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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mar. Sci.</journal-id>
<journal-title>Frontiers in Marine Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mar. Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-7745</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fmars.2022.1079301</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Marine Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Deep submerged speleothems in the Sansha Yongle Blue Hole (South China Sea) as determination of low sea levels during the Last Glacial Maximum</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Yu</surname>
<given-names>Xiaoxiao</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn003">
<sup>&#x2020;</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2032147"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Duan</surname>
<given-names>Baichuan</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Zhao</surname>
<given-names>Jingyao</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/846830"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Gu</surname>
<given-names>Dongqi</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2109780"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Feng</surname>
<given-names>Aiping</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Liu</surname>
<given-names>Yanxiong</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Li</surname>
<given-names>Tiegang</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>First Institute of Oceanography, Ministry of Natural Resources</institution>, <addr-line>Qingdao</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Institute of Global Environmental Change, Xi&#x2019;an Jiaotong University</institution>, <addr-line>Xi&#x2019;an</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Fajin Chen, Guangdong Ocean University, China</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Rui Wang, Guangxi University, China; Zhongping Lai, Shantou University, China; Jiantao Cao, Tongji University, China</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Jingyao Zhao, <email xlink:href="mailto:zjy1230@xjtu.edu.cn">zjy1230@xjtu.edu.cn</email>; Tiegang Li, <email xlink:href="mailto:tgli@fio.org.cn">tgli@fio.org.cn</email>
</p>
</fn>
<fn fn-type="present-address" id="fn003">
<p>&#x2020;Present address: Xiaoxiao Yu, State Key Laboratory of Isotope Geochemistry and CAS Center for Excellence in Deep Earth Science, Guangzhou Institute of Geochemistry, Chinese Academy of Sciences, Guangzhou, China</p>
</fn>
<fn fn-type="other" id="fn002">
<p>This article was submitted to Marine Biogeochemistry, a section of the journal Frontiers in Marine Science</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>20</day>
<month>12</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>9</volume>
<elocation-id>1079301</elocation-id>
<history>
<date date-type="received">
<day>25</day>
<month>10</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>28</day>
<month>11</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Yu, Duan, Zhao, Gu, Feng, Liu and Li</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Yu, Duan, Zhao, Gu, Feng, Liu and Li</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Although Last Glacial Maximum (LGM) sea levels have been the focus of much attention in climate and marine sciences, the timing, duration, and magnitude need further research. Here we present observations and analyses of the deepest speleothems (-116 m) collected from the deepest known blue hole on a global scale, the Sansha Yongle Blue Hole, Xisha Islands, South China Sea. The field investigations illustrate that submerged speleothems are irregular cauliflower-like coatings on the downward cave ceiling from water depths of ~90 to 120 m. The downward growth direction and negative stable carbon and oxygen stable isotopes of submerged speleothems suggest that they may deposit in an air-filled condition through gravity drip, indicating the maximum LGM sea level. The deep submerged speleothems were dated, indicating two U&#x2013;Th ages of 29.16 &#xb1; 0.17 and 26.04 &#xb1; 0.18 ka BP and one radiocarbon age of 18.64 &#xb1; 0.12 ka BP, respectively. The investigated deep submerged speleothems therefore clearly determine the minimum onset and maximum termination times for LGM terms of sea level. The results show that LGM began at ~29 ka BP and ended at ~18.5 ka BP. This study therefore provides initial evidence for the use of deep speleothems to determine LGM sea levels and emphasizes the importance of deep submerged speleothems in the reconstruction of Pleistocene low sea levels.</p>
</abstract>
<kwd-group>
<kwd>sea level</kwd>
<kwd>U&#x2013;Th dating</kwd>
<kwd>
<sup>14</sup>C dating</kwd>
<kwd>speleothem</kwd>
<kwd>LGM</kwd>
<kwd>coastal cave</kwd>
</kwd-group>
<contract-num rid="cn001">T2192951, U1906211</contract-num>
<contract-num rid="cn002">ts20190963</contract-num>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content>
</contract-sponsor>
<contract-sponsor id="cn002">Natural Science Foundation of Shandong Province<named-content content-type="fundref-id">10.13039/501100007129</named-content>
</contract-sponsor>
<counts>
<fig-count count="9"/>
<table-count count="1"/>
<equation-count count="0"/>
<ref-count count="52"/>
<page-count count="11"/>
<word-count count="4420"/>
</counts>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<title>Introduction</title>
<p>When global sea levels declined during past glacial epochs, speleothems might have deposited in air-filled coastal karst caves that were probably flooded by subsequent transgressions (<italic>e</italic>.<italic>g</italic>., <xref ref-type="bibr" rid="B40">Richards et&#xa0;al., 1994</xref>; <xref ref-type="bibr" rid="B32">Melim et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B1">Bard et&#xa0;al., 2002</xref>; <xref ref-type="bibr" rid="B13">Dorale et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B34">Moseley et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B12">De Waele et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B15">Dumitru et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B42">Steidle et&#xa0;al., 2021</xref>). Because elevations and absolute ages of speleothems can be accurately determined, they have significant potential for the determination of past maximum sea levels (<xref ref-type="bibr" rid="B20">Gascoyne et&#xa0;al., 1979</xref>; <xref ref-type="bibr" rid="B40">Richards et&#xa0;al., 1994</xref>; <xref ref-type="bibr" rid="B1">Bard et&#xa0;al., 2002</xref>; <xref ref-type="bibr" rid="B14">Dumitru et&#xa0;al., 2019</xref>). Though previous studies over four decades have thoroughly illustrated variable maximum sea levels using U&#x2013;Th and U&#x2013;Pb dating of speleothems in coastal caves (<xref ref-type="bibr" rid="B24">Harmon et&#xa0;al., 1978</xref>; <xref ref-type="bibr" rid="B20">Gascoyne et&#xa0;al., 1979</xref>; <xref ref-type="bibr" rid="B1">Bard et&#xa0;al., 2002</xref>; <xref ref-type="bibr" rid="B13">Dorale et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B34">Moseley et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B14">Dumitru et&#xa0;al., 2019</xref>), the deepest speleothems collected so far were from -54.9 m of a blue hole in South Andros Island (<xref ref-type="bibr" rid="B40">Richards et&#xa0;al., 1994</xref>). These speleothems are therefore unable to determine Pleistocene low sea levels, which were often over 100 m lower than they are at present (<xref ref-type="bibr" rid="B40">Richards et&#xa0;al., 1994</xref>; <xref ref-type="bibr" rid="B28">Lambeck and Chappell, 2001</xref>; <xref ref-type="bibr" rid="B41">Spratt and Lisiecki, 2016</xref>; <xref ref-type="bibr" rid="B25">Huybers et&#xa0;al., 2022</xref>). Therefore, deep submerged speleothems (-116 m) collected from the Sansha Yongle Blue Hole (SYBH) with reliable ages are useful for determining Last Glacial Maximum (LGM) low sea levels.</p>
<p>One of the most highlighted features of the LGM is its low sea level, which was ~120&#x2013;130 m lower than it is today (<xref ref-type="bibr" rid="B23">Hanebuth et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B47">Yokoyama et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B9">Clark and Mix, 2002</xref>; <xref ref-type="bibr" rid="B8">Clark et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B22">Hanebuth et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B29">Lambeck et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al., 2018</xref>). The onset and termination of the LGM is of particular importance but poorly identified by field data. <xref ref-type="bibr" rid="B33">Mix et&#xa0;al. (2001)</xref> considered the LGM spanned 24&#x2013;18 ka BP, whereas a slightly earlier epoch from 26 to 21 ka BP, depending on global sea level minima, was proposed as the LGM duration by another study (<xref ref-type="bibr" rid="B38">Peltier and Fairbanks, 2006</xref>). A 10-m sea level rise that started around 19.6 ka BP was thought to have terminated the LGM (<xref ref-type="bibr" rid="B23">Hanebuth et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B47">Yokoyama et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B22">Hanebuth et&#xa0;al., 2009</xref>). <xref ref-type="bibr" rid="B8">Clark et&#xa0;al. (2009)</xref> compiled 5,704 reliable global ice-sheet extent data and demonstrated that the LGM extended from 26.5 to 19.0 ka BP. Recently, however, two studies concluded that the LGM ended around 19.0 ka BP and began around 31&#x2013;29 ka BP with a rapid ~40-m sea level falling over 2,000 years (<xref ref-type="bibr" rid="B29">Lambeck et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al., 2018</xref>). These discrepancies about LGM onset and termination suggest that it is imperative to find more evidence, especially from remote areas such as the South China Sea (SCS). In addition to the discrepancies, previous LGM low sea level proxies, such as corals and tidal flat sediments, usually exhibit large errors of up to 5&#x2013;10 m, which could cause large uncertainties of LGM low sea levels (<xref ref-type="bibr" rid="B15">Dumitru et&#xa0;al., 2021</xref>). Speleothems and their phreatic overgrowths, deposited under air-filled conditions indicating maximum sea level, potentially provide more accurate sea level determination (<xref ref-type="bibr" rid="B45">van Hengstum et&#xa0;al., 2019</xref>).</p>
<p>In this study, we reported timing results from the deepest submerged speleothems so far collected from the Sansha Yongle Blue Hole (SYBH), Xisha Islands, SCS (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>). SCS is far removed from the glacial isostatic effect (<xref ref-type="bibr" rid="B37">Peltier, 2004</xref>), and the Xisha Islands have been a tectonic stable marginal setting since the Last Interglacial (<xref ref-type="bibr" rid="B31">Ma et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B50">Yu et&#xa0;al., 2022</xref>); hence, this area is suitable for determining past sea levels. Our speleothems were dated using radiocarbon and <sup>230</sup>Th&#x2013;<sup>234</sup>U&#x2013;<sup>238</sup>U methods. Based on the obtained ages, we determined the onset and termination of the LGM. This novel evidence suggests that deep submerged speleothems may be a promising fingerprint for Pleistocene low sea levels.</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>Location map <bold>(A)</bold> and aerial photography of Sansha Yongle Blue Hole <bold>(B)</bold> in Yongle Atoll, Xisha Islands, South China Sea. The A&#x2013;A&#x2032; cross-section line in the right panel represents vertical profiles of <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g001.tif"/>
</fig>
</sec>
<sec id="s2">
<title>Regional setting</title>
<p>SYBH (latitude: 16&#xb0;31&#x2032;29&#x2033; N; longitude: 111&#xb0;46&#x2032;04&#x2033; E) is the deepest (-301.19 m) known coastal carbonate cave globally. This ocean blue hole is located in the eastern end of the Yongle Atoll (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1A</bold>
</xref>), which consists of highly porous carbonate corals and coralline algae bindstones that initially developed in the early Miocene (19.6 Ma) with a volcanic base belonging to the Xisha uplift (<xref ref-type="bibr" rid="B26">Jiang et&#xa0;al., 2019</xref>). Based on a lithological study of a CK-2 borehole from nearby Chenhang Island, the bottom of SYBH approximately matches with an interface of ~4.0 Ma (<xref ref-type="bibr" rid="B19">Fan et&#xa0;al., 2019</xref>). SYBH has a planform at the surface which is shaped like a comma, with a maximum width of 162.3 m (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1B</bold>
</xref>).</p>
<p>As shown in <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>, SYBH displays a fracture-guide hole pattern which is differentiated from other complex karst caves with branch-work caves (<xref ref-type="bibr" rid="B35">Mylroie et&#xa0;al., 1995</xref>; <xref ref-type="bibr" rid="B30">Li et&#xa0;al., 2018</xref>). SYBH exhibits four distinct and successive sections from top to bottom as caves I to IV, respectively (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2B</bold>
</xref>; <xref ref-type="bibr" rid="B50">Yu et&#xa0;al., 2022</xref>). Corals grow at the uppermost entrance of SYBH, whereas massive sediments and fallen rocks cover the lower hole (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2A</bold>
</xref>). For our study, fortunately, a ceiling (cave III) was observed at water depths between ~90 and 160 m on the northeastern inner wall. Irregular and popcorn-like cave coatings extensively cover the seaward ceiling between water depths of ~90 and 120 m (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2A</bold>
</xref>).</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Cross-section <bold>(A)</bold> and 3-D topography <bold>(B)</bold> of Sansha Yongle Blue Hole.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g002.tif"/>
</fig>
</sec>
<sec id="s3" sec-type="materials|methods">
<title>Materials and methods</title>
<sec id="s3_1">
<title>Sampling and site description</title>
<p>In total, 13 short rock cores (5 cm in diameter) with length &lt; 30 cm were drilled from the SYBH during May and June 2017 using a miniature underwater drilling rig carried by the FCV2000D remotely operated vehicle (ROV; <xref ref-type="bibr" rid="B50">Yu et&#xa0;al., 2022</xref>). Three-dimensional morphology was reconstructed using an unmanned sea-robot ship equipped with a multibeam system above 15 m and a professional-grade ROV equipped with a multibeam system below 15 m (<xref ref-type="bibr" rid="B30">Li et&#xa0;al., 2018</xref>). In addition to morphology, a high-resolution underwater camera was carried by the ROV to gather more detailed knowledge. This study focuses on a short core (length: 26 cm; latitude: 16.52&#xb0;; longitude: 111.77&#xb0;) consisting of speleothems and substrates from the depth of 116-m (Bh116; <xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>). In Bh116, the speleothems broke into small pieces during the drilling processes due to their weak cements. Therefore, the relative positions for these broken pieces could not be accurately reconstructed though we carefully protected them during the collection, transportation, and rinsing.</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Photographs of sample Bh116 <bold>(A)</bold> and two subsamples <bold>(B, C)</bold> showing locations for thin section (blue lines;<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>), scanning electron microscopy (green rectangles; <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>), XRD (cyan rectangles; <xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>), carbon and oxygen isotopes (black circles; <xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref>), U&#x2013;Th dating (red circles; <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>), and radiocarbon dating (orange circles; <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>). The dotted red lines in <bold>(A)</bold> divide the core samples into substrates and speleothems, <italic>i</italic>.<italic>e</italic>., Bh116s1 and Bh116s2.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g003.tif"/>
</fig>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>Thin-section micrographs of sample Bh116. <bold>(A, B)</bold> Micritic areas with sparite, foraminifera, echinoderm brachiopods, coral fragments, and pore structure in Bh116s1. <bold>(C, D)</bold> Laminated microcrystalline fabric structure with secondary cement and pores. The arrows show the growth direction. <bold>(E&#x2013;G)</bold> Microcrystalline and sparite crystals alternating with fabric microporous calcite. <bold>(H, I)</bold> Sediments and sparite in the margin of the pores (see <xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref> for the locations of the thin sections).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g004.tif"/>
</fig>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>SEM images of calcareous speleothem samples <bold>(A&#x2013;F)</bold> and geochemical composition <bold>(G&#x2013;R)</bold>. <bold>(A&#x2013;C)</bold> Secondary cemented pores. <bold>(D, E)</bold> Calcite crystals are dissolved.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g005.tif"/>
</fig>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>Characteristic spectrum of minerals low-Mg calcite <bold>(A)</bold> and high-Mg calcite <bold>(B)</bold> in Bh116.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g006.tif"/>
</fig>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>Stable carbon and oxygen isotopic composition of subsamples from coastal caves. Data of submerged speleothems, marine overgrowth, and phreatic overgrowth are from coastal caves of Belize, Eastern Adriatic Coast, and Mallorca (<xref ref-type="bibr" rid="B43">Suri&#x107; et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B44">Tuccimei et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B21">Gischler et&#xa0;al., 2017</xref>). The mean values of the calcite from Xisha Islands are adopted from <xref ref-type="bibr" rid="B4">Bi et&#xa0;al. (2018)</xref>.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g007.tif"/>
</fig>
</sec>
<sec id="s3_2">
<title>Petrography</title>
<p>We rinsed the subsamples one by one to remove covered slurries contaminated during the drilling process and put them back to their original positions. Substrates and the largest speleothem subsample (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>) were sliced for petrographic investigation under polarization microscopy. Unfortunately, the largest speleothem subsample of Bh116 was broken and lost after thin section grinding. In order to remove possible contaminants, we rinsed the subsamples by ultrasonic cleaning in deionized water for 12 hours and repeated three times before subsequent geochemical analyses. Generally, no debris was observed after the third rinsing. For the high-resolution surface structure analysis of calcite, samples of freshly broken pieces were studied with Hitachi-SU8010 (Japan) at Guangzhou Institute of Geochemistry, Chinese Academy of Sciences (Guangzhou, China). Calcium, carbon, oxygen, and magnesium concentrations of microporous calcite were determined by SAPPHIRE EDAX detector and Apollo X-SDD detector, respectively.</p>
</sec>
<sec id="s3_3">
<title>Mineralogy and elemental analyses</title>
<p>The carbonate mineralogy was determined by X-ray diffraction measurements. Two subsamples (~2 g) were milled from cleaned carbonates (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>) using a stage-mounted dental drill fitted with silicon carbide dental blade and measured using a Rigaku D/max-rB Theta-theta X-ray powder diffractometer at the First Institute of Oceanology, Ministry of Natural Resources. Copper K<sub>&#x3b1;</sub> radiation (40 kV, 100 mA) was used as an X-ray source. Samples were packed into a rectangle cavity in an aluminum holder and scanned in a step-scan mode (0.02&#xb0;/step) over the angular range of 3&#xb0; to 70&#xb0; (2<italic>&#x3b8;</italic>). The mineralogical compositions of samples were constructed using the 104 reflection of calcite with 2<italic>&#x3b8;</italic> from 29.25&#xb0; to 29.80&#xb0;, the 111 reflection of aragonite with 2<italic>&#x3b8;</italic> between 25.5&#xb0; and 26.5&#xb0;, and the 104 reflection of dolomite with 2<italic>&#x3b8;</italic> from 30.58&#xb0; to 31.28&#xb0;. Usually, the calcite 104 reflection branches into two asymmetric peaks, of which both high-magnesium calcite and low-magnesium calcite co-exist (<xref ref-type="bibr" rid="B27">Kontoyannis and Vagenas, 2000</xref>; <xref ref-type="bibr" rid="B10">Csoma et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B51">Zhai et&#xa0;al., 2015</xref>).</p>
<p>For elemental analyses, four samples (~50 mg) were milled after having been repeatedly rinsed with carbonates using a stage-mounted dental drill fitted with tungsten carbide dental burs (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>). Major elements, including Ca and Mg, were analyzed using an inductively coupled plasma optical emission spectrometer (ICP-OES), and minor elements were performed by inductively coupled plasma mass spectrometry (ICP-MS) at the First Institute of Oceanology, Ministry of Natural Resources. First, 50.00 mg carbonate powder was dissolved in 1.50 ml high-purity HNO<sub>3</sub> and 1.50 ml high-purity HF in a digestion bottle with Teflon liner at 190&#xb0;C for 48 h. Solutions in the Teflon liners were evaporated to dryness on a heating plate. Next, the samples were added with 3 ml of 7 N HNO<sub>3</sub> and 0.5 ml Rh internal standard solution and heated at 150&#xb0;C for 8 h. Finally, the samples were diluted to 50.00 g to be measured by ICP-OES (Icap6300, Thermo Fisher, USA). Exactly 10.00 g solutions were extracted from the 50.00 g solutions and diluted to 20.00 g to analyze by ICP-MS (X Series II, Thermo Fisher, USA). These four carbonate samples were measured together with 34 further carbonate samples from the SYBH. Up to three standard solutions and a laboratory blank were used to calculate the calibration curves for each element.</p>
</sec>
<sec id="s3_4">
<title>Stable carbon and oxygen isotopes</title>
<p>Stable carbon and oxygen isotopes were analyzed to discriminate the origins of deep submerged speleothems between seawater and air-filled conditions. Approximately ~10 mg carbonate powder was collected from 11 positions (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>) and measured on a Thermo Scientific MAT-253 Plus mass spectrometer coupled with an online carbonate preparation device (Kiel-IV) in the Isotope Laboratory of the Xi&#x2019;an Jiaotong University. Carbonates were reacted with anhydrous phosphoric acid at 75&#xb0;C. Results are reported relative to the Vienna Pee Dee Belemnite standard. The analytical errors (1 &#x3c3;) are &#xb1;0.06&#x2030; and &#xb1;0.03&#x2030; for &#x3b4;<sup>18</sup>O and &#x3b4;<sup>13</sup>C (<xref ref-type="bibr" rid="B52">Zhao et&#xa0;al., 2021</xref>), respectively.</p>
</sec>
<sec id="s3_5">
<title>U&#x2013;Th and radiocarbon dating</title>
<p>As relative positions for speleothems could not be accurately determined, we chose three subsamples with substrates to determine the possible onset and termination time of speleothems (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>). Approximately 100 mg of carbonate powder was collected from the speleothems (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3B, C</bold>
</xref>) using a stage-mounted dental drill fitted with tungsten carbide dental bur. The U and Th isotopes of these samples were determined by a plasma-sourced multi-collector mass spectrometer (MC-ICP-MS; Neptune-<italic>plus</italic>, Thermo-Finnigan) at the Isotope Laboratory of the Xi&#x2019;an Jiaotong University. Chemistry procedures to separate U and Th followed <xref ref-type="bibr" rid="B16">Edwards et&#xa0;al. (1987)</xref>. <sup>229</sup>Th&#x2013;<sup>233</sup>U&#x2013;<sup>236</sup>U isotope dilution method was applied to correct for instrumental fractionation and to determine Th/U isotopic ratios and concentrations. U and Th isotopes were measured on a Mas-Com multiplier behind the retarding potential quadrupole in a peak-jumping mode. The instrumentation, standardization, and <sup>230</sup>Th&#x2013;<sup>234</sup>U half-lives were reported in <xref ref-type="bibr" rid="B6">Cheng et&#xa0;al. (2000)</xref>; <xref ref-type="bibr" rid="B7">Cheng et&#xa0;al. (2013)</xref>. Uncertainties in U/Th isotopic data, including corrections for blanks, multiplier dark noise, abundance sensitivity, and contents of the same nuclides in spike solution, were calculated offline at 2&#x3c3; level (<xref ref-type="bibr" rid="B7">Cheng et&#xa0;al., 2013</xref>).</p>
<p>In addition to U&#x2013;Th ages, one radiocarbon dating (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>) was determined by accelerator mass spectrometry at Beta Analytic, Inc. (Miami, USA) to provide additional geochronological identification. This radiocarbon date (<xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>) was subsequently calibrated to the calendar age using the recently published IntCal20 curve (<xref ref-type="bibr" rid="B39">Reimer et&#xa0;al., 2020</xref>).</p>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>U-series and radiocarbon ages of sample Bh116 from Sansha Yongle Blue Hole.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="left">Sample number</th>
<th valign="middle" align="center">
<sup>238</sup>U (ppb)</th>
<th valign="middle" align="center">
<sup>232</sup>Th (ppt)</th>
<th valign="middle" align="center">
<sup>230</sup>Th/<sup>232</sup>Th(&#xd7;10<sup>-6</sup>)</th>
<th valign="middle" align="center">&#x3b4;<sup>234</sup>U (0) (&#x2030;)</th>
<th valign="middle" align="center">(<sup>230Th</sup>/<sup>238</sup>U)</th>
<th valign="middle" align="center">Raw <sup>230</sup>Th age (kyr)</th>
<th valign="middle" align="center">&#x3b4;<sup>234</sup>U (T)<sub>corr</sub> (&#x2030;)</th>
<th valign="middle" align="center">Age<sub>corr</sub> (kyr B.P.)</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">Bh116s2c1-s1</td>
<td valign="middle" align="center">1,731.4 &#xb1; 3.9</td>
<td valign="middle" align="center">499.09 &#xb1; 10.03</td>
<td valign="middle" align="center">54 &#xb1; 1</td>
<td valign="middle" align="center">112.7 &#xb1; 2.3</td>
<td valign="middle" align="center">0.9494 &#xb1; 0.029</td>
<td valign="middle" align="center">195.54 &#xb1; 2.04</td>
<td valign="middle" align="center">192 &#xb1; 5</td>
<td valign="middle" align="center">188.21 &#xb1; 5.49</td>
</tr>
<tr>
<td valign="middle" align="left">Bh116s2c1-s2a</td>
<td valign="middle" align="center">6,570.5 &#xb1; 15.5</td>
<td valign="middle" align="center">0.18 &#xb1; 0.01</td>
<td valign="middle" align="center">15,425 &#xb1; 60,911</td>
<td valign="middle" align="center">108.2 &#xb1; 1.8</td>
<td valign="middle" align="center">0.2616 &#xb1; 0.0012</td>
<td valign="middle" align="center">29.23 &#xb1; 0.17</td>
<td valign="middle" align="center">117 &#xb1; 2</td>
<td valign="middle" align="center">29.16 &#xb1; 0.17</td>
</tr>
<tr>
<td valign="middle" align="left">Bh116s2c2-s1</td>
<td valign="middle" align="center">1,530.7 &#xb1; 1.5</td>
<td valign="middle" align="center">225.87 &#xb1; 4.52</td>
<td valign="middle" align="center">104 &#xb1; 2</td>
<td valign="middle" align="center">110.5 &#xb1; 1.2</td>
<td valign="middle" align="center">0.9319 &#xb1; 0.0015</td>
<td valign="middle" align="center">187.48 &#xb1; 1.00</td>
<td valign="middle" align="center">186 &#xb1; 3</td>
<td valign="middle" align="center">183.74 &#xb1; 2.78</td>
</tr>
<tr>
<td valign="middle" align="left">Bh116s2c2-s2a</td>
<td valign="middle" align="center">675.9 &#xb1; 1.1</td>
<td valign="middle" align="center">4.55 &#xb1; 0.09</td>
<td valign="middle" align="center">555 &#xb1; 11</td>
<td valign="middle" align="center">55.3 &#xb1; 1.7</td>
<td valign="middle" align="center">0.2265 &#xb1; 0.0009</td>
<td valign="middle" align="center">26.30 &#xb1; 0.13</td>
<td valign="middle" align="center">59 &#xb1; 2</td>
<td valign="middle" align="center">26.04 &#xb1; 0.18</td>
</tr>
<tr>
<td valign="middle" align="left">Bh116s2c3<xref ref-type="table-fn" rid="fnT1_1">
<sup>a</sup>
</xref>
</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">15.36 &#xb1; 0.04</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">18.64 &#xb1; 0.12</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>&#x3b4;<sup>234</sup>U = ([<sup>234</sup>U/<sup>238</sup>U]<sub>activity</sub> - 1) &#xd7; 1,000. &#x3b4;<sup>234</sup>U (0) was calculated based on <sup>230</sup>Th age (T), i.e., &#x3b4;<sup>234</sup>U (0) = &#x3b4;<sup>234</sup>U<sub>measured</sub> &#xd7; e<sup>(&#x39b;234)&#xd7;T</sup>. &#x3b4;<sup>234</sup>U (T)<sub>corr</sub> = ([<sup>234</sup>U/<sup>238</sup>U]<sub>activity</sub> &#x2013; 1) &#xd7; 1,000. Corrected <sup>230</sup>Th ages assume the initial <sup>230Th</sup>/<sup>232</sup>Th atomic ratio of 4.4 &#xb1; 2.2 &#xd7; 10<sup>-6</sup>. Those are the values for material at secular equilibrium, with the bulk earth <sup>232</sup>Th/<sup>238</sup>U value of 3.8. The errors are arbitrarily assumed to be 50%.</p>
</fn>
<fn id="fnT1_1">
<label>a</label>
<p>Beta-511711: radiocarbon age.</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
</sec>
<sec id="s4" sec-type="results">
<title>Results</title>
<sec id="s4_1">
<title>Morphology and distribution of speleothems in SYBH</title>
<p>The morphologic features of SYBH, interpreted from 3-D topography data (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2B</bold>
</xref>) and underwater photographs (<xref ref-type="fig" rid="f8">
<bold>Figure&#xa0;8</bold>
</xref>), provide meso-to-micro scale surface evidence to trace the deep submerged speleothems. The 3-D topography reveals a downward ceiling from -90 to -160 m along seaside walls (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>). Irregular and popcorn-like cave coatings extensively cover the ceiling between -90 and -120 m (<xref ref-type="fig" rid="f8">
<bold>Figure&#xa0;8</bold>
</xref>). These coating-like speleothems presented in SYBH are small with centimeter dimensions. They prefer to cluster as a cauliflower-like shapes with downward growth direction from their substrates (<xref ref-type="fig" rid="f8">
<bold>Figures&#xa0;8B, C</bold>
</xref>). Most coatings, if not all, display a gravity-fed downward direction (<xref ref-type="fig" rid="f8">
<bold>Figure&#xa0;8</bold>
</xref>), which probably suggests that these speleothems were formed through slow water dripping in air-filled conditions (<xref ref-type="bibr" rid="B3">Bian et&#xa0;al., 2019</xref>).</p>
<fig id="f8" position="float">
<label>Figure&#xa0;8</label>
<caption>
<p>Underwater photographs of deep submerged speleothems from Sansha Yongle Blue Hole with water depths of ~116 <bold>(A)</bold>, ~100 <bold>(B)</bold>, and ~116 m <bold>(C)</bold>. The red circle in the left panel indicates the location of Bh116. Speleothems cluster as cauliflower-like coatings <bold>(B, C)</bold>.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g008.tif"/>
</fig>
</sec>
<sec id="s4_2">
<title>Petrology and geochemistry</title>
<p>Petrographic investigations show the textures and fabrics of Bh116 including substrates and speleothems (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3</bold>
</xref>, <xref ref-type="fig" rid="f4">
<bold>4</bold>
</xref>). The inside substrates and outside speleothems can be identified by the naked eye depending on their distinct structures (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>). The obtained substrates (Bh116s1) are composed of gray and gray-white broken limestone characterized by loose, yellow, fine sediments. The speleothems (Bh116s2), however, consist of popcorn-like precipitates characterized by column fibers (<xref ref-type="fig" rid="f3">
<bold>Figures&#xa0;3B, C</bold>
</xref>). A thin section of the substrates shows that Bh116s1 consists of lagoonal sand with biologic debris consisting of coral fragments, foraminifers, echinoderms, and brachiopods (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4A, B</bold>
</xref>), reflecting a lagoon slope depositional environment, which corresponds to that found by <xref ref-type="bibr" rid="B19">Fan et&#xa0;al. (2019)</xref>. While the speleothems are characterized by more complex textures (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4C&#x2013;I</bold>
</xref>), they contain two recognizable fabrics: laminated microcrystalline fabric (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4B&#x2013;D</bold>
</xref>) and microcrystalline and sparite crystals alternating with fabric microporous calcite (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4E&#x2013;H</bold>
</xref>). Both of these two structures are highly porous, some of which have been cemented by sparite crystal precipitates (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4C</bold>
</xref>). Moreover, the laminated microcrystalline fabric calcites are surrounded by sparite crystal precipitates with dark terminations (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4C, D</bold>
</xref>) (<xref ref-type="bibr" rid="B10">Csoma et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B5">Bontognali et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B12">De Waele et&#xa0;al., 2018</xref>). In addition, brownish fine sediments and broken marine shells are observed at the margin of pores (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4H</bold>
</xref>). The SEM images show secondary calcite crystals (<xref ref-type="fig" rid="f5">
<bold>Figures&#xa0;5A&#x2013;C</bold>
</xref>), dissolution points, and edges of calcites (<xref ref-type="fig" rid="f5">
<bold>Figures&#xa0;5D&#x2013;F</bold>
</xref>). The secondary calcite crystals show an inner-core growth direction (<xref ref-type="fig" rid="f5">
<bold>Figures&#xa0;5B, C</bold>
</xref>), probably indicating the cements re-precipitated from the surrounding dissolved calcites (<xref ref-type="bibr" rid="B44">Tuccimei et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B5">Bontognali et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B12">De Waele et&#xa0;al., 2018</xref>). The geochemical compositions of surrounding calcites and cements are relatively homogeneous, in which MgCO<sub>3</sub> varied between 5% and 20% (<xref ref-type="fig" rid="f5">
<bold>Figures&#xa0;5G&#x2013;R</bold>
</xref>). The presence of Mg in the deep submerged speleothems is also confirmed by the existence of high-magnesium calcite from bulk sample analysis (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>). Based on XRD, the substrates of Bh116 consist entirely of low-magnesium calcite (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6A</bold>
</xref>), while ~85% low-magnesium calcite and ~15% high-magnesium calcite constitute the speleothems in Bh116 (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6B</bold>
</xref>).</p>
<p>Both carbon and oxygen isotope values of speleothems and substrates are negative in the Bh116 (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref>). The speleothems exhibit isotopically depleted values with respect to the substrates in both <sup>18</sup>O and <sup>13</sup>C. In addition, the oxygen and carbon isotope ratios of the speleothems from different subsamples are variable, and the outer one (Bh116s2c2) is more depleted in <sup>13</sup>C and slightly enriched in <sup>18</sup>O with respect to those of the internal subsample (Bh116s2c1).</p>
</sec>
<sec id="s4_3">
<title>Dating</title>
<p>The <sup>232</sup>Th concentrations of substrates in two subsamples are 499.09 and 225.87 ppt (<xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>). In contrast, the <sup>232</sup>Th concentrations of speleothems are 0.18 and 4.55 ppt, which are much lower than the substrates. The <sup>238</sup>U concentrations of speleothems are variable with concentrations of 6570.5 and 675.9 ppb. The U&#x2013;Th ages of substrates are 188.21 &#xb1; 5.49 and 183.74 &#xb1; 2.78 ka BP, suggesting that they may have experienced deposition and secondary alterations and are not suitable for U&#x2013;Th dating. The substrates are expected to have been deposited at about 1.4 Ma based on the depth of nearby borehole CK-2 (<xref ref-type="bibr" rid="B19">Fan et&#xa0;al., 2019</xref>). The U&#x2013;Th ages of the speleothems, Bh116s2c1 and Bh116s2c2, are 29.16 &#xb1; 0.17 and 26.04 &#xb1; 0.18 ka BP, respectively (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref> and <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>). The radiocarbon age of a subsample of speleothems (Bh116s2c3) is 18.64 &#xb1; 0.12 ka BP.</p>
</sec>
</sec>
<sec id="s5" sec-type="discussion">
<title>Discussion</title>
<sec id="s5_1">
<title>Aerial growth of speleothems</title>
<p>It is evident that deep submerged calcite coatings in SYBH are speleothems that precipitated under air-filled conditions during sea level lowstands. Substances of marine origin, including marine overgrowth on speleothems and marine substrates, are excluded for their negative carbon and oxygen isotopes with values as low as -6.7&#x2030; to -5.3&#x2030; and -5.0&#x2030; to -2.8&#x2030; (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref>), respectively. These isotopic features differ from the marine overgrowth on speleothem, marine corals, and substrates but are close to subaerial speleothems collected from other coastal caves (<xref ref-type="bibr" rid="B43">Suri&#x107; et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B44">Tuccimei et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B21">Gischler et&#xa0;al., 2017</xref>). This suggests that the deep submerged calcite coatings developed in SYBH grew under aerial conditions and can be used to determine maximum sea levels (<xref ref-type="bibr" rid="B40">Richards et&#xa0;al., 1994</xref>). The calcareous coatings resemble mushroom-shaped speleothems and phreatic overgrowths on speleothems and are porous (<xref ref-type="bibr" rid="B44">Tuccimei et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B5">Bontognali et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B12">De Waele et&#xa0;al., 2018</xref>), probably suggesting that they exhibit the same aerial origin.</p>
</sec>
<sec id="s5_2">
<title>Determination of LGM low sea levels</title>
<p>As our deep submerged speleothems initially grew at ~29 ka under the air-filled vadose environment through calcite precipitation in coastal karst cave (<xref ref-type="bibr" rid="B18">Fairchild et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B44">Tuccimei et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B12">De Waele et&#xa0;al., 2018</xref>), the maximum sea level at ~29 ka BP should be lower than -116 m relative to the present. Our results agree well with previous data (<xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9A</bold>
</xref>) from Barbados (<xref ref-type="bibr" rid="B2">Bard et&#xa0;al., 1990</xref>; <xref ref-type="bibr" rid="B38">Peltier and Fairbanks, 2006</xref>) and Bonaparte (<xref ref-type="bibr" rid="B49">Yokoyama et&#xa0;al., 2000</xref>), as well as the reconstructed global ice volume equivalent (<xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9B</bold>
</xref>) and mean sea levels (<xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9C</bold>
</xref>) (<xref ref-type="bibr" rid="B29">Lambeck et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al., 2018</xref>). <xref ref-type="bibr" rid="B29">Lambeck et&#xa0;al. (2014)</xref> documented a ~40-m sea level falling around ~31&#x2013;29 ka BP according to compiled data. Our results confirm that this rapid fall in sea level reached as low as -116 m at ~29 ka BP, and LGM was initiated at ~29 ka BP. It is noted that the sea level data from Bonaparte, indicating the onset of LGM (<xref ref-type="bibr" rid="B49">Yokoyama et&#xa0;al., 2000</xref>), have large uncertainties of up to 7.8 m. Our data also refined large sea level errors.</p>
<fig id="f9" position="float">
<label>Figure&#xa0;9</label>
<caption>
<p>Last Glacial Maximum (LGM) sea levels with observational data and ice volume equivalent and global mean sea levels. <bold>(A)</bold> Previously documented LGM sea level data from Bonaparte Gulf (<xref ref-type="bibr" rid="B49">Yokoyama et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B11">De Deckker and Yokoyama, 2009</xref>), Huon Peninsula (<xref ref-type="bibr" rid="B47">Yokoyama et&#xa0;al., 2001</xref>), Sunda Shelf (<xref ref-type="bibr" rid="B23">Hanebuth et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B22">Hanebuth et&#xa0;al., 2009</xref>), Bengal Fan (<xref ref-type="bibr" rid="B46">Wiedicke et&#xa0;al., 1999</xref>), Barbados (<xref ref-type="bibr" rid="B2">Bard et&#xa0;al., 1990</xref>; <xref ref-type="bibr" rid="B38">Peltier and Fairbanks, 2006</xref>), and Great Barrier Reef (<xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al., 2018</xref>). <bold>(B, C)</bold> Previously constructed ice volume equivalent (<xref ref-type="bibr" rid="B29">Lambeck et&#xa0;al., 2014</xref>) and global mean sea levels (<xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al., 2018</xref>).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-09-1079301-g009.tif"/>
</fig>
<p>The LGM was thought to have been terminated by a rise in sea level (<xref ref-type="bibr" rid="B23">Hanebuth et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B49">Yokoyama et&#xa0;al., 2000</xref>). It began at ~19 ka BP, and the sea level rose 10&#x2013;15 m within 500 years based on the interpretation of mangrove muds from the Sunda Shelf and Bonaparte Gulf in which tectonics are stable (<xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9A</bold>
</xref>). Recently, however, both <xref ref-type="bibr" rid="B29">Lambeck et&#xa0;al. (2014)</xref> and <xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al. (2018)</xref> demonstrated that this 10&#x2013;15-m sea level rise was slower and lasted for ~3,000 years from 21 to 18 ka BP (<xref ref-type="fig" rid="f9">
<bold>Figures&#xa0;9B, C</bold>
</xref>). The possible termination of the speleothems from the SYBH with a radiocarbon age of 18.64 &#xb1; 0.12 ka BP suggests that the sea level was lower than -116 m at ~18.5 ka BP. Our results agree well with those sea levels reconstructed from Sunda Shelf and Bonaparte Gulf within errors and suggest that the termination of LGM is slightly later than the previous estimation (<xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9A</bold>
</xref>). However, our obtained results are inconsistent with the data reported from Barbados and the Great Barrier Reef, which experienced a rapid tectonic uplift of up to 0.34 mm/year (<xref ref-type="bibr" rid="B17">Fairbanks, 1989</xref>). The divergence in the conclusions regarding the termination of the LGM based on by sea level data from the SYBH, Bonaparte Gulf (<xref ref-type="bibr" rid="B49">Yokoyama et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B11">De Deckker and Yokoyama, 2009</xref>), and Sunda Shelf (<xref ref-type="bibr" rid="B23">Hanebuth et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B22">Hanebuth et&#xa0;al., 2009</xref>), as well as those determined from Barbados (<xref ref-type="bibr" rid="B2">Bard et&#xa0;al., 1990</xref>; <xref ref-type="bibr" rid="B38">Peltier and Fairbanks, 2006</xref>) and the Great Barrier Reef (<xref ref-type="bibr" rid="B48">Yokoyama et&#xa0;al., 2018</xref>), could be due to diverse and aged carbon, local carbon reservoir effects, and contaminated cement (<xref ref-type="bibr" rid="B36">Nakada et&#xa0;al., 2016</xref>), as they were determined from different materials (<xref ref-type="bibr" rid="B23">Hanebuth et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B49">Yokoyama et&#xa0;al., 2000</xref>). In addition, we confirm that the presence of old carbon was not significant in our samples and would not affect our results. Conversely, subsequent cement observed in thin sections from our obtained submerged speleothems may cause the measured radiocarbon age to be less than its actual value. In addition, our results coincide with the constructed ice volume equivalent and global mean sea level, suggesting that the deep submerged speleothems may be a promising way to determine Pleistocene low sea levels.</p>
</sec>
</sec>
<sec id="s6" sec-type="conclusions">
<title>Conclusions</title>
<p>This study used U&#x2013;Th and radiocarbon ages of deep submerged speleothems (-116 m) from SYBH to determine low LGM sea levels. Our results show that the deep speleothems grew at 29.16 &#xb1; 0.17 ka BP and were submerged at &lt;18.64 &#xb1; 0.12 ka BP under air-filled conditions above sea level. The initial age of the speleothems indicates onset of the LGM at ~29 ka BP, and the obtained radiocarbon age indicates the termination of LGM at ~18.5 ka BP. As elevations and ages can be accurately identified, deep submerged speleothems may be a promising way to determine Pleistocene low sea levels.</p>
</sec>
<sec id="s7" sec-type="data-availability">
<title>Data availability statement</title>
<p>The datasets presented in this study can be found in online repositories. The names of the repository/repositories and accession number(s) can be found below: <uri xlink:href="https://doi.org/10.6084/m9.figshare.13379504.v1">https://doi.org/10.6084/m9.figshare.13379504.v1</uri>.</p>
</sec>
<sec id="s8" sec-type="author-contributions">
<title>Author contributions</title>
<p>TL conceived this study. TL, AF, YL, and DG designed this study. XY, BD, and JZ carried out the laboratory measurements. XY wrote the original manuscript. TL, BD, and JZ reviewed and edited the manuscript. All authors contributed to the article and approved the submitted version.</p>
</sec>
</body>
<back>
<sec id="s9" sec-type="funding-information">
<title>Funding</title>
<p>This study was funded jointly by the National Natural Science Foundation of China (grant nos. T2192951 and U1906211) and the Taishan Scholars Project Funding (grant no. ts20190963). </p>
</sec>
<ack>
<title>Acknowledgments</title>
<p>We would like to thank Prof. David Richards from the University of Bristol for his constructive comments to improve this manuscript.</p>
</ack>
<sec id="s10" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s11" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
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