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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0">
  <front>
    <journal-meta><journal-id journal-id-type="publisher">BG</journal-id><journal-title-group>
    <journal-title>Biogeosciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">BG</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Biogeosciences</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1726-4189</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/bg-16-2923-2019</article-id><title-group><article-title>Sensitivity of atmospheric <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional variability in particulate organic matter remineralization depths</article-title><alt-title>Sensitivity of <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional remineralization</alt-title>
      </title-group><?xmltex \runningtitle{Sensitivity of {$\chem{CO_{2}}$} to regional remineralization}?><?xmltex \runningauthor{J. D. Wilson et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Wilson</surname><given-names>Jamie D.</given-names></name>
          <email>jamie.wilson@bristol.ac.uk</email>
        <ext-link>https://orcid.org/0000-0001-7509-4791</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Barker</surname><given-names>Stephen</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7870-6431</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Edwards</surname><given-names>Neil R.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Holden</surname><given-names>Philip B.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2369-0062</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff4">
          <name><surname>Ridgwell</surname><given-names>Andy</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>BRIDGE, School of Geographical Sciences, University of Bristol, Bristol, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>School of Earth and Ocean Sciences, Cardiff University, Cardiff, UK</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>School of Environment, Earth and Ecosystems, Open University, Milton Keynes, UK</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Department of Earth Sciences, University of California, Riverside, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jamie D. Wilson (jamie.wilson@bristol.ac.uk)</corresp></author-notes><pub-date><day>31</day><month>July</month><year>2019</year></pub-date>
      
      <volume>16</volume>
      <issue>14</issue>
      <fpage>2923</fpage><lpage>2936</lpage>
      <history>
        <date date-type="received"><day>13</day><month>December</month><year>2018</year></date>
           <date date-type="rev-request"><day>17</day><month>December</month><year>2018</year></date>
           <date date-type="rev-recd"><day>5</day><month>July</month><year>2019</year></date>
           <date date-type="accepted"><day>9</day><month>July</month><year>2019</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2019 Jamie D. Wilson et al.</copyright-statement>
        <copyright-year>2019</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019.html">This article is available from https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019.html</self-uri><self-uri xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019.pdf">The full text article is available as a PDF file from https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e159">The concentration of <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the atmosphere is sensitive to changes in the depth at which sinking particulate organic matter is remineralized: often described as a change in the exponent “<inline-formula><mml:math id="M4" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>” of the Martin curve. Sediment trap observations from deep and intermediate depths suggest there is a spatially heterogeneous pattern of <inline-formula><mml:math id="M5" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, particularly varying with latitude, but disagree over the exact spatial patterns. Here we use a biogeochemical model of the phosphorus cycle coupled with a steady-state representation of ocean circulation to explore the sensitivity of preformed phosphate and atmospheric <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to spatial variability in remineralization depths. A Latin hypercube sampling method is used to simultaneously vary the Martin curve independently within 15 different regions, as a basis for a regression-based analysis used to derive a quantitative measure of sensitivity. Approximately 30 % of the sensitivity of atmospheric <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to changes in remineralization depths is driven by changes in the subantarctic region (36 to 60<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) similar in magnitude to the Pacific basin despite the much smaller area and lower export production. Overall, the absolute magnitude of sensitivity is controlled by export production, but the relative spatial patterns in sensitivity are predominantly constrained by ocean circulation pathways. The high sensitivity in the subantarctic regions is driven by a combination of high export production and the high connectivity of these regions to regions important for the export of preformed nutrients such as the Southern Ocean and North Atlantic. Overall, regionally varying remineralization depths contribute to variability in <inline-formula><mml:math id="M9" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> of between around 5 and 15 ppm, relative to a global mean change in remineralization depth. Future changes in the environmental and ecological drivers of remineralization, such as temperature and ocean acidification, are expected to be most significant in the high latitudes where <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity to remineralization is also highest. The importance of ocean circulation pathways to the high sensitivity in subantarctic regions also has significance for past climates given the importance of circulation changes in the Southern Ocean.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e250">Sinking particles of organic matter transfer 5–10 Pg C per year from the upper ocean to the ocean interior <xref ref-type="bibr" rid="bib1.bibx17" id="paren.1"/> as part of a process known as the biological pump.  As these particles sink, they are remineralized through bacterial- and zooplankton-related activity, releasing the carbon and nutrients back into solution at depth.  Vertical fluxes of particulate organic carbon (POC) in the water column have historically been described by the Martin curve, a power-law function that describes the rapid decrease in flux (<inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>z</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) from a maximum value at depth <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, nominally the base of the mixed layer, to a small asymptotic value in deep waters <xref ref-type="bibr" rid="bib1.bibx37" id="paren.2"><named-content content-type="pre">Fig. <xref ref-type="fig" rid="Ch1.F1"/>; Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>;</named-content></xref>:
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M13" display="block"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>z</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:msub><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>z</mml:mi><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mi>b</mml:mi></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <?pagebreak page2924?><p id="d1e327">The dimensionless exponent in the power law (<inline-formula><mml:math id="M14" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>) describes whether organic matter is remineralized predominantly at shallower depths (larger values of <inline-formula><mml:math id="M15" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>; e.g. <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.6</mml:mn></mml:mrow></mml:math></inline-formula>) or deeper in the water column (smaller values of <inline-formula><mml:math id="M17" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>; e.g. <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. <xref ref-type="fig" rid="Ch1.F1"/>). The exponent itself parameterizes the rate at which POC sinks through the water column (units of m d<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and the rate at which it is remineralized (units of d<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; <xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx31" id="altparen.3"/>). In this paper we use the term “remineralization depth”, defined as a depth at which a defined % of POC has been remineralized. Previously, this has been defined as an <inline-formula><mml:math id="M21" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> folding depth: the depth at which <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">63</mml:mn></mml:mrow></mml:math></inline-formula> % of POC has been remineralized (<xref ref-type="bibr" rid="bib1.bibx30" id="altparen.4"/>; although note that the Martin curve is not exponential).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e428">The normalized water column distribution of particulate fluxes defined using the Martin curve. As a comparison, Martin curves are
shown with the exponent found by <xref ref-type="bibr" rid="bib1.bibx37" id="text.5"/> (<inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.858</mml:mn></mml:mrow></mml:math></inline-formula>) and minimum and maximum exponent values used in this study based on sediment trap data compilations <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx36 bib1.bibx14" id="paren.6"><named-content content-type="pre"><inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.6</mml:mn></mml:mrow></mml:math></inline-formula>;</named-content></xref>. All curves have export depth (<inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>) of 120 m.</p></caption>
        <?xmltex \igopts{width=156.490157pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f01.png"/>

      </fig>

      <p id="d1e494">Ocean biogeochemical models predict that the concentration of <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the atmosphere is sensitive to changes in a globally uniform remineralization depth. <xref ref-type="bibr" rid="bib1.bibx30" id="text.7"/> showed that a deepening of the remineralization depth globally of 24 m (from <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> to 0.9) redistributed dissolved inorganic carbon (DIC) from the intermediate waters to the deep ocean, leading to a reduction in atmospheric <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> of between 10 and 27 ppm. The drawdown was also associated with a decrease in the global mean concentration of preformed nutrients in the ocean interior <xref ref-type="bibr" rid="bib1.bibx19" id="paren.8"><named-content content-type="pre">nutrients that are not utilised by biology in the surface ocean and enter the ocean interior via circulation;</named-content></xref>. <xref ref-type="bibr" rid="bib1.bibx30" id="text.9"/> found that an increase in respired carbon in the deep ocean was balanced by a reduction in preformed nutrients exported in the North Atlantic. Deepening of the POC remineralization depth could also drive dissolution of calcium carbonate (<inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CaCO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) in ocean sediments, ultimately drawing down more <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> over millennial timescales <xref ref-type="bibr" rid="bib1.bibx47" id="paren.10"/>. The potential impact of remineralization depth changes on atmospheric <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is therefore a highly relevant component of the marine carbon cycle for both past and current changes in climate <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx18 bib1.bibx39" id="paren.11"/>.</p>
      <p id="d1e582"><?xmltex \hack{\newpage}?>Analyses of global sediment trap observations suggest there is a spatially heterogeneous pattern of remineralization depths in the modern ocean that varies particularly with latitude. A synthesis of observations from deep sediment traps <xref ref-type="bibr" rid="bib1.bibx15" id="paren.12"><named-content content-type="pre"><inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1500</mml:mn></mml:mrow></mml:math></inline-formula>–2000 m;</named-content></xref> suggests that POC fluxes in high latitudes attenuate faster with depth (shallower remineralization depth: <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.6</mml:mn></mml:mrow></mml:math></inline-formula>) than in low latitudes, where a greater proportion of POC is transported to depth (deeper remineralization depth: <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>); see Fig. <xref ref-type="fig" rid="Ch1.F1"/>). However, POC fluxes measured using neutrally buoyant sediment traps at shallower depths (<inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula> m) suggest the inverse of this latitudinal pattern <xref ref-type="bibr" rid="bib1.bibx36" id="paren.13"/>; see also <xref ref-type="bibr" rid="bib1.bibx51" id="text.14"/>. A recent compilation of sediment trap data and profiles of particle size distributions observed in the water column highlight additional intra-basin variability in <inline-formula><mml:math id="M37" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> (e.g. shallower remineralization in the eastern equatorial Pacific than in the western equatorial Pacific) and inter-basin variability (e.g. deeper remineralization in the Atlantic and Indian basins compared to the Pacific) <xref ref-type="bibr" rid="bib1.bibx14" id="paren.15"/>. The uncertainty in the spatial variability of remineralization depths presents a challenge for determining which mechanisms may be responsible for changes in remineralization depths and how these might drive future or past changes in remineralization <xref ref-type="bibr" rid="bib1.bibx1" id="paren.16"><named-content content-type="pre">e.g.</named-content></xref>. Additionally, this also presents a challenge for biogeochemical models, which are beginning to resolve the mechanisms that are potentially responsible for these spatial patterns, such as particle-size-dependent sinking rates <xref ref-type="bibr" rid="bib1.bibx7" id="paren.17"/>, temperature-dependent remineralization <xref ref-type="bibr" rid="bib1.bibx20" id="paren.18"/>, and oxygen dependence <xref ref-type="bibr" rid="bib1.bibx32" id="paren.19"/>.</p>
      <p id="d1e668">A key question in light of the observed spatial variability in remineralization depths and the associated uncertainty in spatial patterns is what the sensitivity of atmospheric <inline-formula><mml:math id="M38" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations to spatial variability in remineralization depths is. <xref ref-type="bibr" rid="bib1.bibx30" id="text.20"/> further quantified the sensitivity of atmospheric <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to basin-scale changes in remineralization depths by perturbing them in each basin individually, finding that the Pacific, Southern Ocean (defined as <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S), Atlantic, and Indian oceans contributed 38 %, 22 %, 21 %, and 19 % of the total <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> drawdown, respectively <xref ref-type="bibr" rid="bib1.bibx30" id="paren.21"/>. The variability in <inline-formula><mml:math id="M43" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity between basins matched the variability in the magnitude of export production integrated over the basins and basin area, suggesting that no one region was more significant when varying the globally uniform remineralization depth <xref ref-type="bibr" rid="bib1.bibx30" id="paren.22"/>. However, this basin-scale analysis does not resolve the sensitivity of atmospheric <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> occurring at the resolution suggested by observations, i.e. a latitudinal and within-basin scale, or at the resolution of ecological and biogeochemical variability <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx10" id="paren.23"/>. Additionally, the analysis does not allow for the identification of potential interactions and feedbacks between regions when remineralization depths are changing simultaneously.</p>
      <p id="d1e757">Here we aim to address these issues by performing a global sensitivity analysis of regionally varying remineralization<?pagebreak page2925?> depths. To this end, we use a transport matrix (a steady-state, computationally efficient representation of ocean transport) derived from the MIT global circulation model (MITgcm) with a model of phosphorus and carbon cycling where the ocean is divided into 15 regions in which remineralization depths can change independently. Remineralization depths are perturbed simultaneously using Latin hypercube sampling and sensitivity quantified using regression analysis,.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Model description</title>
      <p id="d1e775">We provide a brief description of the model here and a more detailed description in Appendix <xref ref-type="sec" rid="App1.Ch1.S1"/>. The approach to quantifying sensitivity used here relies on the ability to run an ensemble of model experiments. To make this approach feasible we use the “transport matrix method” <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx22" id="paren.24"/>, a steady-state, computationally efficient representation of ocean transport and climate derived from a global circulation model. We use monthly mean transport matrices derived from the 2.8<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> global configuration of the MIT global circulation model (MITgcm) with 15 vertical levels <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx22" id="paren.25"/>. These specific matrices have been previously applied to model biogeochemistry <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx28" id="paren.26"/>.</p>
      <p id="d1e798">The biogeochemical model used here is a model of the marine phosphorus and carbon cycle that resolves phosphate (<inline-formula><mml:math id="M46" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), dissolved organic phosphorus (DOP), dissolved inorganic carbon (DIC), total alkalinity, and atmospheric <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Following <xref ref-type="bibr" rid="bib1.bibx30" id="text.27"/>, we calculate the production of organic matter using either a nutrient-restoring scheme, where [<inline-formula><mml:math id="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] is restored to monthly observations of [<inline-formula><mml:math id="M49" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] <xref ref-type="bibr" rid="bib1.bibx12" id="paren.28"/> using a timescale of 30 d (Eq. <xref ref-type="disp-formula" rid="App1.Ch1.S1.E7"/>) or using constant export production, where export production is fixed to that of the control run, unless local nutrients fall below zero. These two schemes represent two end-member scenarios, strictly within the context of this model, where organic matter production either depends entirely on macronutrient concentrations and can increase with higher nutrient fluxes (restoring) or is limited by other factors such as light or micronutrients (constant export). The remineralization of particulate organic matter is parameterized using the Martin curve (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>). To further facilitate a large number of experiments for the sensitivity analysis, we use the model to define a statistical relationship between preformed <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and atmospheric <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and run the model with a phosphorus cycle only (see Sect. <xref ref-type="sec" rid="App1.Ch1.S1.SS2.SSS3"/>).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Experiment design</title>
<sec id="Ch1.S2.SS2.SSSx1" specific-use="unnumbered">
  <title>Defining regions</title>
      <p id="d1e905">We define a set of oceanic regions to approximately encapsulate the large-scale variability in biogeochemistry and patterns of remineralization depths observed in sediment trap studies. We define regions by lines of latitude and basins, similar to the approach used by air–sea flux inversion studies, e.g. <xref ref-type="bibr" rid="bib1.bibx13" id="text.29"/> and <xref ref-type="bibr" rid="bib1.bibx40" id="text.30"/>. All 15 regions are defined based on a partitioning by <xref ref-type="bibr" rid="bib1.bibx13" id="text.31"/>, with some minor changes (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a). The assigned regions broadly correspond with major features in observed surface [<inline-formula><mml:math id="M53" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>], such as higher concentrations in upwelling regions and lower concentrations in the nutrient-depleted gyres (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b). This suggests the regions should be a reasonable analogue for an alternative approach that captures key spatial variability in ecology and biogeochemistry by defining regions using vertical mixing, mixed layer depths, sea ice, and sea surface temperature <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx48 bib1.bibx16 bib1.bibx10" id="paren.32"/>. The regions are also comparable to the ocean biomes defined in previous biological pump studies <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx44" id="paren.33"><named-content content-type="pre">e.g.</named-content></xref>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e943"><bold>(a)</bold> Location and names of the 15 regions defined on the model grid based on <xref ref-type="bibr" rid="bib1.bibx13" id="text.34"/>. Boundaries are at 58<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 36<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 13<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 13<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, and 36<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. The equatorial Pacific is split at 98.75<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, following <xref ref-type="bibr" rid="bib1.bibx40" id="text.35"/>. Each region can be assigned a value of <inline-formula><mml:math id="M60" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> that is independent of other regions. <bold>(b)</bold> Location of regions superimposed on the annual mean surface [<inline-formula><mml:math id="M61" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] from World Ocean Atlas 2013 <xref ref-type="bibr" rid="bib1.bibx12" id="paren.36"/> regridded to the model grid.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f02.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Experiments</title>
      <p id="d1e1049">We perform a set of experiments to explore the sensitivity of atmospheric <inline-formula><mml:math id="M62" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional variability in <inline-formula><mml:math id="M63" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> with the aim of quantitatively ranking the sensitivity of atmospheric <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to remineralization depth changes in each region <xref ref-type="bibr" rid="bib1.bibx45" id="paren.37"><named-content content-type="pre">e.g.</named-content></xref>:
<list list-type="order"><list-item>
      <p id="d1e1088"><italic>Control run</italic>. A pre-industrial control run is set up with export production diagnosed by restoring it to observed surface [<inline-formula><mml:math id="M65" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] values, a globally uniform Martin<?pagebreak page2926?> exponent of 1.0 and initialized with globally uniform tracer concentrations. Atmospheric <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is restored to 278 ppm. A globally uniform Martin exponent gives the lowest volume-weighted root-mean-square misfit compared to annual mean World Ocean Atlas 2013 [<inline-formula><mml:math id="M67" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] observations <xref ref-type="bibr" rid="bib1.bibx12" id="paren.38"/>, as found in other studies using the same MITgcm transport matrices <xref ref-type="bibr" rid="bib1.bibx29" id="paren.39"/>. The control run is spun-up from uniform initial conditions for 5000 years.</p></list-item><list-item>
      <p id="d1e1133"><italic>Global sensitivity</italic>. The Martin curve is varied globally, i.e. all regions are assigned the same exponent, between 0.4 and 1.6 in 0.1 increments, based on the range of spatial variability observed in the modern ocean <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx36 bib1.bibx14" id="paren.40"/>. Each experiment is run for 3000 years continuing from the control run using the nutrient-restoring scheme to predict export production (Eq. <xref ref-type="disp-formula" rid="App1.Ch1.S1.E7"/>) and freely evolving atmospheric <inline-formula><mml:math id="M68" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item>
      <p id="d1e1155"><italic>Regional sensitivity</italic>. Latin hypercube sampling, a stratified random procedure that provides an efficient way of sampling high dimensional parameter space <xref ref-type="bibr" rid="bib1.bibx38" id="paren.41"/>, is used to vary the Martin curves in every region simultaneously. Values of <inline-formula><mml:math id="M69" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> are sampled from a uniform distribution ranging from 0.4 to 1.6 using the “lhsdesign” function in MATLAB with “maximin” sampling (an additional constraint that helps reduce clustering of samples, by maximizing the minimum distance between points, in order to give a well-spread distribution of points across the parameter space). The range of <inline-formula><mml:math id="M70" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> used centres around <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula>, as also used for the control run. We generate a Latin hypercube ensemble with 200 experiments, balancing the need for higher sampling resolution of the parameter space and total computational time. Each experiment is run for 3000 years continuing on from the control run with a phosphorus cycle only. Changes in atmospheric <inline-formula><mml:math id="M72" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are inferred from changes in preformed <inline-formula><mml:math id="M73" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p></list-item></list></p>
      <p id="d1e1212">Both the global and regional sensitivity experiments are repeated with constant-export production that is diagnosed from the control run. All output is diagnosed from the last full simulation year.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Sensitivity analysis</title>
      <p id="d1e1223">We use multiple linear regression analysis to derive the sensitivity of atmospheric <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to changes in <inline-formula><mml:math id="M75" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in each region (<inline-formula><mml:math id="M76" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>) where the fitted coefficients (<inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) give a quantitative measure of the sensitivity <xref ref-type="bibr" rid="bib1.bibx45" id="paren.42"><named-content content-type="pre">e.g.</named-content></xref>:
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M78" display="block"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>k</mml:mi></mml:munder><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi>b</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><?xmltex \opttitle{Sensitivity of {$\protect\chem{CO_{2}}$} to regional variability in remineralization depths}?><title>Sensitivity of <inline-formula><mml:math id="M79" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional variability in remineralization depths</title>
      <p id="d1e1333">To quantify the sensitivity of <inline-formula><mml:math id="M80" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional changes in <inline-formula><mml:math id="M81" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, we fit linear regression models  (Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>) to the results of the Latin hypercube ensembles. The resulting regression models explain a large proportion of the variability between <inline-formula><mml:math id="M82" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M83" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> (<inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.88</mml:mn></mml:mrow></mml:math></inline-formula> and 0.90 for the constant-export and nutrient-restoring ensembles, respectively). Residuals of the regression models showed no significant bias versus the regression output (Fig. S5 in Supplement), suggesting that a linear model was appropriate. Although the relationship between <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and a globally uniform remineralization depth is non-linear (e.g. Fig. <xref ref-type="fig" rid="Ch1.F6"/>), the relationship is near linear around the observed global mean in the centre of the range of <inline-formula><mml:math id="M86" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> tested <xref ref-type="bibr" rid="bib1.bibx30" id="paren.43"><named-content content-type="pre">see also,</named-content></xref>. Overall, the absence of a strongly non-linear relationship suggests the use of a linear regression model is appropriate <xref ref-type="bibr" rid="bib1.bibx45" id="paren.44"/>.</p>
      <p id="d1e1418">When <inline-formula><mml:math id="M87" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is varied as a globally uniform parameter from 0.4 to 1.6, atmospheric <inline-formula><mml:math id="M88" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> varies from 197 to 347 ppm (range of 150 ppm) for the constant-export scheme and from 257 to 288 ppm (range of 31 ppm) for the nutrient-restoring scheme, consistent with previous model experiments <xref ref-type="bibr" rid="bib1.bibx30" id="paren.45"/>. Figure <xref ref-type="fig" rid="Ch1.F3"/> shows how the sensitivity of <inline-formula><mml:math id="M89" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to changes in <inline-formula><mml:math id="M90" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> varies as a function of region. <inline-formula><mml:math id="M91" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is most sensitive to changes in <inline-formula><mml:math id="M92" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> occurring in the subantarctic regions, with <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> being most sensitive to changes in the Indian Ocean sector of the subantarctic (Fig. <xref ref-type="fig" rid="Ch1.F3"/>, Table <xref ref-type="table" rid="Ch1.T1"/>). The Southern Ocean and subtropical gyres, with the exception of the gyre in the North Pacific, are consistently the regions where <inline-formula><mml:math id="M94" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> has the smallest impact on <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Other regions, including the equatorial Indian Ocean, equatorial Pacific, and North Pacific have an intermediate sensitivity. As a region, the subantarctic is responsible for <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> % of the <inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity, comparable to the Pacific basin-scale sensitivity (Table <xref ref-type="table" rid="Ch1.T1"/>).</p>

<?xmltex \floatpos{p}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1541">Key metrics and sensitivity estimates for each region and basin. Representative metrics including area (percentage of global area), region-integrated mean annual POP export (percentage of global POP export), and mean preformed [<inline-formula><mml:math id="M98" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] (percentage of global mean) are taken from the control run. <inline-formula><mml:math id="M99" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity estimates for both the nutrient-restoring and constant-export ensembles are given as  <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from Eq. <xref ref-type="disp-formula" rid="Ch1.E2"/>)  with 95 % confidence intervals and as a percentage (<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right" colsep="1"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right" colsep="1"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" namest="col2" nameend="col4" align="center" colsep="1">Control </oasis:entry>
         <oasis:entry rowsep="1" namest="col5" nameend="col6" align="center" colsep="1">Constant export </oasis:entry>
         <oasis:entry rowsep="1" namest="col7" nameend="col8" align="center">Restoring uptake </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Area (%)</oasis:entry>
         <oasis:entry colname="col3">POP export (%)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M107" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">pre</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (%)</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (%)</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col8"><inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (%)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">SO</oasis:entry>
         <oasis:entry colname="col2">6.70</oasis:entry>
         <oasis:entry colname="col3">2.81</oasis:entry>
         <oasis:entry colname="col4">40.20</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.73</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.33</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">3.83</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.17</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">4.58</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SubPol-PAC</oasis:entry>
         <oasis:entry colname="col2">7.67</oasis:entry>
         <oasis:entry colname="col3">8.35</oasis:entry>
         <oasis:entry colname="col4">5.23</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:mn mathvariant="normal">15.54</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.36</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">10.40</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.70</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">10.55</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">STemp-PAC</oasis:entry>
         <oasis:entry colname="col2">10.37</oasis:entry>
         <oasis:entry colname="col3">7.86</oasis:entry>
         <oasis:entry colname="col4">0.29</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.72</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.34</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">3.83</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.65</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">2.54</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Weq-PAC</oasis:entry>
         <oasis:entry colname="col2">7.21</oasis:entry>
         <oasis:entry colname="col3">7.46</oasis:entry>
         <oasis:entry colname="col4">0.11</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mn mathvariant="normal">8.45</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.35</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">5.66</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.59</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">6.22</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Eeq-PAC</oasis:entry>
         <oasis:entry colname="col2">8.20</oasis:entry>
         <oasis:entry colname="col3">11.53</oasis:entry>
         <oasis:entry colname="col4">0.24</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mn mathvariant="normal">15.91</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">10.64</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.90</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.38</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">7.43</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ntemp-PAC</oasis:entry>
         <oasis:entry colname="col2">9.69</oasis:entry>
         <oasis:entry colname="col3">7.66</oasis:entry>
         <oasis:entry colname="col4">0.26</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mn mathvariant="normal">13.72</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.36</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">9.18</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.29</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">8.94</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NN-PAC</oasis:entry>
         <oasis:entry colname="col2">4.94</oasis:entry>
         <oasis:entry colname="col3">3.50</oasis:entry>
         <oasis:entry colname="col4">4.21</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mn mathvariant="normal">6.32</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.36</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">4.23</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.11</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">4.33</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SubPol-ATL</oasis:entry>
         <oasis:entry colname="col2">4.84</oasis:entry>
         <oasis:entry colname="col3">5.52</oasis:entry>
         <oasis:entry colname="col4">12.22</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mn mathvariant="normal">13.84</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">9.26</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.41</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">9.41</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Stemp-ATL</oasis:entry>
         <oasis:entry colname="col2">4.46</oasis:entry>
         <oasis:entry colname="col3">3.53</oasis:entry>
         <oasis:entry colname="col4">0.14</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.21</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.32</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">3.49</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.15</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">4.49</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Eq-ATL</oasis:entry>
         <oasis:entry colname="col2">5.45</oasis:entry>
         <oasis:entry colname="col3">6.06</oasis:entry>
         <oasis:entry colname="col4">0.10</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mn mathvariant="normal">9.58</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">6.41</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.10</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">8.22</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NTemp-ATL</oasis:entry>
         <oasis:entry colname="col2">5.13</oasis:entry>
         <oasis:entry colname="col3">3.09</oasis:entry>
         <oasis:entry colname="col4">0.04</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.29</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.33</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">2.20</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.76</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">2.97</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">NN-ATL</oasis:entry>
         <oasis:entry colname="col2">4.84</oasis:entry>
         <oasis:entry colname="col3">7.04</oasis:entry>
         <oasis:entry colname="col4">23.54</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mn mathvariant="normal">8.32</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">5.57</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.87</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">7.29</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SubPol-IND</oasis:entry>
         <oasis:entry colname="col2">6.86</oasis:entry>
         <oasis:entry colname="col3">9.18</oasis:entry>
         <oasis:entry colname="col4">13.04</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mn mathvariant="normal">18.29</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.38</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">12.24</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.00</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.38</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">11.73</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">STemp-IND</oasis:entry>
         <oasis:entry colname="col2">6.31</oasis:entry>
         <oasis:entry colname="col3">5.63</oasis:entry>
         <oasis:entry colname="col4">0.20</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mn mathvariant="normal">6.80</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.39</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">4.55</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.08</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.38</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">4.23</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Eq-IND</oasis:entry>
         <oasis:entry colname="col2">7.32</oasis:entry>
         <oasis:entry colname="col3">10.85</oasis:entry>
         <oasis:entry colname="col4">0.20</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mn mathvariant="normal">12.72</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.38</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">8.51</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.81</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.38</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col8">7.06</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">38</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S<inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">26.08</oasis:entry>
         <oasis:entry colname="col3">25.85</oasis:entry>
         <oasis:entry colname="col4">70.68</oasis:entry>
         <oasis:entry colname="col5">53.40</oasis:entry>
         <oasis:entry colname="col6">35.73</oasis:entry>
         <oasis:entry colname="col7">9.29</oasis:entry>
         <oasis:entry colname="col8">36.27</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Subantarctic<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">19.38</oasis:entry>
         <oasis:entry colname="col3">23.04</oasis:entry>
         <oasis:entry colname="col4">30.48</oasis:entry>
         <oasis:entry colname="col5">47.67</oasis:entry>
         <oasis:entry colname="col6">31.90</oasis:entry>
         <oasis:entry colname="col7">8.11</oasis:entry>
         <oasis:entry colname="col8">31.69</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Pacific</oasis:entry>
         <oasis:entry colname="col2">40.41</oasis:entry>
         <oasis:entry colname="col3">37.96</oasis:entry>
         <oasis:entry colname="col4">5.11</oasis:entry>
         <oasis:entry colname="col5">50.11</oasis:entry>
         <oasis:entry colname="col6">33.54</oasis:entry>
         <oasis:entry colname="col7">7.54</oasis:entry>
         <oasis:entry colname="col8">29.46</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Atlantic</oasis:entry>
         <oasis:entry colname="col2">19.88</oasis:entry>
         <oasis:entry colname="col3">19.72</oasis:entry>
         <oasis:entry colname="col4">23.81</oasis:entry>
         <oasis:entry colname="col5">26.40</oasis:entry>
         <oasis:entry colname="col6">17.67</oasis:entry>
         <oasis:entry colname="col7">5.88</oasis:entry>
         <oasis:entry colname="col8">22.97</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Indian</oasis:entry>
         <oasis:entry colname="col2">13.63</oasis:entry>
         <oasis:entry colname="col3">16.48</oasis:entry>
         <oasis:entry colname="col4">0.40</oasis:entry>
         <oasis:entry colname="col5">19.52</oasis:entry>
         <oasis:entry colname="col6">13.06</oasis:entry>
         <oasis:entry colname="col7">2.89</oasis:entry>
         <oasis:entry colname="col8">11.30</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e1623"><inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> For comparison with the Southern Ocean estimate, defined as <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M105" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S in <xref ref-type="bibr" rid="bib1.bibx30" id="text.46"/>. <inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> SubPol-PAC, SubPol-ATL and SubPol-IND.</p></table-wrap-foot></table-wrap>

      <?xmltex \floatpos{p}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e2751">Regional sensitivity  (<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>) of atmospheric <inline-formula><mml:math id="M149" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (ppm) to changes in Martin curves for the constant-export scheme <bold>(a, b)</bold> and nutrient-restoring scheme <bold>(c, d)</bold>. The sensitivity value reflects the increase in <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (preformed <inline-formula><mml:math id="M151" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) for an increase in <inline-formula><mml:math id="M152" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> (shallower remineralization). Error bars in panels <bold>(a)</bold> and <bold>(c)</bold> are 95 % confidence intervals for the linear regression coefficients. Atmospheric <inline-formula><mml:math id="M153" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is inferred from modelled preformed <inline-formula><mml:math id="M154" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> using empirical relationships in Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F7"/> in Appendix A.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f03.png"/>

        </fig>

      <p id="d1e2858">As with the globally uniform changes in <inline-formula><mml:math id="M155" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, the magnitudes of regional sensitivities are smaller when run using nutrient-restoring uptake as opposed to a constant-export scheme because export production is able to convert any increase in surface nutrient and carbon fluxes back into organic matter, limiting any change in <inline-formula><mml:math id="M156" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> fluxes. However, the relative sensitivity ranked across regions remains similar, as shown by expressing <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as a percentage of <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msub><mml:mo>∑</mml:mo><mml:mi>k</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Table <xref ref-type="table" rid="Ch1.T1"/>). Therefore, the regional patterns in Fig. <xref ref-type="fig" rid="Ch1.F3"/> are not sensitive to assumptions about the response of nutrient uptake to the redistribution of nutrients. This suggests that whilst the absolute magnitude of <inline-formula><mml:math id="M159" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity to changes in <inline-formula><mml:math id="M160" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is related to global export production, it is not driven by local changes in export production specific to any region(s).</p>
      <?pagebreak page2928?><p id="d1e2929"><xref ref-type="bibr" rid="bib1.bibx30" id="text.47"/> demonstrated that the sensitivity of <inline-formula><mml:math id="M161" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to basin-scale changes in <inline-formula><mml:math id="M162" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> correlated with the magnitude of export production in each basin. Similarly, we find a general positive correlation between sensitivity and regional export production  (<inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.79</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula> for constant export; <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.47</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula> for restoring uptake), as measured by the mean annual average export production across the 200 ensemble runs (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). The correlation is much weaker with nutrient-restoring uptake compared to the constant-export production. Intuitively, regions with lower export production, i.e. that contribute less to the inventory of regenerated <inline-formula><mml:math id="M167" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, have a smaller impact on the balance between preformed and regenerated nutrients and therefore on atmospheric <inline-formula><mml:math id="M168" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Whilst <inline-formula><mml:math id="M169" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is generally more sensitive to remineralization depths in regions with higher export production, sensitivity varies across regions with similar export production. For example, the sensitivity for the temperate North Pacific (NTemp-PAC; Fig. <xref ref-type="fig" rid="Ch1.F4"/>a) (<inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">13.72</mml:mn></mml:mrow></mml:math></inline-formula>, export production <inline-formula><mml:math id="M171" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn></mml:mrow></mml:math></inline-formula> Tmol P yr<inline-formula><mml:math id="M173" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is approximately double that of the subpolar region of the South Pacific (STemp-PAC; Fig. <xref ref-type="fig" rid="Ch1.F4"/>a) (<inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>b</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.72</mml:mn></mml:mrow></mml:math></inline-formula>, export production <inline-formula><mml:math id="M175" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.17</mml:mn></mml:mrow></mml:math></inline-formula> Tmol P yr<inline-formula><mml:math id="M177" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). There are no apparent relationships between the variability of export production across the ensemble in each region, as shown by the horizontal error bars, and sensitivity (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). This further supports the finding that the response of export production to changes in nutrient distributions are not an important factor in the sensitivity of <inline-formula><mml:math id="M178" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional changes in <inline-formula><mml:math id="M179" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e3174">Relationship between regional <inline-formula><mml:math id="M180" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity and annual export of <inline-formula><mml:math id="M181" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in each region using <bold>(a)</bold> the constant-export scheme and <bold>(b)</bold> the nutrient-restoring scheme. Annual export is shown as the mean of the 200 ensemble experiments with <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> standard deviation error bars.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f04.png"/>

        </fig>

      <p id="d1e3221">The variability in sensitivity not explained by the magnitude of POC export is likely a function of how changing remineralization depths interact with ocean circulation. To quantify this effect we calculate the mean preformed <inline-formula><mml:math id="M183" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the ocean interior derived from each region individually (<inline-formula><mml:math id="M184" display="inline"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>; see Appendix <xref ref-type="sec" rid="App1.Ch1.S1.SS2.SSS3"/>) and repeat the sensitivity regression analysis. In order to compare regression coefficients from different regions with significantly different magnitudes of <inline-formula><mml:math id="M185" display="inline"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> we first normalize the concentrations (<inline-formula><mml:math id="M186" display="inline"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>) to the range of variability across the 200 experiments:
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M187" display="block"><mml:mrow><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:mo>min⁡</mml:mo><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>max⁡</mml:mo><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mo>min⁡</mml:mo><mml:mo>(</mml:mo><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e3412">The new regression analysis (Eq. <xref ref-type="disp-formula" rid="Ch1.E4"/>) now predicts the contribution of changing <inline-formula><mml:math id="M188" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in all regions to the change in <inline-formula><mml:math id="M189" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover></mml:math></inline-formula> derived from a single region, rather than globally (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). The regression analysis is repeated for each region.
            <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M190" display="block"><mml:mrow><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">0</mml:mn><mml:mi>r</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>k</mml:mi></mml:munder><mml:msubsup><mml:mi mathvariant="italic">β</mml:mi><mml:mi>k</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:msub><mml:mi>b</mml:mi><mml:mi>k</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e3500">Figure <xref ref-type="fig" rid="Ch1.F5"/> shows the relative sensitivity of <inline-formula><mml:math id="M191" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover></mml:math></inline-formula> to changes in <inline-formula><mml:math id="M192" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> ranges from 0.82 to 0.97, suggesting that, overall, the linear regression models are appropriate. The regression coefficients specific to a single region are collected from across the 15 regression results in each column of Fig. <xref ref-type="fig" rid="Ch1.F5"/>. By definition, each row of Fig. <xref ref-type="fig" rid="Ch1.F5"/> shows the effect of changing <inline-formula><mml:math id="M194" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in the corresponding region on <inline-formula><mml:math id="M195" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover></mml:math></inline-formula> from all other regions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e3583">Sensitivity of steady-state normalized mean preformed [<inline-formula><mml:math id="M196" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] exported from each region (<inline-formula><mml:math id="M197" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula>). <inline-formula><mml:math id="M198" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula> from each region is expressed as a function of <inline-formula><mml:math id="M199" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> using linear regression.  <inline-formula><mml:math id="M200" display="inline"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> is normalized to the range of values within each region in the ensemble to account for large differences in preformed <inline-formula><mml:math id="M201" display="inline"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> between regions. The regression coefficients are arranged such that each row shows the impact of changing <inline-formula><mml:math id="M202" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in that region on <inline-formula><mml:math id="M203" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover></mml:math></inline-formula> across other regions. Panels <bold>(a)</bold> and <bold>(b)</bold> show the results for the constant-export and nutrient-restoring schemes, respectively.</p></caption>
          <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f05.png"/>

        </fig>

      <?pagebreak page2929?><p id="d1e3733">The sensitivity analysis for each region on an individual basis shows that changes in <inline-formula><mml:math id="M204" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in the subantarctic regions have large impacts on <inline-formula><mml:math id="M205" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover></mml:math></inline-formula> across regions globally (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). In particular, these regions have a particular effect on the <inline-formula><mml:math id="M206" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula> export in the Southern Ocean and in the Atlantic as a basin, comparable in magnitude to the local changes in <inline-formula><mml:math id="M207" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula>. Changes in <inline-formula><mml:math id="M208" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in the equatorial upwelling regions of the Pacific and Indian Oceans also have a large global effect but with a more pronounced local effect. These features are more pronounced with nutrient-restoring uptake (Fig. <xref ref-type="fig" rid="Ch1.F5"/>b). The Southern Ocean and North Atlantic regions are those with the highest <inline-formula><mml:math id="M209" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo stretchy="true" mathvariant="normal">^</mml:mo></mml:mover></mml:math></inline-formula> export across the ensemble (Table <xref ref-type="table" rid="Ch1.T1"/>), consistent with previous findings about the global importance of these regions for preformed <inline-formula><mml:math id="M210" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx44" id="paren.48"/>. This suggests the larger sensitivity of <inline-formula><mml:math id="M211" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to changes in <inline-formula><mml:math id="M212" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in the subantarctic regions is due to the way in which the ocean circulation connects these regions to the Southern Ocean and North Atlantic. In contrast, changing <inline-formula><mml:math id="M213" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in the Southern Ocean and North Atlantic has a relatively minimal effect on <inline-formula><mml:math id="M214" display="inline"><mml:mover accent="true"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi><mml:mi mathvariant="normal">region</mml:mi></mml:msubsup><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo mathvariant="normal" stretchy="true">^</mml:mo></mml:mover></mml:math></inline-formula> (and by inference <inline-formula><mml:math id="M215" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) both locally and globally.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Regional versus global sensitivity</title>
      <p id="d1e3931">Lastly, we explore whether the spatial patterns in sensitivity (Fig. <xref ref-type="fig" rid="Ch1.F3"/>) are significant on a global scale. Global average values of <inline-formula><mml:math id="M216" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> are calculated for each of the 200 Latin hypercube samples using an area-weighted mean and compared against experiments where <inline-formula><mml:math id="M217" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is perturbed uniformly across regions (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). The amount of organic matter reaching the deep ocean is a non-linear function of <inline-formula><mml:math id="M218" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, following from the fact that the Martin curve represents the scenario of a fixed remineralization rate and an increasing sinking rate (<xref ref-type="bibr" rid="bib1.bibx27 bib1.bibx2" id="altparen.49"/>; see Supplement). Therefore, larger values of <inline-formula><mml:math id="M219" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, i.e. shallower remineralization, have disproportionally more weight when calculating a global arithmetic mean of spatially variable <inline-formula><mml:math id="M220" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> values (Fig. S6). To account for this, we find the equivalent <inline-formula><mml:math id="M221" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> folding depths for each Latin hypercube sample, which form a skewed distribution due to higher occurrence of shallower remineralization, calculate the area-weighted geometric mean <inline-formula><mml:math id="M222" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> folding depth for each sample, and re-arrange again for <inline-formula><mml:math id="M223" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> (see Supplement for details).</p>
      <p id="d1e3998">The relationship between <inline-formula><mml:math id="M224" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and the globally averaged <inline-formula><mml:math id="M225" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> values from the sensitivity experiments closely matches the relationship between <inline-formula><mml:math id="M226" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and globally uniform <inline-formula><mml:math id="M227" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> for the both constant-export and nutrient-restoring schemes (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). Note that <inline-formula><mml:math id="M228" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> in each region is varied within the full parameter range but because Latin hypercube sampling varies all parameters across their parameter range simultaneously the global mean does not reach the highest and lowest global <inline-formula><mml:math id="M229" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> values. The average regionally varying <inline-formula><mml:math id="M230" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> values vary within <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>±</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula> ppm of the globally uniform experiments with constant-export experiments and <inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> ppm for the nutrient-restoring experiments, comparable to the change in <inline-formula><mml:math id="M233" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for a globally uniform change in <inline-formula><mml:math id="M234" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> of <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e4116">Comparison of <inline-formula><mml:math id="M236" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity when <inline-formula><mml:math id="M237" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is varied as a globally uniform parameter (solid lines) and when <inline-formula><mml:math id="M238" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is varied regionally in the Latin hypercube samples and calculated as an area-weighted geometric mean of <inline-formula><mml:math id="M239" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> folding depths converted back to <inline-formula><mml:math id="M240" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> to correct for non-linearities in the Martin curve. Runs using the constant-export scheme are shown in black and nutrient-restoring runs are shown in grey.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f06.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
      <?pagebreak page2930?><p id="d1e4173">Sediment trap observations reveal significant spatial variability in remineralization depths. Here we have quantified the sensitivity of atmospheric <inline-formula><mml:math id="M241" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional changes in remineralization depths and show that <inline-formula><mml:math id="M242" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is most sensitive to changes in the subantarctic regions. Much of the observed spatial variability varies across latitudes <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx14 bib1.bibx36 bib1.bibx51" id="paren.50"/>. Additionally, the mechanisms potentially driving these patterns are also likely to vary on a latitudinal basis, with changes in related environmental properties in response to anthropogenic <inline-formula><mml:math id="M243" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions affecting the high latitudes in particular: temperature changes <xref ref-type="bibr" rid="bib1.bibx26" id="paren.51"/> affecting temperature-dependent remineralization rates, a reduction in carbonate saturation state with ocean acidification <xref ref-type="bibr" rid="bib1.bibx42" id="paren.52"/> affecting ballasting and changes in plankton community composition, and cell size <xref ref-type="bibr" rid="bib1.bibx33" id="paren.53"/> affecting aggregation dynamics and particle sinking velocities. Additionally, this is a consideration for changes in remineralization depths occurring in past climates <xref ref-type="bibr" rid="bib1.bibx39" id="paren.54"/>. This suggests that the spatial patterns in <inline-formula><mml:math id="M244" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity could be significant when considering the impact of remineralization depth changes.</p>
      <p id="d1e4236">Changes in the air–sea balance of carbon are commonly related to changes in preformed nutrients. Because of the inefficient utilization of upwelled nutrients in the Southern Ocean, this region has been identified as key to setting the efficiency of the biological pump <xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx6" id="paren.55"/>. Our results show that this is also key for the sensitivity of <inline-formula><mml:math id="M245" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional variability in remineralization depths because of upwelling in subantarctic regions (Fig. <xref ref-type="fig" rid="Ch1.F5"/>). This relationship has implications when invoking changes in the efficiency of the biological pump in past climates such as the Last Glacial Maximum (LGM). Processes that increase the utilization of nutrients in the Southern Ocean, such as iron fertilization, and processes that reduce the delivery of nutrients to the Southern Ocean, such as increased stratification, have been implicated in the drawdown of atmospheric <inline-formula><mml:math id="M246" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> during the LGM <xref ref-type="bibr" rid="bib1.bibx50" id="paren.56"/>. Any changes in stratification will also impact the sensitivity of <inline-formula><mml:math id="M247" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to any additional changes in remineralization depths, such as from changes in ballasting minerals and/or temperature-dependent remineralization <xref ref-type="bibr" rid="bib1.bibx4" id="paren.57"/>. In comparison, processes such as iron fertilization will not impact on this sensitivity. Because the spatial patterns of <inline-formula><mml:math id="M248" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity to regional changes in remineralization are predominantly constrained by ocean circulation pathways, this also suggests that the sensitivity may change with a reorganization of ocean circulation as suggested for the LGM <xref ref-type="bibr" rid="bib1.bibx50" id="paren.58"/>.</p>
      <p id="d1e4298">The Martin curve is a commonly used parameterization of the remineralization of particulate organic matter with depth in marine biogeochemical models and is commonly applied with a globally uniform exponent (<inline-formula><mml:math id="M249" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx18" id="paren.59"/>. However, the Martin curve used in this way has potential limitations: it is an empirical and static parameterization that does not represent the mechanisms affecting remineralization and sinking rates and it does not capture spatial variability in remineralization observed in sediment trap data <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx36 bib1.bibx14" id="paren.60"/>. In our sensitivity analysis, we have shown that <inline-formula><mml:math id="M250" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> has a similar sensitivity to the global mean change in <inline-formula><mml:math id="M251" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula>, as compared to a globally uniform change in <inline-formula><mml:math id="M252" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> with an uncertainty of <inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>–15 ppm, equivalent to a change in <inline-formula><mml:math id="M254" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> of <inline-formula><mml:math id="M255" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula> (Fig. <xref ref-type="fig" rid="Ch1.F6"/>). <xref ref-type="bibr" rid="bib1.bibx30" id="text.61"/> suggest a decrease of 0.3 from the modern remineralization depth is sufficient to explain the increase in deep ocean nutrient concentrations during the Last Glacial Maximum. For the 21st century, <xref ref-type="bibr" rid="bib1.bibx32" id="text.62"/> predict a decrease in POC export at 500 m by 2100 under RCP8.5 in response to temperature- and oxygen-dependent remineralization, equivalent to a decrease in <inline-formula><mml:math id="M256" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> of <inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula>. As such, the global mean change in potential future and past changes in remineralization depth may be larger than the uncertainty associated with spatial variability. This has potentially useful implications for modelling the remineralization of particulate organic matter fluxes. Models resolving the various processes that affect remineralization rates and sinking velocities have recently been developed <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx5" id="paren.63"/>; however, the requirements to model processes such as particle aggregation can be computationally expensive, limiting their application to 1-D models <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx5" id="paren.64"/> or to offline models <xref ref-type="bibr" rid="bib1.bibx7" id="paren.65"/>. A globally uniform change in <inline-formula><mml:math id="M258" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> informed by these models could then be used to calculate the impact on atmospheric <inline-formula><mml:math id="M259" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> if the change in <inline-formula><mml:math id="M260" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is greater than 0.2. However, we note that the modern global mean <inline-formula><mml:math id="M261" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is subject to uncertainty associated with under-sampled spatial variability.</p>
      <?pagebreak page2931?><p id="d1e4435">Our results are dependent on the use of transport matrices derived from one global circulation model. Whilst this model has been widely applied to study biogeochemistry previously, it is subject to a number of caveats. The ocean model predicts significantly larger outcrops of dense water in the Southern Ocean compared to observations <xref ref-type="bibr" rid="bib1.bibx8" id="paren.66"><named-content content-type="pre">see Fig. S3 in Supplement, also</named-content></xref>, leading to deep-water formation occurring at latitudes around 50<inline-formula><mml:math id="M262" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S (Fig. S4 in Supplement). The volumetric fraction of water in the ocean interior derived from the subantarctic is also higher (26 %) compared to data-constrained estimates <xref ref-type="bibr" rid="bib1.bibx25" id="paren.67"><named-content content-type="pre">18 %, Table S1:</named-content></xref>. As such, the sensitivity estimates for the subantarctic may be overestimated. This is also consistent with the higher sensitivity compared to the basin-scale analysis of <xref ref-type="bibr" rid="bib1.bibx30" id="text.68"/>, who found that the Southern Ocean (<inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M264" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) contributed  22 % of the global <inline-formula><mml:math id="M265" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity, compared with 36 % in this study (<inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">38</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M267" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, see Table <xref ref-type="table" rid="Ch1.T1"/>). However, our results have key similarities, including absolute and relative magnitudes of regional preformed <inline-formula><mml:math id="M268" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> export, to other studies using alternative steady-state circulation states <xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx44" id="paren.69"/>. As such, our results should be broadly reproducible with other models. A disadvantage to using a steady-state circulation is that we cannot quantify impact of the <inline-formula><mml:math id="M269" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>–climate feedback on ocean circulation and atmospheric <inline-formula><mml:math id="M270" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Studies exploring the simultaneous effects of warming temperatures on circulation and biology in response to anthropogenic <inline-formula><mml:math id="M271" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions show that changes in circulation could be as important as biological changes (<xref ref-type="bibr" rid="bib1.bibx3" id="altparen.70"/>; <xref ref-type="bibr" rid="bib1.bibx53" id="altparen.71"/>). Quantifying the regional sensitivity with a dynamic ocean is therefore an important focus for future work. Ratios of <inline-formula><mml:math id="M272" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CaCO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to POC vary latitudinally, and could also therefore modify our sensitivity results. <xref ref-type="bibr" rid="bib1.bibx49" id="text.72"/> found important feedbacks involving interactions between calcifiers and silicifiers in an marine ecosystem model when exploring temperature-dependent remineralization rates in the 21st century. Future model experiments including a representation of plankton ecosystems would therefore help explore the impact of CaCO<inline-formula><mml:math id="M273" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> export on regional sensitivity patterns.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e4597">We have presented a sensitivity analysis that quantifies the sensitivity of atmospheric <inline-formula><mml:math id="M274" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to regional variability in particulate organic carbon remineralization depths. <inline-formula><mml:math id="M275" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is most sensitive to changes in remineralization depths occurring in the subantarctic regions, particularly in the Indian Ocean sector. As a whole, the subantarctic regions have a sensitivity similar to that of the Pacific basin despite the smaller area and levels of production. Sensitivity patterns are in part a function of the magnitude of export production in each region and the physical circulation pathways specific to each region. Whilst the overall magnitude of <inline-formula><mml:math id="M276" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sensitivity to regional changes is dependent on the magnitude and response of export production to changes in nutrients, the relative spatial patterns in sensitivity are predominantly constrained by ocean circulation pathways. We also find that the regional variability adds <inline-formula><mml:math id="M277" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>–15 ppm uncertainty to global mean changes in remineralization depths. The regional patterns in sensitivity could be significant if a number of processes that potentially drive changes in remineralization depths, including temperature-dependent remineralization rates and plankton community structure, vary predominantly in the high latitudes. However, this uncertainty is similar to the change in <inline-formula><mml:math id="M278" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for a globally uniform change in <inline-formula><mml:math id="M279" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> of <inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>, meaning that larger changes in <inline-formula><mml:math id="M281" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> could be reliably approximated by a globally uniform <inline-formula><mml:math id="M282" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> as commonly used in biogeochemical models.</p><?xmltex \hack{\newpage}?>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e4691">The transport matrices are publicly available at <uri>http://kelvin.earth.ox.ac.uk/spk/Research/TMM/TransportMatrixConfigs</uri> (<xref ref-type="bibr" rid="bib1.bibx23" id="altparen.73"/>). The model code is freely available at <uri>http://github.com/JamieDWilson/Fortran_Matrix_Lab</uri> (<xref ref-type="bibr" rid="bib1.bibx52" id="altparen.74"/>).</p>
  </notes><?xmltex \hack{\clearpage}?><app-group>

<?pagebreak page2932?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title>Model description</title>
      <p id="d1e4717">The Latin hypercube sampling approach used relies on the ability to run an ensemble of model experiments. To make this approach feasible we use the transport matrix method <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx22" id="paren.75"/>.</p>
<sec id="App1.Ch1.S1.SS1">
  <label>A1</label><title>Steady-state ocean circulation model</title>
      <p id="d1e4730">The matrix used here is the 2.8<inline-formula><mml:math id="M283" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> global configuration of the MIT model with 15 vertical levels driven by seasonally cycling fluxes of momentum, heat, and freshwater (publicly available from <uri>http://kelvin.earth.ox.ac.uk/spk/Research/TMM/TransportMatrixConfigs</uri>; last access: 29 July 2019). Seasonally varying ocean circulation is calculated at each time step by linearly interpolating between monthly mean matrices. An advantage of using transport matrices is that the time step can be made longer to reduce computational expense <xref ref-type="bibr" rid="bib1.bibx22" id="paren.76"/>. Here we extend the circulation time step to 3.8 d.</p>
</sec>
<sec id="App1.Ch1.S1.SS2">
  <label>A2</label><title>Biogeochemical model</title>
      <p id="d1e4756">The biogeochemical model represents the cycle of phosphorus and carbon in the ocean with four dissolved tracers, <inline-formula><mml:math id="M284" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, dissolved organic phosphorus (DOP), dissolved inorganic carbon (DIC), and total alkalinity. The biogeochemical model has the same time step as the ocean circulation model (3.8 d).</p>
<sec id="App1.Ch1.S1.SS2.SSS1">
  <label>A2.1</label><title>Phosphorus cycle</title>
      <p id="d1e4777"><inline-formula><mml:math id="M285" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and DOP are governed by the following equations:

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M286" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="App1.Ch1.S1.E5"><mml:mtd><mml:mtext>A1</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mi mathvariant="bold">A</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">up</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">POP</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">DOP</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="App1.Ch1.S1.E6"><mml:mtd><mml:mtext>A2</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="normal">dDOP</mml:mi><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mi mathvariant="bold">A</mml:mi><mml:mi mathvariant="normal">DOP</mml:mi><mml:mo>+</mml:mo><mml:mi>v</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">up</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">DOP</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M287" display="inline"><mml:mi mathvariant="bold">A</mml:mi></mml:math></inline-formula> denotes the transport matrix calculation of ocean transport and <inline-formula><mml:math id="M288" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> denotes biogeochemical source and sink terms.</p>
      <p id="d1e4910">The uptake of <inline-formula><mml:math id="M289" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> during production of organic matter occurs in the euphotic zone, here defined as the base of the upper two grid boxes (120 m). Following <xref ref-type="bibr" rid="bib1.bibx30" id="text.77"/> we calculate the production of organic matter using either a nutrient-restoring scheme or a constant-export scheme. The nutrient-restoring scheme restores surface concentrations of <inline-formula><mml:math id="M290" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to observed [<inline-formula><mml:math id="M291" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] with a restoring timescale <xref ref-type="bibr" rid="bib1.bibx41" id="paren.78"><named-content content-type="pre"><inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> d</named-content></xref> and is scaled by the fraction of sea ice present (<inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">seaice</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, as monthly average fields from the original global circulation model):
              <disp-formula id="App1.Ch1.S1.E7" content-type="numbered"><label>A3</label><mml:math id="M294" display="block"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">up</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi mathvariant="italic">τ</mml:mi></mml:mfrac></mml:mstyle><mml:mo movablelimits="false">max⁡</mml:mo><mml:mo mathsize="1.5em">(</mml:mo><mml:mo mathsize="1.1em">(</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>-</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">obs</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo mathsize="1.1em">)</mml:mo><mml:mo>,</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo mathsize="1.5em">)</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">seaice</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e5044">Organic matter production in the constant-export scheme is fixed to that of the experiment defined as the control run, unless surface [<inline-formula><mml:math id="M295" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] is depleted below zero, in which case <inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">up</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is set to zero at that time step. The control run is defined as having the run with the lowest root-mean-square misfit compared to annual mean World Ocean Atlas [<inline-formula><mml:math id="M297" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] observations.</p>
      <p id="d1e5080">A fixed fraction (<inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mi>v</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.66</mml:mn></mml:mrow></mml:math></inline-formula>) of the organic matter production integrated across the upper two grid boxes is routed directly to dissolved organic phosphorus (DOP) and remineralized back to <inline-formula><mml:math id="M299" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in a first-order reaction with a decay rate of <inline-formula><mml:math id="M300" display="inline"><mml:mi mathvariant="italic">κ</mml:mi></mml:math></inline-formula> throughout the water column:
              <disp-formula id="App1.Ch1.S1.E8" content-type="numbered"><label>A4</label><mml:math id="M301" display="block"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="normal">DOP</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">κ</mml:mi><mml:mi mathvariant="normal">DOP</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e5132">The remaining fraction of organic matter production (<inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi>v</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.34</mml:mn></mml:mrow></mml:math></inline-formula>) is integrated across the upper two grid boxes and exported as particulate organic phosphorus (POP) at the base of the of the second grid box in the vertical (120 m). The remineralization of POP is parameterized with the Martin curve (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>). POP that has reached the sediment is remineralized fully in the lowermost grid box of the water column, maintaining a closed system with respect to [<inline-formula><mml:math id="M303" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>]. As such, there is no sediment component in this model.</p>

      <?xmltex \floatpos{t}?><fig id="App1.Ch1.S1.F7"><?xmltex \currentcnt{A1}?><label>Figure A1</label><caption><p id="d1e5166">Relationship between preformed <inline-formula><mml:math id="M304" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and atmospheric <inline-formula><mml:math id="M305" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the biogeochemical model using nutrient-restoring and constant-export schemes when the Martin curve is varied globally between 0.4 and 1.6. A quadratic function (<inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mi mathvariant="normal">Δ</mml:mi><mml:msup><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">pre</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">pre</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) is fitted to the combined data with non-linear least squares is shown with 95 % confidence intervals. The coefficients for the two fits are <inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">66.59</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M308" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">22.48</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">187.09</mml:mn></mml:mrow></mml:math></inline-formula> for constant-export schemes and <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">42.80</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M311" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6.69</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M312" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">207.95</mml:mn></mml:mrow></mml:math></inline-formula> for nutrient-restoring schemes.</p></caption>
            <?xmltex \igopts{width=210.550394pt}?><graphic xlink:href="https://bg.copernicus.org/articles/16/2923/2019/bg-16-2923-2019-f07.png"/>

          </fig>

</sec>
<sec id="App1.Ch1.S1.SS2.SSS2">
  <label>A2.2</label><title>Carbon cycle</title>
      <?pagebreak page2933?><p id="d1e5365">The uptake of nutrients and remineralization of particulate and dissolved organic phosphorus are related to dissolved inorganic carbon and alkalinity via Redfield ratios of <inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">16</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">116</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M314" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">P</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">N</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula>). Carbonate chemistry parameters are computed from dissolved inorganic carbon and alkalinity using the method described by <xref ref-type="bibr" rid="bib1.bibx11" id="text.79"/>. The method provides a simplified but accurate solution with computational efficiency. The air–sea gas exchange of <inline-formula><mml:math id="M315" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is calculated as per <xref ref-type="bibr" rid="bib1.bibx43" id="text.80"/>.</p>
</sec>
<sec id="App1.Ch1.S1.SS2.SSS3">
  <label>A2.3</label><?xmltex \opttitle{Preformed {$\protect\chem{PO_{4}}$} and atmospheric {$\protect\chem{CO_{2}}$}}?><title>Preformed <inline-formula><mml:math id="M316" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and atmospheric <inline-formula><mml:math id="M317" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></title>
      <p id="d1e5447">Changes in atmospheric <inline-formula><mml:math id="M318" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> due to changes in the biological pump can be directly related to the inventory or average concentration of preformed <inline-formula><mml:math id="M319" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) if total nutrient concentrations are conserved <xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx35" id="paren.81"/>. This provides a way of relating changes in our model of the phosphorous cycle to changes in atmospheric <inline-formula><mml:math id="M321" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> without simulating a relatively computationally expensive carbon cycle. The distribution of annual mean [<inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>] for each run is calculated by splitting the transport matrices into “interior” matrices (<inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">A</mml:mi><mml:mi>I</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>) and “exterior” matrices (<inline-formula><mml:math id="M324" display="inline"><mml:mi mathvariant="bold">B</mml:mi></mml:math></inline-formula>) for both the explicit and implicit matrices (subscripts e and i, respectively; see <xref ref-type="bibr" rid="bib1.bibx22" id="altparen.82"/>). The annual mean surface [<inline-formula><mml:math id="M325" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] from the end of a simulation is set as a boundary condition and solved for the interior distribution of <inline-formula><mml:math id="M326" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>:
              <disp-formula id="App1.Ch1.S1.E9" content-type="numbered"><label>A5</label><mml:math id="M327" display="block"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msubsup><mml:mi mathvariant="bold">A</mml:mi><mml:mi mathvariant="normal">i</mml:mi><mml:mi>I</mml:mi></mml:msubsup><mml:msubsup><mml:mi mathvariant="bold">A</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mi>I</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mi>I</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mo>(</mml:mo><mml:msubsup><mml:mi mathvariant="bold">A</mml:mi><mml:mi mathvariant="normal">i</mml:mi><mml:mi>I</mml:mi></mml:msubsup><mml:msub><mml:mi mathvariant="bold">B</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="bold">B</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e5629"><?xmltex \hack{\newpage}?>The global mean concentration of <inline-formula><mml:math id="M328" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M329" display="inline"><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>) is related to <inline-formula><mml:math id="M330" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> using a empirical quadratic function (Eq. <xref ref-type="disp-formula" rid="App1.Ch1.S1.E10"/>) fitted to a series of experiments where the Martin curve is varied globally (see below). The function is derived from a non-linear least-squares regression (Fig. <xref ref-type="fig" rid="App1.Ch1.S1.F7"/>). The resulting regression fit (details in the caption of Fig. A1) is used to estimate changes in <inline-formula><mml:math id="M331" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>:
              <disp-formula id="App1.Ch1.S1.E10" content-type="numbered"><label>A6</label><mml:math id="M332" display="block"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msup><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mover accent="true"><mml:mrow><mml:mo>[</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e5757">The approach to predict <inline-formula><mml:math id="M333" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from regional changes in <inline-formula><mml:math id="M334" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is evaluated in the Supplement and shows the approach is robust to factors such as the slow timescale for the air–sea gas exchange of <inline-formula><mml:math id="M335" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx9" id="paren.83"><named-content content-type="pre">e.g.</named-content></xref>.</p><?xmltex \hack{\clearpage}?><supplementary-material position="anchor"><p id="d1e5795">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/bg-16-2923-2019-supplement" xlink:title="pdf">https://doi.org/10.5194/bg-16-2923-2019-supplement</inline-supplementary-material>.</p></supplementary-material>
</sec>
</sec>
</app>
  </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e5808">JDW designed the experiments, developed the model code, and ran the model. JDW prepared the manuscript with input from all co-authors.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e5814">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e5820">This work is based on research originally conducted as part of a PhD project (Jamie D. Wilson) associated with the UK Ocean Acidification Research Programme (UKOARP). We would like to thank Andrew Yool for his comments on the original research. We also thank Samar Khatiwala for making the transport matrices freely available.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e5825">This research has been supported by the Natural Environment Research Council (grant no. NE/H017240/1) and the European Research Council (PALEOGENIE grant no. 617313).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e5831">This paper was edited by Carol Robinson and reviewed by four anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><label>Boyd(2015)</label><mixed-citation>Boyd, P. W.: Toward quantifying the response of the oceans' biological pump to
climate change, Front. Mar. Sci., 2, 77,
<ext-link xlink:href="https://doi.org/10.3389/fmars.2015.00077" ext-link-type="DOI">10.3389/fmars.2015.00077</ext-link>,
2015.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Cael and Bisson(2018)</label><mixed-citation>Cael, B. B. and Bisson, K.: Particle Flux Parameterizations: Quantitative and
Mechanistic Similarities and Differences, Front. Mar. Sci., 5,
395, <ext-link xlink:href="https://doi.org/10.3389/fmars.2018.00395" ext-link-type="DOI">10.3389/fmars.2018.00395</ext-link>,
2018.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Cao and Zhang(2017)</label><mixed-citation>Cao, L. and Zhang, H.: The role of biological rates in the simulated warming
effect on oceanic <inline-formula><mml:math id="M336" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> uptake, J. Geophys. Res.-Biogeo., 122, 1098–1106, <ext-link xlink:href="https://doi.org/10.1002/2016JG003756" ext-link-type="DOI">10.1002/2016JG003756</ext-link>,  2017.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Chikamoto et al.(2012)</label><mixed-citation>Chikamoto, M. O., Abe-Ouchi, A., Oka, A., and Smith, S. L.: Temperature-induced
marine export production during glacial period, Geophys. Res. Lett.,
39, L21601, <ext-link xlink:href="https://doi.org/10.1029/2012GL053828" ext-link-type="DOI">10.1029/2012GL053828</ext-link>,  2012.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Cram et al.(2018)</label><mixed-citation>Cram, J. A., Weber, T., Leung, S. W., McDonnell, A. M. P., Liang, J.-H., and
Deutsch, C.: The Role of Particle Size, Ballast, Temperature, and Oxygen in
the Sinking Flux to the Deep Sea, Global Biogeochem. Cy., 32, 858–876,
<ext-link xlink:href="https://doi.org/10.1029/2017GB005710" ext-link-type="DOI">10.1029/2017GB005710</ext-link>,
2018.</mixed-citation></ref>
      <ref id="bib1.bibx6"><label>DeVries et al.(2012)</label><mixed-citation>DeVries, T., Primeau, F., and Deutsch, C.: The sequestration efficiency of the
biological pump, Geophys. Res. Lett., 39, l13601,
<ext-link xlink:href="https://doi.org/10.1029/2012GL051963" ext-link-type="DOI">10.1029/2012GL051963</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>DeVries et al.(2014)</label><mixed-citation>DeVries, T., Liang, J.-H., and Deutsch, C.: A mechanistic particle flux model applied to the oceanic phosphorus cycle, Biogeosciences, 11, 5381–5398, <ext-link xlink:href="https://doi.org/10.5194/bg-11-5381-2014" ext-link-type="DOI">10.5194/bg-11-5381-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Duteil et al.(2013)</label><mixed-citation>Duteil, O., Koeve, W., Oschlies, A., Bianchi, D., Galbraith, E., Kriest, I., and Matear, R.: A novel estimate of ocean oxygen utilisation points to a reduced rate of respiration in the ocean interior, Biogeosciences, 10, 7723–7738, <ext-link xlink:href="https://doi.org/10.5194/bg-10-7723-2013" ext-link-type="DOI">10.5194/bg-10-7723-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Eggleston and Galbraith(2018)</label><mixed-citation>Eggleston, S. and Galbraith, E. D.: The devil's in the disequilibrium: multi-component analysis of dissolved carbon and oxygen changes under a broad range of forcings in a general circulation model, Biogeosciences, 15, 3761–3777, <ext-link xlink:href="https://doi.org/10.5194/bg-15-3761-2018" ext-link-type="DOI">10.5194/bg-15-3761-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Fay and McKinley(2014)</label><mixed-citation>Fay, A. R. and McKinley, G. A.: Global open-ocean biomes: mean and temporal variability, Earth Syst. Sci. Data, 6, 273–284, <ext-link xlink:href="https://doi.org/10.5194/essd-6-273-2014" ext-link-type="DOI">10.5194/essd-6-273-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>Follows et al.(2006)</label><mixed-citation>Follows, M. J., Ito, T., and Dutkiewicz, S.: On the solution of the carbonate
chemistry system in ocean biogeochemistry models, Ocean Model., 12, 290–301, <ext-link xlink:href="https://doi.org/10.1016/j.ocemod.2005.05.004" ext-link-type="DOI">10.1016/j.ocemod.2005.05.004</ext-link>,
2006.</mixed-citation></ref>
      <ref id="bib1.bibx12"><label>Garcia et al.(2014)</label><mixed-citation>
Garcia, H. E., Locarnini, R. A., Boyer, T. P., Antonov, J. I., Baranova, O. K.,
Zweng, M. M., Reagan, J. R., and Johnson, D. R.: World Ocean Atlas
2013, Volume 4: Dissolved Inorganic Nutrients (phosphate, nitrate,
silicate)., in: NOAA Atlas NESDIS, edited by Levitus, S., U.S. Government
Printing Office, Washington, D.C., 2014.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>Gloor et al.(2001)</label><mixed-citation>Gloor, M., Gruber, N., Hughes, T. M. C., and Sarmiento, J. L.: Estimating net
air-sea fluxes from ocean bulk data: Methodology and application to the heat
cycle, Global Biogeochem. Cy., 15, 767–782,
<ext-link xlink:href="https://doi.org/10.1029/2000GB001301" ext-link-type="DOI">10.1029/2000GB001301</ext-link>,  2001.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>Guidi et al.(2015)</label><mixed-citation>Guidi, L., Legendre, L., Reygondeau, G., Uitz, J., Stemmann, L., and Henson,
S. A.: A new look at ocean carbon remineralization for estimating deepwater
sequestration, Global Biogeochem. Cy.,  29, 1044–1059,
<ext-link xlink:href="https://doi.org/10.1002/2014GB005063" ext-link-type="DOI">10.1002/2014GB005063</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx15"><label>Henson et al.(2012)</label><mixed-citation>Henson, S., Sanders, R., and Madsen, E.: Global patterns in efficiency of
particulate organic carbon export and transfer to the deep ocean, Global
Biogeochem. Cy., 26, GB1028, <ext-link xlink:href="https://doi.org/10.1029/2011GB004099" ext-link-type="DOI">10.1029/2011GB004099</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Henson et al.(2010)</label><mixed-citation>Henson, S. A., Sarmiento, J. L., Dunne, J. P., Bopp, L., Lima, I., Doney, S. C., John, J., and Beaulieu, C.: Detection of anthropogenic climate change in satellite records of ocean chlorophyll and productivity, Biogeosciences, 7, 621–640, <ext-link xlink:href="https://doi.org/10.5194/bg-7-621-2010" ext-link-type="DOI">10.5194/bg-7-621-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx17"><label>Henson et al.(2011)</label><mixed-citation>Henson, S. A., Sanders, R., Madsen, E., Morris, P. J., Le Moigne, F., and
Quartly, G. D.: A reduced estimate of the strength of the ocean's biological
carbon pump, Geophys. Res. Lett., 38, L04606,
<ext-link xlink:href="https://doi.org/10.1029/2011GL046735" ext-link-type="DOI">10.1029/2011GL046735</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx18"><?xmltex \def\ref@label{{H\"{u}lse et~al.(2017)}}?><label>Hülse et al.(2017)</label><mixed-citation>Hülse, D., Arndt, S., Wilson, J. D., Munhoven, G., and Ridgwell, A.:
Understanding the causes and consequences of past marine carbon cycling
variability through models, Earth-Sci. Rev., 171, 349–382,
<ext-link xlink:href="https://doi.org/10.1016/j.earscirev.2017.06.004" ext-link-type="DOI">10.1016/j.earscirev.2017.06.004</ext-link>,
2017.</mixed-citation></ref>
      <ref id="bib1.bibx19"><label>Ito and Follows(2005)</label><mixed-citation>Ito, T. and Follows, M. J.: Preformed phosphate, soft-tissue pump and
atmospheric <inline-formula><mml:math id="M337" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, J. Mar. Res., 64, 813–839, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx20"><label>John et al.(2014)</label><mixed-citation>John, E., Wilson, J., Pearson, P., and Ridgwell, A.: Temperature-dependent
remineralization and carbon cycling in the warm Eocene oceans,
Palaeogeogr. Palaeocl., 413, 158–166,
<ext-link xlink:href="https://doi.org/10.1016/j.palaeo.2014.05.019" ext-link-type="DOI">10.1016/j.palaeo.2014.05.019</ext-link>,
2014.</mixed-citation></ref>
      <ref id="bib1.bibx21"><label>Jokulsdottir and Archer(2016)</label><mixed-citation>Jokulsdottir, T. and Archer, D.: A stochastic, Lagrangian model of sinking biogenic aggregates in the ocean (SLAMS 1.0): model formulation, validation and sensitivity, Geosci. Model Dev., 9, 1455–1476, <ext-link xlink:href="https://doi.org/10.5194/gmd-9-1455-2016" ext-link-type="DOI">10.5194/gmd-9-1455-2016</ext-link>, 2016.</mixed-citation></ref>
      <?pagebreak page2935?><ref id="bib1.bibx22"><label>Khatiwala(2007)</label><mixed-citation>Khatiwala, S.: A computational framework for simulation of biogeochemical
tracers in the ocean, Global Biogeochem. Cy., 21, GB3001,
<ext-link xlink:href="https://doi.org/10.1029/2007GB002923" ext-link-type="DOI">10.1029/2007GB002923</ext-link>,  2007.</mixed-citation></ref>
      <ref id="bib1.bibx23"><label>Khatiwala(2019)</label><mixed-citation>Khatiwala, S.: University of Victoria Earth System Climate Model (ver. 2.9), available at: <uri>http://kelvin.earth.ox.ac.uk/spk/Research/TMM/TransportMatrixConfigs</uri>, last access: 29 July 2019.</mixed-citation></ref>
      <ref id="bib1.bibx24"><label>Khatiwala et al.(2005)Khatiwala, Visbeck, and Cane</label><mixed-citation>Khatiwala, S., Visbeck, M., and Cane, M. A.: Accelerated simulation of passive
tracers in ocean circulation models, Ocean Model., 9, 51–69,
<ext-link xlink:href="https://doi.org/10.1016/j.ocemod.2004.04.002" ext-link-type="DOI">10.1016/j.ocemod.2004.04.002</ext-link>,
2005.</mixed-citation></ref>
      <ref id="bib1.bibx25"><label>Khatiwala et al.(2012)</label><mixed-citation>Khatiwala, S., Primeau, F., and Holze, M.: Ventilation of the deep ocean
constrained with tracer observations and implications for radiocarbon
estimates of ideal mean age, Earth Planet. Sc. Lett., 325–326,
116–125, <ext-link xlink:href="https://doi.org/10.1016/j.epsl.2012.01.038" ext-link-type="DOI">10.1016/j.epsl.2012.01.038</ext-link>,
2012.</mixed-citation></ref>
      <ref id="bib1.bibx26"><label>Kirtman et al.(2013)</label><mixed-citation>
Kirtman, B., Power, S., Adedoyin, J., Boer, G., Bojariu, R., Camilloni, I.,
Doblas-Reyes, F., Fiore, A., Kimoto, M., Meehl, G., Prather, M., Sarr, A.,
Schar, C., Sutton, R., van Oldenborgh, G., Vecchi, G., and Wang, H.:
Near-term Climate Change: Projections and Predictability, in: Climate Change
2013: The Physical Science Basis. Contribution of Working Group I to the
Fifth Assessment Report of the Intergovernmental Panel on Climate Change,
edited by: Stocker, T., Qin, D., Plattner, G.-K., Tignor, M., Allen, S.,
Boschung, J., Nauels, A., Xia, Y., Bex, V., and Midgley, P., Cambridge
University Press, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx27"><label>Kriest and Oschlies(2008)</label><mixed-citation>Kriest, I. and Oschlies, A.: On the treatment of particulate organic matter sinking in large-scale models of marine biogeochemical cycles, Biogeosciences, 5, 55–72, <ext-link xlink:href="https://doi.org/10.5194/bg-5-55-2008" ext-link-type="DOI">10.5194/bg-5-55-2008</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx28"><label>Kriest and Oschlies(2015)</label><mixed-citation>Kriest, I. and Oschlies, A.: MOPS-1.0: towards a model for the regulation of the global oceanic nitrogen budget by marine biogeochemical processes, Geosci. Model Dev., 8, 2929–2957, <ext-link xlink:href="https://doi.org/10.5194/gmd-8-2929-2015" ext-link-type="DOI">10.5194/gmd-8-2929-2015</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx29"><label>Kriest et al.(2012)</label><mixed-citation>Kriest, I., Oschlies, A., and Khatiwala, S.: Sensitivity analysis of simple
global marine biogeochemical models, Global Biogeochem. Cy., 26,
GB2029, <ext-link xlink:href="https://doi.org/10.1029/2011GB004072" ext-link-type="DOI">10.1029/2011GB004072</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx30"><label>Kwon et al.(2009)</label><mixed-citation>Kwon, E. Y., Primeau, F., and Sarmiento, J. L.: The impact of remineralization
depth on the air-sea carbon balance, Nat. Geosci., 2, 630–635,
<ext-link xlink:href="https://doi.org/10.1038/ngeo612" ext-link-type="DOI">10.1038/ngeo612</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx31"><label>Lam et al.(2011)</label><mixed-citation>Lam, P. J., Doney, S. C., and Bishop, J. K. B.: The dynamic ocean biological
pump: Insights from a global compilation of particulate organic carbon,
<inline-formula><mml:math id="M338" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CaCO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and opal concentration profiles from the mesopelagic, Global
Biogeochem. Cy., 25, GB3009, <ext-link xlink:href="https://doi.org/10.1029/2010GB003868" ext-link-type="DOI">10.1029/2010GB003868</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx32"><?xmltex \def\ref@label{{Laufk\"{o}tter et~al.(2017)}}?><label>Laufkötter et al.(2017)</label><mixed-citation>Laufkötter, C., John, J. G., Stock, C. A., and Dunne, J. P.: Temperature
and oxygen dependence of the remineralization of organic matter, Global
Biogeochem. Cy., 31, 1038–1050, <ext-link xlink:href="https://doi.org/10.1002/2017GB005643" ext-link-type="DOI">10.1002/2017GB005643</ext-link>,  2017.</mixed-citation></ref>
      <ref id="bib1.bibx33"><label>Lefort et al.(2015)</label><mixed-citation>Lefort, S., Aumont, O., Bopp, L., Arsouze, T., Gehlen, M., and Maury, O.:
Spatial and body-size dependent response of marine pelagic communities to
projected global climate change, Global. Change Biol., 21, 154–164,
<ext-link xlink:href="https://doi.org/10.1111/gcb.12679" ext-link-type="DOI">10.1111/gcb.12679</ext-link>,
2015.</mixed-citation></ref>
      <ref id="bib1.bibx34"><label>Longhurst(1998)</label><mixed-citation>
Longhurst, A.: Ecological Geography of the Sea, Academic Press, San Diego,
1998.</mixed-citation></ref>
      <ref id="bib1.bibx35"><label>Marinov et al.(2008)</label><mixed-citation>Marinov, I., Gnanadesikan, A., Sarmiento, J. L., Toggweiler, J. R., Follows,
M., and Mignone, B. K.: Impact of oceanic circulation on biological carbon
storage in the ocean and atmospheric <inline-formula><mml:math id="M339" display="inline"><mml:mrow class="chem"><mml:mi>p</mml:mi><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, Global Biogeochem. Cy.,
22, GB3007, <ext-link xlink:href="https://doi.org/10.1029/2007GB002958" ext-link-type="DOI">10.1029/2007GB002958</ext-link>,  2008.</mixed-citation></ref>
      <ref id="bib1.bibx36"><label>Marsay et al.(2015)</label><mixed-citation>Marsay, C., Sanders, R., Henson, S., Pabortsava, K., Achterberg, E., and
Lampitt, R.: Attenuation of sinking particulate organic carbon flux through
the mesopelagic ocean, P. Natl. Acad. Sci. USA, 112,
1089–1094, <ext-link xlink:href="https://doi.org/10.1073/pnas.1415311112" ext-link-type="DOI">10.1073/pnas.1415311112</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bibx37"><label>Martin et al.(1987)</label><mixed-citation>
Martin, J., Knauer, G., Karl, D., and Broenkow, W.: VERTEX: carbon cycling in
the northeast Pacific, Deep-Sea Res., 43, 267–285, 1987.</mixed-citation></ref>
      <ref id="bib1.bibx38"><label>McKay et al.(1979)</label><mixed-citation>
McKay, M. D., Beckman, R. J., and Conover, W. J.: A Comparison of Three Methods
for Selecting Values of Input Variables in the Analysis of Output From a
Computer Code, Technometrics, 21, 239–245, 1979.</mixed-citation></ref>
      <ref id="bib1.bibx39"><label>Meyer et al.(2016)</label><mixed-citation>Meyer, K. M., Ridgwell, A., and Payne, J. L.: The influence of the biological
pump on ocean chemistry: implications for long-term trends in marine redox
chemistry, the global carbon cycle, and marine animal ecosystems, Geobiology,
14, 207–219, <ext-link xlink:href="https://doi.org/10.1111/gbi.12176" ext-link-type="DOI">10.1111/gbi.12176</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx40"><label>Mikaloff Fletcher et al.(2006)</label><mixed-citation>Mikaloff Fletcher, S. E., Gruber, N., Jacobson, A. R., Doney, S. C.,
Dutkiewicz, S., Gerber, M., Follows, M., Joos, F., Lindsay, K., Menemenlis,
D., Mouchet, A., Müller, S. A., and Sarmiento, J. L.: Inverse estimates
of anthropogenic <inline-formula><mml:math id="M340" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> uptake, transport, and storage by the ocean, Global
Biogeochem. Cy., 20, GB2002, <ext-link xlink:href="https://doi.org/10.1029/2005GB002530" ext-link-type="DOI">10.1029/2005GB002530</ext-link>,  2006.</mixed-citation></ref>
      <ref id="bib1.bibx41"><label>Najjar et al.(2007)</label><mixed-citation>Najjar, R. G., Jin, X., Louanchi, F., Aumont, O., Caldeira, K., Doney, S. C.,
Dutay, J.-C., Follows, M., Gruber, N., Joos, F., Lindsay, K., Maier-Reimer,
E., Matear, R. J., Matsumoto, K., Monfray, P., Mouchet, A., Orr, J. C.,
Plattner, G.-K., Sarmiento, J. L., Schlitzer, R., Slater, R. D., Weirig,
M.-F., Yamanaka, Y., and Yool, A.: Impact of circulation on export
production, dissolved organic matter, and dissolved oxygen in the ocean:
Results from Phase II of the Ocean Carbon-cycle Model
Intercomparison Project (OCMIP-2), Global Biogeochem. Cy., 21,
GB3007, <ext-link xlink:href="https://doi.org/10.1029/2006GB002857" ext-link-type="DOI">10.1029/2006GB002857</ext-link>,  2007.</mixed-citation></ref>
      <ref id="bib1.bibx42"><label>Orr et al.(2005)</label><mixed-citation>Orr, J. C., Fabry, V. J., Aumont, O., Bopp, L., Doney, S. C., Feely, R. A.,
Gnanadesikan, A., Gruber, N., Ishida, A., Joos, F., Key, R. M., Lindsay, K.,
Maier-Reimer, E., Matear, R., Monfray, P., Mouchet, A., Najjar, R. G.,
Plattner, G.-K., Rodgers, K. B., Sabine, C. L., Sarmiento, J. L., Schlitzer,
R., Slater, R. D., Totterdell, I. J., Weirig, M.-F., Yamanaka, Y., and Yool,
A.: Anthropogenic ocean acidification over the twenty-first century and its
impact on calcifying organisms, Nature, 437, 681–686,
<ext-link xlink:href="https://doi.org/10.1038/nature04095" ext-link-type="DOI">10.1038/nature04095</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx43"><label>Orr et al.(2017)</label><mixed-citation>Orr, J. C., Najjar, R. G., Aumont, O., Bopp, L., Bullister, J. L., Danabasoglu, G., Doney, S. C., Dunne, J. P., Dutay, J.-C., Graven, H., Griffies, S. M., John, J. G., Joos, F., Levin, I., Lindsay, K., Matear, R. J., McKinley, G. A., Mouchet, A., Oschlies, A., Romanou, A., Schlitzer, R., Tagliabue, A., Tanhua, T., and Yool, A.: Biogeochemical protocols and diagnostics for the CMIP6 Ocean Model Intercomparison Project (OMIP), Geosci. Model Dev., 10, 2169–2199, <ext-link xlink:href="https://doi.org/10.5194/gmd-10-2169-2017" ext-link-type="DOI">10.5194/gmd-10-2169-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx44"><label>Pasquier and Holzer(2016)</label><mixed-citation>Pasquier, B. and Holzer, M.: The plumbing of the global biological pump:
Efficiency control through leaks, pathways, and time scales, J.
Geophys. Res.-Oceans, 121, 6367–6388, <ext-link xlink:href="https://doi.org/10.1002/2016JC011821" ext-link-type="DOI">10.1002/2016JC011821</ext-link>,
2016.</mixed-citation></ref>
      <ref id="bib1.bibx45"><label>Pianosi et al.(2016)</label><mixed-citation>Pianosi, F., Beven, K., Freer, J., Hall, J. W., Rougier, J., Stephenson, D. B.,
and Wagener, T.: Sensitivity analysis of environmental models: A systematic
review with<?pagebreak page2936?> practical workflow, Environ. Modell. Softw., 79, 214–232, <ext-link xlink:href="https://doi.org/10.1016/j.envsoft.2016.02.008" ext-link-type="DOI">10.1016/j.envsoft.2016.02.008</ext-link>,
2016.</mixed-citation></ref>
      <ref id="bib1.bibx46"><label>Riebesell et al.(2009)</label><mixed-citation>Riebesell, U., Kortzinger, A., and Oschlies, A.: Sensitivities of marine carbon
fluxes to ocean change, P. Natl. Acad. Sci. USA, 106, 20602–20609,
<ext-link xlink:href="https://doi.org/10.1073/pnas.0813291106" ext-link-type="DOI">10.1073/pnas.0813291106</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx47"><label>Roth et al.(2014)</label><mixed-citation>Roth, R., Ritz, S. P., and Joos, F.: Burial-nutrient feedbacks amplify the sensitivity of atmospheric carbon dioxide to changes in organic matter remineralisation, Earth Syst. Dynam., 5, 321–343, <ext-link xlink:href="https://doi.org/10.5194/esd-5-321-2014" ext-link-type="DOI">10.5194/esd-5-321-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx48"><label>Sarmiento et al.(2004)</label><mixed-citation>Sarmiento, J. L., Slater, R., Barber, R., Bopp, L., Doney, S. C., Hirst, A. C.,
Kleypas, J., Matear, R., Mikolajewicz, U., Monfray, P., Soldatov, V., Spall,
S. A., and Stouffer, R.: Response of ocean ecosystems to climate warming,
Global Biogeochem. Cy., 18, GB3003, <ext-link xlink:href="https://doi.org/10.1029/2003GB002134" ext-link-type="DOI">10.1029/2003GB002134</ext-link>,  2004.</mixed-citation></ref>
      <ref id="bib1.bibx49"><label>Segschneider and Bendtsen(2013)</label><mixed-citation>Segschneider, J. and Bendtsen, J.: Temperature-dependent remineralization in a
warming ocean increases surface <inline-formula><mml:math id="M341" display="inline"><mml:mrow class="chem"><mml:mi>p</mml:mi><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> through changes in marine ecosystem
composition, Global Biogeochem. Cy., 27, 1214–1225,
<ext-link xlink:href="https://doi.org/10.1002/2013GB004684" ext-link-type="DOI">10.1002/2013GB004684</ext-link>,  2013.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bibx50"><label>Sigman et al.(2010)</label><mixed-citation>Sigman, D. M., Hain, M. P., and Haug, G. H.: The polar ocean and glacial cycles
in atmospheric <inline-formula><mml:math id="M342" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration, Nature, 466, 47–55,
<ext-link xlink:href="https://doi.org/10.1038/nature09149" ext-link-type="DOI">10.1038/nature09149</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx51"><label>Weber et al.(2016)</label><mixed-citation>
Weber, T., Cram, J., Leung, S., DeVries, T., and Deutsch, C.: Deep ocean
nutrients imply large latitudinal variation in particle transfer efficiency,
P. Natl. Acad. Sci. USA, 113, 8606–611, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx52"><label>Wilson(2019)</label><mixed-citation>Wilson, J. D.: Fortran_Matrix_Lab, available at: <uri>http://github.com/JamieDWilson/Fortran_Matrix_Lab</uri>, last access: 29 July 2019.</mixed-citation></ref>
      <ref id="bib1.bibx53"><label>Yamamoto et al.(2018)</label><mixed-citation>Yamamoto, A., Abe-Ouchi, A., and Yamanaka, Y.: Long-term response of oceanic carbon uptake to global warming via physical and biological pumps, Biogeosciences, 15, 4163–4180, <ext-link xlink:href="https://doi.org/10.5194/bg-15-4163-2018" ext-link-type="DOI">10.5194/bg-15-4163-2018</ext-link>, 2018.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Sensitivity of atmospheric CO<sub>2</sub> to regional variability in particulate organic matter remineralization depths</article-title-html>
<abstract-html><p>The concentration of CO<sub>2</sub> in the atmosphere is sensitive to changes in the depth at which sinking particulate organic matter is remineralized: often described as a change in the exponent <q><i>b</i></q> of the Martin curve. Sediment trap observations from deep and intermediate depths suggest there is a spatially heterogeneous pattern of <i>b</i>, particularly varying with latitude, but disagree over the exact spatial patterns. Here we use a biogeochemical model of the phosphorus cycle coupled with a steady-state representation of ocean circulation to explore the sensitivity of preformed phosphate and atmospheric CO<sub>2</sub> to spatial variability in remineralization depths. A Latin hypercube sampling method is used to simultaneously vary the Martin curve independently within 15 different regions, as a basis for a regression-based analysis used to derive a quantitative measure of sensitivity. Approximately 30&thinsp;% of the sensitivity of atmospheric CO<sub>2</sub> to changes in remineralization depths is driven by changes in the subantarctic region (36 to 60°&thinsp;S) similar in magnitude to the Pacific basin despite the much smaller area and lower export production. Overall, the absolute magnitude of sensitivity is controlled by export production, but the relative spatial patterns in sensitivity are predominantly constrained by ocean circulation pathways. The high sensitivity in the subantarctic regions is driven by a combination of high export production and the high connectivity of these regions to regions important for the export of preformed nutrients such as the Southern Ocean and North Atlantic. Overall, regionally varying remineralization depths contribute to variability in CO<sub>2</sub> of between around 5 and 15&thinsp;ppm, relative to a global mean change in remineralization depth. Future changes in the environmental and ecological drivers of remineralization, such as temperature and ocean acidification, are expected to be most significant in the high latitudes where CO<sub>2</sub> sensitivity to remineralization is also highest. The importance of ocean circulation pathways to the high sensitivity in subantarctic regions also has significance for past climates given the importance of circulation changes in the Southern Ocean.</p></abstract-html>
<ref-html id="bib1.bib1"><label>Boyd(2015)</label><mixed-citation>
Boyd, P. W.: Toward quantifying the response of the oceans' biological pump to
climate change, Front. Mar. Sci., 2, 77,
<a href="https://doi.org/10.3389/fmars.2015.00077" target="_blank">https://doi.org/10.3389/fmars.2015.00077</a>,
2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Cael and Bisson(2018)</label><mixed-citation>
Cael, B. B. and Bisson, K.: Particle Flux Parameterizations: Quantitative and
Mechanistic Similarities and Differences, Front. Mar. Sci., 5,
395, <a href="https://doi.org/10.3389/fmars.2018.00395" target="_blank">https://doi.org/10.3389/fmars.2018.00395</a>,
2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Cao and Zhang(2017)</label><mixed-citation>
Cao, L. and Zhang, H.: The role of biological rates in the simulated warming
effect on oceanic CO<sub>2</sub> uptake, J. Geophys. Res.-Biogeo., 122, 1098–1106, <a href="https://doi.org/10.1002/2016JG003756" target="_blank">https://doi.org/10.1002/2016JG003756</a>,  2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Chikamoto et al.(2012)</label><mixed-citation>
Chikamoto, M. O., Abe-Ouchi, A., Oka, A., and Smith, S. L.: Temperature-induced
marine export production during glacial period, Geophys. Res. Lett.,
39, L21601, <a href="https://doi.org/10.1029/2012GL053828" target="_blank">https://doi.org/10.1029/2012GL053828</a>,  2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Cram et al.(2018)</label><mixed-citation>
Cram, J. A., Weber, T., Leung, S. W., McDonnell, A. M. P., Liang, J.-H., and
Deutsch, C.: The Role of Particle Size, Ballast, Temperature, and Oxygen in
the Sinking Flux to the Deep Sea, Global Biogeochem. Cy., 32, 858–876,
<a href="https://doi.org/10.1029/2017GB005710" target="_blank">https://doi.org/10.1029/2017GB005710</a>,
2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>DeVries et al.(2012)</label><mixed-citation>
DeVries, T., Primeau, F., and Deutsch, C.: The sequestration efficiency of the
biological pump, Geophys. Res. Lett., 39, l13601,
<a href="https://doi.org/10.1029/2012GL051963" target="_blank">https://doi.org/10.1029/2012GL051963</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>DeVries et al.(2014)</label><mixed-citation>
DeVries, T., Liang, J.-H., and Deutsch, C.: A mechanistic particle flux model applied to the oceanic phosphorus cycle, Biogeosciences, 11, 5381–5398, <a href="https://doi.org/10.5194/bg-11-5381-2014" target="_blank">https://doi.org/10.5194/bg-11-5381-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Duteil et al.(2013)</label><mixed-citation>
Duteil, O., Koeve, W., Oschlies, A., Bianchi, D., Galbraith, E., Kriest, I., and Matear, R.: A novel estimate of ocean oxygen utilisation points to a reduced rate of respiration in the ocean interior, Biogeosciences, 10, 7723–7738, <a href="https://doi.org/10.5194/bg-10-7723-2013" target="_blank">https://doi.org/10.5194/bg-10-7723-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Eggleston and Galbraith(2018)</label><mixed-citation>
Eggleston, S. and Galbraith, E. D.: The devil's in the disequilibrium: multi-component analysis of dissolved carbon and oxygen changes under a broad range of forcings in a general circulation model, Biogeosciences, 15, 3761–3777, <a href="https://doi.org/10.5194/bg-15-3761-2018" target="_blank">https://doi.org/10.5194/bg-15-3761-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Fay and McKinley(2014)</label><mixed-citation>
Fay, A. R. and McKinley, G. A.: Global open-ocean biomes: mean and temporal variability, Earth Syst. Sci. Data, 6, 273–284, <a href="https://doi.org/10.5194/essd-6-273-2014" target="_blank">https://doi.org/10.5194/essd-6-273-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Follows et al.(2006)</label><mixed-citation>
Follows, M. J., Ito, T., and Dutkiewicz, S.: On the solution of the carbonate
chemistry system in ocean biogeochemistry models, Ocean Model., 12, 290–301, <a href="https://doi.org/10.1016/j.ocemod.2005.05.004" target="_blank">https://doi.org/10.1016/j.ocemod.2005.05.004</a>,
2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Garcia et al.(2014)</label><mixed-citation>
Garcia, H. E., Locarnini, R. A., Boyer, T. P., Antonov, J. I., Baranova, O. K.,
Zweng, M. M., Reagan, J. R., and Johnson, D. R.: World Ocean Atlas
2013, Volume 4: Dissolved Inorganic Nutrients (phosphate, nitrate,
silicate)., in: NOAA Atlas NESDIS, edited by Levitus, S., U.S. Government
Printing Office, Washington, D.C., 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Gloor et al.(2001)</label><mixed-citation>
Gloor, M., Gruber, N., Hughes, T. M. C., and Sarmiento, J. L.: Estimating net
air-sea fluxes from ocean bulk data: Methodology and application to the heat
cycle, Global Biogeochem. Cy., 15, 767–782,
<a href="https://doi.org/10.1029/2000GB001301" target="_blank">https://doi.org/10.1029/2000GB001301</a>,  2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Guidi et al.(2015)</label><mixed-citation>
Guidi, L., Legendre, L., Reygondeau, G., Uitz, J., Stemmann, L., and Henson,
S. A.: A new look at ocean carbon remineralization for estimating deepwater
sequestration, Global Biogeochem. Cy.,  29, 1044–1059,
<a href="https://doi.org/10.1002/2014GB005063" target="_blank">https://doi.org/10.1002/2014GB005063</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Henson et al.(2012)</label><mixed-citation>
Henson, S., Sanders, R., and Madsen, E.: Global patterns in efficiency of
particulate organic carbon export and transfer to the deep ocean, Global
Biogeochem. Cy., 26, GB1028, <a href="https://doi.org/10.1029/2011GB004099" target="_blank">https://doi.org/10.1029/2011GB004099</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Henson et al.(2010)</label><mixed-citation>
Henson, S. A., Sarmiento, J. L., Dunne, J. P., Bopp, L., Lima, I., Doney, S. C., John, J., and Beaulieu, C.: Detection of anthropogenic climate change in satellite records of ocean chlorophyll and productivity, Biogeosciences, 7, 621–640, <a href="https://doi.org/10.5194/bg-7-621-2010" target="_blank">https://doi.org/10.5194/bg-7-621-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Henson et al.(2011)</label><mixed-citation>
Henson, S. A., Sanders, R., Madsen, E., Morris, P. J., Le Moigne, F., and
Quartly, G. D.: A reduced estimate of the strength of the ocean's biological
carbon pump, Geophys. Res. Lett., 38, L04606,
<a href="https://doi.org/10.1029/2011GL046735" target="_blank">https://doi.org/10.1029/2011GL046735</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Hülse et al.(2017)</label><mixed-citation>
Hülse, D., Arndt, S., Wilson, J. D., Munhoven, G., and Ridgwell, A.:
Understanding the causes and consequences of past marine carbon cycling
variability through models, Earth-Sci. Rev., 171, 349–382,
<a href="https://doi.org/10.1016/j.earscirev.2017.06.004" target="_blank">https://doi.org/10.1016/j.earscirev.2017.06.004</a>,
2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Ito and Follows(2005)</label><mixed-citation>
Ito, T. and Follows, M. J.: Preformed phosphate, soft-tissue pump and
atmospheric CO<sub>2</sub>, J. Mar. Res., 64, 813–839, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>John et al.(2014)</label><mixed-citation>
John, E., Wilson, J., Pearson, P., and Ridgwell, A.: Temperature-dependent
remineralization and carbon cycling in the warm Eocene oceans,
Palaeogeogr. Palaeocl., 413, 158–166,
<a href="https://doi.org/10.1016/j.palaeo.2014.05.019" target="_blank">https://doi.org/10.1016/j.palaeo.2014.05.019</a>,
2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Jokulsdottir and Archer(2016)</label><mixed-citation>
Jokulsdottir, T. and Archer, D.: A stochastic, Lagrangian model of sinking biogenic aggregates in the ocean (SLAMS 1.0): model formulation, validation and sensitivity, Geosci. Model Dev., 9, 1455–1476, <a href="https://doi.org/10.5194/gmd-9-1455-2016" target="_blank">https://doi.org/10.5194/gmd-9-1455-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>Khatiwala(2007)</label><mixed-citation>
Khatiwala, S.: A computational framework for simulation of biogeochemical
tracers in the ocean, Global Biogeochem. Cy., 21, GB3001,
<a href="https://doi.org/10.1029/2007GB002923" target="_blank">https://doi.org/10.1029/2007GB002923</a>,  2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>Khatiwala(2019)</label><mixed-citation>
Khatiwala, S.: University of Victoria Earth System Climate Model (ver. 2.9), available at: <a href="http://kelvin.earth.ox.ac.uk/spk/Research/TMM/TransportMatrixConfigs" target="_blank">http://kelvin.earth.ox.ac.uk/spk/Research/TMM/TransportMatrixConfigs</a>, last access: 29 July 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Khatiwala et al.(2005)Khatiwala, Visbeck, and Cane</label><mixed-citation>
Khatiwala, S., Visbeck, M., and Cane, M. A.: Accelerated simulation of passive
tracers in ocean circulation models, Ocean Model., 9, 51–69,
<a href="https://doi.org/10.1016/j.ocemod.2004.04.002" target="_blank">https://doi.org/10.1016/j.ocemod.2004.04.002</a>,
2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Khatiwala et al.(2012)</label><mixed-citation>
Khatiwala, S., Primeau, F., and Holze, M.: Ventilation of the deep ocean
constrained with tracer observations and implications for radiocarbon
estimates of ideal mean age, Earth Planet. Sc. Lett., 325–326,
116–125, <a href="https://doi.org/10.1016/j.epsl.2012.01.038" target="_blank">https://doi.org/10.1016/j.epsl.2012.01.038</a>,
2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>Kirtman et al.(2013)</label><mixed-citation>
Kirtman, B., Power, S., Adedoyin, J., Boer, G., Bojariu, R., Camilloni, I.,
Doblas-Reyes, F., Fiore, A., Kimoto, M., Meehl, G., Prather, M., Sarr, A.,
Schar, C., Sutton, R., van Oldenborgh, G., Vecchi, G., and Wang, H.:
Near-term Climate Change: Projections and Predictability, in: Climate Change
2013: The Physical Science Basis. Contribution of Working Group I to the
Fifth Assessment Report of the Intergovernmental Panel on Climate Change,
edited by: Stocker, T., Qin, D., Plattner, G.-K., Tignor, M., Allen, S.,
Boschung, J., Nauels, A., Xia, Y., Bex, V., and Midgley, P., Cambridge
University Press, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Kriest and Oschlies(2008)</label><mixed-citation>
Kriest, I. and Oschlies, A.: On the treatment of particulate organic matter sinking in large-scale models of marine biogeochemical cycles, Biogeosciences, 5, 55–72, <a href="https://doi.org/10.5194/bg-5-55-2008" target="_blank">https://doi.org/10.5194/bg-5-55-2008</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>Kriest and Oschlies(2015)</label><mixed-citation>
Kriest, I. and Oschlies, A.: MOPS-1.0: towards a model for the regulation of the global oceanic nitrogen budget by marine biogeochemical processes, Geosci. Model Dev., 8, 2929–2957, <a href="https://doi.org/10.5194/gmd-8-2929-2015" target="_blank">https://doi.org/10.5194/gmd-8-2929-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Kriest et al.(2012)</label><mixed-citation>
Kriest, I., Oschlies, A., and Khatiwala, S.: Sensitivity analysis of simple
global marine biogeochemical models, Global Biogeochem. Cy., 26,
GB2029, <a href="https://doi.org/10.1029/2011GB004072" target="_blank">https://doi.org/10.1029/2011GB004072</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Kwon et al.(2009)</label><mixed-citation>
Kwon, E. Y., Primeau, F., and Sarmiento, J. L.: The impact of remineralization
depth on the air-sea carbon balance, Nat. Geosci., 2, 630–635,
<a href="https://doi.org/10.1038/ngeo612" target="_blank">https://doi.org/10.1038/ngeo612</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Lam et al.(2011)</label><mixed-citation>
Lam, P. J., Doney, S. C., and Bishop, J. K. B.: The dynamic ocean biological
pump: Insights from a global compilation of particulate organic carbon,
CaCO<sub>3</sub>, and opal concentration profiles from the mesopelagic, Global
Biogeochem. Cy., 25, GB3009, <a href="https://doi.org/10.1029/2010GB003868" target="_blank">https://doi.org/10.1029/2010GB003868</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>Laufkötter et al.(2017)</label><mixed-citation>
Laufkötter, C., John, J. G., Stock, C. A., and Dunne, J. P.: Temperature
and oxygen dependence of the remineralization of organic matter, Global
Biogeochem. Cy., 31, 1038–1050, <a href="https://doi.org/10.1002/2017GB005643" target="_blank">https://doi.org/10.1002/2017GB005643</a>,  2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Lefort et al.(2015)</label><mixed-citation>
Lefort, S., Aumont, O., Bopp, L., Arsouze, T., Gehlen, M., and Maury, O.:
Spatial and body-size dependent response of marine pelagic communities to
projected global climate change, Global. Change Biol., 21, 154–164,
<a href="https://doi.org/10.1111/gcb.12679" target="_blank">https://doi.org/10.1111/gcb.12679</a>,
2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Longhurst(1998)</label><mixed-citation>
Longhurst, A.: Ecological Geography of the Sea, Academic Press, San Diego,
1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Marinov et al.(2008)</label><mixed-citation>
Marinov, I., Gnanadesikan, A., Sarmiento, J. L., Toggweiler, J. R., Follows,
M., and Mignone, B. K.: Impact of oceanic circulation on biological carbon
storage in the ocean and atmospheric <i>p</i>CO<sub>2</sub>, Global Biogeochem. Cy.,
22, GB3007, <a href="https://doi.org/10.1029/2007GB002958" target="_blank">https://doi.org/10.1029/2007GB002958</a>,  2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Marsay et al.(2015)</label><mixed-citation>
Marsay, C., Sanders, R., Henson, S., Pabortsava, K., Achterberg, E., and
Lampitt, R.: Attenuation of sinking particulate organic carbon flux through
the mesopelagic ocean, P. Natl. Acad. Sci. USA, 112,
1089–1094, <a href="https://doi.org/10.1073/pnas.1415311112" target="_blank">https://doi.org/10.1073/pnas.1415311112</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Martin et al.(1987)</label><mixed-citation>
Martin, J., Knauer, G., Karl, D., and Broenkow, W.: VERTEX: carbon cycling in
the northeast Pacific, Deep-Sea Res., 43, 267–285, 1987.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>McKay et al.(1979)</label><mixed-citation>
McKay, M. D., Beckman, R. J., and Conover, W. J.: A Comparison of Three Methods
for Selecting Values of Input Variables in the Analysis of Output From a
Computer Code, Technometrics, 21, 239–245, 1979.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Meyer et al.(2016)</label><mixed-citation>
Meyer, K. M., Ridgwell, A., and Payne, J. L.: The influence of the biological
pump on ocean chemistry: implications for long-term trends in marine redox
chemistry, the global carbon cycle, and marine animal ecosystems, Geobiology,
14, 207–219, <a href="https://doi.org/10.1111/gbi.12176" target="_blank">https://doi.org/10.1111/gbi.12176</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Mikaloff Fletcher et al.(2006)</label><mixed-citation>
Mikaloff Fletcher, S. E., Gruber, N., Jacobson, A. R., Doney, S. C.,
Dutkiewicz, S., Gerber, M., Follows, M., Joos, F., Lindsay, K., Menemenlis,
D., Mouchet, A., Müller, S. A., and Sarmiento, J. L.: Inverse estimates
of anthropogenic CO<sub>2</sub> uptake, transport, and storage by the ocean, Global
Biogeochem. Cy., 20, GB2002, <a href="https://doi.org/10.1029/2005GB002530" target="_blank">https://doi.org/10.1029/2005GB002530</a>,  2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Najjar et al.(2007)</label><mixed-citation>
Najjar, R. G., Jin, X., Louanchi, F., Aumont, O., Caldeira, K., Doney, S. C.,
Dutay, J.-C., Follows, M., Gruber, N., Joos, F., Lindsay, K., Maier-Reimer,
E., Matear, R. J., Matsumoto, K., Monfray, P., Mouchet, A., Orr, J. C.,
Plattner, G.-K., Sarmiento, J. L., Schlitzer, R., Slater, R. D., Weirig,
M.-F., Yamanaka, Y., and Yool, A.: Impact of circulation on export
production, dissolved organic matter, and dissolved oxygen in the ocean:
Results from Phase II of the Ocean Carbon-cycle Model
Intercomparison Project (OCMIP-2), Global Biogeochem. Cy., 21,
GB3007, <a href="https://doi.org/10.1029/2006GB002857" target="_blank">https://doi.org/10.1029/2006GB002857</a>,  2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>Orr et al.(2005)</label><mixed-citation>
Orr, J. C., Fabry, V. J., Aumont, O., Bopp, L., Doney, S. C., Feely, R. A.,
Gnanadesikan, A., Gruber, N., Ishida, A., Joos, F., Key, R. M., Lindsay, K.,
Maier-Reimer, E., Matear, R., Monfray, P., Mouchet, A., Najjar, R. G.,
Plattner, G.-K., Rodgers, K. B., Sabine, C. L., Sarmiento, J. L., Schlitzer,
R., Slater, R. D., Totterdell, I. J., Weirig, M.-F., Yamanaka, Y., and Yool,
A.: Anthropogenic ocean acidification over the twenty-first century and its
impact on calcifying organisms, Nature, 437, 681–686,
<a href="https://doi.org/10.1038/nature04095" target="_blank">https://doi.org/10.1038/nature04095</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Orr et al.(2017)</label><mixed-citation>
Orr, J. C., Najjar, R. G., Aumont, O., Bopp, L., Bullister, J. L., Danabasoglu, G., Doney, S. C., Dunne, J. P., Dutay, J.-C., Graven, H., Griffies, S. M., John, J. G., Joos, F., Levin, I., Lindsay, K., Matear, R. J., McKinley, G. A., Mouchet, A., Oschlies, A., Romanou, A., Schlitzer, R., Tagliabue, A., Tanhua, T., and Yool, A.: Biogeochemical protocols and diagnostics for the CMIP6 Ocean Model Intercomparison Project (OMIP), Geosci. Model Dev., 10, 2169–2199, <a href="https://doi.org/10.5194/gmd-10-2169-2017" target="_blank">https://doi.org/10.5194/gmd-10-2169-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Pasquier and Holzer(2016)</label><mixed-citation>
Pasquier, B. and Holzer, M.: The plumbing of the global biological pump:
Efficiency control through leaks, pathways, and time scales, J.
Geophys. Res.-Oceans, 121, 6367–6388, <a href="https://doi.org/10.1002/2016JC011821" target="_blank">https://doi.org/10.1002/2016JC011821</a>,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Pianosi et al.(2016)</label><mixed-citation>
Pianosi, F., Beven, K., Freer, J., Hall, J. W., Rougier, J., Stephenson, D. B.,
and Wagener, T.: Sensitivity analysis of environmental models: A systematic
review with practical workflow, Environ. Modell. Softw., 79, 214–232, <a href="https://doi.org/10.1016/j.envsoft.2016.02.008" target="_blank">https://doi.org/10.1016/j.envsoft.2016.02.008</a>,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>Riebesell et al.(2009)</label><mixed-citation>
Riebesell, U., Kortzinger, A., and Oschlies, A.: Sensitivities of marine carbon
fluxes to ocean change, P. Natl. Acad. Sci. USA, 106, 20602–20609,
<a href="https://doi.org/10.1073/pnas.0813291106" target="_blank">https://doi.org/10.1073/pnas.0813291106</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Roth et al.(2014)</label><mixed-citation>
Roth, R., Ritz, S. P., and Joos, F.: Burial-nutrient feedbacks amplify the sensitivity of atmospheric carbon dioxide to changes in organic matter remineralisation, Earth Syst. Dynam., 5, 321–343, <a href="https://doi.org/10.5194/esd-5-321-2014" target="_blank">https://doi.org/10.5194/esd-5-321-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Sarmiento et al.(2004)</label><mixed-citation>
Sarmiento, J. L., Slater, R., Barber, R., Bopp, L., Doney, S. C., Hirst, A. C.,
Kleypas, J., Matear, R., Mikolajewicz, U., Monfray, P., Soldatov, V., Spall,
S. A., and Stouffer, R.: Response of ocean ecosystems to climate warming,
Global Biogeochem. Cy., 18, GB3003, <a href="https://doi.org/10.1029/2003GB002134" target="_blank">https://doi.org/10.1029/2003GB002134</a>,  2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>Segschneider and Bendtsen(2013)</label><mixed-citation>
Segschneider, J. and Bendtsen, J.: Temperature-dependent remineralization in a
warming ocean increases surface <i>p</i>CO<sub>2</sub> through changes in marine ecosystem
composition, Global Biogeochem. Cy., 27, 1214–1225,
<a href="https://doi.org/10.1002/2013GB004684" target="_blank">https://doi.org/10.1002/2013GB004684</a>,  2013.

</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>Sigman et al.(2010)</label><mixed-citation>
Sigman, D. M., Hain, M. P., and Haug, G. H.: The polar ocean and glacial cycles
in atmospheric CO<sub>2</sub> concentration, Nature, 466, 47–55,
<a href="https://doi.org/10.1038/nature09149" target="_blank">https://doi.org/10.1038/nature09149</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>Weber et al.(2016)</label><mixed-citation>
Weber, T., Cram, J., Leung, S., DeVries, T., and Deutsch, C.: Deep ocean
nutrients imply large latitudinal variation in particle transfer efficiency,
P. Natl. Acad. Sci. USA, 113, 8606–611, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>Wilson(2019)</label><mixed-citation>
Wilson, J. D.: Fortran_Matrix_Lab, available at: <a href="http://github.com/JamieDWilson/Fortran_Matrix_Lab" target="_blank">http://github.com/JamieDWilson/Fortran_Matrix_Lab</a>, last access: 29 July 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>Yamamoto et al.(2018)</label><mixed-citation>
Yamamoto, A., Abe-Ouchi, A., and Yamanaka, Y.: Long-term response of oceanic carbon uptake to global warming via physical and biological pumps, Biogeosciences, 15, 4163–4180, <a href="https://doi.org/10.5194/bg-15-4163-2018" target="_blank">https://doi.org/10.5194/bg-15-4163-2018</a>, 2018.
</mixed-citation></ref-html>--></article>
