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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-12-1435-2016</article-id><title-group><article-title>Constant wind regimes during the Last Glacial Maximum and early Holocene:
evidence from Little Llangothlin Lagoon, New England Tablelands, eastern
Australia</article-title>
      </title-group><?xmltex \runningtitle{Constant wind regimes during the Last Glacial Maximum and early Holocene}?><?xmltex \runningauthor{J.~Shulmeister et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Shulmeister</surname><given-names>James</given-names></name>
          <email>james.shulmeister@uq.edu.au</email>
        <ext-link>https://orcid.org/0000-0001-5863-9462</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Kemp</surname><given-names>Justine</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Fitzsimmons</surname><given-names>Kathryn E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9337-0793</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff5">
          <name><surname>Gontz</surname><given-names>Allen</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of Geography, Planning and Environmental Management, University of
Queensland, St. Lucia 4072, Queensland, Australia</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Australian Rivers Institute, Griffith University, Nathan 4111, Queensland,
Australia</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Human Evolution, Max Planck Institute for Evolutionary
Anthropology, Deutscher Platz 6, 04103 Leipzig, Germany</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>School for the Environment, University of Massachusetts Boston, Boston, MA
02125, USA</institution>
        </aff>
        <aff id="aff5"><label>a</label><institution>current address: Department of Geological Sciences, San Diego State
University, San Diego, CA 92182, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">James Shulmeister (james.shulmeister@uq.edu.au)</corresp></author-notes><pub-date><day>5</day><month>July</month><year>2016</year></pub-date>
      
      <volume>12</volume>
      <issue>7</issue>
      <fpage>1435</fpage><lpage>1444</lpage>
      <history>
        <date date-type="received"><day>24</day><month>March</month><year>2016</year></date>
           <date date-type="rev-request"><day>6</day><month>April</month><year>2016</year></date>
           <date date-type="accepted"><day>2</day><month>June</month><year>2016</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016.html">This article is available from https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016.html</self-uri>
<self-uri xlink:href="https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016.pdf">The full text article is available as a PDF file from https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016.pdf</self-uri>


      <abstract>
    <p>Here we present the results of a multi-proxy investigation – integrating
geomorphology, ground-penetrating radar, and luminescence dating – of a high-elevation
lunette and beach berm in northern New South Wales, eastern
Australia. The lunette occurs on the eastern shore of Little Llangothlin
Lagoon and provides evidence for a lake high stand combined with persistent
westerly winds at the Last Glacial Maximum (LGM – centring on 21.5 ka) and
during the early Holocene (ca. 9 and 6 ka). The reconstructed atmospheric
circulation is similar to the present-day conditions, and we infer no
significant changes in circulation at those times, as compared to the
present day. Our results suggest that the Southern Hemisphere westerlies
were minimally displaced in this sector of Australasia during the latter
part of the last ice age. Our observations also support evidence for a more
positive water balance at the LGM and early Holocene in this part of the
Australian sub-tropics.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p>Geomorphology and sediments at Little Llangothlin Lagoon
(30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> 9<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> S, 151<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>46<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>53<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> E), 18 km NE of Guyra, NSW,
showing the locations of GPR transects, sediment cores (right), and the
position of OSL samples.</p></caption>
      <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016-f01.pdf"/>

    </fig>

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>The temperate-latitude westerly wind system influences the southern half of
the Australian continent and dictates not only this region's climate but
also the formation and response of its landscape systems. It plays an
important role in the delivery of winter rainfall to the southern half of
Australia. Understanding the history of the westerlies in the Australasian
region is therefore important for understanding the climate and
environmental history of eastern Australia (Shulmeister et al., 2004;
Fletcher and Moreno, 2012; Lorrey et al., 2012). In addition, changes in the
Southern Hemisphere westerlies are inferred to modulate global atmospheric
carbon dioxide concentrations and potentially trigger global climate changes
(e.g. Denton et al., 2010).</p>
      <p>Here we investigate past wind regime changes in eastern Australia as
reflected in the shoreline marginal landforms of Little Llangothlin
Lagoon (LLL). LLL is a presently shallow lake which sits at 30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S
(30<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>5<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>9<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> S, 151<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>46<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>53<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> E) in northern New South Wales.
It lies close to the present-day northern boundary of the winter westerlies,
therefore providing an excellent opportunity to investigate long-term
changes in prevailing wind direction and intensity. The lagoon has a lunette
(transverse shoreline dune) on its eastern shoreline and a possible beach
berm on its south-eastern margin. These landforms reflect aeolian and
wave-driven transport and deposition of sediments; they consequently also provide
indicators for the orientation of prevailing wind directions and intensity
at the time of sediment deposition (Bowler, 1973, 1983, 1986). In
this study we undertook luminescence dating, combined with geomorphic and
stratigraphic investigations, to reconstruct past periods of westerly, and
possible north-westerly, prevailing wind flow in this region.</p>
      <p>The endorheic LLL basin was formed in gently undulating tableland comprising
Tertiary basalt flows at approximately 1300 m above mean sea level (a.m.s.l.).
The western shoreline of LLL is dominated by a low ridge of basalt, which
rises 30 m above the lake (Fig. 1). On the eastern side of the basin, the
lake is bound by a low hill of granite that forms part of the New England
Batholith (Shaw and Flood, 1981). The lagoon covers an area of 1.2 km<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>
and has a catchment of 3.2 km<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. LLL is a shallow, roughly circular
permanent lake with a maximum depth of 2 m that shallows during droughts,
which in this part of Australia are often associated with El Niño years. As
far as we can determine, the lake has never dried out fully in post-European
settlement times (Woodward et al., 2014b). Another, smaller, lake (Billy
Bung Lagoon) lies ca. 500 m to the south-west of LLL and is separated from the
main lake by the low basalt ridge.</p>
      <p>The origin of the New England “lagoons” is cryptic. Conraeds (1989) showed
that they were associated with former drainage lines that were occupied by
basalt flows. He suggested that uneven infilling of former valleys by basalt
during the Tertiary produced shallow depressions where the shallow lakes and
swamps, locally called lagoons, formed. Similar lakes have been described
elsewhere along the tablelands of the Great Dividing Range, and Ollier (1979)
suggested a tectonic origin for these features, proposing that uplift of the
Eastern Highlands caused back tilting on many streams. Other authors such as
Bell et al. (2008) have suggested a deflationary origin, where intense
weathering occurred as a result of wetting and drying of the basalt. The
mechanisms are not incompatible, and deflation may have enhanced and
maintained the basins, which were created by back tilting.</p>
      <p>Many of these upland lakes have lunettes on their eastern margins (sensu
Bowler,
1976). These are transverse crescentic ridges dominated by wave action and
shoreline drift, with coarse-textured wave-built ridges on downwind margins
(Bowler, 1986). Their regular outline reflects the influence of strong wave
action, while the aeolian deflation of sands from the beach forms foreshore
dunes with an orientation consistent with the winter wind resultant vector
(Bowler, 1971). The proportion of clay and silt in lunettes increases during
periods of shoreline regression and is derived from efflorescence and
pelletisation of saline lacustrine sediments on the drying lake floor. Salt
concentration in upland lakes tends to be weaker owing to groundwater
seepage, restricting the preparation of pelletal clays for deflation and
producing dominantly sandy lunettes.</p>
      <p>The catchment is fed by summer rainfall (mean annual rainfall <inline-formula><mml:math display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 880 mm)
and has a theoretical net annual moisture balance deficit of ca. 400 mm
(Woodward et al., 2014a). The regional vegetation is dominated by montane
open eucalypt woodland, while the lagoon itself contains extensive beds of
tall spike rush (<italic>Eleocharis sphacelata</italic>) and the water plant <italic>Potamogeton tricarinatus</italic> in the deeper parts of the basin.
Other swamp plants, including <italic>Carex gaudichaudiana, </italic>are dominant in the surrounding wet margins of
the lagoon.</p>
      <p>The lagoon has been intensively investigated from a palaeoecological and
environmental viewpoint because it is a major bird reserve as well as a
Ramsar wetland. Furthermore, the site has been identified as a location of
exceptional soil erosion since European settlement (Gale et al., 1995; Gale
and Haworth, 2005), although this has recently been challenged (Woodward et
al., 2011). The site has more recently become a focus for work due to
inferred changes to basin hydrology in response to tree clearance during
European settlement of the New England Tablelands (Woodward et al., 2014a).
There has also been some investigation of the archaeological history of the
lagoon suggesting that landscapes such as these provided relatively rich
resources for Aboriginal people and that New England lagoons became the
foci for ceremonial activities, although the degree to which hydrological
conditions influenced human activity remains poorly understood since
chronological control for the pre-European period has so far been lacking
(Beck et al., 2015).</p>
      <p>This paper examines the geomorphic context of shoreline features on the
western and southern margins of the lagoon and focuses on the history of
lake-margin sediment deposition to reconstruct the climatic circulation from
the Last Glacial Maximum (LGM) into the Holocene.</p>
</sec>
<sec id="Ch1.S2">
  <title>Materials and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Field investigations</title>
      <p>Transects across an apparent beach berm and the lunette were surveyed using
a MALÅ ProEx ground-penetrating radar (GPR) system with a 500 MHz antenna
and integrated high-resolution GPS. The GPR data were collected in transects
forming a rough grid parallel and perpendicular to the trend of hypothesised
beach and lunette landforms. The GPR was hand-dragged at a speed of
<inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 4 kph and fired using time firing at a rate of 10 Hz,
resulting in an average along-track resolution of 0.11 and 0.07 m vertical
resolution, based on a centre frequency of 500 MHz. After acquisition, radar
data were processed using GPR-SLICE software (DC drift; user-defined signal
gain; bandpass lo <inline-formula><mml:math display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 350 MHz, hi <inline-formula><mml:math display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 650 MHz; background removal). Profiles
were topographically corrected using elevation data from the GPS system and
spot-checked using known elevations. While absolute topography was not
reliable, relative elevation was consistently reproducible. Individual
profiles were converted to depth–distance using the published radar velocity
for wet sands of 0.07 m ns<inline-formula><mml:math 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> in the beach ridges and dry sands of 0.12 m ns<inline-formula><mml:math 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> in
the lunette (Neal, 2004). Depth–distance profiles were used to evaluate
sediment thickness and observe true geometry of radar reflectors.</p>
      <p>The sub-surface sediments were logged using a hand auger to a depth of
between 0.6 and 1.2 m, depending on sub-surface conditions. Sub-samples
were collected for grain size analyses. In addition, gravels from the sand
and gravel barrier were treated with HCl for 12 h in order to identify
weathering products such as manganese–iron pisoliths. Four samples were
collected for optically stimulated luminescence (OSL) dating using steel
tubes, wrapped in black plastic, and transported to the Max Planck Institute
for Evolutionary Anthropology in Leipzig for analysis.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S2.SS2">
  <title>OSL dating – equivalent-dose measurements</title>
      <p>Sample preparation and measurement for OSL dating were undertaken in the
luminescence dating laboratory of the Department of Human Evolution, Max
Planck Institute for Evolutionary Anthropology in Leipzig. The OSL samples
were prepared under subdued red light using published methods
(Fitzsimmons et al., 2014). This involved sieving, applying
HCl acid and hydrogen peroxide digestion to remove carbonates and organic
matter respectively; and isolating pure, 180–212 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m quartz grains. The
outer <inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m alpha-irradiated rind of each grain was
removed by etching in hydrofluoric acid, and the sample was then subjected
to a final sieve to remove finer fragments which had broken off during
etching. The quartz grains were then prepared as small aliquots (18 discs;
1 mm diameter) for preheat testing and as single grains (600 grains; six single-grain
discs) for equivalent-dose (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> measurement.</p>
      <p><inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> measurements were undertaken using an automated Risø TL-DA-15
equipped with blue-light-emitting diodes (for preheat and initial dose
estimate testing) and a TL-DA-20 reader with a single-grain attachment
containing a green laser emitting at 532 nm, for light stimulation of single
aliquots and single grains respectively (Botter-Jensen et
al., 2000). Irradiation was provided by calibrated <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn>90</mml:mn></mml:msup><mml:mi mathvariant="normal">Sr</mml:mi><mml:msup><mml:mo>/</mml:mo><mml:mn>90</mml:mn></mml:msup><mml:mi mathvariant="normal">Y</mml:mi></mml:mrow></mml:math></inline-formula> beta
sources. Equivalent doses were determined on single grains using the single
aliquot regenerative dose (SAR) protocol of Murray and Wintle (2000,
2003). Preheat temperatures of 260 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C were chosen based on the
results of the preheat plateau tests (Fig. S2 in the Supplement) for the natural and
regenerative doses, with a preheat temperature of 220 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C for the
test doses (0.94 Gyr).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p>Equivalent dose (<inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, dose rate data, and OSL age estimates for
Little Llangothlin Lagoon. Dose rates are listed as attenuated based on
published factors (Stokes et al., 2003; Mejdahl, 1979).</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.85}[.85]?><oasis:tgroup cols="10">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:colspec colnum="7" colname="col7" align="left"/>
     <oasis:colspec colnum="8" colname="col8" align="left"/>
     <oasis:colspec colnum="9" colname="col9" align="left"/>
     <oasis:colspec colnum="10" colname="col10" align="left"/>
     <oasis:thead>
       <oasis:row>  
         <oasis:entry colname="col1">Sample</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Gyr)</oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula> (%)</oasis:entry>  
         <oasis:entry colname="col4">Th (ppm)</oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (ppm)</oasis:entry>  
         <oasis:entry colname="col6">Beta dose</oasis:entry>  
         <oasis:entry colname="col7">Cosmic dose</oasis:entry>  
         <oasis:entry colname="col8">Water</oasis:entry>  
         <oasis:entry colname="col9">Total dose</oasis:entry>  
         <oasis:entry colname="col10">Age (ka)</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"/>  
         <oasis:entry colname="col6">rate (Gy ka<inline-formula><mml:math 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>)</oasis:entry>  
         <oasis:entry colname="col7">rate (Gy ka<inline-formula><mml:math 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>)</oasis:entry>  
         <oasis:entry colname="col8">content (%)</oasis:entry>  
         <oasis:entry colname="col9">rate (Gy ka<inline-formula><mml:math 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>)</oasis:entry>  
         <oasis:entry colname="col10"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>  
         <oasis:entry colname="col1">L-EVA 1228 (LL1)</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>6.1</mml:mn><mml:mo>±</mml:mo><mml:mn>0.6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.53</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>4.0</mml:mn><mml:mo>±</mml:mo><mml:mn>0.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.3</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.6</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.19</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>10</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.21</mml:mn><mml:mo>±</mml:mo><mml:mn>0.07</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>5.1</mml:mn><mml:mo>±</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">L-EVA 1229 (LL2)</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>19.2</mml:mn><mml:mo>±</mml:mo><mml:mn>0.4</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.34</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>3.5</mml:mn><mml:mo>±</mml:mo><mml:mn>0.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.3</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.5</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.18</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.02</mml:mn><mml:mo>±</mml:mo><mml:mn>0.06</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>18.9</mml:mn><mml:mo>±</mml:mo><mml:mn>1.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">L-EVA 1230 (LL3)</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>26.9</mml:mn><mml:mo>±</mml:mo><mml:mn>0.9</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.69</mml:mn><mml:mo>±</mml:mo><mml:mn>0.04</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>3.0</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.3</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.7</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.18</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">7</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.30</mml:mn><mml:mo>±</mml:mo><mml:mn>0.08</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>20.6</mml:mn><mml:mo>±</mml:mo><mml:mn>1.4</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>  
         <oasis:entry colname="col1">L-EVA 1231 (LL4)</oasis:entry>  
         <oasis:entry colname="col2"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>22.9</mml:mn><mml:mo>±</mml:mo><mml:mn>1.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col3"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.56</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col4"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>2.7</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col5"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.7</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col6"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.5</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col7"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.18</mml:mn><mml:mo>±</mml:mo><mml:mn>0.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col8"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col9"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>0.98</mml:mn><mml:mo>±</mml:mo><mml:mn>0.05</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>  
         <oasis:entry colname="col10"><inline-formula><mml:math display="inline"><mml:mrow><mml:mn>23.4</mml:mn><mml:mo>±</mml:mo><mml:mn>1.8</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <p>Individual grains were analysed for their suitability for OSL dating based
on the selection criteria of Jacobs and Roberts (2007). The single-grain
dose distributions of all samples are &gt; 40 % overdispersed with
complex dose populations (Table S1 in the Supplement), and therefore the finite mixture model
(FMM) was used to identify dose populations (Galbraith and Green, 1990). The
OSL dating results are summarised in Table 1. Equivalent-dose distributions
for the four samples are shown as radial plots, with the FMM-derived dose
populations highlighted, in Fig. 3.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>OSL dating – dose rate calculations</title>
      <p>Uranium, thorium, and potassium (<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mn>40</mml:mn></mml:msup></mml:math></inline-formula>K) activities were measured in the
“Felsenkeller” laboratory at VKTA Rossendorf in Dresden, Germany, using
low-level gamma-ray spectrometry. Dose rates were calculated using the
conversion factors of Stokes et al. (2003) with <inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-attenuation factors
taken from Mejdahl (1979). Beta counting was based on 1 g homogenised
sub-samples and used for the beta component of the dose rate. Measured water
contents ranged from 5 to 10 %, and these values were used for all samples.
Cosmic dose rates were calculated from Prescott and Hutton (1994).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F2" specific-use="star"><caption><p><bold>(a)</bold> GPR transects over the “berm”. See Fig. 1 for location of
transect. GPR line A7 was acquired perpendicular to the shoreline starting
just lakeward of the highest point on the berm. Internal structures are
characteristic of an interfingering beach–wash-over–basin fill sequence over
a spit complex. Upper panel, raw data; lower panel, interpretation.
<bold>(b)</bold> GPR line A9 was acquired from the lake shore to the highest point
on the berm. Internal structures show characteristics of a beach environment
over a spit complex. Top left panel, raw data; top right panel,
interpretation. The lower panel shows a conceptual model based on composite
GPR profiles suggesting a lower lake facies with spit facies underlying
beach, wash-over, and basin fill facies.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016-f02.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p>Equivalent-dose distributions for the LLL samples, illustrated as
radial plots. The shaded populations in each case represent the dominant age
peaks; the lines illustrate the other identified populations.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016-f03.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>Geomorphology</title>
      <p>There are no dune or beach deposits on the western side of the lake (Fig. 1).
The main geomorphic feature on the eastern side of the lake is the
lunette and the low basalt ridge. The lunette comprises a north–south-oriented
ridge less than 2 m high adjacent to the lake, a swale behind that
is occupied by a small stream, and a small sand flat area that extends up to
50 m east of the lake shore.</p>
      <p>The lunette on the eastern shore is composed of poorly sorted medium sand
grading upwards into fine sand with accessory silt contents of 3–15 %.
Particle size results and other stratigraphic information are plotted in
Fig. 1, and particle size analysis curves are provided in
Fig. 1 of the Supplement. GPR transects are shown in Fig. 2a and b.</p>
      <p>On the SE margin of LLL, there is a partly infilled outlet, immediately to
the west of which there is a ca. 100 m long, 50 m wide low (&lt; 1 m) berm. The
berm is poorly to well sorted and has medium and coarse quartz-rich sand with
iron–manganese, pisolithic gravel, and a silt content of 1–14 %.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>GPR results</title>
      <p>The GPR proved effective at mapping stratigraphic architecture and
sub-surface character to a depth shallower than 4 m in the berm (Fig. 2a
and b). GPR data suggest the presence of several distinct units related to
changes in lake level and the development of spit/barrier and berm
formations (Shan et al., 2015; Thompson et al., 2011). The berm showed
strong internal stratification and features perpendicular lines with strong
sigmoidal clinoforms indicating beach progradation to the west (Thompson et
al., 2011) as well as low-angle sub-parallel reflectors dipping to the east
suggesting basin infill via over wash processes. This package is underlain
by a convex-up package of reflections that are sub-parallel with dips to the
east and west. Comparison of this feature with those identified by Shan et al. (2015)
suggests the complex is underlain by a spit complex. Additional
information on the character of the lower units associated with the
interpreted spit are unavailable due to the existing GPR data coverage.</p>
      <p>The internal stratigraphy of the fine-grained lunette was difficult to
assess with the GPR. Evidence of extensive modern bioturbation by rabbits
was observed during the radar acquisition. The shallow penetration did
however show weak internal characteristics commonly associated with lunette
formation (Thomas and Burrough, 2016). These included eastward-dipping
high-angle reflectors that are truncated on the western-facing slope,
coupled with areas of parallel to sub-parallel reflections that change to
steeply dipping reflections. All reflectors are laterally discontinuous and
show evidence of disturbance at all depths observed, rendering the GPR data
ineffective at determining genetic processes or detailed landform
characteristics.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS3">
  <title>OSL results</title>
      <p>The OSL age data are summarised in Table 1 and shown with respect to
stratigraphy and catchment geomorphology in Fig. 1. The three samples
collected from three different locations along the lunette suggest that the
entire landform was active during the LGM, between ca. 24 and 19 ka. Our samples
do not extend to the base of aeolian sedimentation, and it is likely that the
lunette was formed earlier than the LGM. The secondary age populations
identified by FMM are all younger than the LGM phase of deposition (Fig. 3; Table S2) and suggest phases of partial reactivation or pedogenic
infiltration of material into the lunette. The younger age populations from
sites LL3 and LL4 in the central part of the lunette are comparable and
strongly suggest contemporaneous post-depositional infiltration of younger
material or partial reactivation of the lunette in the early Holocene (ca.
9–8 ka; Table S2). Sample L-EVA 1230 (LL3) exhibits a third peak centred on
11.8 Gy BP (9.1 ka). The second major age population from the LL2 site in the
southern part of the lunette dates to the mid-Holocene (<inline-formula><mml:math display="inline"><mml:mrow><mml:mn>5.6</mml:mn><mml:mo>±</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> ka;
Table S2) and suggests spatial and temporal variability in the Holocene
post-depositional pedogenesis (or reactivation) of the lunette.</p>
      <p>The overdispersion on individual <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> results from the berm was too high
(79.9 %; Table S1) to reliably define a depositional age, although the
largest age population yields a mid-Holocene age (<inline-formula><mml:math display="inline"><mml:mrow><mml:mn>5.1</mml:mn><mml:mo>±</mml:mo><mml:mn>0.5</mml:mn></mml:mrow></mml:math></inline-formula> ka; Table 1) comparable with the reactivation of the southern part of the lunette at
LL2. The minor dose populations yield ages of <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>11.1</mml:mn><mml:mo>±</mml:mo><mml:mn>1.6</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>2.3</mml:mn><mml:mo>±</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>1.2</mml:mn><mml:mo>±</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula> ka (Table S2).</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
      <p>There are two separate but related sets of geomorphic features recorded
along the eastern and south-eastern margin of LLL. These are the sand and
gravel berm, which is a lake beach/spit feature, and the lunette, which is an
aeolian feature but tied to the shoreline. Both are supplied with sediment
by wind wave processes in the lake, but the former is a sub-aqueous feature,
while the lunette is an aeolian structure.</p>
<sec id="Ch1.S4.SS1">
  <title>A possible spit/barrier berm in the SE corner of the lagoon</title>
      <p>The most cryptic landform in the basin is the sand and gravel berm on the SE
margins of LLL. The feature was identified by Gale and Haworth (2005), who
interpreted it as part of a relict older lunette feature. From visual
observations alone, this is a reasonable interpretation because the low berm
does look like the erosional shadow of an older ridge. Our sedimentologic
and GPR structural investigations, however, discount this interpretation.
Based on both GPR and field observations from pits, the feature is clearly a
beach berm, with numerous small wash-over structures (see Fig. 2a).</p>
      <p><?xmltex \hack{\newpage}?>The berm barrier feature is composed of pea-sized gravels within a finer
sandy matrix. We assume the sandy matrix to be post-depositional because it
is incompatible with the sedimentary structures and post-depositional
infilling of openwork deposits is common. In addition, the contrast between
locally sourced detrital basalt gravels and reworked quartz-rich sand and
silt is striking. The matrix may have accumulated either through aeolian
accession or through filtration of sands through the barrier during high
lake stands when the berm would have acted as a permeable filter for the
lake. Given the mostly coarse nature of the matrix (medium to coarse sand),
we prefer the two-stage filtration hypothesis.</p>
      <p>The pea-sized gravels are detrital. We suggest that the most likely origin
for this feature is as a spit that developed from the basalt ridge on the SW
edge of the lake and that the basalt gravels were moved along the shoreline
by longshore drift. The barrier ultimately cut off an area to the SW of the
present lake that was part of a larger, ancestral lake feature, for which we
have no age constraint due to the lack of associated sedimentary deposits.
The barrier post-dates the LGM as we have been provided with a radiocarbon
result (R. Haworth, personal communication, 2016) from a depth of 1.5 m close to our LL1
sample (Beta-110588: <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>16 200</mml:mn><mml:mo>±</mml:mo><mml:mn>70</mml:mn></mml:mrow></mml:math></inline-formula> yr BP; median: 19 500 cal yr BP;
calibration from Stuiver and Reimer (1993) (Calib 7.1) with a Southern
Hemisphere correction (SHCal13) from Hogg et al., 2013) that provides a
maximum age for the barrier. The luminescence sample based on the finer
matrix material at 0.5 m depth yielded a highly dispersed dose distribution
with four age populations, which is not unexpected given our hypothesis that
the matrix is post-depositional. The grains may represent the accretion of
fines to the barrier during high stands in the lake in the early (ca. 11 ka),
mid- (ca. 5.6 ka) and late Holocene (ca. 2.3, 1.2 ka).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p>Rose of 09:00 wind direction vs. wind speed in km h<inline-formula><mml:math 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> at Guyra
Hospital, 1332 m a.m.s.l. (Bureau of Meterology, 2014). Only winds above
<inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 22 kph are sand-carrying (based on the 12-knot threshold of
Fryberger, 1979). Sand drift potential is much stronger in winter (August)
than it is in summer (February) because the relationship is a power function
of the wind speed and frequency of very strong winds is much lower in
summer.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/12/1435/2016/cp-12-1435-2016-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <title>Aeolian history of LLL from the lunette</title>
      <p>Based on the morphology, sedimentary composition, and internal structure, the
feature along the eastern shoreline of LLL is clearly a composite beach and
aeolian landform. The quartz-rich sands were most likely derived from the
granites on the eastern side of the catchment, which deposited into the lake
and were subsequently reworked onto the shoreline. Half the basin is
comprised of basalt, yet there is little evidence for basalt-derived
sediments in the lunette system. By contrast, the fine sediments in the
depocentre of the lake basin are primarily derived from basalt. This implies
that there is an effective sorting mechanism within the basin, whereby the
basalt preferentially weathers to mud while the granite generates sand.
Sorting by currents would transport the fines to the depocentre, while the
sands would be transported towards the lake margins. The most parsimonious
candidate for this latter process is wind-blown waves.</p>
      <p>Present-day wind roses for LLL (BOM, 2014) demonstrate that there are two
primary wind directions (Fig. 4), one from the east and the other from the
west to north-west. These prevailing winds have strong seasonal components.
Winter winds (August) are dominated by westerlies and provide the strongest
and most persistent flows (8 % calm) consistent with eastward transport
and deposition of sediments onto a lunette situated on the eastern shoreline
of LLL. Summer winds (February) are dominated by easterlies associated with
onshore circulation on the northern limb of the sub-tropical high-pressure
cell in summer (Fig. 4). These easterly winds are on average weaker (20 %
calm) but do include short periods of relatively high-intensity winds, which
might be expected to result in sediment transport to, and deposition onto,
the western side of the lake. It is curious therefore that all depositional
landforms marginal to LLL are located on the east and south-east sides of
the lake, with no deposition on the western shoreline. Examination of the
wind roses indicates that sand-transporting winds (above <inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 22 km h<inline-formula><mml:math 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>:
Fryberger, 1979) were more than twice as frequent (<inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 14 % vs. <inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 5 %) in August than in February and that
the highest wind speeds occurred more frequently in August. This confirms
that the most effective net sand-transporting wind, associated with lunette
and berm formation, was from the west/north-west. The transport is most
likely to have been primarily sub-aqueous, since the relatively poor sorting
in the foredune indicates only a short-distance aeolian transport pathway.</p>
      <p>In addition to the stronger drift potential there may also be a biological
effect. The rush beds occurring in the shallower parts of the lake are most
fully developed during the summer. Unlike much of Australia, winters are
severe on the New England Tablelands due to the relatively high elevations,
and seasonal die-back of the tall spike rush is observed today. New growth
emerges in spring and dies off in autumn in cooler, high-altitude sites
(Rajapaskse et al., 2006). Consequently, the summer peak in vegetation cover
disrupts the wind fetch over the lake precisely at the same time as the
easterly winds penetrate the tablelands, thereby further reducing the
ability for waves to set up during the warmer months.</p>
      <p>The luminescence ages from the lunette are coherent. All samples are
dominated by grains that are LGM in age. The samples all overlap at 2<inline-formula><mml:math display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> and produce a weighted mean age of <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>20.4</mml:mn><mml:mo>±</mml:mo><mml:mn>0.8</mml:mn></mml:mrow></mml:math></inline-formula> ka, indicating that the
main phase of dune activity at LLL occurred during the late LGM. Our
interpretation that the dominant sediment transport mechanism was sub-aqueous
therefore implies that the LGM oversaw permanent, and probably full, lake
conditions at LLL. Evidence from our unpublished sedimentary archives from
the depocentre of the lake supports the concept of a full lake during the
late LGM (ca. 19 ka). Specifically, the lake sediments from this time
interval are an unoxidised grey clay, which contains numerous sponge
spicules. In addition, pollen records from these latitudes suggest the
survival of rainforest at lower elevations to the east through the LGM (e.g.
Moss et al., 2013), indicating persistence of moisture availability. Our
argument for the persistence, and perhaps intensification, of winter
westerlies throughout the LGM at LLL is also confirmed by observations made
at North Stradbroke Island some 300 km to the north-north-east of our site
(Petherick et al., 2009; McGowan et al., 2008). North Stradbroke Island lies
at the very northern edge of the westerlies zone, and the accession of fine
aeolian material into a dune lake there indicates that the winter westerlies
were operative at the LGM in South East Queensland at 27.20<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S
(Petherick et al., 2009; McGowan et al., 2009), just as the westerlies
operate today in this region.</p>
      <p>A secondary peak in grain ages is observed in all three lunette samples.
This peak is less well defined but in all three cases relates to the early
to mid-Holocene between 9 and 6 ka. Work from the lake (Woodward et al.,
2011) has already demonstrated that the early Holocene was the last phase,
before the modern anthropogenically modified lake, with lake full conditions
as represented by extensive <italic>Eleocharis </italic>beds. Wind waves would have been effective on
the lake, and we infer partial reactivation of the lunette at this time.</p>
      <p>We note a third grain age peak in one lunette sample (EVA1230) at ca. 3 ka.
This is both the weakest individual age peak and not replicated at any other
site. It is possible that this represents a dune re-activation event;
bioturbation; or even Aboriginal usage of the site, which has been proposed
to have intensified during the late Holocene (post 4300 years; Beck et al.,
2015). At this stage this event, if real, is still poorly controlled
chronologically, and we do not interpret it further.</p>
      <p>Overall, our evidence demonstrates that, at the LGM, winter westerly winds
were strong enough to form the eastern shoreline lunette in a single phase,
with possible later reactivation during the early Holocene. Critically,
foredune activation depends as much on high water levels in the lake
allowing the wave delivery of sediment to the eastern beach as it does on
sand-mobilising winds (Bowler, 1983). During the Pleistocene,
elevations above 800 m in the region were subject to extensive, active
development of block deposits, screes, and solifluction lobes, indicating
winter cooling of at least 10.5 <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C relative to present (Slee and
Shulmeister, 2015). Reduced evaporation due to lower temperatures (e.g.
Hesse et al., 2003) and transfer of flow from throughflow/baseflow to
overland flow due to increased snow cover (Reinfelds et al., 2014) at this
time are likely to have been sufficient to cause the change to a positive
hydrological balance in the lake.</p>
      <p>For the intervening periods, at least in the Holocene, the evidence
(Woodward et al., 2014a) suggests that water levels were lower and/or even
that the lake was ephemeral. It is highly unlikely that sand would be
transported to the high-stand beach during low lake levels. If the entire
basin floor fully dried out, pelletised clays might be expected, and yet
none are observed. There are two likely reasons for this. Firstly, this
high-elevation site is unlikely to become very arid even during relatively dry
phases when swampy conditions probably persisted on the basin floor.
Similarly, it is unlikely that salt formation is significant in this setting,
and clay pelletisation may not occur. This is similar to observations from
Lake George, which also lies within a cool temperate climate setting along
the Great Dividing Range (Fitzsimmons and Barrows, 2010).</p>
      <p>In summary, these records strongly suggest that for the two intervals
recorded (the LGM and early Holocene) the overall circulation conditions at
LLL were very similar to the present day. This region presently lies near
the northern limit of westerly penetration in winter. For the intervening
periods, absence of evidence is not evidence of absence; if the winter
westerly winds lay at this latitude during peak warming in the early
Holocene and during the LGM, it seems reasonable to suppose that this track
has been persistent over the last 25 kyr.</p>
      <p>The track of the Australian winter westerlies during the LGM has been a
source of contention for some time, with both poleward and equatorward
changes argued for (e.g. Harrison and Dodson, 1993; Hesse, 1994; Shulmeister
et al., 2004). One possibility is that the westerly lay north of its current
track during the LGM and that the timing of the westerlies at LLL shifted
seasonally. A northward shift of <inline-formula><mml:math display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 3<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (350 km) in
the position of the westerly wind belt during marine isotope stage (MIS) 2 was recorded in
sediments from marine cores in the Tasman Sea (Hesse, 1994). Analysis of the
aeolian component of lake sediments on North Stradbroke Island at 27<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S for the period 25–22 ka indicates dust sources in the SW
Murray–Darling Basin, with a secondary component from WNW of the site
(Petherick et al., 2009). These findings are consistent with either no change
or a possible northward shift in the westerlies but are not consistent with
the poleward contraction of the westerlies in eastern Australia at the LGM.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p>This study indicates that westerly winds activated a lunette at LLL during
the LGM under the influence of high lake levels. This ridge was reactivated
during high lake stands in the early to mid-Holocene. The persistence of
westerly winds at this site during the LGM confirms observations from North
Stradbroke Island at the northern limits of penetration of the temperate-latitude
westerlies. This suggests that the overall circulation pattern in
this part of eastern Australia, at the modern northern limits of westerly
winter flow, remained constant during both the LGM and the early Holocene.
Overall, this points to minimal change in circulation patterns over the last
25 kyr.</p>
</sec>
<sec id="Ch1.S6">
  <title>Data availability</title>
      <p>Summary statistics for rainfall and temperature data from the Guyra Hospital weather station
(30.21<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 151.68<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 1329 m elevation) from 1981 to 2016
and for other climatic variables including wind speed and direction for the period from 1981 to 2010 (see
<uri>http://www.bom.gov.au/climate/averages/tables/cw_056229.shtml</uri>).</p>
</sec>

      
      </body>
    <back><app-group>
        <supplementary-material position="anchor"><p><bold>The Supplement related to this article is available online at <inline-supplementary-material xlink:href="http://dx.doi.org/10.5194/cp-12-1435-2016-supplement" xlink:title="pdf">doi:10.5194/cp-12-1435-2016-supplement</inline-supplementary-material>.</bold></p></supplementary-material>
        </app-group><notes notes-type="authorcontribution">

      <p>James Shulmeister led the project, assisted with field sampling for OSL and
grain size, and led the manuscript development. Justine Kemp assisted in the field
with OSL sample acquisition, conducted grain size analysis, and participated
in manuscript development. Kathryn E. Fitzsimmons undertook the OSL sample analysis
and participated in manuscript development. Allen Gontz led the GPR acquisition
and processing and assisted with OSL sampling and manuscript development.</p>
  </notes><ack><title>Acknowledgements</title><p>This research was funded by Australian Research Council Discovery Grant
DP110103081, “The last glaciation maximum climate conundrum and
environmental responses of the Australian continent to altered climate
states”. We thank S. Hesse for assistance with OSL sample preparation. R. Haworth made a radiocarbon age from underneath the sand and gravel berm
available to us. C. Woodward, J. Chang, and A. Slee assisted with fieldwork.
We thank all the referees for very helpful input that has improved the
paper. We thank NSW National Parks and Wildlife Service for access to the site and
the local farmers for retrieving our vehicle from the bottomless suckhole!<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: A. Lorrey<?xmltex \hack{\newline}?>
Reviewed by: P. Hesse, W. Beck, and one anonymous referee</p></ack><ref-list>
    <title>References</title>

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  </ref-list><app-group content-type="float"><app><title/>

    </app></app-group></back>
    <!--<article-title-html>Constant wind regimes during the Last Glacial Maximum and early Holocene:
evidence from Little Llangothlin Lagoon, New England Tablelands, eastern
Australia</article-title-html>
<abstract-html><p class="p">Here we present the results of a multi-proxy investigation – integrating
geomorphology, ground-penetrating radar, and luminescence dating – of a high-elevation
lunette and beach berm in northern New South Wales, eastern
Australia. The lunette occurs on the eastern shore of Little Llangothlin
Lagoon and provides evidence for a lake high stand combined with persistent
westerly winds at the Last Glacial Maximum (LGM – centring on 21.5 ka) and
during the early Holocene (ca. 9 and 6 ka). The reconstructed atmospheric
circulation is similar to the present-day conditions, and we infer no
significant changes in circulation at those times, as compared to the
present day. Our results suggest that the Southern Hemisphere westerlies
were minimally displaced in this sector of Australasia during the latter
part of the last ice age. Our observations also support evidence for a more
positive water balance at the LGM and early Holocene in this part of the
Australian sub-tropics.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Beck, W., Haworth, R., and Appleton, J.: Aboriginal resources change through
time in New England upland wetlands, south-east Australia, Archaeol Ocean.,
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