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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.2025.1529163</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>Hypoxia lowers cell carbon and nitrogen content and accelerates sinking of a marine diatom <italic>Thalassiosira pseudonana</italic>
</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Chen</surname>
<given-names>Bokun</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2894479"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Song</surname>
<given-names>Hui</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<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/2569336"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Xu</surname>
<given-names>Ge</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Ji</surname>
<given-names>Hongli</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Yang</surname>
<given-names>Xue</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Li</surname>
<given-names>Gang</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/496848"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Institute of Marine Science and Technology, Shandong University</institution>, <addr-line>Qingdao</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Qingdao Key Laboratory of Ocean Carbon Sequestration and Negative Emission Technology, Shandong University</institution>, <addr-line>Qingdao</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Marine Environmental Monitoring Centre of Ningbo, East China Sea Bureau of Ministry of Natural Resources</institution>, <addr-line>Ningbo</addr-line>, <country>China</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Daya Bay Marine Biology Research Station, South China Sea Institute of Oceanology, Chinese Academy of Sciences</institution>, <addr-line>Guangzhou</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Fuminori Hashihama, Tokyo University of Marine Science and Technology, Japan</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Zhangxi Hu, Guangdong Ocean University, China</p>
<p>Yaping Wu, Hohai University, China</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Hui Song, <email xlink:href="mailto:songhui2018@foxmail.com">songhui2018@foxmail.com</email>; Gang Li, <email xlink:href="mailto:ligang@scsio.ac.cn">ligang@scsio.ac.cn</email>
</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>06</day>
<month>02</month>
<year>2025</year>
</pub-date>
<pub-date pub-type="collection">
<year>2025</year>
</pub-date>
<volume>12</volume>
<elocation-id>1529163</elocation-id>
<history>
<date date-type="received">
<day>19</day>
<month>11</month>
<year>2024</year>
</date>
<date date-type="accepted">
<day>15</day>
<month>01</month>
<year>2025</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2025 Chen, Song, Xu, Ji, Yang and Li</copyright-statement>
<copyright-year>2025</copyright-year>
<copyright-holder>Chen, Song, Xu, Ji, Yang 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>The positive or negative effect of a decrease in dissolved O<sub>2</sub> on the photophysiology of phytoplankton is determined by the duration of light exposure. To uncover the underlying mechanisms, the marine model diatom <italic>Thalassiosira pseudonana</italic> was cultured under three dissolved O<sub>2</sub> levels (8.0 mg L<sup>-1</sup>, ambient O<sub>2</sub>; 4.0 mg L<sup>-1</sup>, low O<sub>2</sub>; and 1.3 mg L<sup>-1</sup>, hypoxia) to compare its growth, cell composition, and physiology between the light and dark periods. The results showed that the growth rate under ambient O<sub>2</sub> was 0.60 &#xb1; 0.02 day<sup>-1</sup>, which was half of the growth rate during light period and 15-fold of the growth rate during dark period. Decreasing O<sub>2</sub> increased the growth rate during light period but decreased it during dark period and decreased the cell pigment content in both the light and dark periods. In the light, low O<sub>2</sub> increased cell carbon (C) content, while hypoxia decreased it, with the degree of increase and decrease being greater in the dark. Low O<sub>2</sub> had no significant effect on cell nitrogen (N) content, but hypoxia decreased it. Low O<sub>2</sub> had no significant effect on photosynthetic efficiency but decreased the dark respiration rate. In darkness, low O<sub>2</sub> had no significant effect on cell C loss rate but decreased N loss rate, leading to an increase in the POC/PON ratio. In addition, hypoxia exacerbated cell mortality and sinking, suggesting that diatom-derived carbon burial may be accelerated due to marine deoxygenation in the future.</p>
</abstract>
<kwd-group>
<kwd>lowering O<sub>2</sub>
</kwd>
<kwd>light and dark</kwd>
<kwd>diatom</kwd>
<kwd>cell composition</kwd>
<kwd>sinking rate</kwd>
</kwd-group>
<contract-sponsor id="cn001">Shandong University<named-content content-type="fundref-id">10.13039/100009108</named-content>
</contract-sponsor>
<counts>
<fig-count count="6"/>
<table-count count="1"/>
<equation-count count="10"/>
<ref-count count="41"/>
<page-count count="10"/>
<word-count count="4835"/>
</counts>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-in-acceptance</meta-name>
<meta-value>Marine Biogeochemistry</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>Deoxygenation in global marine ecosystems is increasing in scope and severity due to anthropogenic activities and climate change (<xref ref-type="bibr" rid="B19">Keeling et&#xa0;al., 2010</xref>). According to <xref ref-type="bibr" rid="B4">Breitburg et&#xa0;al. (2018)</xref>, the total dissolved O<sub>2</sub> (DO) content in the ocean has decreased by 2% in recent decades (<xref ref-type="bibr" rid="B4">Breitburg et&#xa0;al., 2018</xref>) and will decrease by a further 1% to 7% by the end of this century (<xref ref-type="bibr" rid="B24">Long et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B32">Schmidtko et&#xa0;al., 2017</xref>), leading to a sharp increase in the frequency and severity of marine hypoxia (dissolved O<sub>2</sub> &lt;2.0 mg L<sup>&#x2212;1</sup>) (<xref ref-type="bibr" rid="B32">Schmidtko et al., 2017</xref>; <xref ref-type="bibr" rid="B29">Rabalais and Turner, 2019</xref>; <xref ref-type="bibr" rid="B37">Wang et al., 2023</xref>). Hypoxia affects most marine aerobic organisms through inhibiting visual function, reproduction, and population development (<italic>e.g</italic>., <xref ref-type="bibr" rid="B25">McCormick and Levin, 2017</xref>; <xref ref-type="bibr" rid="B36">Wang et&#xa0;al., 2016</xref>) and the photoautotrophic macroalgae through photosystem (<italic>e.g</italic>., <xref ref-type="bibr" rid="B26">Peckol and Rivers, 1995</xref>; <xref ref-type="bibr" rid="B1">Alamoudi et&#xa0;al., 2022</xref>) and seagrasses through chlorophyll (<italic>e.g</italic>., <xref ref-type="bibr" rid="B5">Che et&#xa0;al., 2022</xref>). Recently, many field studies have shown that marine phytoplankton that dwell in hypoxic zones are also experiencing the low O<sub>2</sub> level occasionally (<xref ref-type="bibr" rid="B21">Li et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B33">Sun et&#xa0;al., 2022</xref>) or permanently (<xref ref-type="bibr" rid="B17">Gomes et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B39">Xiang et&#xa0;al., 2019</xref>); therefore, many laboratory experiments have been conducted to explore how hypoxia affects phytoplankton (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B41">Zhao et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B12">Eom et&#xa0;al., 2024</xref>; <xref ref-type="bibr" rid="B7">Chen et&#xa0;al., 2024</xref>; <xref ref-type="bibr" rid="B34">Tong et&#xa0;al., 2024</xref>). One of the reasons for this widespread interest is that phytoplankton, apart from their important role as the main primary producer in the ocean, require exogenous O<sub>2</sub> to maintain respiratory metabolism at night (<xref ref-type="bibr" rid="B22">Li et al., 2016</xref>), although this challenge can be met by photosynthesis during the day.</p>
<p>Although marine phytoplankton contribute to about half of the global photosynthetic O<sub>2</sub> (<xref ref-type="bibr" rid="B13">Field et&#xa0;al., 1998</xref>), the death of extensively bloomed phytoplankton often accelerates the formation of hypoxic environments in the water column through O<sub>2</sub> depletion by increasing respiration themselves and the nitrification of microbes supported by organic matter released by the phytoplankton cells (<xref ref-type="bibr" rid="B6">Chen et&#xa0;al., 2007</xref>). In this scenario, phytoplankton are also affected by the lowered O<sub>2</sub> level when they fall into the O<sub>2</sub>-deficient layer due to their own sinking or vertical mixing of the water column, especially in the shallower coastal or estuarine regions (<xref ref-type="bibr" rid="B21">Li et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B40">Zhai et&#xa0;al., 2021</xref>). Theoretically, lowering O<sub>2</sub> level benefits photoautotrophic organisms as it increases the likelihood of CO<sub>2</sub> molecules binding to ribulose-1, 5-bisphosphate carboxylase/oxygenase (RubisCO) (<xref ref-type="bibr" rid="B14">Gao and Campbell, 2014</xref>). It is therefore generally believed that lowering O<sub>2</sub> can promote the photosynthetic production of phytoplankton cells (<xref ref-type="bibr" rid="B28">Pruder and Bolton, 1980</xref>; <xref ref-type="bibr" rid="B30">Raven and Larkum, 2007</xref>) and decrease the consumption of the photosynthates by mitochondrial respiration (<xref ref-type="bibr" rid="B31">Reinfelder et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B16">Giordano et&#xa0;al., 2005</xref>), allowing them to store more products for growth (<xref ref-type="bibr" rid="B33">Sun et&#xa0;al., 2022</xref>). On the other hand, lowering O<sub>2</sub> levels is known to decrease the production of harmful reactive oxygen species (ROS) which often inactivate many cellular enzymes and thus block the cell growth (<xref ref-type="bibr" rid="B27">P&#xe9;rez-P&#xe9;rez et&#xa0;al., 2012</xref>). However, many studies demonstrated the negative effects of lowered O<sub>2</sub> on phytoplankton, such as decreasing the cell size and cell growth of diatoms (<xref ref-type="bibr" rid="B38">Wu et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B41">Zhao et&#xa0;al., 2022</xref>), decreasing the cell carbon content of coccolithophores (<xref ref-type="bibr" rid="B34">Tong et&#xa0;al., 2024</xref>) and increasing the cell mortality of dinoflagellates (<xref ref-type="bibr" rid="B12">Eom et&#xa0;al., 2024</xref>). An inhibitory effect of lowering O<sub>2</sub> was also observed on cellular nitrogen metabolism (<xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>) and calcification (<xref ref-type="bibr" rid="B34">Tong et&#xa0;al., 2024</xref>). These results indeed illustrate the effects of lowering O<sub>2</sub> on phytoplankton physiology but are highly contradictory.</p>
<p>Phytoplankton, like heterotrophic organisms, require exogenous O<sub>2</sub> to sustain their respiration at night. Therefore, the duration of light exposure together with light intensity has been found to influence the responses of phytoplankton to a decrease in O<sub>2</sub>, such as the increase in growth of the diatom <italic>Thalassiosira pseudonana</italic> at short photoperiod or low light intensity, while the growth decreases inversely at long photoperiod or high light intensity (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>, <xref ref-type="bibr" rid="B9">2023</xref>, <xref ref-type="bibr" rid="B7">2024</xref>). These studies mainly focused on the effects of lowered O<sub>2</sub> in the light state and neglected the effects in the dark that phytoplankton often experience in nature, including the rhythmic dark state due to the Earth&#x2019;s rotation or the long-term darkness when sinking out of the euphotic layer. To address this gap, we cultured a representative diatom, <italic>Thalassiosira pseudonana</italic>, under three O<sub>2</sub> levels (8.0, 4.0, and 1.3 mg L<sup>-1</sup>) and comparatively studied its physiochemical differences between the light and dark periods, with emphasis to the changes in biochemical composition and sinking rate of cells during a long-term darkness (84 h). We selected this diatom as a target species because it is one of the dominant groups in hypoxic zones (<xref ref-type="bibr" rid="B17">Gomes et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B39">Xiang et&#xa0;al., 2019</xref>; <xref ref-type="bibr" rid="B33">Sun et&#xa0;al., 2022</xref>), and it can also serve as food to enhance the survival of heterotrophs in hypoxic environments (<xref ref-type="bibr" rid="B12">Eom et&#xa0;al., 2024</xref>). On the other hand, the diatoms have siliceous shells that allow them to settle more easily into the deep layer in nature and encounter low O<sub>2</sub> (<xref ref-type="bibr" rid="B2">Bannon and Campbell, 2017</xref>).</p>
</sec>
<sec id="s2" sec-type="materials|methods">
<label>2</label>
<title>Materials and methods</title>
<sec id="s2_1">
<label>2.1</label>
<title>Culture protocol</title>
<p>In this study, the centric diatom <italic>Thalassiosira pseudonana</italic> (CCMP 1335), originally from the Provasoli-Guillard National Center of Marine Phytoplankton (NCMP), was cultured semi-continuously with 400 mL of sterilized enriched artificial seawater (EASW, NO<sub>3</sub>
<sup>-</sup> 550 &#x3bc;M and PO<sub>4</sub>
<sup>3-</sup> 23 &#x3bc;M) (<xref ref-type="bibr" rid="B3">Berges et&#xa0;al., 2001</xref>) in a 500-mL conical flask at 18&#xb0;C in a plant growth chamber (Zhichu, Shanghai, China). The growth light in the chamber was set to 150 &#x3bc;mol photons m<sup>-2</sup> s<sup>-1</sup> with a 12:12 light/dark cycle. This light intensity is approximately the optimal growth light for <italic>T. pseudonana</italic> (<xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>, <xref ref-type="bibr" rid="B7">2024</xref>; <xref ref-type="bibr" rid="B21">Li et&#xa0;al., 2018</xref>) and was measured using a microspherical quantum sensor (Hansatech, Norfolk, UK) in a culture flask filled with medium. During cultivation, commercially produced air (Qingdao Jinpeng Gas, Qingdao, China) was gently bubbled in the cultures with three O<sub>2</sub> concentrations to maintain dissolved O<sub>2</sub> (DO) at 8.0 &#xb1; 0.65 (ambient O<sub>2</sub>), 4.0 &#xb1; 0.31 (low O<sub>2</sub>), and 1.3 &#xb1; 0.21 mg L<sup>&#x2212;1</sup> (hypoxia), respectively (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>, <xref ref-type="bibr" rid="B9">2023</xref>, <xref ref-type="bibr" rid="B7">2024</xref>). These DO concentrations cover a range of O<sub>2</sub> concentrations in natural hypoxia zones (<xref ref-type="bibr" rid="B21">Li et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B39">Xiang et&#xa0;al., 2019</xref>) and were measured using an optode sensor controlled by the Oxygen Logger software (PyroScience, Aachen, Germany). For each treatment, three replicates were used. Considering the shock effects of the changes in temperature and DO on cell&#x2019;s physiology during medium replacement, the initial medium was kept in the chamber and pre-bubbled with an air stream filtered through a 0.2-&#xb5;m micro-filter before bubbling into the cultures.</p>
<p>To determine the different responses of <italic>T. pseudonana</italic> to lowered O<sub>2</sub> levels during day and night, aliquots of the cultures were taken at the end of cultivation at the beginning (8:00 a.m.) and at the end of illumination (20:00 p.m.) to determine cell composition and physiological parameters as described below.</p>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Growth rate</title>
<p>During cultivation, 3.0 mL of culture was taken from each flask every morning (8:00 a.m.) before and after replacing with fresh medium and taken again at the end of illumination (20:00 p.m.). The optical density of each sample was measured at 680 nm (OD<sub>680</sub>) using a molecular device (BioTec, Dorset, UK). The growth rate of total (8:00 a.m. to next 8:00 a.m.) and during the light (8:00 a.m. to 20:00 p.m.) and dark periods (20:00 p.m. to next 08:00 a.m.) was calculated as follows:</p>
<disp-formula>
<mml:math display="block" id="M1">
<mml:mrow>
<mml:mtext>Growth&#xa0;rate</mml:mtext>
<mml:mo>=</mml:mo>
<mml:mo stretchy="false">[</mml:mo>
<mml:mtext>ln</mml:mtext>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>N</mml:mtext>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>&#x2013;</mml:mo>
<mml:mtext>ln</mml:mtext>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>N</mml:mtext>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo stretchy="false">]</mml:mo>
<mml:mo stretchy="false">/</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>T</mml:mtext>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>T</mml:mtext>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>N</italic>
<sub>1</sub> and <italic>N</italic>
<sub>0</sub> represent the OD<sub>680</sub> at time <italic>T</italic>
<sub>1</sub> and <italic>T</italic>
<sub>0</sub>, respectively.</p>
<p>During cultivation, chlorophyll a concentration (Chl <italic>a</italic>) in the cultures was maintained at 0.40&#x2013;0.95 &#x3bc;g mL<sup>-1</sup>. After nine generations of cultivation, aliquots of the cultures were taken to measure the physio-chemical parameters of <italic>T. pseudonana</italic> and then harvested for measurement of cell composition and physiological parameters as described below.</p>
</sec>
<sec id="s2_3">
<label>2.3</label>
<title>Cell compositions</title>
<p>To measure the cell number, duplicate 5-mL cultures were taken from each flask after gentle shaking and fixed with glutaraldehyde to a final concentration of 1%. The cell number was then counted using a flow cytometer (Becton-Dickinson, Franklin Lakes, USA).</p>
<p>To measure the cell pigments, 30 mL of culture was vacuum-filtered onto a Whatman GF/F glass fiber filter (25 mm in diameter) and extracted with 4 mL of 90% acetone (v/v) saturated with magnesium carbonate overnight at 4&#xb0;C in the dark. After centrifugation for 10 min (10,000 <italic>g</italic>), the optical absorbance of the supernatant was measured spectrophotometrically at 470, 630, 645, 664, and 750 nm. The concentration of Chl <italic>a</italic> and carotenoids (Car) (&#x3bc;g mL<sup>&#x2212;1</sup>) was calculated as follows:</p>
<disp-formula>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:mtext>Chl&#x2004;</mml:mtext>
<mml:mi>a</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>11.47</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>664</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>750</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>0.4</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>630</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>750</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula>
<mml:math display="block" id="M3">
<mml:mrow>
<mml:mtable>
<mml:mtr>
<mml:mtd>
<mml:mtext>Car</mml:mtext>
<mml:mo>=</mml:mo>
<mml:mn>2.11</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>630</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>750</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>10.01</mml:mn>
<mml:mo>&#xd7;</mml:mo>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>645</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>750</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>+</mml:mo>
<mml:mn>4.37</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>470</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>A</mml:mtext>
<mml:mrow>
<mml:mn>750</mml:mn>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:math>
</disp-formula>
<p>To measure the content of particle organic carbon (POC) and nitrogen (PON), 30 mL of cultures was filtered onto a pre-combusted (450&#xb0;C, 5 h) Whatman GF/F filter. The filters containing the cells were exposed to HCl fumes for 3 h, freeze-dried for 24 h, and stored in a desiccator for later analysis. The N and C content was measured using an elemental analyzer (NC Technologies, Marseille, France) with a detection limit for C of 0.002 mg (<italic>R</italic>
<sup>2</sup> &gt; 0.99) and for N of 0.005 mg (<italic>R</italic>
<sup>2</sup> &gt; 0.99), respectively. In addition, triplicate 50 mL medium was filtrated on the pre-combusted GF/F filters, dried, and measured as a blank, which was subtracted for the POC and PON calculation.</p>
</sec>
<sec id="s2_4">
<label>2.4</label>
<title>Photosynthetic parameters</title>
<p>To measure chlorophyll fluorescence, 5 mL of culture was taken from each flask and dark-acclimated for 15 min at growth temperature in the cuvette of a portable fluorometer (AquaPen-C, Photon Systems Instruments, Czech Republic), followed by measurement of maximum (<italic>F</italic>
<sub>M</sub>) and minimum fluorescence (<italic>F</italic>
<sub>O</sub>) with a saturating light pulse (3,000 &#x3bc;mol photons m<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup>, 1 s). The maximum photochemical quantum yield (<italic>F</italic>
<sub>V</sub>/<italic>F</italic>
<sub>M</sub>) of Photosystem II (PSII) was calculated as follows:</p>
<disp-formula>
<mml:math display="block" id="M4">
<mml:mrow>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>V</mml:mtext>
</mml:msub>
<mml:mo stretchy="false">/</mml:mo>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>M</mml:mtext>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>M</mml:mtext>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>O</mml:mtext>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo stretchy="false">/</mml:mo>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>M</mml:mtext>
</mml:msub>
</mml:mrow>
</mml:math>
</disp-formula>
<p>Meanwhile, the relative electron transport rate (rETR) in actinic light of 0, 10, 20, 50, 100, 300, and 500 &#x3bc;mol photon m<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup> was determined to obtain the rapid light curve (RLC) as follows:</p>
<disp-formula>
<mml:math display="block" id="M5">
<mml:mrow>
<mml:mtext>rETR</mml:mtext>
<mml:mo>=</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>M</mml:mtext>
</mml:msub>
<mml:mo>'</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mtext>Ft</mml:mtext>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo stretchy="false">/</mml:mo>
<mml:msub>
<mml:mtext>F</mml:mtext>
<mml:mtext>M</mml:mtext>
</mml:msub>
<mml:mo>'</mml:mo>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>0.5</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mtext>PAR</mml:mtext>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>F</italic>
<sub>M&#x2032;</sub> and Ft are maximum and instantaneous fluorescence under each of the seven actinic lights. The photosynthetic parameters derived from the RLC, i.e., light utilization efficiency (&#x3b1;), maximum rETR (rETR<sub>max</sub>), and saturation irradiance (E<sub>K</sub>, &#x3bc;mol photons m<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup>), were calculated as follows:</p>
<disp-formula>
<mml:math display="block" id="M6">
<mml:mrow>
<mml:mtext>rETR</mml:mtext>
<mml:mo>=</mml:mo>
<mml:mtext>PAR</mml:mtext>
<mml:mo stretchy="false">/</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:mtext>a</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mtext>PAR</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:mtext>b</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:mtext>PAR</mml:mtext>
<mml:mo>+</mml:mo>
<mml:mtext>c</mml:mtext>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula>
<mml:math display="block" id="M7">
<mml:mrow>
<mml:mtable>
<mml:mtr>
<mml:mtd>
<mml:mi>&#x3b1;</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo stretchy="false">/</mml:mo>
<mml:mtext>c</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mtext>&#x2004;</mml:mtext>
<mml:msub>
<mml:mrow>
<mml:mtext>rETR</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>max</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo stretchy="false">/</mml:mo>
<mml:mo stretchy="false">[</mml:mo>
<mml:mtext>b</mml:mtext>
<mml:mo>+</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mtext>a</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:mtext>c</mml:mtext>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo stretchy="false">/</mml:mo>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mo stretchy="false">]</mml:mo>
<mml:mo>,</mml:mo>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mtext>&#x2004;</mml:mtext>
<mml:msub>
<mml:mtext>E</mml:mtext>
<mml:mtext>K</mml:mtext>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mtext>c</mml:mtext>
<mml:mo stretchy="false">/</mml:mo>
<mml:mo stretchy="false">[</mml:mo>
<mml:mtext>b</mml:mtext>
<mml:mo>+</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mtext>a</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:mtext>c</mml:mtext>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo stretchy="false">/</mml:mo>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mo stretchy="false">]</mml:mo>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where a, b, and c are adjusted parameters.</p>
<p>To measure the rate of photosynthetic O<sub>2</sub> evolution, 5 mL of culture was taken from each flask and dark-acclimated for 5 min at 18&#xb0;C, followed by measurement of changes in O<sub>2</sub> concentration in growth light and in the dark using a liquid oxygen electrode (Chlorolab 2, Hansatech Instrument Ltd., UK). The cell-based photosynthetic O<sub>2</sub> rate (P<sub>n</sub>, fmol O<sub>2</sub> cell<sup>&#x2212;1</sup> min<sup>&#x2212;1</sup>) and respiration rate (R<sub>d</sub>, fmol O<sub>2</sub> cell<sup>&#x2212;1</sup> min<sup>&#x2212;1</sup>) was calculated by normalizing the O<sub>2</sub> increase/decrease rate to cell concentration.</p>
</sec>
<sec id="s2_5">
<label>2.5</label>
<title>Sinking rate</title>
<p>To investigate how <italic>T. pseudonana</italic> responds to lowered O<sub>2</sub> in the dark, we supplemented the remaining cultures with fresh media to 400 mL at the end of 12:12 L/D cultivation and continued cultivating. During the cultivation, samples were taken after 0, 12, 24, 36, 48, 60, 72, and 84 h to measure the cell number and C/N content, and the sinking rate (5 mL) was determined at 0, 48, and 84 h.</p>
<p>The rate of sinking was determined using an innovative method described in detail in <xref ref-type="bibr" rid="B2">Bannon and Campbell (2017)</xref> based on changes in Chl <italic>a</italic> fluorescence monitored using a molecular device (Cytation5, BioTek, USA). In brief, the collected sample was placed in a 12-well plate (3 mL per well with a depth of 10 mm), which was placed in the molecular device. Fluorescence (excitation: 445 nm, emission: 680 nm) was measured with the photodiode detector from the top of each well every 0.5 h for a total duration of 4 h. As the cells sank, the fluorescence signal decreased from the initial maximum value to the final minimum value according to the inverse square law and did not change after the cells reached the bottom of the well. Thus, we can collect the relative fluorescence (RFU) of nine detected time-point (RFU<sub>t</sub>) and scale them as follows:</p>
<disp-formula>
<mml:math display="block" id="M8">
<mml:mrow>
<mml:mtext>RFU</mml:mtext>
<mml:mo>'</mml:mo>
<mml:mo>=</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mtext>RFU</mml:mtext>
</mml:mrow>
<mml:mtext>t</mml:mtext>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mtext>RFU</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>min</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo stretchy="false">/</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mtext>RFU</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>max</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mtext>RFU</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>min</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where RFU&#x2032; is the scaled RFU<sub>t</sub>. Due to the shielding effect between the cells, the RFU&#x2032; mainly refers to the uppermost cells, which sink to the bottom of the well according to the inverse square law:</p>
<disp-formula>
<mml:math display="block" id="M9">
<mml:mrow>
<mml:mtext>RFU</mml:mtext>
<mml:mo>'</mml:mo>
<mml:mo>=</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>+</mml:mo>
<mml:mtext>t</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:mtext>s</mml:mtext>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>t</italic> is the elapsed time of cell sinking and <italic>s</italic> is the scaled sinking rate. We can further simplify the formulation by geometric series as follows:</p>
<disp-formula>
<mml:math display="block" id="M10">
<mml:mrow>
<mml:mtext>sqrt&#xa0;</mml:mtext>
<mml:mo stretchy="false">(</mml:mo>
<mml:mtext>RFU</mml:mtext>
<mml:mo>'</mml:mo>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mtext>t</mml:mtext>
<mml:mo>&#xd7;</mml:mo>
<mml:mtext>s</mml:mtext>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where sqrt is the square root. The resulting linear formulation can finally be coupled with the well depth (10 mm) and the measurement time (4 h) to determine the actual sinking velocity (cm day<sup>-1</sup>).</p>
</sec>
<sec id="s2_6">
<label>2.6</label>
<title>Statistical analysis</title>
<p>Data were presented as mean and standard deviations (mean &#xb1; SD) in the figures. Paired <italic>t</italic>-test, one-way analyses of variance (ANOVA) with Tukey post-tests (Prism 10, Graphpad software), and comparisons of linear curve fits were used to detect the significant difference between the cultures of combined O<sub>2</sub> levels and growth light/dark conditions. The confidence level for statistical test was set at 0.05.</p>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results</title>
<p>The growth rate of <italic>T. pseudonana</italic> of total and during the light and dark periods is shown in <xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>. The total growth rate under ambient O<sub>2</sub> was 0.60 &#xb1; 0.02 day<sup>-1</sup> and showed no significant difference from that under low O<sub>2</sub> (<italic>p</italic> = 0.29), while it was decreased by 15% by hypoxia. Under ambient O<sub>2</sub>, the growth rate during light period was about two times the total growth rate, but the growth rate during dark period was only 6% of the total growth rate. Comparing to ambient O<sub>2</sub>, the growth rate during light period was increased by 10% by low O<sub>2</sub> (<italic>p</italic> &lt; 0.05) but showed no significant effect by hypoxia, while the growth rate during dark period was significantly decreased by both low O<sub>2</sub> and hypoxia (<italic>p</italic> &lt; 0.01).</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>Cell growth rate (day<sup>&#x2212;1</sup>) of <italic>T. pseudonana</italic> grown under ambient O<sub>2</sub>, low O<sub>2</sub>, and hypoxia during the total, light, and dark periods. The vertical bar shows one standard deviation of three growth determinations on independently grown cultures (<italic>n</italic> = 3), and different letters on the top of the bars indicate significant differences (<italic>p</italic> &lt; 0.05).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-12-1529163-g001.tif"/>
</fig>
<p>During the light period, cellular Chl <italic>a</italic> content under ambient O<sub>2</sub> was 0.41 &#xb1; 0.02 pg cell<sup>-1</sup> and was decreased by 7% and 20% by low O<sub>2</sub> and hypoxia, respectively (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2A</bold>
</xref>). Chl <italic>a</italic> content under ambient O<sub>2</sub> during the dark period was 20% lower than that during the light period and was further decreased by 12% and 26% by low O<sub>2</sub> and hypoxia, respectively (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2A</bold>
</xref>). Car content was 0.41 &#xb1; 0.02 pg cell<sup>-1</sup> under ambient O<sub>2</sub> and showed a similar trend of lowered O<sub>2</sub> effect as Chl <italic>a</italic> during both light and dark periods (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2B</bold>
</xref>). POC content during the light period was 10.7 &#xb1; 0.14 pg cell<sup>-1</sup> under ambient O<sub>2</sub>, being increased by 15% by low O<sub>2</sub> but decreased by 15% by hypoxia. The POC in the dark period was 20% lower than that in the light period and was increased by 21% by low O<sub>2</sub> but decreased by 17% by hypoxia (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2C</bold>
</xref>). By contrast, the PON content during light (i.e., 1.30 &#xb1; 0.09 pg cell<sup>-1</sup>) and dark periods (i.e., 0.95 &#xb1; 0.09 pg cell<sup>-1</sup>) showed no significant difference between ambient and low O<sub>2</sub> treatment (light period: <italic>p</italic> = 0.27; dark period: <italic>p</italic> = 0.33) (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2D</bold>
</xref>). However, the PON was decreased by 21% and 33% by hypoxia during the light and dark periods, respectively.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Cellular content (pg cell<sup>-1</sup>) of chlorophyll <italic>a</italic> (Chl <italic>a</italic>, <bold>A</bold>), carotenoid (Car, <bold>B</bold>), particulate organic carbon (POC, <bold>C</bold>), and particulate organic nitrogen (PON, <bold>D</bold>) of <italic>T. pseudonana</italic> grown under ambient O<sub>2</sub>, low O<sub>2</sub>, and hypoxia during the light and dark periods. The vertical bar shows one standard deviation of three growth determinations on independently grown cultures (<italic>n</italic> = 3), and different letters on the top of the bars indicate significant differences (<italic>p</italic> &lt; 0.05).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-12-1529163-g002.tif"/>
</fig>
<p>The maximum photochemical quantum yield (F<sub>V</sub>/F<sub>M</sub>) of PSII of <italic>T. pseudonana</italic> was 0.65 &#xb1; 0.01 and 0.73 &#xb1; 0.01 during the light and dark periods, respectively, and showed no significant effect of lowering O<sub>2</sub> (one-way ANOVA, <italic>F</italic>
<sub>2,6</sub> = 2.33, <italic>p</italic> = 0.18) (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>), although the negative effects by lowering O<sub>2</sub> on the RLC-derived light utilization efficiency (&#x3b1;), maximum relative electron transport rate (rETR<sub>max</sub>), and saturation light (E<sub>K</sub>) occurred under both light and dark conditions (<xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>). However, the photosynthetic O<sub>2</sub> evolution rate (P<sub>n</sub>, 2.13 &#xb1; 0.09 fmol O<sub>2</sub> cell<sup>-1</sup> min<sup>-1</sup>) under growth light was reduced by 11% and 26% by low O<sub>2</sub> and hypoxia, respectively (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3B</bold>
</xref>). The dark respiration rate (R<sub>d</sub>) was 0.58 &#xb1; 0.04 and 0.45 &#xb1; 0.02 fmol O<sub>2</sub> cell<sup>-1</sup> min<sup>-1</sup> under growth light and dark conditions, respectively, and decreased with lowering O<sub>2</sub> in both light and dark conditions (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3C</bold>
</xref>).</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Maximal photochemical quantum yield of PSII (F<sub>V</sub>/F<sub>M</sub>, <bold>A</bold>) and the ratio (fmol O<sub>2</sub> cell<sup>-1</sup> min<sup>-1</sup>) of photosynthetic O<sub>2</sub> evolution (P<sub>n</sub>, <bold>B</bold>) and dark respiration (R<sub>d</sub>, <bold>C</bold>) of <italic>T. pseudonana</italic> grown under ambient O<sub>2</sub>, low O<sub>2</sub>, and hypoxia during the light and dark periods. The vertical bar shows one standard deviation of three growth determinations on independently grown cultures (<italic>n</italic> = 3), and different letters on the top of the bars indicate significant differences (<italic>p</italic> &lt; 0.05).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-12-1529163-g003.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>Photosynthetic parameters derived from rapid light curve (RLC), i.e., light utilization efficiency (<italic>&#x3b1;</italic>, slope), maximum relative electron transfer rate (rETR<sub>max</sub>), and saturation irradiance (E<sub>K</sub>, &#xb5;mol photons m<sup>&#x2212;2</sup> s<sup>&#x2212;1</sup>) of diatom <italic>Thalassiosira pseudonana</italic> grown under light and dark conditions at ambient O<sub>2</sub>, low O<sub>2</sub>, and hypoxia.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="center">Photosynthetic parameters</th>
<th valign="middle" align="center">Light state</th>
<th valign="middle" align="center">Amb O<sub>2</sub>
</th>
<th valign="middle" align="center">Low O<sub>2</sub>
</th>
<th valign="middle" align="center">Hypoxia</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="2" align="center">
<italic>&#x3b1;</italic>
</td>
<td valign="middle" align="center">Light</td>
<td valign="middle" align="center">0.31 &#xb1; 0.0024<sup>a</sup>
</td>
<td valign="middle" align="center">0.30 &#xb1; 0.0068<sup>ab</sup>
</td>
<td valign="middle" align="center">0.28 &#xb1; 0.0052<sup>bc</sup>
</td>
</tr>
<tr>
<td valign="middle" align="center">Dark</td>
<td valign="middle" align="center">0.28 &#xb1; 0.0027<sup>bc</sup>
</td>
<td valign="middle" align="center">0.29 &#xb1; 0.010<sup>ac</sup>
</td>
<td valign="middle" align="center">0.28 &#xb1; 0.0051<sup>c</sup>
</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">rETR<sub>max</sub>
</td>
<td valign="middle" align="center">Light</td>
<td valign="middle" align="center">128.08 &#xb1; 1.67<sup>a</sup>
</td>
<td valign="middle" align="center">114.01 &#xb1; 6.09<sup>ab</sup>
</td>
<td valign="middle" align="center">93.03 &#xb1; 2.24<sup>c</sup>
</td>
</tr>
<tr>
<td valign="middle" align="center">Dark</td>
<td valign="middle" align="center">125.58 &#xb1; 7.26<sup>a</sup>
</td>
<td valign="middle" align="center">123.89 &#xb1; 5.12<sup>a</sup>
</td>
<td valign="middle" align="center">105.89 &#xb1; 2.57<sup>bc</sup>
</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">E<sub>K</sub> (&#xb5;mol photons m<sup>-2</sup> s<sup>-1</sup>)</td>
<td valign="middle" align="center">Light</td>
<td valign="middle" align="center">416.52 &#xb1; 6.99<sup>ab</sup>
</td>
<td valign="middle" align="center">382.96 &#xb1; 15.44<sup>b</sup>
</td>
<td valign="middle" align="center">328.67 &#xb1; 8.01<sup>c</sup>
</td>
</tr>
<tr>
<td valign="middle" align="center">Dark</td>
<td valign="middle" align="center">440.58 &#xb1; 21.39<sup>a</sup>
</td>
<td valign="middle" align="center">422.63 &#xb1; 12.97<sup>ab</sup>
</td>
<td valign="middle" align="center">383.18 &#xb1; 7.40<sup>b</sup>
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>Different superscript letters next to numbers indicate significant difference among different light conditions and O<sub>2</sub> levels (<italic>p</italic> &lt; 0.05).</p>
</fn>
</table-wrap-foot>
</table-wrap>
<p>To study the metabolism of diatoms that had dropped out of the euphotic zone, we cultured <italic>T. pseudonana</italic> in the dark for 84 h (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>). At ambient O<sub>2</sub>, the cell density decreased from 1,678 &#xb1; 56 to 513 &#xb1; 95 cell mL<sup>-1</sup> from T0 to T84, with a cell mortality rate of 14 cell mL<sup>-1</sup> h<sup>-1</sup> (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4A</bold>
</xref>). Low O<sub>2</sub> significantly reduced the mortality rate by 30%, while hypoxia exacerbated it by 40%. At ambient O<sub>2</sub>, cellular carbon content (POC) decreased from 10.4 &#xb1; 0.97 to 4.34 &#xb1; 0.29 pg cell<sup>-1</sup> from T0 to T84, with a C loss rate of 0.066 pg cell<sup>-1</sup> h<sup>-1</sup> (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4B</bold>
</xref>), while nitrogen content (PON) decreased from 1.14 &#xb1; 0.05 to 0.33 &#xb1; 0.03 pg cell<sup>-1</sup>, with a N loss rate of 0.011 pg cell<sup>-1</sup> h<sup>-1</sup> (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4C</bold>
</xref>). Lowering O<sub>2</sub> showed no significant effect on the C loss rate (<italic>F</italic> = 0.39, <italic>p</italic> = 0.68) but significantly decreased the N loss rate (<italic>F</italic> = 3.65, <italic>p</italic> = 0.031) (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4C</bold>
</xref>). In addition, a greater decrease in C loss rate than N loss rate led to an increase in the POC/PON ratio with the duration of dark time (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4D</bold>
</xref>). At T0, T48, and T84, cells at ambient O<sub>2</sub> settled in a rate of 4.88 &#xb1; 0.07, 5.12 &#xb1; 0.08, and 5.88 &#xb1; 0.19 cm day<sup>-1</sup>, respectively (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>). Low O<sub>2</sub> showed no significant effect on sinking rate at T0 and T48 but decreased it by 10% at T84; hypoxia, however, increased the sinking rate by 13%. In addition, there was an interactive effect of lowered O<sub>2</sub> and dark duration on the cell sinking rate (two-way ANOVA, <italic>F</italic>
<sub>4,12</sub> = 15.68, <italic>p</italic> &lt; 0.01).</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>Cell density (cells mL<sup>-1</sup>, <bold>A</bold>), cellular content (pg cell<sup>-1</sup>) of particulate organic carbon (POC, <bold>B</bold>) and particulate organic nitrogen (PON, <bold>C</bold>) and POC:PON ratio <bold>(D)</bold> of <italic>T. pseudonana</italic> grown under ambient O<sub>2</sub>, low O<sub>2</sub>, and hypoxia during the 84-h cultivation in the dark. The vertical bars show the standard deviation of three growth determinations on independently grown cultures (<italic>n</italic> = 3). The solid lines show a linear relationship, and the dotted lines show 95% confidence intervals of the fitted lines.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-12-1529163-g004.tif"/>
</fig>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>Sinking rate (cm day<sup>-1</sup>) of <italic>T. pseudonana</italic> grown under ambient O<sub>2</sub>, low O<sub>2</sub>, and hypoxia during the 84-h cultivation in the dark. The vertical bar shows one standard deviation of three growth determinations on independently grown cultures (<italic>n</italic> = 3), and different letters on the top of the bars indicate significant differences (<italic>p</italic> &lt; 0.05).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-12-1529163-g005.tif"/>
</fig>
</sec>
<sec id="s4" sec-type="discussion">
<label>4</label>
<title>Discussion</title>
<p>The effects of lowering O<sub>2</sub> levels on the physiological and metabolic processes of marine aerobic organisms are well documented (e.g., <xref ref-type="bibr" rid="B36">Wang et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B25">McCormick and Levin, 2017</xref>). Many studies have also shown the different photophysiological responses of diatoms to a decrease in O<sub>2</sub> level at different light intensities (<xref ref-type="bibr" rid="B28">Pruder and Bolton, 1980</xref>; <xref ref-type="bibr" rid="B38">Wu et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B41">Zhao et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B33">Sun et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>, <xref ref-type="bibr" rid="B7">2024</xref>) and at different light exposure times, i.e., photoperiod (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>). In this study, we further showed that the diatom <italic>T. pseudonana</italic> responds differently to lowered O<sub>2</sub> level during the day and at night.</p>
<p>Lowering O<sub>2</sub> was generally thought to benefit the photosynthetic carbon fixation of phytoplankton (<xref ref-type="bibr" rid="B30">Raven and Larkum, 2007</xref>), as the carboxylation efficiency of ribulose-1, 5-bisphosphate carboxylase/oxygenase (RubisCO), a rate-limiting enzyme of carbon fixation, was directly relevant to the O<sub>2</sub>/CO<sub>2</sub> ratio (<xref ref-type="bibr" rid="B14">Gao and Campbell, 2014</xref>). Low O<sub>2</sub> means a fewer O<sub>2</sub> molecules that compete for the binding site of RubisCO with CO<sub>2</sub> and thus less energy cost to maintain CO<sub>2</sub> concentrating mechanisms (CCMs) (<xref ref-type="bibr" rid="B31">Reinfelder et&#xa0;al., 2000</xref>; <xref ref-type="bibr" rid="B16">Giordano et&#xa0;al., 2005</xref>), which could make cells allocate more carbon (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2C</bold>
</xref>) to support growth (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>). It is consistent with previous reports on the field phytoplankton communities (<xref ref-type="bibr" rid="B33">Sun et&#xa0;al., 2022</xref>) and laboratory individual species (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B33">Sun et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B7">Chen et&#xa0;al., 2024</xref>). However, previous studies have also noted the negative effects of lowered O<sub>2</sub> on Photosystem II (PS II), especially at a longer photoperiod and a higher light intensity (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>, <xref ref-type="bibr" rid="B7">2024</xref>). During the transformation of photosynthetic electron, oxidization of harmful reactive oxygen species (ROS), and inactivation of photosynthetic components such as the PsbA protein (<xref ref-type="bibr" rid="B27">P&#xe9;rez-P&#xe9;rez et&#xa0;al., 2012</xref>), diatoms had to additionally allocate by up to 15% total nitrogen to repair the damaged PS II (<xref ref-type="bibr" rid="B20">Li et&#xa0;al., 2015</xref>). In this situation, the inhibited nitrogen metabolism by lowered O<sub>2</sub> might further disrupt the balance between damage and repair of PSII (<xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>), resulting in a more significant decrease in photosynthetic capacity during the day (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3A</bold>
</xref>; <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>).</p>
<p>Aerobic metabolic processes of diatoms, such as mitochondrial respiration and the tricarboxylic acid cycle (TCA cycle), are vital for cells to obtain and allocate energy that is normally required to support other metabolic processes, such as nutrient uptake and assimilation (<xref ref-type="bibr" rid="B23">Lomas and Gilbert, 1999</xref>; <xref ref-type="bibr" rid="B11">Clark et al., 2002</xref>) and fatty acid synthesis (<xref ref-type="bibr" rid="B7">Chen et&#xa0;al., 2024</xref>), whose activities are directly related to available O<sub>2</sub> (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B41">Zhao et&#xa0;al., 2022</xref>). These metabolic processes are therefore more sensitive to lowered O<sub>2</sub> levels compared to photosynthesis (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>) and are additionally inhibited and even blocked at night, leading to increased degradation of cellular organic matter (<xref ref-type="fig" rid="f4">
<bold>Figures&#xa0;4B, C</bold>
</xref>) and even cell death (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>). Furthermore, our results showed that the decreased degradation of organic C and N caused by lowered O<sub>2</sub> is disproportionate, such that the C/N ratio increases with the duration of darkness (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4D</bold>
</xref>). According to <xref ref-type="bibr" rid="B38">Wu et&#xa0;al. (2012)</xref>, hypoxia can also decrease the adenylate energy charge of diatom [AEC = (ATP + 0.5 ADP)/(ATP + ADP + AMP)] by ~50%, suggesting the inhibition of ATPase and thus a decrease in cellular protein and fatty acid content (<xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>, <xref ref-type="bibr" rid="B7">2024</xref>) as well as a decrease in chlorophyll and organic N and C content (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>). Such a decrease in chlorophyll content and Chl <italic>a</italic>/Chl <italic>b</italic> ratio due to hypoxia was also observed in the seagrass <italic>Enhalus acoroides</italic> at night (<xref ref-type="bibr" rid="B5">Che et&#xa0;al., 2022</xref>).</p>
<p>In the dark, diatoms normally decomposed the organic substances of, e.g., sugars and fatty acids via the TCA cycle first to obtain energy for their survival, followed by precious proteins (<xref ref-type="bibr" rid="B10">Cheng et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>). Thus, how low O<sub>2</sub> affects cell growth depends on the net accumulation of cell composition. Our findings showed that low O<sub>2</sub> decreases dark respiration (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3C</bold>
</xref>), simultaneously promotes cellular C accumulation (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4B</bold>
</xref>), and decreases the mortality of cells (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4A</bold>
</xref>). However, under hypoxia, the cellular fatty acid content of diatom <italic>T. pseudonana</italic> was reduced by up to ~40% (<xref ref-type="bibr" rid="B7">Chen et&#xa0;al., 2024</xref>), which may have forced the cells to obtain more energy by decomposing functional proteins (<xref ref-type="bibr" rid="B9">Chen et&#xa0;al., 2023</xref>), thus leading to a linear increase in POC/PON ratio (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4D</bold>
</xref>). Such a phenomenon of changing metabolic substrate preference in response to environmental changes was also observed in the diatom <italic>S. dohrnii</italic> (<xref ref-type="bibr" rid="B10">Cheng et&#xa0;al., 2022</xref>).</p>
<p>The sinking speed of <italic>T. pseudonana</italic> was estimated to be ~5.0 cm day<sup>-1</sup>, which is comparable to other studies (<xref ref-type="bibr" rid="B35">Waite et&#xa0;al., 1997</xref>; <xref ref-type="bibr" rid="B2">Bannon and Campbell, 2017</xref>), and increased with duration of darkness (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>). Low O<sub>2</sub> decreased the sinking rate while hypoxia accelerated it, which can be explained by the lower mortality of cells in the former and higher mortality in the latter condition compared to the ambient O<sub>2</sub> condition. On the other hand, diatoms normally aggregate multi-cellularly in nature and accumulate fatty acids to decrease gravity and avoid sinking from the euphotic zone (<xref ref-type="bibr" rid="B15">Ge et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B18">Janssen et&#xa0;al., 2014</xref>). The increased sinking rate under hypoxia could be related to the decrease in cell activity and cell composition as found here (<xref ref-type="fig" rid="f2">
<bold>Figures&#xa0;2</bold>
</xref>, <xref ref-type="fig" rid="f4">
<bold>4</bold>
</xref>) or in other studies (<xref ref-type="bibr" rid="B7">Chen et&#xa0;al., 2024</xref>). Such an increase in sinking rate combined with increasing mortality under hypoxic conditions suggests that the diatom-derived carbon burial may be accelerated under the marine deoxygenation scenario in the future (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>). In addition, our results from individual diatom species grown in the laboratory should be taken with caution, although they provide a potentially mechanistic understanding of the effects of decreasing O<sub>2</sub>. Further studies with a phytoplankton community or multiple species closer to field conditions need to be conducted.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>Simplified representation of decreasing O<sub>2</sub> which affected the cell growth and sinking rate of marine diatom, suggesting the carbon burial derived from diatom being accelerated due to marine deoxygenation.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-12-1529163-g006.tif"/>
</fig>
</sec>
</body>
<back>
<sec id="s5" sec-type="data-availability">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material. Further inquiries can be directed to the corresponding authors.</p>
</sec>
<sec id="s6" sec-type="author-contributions">
<title>Author contributions</title>
<p>BC: Writing &#x2013; original draft. HS: Writing &#x2013; review &amp; editing. GX: Writing &#x2013; original draft. HJ: Writing &#x2013; original draft. XY: Writing &#x2013; original draft. GL: Writing &#x2013; review &amp; editing.</p>
</sec>
<sec id="s7" sec-type="funding-information">
<title>Funding</title>
<p>The author(s) declare financial support was received for the research, authorship, and/or publication of this article. This work was funded by the National Natural Science Foundation of China (42430405, 32371665), Natural Science Foundation of Guangdong Province (2022A1515011461), and Natural Science Foundation of Shandong Province (ZR2024QC354).</p>
</sec>
<ack>
<title>Acknowledgments</title>
<p>We thank Zhao Wei from the Institute of Marine Science and Technology, Shandong University, for assistance with data analysis and measurement of cellular nitrogen and carbon content.</p>
</ack>
<sec id="s8" 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>
<p>The author(s) declared that they were an editorial board member of Frontiers, at the time of submission. This had no impact on the peer review process and the final decision.</p>
</sec>
<sec id="s9" sec-type="ai-statement">
<title>Generative AI statement</title>
<p>The author(s) declare that no Generative AI was used in the creation of this manuscript.</p>
</sec>
<sec id="s10" 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>
</sec>
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