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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.2023.1085542</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>Impact of satellite and regional <italic>in-situ</italic> profile data assimilation on a high-resolution ocean prediction system in the Northwest Pacific</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Chang</surname>
<given-names>Inseong</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1978607"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Kim</surname>
<given-names>Young Ho</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1454572"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Jin</surname>
<given-names>Hyunkeun</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1874272"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Park</surname>
<given-names>Young-Gyu</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1113064"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Pak</surname>
<given-names>Gyundo</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1827052"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Chang</surname>
<given-names>You-Soon</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1268645"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Division of Earth Environmental System Science, Pukyong National University</institution>, <addr-line>Busan</addr-line>, <country>Republic of Korea</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Ocean Circulation Research Center, Korea Institute of Ocean Sciences and Technology</institution>, <addr-line>Busan</addr-line>, <country>Republic of Korea</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Department of Earth Science Education, Kongju National University</institution>, <addr-line>Gongju</addr-line>, <country>Republic of Korea</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Shiqiu Peng, State Key Laboratory of Tropical Oceanography, Chinese Academy of Sciences, China</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Toru Miyama, Japan Agency for Marine-Earth Science and Technology, Japan; Shijian Hu, Institute of Oceanology (CAS), China</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Young Ho Kim, <email xlink:href="mailto:yhokim@pknu.ac.kr">yhokim@pknu.ac.kr</email>
</p>
</fn>
<fn fn-type="other" id="fn002">
<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>23</day>
<month>02</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>10</volume>
<elocation-id>1085542</elocation-id>
<history>
<date date-type="received">
<day>31</day>
<month>10</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>26</day>
<month>01</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Chang, Kim, Jin, Park, Pak and Chang</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Chang, Kim, Jin, Park, Pak and Chang</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 impacts of observation data sets on the high-resolution (1/24&#xb0;) Northwest Pacific prediction system were investigated with the model sensitivity tests. We compared the model experiments assimilating the different combinations of the observation data sets, such as the sea surface height derived from satellite altimetry, sea surface temperature, and <italic>in-situ</italic> profiles, based on the Ensemble Optimal Interpolation. Pseudo-profiles constructed by the method of Cooper and Haines (1996, CH96) were assimilated into the model to assimilate sea surface height data. CH96 applied a conservation principle to derive pseudo-profiles by rearranging preexisting profiles. The comparison of the model experiments suggests that each observation data set enhances the model performance. Especially, the assimilation of the sea surface height reduces the model error by more than 9.81% and 6.44%, respectively, in terms of the root-mean-square error of the ocean temperature and salinity in the subsurface layer. It is interesting that the assimilation of the <italic>in-situ</italic> temperature profiles in the Korean marginal seas contributes to improving the reproducibility of the subsurface temperature and salinity in the East/Japan Sea (EJS) as well as Kuroshio-Kuroshio Extension (K-KE) regions. The improvement in the K-KE region seems to be related to the reproducibility of the Kuroshio axis. As the water mass in the EJS flows into the Pacific Ocean through the Tsugaru Strait, it affects the front of the Sanriku confluence, and it seems to eventually control the Oyashio Current and Kuroshio axis. In conclusion, this study evaluated the contribution of each observation component to ocean analysis in the KOOS-OPEM and confirmed the role of the existing observation networks. This study also suggests that greater attention should be paid to the role of regional ocean observation networks to improve the forecast skill of the ocean prediction system not only in the region but also in the open ocean, such as the Pacific Ocean.</p>
</abstract>
<kwd-group>
<kwd>satellite altimetry</kwd>
<kwd>data assimilation</kwd>
<kwd>ensemble optimal interpolation</kwd>
<kwd>KOOS-OPEM</kwd>
<kwd>regional ocean observing networks</kwd>
</kwd-group>
<contract-num rid="cn001">20180447, 20190344, 20210642</contract-num>
<contract-sponsor id="cn001">Ministry of Oceans and Fisheries<named-content content-type="fundref-id">10.13039/501100003566</named-content>
</contract-sponsor>
<counts>
<fig-count count="10"/>
<table-count count="5"/>
<equation-count count="10"/>
<ref-count count="45"/>
<page-count count="14"/>
<word-count count="6860"/>
</counts>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>The Northwest Pacific (NWP) has a complicated ocean circulation system consisting of several major currents including the North Equatorial Countercurrent, Subtropical Countercurrent, Oyashio current (OYC), and the Kuroshio Current (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>). The Kuroshio current is a strong western boundary current, accompanied by energetic variability associated with mesoscale features such as eddies and meander. In addition, four major marginal seas, the South China Sea (SCS), the East China Sea, the Yellow Sea, and the East/Japan Sea (EJS), are connected by four narrow straits: Taiwan, Korea/Tsushima, Tsugaru, and Soya Strait. As ocean currents between the marginal seas distribute heat, salt, and other material through straits, it is important to determine the circulation and variability in the marginal seas and their relation to each other and the NWP (<xref ref-type="bibr" rid="B6">Cho et&#xa0;al., 2009</xref>). The Korea Institute of Ocean Science and Technology (KIOST) has developed the Korea Operational Oceanographic System&#x2013;Ocean Predictability Experiment for Marine environment (KOOS-OPEM, <xref ref-type="bibr" rid="B31">Park et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B23">Kim et&#xa0;al., 2021</xref>), a high-resolution ocean prediction system for the NWP ocean, to understand the complicated ocean circulation system of the NWP ocean and the relationship between the marginal seas and the NWP and to rapidly respond to extreme marine events and accidents.</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>Ocean current map in Northwest pacific is from <xref ref-type="bibr" rid="B32">Park et&#xa0;al. (2013)</xref>.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g001.tif"/>
</fig>
<p>Ocean models are imperfect and inevitable sources of uncertainties, such as initial and boundary conditions, model parameterization, and force fields, which may affect their outputs. An efficient strategy to address these uncertainties and improve forecasts is to assimilate available satellite and <italic>in-situ</italic> observation data into ocean models, thereby optimizing the initial conditions of the ocean model. Generally, data assimilation techniques are classified into two types: variational and sequential. One of the most commonly used variational methods is 4D-VAR whereas the Ensemble Kalman Filter (EnKF), introduced by <xref ref-type="bibr" rid="B10">Evensen (1994)</xref> and <xref ref-type="bibr" rid="B4">Burgers et&#xa0;al. (1998)</xref>, is the most commonly used sequential method. However, these methods are limited because they are computationally expensive. Therefore, the ensemble optimal interpolation (EnOI), a simplification of the EnKF method, was proposed by <xref ref-type="bibr" rid="B11">Evensen (2003)</xref> and provides a cost-effective alternative to the EnKF. EnOI estimates the background error covariance by using a time-invariant ensemble of model states sampled from long-term model results. EnOI has many advantages, such as inherent multivariate, quasi-dynamically consistent, inhomogeneous, and anisotropic covariance. Accordingly, EnOI has been adopted in many operational ocean forecast systems, such as the data assimilation system of KIOST (DASK, <xref ref-type="bibr" rid="B21">Kim et&#xa0;al., 2015</xref>) and Bluelink Ocean Data Assimilation System (BODAS, <xref ref-type="bibr" rid="B26">Oke et&#xa0;al., 2008</xref>).</p>
<p>Traditionally, observational data used in ocean data assimilation include sea surface temperature (SST), temperature/salinity (T/S) profiles, and sea surface height (SSH) derived from satellite altimetry data. SST observations have been widely used in ocean data assimilation because SST is an important ocean variable that connects many processes, such as the air-sea exchange of energy and the formation of water mass in the upper ocean. The assimilation of the T/S profiles improves the representation of seawater density, indicating the mass of water. In particular, the profiles directly affect the ocean heat content (<xref ref-type="bibr" rid="B45">Zhou et&#xa0;al., 2021</xref>). The assimilation of SSH improves the ocean surface currents. In addition, these data can reflect the state of the subsurface structure, which provides a physical foundation for improving the temperature and salinity structures of ocean prediction models <italic>via</italic> assimilation (<xref ref-type="bibr" rid="B37">Troccoli and Haines, 1999</xref>). However, it is difficult to project satellite altimetry data onto subsurface density structures. In addition, because the assimilation of satellite altimetry data does not impose constraints on the vertical density structure, consistent adjustments of temperature/salinity should be considered to maintain the density structure. However, when the temperature changes due to the assimilation of satellite altimetry data, adjustment of salinity is required to conserve the correct density stratification (<xref ref-type="bibr" rid="B36">Troccoli et&#xa0;al., 2002</xref>; <xref ref-type="bibr" rid="B39">Vialard et&#xa0;al., 2003</xref>). Therefore, if the data assimilation system is not properly applied, the assimilation of satellite altimetry data can negatively affect the salinity field while improving the temperature (<xref ref-type="bibr" rid="B13">Fu and Zhu, 2011</xref>).</p>
<p>Various methods have been proposed to address these problems and effectively assimilate satellite altimetry data. For example, the direct assimilation method for satellite altimetry data using ensemble-based techniques (<xref ref-type="bibr" rid="B29">Parent et&#xa0;al., 2003</xref>; <xref ref-type="bibr" rid="B35">Testut et&#xa0;al., 2003</xref>; <xref ref-type="bibr" rid="B3">Birol et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B26">Oke et&#xa0;al., 2008</xref>; <xref ref-type="bibr" rid="B8">Counillon and Bertino, 2009</xref>; <xref ref-type="bibr" rid="B44">Zheng and Zhu, 2015</xref>) achieved the projection of surface information onto subsurface structures through the inherent multivariate relation derived from the ensembles. <xref ref-type="bibr" rid="B43">Yan et&#xa0;al. (2004)</xref> have proposed an assimilation method based on 3D-VAR by developing a statistical relationship between the SSH and the subsurface structure of temperature and salinity. <xref ref-type="bibr" rid="B7">Cooper and Haines (1996)</xref> (hereafter CH96) applied the conservation principle to project altimetry information into subsurface structures. CH96 derived pseudo-profiles based on the rearrangement of the preexisting water columns of the model while preserving the water properties. The pseudo-profiles at the specific grid points are constructed by vertically replacing the preexisting profile, which reduces the surface pressure difference between the modeled and observed SSH with conserving the bottom pressure.</p>
<p>In this study, to quantitatively evaluate the contribution of <italic>in-situ</italic> T/S profiles and satellite observation data, such as SST and satellite altimetry, to the ocean prediction system, we conducted a sensitivity experiment by applying EnOI to KOOS-OPEM. <xref ref-type="bibr" rid="B9">El-Geziry and Bryden (2010)</xref> stated that Mediterranean circulation affects not only the Mediterranean basin on a regional scale but also the global circulation due to its effective contribution to the North Atlantic circulation system. Like the Mediterranean Sea, the EJS is a semi-enclosed marginal sea exchanging water mass with the open ocean through narrow straits. This study also aimed to investigate the extent to which assimilation of <italic>in-situ</italic> temperature profile data in Korean marginal seas affects not only the Korean marginal seas including the EJS but also the open ocean such as the NWP. The remainder of this paper is organized as follows: the model configuration, details of the data assimilation system, experimental design, and observation data used in this experiment are described in Section 2 and the results of all experiments are compared with respect to observations in Section 3, and Section 4 discusses the results and summarizes the major conclusions.</p>
</sec>
<sec id="s2" sec-type="materials|methods">
<label>2</label>
<title>Materials and methods</title>
<sec id="s2_1">
<label>2.1</label>
<title>Model and data assimilation system</title>
<sec id="s2_1_1">
<label>2.1.1</label>
<title>Model configuration</title>
<p>The KOOS-OPEM is based on the Modular Ocean Model Version 5 (MOM5) developed by the Geophysical Fluid Dynamics Laboratory (GFDL) and includes the Sea Ice Simulator (<xref ref-type="bibr" rid="B42">Winton, 2000</xref>). This model solves primitive equations with hydrostatic and Boussinesq approximations using the Arakawa-B grid system (<xref ref-type="bibr" rid="B2">Arakawa and Lamb, 1977</xref>). The horizontal domain of this model covers the NWP including the Korean marginal seas and the Yellow and East China Seas, ranging from 5&#xb0;N to 63&#xb0;N and 99&#xb0;E to 170&#xb0;E, with a horizontal resolution of 1/24&#xb0; in latitude and longitude. This model has a z-star coordinate system of 51 vertical levels with a finer resolution near the sea surface. K-profile parameterization was employed for the vertical mixing scheme (<xref ref-type="bibr" rid="B38">Troen and Mahrt, 1986</xref>; <xref ref-type="bibr" rid="B24">Large et&#xa0;al., 1994</xref>). This model uses tidal mixing parameterization as implemented by <xref ref-type="bibr" rid="B34">Simmons et&#xa0;al. (2004)</xref>, the GM isopycnal mixing scheme for tracer mixing (<xref ref-type="bibr" rid="B15">Gent and Mcwilliams, 1990</xref>), and the Smagorinsky biharmonic scheme for horizontal momentum mixing (<xref ref-type="bibr" rid="B17">Griffies and Hallberg, 2000</xref>). The model topography was generated by merging the GEBCO 08 data set (<uri xlink:href="http://www.gebco.net">http://www.gebco.net</uri>) and the Korbathy regional dataset (<xref ref-type="bibr" rid="B33">Seo, 2008</xref>).</p>
<p>This model was forced by lateral boundary conditions from the Global Ocean Ensemble Physics Reanalysis, including the daily ocean velocity, temperature, salinity, and SSH provided by the Copernicus Marine Environment Monitoring Service (CMEMS, <uri xlink:href="https://marine.copernicus.eu/">https://marine.copernicus.eu/</uri>). The surface boundary forcings were calculated by applying the bulk formula of <xref ref-type="bibr" rid="B25">Large and Yeager (2004)</xref> to the atmospheric variables, including air temperature, specific humidity, surface net solar radiation, surface thermal radiation, snowfall, runoff, mean sea level pressure, total cloud cover, wind velocity, and precipitation from ERA5, provided by the European Center for Medium-Range Weather Forecasts (ECMWF). To reflect runoff and river discharge, climatological data of 40 rivers obtained from RivDIS (<xref ref-type="bibr" rid="B41">V&#xf6;r&#xf6;smarty et&#xa0;al., 1998</xref>) were inserted into the ocean grid.</p>
</sec>
<sec id="s2_1_2">
<label>2.1.2</label>
<title>EnOI</title>
<p>The basic equation for data assimilation is as follows:</p>
<disp-formula>
<label>(1)</label>
<mml:math display="block" id="M1">
<mml:mrow>
<mml:msup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mi>a</mml:mi>
</mml:msup>
<mml:mo>=</mml:mo>
<mml:msup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mi>f</mml:mi>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:mtext>K(</mml:mtext>
<mml:mi>d</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mtext>H</mml:mtext>
<mml:msup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mi>f</mml:mi>
</mml:msup>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula>
<label>(2)</label>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mtext>K=P</mml:mtext>
</mml:mrow>
<mml:mtext>f</mml:mtext>
</mml:msup>
<mml:msup>
<mml:mtext>H</mml:mtext>
<mml:mi>T</mml:mi>
</mml:msup>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mtext>H</mml:mtext>
<mml:msup>
<mml:mtext>P</mml:mtext>
<mml:mi>f</mml:mi>
</mml:msup>
<mml:msup>
<mml:mtext>H</mml:mtext>
<mml:mi>T</mml:mi>
</mml:msup>
<mml:mo>+</mml:mo>
<mml:mtext>R</mml:mtext>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where &#x3c9;<sup>f</sup> and &#x3c9;<sup>a</sup> represent the forecast and analytical state vectors, respectively; <italic>d</italic> is the vector of observations; K is the Kalman gain matrix; H is an operator that transforms from the model grid to the observation grid. Matrices P<sup>f</sup> and R represent the background error covariance and observation error covariance, respectively. The superscript <italic>T</italic> denotes the matrix transpose.</p>
<p>EnOI is based on the work of <xref ref-type="bibr" rid="B11">Evensen (2003)</xref> and the analysis approach of <xref ref-type="bibr" rid="B4">Burgers et&#xa0;al. (1998)</xref>. The practical implementation of the EnOI is similar to the EnKF; however, the EnOI analysis is estimated in a stationary ensemble composed of long-time model integration, and statistical errors do not develop over time. EnOI estimates the background covariance error matrix P<sup>f</sup> as follows:</p>
<disp-formula>
<label>(3)</label>    <mml:math display="block" id="M3">
<mml:mrow>
<mml:msup>
<mml:mtext>P</mml:mtext>
<mml:mi>f</mml:mi>
</mml:msup>
<mml:mo>=</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
<mml:msup>
<mml:mrow>
<mml:mtext>A'A'</mml:mtext>
</mml:mrow>
<mml:mi>T</mml:mi>
</mml:msup>
<mml:mo stretchy="false">/</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mi>N</mml:mi>
<mml:mi>e</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula>
<label>(4)</label>
<mml:math display="block" id="M4">
<mml:mrow>
<mml:mtext>A'=[</mml:mtext>
<mml:msubsup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mn>1</mml:mn>
<mml:mo>'</mml:mo>
</mml:msubsup>
<mml:mo>,</mml:mo>
<mml:msubsup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mn>2</mml:mn>
<mml:mo>'</mml:mo>
</mml:msubsup>
<mml:mo>,</mml:mo>
<mml:mo>&#x2026;</mml:mo>
<mml:mo>,</mml:mo>
<mml:msubsup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mrow>
<mml:msub>
<mml:mi>N</mml:mi>
<mml:mi>e</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>'</mml:mo>
</mml:msubsup>
<mml:mo>]</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>N<sub>e</sub>
</italic> is the ensemble size, <italic>&#x3b1;</italic> (&#x2208;0,1) is introduced as a scaling factor to reduce the variance (<xref ref-type="bibr" rid="B8">Counillon and Bertino, 2009</xref>), A&#x2019; is a stationary and historical ensemble, and <inline-formula>
<mml:math display="inline" id="im1">
<mml:mrow>
<mml:msubsup>
<mml:mi>&#x3c9;</mml:mi>
<mml:mi>i</mml:mi>
<mml:mo>'</mml:mo>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula>is the <italic>i</italic>
<sup>th</sup> model anomaly. In this study, the scaling factor <italic>&#x3b1;</italic> was considered 0.25 (<xref ref-type="bibr" rid="B28">Oke et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B21">Kim et&#xa0;al., 2015</xref>). The ensemble members were selected from the monthly mean historical data of the 50-months model integration, and the climatological monthly mean was removed.</p>
<p>An ensemble-based data assimilation system can highly estimate correlations between long-distance points that are likely to be independent of each other when a small number of ensemble members are used (<xref ref-type="bibr" rid="B22">Kim et&#xa0;al., 2008</xref>). To reduce this sampling error, we applied localization techniques (<xref ref-type="bibr" rid="B18">Hamill et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B19">Houtekamer and Mitchell, 2001</xref>; <xref ref-type="bibr" rid="B27">Oke et&#xa0;al., 2007</xref>; <xref ref-type="bibr" rid="B21">Kim et&#xa0;al., 2015</xref>) of the Schur product (<xref ref-type="bibr" rid="B14">Gaspari and Cohn, 1999</xref>). After applying localization, the Kalman gain matrix was expressed as follows:</p>
<disp-formula>
<label>(5)</label>
<mml:math display="block" id="M5">
<mml:mrow>
<mml:mi>&#x3c1;</mml:mi>
<mml:mo>&#x2218;</mml:mo>
<mml:mrow>
<mml:mo>[</mml:mo>
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</disp-formula>
<disp-formula>
<label>(6)</label>
<mml:math display="block" id="M6">
<mml:mrow>
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</disp-formula>
<p>where <italic>&#x3c1;</italic> &#xb0; B is calculated by <italic>&#x3c1;</italic>, a function of the distance (<italic>L</italic>) between <italic>x<sub>i</sub>
</italic> and <italic>xj</italic>. <italic>&#x3c1;</italic> is given as a function of the horizontal and vertical decorrelation distance, which has a value of 0&#x2013;1. As the distance between two points increases, <italic>&#x3c1;</italic> becomes closer to 0, and when the distance exceeds a certain length, <italic>&#x3c1;</italic> becomes 0. In the ocean prediction model, <italic>&#x3c1;</italic> can be applied to the horizontal and vertical decorrelation distances. In this study, the horizontal and vertical decorrelation distances were 150&#xa0;km and 100&#xa0;m, respectively.</p>
</sec>
<sec id="s2_1_3">
<label>2.1.3</label>
<title>Altimetry assimilation method</title>
<p>The method used to assimilate satellite altimetry data was based on the CH96 scheme. To construct the pseudo-profiles, CH96 assumes that the bottom pressure and potential vorticity are preserved. Following CH96, the bottom constraint is as below:</p>
<disp-formula>
<label>(7)</label>
<mml:math display="block" id="M7">
<mml:mrow>
<mml:mi>g</mml:mi>
<mml:mstyle displaystyle="true">
<mml:mrow>
<mml:msubsup>
<mml:mo>&#x222b;</mml:mo>
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<mml:mo>&#x2212;</mml:mo>
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</mml:mrow>
</mml:msubsup>
<mml:mrow>
<mml:mi>&#x394;</mml:mi>
<mml:mi>&#x3c1;</mml:mi>
<mml:mi>d</mml:mi>
<mml:mi>z</mml:mi>
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<mml:mi>p</mml:mi>
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</mml:msub>
</mml:mrow>
</mml:mrow>
</mml:mstyle>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where &#x394;<italic>&#x3c1;</italic>, &#x394;p<sub>s</sub>, and <italic>H</italic> are density increment of the water column, change in surface pressure, and depth of the water column, respectively. The change in SSH should be compensated for by the change in the weight of the entire water column. If the model SSH is higher than the observed SSH, the water columns of the model are displaced upward, and some light water masses at the surface are removed and replaced by heavy water masses at the bottom. Similarly, if the model SSH was lower than the observed SSH, the water columns of the model were displaced downward to decrease the density of the water column. The amount of vertical displacement of the water columns was such that the bottom pressure did not change. The displacement &#x394;h is expressed as follows:</p>
<disp-formula>
<label>(8)</label>
<mml:math display="block" id="M8">
<mml:mrow>
<mml:mi>&#x394;</mml:mi>
<mml:mtext>h=</mml:mtext>
<mml:mfrac>
<mml:mrow>
<mml:mi>&#x394;</mml:mi>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mi>g</mml:mi>
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</mml:msup>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
</disp-formula>
<p>The pseudo-profiles created by CH96 were assimilated into the ocean prediction model instead of SSH observation data through EnOI. The characteristic of CH96 is that convection does not occur because the density structure is preserved, except for the top and bottom, which are removed or added according to the change in surface pressure by conserving the volume of the water mass. In addition, conserving the bottom pressure prevents changes in the bottom torques, thereby decreasing the interactions with steep topography (<xref ref-type="bibr" rid="B1">Alves et&#xa0;al., 2001</xref>).</p>
</sec>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Experiments and observation</title>
<sec id="s2_2_1">
<label>2.2.1</label>
<title>Experimental design</title>
<p>To investigate the impact of the data assimilation of <italic>in-situ</italic> and satellite observations and this indirect assimilation system, we performed six experiments based on observation data from 1993. In all simulations, the model was sequentially integrated forward in time using the initial conditions, which assimilated the SST and T/S profiles from 1990 to 1992. Posterior analysis of the previous cycle was used for the prior initial conditions for each cycle.</p>
<p>For comparison, the first experiment (CTR) was a control experiment without assimilation. The second experiment (EXP01) assimilated the SST. The third and fourth experiments (EXP02 and EXP03) assimilated the SST and T/S profiles. The fifth and sixth experiments (EXP04 and EXP05) assimilated all the variables. To investigate how the assimilation of data obtained in the marginal sea affects the other regions, EXP03 and EXP05 additionally assimilated the Korea Oceanographic Data Center (KODC, <uri xlink:href="https://www.nifs.go.kr/kodc">https://www.nifs.go.kr/kodc</uri>) profile data. Details for the experiments are shown in <xref ref-type="table" rid="T1">
<bold>Table&#xa0;1</bold>
</xref>.</p>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>Summary of the sensitivity experiment.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left"/>
<th valign="middle" align="center">SST</th>
<th valign="middle" align="center">T/S profiles</th>
<th valign="middle" align="center">KODC profiles</th>
<th valign="middle" align="center">SSH (pseudo-profile)</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">
<bold>CTR</bold>
</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>EXP01</bold>
</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>EXP02</bold>
</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">&#x2013;</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>EXP03</bold>
</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">&#x2013;</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>EXP04</bold>
</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">&#x2013;</td>
<td valign="middle" align="center">o</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>EXP05</bold>
</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
<td valign="middle" align="center">o</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>SST, sea surface temperature; T/S, temperature/saline; KODC, Korea Oceanographic Data center; SSH, sea surface height; CTR, control; EXP, experiment.</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s2_2_2">
<label>2.2.2</label>
<title>
<italic>In-situ</italic> data</title>
<p>
<italic>In-situ</italic> T/S profile data, which were obtained from various platforms, including conductivity temperature and depth (CTD) sensors, ocean station data (OSD), expendable bathythermographs (XBT), and moored buoys (MRB), were obtained from the World Ocean Database 2018 (WOD). The National Institute of Fisheries Science (NIFS) has produced a KODC database by researching the marine environment, including temperature, as well as other variables such as nutrient concentration and salinity, using CTD at standard observation depths (0, 10, 20, 30, 50, 75, 100, 125, 150, 200, 250, 300, 400, and 500&#xa0;m), in the seas around the Korean Peninsula six times a year (for even months) from 1961 to the present. The temperature profiles obtained from the KODC were used in this study. KODC salinity data were not used in this study because they contained serious time-dependent bias errors as previously reported by <xref ref-type="bibr" rid="B30">Park (2021)</xref>. <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2A</bold>
</xref> shows the KODC and WOD temperature profile data used when assimilating the profile in February. We used 852 temperature data points collected from 23 stations. These <italic>in-situ</italic> profile data were assimilated into KOOS-OPEM every seven days.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Distribution of <italic>in-situ</italic> temperature profiles used in data assimilation and validation. <bold>(A)</bold> temperature profiles used in data assimilation in February 1993. Crimson and orange dots denote profiles taken from World Ocean Database 2018 and Korea Oceanographic Data Center (KODC), respectively. <bold>(B)</bold> temperature profiles used in validation. Red, magenta, yellow, cyan and green dots denote temperature profiles located Northwestern Pacific (NWP), South China Sea (SCS), Oyashio Current (OYC), East/Japan Sea (EJS) and Kuroshio-Kuroshio Extension (K-KE) region, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g002.tif"/>
</fig>
<p>To compare the performance of the vertical profiles of temperature and salinity, the independent T/S profiles (depth above approximately 500&#xa0;m) of WOD and KODC, not used for assimilation, were used. When selecting the validation data, one-third of the total data was randomly selected. The spatial distribution of the validation profile is shown in <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2B</bold>
</xref>.</p>
</sec>
<sec id="s2_2_3">
<label>2.2.3</label>
<title>Satellite data</title>
<p>The National Centers for Environmental Information (NOAA)&#x2019;s 1/4&#xb0; daily optimum SST (OISST) generated by interpolating and extrapolating observations from different platforms such as satellites, buoys, ships, and Argo floats were assimilated into KOOS-OPEM every day. The along-track SSH data from TOPEX/POSEIDON and ERS-1 were downloaded from CMEMS and used to construct the pseudo-profiles. The original resolution of the along-track SSH data was approximately 7&#xa0;km; however, we used along-track data subsampled every 50&#xa0;km to efficiently use computational resources. The pseudo-profiles derived from the along-track data were also assimilated daily.</p>
<p>To compare the performance of SST, the Operational Sea Surface Temperature and Sea Ice Analysis (OSTIA; <xref ref-type="bibr" rid="B16">Good et al., 2020</xref>) analysis downloaded from CMEMS was used. These data were generated from satellite and <italic>in-situ</italic> data through high-resolution analysis and intercomparison with spatial and temporal resolutions of 0.054&#xb0; and daily, respectively. Gridded absolute dynamic topography data were used to compare the performance of the SSH. The temporal and spatial resolution of these data were one day and 1/4&#xb0;, respectively. Because the gridded SSH data were generated by merging SSH measurements from multiple satellite altimetry, it can be suggested that the generated data are dependent on along-track data. However, as we did not directly assimilate the along-track data but assimilated pseudo-profiles instead, the results are independent of the gridded data.</p>
</sec>
<sec id="s2_2_4">
<label>2.2.4</label>
<title>Statistical metrics</title>
<p>The metrics used to assess assimilation performance were the root-mean-square error (RMSE) and impact of assimilation (IOA), as defined by <xref ref-type="bibr" rid="B5">Chen et&#xa0;al. (2018)</xref>. These metrics are defined as follows:</p>
<disp-formula>
<label>(8)</label>
<mml:math display="block" id="M9">
<mml:mrow>
<mml:mtext>RMSE=</mml:mtext>
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</mml:msqrt>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula>
<label>(9)</label>
<mml:math display="block" id="M10">
<mml:mrow>
<mml:mtext>IOA=</mml:mtext>
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<mml:mi>R</mml:mi>
<mml:mi>M</mml:mi>
<mml:mi>S</mml:mi>
<mml:msub>
<mml:mi>E</mml:mi>
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:mi>X</mml:mi>
<mml:mi>P</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>M</mml:mi>
<mml:mi>S</mml:mi>
<mml:msub>
<mml:mi>E</mml:mi>
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mi>T</mml:mi>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>100</mml:mn>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where M<italic>
<sub>i</sub>
</italic> is the i<sup>th</sup> model result of each experiment, O<italic>
<sub>i</sub>
</italic> is the i<sup>th</sup> observation, n is the number of values, and the overbar is the average over all periods. <italic>RMSE<sub>CTR</sub>
</italic> and <italic>RMSE<sub>EXP</sub>
</italic> denote the RMSEs of the CTR and assimilation experiment with respect to the observation, respectively. IOA is a metric that indicates the improvement of the RMSE compared to CTR. The larger the IOA, the greater the improvement in ocean analysis by the assimilation of each variable.</p>
</sec>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results</title>
<sec id="s3_1">
<label>3.1</label>
<title>Sea surface temperature</title>
<p>
<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref> shows the comparison of the spatial distribution of the RMSE for SST with respect to OSTIA of all experiments. All experiments showed a large RMSE near the Korean and Chinese coastlines. The RMSE of the CTR was large in the middle and high-latitude regions, including the EJS and Kuroshio-Kuroshio Extension (K-KE), and was the largest in K-KE. The RMSEs of all assimilation experiments were greatly reduced in most regions by SST assimilation. In particular, the RMSEs of all experiments were significantly improved in the EJS and K-KE regions with a large RMSE in the CTR. However, the difference in the RMSE of SST is not significant in <xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref> for the SST is constrained in all experiments by assimilating the OISST. The contributions of <italic>in-situ</italic> T/S profiles and SSH will be shown in next sections.</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Spatial distribution of RMSE for SST with respect to OSTIA SST. Spatial averaged RMSEs of each experiment are shown on each figure. <bold>(A-F)</bold> represent the results of CTR and EXP01-05, respectively. RMSE, root-mean-square error; SST, sea salt temperature; CTR, control; EXP, experiment; OSTIA, Operational Sea Surface Temperature, and Sea Ice Analysis.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g003.tif"/>
</fig>
<p>
<xref ref-type="table" rid="T2">
<bold>Table&#xa0;2</bold>
</xref> compares the RMSE and IOA for SST by region for all assimilation experiments. The EXP01 of the average IOA was approximately 23.77%, and IOA was the highest in the K-KE region. In the NWP and OYC regions, the RMSE further improved after assimilating the T/S profiles. In the K-KE and EJS regions, the RMSE improved after assimilating the pseudo-profiles; however, in the OYC region, the RMSE increased. In the EJS region, EXP03 and EXP05, in which the profiles of KODC were assimilated, showed a higher IOA than EXP02 and EXP04, and EXP03 which did not assimilate the pseudo-profiles showed a lower RMSE than EXP04. These results indicate that the assimilation of SST satellite data plays a major role in improving the SST field, and that T/S and pseudo-profiles also play a partial role. However, the assimilation of the pseudo-profiles resulted in a slight increase in the RMSE at higher latitudes, such as the OYC region. Moreover, the KODC data reduced the RMSE for SST in the EJS; however, this effect was not observed in other regions.</p>
<table-wrap id="T2" position="float">
<label>Table&#xa0;2</label>
<caption>
<p>Root-mean-square error (RMSE) averaged in space and time for SST by region from all experiments.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left"/>
<th valign="middle" align="center">CTR</th>
<th valign="middle" align="center">EXP01</th>
<th valign="middle" align="center">EXP02</th>
<th valign="middle" align="center">EXP03</th>
<th valign="middle" align="center">EXP04</th>
<th valign="middle" align="center">EXP05</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">
<bold>Northwest Pacific</bold>
</td>
<td valign="middle" align="center">0.45</td>
<td valign="middle" align="center">0.38 (15.56%)</td>
<td valign="middle" align="center">0.37 (17.78%)</td>
<td valign="middle" align="center">0.37 (17.78%)</td>
<td valign="middle" align="center">0.37 (17.78%)</td>
<td valign="middle" align="center">0.37 (17.78%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>South China Sea</bold>
</td>
<td valign="middle" align="center">0.65</td>
<td valign="middle" align="center">0.53 (18.46%)</td>
<td valign="middle" align="center">0.53 (18.46%)</td>
<td valign="middle" align="center">0.53 (18.46%)</td>
<td valign="middle" align="center">0.51 (21.54%)</td>
<td valign="middle" align="center">0.51 (21.54%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>Oyashio</bold>
</td>
<td valign="middle" align="center">1.21</td>
<td valign="middle" align="center">0.95 (21.49%)</td>
<td valign="middle" align="center">0.94 (22.31%)</td>
<td valign="middle" align="center">0.94 (22.31%)</td>
<td valign="middle" align="center">0.96 (20.66%)</td>
<td valign="middle" align="center">0.96 (20.66%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>East/Japan sea</bold>
</td>
<td valign="middle" align="center">1.76</td>
<td valign="middle" align="center">1.22 (30.68%)</td>
<td valign="middle" align="center">1.22 (30.68%)</td>
<td valign="middle" align="center">1.17 (33.52%)</td>
<td valign="middle" align="center">1.18 (32.95%)</td>
<td valign="middle" align="center">1.17 (33.52%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>Kuroshio-Kuroshio Extension</bold>
</td>
<td valign="middle" align="center">1.47</td>
<td valign="middle" align="center">0.99 (32.65%)</td>
<td valign="middle" align="center">0.99 (32.65%)</td>
<td valign="middle" align="center">0.99 (32.65%)</td>
<td valign="middle" align="center">0.97 (34.01%)</td>
<td valign="middle" align="center">0.97 (34.01%)</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>The number in the parentheses below RMSE represents the impact of assimilation (IOA).</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Vertical structure</title>
<p>The vertical performance of each experiment was evaluated using WOD18 and KODC data, which were not used for assimilation. To investigate regional effects, the domain was separated into five regions: NWP, SCS, OYC, EJS, and K-KE. Each region is denoted by a colored dot in <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2B</bold>
</xref>.</p>
<p>
<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref> shows the vertical profile of the RMSE for both temperature and salinity in each region. In the NWP region, the more observation data are assimilated, the lower the RMSE for the temperature and salinity at the overall depth. However, after assimilating SST, the RMSE for salinity in the subsurface layer increased compared to that of the CTR. Pseudo-profiles were the observational data that contributed the most to improving the RMSE for temperature and salinity in the NWP region. After the assimilation of these data, the RMSE for the temperature and salinity of the subsurface layer decreased substantially. Similar to the NWP region, in the SCS region, the pseudo-profiles contributed the most to reducing the RMSE, and assimilation of KODC data decreased the RMSE for temperature but increased that for salinity. In the OYC region, all experiments showed higher RMSE for temperature than that of the CTR at 50&#xa0;m. However, in the subsurface layer, the RMSE decreased after assimilating the pseudo-profiles. The pseudo-profiles also contributed the most to reducing the RMSE in EJS and K-KE regions, and after assimilating KODC data, the RMSE for temperature decreased whereas that for salinity improved in both regions, although the salinity data of KODC were not assimilated. <xref ref-type="table" rid="T2">
<bold>Tables&#xa0;2</bold>
</xref> and <xref ref-type="table" rid="T3">
<bold>3</bold>
</xref> show the average RMSE of the profiles in <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref> by region. As mentioned above, because the RMSE of the other experiments was larger than that of the CTR at 50&#xa0;m in the OYC, the average RMSE for the entire depth was larger than that of the CTR. These results indicate that pseudo-profiles derived from satellite altimetry data in most areas significantly contribute to improving the vertical structure of temperature and salinity, and the assimilation of KODC data improved the vertical structure of temperature and salinity in the K-KE and EJS regions. (<xref ref-type="table" rid="T4">
<bold>Table&#xa0;4</bold>
</xref>)</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>RMSE for temperature and salinity profiles at the region of <bold>(A)</bold> Northwestern Pacific (NWP), <bold>(B)</bold> South China Sea (SCS), <bold>(C)</bold> Oyashio Current (OYC), <bold>(D)</bold> East/Japan Sea (EJS), and <bold>(E)</bold> Kuroshio-Kuroshio extension (K-KE). Gray, black, violet, blue, green and red lines denote CTR and EXP01-05, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g004.tif"/>
</fig>
<table-wrap id="T3" position="float">
<label>Table&#xa0;3</label>
<caption>
<p>RMSE averaged in space and time for temperature by region from all experiments.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left"/>
<th valign="middle" align="center">CTR</th>
<th valign="middle" align="center">EXP01</th>
<th valign="middle" align="center">EXP02</th>
<th valign="middle" align="center">EXP03</th>
<th valign="middle" align="center">EXP04</th>
<th valign="middle" align="center">EXP05</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">
<bold>Northwest pacific</bold>
</td>
<td valign="middle" align="center">1.38</td>
<td valign="middle" align="center">1.37 (0.72%)</td>
<td valign="middle" align="center">1.31 (5.07%)</td>
<td valign="middle" align="center">1.31 (5.07%)</td>
<td valign="middle" align="center">1.25 (9.42%)</td>
<td valign="middle" align="center">1.25 (9.42%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>South China Sea</bold>
</td>
<td valign="middle" align="center">1.46</td>
<td valign="middle" align="center">1.82 (-24.66%)</td>
<td valign="middle" align="center">1.58 (-8.22%)</td>
<td valign="middle" align="center">1.42 (2.74%)</td>
<td valign="middle" align="center">1.19 (18.49%)</td>
<td valign="middle" align="center">1.16 (20.55%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>Oyashio</bold>
</td>
<td valign="middle" align="center">0.95</td>
<td valign="middle" align="center">1.18 (-24.21%)</td>
<td valign="middle" align="center">1.10 (-15.79%)</td>
<td valign="middle" align="center">1.13 (-18.95%)</td>
<td valign="middle" align="center">1.06 (-11.58%)</td>
<td valign="middle" align="center">1.04 (-9.47%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>East/Japan sea</bold>
</td>
<td valign="middle" align="center">3.07</td>
<td valign="middle" align="center">2.66 (13.36%)</td>
<td valign="middle" align="center">2.35 (23.45%)</td>
<td valign="middle" align="center">2.34 (23.78%)</td>
<td valign="middle" align="center">2.33 (24.10%)</td>
<td valign="middle" align="center">2.16 (29.64%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>Kuroshio-Kuroshio Extension</bold>
</td>
<td valign="middle" align="center">2.96</td>
<td valign="middle" align="center">2.25 (23.99%)</td>
<td valign="middle" align="center">2.26 (23.65%)</td>
<td valign="middle" align="center">2.15 (27.36%)</td>
<td valign="middle" align="center">1.90 (35.81%)</td>
<td valign="middle" align="center">1.78 (39.86%)</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>The number in the parentheses below RMSE represents IOA.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<table-wrap id="T4" position="float">
<label>Table&#xa0;4</label>
<caption>
<p>RMSE averaged in space and time for salinity by region from all experiments.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left"/>
<th valign="middle" align="center">CTR</th>
<th valign="middle" align="center">EXP01</th>
<th valign="middle" align="center">EXP02</th>
<th valign="middle" align="center">EXP03</th>
<th valign="middle" align="center">EXP04</th>
<th valign="middle" align="center">EXP05</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">
<bold>Northwest Pacific</bold>
</td>
<td valign="middle" align="center">0.19</td>
<td valign="middle" align="center">0.19 (0.00%)</td>
<td valign="middle" align="center">0.18 (5.26%)</td>
<td valign="middle" align="center">0.18 (5.26%)</td>
<td valign="middle" align="center">0.18 (5.26%)</td>
<td valign="middle" align="center">0.17 (10.53%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>South China Sea</bold>
</td>
<td valign="middle" align="center">0.24</td>
<td valign="middle" align="center">0.24 (0.00%)</td>
<td valign="middle" align="center">0.23 (4.17%)</td>
<td valign="middle" align="center">0.24 (0.00%)</td>
<td valign="middle" align="center">0.20 (16.67%)</td>
<td valign="middle" align="center">0.23 (4.17%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>Oyashio</bold>
</td>
<td valign="middle" align="center">0.16</td>
<td valign="middle" align="center">0.17 (-6.25%)</td>
<td valign="middle" align="center">0.16 (0.0)</td>
<td valign="middle" align="center">0.16 (0.0)</td>
<td valign="middle" align="center">0.15 (6.25%)</td>
<td valign="middle" align="center">0.15 (6.25%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>East/Japan sea</bold>
</td>
<td valign="middle" align="center">0.20</td>
<td valign="middle" align="center">0.18 (10.00%)</td>
<td valign="middle" align="center">0.16 (20.00%)</td>
<td valign="middle" align="center">0.17 (15.00%)</td>
<td valign="middle" align="center">0.16 (20.00%)</td>
<td valign="middle" align="center">0.15 (25.00%)</td>
</tr>
<tr>
<td valign="middle" align="left">
<bold>Kuroshio-Kuroshio extension</bold>
</td>
<td valign="middle" align="center">0.30</td>
<td valign="middle" align="center">0.26 (13.33%)</td>
<td valign="middle" align="center">0.26 (13.33%)</td>
<td valign="middle" align="center">0.25 (16.67%)</td>
<td valign="middle" align="center">0.23 (23.33%)</td>
<td valign="middle" align="center">0.22 (26.67%)</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>The number in the parentheses below RMSE represents IOA.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<p>To comprehensively evaluate the contribution of each observation data by region at the subsurface layer, IOA using the RMSE of the experiment according to the depth (100&#x2013;500 m) with respect to the profile used for each independent validation was calculated and compared by averaging at intervals of 10&#xb0; for the latitude and longitude.</p>
<p>Temperature (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>), when only SST was assimilated (EXP01), had a negative effect on the subsurface layer of most regions, except for some regions in high-latitude regions. EXP02 and EXP03 that assimilated T/S profiles had improved RMSE over EXP01 in the NWP and SCS regions. The assimilation of pseudo-profiles (EXP04 and EXP05) significantly improved the RMSE in most areas, especially in the NWP and regions where the Kuroshio Current passes (120&#xb0;E&#x2013;140&#xb0;E, 25&#xb0;N&#x2013;35&#xb0;N). However, it did not have a significant effect in high-latitude regions (140&#xb0;E&#x2013;170&#xb0;E, 35&#xb0;N&#x2013;65&#xb0;N), except for the EJS. The assimilation of KODC data (EXP03 and EXP05) considerably improved the RMSE not only in the EJS but also in the region where Kuroshio passes and the K-KE region.</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>Distribution of mean IOA for temperature at subsurface layer. <bold>(A-E)</bold> represent the results of EXP01-05, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g005.tif"/>
</fig>
<p>In addition, by comparing the IOA for salinity in each experiment (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>), we found that the assimilation of SST did not improve the RMSE for salinity in the subsurface layer in most regions. The assimilation of the T/S profile substantially improved the RMSE in the NWP and SCS regions, and the assimilation of the pseudo-profiles or the temperature substantially improved the RMSE in the regions where the Kuroshio Current passed; however, the effect of the assimilation of the temperature was not substantial in high-latitude regions. In the assimilation of KODC (EXP03 and EXP05), the RMSE of EXP05, which also assimilated pseudo-profiles, improved in both the EJS and K-KE regions. These results show that the assimilation of SST did not have a significant impact on the subsurface layer whereas that of T/S profiles improved the RMSE in most regions. In addition, the assimilation of pseudo-profiles played a significant role in improving the temperature and salinity at the subsurface layer, similar to the <italic>in-situ</italic> T/S profile data; however, it did not show a significant contribution in high-latitude regions. The assimilation of KODC data, which is Korean marginal sea data, improved the temperature at the subsurface layer in the K-KE and EJS regions, and salinity at the subsurface layer was improved when assimilated with pseudo-profiles.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>Distribution of mean IOA for salinity at subsurface layer. <bold>(A-E)</bold> represent the results of EXP01-05, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g006.tif"/>
</fig>
</sec>
<sec id="s3_3">
<label>3.3</label>
<title>Sea surface height</title>
<p>
<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref> shows the time series of monthly spatial-averaged RMSE for SSH from all experiments according to each region. Pseudo-profiles and SST contributed the most to improving the RMSE for SSH in all regions. SST also improved the RMSE for SSH in all regions. The T/S profiles improved the RMSE for SSH regardless of the season in the NWP region; however, it did not significantly improve the RMSE for SSH in the OYC regions and increased it during the summer season in the K-KE and EJS regions. Moreover, the RMSE of EXP03, which assimilated KODC data, increased from August to November compared to that of EXP02. Notably, the RMSE of EXP05 which assimilated KODC and pseudo-profiles improved from May to September compared to that of EXP04 which did not assimilate KODC data. The data assimilation of KODC data appeared to be more effective in EXP05 with SSH assimilation that in EXP03 without SSH assimilation. The RMSE of EXP05, which assimilated pseudo-profiles, was improved in the NWP during the summer and in the K-KE region from April to June and September to October.</p>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>Monthly mean RMSE for sea surface height at the region of <bold>(A)</bold> Northwestern Pacific (NWP), <bold>(B)</bold> Kuroshio-Kuroshio extension (K-KE), <bold>(C)</bold> East/Japan Sea (EJS) and <bold>(D)</bold> Oyashio Current (OYC). Gray, black, violet, blue, green and red lines denote CTR and EXP01-05, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g007.tif"/>
</fig>
<p>To evaluate the oceanic variability associated with the K-KE region, the Kuroshio axis of the AVISO gridded data and that of each experiment were compared (<xref ref-type="fig" rid="f8">
<bold>Figure&#xa0;8</bold>
</xref>). In January and February, the assimilation effect of each experiment did not appear significant; however, the assimilation effect of each experiment became evident over time, starting in March. The experiments that did not assimilate the pseudo-profiles, including CTR, excessively simulated mesoscale features, such as meandering and eddies. However, experiments that assimilated the pseudo-profiles constrained the features excessively simulated in other experiments. EXP05, which assimilated KODC data, better simulated the Kuroshio axis in most months, except for July and August, compared to EXP04.</p>
<fig id="f8" position="float">
<label>Figure&#xa0;8</label>
<caption>
<p>Monthly mean Kuroshio axis is denoted by the 0.6m SSH. <bold>A&#x2013;L</bold> represent results in January-December, respectively. Orange line denotes Kuroshio axis from the AVISO gridded data. Gray, black, violet, blue, green and red lines denote Kuroshio axis of CTR and EXP01-05, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g008.tif"/>
</fig>
<p>To evaluate this result more quantitatively, the RMSE for the latitude of the Kuroshio axis with respect to the observational data of each experiment was calculated and compared (<xref ref-type="fig" rid="f9">
<bold>Figure&#xa0;9</bold>
</xref>). The observation data that contributed the most to improving the Kuroshio axis were the pseudo-profiles derived from satellite altimetry data except in January and February. The system seems to become unstable in the beginning as the psudo-profiles from satellite altimetry have been newly assimilated. However, from March, EXP04 and EXP05 show better representation of the Kuroshio axis rather than other experiments. The SST data also contributed to improving the Kuroshio axis to some extent whereas the T/S profiles did not show a significant impact. EXP05, which assimilated all observations presented in this study, including KODC, reduced the RMSE for the latitude of the Kuroshio axis, except for March and the summer season, compared to EXP04, which assimilated all observations except KODC. <xref ref-type="table" rid="T5">
<bold>Table&#xa0;5</bold>
</xref> also confirms the contribution of the satellite altimetry and KODC profile data to the significant reduction in RMSE for latitude of the Kuroshio axis. These results suggest that regional ocean observation networks may improve the forecast skill of the ocean prediction system not only in the region but also in the open ocean, such as the Pacific Ocean.</p>
<fig id="f9" position="float">
<label>Figure&#xa0;9</label>
<caption>
<p>Monthly mean RMSEs for the latitude of the Kuroshio axis with respect to the observation data of each experiment. Gray, black, violet, blue, green and red bars denote CTR and EXP01-05, respectively.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g009.tif"/>
</fig>
<table-wrap id="T5" position="float">
<label>Table&#xa0;5</label>
<caption>
<p>RMSE averaged in space and time for the latitude of the Kuroshio axis with respect to AVISO gridded data in each experiment.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left"/>
<th valign="middle" align="center">CTR</th>
<th valign="middle" align="center">EXP01</th>
<th valign="middle" align="center">EXP02</th>
<th valign="middle" align="center">EXP03</th>
<th valign="middle" align="center">EXP04</th>
<th valign="middle" align="center">EXP05</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">
<bold>RMSE (IOA)</bold>
</td>
<td valign="middle" align="center">3.40</td>
<td valign="middle" align="center">3.06 (10.00%)</td>
<td valign="middle" align="center">3.30 (3.03%)</td>
<td valign="middle" align="center">3.14 (8.28%)</td>
<td valign="middle" align="center">2.28 (49.12%)</td>
<td valign="middle" align="center">2.18 (55.96%)</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>The number in the parentheses below RMSE represents IOA.</p>
<p>RMSE, root-mean-square error; IOA, impact of assimilation. CTR, control; EXP, experiment.</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
</sec>
<sec id="s4" sec-type="discussion">
<label>4</label>
<title>Discussion</title>
<p>In this study, sensitivity experiments were conducted to evaluate the impacts of <italic>in-situ</italic> T/S profiles and satellite observation data, including SST and altimetry data, on a high-resolution ocean circulation prediction system, so called the KOOS-OPEM. KOOS-OPEM adopts localized EnOI to assimilate the ocean observation data into the model. The satellite altimetry information was projected into the subsurface layer following CH96 which did not directly assimilate the altimetry but rather pseudo temperature and salinity profiles. The contribution of each observation data was evaluated as follows: IOA of EXP01 for SST data; average of IOA differences of EXP02 and EXP03 with respect to EXP01 for <italic>in-situ</italic> T/S profile data; average of IOA differences between EXP02 and EXP03, and between EXP04 and EXP05 for KODC data; average of IOA differences between EXP02 and EXP04, and between EXP03 and EXP05 for altimetry data.</p>
<p>The comparisons of model experiments suggest that the satellite SST data set has the most contribution (EXP01, 23.77%) to the modeled SST improvement in terms of the RMSE compared to the CTR. Especially, the largest improvement was found in the K-KE region (32.65%). Additionally, assimilating the <italic>in-situ</italic> profiles insignificant impact on the modeled SST performance (EXP02), while the <italic>in-situ</italic> profiles have the greatest influence on the vertical structure of temperature (average 10.26%) and salinity (average 7.50%), especially in the EJS (EXP02 and EXP03). The altimetry assimilation (EXP04 and EXP05) also contributes to improving the subsurface vertical profile structure of ocean temperature (average 12.33%) and salinity (average 10.00%), especially in the K-KE region. It is highlighted that the <italic>in-situ</italic> profiles in the Korean marginal seas provided by KODC have significant impact on the vertical structure of ocean temperature and salinity in not only the EJS but also the K-KE region (EXP03 and EXP05).</p>
<p>The assimilation of SST had a negative effect on both temperature and salinity in the subsurface layer in most areas (<xref ref-type="fig" rid="f5">
<bold>Figures&#xa0;5</bold>
</xref>, <xref ref-type="fig" rid="f6">
<bold>6</bold>
</xref>). In the OYC region, moreover, the SST assimilation seems to increase the RMSE of the temperature around 50&#xa0;m depth, where the background error variance has a maximum (not shown here). Indeed, it has been observed that the model overestimates the variability of the temperature more than the observation around 50&#xa0;m depth in the OYC region. The background error covariance calculated from the historical simulation may induce the temperature degradation in this region. In addition, the number of <italic>in-situ</italic> T/S profiles is not sufficient and the contribution of SSH seems to be limited in this region. To resolve the temperature degradation in the OYC region, it is necessary to add a new dataset or improve the model performance, which is left for the next study.</p>
<p>
<italic>In-situ</italic> T/S profile data assimilation was effective in most regions, and pseudo-profile data also substantially contributed to improving both temperature and salinity vertical structures as effectively as the <italic>in-situ</italic> T/S profile data. However, the contribution of pseudo-profiles at high latitudes was lower than at low- and middle-latitudes. In high latitude oceans, where stratification is weak, small changes in surface height are assimilated into large vertical displacements of the water column, which can rather lead to errors (<xref ref-type="bibr" rid="B12">Fox et&#xa0;al., 2000</xref>). Therefore, when using the altimetry assimilation method based on CH96, it is necessary to introduce latitude dependency (<xref ref-type="bibr" rid="B40">Vidard et&#xa0;al., 2009</xref>) for the next version. As mentioned above, KODC data improved the temperature in the subsurface layer not only in the East Sea but also in the K-KE region; when assimilation was performed using KODC data and pseudo-profiles, the salinity of the subsurface layer improved. Moreover, the assimilation of KODC data affected a large area (from 120&#xb0;E to 160&#xb0;E and 35&#xb0;N to 45&#xb0;N). Each observation also contributed to the improvement in the Kuroshio axis. When compared qualitatively, the pseudo-profiles derived from satellite altimetry data constrained mesoscale features, such as meander and eddy that were excessively simulated. When compared quantitatively (<xref ref-type="table" rid="T5">
<bold>Table&#xa0;5</bold>
</xref>), the pseudo-profiles were the main contributors to the reduction in the RMSE for the latitude of the Kuroshio axis with respect to the AVISO gridded data by an average of 46.89%. SST satellite data also made the second largest contribution, improving the Kuroshio axis by 10.00%. The KODC data also improved the Kuroshio axis by 6.84% when assimilated with the pseudo-profiles.</p>
<p>This study suggests the quantitative impacts of each observation data sets for improvement of the high-resolution ocean prediction system. Notably, pseudo-profiles derived from satellite altimetry data significantly contributed to the ocean analysis field by improving the vertical structure of temperature and salinity. Especially, we clearly showed that the assimilation of the regional ocean observation provided by the Korean regional observation network has non-negligible impacts on the upper layer structure in the open ocean and the representation of the Kuroshio axis. These results highlight the role of regional ocean observation networks in ocean prediction systems to improve the analysis and forecast skills in the open ocean as well as in the region. In particular, it is interesting that data assimilation of the KODC data obtained around Korea peninsula contributes to the improvement of representation of the Kuroshio axis. <xref ref-type="fig" rid="f10">
<bold>Figures&#xa0;10A-D</bold>
</xref> show the upper ocean structures of temperature and current speed between EXP04 and EXP05, respectively, in October. It is noteworthy that the differences in temperature and current between EXP04 and EXP05 was pronounced in the EJS, east of the Tsugaru strait and Kuroshio downstream region rather than in the Kuroshio upstream region. In EXP05, compared to EXP04, the warm water from the Tsugaru Strait extended to the east, and the cold water from the Okhotsk Sea and the Subarctic Pacific was extended to the south. <xref ref-type="bibr" rid="B20">Itoh et&#xa0;al. (2022)</xref> analyzed high-resolution observation data and reported that a sharp front often develops in the Sanriku confluence where Tsugaru Warm Current, Oyasio Current, and Kuroshio Current meet. EXP05 may better simulate the representation of the front in the Sanriku confluence by improving the physical properties of the Tsugaru Warm current through the assimilation of KODC data taken around Korean Peninsula. In addition, the better representation of the front may help the Oyashio Current extend to the south where the Kuroshio Current separate from the coast, which affects the fluctuations of the Kuroshio axis. In fact, the IOA from the temperature profiles for EXP04 and EXP05 (<xref ref-type="fig" rid="f10">
<bold>Figures&#xa0;10E, F</bold>
</xref>) shows that the KODC profiles contribute to improving the vertical temperature structure not only around the Korean Peninsula but also in the west of the Tsugaru strait and in the Sanriku confluence. Although the dynamic relationship between the circulation of the Korea marginal seas and Kuroshio was not fully understood in this study, it seems worthwhile for future research. This study also suggests that greater attention should be paid to the role of regional ocean observation networks to improve the forecast skill of the ocean prediction system not only in the region but also in the open ocean, such as the Pacific Ocean.</p>
<fig id="f10" position="float">
<label>Figure&#xa0;10</label>
<caption>
<p>Monthly mean temperature (upper panels), current speed (middle panels) averaged over 0 to 100m, and IOA (lower panels) for the temperature profiles over 0 to 100m in EXP04 (left panels) and EXP05 (right panels) in October.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1085542-g010.tif"/>
</fig>
</sec>
<sec id="s5" sec-type="data-availability">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material, Further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s6" sec-type="author-contributions">
<title>Author contributions</title>
<p>IC and YK: conducting the experiment and writing the first manuscript. IC: carrying out experiment and visualization. YK: supervision. YK, HJ and GP: deriving additional analysis ideas. YK, HJ, GP, Y-GP and Y-SC: review and editing. All authors contributed to the article and approved the submitted version.</p>
</sec>
</body>
<back>
<sec id="s7" sec-type="funding-information">
<title>Funding</title>
<p>This research was part of projects titled &#x2018;Investigation and prediction system development of marine heatwave around the Korean Peninsula originated from the subarctic and western Pacific&#x2019; (20190344) and &#x2018;Improvements of ocean prediction accuracy using numerical modeling and artificial intelligence technology&#x2019; (20180447) funded by the Ministry of Oceans and Fisheries, Korea. This work was supported by Korea Institute of Marine Science and Technology Promotion(KIMST) funded by the Ministry of Oceans and Fisheries, Korea (Development of 3-D Ocean Current Observation Technology for Efficient Response to Maritime Distress, 20210642). YK was supported by by the Pukyong National University Research Fund (CD20191541).</p>
</sec>
<ack>
<title>Acknowledgments</title>
<p>We would like to thank Gary Brassington for his valuable discussions and comments.</p>
</ack>
<sec id="s8" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s9" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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