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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ACP</journal-id><journal-title-group>
    <journal-title>Atmospheric Chemistry and Physics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1680-7324</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/acp-25-16363-2025</article-id><title-group><article-title>Black carbon aerosols in China: spatial-temporal variations and lessons from long-term atmospheric observations</article-title><alt-title>Black carbon aerosols in China</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zheng</surname><given-names>Huang</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff2">
          <name><surname>Kong</surname><given-names>Shaofei</given-names></name>
          <email>kongshaofei@cug.edu.cn</email>
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff3 aff4">
          <name><surname>Ding</surname><given-names>Deping</given-names></name>
          <email>zytddp@vip.sina.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5 aff6">
          <name><surname>Savadkoohi</surname><given-names>Marjan</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3707-2601</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Song</surname><given-names>Congbo</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7948-4834</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Zheng</surname><given-names>Mingming</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9 aff10">
          <name><surname>Harrison</surname><given-names>Roy M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2684-5226</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>College of Resource and Environmental Engineering, Wuhan University of Science and Technology, 430081 Wuhan, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Atmospheric Sciences, School of Environmental Studies, China University of Geosciences, Wuhan, 430078, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Beijing Weather Modification Center, Beijing, 100089, China</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Beijing Key Laboratory of Cloud, Precipitation and Atmospheric Water Resources, Beijing, 100089, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Institute of Environmental Assessment and Water Research (IDAEA-CSIC), 08034, Barcelona, Spain</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Department of Mining, Industrial and ICT Engineering (EMIT), Manresa School of Engineering (EPSEM), Universitat Politécnica de Catalunya (UPC), Manresa, 08242, Spain</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>National Centre for Atmospheric Science (NCAS), Department of Earth and Environmental Science, The University of Manchester, Manchester M13 9PL, UK</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>School of Chemical and Environmental Engineering, Wuhan Polytechnic University, Wuhan, 430023, China</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>School of Geography, Earth and Environment Sciences, University of Birmingham, Birmingham B15 2TT, UK</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>Department of Environmental Sciences, Faculty of Meteorology, Environment and Arid Land Agriculture, King Abdulaziz University, PO Box 80203, Jeddah, Saudi Arabia</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Shaofei Kong (kongshaofei@cug.edu.cn) and Deping Ding (zytddp@vip.sina.com)</corresp></author-notes><pub-date><day>20</day><month>November</month><year>2025</year></pub-date>
      
      <volume>25</volume>
      <issue>22</issue>
      <fpage>16363</fpage><lpage>16386</lpage>
      <history>
        <date date-type="received"><day>7</day><month>May</month><year>2025</year></date>
           <date date-type="rev-request"><day>3</day><month>June</month><year>2025</year></date>
           <date date-type="rev-recd"><day>15</day><month>October</month><year>2025</year></date>
           <date date-type="accepted"><day>22</day><month>October</month><year>2025</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2025 Huang Zheng et al.</copyright-statement>
        <copyright-year>2025</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025.html">This article is available from https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e209">Black carbon (BC) significantly influences climate, air quality, and public health, and long-term observations are essential for understanding its adverse effects. While previous studies have primarily focused on spatiotemporal variations, deeper insights from such datasets remain uncovered. Using 13 years (2008–2020) of continuous measurements of equivalent black carbon (eBC) in China, this study reported the spatial-temporal variations of eBC and its sources, including solid fuel (eBC<sub>sf</sub>) and liquid fuel combustion (eBC<sub>lf</sub>). The results showed that eBC and its sources exhibited higher concentrations in eastern and northern China compared to western and southern China. Seasonal variations of eBC and eBC<sub>sf</sub> generally showed lower values during summer and higher values during winter at most stations. Long-term trends indicated that eBC and eBC<sub>lf</sub> decreased most rapidly at urban stations, while eBC<sub>sf</sub> declined faster at rural stations. Comparisons of eBC concentrations and trends between this study and global observations revealed higher eBC levels but lower reduction rates in China. These long-term observations showed that the model simulations performed well in simulating spatial distribution but poorly in capturing inter-annual variations. The weather-normalized eBC concentrations showed potential for adjusting emission estimates. The normalized results also suggested that emission control was the dominant driver of the BC reduction. This decrease was primarily driven by reductions from solid fuel combustion at rural and background stations. This study provides insights for reducing uncertainties in black carbon emission inventories and improving model performance in simulating surface concentrations.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National Natural Science Foundation of China</funding-source>
<award-id>42307147</award-id>
<award-id>42307151</award-id>
<award-id>41830965</award-id>
</award-group>
<award-group id="gs2">
<funding-source>Ministry of Science and Technology of the People's Republic of China</funding-source>
<award-id>2016YFA0602002</award-id>
</award-group>
<award-group id="gs3">
<funding-source>European Commission</funding-source>
<award-id>101036245</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e266">Despite being a small fraction of the aerosol chemical composition <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx54 bib1.bibx105" id="paren.1"/>, black carbon (BC) is important for climate, air pollution, and human health. Globally, BC can cause up to <inline-formula><mml:math id="M6" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.41 W m<sup>−2</sup> effective radiative forcing <xref ref-type="bibr" rid="bib1.bibx104" id="paren.2"/>. At the regional scale, BC aerosol can suppress the deepening of the planetary boundary layer, thereby enhancing haze pollution <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx113" id="paren.3"/> and radiative forcing <xref ref-type="bibr" rid="bib1.bibx85" id="paren.4"/>. Personal exposure to BC can cause adverse health effects, such as carcinogenic risks and elevated blood pressure, and BC can reach the fetal side of the human placenta <xref ref-type="bibr" rid="bib1.bibx78 bib1.bibx9 bib1.bibx64" id="paren.5"/>. As a short-lived climate forcer, the atmospheric lifetime of BC is about 5.5 d <inline-formula><mml:math id="M8" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 35 % (median <inline-formula><mml:math id="M9" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1 standard deviation, hereafter), according to an ensemble of 14 models <xref ref-type="bibr" rid="bib1.bibx37" id="paren.6"/>. Therefore, the study of BC aerosol is important to reduce its adverse impacts.</p>
      <p id="d2e321">To better understand the climate, environmental, and health effects of BC, it is important to model its atmospheric abundance. Although Chemistry Transport Models (CTMs) can capture the spatial-temporal variations of BC, their simulation accuracy is often poor, and there are discrepancies among different simulations. For instance, 17 global models overestimated the abundance of BC, with the ratio of simulated to observed values ranging from 0.5 to 10 in Europe <xref ref-type="bibr" rid="bib1.bibx59" id="paren.7"/>. Similarly, <xref ref-type="bibr" rid="bib1.bibx55" id="text.8"/> evaluated the performance of six BC emission inventories and found an overestimation of modeled BC concentrations by a factor of 1.24 to 2.16 in China. In contrast, some simulations underestimated the annual mean BC levels in China, with normalized mean bias ranging from <inline-formula><mml:math id="M10" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>83 % to <inline-formula><mml:math id="M11" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>22 % <xref ref-type="bibr" rid="bib1.bibx73" id="paren.9"/>. The high uncertainties in the simulation of BC arise from the emission inventory and physical mechanisms. One method to constrain the model results is to use long-term observation datasets to evaluate the emission inventory, transport, and removal processes <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx111 bib1.bibx2 bib1.bibx46 bib1.bibx24" id="paren.10"/>. For instance, <xref ref-type="bibr" rid="bib1.bibx24" id="text.11"/> coupled BC observations with a top-down method to constrain emissions, and the posterior simulated BC concentrations showed better agreement with observations. <xref ref-type="bibr" rid="bib1.bibx16" id="text.12"/> utilized long-term observations of BC to CO ratios to validate the regional emission inventory in Asia. They found that emissions in East and South Korea were overestimated, while emissions in North Korea were underestimated. Using long-term observations of BC and CO from 2009 to 2015 at Fukue Island, <xref ref-type="bibr" rid="bib1.bibx58" id="text.13"/> constrained the wet removal rate of BC and proposed a stretched exponential decay equation to describe the wet removal rate. Based on BC observations from 2010 to 2016 at three representative background sites in East Asia, <xref ref-type="bibr" rid="bib1.bibx15" id="text.14"/> estimated the average transport efficiency of BC to be 0.73, which was lower than the mean rate of 0.91 from the FLEXible PARTicle Lagrangian transport model (FLEXPART, version 10.4).</p>
      <p id="d2e363">Long-term observation of BC aerosol also contributes to a better understanding of the effectiveness of air quality management <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx32 bib1.bibx34" id="paren.15"/>. For instance, a decreasing trend in BC from 2010 to 2014 in London was attributed to the application of diesel particle filters <xref ref-type="bibr" rid="bib1.bibx32" id="paren.16"/>. Long-term observation of BC at 16 sites from 2009 to 2018 in Germany showed the greatest decreases at roadside and urban background sites, implying strong evidence of reduced traffic emissions in urban areas <xref ref-type="bibr" rid="bib1.bibx102" id="paren.17"/>. The decreasing trend of BC at traffic sites in the Helsinki metropolitan area suggested the success of vehicle exhaust particle mitigation <xref ref-type="bibr" rid="bib1.bibx70" id="paren.18"/>. In China, similar conclusions were drawn. For instance, a 38 % reduction in BC concentration was observed in Beijing between 2005 and 2013, primarily due to the relocation of industries and a decrease in coal and coke consumption <xref ref-type="bibr" rid="bib1.bibx12" id="paren.19"/>. Continuous observations of BC in Beijing from 2012 to 2020 revealed a 71 % reduction, with the largest decrease occurring at night. This suggests that pollution control measures implemented since 2013 have effectively reduced primary emissions <xref ref-type="bibr" rid="bib1.bibx103" id="paren.20"/>. The long-term trend of BC in Wuhan suggested a positive role for pollution control measures across China in reducing BC at the observational site <xref ref-type="bibr" rid="bib1.bibx137" id="paren.21"/>. Continuous observation of BC at Mt. Waliguan showed a decreasing rate of 2 % yr<sup>−1</sup> from 2008 to 2017, reflecting the reduction of BC emissions in China <xref ref-type="bibr" rid="bib1.bibx20" id="paren.22"/>.</p>
      <p id="d2e403">As summarized above, long-term observation of BC is important for improving CTM simulations and evaluating the effectiveness of air pollution control measures on air pollutants. Long-term surface observations of BC aerosol have been widely reported <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx8 bib1.bibx60" id="paren.23"/>. For instance, the earliest continuous in situ observation of BC was launched at 150 urban and rural stations in 1962 in the United Kingdom <xref ref-type="bibr" rid="bib1.bibx82" id="paren.24"/>. Compared to long-term observations at a single or a small number of stations, a monitoring network consisting of many stations can provide more information about the spatial-temporal variations of air pollutants. However, long-term in situ observation networks are few. At present, the worldwide monitoring networks include the World Meteorological Organization Global Atmosphere Watch (WMO-GAW) <xref ref-type="bibr" rid="bib1.bibx7" id="paren.25"/>, European Monitoring and Evaluation Programme (EMEP) <xref ref-type="bibr" rid="bib1.bibx122" id="paren.26"/>, German Ultrafine Aerosol Network (GUAN) <xref ref-type="bibr" rid="bib1.bibx4" id="paren.27"/>, UK Black Carbon Network <xref ref-type="bibr" rid="bib1.bibx100" id="paren.28"/>, National Air Pollution Monitoring Network (NABEL) in Switzerland <xref ref-type="bibr" rid="bib1.bibx40" id="paren.29"/>, Interagency Monitoring of Protected Visual Environments network (IMPROVE) in the US <xref ref-type="bibr" rid="bib1.bibx71" id="paren.30"/>, Canadian Aerosol Baseline Measurement (CABM) <xref ref-type="bibr" rid="bib1.bibx11" id="paren.31"/>, Aerosol Radiative Forcing over India Network (ARFINET) in India <xref ref-type="bibr" rid="bib1.bibx72" id="paren.32"/>, and China Black Carbon Observational Network (CBNET) <xref ref-type="bibr" rid="bib1.bibx130" id="paren.33"/>. Research from these observational networks is mainly focused on the spatial-temporal variations of BC <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx72 bib1.bibx130 bib1.bibx95" id="paren.34"/>. More valuable information from long-term observations, however, remains untapped.</p>
      <p id="d2e445">Therefore, this study presents a comprehensive BC dataset collected from CBNET covering the period from 2008 to 2020. Spatial-temporal characteristics, sources, and long-term trends of BC are reported. The information behind the results is explored with a focus on three questions: (1) What can we learn from the comparison between BC ground observations and CTM simulations? (2) Can the inter-annual variations of BC be used as an indicator of BC emissions? (3) Which factors dominated the variations of BC in China during the past 13 years? By analyzing the data from continuous measurements of BC in China, this study is expected to provide insights into reducing the uncertainties in BC emissions and simulations from CTMs.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methodology</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Observation sites</title>
      <p id="d2e463">The CBNET, established in 2006, is a part of the China Atmosphere Watch Network (CAWNET). There are 68 stations across China, and the number of stations has increased recently. In this study, 48 sites with observations during 2008–2020 were selected (Fig. S1). According to the land type and surrounding environment, these 48 sites can be divided into baseline (<inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula>), urban (<inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">23</mml:mn></mml:mrow></mml:math></inline-formula>), and rural (<inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">18</mml:mn></mml:mrow></mml:math></inline-formula>) stations <xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx129 bib1.bibx130" id="paren.35"/>. The rural stations are situated around 50–100 km distant from local sources or nearby major cities, and they are positioned at a moderate height above the local elevation of the area. For the urban stations, the sampling heights are deliberately set to be 50–100 m higher than the average elevation of the city. Baseline stations are established in areas remote from strong emission sources and human activities to monitor the long-range transport of BC aerosols and their natural emissions. For instance, the Lin'an (LA) baseline station is situated at an altitude of 139 m a.s.l. in Zhejiang province, positioned approximately 150 km northeast of Shanghai and 50 km west of Hangzhou city. This strategic placement aims to collect samples that represent the entire region rather than just the immediate local surroundings <xref ref-type="bibr" rid="bib1.bibx129" id="paren.36"/>. More details about the selected stations can be found in Table S1.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Instruments and data prepossessing</title>
      <p id="d2e516">The instruments used at each monitoring site are provided in Table S1 in the Supplement. The BC mass concentration was measured by filter-based absorption Aethalometers. Most stations utilized the AE31 to measure BC throughout the entire period (i.e., 2008–2020), and some stations used both the AE31 and AE33 (Table S1). Details about the principles, operations, and algorithms of AE31 and AE33 can be found elsewhere <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx89" id="paren.37"/>. Briefly, ambient aerosol is drawn through a cyclone with a cut-off size of 2.5 <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> at a flow rate of 2–5 L min<sup>−1</sup> and deposited on a quartz fiber tape (AE31) or tetrafluoroethylene-coated glass filter (AE33). Changes in attenuation before and after sampling are measured and converted into aerosol absorption coefficients (<inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), then into mass concentrations using the pre-defined mass attenuation cross-section (for AE31) or mass absorption cross-sections (for AE33) at 7 channels (370, 470, 520, 590, 660, 880, 950 nm). It should be noted that we adopted the acronym MAC throughout this paper to collectively denote both the mass attenuation cross-section and mass absorption cross-section. The BC mass concentration reported by the Aethalometer is referred to as equivalent black carbon (eBC) <xref ref-type="bibr" rid="bib1.bibx86 bib1.bibx96" id="paren.38"/>. However, due to multiple scattering and loading effects, the reported eBC mass concentration differs from that in ambient air. To correct the loading and multiple scattering effects, the parameterization scheme developed by <xref ref-type="bibr" rid="bib1.bibx114" id="text.39"/> was used for <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> reported by AE31. For AE33, the filter loading effect is compensated by a new real-time loading effect compensation algorithm, and the multiple-scattering effect is corrected by a multiple-scattering enhancement correction (<inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx23" id="paren.40"/>. The <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> values differ between AE31 (<inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2.14</mml:mn></mml:mrow></mml:math></inline-formula>) and AE33 (<inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.39</mml:mn></mml:mrow></mml:math></inline-formula>) due to differences in tape materials (quartz fiber for AE31 and tetrafluoroethylene-coated glass filter for AE33). Another factor that influences eBC mass concentration is the MAC, which is determined by particle size, the mixing state of aerosol components, and the morphology of BC particles<xref ref-type="bibr" rid="bib1.bibx6 bib1.bibx7 bib1.bibx123" id="paren.41"/>, and it shows spatial-temporal variations <xref ref-type="bibr" rid="bib1.bibx84 bib1.bibx124 bib1.bibx40 bib1.bibx42 bib1.bibx96" id="paren.42"/>. Therefore, using the nominal MAC from default settings (e.g., 16.6 m<sup>2</sup> g<sup>−1</sup> for AE31 and 7.77 m<sup>2</sup> g<sup>−1</sup> for AE33 at 880 nm) without considering MAC spatial-temporal variability can result in misleading eBC estimations <xref ref-type="bibr" rid="bib1.bibx96" id="paren.43"/>. To minimize the impact of MAC on eBC mass concentration, station-specific MAC values (Table S1) from previous studies <xref ref-type="bibr" rid="bib1.bibx129 bib1.bibx42 bib1.bibx138" id="paren.44"/>, which utilized synchronous measurements of <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and elemental carbon (EC) to derive MAC values, were used.</p>
      <p id="d2e695">Before data analysis, the raw data (5 min for AE31 and 1 min for AE33) acquired from the Aethalometers was checked and the outliers were removed according to the following procedures: (1) negative values of attenuation at time t and the next observation time (e.g., <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> min) were removed at all 7 wavelengths; (2) the observations which failed to comply with the principle that the light absorption decreases with increasing wavelength were removed and hourly mean values of remaining observations were calculated; (3) the outliers of the hourly time series during the entire observation period were removed using the seasonal decomposition algorithm <xref ref-type="bibr" rid="bib1.bibx21" id="paren.45"/>. It should be noted that our method to process the negative value differed from the manufacturer's protocol, which recommends retaining negative values and applying smoothing techniques to exclude anomalous data points. In our method, the negative values were directly removed. This is because the Aethalometer employs the time-differential method to measure the optical attenuation (ATN) at the sampling point and subsequently converts ATN into BC mass concentration. The time-differential method implies that if the difference between the ATN in the current observation period (ATN<sub><italic>t</italic></sub>) and that of the previous observation period (e.g., ATN<sub><italic>t</italic>−5 min</sub>) is negative, the calculated BC mass concentration for period t will be negative. Furthermore, the difference between the ATN in the next observation period (e.g., ATN<sub><italic>t</italic>+5 min</sub>) and that at time <inline-formula><mml:math id="M33" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> (ATN<sub><italic>t</italic></sub>) will be overestimated, consequently resulting in an overestimation of the BC concentration at time <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> min. The absorption Ångström exponent of aerosol was calculated using the power law fitting between <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and wavelengths at seven wavelengths and reported as AAE<sub>370–950</sub>. Observations with a <italic>p</italic>-value for fitting higher than 0.001 were considered as outliers and excluded from further analysis.</p>
      <p id="d2e808">After data quality control, the data availability in each station of each year was calculated (Fig. S2). To get robust spatial-temporal variations of BC, the stations with annual data records exceeding 50 % were used. The 50 % threshold was selected to maximize the inclusion of monitoring stations while ensuring the collected data effectively captures the temporal variations of BC. To ensure data robustness, systematic screening criteria were applied: (1) long-term trend analysis required stations with more than 8 years of eBC observations, each year maintaining <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> % data availability; (2) spatial-temporal pattern analysis included stations with more than 2 years of valid observations during 2015 and 2017, where annual data completeness exceeded 50 %. According to these rules, 34 and 25 stations were selected for spatial-temporal and long-term trend analysis, respectively (Fig. <xref ref-type="fig" rid="F1"/>). It should be noted that data from other stations with data availability higher than 50 % were also used (e.g., Sect. 4.1 for validation of the BC model simulations).</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e826">Spatial distribution of ground-level black carbon monitoring stations. The dots with white circular frame and white crosses represent the stations used for spatial-temporal variation analysis between 2015 and 2017 (<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">34</mml:mn></mml:mrow></mml:math></inline-formula>) and long-term analysis from 2008 to 2020 (<inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula>), respectively. The colors of the dots indicate different types of stations. The black diagonal line represents the “Hu-Line”, which separates China into eastern and western parts. The red polyline represents the “Qinling-Huaihe Line”, which separates China into northern and southern parts. The full names of acronyms can be found in Table S1.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Aethalometer model and eBC source apportionment</title>
      <p id="d2e867">BC is formed via the combustion processes of carbonaceous matter and is mainly from residential, power, industrial, and transport sectors <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx63 bib1.bibx75" id="paren.46"/>. To apportion the sources of BC, an Aethalometer model using aerosol absorption measurements at two wavelengths was developed by <xref ref-type="bibr" rid="bib1.bibx94" id="text.47"/>. The Aethalometer model operates on the assumption that light-absorbing aerosols originate predominantly from two source types <xref ref-type="bibr" rid="bib1.bibx94" id="paren.48"/>, e.g., liquid fuel combustion and solid fuel combustion, which are characterized by distinct Absorption Ångström Exponent (AAE) values. Aerosols derived from solid fuel combustion (AAE<sub>sf</sub>) generally exhibit higher and more variable AAE values compared to those from liquid fuel combustion (AAE<sub>lf</sub>). The elevated AAE<sub>sf</sub> values are attributed to the presence of significant amounts of organic carbon species, which absorb strongly in the ultraviolet and lower visible wavelength ranges <xref ref-type="bibr" rid="bib1.bibx94" id="paren.49"/>. In contrast, the lower AAE<sub>lf</sub> values result from the dominant contribution of BC, which absorbs light broadly across the visible spectrum. These source-specific AAE characteristics are consistent with laboratory combustion experiments, which also report higher AAE values for solid fuel emissions and lower values for liquid fuel emissions <xref ref-type="bibr" rid="bib1.bibx83" id="paren.50"/>. Consequently, measured ambient AAE values can serve as an indicator of dominant BC sources, e.g., lower AAE values are typically associated with environments strongly influenced by liquid fuel combustion, such as road tunnels <xref ref-type="bibr" rid="bib1.bibx5" id="paren.51"/>.</p>
      <p id="d2e925">This method has been widely used in eBC source apportionment <xref ref-type="bibr" rid="bib1.bibx45 bib1.bibx136 bib1.bibx137 bib1.bibx138 bib1.bibx95" id="paren.52"/>, and the results of this method are generally consistent with other methods, e.g., receptor models <xref ref-type="bibr" rid="bib1.bibx30 bib1.bibx49 bib1.bibx67" id="paren.53"/>. In this study, eBC was apportioned into solid fuel combustion (eBC<sub>sf</sub>) and liquid fossil fuel combustion (eBC<sub>lf</sub>) rather than biomass burning (eBC<sub>bb</sub>) and fossil fuel combustion (eBC<sub>ff</sub>) as reported by previous studies conducted in China <xref ref-type="bibr" rid="bib1.bibx137 bib1.bibx112 bib1.bibx118 bib1.bibx28" id="paren.54"/>. The rationale for differentiating eBC into solid fuel (e.g., coal and biomass) combustion and liquid fossil fuel combustion (e.g., vehicle emissions) was based on the following reasons. (1) Bottom-up BC emission inventories showed that BC from coal, solid bio-fuel, and liquid fossil combustion contributed 28.6 %, 19.6 %, and 28.0 %, respectively, to total emissions (Fig. S3a). The discrepancy between the fraction of solid fuel combustion emissions and the attribution of eBC to eBC<sub>sf</sub> results (48.2 % vs. 48.2 <inline-formula><mml:math id="M49" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 7.14 %) was smaller than that between biomass burning emissions and the attribution of eBC to eBC<sub>bb</sub> results (19.6 % vs. 48.2 <inline-formula><mml:math id="M51" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 7.14 %). (2) Based on experimental measurements of the AAE conducted on various aerosol types (Fig. S3b), the discrepancy between AAE values for aerosols from biomass burning and coal combustion (1.76 <inline-formula><mml:math id="M52" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.40 vs. 1.47 <inline-formula><mml:math id="M53" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13) was smaller than that between liquid fossil fuel and solid fossil fuel combustion (1.00 <inline-formula><mml:math id="M54" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.04 vs. 1.47 <inline-formula><mml:math id="M55" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13). Given these two reasons, eBC was apportioned into eBC<sub>sf</sub> and eBC<sub>lf</sub> in this study.</p>
      <p id="d2e1047">The two key issues of using the Aethalometer model are the selection of the wavelengths and the AAE for aerosol from liquid fossil fuel combustion and solid fuel combustion. According to <xref ref-type="bibr" rid="bib1.bibx145" id="text.55"/>, wavelength of 470 nm as a near-ultraviolet wavelength is recommended while the choice between 950 and 880 nm in the near-infrared is less critical. Following previous studies <xref ref-type="bibr" rid="bib1.bibx94 bib1.bibx145" id="paren.56"/>, wavelengths of 470 and 950 nm were chosen in this study. The selection of AAE<sub>lf</sub> and AAE<sub>sf</sub>, however, is more complicated. The AAE is used to describe the wavelength dependence of aerosol absorption. Although the aerosol AAE is impacted by particle size <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx65" id="paren.57"/>, chemical composition <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx121" id="paren.58"/>, and morphology <xref ref-type="bibr" rid="bib1.bibx68 bib1.bibx62" id="paren.59"/>, it can act as a proxy of aerosol composition <xref ref-type="bibr" rid="bib1.bibx120 bib1.bibx92" id="paren.60"/>. As summarized in previous studies <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx138" id="paren.61"/>, aerosol from liquid fossil fuel combustion has an AAE value of <inline-formula><mml:math id="M60" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1.0, while aerosol from solid fuel combustion is characterized by a higher AAE value. Different methods were used to constrain the optimal AAE combinations, and it showed spatial heterogeneity <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx3 bib1.bibx145 bib1.bibx47 bib1.bibx79 bib1.bibx138" id="paren.62"/>. Due to the lack of auxiliary measurements (e.g., radiocarbon, levoglucosan, and potassium) to constrain the station-specific AAE combination, the measured aerosol AAE frequency distribution <xref ref-type="bibr" rid="bib1.bibx106 bib1.bibx91 bib1.bibx80 bib1.bibx97" id="paren.63"/> was used to select the station-specific AAE<sub>lf</sub> and AAE<sub>sf</sub> values here. Specifically, the AAE<sub>lf</sub> and AAE<sub>sf</sub> were determined as the 1st and 99th percentiles of aerosol AAE, respectively. It should be noted that aerosol AAE was determined by power law fitting between light absorptions and wavelengths, and the fittings with the determinate coefficient (<inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) less than 0.99 were excluded <xref ref-type="bibr" rid="bib1.bibx97" id="paren.64"/>. By this method, the station-specific AAE values for the Aethalometer model were determined (Table S2). Compared to the default AAE values (AAE<inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mi mathvariant="normal">lf</mml:mi></mml:msub><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 1.0, AAE<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mi mathvariant="normal">sf</mml:mi></mml:msub><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 2.0), applying station-specific AAE values resulted in a mean change of 22.3 <inline-formula><mml:math id="M68" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 8.10 % in the fractions of eBC<sub>sf</sub> and eBC<sub>lf</sub> across most stations (Table S2). The source apportionment using station-specific AAE values better matched the proportions of BC from different fuel types in China (Fig. S3a). Validation against dual-carbon isotope data from previous studies <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx81" id="paren.65"/> supports the use of station-specific AAE values. As shown in Fig. S4a, compared to results using default AAE values, the eBC<sub>sf</sub> fraction calculated with station-specific AAE values showed a stronger Pearson correlation (<inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.37 vs. 0.20) with the solid-fuel combustion fraction (coal + biomass) determined by dual-carbon isotopes. Seasonal patterns of eBC<sub>sf</sub> derived from the Aethalometer model were consistent with those from carbon isotope analysis (Fig. S4b). Therefore, station-specific AAE values were adopted for BC source apportionment in this study.</p>
      <p id="d2e1236">While using station-specific AAE values derived from percentiles improved agreement with dual-carbon isotope results, the Aethalometer model still has several uncertainties. These include sensitivity to wavelength selection, the choice between fixed and variable AAE values, measurement noise, interference from non-BC absorbing components, source-specific variability, and limitations in temporal resolution <xref ref-type="bibr" rid="bib1.bibx138 bib1.bibx97" id="paren.66"/>. The percentile-based approach is especially sensitive to sources with high brown carbon content (such as coal combustion) and complex source mixtures <xref ref-type="bibr" rid="bib1.bibx97" id="paren.67"/>. Due to the unknown of the “real” BC source apportionment results, the accuracy of the Aethalometer model was assessed through error propagation <xref ref-type="bibr" rid="bib1.bibx74 bib1.bibx137" id="paren.68"/>. The primary sources of uncertainty considered were the absorption coefficient and the AAE values. The uncertainty of <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mi mathvariant="normal">abs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was reported as 5 % <xref ref-type="bibr" rid="bib1.bibx44" id="paren.69"/> and this value was adopted for this study. For the uncertainty of AAE values, their uncertainties were defined as the difference between the values derived from the percentile method and the isotope-constrained values from <xref ref-type="bibr" rid="bib1.bibx145" id="text.70"/>, e.g., 0.90 for AAE<sub>lf</sub> and 1.68 for AAE<sub>wb</sub>. This approach was justified as the mean optimal AAE<sub>lf</sub> and AAE<sub>sf</sub> values obtained here (0.90 <inline-formula><mml:math id="M78" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.05 and 1.70 <inline-formula><mml:math id="M79" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.23, respectively) were closely aligned with the literature values. The error propagation analysis revealed station-specific relative uncertainties in the range of 19.8 %–53.8 % for eBC<sub>sf</sub> and 23.7 %–54.0 % for eBC<sub>lf</sub> (Table S3). The reported uncertainties here were comparable to previous studies, e.g., 41 % for fossil fuel combustion and 42 % for wood burning estimated by <xref ref-type="bibr" rid="bib1.bibx74" id="text.71"/>. Despite the relatively high estimated uncertainty, the spatial and temporal patterns of BC sources resolved from the Aethalometer model were believed reliable here.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Weather normalization of eBC and its sources</title>
      <p id="d2e1340">To normalize the impact of meteorological conditions on variations in eBC and its sources, a machine learning method <xref ref-type="bibr" rid="bib1.bibx39" id="paren.72"/> was used in this study. According to previous research <xref ref-type="bibr" rid="bib1.bibx140" id="paren.73"/>, the random forest (RF) model with hyperparameters tuned during model training and temporal variables excluded in weather normalization can reduce the bias in long-term trends of air pollutants. We adopted these recommendations to normalize the impact of weather on BC and its sources at each station. The entire observation dataset was divided into two parts: 70 % was used to train the model, and the remaining 30 % was used to evaluate model performance. The variables used to train the model included meteorological conditions, temporal variables, and a transport indicator. Specifically, temperature at 2 m (t2m), surface pressure (sp), wind components at 10 m (u10, v10), relative humidity (rh), accumulated precipitation along the trajectory (apt), boundary layer height (blh), surface downward solar radiation (ssr), and total cloud cover (tcc) were used. The temporal variables included Unix time (number of seconds since 1 January 1970) as a linear trend term, Julian day (day of the year) as the seasonal term, and day of the week. The transport indicator was the cluster category of air masses reaching the observational site, calculated by the Hybrid Single-Particle Lagrangian Integrated Trajectory (HYSPLIT) <xref ref-type="bibr" rid="bib1.bibx101" id="paren.74"/>. Three key hyperparameters, including the number of trees (ntree), the number of variables that may split at each node (mtry), and the minimum size of terminal nodes (min.node.size), were tuned by random search with 5-fold cross-validation after 100 evaluations. The search space was 100–1000, 1–13, and 1–13 for ntree, mtry, and min.node.size, respectively. After tuning, the optimal parameter combination (Table S4) with the lowest root mean square error (RMSE) was used to train the RF model. Although the differences in statistical metrics between the RF model with tuned and untuned parameters were not significant (Fig. S5), the tuned model increased the Pearson correlation coefficient (<inline-formula><mml:math id="M82" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>) and index of agreement (IOA), and reduced the RMSE. For instance, the <inline-formula><mml:math id="M83" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> between observations and modeled eBC increased from 0.64 <inline-formula><mml:math id="M84" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07 (untuned) to 0.66 <inline-formula><mml:math id="M85" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07 (tuned). Therefore, the tuned parameters in Table S4 were used to train the RF model. After training, weather normalization of daily eBC and its sources was achieved by repeatedly resampling predictors and predicting with the trained RF model. For each prediction, the explanatory variables (meteorological conditions) in model training were randomly sampled from the entire dataset without replacement. This predictive process was repeated 1000 times, and the arithmetic mean of these predictions was considered the emission-related concentration <xref ref-type="bibr" rid="bib1.bibx139 bib1.bibx140" id="paren.75"/>.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Auxiliary dataset, data analysis and visualization</title>
      <p id="d2e1393">The auxiliary datasets used in this study included meteorological reanalysis data, surface BC mass concentrations from CTM simulations, and BC emission inventories. Meteorological conditions were obtained from the fifth generation of the European Centre for Medium-Range Weather Forecasts (ECMWF) reanalysis for global climate and weather (ERA5) <xref ref-type="bibr" rid="bib1.bibx50" id="paren.76"/>. Monthly mean surface BC mass concentrations from 2008 to 2020 were sourced from the Modern-Era Retrospective analysis for Research and Applications, Version 2 (MERRA-2) <xref ref-type="bibr" rid="bib1.bibx38" id="paren.77"/> and Tracking Air Pollution in China (TAP) <xref ref-type="bibr" rid="bib1.bibx69" id="paren.78"/>. Additionally, monthly mean BC concentrations from AeroChemMIP, endorsed by the Coupled Model Intercomparison Project 6 (CMIP6), were used in this study. We utilized the historical experiment from CMIP6, which incorporates time-varying emissions of greenhouse gases, aerosols, and ozone, as well as volcanic and solar forcing, spanning the period from 2008 to 2014. Model simulations from the Community Earth System Model 2 (CESM2), Centre National de Recherches Météorologiques (CNRM), Geophysical Fluid Dynamics Laboratory (GFDL), NASA Goddard Institute for Space Studies (GISS), Japan Meteorological Research Institute (MRI), UK Earth System Model (UKESM1) were used here (see Table S5 for details). This dataset provides a comprehensive representation of the key drivers of climate change, allowing assessment of the impacts of both anthropogenic and natural factors on global climate patterns during this period. Yearly BC emission inventories in China were obtained from several datasets, including the Copernicus Atmosphere Monitoring Service (CAMS <xref ref-type="bibr" rid="bib1.bibx41" id="altparen.79"/>), Community Emissions Data System (CEDS <xref ref-type="bibr" rid="bib1.bibx52" id="altparen.80"/>), Emissions Database for Global Atmospheric Research (EDGAR, versions V4.3.2 <xref ref-type="bibr" rid="bib1.bibx17" id="paren.81"/>, V5 <xref ref-type="bibr" rid="bib1.bibx18" id="paren.82"/>, and V6 <xref ref-type="bibr" rid="bib1.bibx77" id="altparen.83"/>), Hemispheric Transport of Air Pollution (HTAP, version V3 <xref ref-type="bibr" rid="bib1.bibx19" id="altparen.84"/>), and the Multi-resolution Emission Inventory model for Climate and air pollution research (MEIC, version 1.4 <xref ref-type="bibr" rid="bib1.bibx36" id="altparen.85"/>).</p>
      <p id="d2e1427">Data analysis was conducted using the <italic>R</italic> language <xref ref-type="bibr" rid="bib1.bibx88" id="paren.86"/>. Outlier detection was performed using the “<italic>anomalize</italic>” package <xref ref-type="bibr" rid="bib1.bibx21" id="paren.87"/>. The “<italic>rmweather</italic>” <xref ref-type="bibr" rid="bib1.bibx39" id="paren.88"/> and “<italic>mlr3</italic>” <xref ref-type="bibr" rid="bib1.bibx61" id="paren.89"/> packages and their extensions were used for weather normalization analysis. Model performance statistics were calculated using “<italic>openair</italic>” <xref ref-type="bibr" rid="bib1.bibx10" id="paren.90"/>. Figures in this study were generated using “ggplot2” <xref ref-type="bibr" rid="bib1.bibx115" id="paren.91"/> and its extensions. Other packages (e.g., “<italic>lubridate</italic>”, “<italic>plyr</italic>”) used in this study are available from the Comprehensive R Archive Network (CRAN, <uri>https://cran.r-project.org</uri>, last access: 3 June 2025).</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Spatial-temporal variations</title>
      <p id="d2e1490">Table S6 summarizes the statistics of eBC mass concentrations, source apportionment results, and AAE<sub>370–950</sub> values at 34 monitoring stations during the study period (2015–2017). The average mass concentrations of eBC, eBC<sub>lf</sub>, and eBC<sub>sf</sub>, as well as AAE<sub>370–950</sub>, were 2.05 <inline-formula><mml:math id="M90" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.85, 1.08 <inline-formula><mml:math id="M91" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.73, 0.97 <inline-formula><mml:math id="M92" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.52 <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, and 1.33 <inline-formula><mml:math id="M95" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.29, respectively. Fig. <xref ref-type="fig" rid="F2"/> shows the spatial distributions of eBC mass concentrations and their source apportionment results between 2015 and 2017. As shown in Fig. <xref ref-type="fig" rid="F2"/>a, BC from MERRA-2 showed higher levels in the east of the “Hu-Line” compared to those west of the line. As shown in Fig. <xref ref-type="fig" rid="F2"/>b, ground observations also showed higher levels in eastern China (2.25 <inline-formula><mml:math id="M96" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.82 <inline-formula><mml:math id="M97" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>) than in western China (1.51 <inline-formula><mml:math id="M99" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.86 <inline-formula><mml:math id="M100" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>). Similarly, the spatial distribution of eBC observations showed higher levels in northern China (2.19 <inline-formula><mml:math id="M102" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3.45 <inline-formula><mml:math id="M103" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>) than in southern China (1.91 <inline-formula><mml:math id="M105" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.05 <inline-formula><mml:math id="M106" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>). The eBC concentrations at different types of stations also showed spatial heterogeneity, with the highest values at urban stations (2.67 <inline-formula><mml:math id="M108" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3.41 <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>), which were significantly higher than those at rural (1.25 <inline-formula><mml:math id="M111" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.50 <inline-formula><mml:math id="M112" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) and baseline (1.07 <inline-formula><mml:math id="M115" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.15 <inline-formula><mml:math id="M116" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>) stations. The percentages of solid fuel combustion in eBC ranged from 33.5 <inline-formula><mml:math id="M119" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 24.9 % to 65.2 <inline-formula><mml:math id="M120" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 24.8 %, with the highest mean value at baseline stations (49.9 <inline-formula><mml:math id="M121" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 10.9 %). Regarding the spatial distribution (Fig. <xref ref-type="fig" rid="F2"/>c), eBC<sub>sf</sub> in eastern China (49.7 <inline-formula><mml:math id="M123" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 7.43 %) and northern China (50.0 <inline-formula><mml:math id="M124" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 7.25 %) were higher than those in western China (44.4 <inline-formula><mml:math id="M125" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 4.55 %) and southern China (46.5 <inline-formula><mml:math id="M126" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 6.77 %) without statistical differences. As shown in Fig. <xref ref-type="fig" rid="F2"/>d, the station-specific AAE<sub>370–950</sub> values were in the range of 1.11 <inline-formula><mml:math id="M128" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13–1.66 <inline-formula><mml:math id="M129" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.40 and the urban stations had the lowest mean values (1.29 <inline-formula><mml:math id="M130" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.11) compared to those in baseline stations (1.40 <inline-formula><mml:math id="M131" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09) and rural stations (1.40 <inline-formula><mml:math id="M132" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.16). Similar to the spatial distribution of eBC<sub>sf</sub>, AAE<sub>370–950</sub> in northern China (1.43 <inline-formula><mml:math id="M135" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12) was significantly higher (<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.001</mml:mn></mml:mrow></mml:math></inline-formula>) than those in southern China (1.24 <inline-formula><mml:math id="M137" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07) and AAE<sub>370–950</sub> in western China (1.44 <inline-formula><mml:math id="M139" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13) was also significantly higher than those in eastern China (1.30 <inline-formula><mml:math id="M140" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12) at 0.01 levels.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e1997">Spatial distributions of mean values of BC concentrations, sources of eBC including solid fuel (eBC<sub>sf</sub>) and liquid fuel (eBC<sub>lf</sub>) combustion, and absorption Ångström exponent between 2015 and 2017 <bold>(a)</bold>, and their box plots <bold>(b)</bold>–<bold>(d</bold>) showing station-specific values for different types of stations, including baseline (B), rural (RU), and urban (U), as well as different regions in China: eastern China (EC), western China (WC), southern China (SC), and northern China (NC). The sizes and colors of the dots in panel <bold>(a)</bold> correspond to the mean values of AAE and eBC, respectively.  The donuts in panel <bold>(a)</bold> represent the source apportionment results of eBC in each station. The data in the filled grid in panel <bold>(a)</bold> is from MERRA-2. NS, <sup>*</sup>, <sup>**</sup>, and <sup>***</sup> in panels <bold>(b)</bold>–<bold>(d)</bold> indicate differences between two paired groups that are not significant (<inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>) or significant at the 0.05, 0.01, and 0.001 levels, respectively.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f02.png"/>

        </fig>

      <p id="d2e2097">The monthly variations of eBC, eBC<sub>sf</sub>, and AAE<sub>370–950</sub> are shown in Fig. <xref ref-type="fig" rid="F3"/>. Generally, the lowest values of eBC (1.46 <inline-formula><mml:math id="M149" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.72 <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>), eBC<sub>sf</sub> (36.3 <inline-formula><mml:math id="M153" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 24.7 %), and AAE<sub>370–950</sub> (1.21 <inline-formula><mml:math id="M155" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.28) occurred during summer (JJA), while the highest values were observed during winter (DJF). The higher values in winter were related to unfavorable meteorological conditions that hindered the dispersion of surface BC. Increased demand for heating also contributed to higher BC levels in winter, as evidenced by higher percentages of eBC<sub>sf</sub> (60.2 <inline-formula><mml:math id="M157" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 22.7 %) and higher AAE<sub>370–950</sub> values (1.45 <inline-formula><mml:math id="M159" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.26). Some stations (e.g., 58370 and 58448), however, showed the highest eBC mass concentrations during May and July. These anomalously high eBC levels were related to biomass burning during the summer harvest season, as indicated by high eBC<sub>sf</sub> percentages. Previous studies also showed that these stations or regions were impacted by biomass burning during the summer harvest <xref ref-type="bibr" rid="bib1.bibx125 bib1.bibx142" id="paren.92"/>. Another station with high levels of AAE<sub>370–950</sub> during summer was Tazhong (51747), which was largely impacted by dusty weather from March to July <xref ref-type="bibr" rid="bib1.bibx143" id="paren.93"/>.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e2243">Monthly variations of black carbon concentrations (eBC, <bold>a</bold>, <bold>b</bold>), the fraction of BC from solid fuel combustion (eBC<sub>sf</sub>, <bold>c</bold>, <bold>d</bold>), and the absorption Ångström exponent calculated by power law fitting at seven wavelengths (AAE<sub>370–950</sub>, <bold>e</bold>, <bold>f</bold>). The filled grids in the left panels represent the scaled monthly values, ranging from 0 to 1 to better show the station-specific monthly variations. Note that the darker the color represents the higher the value.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f03.png"/>

        </fig>

      <p id="d2e2289">To investigate the drivers of spatial-temporal variations in BC, we performed a correlation analysis between BC concentrations, emissions, and meteorological parameters. BC emissions from different fuel types were obtained from CEDS-MAPS, which divides sources into solid bio-fuel, coal, liquid fuel plus natural gas, and process emissions <xref ref-type="bibr" rid="bib1.bibx75" id="paren.94"/>. Meteorological data for 2015–2017 were sourced from the ERA5 reanalysis dataset <xref ref-type="bibr" rid="bib1.bibx50" id="paren.95"/>. As shown in Fig. S6, mean BC concentrations during 2015–2017 were positively correlated with emissions at most stations (<inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">32</mml:mn></mml:mrow></mml:math></inline-formula>), with Pearson coefficients of 0.65 for eBC, 0.56 for eBC<sub>sf</sub>, and 0.58 for eBC<sub>lf</sub>. This significant correlation indicates that the spatial distribution of BC closely follows its emission patterns, which are higher in northern and eastern China <xref ref-type="bibr" rid="bib1.bibx110" id="paren.96"/>. On a monthly scale, BC concentrations were positively correlated with emissions and negatively correlated with ambient temperature, boundary layer height, and wind speed at most stations (Fig. S6). Elevated BC levels in colder months were attributed to increased heating-related emissions and less favorable dispersion conditions (lower boundary layer height and wind speed) <xref ref-type="bibr" rid="bib1.bibx130 bib1.bibx117" id="paren.97"/>. Overall, both emission patterns and meteorological factors jointly controlled the spatial-temporal variability of BC in China.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Long-term trends from 2008 to 2020</title>
      <p id="d2e2343">Figure <xref ref-type="fig" rid="F4"/> shows the time series of eBC, eBC<sub>lf</sub>, and eBC<sub>sf</sub> from 2008 to 2020. Despite eBC and its sources showing overall decreasing trends from 2008 to 2020, the year with peak values differed among the different types of stations. As shown in Fig. <xref ref-type="fig" rid="F4"/>a, the annual mean concentrations of eBC and its sources at urban stations increased from 2008 to 2012 and then showed a downward trend to 2020. The inter-annual variations of eBC, eBC<sub>lf</sub>, and eBC<sub>sf</sub> at rural stations showed peak values in 2009 and then continuously decreased until 2020. At baseline stations, eBC and its sources also showed downward trends with fewer variations compared to those at urban and rural stations. Using the Theil-Sen method, the slopes of eBC and its sources at each station were calculated. As listed in Table S7, most stations showed decreasing trends, while only a few sites (e.g., Yushe in Shanxi province) exhibited an increasing trend. The stations with decreasing trends had a mean slope of <inline-formula><mml:math id="M171" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.17 <inline-formula><mml:math id="M172" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.20 <inline-formula><mml:math id="M173" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> for eBC, <inline-formula><mml:math id="M176" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.12 <inline-formula><mml:math id="M177" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.14 <inline-formula><mml:math id="M178" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> for eBC<sub>lf</sub>, and <inline-formula><mml:math id="M182" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.06 <inline-formula><mml:math id="M183" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09 <inline-formula><mml:math id="M184" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> for eBC<sub>sf</sub>, respectively. Regarding the trends in the different types of stations (Fig. <xref ref-type="fig" rid="F4"/>b), eBC in urban stations (N = 14) showed the fastest decreasing rate with a slope of <inline-formula><mml:math id="M188" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.20 <inline-formula><mml:math id="M189" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.23 <inline-formula><mml:math id="M190" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>, which was quicker than that in rural stations (<inline-formula><mml:math id="M193" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.17 <inline-formula><mml:math id="M194" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.21 <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>, <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula>) and baseline stations (<inline-formula><mml:math id="M199" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.10 <inline-formula><mml:math id="M200" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07 <inline-formula><mml:math id="M201" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>, <inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>). Similarly, as shown in Fig. <xref ref-type="fig" rid="F4"/>d, eBC<sub>lf</sub> also showed the fastest decreasing rates in urban stations (<inline-formula><mml:math id="M206" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.15 <inline-formula><mml:math id="M207" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.16 <inline-formula><mml:math id="M208" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>), followed by rural stations (<inline-formula><mml:math id="M211" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.09 <inline-formula><mml:math id="M212" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.12 <inline-formula><mml:math id="M213" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>) and baseline stations (<inline-formula><mml:math id="M216" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.05 <inline-formula><mml:math id="M217" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.04 <inline-formula><mml:math id="M218" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>). The decreasing rates of eBC<sub>sf</sub> in baseline (<inline-formula><mml:math id="M222" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.05 <inline-formula><mml:math id="M223" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.04 <inline-formula><mml:math id="M224" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>) and urban stations (<inline-formula><mml:math id="M227" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.06 <inline-formula><mml:math id="M228" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10 <inline-formula><mml:math id="M229" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>) were larger than those in rural stations (<inline-formula><mml:math id="M232" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>0.08 <inline-formula><mml:math id="M233" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09 <inline-formula><mml:math id="M234" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup>). The differences in trends of eBC, eBC<sub>lf</sub>, and eBC<sub>sf</sub> between southern/western China and northern/eastern China showed no statistical significance, but higher decreasing rates were found in southern China and western China (Fig. S7).</p>

      <fig id="F4"><label>Figure 4</label><caption><p id="d2e3058">Annual concentrations of black carbon <bold>(a)</bold>, black carbon from liquid fossil fuel combustion (eBC<sub>lf</sub>, <bold>c</bold>), and solid fuel combustion (eBC<sub>sf</sub>, <bold>e</bold>) from 2008 to 2020 and box plots <bold>(b, d, f)</bold> of their trends in different types of stations including baseline (B), rural (RU), and urban (U) stations. The solid line in panels <bold>(a)</bold>, <bold>(c)</bold>, and <bold>(e)</bold> represents the annual mean values, and the filled ribbons represent the 99 % confidence intervals of mean values.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f04.png"/>

        </fig>

      <p id="d2e3107">Long-term observational studies across China have widely reported decreases in BC concentrations over various periods. For example, BC concentrations in Beijing declined at an average rate of 0.19 <inline-formula><mml:math id="M241" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>  per year between 2013 and 2022 <xref ref-type="bibr" rid="bib1.bibx117" id="paren.98"/>. Similarly, an annual decrease of 0.10 <inline-formula><mml:math id="M243" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>  was observed in Nanjing from 2014 to 2021 <xref ref-type="bibr" rid="bib1.bibx1" id="paren.99"/>, while a trend of <inline-formula><mml:math id="M245" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.12 <inline-formula><mml:math id="M246" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> was recorded at Mt. Lushan from 2008 to 2022 <xref ref-type="bibr" rid="bib1.bibx66" id="paren.100"/>. These single-site observations consistently highlight the effectiveness of air pollution control policies in reducing BC concentrations. Our study reinforces these findings from a broader spatial perspective, confirming that the observed reduction in BC levels can be attributed to the implementation of national regulatory measures, such as the China Clean Air Action Plan and the Three-Year Action Plan.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Comparison with global observations</title>
      <p id="d2e3213">To better understand the levels of eBC and its characteristics in China, the results from this study were compared to those from other regions during the same observational period (2015–2017) on a global scale. Specifically, the observations were sourced from published papers, observation networks, and publicly accessible websites. Data for European countries and the US were obtained from EBAS (<uri>https://ebas-data.nilu.no/Default.aspx</uri>, last access: 18 July 2025) and the US EPA (<uri>https://aqs.epa.gov/aqsweb/airdata/download_files.html</uri>, last access: 18 July 2025), respectively. The location, station type, and instruments used in these observations are listed in Table S8. The data processing procedures for these observational datasets are described in Section S1 in the Supplement. Briefly, by harmonizing wavelengths, MAC, and AAE combinations, biases were minimized to ensure reliable comparisons.</p>
      <p id="d2e3222">Figure <xref ref-type="fig" rid="F5"/> shows the global distributions of mass concentrations of eBC, eBC<sub>sf</sub> percentages, and AAE values from previous studies or observation networks during 2015 and 2017. Despite differences among the sampling inlets and monitoring instruments (Table S8), the mean values of eBC observations in China (2.04 <inline-formula><mml:math id="M250" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.53 <inline-formula><mml:math id="M251" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">35</mml:mn></mml:mrow></mml:math></inline-formula>) were significantly lower than those in India (6.30 <inline-formula><mml:math id="M254" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 4.12 <inline-formula><mml:math id="M255" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">23</mml:mn></mml:mrow></mml:math></inline-formula>) at the 0.001 levels, but significantly higher than those in the UK (1.22 <inline-formula><mml:math id="M258" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.10 <inline-formula><mml:math id="M259" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">14</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.05), Spain (1.07 <inline-formula><mml:math id="M263" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.98 <inline-formula><mml:math id="M264" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.05), US (0.83 <inline-formula><mml:math id="M268" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.63 <inline-formula><mml:math id="M269" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M271" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">65</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M272" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.001), Germany (0.74 <inline-formula><mml:math id="M273" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.64 <inline-formula><mml:math id="M274" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M276" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M277" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.001), and Switzerland (0.61 <inline-formula><mml:math id="M278" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.47 <inline-formula><mml:math id="M279" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, <inline-formula><mml:math id="M281" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.001). Regarding BC from solid fuel combustion derived from the Aethalometer model, the results are influenced by the choice of wavelength pair and AAE combination. Other factors such as station type (e.g., background vs. traffic), instruments, and sampling inlets also impact the Aethalometer model results. The comparison here used an AAE combination of 1.0 for AAE<sub>lf</sub>, 2.0 for AAE<sub>sf</sub>, and the wavelength pair of 370 nm and 880 nm to minimize the influence of AAE combination and wavelength pair selection on source apportionment results. As shown in Fig. <xref ref-type="fig" rid="F5"/>e, eBC<sub>sf</sub> had the highest contribution in the US (30.2 <inline-formula><mml:math id="M286" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 12.8 %, <inline-formula><mml:math id="M287" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula>), which was higher than that in this study (28.1 <inline-formula><mml:math id="M288" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 10.9 %, <inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">34</mml:mn></mml:mrow></mml:math></inline-formula>). The lowest contribution of eBC<sub>sf</sub> was found in Spain (13.3 <inline-formula><mml:math id="M291" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 5.51 %, <inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>), which was lower than that in China (<inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo></mml:mrow></mml:math></inline-formula> 0.05). Similar to the spatial distribution of eBC<sub>sf</sub>, AAE also showed the highest value in the US (1.40 <inline-formula><mml:math id="M295" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.13, <inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">26</mml:mn></mml:mrow></mml:math></inline-formula>) and the lowest value in Spain (1.21 <inline-formula><mml:math id="M297" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.06, <inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>). The comparison of eBC trends between this study and other observations from 2008 to 2020 is shown in Fig. <xref ref-type="fig" rid="F6"/>. Results from 88 stations (34 in this study and 54 from other observations) showed widespread decreasing trends of eBC in most stations (<inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">83</mml:mn></mml:mrow></mml:math></inline-formula>), with mean trends of <inline-formula><mml:math id="M300" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.36 <inline-formula><mml:math id="M301" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3.06 % yr<sup>−1</sup>. The slopes for eBC from 2008 to 2020 showed the fastest decreasing trend in the UK (<inline-formula><mml:math id="M303" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>5.94 <inline-formula><mml:math id="M304" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.26 % yr<sup>−1</sup>, <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula>) and the slowest decreasing trend in the US (<inline-formula><mml:math id="M307" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>2.61 <inline-formula><mml:math id="M308" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.04 % yr<sup>−1</sup>, <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">18</mml:mn></mml:mrow></mml:math></inline-formula>). The eBC decreasing rates in Germany (<inline-formula><mml:math id="M311" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>4.93 <inline-formula><mml:math id="M312" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.51 % yr<sup>−1</sup>, <inline-formula><mml:math id="M314" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">16</mml:mn></mml:mrow></mml:math></inline-formula>) and Switzerland (<inline-formula><mml:math id="M315" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>5.66 <inline-formula><mml:math id="M316" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 5.44 % yr<sup>−1</sup>, <inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula>) were also faster than those in this study for China (<inline-formula><mml:math id="M319" display="inline"><mml:mo lspace="0mm">-</mml:mo></mml:math></inline-formula>3.98 <inline-formula><mml:math id="M320" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 3.41 % yr<sup>−1</sup>, <inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">25</mml:mn></mml:mrow></mml:math></inline-formula>).</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e3969">Spatial distributions and box plots in black carbon concentrations <bold>(a, d)</bold>, black carbon from solid fuel combustion <bold>(b, e)</bold>, and absorption Ångström exponent <bold>(c, f)</bold> during 2015–2017. The filled base maps of panels <bold>(a)</bold> and <bold>(c)</bold> are from MERRA-2 and the base map of panel <bold>(b)</bold> is from CEDS-MAPS <xref ref-type="bibr" rid="bib1.bibx75" id="paren.101"/>. The dots in panels <bold>(a)</bold>–<bold>(c)</bold> represent the observation values (see Table S8 for details) and the size of each dot is mapped to its value. Panels <bold>(d)</bold>–<bold>(f)</bold> are box plots of observations in different countries including India (IN), Switzerland (CH), China (CN), United Kingdom (UK), Spain (ES), Germany (DE), and the United States (US).</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f05.png"/>

        </fig>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e4015">Spatial distribution of black carbon concentration trends <bold>(a)</bold> and box plots of trends in different countries <bold>(b)</bold> from 2008 to 2020. The size of dots in panel <bold>(a)</bold> corresponds to the absolute value of slope. The fill color in panel <bold>(b)</bold> corresponds to the mean slope value in each country. Detailed information about slopes at each station can be found in Table S9.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f06.png"/>

        </fig>

      <p id="d2e4036">This international comparison provides a global context for evaluating China's BC concentrations and trends, allowing for direct comparison with both developing countries (e.g., India) and developed countries (e.g., the United States, United Kingdom, Germany, Switzerland). The results highlight that while China achieved reductions in BC concentration, its concentrations still remain higher, and its rates of decline were slower than those observed in developed nations. In these countries, rapid BC reductions have been achieved through the implementation of stringent regulations <xref ref-type="bibr" rid="bib1.bibx70" id="paren.102"/> and the adoption of cleaner technologies <xref ref-type="bibr" rid="bib1.bibx32" id="paren.103"/>. These findings underscore the need for continued policy efforts in China, particularly targeting industrial and residential sources, and support the refinement of emission inventories to further reduce BC emissions.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Comparison with CTM simulations</title>
      <p id="d2e4061">Due to the lack of long-term global-scale observations, knowledge of atmospheric BC abundance continues to rely on CTM simulations. Therefore, it is important to evaluate the performance of CTMs in simulating the spatial-temporal variations of BC. Owing to the availability of long-term BC observations in China, the BC simulation results from different models (see Sect. 2.5 for details) were evaluated in this study. Regarding model performance in simulating the spatial distribution of BC, these models showed high values in East China, which were consistent with ground observations (Fig. <xref ref-type="fig" rid="F7"/>). The <inline-formula><mml:math id="M323" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> between mean values of simulations and observations from 2008 to 2014 ranged from 0.51 (MRI) to 0.70 (TAP). Compared to the observations, the CTMs underestimated the surface BC mass concentrations by 80.8 % (GISS) to 42.1 % (UKEMS1) in China from 2008 to 2014. The underestimation of surface BC concentrations by CTMs has been widely reported elsewhere <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx33 bib1.bibx73 bib1.bibx87" id="paren.104"/>. Among the different types of stations, the CTMs showed the highest performance in reproducing the surface BC concentrations at baseline stations (<inline-formula><mml:math id="M324" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.83 <inline-formula><mml:math id="M325" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.07, slope <inline-formula><mml:math id="M326" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.88 <inline-formula><mml:math id="M327" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.42), followed by urban (<inline-formula><mml:math id="M328" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.65 <inline-formula><mml:math id="M329" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10, slope <inline-formula><mml:math id="M330" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.44 <inline-formula><mml:math id="M331" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.26), and rural stations (<inline-formula><mml:math id="M332" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.20 <inline-formula><mml:math id="M333" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.10, slope <inline-formula><mml:math id="M334" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.13 <inline-formula><mml:math id="M335" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.08). The higher performance of CTMs in simulating BC in urban areas compared to rural areas is related to uncertainty in BC emissions. For instance, BC is mainly from vehicle exhaust in urban areas and is dominated by biomass burning and coal combustion in rural regions. The uncertainty in BC emission factors for gasoline and diesel vehicles is lower than that for biomass burning <xref ref-type="bibr" rid="bib1.bibx93" id="paren.105"/>. As a result, BC emissions in urban areas show less uncertainty <xref ref-type="bibr" rid="bib1.bibx133 bib1.bibx126" id="paren.106"/>, and simulations from CTMs produce less deviation from observations in urban areas.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e4179">Spatial distributions of surface BC observations and simulations from different chemical transport models during 2008–2014 and the statistical metrics of model performance. The NMB and IOA represent normalized mean bias and index of agreement, respectively.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f07.png"/>

        </fig>

      <p id="d2e4188">Regarding the temporal variations of BC in China, the simulations from CMIP6, MERRA-2, and TAP showed similar monthly variations, with higher concentrations in winter and lower values in summer (Fig. <xref ref-type="fig" rid="F8"/>a). The <inline-formula><mml:math id="M336" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> between CTMs and observations ranged from 0.63 (GISS) to 0.87 (MERRA-2) on a monthly resolution. On the annual scale (Fig. <xref ref-type="fig" rid="F8"/>b), except for TAP, annual concentrations of BC from CMIP6 historical experiments and MERRA-2 showed increasing trends from 2008 to 2014, while the ground observations and TAP showed decreasing trends in China. Except for TAP and MERRA-2, the correlations between observations and CMIP6 results were negative at the annual scale (Fig. <xref ref-type="fig" rid="F8"/>d), suggesting these models failed to reproduce the yearly variations of surface BC. The upward trends of BC from CMIP6 historical experiments and MERRA-2 were related to their inter-annual BC emissions, which also showed increasing trends from 2008 to 2014 in China (Fig. S8). Similarly, the downward trends of surface BC concentrations from TAP were also in accordance with their emissions (MEIC), which showed a decreasing trend from 2008 to 2014 (Fig. S8). The opposite BC trends between ground observations and model simulations from CMIP6 in this study were similar to previous studies <xref ref-type="bibr" rid="bib1.bibx130 bib1.bibx90" id="paren.107"/>. For instance, aerosol optical depth from observations showed a decrease, while CMIP6 simulations showed increasing trends during 2002–2018 in China <xref ref-type="bibr" rid="bib1.bibx90" id="paren.108"/>. Therefore, caution should be exercised when interpreting the temporal variations of aerosols using simulations from CMIP6.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e4214">Monthly <bold>(a)</bold> and inter-annual <bold>(c)</bold> variations of BC observations and surface BC simulations from different chemical transport models during 2008–2014, and their Taylor Diagrams showing model performance at monthly <bold>(b)</bold> and yearly <bold>(d)</bold> scales.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f08.png"/>

        </fig>

      <p id="d2e4235">Due to the chemical inertness of BC particles, the deviations between observations and simulations arise from uncertainties in two aspects: emissions and deposition <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx27" id="paren.109"/>. The underestimation of BC emissions in China results in lower simulations of BC by CTMs. For instance, BC simulations were underestimated by 35 %–60 % in different seasons using the bottom-up BC emissions in China, while the CTM showed better performance with BC underestimated only by 22 %–9 % using the top-down constrained emissions (1.59 times higher than bottom-up emissions) <xref ref-type="bibr" rid="bib1.bibx33" id="paren.110"/>. Similarly, the RMSE for annual BC simulation decreased by 31.6% if the BC emissions in China increased by 1.8 times <xref ref-type="bibr" rid="bib1.bibx109" id="paren.111"/>. Using the MEIC instead of the emissions inventory for the Intergovernmental Panel on Climate Change Fifth Assessment Report (BC emissions increased by 13.4 %), the CTM improved the BC concentrations by 42.6 % <xref ref-type="bibr" rid="bib1.bibx26" id="paren.112"/>. Despite the increase of BC emissions in CTMs, the models still underestimated the BC concentrations, suggesting an overestimation of BC deposition within CTMs. For instance, a better agreement between observations and simulations was achieved by reducing the BC dry deposition velocity by 50 % <xref ref-type="bibr" rid="bib1.bibx53" id="paren.113"/>. Similarly, using the lower dry deposition, the CTM simulations resulted in a lower global mean BC dry deposition flux and a higher correlation between simulations and observations <xref ref-type="bibr" rid="bib1.bibx116" id="paren.114"/>. The observations also suggested an overestimation of the BC aging degree in the CTMs, and sensitive simulations showed that slowing down the BC aging degree in model simulation can reduce the large model bias in the simulation of surface BC concentration over China <xref ref-type="bibr" rid="bib1.bibx99" id="paren.115"/>.</p>
      <p id="d2e4260">To identify which factor (uncertainty in emission or deposition) makes a greater contribution to the uncertainty of BC simulation, we used the importance of each variable in RF model building (Sect. 2.4). As shown in Fig. S9, generally, date_unix was the variable with the greatest importance for the prediction of eBC, eBC<sub>lf</sub>, and eBC<sub>sf</sub> in the RF model. Additionally, Julian day (seasonal term) had the third largest importance for the prediction of eBC and eBC<sub>lf</sub>, while temperature showed higher importance for the prediction of eBC<sub>sf</sub>. These explanatory variables can serve as proxies for emissions of BC, e.g., more biomass burning during colder months for heating. The explanatory variables related to deposition (e.g., wind speed, precipitation), however, had less importance for prediction. Therefore, emissions were more important than deposition when explaining BC concentrations.</p>
      <p id="d2e4299">The comparison between the observed BC concentration values and simulations suggests that to improve the model's accuracy, more attention should be given to updating the BC emission inventory. Here, we only discuss how to use BC observation data for updating the BC emission inventory, rather than attempting to complete this task. In practice, the BC emission inventory, observed concentrations, FLEXPART simulations, and Bayesian inversion framework can be integrated to update BC emissions <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx25 bib1.bibx56" id="paren.116"/>. For instance, <xref ref-type="bibr" rid="bib1.bibx25" id="text.117"/> used BC observations, outdated prior BC emissions, and an inversion framework to estimate BC emissions during the COVID-19 lockdown in Europe. Their results showed a 23 % decline in BC emissions during the lockdown compared to the same period in the previous five years (2015–2019). Similarly, <xref ref-type="bibr" rid="bib1.bibx56" id="text.118"/> estimated a maximum weekly emission reduction of 70 % in eastern China and 48 % in northern China from 1 January  to 10 March  2020. These studies showed improved accuracy of model simulations using posterior BC emissions compared to the prior emission inventory, highlighting the potential to reduce BC simulation uncertainty by incorporating BC observations and prior emissions.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Weather normalized concentrations: an indicator of BC emissions</title>
      <p id="d2e4319">Using the weather normalization method, the concentrations of eBC and its two sources (eBC<sub>lf</sub> and eBC<sub>sf</sub>) were normalized. Compared to the eBC observations, a higher correlation between weather-normalized eBC concentrations and BC emissions was found (Fig. S10), suggesting that the normalized eBC concentration can better reflect emission variations. Therefore, the weather-normalized eBC concentration was used here to discuss its relationship with BC emissions. As shown in Fig. <xref ref-type="fig" rid="F9"/>a, except for MEIC, BC from other emission inventories showed increasing trends since 2008, reaching peak values in certain years and then decreasing. In contrast, BC emissions from MEIC showed a continuous decrease since 2008, and their inter-annual variation was more consistent with weather-normalized eBC concentrations. In 2010, China began to fight against air pollution, and the Action Plan on the Prevention and Control of Air Pollution and the Three-Year Action Plan were implemented during 2013–2017 and 2018–2020, respectively. As a result of these actions, emission standards and activity levels changed over time. These factors are considered in the MEIC framework, which employs a technology-driven methodology to track China's energy statistics and technological advancements, reflecting shifts in emission characteristics across various sectors, fuels, products, combustion/process technologies, and emission control technologies in recent years <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx135 bib1.bibx36" id="paren.119"/>. Therefore, the BC emissions from MEIC coincided more closely with weather-normalized concentrations. The BC emissions from other inventories, such as CEDS, are not calibrated; instead, they are derived from default emissions using the Speciated Pollutant Emission Wizard, due to the limited availability of national BC inventory estimates in other countries. The similar reduction rates of surface BC concentrations and emissions (53.6 % vs. 51.9 %) and their similar inter-annual variations from 2008 to 2020 in China also suggest that the normalized BC concentrations can be used as a proxy to scale BC emissions in recent years. Updating bottom-up BC emissions is time-consuming, as it requires collecting activity data (e.g., energy consumption). As summarized in Table S8 and mentioned above, there are several BC observation networks worldwide (e.g., UK, US, Germany, and India); the normalized BC observations can be used to calibrate the total BC emissions in these countries.</p>

      <fig id="F9"><label>Figure 9</label><caption><p id="d2e4347">The inter-annual variations of black carbon emissions from different emission inventories and observations (eBC) during 2008–2020 <bold>(a)</bold> and the BC emissions from solid fuel combustion (EMI<sub>sf</sub>) and liquid fossil fuel combustion (EMI<sub>lf</sub>) derived from MEIC and the BC sources including solid fuel combustion (eBC<sub>sf</sub>) and liquid fossil fuel combustion (eBC<sub>lf</sub>) derived from the Aethalometer model <bold>(b)</bold>.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f09.png"/>

        </fig>

      <p id="d2e4399">To further explore whether the weather-normalized BC source contributions can be used as an indicator of BC emissions from different fuel types, the BC emissions from MEIC were used here. The sectors in MEIC (industrial, power, residential, and transportation) were further broken down into fossil fuel (liquid fuel <inline-formula><mml:math id="M347" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> coal) and biomass burning according to <xref ref-type="bibr" rid="bib1.bibx110" id="paren.120"/>. As shown in Fig. <xref ref-type="fig" rid="F9"/>b, the variations of eBC<sub>lf</sub> concentrations from the Aethalometer model aligned with their emissions, showing a continuous reduction from 2008 to 2020. In contrast, the inter-annual variation of eBC<sub>sf</sub> was not in line with its emissions, with a small peak in emissions in 2013, while its concentration continuously decreased since 2008. The higher correlation between eBC<sub>lf</sub> and liquid fuel combustion emissions compared to that between eBC<sub>sf</sub> and solid fuel emissions (Fig. S11) suggests higher uncertainty in BC emissions from solid fuel combustion, as discussed in Sect. 4.1 and previous studies <xref ref-type="bibr" rid="bib1.bibx134 bib1.bibx126" id="paren.121"/>. Therefore, to further improve the accuracy in the BC emission inventory, more attention should be paid to the solid fuel combustion sub-sector, e.g., focusing on surveys of activity rates and measurements of local emission factors <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx57" id="paren.122"/>.</p>
      <p id="d2e4458">Accuracy in sectoral emissions is important to improve the performance of CTMs. Previous studies have demonstrated that uncertainties in BC emission inventory, originating from incomplete activity data, unrepresentative emission factors , and sectoral inconsistencies <xref ref-type="bibr" rid="bib1.bibx63" id="paren.123"/>, will propagate significant biases into chemical transport models. For instance, sectoral uncertainties are pronounced for residential and industrial sources in developing countries due to inconsistent emission factors and activity data. From a modeling perspective, these uncertainties dominate over other processes (e.g., aging, deposition) in near-source regions, while transport and removal uncertainties amplify errors in remote areas <xref ref-type="bibr" rid="bib1.bibx107" id="paren.124"/>. Another study showed that BC simulation was overestimated by a factor of 2.22, which can be attributed to the highest domestic emissions during winter in East Asia <xref ref-type="bibr" rid="bib1.bibx55" id="paren.125"/>. Results from a top-down study showed the largest bias in residential and transportation sectors during January and July, and the bias of BC was reduced using the posterior emission inventory compared to the prior emission inventory <xref ref-type="bibr" rid="bib1.bibx132" id="paren.126"/>.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Drivers of black carbon variations in China</title>
      <p id="d2e4481">Using the weather-normalization method, the contributions of emissions and meteorology to the inter-annual variations of air pollutants can be quantified <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx137 bib1.bibx140" id="paren.127"/>. As shown in Fig. S12, compared to the observations, the emission-related (weather-normalized) concentrations of BC were higher in each year. For instance, the national mean concentrations of emission-related and observed eBC in 2008 were 3.59 and 3.47 <inline-formula><mml:math id="M352" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>, respectively, yielding meteorology-related concentrations of <inline-formula><mml:math id="M354" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.12 <inline-formula><mml:math id="M355" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup>. The negative value of the meteorology-related concentration indicates favorable meteorological conditions for reducing BC concentrations. Similarly, meteorology also contributed to lowering the concentrations of eBC<sub>lf</sub> and eBC<sub>sf</sub> at different types of stations (Fig. S12). To quantify the contributions of emission and meteorology to the reduction of BC concentrations, the slope between weather-normalized and observational trends was used. Results from Fig. <xref ref-type="fig" rid="F10"/>a indicate that the reductions of eBC, eBC<sub>lf</sub>, and eBC<sub>sf</sub> were dominated by emission-related reductions, with relative contributions of 89 %, 87 %, and 62 %, respectively, implying the effectiveness of human efforts in BC emission reduction. These results are consistent with previous studies showing that the inter-annual variations of air pollutants were dominated by emission changes <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx14 bib1.bibx127 bib1.bibx137 bib1.bibx141" id="paren.128"/>. Compared to eBC and eBC<sub>lf</sub>, eBC<sub>sf</sub> was more strongly impacted by variations in meteorological conditions, e.g., more coal and biomass were consumed for heating during colder months. To better understand which sources dominated the reduction of BC, the results from the Aethalometer model were used. As shown in Fig. <xref ref-type="fig" rid="F10"/>b, the slopes of the fittings between eBC<sub>sf</sub> and eBC<sub>lf</sub> in baseline and rural stations were greater than 1, suggesting the dominant role of BC emission reduction from solid fuel in the decreases of ambient eBC concentrations in these two types of regions. In contrast, the slope between eBC<sub>sf</sub> and eBC<sub>lf</sub> in urban stations was less than 1, suggesting the dominant role of BC emission reductions from liquid fuel (e.g., vehicle emissions) in the decrease of eBC concentration in urban areas. The control measures related to BC emission reductions include stricter vehicle emission and industrial standards, eliminating outdated industrial capacity, prohibiting agricultural residue burning and scattered coal combustion, and replacing coal with natural gas and electricity <xref ref-type="bibr" rid="bib1.bibx135" id="paren.129"/>. The focus of BC mitigation measures, however, differs between rural and urban areas. In urban areas, BC emission reductions are related to stricter vehicle emission standards, improved fuel quality, and eliminating outdated industrial capacity <xref ref-type="bibr" rid="bib1.bibx119 bib1.bibx135 bib1.bibx108 bib1.bibx128" id="paren.130"/>, which result in less BC emissions from liquid fuel. In rural areas, BC emission reductions result from prohibiting agricultural residue burning, household stove upgrading, and energy switching, e.g., from coal to natural gas and electricity <xref ref-type="bibr" rid="bib1.bibx144 bib1.bibx76 bib1.bibx98" id="paren.131"/>. These measures lead to BC emission reductions from biomass burning and coal combustion. The results here are consistent with the differences in BC emission reduction measures between cities and rural areas, with rapid decreases of eBC<sub>sf</sub> in rural areas and eBC<sub>lf</sub> in urban regions. Due to the limitation of the Aethalometer model, the BC sources are apportioned into eBC<sub>sf</sub> and eBC<sub>lf</sub>, while the contributions of solid fossil fuel (e.g., coal) and biomass cannot be further separated from eBC<sub>sf</sub> <xref ref-type="bibr" rid="bib1.bibx138" id="paren.132"/>. To further understand which types of fuels (e.g., biomass, coal, liquid fuel) dominated the BC reductions in China, we used the estimated BC emissions from different fuels derived from MEIC. As shown in Fig. <xref ref-type="fig" rid="F10"/>c, BC from coal combustion decreased by 0.38 Tg from 2008 to 2020 in China, followed by liquid fuel (0.16 Tg), and biomass burning (0.09 Tg). Therefore, emission reduction from coal combustion dominated the BC reduction in China, with a contribution of 60.3 %.</p>

      <fig id="F10" specific-use="star"><label>Figure 10</label><caption><p id="d2e4700">The drivers of BC reduction including contributions from emission variations <bold>(a)</bold>, different sources <bold>(b)</bold>, and fuel types including liquid fossil fuel (LF), coal combustion, and biomass burning (BB) <bold>(c)</bold> in China.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/25/16363/2025/acp-25-16363-2025-f10.png"/>

        </fig>

      <p id="d2e4718">In line with previous long-term observations of BC conducted in urban areas <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx137 bib1.bibx103 bib1.bibx117 bib1.bibx1" id="paren.133"/>, these studies identified the predominant driving factor for BC reduction was the reduced emissions from fossil fuel combustion (e.g., coal and petroleum). Representative examples include studies in Wuhan <xref ref-type="bibr" rid="bib1.bibx137" id="paren.134"/>, Beijing <xref ref-type="bibr" rid="bib1.bibx117" id="paren.135"/>, and Nanjing <xref ref-type="bibr" rid="bib1.bibx1" id="paren.136"/>. Unlike previous studies, this research also analyzed the driving factors behind BC reduction at rural and background sites. The results demonstrate that the decrease in BC concentrations is mainly attributed to reduced emissions from both coal and biomass combustion in rural and baseline areas. Evidence from BC emission data further support these findings. As shown in Fig. S13, BC emissions derived from the MEIC inventory <xref ref-type="bibr" rid="bib1.bibx36" id="paren.137"/> for biomass burning, solid fuel combustion, and liquid fuel combustion exhibited widespread reductions across most regions of eastern China between 2008 and 2020. Temporally, emissions from these sources showed consistent decreasing trends from 2008 to 2020 at rural, baseline, and urban stations. For example, BC emissions from rural residential energy consumption in northern China decreased from 0.85 Tg in 2010 to 0.55 Tg in 2020 <xref ref-type="bibr" rid="bib1.bibx131" id="paren.138"/>. These findings present novel and previously unreported conclusions based on observational data.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Conclusions</title>
      <p id="d2e4750">In this study, 13 years of continuous measurements of black carbon aerosol were analyzed from 48 stations in China. Using station-specific AAE<sub>lf</sub> and AAE<sub>sf</sub>, the sources of eBC were apportioned. The levels, spatial-temporal characteristics, and trends of black carbon aerosol were reported, and the key findings of this unique dataset are listed as follows.</p>
      <p id="d2e4771">Observations of black carbon aerosols from 2015–2017 showed averages of 2.05 <inline-formula><mml:math id="M374" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.85, 1.08 <inline-formula><mml:math id="M375" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.73, 0.97 <inline-formula><mml:math id="M376" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 1.52, and 1.33 <inline-formula><mml:math id="M377" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.29 for eBC, eBC<sub>lf</sub>, eBC<sub>sf</sub>, and AAE<sub>370–950</sub>, respectively, in China. Long-term trends of eBC, eBC<sub>sf</sub>, and eBC<sub>lf</sub> indicated reductions from 2008 to 2020, with mean slopes of <inline-formula><mml:math id="M383" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.17 <inline-formula><mml:math id="M384" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.20 <inline-formula><mml:math id="M385" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> for eBC, <inline-formula><mml:math id="M388" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.12 <inline-formula><mml:math id="M389" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.14 <inline-formula><mml:math id="M390" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> for eBC<sub>lf</sub>, and <inline-formula><mml:math id="M394" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.06 <inline-formula><mml:math id="M395" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.09 <inline-formula><mml:math id="M396" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> m<sup>−3</sup> yr<sup>−1</sup> for eBC<sub>sf</sub> on a national scale. Spatial distributions of eBC and eBC<sub>sf</sub> were higher in eastern and northern China compared to western and southern regions. Among different types of stations, urban stations exhibited the highest eBC values, while baseline stations had the highest fractions of eBC<sub>sf</sub> and AAE<sub>370–950</sub>. The seasonal variations of eBC, eBC<sub>sf</sub>, and AAE<sub>370–950</sub> typically showed the lowest values in summer and the highest in winter. However, some stations recorded abnormally high eBC levels during summer, which were associated with biomass burning and dusty weather events. The spatial-temporal patterns of BC in China can be explained by its emission variations and meteorological conditions. The weather normalized BC concentrations showed that emission reductions were the primary driver, accounting for 89 % of the decrease in eBC, 87 % in eBC<sub>lf</sub>, and 62 % in eBC<sub>sf</sub>. Urban stations showed the most rapid declines in  eBC<sub>lf</sub>, with the ratio of eBC<sub>lf</sub> to eBC<sub>sf</sub> trends exceeding 1, indicating that reductions in liquid fuel combustion emissions were the main contributor to BC decreases in urban areas. In contrast, rural and baseline stations exhibited the fastest declines in eBC<sub>sf</sub>, suggesting that emission reductions from solid fuel combustion were the dominant factor in these regions.</p>
      <p id="d2e5114">This study provides valuable insights from China's long-term observations of BC aerosol, with significant implications for refining emission inventories and reducing model uncertainties. The comparison between observations and simulations revealed that most models failed to capture the inter-annual variation while the simulation with MEIC inventory was capable to reproducing the spatial and temporal variations of BC. Therefore, BC emissions from MEIC is recommended for modeling BC concentrations in China. Furthermore, a systematic model underestimation of BC was found particularly at rural stations, which emphasized the need to refine both emission source strengths and deposition processes to improve model accuracy. This study showed that the weather normalization is a promising technique for refining BC emission inventories, as the weather normalized BC concentrations showed a stronger correlation with the reported BC emissions than raw observations. Further analysis revealed a higher correlation between emissions and concentrations of BC from liquid fuel combustion. To reduce uncertainties in BC emissions, a target effort to improving accuracy of emission from the solid fuel combustion sub-sector is needed, including the collection of accurate BC emission factors from biomass and coal burning, as well as updating activity data in rural areas.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d2e5121">The code and data used to produce all figures are available from the Huang Zheng (zhengh@wust.edu.cn) and corresponding authors under reasonable request. The authors do not have the right to share the ground BC observations dataset; The BC from TAP can be downloaded from <uri>http://tapdata.org.cn</uri> (last access: 28 July 2023). BC mass concentrations from MERRA-2 can be downloaded from <uri>https://disc.gsfc.nasa.gov/datasets</uri> (last access: 17 August 2023); Surface BC observations in UK and USA can be accessed via <uri>https://uk-air.defra.gov.uk</uri> (last access: 6 November 2023) and <uri>https://www.epa.gov/outdoor-air-quality-data</uri> (last access: 21 August 2023). The light absorption coefficient to calculate BC mass concentration and AAE values are from EBAS (<uri>https://ebas-data.nilu.no/Default.aspx</uri> (last access: 6 November 2023); Historical simulations of surface BC during 2008–2014 from CMIP6 are available from <uri>https://esgf-node.llnl.gov/projects/cmip6/</uri> (last access: 4 November 2023). The BC emission inventory used in this study can be downloaded from <uri>https://eccad.aeris-data.fr</uri> (last access: 25 September 2023), <uri>http://inventory.pku.edu.cn/home</uri> (last access: 14 November 2025), and <uri>http://meicmodel.org.cn</uri> (last access: 10 November 2023). Surface meteorological parameters from ERA5 are available at the Climate Data Store (<uri>https://cds.climate.copernicus.eu/datasets/reanalysis-era5-single-levels?tab=overview</uri>, last access: 4 October 2023). GDAS1 to drive HYSPLIT is available at <uri>https://www.ready.noaa.gov/data/archives/gdas1/</uri> (last access: 29 October 2023).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d2e5158">The supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-25-16363-2025-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-25-16363-2025-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e5167">HZ conducted the data analysis, data visualization, and wrote the paper. SK designed and edited the paper. DD provided the eBC observations in China and MS processed the pan-European eBC observations. CS, MZ, and RMH reviewed and commented on the paper. All co-authors reviewed and commented on the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e5173">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e5179">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. While Copernicus Publications makes every effort to include appropriate place names, the final responsibility lies with the authors. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e5185">We greatly thank the staff from the Chinese Meteorological Administration for maintaining the instruments.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e5190">This research has been supported by the National Natural Science Foundation of China (grant nos. 42307147, 42307151, and 41830965), the Ministry of Science and Technology of the People's Republic of China (grant no. 2016YFA0602002), and the European Commission, EU Horizon 2020 Framework Programme (grant no. 101036245).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e5196">This paper was edited by Gunnar Myhre and reviewed by two anonymous referees.</p>
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