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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.2021.729954</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>Deep Learning for Simulating Harmful Algal Blooms Using Ocean Numerical Model</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Baek</surname> <given-names>Sang-Soo</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Pyo</surname> <given-names>JongCheol</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Kwon</surname> <given-names>Yong Sung</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1383793/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Chun</surname> <given-names>Seong-Jun</given-names></name>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Baek</surname> <given-names>Seung Ho</given-names></name>
<xref ref-type="aff" rid="aff5"><sup>5</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Ahn</surname> <given-names>Chi-Yong</given-names></name>
<xref ref-type="aff" rid="aff6"><sup>6</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/673913/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Oh</surname> <given-names>Hee-Mock</given-names></name>
<xref ref-type="aff" rid="aff6"><sup>6</sup></xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Kim</surname> <given-names>Young Ok</given-names></name>
<xref ref-type="aff" rid="aff7"><sup>7</sup></xref>
<xref ref-type="corresp" rid="c002"><sup>&#x002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1311954/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Cho</surname> <given-names>Kyung Hwa</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/266756/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>School of Urban and Environmental Engineering, Ulsan National Institute of Science and Technology</institution>, <addr-line>Ulsan</addr-line>, <country>South Korea</country></aff>
<aff id="aff2"><sup>2</sup><institution>Center for Environmental Data Strategy, Korea Environment Institute</institution>, <addr-line>Sejong</addr-line>, <country>South Korea</country></aff>
<aff id="aff3"><sup>3</sup><institution>Environmental Impact Assessment Team, Division of Ecological Assessment Research, National Institute of Ecology</institution>, <addr-line>Seocheon</addr-line>, <country>South Korea</country></aff>
<aff id="aff4"><sup>4</sup><institution>LMO Research Team, Bureau of Ecological Research, National Institute of Ecology (NIE)</institution>, <addr-line>Seocheon</addr-line>, <country>South Korea</country></aff>
<aff id="aff5"><sup>5</sup><institution>Risk Assessment Research Center, Korea Institute of Ocean Science &#x0026; Technology</institution>, <addr-line>Geoje</addr-line>, <country>South Korea</country></aff>
<aff id="aff6"><sup>6</sup><institution>Cell Factory Research Center, Korea Research Institute of Bioscience and Biotechnology (KRIBB)</institution>, <addr-line>Daejeon</addr-line>, <country>South Korea</country></aff>
<aff id="aff7"><sup>7</sup><institution>Marine Ecosystem Research Center, Korea Institute of Ocean Science and Technology</institution>, <addr-line>Busan</addr-line>, <country>South Korea</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Kenneth Mei Yee Leung, City University of Hong Kong, Hong Kong SAR, China</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Yongquan Yuan, Institute of Oceanology, Chinese Academy of Sciences (CAS), China; Hai Doan-Nhu, Institute of Oceanography in Nhatrang, Vietnam</p></fn>
<corresp id="c001">&#x002A;Correspondence: Kyung Hwa Cho, <email>khcho@unist.ac.kr</email></corresp>
<corresp id="c002">Young Ok Kim, <email>yokim@kiost.ac.kr</email></corresp>
<fn fn-type="other" id="fn004"><p>This article was submitted to Marine Pollution, a section of the journal Frontiers in Marine Science</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>12</day>
<month>10</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>8</volume>
<elocation-id>729954</elocation-id>
<history>
<date date-type="received">
<day>24</day>
<month>06</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>15</day>
<month>09</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2021 Baek, Pyo, Kwon, Chun, Baek, Ahn, Oh, Kim and Cho.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Baek, Pyo, Kwon, Chun, Baek, Ahn, Oh, Kim and Cho</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>In several countries, the public health and fishery industries have suffered from harmful algal blooms (HABs) that have escalated to become a global issue. Though computational modeling offers an effective means to understand and mitigate the adverse effects of HABs, it is challenging to design models that adequately reflect the complexity of HAB dynamics. This paper presents a method involving the application of deep learning to an ocean model for simulating blooms of <italic>Alexandrium catenella</italic>. The classification and regression convolutional neural network (CNN) models are used for simulating the blooms. The classification CNN determines the bloom initiation while the regression CNN estimates the bloom density. GoogleNet and Resnet 101 are identified as the best structures for the classification and regression CNNs, respectively. The corresponding accuracy and root means square error values are determined as 96.8% and 1.20 [log(cells L<sup>&#x2013;1</sup>)], respectively. The results obtained in this study reveal the simulated distribution to follow the <italic>Alexandrium catenella</italic> bloom. Moreover, Grad-CAM identifies that the salinity and temperature contributed to the initiation of the bloom whereas NH<sub>4</sub>-N influenced the growth of the bloom.</p>
</abstract>
<kwd-group>
<kwd>harmful algal blooms</kwd>
<kwd>deep learning</kwd>
<kwd>convolutional neural network</kwd>
<kwd>classification</kwd>
<kwd>regression</kwd>
</kwd-group>
<contract-sponsor id="cn001">Ministry of Science, ICT and Future Planning<named-content content-type="fundref-id">10.13039/501100003621</named-content></contract-sponsor>
<contract-sponsor id="cn002">Korea Institute of Ocean Science and Technology<named-content content-type="fundref-id">10.13039/501100007049</named-content></contract-sponsor>
<counts>
<fig-count count="6"/>
<table-count count="1"/>
<equation-count count="0"/>
<ref-count count="79"/>
<page-count count="13"/>
<word-count count="10295"/>
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</article-meta>
</front>
<body>
<sec sec-type="intro" id="S1">
<title>Introduction</title>
<p>The occurrence, period, and frequency of harmful algal blooms (HABs) have increased in recent years, thereby posing a serious threat to the aquatic ecosystem (<xref ref-type="bibr" rid="B75">Weiher and Sen, 2006</xref>; <xref ref-type="bibr" rid="B26">Gobler et al., 2017</xref>). The United States spends &#x0024;22 million annually on public-health damages and suffers an annual loss of &#x0024;75 million due to HABs (<xref ref-type="bibr" rid="B33">Hoagland et al., 2002</xref>; <xref ref-type="bibr" rid="B75">Weiher and Sen, 2006</xref>; <xref ref-type="bibr" rid="B2">Anderson et al., 2012</xref>). In South Korea, the economic loss incurred due to HAB over the past three decades was &#x0024;121 million (<xref ref-type="bibr" rid="B57">Park et al., 2013</xref>). China and Japan have similarly incurred enormous economic losses in northeast Asia (<xref ref-type="bibr" rid="B73">Wang and Wu, 2009</xref>; <xref ref-type="bibr" rid="B36">Itakura and Imai, 2014</xref>). These damages can be attributed to the changes in the aquatic environmental conditions due to climate change and/or nutrient enrichment caused by such human activities as agriculture, industrialization, tourism, and urbanization (<xref ref-type="bibr" rid="B31">Heisler et al., 2008</xref>; <xref ref-type="bibr" rid="B26">Gobler et al., 2017</xref>). Accordingly, HABs have escalated to become a global concern. Anthropogenic global warming is visible in the northward expansion of the warm pool to the northwestern Pacific. The Korean Peninsula, which is closed on the marginal sea of the northwestern Pacific, has been reported as a vulnerable region in the new normal climate. Accordingly, there exists the threat of HAB expansion into the Korean coastal waters owing to changes in HAB dynamics due to global warming. Outbreaks of PSP in Korean coastal waters have been perceived as spring events since the first record in 1986 (<xref ref-type="bibr" rid="B10">Chang et al., 1987</xref>). Recurrent PSP events in the spring of Korea have been linked to the spring blooms of <italic>Alexandrium catenella</italic> (<italic>A. catenella</italic>) (previously reported as <italic>A. tamarense</italic>). The spring blooms of the toxic dinoflagellate population are regular in the coastal waters of marginal sea connected to the northwestern Pacific (<xref ref-type="bibr" rid="B27">Han et al., 1992</xref>; <xref ref-type="bibr" rid="B35">Ishikawa et al., 2014</xref>).</p>
<p>Prior research concerning HABs has mainly focused on increasing awareness and improving monitoring techniques (<xref ref-type="bibr" rid="B43">Kim et al., 2002</xref>; <xref ref-type="bibr" rid="B74">Wang et al., 2008</xref>). Since the 1970s, a significant amount of infrastructure, labor, and time has been required for HAB field monitoring. However, the extent of this requirement has differed based on the properties of HAB. Moreover, given the need for HAB monitoring and relevant analyses, computational modeling has been considered to be an alternative approach to understand and mitigate the effects of HABs (<xref ref-type="bibr" rid="B78">Yoshioka and Yaegashi, 2018</xref>; <xref ref-type="bibr" rid="B60">Pyo et al., 2019</xref>). <xref ref-type="bibr" rid="B59">Pinto et al. (2016)</xref> simulated the abundance of HAB species using a particle-tracking model. Likewise, <xref ref-type="bibr" rid="B30">He et al. (2008)</xref> developed a mathematical model for simulating <italic>A. catenella</italic> (former <italic>A. fundyense</italic>) bloom in the western Gulf of Maine. Although these efforts have contributed toward the improvement of the simulation performance of algal blooms, overcoming the limitations of these models remains a major challenge owing to the complexity of HAB dynamics that are dependent on the multiple effects from physical, chemical, and biological systems (<xref ref-type="bibr" rid="B50">McGillicuddy, 2010</xref>).</p>
<p>A data-driven deep-learning model can push the frontiers of the aforementioned models further. Deep learning has been proposed as a promising technique owing to its big-data handling capabilities (<xref ref-type="bibr" rid="B71">Szegedy et al., 2015</xref>). Deep learning has been adopted in several fields, including speech recognition, image analysis, and biological mechanisms (<xref ref-type="bibr" rid="B12">Chen and Manning, 2014</xref>; <xref ref-type="bibr" rid="B79">Young et al., 2018</xref>). <xref ref-type="bibr" rid="B67">Shen et al. (2019)</xref> estimated cyanobacteria blooms in river waters using a support vector machine. Additionally, <xref ref-type="bibr" rid="B61">Pyo et al. (2020)</xref> simulated algal blooms in freshwater systems using a convolutional neural network (CNN). However, these studies focused on HABs in inland waters, which further access is necessary to undergo more dynamic and complex hydrological and ecological cycles in seawater. Recently, <xref ref-type="bibr" rid="B6">Baek et al. (2021)</xref> suggested a method for identifying factors that influence <italic>A. catenella</italic> bloom using decision tree and hydrodynamic models. They revealed that water temperature and nutrients affected the growth of <italic>A. catenella</italic>. However, this approach is not suitable for continuous <italic>A. catenella</italic> bloom simulation because it can only generate four bloom levels based on cell density.</p>
<p>This study evaluates the applicability of deep learning for HAB simulation with the ocean model to generate the temporal&#x2013;spatial distribution of physical, chemical, and biological variables. Using these variables and CNNs, we simulated the temporal distribution of <italic>A. catenella</italic>, a notorious dinoflagellate species causing paralytic shellfish poisoning (PSP). Convolutional neural network-based deep learning models can extract the features of multi-dimensional data using convolutional filters (<xref ref-type="bibr" rid="B21">Deng et al., 2009</xref>). Additionally, using gradient-weighted class activation mapping (Grad-CAM), we identified the factors that influence the simulation of <italic>A. catenella</italic> (<xref ref-type="bibr" rid="B65">Selvaraju et al., 2017</xref>).</p>
</sec>
<sec id="S2" sec-type="materials|methods">
<title>Materials and Methods</title>
<sec id="S2.SS1">
<title>Data Collection</title>
<p>We conducted spatial&#x2013;temporal monitoring to investigate the occurrence of <italic>A. catenella</italic>. The monitoring site is located on the southeastern coast near Namhae, Geoje Island, and Busan, South Korea (<xref ref-type="fig" rid="F1">Figure 1</xref>), opened toward off sea, causing fresh and oceanic water intrusion (<xref ref-type="bibr" rid="B39">Kang et al., 2012</xref>). In particular, the eastern coast of Geoje Island has frequently occurring PSP initiation (<xref ref-type="bibr" rid="B55">National Fisheries Research and Development Institute, 2020</xref>). PSP outbreaks provoked by <italic>A. catenella</italic> bloom in our study area have been reported (<xref ref-type="bibr" rid="B10">Chang et al., 1987</xref>; <xref ref-type="bibr" rid="B44">Kim et al., 2015</xref>). Water surface elevation, wind, and wind velocity data were measured by the Korea Ocean Observing and Forecasting System and used to set up the model. Two observations at stations 1 and 2 were used to calibrate the water level, temperature, and salinity. Another three observations at stations 3, 4, and 5 were used to calibrate NH4-N and PO4-P (<xref ref-type="fig" rid="F1">Figure 1</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption><p>Study site&#x2014;red dots indicate the observation station for water elevation, salinity, and temperature; blue dots indicate the observation point for NH<sub>4</sub>-N and PO<sub>4</sub>-P; yellow circles indicates the monitoring point for <italic>A. catenella</italic>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-08-729954-g001.tif"/>
</fig>
<p>One-thousand one-hundred and seventy-five samples were collected from the water surface at the sampling sites, which had water depths of 12 to 59 m. The monitoring period was from January 2017 to December 2019. Water samples were acquired with a Van Dorn bottle and fixed with Lugol solution (final conc., 2%) from 9:00 AM to 4:00 PM. The fixed seawater was concentrated to 5&#x2013;50 mL aliquots by overnight sedimentation. <italic>Alexandrium catenella</italic> cells were enumerated using a Sedgwick&#x2013;Rafter counting slide at a 200&#x00D7; magnification with a light microscope (Zeiss Axioscope 2). To identify the species based on morphological and molecular analyses, the cells were processed as described by <xref ref-type="bibr" rid="B42">Kim et al. (2020)</xref>. Cysts of <italic>A. catenella</italic> were isolated from sediment samples collected using a core sampler and incubated at bottom temperatures on the sampling dates. The germination ratio of the cysts was estimated by the percentage of cysts germinating within one month. Growth experiments of <italic>A. catenella</italic> were conducted under several temperature and salinity conditions, reflecting the sampling site environments. The measurements of germination ratio and growth rate were described in detail by <xref ref-type="bibr" rid="B42">Kim et al. (2020)</xref>.</p>
</sec>
<sec id="S2.SS2">
<title>Preparation of Input Data for Deep Learning</title>
<p>The input data in this study consisted of two parts: (1) ocean physical data (e.g., water velocity, water temperature, water elevation, and retention time) and chemical data (e.g., salinity, PO<sub>4</sub>-P, and NH<sub>4</sub>-N) and (2) ocean biological data [e.g., germination ratio, growth rate, and operational taxonomic unit (OTU)]. This study applied the environmental fluid dynamics code (EFDC) model, adopted for simulating ocean and coastal waters (<xref ref-type="bibr" rid="B20">Dai et al., 2011</xref>; <xref ref-type="bibr" rid="B22">Du and Shen, 2016</xref>) to generate the ocean physical and chemical data. The EFDC model is a fluid simulation model that includes three-dimensional flow and biochemical transport in the ocean, estuaries, and lakes. EFDC can solve free surface, vertical hydrostatic, and turbulent equations for fluids with different densities. The governing equation was derived using the vertical hydrostatic boundary with turbulent equations and consists of the momentum [Eq. (S1, S2)], vertical hydrostatic pressure (Eq. S3), and continuity equations [Eq. (S4, S5)] (<xref ref-type="bibr" rid="B38">Jeong et al., 2010</xref>). The ocean physical and chemical data included the temporal and spatial distributions of water velocity, water temperature, water elevation, retention time, salinity, PO<sub>4</sub>-P, and NH<sub>4</sub>-N. These data have been verified as variables that influence the life cycle of <italic>A. catenella</italic> (<xref ref-type="bibr" rid="B37">Itakura and Yamaguchi, 2001</xref>; <xref ref-type="bibr" rid="B41">Kim and Yoo, 2007</xref>; <xref ref-type="bibr" rid="B4">Armi et al., 2011</xref>; <xref ref-type="bibr" rid="B42">Kim et al., 2020</xref>). The ocean physical and chemical distributions were calculated by the EFDC model. Ocean biological data included the temporal and spatial distributions of the germination ratio of <italic>A. catenella</italic> cysts, growth rate of vegetative cells of the species, and OTU of bacteria. The cyst germination and growth rates are critical elements in recurrent outbreaks of <italic>A. catenella</italic> blooms <italic>in situ</italic>, although dormant populations are significantly affected by environmental variables. Hence, we adopted these rates as the input data to simulate <italic>A. catenella</italic>. The data pertaining to cyst germination and growth rate were obtained by <xref ref-type="bibr" rid="B42">Kim et al. (2020)</xref>. The microbial community data in this area, including the OTU data, were extracted from the previous study (<xref ref-type="bibr" rid="B19">Cui et al., 2020</xref>). operational taxonomic units were analyzed at a distance of 0.01 using the mothur v1.39.3 pipeline with SILVA database, release 132 (<xref ref-type="bibr" rid="B64">Schloss et al., 2009</xref>; <xref ref-type="bibr" rid="B46">Kozich et al., 2013</xref>). Three representative OTUs (OTU1, OTU2, and OTU3), which were identified as <italic>A. catenella</italic>-related OTUs based on ecological network analysis in the previous study (<xref ref-type="bibr" rid="B19">Cui et al., 2020</xref>), were selected for further analysis in this study. Taxonomically, OTU1, OTU2, and OTU3 were assigned to genera Fluviicola (family Crocinitomicaceae), Ascidiaceihabitans (family Rhodobacteraceae), Candidatus Actinomarina (family Candidatus Actinomarinaceae), respectively. <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref> presents the process used to generate the temporal and spatial distribution of biological data. A linear model was adopted to generate the variation of biological data by changing the environmental variables. The linear regressions of the germination ratio and growth rate were calculated using temperature and salinity from <italic>in vivo</italic> experiments (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1A</xref>), whereas that of the OTU distribution was generated using the temperature, salinity, PO<sub>4</sub>-P, and NH<sub>4</sub>-N values from monitoring (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1B</xref>). A linear regression model explains the relationship between one response variable and multiple explanatory variables (<xref ref-type="bibr" rid="B53">Montgomery et al., 2021</xref>); therefore, these linear models used the simulated water temperature, salinity, PO<sub>4</sub>-P, and NH<sub>4</sub>-N from EFDC to determine the temporal and spatial distribution of biological data (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1C</xref>). The simulation period was from January 2017 to December 2019. These ocean physical, chemical, and biological data were validated using observational data. The EFDC grid was a Cartesian grid with a cell size of 200 m &#x00D7; 400 m. Observations of wind direction, velocity and water surface elevation were used to set up the EFDC model. More details of the experiments on germination ratio, growth rate, and OTU are presented in the <xref ref-type="supplementary-material" rid="DS1">Supplementary Information</xref>.</p>
<p><xref ref-type="fig" rid="F2">Figure 2</xref> shows the two-step process of generating input data to apply CNN for simulating the bloom of <italic>A. catenella</italic>: (1) extracting the spatial&#x2013;temporal distribution of the physical, chemical, and biological information at the study site (<xref ref-type="fig" rid="F2">Figures 2A,B</xref>) and (2) converting the input data to two-dimensional data (<xref ref-type="fig" rid="F2">Figure 2C</xref>). These physical, chemical, and biological data have three dimensions, <italic>m</italic> &#x00D7; <italic>m</italic> &#x00D7; (<italic>n</italic> + 1), and the simulation point of <italic>A. catenella</italic> is located in the center. Here, <italic>m</italic> is the size (i.e., height &#x00D7; width) of the input window that includes the simulation point, and <italic>n</italic> is the lookback, which indicates the number of time steps included based on the current simulation time. For example, when <italic>m</italic> = 3 and <italic>n</italic> = 5, the data size is 3 &#x00D7; 3 &#x00D7; (5 + 1). Because the CNN approach was developed focusing on two-dimensional data (length &#x00D7; height) or RGB data (length &#x00D7; height &#x00D7; 3), we converted these inputs into two-dimensional data before applying the CNN (<xref ref-type="bibr" rid="B69">Shin et al., 2016</xref>; <xref ref-type="bibr" rid="B45">Koundinya et al., 2018</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption><p>Preparation of input data for CNN&#x2014;<bold>(A)</bold> physical and chemical data obtained using EFDC, <bold>(B)</bold> biological data obtained using EFDC and linear equation, and <bold>(C)</bold> two-dimensional input data. Here, <italic>m</italic> denotes the input window (i.e., height &#x00D7; width), including the simulation point located at the center of input window while <italic>n</italic> denotes the lookback size. Red boxes indicate the simulation point.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-08-729954-g002.tif"/>
</fig>
</sec>
<sec id="S2.SS3">
<title>Simulation of <italic>Alexandrium catenella</italic> Based on DL</title>
<p>The simulation layout of <italic>A. catenella</italic> is presented in <xref ref-type="fig" rid="F3">Figure 3</xref>. The simulation comprises of the following three steps: (1) optimizing the input and CNN structures, (2) simulating the bloom of <italic>A. catenella</italic> based on the optimal input and CNN structures, and (3) identifying <italic>A. catenella</italic> bloom factors based on Grad-CAM. Because these CNN structures (e.g., Resnet, GoogLeNet, and Inception) were developed using data of size 299 &#x00D7; 299, the input data had to be converted (<xref ref-type="bibr" rid="B72">Szegedy et al., 2016</xref>; <xref ref-type="bibr" rid="B1">Akiba et al., 2017</xref>). Subsequently, the converted data are fed to the classification and regression CNN models; the classification CNN model decided the initiation of <italic>A. catenella</italic>, while the regression CNN model generated the density after <italic>A. catenella</italic> was initiated. The initiation and the density indicated the occurrence and the number of <italic>A. catenella</italic> cells, respectively. The use of two CNNs with different roles can prevent bias in model training, as most of our monitoring data were zero, indicating that <italic>A. catenella</italic> did not occur. In addition, we optimized the input window (<italic>m</italic>), lookback (<italic>n</italic>), and CNN structures (<xref ref-type="fig" rid="F3">Figure 3A</xref>) to generate the spatial&#x2013;temporal distribution of <italic>A. catenella</italic> (<xref ref-type="fig" rid="F3">Figure 3B</xref>). Using the optimal parameter values and CNN structures, we analyzed the performance of <italic>A. catenella</italic> forecasting with increasing forecast lead times (days) of up to seven days. Model training was performed using Intel <sup>&#x00AE;</sup> Xeon CPU E-52687W v4 @ 3.00 GHz, 128 GB RAM, and NVIDIA GTX 1080 Ti. CNN was implemented with the machine and deep learning toolboxes in MATLAB. Accuracy was used for evaluating the classification CNN model, while RMSE and R<sup>2</sup> were used for the regression CNN model. Relevant explanations can be found in the <xref ref-type="supplementary-material" rid="DS1">Supplementary Information</xref>.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption><p>Procedure of simulating <italic>A. catenella</italic> using CNN&#x2014;<bold>(A)</bold> optimizing input data and CNN structures, <bold>(B)</bold> predicting bloom of <italic>A. catenella</italic> based on optimal input and structures, and <bold>(C)</bold> identifying factors for bloom of <italic>A. catenella</italic> using Grad-CAM. Brown and blue lines indicate the processes of classification and regression CNN models, respectively.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-08-729954-g003.tif"/>
</fig>
</sec>
<sec id="S2.SS4">
<title>Convolutional Neural Network</title>
<p>Convolutional Neural Network (CNN) is a popular deep learning model that extracts data features using convolving filters (<xref ref-type="bibr" rid="B21">Deng et al., 2009</xref>). A typical CNN architecture consists of convolutional, pooling, ReLU, batch normalization, concatenation, normalized, and fully connected layers (<xref ref-type="bibr" rid="B47">LeCun et al., 2015</xref>). Each layer has a specialized role in the architecture: convolutional and pooling layers are used for feature extraction. ReLU and normalization layers are used for a linear and normalization calculation, respectively (<xref ref-type="bibr" rid="B47">LeCun et al., 2015</xref>). These layers can be combined to enhance model performance (<xref ref-type="bibr" rid="B72">Szegedy et al., 2016</xref>; <xref ref-type="bibr" rid="B40">Khan et al., 2019</xref>). Details concerning the CNN layers can be found in the <xref ref-type="supplementary-material" rid="DS1">Supplementary Materials</xref> document. <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 2</xref> shows the CNN structures employed in this study. GoogleNet and Inception v3 models adopt parallel CNN layers (<xref ref-type="bibr" rid="B72">Szegedy et al., 2016</xref>). ResNet 50 and ResNet 101 have skip connections, i.e., the information of the output layer is transferred into the next layer, and into the earlier layer (<xref ref-type="bibr" rid="B72">Szegedy et al., 2016</xref>). This structure can increase model performance by reducing overfitting and vanishing gradient problems (<xref ref-type="bibr" rid="B28">He et al., 2016a</xref>). In our study, the softmax and mean squared error (MSE) (see <xref ref-type="supplementary-material" rid="DS1">Supplementary Information</xref> for more details) were used as the loss function for classification and regression CNN, respectively. The loss functions were applied for calculating the error between simulation and observation during model training. For model training, the CNN used hyperparameters, including epoch number, batch size, and learning rate (<xref ref-type="bibr" rid="B48">Loussaief and Abdelkrim, 2018</xref>). Epoch is the number of times the learning worked in the entire dataset, whereas batch size is the number of samples used for training (<xref ref-type="bibr" rid="B63">Robert, 2014</xref>). The learning rate controls the step size at each iteration to minimize the loss function (<xref ref-type="bibr" rid="B63">Robert, 2014</xref>). The CNN comprised 500 epochs with a mini-batch size of 32; the applied learning rates equaled 0.001 and 0.0001 for the first 200 and remaining 300 epochs, respectively. Each epoch generated a corresponding model, and the final model was selected to produce the lowest validation accuracy and MSE. Our study adopted random sampling to divide <italic>A. catenella</italic> observations into training and validation sets. A uniform distribution was used for the random sampling. Previous studies have also used random sampling with a uniform distribution to divide the data into training and validation sets (<xref ref-type="bibr" rid="B8">Brion et al., 2002</xref>; <xref ref-type="bibr" rid="B9">Caruana and Niculescu-Mizil, 2006</xref>).</p>
</sec>
<sec id="S2.SS5">
<title>Gradient-Weighted Class-Activation Mapping</title>
<p>The deep-learning model used in this study applied Grad-CAM for identifying factors contributing to <italic>A. catenella</italic> bloom (<xref ref-type="fig" rid="F3">Figure 3C</xref>). The Grad-CAM localization map describes the simulation results by highlighting the important regions (<xref ref-type="bibr" rid="B65">Selvaraju et al., 2017</xref>). The model interpretability technique is proposed as a strategy that enables the input-based understanding of the results obtained because neural networks are incapable of explaining model results (<xref ref-type="bibr" rid="B65">Selvaraju et al., 2017</xref>). Several prior studies have verified the use of Grad-CAM in the visualization of model features (<xref ref-type="bibr" rid="B65">Selvaraju et al., 2017</xref>; <xref ref-type="bibr" rid="B13">Chen et al., 2020</xref>). This method is based on class activation mapping (CAM) that can extract the significant features by emphasizing the input data region. However, the use of CAM is restricted to CNN structures that comprise a global average pooling layer (<xref ref-type="bibr" rid="B66">Selvaraju et al., 2016</xref>). Grad-CAM overcomes this limitation using gradient information from the final convolutional layer for visualizing the important input data regions (<xref ref-type="bibr" rid="B65">Selvaraju et al., 2017</xref>). A detailed description of Grad-CAM is presented by <xref ref-type="bibr" rid="B65">Selvaraju et al. (2017)</xref>.</p>
</sec>
</sec>
<sec sec-type="results" id="S3">
<title>Results</title>
<sec id="S3.SS1">
<title>Ocean Modeling Results</title>
<p>We compared the simulated and observed water elevation, salinity, water temperature, NH<sub>4</sub>-N, and PO<sub>4</sub>-P results. The physical and chemical simulations are illustrated in <xref ref-type="supplementary-material" rid="DS1">Supplementary Figures 3</xref>, <xref ref-type="supplementary-material" rid="DS1">4</xref>. The coefficient of determination (R<sup>2</sup>) of water temperature and elevation was above 0.90 at stations 1 and 2, while salinity was 0.26 and 0.65 at stations 1 and 2, respectively. The average root-mean-squared errors (RMSEs) of water temperature, elevation, and salinity were 0.82&#x00B0;C, 0.07 m, and 1.12, respectively. Compared to water temperature and elevation simulations, the salinity simulation had a larger error than observation. The average coefficient of determination (R<sup>2</sup>) of NH<sub>4</sub>-N and PO<sub>4</sub>-P were 0.67 and 0.30, and the average RMSE values were 0.09 and 0.01 mg L<sup>&#x2013;1</sup>, respectively. Although both NH<sub>4</sub>-N and PO<sub>4</sub>-P simulations follow the observation trend, their values were underestimated at the peak point. The linear regression equations of growth rate, germination rate, and OTU are presented in <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 5</xref>. The growth and germination rates were more strongly influenced by temperature and salinity, respectively, whereas the OTUs related to <italic>A. catenella</italic> were affected by salinity and PO<sub>4</sub>-P.</p>
</sec>
<sec id="S3.SS2">
<title>Optimal Input Window Design</title>
<p><xref ref-type="fig" rid="F4">Figures 4</xref>(A.1-4,B.1-4) shows the performance of classification and regression CNN, respectively, with respect to input window size (<italic>m</italic>) and lookback (<italic>n</italic>). Here, <italic>m</italic> denotes the input window size (e.g., height &#x00D7; width), including the simulation point that was located at the center of the input window, and <italic>n</italic> is the number of time steps. For example, if the input window size is three and lookback is five, the model considers a spatial distribution with 3 &#x00D7; 3 grid cells and temporal information from the previous five days to the current simulation time. In the classification model, except GoogleNet, there existed multiple optimal designs (<italic>m</italic>, <italic>n</italic>) in each structure; GoogleNet had an optimal design structure of (3, 30). The model performance of other structures deteriorated when <italic>m</italic> was above five and <italic>n</italic> was below fifteen (days). In the regression model, Resnet 50 and Resnet 101 had a similar optimal design of (1, 29), while GoogleNet and Inception v3 required different (m, n) designs; the optimal design of GoogleNet was (1, 2) and that of Inception v3 was (1, 27).</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption><p>Optimal input and simulation results of <italic>A. catenella</italic>&#x2014;<bold>(A)</bold> optimal input (<italic>m</italic> and <italic>n</italic>) of classification CNN structures: <bold>(A.1)</bold> Resnet 50, <bold>(A.2)</bold> Resnet 101, <bold>(A.3)</bold> GoogleNet, and <bold>(A.4)</bold> Inception v3; <bold>(B)</bold> optimal input (<italic>m</italic> and <italic>n</italic>) of regression CNN structures: <bold>(B.1)</bold> Resnet 50, <bold>(B.2)</bold> Resnet 101, <bold>(B.3)</bold> GoogleNet, and <bold>(B.4)</bold> Inception v3; <bold>(C)</bold> simulated and observed densities of <italic>A. catenella</italic> with regression CNN structures [e.g., <bold>(C.1)</bold> Resnet 50, <bold>(C.2)</bold> Resnet 101, <bold>(C.3)</bold> GoogleNet, and <bold>(C.4)</bold> Inception v3] with optimal input. In <bold>(A)</bold> and <bold>(B)</bold>, <italic>m</italic> and <italic>n</italic> denote the input window (i.e., height &#x00D7; width) and lookback sizes, respectively, whereas the color range indicates the accuracy from the lowest (blue) to the highest (red) values. In <bold>(C)</bold>, the red and blue circles indicate the training and validation sets, respectively. The observed line has a slope of 1:1.</p></caption>
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</fig>
</sec>
<sec id="S3.SS3">
<title>Simulation of <italic>Alexandrium catenella</italic></title>
<p>The model performance with optimal input design is summarized in <xref ref-type="table" rid="T1">Table 1</xref>. Among them, GoogleNet and Resnet 101 offer the best classification performance with an accuracy of 96.83% and RMSE of 1.20 [log(cells L<sup>&#x2013;1</sup>)], respectively. The model performance of Resnet 50 was similar to Resnet 101 with accuracy and RMSE of 96.29% and 1.29 [log(cells L<sup>&#x2013;1</sup>)], respectively. Inception v3 (accuracy of 95.76%) and GoogleNet [RMSE of 1.66 log(cells L<sup>&#x2013;1</sup>)] presented the worst performance in classification (with 95.76% accuracy) and regression models, respectively.</p>
<table-wrap position="float" id="T1">
<label>TABLE 1</label>
<caption><p>Model performance and optimal inputs (<italic>m</italic> and <italic>n</italic>).</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<tbody>
<tr>
<td valign="top" align="left"><inline-graphic xlink:href="fmars-08-729954-t001.jpg"/></td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn><p><italic>Yellow indicates the optimum structure; &#x002A; indicates that existence of multiple optimum designs.</italic></p></fn>
</table-wrap-foot>
</table-wrap>
<p>The results of the regression CNN model are plotted against observed <italic>A. catenella</italic> in <xref ref-type="fig" rid="F4">Figures 4C.1-4</xref>. In Resnet 101, the simulated <italic>A. catenella</italic> showed good agreement with observations. GoogleNet showed that the simulated <italic>A. catenella</italic> was overestimated in the low-density cells and underestimated in the high-density cells. The temporal-spatial distribution of <italic>A. catenella</italic> is presented with observation using GoogleNet and ResNet 101 because these structures showed the best performance in classification and regression CNN (<xref ref-type="fig" rid="F5">Figure 5A</xref>). The simulated distribution substantially followed actual <italic>A. catenella</italic> blooms. On December 17, 2016, and May 23, 2017, most areas did not provoke <italic>A. catenella</italic> bloom in both simulated and observed distribution, indicating that our model can simulate this phenomenon. On March 27, 2018, <italic>A. catenella</italic> blooms were observed in the coastal water. During this period, the simulated distribution of blooms can describe the actual spatial features; the eastern coast presented a relatively higher density than the western one. The data on March 28 and April 25 of 2017 shows increasing <italic>A. catenella</italic> spring bloom in the study area. The simulated distribution in both periods was in line with the actual distribution; the model generated high-density cells in the eastern coast and non-bloom near Geoje Island of the west coast. On August 19, 2019, the model determined the non-bloom and substantially low density on the western coast. Mismatched results of the spatial distributions are revealed in three spaces without observed data; the channel connected to the northern enclosed bay on May 23, 2017, the western off sea on March 28, 2017, and the enclosed bay on August 19, 2019. <xref ref-type="fig" rid="F5">Figure 5B</xref> shows the performance of <italic>A. catenella</italic> forecasting with various lead times. All forecast results were found to be worse than those of nowcasting. The average accuracy of the classification model was 95.85% for a lead of up to five days, decreasing sharply thereafter. The average RMSE of the regression model was 1.36 [log(cells L<sup>&#x2013;1</sup>)] until five forecast lead (days) and increased sharply thereafter.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption><p>Spatial distribution of <italic>A. catenella</italic> and forecast performance with lead time&#x2014;<bold>(A)</bold> spatial distribution of <italic>A. catenella</italic> on December 17, 2016, March 28, 2017, April 25, 2017, May 23, 2017, March 27, 2018, and August 19, 2019; <bold>(B)</bold> <italic>A. catenella</italic> forecast performance with lead time. In <bold>(A)</bold>, the left and right figures indicate the simulated and observed distributions of <italic>A. catenella</italic>, respectively. The color range indicates the density variation in <italic>A. catenella</italic> from the lowest (blue) to the highest (red) value. The spatial distributions were generated using GoogleNet and ResNet 101. In <bold>(B)</bold>, the blue and red curves indicate the performance of regression and classification CNN models, respectively. The x and y (left and right) axes denote the forecast lead time (days), root-mean-square error (RMSE) of the regression model, and accuracy of the classification model, respectively. The model with lower RMSE is considered for regression while that with higher accuracy is selected for classification.</p></caption>
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</fig>
</sec>
<sec id="S3.SS4">
<title>Model Interpretability for Gradient-Weighted Class Activation Mapping</title>
<p>Gradient-weighted class activation mapping (Grad-CAM) shows the feature maps of classification and regression CNN models with GoogleNet and Resnet 101 structures, respectively (<xref ref-type="fig" rid="F6">Figure 6</xref>). These maps were generated depending on the outbreak of <italic>A. catenella</italic> blooms (e.g., bloom and non-bloom) and density level (e.g., 5&#x2013;25<sup>th</sup> percentile, 25&#x2013;50<sup>th</sup> percentile, 50&#x2013;75<sup>th</sup> percentile, and 75&#x2013;95<sup>th</sup> percentile). The regions with high values are regarded as important features in the map. In the classification model, the important features are affiliated with salinity, temperature, water elevation, latitude-velocity of water, and NH<sub>4</sub>-N from 20 to 28 days of lookback when the bloom is not provoked (<xref ref-type="fig" rid="F6">Figure 6(A.1)</xref>). Among these variables, temperature and salinity are the most influenced variables, as evident from the high feature map values. In contrast, the important bloom features highlighted the variables from 3 to 12 days (<xref ref-type="fig" rid="F6">Figure 6(A.2)</xref>). In the regression CNN model, the 5&#x2013;25<sup>th</sup> percentile density show salinity, temperature, water elevation, and NH<sub>4</sub>-N from 5 to 30 days of lookback as important variables (<xref ref-type="fig" rid="F6">Figure 6(B.1)</xref>). The important variables in the 25&#x2013;50<sup>th</sup> percentile were similar to the 5&#x2013;25<sup>th</sup> percentile density (<xref ref-type="fig" rid="F6">Figure 6(B.2)</xref>). In the 50&#x2013;75<sup>th</sup> percentile, the lookback from 6 to 27 days is highlighted in the model, while that in the 75&#x2013;95<sup>th</sup> percentiles ranged from 4 to 22 days (<xref ref-type="fig" rid="F6">Figures 6(B.3), (B.4)</xref>) respectively).</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption><p>Feature heat maps of classification <bold>(A)</bold> and regression <bold>(B)</bold> CNN models obtained using Grad-CAM for the (A.1) bloom and (A.2) no-bloom conditions as well as cases wherein the <italic>A. catenella</italic> density lies in the (B.1) 5&#x2013;25, (B.2) 25&#x2013;50, (B.3) 50&#x2013;75, and (B.4) 75&#x2013;90 percentile ranges. The x and y axes represent the lookback and variables values, respectively. The color indicates the degree importance from the lowest (black) to the highest (white). The larger the variable value in a given cell, the greater is its importance. VELX, VELY, WSEL, SAL, TEM, OTU1, OUT2, and OUT3 denote the longitudinal velocity, latitudinal velocity, water-surface elevation, salinity, water temperature, microparticle-associated bacteria, nanoparticle-associated (NP) bacteria, and free-living (FL) bacteria, respectively.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-08-729954-g006.tif"/>
</fig>
</sec>
</sec>
<sec sec-type="discussion" id="S4">
<title>Discussion</title>
<sec id="S4.SS1">
<title>Ocean Modeling Results</title>
<p>The physical and chemical simulation results showed good agreement with the observation results (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figures 3</xref>, <xref ref-type="supplementary-material" rid="DS1">4</xref>, respectively). However, the salinity simulation was worse than that of water temperature and elevation. Previous studies have also shown that salinity cannot improve model accuracy (<xref ref-type="bibr" rid="B32">Hj&#x00F8;llo et al., 2009</xref>; <xref ref-type="bibr" rid="B49">Martyr-Koller et al., 2017</xref>) because it is vulnerable to external sources (e.g., rainfall and freshwater), increasing simulation uncertainty (<xref ref-type="bibr" rid="B3">Arfib and Charlier, 2016</xref>). The simulated water temperature at station 1 was overestimated during winter (December to February), while station 2 provided reliable outcomes in this season. This is because the model was limited to tracking water temperature at two different points if the difference between them was more than 5 &#x00B0;C. Moreover, the NH<sub>4</sub>-N simulation followed the observed trends, whereas the PO<sub>4</sub>-P simulation was less accurate. Specifically, the simulated NH<sub>4</sub>-N was underestimated at the peak point of observation and the simulated PO<sub>4</sub>-P was only able to follow the variation in observation. This demonstrated that the simulation of PO<sub>4</sub>-P and NH<sub>4</sub>-N could not improve model accuracy because these nutrients were observed in low concentrations, making the model sensitive to external sources. <xref ref-type="bibr" rid="B23">Eilola et al. (2009)</xref> and <xref ref-type="bibr" rid="B24">Feng et al. (2015)</xref> demonstrated that the simulated PO<sub>4</sub>-P was underestimated when compared with the observed values, and the simulated nitrogen encountered limitations when following the peak concentration. Additionally, the validation of these simulations is still limited by the lack of observed data. In further research, we will collect more data from additional sites.</p>
</sec>
<sec id="S4.SS2">
<title>Optimal Input Design</title>
<p>In general, the optimal inputs of both the models yielded a small window size below five and long lookback of more than 19 days (<xref ref-type="fig" rid="F4">Figures 4A,B</xref>). Therefore, spatial information below 5 5 grids was sufficient for simulating <italic>A. catenella</italic>, and temporal information from past 30 days was adequate for improving the simulation performance. The suitable range of grid sizes for the spatial distribution reflected the behavioral characteristics of the species. For the models with window sizes of seven and nine, the simulation performances decreased sharply, indicating that superfluous information might deteriorate the model accuracy. Previous studies have demonstrated that needless data could restrict the effectiveness of model training (<xref ref-type="bibr" rid="B15">Chulkov et al., 2019</xref>; <xref ref-type="bibr" rid="B18">Cova and Pais, 2019</xref>; <xref ref-type="bibr" rid="B77">Xu et al., 2019</xref>). In contrast, in the classification model, the optimal size (<italic>m</italic>, <italic>n</italic>) of the input varied depending on the structure based on whether the CNN structures adopted a skip connection or a parallel CNN layer (<xref ref-type="bibr" rid="B29">He et al., 2016b</xref>; <xref ref-type="bibr" rid="B72">Szegedy et al., 2016</xref>). This demonstrated that the model performance was affected by the structure and the properties of the input data. In addition, a simpler structure, such as GoogLeNet, was appropriate for classifying both bloom and non-bloom (<xref ref-type="fig" rid="F4">Figure 4(A.3)</xref>). In the regression model, Resnet 50 and 101 had similar optimal input properties, whereas GoogleNet and Inception v3 showed lower performances than Resnet. Among the structures, Resnet 101 was the best regression model. This demonstrates that skip connection is appropriate for estimating the density of <italic>A. catenella</italic> as it can directly connect information from a previous layer to the next layer using skipped layers (<xref ref-type="bibr" rid="B40">Khan et al., 2019</xref>). On the contrary, GoogleNet and Inception v3 applied parallel CNN layers having 1 &#x00D7; 1, 3 &#x00D7; 3, and 5 &#x00D7; 5 filter sizes. Hence, the optimization process is important to improve how the input data and model structures affect model training.</p>
</sec>
<sec id="S4.SS3">
<title>Simulation of <italic>Alexandrium catenella</italic></title>
<p>ResNet 101 offered the best performance in terms of simulating the cell density of <italic>A. catenella</italic> that followed the observation distribution, whereas GoogLeNet showed limited performance in simulating <italic>A. catenella</italic> in low and high densities (<xref ref-type="fig" rid="F4">Figure 4C</xref>). Specifically, the simulated <italic>A. catenella</italic> from GoogLeNet was overestimated in the case of low density and underestimated in the case of high density, indicating that this model was trained with a narrower range of cell density than that of the other models. The performance discrepancy between ResNet 101 and GoogLeNet may be attributed to the number of layers; ResNet 101 had more layers than GoogLeNet. This demonstrates that the number of layers could affect a model&#x2019;s performance. According to previous studies concerning CNNs (<xref ref-type="bibr" rid="B40">Khan et al., 2019</xref>; <xref ref-type="bibr" rid="B5">Baek et al., 2020</xref>), the performance of deep learning models can be influenced by the number of layers. However, a higher number of layers can increase model complexity, leading to the overfitting problem, i.e., the simulated results will correspond too closely to the training data, thereby failing to fit the validation data and predict future simulated results in a reliable manner (<xref ref-type="bibr" rid="B17">Cortes et al., 2017</xref>). In contrast, GoogLeNet demonstrated the attainment of a superior validation accuracy (96.83%) as compared to other structures. This confirms that a complex structure is not necessary to identify bloom occurrence and that sufficiently accurate results can be obtained via cell estimation. The simulated distribution substantially followed the feature of actual <italic>A. catenella</italic> blooms (<xref ref-type="fig" rid="F5">Figure 5A</xref>). Depending on bloom and non-bloom, the model generated similar spatial patterns of density with observation: on December 17, 2016, May 23, 2017, and August 19, 2019, there were no bloom outbreaks in both simulated and observed distributions; on March 27, 2018, the <italic>A. catenella</italic> blooms were observed in both the distributions; on March 28, 2017, and April 25, 2017, both distributions showed the bloom and non-bloom area in the coast. However, on March 28, 2017, the simulated distribution was determined as blooms in most areas, while there was no bloom of the observed distribution in the western sea. The high uncertainty in population dynamics could be due to <italic>in situ</italic> environmental and biological variables heterogeneously influencing the initiation, development, and ultimate demise of HABs (<xref ref-type="bibr" rid="B51">McGillicuddy et al., 2015</xref>; <xref ref-type="bibr" rid="B7">Brandenburg et al., 2017</xref>). The model generated a notable density in the specific spaces without observed data; the simulation of May 23, 2017, and August 19, 2019, presented a higher density in the channel connected to the northern enclosed bay and the enclosed bay, respectively. The mismatch results between simulation and observation also increase the model uncertainty by limiting the quantification of the exact spatial distribution of HABs. Remote sensing can solve this by improving model performance with the spatial distribution of physical, chemical, biological, and atmospheric factors (<xref ref-type="bibr" rid="B68">Shen et al., 2020</xref>). Forecast simulation showed lower performance than nowcasting. The performance of the classification and regression model decreased with increasing lead time and deteriorated sharply at a specific date (<xref ref-type="fig" rid="F5">Figure 5B</xref>). These simulation results showed that the model performance would degrade with increasing forecast lead time (days) because the input data might correspond poorly with the future ocean physical and biological processes affecting <italic>A. catenella</italic>. Prior studies have reported a decline in model performance with increasing lead time. <xref ref-type="bibr" rid="B11">Chattopadhyay et al. (2020)</xref> reported a decrease in the model performance from 73 to 47% while predicting a cold-spell class as the lead time changed from 1 to 5 days. <xref ref-type="bibr" rid="B61">Pyo et al. (2020)</xref> observed the validation accuracy to decrease with increasing lead time when simulating Microcystis&#x2014;a causative algal taxon of freshwater HAB. As reported by <xref ref-type="bibr" rid="B52">Miao et al. (2019)</xref>, an increase in the forecast lead time causes an increase in model uncertainty and imperfect representation of the extracted features. This deteriorated model training and reduced the forecast accuracy. Therefore, this study demonstrated the robust short-term <italic>A. catenella</italic> forecasting ability of the DL model.</p>
</sec>
<sec id="S4.SS4">
<title>Model Interpretability for Gradient-Weighted Class Activation Mapping</title>
<p>Temperature and salinity are factors with the greatest influence on the classification and regression models, as confirmed by the high values observed in the feature map (<xref ref-type="fig" rid="F6">Figures 6A,B</xref>). Temperature and salinity affect cyst germination and <italic>A. catenella</italic> growth, thereby causing the proliferation of <italic>A. catenella</italic> cells (<xref ref-type="bibr" rid="B37">Itakura and Yamaguchi, 2001</xref>; <xref ref-type="bibr" rid="B54">Nagai et al., 2004</xref>). <xref ref-type="bibr" rid="B34">Ichimi et al. (2001)</xref> reported that temperature plays a critical role in cyst germination and algal bloom. <xref ref-type="bibr" rid="B58">Parkhill and Cembella (1999)</xref> demonstrated that salinity influences <italic>A. catenella</italic> growth. NH<sub>4</sub>-N and water elevation were also highlighted. <italic>A. catenella</italic> uses a nitrogen source for growth and prefers ammonium uptake (<xref ref-type="bibr" rid="B70">Siu et al., 1997</xref>). <xref ref-type="bibr" rid="B16">Collos et al. (2006)</xref> observed that the growth of <italic>A. catenella</italic> is limited by ammonium uptake and accumulation. Moreover, an increase in water elevation tends to weaken and accelerate the advection and dispersion of algal blooms, respectively (<xref ref-type="bibr" rid="B76">Wu and Kong, 2009</xref>). Additionally, <xref ref-type="bibr" rid="B25">Giddings et al. (2014)</xref> demonstrated that the physical factors of oceans influence HAB development. The regression CNN model identifies fewer important features that increase the density of <italic>A. catenella.</italic> In particular, factors, such as the salinity, temperature, and NH<sub>4</sub>-N concentration over a 5&#x2013;30-day lookback period were highlighted in the 5&#x2013;25<sup>th</sup> percentile while higher densities were simulated considering variables over 6&#x2013;22-day lookback period. The results can be related to the initiation for bloom development of a given inoculum size at a suitable time. The Grad-CAM result reveals that the proposed model generates cell density by changing the highlighted variables. This is because the variables of influence differ depending on the life cycle <italic>A. catenella</italic>. The water temperature and salinity initiate the development of <italic>A. catenella</italic> while the nutrient and retention time accelerate its growth (<xref ref-type="bibr" rid="B37">Itakura and Yamaguchi, 2001</xref>; <xref ref-type="bibr" rid="B54">Nagai et al., 2004</xref>; <xref ref-type="bibr" rid="B4">Armi et al., 2011</xref>). Previous studies have reported the transitions in the highlighted region as change input. <xref ref-type="bibr" rid="B56">Panwar et al. (2020)</xref> adopted Grad-CAM to identify important areas of COVID-19 detection and demonstrated the change in the highlighted area as an input image. <xref ref-type="bibr" rid="B14">Cheng et al. (2019)</xref> extracted hip-fracture features using Grad-CAM and X-ray images. This study estimates the spatiotemporal distribution of <italic>A. catenella</italic> using CNN and determines the cause of bloom using Grad-CAM. Most previously reported algal simulations have focused on inland water species, such as cyanobacteria, green algae, and diatom. However, only few studies have addressed HAB modeling in seawater and only analyzed limited species (e.g., <italic>A. fundyense</italic>). HAB modeling in marine ecosystems should consider several environmental factors, such as the temperature, salinity, and velocity of water as well as symbiosis among different species. The paucity of relevant research in this domain could be attributed to the need for the use of complex modeling techniques and availability of limited observations (<xref ref-type="bibr" rid="B62">Ralston and Moore, 2020</xref>). This study overcomes this limitation via successful application of deep learning for simulating <italic>A. catenella</italic> HAB using an ocean model. Further research can be performed considering other species (e.g., <italic>Cochlodinium</italic> and <italic>Karenia</italic>) with additional monitoring. The findings of this research are expected to improve the applicability, expendability, and accuracy of HAB modeling using the deep learning models. Therefore, the proposed approach can be considered useful in establishing HAB management in marine environments.</p>
</sec>
</sec>
<sec sec-type="conclusion" id="S5">
<title>Conclusion</title>
<p>This study applied regression and classification using CNN models for simulating spring blooms of <italic>A. catenella</italic>. The classification was used to analyze the initiation of <italic>A. catenella</italic>, while the regression generated the density of the genera. GoogLeNet and Resnet 101 were identified as the best deep learning structures for classification and regression using CNNs, yielding an accuracy and RMSE of 96.8% and 1.20 [log(cells L<sup>&#x2013;1</sup>)], respectively. Using Grad-CAM, the salinity, temperature, and NH<sub>4</sub>-N were found to be significant variables that influence the bloom of <italic>A. catenella</italic>. In particular, factors such as the salinity, temperature, and NH<sub>4</sub>-N concentration over a 5&#x2013;30-day lookback period were highlighted in the 5&#x2013;25th percentile, while higher densities were simulated considering variables over the 6&#x2013;22 day lookback period. The results can be related to the initiation for bloom development of a given inoculum size at a suitable time. As per the authors, the study makes a significant contribution to the literature because understanding and mitigating harmful algal blooms (HABs) are important for reducing economic losses and public health damages. In contrast to modeling methods that can only measure simulation performance, the proposed model can simulate the initiation and growth of HABs based on influencing factors. However, to establish an AI-based HAB modeling system, the following challenges remain: (1) additional monitoring that includes environmental variables (NH<sub>4</sub>-N and PO<sub>4</sub>-P) and target species (<italic>A. catenella</italic>) is required, and (2) models should be trained using observations from various sites to improve model adaptability. Further research can improve the models via continuous data acquisition. Hence, the suggested models could be useful in establishing HAB management systems for aquatic environments.</p>
</sec>
<sec sec-type="data-availability" id="S6">
<title>Data Availability Statement</title>
<p>All data needed to evaluate the conclusions in the paper are present in the paper and/or the <xref ref-type="supplementary-material" rid="DS1">Supplementary Material</xref>. Additional data related to this paper may be requested from the authors.</p>
</sec>
<sec id="S7">
<title>Author Contributions</title>
<p>S-SB, YOK, and KHC conceptualized the proposed research. S-SB was responsible for preparing the methodology, data visualization, and preparing the original draft of the manuscript. YSK and JCP performed the data curation. SHB, C-YA, and H-MO performed the data validation. YOK and KHC handled funding acquisition. All authors reviewed and edited the manuscript, subsequent to the first draft.</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>
<sec sec-type="disclaimer" id="s8">
<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>
</body>
<back>
<sec sec-type="funding-information" id="s10">
<title>Funding</title>
<p>This study was supported by the Ministry of Science, ICT &#x0026; Future Planning (grant NRF-2016M1A5A1027457) and Korean Institute of Ocean Science and Technology (PE99912).</p>
</sec>
<sec id="S9" sec-type="supplementary-material">
<title>Supplementary Material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fmars.2021.729954/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmars.2021.729954/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Data_Sheet_1.docx" id="DS1" mimetype="application/vnd.openxmlformats-officedocument.wordprocessingml.document" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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