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  <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-15-7111-2018</article-id><title-group><article-title>Pacific Decadal Oscillation and recent oxygen decline in the eastern
tropical Pacific Ocean</article-title><alt-title>Pacific Decadal Oscillation and recent oxygen decline</alt-title>
      </title-group><?xmltex \runningtitle{Pacific Decadal Oscillation and recent oxygen decline}?><?xmltex \runningauthor{O. Duteil et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Duteil</surname><given-names>Olaf</given-names></name>
          <email>oduteil@geomar.de</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Oschlies</surname><given-names>Andreas</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Böning</surname><given-names>Claus W.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6251-5777</ext-link></contrib>
        <aff id="aff1"><institution>GEOMAR – Helmholtz Centre for Ocean Research Kiel,
Düsternbrooker Weg. 20, 24103 Kiel, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Olaf Duteil (oduteil@geomar.de)</corresp></author-notes><pub-date><day>29</day><month>November</month><year>2018</year></pub-date>
      
      <volume>15</volume>
      <issue>23</issue>
      <fpage>7111</fpage><lpage>7126</lpage>
      <history>
        <date date-type="received"><day>10</day><month>January</month><year>2018</year></date>
           <date date-type="rev-request"><day>19</day><month>January</month><year>2018</year></date>
           <date date-type="rev-recd"><day>8</day><month>October</month><year>2018</year></date>
           <date date-type="accepted"><day>10</day><month>October</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <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/15/7111/2018/bg-15-7111-2018.html">This article is available from https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018.html</self-uri><self-uri xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018.pdf">The full text article is available as a PDF file from https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018.pdf</self-uri>
      <abstract>
    <p id="d1e95">The impact of the positive and negative phases of the Pacific Decadal
Oscillation (PDO) on the extension of the poorly oxygenated regions of the
eastern Pacific Ocean was assessed using a coupled ocean
circulation–biogeochemical model. We show that during a “typical”
PDO-positive phase the volume of the suboxic regions expands by 7 % over 50
years due to a slowdown of the large-scale circulation related to the
decrease in the intensity of the trade winds. Changes in oxygen levels are
mostly controlled by advective processes between 10<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and
10<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, whereas diffusive processes are dominant poleward of
10<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>: in a “typical” PDO-positive phase the sluggish equatorial
current system provides less oxygen to the eastern equatorial part of the
basin while the oxygen transport by diffusive processes significantly
decreases south of 10<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. The suboxic region located north of
10<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N displays less sensitivity to the phase of the PDO as the
local upwelling-related processes play a dominant role compared to the
large-scale circulation in setting the oxygen concentration. Our study
suggests that the prevailing PDO-positive conditions since 1975 may explain a
significant part of the current deoxygenation occurring in the eastern
Pacific Ocean.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e150">Oxygen is one of the most important chemical elements in the ocean, as
marine organisms ranging from microorganisms to vertebrates use it for
respiration. Its concentration is regulated by both circulation and
biogeochemical processes. In general, high-latitude regions are
characterized by high oxygen concentrations, whereas subsurface tropical
regions are poorly oxygenated. Particularly in the eastern parts of the
tropical oceans, the large export of organic material out of productive
surface layers combined with sluggish circulation depletes oxygen levels
at depth, resulting in the formation of large suboxic regions where the
oxygen concentration falls below 20 mmol m<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Karstensen et al., 2008).
The overall contrast between high latitudes and tropical shadow zones is
generally well reproduced by ocean models (Bopp et al., 2013; Cocco et al.,
2013; Cabré et al., 2015; Shigemitsu et al., 2017).</p>
      <p id="d1e165">The temporal variability of oxygen concentrations in the ocean interior is,
nevertheless, still poorly understood; this is particularly true for the eastern tropical
Pacific Ocean, where oxygen concentrations are among the lowest in the world
(Karstensen et al., 2008). A strong decrease in oxygen concentrations in
these regions has been inferred from observations ranging from the 1960s to the
2000s (Stramma et al., 2008, 2012; Schmidtko et al., 2017). This
deoxygenation is not correctly reproduced by current ocean models (Oschlies
et al., 2017). It is not clear whether the changes in oxygen concentration
are due to anthropogenic changes (Matear et al., 2003; Long et al., 2016;
Ito et al., 2017), or are related to natural low-frequency climate
oscillations such as the Pacific Decadal Oscillation (PDO) (Deutsch et al.,
2014), which is a robust and recurring pattern of ocean atmosphere climate
variability centered over the midlatitude north Pacific basin (Mantua et
al., 1997).</p>
      <p id="d1e168">The stronger trade winds that occur during a negative phase of the PDO cause
a shoaling of the eastern thermocline of the tropical and subtropical
Pacific Ocean (Miller et al., 1994) (see the Supplement Fig. S1 for an
overview of the mechanisms controlling the oxygen levels in the eastern
tropical Pacific Ocean). Deutsch et al. (2011, 2014) showed that the depth of the
thermocline regulates the oxygen<?pagebreak page7112?> levels in the northeastern subtropical
Pacific Ocean. In these regions, a shallower thermocline fosters low oxygen
concentrations in the intermediate ocean as a larger amount of organic
material is respired below the mixed layer (Deutsch et al., 2011).
Simultaneously, in the tropical regions the zonal volume transport by the
equatorial current system increases during a negative PDO event as does the
meridional transport by the subtropical cells (STCs) (Hong et al., 2014),
which connect the subtropics to the tropics (McCreary and Lu, 1994). The
variability of the strength of the STCs forces the variability of the oxygen
transport in the upper thermocline of the equatorial Pacific Ocean (Duteil
et al., 2014a). Therefore, competition takes place between the increased oxygen
transport and the increased respiration as primary production is enhanced by
the increased nutrient supply. Finally, stronger trade winds also increase
the subduction volume of the North Pacific
Eastern Subtropical Mode Water (Qu et al., 2009) and the South Pacific
Eastern Subtropical Mode Water (Luo et al., 2011).
A subtropical increase
in productivity related to an increase in the trade winds causes a negative
oxygen anomaly in these mode waters, which is transported equatorward and
leads to a delayed oxygen decrease in tropical regions as shown by Ridder
and England (2014) in an Earth system model of intermediate complexity.</p>
      <p id="d1e171">All of these studies highlight the potential effect of the PDO on oxygen
concentrations and show that the processes at play are diverse and strongly
region dependent. However, we still do not have a clear picture of the
impact of the PDO on the suboxic regions and on the oxygen levels of the
eastern Pacific Ocean. Indeed, the studies cited above focus either
specifically on the suboxic regions of the northeastern Pacific region
(Deutsch et al., 2011, 2014) or on the upper thermocline of the tropical
Pacific Ocean (Duteil et al., 2014a). A caveat of the model used by Ridder
and England (2014) is that the equatorial undercurrent (EUC) is poorly represented,
as is the case for most coarse-resolution (lower than 0.5<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
at the equator) models (Karnauskas et al., 2012). The EUC indeed ventilates
the suboxic regions, as shown by Cabre et al. (2015) and Shigemitsu et al. (2017)
in a range of models as part of the Coupled Model Intercomparison
Project 5 (CMIP5).</p>
      <p id="d1e184">A precise understanding of the role of the PDO in setting oxygen levels is
difficult in “traditional” 50-year hindcasts experiments (Deutsch et
al., 2011; Ito and Deutsch, 2013; Duteil et al., 2014a) due to the superposition of
a long-term climate trend and higher-frequency climate oscillations such as
the El Niño–Southern Oscillation (ENSO) (Ito and Deutsch, 2013, 2016; Eddebbar et
al., 2017). Ito and Deutsch (2013) showed that the temporal spectrum of oxygen
concentrations in the northeastern tropical Pacific Ocean is characterized
by a strong decadal variance which may partly arise from the “reddening” of
the variability spectrum of the physical and biological drivers (Ito and
Deutsch, 2010), suggesting, e.g., a contribution of ENSO to the decadal
oxygen variability, in addition to the PDO.</p>
      <p id="d1e187">Rather than performing a “hindcast” experiment, in this study we specifically
isolate and assess the role of the phase of the PDO on the oxygen levels in
the tropical eastern Pacific Ocean by forcing a coupled circulation–biogeochemical model using “typical” conditions characteristic of the
negative and positive PDO phases. These idealized atmospheric forcings are
derived from monthly averages of realistic winds and heat fluxes from the 1948–2007 COREv2 dataset (Large and Yeager, 2009). Our aim is to understand
whether and by which processes (oxygen advection, diffusion, respiration)
the PDO may be responsible for the observed oxygen decline in the suboxic
regions of the tropical eastern Pacific Ocean.</p>
      <p id="d1e190">This paper is organized as follows. Section 2 describes the construction
of the “typical” PDO forcings and the configuration of the experiments
that we perform. In Sect. 3, we assess the basin-scale circulation of our
experiments. In Sect. 4, we present the difference in oxygen levels
between a “typical” positive and a “typical” negative PDO phase. The mechanisms
regulating the oxygen levels are described in Sect. 5. Temporal aspects
are discussed in Sect. 6. In Sect. 7 we discuss the changes in the
upwelling systems and the impact on suboxia. We then summarize our results in
Sect. 8.</p>
</sec>
<sec id="Ch1.S2">
  <title>Forcings and experiments</title>
      <p id="d1e199">The NEMO ocean model version v3.6 (Madec, 2008) was used in the
standard ORCA2 configuration. This configuration has been widely used in
previous studies and constitutes the ocean component of the ISPL-CM5A model,
which is part of the Coupled Model Intercomparison Project (CMIP5) effort (Dufresnes
et al., 2013). Its zonal resolution is 2 degrees. The mean meridional
resolution is 2 degrees outside the tropics and increases to 0.5 degrees
close to the Equator. The resolution of ORCA2 is sufficient to realistically
reproduce the EUC (Cravatte et al., 2007) and the subtropical–tropical
connectivity (Luebbecke et al., 2008). The circulation model has been
coupled to a six-compartment (nutrient, phytoplankton, zooplankton,
particulates and dissolved detritus, oxygen) biogeochemical model. This
model is described in detail by Kriest et al. (2010). It was adapted to the NEMO framework by
Duteil et al. (2014a, b).</p>
      <p id="d1e202">We constructed three atmospheric forcing datasets derived from the interannual
1948–2007 COREv2, 6 h temporal resolution, forcing dataset (Large and
Yeager, 2009):
<list list-type="bullet"><list-item>
      <p id="d1e207">MEAN: (1) a low-pass filter was applied to remove the frequencies
with a period shorter than 1 month. (2) The long term trend 1948–2007
(Yang et al., 2016) was removed. (3) The corresponding time steps of the
individual annual forcings for the 1948–2007 period were averaged to
reconstruct a climatological annually cycling forcing set. The difference
between MEAN and the COREv2 “normal year” is the absence of high-frequency
variability (<inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mi mathvariant="italic">&lt;</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> month) and the removal of<?pagebreak page7113?> the long-term trend
implicitly contained in the “normal year”.</p></list-item><list-item>
      <p id="d1e221">PDO_PLUS (PDO_MINUS): steps (1) and (2)
are similar to the first two steps mentioned above. In PDO_PLUS (PDO_MINUS),
the corresponding time step of the years characterized by a positive
(negative) PDO phase (Fig. 1a) were averaged, leading to the
reconstruction of a 1 year, 6 h temporal resolution, climatological forcing
“typical” of a PDO-positive (negative) phase.</p></list-item></list></p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e226"><bold>(a)</bold> Pacific Decadal Oscillation (PDO) index (1900–2017 annual averages; data from the “Joint Institute for the Study of the Atmosphere
and Ocean – University of Washington, USA:
<uri>http://research.jisao.washington.edu/data_sets/pdo</uri>). The
1948–2007 period has been highlighted (blue/red); the contour line is the smoothed
PDO index (20-year running mean). <bold>(b)</bold> Average of the zonal 10 m wind
component (m s<inline-formula><mml:math id="M9" 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>) of the PDO positive (PDO_PLUS
experiment) phase minus the PDO negative phase (PDO_MINUS
experiment). The contour is the zonal wind component average (m s<inline-formula><mml:math id="M10" 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>)
1948–2007. <bold>(c)</bold> Average of the meridional wind component (m s<inline-formula><mml:math id="M11" 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>) of the
PDO positive phase (PDO_PLUS experiment) minus the PDO negative
phase (PDO_MINUS experiment). The contour is the meridional wind
component average (m s<inline-formula><mml:math id="M12" 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>) 1948–2007. <bold>(d)</bold> Average of the 10 m air
temperature (<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) of the PDO positive phase (PDO_PLUS experiment) minus the PDO negative phase (PDO_MINUS
experiment). The contour is the average of the 10 m air temperature (<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)
1948–2007. <bold>(e)</bold> Difference between the barotropic streamfunction
(BSf) for PDO_PLUS and PDO_MINUS (Sv). The black contour represents
PDO_MINUS BSf, and the red contour represents PDO_PLUS BSf. The
sense of rotation is clockwise for positive values. <bold>(f)</bold> Difference between
the sea surface height (SSH) for PDO_PLUS and PDO_MINUS (m).
The black contour represents PDO_MINUS SSH, and the red contour represents PDO_PLUS SSH.
<bold>(g)</bold> Difference between the meridional overturning
(MOC) for PDO_PLUS and PDO_MINUS (Sv). The black
contour represents PDO_MINUS MOC, and the red contour represents PDO_PLUS MOC. The sense of rotation is clockwise for positive values. All
the of the differences between PDO_PLUS and PDO_MINUS are
averaged over 50 years of integration time.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f01.png"/>

      </fig>

      <p id="d1e326">In PDO_PLUS the zonal wind speed decreases by about 0.2 to
0.5 ms<inline-formula><mml:math id="M15" 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> compared to MEAN in the mid-equatorial Pacific Ocean, where
the winds are strongest (at least 8 ms<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (Fig. 1b). It increases
close to the eastern coast by up to 0.3 ms<inline-formula><mml:math id="M17" 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>, where the winds are
weaker (2 to 8 ms<inline-formula><mml:math id="M18" 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>). A similar pattern was described by both
Merrifield et al. (2012) and Zhou et al. (2017). The meridional wind speed
decreases by about 0.2 ms<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> (Fig. 1c). The 10 m air temperature
increases by 0.1 to 0.3 <inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in the eastern Pacific Ocean and
decreases in the gyres (Fig. 1d). PDO_MINUS presents the
opposite pattern.</p>
      <p id="d1e400">We spun up the model over 1000 years using the MEAN forcing dataset. We
subsequently performed two experiments using the
PDO_PLUS and PDO_MINUS forcing datasets, respectively, which we
integrated for a period of 50 years: this integration period corresponds to the typical
oscillation period of the PDO over the past 200 years (Mc Donald and Case,
2005).</p>
</sec>
<sec id="Ch1.S3">
  <title>Basin-scale circulation</title>
<sec id="Ch1.S3.SS1">
  <title>Gyres</title>
      <p id="d1e414">The subtropical gyres (STG) slow down and extend equatorward in
PDO_PLUS, constraining the tropical gyres (TG) (Fig. 1e). The
slowdown reaches up to 5 Sv (or 5 %–10 %). These results are consistent
with those from Messie and Chavez (2011), who analyzed the variability of the
Extended Reconstruction Sea Surface Temperature (1910–2010) product
(Smith et al., 2008) and showed that the intensity of the northern and
southern Pacific subtropical gyres decreases during a positive PDO event
(their Fig. 10). The thermocline depth shoals in PDO_PLUS in
the STG and deepens in the eastern tropical part of the basin, correlated
with a rise in sea level (Fig. 1f). The large signal observed at
10<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N is related to the extension of the STG. The passive
adjustment time of the ocean (without considering ocean–atmosphere
feedbacks) is quick (a few years), which is coherent with previous studies
(Zhang and Delworth, 2015; Deser et al., 1999; Hong et al., 2014).</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Meridional overturning</title>
      <p id="d1e433">The shallow meridional overturning is characterized by the presence of the
STCs (Fig. 1g). These cells are shallow (upper 500 m) structures
connecting the subtropical and tropical regions (McCreary and Lu, 1994) and
respond to a change in wind stress by baroclinic adjustment (Hong et al.,
2014). The strength of the STCs (and therefore of the whole tropical current
system, including the equatorial upwelling and the equatorial undercurrent)
decreases by up to 5 Sv (10 %) in PDO_PLUS compared to
PDO_MINUS. The order of magnitude of the strength of the STCs
in the PDO_PLUS and PDO_MINUS experiments are
in line with other modeling studies (Lohman and Latif, 2005; Luebbecke et
al., 2008; Hong et al., 2014) and with the observational study by McPhaden
and Zhang (2002), which showed that the equatorial upwelling decreased by 10 % from 1970–77 (47 Sv) to 1980–89 (42 Sv) related to a shift of the
phase of the PDO.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p id="d1e438"><bold>(a)</bold> Oxygen concentration (mmol m<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) at the end of the
spin-up (average 100–700 m). The contours represent the oxygen concentrations of the World Ocean
Atlas (WOA; mmol m<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) (average 100–700 m).
<bold>(b)</bold> Thickness (m) of the
suboxic regions (oxygen lower than 20 mmol m<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) of the WOA and <bold>(c)</bold> at the
end of the spin-up. <bold>(d)</bold> Difference in percentage between the oxygen
concentrations in PDO_PLUS and in PDO_MINUS
(average 100–700 m). Black contours represent the oxygen concentration in
PDO_MINUS, and the red contours represent the oxygen concentration in PDO_PLUS
(mmol m<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). <bold>(e)</bold> Difference between the oxygen concentration
(mmol m<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in PDO_PLUS and in PDO_MINUS
vertically averaged over the suboxic regions SUB20 (defined as the region
where the oxygen concentration is lower than 20 mmol m<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at the end of
the spin-up). The contours represent the differences between the oxygen concentrations
(mmol m<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in PDO_PLUS and PDO_MINUS
(average 100–700 m). <bold>(f)</bold> Difference between the thickness (m) of the suboxic
regions in PDO_PLUS and PDO_MINUS. All of the
differences between PDO_PLUS and PDO_MINUS are
averaged after 50 years of integration time.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f02.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Oxygen concentration</title>
<sec id="Ch1.S4.SS1">
  <title>Comparison with the World Ocean Atlas</title>
      <p id="d1e562">At the end of the spin-up, the model reproduces the large-scale features of
the observed World Ocean Atlas (WOA) (Garcia et al., 2010) oxygen
concentration field (Fig. 2a). The thickness of the SUB20 regions, defined
as the regions where oxygen concentrations are lower than 20 mmol m<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
at the end of the spin-up, reaches more than 700 m north of the Equator both
in the WOA (Fig. 2b) and in the model (Fig. 2c). “Typical” biases (Bopp et
al., 2013; Cabre et al., 2015) are present in our model. In particular, (1)
the OMZ region does not extend far enough westward, in particular north of
the Equator, and (2) oxygen concentrations at the Equator are too low, maybe due
to a poor representation of the intermediate current system, located below
the EUC, in relatively coarse-resolution models (Marin et al., 2010;
Getzlaff and Dietze, 2013). Nevertheless, the thickness of the suboxic regions is
lower in the equatorial region compared to the tropics, as
shown in Fig. 2c.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <title>Perturbation by the PDO</title>
      <?pagebreak page7115?><p id="d1e583">After 50 years of integration time, the oxygen
concentration (average 100–700 m) is lower in the eastern part of the basin in
PDO_PLUS compared with PDO_MINUS (Fig. 2d). This
decrease reaches up to 100 % in regions where the oxygen is very low
(below 5 mmol m<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and about 5 %–10 % in regions where the oxygen
concentration is lower than approximately 20 mmol m<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Fig. 2e). The volume of
the SUB20 regions is 7 % larger in PDO_PLUS and the
thickness of the suboxic layer increases by up to 100 m close to the coast
between 10<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and 10<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and at the outer boundary of the
SUB20 regions (Fig. 2f; note that the “stepwise shape” of the anomaly is
due to the discretization of the vertical grid of the ocean model). The
oxygen concentration in the SUB20 regions decreases by 2–10 mmol m<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in
PDO_PLUS compared with PDO_MINUS (0.04 to 0.2 mmol m<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M36" 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>). Conversely, in the mid-Pacific Ocean oxygen
concentrations are 2 %–20 % higher in PDO_PLUS. This
increase is localized (5–10<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and 5–10<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and eastward
of 160<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W).</p>
      <p id="d1e692">Our results can be put in perspective with observations. An oxygen decrease
of 1 mmol m<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M41" 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> has been monitored in the eastern equatorial
region (85<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, 2<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S to 8<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) since 1976
(Czeschel et al., 2012). Schmidtko et al. (2017) also found a global decrease of
the integrated oxygen concentration in the water column between 1960s and 2010s. This
decrease was of the order of 0.2 mmol m<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the equatorial
Pacific Ocean at 300 m depth. Similarly, Ito et al. (2017) showed that
oxygen has declined at 400 m depth by 0.2 mmol m<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M48" 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> since 1958 in the
eastern Pacific Ocean; at 100 m depth, oxygen has decreased by up to 0.4 mmol m<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M50" 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>. However, Ito et al. (2017) observed a localized oxygen
increase at 10<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, similar to the one that we described above. Our
simulations suggest that a shift from a negative to a positive phase of the
PDO may be responsible for a large fraction of the observed oxygen decrease.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <title>Regulation of the oxygen levels</title>
      <p id="d1e837">The oxygen level below the euphotic zone is determined by the balance
between consumption (respiration) and supply (transport). The supply is
decomposed into advective, diapycnal and isopycnal diffusion terms. The
analysis is based on the average of the 50 years of integration time.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e842">Budget of the oxygen concentration (average 100–700 m;
(mmol m<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M53" 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>) at the end of the spin-up <bold>(a–d)</bold> and the difference
between PDO_PLUS and PDO_MINUS averaged over
50 years of integration time <bold>(e–f)</bold>. <bold>(a, e)</bold> Respiration; <bold>(b, f)</bold> total supply; <bold>(c, g)</bold>
advective processes; and <bold>(d, h)</bold> diffusive processes. The oxygen concentration
(mmol m<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is displayed using the contours in <bold>(a)</bold>–<bold>(d)</bold>. The oxygen difference
between PDO_PLUS and PDO_MINUS (mmol m<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)
is displayed using the contours in <bold>(e)</bold>–<bold>(f)</bold>. As a note of caution, a positive value
corresponds to a source of oxygen while a negative value corresponds to a
sink in <bold>(a)</bold>–<bold>(d)</bold>, while differences between the two experiments are displayed in <bold>(e)</bold>–<bold>(f)</bold>.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f03.png"/>

      </fig>

<?xmltex \hack{\newpage}?>
<?pagebreak page7116?><sec id="Ch1.S5.SS1">
  <?xmltex \opttitle{Intermediate (100--700\,m) tropical Pacific Ocean}?><title>Intermediate (100–700 m) tropical Pacific Ocean</title>
      <p id="d1e952">Respiration processes remove oxygen (Fig. 3a), especially in the
tropical regions (up to 10 mmol m<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the 100–700 m layer),
as biological production is high along the Equator and close to the
coast. In the PDO_PLUS experiment the basin-scale circulation
is more sluggish than in PDO_MINUS (see Sect. 3), leading to a decrease in the concentration of nutrients in
the euphotic zone (see Sect. 7). The respiration
term becomes “less negative” in PDO_PLUS (positive anomaly
of 1–2 mmol m<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the equatorial region; Fig. 2d).</p>
      <?pagebreak page7117?><p id="d1e1003">The consumption of oxygen is compensated for by supply processes (Fig. 3b),
which are partly performed by advective processes (Fig. 3c) that dominate the supply
between 5<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and 5<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and in the eastern part of the
basin; this shows the preponderant role of the equatorial current system
regarding supplying oxygen to the oxygen-depleted regions (Cabre et al., 2015; Shigemitsu
et al., 2017). Conversely, the diffusive processes (isopycnal and diapycnal
mixing) dominate the supply outside of the equatorial region (poleward of
10<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>; Fig. 3d). The ocean currents shape the thermocline and
high oxygen concentrations are transferred by isopycnal diffusion from the
core of the EUC to the poleward intermediate ocean. The PDO_PLUS–PDO_MINUS positive oxygen anomaly in the western part
of the basin is caused by the decrease in the respiration (“less negative”
values), which is not completely compensated for by the decrease in the supply
terms.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e1035"><bold>(a)</bold> Zonal integration of the vertically averaged oxygen supply
in the suboxic regions SUB20 (oxygen lower than 20 mmol m<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>;
mmol m<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M65" 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>) at the end of the spin-up. Black represents total
supply, red represents advective processes, blue represents isopycnal diffusion and green represents diapycnal
diffusion. <bold>(b)</bold> Relative importance of the advective processes (red),
isopycnal diffusion (blue) and diapycnal diffusion (green) in the total
oxygen supply in SUB20 (the solid line represents the PDO_MINUS experiment, and the dashed line represents the PDO_PLUS experiment). <bold>(c)</bold> Zonal integration of the
vertically averaged difference of oxygen supply/removal in
PDO_PLUS minus PDO_MINUS (mmol m<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in SUB20. Black denotes supply, green is
respiration and red represents supply <inline-formula><mml:math id="M68" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> respiration. <bold>(d)</bold> Zonal integration of the vertically
averaged difference of oxygen supply in PDO_PLUS minus
PDO_MINUS (mmol m<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in SUB20. Black is
total supply, red denotes advective processes, blue is isopycnal diffusion and
green is diapycnal diffusion.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S5.SS2">
  <title>SUB20 regions</title>
      <p id="d1e1154">The contribution of each process was vertically and zonally averaged
over the SUB20 region of the Pacific Ocean (Fig. 4a) and multiplied by the
longitudinal extension of the SUB20 of the experiment PDO_MINUS. The total supply term (black line in Fig. 4a) is characterized by a large
supply in the equatorial region, between 10<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and 10<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, due to advective processes (red line in Fig. 4a). The role of the westward
south and north equatorial currents is clearly apparent at 5<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N
and 5<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. At this location the thermocline exhibits a strong slope
with strong oxygen gradients, fostering isopycnal diffusion (blue line in Fig. 4a), removing oxygen from the Equator (and the EUC) and transferring it to
the deeper, adjacent regions. The effect of the jets and the isopycnal
diffusion add up and cause the strong peak in oxygen supply, located
between 5 and 10<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S (and to a lesser extent between
5 and 10<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N). The role of the oxygen supply by
diapycnal diffusion (green line in Fig. 4a) is relatively small in the equatorial
region (about 20 % of the total supply), but more significant between
30 and 10<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S (about one-third of the total supply)
and dominant north of 10<inline-formula><mml:math id="M78" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N (Fig. 4b). Between 10 and
30<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, the isopycnal diffusion term (blue line in Fig. 4a) plays a
dominant role, possibly due the outcrop of isopycnals and the formation of
mode waters close to the southern part of SUB20. The importance of the
isopycnal diffusion in setting the oxygen levels in the region off Chile
(around 30<inline-formula><mml:math id="M80" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) has been previously highlighted by sensitivity
tests to the Redi mixing coefficient (Gnanadesikan et al., 2012). Stramma et al. (2010) roughly estimated
the oxygen budget (30<inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–30<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) in the suboxic regions based on observational data. Despite
large uncertainties, the observational budget estimate points to an
allocation of about 33 % by advection, 22 % by vertical mixing and 45 % by eddy mixing (Brandt et al., 2015). In our model, averaging the SUB20
budget between 30<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and 30<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S gives comparable
magnitudes (Fig. 4b) (in PDO_MINUS 21 % of the supply
occurs by advection, 29 % by diapycnal mixing and 50 % by isopycnal
mixing, strongly related to mesoscale activity).</p>
      <p id="d1e1285">In the PDO_PLUS experiment, the supply of oxygen by
circulation processes decreases (black line in Fig. 4c) due to a reduction in the
advective supply in the equatorial region (Fig. 4d – red) and of the
diapycnal and isopycnal diffusion poleward of 10<inline-formula><mml:math id="M85" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and
10<inline-formula><mml:math id="M86" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S (green and blue lines in Fig. 4d, respectively). The primary production
decreases as well, resulting in a positive anomaly of the respiration term
(which is “less negative”; green line in Fig. 4c). The decrease in respiration
nearly compensates for the reduced supply of oxygen, especially in the equatorial
region; however, the decrease in the circulation supply terms is larger,
leading to a net<?pagebreak page7118?> decrease in oxygen levels in SUB20 (red line in Fig. 4c). In the
10–30<inline-formula><mml:math id="M87" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N region, about half of the oxygen decrease is
caused by changes in the supply, while the other half is due to changes in
respiration, triggered by changes in the advective processes (see Sect. 7).
In the 10–30<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S region, the decrease in the oxygen levels is principally due to a decrease in the
isopycnal and mixing processes (Fig. 4d). As the ocean circulation is
generally weaker in PDO_PLUS, the relative importance of
diffusion increases in the PDO_PLUS experiment compared to
PDO_MINUS (20 % of the supply occurs by advection, 27 %
by diapycnal mixing and 53 % by isopycnal mixing; Fig. 4b)</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e1326"><bold>(a)</bold> Time series (50 years) of the difference between
PDO_PLUS and PDO_MINUS regarding the oxygen
concentration (mmol m<inline-formula><mml:math id="M89" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in the EQ region (average 10<inline-formula><mml:math id="M90" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–10<inline-formula><mml:math id="M91" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 160<inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E–140<inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, 100–700 m; black),
the SUB20EQ region (equatorial part of SUB20: 10<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–10<inline-formula><mml:math id="M95" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N;
dark blue), the SUB20N region (northern part of SUB20: 10–30<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N; cyan) and the SUB20S region (southern part of SUB20: 10–30<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S; pink). <bold>(b, c, d)</bold> Oxygen (mmol m<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) difference (average 100–700 m)
between PDO_PLUS and PDO_MINUS after <bold>(b)</bold> 2
years, <bold>(c)</bold> 10 years and <bold>(d)</bold> 20 years of integration time. <bold>(e–h)</bold> Time series (50 years) of
the difference between the PDO_PLUS and the PDO_MINUS oxygen budget (mmol m<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in <bold>(e)</bold> EQ, <bold>(f)</bold> SUB20EQ,
<bold>(g)</bold> SUB20N and <bold>(h)</bold> SUB20S. The bold black line is total supply, the blue line is advective supply,
the pink line is diapycnal diffusion, the cyan line is diapycnal <inline-formula><mml:math id="M101" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> isopycnal diffusion, the bold
green line is respiration and the bold red line represents supply <inline-formula><mml:math id="M102" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> respiration.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f05.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S6">
  <title>Temporal aspects</title>
<sec id="Ch1.S6.SS1">
  <?xmltex \opttitle{Intermediate (100--700\,m) tropical Pacific Ocean}?><title>Intermediate (100–700 m) tropical Pacific Ocean</title>
      <p id="d1e1514">In the western part of the basin (160<inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E–140<inline-formula><mml:math id="M104" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W,
10<inline-formula><mml:math id="M105" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–10<inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S), oxygen concentrations decrease in
PDO_PLUS compared with PDO_MINUS in the first few
years of the experiment (initial shock, highlighting the timescale of the
response of productivity to a change in circulation) and increase afterwards
(Fig. 5a–d). The changes in the advective processes (blue line in Fig. 5e) are
largely responsible for the total changes in the supply (bold black line in Fig. 5e).
The decrease in respiration (green in Fig. 6e) offsets these changes,
leading to net a positive anomaly (bold red line in Fig. 5e). After 50 years the
positive anomaly is still growing but at a slower pace (Fig. 5a): diffusive
processes (cyan) and more specifically diapycnal diffusion (pink) act in
the same direction as the current-driven changes as a result of a less
stratified upper ocean under PDO_PLUS conditions. (While the
PDO_PLUS surface fluxes warm the surface ocean and foster a
strong upper ocean stratification, the PDO_PLUS winds weaken
the upwelling, warm the subsurface ocean and foster a weak upper ocean
stratification. The latter effect overcompensates for the surface warming and
explains that the ocean is less stratified under PDO_PLUS
conditions compared to PDO_MINUS conditions).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p id="d1e1555"><bold>(a)</bold> Difference (%) of the vertically integrated phytoplankton
concentration between PDO_PLUS and PDO_MINUS
(average of 50 years of integration time). The vertically integrated phytoplankton
concentration of PDO_MINUS is shown using the contours
(mmol m<inline-formula><mml:math id="M107" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). <bold>(b)</bold> Difference (%) of the surface phosphate
concentration between PDO_PLUS and PDO_MINUS
(average of 50 years of integration time). The surface phosphate concentration of
PDO_MINUS is shown using the contours (mmol m<inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). <bold>(c, e, g)</bold> Average
of the 10–20<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/90–60<inline-formula><mml:math id="M110" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W region and
<bold>(d, f, h)</bold> the 10<inline-formula><mml:math id="M111" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N: 20<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N/120–90<inline-formula><mml:math id="M113" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W region <bold>(c, d)</bold> upwelling (m yr<inline-formula><mml:math id="M114" 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>; blue – PDO_MINUS,
red – PDO_PLUS) and <bold>(e, f)</bold> phytoplankton concentration (mmol m<inline-formula><mml:math id="M115" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; contours represent phosphate concentration) at the end of the spin-up.
<bold>(g, h)</bold> Difference between PDO_PLUS and PDO_MINUS phytoplankton concentration (mmol m<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; contours represent difference
between the PDO_MINUS and PDO_PLUS phosphate concentration).</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f06.png"/>

        </fig>

</sec>
<sec id="Ch1.S6.SS2">
  <title>SUB20 regions</title>
      <p id="d1e1697">The picture described above shows similarities to that of the
equatorial region (10<inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–10<inline-formula><mml:math id="M118" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) of SUB20, where a strong
decrease in the oxygen supply (bold black line in Fig. 5f) due to advective
processes (blue line in Fig. 5f) occurs. However, the role of diffusion (pink line in Fig. 5f)
is larger in SUB20 compared with the mid-Pacific equatorial region.
Respiration changes (green line in Fig. 5f) do not offset the weaker supply, as
in the western tropical Pacific Ocean, leading to a net decrease in the oxygen
concentration (Fig. 5a–d). In the northern part (10–30<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) of SUB20 an increase in oxygen transport by advective
processes (blue line in Fig. 5g) is compensated for by a strong decrease due to diffusion
processes (less mixing), leading to a net decrease in the oxygen supply. Primary
production and respiration increases (see Sect. 7),
reinforcing the decrease in oxygen levels. In the southern part
(10–30<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) of SUB20 the decrease in the oxygen supply
by advective transport (blue line in Fig. 5h) is accompanied by a strong decrease
in the supply by diapycnal (pink in Fig. 6h) and isopycnal mixing (cyan line in Fig. 5h). The adjustment occurs on a (multi) decadal timescale (Fig. 5a–d). The
strong changes in the supply mechanisms in the northern/southern part of
the SUB20 regions are likely linked to the stronger influence of the
subtropical regime in PDO_PLUS than in PDO_MINUS in SUB20 (see Sect. 3), which explains the
“initial shock” related to a change of regime.</p>
      <p id="d1e1736">The simulated PDO-induced changes are significant after at least 5 years (in
the equatorial Pacific Ocean) to a few decades (in the southern part of the
suboxic regions). Significant changes occurred after a similar timescale in
the study by Ridder and England, 2014. This suggests that higher-frequency
climate oscillations such as the El Niño–Southern Oscillation (ENSO) – or
“short-lasting” PDO events – have a very limited impact on oxygen
concentrations of the suboxic eastern tropical Pacific, which is in agreement with
Deutsch et al. (2011) and Ito and Deutsch (2013). However, ENSO may have an impact
on the surface air/sea oxygen exchanges (Eddebar et al., 2017) and
“short-lasting” PDO events (less than 10 years) may impact the oxygen
concentration of the upper thermocline in the mid-Pacific Ocean (Duteil et
al., 2014b). In the southern region (10–30<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S), the
system is still losing oxygen after 50 years of integration time suggesting that
extra-tropical processes are involved. Getzlaff et al. (2016) showed that a
vigorous South Pacific subtropical gyre, driven by an increase in the
Southern Hemisphere westerlies, supplies oxygen to the tropics. Yamamoto et al. (2015) and Keller et al. (2016) showed that high latitudes may constrain
tropical suboxic regions at multi-decadal to centennial timescale.</p>
</sec>
</sec>
<sec id="Ch1.S7">
  <title>Productivity and upwelling</title>
      <p id="d1e1755">As previously seen, changes in respiration play a significant role in
setting the oxygen levels. Respiration either compensates for the changes in
supply in the equatorial region or acts in synergy with the decrease in
supply to deplete oxygen in the northern part of SUB20 in the
PDO_PLUS experiment. While the changes in the oxygen supply and
transport are primarily linked to changes in the structure of the interior
ocean, the change in respiration is principally linked to the surface and
upper thermocline productivity, which ultimately depends on the supply of
nutrients to the mixed layer.</p>
<sec id="Ch1.S7.SS1">
  <title>Upwelling strength and seasonality</title>
      <?pagebreak page7120?><p id="d1e1763">In the PDO_PLUS experiment, the nutrient supply decreases
over most of the basin, leading to a decrease in the nutrient uptake and the
productivity. The decrease in the supply is caused both by a slowing-down of
the circulation and by a thermocline deepening (as seen in Sect. 3).
However, counter intuitively, nutrient levels increase and
production is slightly (2 %–5 %) higher in PDO_PLUS in
the eastern upwelling systems. Figure 6a presents similarities with the
imprint of the PDO on the deseasonalized chlorophyll concentration inferred from
satellite data (Thomas et al., 2012). Thomas et al. (2012) found that a positive phase of
the PDO is associated with a general decrease in the chlorophyll concentration
in the tropical Pacific Ocean. However, in the region located between 15 and 30<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and east of 140<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, and in the region south of
10<inline-formula><mml:math id="M124" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and east of 120<inline-formula><mml:math id="M125" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W the correlation between PDO and
deseasonalized chlorophyll is positive (Fig. 7 in Thomas et al., 2012).
Furthermore, other climate oscillations, such as the North Pacific Gyre
Oscillation (NPGO) constrain the strength of the upwelling cells in the ETNP
in addition to the PDO (DiLorenzo et al., 2008; Macias et al., 2012).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e1804"><bold>(a)</bold> Difference between the sea surface height (m) of the
PDO_PLUS50 and the PDO_MINUS50 experiments (colored legend)
and the PDO_PLUS and PDO_MINUS experiments (contours). <bold>(b)</bold>
Difference between the vertically integrated phytoplankton concentration
(mmol m<inline-formula><mml:math id="M126" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) of the PDO_PLUS50 and
PDO_MINUS50 experiments (colored legend) and the PDO_PLUS and
PDO_MINUS experiments (contours). <bold>(c)</bold> Difference between the average 100–700 m oxygen concentration (mmol m<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) for the
PDO_PLUS50 and PDO_MINUS50 experiments (colored legend) and the
PDO_PLUS and PDO_MINUS experiments (contours).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f07.png"/>

        </fig>

      <?pagebreak page7121?><p id="d1e1845">The productivity increase in PDO_PLUS is due to the change in the
seasonality of the upwelling system in our experiments. The eastern tropical
South Pacific (ETSP) region (average 10–30<inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S,
90–60<inline-formula><mml:math id="M129" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) is characterized by a strong downwelling in
May/April and a strong upwelling in August/September in
PDO_MINUS (Fig. 6c). Conversely, in PDO_PLUS,
the ETSP is characterized by a weaker upwelling which persists throughout the
year, continuously supplying nutrients into the mixed layer and the upper ocean
and creating a positive anomaly in nutrients and productivity (Fig. 6e and
g). In the eastern tropical North Pacific (ETNP) (10–30<inline-formula><mml:math id="M130" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 120–90<inline-formula><mml:math id="M131" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W), a strong upwelling
occurs 1 month earlier in PDO_PLUS than in
PDO_MINUS (Fig. 6d), leading to an increase in the nutrient
concentrations in the upper ocean (Fig. 6f and h) in a season when
irradiance is high, fostering primary production. The positive PDO years
used to construct the PDO_PLUS forcing are made up of 30 % of positive NPGO years, which may explain the shift in the upwelling
seasonality and the stimulation of productivity in the ETNP (Chenillat et
al., 2012).</p>
</sec>
<sec id="Ch1.S7.SS2">
  <title>Role of local vs. large scale circulation</title>
      <p id="d1e1890">In order to disentangle the changes in the local forcing related to
upwelling, and the remote forcing (trade winds) in the eastern Pacific Ocean
oxygen levels and productivity, we perform two supplementary experiments,
PDO_MINUS50 and PDO_PLUS50. These experiments
are similar to PDO_MINUS and PDO_PLUS.
However, where oxygen is lower than 50 mmol m<inline-formula><mml:math id="M132" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, anywhere in the water column, at the end of the spin-up (green line in the Fig. 7a–c), the
MEAN surface forcing is employed (see Sect. 2). As
the resolution of the CORE forcing is relatively coarse (1.9<inline-formula><mml:math id="M133" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>)
and the NEMO circulation model interpolates the forcing on the ocean grid,
we did not perform any explicit smoothing between the regions where the MEAN
and the PDO_MINUS/PDO_PLUS forcings are used.</p>
      <p id="d1e1914">The PDO_PLUS50–PDO_MINUS50 SSH anomaly (Fig. 7a) presents a similar pattern to the
PDO_PLUS–PDO_MINUS SSH anomaly. However, the amplitude of PDO_PLUS50–PDO_MINUS50 is weaker than the amplitude of
PDO_PLUS–PDO_MINUS in the eastern part of the
Pacific basin (east of the green line – Fig. 7a), showing that both remote
and local forcings control the circulation properties east of 130<inline-formula><mml:math id="M134" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W in the equatorial region. This is consistent with the results of Zhang and
McPhaden (2008) who showed that both the large scale circulation and the
local wind stress anomalies impact the surface temperature variability in
the NINO3 (150–90<inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W; 5<inline-formula><mml:math id="M136" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–5<inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S)
region.</p>
      <p id="d1e1953">The PDO_PLUS50–PDO_MINUS50 productivity
anomaly (Fig. 7b) and the PDO_PLUS–PDO_MINUS
productivity anomaly display similar patterns in the western part of the
basin. However, in the eastern part (east of the green line – Fig. 7), the
productivity is nearly identical in PDO_PLUS50 and
PDO_MINUS50 suggesting that the change in productivity in the
SUB20 regions is mostly driven by local forcings. The nutrients are indeed
supplied into the euphotic zone by the upwelling systems, which are<?pagebreak page7122?> primarily
driven by alongshore wind stress and curl (e.g Albert et al., 2010;
Belmadani et al., 2014).</p>
      <p id="d1e1956">The oxygen concentration depends on both changes in circulation and in
productivity. In the eastern part of the basin (east of the green line – Fig. 7), the
PDO_PLUS50–PDO_MINUS50 oxygen anomaly is
similar to the PDO_PLUS–PDO_MINUS oxygen
anomaly in the equatorial and southern part of SUB20: a change in local
forcings has almost no impact on the simulated oxygen fields. These
experiments suggest that the changes in oxygen concentration related to the
change from a negative to a positive PDO phase are not directly related to
changes in the coastal productivity and in the upwelling strength, but
rather to changes in the large-scale circulation in the equatorial and
southern part of SUB20. Conversely, in the northern part of SUB20, local
forcings play a dominant role as the PDO_PLUS50–PDO_MINUS50 oxygen anomaly is positive while the
PDO_PLUS–PDO_MINUS anomaly is negative.</p>
</sec>
</sec>
<sec id="Ch1.S8" sec-type="conclusions">
  <title>Summary of the processes at play and conclusions</title>
      <p id="d1e1966">In this study we tested whether the PDO impacts the oxygen concentration in the
eastern part of the Pacific Ocean. We use the forced ocean model NEMO
coupled to a simple NPZD (Nutrient Phytoplankton Zooplankton Detritus) model. After spin-up, the NEMO-NPZD model
was forced by “typical” PDO positive (experiment PDO_PLUS) and
negative (experiment PDO_MINUS) conditions derived from the
COREv2 atmospheric forcings. A PDO-positive phase is characterized by an
approximate 5 % to 10 % decrease in the zonal and meridional wind speed over the Pacific
Ocean, while the sea surface temperature increases by
0.2 <inline-formula><mml:math id="M138" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. A PDO-negative event shows the opposite pattern. In
agreement with observations (McPhaden and Zhang, 2002), the circulation of
the tropical Pacific Ocean is more sluggish (by 5 % to 10 %) in the
PDO_PLUS experiment compared with the PDO_MINUS experiment. After 50 years of integration time,
the volume of the suboxic regions (oxygen lower then 20 mmol m<inline-formula><mml:math id="M139" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) is 7 % larger and the
oxygen concentration decreases by 5 % to 50 % in the suboxic regions in
PDO_PLUS compared with PDO_MINUS.</p>
      <p id="d1e1990">Recent analyses of the observational datasets showed that the oxygen
concentration has decreased by about 5 % in the eastern equatorial Pacific
Ocean region since 1960 (Schmidtko et al., 2017; Ito et al., 2017). We show
here that a PDO_PLUS PDO event lasting for 50 years may
impact the suboxic region by at least a similar order of magnitude. The
shift from a PDO-negative phase (prevailing conditions before 1975) to a PDO
positive phase (prevailing conditions since 1975) may therefore explain a
significant percentage of the large deoxygenation that has occurred over the
last few decades.</p>
      <p id="d1e1993">The simulated suboxic regions are divided into equatorial (10<inline-formula><mml:math id="M140" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N–10<inline-formula><mml:math id="M141" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S), northern (10–30<inline-formula><mml:math id="M142" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) and southern
(10–30<inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) parts. The oxygen levels of each subregion
are constrained by different processes. In the equatorial part, the oxygen
levels are set by advective processes (Cabre et al., 2015; Shigemitsu et
al., 2017). In the PDO_PLUS experiment, the slowing-down of
the equatorial current system (and more particularly of the equatorial
undercurrent) decreases the supply of oxygen (Fig. 8). Simultaneously, the
supply of nutrients decreases, leading to a decrease in productivity and
respiration. In the eastern part of the basin (in the suboxic regions), the
decrease of supply dominates the change in respiration leading to a net
oxygen decrease. Inversely, the change in respiration is dominant in the
mid-Pacific Ocean, highlighting the importance of the parameterization of the
biogeochemical processes (Kriest et al., 2010; Kriest and Oschlies, 2015)
and more particularly the response of the phytoplankton growth to a change
in nutrient concentration.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e2034">Summary of the processes at play during a PDO positive (red) and
negative phase (blue).</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://bg.copernicus.org/articles/15/7111/2018/bg-15-7111-2018-f08.png"/>

      </fig>

      <p id="d1e2044">The southern part of the suboxic regions is mostly constrained by isopycnal
diffusion processes (Gnanadesikan et al., 2012). In the PDO_PLUS experiment, the supply of oxygen by isopycnal processes from the
equatorial regions and the subtropical gyres to the tropics decreases
compared to PDO_MINUS. In the northern part, the role of
diapycnal processes is dominant. In the PDO_PLUS experiment,
the oxygen decrease is caused by changes in the upwelling system,
stimulating productivity and respiration.</p>
      <p id="d1e2047">The general slowdown of the large-scale circulation caused by a decrease in
the intensity of the trade winds is not reflected in the upwelling strength
(Narayan et al., 2010), which is mainly forced by local processes. The
strength and seasonality of the upwelling constrain the amount of
productivity and the subsequent respiratory oxygen consumption in the
suboxic regions. A shift in the upwelling seasonality explains the larger
respiration in PDO_PLUS compared with PDO_MINUS
in the northern part of the suboxic region. This shift is potentially linked
to the NPGO (DiLorenzo et al.,<?pagebreak page7123?> 2008), a decadal climate oscillation which has
a signature that is implicitly contained in the “typical” PDO forcing. Using two
supplementary experiments where the PDO_PLUS and
PDO_MINUS forcings are only applied in the mid-Pacific Ocean
above the tropical Pacific low-oxygen areas, we highlighted that a change in
the large-scale wind pattern constrains changes in the equatorial and
southern oxygen levels, while oxygen changes in the northern part are
constrained by local processes.</p>
      <p id="d1e2050">One of the largest limitations of our study is that the idealized PDO
forcings were prepared using a relatively short period extending from 1948
to 2007 (the COREv2 dataset). The implicit contribution of statistically
independent climate oscillations such as the NPGO (DiLorenzo et al., 2008)
can therefore not be completely ruled out.</p>
      <p id="d1e2053">Finally, another limitation is the resolution of the model. The role of
mesoscale activity has been previously demonstrated in the supply of oxygen
to the suboxic regions of the eastern Pacific Ocean (Montes et al., 2014;
Bettencourt et al., 2015; Vergara et al., 2016). The relative increase in
the isopycnal diffusive supply in a PDO-positive phase suggests the
importance of the role of mesoscale activity during this period.</p>
      <p id="d1e2056">Our study suggests that the shift from a prolongated (multi-decadal) negative
to a prolongated positive PDO phase is accompanied by a decrease in the oxygen
levels in the eastern tropical Pacific Ocean. Several multi-decadal PDO
shifts have occurred in the last century. For instance, the period from 1943 to 1976 is
characterized by a negative PDO phase, while a positive PDO phase occurred
from 1977 to 2011 (Fig. 1a). Such shifts have occurred roughly every few decades
during the last 1000 years, as shown by PDO reconstructions (MacDonald and
Case, 2005). An open question is whether the succession of these alternate
shifts may cause a change in the oxygen concentration on centennial to
millennial timescales.</p>
      <p id="d1e2059">Our study can be compared to the study of Deutsch et al. (2011) (hereafter
referred to as D2011). Based on a 1959–2005 hindcast experiment, D2011 showed that the
global suboxic volume (O<inline-formula><mml:math id="M144" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> &lt; 5 mmol m<inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), 95 % of which is
contained in the northeastern tropical Pacific Ocean (0 to
30<inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 140<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W to the coast), is controlled by the depth
of the thermocline that constrains the productivity and the amount of oxygen
respired around the suboxic volume. The depth of the thermocline is strongly
related to the strength of the PDO, which explains 24 % of the
variability of the suboxic volume in the hindcast simulation of D2011. In
D2011, a PDO-negative phase was characterized by a large extent of the
suboxic regions resulting from enhanced respiration with only negligible
effects of changes in oxygen supply. Our results differ from D2011 because
the increase in the respiration in a PDO-negative phase (higher primary
production) is more than compensated for by an increase in the oxygen supply
due to advective/diffusive processes, which ultimately leads to elevated oxygen
levels and smaller suboxic regions in a PDO-negative state. Considering that
the models used by D2011 and those used in our study are similar with similar grid
resolution, the balance between changes in the oxygen consumption (dominant
effect in D2011) and the transport (dominant effect in our study) depends on (i)
the response of primary productivity and export production to a nutrient
increase, and (ii) the depth of the suboxic regions, as respiration changes
are stronger, and more difficult to compensate for by oxygen supply changes, at
shallower than at greater depths. While the biogeochemical model used in our
study contains fully prognostic nutrient, phytoplankton, zooplankton and
detritus fields, D2011 used a simple restoring model that diagnosed export
production from restoring simulated against observed surface phosphate
concentrations. Therefore, the model from D2011 did not account for possible
PDO-driven changes in surface nutrient concentrations and instead likely
overestimated the variability in export and respiration at depth.</p>
      <p id="d1e2102">While our modeling framework captures the general patterns of primary and
export production reasonably well, it does not include an iron cycle;
thus, despite displaying a well-tuned mean state, it may exhibit systematic errors
regarding its sensitivity to environmental changes. Furthermore, the model's
representation of the respiration processes is relatively pragmatic. In
particular, our model lacks an explicit nitrogen cycle including anaerobic
remineralization by denitrification under low oxygen conditions (Paulmier et
al., 2009). Other limitations include, for instance, a simplistic
parameterization of the attenuation of the flux of particulate organic
matter which, in our model, neglects any dependence on temperature or oxygen
(Laufkötter et al., 2017). Also not considered in the model is the diel
vertical migration of zooplankton that actively transports material into the
deep ocean (Bianchi et al., 2013). Anthropogenic activities impact the
global biogeochemical cycles. In particular, atmospheric deposition of
anthropogenic nitrogen and iron may partially relax the iron limitation in
the tropical Pacific Ocean (Ito et al., 2016). Industrial fishing may affect
the mortality rate of the zooplankton and possibly feed back on productivity
and respiration (Getzlaff and Oschlies, 2017). Each of these `missing'
processes may modulate respiration rates and may possibly be correlated with
the state of the PDO. An important result of our study is that the
PDO-induced changes in respiration are smaller than the PDO-induced changes
in oxygen supply by a few percent in most of the eastern tropical Pacific
Ocean. We show that this small imbalance integrated over a few decades
results in a significant PDO-driven oxygen anomaly that may explain a large
part of the observed oxygen decline over the past few decades in this region.
Experiments including different biogeochemical parameterizations and
processes will need to be performed to better assess the robustness of our
results.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability">

      <?pagebreak page7124?><p id="d1e2109">The Coordinated Ocean-ice Reference Experiments (CORE2)
forcing dataset is available at:
<uri>https://data1.gfdl.noaa.gov/nomads/forms/core/COREv2.html</uri> (Large and
Yeager, 2009). The code for the Nucleus for European Modeling of the Ocean
(NEMO) is available at: <uri>https://www.nemo-ocean.eu/</uri> (last access:
27 November 2018). The experiments performed in this study are available at:
<uri>https://data.geomar.de/thredds/catalog/open_access/duteil_et_al_2018_bg/catalog.html</uri>
(Duteil et al., 2018).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2121">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/bg-15-7111-2018-supplement" xlink:title="pdf">https://doi.org/10.5194/bg-15-7111-2018-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution">

      <p id="d1e2130">OD designed the study and performed the model experiments. All authors contributed to the analysis
and to writing the paper.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e2137">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2143">This work is a contribution of the SFB754, supported by the Deutsche
Forschungsgemeinschaft. The simulations were performed at the North German
Supercomputing Alliance (HLRN). <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> The article
processing charges for this open-access <?xmltex \hack{\newline}?> publication were
covered by a Research <?xmltex \hack{\newline}?> Centre of the Helmholtz
Association.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by:
M. Grégoire<?xmltex \hack{\newline}?> Reviewed by: two anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Pacific Decadal Oscillation and recent oxygen decline in the eastern tropical Pacific Ocean</article-title-html>
<abstract-html><p>The impact of the positive and negative phases of the Pacific Decadal
Oscillation (PDO) on the extension of the poorly oxygenated regions of the
eastern Pacific Ocean was assessed using a coupled ocean
circulation–biogeochemical model. We show that during a <q>typical</q>
PDO-positive phase the volume of the suboxic regions expands by 7&thinsp;% over 50
years due to a slowdown of the large-scale circulation related to the
decrease in the intensity of the trade winds. Changes in oxygen levels are
mostly controlled by advective processes between 10°&thinsp;N and
10°&thinsp;S, whereas diffusive processes are dominant poleward of
10°: in a <q>typical</q> PDO-positive phase the sluggish equatorial
current system provides less oxygen to the eastern equatorial part of the
basin while the oxygen transport by diffusive processes significantly
decreases south of 10°&thinsp;S. The suboxic region located north of
10°&thinsp;N displays less sensitivity to the phase of the PDO as the
local upwelling-related processes play a dominant role compared to the
large-scale circulation in setting the oxygen concentration. Our study
suggests that the prevailing PDO-positive conditions since 1975 may explain a
significant part of the current deoxygenation occurring in the eastern
Pacific Ocean.</p></abstract-html>
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