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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.2021.676537</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Marine Science</subject>
<subj-group>
<subject>Mini Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Radiometry on Argo Floats: From the Multispectral State-of-the-Art on the Step to Hyperspectral Technology</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Jemai</surname> <given-names>Ahlem</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1255749/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Wollschl&#x00E4;ger</surname> <given-names>Jochen</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/217826/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Vo&#x00DF;</surname> <given-names>Daniela</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/948091/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Zielinski</surname> <given-names>Oliver</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/217871/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Center for Marine Sensors (ZfMarS), Institute for Chemistry and Biology of the Marine Environment (ICBM), Carl von Ossietzky University Oldenburg</institution>, <addr-line>Wilhelmshaven</addr-line>, <country>Germany</country></aff>
<aff id="aff2"><sup>2</sup><institution>Marine Perception Research Department, German Research Center for Artificial Intelligence (DFKI)</institution>, <addr-line>Oldenburg</addr-line>, <country>Germany</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Fei Chai, Second Institute of Oceanography, Ministry of Natural Resources, China</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Xiaogang Xing, Second Institute of Oceanography, Ministry of Natural Resources, China; Emanuele Organelli, National Research Council (CNR), Italy</p></fn>
<corresp id="c001">&#x002A;Correspondence: Ahlem Jemai, <email>Ahlem.jemai@uni-oldenburg.de</email></corresp>
<fn fn-type="other" id="fn004"><p>This article was submitted to Ocean Observation, a section of the journal Frontiers in Marine Science</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>22</day>
<month>07</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>8</volume>
<elocation-id>676537</elocation-id>
<history>
<date date-type="received">
<day>05</day>
<month>03</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>25</day>
<month>06</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2021 Jemai, Wollschl&#x00E4;ger, Vo&#x00DF; and Zielinski.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Jemai, Wollschl&#x00E4;ger, Vo&#x00DF; and Zielinski</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>Over the past two decades, robotic technology such as Argo floats have revolutionized operational autonomous measurement of the oceans. Recently, Biogeochemical Argo floats (BGC-Argo floats) have measured optical and biogeochemical quantities down to a depth of 2,000 m. Among these parameters, are measurements of the underwater light field from which apparent optical properties (AOPs), such as the diffuse attenuation coefficient for downwelling irradiance K<sub>d</sub>(&#x03BB;), can be derived. Presently, multispectral observations are available on this platform at three wavelengths (with 10&#x2013;20 nm bandwidths) in the ultraviolet and visible part of the spectrum plus the Photosynthetically Available Radiation (<italic>PAR</italic>; integrated radiation between 400 and 700 nm). This article reviews studies dealing with these radiometric observations and presents the current state-of-the-art in Argo radiometry. It focus on the successful portability of radiometers onboard Argo float platforms and covers applications of the obtained data for bio-optical modeling and ocean color remote sensing. Generating already high-quality datasets in the existing configuration, the BGC-Argo program must now investigate the potential to incorporate hyperspectral technology. The possibility to acquire hyperspectral information and the subsequent development of new algorithms that exploit these data will open new opportunities for bio-optical long-term studies of global ocean processes, but also present new challenges to handle and process increased amounts of data.</p>
</abstract>
<kwd-group>
<kwd>radiometry</kwd>
<kwd>Argo floats</kwd>
<kwd>underwater light field</kwd>
<kwd>apparent optical properties</kwd>
<kwd>ocean sensing</kwd>
</kwd-group>
<counts>
<fig-count count="1"/>
<table-count count="1"/>
<equation-count count="2"/>
<ref-count count="87"/>
<page-count count="10"/>
<word-count count="0"/>
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</front>
<body>
<sec id="S1">
<title>Introduction</title>
<p>The marine environment is highly complex, and conventional <italic>in situ</italic> measurements carried out, e.g., on research cruises, can only provide a series of snapshots. Therefore, uncovering the real dynamics requires complementation with data of higher spatiotemporal coverage, which could be provided by autonomous measurements (<xref ref-type="bibr" rid="B86">Zielinski et al., 2009</xref>; <xref ref-type="bibr" rid="B12">Chai et al., 2020</xref>). The Argo network of autonomous floats<sup><xref ref-type="fn" rid="footnote1">1</xref></sup> has revolutionized the capability for operational observations (<xref ref-type="bibr" rid="B62">Roemmich, 2001</xref>) to be the main source of CTD measurements (<xref ref-type="bibr" rid="B61">Riser et al., 2016</xref>). Biogeochemical Argo floats (BGC-Argo floats) (<xref ref-type="bibr" rid="B6">Biogeochemical-Argo Planning Group, 2016</xref>), the extension of the Argo core mission, supply the optical and biogeochemical observations necessary to construct a global, full-depth, and multidisciplinary ocean-observing system (<xref ref-type="bibr" rid="B24">IOCCG, 2011</xref>; <xref ref-type="bibr" rid="B7">Bittig et al., 2019</xref>; <xref ref-type="bibr" rid="B14">Claustre et al., 2020</xref>). This type of float accommodates up to six essential biogeochemical and bio-optical variables (<xref ref-type="fig" rid="F1">Figure 1</xref>): oxygen (O<sub>2</sub>), pH, nitrate (NO<sub>3</sub>), suspended particles, chlorophyll-a (chl-a), and radiometry.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption><p>Map depicting active floats and their equipped sensors (color classification), as of May 2021. For updated maps see the Biogeochemical-Argo website. Up to 40548 downwelling irradiance profiles have been acquired as of May 2021 (for an updated summary, see the Bio-geochemical-Argo website <ext-link ext-link-type="uri" xlink:href="https://biogeochemical-argo.org/cloud/document/implementation-status/BGC_summary.pdf">https://biogeochemical-argo.org/cloud/document/implementation-status/BGC_summary.pdf</ext-link>).</p></caption>
<graphic xlink:href="fmars-08-676537-g001.tif"/>
</fig>
<p>The basic radiometric measurement is the spectral radiance, <italic>L</italic>(&#x03BB;), representing the radiant flux from a defined direction through a defined area. From radiance, all other integral measures of the light field can be derived, such as irradiance <italic>E</italic>(&#x03BB;),which is the total radiant flux per unit area of horizontal surface measured in the direction of the incoming light. The downwelling irradiance <italic>E</italic><sub><italic>d</italic></sub>(&#x03BB;), thus the irradiance measured toward the sea surface, is the parameter that is regularly measured by the BGC-Argo floats (<xref ref-type="bibr" rid="B55">Organelli et al., 2016</xref>). However, some initiatives have started to look also at the upwelling radiance <italic>L<sub>u</sub></italic> (<xref ref-type="bibr" rid="B17">Gerbi et al., 2016</xref>; <xref ref-type="bibr" rid="B36">Leymarie et al., 2018</xref>; <xref ref-type="bibr" rid="B75">Wojtasiewicz et al., 2018</xref>). The propagation of E<sub>d</sub>(&#x03BB;) in the water column can be described approximately as an exponential function of depth (<xref ref-type="bibr" rid="B45">Mobley, 1994</xref>):</p>
<disp-formula id="S1.E1">
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<mml:mo largeop="true" symmetric="true">&#x222B;</mml:mo>
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<mml:mo>-</mml:mo>
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<mml:mi mathvariant="normal">K</mml:mi>
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<mml:mo>&#x2062;</mml:mo>
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<p>In case a layer-averaged K<sub>d</sub> (from 0 to z) is used, light decline is calculated according to:</p>
<disp-formula id="S1.E2">
<label>(2)</label>
<mml:math id="M2">
<mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mtext>E</mml:mtext>
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</mml:mrow>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
<mml:mrow>
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<mml:mo>,</mml:mo>
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<mml:mo rspace="5.8pt">)</mml:mo>
</mml:mrow>
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<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:msub>
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<mml:mrow>
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<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mtext>K</mml:mtext>
</mml:mrow>
<mml:mrow>
<mml:mtext>d</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
<mml:mrow>
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</mml:msup>
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<p>There, z [m] is water depth, E<sub>d</sub>(&#x03BB;,0<sup>&#x2212;</sup>)[Wm<sup>&#x2212;2</sup>sr<sup>&#x2212;1</sup>nm<sup>&#x2212;1</sup>] the irradiance right below the surface, and K<sub>d</sub>(&#x03BB;,z)[m<sup>&#x2212;1</sup>] the diffuse attenuation coefficient of downwelling irradiance, which can be deduced from measurements of E<sub>d</sub> in different depths. Both E<sub>d</sub> and K<sub>d</sub> are spectral quantities, indicated by &#x03BB;[<italic>nm</italic>] for wavelength.</p>
<p>The slope of this exponential decline, thus K<sub>d</sub>(&#x03BB;), depends on the absorption (<italic>a</italic>)and backscattering properties (<italic>b</italic><sub>b</sub>) of the water (<xref ref-type="bibr" rid="B35">Lee et al., 2005</xref>), i.e., termed the inherent optical properties (IOPs), which are in turn determined by the water molecules themselves as well as the properties and concentration optically active substances (OAS) within the water column, such as phytoplankton, detrital matter, and colored dissolved organic matter (CDOM; see also <xref ref-type="bibr" rid="B28">Kirk, 2011</xref>). From E<sub><italic>d</italic></sub>(&#x03BB;) and L<sub><italic>u</italic></sub>(&#x03BB;), other quantities, commonly known as apparent optical properties (AOPs), can be derived. In addition to K<sub>d</sub>(&#x03BB;), a frequently derived AOP is radiance reflectance, r<sub>rs</sub>(&#x03BB;), (or remote sensing reflectance, R<sub>rs</sub>(&#x03BB;), when measured just above the sea surface). It is defined as the ratio of L<sub>u</sub>(&#x03BB;)/E<sub>d</sub>(&#x03BB;) (see <xref ref-type="bibr" rid="B47">Morel and Gentili, 1996</xref>). A multiplication with the extraterrestrial solar spectral irradiance, gives another important parameter, the normalized water-leaving radiance, L<sub>wn</sub>(&#x03BB;) (see <xref ref-type="bibr" rid="B19">Gordon and Clark, 1981</xref>). K<sub>d</sub>(&#x03BB;), r<sub>rs</sub>(&#x03BB;), and R<sub>rs</sub>(&#x03BB;) are also the most commonly studied parameters of interest in remote sensing applications, notably satellite observation (<xref ref-type="bibr" rid="B3">Austin and Petzold, 1981</xref>; <xref ref-type="bibr" rid="B72">Werdell and Bailey, 2005</xref>). However, converting a radiometric signal captured by a spaceborne sensor to an end-user product carries uncertainties. High demands for accuracy in absolute calibration of satellite remote sensing data (<xref ref-type="bibr" rid="B25">IOCCG, 2013</xref>) and high quality field observations are required for satellite product validation/evaluation (<xref ref-type="bibr" rid="B48">Mueller and Austin, 1992</xref>; <xref ref-type="bibr" rid="B85">Zibordi and Voss, 2014</xref>). For both optical <italic>in situ</italic> and remote sensing observation, various bio-optical algorithms have been developed to relate features of the water signal to in-water quantities of interest (e.g., <xref ref-type="bibr" rid="B51">O&#x2019;Reilly et al., 1998</xref>; <xref ref-type="bibr" rid="B40">Maritorena et al., 2002</xref>). Improving these retrieval algorithms (existing) and develop enhanced ones that exploit forthcoming technologies remains a priority for ocean optics community.</p>
<p>Ocean optics research has recently undergone a shift from multispectral (with broadband data) to hyperspectral instrumentation, both <italic>in situ</italic> and remotely (<xref ref-type="bibr" rid="B13">Chang et al., 2004</xref>). The higher number of available bands in hyperspectral observations allows a more detailed examination regarding spectral resolution of AOPs and IOPs within the water column. This makes applications requiring higher resolution feasible, e.g., the discrimination of phytoplankton groups, the determination of particle size, and more detailed determination of CDOM spectral properties. Conventional Argo floats already provide sustained high-quality data at unprecedented temporal and spatial resolution. Thus, the addition of hyperspectral observation capabilities will allow Argo platforms to meet demands regarding more sophisticated approaches from the field of optical models and remote sensing. The exploitation of such high-resolution data (in the spatial, temporal, and spectral dimension), measured by a single system that carries also IOP sensors, will certainly open new avenues for bio-optical research in the future. This exciting combination (Argo platform + hyperspectral radiometers) could be the next logical step for Argo floats network (<xref ref-type="bibr" rid="B14">Claustre et al., 2020</xref>). With this in mind, this review summarizes the current state-of-the-art of radiometric measurements on Argo floats, and identifies emerging future pathways for the development of hyperspectral Argo radiometry and data exploitation. In our search, we referred to the list of the BGC Argo mission bibliography,<sup><xref ref-type="fn" rid="footnote2">2</xref></sup> from which we selected studies involving radiometric measurements (including papers describing data management approaches and quality-control procedures). We made additional research using Google Scholar and Scopus for verification.</p>
</sec>
<sec id="S2">
<title>Argo-Radiometry: State-Of-The-Art</title>
<sec id="S2.SS1">
<title>Instrumentation</title>
<p>The radiometer mounted on BGC-Argo floats at the time of this review is the multispectral Ocean Color Radiometer (OCR-504, SATLANTIC Inc./Sea-Bird Scientific, United States) (<xref ref-type="bibr" rid="B63">SATLANTIC, 2013</xref>), which measures irradiance commonly at four channels. Three channels are usually dedicated to narrow-wavelengths (around 10 or 20 nm bandwidth) from the ultraviolet to the visible range of the spectrum, while the fourth channel measures the Photosynthetically Available Radiation (<italic>PAR</italic>; integrated radiation between 400 and 700 nm). Two different sets of waveband configurations have been documented in the literature. Depending on the funding program, the earlier studies have applicated 412, 490, and 555 nm (<xref ref-type="bibr" rid="B83">Xing et al., 2011</xref>, <xref ref-type="bibr" rid="B84">2012</xref>, <xref ref-type="bibr" rid="B82">2014</xref>; <xref ref-type="bibr" rid="B44">Mignot et al., 2014</xref>). Later studies have selected 380 nm instead of 555 nm (<xref ref-type="bibr" rid="B55">Organelli et al., 2016</xref>; <xref ref-type="bibr" rid="B52">Organelli et al., 2017a</xref>,<xref ref-type="bibr" rid="B54">b</xref>; <xref ref-type="bibr" rid="B43">Mignot et al., 2018</xref>; <xref ref-type="bibr" rid="B53">Organelli and Claustre, 2019</xref>). The fourth channel dedicated to PAR was used in the context of determining overall light available for primary production in the ocean (<xref ref-type="bibr" rid="B31">Lacour et al., 2017</xref>, <xref ref-type="bibr" rid="B32">2019</xref>; <xref ref-type="bibr" rid="B43">Mignot et al., 2018</xref>; <xref ref-type="bibr" rid="B4">Barbieux et al., 2019</xref>; <xref ref-type="bibr" rid="B70">Terzi&#x0107; et al., 2019</xref>). However, studies that measured both <italic>E<sub>d</sub></italic> and <italic>L<sub>u</sub></italic> have used the four wavelengths centered at 412, 443, 488, and 555 nm (<xref ref-type="bibr" rid="B17">Gerbi et al., 2016</xref>; <xref ref-type="bibr" rid="B75">Wojtasiewicz et al., 2018</xref>), and up to 7 wavelengths plus <italic>PAR</italic> using OCR507 (see <xref ref-type="bibr" rid="B36">Leymarie et al., 2018</xref>). <xref ref-type="table" rid="T1">Table 1</xref> summarizes available studies that made use of radiometric data obtained with Argo floats, with the exception of studies that exploit the data only as additional or support information. We also excluded studies that covered primarily data management or quality control protocols.</p>
<table-wrap position="float" id="T1">
<label>TABLE 1</label>
<caption><p>Summary of studies that used Argo radiometric data for their main research aim.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left">Type of Argo float</td>
<td valign="top" align="left">Optical quantity</td>
<td valign="top" align="left">Derived AOPs</td>
<td valign="top" align="left">Area studied</td>
<td valign="top" align="left">Aim</td>
<td valign="top" align="left">Author</td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Not specified</td>
<td valign="top" align="left"><italic>PAR</italic></td>
<td valign="top" align="justify"/>
<td valign="top" align="left">Black Sea</td>
<td valign="top" align="left">Vertical distribution of chlorophyll concentration</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B60">Ricour et al., 2021</xref></td>
</tr>
<tr>
<td valign="top" align="left">ProIce</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(380,&#x2005;412,&#x2005;490)+ <italic>PAR</italic></td>
<td valign="top" align="justify"/>
<td valign="top" align="left">Arctic</td>
<td valign="top" align="left">Study the phytoplankton growth</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B57">Randelhoff et al., 2020</xref></td>
</tr>
<tr>
<td valign="top" align="left">Not specified</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(380,&#x2005;412,&#x2005;490)+ <italic>PAR</italic></td>
<td valign="top" align="justify"/>
<td valign="top" align="left">Mediterranean Sea</td>
<td valign="top" align="left">Validation of numerical model of radiative transfer</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B33">Lazzari et al., 2021</xref></td>
</tr>
<tr>
<td valign="top" align="left">Not specified</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(380,&#x2005;412,&#x2005;490)+ <italic>PAR</italic></td>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(<italic>PAR</italic>); <italic>K</italic><sub><italic>d</italic></sub>(490)</td>
<td valign="top" align="left">World&#x2019;s ocean (Southern Ocean, Subpolar Gyre, Transition zone, Red Sea, Black Sea, Mediterranean Sea, Subtropical Gyre, Arctic Sea, New Caledonia)</td>
<td valign="top" align="left">Evaluation of ocean color remote sensing algorithms for diffuse attenuation and optical depths</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B80">Xing et al., 2020</xref></td>
</tr>
<tr>
<td valign="top" align="left">PROVOR (NKE Marine Electronics Inc., France)</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(380,&#x2005;412,&#x2005;490)+ <italic>PAR</italic></td>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(380); <italic>K</italic><sub><italic>bio</italic></sub>(380); <italic>K</italic><sub><italic>star</italic></sub>(380); <italic>K</italic><sub><italic>d</italic></sub>(490); <italic>K</italic><sub><italic>bio</italic></sub>(490)); <italic>K</italic><sub><italic>star</italic></sub>(490)</td>
<td valign="top" align="left">North Atlantic subtropical gyre</td>
<td valign="top" align="left">Understand the potential driver of CDOM</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B53">Organelli and Claustre, 2019</xref></td>
</tr>
<tr>
<td valign="top" align="left">Not specified</td>
<td valign="top" align="left"><italic>PAR</italic></td>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(<italic>PAR</italic>)</td>
<td valign="top" align="left">Mediterranean Sea</td>
<td valign="top" align="left">Improve the simulation of chl-a dynamics</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B70">Terzi&#x0107; et al., 2019</xref></td>
</tr>
<tr>
<td valign="top" align="left">PROVOR (NKE Marine Electronics Inc., France)</td>
<td valign="top" align="left"><italic>PAR</italic></td>
<td valign="top" align="left">Euphotic depth (Zeu)</td>
<td valign="top" align="left">North Atlantic subpolar Ocean</td>
<td valign="top" align="left">Light penetration information</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B31">Lacour et al., 2017</xref>, <xref ref-type="bibr" rid="B32">2019</xref></td>
</tr>
<tr>
<td valign="top" align="left">Navis (Sea-Bird Scientific, Inc., United States)</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(412,&#x2005;443,&#x2005;490,&#x2005;555) <italic>L</italic><sub><italic>u</italic></sub>(412,&#x2005;443,&#x2005;490,&#x2005;555)</td>
<td valign="top" align="left"><italic>R</italic><sub><italic>rs</italic></sub>(412,&#x2005;443,&#x2005;490,&#x2005;555)</td>
<td valign="top" align="left">Indian Ocean subtropical gyres</td>
<td valign="top" align="left">Validation of remote sensing reflectance</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B75">Wojtasiewicz et al., 2018</xref></td>
</tr>
<tr>
<td valign="top" align="left">PROVOR (NKE Marine Electronics Inc., France)</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(380,&#x2005;443,&#x2005;490,&#x2005;510,560,665) + <italic>PAR L</italic><sub><italic>u</italic></sub>(380,&#x2005;443,&#x2005;490,&#x2005;510,560,665) <italic>E</italic><sub><italic>d</italic></sub>(412,&#x2005;443,&#x2005;490,&#x2005;510,560,665) + <italic>PAR L</italic><sub><italic>u</italic></sub>(380,&#x2005;443,&#x2005;490,&#x2005;510,&#x2005;560,&#x2005;665)</td>
<td valign="top" align="justify"/>
<td valign="top" align="left">Mediterranean Sea Southern Ocean</td>
<td valign="top" align="left">Test the applicability of the new PROVOR float (CTS5) in ocean color validation activities</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B36">Leymarie et al., 2018</xref></td>
</tr>
<tr>
<td valign="top" align="left">Not specified</td>
<td valign="top" align="left"><italic>PAR</italic></td>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(<italic>PAR</italic>)</td>
<td valign="top" align="left">North Atlantic subpolar Ocean</td>
<td valign="top" align="left">Determine the euphotic layer depth</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B43">Mignot et al., 2018</xref></td>
</tr>
<tr>
<td valign="top" align="left">PROVOR CTS-4 (NKE Marine Electronics Inc., France)</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(380,&#x2005;412,&#x2005;490)+ <italic>PAR</italic></td>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(380); <italic>K</italic><sub><italic>d</italic></sub>(490)</td>
<td valign="top" align="left">Black Sea; Subtropical gyres (Atlantic and Pacific); High latitudes (North Atlantic and southern oceans); Mediterranean Sea</td>
<td valign="top" align="left">Reexamine the regional variability of relationship between CDOM and phytoplankton light absorption properties referring to existing bio-optical models</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B54">Organelli et al., 2017b</xref></td>
</tr>
<tr>
<td valign="top" align="left">APEX (Teledyne Webb Research., United States)</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(412,&#x2005;443,&#x2005;488,&#x2005;555)<italic>L</italic><sub><italic>u</italic></sub>(412,&#x2005;443,&#x2005;488,&#x2005;555)</td>
<td valign="top" align="left"><italic>R</italic><sub><italic>rs</italic></sub>(412,&#x2005;443,&#x2005;488,&#x2005;555)</td>
<td valign="top" align="left">Mediterranean Sea; Pacific Ocean; Atlantic Ocean</td>
<td valign="top" align="left">Validation of remote sensing reflectance</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B17">Gerbi et al., 2016</xref></td>
</tr>
<tr>
<td valign="top" align="left">PROVOR (NKE Marine Electronics Inc., France)</td>
<td valign="top" align="left"><italic>E</italic><sub><italic>d</italic></sub>(412,&#x2005;490,&#x2005;555)</td>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(412); <italic>K</italic><sub><italic>bio</italic></sub>(412)); <italic>K</italic><sub><italic>bio</italic></sub>(490)</td>
<td valign="top" align="left">Mediterranean Sea; North Atlantic; North Pacific gyre</td>
<td valign="top" align="left">Quantification of biogeochemical quantities</td>
<td valign="top" align="left"><xref ref-type="bibr" rid="B83">Xing et al., 2011</xref>, <xref ref-type="bibr" rid="B84">2012</xref></td>
</tr>
</tbody>
</table></table-wrap>
</sec>
<sec id="S2.SS2">
<title>Exploitation of the Radiometric Data Obtained From Argo</title>
<p>The mapping of phytoplankton is an area of environmental monitoring that has particularly benefitted from the Argo radiometric observations. Indeed, the <italic>PAR</italic> observations acquired in high sampling frequency provide a comprehensive picture of the vertical distribution of phytoplankton chlorophyll over the different layers in the euphotic zone (surface layer, mixed layer, and deep chlorophyll maximum layer) (<xref ref-type="bibr" rid="B44">Mignot et al., 2014</xref>; <xref ref-type="bibr" rid="B31">Lacour et al., 2017</xref>, <xref ref-type="bibr" rid="B32">2019</xref>; <xref ref-type="bibr" rid="B4">Barbieux et al., 2019</xref>; <xref ref-type="bibr" rid="B60">Ricour et al., 2021</xref>). Gaining such dynamic illustration of the light gradient, including the critical depth of the upper euphotic mixed layer, revealed the magnitude and timing of blooms occurring in otherwise inaccessible locations in different seasons (<xref ref-type="bibr" rid="B57">Randelhoff et al., 2020</xref>). However, with respect to phytoplankton diversity, these ecological events are still in demand for a monitoring in terms of pigment groups or functional types (<xref ref-type="bibr" rid="B30">Kutser, 2009</xref>), for which multispectral data provide not enough spectral resolution. Readily, this dataset has demonstrated also its utility in improving numerical biogeochemical modeling (<xref ref-type="bibr" rid="B70">Terzi&#x0107; et al., 2019</xref>). Other reviewed studies provided that <italic>PAR</italic> and/or <italic>Ed</italic> have also successfully used to validate IOP parameterizations (<xref ref-type="bibr" rid="B33">Lazzari et al., 2021</xref>). Biogeochemical quantities like chl-a and CDOM were also retrieved from <italic>K</italic><sub><italic>d</italic></sub>(490) and <italic>K</italic><sub><italic>d</italic></sub>(412), respectively (<xref ref-type="bibr" rid="B83">Xing et al., 2011</xref>, <xref ref-type="bibr" rid="B84">2012</xref>), and other related studies disclosed their main drivers (<xref ref-type="bibr" rid="B53">Organelli and Claustre, 2019</xref>). The estimations of such biogeochemical quantities are still in need to be refined and improved better resolved with respect to their relative contribution to the in-water optical properties via their absorption and scattering signatures (<xref ref-type="bibr" rid="B14">Claustre et al., 2020</xref>). Acquiring radiometric data over the entire spectrum will permit the construction of continuous spectral diffuse attenuation information that, in turn, enables for depth-dependent IOPs characteristics of the OAS in the water column. Such analysis would be rather difficult with the fewer bands of a multispectral sensor (<xref ref-type="bibr" rid="B13">Chang et al., 2004</xref>).</p>
<p>Argo radiometric data plays further a significant role in increasing the amount of data available for satellite matchups in remote areas (<xref ref-type="bibr" rid="B52">Organelli et al., 2017a</xref>; <xref ref-type="bibr" rid="B75">Wojtasiewicz et al., 2018</xref>), as well as for evaluating the performance of ocean color remote sensing retrievals (<xref ref-type="bibr" rid="B52">Organelli et al., 2017a</xref>; <xref ref-type="bibr" rid="B80">Xing et al., 2020</xref>). Thus, a further exploitation of the Argo platform capabilities is reasonable to enhance the utilization of satellite data in terms of product retrievals (with less uncertainties). A frequent requested product in this respect are e.g., the phytoplankton accessory pigments in order to characterize phytoplankton dynamics in more detail instead just in terms of biomass (<xref ref-type="bibr" rid="B49">Mueller and Fargion, 2002</xref>). Other reviewed papers here have implicated the radiometric Argo data as a metric to get supplementary information about the euphotic zone and optical depth (<xref ref-type="bibr" rid="B16">Doxaran et al., 2014</xref>; <xref ref-type="bibr" rid="B41">Mayot et al., 2017</xref>), and to resolve events undetectable by satellite observations or classical sampling, for example, variation in optical depth preceding and following a typhoon event (<xref ref-type="bibr" rid="B16">Doxaran et al., 2014</xref>).</p>
<p>Other gains sum up in inclusion this dataset in those procedures of fluorometer (accompanied sensor on Argo float) calibration. For instance, measurement of <italic>E</italic><sub><italic>d</italic></sub>(490) enables the retrieval of a scaling factor required for the calibration of the chl-a fluorometers (<xref ref-type="bibr" rid="B83">Xing et al., 2011</xref>). The reliability of this method was supported by later works (<xref ref-type="bibr" rid="B84">Xing et al., 2012</xref>, <xref ref-type="bibr" rid="B82">2014</xref>; <xref ref-type="bibr" rid="B44">Mignot et al., 2014</xref>; <xref ref-type="bibr" rid="B1">Ardyna et al., 2019</xref>; <xref ref-type="bibr" rid="B29">Kubryakov et al., 2019</xref>). Argo <italic>PAR</italic> profiles have been also used to ameliorate the non-photochemical quenching (NPQ) correction of Argo chl-a fluorescence measurements (<xref ref-type="bibr" rid="B81">Xing et al., 2018</xref>).</p>
</sec>
<sec id="S2.SS3">
<title>Data Availability and Quality Control</title>
<p>As with all BGC-Argo variables, radiometric datasets are available within 24 h of transmission to the public in the Argo Global Data Assembly Centers (GDACs) along with the corresponding CTD data (<xref ref-type="bibr" rid="B78">Wong et al., 2020</xref>). The international Argo Data Management Team (ADMT) supervises the development of data management procedures of Argo data (<xref ref-type="bibr" rid="B2">Argo Data Management Team, 2021</xref>). As expected, this review observed a regular protocol in the way of acquiring and processing radiometric data (<xref ref-type="bibr" rid="B64">Schmechtig et al., 2017</xref>). In terms of quality control, two levels are generally applied: the &#x201C;real time mode&#x201D; that effectuates quick automatic checks (e.g., global range test) to ensure data provision to the user in near real time (<xref ref-type="bibr" rid="B56">Poteau et al., 2019</xref>); and the &#x201C;delayed mode&#x201D; based on scientific judgement, to account for confounding effects such as biofouling and sensor drift (<xref ref-type="bibr" rid="B65">Schmid et al., 2007</xref>), as well as other sources of uncertainty, e.g., the temperature effect on dark counts (<xref ref-type="bibr" rid="B52">Organelli et al., 2017a</xref>; <xref ref-type="bibr" rid="B75">Wojtasiewicz et al., 2018</xref>). In the earliest stage of the BGC-Argo program, <xref ref-type="bibr" rid="B83">Xing et al. (2011)</xref> relied on interpreting the chl-a fluorescence profiles that accompanied the downwelling irradiance measurements to obtain noise-free radiometric profiles. Later, <xref ref-type="bibr" rid="B55">Organelli et al. (2016)</xref> developed a quality-control procedure based on statistical and mathematical analyses that targets the major issues related to vertical in-water light field measurements (e.g., dark signal, clouds, wave-focusing, general spike detection; see also <xref ref-type="bibr" rid="B50">Mueller et al., 2003</xref>), taking into account the specific circumstances of the Argo platform (e.g., lack of operator control and float recovery precluding post-deployment check or recalibration of the radiometer). As no above-water measurements are available to validate the subsurface radiometric measurement, the comparison of the near-surface measurements with the output of clear-sky optical models (<xref ref-type="bibr" rid="B21">Gregg and Carder, 1990</xref>) was suggested to evaluate the obtained measurements (<xref ref-type="bibr" rid="B83">Xing et al., 2011</xref>; <xref ref-type="bibr" rid="B55">Organelli et al., 2016</xref>).</p>
</sec>
</sec>
<sec id="S3">
<title>Future Prospects</title>
<p>Argo radiometric measurements are currently limited to observations measuring, depending on configuration, either irradiance or radiance at up to four channels. Acquisition of radiometric observations takes place in discrete spectral bands, selected to detect major variations in underwater optical properties, allowing these multispectral devices to be effective in deriving the relative concentration of in-water constituents over the water column. Taking the example of phytoplankton, the retrieval of more details regarding species composition (which is oftentimes called for) has been challenging because of the insufficient spectral resolution of the multispectral sensor (<xref ref-type="bibr" rid="B8">Bracher et al., 2017</xref>). Hyperspectral radiometers successfully achieved this discrimination (e.g., <xref ref-type="bibr" rid="B26">Isada et al., 2015</xref>; <xref ref-type="bibr" rid="B79">Xi et al., 2015</xref>), as well as the retrieval of phytoplankton functional types (<xref ref-type="bibr" rid="B76">Wolanin et al., 2016</xref>), as they provide measurements at hundreds of contiguous wavebands distributed equally from the ultraviolet to the near-infrared segment of the spectrum with a resolution of the order of 5 nm. This has led to more frequent use of hyperspectral instrumentation in ocean optics research (<xref ref-type="bibr" rid="B13">Chang et al., 2004</xref>). Bringing hyperspectral devices into play on robotic platforms such as Argo floats is therefore the next logical step (<xref ref-type="bibr" rid="B14">Claustre et al., 2020</xref>). In some, especially remote areas affected by regularly occurring (harmful) algal blooms, monitoring strategies require increased observing capabilities (<xref ref-type="bibr" rid="B67">Sellner et al., 2003</xref>). Whilst detection and characterization of the spatial and temporal development of phytoplankton biomass is already feasible using existing multispectral Argo floats, the transformation toward hyperspectral technology will provide additional opportunities of tracking its composition and predict harmful algal bloom development (<xref ref-type="bibr" rid="B68">Shen et al., 2012</xref>; <xref ref-type="bibr" rid="B15">Dierssen et al., 2020</xref>). Ultimately, hyperspectral data based on Argo float may pave the way toward harmful algal bloom forecasting programs that require nearly real time observations from a global communication network (<xref ref-type="bibr" rid="B27">Jochens et al., 2010</xref>).</p>
<p>Hyperspectral data is further advantageous for calibration and validation purposes (<xref ref-type="bibr" rid="B42">McClain and Meister, 2012</xref>) of current and future hyperspectral ocean color missions such as the Environmental Mapping and Analysis Program (EnMAP) (<xref ref-type="bibr" rid="B23">Guanter et al., 2015</xref>), the Hyperspectral Precursor of the Application Mission (PRISMA) (<xref ref-type="bibr" rid="B37">Loizzo et al., 2018</xref>), and the Pre-Aerosol, Clouds, and ocean Ecosystem (PACE) mission (<xref ref-type="bibr" rid="B22">Gregg and Rousseaux, 2017</xref>). Indeed, hyperspectral radiometric observations measured by Argo will provide high-resolution data (in the context of spatial, temporal and spectral resolution) that will be more appropriate to match the spectral bands of these advanced sensors (<xref ref-type="bibr" rid="B74">Werdell et al., 2013</xref>; <xref ref-type="bibr" rid="B9">Brewin et al., 2016</xref>). This would subsequently improve the assessment of derived products and thereby upgrade the validation metrics (<xref ref-type="bibr" rid="B39">Maritorena and Siegel, 2005</xref>; <xref ref-type="bibr" rid="B38">Maritorena et al., 2010</xref>; <xref ref-type="bibr" rid="B66">Seegers et al., 2018</xref>). A particular benefits of such datasets would be that they offer the possibility to develop new algorithms with more freedom in selecting spectral bands for bio-optical studies. Such developments would in turn improve both empirical remote-sensing (<xref ref-type="bibr" rid="B18">Gordon and Morel, 1983</xref>; <xref ref-type="bibr" rid="B34">Lee et al., 1998</xref>; <xref ref-type="bibr" rid="B69">Stramska et al., 2003</xref>) and semi-analytical approaches (<xref ref-type="bibr" rid="B11">Carder et al., 1999</xref>), including the evaluation of radiative transfer modeling simulations (<xref ref-type="bibr" rid="B46">Mobley and Sundman, 2008</xref>). This would also serve as a contribution to the tuning of existing (heritage) IOP retrieval approaches (<xref ref-type="bibr" rid="B73">Werdell et al., 2018</xref>).</p>
<p>Hyperspectral Argo data, on other hand, will have their own scientific value in lieu of just supporting satellite missions. The exploitation of high-resolution data (in the spatial, temporal, and spectral extension), measured by a single system that carries also IOP sensors, would potentially reduce uncertainties (due to temporal or spatial biases) in existing inverse algorithms (<xref ref-type="bibr" rid="B58">Rehm and McCormick, 2011</xref>). Thence, the availability of hyperspectral AOPs quantities will enable the derivation of high spectral resolution IOP data, and this will considerably reduce the ambiguities introduced by the relative contribution of different accessory phytoplankton pigments for example, as well as retrieving CDOM spectral optical properties which bring additional biogeochemical information (<xref ref-type="bibr" rid="B20">Gordon et al., 2009</xref>). The investigation of such contemporaneous measurements is demonstrated in the work of <xref ref-type="bibr" rid="B59">Rehm and Mobley (2013)</xref> where they estimated absorption and backscattering coefficients to an accuracy of &#x00B1;0.01 m<sup>&#x2013;1</sup> and &#x00B1;0.0005 m<sup>&#x2013;1</sup> respectively, based on hyperspectral vertical radiometric observations and concurrent measurements of the beam attenuation coefficient at 650 nm in optically simple oligotrophic waters. In the more optically complex waters where OAS do not covary with chl-a, <xref ref-type="bibr" rid="B77">Wollschl&#x00E4;ger et al. (2020)</xref> obtained a moderately complex parametrization of the underwater light field based on hyperspectral light measurements. Such parametrizations could be strongly improved by accounting for seasonal and regional variation based on data coming from hyperspectral Argo-floats. Increasing the number of bands will moreover allow testing of various wavelengths combinations based on the spectral diffuse attenuation to better link IOPs features (<xref ref-type="bibr" rid="B10">Brown et al., 2004</xref>), as well as to check for consistency of calibration of fluorescence observations (accompanied sensor on Argo float) (<xref ref-type="bibr" rid="B83">Xing et al., 2011</xref>).</p>
<p>The deployment of hyperspectral radiometers on unattended platforms like Argo floats applies higher demands on the capabilities of the sensors than conventional in-water radiometry. Some studies which performed hyperspectral light field measurements using drifting devices (<xref ref-type="bibr" rid="B87">Zielinski et al., 2006</xref>; <xref ref-type="bibr" rid="B5">Barnard et al., 2018</xref>) have already demonstrated stable short-term field deployment of autonomous hyperspectral radiance and irradiance measurements. However, both studies highlight the importance of technical features like radiometer power consumption, long-term stability and reliability, standardized interfaces and protocols, as well as intelligent data handling. At present, the first studies are performed to evaluate the use of hyperspectral radiometers on Argo floats. The sensor used for these studies is an improved, 1,000 m-depth rated RAMSES radiometer (TRIOS, Rastede, Germany) designed to collect the incoming irradiance in the spectral range of 320&#x2013;950 nm, with a spectral resolution of 2.2 nm and a spectral accuracy of 0.2 nm. The sensor also features the new G2 Modbus-interface for easier platform integration (<xref ref-type="bibr" rid="B71">Trios, 2021</xref>). An important consideration for Argo-users is that the increased information content increases the demand for data transfer and processing capabilities. Handling huge amounts of data within a timeframe of 24 h as strived by the Argo community will be a demanding task. In case of the mentioned RAMSES radiometer, the data size is approximately six times that of the OCR-504. Together with the moderately higher power consumption (45 mA compared to 25 mA for the OCR-504), this constrains either the measurement frequency or deployment duration of an Argo float equipped with this sensor. Therefore, reducing power consumption of the sensor and the dimension of the data onboard the platform prior to transmission could be important future steps. This process would probably demand embedded computing power in the sensor and the platform itself, which poses challenges on the commercially available instrumentation.</p>
</sec>
<sec id="S4">
<title>Conclusion</title>
<p>This review captures the current state of light field measurements onboard Argo floats, describes their application in bio-optical ocean studies, and points to future directions in the transition from multispectral toward hyperspectral radiometry. This transition would allow an exploitation of light field measurements far beyond to what is covered to date.</p>
<p>Moving forward in operating Argo radiometry, hyperspectral observations would provide more detailed insights through direct hyperspectral investigation of the depth-resolved light distribution in different waters bodies and would be relevant to ocean color products. The development of novel approaches that exploit this information will open new avenues for bio-optical long-term studies of global ocean change and foster its relevance for carbon cycle investigation by addressing phytoplankton not only in terms of biomass, but also with respect to taxonomic composition. Critically, exploiting these advantages requires the development, in parallel, of new algorithms and procedures for quality assessment, data management, and on-board data reduction, all of which are intrinsically related to the technical features of both sensor and platform.</p>
</sec>
<sec id="S5">
<title>Author Contributions</title>
<p>AJ made the draft version. JW and OZ participated on the outline of the manuscript. All authors contributed to manuscript revisions and agreed to the submitted version.</p>
</sec>
<sec sec-type="COI-statement" id="conf1">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</body>
<back>
<fn-group>
<fn fn-type="financial-disclosure">
<p><bold>Funding.</bold> This work is part of the Spectral Argo-N project funded by the German Federal Ministry of Education and Research (Grant No. 03V01478).</p>
</fn>
</fn-group>
<ack>
<p>The authors would like to thank the reviewers of this manuscript who helped to improve its quality by their constructive comments and suggestions.</p>
</ack>
<app-group>
<app id="A1">
<title>Appendix</title>
<table-wrap position="float" id="T2">
<label>APPENDIX A</label>
<caption><p>Notations used in this review.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left">Symbol or abbreviation</td>
<td valign="top" align="left">Significance/units</td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left"><italic>L</italic></td>
<td valign="top" align="left">Radiance (W m<sup>&#x2013;2</sup>sr<sup>&#x2013;1</sup>nm<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>L<sub>u</sub></italic></td>
<td valign="top" align="left">Upwelling radiance (W m<sup>&#x2013;2</sup>sr<sup>&#x2013;1</sup>nm<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>E<sub>d</sub></italic></td>
<td valign="top" align="left">Downward irradiance (W m<sup>&#x2013;2</sup>nm<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>L</italic><sub><italic>wn</italic></sub>(&#x03BB;)</td>
<td valign="top" align="left">Water-leaving radiance (W m<sup>&#x2013;2</sup>sr<sup>&#x2013;1</sup>nm<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>r</italic><sub><italic>rs</italic></sub>(&#x03BB;)</td>
<td valign="top" align="left">Under-water surface remote sensing reflectance (sr<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>R</italic><sub><italic>rs</italic></sub>(&#x03BB;)</td>
<td valign="top" align="left">Above-water surface remote sensing reflectance (sr<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(&#x03BB;)</td>
<td valign="top" align="left">Diffuse attenuation coefficient at wavelength &#x03BB; (m<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>K</italic><sub><italic>bio</italic></sub>(&#x03BB;)</td>
<td valign="top" align="left">Non-watery diffuse attenuation coefficient at wavelength &#x03BB; (m<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>K</italic><sub><italic>star</italic></sub>(&#x03BB;)</td>
<td valign="top" align="left">Chlorophyll-specific attenuation coefficient at wavelength &#x03BB; (units of square meters per milligram of chlorophyll)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>PAR</italic></td>
<td valign="top" align="left">Photosynthetically Available Radiation (&#x03BC;mole photons m<sup>&#x2013;2</sup> s<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>K</italic><sub><italic>d</italic></sub>(<italic>PAR</italic>)</td>
<td valign="top" align="left">Diffuse attenuation coefficient of PAR (m<sup>&#x2013;1</sup>)</td>
</tr>
<tr>
<td valign="top" align="left">chl-a</td>
<td valign="top" align="left">Chlorophyll-a concentration (mg m<sup>&#x2013;3</sup>)</td>
</tr>
<tr>
<td valign="top" align="left">CDOM</td>
<td valign="top" align="left">Colored dissolved organic matter</td>
</tr>
<tr>
<td valign="top" align="left">Z<sub><italic>eu</italic></sub></td>
<td valign="top" align="left">Euphotic depth (m)</td>
</tr>
<tr>
<td valign="top" align="left">IOP</td>
<td valign="top" align="left">Inherent optical property</td>
</tr>
<tr>
<td valign="top" align="left">AOP</td>
<td valign="top" align="left">Apparent optical property</td>
</tr>
</tbody>
</table></table-wrap>
</app>
</app-group>
<ref-list>
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