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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mar. Sci.</journal-id>
<journal-title>Frontiers in Marine Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mar. Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-7745</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fmars.2024.1348161</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Marine Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A carbonate system time series in the Eastern Mediterranean Sea. Two years of high-frequency <italic>in-situ</italic> observations and remote sensing</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Frangoulis</surname>
<given-names>C.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Stamataki</surname>
<given-names>N.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
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</contrib>
<contrib contrib-type="author">
<name>
<surname>Pettas</surname>
<given-names>M.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Michelinakis</surname>
<given-names>S.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>King</surname>
<given-names>A. L.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Giannoudi</surname>
<given-names>L.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
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<contrib contrib-type="author">
<name>
<surname>Tsiaras</surname>
<given-names>K.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/345245"/>
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<contrib contrib-type="author">
<name>
<surname>Christodoulaki</surname>
<given-names>S.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Sepp&#xe4;l&#xe4;</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Thyssen</surname>
<given-names>M.</given-names>
</name>
<xref ref-type="aff" rid="aff6">
<sup>6</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Borges</surname>
<given-names>A.V.</given-names>
</name>
<xref ref-type="aff" rid="aff7">
<sup>7</sup>
</xref>
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<contrib contrib-type="author">
<name>
<surname>Krasakopoulou</surname>
<given-names>E.</given-names>
</name>
<xref ref-type="aff" rid="aff8">
<sup>8</sup>
</xref>
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<aff id="aff1">
<sup>1</sup>
<institution>Institute of Oceanography, Hellenic Centre for Marine Research</institution>, <addr-line>Heraklion</addr-line>, <country>Greece</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Department of Physics, Section of Environmental Physics and Meteorology, National and Kapodistrian University of Athens</institution>, <addr-line>Athens</addr-line>, <country>Greece</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Department of Oceanography, Norwegian Institute for Water Research</institution>, <addr-line>Oslo</addr-line>, <country>Norway</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Institute of Oceanography, Hellenic Centre for Marine Research</institution>, <addr-line>Athens</addr-line>, <country>Greece</country>
</aff>
<aff id="aff5">
<sup>5</sup>
<institution>Research Infrastructure, Finnish Environment Institute</institution>, <addr-line>Helsinki</addr-line>, <country>Finland</country>
</aff>
<aff id="aff6">
<sup>6</sup>
<institution>Aix Marseille Universit&#xe9;, Universit&#xe9; de Toulon, Centre National de la Recherche Scientifique, Institut de Recherche et de D&#xe9;veloppement, Mediterranean Institute of Oceanology</institution>, <addr-line>Marseille</addr-line>, <country>France</country>
</aff>
<aff id="aff7">
<sup>7</sup>
<institution>Chemical Oceanography Unit, Freshwater and OCeanic science Unit of reSearch</institution>, <addr-line>Li&#xe8;ge, Wallonia</addr-line>, <country>Belgium</country>
</aff>
<aff id="aff8">
<sup>8</sup>
<institution>Department of Marine Sciences, University of the Aegean</institution>, <addr-line>Mytilene</addr-line>, <country>Greece</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Abed El Rahman Hassoun, Helmholtz Association of German Research Centres (HZ), Germany</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Naohiro Kosugi, Japan Meteorological Agency, Japan</p>
<p>Marta &#xc1;lvarez, Spanish Institute of Oceanography (IEO), Spain</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: C. Frangoulis, <email xlink:href="mailto:cfrangoulis@hcmr.gr">cfrangoulis@hcmr.gr</email>
</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>15</day>
<month>02</month>
<year>2024</year>
</pub-date>
<pub-date pub-type="collection">
<year>2024</year>
</pub-date>
<volume>11</volume>
<elocation-id>1348161</elocation-id>
<history>
<date date-type="received">
<day>01</day>
<month>12</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>29</day>
<month>01</month>
<year>2024</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2024 Frangoulis, Stamataki, Pettas, Michelinakis, King, Giannoudi, Tsiaras, Christodoulaki, Sepp&#xe4;l&#xe4;, Thyssen, Borges and Krasakopoulou</copyright-statement>
<copyright-year>2024</copyright-year>
<copyright-holder>Frangoulis, Stamataki, Pettas, Michelinakis, King, Giannoudi, Tsiaras, Christodoulaki, Sepp&#xe4;l&#xe4;, Thyssen, Borges and Krasakopoulou</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>The rate of ocean uptake of anthropogenic CO<sub>2</sub> has declined over the past decade, so a critical question for science and policy is whether the ocean will continue to act as a sink. Large areas of the ocean remain without observations for carbonate system variables, and oceanic CO<sub>2</sub> observations have declined since 2017. The Mediterranean Sea is one such an area, especially its eastern part, where there is a paucity of carbonate system data, with large areas not sampled or only sampled by ship-based discrete measurements as opposed to high frequency, sensor-equipped time-series fixed stations. The aim of this study was to analyze a multi-year time-series of high-frequency (hourly) partial pressure CO<sub>2</sub> (pCO<sub>2</sub>) and pH measurements in the Eastern Mediterranean, along with low-frequency (monthly) measurements of total dissolved inorganic carbon and total alkalinity. The pCO<sub>2</sub> time-series was the first obtained in the Eastern Mediterranean. The study was conducted at a fixed platform of the POSEIDON system (Heraklion Coastal Buoy) located near Crete Island. Temperature was the dominant factor controlling the temporal variability of pCO<sub>2</sub> and pH, while the remaining non-thermal variability appeared to be related to evaporation, water mixing, and biological remineralization-production. The air-sea CO<sub>2</sub> fluxes indicated a transition from a winter-spring sink period to a summer-autumn source period. The annual air-sea CO<sub>2</sub> flux was too low (-0.16 &#xb1; 0.02 mol m<sup>-2</sup> yr<sup>-1</sup>) and variable to conclusively characterize the area as a net source or sink of CO<sub>2</sub>, highlighting the need for additional high frequency observation sites. Algorithms were developed using temperature, chlorophyll and salinity data to estimate pCO<sub>2</sub> and total alkalinity, in an effort to provide tools for estimates in poorly observed areas/periods from remotely sensed products. The applicability of the algorithms was tested using Surface Ocean CO<sub>2</sub> Atlas (SOCAT) data from the Eastern Mediterranean Sea (1999 to 2020) which showed that the algorithm pCO<sub>2</sub> estimates were generally within &#xb1;20 &#x3bc;atm of the pCO<sub>2</sub> values reported by SOCAT. Finally, the integration and analysis of the data provided directions on how to optimize the observing strategy, by readapting sensor location and using estimation algorithms with remote sensing data.</p>
</abstract>
<kwd-group>
<kwd>carbonate algorithms</kwd>
<kwd>CO<sub>2</sub> flux</kwd>
<kwd>oligotrophic</kwd>
<kwd>satellite salinity</kwd>
<kwd>source or sink</kwd>
</kwd-group>
<counts>
<fig-count count="7"/>
<table-count count="0"/>
<equation-count count="8"/>
<ref-count count="93"/>
<page-count count="16"/>
<word-count count="8850"/>
</counts>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-in-acceptance</meta-name>
<meta-value>Ocean Observation</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>Although the ocean has absorbed 25 &#xb1; 2% of the total anthropogenic CO<sub>2</sub> emissions from the early 1960s to the late 2010s (<xref ref-type="bibr" rid="B36">Gruber et&#xa0;al., 2023</xref>), a critical question for climate science and climate policy is whether the ocean will continue to act as a sink for this human-induced CO<sub>2</sub> burden (<xref ref-type="bibr" rid="B3">Aric&#xf2; et&#xa0;al., 2021</xref>), as the rate of ocean uptake of anthropogenic CO<sub>2</sub> has declined over the past decade (<xref ref-type="bibr" rid="B32">Friedlingstein et&#xa0;al., 2022</xref>). The answer to this question is becoming more difficult, as the number of oceanic CO<sub>2</sub> observations has almost halved between 2017 and 2023 as shown in the Surface Ocean CO<sub>2</sub> Atlas (SOCAT) data portal version 2023 (<xref ref-type="bibr" rid="B4">Bakker et&#xa0;al., 2023</xref>) increasing the uncertainty in estimates of the oceans&#x2019; role in the carbon pump. This uncertainty is further increased by the sparseness of partial pressure CO<sub>2</sub> (pCO<sub>2</sub>) measurements with limited spatiotemporal coverage, while large areas of the ocean are completely void of observations for carbonate system variables (SOCAT portal, <xref ref-type="bibr" rid="B5">Bakker et&#xa0;al., 2016</xref>).</p>
<p>This global situation is further exacerbated at the scale of the Mediterranean Sea. Although the Mediterranean Sea has been identified as an important anthropogenic carbon storage area because the column inventory is much higher than in the Atlantic or Pacific Oceans (<xref ref-type="bibr" rid="B75">Schneider et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B58">Lee et&#xa0;al., 2011</xref>), there is a general paucity and sparseness in time and space of reliable measurements of the carbonate system variables both in the surface and in the water column (<xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref>).</p>
<p>The Mediterranean Sea carbonate system is unique in several ways: overall high total alkalinity (AT) (especially in the eastern basin), pH values higher than the waters of the North Atlantic and the Pacific Oceans, and dissolved inorganic carbon (CT) values comparable only to the North Pacific Ocean, although induced by different processes (<xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref>). The Mediterranean Sea, with warm, high alkalinity surface waters, a low Revelle factor (close to 10), and corresponding to a high buffering capacity, can contribute to atmospheric CO<sub>2</sub> uptake and transport to the deep and abyssal layers through the active overturning circulation (<xref ref-type="bibr" rid="B75">Schneider et&#xa0;al., 2010</xref>). Some locations in the Mediterranean Sea (e.g. Aegean Sea, Gulf of Lions) with intermediate and deep-water mass formation events (<xref ref-type="bibr" rid="B25">Durrieu de Madron et&#xa0;al., 2005</xref>) have an increased potential to transfer anthropogenic CO<sub>2</sub> to deep layers (<xref ref-type="bibr" rid="B83">Touratier et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B54">Krasakopoulou et&#xa0;al., 2017</xref>). The significant contribution of the Mediterranean Sea outflowing waters to the North Atlantic anthropogenic carbon inventories has already been identified (<xref ref-type="bibr" rid="B10">Carracedo et&#xa0;al., 2018</xref> and references therein). Due to the anti-estuarine circulation at the strait of Gibraltar, the Mediterranean Sea receives natural and anthropogenic carbon from the Atlantic in the surface layer and exports carbon in the deeper layer (<xref ref-type="bibr" rid="B29">Flecha et&#xa0;al., 2019</xref> and references therein). This deep outflow transfers carbon to the intermediate water layers in the Atlantic, where it remains isolated from the atmosphere for several centuries, contributing to CO<sub>2</sub> sequestration (<xref ref-type="bibr" rid="B8">Bethoux et&#xa0;al., 2005</xref>).</p>
<p>The study of the CO<sub>2</sub> cycle in the Mediterranean may prove significant beyond regional questions, as this sea acts as a miniature world ocean, experiencing faster changes of its oceanographic and biogeochemical conditions in response to natural and anthropogenic pressures (<xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref>). In fact, specific processes that also occur in the world ocean can be studied in the Mediterranean Sea at shorter timescales. These include the impact of climate on various hydrodynamic circulation features (e.g. <xref ref-type="bibr" rid="B72">Robinson and Golnaraghi, 1994</xref>; <xref ref-type="bibr" rid="B7">Bergamasco and Malanotte-Rizzoli, 2010</xref>), assessing the functioning of ecosystems with contrasting trophic status (<xref ref-type="bibr" rid="B60">Malanotte-Rizzoli and Eremeev, 1999</xref>), and understanding the functioning of low nutrient-low chlorophyll regions with respect to CO<sub>2</sub> fluxes (<xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>).</p>
<p>The Mediterranean Sea, especially the eastern part, has been undersampled and efforts to observe the carbonate system have mainly been carried out with research vessel (R/V) cruises (<xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref> and references therein; <xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref> and references therein), making it difficult to establish an annual budget as a source or sink of atmospheric CO<sub>2</sub>. The paucity of high-frequency time-series does not allow a full understanding of the drivers of carbonate system temporal variability. High frequency time-series are key for understanding the biological component of carbonate system variability providing information how plankton production and respiration contribute to carbon flux (<xref ref-type="bibr" rid="B27">Fassbender et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B93">Xue et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B64">Parard et&#xa0;al., 2010</xref>). The value of these time-series observations is not only local, as they can be used for deriving relationships between physical and biochemical sea-surface data and the measurable carbonate variables. These relationships can lead to regional remote sensing algorithms which are particularly important for estimating carbonate variables in poorly covered areas. It has been hypothesized that surface temperature, remotely sensed from space, can be used as a tool for extrapolation of CO<sub>2</sub> dynamics over larger spatial scales in the Eastern Mediterranean Sea (<xref ref-type="bibr" rid="B22">D&#x2019;Ortenzio et&#xa0;al., 2008</xref>; <xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>).</p>
<p>Over the last few years, POSEIDON (<ext-link ext-link-type="uri" xlink:href="http://www.poseidon.hcmr.gr">www.poseidon.hcmr.gr</ext-link>), the Eastern Mediterranean ocean observatory dedicated to multiple <italic>in-situ</italic> observations, has been progressively integrating pH and pCO<sub>2</sub> sensors in the Cretan Sea which is the most platform-dense (supersite) subsystem of POSEIDON with two fixed platforms (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>) and moving ones like gliders, Argos and a Ferrybox (<xref ref-type="bibr" rid="B65">Petihakis et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B31">Frangoulis et&#xa0;al., 2019</xref>). These carbonate system observations contribute to the JERICO-coastal research infrastructure, aiming to close the gaps in the coastal ocean monitoring efforts, both in terms of spatio-temporal range of observations and of variables included (<xref ref-type="bibr" rid="B26">Farcy et&#xa0;al., 2019</xref>). Based on observations supported by this infrastructure, the aim of the present paper is to analyze the first high-frequency, multi-year time-series of pCO<sub>2</sub> measurements in the Eastern Mediterranean (Adriatic Sea excluded), in parallel with high-frequency measurements of pH and low-frequency (monthly) discrete measurements of other carbonate system variables such as CT and AT. These analyses will be used to understand the main drivers of the temporal variability of the carbonate system and to evaluate the area as a source or sink of atmospheric CO<sub>2</sub>. These <italic>in-situ</italic> data will be used to develop and evaluate algorithms to estimate sea surface carbonate variables (pCO<sub>2</sub> and AT) using sea surface data (<italic>in-situ</italic> or satellite).</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>    <p>Map of the Eastern Mediterranean Sea with location of Heraklion Coastal Buoy (HCB), E1-M3A buoy and FINOKALIA atmospheric station (bottom left inset). Color tracks (z axis) indicated difference between observed and estimated sea surface pCO<sub>2</sub> (&#x394;<sub>obs-est</sub>), using <xref ref-type="disp-formula" rid="eq8">Equation 8</xref>  with <italic>in-situ</italic> temperature and pCO<sub>2</sub> measurements (from SOCAT dataset). Top right inset shows frequency of observations vs &#x394;<sub>obs-est</sub>. <italic>In-situ</italic> data excluded values above latitude 39.8&#xb0;N and data from the present study.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g001.tif"/>
</fig>
</sec>
<sec id="s2" sec-type="materials|methods">
<label>2</label>
<title>Materials and methods</title>
<p>Data were collected from sensors placed on one of the POSEIDON fixed platforms, the Heraklion Coastal Buoy (HCB), as well as regular (monthly frequency) R/V missions at the same location (35.43&#xb0;N, 25.07&#xb0;E, depth 180 m) (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>). The buoy used during the study period was an Oceanor Wavescan buoy. Details on the buoy configuration can be found in <xref ref-type="bibr" rid="B65">Petihakis et&#xa0;al. (2018)</xref>. Although the nearest coast to HCB is 4 km away and the nearest urban area 11 km away, due to the site depth and the lack of important rivers (<xref ref-type="bibr" rid="B68">Poulos et&#xa0;al., 2009</xref>), the site receives little coastal influence, except during extreme rain events.</p>
<sec id="s2_1">
<label>2.1</label>
<title>Mooring sensors</title>
<sec id="s2_1_1">
<label>2.1.1</label>
<title>Mooring carbonate data</title>
<p>A spectrophotometric pH sensor using non-purified m-cresol purple dye, SP200-SM (Sensorlab), was deployed at subsurface (inlet at 1.5 m), on HCB providing pH data (at total scale) every 3 hours in near real time to the POSEIDON database. A description of the sensor and its principle of operation can be found in <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al. (2016)</xref>. The sensor was tested in the laboratory with TRIS (2-amino-2-hydroxymethyl-1,3-propanediol)-buffer standards prior and after each deployment. The repeated analyses for each of those tests (n = 6) presented accuracy that was within &#xb1;0.002 pH units (close to the ones described by <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>). Discrete samples for pH analysis were also taken during its deployment (see section 2.2.1 discrete carbonate data).</p>
<p>A pCO<sub>2</sub> sensor, CO<sub>2</sub>-Pro Atmosphere (ProOceanus) based on non-dispersive infrared spectrometry, was also deployed on HCB next to the pH sensor, providing air (inlet at 2 m above the surface layer) and seawater (inlet at 1.5 m) CO<sub>2</sub> data every 6 hours in delayed mode. Description of the sensor and its principle of operation can be found in <xref ref-type="bibr" rid="B47">Jiang et&#xa0;al. (2014)</xref>. The sensor was removed from April to August 2021 in order to participate in the Integrated Carbon Observation System (ICOS) pCO<sub>2</sub> instrument inter-comparison workshop. Periods of non-operation in 2022 were for servicing. Three standard gases (351, 420, 493 &#x3bc;atm) were connected to the sensor prior and after each deployment. In addition, during deployment, one standard gas (420 &#x3bc;atm) was connected regularly (6 times over the total deployment period). Based on these laboratory and field data a 3.6 to 4.9 &#x3bc;atm (depending on the gas reference) drift per year was observed. Correction was not applied for this drift as the value obtained was below the uncertainty of the sensor when operating on a mooring, including uncertainties of references (8.7 &#xb1; 14 &#x3bc;atm; <xref ref-type="bibr" rid="B47">Jiang et&#xa0;al., 2014</xref>).</p>
<p>Quality control was applied to pH and pCO<sub>2</sub> sensor data by taking into consideration minimum and maximum ranges, spikes and stuck values.</p>
</sec>
<sec id="s2_1_2">
<label>2.1.2</label>
<title>Mooring ancillary data</title>
<p>The HCB buoy is equipped with sub-surface (at 1 m) sensors for currents, temperature (SST) and salinity (conductivity) (SSS) monitoring, as well as wave (height and direction) and aerial meteorological sensors at 3 m above the surface layer (wind speed and direction, air temperature, atmospheric pressure, humidity). Temperature and salinity (conductivity) data used in the present study were measured by a SBE 37-SIP or SBE 37. Details about other seawater sensors specifications and variables measured can be found in <xref ref-type="bibr" rid="B65">Petihakis et&#xa0;al. (2018)</xref>.</p>
</sec>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Research vessel cruises</title>
<sec id="s2_2_1">
<label>2.2.1</label>
<title>Research vessel cruises discrete carbonate data</title>
<p>During regular (monthly frequency) R/V visits at HCB, water samples were taken near to the CO<sub>2</sub> and pH sensors (at 2 m depth and at 2.5 m horizontal distance from both sensors inlet) and within &#xb1;15 min of sensor measurements. Three samples were taken from different Niskin bottles for pH analysis as well three samples for CT and AT analysis according to the collection and storage recommendations of <xref ref-type="bibr" rid="B21">Dickson et&#xa0;al. (2007)</xref>. The pH samples were analyzed thermostatted at 25&#xb0;C within 6 hours from sampling using a spectrophotometric lab pH instrument with purified m-cresol purple dye (AFT-pH, Sunburst Sensors) which was regularly checked against the TRIS buffer. The measurements of CT and AT were carried out thermostatted at 25&#xb0;C using a VINDTA 3C checked with CRMs. TRIS buffers and CRMs were from Dr. Andrew Dickson, Marine Physical Laboratory, Scripps Institution of Oceanography. Based on the TRIS buffers and CRMs the accuracy was estimated to be &#xb1; 2.0 &#x3bc;mol kg<sup>-1</sup> for AT, &#xb1; 3.0 &#x3bc;mol kg<sup>-1</sup> for CT, and &#xb1;0.004 units for pH. Based on triplicate samples from different Niskin bottles, the precision was estimated to be ~1 &#x3bc;mol kg<sup>-1</sup> for AT, ~3 &#x3bc;mol kg<sup>-1</sup> for CT, and ~0.004 units for pH. During the second year, several major technical issues with the VINDTA 3C analyser prevented access to good quality data.</p>
</sec>
<sec id="s2_2_2">
<label>2.2.2</label>
<title>Research vessel cruises ancillary data</title>
<p>During regular (monthly frequency) R/V visits at HCB, CTD (Conductivity, Temperature, Depth) casts (with SBE19+) were made from surface to close to the bottom, at a distance varying from 20 m to 200 m from HCB. Water samples were also taken at various depths (2, 10, 20, 50, 75, 100, 120 m) for nutrients and chlorophyll a (Chla) determination and stored at -20&#xb0;C until their analysis. For nutrients, the concentration of orthophosphate was measured according to <xref ref-type="bibr" rid="B71">Rimmelin and Moutin (2005)</xref>, the concentration of nitrate, nitrite and silicate according to <xref ref-type="bibr" rid="B79">Strickland and Parsons (1972)</xref> and the concentration of dissolved ammonium according to <xref ref-type="bibr" rid="B46">Ivan&#x10d;i&#x10d; and Degobbis (1984)</xref>. The detection limits for phosphate (PO<sub>4</sub>), nitrate+nitrite (NO<sub>3</sub>+NO<sub>2</sub>), silicate (SiO<sub>4</sub>) and ammonium (NH<sub>4</sub>) were 0.8 nM, 0.017, 0.10 and 0.019 &#x3bc;M, respectively. Chla was measured fluorometrically (<xref ref-type="bibr" rid="B42">Holm-Hansen et&#xa0;al., 1965</xref>) as described in <xref ref-type="bibr" rid="B55">Lagaria et&#xa0;al. (2017)</xref>.</p>
</sec>
</sec>
<sec id="s2_3">
<label>2.3</label>
<title>Calculation of derived parameters of the carbonate system</title>
<p>Derived seawater carbonate system parameters, using pairs of measured carbonate variables were estimated using the software program CO2SYS (version 3.0, <xref ref-type="bibr" rid="B66">Pierrot et&#xa0;al., 2021</xref>) considering temperature, salinity and nutrient concentrations (silicate and phosphate) and with the output from CO2SYS at <italic>in-situ</italic> temperature conditions. The pH data from the pH sensor collected at <italic>in-situ</italic> temperature were converted to pH at 25&#xb0;C using the CO2SYS program and AT estimated from salinity (see below).</p>
<p>Carbonate variables were estimated using pairwise combination of carbonate variables (using CO2SYS, version 3.0, <xref ref-type="bibr" rid="B66">Pierrot et&#xa0;al., 2021</xref>). For estimations of AT, CT and pH (using pH&amp;CT, pH&amp;AT, and AT&amp;CT, respectively), we followed the recommendation by <xref ref-type="bibr" rid="B2">&#xc1;lvarez et&#xa0;al. (2014)</xref> based upon a large Mediterranean pH&amp;AT&amp;CT dataset: carbonic acid dissociation constants K1 and K2 from <xref ref-type="bibr" rid="B61">Mehrbach et&#xa0;al. (1973)</xref> as refitted by <xref ref-type="bibr" rid="B20">Dickson and Millero (1987)</xref> and the dissociation constant for HSO<sub>4</sub>
<sup>-</sup> from <xref ref-type="bibr" rid="B19">Dickson (1990)</xref>. The Root Mean Square Deviation (RMSD) between observed and estimated values of AT, CT and pH were 19.5 &#x3bc;mol kg<sup>-1</sup>, 17.6 &#x3bc;mol kg<sup>-1</sup> and 0.033 pH units, respectively. For estimations of pCO<sub>2</sub> (using AT&amp;CT, pH&amp;AT, pH&amp;CT), various CO2SYS program options were tested (as pCO<sub>2</sub> measurements were not performed by <xref ref-type="bibr" rid="B2">&#xc1;lvarez et&#xa0;al., 2014</xref>) to identify the K1, K2 option that gave the lowest &#x394;pCO<sub>2 obs-est</sub>. Although the present study is the first in the Mediterranean Sea measuring four variables: AT, CT, pH (bottle data) and CO<sub>2</sub> (sensor data), and thus could in principle be used to examine internal consistency, this was attempted but abandoned due to several reasons explained in <xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Material</bold>
</xref>. Therefore, the same K1, K2 option for estimating CO<sub>2</sub> (using AT&amp;CT, pH&amp;AT) as above (<xref ref-type="bibr" rid="B2">&#xc1;lvarez et&#xa0;al., 2014</xref>) was deemed more appropriate and internally consistent. Using this option the comparison of seawater pCO<sub>2</sub> from the sensor with calculated pCO<sub>2</sub> had RMSD ~29 and 9 &#x3bc;atm when calculated from AT&amp;CT and pH&amp;AT, respectively.</p>
<p>The method proposed by <xref ref-type="bibr" rid="B82">Takahashi et&#xa0;al. (2002)</xref>, with terminology as adapted by <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al. (2016)</xref>, was used in order to estimate the variability of pCO<sub>2</sub> recorded by the buoy sensor resulting from the contribution of the thermal (pCO<sub>2TH</sub>) and non-thermal (pCO<sub>2NT</sub>) control using the <xref ref-type="disp-formula" rid="eq1">Equations 1</xref> and <xref ref-type="disp-formula" rid="eq2">2</xref>:</p>
<disp-formula id="eq1">
<label>(1)</label>
<mml:math display="block" id="M1">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mtext>TH</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:msup>
<mml:mtext>mean&#xa0;</mml:mtext>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mtext>exp</mml:mtext>
<mml:mo stretchy="false">(</mml:mo>
<mml:msup>
<mml:mn>0.0423&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mtext>SST</mml:mtext>
<mml:mo>&#x2212;</mml:mo>
<mml:mtext>SSTmean</mml:mtext>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula id="eq2">
<label>(2)</label>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mtext>NT</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mtext>&#xa0;pCO</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
<mml:mo>&#x2217;</mml:mo></mml:msubsup>
<mml:mtext>exp</mml:mtext>
<mml:mo stretchy="false">(</mml:mo>
<mml:msup>
<mml:mn>0.0423&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mtext>SSTmean</mml:mtext>
<mml:mo>&#x2212;</mml:mo>
<mml:mtext>SST</mml:mtext>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where pCO<sub>2</sub> and SST are the values obtained from HCB seawater sensors and pCO<sub>2</sub>mean (410 &#x3bc;atm) and SSTmean (20.58&#xb0;C) their respective annual mean values.</p>
</sec>
<sec id="s2_4">
<label>2.4</label>
<title>Air-sea CO<sub>2</sub> flux</title>    <p>The air-sea interface CO<sub>2</sub> exchange flux FCO<sub>2</sub>, (mmol m<sup>-2</sup> d<sup>-1</sup>) calculation was made according to <xref ref-type="disp-formula" rid="eq3">Equation 3</xref> from <xref ref-type="bibr" rid="B88">Wanninkhof (2014)</xref>
</p>
<disp-formula id="eq3">
<label>(3)</label>
<mml:math display="block" id="M3">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>FCO</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mtext>k&#xa0;</mml:mtext>
<mml:mo>&#x2217;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mtext>&#xa0;K</mml:mtext>
</mml:mrow>
<mml:mn>0</mml:mn>
<mml:mo>&#x2217;</mml:mo></mml:msubsup>
<mml:mtext>&#xa0;</mml:mtext>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msubsup>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
<mml:mrow>
<mml:mtext>&#xa0;&#xa0;SW</mml:mtext>
</mml:mrow>
</mml:msubsup>
<mml:mo>&#x2212;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mtext>&#xa0;pCO</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
<mml:mrow>
<mml:mtext>&#xa0;&#xa0;ATM</mml:mtext>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
</disp-formula>    <p>where K<sub>0</sub> (moles L<sup>-1</sup> atm<sup>-1</sup>) is the solubility of CO<sub>2</sub> in seawater (<xref ref-type="bibr" rid="B89">Weiss, 1974</xref>), and pCO<sub>2</sub>
<sup>SW</sup> and pCO<sub>2</sub>
<sup>ATM</sup> are the surface seawater and atmospheric partial pressure of CO<sub>2</sub> (&#x3bc;atm) and k (cm h<sup>-1</sup> by convention <xref ref-type="disp-formula" rid="eq4">Equation 4</xref>) is the gas transfer coefficient expressed as</p>
<disp-formula id="eq4">
<label>(4)</label>
<mml:math display="block" id="M4">
<mml:mrow>
<mml:mtext>k</mml:mtext>
<mml:mo>=</mml:mo>
<mml:msup>
<mml:mn>0.251&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msubsup>
<mml:mtext>U</mml:mtext>
<mml:mn>10</mml:mn>
<mml:mrow>
<mml:mtext>&#xa0;&#xa0;&#xa0;&#xa0;</mml:mtext>
<mml:mn>2</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:mrow>
</mml:msubsup>
<mml:msup>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mtext>Sc</mml:mtext>
<mml:mo stretchy="false">/</mml:mo>
<mml:mn>660</mml:mn>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2013;</mml:mo>
<mml:mn>0.5</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where U<sub>10</sub> is the wind speed (m s<sup>-1</sup>), Sc is the CO<sub>2</sub> Schmidt number (dimensionless) normalized to 660 (the Sc for CO<sub>2</sub> in seawater at 20&#xb0;C and salinity 35) and the coefficient 0.251 has units of (cm h<sup>-1</sup>) (m s<sup>-1</sup>)<sup>-2</sup>.</p>
<p>A positive flux indicates a release of CO<sub>2</sub> from the ocean toward the atmosphere.</p>
<p>Fluxes of CO<sub>2</sub> were computed using pCO<sub>2</sub>
<sup>SW</sup> from HCB, pCO<sub>2</sub>
<sup>ATM</sup> data from nearest (54 km distance) land-based coastal atmosphere observation station of FINOKALIA and wind data from HCB (measured every 3 h). Description of FINOKALIA station (<ext-link ext-link-type="uri" xlink:href="https://www.icos-cp.eu/observations/national-networks/icos-greece">https://www.icos-cp.eu/observations/national-networks/icos-greece</ext-link>) and its air CO<sub>2</sub> time-series can be found in <xref ref-type="bibr" rid="B34">Gialesakis et&#xa0;al. (2023)</xref>. Wind data from the nearest (34 km distance) sea-based meteorological station of E1-M3A were used to complete meteorological data gaps of HCB (air pressure, wind). Description of E1-M3A can be found in <xref ref-type="bibr" rid="B65">Petihakis et&#xa0;al. (2018)</xref>. Wind speed measurements obtained at 3 m were adjusted to 10 m above sea surface (U<sub>10</sub>) based on <xref ref-type="bibr" rid="B44">Hsu et&#xa0;al. (1994)</xref>. Due to a gap of wind data from 07/06/2021 to 12/09/21 (in both HCB and E1-M3A), a constant value of wind speed (5.50 m s<sup>-1</sup>) was used during that period, obtained by the average of summer values from the E1-M3A time-series data (ten years).</p>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results</title>
<sec id="s3_1">
<label>3.1</label>
<title>Hydrography, Chla and nutrients</title>
<p>Subsurface temperature and salinity have been measured at the POSEIDON HCB mooring site since 2016. Between November 2020 and May 2023, the mooring captured seasonal variability in temperature and salinity over the ~2.5 year observation period (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>). There were some minor gaps in the salinity data (mostly &lt;3 day periods), while a larger gap occurred from mid-July to November 2022. Over the ~2.5 year observation period, the SST ranged from 15.3&#xb0;C in winter to 28.3&#xb0;C in summer. According to the entire temperature and salinity data record of HCB station (available at <ext-link ext-link-type="uri" xlink:href="https://poseidon.hcmr.gr">https://poseidon.hcmr.gr</ext-link>) the hydrological situation over the studied period showed no extreme climatic events. The drop in salinity observed in May 2022 could be due to the intrusion of a different water mass (see Discussion). The SST satellite product (daily values) showed a consistent relationship with the <italic>in-situ</italic> data during the entire period (<xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>). The SSS satellite product (weekly values) difference with <italic>in-situ</italic> data varied generally between ~0.2 and ~0.4 units.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Time series of temperature (&#xb0;C) (top panel) and salinity (lower panel) at HCB buoy from sensors on buoy (black dots) and from satellite data (green dots).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g002.tif"/>
</fig>
<p>The variations in Chla concentration over the studied period displayed smooth seasonal patterns (especially 0-120 m mean depth-integrated values), with somewhat higher values in winter-spring (December to May) and lower in summer-autumn (June to November). The highest concentrations were observed during spring 2022 which was the only time during the study period when Chla exceeded ~0.2 &#xb5;g L<sup>-1</sup> (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>). Mean depth-integrated Chla values during the summer-autumn period were generally greater than surface Chla values, reflecting the deepening of the Chla maximum. The Chla satellite product was generally higher than <italic>in-situ</italic> surface data with the difference being generally less that ~0.05 &#xb5;g L<sup>-1</sup>.</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Time series of chlorophyll a (Chla in &#x3bc;g L<sup>-1</sup>) at HCB Station from bottle data (black dots), from bottle data integrated over 120 m (white dots) and from satellite data (blue dots-line).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g003.tif"/>
</fig>
<p>The variations in inorganic nutrients surface concentrations over the studied period (<xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Material Figure&#xa0;1</bold>
</xref>) were overall low (&lt;0.92 &#x3bc;M for NO<sub>3</sub>+NO<sub>2</sub>, &lt;0.02 &#x3bc;M for PO<sub>4</sub>, &lt;0.88 &#x3bc;M for NH<sub>4</sub>, &lt;1.50 &#x3bc;M for SiO<sub>4</sub>) without any distinct seasonal pattern.</p>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Carbonate system variables</title>
<sec id="s3_1_1">
<label>3.2.1</label>
<title>Carbonate data</title>
<p>
<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref> shows the time-series variations of the measured sea surface carbonate system variables. For pH, twenty months of continuous records were obtained from the <italic>in-situ</italic> sensor at a frequency of 3 hours. The pH at <italic>in-situ</italic> temperature ranged from 7.97 (July) to 8.13 (February-March). During the last seven months (January-July 2022), pH measurements were less precise (the spread of data increased) which was mostly due to issues with the sensor&#x2019;s operation, which was consequently removed for servicing in July 2022. Bottle pH data were collected periodically during the entire period of sensor deployment and also for the period between July 2022-March 2023 when the sensor was not deployed. Bottle pH and sensor pH data had a RMSD = 0.006 pH units. Part of the difference observed between the two methods (-0.001 &#xb1; 0.006 pH units) could be due to the pH lab analysis using purified m-cresol purple (<xref ref-type="bibr" rid="B59">Liu et&#xa0;al., 2011</xref> for calculations) versus the sensor using non-purified m-cresol purple (<xref ref-type="bibr" rid="B14">Clayton and Byrne, 1993</xref> for calculations). In fact, non-purified m-cresol purple can result in differences of -0.001 to ~-0.02 depending on which m-cresol purple brand/batch is used and at what pH range (<xref ref-type="bibr" rid="B23">Douglas and Byrne, 2017</xref>).</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>Time series of carbonate variables at the HCB buoy at subsurface (2 m). <bold>(A)</bold> pH data from sensor on buoy at <italic>in-situ</italic> temperature (black dots) and at 25&#xb0;C (grey dots) together with pH from bottle data at 25&#xb0;C (green dots). <bold>(B)</bold> pCO<sub>2</sub> data from sensor on buoy (black dots), estimated pCO<sub>2</sub> from bottle pH and AT data (green dots), estimated pCO<sub>2</sub> from pH and sea surface salinity (SSS) data from buoy sensors (blue line), <bold>(C)</bold> AT from discrete measurements (green dots), AT data estimated from SSS data from buoy sensor (black dots) and AT estimated from SSS satellite data (blue dots). <bold>(D)</bold> CT from bottle data (green dots), CT data estimated from discrete measurements of pH and AT (blue dots) and CT estimated from pH&amp;SSS (grey dots).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g004.tif"/>
</fig>
<p>For pCO<sub>2</sub>, nineteen months of data were obtained (with 17 months at high frequency i.e. 6 hours) within a total period of 31 months. The densest period of data recording was 11 months within the period from April 2022 to May 2023. Periods of interruption were due to participation in an ICOS workshop (2021) and for servicing and maintenance. pCO<sub>2</sub> data was acquired during all months except August, September and mid-January to mid-February. The seawater pCO<sub>2</sub> values over the period of measurements ranged from ~350 &#x3bc;atm (March and April) to ~500 &#x3bc;atm (September). Concurrently, CO<sub>2</sub> and pH were measured over a total period of 12 months.</p>
<p>AT and CT bottle data were obtained mainly during the first year (during the second year several major technical issues with the VINDTA 3C analyzer impacted the amount of high-quality data). During the first year AT varied between 2628 and 2654 &#x3bc;mol kg<sup>-1</sup>, decreasing from December to March, then increasing from April to October.</p>
<p>When excluding one seasonal deviation (December 2020), AT was linearly related to SSS (r<sup>2</sup> = 0.7, p&lt; 0.0001, n=39, <xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Material Figure&#xa0;3</bold>
</xref>) according to:</p>
<disp-formula id="eq5">
<label>(5)</label>
<mml:math display="block" id="M5">
<mml:mrow>
<mml:mtext>AT</mml:mtext>
<mml:mo>=</mml:mo>
<mml:msup>
<mml:mtext>SSS&#xa0;</mml:mtext>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mn>59</mml:mn>
<mml:mo>+</mml:mo>
<mml:mn>314</mml:mn>
</mml:mrow>
</mml:math>
</disp-formula>
<p>with &#x394;AT<sub>obs-est</sub> having a RMSD ~6.3 &#x3bc;mol kg<sup>-1</sup>.</p>
<p>Bottle CT data varied between 2236 and 2300 &#x3bc;mol kg<sup>-1</sup> without a clear seasonal pattern. CT was also estimated from other variables, as described in the next section.</p>
</sec>
<sec id="s3_1_2">
<label>3.2.2</label>
<title>Estimation algorithms</title>
<p>The relationship found between AT and SSS (see previous section) was used to estimate AT from SSS from buoy sensor (buoySSS) and satellite SSS (satSSS) data (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>) downloaded from COPERNICUS (see data availability for the exact reference). These derived AT<sub>buoysss</sub> data were used in combination with the pH <italic>in-situ</italic> data (from sensor) to calculate CT (CT<sub>buoySSS&amp;pH</sub>) and pCO<sub>2</sub> (pCO<sub>2buoySSS&amp;pH</sub>) using CO2SYS with the above-mentioned options. The obtained estimate CT<sub>buoySSS&amp;pH</sub> data giving indication of the seasonal variability of CT (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>) should be considered with caution as it is based on the AT relationship to salinity (previous section). The obtained estimate of pCO<sub>2buoySSS&amp;pH</sub> data when compared to CO<sub>2</sub> sensor data showed a RMSD= 17 &#x3bc;atm.</p>
<p>Algorithms were developed to calculate sea surface pCO<sub>2</sub> with exclusive use of satellite SST and Chla data downloaded from COPERNICUS (see data availability for the exact reference). A linear regression model (cftool, MATLAB) was applied that used a quadratic polynomial, univariate for the SST algorithm and bivariate for SST and Chla algorithm. The regression model used a linear square differences method to fit the <italic>in-situ</italic> pCO<sub>2</sub> data. The satellite data fused to the regression model were first normalized to their mean and standard deviation value. Coefficients of the regression model/algorithms were calculated with 95% confidence bounds and the goodness of fit was evaluated through R-squared and RMSE.</p>
<p>The first algorithm (<xref ref-type="disp-formula" rid="eq6">Equation 6</xref>) was based on a single variable, satellite SST (satSST):</p>
<disp-formula id="eq6">
<label>(6)</label>
<mml:math display="block" id="M6">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mtext>&#xa0;satSST</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mtext>&#xa0;</mml:mtext>
<mml:msup>
<mml:mn>0.8627&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mtext>satSST</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mn>25.225&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mtext>satSST</mml:mtext>
<mml:mo>+</mml:mo>
<mml:mn>542</mml:mn>
</mml:mrow>
</mml:math>
</disp-formula>    <p>The second algorithm (<xref ref-type="disp-formula" rid="eq7">Equation 7</xref>) was based on two variables, satellite SST and Chla (satChla):</p>
<disp-formula id="eq7">
<label>(7)</label>
<mml:math display="block" id="M7">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mtext>&#xa0;satSST&amp;Chla</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>704</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mn>32.145&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mtext>satSST</mml:mtext>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mn>1983.2&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mtext>satChla</mml:mtext>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mn>0.9152&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mtext>satSST</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mn>48.656&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msup>
<mml:mtext>satSST&#xa0;</mml:mtext>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mtext>satChla</mml:mtext>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mn>5354.5&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mtext>satChla</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>Estimated pCO<sub>2</sub> from SST (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>) compared to sensor data displayed a RMSD= 13 &#x3bc;atm, while using the estimate from SST&amp;Chla (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>) the RMSD value was 14 &#x3bc;atm.</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>Measured pCO<sub>2</sub> (black dots), and estimated pCO<sub>2</sub> from pH and SSS data from buoy sensors (blue interrupted line), from SST satellite data (orange line) and from SST&amp;Chla satellite data (green line).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g005.tif"/>
</fig>    <p>To test the validity of the algorithm pCO<sub>2satSST</sub> over a wider spatiotemporal scale, available data of <italic>in-situ</italic> sea surface pCO<sub>2</sub> with their respective temperature measurements from the Eastern Mediterranean Sea (selected area shown in <xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>) were taken from SOCAT database with addition of one previously unpublished dataset (<xref ref-type="bibr" rid="B52">Krasakopoulou and Rapsomanikis, 2023</xref>), hereinafter together referred to as &#x201c;SOCAT dataset&#x201d;. Data were available in 1999, 2006, 2008, 2015, 2016, 2018 and 2020-2022. After excluding data from 2020-2022, which were the ones in the present study, the remaining dataset had 37372 values. After exclusion from this dataset the data collected at salinities below 35 PSU (i.e. above 39.8&#xb0;N latitude, North Aegean and Dardanelles straits), a large part of which showed high &#x394;<sub>obs-est</sub>, the remaining dataset (35179 values) was used to modify the <xref ref-type="disp-formula" rid="eq6">Equation 6</xref> to make it applicable at the period 1999 to 2019 and the area from 32.0&#xb0;N to 39.0&#xb0;N and from 19.5&#xb0;E to 32.0&#xb0;E (<xref ref-type="disp-formula" rid="eq8">Equation 8</xref>):</p>
<disp-formula id="eq8">
<label>(8)</label>
<mml:math display="block" id="M8">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>pCO</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mtext>&#xa0;satSST</mml:mtext>
<mml:mo>+</mml:mo>
</mml:mrow>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:msup>
<mml:mn>0.8627&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mtext>satSST</mml:mtext>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mn>25.225&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mtext>satSST</mml:mtext>
<mml:mo>+</mml:mo>
<mml:mn>554</mml:mn>
<mml:mo>+</mml:mo>
<mml:msup>
<mml:mn>1.7&#xa0;</mml:mn>
<mml:mo>&#x2217;</mml:mo>
</mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mn>2019</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mtext>y</mml:mtext>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where the last term accounts for the long-term increase of pCO<sub>2</sub>, with y being the year. Using this algorithm, the deltas obtained varied between -40 and +40 &#x3bc;atm (<xref ref-type="fig" rid="f1"><bold>Figure 1</bold></xref>) with 91% of values being between -20 and +20 &#x3bc;atm.</p>
</sec>
<sec id="s3_1_3">
<label>3.2.3</label>
<title>Thermal vs non-thermal effects on pCO<sub>2</sub>
</title>
<p>The contribution of the thermal and non-thermal control on the pCO<sub>2</sub> variations recorded by the buoy sensor was examined in <xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref> (CO<sub>2</sub> sensor data gaps were completed by pCO<sub>2buoySSS&amp;pH</sub>). The thermal/non-thermal ratio was lower than 1 (<xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Material Figure&#xa0;1</bold>
</xref>) for almost 6 months in winter-spring (mid-December to May, with minimum ratio ~0.7 at March-April), indicating that non-thermal drivers exerted a greater control than temperature during that period. The ratio was above 1; hence, thermal control was predominant in the remaining 6 months in summer-autumn (June to early December, maximum ratio ~1.5 in July-August) (<xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Material Figure&#xa0;3</bold>
</xref>). Although the periods during which thermal or non-thermal controls predominate were almost equal, when the magnitude of the change they produce is examined (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>), it appears that the thermal term was more than twice as large as the non-thermal term.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>Thermal and non-thermal components of pCO<sub>2</sub> (&#x3bc;atm, estimated from pH and SSS data, blue line in <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>) calculated respectively from <xref ref-type="disp-formula" rid="eq1">Equations 1</xref>, <xref ref-type="disp-formula" rid="eq2">2</xref> and expressed as difference from measured values (&#x394;pCO<sub>2</sub>). Smoothed curves were created from the data points shown using the least-squares spline approximation (spap2 function of Matlab R2018b*) with the spline of order 3.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g006.tif"/>
</fig>
</sec>
</sec>
<sec id="s3_3">
<label>3.3</label>
<title>Air-sea CO<sub>2</sub> fluxes</title>
<p>The area acted as a sink of atmospheric CO<sub>2</sub> during approximately 7.5 months in winter-spring, between mid-October and May, and as source during approximately 4.5 months in summer-autumn, between June and mid-October. In the winter-spring (sink) period, the highest negative flux was -18.0 mmol CO<sub>2</sub> m<sup>-2</sup> d<sup>-1</sup>, whereas the summer-autumn (source) period the highest positive flux was +13.1 mmol m<sup>-2</sup> d<sup>-1</sup>. A strong variability was observed in both periods (+3.8 &#xb1; 2.3 and -3.5 &#xb1; 3.5 mmol m<sup>-2</sup> d<sup>-1</sup>) with wind being the main driver of the flux variability (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref>). To estimate the net flux over the entire source/sink acting periods, sea surface pCO<sub>2</sub> data-lacking periods were completed using pCO<sub>2buoySSS&amp;pH</sub>, and the remaining gaps using pCO<sub>2satSST&amp;Chla</sub>. Based on this composite pCO<sub>2</sub> dataset, the total flux integrated over the sink period was between -834 and -662 mmol CO<sub>2</sub> m<sup>-2</sup> (over 219 and 234 days, during the first- and second-year period respectively), whereas the total flux integrated over the source period was between +607 and +563 mmol CO<sub>2</sub> m<sup>-2</sup> (over 154 and 144 days, during the first- and second-year period respectively). The estimated annual flux ranged between -0.23 &#xb1; 0.02 and -0.10 &#xb1; 0.01 mol CO<sub>2</sub> m<sup>-2</sup> y<sup>-1</sup> (during the first- and second-year period respectively).</p>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>    <p>Daily average values of CO<sub>2</sub> air-sea flux calculated using daily average values of <italic>in-situ</italic> wind measured at HCB and E1-M3A, temperature and salinity measured at HCB (salinity data gaps completed by annual average), air CO<sub>2</sub> from FINOKALIA station and seawater pCO<sub>2</sub> data: from pCO<sub>2</sub> sensor at HCB (black line), estimated using AT derived from sensor SSS (<xref ref-type="disp-formula" rid="eq5">Equation 5</xref>) and sensor pH (blue line), estimated using AT derived from buoy sensor SSS (<xref ref-type="disp-formula" rid="eq5">Equation 5</xref>) and buoy sensor pH with constant wind (green line) and estimated using satellite SST and Chla (<xref ref-type="disp-formula" rid="eq7">Equation 7</xref>) (grey line). A positive flux indicates a release of CO<sub>2</sub> from the ocean toward the atmosphere. Due to a gap of wind data from 07/06/2021 to 12/09/21, a constant value of wind speed (5.50 m s<sup>-1</sup>) was used during that period, obtained by the average of summer values from the E1-M3A time-series data.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-11-1348161-g007.tif"/>
</fig>
</sec>
</sec>
<sec id="s4" sec-type="discussion">
<label>4</label>
<title>Discussion</title>
<sec id="s4_1">
<label>4.1</label>
<title>Time-series observations in the Eastern Mediterranean Sea</title>
<p>There are few time-series stations in the Mediterranean that monitor the carbonate system, with the vast majority being in the northwestern Mediterranean and the Northern Adriatic (<xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref> and references therein; <xref ref-type="bibr" rid="B11">Champenois and Borges, 2021</xref>; <xref ref-type="bibr" rid="B92">Wimart-Rousseau et&#xa0;al., 2023</xref>). Among these, high-frequency (daily to hourly scale) published data in the Eastern Mediterranean are found sporadically in the Northern Adriatic (e.g. <xref ref-type="bibr" rid="B85">Turk et&#xa0;al., 2010</xref>, <xref ref-type="bibr" rid="B84">2013</xref>) although initiatives are maintained (<xref ref-type="bibr" rid="B45">ICOS RI, 2022</xref>), and one year in the Saronikos Gulf (<xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>). The eutrophic Northern Adriatic is a particular case where the carbonate system in under strong riverine influence and strong benthic pelagic coupling due to its shallowness (<xref ref-type="bibr" rid="B86">Urbini et&#xa0;al., 2020</xref> and references therein), thus not representative of the generally oligotrophic and deep system of the Eastern Mediterranean and therefore we will not include it in the following when mentioning &#x201c;Eastern Mediterranean&#x201d;. Time-series in the remaining Eastern Mediterranean are in the South-Eastern Levantine sub-basin (5- to 6-year cycles in Lebanese and Israeli coast, respectively <xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B39">Hassoun et&#xa0;al., 2019</xref>) and one in the Aegean Sea (one-year cycle in Saronikos Gulf; <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>). Furthermore, a fourth one-year cycle in the North-Western Levantine (South of Crete) could be considered a reconstructed time-series out of three cruises and Argo floats casts (<xref ref-type="bibr" rid="B91">Wimart-Rousseau et&#xa0;al., 2021</xref>). In fact, the carbonate observing effort devoted to the Eastern Mediterranean, has been essentially with R/V cruises, mostly measuring CT, AT and pH (<xref ref-type="bibr" rid="B91">Wimart-Rousseau et&#xa0;al., 2021</xref> and references therein; <xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref> and references therein; <xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref> and references therein). In addition, high frequency (hourly to daily scale) measurements are also scarce in the Mediterranean (<xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref> and references therein), with the Eastern Mediterranean having before the present study only one annual high frequency cycle of pH (<xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>).</p>
</sec>
<sec id="s4_2">
<label>4.2</label>
<title>Drivers</title>
<p>Observations at high frequency are important as they provide more information on changes in ocean chemistry essential for the assessment of the marine ecosystem&#x2019;s responses to warming, eutrophication, and the oceanic CO<sub>2</sub> uptake (<xref ref-type="bibr" rid="B28">Flecha et&#xa0;al., 2015</xref>), on how diel variations in plankton production and respiration contribute to the variability of the carbonate system (<xref ref-type="bibr" rid="B43">Honkanen et&#xa0;al., 2021</xref>), as well as on developing/validating algorithms and exploring drivers connected with sub-mesoscale phenomena. Measuring from moving platforms may compromise the results as biological diurnal oscillations may not be appropriately accounted for (<xref ref-type="bibr" rid="B43">Honkanen et&#xa0;al., 2021</xref>). The present study provides the first marine pCO<sub>2</sub> time series in the Eastern Mediterranean measuring pCO<sub>2</sub> directly and at high frequency (hourly scale) and the second pH time-series cycle also at high frequency (a previous annual cycle done in Saronikos Gulf in 2013; <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>). This allowed for the examination of the drivers of surface pCO<sub>2</sub> and pH temporal variability over a period of almost two years. In the area studied the strong seasonal variability and low values of net air-sea CO<sub>2</sub> flux demonstrate the need of high frequency <italic>in-situ</italic> observations (including measurements of pCO<sub>2</sub>, temperature and wind speed) in order to reduce the uncertainty of the estimation.</p>
<p>Temperature plays a major role in driving seawater pCO<sub>2</sub> and pH variability whereas changes induced by non-thermal processes are considered to be mainly due to biological activity, but could also include changes due to advection, vertical diffusion, and air-sea gas exchanges (<xref ref-type="bibr" rid="B81">Takahashi et&#xa0;al., 1993</xref>). The main drivers in determining pCO<sub>2</sub> and pH on continental shelves include water temperature, water mixing, presence of organic matter in river plumes and biological control. At the low latitudes non-upwelling shelves, which are typically oligotrophic, the biological pump is less effective (review by <xref ref-type="bibr" rid="B13">Chen et&#xa0;al., 2013</xref>). Therefore, the importance of pCO<sub>2</sub> seawater variability due to biological control is revisited in the Eastern Mediterranean (<xref ref-type="bibr" rid="B91">Wimart-Rousseau et&#xa0;al., 2021</xref>). Decomposing the drivers contributing to thermal control (pCO<sub>2TH</sub>) and non-thermal control (pCO<sub>2NT</sub>) (which in general cancel each other out) is important for understanding which drivers are more important (<xref ref-type="bibr" rid="B50">Ko et&#xa0;al., 2021</xref>). In our study area and period, we infer that pCO<sub>2TH</sub> was the main factor followed by pCO<sub>2NT</sub> due to evaporation, water mixing and biological remineralization-production, as explained below. Temperature is the dominant factor controlling the diel to seasonal variability of pCO<sub>2</sub> (and pH), as previously described by other studies in the Eastern Mediterranean (<xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B90">Wimart-Rousseau et&#xa0;al., 2020</xref>). The observed annual cycle of pCO<sub>2NT</sub> was similar to the one described in the North-Western Mediterranean (<xref ref-type="bibr" rid="B62">Merlivat et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B92">Wimart-Rousseau et&#xa0;al., 2023</xref>), however with biological control (remineralisation-production) and evaporation being the main non-thermal drivers, as suggested for the North-Western Levantine (<xref ref-type="bibr" rid="B91">Wimart-Rousseau et&#xa0;al., 2021</xref>). Starting from March, the pCO<sub>2NT</sub> decrease from March to May would be associated with photosynthetic uptake (decreasing CT and slightly increasing AT) as indicated by Chla higher values and progressively also associated with evaporation (mainly increasing AT). Then from June to September, the decrease of pCO<sub>2NT</sub> would be linked to the effect of AT increase related to evaporation (indicated by the salinity increase) as well as, but to a lesser extent, to autotrophic processes. The effect of remineralization would increase progressively from summer onwards. In fact though the biomass of heterotrophs is higher than autotrophs in this oligotrophic area during summer (<xref ref-type="bibr" rid="B77">Siokou-Frangou et&#xa0;al., 2002</xref>), the low amount of organic matter reduces the importance of remineralization in summer. It is only after accumulation of organic matter, with simultaneous decrease of autotrophic and evaporation processes that the increase of pCO<sub>2NT</sub> due to remineralization would appear in October (initiating the increase of CT). This increase of pCO<sub>2NT</sub> (and CT) would be supported by winter water mixing after December for a period lasting 1 to 3 months (<xref ref-type="bibr" rid="B53">Krasakopoulou et&#xa0;al., 2009</xref>; Tsiaras et&#xa0;al., this issue). Then pCO<sub>2NT</sub> increase would progressively be slowed down by autotrophs after February, closing the annual cycle. On the other hand, physical factors other than evaporation (i.e. land-based fluxes, precipitation, lateral advection) appear to play a minor role in the pCO<sub>2NT</sub> in the study area and period. In fact, land-based water fluxes are generally low as there are only small rivers in the area (<xref ref-type="bibr" rid="B68">Poulos et&#xa0;al., 2009</xref>) and as precipitation data (from land-based meteorological station data located in Heraklion city, <xref ref-type="bibr" rid="B56">Lagouvardos et&#xa0;al., 2017</xref>) showed no significant rain events during the period of pCO<sub>2</sub> records (as confirmed by the absence of salinity decreases at HCB during rain events). Lateral advection appears to have negligible effect in pCO<sub>2NT</sub> at HCB. At this location, depending on the prevailing circulation pattern, local high salinity surface water shares occasionally the surface layers with less saline Modified Atlantic Water (MAW), karst waters (<xref ref-type="bibr" rid="B33">Georgopoulos et&#xa0;al., 2000</xref>) or Modified Black Sea Water (MBSW) (<xref ref-type="bibr" rid="B87">Velaoras et&#xa0;al., 2019</xref>; <xref ref-type="bibr" rid="B49">Kassis and Korres, 2021</xref>). A surface water mass of MAW or MBSW could explain the drop in salinity observed in May 2021 (but not karst waters since AT-SSS relation was not affected). This water mass intrusion did not affect pCO<sub>2</sub>.</p>
</sec>
<sec id="s4_3">
<label>4.3</label>
<title>Air-sea CO<sub>2</sub> flux</title>    <p>Marginal seas are often an important sink for atmospheric CO<sub>2</sub> and overall play a significant role in the global carbon cycle, as they transfer carbon to deeper layers, however, not all marginal seas are CO<sub>2</sub> sinks and some function as CO<sub>2</sub> sources (<xref ref-type="bibr" rid="B9">Borges, 2005</xref>; <xref ref-type="bibr" rid="B13">Chen et&#xa0;al., 2013</xref>; <xref ref-type="bibr" rid="B18">Dai et&#xa0;al., 2013</xref>). The current assessment of the whole Mediterranean as source or sink of CO<sub>2</sub> lies mainly on modelling studies that describe it as close to equilibrium with the atmosphere, or at most functioning as a weak sink for atmospheric CO<sub>2</sub> (<xref ref-type="bibr" rid="B22">D&#x2019;Ortenzio et&#xa0;al., 2008</xref>; <xref ref-type="bibr" rid="B63">Palmi&#xe9;ri et&#xa0;al., 2015</xref>). In fact, the Mediterranean <italic>in-situ</italic> studies on pCO<sub>2</sub> variability and air-sea fluxes are based upon a sparse time-series of pCO<sub>2</sub> observations mainly located in the North-Western Mediterranean and the Adriatic Sea. There is lack of surface ocean pCO<sub>2</sub> data with adequate spatial and/or temporal coverage in large areas of the Mediterranean, especially in the Eastern basin and the whole southern part of the basin (<xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref>). In the present study, the pCO<sub>2</sub> time series measurements allowed for estimation of the air-sea fluxes, indicating a transition from a winter-spring CO<sub>2</sub> sink (between mid-October and May) to a summer-autumn CO<sub>2</sub> source (June to mid-October). These periods are in agreement with other field studies providing direct measurements of pCO<sub>2</sub> or pCO<sub>2</sub> calculated from AT-CT in the Aegean Sea in February and May (<xref ref-type="bibr" rid="B51">Krasakopoulou et&#xa0;al., 2006</xref>, <xref ref-type="bibr" rid="B53">2009</xref>, respectively), estimates of pCO<sub>2</sub> (by AT-pH) during an annual cycle in the Aegean (<xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>) and from reconstructed time-series out of seasonal cruises in the South-East (<xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>) and the North-West Levantine Sea (<xref ref-type="bibr" rid="B91">Wimart-Rousseau et&#xa0;al., 2021</xref>). Among these studies, those that estimated annual air-sea CO<sub>2</sub> fluxes (<xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>), suggest their area to be a weak CO<sub>2</sub> source, which supports a previous hypothesis for the whole Eastern Mediterranean Sea (<xref ref-type="bibr" rid="B24">Durieu de Madron et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B80">Taillandier et&#xa0;al., 2012</xref>). The estimated annual flux obtained in the present study between -0.15 and -0.18 mol CO<sub>2</sub> m<sup>-2</sup> y<sup>-1</sup> is close to the one obtained by modelling (Tsiaras et&#xa0;al., this issue) for the Levantine Basin (-0.25 mol CO<sub>2</sub> m<sup>-2</sup> y<sup>-1</sup> for 2010-2022). However, it should be stressed that the area examined in the present study cannot be characterized as a CO<sub>2</sub> sink due to a) the flux being low and b) the significant variability in the flux mostly related to wind speed. This is the case also for a general characterization of the Eastern Mediterranean as source or sink. The few field studies up to now, with direct CO<sub>2</sub> measurements, suggest the flux being weak (either sink or source) while they are limited temporally to the present time-series and spatially to few cruises (<xref ref-type="bibr" rid="B51">Krasakopoulou et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B53">Krasakopoulou et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B5">Bakker et&#xa0;al., 2016</xref>) with most CO<sub>2</sub> data being estimates from other carbonate system parameters (review by <xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref>). We hypothesize that most areas in the oligotrophic Eastern Mediterranean Sea currently act as either weak source or sink of CO<sub>2</sub>. This could be a transition period and with the rapid warming and increasing of atmospheric CO<sub>2</sub>, the balance may change to a strong sink as predicted by modelling studies (<xref ref-type="bibr" rid="B16">Cossarini et&#xa0;al., 2021</xref>; Tsiaras et&#xa0;al., this issue). Additional field studies, especially time series measuring CO<sub>2</sub> (ideally at high frequency), are needed to support model and algorithm validation, to allow specifying the spatiotemporal extent as CO<sub>2</sub> source or sink of this area.</p>
</sec>
<sec id="s4_4">
<label>4.4</label>
<title>Carbonate variables estimation</title>
<p>Overall, the above described (section 4.2) dependencies of pCO<sub>2</sub> mainly with temperature, evaporation (shown by salinity) and biological production (shown by Chla) support that remote sensing could be used to estimate pCO<sub>2</sub>, as discussed further below. In the Mediterranean Sea, only a few algorithms have been proposed for the estimation of pCO<sub>2</sub> using temperature (or other non-carbonate variables) despite that temperature appears to be a dominant factor in determining surface pCO<sub>2</sub> in the Mediterranean Sea. In the Eastern Mediterranean Sea, to our knowledge, only two studies have provided such relationships (<xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>). The present study provides the first pCO<sub>2</sub> algorithm developed from <italic>in-situ</italic> CO<sub>2</sub> measurements and remotely sensed SST data (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>) confirming the potential for the prediction of pCO<sub>2</sub> based on satellite data, as used in other marine regions (e.g. Eastern North Pacific, <xref ref-type="bibr" rid="B37">Hales et&#xa0;al., 2012</xref>). Moreover, it is suggested as a tool for extrapolation of CO<sub>2</sub> dynamics over wider spatial scales in the Mediterranean Sea (<xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>). Satellite Chla data were also accounted for, in the developed algorithm similarly to other studies (<xref ref-type="bibr" rid="B30">Ford et&#xa0;al., 2022</xref> and references therein) together with the SST satellite data. However, the outcome showed no improvement of the agreement with the <italic>in-situ</italic> data. The weak role of biological non-thermal control of pCO<sub>2</sub> was shown and discussed in the previous section. This could be explained by the generally low Chla concentration, both on average and in the amplitude of the seasonal variation, which is consistent with the oligotrophic character of the entire Cretan Sea, both in terms of Chla and primary production (<xref ref-type="bibr" rid="B69">Psarra et&#xa0;al., 2000</xref>). In addition, the fact that pCO<sub>2</sub> measurements did not fully cover the late winter-spring bloom periods could weaken the correlation. It should be noted that extrapolation of <italic>in-situ</italic> observations of pCO<sub>2</sub> using satellite observations like SST and Chla (<xref ref-type="bibr" rid="B12">Chen and Hu, 2019</xref> and references therein; <xref ref-type="bibr" rid="B30">Ford et&#xa0;al., 2022</xref> and references therein) should be done cautiously as application outside of the time&#x2013;space domain in which it was developed is less reliable, essentially because of its empirical nature (<xref ref-type="bibr" rid="B22">D&#x2019;Ortenzio et&#xa0;al., 2008</xref>). To examine the present algorithms&#x2019; spatiotemporal domain, we applied it (<xref ref-type="disp-formula" rid="eq7">Equation 8</xref>) to a CO<sub>2</sub> dataset from a wider area of the Eastern Mediterranean (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>) spanning from 1999 to present. Data in the North Aegean with low salinities (&lt;35) were excluded as the algorithm displayed high bias, which can be attributed to the carbonate system of this area being mostly related to Black Sea Water inflow and river runoff (<xref ref-type="bibr" rid="B54">Krasakopoulou et&#xa0;al., 2017</xref>). A linear term of +1.7 units per year accounted for long-term increase of pCO<sub>2</sub> was included (related to atmospheric CO<sub>2</sub> increase), as suggested by other studies (<xref ref-type="bibr" rid="B12">Chen and Hu, 2019</xref>). A +1.7 &#x3bc;atm pCO<sub>2</sub> yr<sup>-1</sup> (from 1983 to 2014), was also reported in the BATS and HOT stations (<xref ref-type="bibr" rid="B6">Bates et&#xa0;al., 2014</xref>), whereas in the Mediterranean Sea, reported values varied between +0.6 and +1.5 &#x3bc;atm pCO<sub>2</sub> yr<sup>-1</sup> (from 2010 to 2022, Tsiaras et&#xa0;al., this issue) and +3.5 &#xb5;atm pCO<sub>2</sub> yr<sup>-1</sup> (from 2007 to 2015, <xref ref-type="bibr" rid="B48">Kapsenberg et&#xa0;al., 2017</xref>). Based upon the algorithm applicability analysis, it appeared that within the area and time window tested most (91%) of &#x394;<sub>obs-est</sub> were between -20 and +20 &#x3bc;atm which is one order of magnitude below the amplitude of seasonal range (~150 &#x3bc;atm in the present study, ~200 &#x3bc;atm review by <xref ref-type="bibr" rid="B1">&#xc1;lvarez et&#xa0;al., 2023</xref>). We thus consider that the algorithm could be useful when used, within the spatiotemporal window it was constructed, as an additional data quality control test, or to fill out data gaps of limited spatiotemporal extent. This analysis supports that the HCB station is indicative of a wider area of the Eastern Mediterranean Sea with respect to pCO<sub>2</sub>, as previously suggested for E1-M3A for temperature, Chla, primary production, pH, and oxygen (<xref ref-type="bibr" rid="B41">Henson et&#xa0;al., 2016</xref>).</p>
<p>Contrary to the few published relationships used to estimate pCO<sub>2</sub> from temperature, many relationships used to estimate AT from salinity have been proposed for the different Mediterranean Sea sub-basins (<xref ref-type="bibr" rid="B15">Copin-Mont&#xe9;gut, 1993</xref>; <xref ref-type="bibr" rid="B76">Schneider et&#xa0;al., 2007</xref>; <xref ref-type="bibr" rid="B17">Cossarini et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B40">Hassoun et&#xa0;al., 2015</xref> and references therein; <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al., 2016</xref>) and widely applied, for example, to reconstruct AT time-series (<xref ref-type="bibr" rid="B91">Wimart-Rousseau et&#xa0;al., 2021</xref>). Among these published AT-SSS relationships, the ones that performed better with the present study&#x2019;s dataset were the ones of <xref ref-type="bibr" rid="B40">Hassoun et&#xa0;al. (2015)</xref> for Cretan Straits waters, followed by the one of <xref ref-type="bibr" rid="B35">Gonz&#xe1;lez-D&#xe1;vila et&#xa0;al. (2016)</xref>. Despite the rather extended use of these AT-SSS relationships, satellite SSS data have been used only in preliminary estimates of AT in the Mediterranean (<xref ref-type="bibr" rid="B73">Sabia et&#xa0;al., 2020</xref>), probably as SSS satellite products have become mature only in recent years (<xref ref-type="bibr" rid="B57">Land et&#xa0;al., 2015</xref>). A comparison with latest satellite SSS products shows a difference of 0.3 salinity units demonstrating the upcoming potential to estimate AT from satellite SSS (<xref ref-type="fig" rid="f2">
<bold>Figures&#xa0;2</bold>
</xref>, <xref ref-type="fig" rid="f4">
<bold>4</bold>
</xref>).</p>
</sec>
</sec>
<sec id="s5" sec-type="conclusions">
<label>5</label>
<title>Conclusions</title>
<p>The present study contributes to the recommendation to improve ocean acidification studies in the Mediterranean by increasing data coverage and availability, especially of time-series (<xref ref-type="bibr" rid="B38">Hassoun et&#xa0;al., 2022</xref>). There is a clear need to sustain the time-series in this area of scarce CO<sub>2</sub> data affected by rapid warming (<xref ref-type="bibr" rid="B78">Sisma-Ventura et&#xa0;al., 2017</xref>). The provision of this new <italic>in-situ</italic> carbonate time series in a poorly covered area is also important internationally for databases such as SOCAT, and contributes to the United Nations Sustainable Development Goals (SDG) 13 Climate Action and SDG 14 Life Below Water [in particular 14.3.1 Average marine acidity (pH)]. In addition to providing data per se, the high frequency measurements of CO<sub>2</sub> and pH allowed for a better understanding in the drivers of the temporal variability of the carbonate system, to develop new estimation algorithms, to support model validation, and to advance the current view of the Eastern Mediterranean air-sea flux. At this time, the net air-sea CO<sub>2</sub> flux cannot be conclusively characterized as source or sink. Comparison of the fluxes from the 1980s and 2000s already showed a tendency for the Eastern Mediterranean to become a weaker CO<sub>2</sub> source (<xref ref-type="bibr" rid="B80">Taillandier et&#xa0;al., 2012</xref>). The same trend was predicted by a study covering the period 1999-2019 (<xref ref-type="bibr" rid="B16">Cossarini et&#xa0;al., 2021</xref>). In the near future, the warmer Eastern Mediterranean is expected to become more stratified and oligotrophic (<xref ref-type="bibr" rid="B70">Reale et&#xa0;al., 2022</xref>). The present study emphasizes that in addition to future changes in temperature, atmospheric CO<sub>2</sub> and biological productivity, it is crucial to consider future changes in the wind regime. One should consider not only whether the total wind stress will change, but also whether this change will occur mainly during the winter (sink) or summer (source) period. It is also important to consider the hypothesis that a transition is occurring in the Aegean Sea after 2020 with periods of deep water formation due to persistence of high salinity in upper and intermediate layers (<xref ref-type="bibr" rid="B49">Kassis and Korres, 2021</xref>; <xref ref-type="bibr" rid="B67">Potiris et&#xa0;al., 2023</xref>).</p>
<p>Another point that emerged was the benefit of a multi-platform approach (satellite, R/V cruises, buoy, atmospheric station) adopted in the present study, with a high sampling effort for 2.5 years. This can provide guidance for future observing activities with a cost-benefit approach, which is particularly important for countries with less available funds, such as those in the Eastern Mediterranean and the North African countries.</p>
<p>Indeed, the data obtained provided new carbonate estimation algorithms that can utilize remote sensing data (satellite SSS, SST and Chla) to fill data gaps of limited spatio-temporal extent. In addition to these algorithms, the results of the present study provide indications on how to optimize an <italic>in-situ</italic> observation strategy. Having in mind that direct measurements of the variable of interest (pH or pCO<sub>2</sub>) is the best, if a well-established local AT/SSS relationship exists (and its limitations known), then a pH (or pCO<sub>2</sub>) sensor could be used to estimate pCO<sub>2</sub> (or pH) together with an <italic>in-situ</italic> SSS sensor. For example, in this case, since the estimation of pCO<sub>2</sub> from pH (or pH from pCO<sub>2</sub>) together with SSS obtained from sensor at HCB is satisfactory, then the pH (or pCO<sub>2</sub>) sensor could be moved to the nearby (34 km) observing platform of the E1-M3A, thus increasing the spatial extent of observations without significant additional effort (instead of having both sensors at the same location).</p>
</sec>
<sec id="s6" sec-type="data-availability">
<title>Data availability statement</title>
<p>The datasets presented in this study can be found in online repositories. The names of the repository/repositories and accession number(s) can be found below: The datasets generated and analyzed for this study can be found: a) POSEIDON buoy marine (physical and biogeochemical) and meteorological data, as well as physical and biogeochemical data collected during the R/V cruises at HCB and E1-M3A are available in the Mediterranean Sea <italic>in situ</italic> near-real-time observations product on the Copernicus Marine Environment Monitoring Service (<uri xlink:href="https://data.marine.copernicus.eu/product/INSITU_MED_PHYBGCWAV_DISCRETE_MYNRT_013_035/description">https://data.marine.copernicus.eu/product/INSITU_MED_PHYBGCWAV_DISCRETE_MYNRT_013_035/description</uri>) (<uri xlink:href="https://doi.org/10.48670/moi-00044">https://doi.org/10.48670/moi-00044</uri>), and in the POSEIDON system online repository (<uri xlink:href="https://poseidon.hcmr.gr/services/ocean-data">https://poseidon.hcmr.gr/services/ocean-data</uri>). b) the satellite data analyzed (SST, SSS, Chl-a) were found in the EU Copernicus Marine Service information respectively, <uri xlink:href="https://doi.org/10.48670/moi-00051">https://doi.org/10.48670/moi-00051</uri>, <uri xlink:href="https://doi.org/10.48670/moi-00051">https://doi.org/10.48670/moi-00051</uri>, <uri xlink:href="https://doi.org/10.48670/moi-00300">https://doi.org/10.48670/moi-00300</uri>. c) Seawater and atmospheric CO<sub>2</sub> data from the HCB can be found in the Surface Ocean CO<sub>2</sub> Atlas (SOCAT) online repository, DOI:10.25921/1h9f-nb73 (Version 2022), DOI: 10.25921/r7xa-bt92 (Version 2023). d) the SOCAT data from the Eastern Mediterranean analyzed were obtained from <uri xlink:href="https://socat.info/index.php/data-access/">https://socat.info/index.php/data-access/</uri>, DOI: 10.25921/r7xa-bt92 e) the atmospheric CO<sub>2</sub> data from the atmospheric observation station of FINOKALIA analyzed can be found in the Integrated Carbon Observation System, ICOS online repository (<uri xlink:href="https://www.icos-cp.eu/observations/national-networks/icos-greece">https://www.icos-cp.eu/observations/national-networks/icos-greece</uri>), DOI: 10.18160/PEKQ-M4T1 f) the pH data from HCB and R/V cruises can be found in the SDG 14.3.1 Data Portal online repository (<uri xlink:href="https://oa.iode.org/">https://oa.iode.org/</uri>) with the title HCMR_HCB_Mooring, HCMR_HCB_Bottle). g) the AT and CT bottle data collected during the R/V cruises at HCB can be found in the European Marine Observation and Data Network (EMODnet), <uri xlink:href="https://www.emodnet-ingestion.eu/submissions/">https://www.emodnet-ingestion.eu/submissions/</uri>) with the title Heraklion Coastal Buoy carbonate system parameters 2020-2022). <xref ref-type="fig" rid="f1"><bold>Figure 1</bold></xref> was created using Ocean data view software (<xref ref-type="bibr" rid="B74">Schlitzer, 2021</xref>). Other figures were created using GraphPad Prism.</p>
</sec>
<sec id="s7" sec-type="author-contributions">
<title>Author contributions</title>
<p>FC: Conceptualization, Formal analysis, Funding acquisition, Investigation, Methodology, Project administration, Resources, Supervision, Validation, Visualization, Writing &#x2013; original draft, Writing &#x2013; review &amp; editing. NS: Conceptualization, Formal analysis, Investigation, Methodology, Resources, Software, Validation, Visualization, Writing &#x2013; review &amp; editing. PM: Investigation, Methodology, Resources, Writing &#x2013; review &amp; editing. MS: Investigation, Methodology, Resources, Writing &#x2013; review &amp; editing. KA: Conceptualization, Funding acquisition, Methodology, Writing &#x2013; review &amp; editing. GL: Investigation, Methodology, Writing &#x2013; review &amp; editing. TK: Writing &#x2013; review &amp; editing. CS: Project administration, Writing &#x2013; review &amp; editing. SJ: Conceptualization, Funding acquisition, Writing &#x2013; review &amp; editing. TM: Conceptualization, Funding acquisition, Writing &#x2013; review &amp; editing. BA: Writing &#x2013; review &amp; editing. KE: Writing &#x2013; review &amp; editing.</p>
</sec>
</body>
<back>
<sec id="s8" sec-type="funding-information">
<title>Funding</title>
<p>The author(s) declare financial support was received for the research, authorship, and/or publication of this article. This work was partially supported by the JERICO-S3 project. The JERICO-S3 project is funded by the European Commission&#x2019;s H2020 Framework Programme under grant agreement No. 871153.</p>
</sec>
<ack>
<title>Acknowledgments</title>
<p>We would like to thank Dionysios Ballas and Paris Pagonis for technical assistance with the HCB and E1-M3A buoys, Maria Sotiropoulou for data management and processing in the POSEIDON system, Frangoulis Stamatis for help with manuscript editing, George Kouvarakis for guidance on comparisons with the Finokalia station. Special thanks also to Marta &#xc1;lvarez, Melchor Gonz&#xe1;lez-D&#xe1;vila and Sabine Marty for best practices with the pH sensors. We would also like to thank Thanos Gritzalis for his helpful advice on CO<sub>2</sub> data processing and submission to the SOCAT database. Special thanks to George Petihakis and Leonidas Perivoliotis for their support, guidance and recommendations for this research study. We wish to thank the captain and crew of the R/V AEGAEO for their assistance for maintenance of POSEIDON buoys and for sampling. We also thank Stella Psarra, Eleni Dafnomili and Snezana Zivanovic for nutrients and Chla samples analysis. BA is a research director at FNR.</p>
</ack>
<sec id="s9" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
<p>The author(s) declared that they were an editorial board member of Frontiers, at the time of submission. This had no impact on the peer review process and the final decision.</p>
</sec>
<sec id="s10" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec id="s11" sec-type="supplementary-material">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fmars.2024.1348161/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmars.2024.1348161/full#supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet_1.docx" id="SM1" mimetype="application/vnd.openxmlformats-officedocument.wordprocessingml.document"/>
</sec>
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