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  <front>
    <journal-meta><journal-id journal-id-type="publisher">CP</journal-id><journal-title-group>
    <journal-title>Climate of the Past</journal-title>
    <abbrev-journal-title abbrev-type="publisher">CP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Clim. Past</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1814-9332</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/cp-18-975-2022</article-id><title-group><article-title>Humidity changes and possible forcing mechanisms over the last millennium in arid Central Asia</article-title><alt-title>Humidity changes and possible forcing mechanisms</alt-title>
      </title-group><?xmltex \runningtitle{Humidity changes and possible forcing mechanisms}?><?xmltex \runningauthor{S. Feng et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Feng</surname><given-names>Shengnan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Liu</surname><given-names>Xingqi</given-names></name>
          <email>xqliu@cnu.edu.cn</email>
        <ext-link>https://orcid.org/0000-0002-8811-0268</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3 aff4">
          <name><surname>Shi</surname><given-names>Feng</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3963-1822</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff5">
          <name><surname>Mao</surname><given-names>Xin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Li</surname><given-names>Yun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Wang</surname><given-names>Jiaping</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>College of Resource, Environment and Tourism, Capital Normal
University, Beijing 100048, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Key Laboratory of Cenozoic Geology and Environment, Institute of
Geology and Geophysics,<?xmltex \hack{\break}?> Chinese Academy of Sciences, Beijing 100029, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Georges Lemaître Centre for Earth and Climate Research, Earth
and Life Institute, <?xmltex \hack{\break}?> Université Catholique de Louvain, Louvain-la-Neuve
1348, Belgium</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>CAS Center for Excellence in Life and Paleoenvironment, Beijing
100044, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Institute of Hydrogeology and Environmental Geology, Chinese
Academy of Geological Sciences, <?xmltex \hack{\break}?>  Shijiazhuang 050061, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Qinghai Institute of Salt Lakes, Chinese Academy of Sciences,
Xining 810008, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Xingqi Liu (xqliu@cnu.edu.cn)</corresp></author-notes><pub-date><day>6</day><month>May</month><year>2022</year></pub-date>
      
      <volume>18</volume>
      <issue>5</issue>
      <fpage>975</fpage><lpage>988</lpage>
      <history>
        <date date-type="received"><day>11</day><month>October</month><year>2021</year></date>
           <date date-type="rev-request"><day>22</day><month>October</month><year>2021</year></date>
           <date date-type="accepted"><day>11</day><month>April</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Shengnan Feng et al.</copyright-statement>
        <copyright-year>2022</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022.html">This article is available from https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022.html</self-uri><self-uri xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022.pdf">The full text article is available as a PDF file from https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e164">Hydroclimate changes have exerted a significant influence on the historical
trajectory of ancient civilizations in arid Central Asia where the central
routes of the Silk Road have been hosted. However, the climate changes on
different timescales and their possible forcing mechanisms over the last
millennium remain unclear due to low-resolution records. Here, we provide a
continuous high-resolution humidity history in arid Central Asia over the
past millennium based on the <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1.8</mml:mn></mml:mrow></mml:math></inline-formula>-year high-resolution
multiproxy records with good chronological control from Lake Dalongchi in
the central Tian Shan. Generally, the climate was dry during the
Medieval Warm Period (MWP) and Current Warm Period (CWP) and wet during the
Little Ice Age (LIA), which could be attributed to the influence of the
North Atlantic Oscillation (NAO) and the Atlantic Multidecadal Oscillation
(AMO). Furthermore, we find that the humidity oscillation was dramatic and
unstable at multidecadal to century scales. Especially within the LIA, four
wet episodes and three dry periods occurred. The continuous wavelet analysis
and wavelet coherence show that the humidity oscillation is modulated by the
Gleissberg cycle at the century scale and by the quasi-regular period of El
Niño–Southern Oscillation (ENSO) at the multidecadal scale. Our findings
suggest that the effect of the solar cycle and the quasi-regular period of
ENSO should be seriously evaluated for hydroclimate predictions and climate
simulations in arid Central Asia in the future.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e186">Arid Central Asia (ACA), far away from the ocean, is not only one of the
driest and largest inland regions worldwide, but also the birthplace of the
far-reaching ancient civilizations that spread along the Silk Road
(Li et al., 2016; Narisma et al., 2007). Scarce precipitation,
intense evaporation, and fragile ecosystems render this region sensitive to
abrupt changes in effective humidity. Arid Central Asia is primarily
controlled by the prevailing westerlies (F. Chen et al., 2019; Aizen et
al., 2001; Sorrel et al., 2021; Huang et al., 2015b, 2014;
Lauterbach et al., 2014). The moisture vapor was predominantly transported
via the westerlies and originated from the North Atlantic Ocean,
Mediterranean, Black Sea, and Aral–Caspian Sea  (Lan et al., 2018; Chen et
al., 2010; Huang et al., 2015b; Aizen et al., 2001; Mathis et al., 2014).
Proxy records from ACA are valuable for understanding the driving factors
and processes of underlying hydroclimate evolution in the inland region,
which provides useful reference for human adaptation to hydroclimate changes
at present and into the future  (Li et al., 2016). On the sub-orbital scale,
solar radiation controlled the intensity of the westerlies through the
variation of the meridional radiation gradient between high and middle latitudes,
thus having the dominant influence on moisture changes of ACA during the
Holocene  (F. Chen et al., 2019; Jin et al., 2011). In addition, the
sub-orbital-scale hydroclimate changes are also related to the shift of the
Subtropical High, the strength and position of the Siberian High, North
Atlantic Oscillation (NAO) mode, and the changes of the Laurentide and
Scandinavian Ice Sheets  (Sorrel et al., 2021; F. Chen et al., 2019; Carlson
and Clark, 2012; Aichner et al., 2015; Wolff et al., 2016; Huang et al.,
2014; Schwarz et al., 2017; Lauterbach et al., 2014).</p>
      <p id="d1e189">In the past decades, a couple of proxy archives from ACA have been recorded
the hydroclimate changes during the key periods such as the Medieval Warm
Period (MWP) and Little Ice Age (LIA) over the past millennium  (Ling et
al., 2018; He et al., 2013; Lan et al., 2019; Song et al., 2015; Ma et al.,
2008; Zhang et al., 2009; Rousseau et al., 2020; Chen et al., 2006; J. Chen et al., 2019). In earlier studies, a humid climate during the MWP and a dry
climate condition during the LIA was documented by the tree ring of <italic>Sabina przewalskii</italic> (Kom.) (Zhang et al., 2003). This climate pattern was further
demonstrated by the records from Lake Lop Nur and Daxigou profile on the
northern slope of the central Tian Shan  (Zhang et al., 2009; Ma et
al., 2008). However, a growing body of studies based on the lacustrine
sediments, ice cores, tree ring, and peat profiles show a generally similar
climate pattern of a relatively dry MWP and a wet LIA in ACA over the last
millennium  (Chen et al., 2015, 2010; F. Chen et al., 2019; J. Chen et al., 2019; Lei et al., 2014; Rousseau et al., 2020; Lan et al.,
2019; He et al., 2013; Song et al., 2015). Furthermore, there is some debate
regarding the driving mechanism of the natural hydroclimate evolution over
the last millennium. Many studies emphasize that internal climate
variability (i.e., major sea and atmospheric modes) is supposed to be more
marked than external factors (e.g., solar forcing) in influencing
hydroclimate changes  (F. Chen et al., 2019; Chen et al., 2006; Lan et al.,
2019). According to this theory, the NAO and Atlantic Multidecadal Oscillation
(AMO) play important roles by controlling the strength and shift of the
westerly jet stream in determining hydroclimatic changes in ACA (Chen et
al., 2015, 2010; Aichner et al., 2015; Lan et al., 2018, 2019). The El Niño–Southern Oscillation (ENSO) also contributes the
climate variability in ACA on a multi-centennial timescale  (Chen et al.,
2015; F. Chen et al., 2019). In contrast, several paleoclimate records prefer
to highlight the possible solar forcing to the humidity oscillation over the
last millennium  (Song et al., 2015; Zhao et al., 2009; He et al., 2013;
Ling et al., 2018). For example, the solar imprint on the effective humidity
fluctuations in ACA was proved by wavelet spectral analysis of the sediment
record from Lake Manas  (Song et al., 2015). Also, the <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">200</mml:mn></mml:mrow></mml:math></inline-formula>-year moisture oscillations are related to the solar forcing recorded by the
lake-level changes during the past 1000 years from Lake Hurleg
(Zhao et al., 2009). Therefore, the climate changes on different time
scales and their possible forcing mechanisms over the
last millennium remain controversial. These controversies are largely attributed to
low-resolution records or chronological uncertainties due to the old carbon
effect  (Chen et al., 2010; Q. Zhang et al., 2021), which limit our
understanding of the hydroclimate evolution on decadal to centennial scales
and of the relative role of external and internal drivers over the past
millennium. More well-dated, high-resolution records are needed to further
investigate the humidity evolution.</p>
      <p id="d1e205">Here, we present a continuous <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1.8</mml:mn></mml:mrow></mml:math></inline-formula>-year high-resolution
humidity reconstruction with good chronological control from Lake Dalongchi
in the central Tian Shan of ACA over the past millennium (1180–2018 CE). Low- and high-frequency signals recovered from our reconstruction offer
the potential to detect climate fluctuations at decadal to centennial
scales, as well as long-term changes. Then, we explore the contribution of
internal climate variability (which mainly refers to the NAO, AMO, and ENSO in
this study) and solar activity to humidity oscillations on different
timescales over the past millennium.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Study site</title>
      <p id="d1e226">Lake Dalongchi (42<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula><inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">26</mml:mn><mml:mo>′</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">31</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M6" display="inline"><mml:mn mathvariant="normal">42</mml:mn></mml:math></inline-formula><inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula><inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">26</mml:mn><mml:mo>′</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">58</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> N, 83<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula><inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">16</mml:mn><mml:mo>′</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">48</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M11" display="inline"><mml:mn mathvariant="normal">83</mml:mn></mml:math></inline-formula><inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula><inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">18</mml:mn><mml:mo>′</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">15</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> E, 2400 m above sea level), located on the south slope of the central Tian Shan, is an ideal location for investigating hydroclimate changes in
ACA (Fig. 1a), as the lake sits in the core area of the “westerlies
dominated climatic regime (WDCR)” (F. Chen et al., 2019). The bedrock
in the catchment of Lake Dalongchi is composed of pillow lava, gabbro, and
limestone blocks included in a matrix of sheared calcareous turbidites. The
ophiolitic mélanges are juxtaposed against Paleozoic sedimentary rocks,
gneissic granitoids, and andalusite cordierite-bearing micaschist (Xiao
et al., 2013; Ma et al., 2006; Gao et al., 1998). The main aquifer is hosted
by ophiolitic rocks and categorized as a fissured rock aquifer
(<uri>http://gis.geoscience.cn/website/hg/viewer.htm</uri>, last access: 8 January 2022). This aquifer has
multi-scale hydraulic discontinuities and low groundwater potentiality due
to the structural heterogeneities of the ophiolitic rocks (Lods et al.,
2020; Jeanpert et al., 2019; Boroninaa et al., 2003).</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="d1e355">Maps of the study site. <bold>(a)</bold> Locations of Lake Dalongchi and other
humidity records in arid Central Asia, mentioned in the text. Sites 1–6
denote the Bayanbuluk meteorological station, Lake Bosten (Chen et
al., 2006), Badian Jaran Desert  (Ma and Edmunds, 2006; Gates et
al., 2008), Lake Sugan (He et al., 2013), Lake Gahai (He
et al., 2013), and Lake Ala Kol  (Rousseau et al., 2020),
respectively. The dashed yellow line indicates the boundary of the modern
Asian summer monsoon; the mid-latitude inland region on the western side of
the modern Asia summer monsoon boundary line is arid central Asia (ACA)
(Chen et al., 2010; F. Chen et al., 2019). The map was generated using ArcMap
10.2 software (ESRI, USA, <uri>http://www.esri.com</uri>, last access: 9 February 2020). <bold>(b)</bold> Watershed
map of the study site. <bold>(c)</bold> Bathymetric contour map of Lake Dalongchi with
the coring site.</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f01.png"/>

      </fig>

      <p id="d1e376">Lake Dalongchi is a small alpine freshwater lake formed by glacial moraine
damming and has a mean pH of 8.03 and a salinity of 0.31 g L<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Both
the north and south sides of the lake are surrounded by steep mountains
(Fig. 1b). The lake is mainly fed by the river originating from mountains on
the east, precipitation within the catchment, and glacial meltwater from the
surrounding mountains at high elevations. The lake water flows out into Lake
Xiaolongchi through a tunnel under the moraine and the outflow discharge is
low. Then the lake water from Xiaolongchi flows westwards into the Kuche
River basin (Fig. 1b).</p>
      <p id="d1e392">Measured in July 2018, the lake covers a surface area of <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1.4</mml:mn></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> and has a catchment area of <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">131</mml:mn></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. The
maximum water depth of Lake Dalongchi reaches 7.4 m in the western lake, and
its depth largely decreases from west to east (Fig. 1c). Alpine coniferous
forests dominated by Picea primarily thrive on the southern and western
slopes of the surrounding mountains, while the northern slope is covered by
herbs such as Chenopodiaceae, <italic>Artemisia</italic>, Poaceae, and Cyperaceae. According to the
records from 1958 to 2019 at Bayanbuluk Station which is located
<inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> km to the northeast of Lake Dalongchi, the mean annual
temperature is <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4.6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C with a July average of 10.9 <inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C
and a January average of <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">26.4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, and the mean annual
precipitation and evaporation are 270 and 3200 mm, respectively. The mean
annual precipitation is far less than the evaporation capacity. Moreover,
most of the precipitation occurs as convective rainfall from June–August
(Lan et al., 2018). The prevailing wind is from the northwest, and
the annual average wind speed is only 2.73 m s<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The average number of
sandstorm days is less than 5 d yr<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> based on the meteorological records
from 1959 to 1998  (B. Zhang et al., 2021; Zhou et al., 2002).</p>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Materials and methods</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Sampling</title>
      <p id="d1e534">In July 2018 and August 2019, we retrieved several parallel long sediment
cores from Lake Dalongchi at a maximum water depth of 7.4 m using the UWITEC
platform manufactured in Austria, and several short cores using a piston
gravity corer (Fig. 1c). To determine overlaps and ensure the continuity of
the cores, magnetic susceptibility (MS) nondestructive scanning of all long
and short sediment cores was used to obtain a 6.95 m long composite core
(DLC1819) (Fig. 2).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e539">Sedimentary lithology and multi-proxy variation versus depth for
the composite DLC1819 core.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f02.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Laboratory analysis</title>
      <p id="d1e556">The DLC1819 core was subsampled at 1 cm intervals. All subsamples were stored in
a freezer in our laboratory at a constant temperature of 4 <inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and
used for MS, grain size, total organic carbon (TOC), and total nitrogen (TN)
analyses. Samples for MS were dried at below 40 <inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in a constant
temperature air-blast drying oven and ground and packed into standard
plastic boxes with a capacity of <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula>. A Bartingon MS2
susceptibility meter was used to measure magnetic susceptibility. Samples
used for grain size measurement were pretreated with 10–20 mL of 10 %
<inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to remove organic matter and then with 10 mL of 10 % HCl to
remove carbonates; next, samples were rinsed with deionized water and
finally treated with 10 mL 0.05 M (<inline-formula><mml:math id="M32" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NaPO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M33" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msub></mml:math></inline-formula> on an ultrasonic
vibrator for 10 min to promote dispersion. Grain size distributions were
determined using Malvern/MS 3000 laser grain size analyzer. The samples used
for TOC and TN determination were decalcified with 10 % HCl and rinsed
repeatedly with deionized water. Then, <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>–5 mg dried and
ground samples were analyzed using the EURO EA 3000 elemental analyzer.</p>
      <p id="d1e649">Terrestrial plant remains at different depths in the DLC1819 core were used for
accelerator mass spectrometry (AMS) <inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">14</mml:mn></mml:msup></mml:math></inline-formula>C measurements at Beta Analytic
Inc., U.S.A. (Table 1). The uppermost sediments were used for the
radiometric dating by measuring the activity of <inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">137</mml:mn></mml:msup></mml:math></inline-formula>Cs as a function of
depth. The samples of the uppermost sediments at 0.5 cm intervals were dried
and ground to less than 100 mesh and then loaded into the 5 mL cylindrical
PVC tube. Radio-activity of <inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">137</mml:mn></mml:msup></mml:math></inline-formula>Cs was measured using a
spectrum analysis system consisting of a high-purity germanium well detector
produced by EG&amp; G Ortec Company (USA), Ortec 919 spectrum controller,
and IBM microcomputer with a 16 K channel multichannel analyzer.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e682">Accelerator mass spectrometry (AMS) <inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">14</mml:mn></mml:msup></mml:math></inline-formula>C dating results of
DLC1819 core.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">Composite</oasis:entry>
         <oasis:entry colname="col5">Analyzed</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">13</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>C</oasis:entry>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8">Calendar</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">No.</oasis:entry>
         <oasis:entry colname="col2">Lab. no</oasis:entry>
         <oasis:entry colname="col3">Sample ID</oasis:entry>
         <oasis:entry colname="col4">depth (cm)</oasis:entry>
         <oasis:entry colname="col5">material</oasis:entry>
         <oasis:entry colname="col6">(‰)</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">14</mml:mn></mml:msup></mml:math></inline-formula>C age/BP</oasis:entry>
         <oasis:entry colname="col8">age/CE</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">Beta – 514897</oasis:entry>
         <oasis:entry colname="col3">DLC-1-1-61</oasis:entry>
         <oasis:entry colname="col4">69</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">24.9</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mn mathvariant="normal">90</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1870–1928</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">Beta – 507553</oasis:entry>
         <oasis:entry colname="col3">DLC-1-1-135</oasis:entry>
         <oasis:entry colname="col4">143</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">27.4</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mn mathvariant="normal">170</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1721–1818</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">Beta – 507554</oasis:entry>
         <oasis:entry colname="col3">DLC-1-2-82</oasis:entry>
         <oasis:entry colname="col4">210</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">31.4</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mn mathvariant="normal">230</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1635–1684</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">Beta – 507555</oasis:entry>
         <oasis:entry colname="col3">DLC-1-2-155</oasis:entry>
         <oasis:entry colname="col4">283</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">26.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:mn mathvariant="normal">340</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1470–1640</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">5</oasis:entry>
         <oasis:entry colname="col2">Beta – 507556</oasis:entry>
         <oasis:entry colname="col3">DLC-1-3-61</oasis:entry>
         <oasis:entry colname="col4">324</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">28.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mn mathvariant="normal">430</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1420–1498</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">6</oasis:entry>
         <oasis:entry colname="col2">Beta – 507557</oasis:entry>
         <oasis:entry colname="col3">DLC-1-3-119</oasis:entry>
         <oasis:entry colname="col4">382</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">22.3</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mn mathvariant="normal">440</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1416–1490</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">7</oasis:entry>
         <oasis:entry colname="col2">Beta – 514898</oasis:entry>
         <oasis:entry colname="col3">DLC-1-3-131</oasis:entry>
         <oasis:entry colname="col4">394</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">23.7</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mn mathvariant="normal">370</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1446–1528</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">8</oasis:entry>
         <oasis:entry colname="col2">Beta – 514901</oasis:entry>
         <oasis:entry colname="col3">DLC-3-5'-37</oasis:entry>
         <oasis:entry colname="col4">585</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">23.6</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mn mathvariant="normal">670</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1274–1320</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">9</oasis:entry>
         <oasis:entry colname="col2">Beta – 542591</oasis:entry>
         <oasis:entry colname="col3">DLC2019-1-5-76</oasis:entry>
         <oasis:entry colname="col4">625</oasis:entry>
         <oasis:entry colname="col5">Wood</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">23.1</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mn mathvariant="normal">800</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">1184–1275</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Lithology and chronology</title>
      <p id="d1e1223">DLC1819 core is mainly composed of clayey silt and can be divided into two
lithology units from bottom to top (Fig. 2). Unit A (695–430 cm) is mainly
composed of dark or light brown clayey silt with clear lamination. Unit B
(430–0 cm) has a dramatic lithological variation characterized by brown or
greyish-green clayey silt without obvious lamination. There are lots of the
plant residues in the core, but they are more abundant in Unit B than in Unit A
(Fig. 2).</p>
      <p id="d1e1226">A significant increase in <inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">137</mml:mn></mml:msup></mml:math></inline-formula>Cs activities occurred at approximately 71 cm, which could be attributed to the onset of rising concentrations of
<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">137</mml:mn></mml:msup></mml:math></inline-formula>Cs in the Northern Hemisphere (NH) at 1952 CE (Fig. 3a). The
distinct peak at the depth of 64 cm was taken as the 1963 CE global fallout
maximum  (Pennington et al., 1973) (Fig. 3a). We established the
age–depth model of DLC1819 based on the 2 <inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">137</mml:mn></mml:msup></mml:math></inline-formula>Cs ages and nine radiocarbon
ages by the Bacon 2.5.7 procedure in R software using the Bayesian method
(Blaauw and Christen, 2011) (Fig. 3b). Chronology results show that
the DLC1819 core covers the past 840 years with an approximate average
sedimentation rate of 9.0 mm yr<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Unit A has unusually stable sediment
accumulation rates with an average of 10.3 mm yr<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, while the sediment
accumulation rates vary greatly from 4.9 to 10.6 mm yr<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in Unit B (Fig. 2).</p><?xmltex \hack{\newpage}?><?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1295">Age–depth model for the DLC1819 core of Lake Dalongchi. <bold>(a)</bold> The
<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">137</mml:mn></mml:msup></mml:math></inline-formula>Cs activity versus depth in the uppermost sediments. <bold>(b)</bold> Bayesian
age-model for the calibrated ages. The black dotted lines indicate the
95 % probability intervals of the model.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f03.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>TOC, TN, C/N, MS, grain size</title>
      <p id="d1e1327">TOC and TN results show broadly similar changes and vary between 1.14 %
and 8.33 % and between 0.09 % and 0.59 %, respectively (Fig. 2). <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios fluctuate between 7.95 and 18.42 with an average of 10.88, and the
values of <inline-formula><mml:math id="M67" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios exceed 10 at the depths of 440–650 cm, 330–400 cm,
230–300 cm, and 130–180 cm (Fig. 2). MS values of the DLC1819 core vary between
5.90 and <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mn mathvariant="normal">41.89</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> Kg<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> with an average of
<inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mn mathvariant="normal">20.66</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> Kg<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Fig. 2). The silt percentage
fluctuates from 43.64 % to 88.50 % with an average of 71.91 % while
the variation of clay percentage has an opposite trend to that of silt, and
its values vary from 11.84 % to 54.26 % with an average of 25.97 %
(Fig. 2). Sand content only accounts for 2.43 % of the total grain size on
average. Generally, the higher values of the MS and silt content and the
lower clay content correspond to the higher <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios and vice versa (Fig. 2).</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Proxy interpretation and humidity index reconstruction</title>
      <p id="d1e1462">The characteristics of 125–500 <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m particles with well-developed
surface structure can fully reflect the transport distance and dynamic
conditions of sediment in a specific environment; short distances and weak
transport dynamics usually result in a poor grain roundness of sediments
(Moral Cardona et al., 2005; Mahaney et al., 2004). The surface
microscopic properties of four randomly selected samples in the DLC1819 core
show that the grains in the range of 125–500 <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m are characterized by
poor roundness with an angular outline which is quite different from the
eolian materials (M. Zhang et al., 2021) (Fig. S1 in the
Supplement), excluding the possibility that the clastic particles are
derived from eolian deposition in Lake Dalongchi.</p>
      <p id="d1e1481"><?xmltex \hack{\newpage}?>Terrestrial plants usually have <inline-formula><mml:math id="M77" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios of more than 20
(Meyers, 1994, 2003), so the increased <inline-formula><mml:math id="M78" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios in Lake
Dalongchi sediments reflect the input amount of allochthonous organic matter
(Fig. 2). Synchronously, the increase in the MS values and silt content also
indicates the increased input of detrital materials and the intensified
erosion of the basin (Fig. 2). Given that the weak inflows of the runoff
into Lake Dalongchi, which is a shallow and a small lake with an area only of
1.4 km<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, the distance from the lakeshore to the sampling site is the
key to determining the amount of exogenous detrital materials in the core.
Therefore, during the humid (dry) period represented by high (low) lake level
and enlarged (reduced) lake area, exogenous materials containing magnetic
minerals, coarse grain components, and terrestrial plants were poorly (easily)
transported to the sampling site due to the long (short) distance from the
lakeshore and reduction (intensified) erosion in the basin (Fig. 4). Thus, the
high MS values, silt content, and <inline-formula><mml:math id="M80" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios indicate a dry climate and vice
versa (Fig. 4).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e1532">Schematic diagram illustrating a simple explanation of the
lacustrine depositional process in the Lake Dalongchi region. Lake level
condition and the transport process of exogenous materials in the humid
period <bold>(a)</bold> and the dry period <bold>(b)</bold>.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f04.png"/>

        </fig>

      <p id="d1e1548">Accordingly, multiple proxies, such as <inline-formula><mml:math id="M81" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios, MS, silt, and clay
fractions, were synthetically employed to reconstruct the humidity index
(HI) in the Lake Dalongchi region over the past millennium (Fig. 5). As the high
values of <inline-formula><mml:math id="M82" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">C</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> ratios, MS, and silt contents and low values of clay content
reflect the arid climatic environment, the first three records multiplied by
<inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> and clay content were normalized to a <inline-formula><mml:math id="M84" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> score (Fig. 5b, c, d, e). Then
the HI was derived from the average of the normalized standard <inline-formula><mml:math id="M85" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores.
Positive and negative <inline-formula><mml:math id="M86" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores indicate wet and dry climatic conditions
(Fig. 5a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e1609">Humidity index reconstruction <bold>(a)</bold> based on the <inline-formula><mml:math id="M87" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores of total
organic carbon <inline-formula><mml:math id="M88" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> total nitrogen (<inline-formula><mml:math id="M89" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">TOC</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">TN</mml:mi></mml:mrow></mml:math></inline-formula>) ratios <bold>(b)</bold>, the <inline-formula><mml:math id="M90" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores of magnetic
susceptibility (MS) <bold>(c)</bold>, the <inline-formula><mml:math id="M91" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores of silt fraction <bold>(d)</bold>, and the <inline-formula><mml:math id="M92" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> scores
of clay fraction variation <bold>(e)</bold> in the DLC1819 core in Lake Dalongchi. Light
grey bars highlight intervals of increased humidity in Lake Dalongchi during
the LIA.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f05.png"/>

        </fig>

</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Humidity changes over the last millennium</title>
      <p id="d1e1689">There is a generally positive correlation (<inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.298</mml:mn><mml:mo>*</mml:mo></mml:mrow></mml:math></inline-formula>) between the
reconstructed HI and the instrumental relative humidity records over the
past 60 years from the nearby Bayanbuluk meteorological station at the 0.05
significance level, verifying the reliability of the humidity reconstruction
(Fig. 6a). The HI changes show that the climate was dry during the MWP
(1180–1420 CE) and CWP (1920–2018 CE) and wet during the LIA (1420–1920 CE)
(Fig. 6b). Moreover, our preliminary palynological data also show a dry
climate characterized by herb pollen (<inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">71</mml:mn></mml:mrow></mml:math></inline-formula> %) dominated by
<italic>Artemisia</italic>, Chenopodiaceae, and Poaceae during the MWP and a wet climate
characterized by the rapid increased tree pollen dominated by <italic>Picea</italic> (up to
45 %) during the LIA (unpublished data). This multi-centennial climate
pattern is generally in agreement with the hydroclimatic patterns revealed
by recent numerous studies in ACA (Chen et al., 2006; Song et al., 2015;
Lan et al., 2018, 2019; Zhao et al., 2009; He et al., 2013; Ma
and Edmunds, 2006; Gates et al., 2008; Rousseau et al., 2020) (Fig. 6c, d,
e, f, g, h), although several studies tend to suggest humid climate
conditions during the MWP in ACA  (Zhang et al., 2009; Ma et al., 2008;
Zhang et al., 2003). A total 5 of the 17 records selected on the basis of reliable
chronologies and robust proxies from ACA show a relatively dry MWP, and a
wet LIA characterized not only by relatively humid but also by high
precipitation  (Chen et al., 2010) (Fig. 6c). Recently, records
from Lake Ala Kol, Kyrgyzstan, reveal the cold and wet climate conditions
during the LIA indicated by the prominent glacier advances (Rousseau et
al., 2020) (Fig. 6h), which corresponds to the maximal ice accumulation in
the Guliya ice core  (Rousseau et al., 2020; Yang et al., 2009). Thus, the
humidity changes of Dalongchi lake do not indicate a local signal but a
regional signal, i.e., the typical “westerlies-dominated climatic regime”
(WDCR) (F. Chen et al., 2019).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e1724">Humidity index (HI) of Lake Dalongchi and comparison to other
records in ACA over the last millennium. <bold>(a)</bold> Comparison between the HI (blue
line) and the standardized instrumental effective humidity recorded by
Bayanbuluk meteorological station (grey line). An asterisk (<inline-formula><mml:math id="M95" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula>) represents the 0.05
significance level. <bold>(b)</bold> The reconstructed HI for the past millennium
(1180–2018 CE). <bold>(c)</bold> The synthesized moisture curve over the last millennium
in ACA (Chen et al., 2010). <bold>(d)</bold> Variations in the mean grain size
along the BST04H core in Lake Bosten (Chen et al., 2006). <bold>(e)</bold> The
unsaturated recharge history in Badian Jaran  (Gates et al., 2008;
Ma and Edmunds, 2006). <bold>(f)</bold> Chironomid inferred salinity (Salch) in SG03I of
Sugan Lake (Chen et al., 2009). <bold>(g)</bold> %C<inline-formula><mml:math id="M96" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">37</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> from Lake Gahai
(He et al., 2013). <bold>(h)</bold> <inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">Ca</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">inc</mml:mi></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M98" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> coh from Lake Ala Kol
(Rousseau et al., 2020). <bold>(i)</bold> The reconstructed NAO
(Ortega et al., 2015). <bold>(j)</bold> The reconstructed AMO
(Wang et al., 2017). Light grey bars highlight intervals of increased
humidity in Lake Dalongchi during the LIA.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f06.png"/>

        </fig>

      <p id="d1e1807">The previous study shows that the higher anomalous climatic instability
during the LIA compared to the MWP, suggesting the moisture instability
prefers to occur within the conditions of an overall cold climate  (J. Chen
et al., 2019). However, it is not clear how the specific unstable wet and
dry climate fluctuated during the LIA, due to the relatively low-resolution
records in ACA  (Chen et al., 2006; Zhao et al., 2009; Lan et al., 2019).
The HI reconstruction of Lake Dalongchi provides new evidence for the
unstable hydroclimatic variability during the LIA (Fig. 6b). Four wet
episodes with the sharp high HI values were recorded for 1420–1470,
1550–1600, 1650–1720, and 1800–1920 CE, and three dramatic dry periods with the
low HI values were recorded for 1470–1550, 1600–1650, and 1720–1800 CE during
the LIA (Fig. 6b). Our high-resolution reconstruction clearly documented
several obvious and dramatic secondary humidity fluctuations within the LIA,
which are not clearly captured in other current records from ACA  (Chen et
al., 2006; Ma and Edmunds, 2006; Gates et al., 2008; He et al., 2013) (Fig. 6). The climatic instability during the LIA can also be reflected by the
dramatic lithological variations and the unstable sediment accumulation
rates in Unit B (Fig. 2). Moreover, continuous wavelet transform (CWT) of HI
exhibits a significant century-scale dominant oscillation ranging from
<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">88</mml:mn></mml:mrow></mml:math></inline-formula> to 146 years, which is nearly throughout the entire time
series and prominent in 1450–1800 CE, as well as a strong <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula>-
to 65-year multidecadal oscillation at a 95 % confidence level relative to
the red noise spectrum (Fig. 7a).</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e1833">The wavelet analysis of the HI and the relationship between the HI
and the TSI or ENSO. <bold>(a)</bold> Continuous wavelet (CWT) power spectrum of the HI.
The irregular thick black contour represents the 95 % confidence level
against red noise, and the thin curved black solid line is the cone of
influence (COI)  (Grinsted et al., 2004). <bold>(b)</bold> A comparison between
the HI and the reconstructed total solar irradiance (TSI)  (Bard et
al., 2000). Wolf, Spörer, Maunder, and Dalton represent several grand
solar minimums that occurred during the LIA. <bold>(c)</bold> The wavelet coherence (WTC)
result between the HI and the TSI  (Bard et al., 2000). <bold>(d)</bold> As <bold>(b)</bold>,
but for ENSO variance reconstruction  (Li et al., 2011). Orange arrows
represent the enhanced ENSO amplitude trend. <bold>(e)</bold> As <bold>(c)</bold>, but for ENSO
variance  (Li et al., 2011). <bold>(f)</bold> A comparison between the century
component of HI and TSI (Bard et al., 2000). <bold>(g)</bold> A comparison
between the multidecadal component of the HI and ENSO variance
reconstruction (Li et al., 2011). The 95 % confidence level against
red noise is shown as an irregular thick black contour. The black arrows
illustrate the relative phase relationship: arrows pointing right are
in phase and those pointing left are anti-phase (Grinsted et al., 2004). Two asterisks (**)
represent the 0.01 significance level.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://cp.copernicus.org/articles/18/975/2022/cp-18-975-2022-f07.png"/>

        </fig>

</sec>
<sec id="Ch1.S5.SS3">
  <label>5.3</label><title>Possible forcing mechanisms</title>
<sec id="Ch1.S5.SS3.SSS1">
  <label>5.3.1</label><title>The influence of NAO and AMO</title>
      <p id="d1e1885">Several studies have linked hydroclimate changes in arid Central Asia to the
NAO and the AMO over the last millennium  (Aichner et al., 2015; Yan et
al., 2019; Chen et al., 2006; Lan et al., 2018; F. Chen et al., 2019; J. Chen et al., 2019). On multidecadal timescales, most records show that the NAO and
AMO are dominated by alternating sea surface temperatures (SSTs) and
sea-level pressure (SLP) anomalies, respectively  (Ortega et al., 2015;
Knudsen et al., 2014). The climatic instability during the LIA may be link
to the NAO and AMO via the westerlies  (J. Chen et al., 2019). However,
the relationship between HI, NAO, and AMO is ambiguous on multidecadal
timescales (Fig. 6b, i, g). Although the wavelet coherence (WTC) results
show that the NAO and HI have approximately <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula>-, 50-, and
128 year periodicities, and the AMO and HI have the periodicities of
<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">32</mml:mn></mml:mrow></mml:math></inline-formula>, 70, and 128 years, these periodicities are
nonpersistent (Fig. S2). Therefore, our results suggest
that the periodic variations in NAO and AMO themselves have little influence
on the humidity fluctuation in Lake Dalongchi at the multidecadal timescale.</p>
      <p id="d1e1908">However, on multi-centennial timescales, the dominant dry climate conditions
during the MWP and humid climate conditions during the LIA seems related to
the relatively positive and negative phases exhibited in the NAO and AMO,
respectively (Fig. 6b, i, g). Previous studies indicate the negative phase
of the NAO and AMO during the LIA favors increasing precipitation in ACA
(J. Chen et al., 2019; Chen et al., 2015, 2006, 2016; Lan et al., 2018; Aichner et al.,
2015). During the MWP, the positive
phase of the NAO with enhanced pressure between the Azores High and the
Icelandic Low would lead to strengthened zonal flow, and the axis of maximum
moisture transport and preferred storm track extend to the north and east
(Trouet et al., 2009). In contrast, the axis of maximum moisture
transport and preferred storm track migrated southwards when the NAO was in
a negative phase during the LIA  (Hurrell, 1995). A general
cold (warm) phase of the AMO corresponds to the negative (positive) NAO
phase during the LIA (MWP) (Wang et al., 2017; Ortega et al., 2015),
leading to a weaker (strong) upper-level jet stream intensity and further
resulting in development (recession) of the through-ridge system,
consequently contributing to the increased (decreased) precipitation in ACA
(J. Chen et al., 2019). Thus, the multi-centennial behavior in our
reconstruction might be related to the influence of the NAO and AMO on
hydroclimate changes between the MWP and the LIA.</p>
</sec>
<sec id="Ch1.S5.SS3.SSS2">
  <label>5.3.2</label><title>The role of the Gleissberg cycle</title>
      <p id="d1e1919">Solar forcing has been treated as a critical factor for influencing key
components (e.g., temperature, precipitation, evaporation, winds, ocean
circulation, and iceberg transport) of the climate system  (Sha et al.,
2016; Bond et al., 2001; Bard and Frank, 2006; Knudsen et al., 2014). As the
largest dry inland regions on the globe, the climate records from ACA are
valuable for investigating the fingerprint of solar forcing. We compared HI
with the reconstructed total solar irradiance (TSI)  (Bard et al.,
2000) and found a strong link and inverse relationship between the HI and
TSI, especially during the LIA (Fig. 7b). The HI increased significantly and
reached its peak during the several grand solar minimums (Wolf, Spörer,
Maunder, Dalton), whereas the humidity decreased rapidly in the maximum
solar activity period (Fig. 7b). The WTC spectrum between HI and TSI shows a
strong correlation and anti-phase pattern (Fig. 7c). Periodicities of
significant coherence for HI and TSI occurred at <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">88</mml:mn></mml:mrow></mml:math></inline-formula> to 146 years, particularly from 1400 CE to the present. Arrows in the significant
coherence spectral area point almost entirely to the left, implying the
persistent negative correlation of HI and TSI (Fig. 7c). Therefore, the WTC
result confirms that the persistent <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">88</mml:mn></mml:mrow></mml:math></inline-formula>–146-year cycle of HI
in CWT is associated with solar activity (Fig. 7a, c). The cycle of 88–146 years should be attributed to the century-scale solar cycle of Gleissberg
(Gleissberg, 1958, 1965; Ogurtsov et al., 2015) (Fig. 7a).
Accordingly, we extracted this century signal from the original HI series
based on the ensemble empirical mode decomposition (EEMD), a new
noise-assisted data analysis (NADA) method  (Wu and Huang, 2009;
Huang et al., 1998). The relationship between the century component and TSI
has an apparent correlation (<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.217</mml:mn><mml:mo>*</mml:mo><mml:mo>*</mml:mo></mml:mrow></mml:math></inline-formula>) and a clear coherence spectral
area (Figs. 7f and S3a). The HI shows an extreme
instability accompanied by obvious secondary oscillations of cold–wet and
warm–dry at century timescales during the LIA under the regulation of solar
activity (Fig. 7f). This verifies the critical role of the Gleissberg solar
cycle in controlling the effective humidity at the century scale during the
last millennium in ACA. Shindell et al. examined the climate response to the
solar forcing at the Maunder minimum and indicated that even relatively
little solar activity might play a primary role in century-scale climate
change in NH  (Shindell et al., 2001). The possible solar
contribution of the Gleissberg century cycle to climate changes over at
least the last millennium has been reported from the North Atlantic region
(Moffa-Sánchez et al., 2014; Ogurtsov et al., 2002a, b, 2015). In arid Central Asia, several records
documented the solar fingerprint by the evidence of <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">200</mml:mn></mml:mrow></mml:math></inline-formula>-year
periodicity between the proxy data and solar activity time series
(Zhao et al., 2009; Yin et al., 2016), and sediment records from
Lake Toson and Lake Manas exhibited periodicities of 93 years and 70 to 100 years respectively through the spectral and wavelet analysis, which may be
linked with the Gleissberg solar cycle (Ling et al., 2018; Song et al.,
2015). However, still, rare records in ACA documented the good relationship
between the effective humidity changes and the fluctuations of the
Gleissberg cycle. Our reconstruction provides strong evidence for negative
link between the Gleissberg solar cycle and humidity changes at century
timescales during the last millennium in ACA.</p>
      <p id="d1e1970">The confusion we focus on now is how solar activity significantly affected
hydroclimate fluctuations in ACA over the last millennium. Several studies
proposed that the solar forcing may influence the variability of the
sea–atmospheric modes, the NAO in particular  (Swingedouw et al., 2011;
Kirov and Georgieva, 2002; Kodera, 2002; Gimeno et al., 2003). Kodera (2002) suggests that the NAO extends to the stratosphere during the high
solar activity and to the troposphere during the low solar activity. Such a
relationship between the solar activity and troposphere or stratosphere
subsequently determines the positive or negative phase of NAO  (Shindell
et al., 2001; Kodera and Kuroda, 2002; Gray, 2003). Solar irradiance also
has been served as a trigger for the shifts of the precipitation-bearing
westerlies during winter  (Brahim et al., 2018; Kodera, 2002; Yukimoto et
al., 2017). Ultimately, the solar variability indirectly affects the
hydroclimate changes through modulating the NAO state, suggesting solar
regulation for hydroclimate might be amplified on a regional scale through
atmospheric circulation  (Ineson et al., 2011; Shindell et al., 2001;
Gray, 2003; Brahim et al., 2018; Kodera, 2002; Yukimoto et al., 2017).</p>
      <p id="d1e1973">However, for ACA far from the ocean with scarce precipitation and intense
evaporation, the mechanism of solar forcing on humidity may be direct. Our
reconstruction reveals the robust negative relationship between the TSI and
HI, but the ambiguous relationship between the NAO and HI (Figs. 6, 7). The
paleoclimate records from ACA also highlight that the intense evaporation
and direct heating caused by the enhanced solar irradiance control the
effective humidity  (Liu et al., 2019; Song et al., 2015; He et al., 2013;
Wu et al., 2020; Ling et al., 2018; Zhao et al., 2009). To further
investigate the potential feedback processes between the solar variability
and effective humidity at century timescales in ACA, we performed a transient
experiment forced only by the TSI for the last millennium using the Max
Planck Institute Earth System Model (MPI-ESM) (Jungclaus et al.,
2014) (Fig. S4). Most of the precipitation occurs in
June–August in the study area, and the evaporation process is intensified in
summer  (Lan et al., 2018), so we mainly considered the results of
June–July–August (JJA). There is a positive relationship between the TSI,
temperature, and evaporation (Fig. S4), indicating that
high solar output favors high temperature and intensified evaporation at
century timescales in arid Central Asia. Moreover, the effective humidity
shows a negative association with evaporation, temperature, and TSI
variability (Fig. S4). However, the relationship between
precipitation and effective humidity appears to be obscure at the century
timescale (Fig. S4). Therefore, the solar forcing has a
direct contribution to regulating the humidity in ACA by the
Gleissberg century cycle forcing on the temperature and evaporation over the last
millennium, although water vapor transported by westerlies and
precipitation might be affected by ocean–atmosphere modes.</p>
</sec>
<sec id="Ch1.S5.SS3.SSS3">
  <label>5.3.3</label><title>Linkage to ENSO</title>
      <p id="d1e1984">ENSO is a mode of variability representing changes in sea-surface
temperatures and atmospheric circulation across the equatorial Pacific Ocean
(Jiménez-Moreno et al., 2021; Cane, 2005). Paleoclimatic
proxies and historical records suggest ENSO has long-term variability in
amplitude and frequency on multidecadal to centennial timescales  (Yeh and
Kirtman, 2007; D'Arrigo et al., 2005; Li et al., 2011; Mann et al., 2000).
The amplitude of ENSO variability is the important factor to affect the
occurrence of climate extremes over the globe (Mcphaden et al.,
2006; Cheng et al., 2008). On the multi-centennial timescale (i.e., MWP to
LIA), the HI and ENSO variance  (Li et al., 2011) show a similar trend
in amplitude changes (Fig. 7d). The amplitudes of HI and ENSO variance both
show a distinctly increasing trend during the LIA and maintain a relatively
high level from <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1650</mml:mn></mml:mrow></mml:math></inline-formula> to 1950 CE (Fig. 7d). This trend
suggests that the relatively humid environment and unstable hydroclimate in
ACA may be associated with the increase in ENSO variance amplitude  (Li
et al., 2011) and more frequent ENSO events  (Rustic et al., 2015) during
the LIA, which are possible owing to a major reorganization within the tropical
ocean–atmosphere system or significant ENSO teleconnection changes from the
MWP to LIA  (Rustic et al., 2015; Li et al., 2011). The results here
support previous studies showing that ENSO might affect hydroclimate
variability in ACA at multi-centennial timescales with La Niña-like (EI
Niño-like) conditions during the MWP (LIA) (F. Chen et al., 2019; Chen  et al., 2015). During the LIA with relatively warm EI Niño-like
conditions, the Western Pacific Subtropical High enhanced and extended
westwards, and a low-pressure trough related to the weakening of the
Siberian High over the central–southwest Asia region formed, together
resulting wetter climatic conditions in arid Central Asia (Chen et al.,
2015; F. Chen et al., 2019a; Feng et al., 2016; Syed et al., 2006).</p>
      <p id="d1e1997">On the multidecadal timescales, however, the WTC between the HI and ENSO
variance shows a robust negative phase relationship (Fig. 7e). In
particular, the WTC result shows that the HI has a similar quasi-regular
cycle of ENSO variance from 82–90 years during the MWP to 50–60 years thereafter
(Li et al., 2011), which reveals the potential modulation of these
quasi-regular cycles of ENSO variance to extreme humidity oscillations at
the multidecadal timescales in ACA (Fig. 7e). Furthermore, the multidecadal
component of the HI extracted by the EEMD (Wu and Huang, 2009;
Huang et al., 1998) also exhibits an obvious inverse relationship with ENSO
variance (Fig. 7g). The influence of ENSO on the extratropical climate has
been shown to be modulated by ENSO variance at multidecadal timescales, and
the calculated 31-year running correlations between the reconstructed ENSO
variance and other records of ENSO teleconnections shows that the ENSO
teleconnection is robust over Central Asia during the past seven centuries
only except for the Maunder minimum (Li et al., 2013). The
quasi-regular periodic variation of ENSO variance effects on the hydroclimate
changes of ACA at multidecadal timescales might be through modulating the
extreme precipitation. The water vapor from the Arabian Sea may be
transported to the Xinjiang region and cause heavy precipitation, although
the water vapor fluxes mostly come from the west transported by the
prevailing westerlies (Huang et al., 2015a, 2013). Daily
observational precipitation and National Center for Environmental Prediction
(NCEP) reanalysis data also suggest that the low-level water vapor fluxes
from the Indian Ocean, transported along the eastern periphery of the
Tibetan Plateau, are the most important factor leading to rainstorms in ACA
(Huang et al., 2017). However, our knowledge of the cause of ENSO
variance influence on hydroclimate oscillations in ACA at multidecadal
timescales is still in its infancy and remains uncertain, owing to the
complicated interactions of the tropical and subtropical ocean basins at
decadal to multidecadal timescales  (Cai et al., 2019). The mechanisms for
the different timescales between the ENSO amplitude and hydroclimate changes
in ACA require further exploration through high-resolution records and
simulation experiments.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e2010">We present the humidity index (HI) in ACA over the past millennium based on
the <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1.8</mml:mn></mml:mrow></mml:math></inline-formula>-year high-resolution multiproxy records from Lake
Dalongchi in the central Tian Shan. Our results reveal dramatic and
unstable multidecadal to century-scale humidity oscillations over the last
millennium, especially within the LIA, which is distinct from other records
of ACA. Our findings emphasize that the Gleissberg solar cycle and
quasi-regular period of ENSO amplitude play critical roles in controlling
the effective humidity in ACA at century and multidecadal timescales,
respectively. However, high-resolution records on different timescales and
climate model simulations are still needed to improve our understanding of
the physical mechanisms of the links between solar irradiance and
ocean–atmosphere modes and how their coupling affects moisture variation in ACA.</p>
</sec>

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

      <p id="d1e2027">The reconstructed humidity index in this study has been submitted to the datasets
of the 4TU Center for Research Data, which can will be permanently available at
<ext-link xlink:href="https://doi.org/10.4121/16570398" ext-link-type="DOI">10.4121/16570398</ext-link> (Feng et al., 2022).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2033">The supplement related to the article contains the supplementary methods and four supplementary diagrams. The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/cp-18-975-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/cp-18-975-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2042">SF and XL conceived this study, carried out the laboratory analysis and data
interpretation, and wrote the paper. FS and YL performed the data
analysis. XM and JW participated in the retrieval of the sediment core and
sampling. All authors discussed the results and commented on the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2048">The contact author has declared that neither they nor their co-authors have any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2054">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="d1e2060">We are grateful to the three anonymous reviewers and editor Mary Gagen for their insightful comments and constructive suggestions, which helped to improve the manuscript. We thank Junfeng Li, Weihan Jia, Huashu Li, Huihui Qi, and Qi Zhang for their help with the field work.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2065">This research has been supported by the National Key Research and
Development Program of China (grant no. 2018YFA0606400), the National
Natural Science Foundation of China (grant no. 41907375), and the
Basic Research Program of the Institute of Hydrogeology and Environmental Geology
CAGS (grant no. SK202007).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2072">This paper was edited by Mary Gagen and reviewed by three anonymous referees.</p>
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