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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-17-1443-2021</article-id><title-group><article-title>Precise timing of MIS 7 substages from the Austrian Alps</article-title><alt-title>Precise timing of MIS 7 substages from the Austrian Alps</alt-title>
      </title-group><?xmltex \runningtitle{Precise timing of MIS~7 substages from the Austrian Alps}?><?xmltex \runningauthor{K.~A.~Wendt~et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff4">
          <name><surname>Wendt</surname><given-names>Kathleen A.</given-names></name>
          <email>kathleen.wendt@oregonstate.edu</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Li</surname><given-names>Xianglei</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8464-9020</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Edwards</surname><given-names>R. Lawrence</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff2">
          <name><surname>Cheng</surname><given-names>Hai</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Spötl</surname><given-names>Christoph</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7167-4940</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Institute of Geology, University of Innsbruck, Innrain 52, 6020 Innsbruck, Austria</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Earth Sciences, University of Minnesota, 116 Church Street SE, Minneapolis, MN 55455, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Institute of Global Environmental Change, Xi'an Jiaotong University, Xi'an 710049, China</institution>
        </aff>
        <aff id="aff4"><label>a</label><institution>current address: College of Earth, Ocean, and Atmospheric Sciences, Oregon State University, Corvallis, OR 97331, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Kathleen A. Wendt (kathleen.wendt@oregonstate.edu)</corresp></author-notes><pub-date><day>9</day><month>July</month><year>2021</year></pub-date>
      
      <volume>17</volume>
      <issue>4</issue>
      <fpage>1443</fpage><lpage>1454</lpage>
      <history>
        <date date-type="received"><day>11</day><month>November</month><year>2020</year></date>
           <date date-type="accepted"><day>2</day><month>June</month><year>2021</year></date>
           <date date-type="rev-recd"><day>27</day><month>May</month><year>2021</year></date>
           <date date-type="rev-request"><day>20</day><month>November</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 Kathleen A. Wendt et al.</copyright-statement>
        <copyright-year>2021</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/17/1443/2021/cp-17-1443-2021.html">This article is available from https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021.html</self-uri><self-uri xlink:href="https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021.pdf">The full text article is available as a PDF file from https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e138">Investigating the precise timing of regional-scale climate changes during glacial terminations and the interglacial periods that follow is key to
unraveling the mechanisms behind these global climate shifts. Here, we present a high-precision time series of climate changes in the Austrian Alps
that coincide with the later portion of Termination III (TIII), the entire penultimate interglacial (Marine Isotope Stage (MIS) 7), Termination IIIa
(TIIIa), and the penultimate glacial inception (MIS 7–6 transition). Using state-of-the-art mass spectrometry techniques, we have constructed a
uranium-series chronology with relative age uncertainties averaging 1.7 ‰ (2<inline-formula><mml:math id="M1" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>) for our study period (247 to 191 thousand years
before present, <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>). Results reveal the onset of warming in the Austrian Alps associated with TIII at 242.5 <inline-formula><mml:math id="M3" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> and the
duration of MIS 7e warming between 241.8 and 236.7 (<inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. An abrupt shift towards higher <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values at
216.8 <inline-formula><mml:math id="M8" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> marks the onset of regional warming associated with TIIIa. Two periods of high <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values (greater than
<inline-formula><mml:math id="M10" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 ‰ Vienna Pee Dee Belemnite (VPDB)) between 215.9–213.3 and 204.3–197.5 (<inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> coincide with interglacial substages MIS 7c and 7a,
respectively. Multiple fluorescent inclusions suggest a partial retreat of the local Alpine glacier during peak obliquity forcings at
214.3 <inline-formula><mml:math id="M13" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.4 <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Two newly collected stalagmites from Spannagel Cave (SPA146 and 183) provide high-resolution replications of the
latter portion of the MIS 7a-to-6e transition. The resulting multi-stalagmite record reveals important chronological constraints on climate shifts in
the Austrian Alps associated with MIS 7 while offering new insight into the timing of millennial-scale changes in the North Atlantic realm leading
up to TIII and TIIIa.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e278">Marine Isotope Stage (MIS) 7 (ca. 246–186 thousand years before present (ka), where present is 1950 CE) stands distinctively
apart from the last several interglacial cycles. Following the low-amplitude glacial Termination III (TIII), MIS 7e was a relatively weak interglacial
that returned to glacial conditions (MIS 7d) within 20 thousand years (<inline-formula><mml:math id="M15" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ky</mml:mi></mml:mrow></mml:math></inline-formula>) (PAGES, 2016). Glacial conditions terminated with a second
deglaciation (TIIIa), which gave way to a second interglacial with three distinct substages (MIS 7c, b, a). Although the inception of an
interglacial is ultimately paced by astronomical forcing, the precise timing (millennial scale) of each glacial termination and the strength of the
successive interglacial depends on various global climate parameters and feedbacks. Investigating these internal forcings requires the intercomparison
of precisely dated climate records in order to identify leads, lags, and synchronicities across different climate zones. The role of forcings that led
to the last two glacial terminations and the variability within the last two interglacial periods (MIS 5e and Holocene) have been well
studied. Obtaining records from MIS 7 and the penultimate glaciation that contain sufficient resolution and chronological precision to make meaningful
regional comparisons, however, has proved challenging. In the North Atlantic realm, marine records show that major meltwater pulse events punctuated a
period of rapid sea surface warming associated with TIII and TIIIa (e.g., Channell et al., 2012; Hodell et al., 2008; Martrat et al., 2004, 2007). The
chronologies of these marine records, however, are frequently dependent on orbital tuning or alignment to global benthic <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> stacks,
which feature large uncertainties of <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> during MIS 7 (e.g., LR04<?pagebreak page1444?> stack; Lisiecki and Raymo, 2005). In continental Europe, cave and
lacustrine records indicate abrupt environmental shifts associated with the MIS 7 substages (e.g., Tzedakis et al., 2003; Roucoux et al., 2008; Despart et al., 2006) and TIII (Pérez-Mejías et al., 2017) accompanied by regional temperature and atmospheric circulation changes
(e.g., Spötl et al., 2008; Badertscher et al., 2011; Columbu et al., 2019) often in step with North Atlantic climate change (Denniston et al.,
2018). However very few terrestrial records span the entirety of MIS 7 and its glacial transitions. A
lack of absolute-dated, continuous records hinders the ability to capture the timing and full duration of regional climate changes, resulting in
critical gaps in knowledge.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e324"><bold>(a, b)</bold> Location of paleorecords described in this paper. <bold>(c)</bold> Google Earth image of the Tux Valley showing the location of Spannagel Cave (yellow) adjacent to the glaciated main ridge of the Alps (oblique view towards SSE) © Google Earth.</p></caption>
        <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021-f01.png"/>

      </fig>

      <p id="d1e338">This study aims to determine the onset of warming in continental Europe associated with TIII and TIIIa, as well as the regional climate variations
during the five substages of MIS 7. To do so, we turn to the Austrian Alps (Fig. 1). Over the last century, the Alps experienced twice the amplitude
of temperature change relative to the mean Northern Hemisphere (Auer et al., 2007), contributing to a 45 % reduction of glacier surface and
roughly 50 % of ice volume between 1900 and 2011 (Huss, 2012). This high degree of sensitivity renders the Austrian Alps an ideal location to
pinpoint the timing of continental temperature variations. Here, we focus on Spannagel Cave – a high-altitude marble cave located in the central
Austrian Alps. Drip waters in this cave are fed by glacial and snowpack melt (Mangini et al., 2005). Past studies demonstrate that Spannagel
speleothem <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> represents a robust proxy of local winter temperatures and moisture sources, the latter being dominated by the North
Atlantic Ocean (Mangini et al., 2005; see Sect. 2.1). Pioneering work by Holzkämper et al. (2005) and Spötl et al. (2007, 2008) presented
multiple MIS 7 stalagmites and flowstones deposited in Spannagel Cave. Since these studies, new developments in the measurement precision of U and Th
isotopes by Cheng et al. (2013) and Craig et al. (2016, 2017) have allowed for ultra-high age precision, with 2<inline-formula><mml:math id="M20" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> absolute age uncertainties averaging
<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">300</mml:mn></mml:mrow></mml:math></inline-formula> years for MIS 7. In addition, two newly discovered stalagmites from Spannagel Cave provide further insight into the penultimate glacial
inception (MIS 7–6 transition). The resulting Spannagel <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> record provides a high-precision chronology of abrupt climate change in
Europe during MIS 7 while addressing the need for absolute-dated paleorecords from regions that are sensitive to the North Atlantic realm.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Study site</title>
      <p id="d1e396">Spannagel Cave (Fig. 1; 47<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>04<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>54<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 11<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>40<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>2<inline-formula><mml:math id="M28" 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; 2300 to 2530 <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>)
is located above the timberline in the vicinity of a retreating glacier (Hintertux Glacier) close to the main Alpine crest. Previous publications
provide details on the setting of this cave (Spötl et al., 2004; Spötl and Mangini 2007, 2010). A few salient features relevant for this study
are summarized here. Spannagel Cave developed in a ca. 20 <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> thick Upper Jurassic marble (Hochstegen Formation) sandwiched between gneiss
bedrock. An interesting feature of Spannagel Cave drip waters is that they are rich in U. Cave water U concentrations range from 5 <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> (small
cave stream) to 33 <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppb</mml:mi></mml:mrow></mml:math></inline-formula> (stalactite drip water). As a result, calcitic speleothems from this cave are exceptionally high in U concentrations (3
to 399 <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppm</mml:mi></mml:mrow></mml:math></inline-formula>). The U is most likely sourced from the overlying gneiss which yields significantly higher U concentrations (3.4–12.0 <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppm</mml:mi></mml:mrow></mml:math></inline-formula>)
than the marble (0.3–2.2 <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppm</mml:mi></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d1e530">Spannagel is a well-ventilated cave system with stable air temperatures in the interior of the cave that stay within a narrow range of <inline-formula><mml:math id="M36" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1.8 to
<inline-formula><mml:math id="M37" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>2.2 <inline-formula><mml:math id="M38" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> (measured at several sites using data loggers over a period of about 20 years). These values are about
2 <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> higher than the mean annual air temperature at the elevation of the cave, which is a reflection of the small positive thermal
anomaly due to the ascending geometry of the cave (chimney effect; Spötl and Pavuza, 2016). Relative humidity in the cave interior is invariably
higher than 96 %. Today, the actively retreating Hintertux Glacier terminates ca. 500 <inline-formula><mml:math id="M40" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> south of Spannagel Cave. During the last glacial
maximum, the cave was completely covered by as much as 150–250 <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> of glacial ice (van Husen, 1987). The deposition of speleothems during
several cold climate periods suggests that the Hintertux Glacier has remained largely temperate, or warm-based (Spötl and Mangini, 2007). Under
glacial conditions, it is thought that the oxidation of pyrite in the host rock allowed karst dissolution beneath the glacier without the input of
soil-derived carbon dioxide (Spötl and Mangini, 2007).</p>
      <p id="d1e588">Stalagmite SPA121 (Fig. S1 in the Supplement) was found in the northern segment of the cave embedded in unconsolidated silty sand which was most
likely transported into the cave by high-discharge streams during the last deglaciation. The stalagmite is 19.3 <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> tall and was found attached
to a platy and angular piece of calcite-cemented gravel. The surface of the sample is covered by a thin layer of medium gray, clay-rich calcite, but
the interior preserves mostly transparent, inclusion-poor calcite, showing a striking pattern of cracks. The origin of these cracks is enigmatic but
may be related to freezing of the cave or the sediments in which the sample was embedded during peak glacial periods. SPA183 is a 39 <inline-formula><mml:math id="M43" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> tall
stalagmite collected from the central part of the cave and a slightly higher altitude than SPA 121. SPA183 revealed three distinct growth axes that
are marked by variations in color (Fig. S1). SPA146 is a 24 <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> tall stalagmite which grew in the same small chamber as SPA183. Both
stalagmites were detached from their growth substrate and embedded in sand but likely transported less than a few meters. SPA146 shows two distinct
growth axes (Fig. S1).</p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Climate setting</title>
      <p id="d1e622">The Austrian Alps are intermediately situated between the westerlies and northerly flowing Mediterranean air masses.<?pagebreak page1445?> Back-trajectory studies show that
regional precipitation is predominantly sourced from North Atlantic and Arctic oceans (<inline-formula><mml:math id="M45" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 60 %) and the Mediterranean Sea (<inline-formula><mml:math id="M46" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 20 %)
(Kaiser et al., 2002; Sodemann and Zubler, 2010). Seasonally, strong westerly flow during winter months transports moisture from the North Atlantic
Ocean, whereas infrequent northerly flow from the Mediterranean Sea is more common during summer months (Kaiser et al., 2002; Sodemann and Zubler,
2010). Winter precipitation is stored in Alpine glaciers and snow cover. Glacial and snowpack melt is the dominant source of groundwater recharge in
the Alps and the largest supplier to Spannagel drip waters (Mangini et al., 2005; Spötl and Mangini, 2007). Variations in the <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>
of calcite (<inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula>) that precipitates from drip waters have been shown to reflect variations in winter
precipitation <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (Mangini et al., 2005; Spötl et al., 2006; Spötl and Mangini, 2002, 2007).</p>
      <p id="d1e687">The Austrian Network for Isotopes in Precipitation (ANIP) reveals a tight coupling between the mean annual <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> of regional
precipitation and air temperatures (Kaiser et al., 2002) in concordance with other locations across the European Alps (e.g., Schürch et al., 2003;
Field, 2010). On subannual scales, the mean monthly <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> of ANIP stations show an almost parallel evolution with average air
temperatures (Hager and Foelsche, 2015). Additional influences on <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> may include changes in the proportion of seasonal
precipitation, which is linked to moisture source. Stable isotope analysis of rainfall collected from the Patscherkofel mountain station
(20 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> northwest of Hintertux; 2200 <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>)  suggests that <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> precipitation sourced from the North Atlantic Ocean
is depleted relative to Mediterranean sources, due to (i) the lower isotopic value of Atlantic Ocean water and (ii) a longer transport pathway (Kaiser
et al., 2002). However, due to the high elevation of our study site, orographic effects are likely to smooth any large source-based differences in
precipitation <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e795">Spannagel <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> is a robust proxy for (predominantly winter) surface air temperatures on annual to orbital timescales (Mangini
et al., 2005; Spötl et al., 2006; Spötl and Mangini, 2002, 2007), as similarly documented in speleothem records across the European Alps
(e.g., Boch et al., 2011; Moseley et al., 2014; Johnston et al., 2018; Wilcox et al., 2020). Major shifts in Spannagel <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> may be
further amplified by (i) changes to the <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> of moisture sources, such as meltwater pulses in the North Atlantic (e.g., Mangini
et al., 2007), (ii) changes in the degree of moisture recycling along flow paths, and (iii) changes in the seasonal proportions of annual totals. For
example, a northerly displaced polar front and warmer sea surface temperatures (SSTs) likely contributed to increased advection across the Mediterranean during interglacial
periods (Drysdale et al., 2009), resulting in a greater input of heavier <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> Mediterranean moisture to the Austrian Alps during the
summer (Moseley et al., 2015). Such a change in atmospheric circulation would act as a positive, yet relatively minor, feedback to the
temperature-dominated Spannagel <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> signal.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methods</title>
      <?pagebreak page1446?><p id="d1e891">Stalagmites SPA121, 146, and 183 were halved and polished. Subsamples for U–Th dating (<inline-formula><mml:math id="M62" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M63" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 40) were hand drilled along the growth axis of halved
stalagmites. Subsample trenches were drilled no larger than 1 <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> in width, such that the sampling error (<inline-formula><mml:math id="M65" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 175 years) remained within
the analytical uncertainties (see Results). Target sample weights ranged from 200 to 20 <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mg</mml:mi></mml:mrow></mml:math></inline-formula> in concordance with changes in
U concentration. Subsamples were spiked with a mixed <inline-formula><mml:math id="M67" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">233</mml:mn></mml:msup><mml:mi mathvariant="normal">U</mml:mi></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M68" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">236</mml:mn></mml:msup><mml:mi mathvariant="normal">U</mml:mi></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M69" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">229</mml:mn></mml:msup><mml:mi mathvariant="normal">Th</mml:mi></mml:mrow></mml:math></inline-formula> spike similar to that described in Edwards
et al. (1987). Procedures for U and Th chemical separation and preparation of reagent solutions follow the methods described in Edwards et al. (1987)
and Shen et al. (2002).</p>
      <p id="d1e968">U and Th isotopic measurements were made on a Thermo Scientific Neptune Plus MC-ICP-MS following the instrument calibration and the Faraday cup
measurement method described in Cheng et al. (2013). In addition, a 10<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="normal">Ω</mml:mi></mml:math></inline-formula>
amplifier was installed within the detection system in order to collect low ion beam intensities (e.g., <inline-formula><mml:math id="M72" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">234</mml:mn></mml:msup><mml:mi mathvariant="normal">U</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M73" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">230</mml:mn></mml:msup><mml:mi mathvariant="normal">Th</mml:mi></mml:mrow></mml:math></inline-formula>) (Craig
et al., 2016, 2017, and references therein). The methods of gain calibration and dynamic time correction of the high resistor are largely based on
Craig et al. (2016, 2017). Each sample was measured for 300 <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:math></inline-formula> or longer. Intensities of <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">234</mml:mn></mml:msup><mml:mi mathvariant="normal">U</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">230</mml:mn></mml:msup><mml:mi mathvariant="normal">Th</mml:mi></mml:mrow></mml:math></inline-formula> beams were on
average 15 and 5 <inline-formula><mml:math id="M77" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mV</mml:mi></mml:mrow></mml:math></inline-formula>, respectively.</p>
      <p id="d1e1052">Stable isotope samples were micromilled continuously along the growth axis of each stalagmite at 0.15–0.20 <inline-formula><mml:math id="M78" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> increments. A total of 946 stable isotope
measurements on stalagmite SPA121 were previously published in Spötl et al. (2008), 890 and 583 new stable isotope measurements from stalagmites
SPA183 and SPA146, respectively, are reported here. A total of 13 Hendy tests were drilled along individual growth layers from stalagmites SPA146 and
SPA 183 (Figs. S4 and S5 in the Supplement). All calcite powders were analyzed using a GasBench II coupled
with a Delta V Plus isotope ratio mass spectrometer. The 1<inline-formula><mml:math id="M79" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> precision is 0.06 and 0.08 ‰ for <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>, respectively. Results are reported relative to Vienna Pee Dee Belemnite (VPDB).</p>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
      <p id="d1e1108">Resulting U–Th ages and their respective replicates are in stratigraphic order within uncertainties (Table S1). This study focuses on the MIS 7
portion of stalagmite SPA121, which was deposited without interruption between 248.5 and 191.5 (<inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M83" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (see Spötl et al., 2008, for
details on all SPA121 growth phases). New U–Th ages for this stalagmite fall within age uncertainties of the previously published ages (Spötl
et al. 2008; Fig. 2). Similar <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">234</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">U</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values and <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">232</mml:mn></mml:msup><mml:mi mathvariant="normal">Th</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M86" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">238</mml:mn></mml:msup><mml:mi mathvariant="normal">U</mml:mi></mml:mrow></mml:math></inline-formula> concentrations further underscore a high degree
of reproducibility between the two SPA121 data sets, which were measured in different laboratories using different instruments (MC-ICP-MS
vs. TIMS). New SPA121 ages improve the precision of previously published age uncertainties by an order of magnitude (Fig. 2), from an average of
1.7 % to 0.17 %.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1173">Depth vs. age along the growth axis of stalagmite SPA121 with associated 2<inline-formula><mml:math id="M87" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> age uncertainties from this study <bold>(a)</bold> and Spötl et al. (2008) <bold>(b)</bold>. Gray lines show upper and lower 2<inline-formula><mml:math id="M88" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> uncertainties of each age model.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021-f02.png"/>

      </fig>

      <p id="d1e1202">The late MIS 7 growth phase of stalagmites SPA183 and SPA146 occurred between 191.9–190.6 (<inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M90" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> and 191.6–182.3
(<inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M92" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, respectively. The exact onset of growth is unknown, as both stalagmites show evidence of diagenesis spanning first
2–3 <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> of the late MIS 7 growth phase (Fig. S2 in the Supplement; Table S1 in the Supplement). Evidence of diagenetic alteration includes a
conspicuously white, milky calcite fabric and U–Th ages that are out of stratigraphic order and unable to be replicated. As a result, this study
focuses only on the unaltered portion of the late MIS 7 growth phases of stalagmites SPA183 and SPA146 (Fig. S1). Relative age uncertainties of SPA146
and 183 average 0.09 % and 0.16 %, respectively. Significantly higher <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">234</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">U</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values from SPA146 and 183 relative to SPA121
suggest differing drip sources between the first two neighboring stalagmites and SPA121. Growth rates calculated from new SPA121 ages closely agree
with previously published data in Spötl et al. (2008) (Fig. 2). The average growth rate is 5.6 <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, excluding one period of
exceptionally low growth rate (0.8 <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) between 231.1 and 219.6 (<inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M98" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. In contrast, average growth rates of
SPA183 and SPA146 are higher (63 and 140 <inline-formula><mml:math id="M99" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, respectively). Differences in growth rates are likely due to differing drip sources.</p>
      <p id="d1e1344">SPA121 stable isotope values used in this study are from Spötl et al. (2008). New stable isotope data from SPA146 and 183 are reported in Table S2
in the Supplement. The range of SPA121 <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values (<inline-formula><mml:math id="M101" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>8.1 ‰ to <inline-formula><mml:math id="M102" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>14.7 ‰) and <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values
(9.7 ‰ to 0.8 ‰) is in agreement with newly measured <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values from SPA146 and SPA183 (Fig. S3 in the
Supplement). Slight (<inline-formula><mml:math id="M105" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> 1 ‰) offsets in absolute values between stalagmites are observed, but do not influence the relative variations in
stable isotopes which are the focus of this study. Hendy test results (Figs. S4 and S5; Spötl et al.,
2008) show no evidence for significant kinetic fractionation during the deposition of all three stalagmites.</p>
      <p id="d1e1420">The <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> signature of SPA stalagmites is depleted during the MIS 7 warm intervals (average <inline-formula><mml:math id="M107" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9.2 ‰) relative to the
Holocene (average <inline-formula><mml:math id="M108" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>7.8 ‰; Spötl et al., 2004), which suggests cooler winter temperatures during MIS 7. This is consistent with globally
distributed evidence suggesting cooler Northern Hemisphere temperatures throughout MIS 7 (PAGES, 2016) in conjunction with lower sea levels (Robinson
et al., 2002; Thompson and Goldstein, 2005; Dutton et al., 2009; Andersen et al., 2010; Murray-Wallace, 2002) and atmospheric <inline-formula><mml:math id="M109" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula><inline-formula><mml:math id="M110" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (Bazin
et al., 2013) relative to the Holocene.</p>
      <p id="d1e1472">The <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> signature of all three stalagmites is higher relative to modern and Holocene speleothems (<inline-formula><mml:math id="M112" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>10 ‰ to
<inline-formula><mml:math id="M113" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>7 ‰), reflecting a signal that is buffered by the isotopic composition of the host rock (Spötl et al., 2004). High and commonly
positive <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values indicate no significant input of organic C into the system, thereby indicating an absence of soil and vegetation
above the cave throughout the duration of speleothem deposition (Spötl et al., 2008). Cooler surface temperatures and the absence of soil argue
for a significantly larger Hintertux Glacier during MIS 7 relative to today, likely covering a large portion of the cave. The growth of speleothems
during cold climate periods of MIS 7 is likely<?pagebreak page1447?> due to the warm-based nature of the glacier, which provides a supply of meltwater while preventing the
cave from freezing.</p>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
      <p id="d1e1528">The new Spannagel <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> record spans the period of Northern Hemisphere warming associated with the later portion of TIII, the five
substages of MIS 7, TIIIa, and the MIS 7–6 glacial inception (Fig. 3). Due to our unprecedented age control, we can determine the precise timing of
regional changes associated with each MIS 7 substage, as well as the onset of warming in the Austrian Alps associated with TIII and TIIIa
(Fig. 4). While terrestrial records cannot directly date changes to the ocean–cryosphere system during a glacial termination, the climatic excursions
in high-sensitivity regions, such as the Austrian Alps, provide key temporal constraints on the climate events leading up to and during these
transitions.</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="d1e1548">Obliquity (blue), precession (dashed blue), and 65<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N July insolation (dark purple) from Berger (1978). Spannagel <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> from stalagmites SPA121 (green), SPA183 (yellow), and SPA146 (dark blue) (this study). Global stacked benthic <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (black; Lisiecki and Raymo, 2005) plotted with MIS substage labels (gray) for reference. Arrow represents the age of fluorescent inclusions, which suggest a partial retreat of the Hintertux Glacier (214.3 <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M120" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
        <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021-f03.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e1616">Millennial-scale events leading up to glacial terminations III and IIIa. <inline-formula><mml:math id="M121" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Sr</mml:mi></mml:mrow></mml:math></inline-formula> ratios (a proxy for IRD) from North Atlantic sediment cores U1308 (brown; Channell et al., 2012) and U1302 and U1303 (yellow; Hodell et al. 2008), Chinese stalagmite <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (orange; Cheng et al., 2016), Ejulve cave <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (blue) and <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (green) from southeastern Spain (Pérez-Mejías et al., 2017), and Spannagel Cave <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> from the Austrian Alps (black; this study). Major IRD events highlighted in gray.</p></caption>
        <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021-f04.png"/>

      </fig>

      <p id="d1e1698">Following the start of speleothem growth at 247.3 <inline-formula><mml:math id="M126" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 <inline-formula><mml:math id="M127" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, an abrupt shift towards higher <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values at
242.5 <inline-formula><mml:math id="M129" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M130" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> marks the onset of regional warming associated with the TIII deglaciation. The ensuing interglacial period (MIS 7e) is
characterized by high <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values (greater than <inline-formula><mml:math id="M132" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 ‰) and spanned 5 <inline-formula><mml:math id="M133" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ky</mml:mi></mml:mrow></mml:math></inline-formula> from 241.8 to 236.0
(<inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M135" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Depleted <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values (less than <inline-formula><mml:math id="M137" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>12 ‰) between 234.3 and 216.9 (<inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M139" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> coincide
with MIS 7d. Maximum regional cooling occurred between 231.3–228.6 (<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M141" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. An abrupt shift towards higher <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>
values at 216.8 <inline-formula><mml:math id="M143" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M144" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> marks the onset of regional warming associated with TIIIa. Two periods of high <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values
between 215.7–212.9 (<inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M147" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M148" display="inline"><mml:mo lspace="0mm">&gt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M149" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 ‰) and 201.8–197.1 (<inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M151" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M152" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>8.7 ‰) coincide with
interglacial periods MIS 7c and 7a, respectively. A final shift towards lower <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values from 197.1 to 191.4 (<inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M155" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>
coincides with the MIS 7–6 transition, the latter portion of which is replicated by stalagmites SPA 146 and 183.</p>
      <p id="d1e1992">On millennial timescales, remarkable similarities are observed between Spannagel <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> and paleorecords that are sensitive to the
North Atlantic climate (Fig. 4). These similarities highlight the rapid climatic link between the European Alps and North Atlantic realm, as observed
in later interglacial periods (e.g., Holzkämper et al., 2004; Mangini et al., 2007; Wilcox et al.,
2020) and glacial periods (e.g., Moseley et al., 2014; Mayr et al., 2019). Most striking is the millennial-scale covariance of Spannagel
<inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> and Chinese monsoon <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>, which is explained through the following teleconnections: temperature anomalies in
the North Atlantic region influence the intensity of heat transport by northern Hadley cell circulation, which triggers a latitudinal shift in its
ascending branch, known as the Intertropical Convergence Zone (ITCZ). Latitudinal shifts in the ITCZ, in turn, influence the Chinese monsoon strength
(see Cheng et al., 2016, for details). Thus, both Chinese and Spannagel speleothems respond to common climate forcings on millennial
timescales. Identifying the mechanisms behind North Atlantic-forced excursions in Spannagel <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> is challenging due to the
complex array of processes that influence Spannagel <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> but is likely linked to synchronous temperature changes and/or latitudinal
shifts in the westerlies. In alignment with previous work, we interpret Spannagel <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> as a faithful recorder of millennial-scale
changes in the North Atlantic realm during MIS 7.</p>
      <p id="d1e2092">For the remainder of this discussion, we will examine the variations in Spannagel <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> associated with MIS 7 in order to provide new
temporal constraints on climate changes in the Austrian Alps, as well as new insights into millennial-scale changes in the North Atlantic leading up
to TIII and TIIIa.</p>
<?pagebreak page1448?><sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Termination III</title>
      <p id="d1e2117">The last four main glacial terminations can be separated into two categories: those that were interrupted by Northern Hemisphere stadial events (TI
and TIII) and those that were uninterrupted or minimally interrupted (TII and TIV) (Cheng et al., 2009). During TI, multiple meltwater pulses sourced
from the decaying Northern Hemisphere ice sheets resulted in a stratification of surface waters and expansion of winter sea ice in the North Atlantic
realm (Denton et al., 2010). The expansion of sea ice amplified seasonality, such that Europe experienced cold and arid winter conditions
(e.g., Renssen and Isarin, 2001).</p>
      <p id="d1e2120">Peak concentrations of ice-rafted detritus (IRD) in North Atlantic sediments indicate that TIII, similar to TI, was punctuated by two discharge
events, S8.2 and S8.1 (Fig. 4; Channell et al., 2012). Well-dated Spanish speleothems constrain the timeline of these events, starting with S8.2, at
249–247.4 <inline-formula><mml:math id="M163" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Pérez-Mejías et al., 2017). The onset of speleothem deposition in Spannagel Cave coincides with the end of the S8.2
event (Fig. 4). We interpret the lack of deposition during and prior to the S8.2 event as possible evidence for freezing conditions in Spannagel Cave
during stadial conditions. Following the S8.2 event, a resumption of warmer North Atlantic conditions contributed to increased humidity in Spain
(248 <inline-formula><mml:math id="M164" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2 <inline-formula><mml:math id="M165" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>; Pérez-Mejías et al., 2017), an abrupt strengthening of the Chinese monsoon (247.6 <inline-formula><mml:math id="M166" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M167" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>; Cheng
et al., 2009), and above-freezing temperatures in the central Alps prompting speleothem growth (247.3 <inline-formula><mml:math id="M168" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 <inline-formula><mml:math id="M169" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e2179">MIS 7 records from the circum-Mediterranean region. Spannagel Cave <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (black; this study), Crovassa Azzurra (Sardinia, Italy) <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (blue) and <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (green) (Columbu et al., 2019), western Mediterranean SST (Martrat et al., 2004), and Mediterranean sea-level reconstructions (purple; Dutton et al., 2009) (pink; Bard et al., 2002). Purple dashed lines are for visual aid only; absolute sea levels are unknown. Spannagel <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> events that are decoupled from Mediterranean temperatures and humidity records represent evidence for temperature-driven <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> excursions in the Austrian Alps, as opposed to changes in the proportion of Mediterranean-sourced moisture arriving at our study site.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://cp.copernicus.org/articles/17/1443/2021/cp-17-1443-2021-f05.png"/>

        </fig>

      <p id="d1e2264">A second discharge event (S8.1) occurred at 244.7–241 <inline-formula><mml:math id="M175" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> and coincided with a depletion in Spanish speleothem <inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula>
(Pérez-Mejías et al., 2017), which is interpreted as the sudden arrival of meltwater (depleted <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>) into North Atlantic
intermedial latitudes similar to processes observed during TI. The depleted <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> signal was likely transported downstream to the
Austrian Alps. The short negative excursion in Spannagel <inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> starting at 242.6 <inline-formula><mml:math id="M180" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M181" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> may represent the muted
signature of this event. Following the event, Spannagel <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> exhibits an abrupt increase between 242.5 and 241.9
(<inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M184" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. This major shift in Spannagel <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> coincides with remarkable precision with well-dated records that are
sensitive to North Atlantic climate changes, including vegetation productivity in the Iberian Peninsula (241.6–240.7 <inline-formula><mml:math id="M186" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.6 <inline-formula><mml:math id="M187" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>;
Pérez-Mejías et al., 2017) and Chinese monsoon intensity (242.8–241.01 <inline-formula><mml:math id="M188" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M189" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>; Cheng et al., 2009, 2016). The Spannagel
timing of TIII additionally coincides (within uncertainties) with an abrupt warming of SSTs in the North Atlantic (Martrat
et al., 2007) and Mediterranean (Fig. 5; Martrat et al., 2004). Combined, these globally distributed records point to a rapid warming in the North
Atlantic realm at this time. We interpret the <inline-formula><mml:math id="M190" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 3 ‰ increase in Spannagel <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> as an abrupt rise in local winter
temperatures. A possible increase in the advection of isotopically enriched Mediterranean moisture to the Austrian Alps<?pagebreak page1449?> may have amplified this
warming signal, although the extent to which Mediterranean-sourced precipitation influences the <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> signature at our study site is
still unclear. Using our high-precision chronology, we assign the onset of warming to 242.5 <inline-formula><mml:math id="M193" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M194" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e2492">The Spannagel <inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> record indicates a 7.6 <inline-formula><mml:math id="M196" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M197" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ky</mml:mi></mml:mrow></mml:math></inline-formula> lag in the onset of regional warming relative to the rise in
65<inline-formula><mml:math id="M198" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N summer insolation associated with TIII (Berger, 1978). The observed lag is similar but greater than the 5.1 <inline-formula><mml:math id="M199" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M200" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ky</mml:mi></mml:mrow></mml:math></inline-formula> lag
in regional warming relative to TII, as recorded in a speleothem from Hölloch on the northern rim of the Alps (Moseley et al., 2015). A likely
explanation for a longer lag time may be the low obliquity forcings during TIII, resulting in lower-than-average insolation during boreal summers,
which may have delayed warming in the Alps until near-peak insolation.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>MIS 7e and 7d</title>
      <p id="d1e2558">Following TIII, a period of high Spannagel <inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values (<inline-formula><mml:math id="M202" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>10 ‰) between 241.8 and 236.0 (<inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M204" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> marks warmer
temperatures in the Austrian Alps associated with MIS 7e (Fig. 3). This interval coincides with increased humidity in the Iberian Peninsula
(Pérez-Mejías et al., 2017) and Italy (Columbu et al., 2019) and an expansion of forests in Greece (Tzedakis et al., 2003; Roucoux et al., 2008). Spannagel <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values reach a maximum at 240.5 <inline-formula><mml:math id="M206" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M207" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, coinciding with peak
65<inline-formula><mml:math id="M208" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N summer insolation at 241.0 <inline-formula><mml:math id="M209" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Berger at al., 1978). The end of MIS 7e is characterized by a slow decline starting at
236.0 <inline-formula><mml:math id="M210" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M211" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, followed by an abrupt drop (<inline-formula><mml:math id="M212" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>9.9 ‰ to <inline-formula><mml:math id="M213" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>12 ‰) between 236.0 and 234.3 (<inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M215" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. This
period coincides with a steady decline of vegetation productivity in the Iberian Peninsula starting at 238.4 <inline-formula><mml:math id="M216" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2 <inline-formula><mml:math id="M217" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>
(Pérez-Mejías et al., 2017) and a shift towards cooler conditions between <inline-formula><mml:math id="M218" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 237 and 239 <inline-formula><mml:math id="M219" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> in southeastern Europe (Tzedakis et al., 2003; Roucoux et al., 2008). Sardinian stalagmites, however, indicate persistent Mediterranean advection (as suggested by humid conditions) up to
230.1 <inline-formula><mml:math id="M220" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.6 <inline-formula><mml:math id="M221" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 5; Columbu et al., 2019). A decoupling of Spannagel and Sardinian <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values at this time further
underscores that temperature, not moisture source, was the primary driver of Spannagel <inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> depletion at this time.</p>
      <?pagebreak page1450?><p id="d1e2773">Depleted Spannagel <inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values (<inline-formula><mml:math id="M225" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M226" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>12 ‰) from 234.3 to 216.9 (<inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M228" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> coincide with MIS 7d
(Fig. 3). Depleted Spannagel <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values during this time can be attributed to cooler local temperatures, although uninterrupted
stalagmite deposition indicates that temperatures remained above freezing in this cave (Spötl and Mangini, 2007). Maximum cooling
(<inline-formula><mml:math id="M230" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M231" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>13 ‰) occurred between 231.3 and 228.6 (<inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M233" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Maximum cooling coincides with the lowest 65<inline-formula><mml:math id="M234" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N summer
insolation value (387 <inline-formula><mml:math id="M235" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) over the last 800 <inline-formula><mml:math id="M236" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, centered at 230.0 <inline-formula><mml:math id="M237" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Berger, 1978). Maximum cooling in the Alps also
coincides with an abrupt weakening of the Chinese monsoon within <inline-formula><mml:math id="M238" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1 <inline-formula><mml:math id="M239" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> uncertainties (Cheng et al., 2009), suggesting Northern
Hemisphere-wide cooling. During this time, sea level fell between <inline-formula><mml:math id="M240" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.5 <inline-formula><mml:math id="M241" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M242" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>21 <inline-formula><mml:math id="M243" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> relative to modern levels throughout (Dutton
et al., 2009), atmospheric <inline-formula><mml:math id="M244" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula><inline-formula><mml:math id="M245" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> dipped below 203 <inline-formula><mml:math id="M246" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:mrow></mml:math></inline-formula> between 229.6 and 220.9 (<inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M248" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Bazin et al., 2013), and
North Atlantic SSTs fell to near glacial levels (Martrat et al., 2007). In Europe, <inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> records from the Iberian Peninsula
(Pérez-Mejías et al., 2017) and pollen records from Albania (Francke et al., 2016) and Greece (Tzedakis et al., 2003; Roucoux et al., 2008) indicate glacial-like conditions during MIS 7d. In the Mediterranean realm, increased aridity recorded by Sardinian
speleothems between 225–221 (<inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M251" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 5; Columbu et al., 2019) and Peqiin Cave in northern Israel at 223 <inline-formula><mml:math id="M252" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 4 <inline-formula><mml:math id="M253" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Bar-Matthews
et al., 2003) overlap within age uncertainties of Spannagel-determined MIS 7d. Overall, the Spannagel record provides new age constraints for the
timing and duration of maximum stadial conditions in Europe associated with MIS 7d.</p>
      <p id="d1e3053">Following the 2.7 <inline-formula><mml:math id="M254" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ky</mml:mi></mml:mrow></mml:math></inline-formula> time period of maximum cooling, Spannagel <inline-formula><mml:math id="M255" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values plateau at low (<inline-formula><mml:math id="M256" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M257" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>12 ‰) values
until 216.8 <inline-formula><mml:math id="M258" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M259" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Low Mediterranean Sea levels (Dutton et al., 2009) and meltwater pulses in the Black Sea (Badertscher et al.,
2011) between <inline-formula><mml:math id="M260" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 230 and 217 <inline-formula><mml:math id="M261" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> support the presence of Eurasian ice sheets, which likely contributed to cooler temperatures and/or
southerly shifted westerlies over Europe.</p>
</sec>
<sec id="Ch1.S5.SS3">
  <label>5.3</label><title>Termination IIIa</title>
      <p id="d1e3132">TIIIa is often referred to an “extra” termination that resulted from the collapse of MIS 7d ice sheets in response to anomalously high
insolation. Similar to main glacial terminations, TIIIa is characterized by a rapid rise in North Atlantic SSTs (e.g., Martrat et al., 2007),
atmospheric <inline-formula><mml:math id="M262" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula><inline-formula><mml:math id="M263" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (Bazin et al., 2013), global benthic marine <inline-formula><mml:math id="M264" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> (Lisiecki and Raymo, 2005), and an abrupt rise in sea
level (e.g., Dutton et al., 2009). However, due to large age uncertainties, the exact timing of TIIIa in marine and ice records remains unclear. To
resolve this issue, the timing of TIIIa has been previously determined by precisely dated Chinese stalagmites, which<?pagebreak page1451?> reveal millennial-scale weak
monsoon intervals that correspond to meltwater discharge events in the North Atlantic (Cheng et al., 2009, 2016). The exact weak monsoon interval
corresponding to TIIIa, however, remains a topic of debate. Cheng et al. (2009) first interpreted TIIIa as the weak monsoon interval occurring at
228 <inline-formula><mml:math id="M265" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.8 <inline-formula><mml:math id="M266" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Cheng et al. (2016) later revised this interpretation by associating TIIIa with the weak monsoon interval at
217.1 <inline-formula><mml:math id="M267" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M268" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e3198">An abrupt rise in Spannagel <inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> between 216.8 and 216.1 (<inline-formula><mml:math id="M270" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M271" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> supports the timing of TIIIa defined in Cheng
et al. (2016). Similar to TIII, a brief negative excursion in Spannagel <inline-formula><mml:math id="M272" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> prior to the abrupt rise may correspond to the peak
in North Atlantic IRD at 216 <inline-formula><mml:math id="M273" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 4; Channell et al., 2012) that, when aligned to our chronology, suggests that a major meltwater pulse
associated with TIIIa occurred no later than 216.9 <inline-formula><mml:math id="M274" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.5 <inline-formula><mml:math id="M275" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. This timing agrees within uncertainties with the Chinese monsoon weak
interval at 217.1 <inline-formula><mml:math id="M276" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M277" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Our record reveals that the onset of Spannagel <inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> increase occurred 1.2 <inline-formula><mml:math id="M279" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ky</mml:mi></mml:mrow></mml:math></inline-formula>
after peak 65<inline-formula><mml:math id="M280" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N summer insolation. A lack of change in stable isotopes from Mediterranean-dominated records during this time (e.g., Columbu
et al., 2019) further suggests the abrupt increase of Spannagel <inline-formula><mml:math id="M281" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> was primarily driven by warming temperatures in the Austrian
Alps (Fig. 5).</p>
</sec>
<sec id="Ch1.S5.SS4">
  <label>5.4</label><title>MIS 7c and 7a</title>
      <p id="d1e3357">High <inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values associated with MIS 7c occur between 215.7 and 212.9 (<inline-formula><mml:math id="M283" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M284" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, with slightly lower values
(<inline-formula><mml:math id="M285" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M286" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10.6 ‰) extending until 212.0 <inline-formula><mml:math id="M287" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.4 <inline-formula><mml:math id="M288" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 3). <inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> drops abruptly between 212.0 and 211.7
(<inline-formula><mml:math id="M290" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M291" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> and remains low between 211.7 and 204.1 (<inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M293" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. This period of depleted <inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values
coincides within uncertainties with low 65<inline-formula><mml:math id="M295" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N summer insolation (207 <inline-formula><mml:math id="M296" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>) associated with MIS 7b. Spannagel <inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula>
rises between 204.1 and 201.5 (<inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M299" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> and remains high for the remainder of MIS 7a until 197.1 (<inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M301" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e3559">Maximum <inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values during MIS 7a and 7c indicate warmer winter temperatures in the Alps relative to MIS 7e, with MIS 7a the warmest
substage. This MIS 7 substage comparison is in agreement with planktonic foraminiferal assemblages on an Iberian Margin sediment core, which suggest
higher winter temperatures (<inline-formula><mml:math id="M303" display="inline"><mml:mo lspace="0mm">+</mml:mo></mml:math></inline-formula>1.5 <inline-formula><mml:math id="M304" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>) during MIS 7a relative to MIS 7e (Desprat et al., 2006). European micropaleontological data indicate that
MIS 7c and 7a had the longest duration, the most diverse and complete forest succession, and the warmest temperatures relative to MIS 7e (Penaud et al.,
2008; Tzedakis et al., 2003; Roucoux et al., 2008). Enriched Spannagel <inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values during MIS 7a and 7c may have been further amplified by an increase in
northerly advection from the Mediterranean, as suggested by humid conditions in Sardinia (Columbu et al., 2019) and eastern Mediterranean sapropel
deposits (e.g., Ziegler et al., 2010), although the extent to which Mediterranean-sourced precipitation influences the <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> signature
at our study site is still unclear.</p>
      <p id="d1e3632">Spötl et al. (2008) proposed that four fluorescent inclusions (i.e., dust layers) identified in SPA 121 reflect a partial retreat (or repeated
partial retreats) of the Hintertux Glacier. Our updated chronology places the timing of the dust layers at 214.3 <inline-formula><mml:math id="M307" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.4 <inline-formula><mml:math id="M308" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, which
coincides with maximum obliquity forcing (Fig. 3; Berger, 1978). This finding supports previous work which argues that changes in obliquity act as a
major control on Alpine glacier mass balance by influencing the latitudinal distribution of solar radiation (e.g., Huybers,
2006). High obliquity and insolation forcing likely drove increased ablation of the Hintertux Glacier
and warm regional temperatures (as suggested by maximum MIS 7c <inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> values) at 214.3 <inline-formula><mml:math id="M310" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.4 <inline-formula><mml:math id="M311" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S5.SS5">
  <label>5.5</label><title>MIS 7–6 transition</title>
      <p id="d1e3691">A drop in Spannagel <inline-formula><mml:math id="M312" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> starting at 197.1 <inline-formula><mml:math id="M313" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 <inline-formula><mml:math id="M314" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> marks the end of MIS 7a in the Alps (Fig. 3). We define the
Spannagel MIS 7–6 transition to between 197.1–191.4 (<inline-formula><mml:math id="M315" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M316" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>, which coincides with a drop of the Mediterranean Sea level, as shown by
Bard et al. (2002). Two newly collected stalagmites from this cave (SPA146 and 183) that grew between 191.8 and 182.3 (<inline-formula><mml:math id="M317" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M318" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>
provide additional records of the late MIS 7a-to-6e transition and early MIS 6e. All three stalagmites show a gradual decreasing trend in
<inline-formula><mml:math id="M319" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> until approximately 187 <inline-formula><mml:math id="M320" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. A lack of calcite deposition after 182.3 <inline-formula><mml:math id="M321" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 <inline-formula><mml:math id="M322" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> suggests unfavorable
conditions in Spannagel Cave, possibly related to due to partly cold-base conditions of the glacier above the cave.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <?pagebreak page1452?><p id="d1e3811">The response of climatically sensitive regions to glacial–interglacial cycles and their abrupt transitions provides key insight into the timing of
global climate change. In this study, we present the first ever paleorecord of MIS 7 with relative age uncertainties <inline-formula><mml:math id="M323" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 2 ‰. Using this
chronology, we can determine the precise timing and duration of climate variations in the Austrian Alps in response to the MIS 7 substages and
associated glacial terminations. Following the start of speleothem growth, an abrupt increase of <inline-formula><mml:math id="M324" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values at
242.5 <inline-formula><mml:math id="M325" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M326" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> marks the onset of regional warming associated with TIII. The ensuing interglacial period (MIS 7e) is characterized by
enriched <inline-formula><mml:math id="M327" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values (<inline-formula><mml:math id="M328" display="inline"><mml:mo lspace="0mm">&gt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M329" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 ‰) from 241.8 to 236.0 (<inline-formula><mml:math id="M330" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M331" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. Depleted <inline-formula><mml:math id="M332" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values
(<inline-formula><mml:math id="M333" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M334" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>12 ‰) between 234.3 and 216.9 (<inline-formula><mml:math id="M335" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M336" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> coincide with the Northern Hemisphere cool period. Similar to TIII, a brief
negative excursion in Spannagel <inline-formula><mml:math id="M337" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> prior to the abrupt rise associated with TIIIa suggests that a major meltwater pulse
occurred in the North Atlantic around 216.9 <inline-formula><mml:math id="M338" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>. An abrupt shift towards higher <inline-formula><mml:math id="M339" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values at 216.8 <inline-formula><mml:math id="M340" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3 <inline-formula><mml:math id="M341" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula>
marks the onset of regional warming associated with TIIIa. Two periods of high <inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values between 215.7–212.9
(<inline-formula><mml:math id="M343" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M344" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> and 201.8–197.1 (<inline-formula><mml:math id="M345" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M346" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> coincide with interglacial periods MIS 7c and 7a, respectively. A final shift towards
lower <inline-formula><mml:math id="M347" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">18</mml:mn></mml:msup><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> values from 197.1 to 191.4 (<inline-formula><mml:math id="M348" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M349" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ka</mml:mi></mml:mrow></mml:math></inline-formula> coincides with the MIS 7–6 transition. In total, this
multi-stalagmite record provides important chronological constraints on climate shifts in the Austrian Alps associated with MIS 7 while providing new
insight into the timing of millennial-scale changes in the North Atlantic realm.</p>
</sec>

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

      <p id="d1e4093">The data presented in this paper are available for download from the NOAA/World Data Service for Paleoclimatology archives: <uri>https://www.ncdc.noaa.gov/paleo/study/33653</uri> (Wendt et al., 2021).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e4099">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/cp-17-1443-2021-supplement" xlink:title="pdf">https://doi.org/10.5194/cp-17-1443-2021-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e4108">CS collected the samples. KAW and XL conducted measurements and analyzed results. HC, RLE, and CS provided scientific guidance, laboratory facilities, and funding. All authors contributed to the final manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e4114">The authors declare that they have no conflict of interest.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e4120">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="d1e4126">Special thanks are owed to  Manuela Wimmer and Mathieu Pythoud for their assistance in the laboratory.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e4131">This research has been supported by grants from the Austrian Science Fund (FWF) awarded to Christoph Spötl, NSFC 41888101 to Hai Cheng, and NSF1702816 to R. Lawrence Edwards.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e4138">This paper was edited by Amaelle Landais and reviewed by two anonymous referees.</p>
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    <!--<article-title-html>Precise timing of MIS 7 substages from the Austrian Alps</article-title-html>
<abstract-html><p>Investigating the precise timing of regional-scale climate changes during glacial terminations and the interglacial periods that follow is key to
unraveling the mechanisms behind these global climate shifts. Here, we present a high-precision time series of climate changes in the Austrian Alps
that coincide with the later portion of Termination III (TIII), the entire penultimate interglacial (Marine Isotope Stage (MIS) 7), Termination IIIa
(TIIIa), and the penultimate glacial inception (MIS 7–6 transition). Using state-of-the-art mass spectrometry techniques, we have constructed a
uranium-series chronology with relative age uncertainties averaging 1.7&thinsp;‰ (2<i>σ</i>) for our study period (247 to 191 thousand years
before present, ka). Results reveal the onset of warming in the Austrian Alps associated with TIII at 242.5&thinsp;±&thinsp;0.2&thinsp;ka and the
duration of MIS 7e warming between 241.8 and 236.7 (±0.6)&thinsp;ka. An abrupt shift towards higher <i>δ</i><sup>18</sup>O values at
216.8&thinsp;ka marks the onset of regional warming associated with TIIIa. Two periods of high <i>δ</i><sup>18</sup>O values (greater than
−10&thinsp;‰ Vienna Pee Dee Belemnite (VPDB)) between 215.9–213.3 and 204.3–197.5 (±0.4)&thinsp;ka coincide with interglacial substages MIS 7c and 7a,
respectively. Multiple fluorescent inclusions suggest a partial retreat of the local Alpine glacier during peak obliquity forcings at
214.3&thinsp;±&thinsp;0.4&thinsp;ka. Two newly collected stalagmites from Spannagel Cave (SPA146 and 183) provide high-resolution replications of the
latter portion of the MIS 7a-to-6e transition. The resulting multi-stalagmite record reveals important chronological constraints on climate shifts in
the Austrian Alps associated with MIS 7 while offering new insight into the timing of millennial-scale changes in the North Atlantic realm leading
up to TIII and TIIIa.</p></abstract-html>
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