3). This is consistent with the lack of correlation between MSA and
sea ice at this site, despite previous studies observing a positive
relationship between MSA and sea ice extent in this region (Abram et al., 2010; Thomas and Abram, 2016). These findings suggest that diatom (and MSA) variability at SHIC is not exclusively driven by either marine primary
productivity or changes in sea ice cover. This can be explained by the
effect of a bidirectional pattern of winds at SHIC, drawing air masses from
both the east coast (Bryan Coast) and the west coast (Amundsen Sea
Embayment) (Tetzner et al., 2019), resulting in two distinct sources of
aerosols to the ice core site. Additionally, the onset of the sea ice
breakup and duration of ice-free conditions at the Bryan Coast, Eights Coast
and the Amundsen Sea Embayment do not follow a clear pattern. Some years
present these coastal regions as completely ice-free, while others present
either one or more of these regions as ice-covered (Arrigo et al., 2008). The
development of coastal polynyas near SHIC (see Fig. 1) will contribute to
the increased availability of diatoms in some years (Arrigo and van Dijken,
2003; Arrigo et al., 2015). The potential input of diatoms from coastal
sources from opposite directions, along with the variability in the
distribution and duration of the sea ice cover and the occasional
development of coastal polynyas, adds an additional and non-negligible source
of variability to the diatom record at SHIC.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>POOZ controls on diatom variability at inland sites (JUR and SKBL)</title>
      <p id="d1e2726">The diatom source region identified by the spatial correlation analyses and
diatom ecological affiliations for JUR and SKBL is in the northern Amundsen
Sea within the POOZ (Figs. 1 and 3). This oceanographic zone is characterized by the lowest seasonal and interannual variability in primary productivity for the whole SO (Arrigo et al., 2008; Soppa et al., 2016). The
absence of sea ice in the POOZ reduces the seasonal extremes in primary
productivity evident within the SSIZ (Tetzner et al., 2022a). The diatom
availability in the northern Amundsen Sea POOZ presents a low variability
year-round (Arrigo et al., 2008; Soppa et al., 2016), limiting the impact of
interannual changes in primary productivity on the diatom record and
upholding the idea that temporal variability in the JUR and SKBL diatom records is
derived mainly from changes in wind strength at the source. This POOZ source
is also supported by back-trajectory analyses showing that air masses reaching
high-elevation sites on the Antarctic Peninsula are a
considerable distance over the ocean at sea level and are higher in the atmosphere when
they traverse the peninsula coast (Thomas and Bracegirdle, 2015; Allen et
al., 2020). The marine source region supplying diatoms to JUR and SKBL is in
the core of the SHWW belt. The significant positive correlation between wind
strength and annual diatom abundance (<inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.78</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) demonstrates that the diatom records from these sites can be used as a proxy
for interannual changes in the strength of the SHWWs. However, changes in
ocean primary productivity may contribute to diatom variability over longer
timescales.</p>
      <p id="d1e2757">Results presented here are consistent with the relationship identified
between SHWW strength and diatoms in an EL ice core (Allen et al., 2020).
Specifically, our results show close agreement with the location
(50–60<inline-formula><mml:math id="M165" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 140<inline-formula><mml:math id="M166" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) and magnitude of the strongest
correlation (<inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.61</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) between annual SHWW anomalies and
calibrated diatom flux at the Ferrigno ice core site (Fig. 1) (Allen et
al., 2020). Unlike JUR and SKBL, the Ferrigno diatom assemblage was
characterized by the absence of sea ice diatoms. This can be explained by
the more north-westerly location of the Ferrigno diatom source (compared to
the JUR and SKBL source region) that is less likely to receive inputs from
the SSIZ. Additionally, the absence of sea ice diatoms at Ferrigno supports
the conclusion that inland sites have limited influence from low-elevation
air masses in contact with the SSIZ (Tetzner et al., 2022a).</p>
</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <label>4.1.3</label><title>Recent regional environmental changes and the diatom record</title>
      <p id="d1e2810">Ice core diatom records have the potential to capture regional environmental
changes. The correlation between the annual diatom abundance variability at
JUR and SKBL and changes in the wind strength in the SHWW belt (Figs. 3, 4a and b) strongly suggests that the recent increase in diatoms at
these ice core sites (Tetzner et al., 2022a) is driven by a strengthening of
the SHWW belt during the satellite era (Mayewski et al., 2013; Young and
Ribal, 2019; Goyal et al., 2021). This link is further supported by
sea spray production experiments showing that a <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> % increase in wind strength (<inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> m s<inline-formula><mml:math id="M171" 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>) has the potential to double the production of spume drops and sea spray aerosol, including microalgae (Monahan et al., 1986; Wu, 1993; Anguelova et al., 1999). Increasing the entrainment of aerosols into the atmosphere would likely increase the supply of diatoms to the ice core sites and therefore the number of diatoms contained in the ice. Despite SHIC exhibiting a similar increase in annual diatom abundance, the intrinsic relationship between the SHIC diatom record, the sea ice cover in SSIZ and winds over the SSIZ prevents establishing a direct link between the increases in annual diatom abundance at SHIC and the strengthening of the SHWW belt (Fig. 4c).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e2852">Time series of diatom abundance and mean wind speed inside the quadrants of highest correlation (QHC) for each ice core site highlighted in Fig. 3. Data points represent the annual austral winter-to-winter average and were plotted over the correspondent austral summer. Colour-coded symbols for the SHIC ice core represent the time series of wind speed on each QHC identified for that site. QHC-BS: quadrant of high correlation over the
Bellingshausen Sea. QHC-ASE: quadrant of high correlation over the
Amundsen Sea Embayment. QHC-BC: quadrant of high correlation over the
Bryan Coast.</p></caption>
            <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/1709/2022/cp-18-1709-2022-f04.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>The diatom wind proxy and the traditional ice core wind and atmospheric circulation proxies</title>
      <p id="d1e2870">We have demonstrated that the annual diatom abundance shows promise as a
wind proxy for SHWW at multiple sites. To assess the full scope and validity
of this novel proxy, we compared the new diatom records with established ice
core wind and atmospheric circulation proxies.</p>
      <p id="d1e2873">MPC, nssCa<inline-formula><mml:math id="M172" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, ssNa<inline-formula><mml:math id="M173" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> and nssK<inline-formula><mml:math id="M174" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> have been used to infer past
variability in regional-to-hemispheric atmospheric circulation from annual
to millennial timescales. Our results reveal the limitations in these
traditional proxies, which fail to reproduce the interannual variability of
wind strength upwind from the ice core sites. Even though many of these
records show a strong link with wind strength, their region of correlation
did not fit  their expected sources and was not consistent between
sites. This refutes a direct link between wind strength and  in situ
aerosol production. For example, there are strong correlations between
continental ions and wind strength over regions in the middle of the ocean,
where it is not feasible to entrain continental ions (JUR nssK<inline-formula><mml:math id="M175" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>
record). Similarly, some records are strongly linked to other environmental
parameters such as precipitation, suggesting that source (JUR nssCa<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>
record) or site conditions (MPC record at SHIC), rather than wind strength,
dominate the variability of these species. Some proxies (MPC at JUR and
ssNa<inline-formula><mml:math id="M177" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> at SKBL) were strongly linked to wind strength over regions north
(<inline-formula><mml:math id="M178" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 40–45<inline-formula><mml:math id="M179" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) of the core of the SHWW belt (Appendix B – Fig. B1). These results suggest that those records could indicate changes in wind strength over continental or marine regions far from the
core of the SHWW belt. Previous studies have demonstrated  that MPC and chemical
species are valuable records to infer past changes in
regional-to-hemispheric wind regimes and atmospheric circulation. However,
it must be acknowledged that the variability of these tracers represents the
cumulative effect of several factors (McConnell et al., 2007; Lambert et
al., 2008; Li et al., 2010; Wolff et al., 2010; Bullard et al., 2016;
Delmonte et al., 2017). These include (1) wind strength at the source(s),
(2) air mass transport pathways, (3) primary production of the tracer at the
source(s), (4) the humidity and precipitation while transported in the atmosphere, and (5) snow accumulation rate in Antarctica. The numerous factors influencing the variability of these records hinder their capacity to accurately represent changes in winds strength. Despite our results
confirming that these tracers are not the ideal records to infer past wind strength
variability, they do not invalidate their use to reconstruct wind and
atmospheric circulation changes in a broad sense. Additionally, our results
highlight the need for a thorough site and proxy evaluation before using
these chemical and MPC species to reconstruct wind changes through time.</p>
      <p id="d1e2953">The ssNa<inline-formula><mml:math id="M180" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux was the only record with a regionally consistent
relationship with the diatom abundance (yellow cells in Table S3). Despite the strong correlations at each ice core site,
they presented opposite signs (<inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> for JUR and <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> for
SHIC and SKBL), suggesting that the interannual variability of diatom
abundance and ssNa<inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> flux is not driven exclusively by the same
environmental parameters across the AP and EL region.</p>
      <p id="d1e2998">Correlation analyses of ice core proxies between sites confirm that diatom
abundance is the only record with a consistent, statistically significant
and strong correlation (JUR vs. SKBL, <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.84</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) (grey cell
in Table S3), supporting the regional validity of the diatom-based wind proxy at the high-elevation sites.</p>
      <p id="d1e3026">Previous studies have proposed MPC as a proxy for winds and atmospheric
circulation in the AP and EL region (Mosley-Thompson et al., 1990, 1991; Thompson et al., 1994), suggesting that the MPC record is indicative of long-term regional environmental changes. However, low background concentrations reported in those studies suggest that the
MPC annual record from the AP and EL region could be biased by the
occurrence of sporadic major dust events reaching the high southern
latitudes (Li et al., 2010). Our results are in close agreement, showing
that the regional MPC record preserved in ice cores from the AP and EL is
not a robust indicator of interannual wind strength variability, possibly
due to the numerous factors driving MPC variability. In contrast, the WAIS
Divide ice core in neighbouring Marie Byrd Land revealed a link between the
coarse particle percentage (analogous to MPC) and interannual zonal wind
strength variability at both 700 and 850 hPa over the satellite era
(<inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.3–0.5, <inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>) (Koffman et al., 2014). This contrasting
behaviour can be partly explained by the diametrically opposed continental
regions supplying mineral dust to Antarctica (Sudarchikova et al., 2015;
Neff and Bertler, 2015) and the higher dependence of Antarctic Peninsula
sites on extreme precipitation events (Turner et al., 2019). Similarly,
differences in transport pathways and the role of local meteorology have
also been used to explain the different behaviour observed in sea ice
proxies (MSA) around Antarctica (Abram et al., 2013; Thomas et al., 2019).
Our findings provide further evidence that ice core proxies perform
differently depending on the geographical region and the temporal resolution
over which they are assessed.</p>
      <p id="d1e3051">The temporal variability of chemical tracers (nssCa<inline-formula><mml:math id="M188" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, nssK<inline-formula><mml:math id="M189" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>,
ssNa<inline-formula><mml:math id="M190" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>) in a network of ice cores across Marie Byrd Land (ITASE) has
been proposed as a tracer of long-term (multi-year) changes in atmospheric
circulation (Dixon et al., 2012; Mayewski et al., 2013). However, only
nssCa<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> proved reliable in capturing interannual variability in
atmospheric circulation patterns over the satellite era (<inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.37</mml:mn><mml:mo>≤</mml:mo><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.59</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>), although not directly related to wind strength but
to northerly air mass incursions (Dixon et al., 2012). Thus, there is
clearly a need for a reliable proxy for past wind strength in this important
region of Antarctica. Based on our results, we propose that diatoms show the
most promise as a tool to reconstruct the interannual variability of SHWW
strength.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Recommendations</title>
      <p id="d1e3133">Our findings demonstrate that diatoms show the most promise as a proxy for
past wind strength in AP and EL ice cores when compared with a range of
traditional chemical and MPC records. At inland sites, diatom abundance is
most strongly dependent on annual changes in the strength of the SHWWs and
has excellent potential as a proxy to reconstruct past changes in the
strength of the SHWWs over the northern Amundsen Sea.</p>
      <p id="d1e3136">Based on our results, we propose three candidate ice core sites across the
AP and EL region where multi-decadal to centennial-scale reconstructions of
winds could be achieved: the Jurassic, Ferrigno and Palmer ice cores (Thomas
and Bracegirdle, 2015) (see Fig. 1). Evaluations have already confirmed
the suitability of the JUR site (this study) and the Ferrigno site (Allen et
al., 2020) in reproducing recent changes in the SHWW strength. Previous
studies on the Ferrigno ice core have confirmed that this ice core covers
the last 3 centuries (Thomas et al., 2015; Thomas and Abram, 2016),
making it a good candidate for extending an SHWW reconstruction back to the
core of the Little Ice Age (<inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1700</mml:mn></mml:mrow></mml:math></inline-formula> CE), while the JUR site has
the potential to capture changes over the last 140 years (Emanuelsson et
al., 2022). The diatom record from the Palmer ice core has not yet been
explored; however, this high-elevation, low-snow-accumulation site (Thomas
and Bracegirdle, 2015) has the potential to hold a 390-year record
(Emanuelsson et al., 2022), one of the longest records in the region. An
annually resolved wind strength reconstruction from any of these three ice
cores will establish if the recent intensification of the SHWW belt is
unprecedented over the last few centuries and will clearly identify the
timing of onset (Abram et al., 2013; Koffman et al., 2014; Turney et al., 2016; Perren et al., 2020).</p>
      <p id="d1e3149">Despite the consistency of the observations presented in this work, it must
be acknowledged that they are from a particular region in Antarctica.
Antarctica is a vast continent with contrasting environmental conditions in
different sectors (Jones et al., 2016; Stenni et al., 2017; Thomas et al., 2017, 2019). Thus, we recommend conducting a detailed assessment of the diatom proxy outside the AP–EL regions.</p><?xmltex \hack{\newpage}?>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e3163">Ice cores capture changes in past wind strength and atmospheric variability,
with several chemical and microparticles suggested as potential proxies. In
this study, we propose an exciting new wind proxy based on diatoms that
performs better than traditional ice core wind proxies in ice cores from the
southern Antarctic Peninsula and Ellsworth Land. A set of ice cores from
this region have been analysed to demonstrate that the temporal variability
of the diatom record preserved in inland ice cores is exclusively driven by
changes in the wind strength within the core of the Southern Hemisphere
westerly wind belt, while the temporal variability of the diatoms preserved
in coastal ice cores is driven by a combination of wind strength and sea ice
dynamics within the seasonal sea ice zone.</p>
      <p id="d1e3166">The lack of coherence between ice core chemical and dust proxies at sites
from the same region suggests that these proxies should be used with caution.
For these proxies, both the production at the source and the deposition at
the ice core sites drive the variability, making it hard to resolve the
signal of wind strength. These findings demonstrate the importance of a
thorough site evaluation before extending environmental interpretations back
in time, with no single proxy suitable for reconstructions across all of
Antarctica.</p>
      <p id="d1e3169">We propose that the diatom record preserved in ice cores from the Antarctic
Peninsula and Ellsworth Land regions is the optimal proxy for reconstructing
the interannual wind strength variability in the Pacific sector of the
Southern Hemisphere westerly wind belt. Further research should be focused
on expanding the study of the diatom record and its potential as a wind
proxy in other regions of Antarctica and over longer timescales.</p><?xmltex \hack{\clearpage}?>
</sec>

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

<app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title/>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S1.T2"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{A1}?><label>Table A1</label><caption><p id="d1e3187">Relative abundance (%) and frequency (no. of samples) of main
diatom taxa in annual diatom records for each ice core. (<inline-formula><mml:math id="M195" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula>) Specimens of
<italic>Cyclotella</italic> sensu lato (including <italic>Lindavia</italic>, <italic>Discostella</italic>, <italic>Tertiarius</italic> and <italic>Pantocsekiella</italic>). (s): sea-ice-affiliated diatom. (o-SSIE): open ocean – diatom affiliated with the seasonal sea ice edge. (o-POOZ): open ocean – diatom species or group affiliated with the permanently open ocean zone. Table modified from Tetzner et al. (2022a).</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.92}[.92]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">SHIC</oasis:entry>
         <oasis:entry colname="col3">JUR</oasis:entry>
         <oasis:entry colname="col4">SKBL</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Annual record</oasis:entry>
         <oasis:entry colname="col2">(1999–2019 CE)</oasis:entry>
         <oasis:entry colname="col3">(1992–2012 CE)</oasis:entry>
         <oasis:entry colname="col4">(1999–2019 CE)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Fragilariopsis cylindrus</italic> (s)</oasis:entry>
         <oasis:entry colname="col2">63.7 % (20)</oasis:entry>
         <oasis:entry colname="col3">18.2 % (14)</oasis:entry>
         <oasis:entry colname="col4">21.3 % (15)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Shionodiscus gracilis</italic> (o-SSIE)</oasis:entry>
         <oasis:entry colname="col2">18.5 % (18)</oasis:entry>
         <oasis:entry colname="col3">17.6 % (17)</oasis:entry>
         <oasis:entry colname="col4">10.9 % (10)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Fragilariopsis curta</italic> (s)</oasis:entry>
         <oasis:entry colname="col2">4.1 % (10)</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Fragilariopsis pseudonana</italic> (o-POOZ)</oasis:entry>
         <oasis:entry colname="col2">3.6 % (11)</oasis:entry>
         <oasis:entry colname="col3">9.2 % (11)</oasis:entry>
         <oasis:entry colname="col4">15.3 % (10)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Cyclotella</italic> group<inline-formula><mml:math id="M196" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">6.8 % (19)</oasis:entry>
         <oasis:entry colname="col3">29.1 % (19)</oasis:entry>
         <oasis:entry colname="col4">37.2 % (20)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Navicula</italic> group</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
         <oasis:entry colname="col3">7.4 % (12)</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Nitzschia</italic> group</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">6 % (12)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Pseudonitzschia</italic> spp. (o-POOZ)</oasis:entry>
         <oasis:entry colname="col2">3.3 % (10)</oasis:entry>
         <oasis:entry colname="col3">6.5 % (7)</oasis:entry>
         <oasis:entry colname="col4">9.3 % (8)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Achnanthes</italic> group</oasis:entry>
         <oasis:entry colname="col2">–</oasis:entry>
         <oasis:entry colname="col3">11.9 % (10)</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</app>

<app id="App1.Ch1.S2">
  <?xmltex \currentcnt{B}?><label>Appendix B</label><title/>

      <?xmltex \floatpos{b!}?><fig id="App1.Ch1.S2.F5"><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Figure}?><label>Figure B1</label><caption><p id="d1e3435">Regional maps showing spatial correlations between environmental parameters and chemical species, MPC and diatom abundance. Colour-coded polygons in the maps indicate highly correlated regions (<inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>≤</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>). All polygons plotted are statistically significant (<inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). Pale grey latitudinal band indicates the core of the Southern Hemisphere westerly wind (SHWW) belt. Pale blue polygons indicate the region covered by seasonal sea ice. Pale orange polygons indicate the region covered by perennial sea ice. Black squares represent a <inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> quadrant around the point of highest correlation (QHC) between wind strength and diatom abundance. Spatial correlations between MSA and environmental parameters were excluded because they were below the threshold (<inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>&gt;</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>). Regional maps only present areas of spatial correlation larger than <inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>. Degrees of freedom (DF) for each spatial correlation can be obtained using the following expression dependent on the sample size (<inline-formula><mml:math id="M205" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>); DF <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
        <?xmltex \hack{\hsize\textwidth}?>
        <?xmltex \igopts{width=441.017717pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/1709/2022/cp-18-1709-2022-f05.png"/>

      </fig>

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

      <p id="d1e3590">Datasets original to this work will be available at the UK Polar Data Centre (<ext-link xlink:href="https://doi.org/10.5285/9ce1fd9f-cfaf-44fa-aa5d-45c24c0a76cc" ext-link-type="DOI">10.5285/9ce1fd9f-cfaf-44fa-aa5d-45c24c0a76cc</ext-link>, Tetzner et al., 2022b).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e3596">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/cp-18-1709-2022-supplement" xlink:title="zip">https://doi.org/10.5194/cp-18-1709-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e3605">DRT did the initial conceptualization. DRT and MMG were in charge of data curation. DRT, ERT and CSA conducted the formal analysis. DRT was in charge of the investigation. DRT, ERT and CSA designed the methodology. DRT prepared the original paper. ERT, CSA and MMG contributed to the reviewing and editing of the original paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e3611">At least one of the (co-)authors is a member of the editorial board of <italic>Climate of the Past</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e3620">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3626">We would like to thank Sarah Crowsley, Tom King, Isobel Rowell and Dr. Robert
Mulvaney for their help while drilling the SHIC and SKBL ice cores included
in this work. We would like to thank Shaun Miller, Jack Humby, Diana
Vladimirova and Daniel Emanuelsson from the Ice Core Lab, British
Antarctic Survey, for their help while cutting the ice and conducting the
continuous flow analysis (CFA). We would like to thank Eric Wolff
from the Earth Sciences Department, University of Cambridge, for his
valuable comments during the final review and editing of this paper.
SEM work was partly supported by a Royal Society Research Professorships
Enhancement Award (RP/EA/180006). We would like to thank Iris Buisman and   Giulio Lampronti from the Microscopy Lab, Earth Sciences Department, University of Cambridge, for their technical support in the use of the SEM. Fieldwork conducted for this research was supported by the Collaborative Antarctic Science Scheme (CASS-168). This research was funded by CONICYT–Becas Chile and Cambridge Trust funding programme for PhD studies under grant number 72180432. Finally, the authors thank two anonymous reviewers and the editor for their constructive comments that led to an improved paper.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e3631">This research has been supported by the Comisión Nacional de Investigación Científica y Tecnológica (grant no. 72180432).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e3637">This paper was edited by Barbara Stenni and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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