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<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Environ. Sci.</journal-id>
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<journal-title>Frontiers in Environmental Science</journal-title>
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<issn pub-type="epub">2296-665X</issn>
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<article-id pub-id-type="publisher-id">1787337</article-id>
<article-id pub-id-type="doi">10.3389/fenvs.2026.1787337</article-id>
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<subj-group subj-group-type="heading">
<subject>Data Report</subject>
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<title-group>
<article-title>An evaluated aerosol extinction coefficient dataset and its application to improve visibility forecasts in Xiong&#x2019;an, China</article-title>
<alt-title alt-title-type="left-running-head">Wen et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fenvs.2026.1787337">10.3389/fenvs.2026.1787337</ext-link>
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<contrib contrib-type="author">
<name>
<surname>Wen</surname>
<given-names>Wei</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
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<surname>Liu</surname>
<given-names>Xiaoqi</given-names>
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<name>
<surname>Ma</surname>
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<xref ref-type="aff" rid="aff2">
<sup>2</sup>
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<xref ref-type="aff" rid="aff3">
<sup>3</sup>
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<sup>4</sup>
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<xref ref-type="corresp" rid="c001">&#x2a;</xref>
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<surname>Shen</surname>
<given-names>Liyao</given-names>
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<sup>1</sup>
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<surname>Wang</surname>
<given-names>Shaorui</given-names>
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<contrib contrib-type="author">
<name>
<surname>Zuo</surname>
<given-names>Dapeng</given-names>
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<sup>3</sup>
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<contrib contrib-type="author">
<name>
<surname>Zhang</surname>
<given-names>Danlu</given-names>
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<sup>3</sup>
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<aff id="aff1">
<label>1</label>
<institution>School of Energy and Environmental Engineering, University of Science and Technology Beijing</institution>, <city>Beijing</city>, <country country="CN">China</country>
</aff>
<aff id="aff2">
<label>2</label>
<institution>CMA Earth System Modeling and Prediction Centre (CEMC)</institution>, <city>Beijing</city>, <country country="CN">China</country>
</aff>
<aff id="aff3">
<label>3</label>
<institution>China Meteorological Administration Xiong&#x2019;an Atmospheric Boundary Layer Key Laboratory</institution>, <city>Xiong&#x2019;an</city>, <country country="CN">China</country>
</aff>
<aff id="aff4">
<label>4</label>
<institution>National Meteorological Center</institution>, <city>Beijing</city>, <country country="CN">China</country>
</aff>
<author-notes>
<corresp id="c001">
<label>&#x2a;</label>Correspondence: Xin Ma, <email xlink:href="mailto:max@cma.gov.cn">max@cma.gov.cn</email>; Jikang Wang, <email xlink:href="mailto:wangjk@cma.gov.cn">wangjk@cma.gov.cn</email>
</corresp>
</author-notes>
<pub-date publication-format="electronic" date-type="pub" iso-8601-date="2026-02-10">
<day>10</day>
<month>02</month>
<year>2026</year>
</pub-date>
<pub-date publication-format="electronic" date-type="collection">
<year>2026</year>
</pub-date>
<volume>14</volume>
<elocation-id>1787337</elocation-id>
<history>
<date date-type="received">
<day>14</day>
<month>01</month>
<year>2026</year>
</date>
<date date-type="rev-recd">
<day>28</day>
<month>01</month>
<year>2026</year>
</date>
<date date-type="accepted">
<day>29</day>
<month>01</month>
<year>2026</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2026 Wen, Liu, Ma, Wang, Sheng, Shen, Wang, Zuo and Zhang.</copyright-statement>
<copyright-year>2026</copyright-year>
<copyright-holder>Wen, Liu, Ma, Wang, Sheng, Shen, Wang, Zuo and Zhang</copyright-holder>
<license>
<ali:license_ref start_date="2026-02-10">https://creativecommons.org/licenses/by/4.0/</ali:license_ref>
<license-p>This is an open-access article distributed under the terms of the <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution License (CC BY)</ext-link>. 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.</license-p>
</license>
</permissions>
<kwd-group>
<kwd>aerosol extinction coefficient</kwd>
<kwd>CMA-MESO</kwd>
<kwd>dataset</kwd>
<kwd>multi-source data fusion</kwd>
<kwd>PM<sub>2.5</sub>
</kwd>
<kwd>visibility forecasting</kwd>
</kwd-group>
<funding-group>
<funding-statement>The author(s) declared that financial support was received for this work and/or its publication. This work was supported by the Opening Foundation of China Meteorological Administration Xiong&#x2019;an Atmospheric Boundary Layer Key Laboratory (No. 2023LABL-B23), and the Joint Fund of the National Natural Science Foundation of China and the China Meteorological Administration (U2442211).</funding-statement>
</funding-group>
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<meta-name>section-at-acceptance</meta-name>
<meta-value>Atmosphere and Climate</meta-value>
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</front>
<body>
<sec sec-type="intro" id="s1">
<label>1</label>
<title>Introduction</title>
<p>With growing urbanization and industrialization in China, air pollution has become a major environmental issue affecting visibility across the country, especially in rapidly developing urban areas (<xref ref-type="bibr" rid="B8">Guo et al., 2014</xref>; <xref ref-type="bibr" rid="B28">Yue et al., 2017</xref>). Research demonstrates that particulate matter (PM<sub>2.5</sub>, PM<sub>10</sub>), aerosols, and other pollutants significantly reduce visibility by scattering and absorbing light, thereby causing severe impacts on public health, traffic safety, and economic activities (<xref ref-type="bibr" rid="B5">De Marco et al., 2019</xref>; <xref ref-type="bibr" rid="B11">Hao et al., 2021</xref>; <xref ref-type="bibr" rid="B23">Su et al., 2020</xref>). To quantify the influence of various factors on visibility, the atmospheric extinction coefficient is introduced; it represents the cumulative effect of multiple light-extinguishing substances in the atmosphere across visible and near-infrared wavelengths. Particularly during hazy conditions, aerosol extinction becomes a primary factor affecting visibility (<xref ref-type="bibr" rid="B25">Ting et al., 2022</xref>; <xref ref-type="bibr" rid="B13">Hu et al., 2017</xref>). The aerosol extinction coefficient (AEC), which is governed by particulate mass concentration, chemical composition, and hygroscopicity, constitutes a major source of uncertainty in visibility forecasting (<xref ref-type="bibr" rid="B1">Bhattacharjee et al., 2023</xref>).</p>
<p>The primary technical methods for calculating the aerosol extinction coefficient include the physics-based Mie scattering theory, the statistics-based empirical formula method, and the remote sensing-based retrieval method, each possessing distinct advantages and application limitations. Mie scattering theory (<xref ref-type="bibr" rid="B20">Mie, 1908</xref>) calculates scattering and absorption coefficients based on aerosol particle size distribution, refractive index, and wavelength, forming the theoretical foundation for AEC computation. This method assumes aerosols are spherical particles and enables precise calculation of extinction efficiency by integrating particle size distribution with chemical composition (<xref ref-type="bibr" rid="B21">Ohta et al., 1990</xref>; <xref ref-type="bibr" rid="B24">Sumlin et al., 2018</xref>). <xref ref-type="bibr" rid="B9">Han et al. (2013)</xref> utilized a Mie scattering model within the Regional Atmospheric Modeling System&#x2013;Community Multiscale Air Quality (RAMS-CMAQ) modeling system to simulate visibility during pollution episodes in Beijing and the North China Plain. Their results indicated that the low visibility events in this region were primarily caused by high concentrations of PM<sub>2.5</sub>, resulting from the accumulation of local pollutant emissions and long-range transport. In related studies, Mie scattering theory is also frequently employed to analyze the extinction characteristics of PM<sub>2.5</sub>. For instance, the hygroscopic growth of ammonium sulfate and ammonium nitrate under high-humidity conditions significantly enhances AEC (<xref ref-type="bibr" rid="B6">Gao et al., 2021</xref>). However, this method requires detailed particle size spectra and chemical composition data, which are difficult to obtain, and its high computational complexity constrains its application in real-time forecasting (<xref ref-type="bibr" rid="B29">Zhan et al., 2025</xref>; <xref ref-type="bibr" rid="B7">Garc&#xed;a-Arroyo and Osca, 2017</xref>).</p>
<p>Secondly, the empirical formula method establishes a functional relationship between AEC and variables such as PM<sub>2.5</sub> concentration and humidity through statistical regression, and it is widely used in air quality and visibility models. For example, <xref ref-type="bibr" rid="B18">Liu et al. (2022)</xref> developed a multiple regression equation relating visibility to PM<sub>2.5</sub> concentration, temperature, and dew point temperature, which effectively reproduced the variation of winter visibility from 2016 to 2020 in the Beijing-Tianjin-Hebei and Yangtze River Delta regions. Among these methods, the US Interagency Monitoring of Protected Visual Environments (IMPROVE) program, based on long-term observations and research on key optical parameters related to visibility and aerosol composition, reconstructed the relationship between aerosol chemical component mass concentration and the extinction coefficient (<xref ref-type="bibr" rid="B10">Hand and Malm, 2007</xref>; <xref ref-type="bibr" rid="B19">Malm et al., 1994</xref>). This program has become the most widely used empirical method for estimating the extinction coefficient. The IMPROVE empirical method estimates AEC based on PM<sub>2.5</sub> chemical components such as sulfate, nitrate, and organic carbon (<xref ref-type="bibr" rid="B22">Pitchford et al., 2007</xref>). This algorithm incorporates the hygroscopic growth factor (f (Relative Humidity, RH)), effectively characterizing the influence of humidity on extinction (<xref ref-type="bibr" rid="B31">Zhao et al., 2019</xref>). For instance, researchers applying the IMPROVE algorithm to assess visibility impairment in China&#x2019;s Beijing-Tianjin-Hebei and Yangtze River Delta regions found that ammonium sulfate and organic matter contributed approximately 40% and 24%, respectively, to the extinction coefficient (<xref ref-type="bibr" rid="B6">Gao et al., 2021</xref>). However, this method relies on region-specific chemical composition data, exhibits poor versatility, and responds inadequately to dynamic changes in PM<sub>2.5</sub> composition.</p>
<p>Furthermore, satellite and radar retrieval methods are often used for AEC calculation, utilizing remote sensing data such as those from the Cloud-Aerosol Lidar (CALIPSO) and Moderate Resolution Imaging Spectroradiometer (MODIS). CALIOP data provide the aerosol vertical distribution, which, combined with MODIS Aerosol Optical Depth (AOD), enables the estimation of surface AEC via a two-layer model (<xref ref-type="bibr" rid="B12">He et al., 2012</xref>). Research in Shanghai, China, demonstrated that the AEC estimated using the two-layer model using combined CALIOP and MODIS data was highly correlated with observed visibility, with a correlation coefficient of 0.86 (<xref ref-type="bibr" rid="B12">He et al., 2012</xref>). However, satellite retrieval is often limited by cloud contamination and relatively coarse spatial resolution, which restricts its ability to meet the demands of numerical forecasting.</p>
<p>The atmospheric extinction coefficient is a core physical quantity that quantifies the interaction between light and the atmosphere. As a key input for numerical simulations of visibility, it supports the analysis of aerosol physical and chemical properties, research on atmospheric radiative transfer, and assessment of climate effects, thereby forming a scientific bridge connecting fundamental research with practical needs such as pollution control and climate policy formulation. China&#x2019;s Xiong&#x2019;an New Area, officially established in 2017 as a national-level new district, is designed to relieve Beijing of functions non-essential to its role as the capital and promote the coordinated regional development of the Beijing-Tianjin-Hebei area (<xref ref-type="bibr" rid="B17">Liao and Huang, 2020</xref>). As shown in <xref ref-type="sec" rid="s11">Supplementary Figure S1</xref>, this region is characterized by unique geographical attributes: nestled against the eastern slopes of the Taihang Mountains in the west, adjacent to the North China Plain in the east, fronting the Bohai Bay, and cradling the renowned Baiyang Lake Wetland, often called the &#x201c;Pearl of North China&#x201d; Xiong&#x2019;an has a warm-temperate monsoon continental climate. Situated at the lower reach of nine rivers, the area is jointly influenced by its complex terrain and the northern fringe of the East Asian monsoon belt, with prevailing northeasterly-to-southwesterly airflow throughout the year. This makes the climate highly sensitive and variable, and prone to meteorological hazards such as low-visibility events. This specific geographical and climatic context, compounded by multifaceted pressures such as persistently high PM<sub>2.5</sub> concentrations, pronounced humidity variability, and concentrated local emissions (<xref ref-type="bibr" rid="B30">Zhang et al., 2023</xref>), collectively establishes the region as a prototypical area for investigating atmospheric extinction characteristics, visibility evolution, and aerosol effects amid rapid urbanization.</p>
<p>This study focuses on the Chinese Xiong&#x2019;an New Area as a case study. By establishing a multi-source data fusion approach integrated with numerical simulation techniques, we have constructed a comprehensive dataset of aerosol extinction coefficients. This effort compensates for the limitations inherent in relying solely on the IMPROVE empirical formula or satellite retrieval methods for constructing extinction coefficient datasets, thereby providing a novel methodology for related fields. The dataset enabled regional visibility simulations using the China Meteorological Administration Mesoscale model (CMA-MESO), the outcomes of which were rigorously evaluated against ground-based observational data. The dataset encompasses an optimized aerosol extinction coefficient series and visibility forecast products. Its construction methodology is not only applicable to visibility simulation and forecasting evaluation in urban environments but also provides scientific data support and practical reference for regional air quality management, sustainable urban planning, atmospheric radiation transfer modeling, and climate impact analysis.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>Methods</title>
<sec id="s2-1">
<label>2.1</label>
<title>Extinction coefficient calculation methods</title>
<p>This research is dedicated to constructing an aerosol extinction coefficient dataset through a multi-source data fusion approach, primarily to serve visibility prediction in mesoscale numerical weather modeling. This study is based on the CMA-MESO model, a mesoscale numerical weather prediction system independently developed by the China Meteorological Administration (CMA) which has been under continuous development and refinement since 2001 (<xref ref-type="bibr" rid="B3">Chen et al., 2008</xref>; <xref ref-type="bibr" rid="B32">Zhuang et al., 2023</xref>; <xref ref-type="bibr" rid="B15">Jishan, 2004</xref>). The system operates on the principles of mesoscale meteorological dynamics, utilizing high-resolution numerical simulation and multi-source data assimilation to generate refined weather element forecasts. It provides critical support for both daily meteorological operations and the safeguarding of major public events (<xref ref-type="bibr" rid="B2">Chen and Shen, 2006</xref>; <xref ref-type="bibr" rid="B14">Huang et al., 2017</xref>).</p>
<p>In this study, two methods were applied in the CMA_MESO model to simulate visibility data in China, which were labelled as S1 and S2.</p>
<sec id="s2-1-1">
<label>2.1.1</label>
<title>The S1 scheme</title>
<p>S1 is a set of algorithms based on historical station observation data. <xref ref-type="bibr" rid="B26">Wang et al. (2020)</xref> found the PM<sub>2.5</sub> concentration showed a good linear relationship with the extinction coefficients at different relative humidity in most parts of China, according to observation data. Especially in Beijing, the correlation coefficients between extinction coefficient and PM<sub>2.5</sub> concentration always fluctuate around 0.90, with relative humidity ranging from 20% to 90%. The relationship equations between PM<sub>2.5</sub> concentration and extinction coefficient are given by <xref ref-type="disp-formula" rid="e1">Equation 1</xref>.<disp-formula id="e1">
<mml:math id="m1">
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>e</mml:mi>
<mml:mi>x</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>a</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>H</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#xd7;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>M</mml:mi>
</mml:mrow>
<mml:mn>2.5</mml:mn>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>b</mml:mi>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
</p>
<p>Where <italic>&#x3b4;ext</italic> is the extinction coefficient, <italic>m</italic>
<sup>&#x2212;1</sup>; <inline-formula id="inf1">
<mml:math id="m2">
<mml:mrow>
<mml:mi>a</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>H</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> is the extinction efficiency of the aerosol produced by PM<sub>2.5</sub> under different relative humidity; PM<sub>2.5</sub> is the fine particulate matter concentration, &#x3bc;g/m<sup>3</sup> b is the additional extinction coefficient arising from Rayleigh scattering and gas absorption, <italic>m</italic>
<sup>&#x2212;1</sup>.</p>
<p>The value of (<italic>RH</italic>) and b were referred to <xref ref-type="bibr" rid="B26">Wang et al. (2020)</xref>. Based on hourly observational data of PM<sub>2.5</sub> and relative humidity from 2018 to 2023, the aerosol extinction coefficient in Xiong&#x2019;an was calculated using <xref ref-type="disp-formula" rid="e1">Formula 1</xref>. Considering the significant differences in particulate pollution characteristics across seasons and distinct diurnal variation patterns, the hourly data for each respective month over the 5-year period were averaged, forming the basis for the extinction coefficient dataset under the S1 scheme. The average value is calculated using <xref ref-type="disp-formula" rid="e2">Equation 2</xref>, as follows:<disp-formula id="e2">
<mml:math id="m3">
<mml:mrow>
<mml:msub>
<mml:mover accent="true">
<mml:mi>&#x3b4;</mml:mi>
<mml:mo>&#xaf;</mml:mo>
</mml:mover>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>h</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msubsup>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>y</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mn>5</mml:mn>
</mml:msubsup>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>y</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>h</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mn>5</mml:mn>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
</p>
<p>Where y stands for year, m for month, and h for hour. <inline-formula id="inf2">
<mml:math id="m4">
<mml:mrow>
<mml:msub>
<mml:mover accent="true">
<mml:mi>&#x3b4;</mml:mi>
<mml:mo>&#xaf;</mml:mo>
</mml:mover>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>h</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> represents the final required average extinction coefficient for the m-th month and h-th hour, while <inline-formula id="inf3">
<mml:math id="m5">
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>y</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>m</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>h</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> denotes the original extinction coefficient data for the h-th hour of the m-th month in the y-th year.</p>
</sec>
<sec id="s2-1-2">
<label>2.1.2</label>
<title>The S2 scheme</title>
<p>S2 is generated from S1 through the integration of satellite aerosol extinction data. This approach employs the Space-Time Multiscale Analysis System (STMAS), an advanced data assimilation system developed by the Earth System Research Laboratory (ESRL) of the National Oceanic and Atmospheric Administration (NOAA), to merge the baseline data produced by <xref ref-type="disp-formula" rid="e1">Formula 1</xref> with the MERRA-2 reanalysis product, thereby creating the new dataset. MERRA-2 provides globally covered reanalysis data and significantly improves the spatiotemporal consistency and accuracy of atmospheric variables (such as aerosols) by assimilating multi-source satellite observations. The core algorithm of STMAS is the multigrid sequential variational method, which performs iterative analysis from coarse to fine grids. This method utilizes coarse grids to accelerate the convergence of large-scale, low-frequency patterns, thereby providing an initial field for the fine-grid analysis. This process effectively eliminates aliasing effects across different scales, ultimately producing a fused product with high spatiotemporal resolution (<xref ref-type="bibr" rid="B27">Xie et al., 2011</xref>).</p>
<p>The objective function on each grid is given by <xref ref-type="disp-formula" rid="e3">Equation 3</xref>:<disp-formula id="e3">
<mml:math id="m6">
<mml:mrow>
<mml:msup>
<mml:mi mathvariant="normal">J</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:mfrac>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mrow>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mi>T</mml:mi>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:mfrac>
<mml:msup>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msup>
<mml:mi>H</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mi>T</mml:mi>
</mml:msup>
<mml:msup>
<mml:mi>O</mml:mi>
<mml:mrow>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2010;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msup>
<mml:mi>H</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mtext>&#x2002;</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>3</mml:mn>
<mml:mo>,</mml:mo>
<mml:mi>L</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>
</p>
<p>The Y value on each grid is calculated using <xref ref-type="disp-formula" rid="e4">Equation 4</xref> as follows:<disp-formula id="e4">
<mml:math id="m7">
<mml:mrow>
<mml:mfenced open="{" close="" separators="|">
<mml:mrow>
<mml:mtable columnalign="left">
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mtext mathvariant="italic">obs</mml:mtext>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>H</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>b</mml:mi>
</mml:msup>
<mml:mtext>&#x2003;</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x2010;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>H</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x2010;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x2010;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>3</mml:mn>
<mml:mo>,</mml:mo>
<mml:mi>L</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>
</p>
<p>The final analysis result is derived from the superposition of the results of each heavy grid analysis, as expressed in <xref ref-type="disp-formula" rid="e5">Equation 5</xref>:<disp-formula id="e5">
<mml:math id="m8">
<mml:mrow>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>a</mml:mi>
</mml:msup>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>b</mml:mi>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>X</mml:mi>
<mml:mi>L</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>b</mml:mi>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>N</mml:mi>
</mml:munderover>
</mml:mstyle>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(5)</label>
</disp-formula>
</p>
<p>Among them <inline-formula id="inf4">
<mml:math id="m9">
<mml:mrow>
<mml:mi mathvariant="normal">Y</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mi>o</mml:mi>
<mml:mi>b</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>H</mml:mi>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>b</mml:mi>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula>, <inline-formula id="inf5">
<mml:math id="m10">
<mml:mrow>
<mml:mi mathvariant="normal">X</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>a</mml:mi>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>b</mml:mi>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula>. O is the observation error covariance matrix; <inline-formula id="inf6">
<mml:math id="m11">
<mml:mrow>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>b</mml:mi>
</mml:msup>
<mml:mo>,</mml:mo>
<mml:msup>
<mml:mi>X</mml:mi>
<mml:mi>a</mml:mi>
</mml:msup>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>a</mml:mtext>
<mml:mtext>n</mml:mtext>
<mml:mtext>d</mml:mtext>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mtext>&#x2009;</mml:mtext>
<mml:msup>
<mml:mi>Y</mml:mi>
<mml:mrow>
<mml:mi>o</mml:mi>
<mml:mi>b</mml:mi>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> are the background field, analysis field, and observation field vectors, respectively; H is the bilinear interpolation operator from the model grid to the observation point; X represents the correction vector relative to the model field vector, calculated by the variational data assimilation system; Y is the difference between the observation field and the model field; n represents the nth grid, and N is the total number of grids. The element data is fused according to the multi-grid variational analysis method to generate a fusion product.</p>
<p>The development of the S2 extinction coefficient dataset involved transforming the S1-derived data into a 3-km resolution grid through the application of the Cressman (<xref ref-type="bibr" rid="B4">Cressman, 1959</xref>) interpolation method, which was selected for its demonstrated advantages in spatiotemporal distribution accuracy. The Cressman objective analysis method employs a successive correction technique to interpolate data from discrete observation stations onto regular grid points. The specific procedure is as follows: First, an initial guess field for the grid points is established, which in this study is defined as the regional mean within the scanning radius R. Subsequently, observational data within this radius are used to correct the initial guess field by calculating the analysis increment (<inline-formula id="inf7">
<mml:math id="m12">
<mml:mrow>
<mml:mo>&#x394;</mml:mo>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>) between the observed values and the initial field. This correction process is repeated iteratively until the adjusted field converges satisfactorily with the observations. In practice, a single objective analysis typically requires configuring the configuration of multiple scanning radii R and several iterations of the Cressman method to achieve optimal results. The formula is expressed as follows in <xref ref-type="disp-formula" rid="e6">Equations 6</xref>&#x2013;<xref ref-type="disp-formula" rid="e9">9</xref>:<disp-formula id="e6">
<mml:math id="m13">
<mml:mrow>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mi>n</mml:mi>
</mml:msubsup>
<mml:mo>&#x3d;</mml:mo>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x2010;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msubsup>
<mml:mo>&#x2b;</mml:mo>
<mml:mo>&#x394;</mml:mo>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(6)</label>
</disp-formula>
<disp-formula id="e7">
<mml:math id="m14">
<mml:mrow>
<mml:mo>&#x394;</mml:mo>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msubsup>
<mml:mrow>
<mml:mo>&#x2211;</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mi>k</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>K</mml:mi>
</mml:msubsup>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mi>k</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x3b4;</mml:mi>
</mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:msubsup>
<mml:mrow>
<mml:mo>&#x2211;</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mi>k</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>K</mml:mi>
</mml:msubsup>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(7)</label>
</disp-formula>
<disp-formula id="e8">
<mml:math id="m15">
<mml:mrow>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mtext mathvariant="italic">ijk</mml:mtext>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfenced open="{" close="" separators="|">
<mml:mrow>
<mml:mtable columnalign="left">
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msup>
<mml:mi>R</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
<mml:mrow>
<mml:msup>
<mml:mi>R</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2b;</mml:mo>
<mml:msup>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2264;</mml:mo>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mrow>
<mml:mn>0</mml:mn>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3e;</mml:mo>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(8)</label>
</disp-formula>
<disp-formula id="e9">
<mml:math id="m16">
<mml:mrow>
<mml:msubsup>
<mml:mi mathvariant="normal">&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msubsup>
<mml:mo>&#x3d;</mml:mo>
<mml:msup>
<mml:mi>V</mml:mi>
<mml:mi>R</mml:mi>
</mml:msup>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msubsup>
<mml:mo>&#x2b;</mml:mo>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>V</mml:mi>
<mml:mi>R</mml:mi>
</mml:msup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mtext mathvariant="italic">ij</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>R</mml:mi>
<mml:mo>&#x2010;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
</mml:math>
<label>(9)</label>
</disp-formula>
</p>
<p>Where R represents the scanning radius, <inline-formula id="inf8">
<mml:math id="m17">
<mml:mrow>
<mml:msub>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> denotes the distance between the k-th observation within the scanning radius and the grid point (i,j), <inline-formula id="inf9">
<mml:math id="m18">
<mml:mrow>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the influence weight of the k-th observation on grid point (i,j), <inline-formula id="inf10">
<mml:math id="m19">
<mml:mrow>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mi>k</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> represents the k-th observational value within the scanning radius, <inline-formula id="inf11">
<mml:math id="m20">
<mml:mrow>
<mml:msub>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the value of the initial guess field, and <inline-formula id="inf12">
<mml:math id="m21">
<mml:mrow>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
</mml:mrow>
<mml:mi>n</mml:mi>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula> denotes the Cressman analysis value after the (n&#x2212;1)-th iteration. <inline-formula id="inf13">
<mml:math id="m22">
<mml:mrow>
<mml:msup>
<mml:mi>V</mml:mi>
<mml:mi>R</mml:mi>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> represents the Cressman analysis weight for scanning radius R, where the dimensions of V and R are identical. <inline-formula id="inf14">
<mml:math id="m23">
<mml:mrow>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula> is the Cressman analysis result for scanning radius R, while <inline-formula id="inf15">
<mml:math id="m24">
<mml:mrow>
<mml:msubsup>
<mml:mi>&#x3b4;</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>R</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
</mml:math>
</inline-formula> corresponds to the analysis result for scanning radius R&#x2212;1.</p>
<p>The 3-km gridded data, obtained through the aforementioned interpolation method, were subsequently fused with the MERRA-2 reanalysis aerosol extinction data using the data assimilation approach described in <xref ref-type="disp-formula" rid="e3">Equation 3</xref>. This procedure yielded the integrated grid data that form the S2 extinction coefficient dataset.</p>
<p>The aerosol extinction coefficients calculated by the S1 and S2 schemes will be converted into visibility via Koschmieder&#x2019;s law for the purpose of evaluating the dataset quality and its application effectiveness, as given in <xref ref-type="disp-formula" rid="e10">Equation 10</xref>.<disp-formula id="e10">
<mml:math id="m25">
<mml:mrow>
<mml:mtext>Vis</mml:mtext>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mn>3.912</mml:mn>
<mml:mrow>
<mml:mi>&#x3b2;</mml:mi>
<mml:mo>&#xd7;</mml:mo>
<mml:mi>ln</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mn>10</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(10)</label>
</disp-formula>
</p>
</sec>
</sec>
<sec id="s2-2">
<label>2.2</label>
<title>Test methods</title>
<p>To verify the accuracy of the extinction coefficient, this study assessed its impact on visibility forecasting. The performance of the two calculation schemes (S1 and S2) was evaluated through statistical and graded verification tests, following the methodology detailed in <xref ref-type="sec" rid="s11">Supplementary Table S1</xref> (<xref ref-type="bibr" rid="B16">Jongeward et al., 2016</xref>).</p>
<p>The statistical test metrics comprise the mean error (ME) defined in <xref ref-type="disp-formula" rid="e11">Equation 11</xref>, the normalized mean bias (NMB) given by <xref ref-type="disp-formula" rid="e12">Equation 12</xref>, and the root-mean-square error (RMSE) expressed in <xref ref-type="disp-formula" rid="e13">Equation 13</xref>.<disp-formula id="e11">
<mml:math id="m26">
<mml:mrow>
<mml:mi>M</mml:mi>
<mml:mi>E</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>N</mml:mi>
</mml:munderover>
</mml:mstyle>
<mml:mrow>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mo>/</mml:mo>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(11)</label>
</disp-formula>
<disp-formula id="e12">
<mml:math id="m27">
<mml:mrow>
<mml:mi>N</mml:mi>
<mml:mi>M</mml:mi>
<mml:mi>B</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>N</mml:mi>
</mml:munderover>
</mml:mstyle>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
<mml:mo>/</mml:mo>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>N</mml:mi>
</mml:munderover>
</mml:mstyle>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#xd7;</mml:mo>
<mml:mn>100</mml:mn>
<mml:mo>%</mml:mo>
</mml:mrow>
</mml:math>
<label>(12)</label>
</disp-formula>
<disp-formula id="e13">
<mml:math id="m28">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>M</mml:mi>
<mml:mi>S</mml:mi>
<mml:mi>E</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:msqrt>
<mml:msup>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>N</mml:mi>
</mml:munderover>
</mml:mstyle>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>O</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:msqrt>
</mml:mrow>
</mml:math>
<label>(13)</label>
</disp-formula>
</p>
<p>Where i represents the values for each hour, <italic>Fi</italic> is the i-th forecast value of the scheme, <italic>Oi</italic> is the i-th observed value, and <italic>N</italic> is the total number of samples.</p>
<p>For the grading test, the Threat Score (TS) was computed using the three visibility classes in <xref ref-type="sec" rid="s11">Supplementary Figure S1</xref>. The parameters were calculated as specified in <xref ref-type="disp-formula" rid="e14">Equation 14</xref>.<disp-formula id="e14">
<mml:math id="m29">
<mml:mrow>
<mml:mi>T</mml:mi>
<mml:mi>S</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>N</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>N</mml:mi>
<mml:mi>A</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>N</mml:mi>
<mml:mi>B</mml:mi>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>N</mml:mi>
<mml:mi>C</mml:mi>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(14)</label>
</disp-formula>
</p>
<p>Where <italic>NA</italic> is the number of correct forecasts, <italic>NB</italic> is the number of empty reports, and <italic>NC</italic> is the number of missed reports. A higher TS signifies superior forecast quality.</p>
</sec>
<sec id="s2-3">
<label>2.3</label>
<title>The source of data</title>
<p>The surface observation data used in this case study include PM<sub>2.5</sub> concentration, relative humidity, and visibility. The pollution data were obtained from the Environmental Meteorological Service Platform (<ext-link ext-link-type="uri" xlink:href="http://eia-data.com/">http://eia-data.com/</ext-link>), and the meteorological data are from the Xiaozuanfeng platform (<ext-link ext-link-type="uri" xlink:href="https://meteo.agrodigits.com/">https://meteo.agrodigits.com/</ext-link>), a publicly accessible platform providing meteorological observations for research applications. All observational data were collected from stations in the Xiong&#x2019;an area. The case study focused on the Xiong&#x2019;an region and utilized data from these observation station covering the period from 1 December 2018, to 1 December 2023, covering a 5-year period.</p>
<p>The MERRA-2 (Modern Era Retrospective-Analysis for Research, version 2) (<ext-link ext-link-type="uri" xlink:href="https://disc.gsfc.nasa.gov/datasets/M2TMNXAER_5.12.4/summary">https://disc.gsfc.nasa.gov/datasets/M2TMNXAER_5.12.4/summary</ext-link>) is a long-term reanalysis product that includes various meteorological variables. In this study, we used the monthly average aerosol extinction coefficient at 550&#xa0;nm data from the MERRA-2 reanalysis dataset, covering the date range 1 December 2018, to 1 December 2023.</p>
</sec>
<sec id="s2-4">
<label>2.4</label>
<title>Data records</title>
<p>The outputs of this study have been systematically archived as the following four data files:<list list-type="order">
<list-item>
<p>PM<sub>2.5</sub> concentration observations in Xiong&#x2019;an. This dataset contains daily PM<sub>2.5</sub> concentration measurements from five monitoring stations in the Xiong&#x2019;an area-Rongcheng Middle School, Civil Affairs Bureau of Anxin County, Electric Power Bureau of Anxin County, Environmental Protection Bureau of Xiong County, and Natural Resources Bureau of Xiong County, covering the period from September 1 to 30, 2023. Daily average concentrations are provided.</p>
</list-item>
<list-item>
<p>Relative humidity observations in Xiong&#x2019;an. This file includes hourly relative humidity records from Xiong&#x2019;an monitoring stations during the same period (September 1&#x2013;30, 2023), with data recorded at 24-h intervals.</p>
</list-item>
<list-item>
<p>MERRA-2 monthly mean aerosol extinction coefficient. This dataset provides global monthly mean aerosol extinction coefficient data for September 2023, derived from the MERRA-2 reanalysis product.</p>
</list-item>
<list-item>
<p>Fused aerosol extinction coefficient from Scheme S2. This archive contains hourly aerosol extinction coefficient data for September 2023, generated using the fusion approach of Scheme S2. The data cover the Beijing-Tianjin-Hebei region (112&#xb0;E&#x2212;120&#xb0;E, 35&#xb0;N&#x2013;43&#xb0;N). The file includes 24 individual data files, one for each hour, each containing variables such as longitude, latitude, and aerosol extinction coefficient.</p>
</list-item>
</list>
</p>
</sec>
</sec>
<sec id="s3">
<label>3</label>
<title>Technical validation</title>
<sec id="s3-1">
<label>3.1</label>
<title>Visibility forecast performance</title>
<p>To validate the dataset constructed using Schemes S1 and S2, we assessed its impact on visibility forecasting for the period from September to November 2023. <xref ref-type="sec" rid="s11">Supplementary Figure S2</xref>; <xref ref-type="table" rid="T1">Table 1</xref> summarize the visibility forecast performance of the S1 and S2 schemes in the Xiong&#x2019;an New Area during this period. The S1 method considerably overestimates visibility, with ME range of 11.755&#x2013;15.594&#xa0;km, NMB of 1.414%&#x2013;2.329%, and RMSE of 13.960&#x2013;17.080&#xa0;km. The uneven distribution of meteorological stations and PM<sub>2.5</sub> monitoring stations, along with their incomplete spatial overlap, introduces uncertainties into ground-based aerosol extinction calculations. Moreover, the use of a fixed climatological AEC in S1 fundamentally fails to capture the day-to-day synoptic variability in pollution and meteorology, which constitutes the primary source of its substantial forecasting errors. In contrast, the S2 scheme significantly reduces the error by incorporating the 5-year mean PM<sub>2.5</sub> and RH data. Its performance shows an ME range of &#x2212;6.823 to 1.360&#xa0;km, NMB of &#x2212;0.298% to 0.121%, and RMSE of 4.290&#x2013;10.981&#xa0;km, demonstrating notable improvement over S1. Compared to S1, the S2 scheme achieves substantial reductions across all error metrics. Specifically, ME decreases by 58.0%&#x2013;108.1%, NMB is lowered by 107.7%&#x2013;120.4%, and RMSE shows a reduction of 35.7%&#x2013;74.9%.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>The ME, NMB and RMSE results of three schemes for each month.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th colspan="2" align="center">Xiong&#x2019;an area</th>
<th align="center">September</th>
<th align="center">October</th>
<th align="center">November</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="2" align="center">ME (km)</td>
<td align="center">S1</td>
<td align="center">15.594</td>
<td align="center">14.946</td>
<td align="center">11.755</td>
</tr>
<tr>
<td align="center">S2</td>
<td align="center">1.360</td>
<td align="center">&#x2212;4.821</td>
<td align="center">&#x2212;6.823</td>
</tr>
<tr>
<td rowspan="2" align="center">NMB (%)</td>
<td align="center">S1</td>
<td align="center">2.329</td>
<td align="center">1.896</td>
<td align="center">1.414</td>
</tr>
<tr>
<td align="center">S2</td>
<td align="center">0.121</td>
<td align="center">&#x2212;0.307</td>
<td align="center">&#x2212;0.298</td>
</tr>
<tr>
<td rowspan="2" align="center">RMSE (km)</td>
<td align="center">S1</td>
<td align="center">17.080</td>
<td align="center">16.345</td>
<td align="center">13.960</td>
</tr>
<tr>
<td align="center">S2</td>
<td align="center">4.290</td>
<td align="center">8.820</td>
<td align="center">10.981</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>
<xref ref-type="fig" rid="F1">Figure 1</xref> shows the daily mean PM<sub>2.5</sub> concentration and corresponding visibility during three selected episodes. From September 3rd to 11th, PM<sub>2.5</sub> concentrations fluctuated between 60 and 100&#xa0;&#x3bc;g/m<sup>3</sup>, accompanied by a decrease in visibility to 2&#x2013;4&#xa0;km. Between October 24 to 26, PM<sub>2.5</sub> concentrations remained low (40&#x2013;50&#xa0;&#x3bc;g/m<sup>3</sup>), and visibility improved to 5&#x2013;7&#xa0;km. From November 21st to 22nd, PM<sub>2.5</sub> concentrations rose to around 80&#xa0;&#x3bc;g/m<sup>3</sup>, and visibility dropped to 3&#x2013;5&#xa0;km. These three episodes were selected to evaluate the performance of the visibility forecasts.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>The daily average PM<sub>2.5</sub> and visibility observation data in the Xiong&#x2019;an area for the selected time period: <bold>(a)</bold> 3&#x2013;11 September 2023, <bold>(b)</bold> 24&#x2013;26 September 2023, <bold>(c)</bold> 21&#x2013;22 November 2023.</p>
</caption>
<graphic xlink:href="fenvs-14-1787337-g001.tif">
<alt-text content-type="machine-generated">Three line charts labeled a, b, and c compare visibility in meters and PM2.5 concentration in micrograms per cubic meter over time. Each graph shows visibility (black line) inversely related to PM2.5 (red line) on specific dates in 2023, with higher PM2.5 corresponding to lower visibility.</alt-text>
</graphic>
</fig>
<p>As shown in <xref ref-type="fig" rid="F2">Figure 2</xref>, the S2 scheme consistently achieved lower daily mean ME, NMB, and RMSE values across all three periods. The inverse relationship between PM<sub>2.5</sub> and visibility observed in <xref ref-type="fig" rid="F1">Figure 1</xref> is directly reflected in the forecast performance metrics of <xref ref-type="fig" rid="F2">Figure 2</xref>. Specifically, S2 yielded a daily average RMSE of approximately 6&#x2013;8&#xa0;km, outperforming S1, which had an RMSE of 12&#x2013;15&#xa0;km. Notably, although the RMSE of S2 increased from September (with a maximum of 4.29&#xa0;km) to November (with a maximum of 10.98&#xa0;km), this likely reflects the greater challenge of forecasting visibility during the more dynamically complex and polluted autumn season in North China. During October 24th&#x2013;26th, when PM<sub>2.5</sub> concentrations was low, S1 overestimated visibility, with an NMB ranging from 1% to 10%, while S2 remained stable (NMB&#x2248;&#x2212;0.5%). On November 21st&#x2013;22nd, as PM<sub>2.5</sub> concentration increased, S2 maintained a lower RMSE (about 6&#xa0;km) compared to S1. These results demonstrate the ability of the S2 scheme to deliver relatively accurate visibility predictions under varying PM<sub>2.5</sub> concentration conditions.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>The ME, NMB and RMSE of daily visibility forecasts for the selected time period: <bold>(a)</bold> 3&#x2013;11 September 2023, <bold>(b)</bold> 24&#x2013;26 September 2023, <bold>(c)</bold> 21&#x2013;22 November 2023.</p>
</caption>
<graphic xlink:href="fenvs-14-1787337-g002.tif">
<alt-text content-type="machine-generated">Three panels labeled (a), (b), and (c) each display three time series line charts comparing ME, NMB, and RMSE metrics for S1 and S2 scenarios using black and red lines. Panels show trends over different date ranges in September, October, and November 2023, with S1 values consistently higher and generally declining while S2 values remain lower and relatively stable or slightly increasing.</alt-text>
</graphic>
</fig>
</sec>
<sec id="s3-2">
<label>3.2</label>
<title>Forecasting capability in visibility intervals</title>
<p>As shown in <xref ref-type="table" rid="T2">Table 2</xref>; <xref ref-type="sec" rid="s11">Supplementary Figure S3</xref>, the S2 scheme achieves higher TS values than S1 across most visibility intervals, demonstrating its improved capability in simulating aerosol effects on visibility. In the 1&#x2013;3&#xa0;km interval, the S2 scheme achieves higher TS values (0.0440&#x2013;0.0663) than S1 (0.0048&#x2013;0.0295). The peak TS for S2 in September (0.0663) coincides with an observed PM<sub>2.5</sub> concentration of approximately 100&#xa0;&#x3bc;g/m<sup>3</sup>, underscoring its accuracy in capturing haze episodes. For the 3&#x2013;5&#xa0;km interval, S2 performs slightly better than S1 in September (TS &#x3d; 0.0373) and October (TS &#x3d; 0.0697). Similarly, in the higher visibility range (5&#x2013;10&#xa0;km), S2 outperforms S1 in September (0.1673) and November (0.1730). The consistently higher TS values of S2 across most ranges confirm its enhanced ability to simulate the aerosol effect.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>TS scores by Month and Visibility Range.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">VIS level</th>
<th align="center">Scheme</th>
<th align="center">September</th>
<th align="center">October</th>
<th align="center">November</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="2" align="center">1-3&#xa0;km</td>
<td align="center">S1</td>
<td align="center">0.0295</td>
<td align="center">0.0048</td>
<td align="center">0.0106</td>
</tr>
<tr>
<td align="center">S2</td>
<td align="center">0.0663</td>
<td align="center">0.0513</td>
<td align="center">0.0440</td>
</tr>
<tr>
<td rowspan="2" align="center">3-5&#xa0;km</td>
<td align="center">S1</td>
<td align="center">0.0268</td>
<td align="center">0.0668</td>
<td align="center">0.0864</td>
</tr>
<tr>
<td align="center">S2</td>
<td align="center">0.0373</td>
<td align="center">0.0697</td>
<td align="center">0.0343</td>
</tr>
<tr>
<td rowspan="2" align="center">5-10&#xa0;km</td>
<td align="center">S1</td>
<td align="center">0.1353</td>
<td align="center">0.1783</td>
<td align="center">0.1591</td>
</tr>
<tr>
<td align="center">S2</td>
<td align="center">0.1673</td>
<td align="center">0.1177</td>
<td align="center">0.1730</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec sec-type="conclusion" id="s4">
<label>4</label>
<title>Conclusion</title>
<p>In response to the severe visibility degradation caused by air pollution in China, this study focused on the pivotal role of the aerosol extinction coefficient in quantifying visibility and established a dedicated dataset to support related research. Two calculation schemes (S1, S2) within the CMA-MESO model were optimized, with a specific focus on the Xiong&#x2019;an New Area. Scheme S1 calculates the aerosol extinction coefficient based on 5&#xa0;years of observational data using empirical methods, while Scheme S2 integrates the extinction coefficient derived from S1 with MERRA-2 reanalysis data by applying the STMAS data fusion technique.</p>
<p>Evaluation of visibility forecasts in the Xiong&#x2019;an area shows that S2 outperforms S1, with ME ranging from &#x2212;6.823&#xa0;km to 1.360&#xa0;km and RMSE between 4.290&#xa0;km and 10.981&#xa0;km. Moreover, S2 exhibits a superior ability to capture haze events, as indicated by its higher TS in the visibility range of 1&#x2013;3&#xa0;km.</p>
<p>This study provides a methodological framework and a validated dataset that offer a scientific basis for air quality management and visibility forecasting in rapidly urbanizing regions.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s5">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="sec" rid="s11">Supplementary Material</xref>, further inquiries can be directed to the corresponding authors.</p>
</sec>
<sec sec-type="author-contributions" id="s6">
<title>Author contributions</title>
<p>WW: Conceptualization, Methodology, Supervision, Validation, Data curation, Writing &#x2013; review and editing. XL: Investigation, Writing &#x2013; review and editing, Resources, Writing &#x2013; original draft, Visualization. XM: Writing &#x2013; review and editing, Supervision, Investigation, Validation, Data curation, Conceptualization, Methodology. JW: Visualization, Writing &#x2013; original draft, Resources, Writing &#x2013; review and editing, Investigation. LiS: Conceptualization, Visualization, Writing &#x2013; review and editing. LoS: Writing &#x2013; review and editing, Visualization, Conceptualization. SW: Writing &#x2013; review and editing, Formal Analysis, Data curation. DZu: Data curation, Writing &#x2013; review and editing, Formal Analysis. DZh: Data curation, Writing &#x2013; review and editing, Formal Analysis.</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of interest</title>
<p>The author(s) declared that this work 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="ai-statement" id="s9">
<title>Generative AI statement</title>
<p>The author(s) declared that generative AI was not used in the creation of this manuscript.</p>
<p>Any alternative text (alt text) provided alongside figures in this article has been generated by Frontiers with the support of artificial intelligence and reasonable efforts have been made to ensure accuracy, including review by the authors wherever possible. If you identify any issues, please contact us.</p>
</sec>
<sec sec-type="disclaimer" id="s10">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec sec-type="supplementary-material" id="s11">
<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/fenvs.2026.1787337/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fenvs.2026.1787337/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="Supplementaryfile1.docx" id="SM1" mimetype="application/docx" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
<fn-group>
<fn fn-type="custom" custom-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1737983/overview">Yucong Miao</ext-link>, Chinese Academy of Meteorological Sciences, China</p>
</fn>
<fn fn-type="custom" custom-type="reviewed-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/3349479/overview">Xiaoqi Wang</ext-link>, Beijing University of Technology, China</p>
</fn>
</fn-group>
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