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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-26-33-2026</article-id><title-group><article-title>NMVOC emission optimization in China through assimilating formaldehyde retrievals from multiple satellite products</article-title><alt-title>Constraining China's NMVOC Emissions with Multi-Satellite HCHO</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Xu</surname><given-names>Canjie</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Jin</surname><given-names>Jianbing</given-names></name>
          <email>jianbing.jin@nuist.edu.cn</email>
        <ext-link>https://orcid.org/0000-0002-2868-9343</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Ke</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9181-3562</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Qi</surname><given-names>Yinfei</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Xia</surname><given-names>Ji</given-names></name>
          
        <ext-link>https://orcid.org/0009-0006-3435-3148</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4">
          <name><surname>Lin</surname><given-names>Hai Xiang</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1653-4854</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Liao</surname><given-names>Hong</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>State Key Laboratory of Climate System Prediction and Risk Management, Jiangsu Key Laboratory of Atmospheric Environment Monitoring and Pollution Control, Jiangsu Collaborative Innovation Center of Atmospheric Environment and Equipment Technology, School of Environmental Science and Engineering, Nanjing University of Information Science &amp; Technology, Nanjing, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>College of Geography and Remote Sensing, Hohai University, Nanjing, Jiangsu, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Institute of Environmental Sciences, Leiden University, Leiden, the Netherlands</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Delft Institute of Applied Mathematics, Delft University of Technology, Delft, the Netherlands</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jianbing Jin (jianbing.jin@nuist.edu.cn)</corresp></author-notes><pub-date><day>5</day><month>January</month><year>2026</year></pub-date>
      
      <volume>26</volume>
      <issue>1</issue>
      <fpage>33</fpage><lpage>58</lpage>
      <history>
        <date date-type="received"><day>13</day><month>January</month><year>2025</year></date>
           <date date-type="rev-request"><day>7</day><month>May</month><year>2025</year></date>
           <date date-type="rev-recd"><day>8</day><month>December</month><year>2025</year></date>
           <date date-type="accepted"><day>12</day><month>December</month><year>2025</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Canjie Xu et al.</copyright-statement>
        <copyright-year>2026</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/26/33/2026/acp-26-33-2026.html">This article is available from https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e156">Non-methane volatile organic compounds (NMVOCs) are key precursors of ozone and secondary organic aerosols. As one of the world’s largest NMVOC emitters, accurate emission inventories are essential for understanding and mitigating air pollution in China. Commonly-used inventories (e.g., MEIC) are largely based on bottom-up methods, which often fail to capture the spatiotemporal variability of NMVOC emissions, resulting in significant model-observation mismatches. This study evaluates the shape factor, filtered data volume, and monthly mean biases of OMI, OMPS, and TROPOMI formaldehyde products, with the latest OMPS and TROPOMI retrievals offering substantially higher effective spatiotemporal coverage. Monthly NMVOC emissions over China in 2020 are then optimized by independently assimilating formaldehyde retrievals either from OMPS or from TROPOMI, using a self-developed 4DEnVar assimilation emission inversion system. The OMPS- and TROPOMI-driven assimilation yields consistent seasonal and regional increments in NMVOC emissions in general, but distinctions are also notable. A consistency analysis is introduced to assess the reliability of these two posterior emissions. Highly consistent increments are obtained in the North China Plain (May–June), the Yangtze River Delta and Pearl River Delta (January–March, October–December), and the Sichuan Basin (January, June–December). These adjustments significantly improve surface ozone simulations, with 81.25 % of consistent cases demonstrating reduced biases and an average RMSE reduction of 24.7 %. These findings highlight the effectiveness of OMPS and TROPOMI formaldehyde assimilation, coupled with consistency analysis, in refining NMVOC emission estimates and enhancing ozone simulation accuracy. Similar promising results are achieved in the OMPS/TROPOMI-based NMVOC emission inversion in 2019.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National Key Research and Development Program of China</funding-source>
<award-id>2022YFE0136100</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="d2e168">Non-methane volatile organic compounds (NMVOCs) are significant components of the atmosphere, serving as key precursors to ozone (O<sub>3</sub>) and secondary organic aerosols (SOA) <xref ref-type="bibr" rid="bib1.bibx64" id="paren.1"/>. They engage in numerous photochemical reactions, exerting a considerable influence on atmospheric oxidative capacity and air quality <xref ref-type="bibr" rid="bib1.bibx111" id="paren.2"/>. Moreover, NMVOCs such as benzene, trichloroethylene, and chloroform are recognized for their toxicity <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx54" id="paren.3"/>, and prolonged exposure to elevated concentrations can pose significant health risks <xref ref-type="bibr" rid="bib1.bibx40" id="paren.4"/>. China has seen a rapid anthropogenic NMVOC emissions increase over the last three decades, gradually becoming one of the important contributors to global NMVOC emissions <xref ref-type="bibr" rid="bib1.bibx62" id="paren.5"/>. Investigating NMVOC dynamics and their emission distributions is critical for addressing air pollution challenges in China <xref ref-type="bibr" rid="bib1.bibx109 bib1.bibx38" id="paren.6"/>.</p>
      <p id="d2e199">NMVOCs are primarily released through anthropogenic activities, biogenic emissions, and biomass burning processes. Huge efforts have been devoted to constructing inventories recording these emissions in a bottom-up way, such as the global Community Emission Data System (CEDS) <xref ref-type="bibr" rid="bib1.bibx41" id="paren.7"/>, the regional Multi-resolution Emission Inventory for China (MEIC) <xref ref-type="bibr" rid="bib1.bibx62" id="paren.8"/>, and the Model of Emissions of Gases and Aerosols from Nature v2.1 (MEGAN) <xref ref-type="bibr" rid="bib1.bibx35" id="paren.9"/>. For biomass burning, widely used inventories include the Global Fire Emissions Database (GFED) <xref ref-type="bibr" rid="bib1.bibx93" id="paren.10"/> and the Fire INventory from NCAR (FINN) <xref ref-type="bibr" rid="bib1.bibx100" id="paren.11"/>. Coupled with chemical transport models like GEOS-Chem <xref ref-type="bibr" rid="bib1.bibx44" id="paren.12"/> and WRF-Chem <xref ref-type="bibr" rid="bib1.bibx3" id="paren.13"/>, these inventories are widely used to simulate transport, deposition, and chemical transformations of NMVOCs, supporting air quality assessments and emission control strategies. However, bottom-up estimates remain highly uncertain because both emission factors and activity data vary greatly in space and time and are often poorly constrained <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx83" id="paren.14"/>. For anthropogenic sources, nationwide uncertainties of <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">68</mml:mn></mml:mrow></mml:math></inline-formula> %–78 % have been reported due to variable activity data and emission factors under rapid structural transitions in industry, solvent use, and transportation <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx62" id="paren.15"/>. Biogenic emissions are even more uncertain, highly sensitive to land-cover, meteorology, and parameterizations, with Chinese BVOC estimates varying from 10 to 58.9 Tg C yr<sup>−1</sup> <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx97 bib1.bibx78" id="paren.16"/>. Biomass burning emissions also show large discrepancies across inventories (e.g., GFED, FINN, GFAS) <xref ref-type="bibr" rid="bib1.bibx48" id="paren.17"/>, largely driven by uncertainties in burned area, fuel loading, and emission factors <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx42" id="paren.18"/>. In addition, strict air pollution controls implemented in recent years targeting industry, residential use, and transportation have significantly altered emission patterns <xref ref-type="bibr" rid="bib1.bibx103 bib1.bibx61 bib1.bibx110" id="paren.19"/>. Consequently, bottom-up inventories carry substantial uncertainties <xref ref-type="bibr" rid="bib1.bibx60 bib1.bibx80" id="paren.20"/>. For example, estimates of China’s total NMVOC emissions for 2012 range between 18 and 27 Tg depending on the inventory used <xref ref-type="bibr" rid="bib1.bibx51 bib1.bibx103 bib1.bibx91" id="paren.21"/>, posing major challenges for accurately assessing the role of NMVOCs in air quality and climate <xref ref-type="bibr" rid="bib1.bibx37 bib1.bibx96" id="paren.22"/>.</p>
      <p id="d2e275">There are numerous well-established techniques for measuring the concentrations of various volatile organic compounds in the atmosphere. These include gas chromatography, mass spectrometry, Fourier transform infrared spectroscopy, and non-dispersive infrared analysis. While these methods are highly effective for meeting the requirements of experimental studies and real-time monitoring, their complexity and the associated high labor costs pose significant challenges for long-term measurements or assessments across large spatial scales <xref ref-type="bibr" rid="bib1.bibx81 bib1.bibx16 bib1.bibx105" id="paren.23"/>. Among the various NMVOCs, the optical properties of formaldehyde and glyoxal make them particularly suitable for detection via remote sensing technologies. These properties enable formaldehyde and glyoxal to be among the few NMVOCs that can be monitored from satellites. Remote sensing observations of these compounds typically rely on spectral channels in the ultraviolet-visible (UV–Vis) range, with their primary absorption features occurring between 330 and 460 nm <xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx55 bib1.bibx21" id="paren.24"/>.</p>
      <p id="d2e284">Satellite remote sensing of formaldehyde has made substantial progress since the atmospheric formaldehyde abundance was first retrieved in 1997 <xref ref-type="bibr" rid="bib1.bibx10" id="paren.25"/>. The earliest retrievals of formaldehyde vertical column densities were based on the Global Ozone Monitoring Experiment (GOME) <xref ref-type="bibr" rid="bib1.bibx92 bib1.bibx14" id="paren.26"/>. Subsequently, the Scanning Imaging Absorption Spectrometer for Atmospheric Chartography (SCIAMACHY) served as an important transitional instrument between GOME and GOME-2, offering significantly improved spatial resolution compared to GOME <xref ref-type="bibr" rid="bib1.bibx20" id="paren.27"/>. In 2004, the launch of NASA’s Aura satellite carrying the Ozone Monitoring Instrument (OMI) provided high signal-to-noise-ratio ultraviolet–visible (UV–Vis) spectra that greatly advanced trace-gas retrieval studies <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx32" id="paren.28"/>. Approximately four years after GOME effectively ceased operational observations, its successor, GOME-2, began routine operations in 2007 and started delivering formaldehyde data <xref ref-type="bibr" rid="bib1.bibx21" id="paren.29"/>. In recent years, high-resolution formaldehyde observations have continued to emerge, including those from the Ozone Mapping and Profiler Suite (OMPS) onboard the Suomi National Polar-orbiting Partnership (Suomi NPP) and NOAA-20 satellites <xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx32 bib1.bibx33 bib1.bibx71" id="paren.30"/>, as well as from the Tropospheric Monitoring Instrument (TROPOMI) aboard the Sentinel-5 Precursor (Sentinel-5P) launched in 2017. TROPOMI’s exceptional spatial resolution and near-daily global coverage have marked a new era in satellite formaldehyde monitoring <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx25" id="paren.31"/>. Furthermore, geostationary satellites now provide formaldehyde observations with high temporal resolution, including the Geostationary Environment Monitoring Spectrometer (GEMS) over East Asia <xref ref-type="bibr" rid="bib1.bibx52 bib1.bibx49" id="paren.32"/>, the Tropospheric Emissions: Monitoring of Pollution (TEMPO) instrument over North America <xref ref-type="bibr" rid="bib1.bibx15" id="paren.33"/>, and Sentinel-4, successfully launched on 1 July 2025, which is conducting geostationary formaldehyde observations over Europe <xref ref-type="bibr" rid="bib1.bibx36" id="paren.34"/>.</p>
      <p id="d2e319">Glyoxal retrieval product from satellite platform began relatively late, with the first global differential optical absorption spectroscopy (DOAS) retrievals reported by <xref ref-type="bibr" rid="bib1.bibx101" id="text.35"/> using SCIAMACHY, followed by their application to constrain NMVOC emissions by <xref ref-type="bibr" rid="bib1.bibx88" id="text.36"/>. Because glyoxal is retrieved in a longer wavelength range (<inline-formula><mml:math id="M4" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 435–460 nm) than formaldehyde (<inline-formula><mml:math id="M5" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 330–360 nm), it exhibits markedly lower sensitivity to molecular scattering, which in turn increases the sensitivity of the measurement to the lower troposphere <xref ref-type="bibr" rid="bib1.bibx74 bib1.bibx12" id="paren.37"/>. Glyoxal optical depths are very weak (order of <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), rendering the retrieval highly susceptible to fitting residuals from stronger absorbers, uncertainties in absolute radiometric calibration, and spectral features in surface reflectivity <xref ref-type="bibr" rid="bib1.bibx85 bib1.bibx2" id="paren.38"/>. For instruments with comparatively modest spectral resolution and signal-to-noise ratios, such as OMI, these interference effects are further amplified, leading to larger retrieval uncertainties for glyoxal columns than for formaldehyde <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx11" id="paren.39"/>. Consequently, glyoxal satellite observations remain considerably less suitable than formaldehyde for high-spatiotemporal-resolution assimilation studies. Beyond glyoxal and formaldehyde, retrievals of other VOCs are also progressing, as exemplified by <xref ref-type="bibr" rid="bib1.bibx30" id="text.40"/> and <xref ref-type="bibr" rid="bib1.bibx98 bib1.bibx99" id="text.41"/>, who derived isoprene columns from Cross-track Infrared Sounder (CrIS) observations, representing an important step toward next-generation satellite constraints on volatile organic compounds.</p>
      <p id="d2e386">Top-down approaches, mainly assimilation techniques, with satellite formaldehyde columns have become the primary method for constraining NMVOC emissions. <xref ref-type="bibr" rid="bib1.bibx75" id="text.42"/> pioneered applying a Bayesian inversion framework with GOME formaldehyde observations for constraining isoprene emissions over North America. The approach was subsequently extended to global and European domains by <xref ref-type="bibr" rid="bib1.bibx84" id="text.43"/> and <xref ref-type="bibr" rid="bib1.bibx26" id="text.44"/>, respectively. With the availability of OMI and GOME-2 formaldehyde products, inversion algorithms were further refined. <xref ref-type="bibr" rid="bib1.bibx89" id="text.45"/> first introduced an adjoint-based inversion to optimize biogenic emissions and, in a companion study the same year, revealed substantial underestimation of continental glyoxal sources worldwide <xref ref-type="bibr" rid="bib1.bibx88" id="paren.46"/>. Concurrently, <xref ref-type="bibr" rid="bib1.bibx68" id="text.47"/> used OMI formaldehyde and identified an underestimation of isoprene emissions over the north-central United States, while <xref ref-type="bibr" rid="bib1.bibx112" id="text.48"/> reported that anthropogenic emissions of highly reactive VOCs (HRVOCs) in the Houston area were underestimated by a factor of 4.8 <inline-formula><mml:math id="M8" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 2.7 compared to the US Environmental Protection Agency inventory. Formaldehyde product with much higher spatial resolution were then available since the launch of TROPOMI and OMPS, and made the city-scale emission optimizations possible <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx24 bib1.bibx25" id="paren.49"/>. In recent years, studies leveraging these new-generation instruments have proliferated. <xref ref-type="bibr" rid="bib1.bibx17" id="text.50"/> assimilated OMPS and OMI observations into an updated 4DVar system for East Asia during May–June 2016. Their inversion revealed a 47 % increase in VOC emissions across Northeast Asia relative to the prior inventory, indicating that isoprene emissions over South Korea and anthropogenic NMVOC emissions over eastern China were underestimated in the bottom-up inventory. <xref ref-type="bibr" rid="bib1.bibx72" id="text.51"/> used weekly-averaged TROPOMI formaldehyde observations from 2018–2021 with the MAGRITTEv1.1 adjoint model to derive top-down biogenic, pyrogenic, and anthropogenic VOC fluxes over Europe, substantially correcting previous underestimates of isoprene emissions. <xref ref-type="bibr" rid="bib1.bibx28" id="text.52"/> applied an Ensemble Kalman Filter (EnKF) approach to optimize August 2022 NMVOC emissions over China, revealing overestimation of biogenic emissions during an extreme heatwave and demonstrating consequential impacts on summertime ozone simulations. The advent of geostationary satellites (e.g., GEMS, TEMPO) with high-frequency observations has enabled the incorporation of diurnal cycle information into algorithm frameworks, making daily-scale top-down emission optimization feasible <xref ref-type="bibr" rid="bib1.bibx52 bib1.bibx53" id="paren.53"/>. Meanwhile, multi-species constraint is gaining traction; <xref ref-type="bibr" rid="bib1.bibx73" id="text.54"/> developed a novel inversion technique that simultaneously optimizes monthly-mean VOCs and NO<sub><italic>x</italic></sub> emissions from 2019 TROPOMI observations, uncovering severe underestimation of both NO<sub><italic>x</italic></sub> and VOCs in prior inventories over Africa.</p>
      <p id="d2e455">Although substantial progress has been made globally in satellite-based top-down constraints on NMVOC emissions, high-resolution top-down emission optimization studies specifically over China remain scarce. <xref ref-type="bibr" rid="bib1.bibx84" id="text.55"/> first used GOME formaldehyde observations in a global Bayesian inversion framework to constrain isoprene emissions. While their domain encompassed East Asia including China, the study lacked a dedicated focus on China and was limited by coarse model resolution (4° <inline-formula><mml:math id="M11" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 5°). <xref ref-type="bibr" rid="bib1.bibx90" id="text.56"/> performed a regional inversion over eastern China using multi-year GOME and OMI formaldehyde columns, revealing that post-harvest agricultural burning in June contributed more than twice the VOC emissions of all other anthropogenic sources combined over the North China Plain during 2005–2012. <xref ref-type="bibr" rid="bib1.bibx11" id="text.57"/> conducted one of the most systematic satellite-constrained inversions for China to date, applying a 4DVar assimilation of OMI and GOME-2A formaldehyde products to estimate monthly NMVOC emissions in 2007, yet the analysis was still constrained by the same coarse 4° <inline-formula><mml:math id="M12" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 5° resolution. <xref ref-type="bibr" rid="bib1.bibx17" id="text.58"/> assimilated OMPS and OMI formaldehyde columns into a regional 4DVar system over East Asia but only for May–June; similarly, the top-down optimization of Chinese NMVOC emissions by <xref ref-type="bibr" rid="bib1.bibx28" id="text.59"/> was limited to a single month (August 2022). Given the increasingly stringent air pollution control policies in China <xref ref-type="bibr" rid="bib1.bibx102" id="paren.60"/>, there is an urgent need for high spatial- and temporal-resolution top-down NMVOC emission optimization to support more accurate air quality forecasting and effective regulatory strategies. In terms of the observation sources for assimilation, the OMI formaldehyde product remains one of the most widely used datasets in related studies to date. However, it has been affected globally by the persistent row anomaly since 2007 <xref ref-type="bibr" rid="bib1.bibx50 bib1.bibx114" id="text.61"/>, which degrades data quality in certain across-track positions and may reduce assimilation accuracy, particularly in high-resolution configurations. Although rigorous quality filtering and row anomaly flagging can mitigate this problem, the number of valid grid cells remaining after such screening is often severely limited, rendering OMI data insufficient for nationwide high-resolution emission inversion. In contrast, newer-generation instruments such as TROPOMI and OMPS provide formaldehyde products that are unaffected by the row anomaly, offer significantly higher spatial resolution and better data coverage (Sect. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS3"/>), and are therefore considerably more suitable for high-resolution top-down optimization of NMVOC emissions over China.</p>
      <p id="d2e496">In this study, we conduct monthly optimization of anthropogenic NMVOC emissions over China at 0.5° latitude <inline-formula><mml:math id="M13" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625° longitude horizontal resolution. It is achieved based on an emission inversion system that couples the four-dimensional ensemble variational (4DEnVar) data assimilation algorithm with the nested version of the GEOS-Chem model. The effectiveness of this emission inversion system has been evaluated in our recent studies of ammonia <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx104" id="paren.62"/>. Two independent assimilation experiments are performed: one assimilating OMPS total formaldehyde columns and the other assimilating TROPOMI tropospheric formaldehyde columns. In both cases, the satellite retrievals have been harmonized with the model by replacing the original shape profiles with GEOS-Chem profiles before assimilation. We focus on the year 2020 for the main analysis, while results for 2019 are also presented in the Supplement to provide additional context and support. This paper is organized as follows: Sect. <xref ref-type="sec" rid="Ch1.S2"/> describes the dataset and methodology, focusing on GEOS-Chem model, input emission sources (anthropogenic, biogenic, and biomass burning), and the satellite and ground-based observations utilized. Sect. <xref ref-type="sec" rid="Ch1.S3"/> provides an analysis of the assimilation results, including the estimation of posterior NMVOC emissions and the validation of both formaldehyde columns and ground-level ozone simulations. Sect. <xref ref-type="sec" rid="Ch1.S4"/> summarizes the key findings and concludes the study.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
      <p id="d2e523">This section begins by introducing the GEOS-Chem model utilized for simulations in Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/>. Section <xref ref-type="sec" rid="Ch1.S2.SS2"/> presents an overview of the emissions used as the prior NMVOC inventories, including anthropogenic, biogenic, and biomass burning inventories. Section <xref ref-type="sec" rid="Ch1.S2.SS3"/> introduces the three satellite observations employed in the analysis in this study. In Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>, the ground observations used for ozone validation are presented. Section <xref ref-type="sec" rid="Ch1.S2.SS5"/> introduces the 4DEnVar algorithm used for data assimilation. </p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Model simulation</title>
      <p id="d2e544">GEOS-Chem is a chemical transport model driven by meteorological data from the Goddard Earth Observing System (GEOS) of NASA's Global Modeling and Assimilation Office (GMAO) <xref ref-type="bibr" rid="bib1.bibx6" id="paren.63"/>. In this study, we use GEOS-Chem Classic (GCC) v14.1.1 to simulate formaldehyde columns to constrain NMVOC emissions over China. The global simulation is run at 2° <inline-formula><mml:math id="M14" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5° resolution and provides lateral chemical boundary conditions to the nested Asia domain updated every 3 h. The nested region (72–136° E, 17.5–54° N) has a horizontal resolution of 0.5° latitude <inline-formula><mml:math id="M15" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625° longitude and 47 vertical layers. Modern-Era Retrospective analysis for Research and Applications, Version 2 (MERRA-2) meteorological fields <xref ref-type="bibr" rid="bib1.bibx31" id="paren.64"/> are used to drive GEOS-Chem. Each simulation includes a 6-month spin-up period.</p>
      <p id="d2e567">This model version incorporates detailed O<sub>3</sub>-HO<sub><italic>x</italic></sub>-NO<sub><italic>x</italic></sub> photochemistry and fully coupled aerosol-O<sub>3</sub>-NO<sub><italic>x</italic></sub>-VOCs chemistry representation <xref ref-type="bibr" rid="bib1.bibx77" id="paren.65"/>, coupled with a scheme for primary carbonaceous aerosols, dust, sea salt, and secondary inorganic species (sulfates, nitrates, and ammonium) and their distribution. To better simulate oxidant-aerosol reactions in the troposphere, GEOS-Chem v14.1.1 includes state-of-the-science tropospheric chemistry with recent updates to the oxidation mechanisms of isoprene <xref ref-type="bibr" rid="bib1.bibx4" id="paren.66"/>, aromatics <xref ref-type="bibr" rid="bib1.bibx5" id="paren.67"/>, ethylene, and acetylene <xref ref-type="bibr" rid="bib1.bibx53" id="paren.68"/>. Since the satellite overpasses China mainly between 12:00 and 14:00 local time, the model outputs within this time window are sampled to calculate the formaldehyde columns for fair comparison with the satellite observations. After this temporal collocation and post-processing, samples of the formaldehyde tropospheric column simulation are presented in Fig. <xref ref-type="fig" rid="F1"/>a.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e632">Spatial distributions of formaldehyde columns from GEOS-Chem model-simulated prior tropospheric columns <bold>(a)</bold> and posterior tropospheric columns constrained by OMPS assimilation <bold>(b)</bold>, satellite observations of OMPS total columns <bold>(c)</bold>, and satellite observations of TROPOMI tropospheric columns <bold>(d)</bold>, both reprocessed to be consistent with the GEOS-Chem shape profile. Panels <bold>(a.1)</bold>–<bold>(d.1)</bold>, <bold>(a.2)</bold>–<bold>(d.2)</bold>, <bold>(a.3)</bold>–<bold>(d.3)</bold>, and <bold>(a.4)</bold>–<bold>(d.4)</bold> show February, May, August, and November of 2020, respectively.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f01.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Prior NMVOC emission inventories</title>
      <p id="d2e687">The anthropogenic NMVOC emission input into the model mainly comes from the Multi-resolution Emission Inventory for China (MEIC; <xref ref-type="bibr" rid="bib1.bibx110" id="altparen.69"/>). Since the MEIC inventory tailored for the existing chemical species in GEOS-Chem only extends to 2017, the MEIC inventory used in this study is the 2017 emission inventory. This inventory has a spatial resolution of 0.25° latitude <inline-formula><mml:math id="M21" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.25° longitude and includes industrial, transportation, power generation, and residential emissions. For chemical species used in GEOS-Chem but not included in MEIC and anthropogenic NMVOC emissions outside China, we use the 2019 CEDS global inventory as a supplement. The prior estimates of biogenic NMVOC emissions in this study are obtained from the MEGAN 2.1 model <xref ref-type="bibr" rid="bib1.bibx35" id="paren.70"/>. Field straw burning is considered a major seasonal source of NMVOCs in China <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx65 bib1.bibx90" id="paren.71"/>. In this study, the biomass burning emissions are taken from the GFED version 4 (GFED4) global inventory for 2020 <xref ref-type="bibr" rid="bib1.bibx93" id="paren.72"/>. Before these prior emissions are used to drive GEOS-Chem simulations, the spatial resolution is coarsened to an average value on a 0.5° <inline-formula><mml:math id="M22" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625° grid resolution consistent with the model configuration as used in Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/>.</p>
      <p id="d2e721">Figure <xref ref-type="fig" rid="F2"/>a presents the prior NMVOC emission inventories for 2020, which primarily relies on the anthropogenic emission inventory from MEIC, supplemented by the CEDS inventory for species not included in MEIC. Additionally, biogenic emissions are provided by MEGAN (offline calculation) for the year 2020 with an hourly temporal resolution, directly through the HEMCO emission component of GEOS-Chem; in this study, we did not run the MEGAN model separately. Biomass burning emissions are taken from GFED4. The combination of these three sources is treated as the prior emission inventory used in the following NMVOC emission optimization.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e728">Spatial distributions of the total NMVOC emissions from the prior <bold>(a)</bold> and posterior <bold>(b)</bold> results in February <bold>(a.1, b.1)</bold>, May <bold>(a.2, b.2)</bold>, August <bold>(a.3, b.3)</bold>, November <bold>(a.4, b.4)</bold> 2020. Panels <bold>(d.1)</bold>–<bold>(d.4)</bold> and <bold>(e.1)</bold>–<bold>(e.4)</bold> show the corresponding emission increments (posterior minus prior) derived from OMPS and TROPOMI assimilation.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f02.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Formaldehyde Satellite measurements</title>
<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>NOAA-20 OMPS</title>
      <p id="d2e783">Ozone Mapping and Profiler Suite (OMPS) was launched on Suomi National Polar-orbiting Partnership (SNPP) satellite on 28 October 2011, and on the JPSS-1 satellite (now known as NOAA-20) on 18 November 2017. OMPS/SNPP consists of three instruments: the nadir mapper (OMPS-NM), the profile mapper (OMPS-NP), and the limb profiler (OMPS-LP), while OMPS/NOAA-20 includes only the nadir package (OMPS-NM and OMPS-NP). This study uses OMPS-N20 Level 2 NM formaldehyde Total Column swath orbital Version 1 product <xref ref-type="bibr" rid="bib1.bibx1" id="paren.73"/>. OMPS-NM is a hyperspectral nadir viewing spectrometer that measures backscattered light with a spectral resolution of approximately 1 nm. The NOAA-20 spectral measurement range is 300–420 nm. The instrument employs a 2-D CCD array detector in a pushbroom geometry, observing the two-dimensional field below the satellite’s orbit over a swath width of about 2800 km. With 14 or 15 orbits per day, OMPS-NM provides daily global coverage of trace gas columns in the early afternoon local time, with an equatorial crossing time of approximately 13:30. The spatial resolution of OMPS/NOAA-20 was 17 km <inline-formula><mml:math id="M23" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 17 km until 13 February 2019, when it was changed to 12 km <inline-formula><mml:math id="M24" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 17 km <xref ref-type="bibr" rid="bib1.bibx29 bib1.bibx76 bib1.bibx82" id="paren.74"/>.</p>
      <p id="d2e806">In this study, the quality control scheme recommended in OMPS product documentation was applied. Data points with formaldehyde column densities exceeding <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">17</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> molec. cm<sup>−2</sup> were excluded to minimize the impact of outliers. After removing outliers, we further excluded data points where the sum of formaldehyde column and twice the observation uncertainty was less than zero. Furthermore, the geometric air mass factors (AMF<sub>G</sub>) were defined as follows:

              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M28" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">AMF</mml:mi><mml:mi mathvariant="normal">G</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">sec</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">SZA</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi mathvariant="normal">sec</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">VZA</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

            Here, SZA represents the solar zenith angle and VZA denotes the viewing zenith angle. Additional data screening was applied by excluding observations with SZA greater than 70°, an air mass factor less than 0.1, a geometric air mass factor greater than 4, a cloud fraction exceeding 0.4, or with positive snow and ice fractions. All screened data were then averaged to a spatial resolution of 0.5° latitude <inline-formula><mml:math id="M29" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625° longitude on a monthly basis, consistent with the GEOS-Chem model configuration. To make a fair comparison between the observed and simulation formaldehyde column in the assimilation, we further imposed constraints on the number of observations within each grid cell. Specifically, two filtering schemes were tested, in which grid cells with fewer than 10 or fewer than 50 original observations were excluded. The OMPS formaldehyde columns after applying the threshold of 50 are shown in Fig. <xref ref-type="fig" rid="F1"/>c, while the results with the threshold of 10 are provided in the Supplement. The differences between the two filtering schemes are minor, particularly across the four study regions considered in this work.</p>
      <p id="d2e886">Formaldehyde vertical column densities (VCDs) retrieved from satellite observations are derived using air mass factors (AMF), which strongly depend on the a priori vertical profiles of formaldehyde. Direct comparisons between satellite products and model simulations may be biased if the a priori profiles used in the retrieval differ from the simulated ones. To ensure consistency between the satellite observations and GEOS-Chem simulation, we applied an AMF correction by recalculating the AMF with model-simulated profiles following the method used in <xref ref-type="bibr" rid="bib1.bibx74" id="text.75"/>:

              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M30" display="block"><mml:mrow><mml:mi mathvariant="normal">AMF</mml:mi><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow><mml:mn mathvariant="normal">0</mml:mn></mml:munderover><mml:mi>w</mml:mi><mml:mfenced close=")" open="("><mml:mi>p</mml:mi></mml:mfenced><mml:mi>S</mml:mi><mml:mfenced open="(" close=")"><mml:mi>p</mml:mi></mml:mfenced><mml:mi mathvariant="normal">d</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></disp-formula></p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e929">Shape factors of regional-mean formaldehyde columns, as derived from the a priori profiles, followed by normalization, from GEOS-Chem model-simulated prior (black) and satellite observations by OMPS (blue), TROPOMI (red), and OMI (green). Panels <bold>(a)</bold>–<bold>(d)</bold> correspond to the North China Plain, Yangtze River Delta, Pearl River Delta, and Northeast China, respectively. Sub-panels <bold>(a.1)</bold>–<bold>(d.1)</bold>, <bold>(a.2)</bold>–<bold>(d.2)</bold>, <bold>(a.3)</bold>–<bold>(d.3)</bold>, and <bold>(a.4)</bold>–<bold>(d.4)</bold> represent February, May, August, and November 2020, respectively. Values in parentheses indicate the biases of satellite observations relative to the prior simulation. Shaded areas denote the observational uncertainties.</p></caption>
            <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f03.png"/>

          </fig>

      <p id="d2e969">The right-hand side of the equation represents the vertically integrated product of the scattering weight <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mi>w</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and the shape factor <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mi>S</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> as a function of pressure <inline-formula><mml:math id="M33" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>, where <inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mi>w</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> characterizes the sensitivity of the satellite measurement to a given atmospheric layer and <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>S</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> describes the normalized vertical profiles of the a priori profiles. The scattering weights <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mi>w</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> are primarily determined by satellite observational geometry (e.g., solar and viewing zenith angles), surface albedo, and cloud fraction, while the shape factor <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mi>S</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> depends on the vertical profiles of formaldehyde. The integration is performed over the pressure coordinate from the surface (<inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) to the top of the atmosphere. Figure <xref ref-type="fig" rid="F3"/> illustrates the vertical distribution of the shape profile, highlighting the relative contributions of different layers. The vertical column density (VCD) is obtained from the ratio of the slant column density (SCD) to the AMF:

              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M39" display="block"><mml:mrow><mml:mi mathvariant="normal">VCD</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="normal">SCD</mml:mi><mml:mi mathvariant="normal">AMF</mml:mi></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1092">In the OMPS formaldehyde product, the SCD is derived as the sum of three components: the fitted differential slant column amount (<inline-formula><mml:math id="M40" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SCD), the reference sector correction (SCD<sub>Ref</sub>), and the bias correction (SCD<sub>B</sub>):

              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M43" display="block"><mml:mrow><mml:mi mathvariant="normal">SCD</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">SCD</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">SCD</mml:mi><mml:mi mathvariant="normal">Ref</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">SCD</mml:mi><mml:mi mathvariant="normal">B</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula>

            Here, <inline-formula><mml:math id="M44" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>SCD represents the differential slant column amount retrieved from the DOAS spectral fitting, SCD<sub>Ref</sub> is the reference sector correction that accounts for background contributions and instrumental offsets by using clean reference regions, and SCD<sub>B</sub> denotes an additional bias correction to mitigate systematic errors.</p>
      <p id="d2e1174">The OMPS observations were assimilated as total columns after re-calculation of the air mass factor using GEOS-Chem shape profiles for consistency with the model vertical profile. These reprocessed total columns are shown in Fig. <xref ref-type="fig" rid="F1"/>c.1–c.4. The original a priori shape factors used in the official satellite products (before reprocessing) are displayed as red lines in Fig. <xref ref-type="fig" rid="F3"/>.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Sentinel-5P TROPOMI</title>
      <p id="d2e1189">Sentinel-5 Precursor (Sentinel-5P) is a member of the European Space Agency's (ESA) Sentinel satellite series. It is in a low-Earth afternoon polar orbit with a swath of 2600 km, allowing for daily global coverage <xref ref-type="bibr" rid="bib1.bibx94" id="paren.76"/>. Its sole payload is Tropospheric Monitoring Instrument (TROPOMI), a nadir-viewing, 108° field-of-view push-broom grating hyperspectral spectrometer. TROPOMI covers the ultraviolet-visible (UV-VIS, 270 to 495 nm), near-infrared (NIR, 675 to 775 nm), and shortwave infrared (SWIR, 2305 to 2385 nm) spectral ranges. Its Level 2 products include vertical columns of ozone, sulfur dioxide, nitrogen dioxide, formaldehyde, carbon monoxide, and methane, as well as ozone profiles, aerosol layer height, cloud information, and aerosol index. The initial spatial resolution was 3.5 km <inline-formula><mml:math id="M47" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 7 km, which was improved to 3.5 km <inline-formula><mml:math id="M48" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 5.5 km on 6 August 2019.</p>
      <p id="d2e1209">The retrieval algorithm for TROPOMI formaldehyde is based on the DOAS method and is directly inherited from the OMI QA4ECV product retrieval algorithm <xref ref-type="bibr" rid="bib1.bibx23" id="paren.77"/>. This study uses the Sentinel-5P TROPOMI Level 2 Tropospheric formaldehyde Version 2 product <xref ref-type="bibr" rid="bib1.bibx19" id="paren.78"/>. <xref ref-type="bibr" rid="bib1.bibx95" id="text.79"/> evaluated this TROPOMI formaldehyde product using ground-based solar-absorption FTIR (Fourier-transform infrared) measurements, demonstrating its good quality. <xref ref-type="bibr" rid="bib1.bibx25" id="text.80"/> further assessed TROPOMI formaldehyde using OMI observations and MAX-DOAS network column measurements, also showing favorable results. When using Level 2 TROPOMI formaldehyde data for the validation in this study, we applied the recommended quality assurance filtering by retaining only pixels with a qa value greater than 0.5. This criterion ensures the exclusion of error flags and requires that the cloud radiance fraction at 340 nm is below 0.5, the solar zenith angle (SZA) does not exceed 70°, the surface albedo is below 0.2, no snow or ice warning is present, and the air mass factor (AMF) is larger than 0.1. The operational TROPOMI HCHO Level-2 product provides tropospheric vertical columns together with averaging kernels and a priori profiles defined on 34 vertical layers (from the surface to <inline-formula><mml:math id="M49" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.1 hPa). Because stratospheric formaldehyde is  negligible <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx25" id="paren.81"/>, we directly use the reported tropospheric columns in this study without reconstructing total columns. After filtering, the TROPOMI observations were aggregated to monthly means on a 0.5° <inline-formula><mml:math id="M50" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625° grid, ensuring consistency with the resolution used in the GEOS-Chem simulations. In addition, we further constrained the number of observations per grid cell: Fig. <xref ref-type="fig" rid="F1"/>d shows the results after excluding grid cells with fewer than 50 observations, while the results with a threshold of 10 are also provided in the Supplement. The differences between the two filtering schemes are minor, particularly over the study regions.</p>
      <p id="d2e1244">Beyond the recommended quality filtering, a critical consideration when comparing TROPOMI formaldehyde retrievals with model simulations is the sensitivity of the retrieved columns to the a priori vertical profile assumed in the retrieval algorithm. In this study, OMPS and OMI formaldehyde products are harmonized with the model by recalculating the AMF using GEOS-Chem shape factors, following the conventional approach. For TROPOMI, the officially provided averaging kernels (AVK) are applied instead. Importantly, these two correction strategies are mathematically equivalent. The averaging kernel represents the ratio of the altitude-resolved sensitivity to the total AMF used in the operational retrieval. Consequently, convolving the model profile with the AVK and adding the same background column yields identical results to recalculating the total AMF with the model profile and applying it to the slant column, provided that the background correction and a priori profile replacement are handled consistently <xref ref-type="bibr" rid="bib1.bibx74 bib1.bibx27 bib1.bibx9 bib1.bibx25" id="paren.82"/>. Both approaches achieve the same objective: removing the influence of the satellite’s a priori profile and replacing it with the GEOS-Chem profile, thereby ensuring observational–model consistency prior to assimilation. The AVK application for TROPOMI employed here follows the methodology established for the IASI NH<sub>3</sub> version 4 product <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx104" id="paren.83"/>. The corrected column is calculated as:

              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M52" display="block"><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mi mathvariant="normal">m</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msup><mml:mo>-</mml:mo><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mo>∑</mml:mo><mml:mi>p</mml:mi></mml:msub><mml:msubsup><mml:mi>A</mml:mi><mml:mi>p</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msubsup><mml:msub><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi>B</mml:mi></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi mathvariant="normal">m</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> denotes the formaldehyde column adjusted with the model profile, <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> is the retrieved column based on the a priori profile, and <inline-formula><mml:math id="M55" display="inline"><mml:mi>B</mml:mi></mml:math></inline-formula> is the background concentration. The term <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:msubsup><mml:mi>A</mml:mi><mml:mi>p</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> represents the AVK at pressure level <inline-formula><mml:math id="M57" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the normalized model shape factor at the same level, defined as:

              <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M59" display="block"><mml:mrow><mml:msub><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>M</mml:mi><mml:mi>p</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msub><mml:mi>B</mml:mi><mml:mi>p</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msup><mml:mi>M</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msup><mml:mo>-</mml:mo><mml:mi>B</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

            The TROPOMI tropospheric columns were assimilated after application of GEOS-Chem shape profiles. These reprocessed tropospheric columns are shown in Fig. <xref ref-type="fig" rid="F1"/>d.1–d.4, with their vertical shape factors shown in Fig. <xref ref-type="fig" rid="F3"/> (green line) to illustrate the normalized contribution of each pressure layer to the tropospheric columns. We adopted tropospheric rather than total columns because the retrieval product itself provides tropospheric columns.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <label>2.3.3</label><title>Aura OMI</title>
      <p id="d2e1435">The Ozone Monitoring Instrument (OMI) is an important satellite instrument onboard the Aura satellite, launched on 15 July 2004, with the objective of monitoring atmospheric gases, aerosols, and clouds to improve our understanding of atmospheric chemistry and climate change. OMI provides daily global coverage with a wide swath of 2600 km and a spatial resolution of approximately 13 <inline-formula><mml:math id="M60" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 24 km at nadir, with an equator crossing time of about 13:45 LT. The sensor contains three spectral channels (UV-1, UV-2, and VIS), covering the wavelength ranges of 264–311, 307-383, and 349-504 nm, respectively, which enable the retrieval of key trace gases including O<sub>3</sub>, NO<sub>2</sub>, SO<sub>2</sub>, and formaldehyde <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx57" id="paren.84"/>.</p>
      <p id="d2e1475">In this study, we use the OMI/Aura formaldehyde Total Column Daily L2 Global Version 3 product <xref ref-type="bibr" rid="bib1.bibx13" id="paren.85"/>. In order to minimize the influence of poor-quality data, we applied strict quality filtering. Only pixels with cloud fraction <inline-formula><mml:math id="M64" display="inline"><mml:mo>⩽</mml:mo></mml:math></inline-formula> 0.3, solar zenith angle <inline-formula><mml:math id="M65" display="inline"><mml:mo>⩽</mml:mo></mml:math></inline-formula> 70°, and a main data quality flag <inline-formula><mml:math id="M66" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0 were retained. To avoid poor-quality measurements at large pixel sizes, the five marginal pixels on each side of the swath were discarded, and only pixels within rows 6–55 were used <xref ref-type="bibr" rid="bib1.bibx114 bib1.bibx108" id="paren.86"/>. Because OMI has experienced a row anomaly since 2007, pixels with Xtrack quality flags <inline-formula><mml:math id="M67" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0 were further selected to eliminate its impact. Additionally, given the large uncertainties in formaldehyde retrievals, pixels with a fitting root mean square (RMS) <inline-formula><mml:math id="M68" display="inline"><mml:mo>⩽</mml:mo></mml:math></inline-formula> 0.003 were retained to remove most outliers <xref ref-type="bibr" rid="bib1.bibx86" id="paren.87"/>.</p>
      <p id="d2e1523">The OMI observations are then aggregated to monthly means on a 0.5° <inline-formula><mml:math id="M69" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.625° grid, consistent with the GEOS-Chem model resolution. To ensure sufficient sampling per grid cell, we also applied two filtering schemes based on the number of observations, excluding grid cells with fewer than 10 or fewer than 50 valid pixels. Unlike OMPS and TROPOMI, however, OMI shows a strong reduction in data coverage under these constraints, and the product becomes sparse after applying the threshold of 50 observations. This indicates that OMI suffers from insufficient sampling density in China for high-resolution assimilation. The vertical profile correction of OMI formaldehyde was conducted using the same approach as applied to OMPS, by recalculating AMF with model-simulated vertical profiles. The resulting OMI columns after profile correction and the two data-volume filters are shown in Fig. S3.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Ozone ground station observation</title>
      <p id="d2e1543">This study aims to constrain the NMVOC emissions in China by assimilating multiple formaldehyde satellite products. As aforementioned, formaldehyde is an important precursor to ozone, the optimization of the NMVOC emission inventories and concentrations are supposed to improve the ozone simulation simultaneously. To evaluate the magnitude and quality of this impact, the ground level ozone concentrations from the National Urban Air Quality Real-time Publishing Platform of the China National Environmental Monitoring Center (CNEMC, last access: 15 May 2024) are used in the validation.  The ozone measurements utilized in this study are from 1602 sites across China. The MDA8 values of surface ozone observations are calculated based on the hourly data before they are compared against the model simulation. Results of the comparison will be described in Sect. 3.4.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Assimilation algorithm</title>
      <p id="d2e1554">This study employs the four-dimensional ensemble variational (4DEnVar) methodology to optimize NMVOC emissions with satellite formaldehyde observations. The goal of the assimilation is to find the most likely estimate of the state vector, which is the monthly NMVOC emission inventories <inline-formula><mml:math id="M70" display="inline"><mml:mi mathvariant="bold-italic">f</mml:mi></mml:math></inline-formula> over the entire model domain. Note that <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="bold-italic">f</mml:mi></mml:math></inline-formula> represents the vector of total NMVOC emissions, rather than separately gridded anthropogenic, biogenic, or biomass burning VOC emissions. To optimize emissions from these three sectors, additional observations or a well-defined spatial correlation structure are required, which are not available in this study. The prior estimate <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is from the inventories described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>, and the formaldehyde observations <inline-formula><mml:math id="M73" display="inline"><mml:mi mathvariant="bold-italic">y</mml:mi></mml:math></inline-formula> are described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS3"/>.  Mathematically, assimilation is performed via minimizing the cost function <inline-formula><mml:math id="M74" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> as follows:

            <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M75" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="script">J</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:msup><mml:mo>)</mml:mo><mml:mi>T</mml:mi></mml:msup><mml:msup><mml:mi mathvariant="bold">B</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced open="{" close="}"><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="script">H</mml:mi><mml:mi mathvariant="script">M</mml:mi><mml:mfenced close=")" open="("><mml:mi mathvariant="bold-italic">f</mml:mi></mml:mfenced></mml:mrow></mml:mfenced><mml:mi>T</mml:mi></mml:msup><mml:msup><mml:msup><mml:mi mathvariant="bold">O</mml:mi><mml:mo>-</mml:mo></mml:msup><mml:mn mathvariant="normal">1</mml:mn></mml:msup><mml:mfenced close="}" open="{"><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="script">H</mml:mi><mml:mi mathvariant="script">M</mml:mi><mml:mfenced open="(" close=")"><mml:mi mathvariant="bold-italic">f</mml:mi></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>

          The cost function <inline-formula><mml:math id="M76" display="inline"><mml:mi mathvariant="script">J</mml:mi></mml:math></inline-formula> is the sum of two parts: background and observation penal term. The background term quantifies the difference between the optimal <inline-formula><mml:math id="M77" display="inline"><mml:mi mathvariant="bold-italic">f</mml:mi></mml:math></inline-formula> and the prior emission inventories <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, while the observation term calculates the difference between the simulation driven by <inline-formula><mml:math id="M79" display="inline"><mml:mi mathvariant="bold-italic">f</mml:mi></mml:math></inline-formula> and the satellite observations <inline-formula><mml:math id="M80" display="inline"><mml:mi mathvariant="bold-italic">y</mml:mi></mml:math></inline-formula>. In addition to the <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> that represents the prior NMVOC emission vector calculated from the anthropogenic, biogenic, and biomass burning sources as been illustrated in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>. The uncertainty in the NMVOCs simulation is assumed to be attributed to errors in the emission inventories, and can be compensated using a spatially varying tuning factor <inline-formula><mml:math id="M82" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>:

            <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M83" display="block"><mml:mrow><mml:mi>f</mml:mi><mml:mfenced open="(" close=")"><mml:mi>i</mml:mi></mml:mfenced><mml:mo>=</mml:mo><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>i</mml:mi></mml:mfenced><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mfenced open="(" close=")"><mml:mi>i</mml:mi></mml:mfenced></mml:mrow></mml:math></disp-formula>

          in here <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>i</mml:mi></mml:mfenced></mml:mrow></mml:math></inline-formula> denotes the NMVOC emission rate in the given grid cell <inline-formula><mml:math id="M85" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>. The <inline-formula><mml:math id="M86" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> values are defined to be random variables with a mean of 1.0, a minimum of 0.1 and a standard deviation of 0.4, corresponding to a uniform 120 % uncertainty applied to the total NMVOC emissions rather than sector-specific settings as adopted in previous studies <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx47 bib1.bibx87" id="paren.88"/>. The rationale for this choice is provided in the Supplement. This empirical value was found to provide sufficient spaces for resolving the observation-minus-simulation errors. A background covariance <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">B</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is formulated as a product of the constant standard deviation and a spatial correlation matrix <inline-formula><mml:math id="M88" display="inline"><mml:mi mathvariant="bold">C</mml:mi></mml:math></inline-formula>:

            <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M89" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold">B</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mi mathvariant="bold">C</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mi mathvariant="bold">C</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula> represents a distance-based spatial correlation between two <inline-formula><mml:math id="M91" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>s in the grid cell <inline-formula><mml:math id="M92" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M93" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>, and is defined as:

            <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M94" display="block"><mml:mrow><mml:mi mathvariant="bold">C</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>/</mml:mo><mml:mi>l</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> represents the distance between two grid cells <inline-formula><mml:math id="M96" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M97" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M98" display="inline"><mml:mi>l</mml:mi></mml:math></inline-formula> here denotes the correlation length scale which controls the spatially variability freedom of the <inline-formula><mml:math id="M99" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>s. A small value of <inline-formula><mml:math id="M100" display="inline"><mml:mi>l</mml:mi></mml:math></inline-formula> indicates that the tuning factors <inline-formula><mml:math id="M101" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>s are less spatially correlated, thereby enabling emission optimization at a finer spatial scale. However, this also necessitates a larger number of ensemble runs to adequately represent the model realization from emission to simulation. An empirical parameter <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mi>l</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">300</mml:mn></mml:mrow></mml:math></inline-formula> km which is used in <xref ref-type="bibr" rid="bib1.bibx46" id="text.89"/> to nudge the ammonia emission that has a rapid spatially variability is also taken in this study. With the covariance matrix <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">B</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the NMVOC emission background covariance <inline-formula><mml:math id="M104" display="inline"><mml:mi mathvariant="bold">B</mml:mi></mml:math></inline-formula> is obtained via a Schur Product:

            <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M105" display="block"><mml:mrow><mml:mi mathvariant="bold">B</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">B</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub><mml:mo>∘</mml:mo><mml:mi mathvariant="bold">C</mml:mi></mml:mrow></mml:math></disp-formula>

          In the observation term, <inline-formula><mml:math id="M106" display="inline"><mml:mi mathvariant="bold-italic">y</mml:mi></mml:math></inline-formula> is the observation vector, representing satellite observations, <inline-formula><mml:math id="M107" display="inline"><mml:mi mathvariant="script">M</mml:mi></mml:math></inline-formula> is the GEOS-Chem model driven by emissions <inline-formula><mml:math id="M108" display="inline"><mml:mi mathvariant="bold-italic">f</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M109" display="inline"><mml:mi mathvariant="script">H</mml:mi></mml:math></inline-formula> is the observation operator that transfers the three-dimensional concentration into the observational space, and <inline-formula><mml:math id="M110" display="inline"><mml:mi mathvariant="bold">O</mml:mi></mml:math></inline-formula> is the observation covariance matrix. In this study, the assimilated observations include the OMPS total columns and TROPOMI tropospheric columns. A distinct observation operator <inline-formula><mml:math id="M111" display="inline"><mml:mi mathvariant="script">H</mml:mi></mml:math></inline-formula> is configured to enable a fair comparison of the observation-minus-simulation mismatch. The satellite formaldehyde observations are assumed to be independent, therefore <inline-formula><mml:math id="M112" display="inline"><mml:mi mathvariant="bold">O</mml:mi></mml:math></inline-formula> is a diagonal matrix. The diagonal value here is calculated as:

            <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M113" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>total</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>instrument</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>represent</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:msqrt></mml:mrow></mml:math></disp-formula>

          In Eq. (<xref ref-type="disp-formula" rid="Ch1.E12"/>), <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>total</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is defined as the total uncertainty, which is the square root of the sum of the squares of the instrument uncertainty <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>instrument</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> from the formaldehyde observations and the representative uncertainty <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>represent</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> introduced when processing the data into monthly averages. The representative uncertainty <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mtext>represent</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> is represented by the standard deviation of the data. The spatial distribution of the total uncertainty is provided in Fig. S2 in the Supplement.</p>
      <p id="d2e2219">The assimilation methodology used in this paper is the four-dimensional ensemble variational (4DEnVar). Different from the classic 4DVar that requires adjoint in the cost function minimization, 4DEnVar emulates the GEOS-Chem formaldehyde simulating model using an ensemble-based linear approximation and hence is adjoint-free. The method is first proposed by <xref ref-type="bibr" rid="bib1.bibx63" id="text.90"/> and successfully implemented in our recent dust aerosol <xref ref-type="bibr" rid="bib1.bibx45" id="paren.91"/> and ammonia emission inversion <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx104" id="paren.92"/>. The detailed procedures for minimizing the cost function Eq. (<xref ref-type="disp-formula" rid="Ch1.E7"/>) are illustrated in section “Minimization of the Cost Function in 4DEnVar” in the Supplement.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
      <p id="d2e2242">This section first presents the three satellite observations evaluation in terms of the vertical profile structure, qualified-data volume and monthly mean biases. Independent assimilations are then performed by either assimilating the OMPS or assimilating the TROPOMI retrievals independently. Posterior of the NMVOC emission, formaldehyde column results and the impact on ozone simulation are discussed. A consistency analysis is introduced to assess the reliability of the two posterior emission.</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Satellite data evaluation</title>
      <p id="d2e2252">Figure <xref ref-type="fig" rid="F3"/> shows the vertical profiles of formaldehyde shape factors used to compute the reported satellite vertical columns before any model-based profile correction is applied. Both the OMI and OMPS retrievals use GEOS-Chem model outputs as their a priori profiles <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx33 bib1.bibx71" id="paren.93"/>. Consequently, their shape factors are highly similar. formaldehyde shape factors generally decrease with altitude but exhibit characteristic peaks and troughs: a minimum at 750–850 hPa, a first peak <inline-formula><mml:math id="M118" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 30 hPa above it, a second prominent peak at 600–700 hPa, and a third peak near 350 hPa that is strongest in April and August and weaker in January and November. Above 350 hPa, shape factor decay toward zero. These features agree well with previously reported formaldehyde profile shapes over China <xref ref-type="bibr" rid="bib1.bibx113 bib1.bibx115" id="paren.94"/>. Overall, the OMPS profile most closely matches GEOS-Chem, whereas OMI shows slight peak shifts or spurious upper-level enhancements in some regions, particularly during May and August.</p>
      <p id="d2e2270">In contrast, the operational TROPOMI retrieval uses the a priori profiles from the TM5-MP model <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx25" id="paren.95"/>, which places substantially more mass near the surface. This results in a markedly different vertical structure: an approximately logarithmic monotonic decrease with altitude, with only minor perturbations over SCB (<inline-formula><mml:math id="M119" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 300 hPa) and PRD (<inline-formula><mml:math id="M120" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 800 hPa) and very high near-surface shape factor. These differences in a priori profile shape are the primary reason why profile correction is essential for meaningful satellite–model comparisons <xref ref-type="bibr" rid="bib1.bibx27" id="paren.96"/>.</p>
      <p id="d2e2293">Additionally, Fig. <xref ref-type="fig" rid="F3"/> clearly shows that stratospheric formaldehyde (<inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mo>∼</mml:mo></mml:mrow></mml:math></inline-formula> 200 hPa) can be largely neglected in both the GEOS-Chem simulation and the OMPS and TROPOMI retrievals     <xref ref-type="bibr" rid="bib1.bibx32 bib1.bibx24" id="paren.97"/>. Because the stratospheric contribution is negligible and no explicit stratospheric correction is applied in either retrieval, we hereafter use the term ”formaldehyde column” without distinguishing between total and tropospheric columns in subsequent discussion.</p>
      <p id="d2e2311">Uncertainty is a key component in the assimilation process and serves as a crucial indicator of satellite data quality. Fig. <xref ref-type="fig" rid="F3"/> illustrates the vertical distribution of retrieval uncertainties. In the mid- to upper troposphere (200–600 hPa), OMPS and OMI show comparable levels of uncertainty. However, below 600 hPa, OMPS uncertainties become substantially larger, likely due to cloud contamination and retrieval algorithm approximations <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx71" id="paren.98"/>. As shown in Supplement Fig. S2, the overall uncertainty of OMPS is significantly higher than that of the other two satellite datasets. At first glance, OMI data may appear superior, but this advantage largely results from strict filtering, which excludes a substantial fraction of problematic data. As illustrated in Supplement Fig. S3a, b, applying a threshold of 50 observations per grid cell drastically reduces spatial coverage, rendering OMI unsuitable for national-scale assimilation. Previous studies that assimilated OMI over China have typically interpolated the data to coarser resolutions to ensure applicability <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx69" id="paren.99"/>. Therefore, only OMPS and TROPOMI formaldehyde columns are assimilated in this study, while OMI is excluded for our high-resolution emission inversion due to the poor data coverage.</p>
      <p id="d2e2323">Figure <xref ref-type="fig" rid="F3"/> also presents satellite retrieval deviations from the prior model estimates. When all three satellite datasets exhibit the same sign of deviation (positive or negative) relative to the model, they are considered consistent. Such consistency is observed, for example, in February, May, and November over NCP and in February over PRD and SCB, where all three datasets show positive deviations; and in February and November over YRD and in August over SCB, where all show negative deviations. These cases indicate stronger reliability. In other situations, when OMPS and TROPOMI exhibit the same bias direction, they are also considered consistent, as in November over PRD and SCB. Overall, 10 out of 16 cases (62.5 %) exhibit consistency, with higher coherence primarily occurring in the cold season and during spring and autumn months over NCP and SCB. Subsequent analyses will explicitly consider this consistency to enhance the robustness of the conclusions.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>NMVOC emissions</title>
      <p id="d2e2336">The spatial characteristics of the NMVOC emissions in 2020 are clearly shown in Fig. <xref ref-type="fig" rid="F2"/> which presents the spatial distribution of four monthly average emissions from the prior simulation (a.1–a.4) and the posterior estimates constrained by OMPS (b.1–b.4) and TROPOMI (c.1–c.4) formaldehyde observations. Significant emission increments relative to the prior estimates are mainly concentrated in eastern and southern China. In most regions, the posterior results constrained by OMPS (d.1–d.4) and TROPOMI (e.1-e.4) exhibit broadly consistent adjustment patterns. However, notable differences between the two posterior estimates can still be observed, particularly over eastern China in August and southern China in May. The results reveal pronounced seasonal variability and regional heterogeneity in emission intensity, with the NCP, YRD, PRD, and SCB identified as major emission hotspots throughout the year.</p>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e2343">Monthly NMVOC emissions in 2020 from the prior simulation (blue) and the posterior simulations constrained by assimilating OMPS (red) and TROPOMI (green) formaldehyde observations. Panels show anthropogenic emissions <bold>(a)</bold>, biogenic emissions <bold>(b)</bold>, biomass burning emissions <bold>(c)</bold>, and total emissions <bold>(d)</bold>. The annual totals for each category are indicated in the legends.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f04.png"/>

        </fig>

      <p id="d2e2364">Although the major high-emission regions can be clearly identified, the complexity of emission source types and the wide range of emission magnitudes render the maps visually dense, making it difficult to directly interpret regional characteristics and seasonal changes. Therefore, subsequent analyses are focused on these four representative regions to enable a more detailed investigation. Figure <xref ref-type="fig" rid="F4"/> further displays the monthly and annual totals of NMVOC emissions across China in 2020. In general, the two posterior estimates exhibit good agreement for most months. Specifically, both show consistent decreases during January, February, and October to December, while simultaneous increases are observed from March to May. But notable discrepancies are observed during the June–September period, which account for approximately 83 % of the total annual difference between the two posterior datasets – with July and August alone contributing around 56 %. This leads to different estimates of annual emissions: the annual total constrained by OMPS assimilation is estimated at 40.82 Tg, while that constrained by TROPOMI is 34.83 Tg, both differing from the prior estimate of 39.26 Tg. To more accurately assess the regional emission responses under different observational constraints, the consistent and inconsistent months are discussed separately in the following sections.</p>
      <p id="d2e2370">In months with high consistency, January–February, during the transition from winter to spring, both assimilation results show a reduction in emissions, with anthropogenic emissions exhibiting a particularly significant decline. This may be because the emission inventory includes winter heating emissions, while the actual heating demand has been reduced due to global warming, resulting in an overestimation <xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx107" id="paren.100"/>. In spring, March-May, emissions gradually increase, likely driven by enhanced biogenic emissions due to rising temperatures and vigorous vegetation growth <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx70" id="paren.101"/>. After November, as the season shifts from autumn to winter, emissions decline again, with notable fluctuations in biogenic emissions in October, though anthropogenic emissions remain the primary contributor to the overall trend. In the inconsistent months (June–September, corresponding to summer and autumn), discrepancies arise between OMPS and TROPOMI results. These differences may arise from variations in emission characterization during summer, marked by strong convection, high humidity, and elevated cloud and aerosol content, which differentially impact the retrieval of optical depth and columns by OMPS and TROPOMI.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e2381">Monthly increments in total NMVOC emissions between the posterior and prior simulations derived from the assimilation of OMPS and TROPOMI formaldehyde observations over four key regions of China: the North China Plain, Yangtze River Delta, Pearl River Delta, and Sichuan Basin in 2020. Positive values indicate an increase in posterior emissions relative to the prior, while negative values indicate a decrease.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f05.png"/>

        </fig>

      <p id="d2e2390">A clear regional divergence in NMVOC emission increments after assimilation is revealed in Fig. <xref ref-type="fig" rid="F5"/>, with further analysis highlighting the sources of these discrepancies. In the NCP, OMPS assimilation results for July indicate a significant emission increase of 62.04 %, while TROPOMI shows a smaller increase. In August and September, the two datasets exhibit opposing trends. In contrast, increment differences are relatively minor in March–April, with OMPS assimilation results showing an increase of approximately 14 %, while TROPOMI remains largely unchanged. During January–February and November-December, both datasets display minimal changes. Overall, the prior inventory for the NCP appears underestimated in May–June. In the YRD, except for May and July, other months (e.g., June, August, and September) show opposing trends. In the PRD, nearly all months from March to September are classified as inconsistent. However, both regions demonstrate consistent emission reductions during the cold season, suggesting an overestimation in the a priori emission inventory for winter. In the SCB, negative emission increments during the warm season are particularly pronounced, generally exceeding 20 %, with reductions in June–July surpassing 35 %. During the cold season (January and October–December), both datasets show consistent declines with comparable values. Months with lower consistency are primarily concentrated in February-May, indicating a likely overestimation in the a priori emission inventory for this region.</p>
      <p id="d2e2395">In 2020, anthropogenic emissions in China were influenced by the COVID-19 pandemic, leading to observable changes. To better evaluate the general applicability of the proposed method, it is also necessary to conduct a comparative analysis for the pre-pandemic year of 2019. Fig. S5 in the Supplement presents the total NMVOC emission increments for the four major regions in 2019, based on data assimilation of OMPS and TROPOMI observations. In the NCP region, strong consistency is again observed in June, with posterior emissions increasing by 57.71 % and 30.09 % from OMPS and TROPOMI assimilation, respectively, further confirming the underestimation of prior emissions in this period. In the YRD, February, October, and November are identified as consistent months, aligning with the consistent periods in 2020, suggesting a likely overestimation in the prior inventory during these months. In the PRD region, consistency is found in January, February, June, July, November, and December, while in the SCB region, it occurs in January and from April to December. These consistent months largely overlap with those in 2020, though some differences are evident. For example, June and July emerge as new consistent months in PRD, while October and November remain consistent but exhibit notably smaller emission decreases compared to 2020. In SCB, April and May appear as additional consistent months, while the remaining consistent periods continue to exhibit decreases in emissions. Notably, from June to November, the two posterior datasets show an average decrease of 42.26 % compared to the prior emissions, indicating a high probability of overestimation in the prior inventory for this region during that period.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Formaldehyde columns evaluation</title>
      <p id="d2e2406">The spatial distributions of formaldehyde columns in February, May, August, and November 2020 are shown in Fig. <xref ref-type="fig" rid="F1"/>. Panels (a.1)–(a.4) display the prior simulations of formaldehyde columns, (b.1)–(b.4) present the posterior simulations of formaldehyde columns assimilated by OMPS, (c.1)–(c.4) show the OMPS satellite observations of formaldehyde columns, and (d.1)–(d.4) illustrate the TROPOMI satellite observations of formaldehyde columns. In addition, the prior and posterior simulations of formaldehyde columns for 2020 are also provided in the Supplement Fig. S7. Regarding the spatial patterns, high formaldehyde columns in February are concentrated in the NCP, YRD, and PRD regions, with the posterior results showing an expanded high-value area in the NCP but a reduced coverage in the YRD. In May, overall formaldehyde columns increase nationwide, with particularly pronounced growth in the NCP and PRD. In August, formaldehyde columns increase in the NCP, YRD, and PRD, while they decrease in the SCB. In November, the changes are modest, but all four regions exhibit reduced formaldehyde columns.</p>

      <fig id="F6" specific-use="star"><label>Figure 6</label><caption><p id="d2e2413">Scatter density plots comparing GEOS-Chem simulated formaldehyde columns with TROPOMI observations in 2020. Panels <bold>(a.1)</bold>–<bold>(e.1)</bold> show comparisons between prior simulations and TROPOMI, while panels <bold>(a.2)</bold>–<bold>(e.2)</bold> show comparisons between posterior simulations constrained by assimilating OMPS observations and TROPOMI. The regions considered are China <bold>(a)</bold>, the North China Plain <bold>(b)</bold>, the Yangtze River Delta <bold>(c)</bold>, the Pearl River Delta <bold>(d)</bold>, and the Sichuan Basin <bold>(e)</bold>. The probability density of the data points is indicated by the color scale. The correlation coefficient (<inline-formula><mml:math id="M122" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>), coefficient of determination (<inline-formula><mml:math id="M123" 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>), mean absolute error (MAE), root mean square error (RMSE), regression slope, and intercept are reported in each panel.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f06.png"/>

        </fig>

      <p id="d2e2468">The prior and OMPS-driven posterior simulations of formaldehyde columns were compared with the TROPOMI formaldehyde columns to evaluate the changes in formaldehyde. Scatter plots together with statistical metrics (<inline-formula><mml:math id="M124" 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>, <inline-formula><mml:math id="M125" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>, MAE, and RMSE) for the whole country and four subregions in 2020 are presented in Fig. <xref ref-type="fig" rid="F6"/>. The prior simulation already shows reasonably good performance (a.1)–(e.1), with most points distributed close to the <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line and exhibiting strong correlations with observations. Nevertheless, further improvements are still possible. After assimilating OMPS data, the posterior results compared with TROPOMI show higher <inline-formula><mml:math id="M127" 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> values across all regions, indicating strengthened correlations. For China and NCP, the improvements are comparable, with <inline-formula><mml:math id="M128" 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> increasing by about 0.027 (from 0.870 to 0.897 for China, and from 0.774 to 0.812 for NCP). In the YRD, the improvement is more pronounced, with <inline-formula><mml:math id="M129" 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> rising from 0.882 to 0.918, and the scatter around the regression line substantially reduced, with many outliers corrected. The most significant improvements occur in PRD and SCB, where <inline-formula><mml:math id="M130" 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> increases by approximately 0.05. In these regions, the overestimations present in the prior simulations are effectively mitigated, particularly for high-value cases. In terms of RMSE and MAE, decreases are observed in all regions except NCP. A comparison between Figures (b.1) and (b.2) indicates improvements in the low- and mid-value ranges, whereas substantial overestimations appear in the high-value range. This issue is likely related to the instrumental errors of OMPS observations, as discussed in Sects. <xref ref-type="sec" rid="Ch1.S2.SS3.SSS1"/> and <xref ref-type="sec" rid="Ch1.S3.SS2"/>, which introduce considerable uncertainties.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e2555">Monthly mean formaldehyde columns in 2020 from the prior simulation (gray), posterior simulations constrained by assimilating OMPS (black dashed) and TROPOMI (black dotted) observations, and satellite observations from OMPS (blue) and TROPOMI (green). Panels show results over China <bold>(a)</bold>, the North China Plain <bold>(b)</bold>, the Yangtze River Delta <bold>(c)</bold>, the Pearl River Delta <bold>(d)</bold>, and the Sichuan Basin <bold>(e)</bold>.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f07.png"/>

        </fig>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e2581">Monthly increments in <bold>(a)</bold> formaldehyde columns between posterior and prior simulations and <bold>(b)</bold> the relative changes in MDA8 ozone RMSE (<inline-formula><mml:math id="M131" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSE) after assimilating OMPS and TROPOMI observations in 2020. Results are shown for the North China Plain, Yangtze River Delta, Pearl River Delta, and Sichuan Basin. Positive values indicate an increase relative to the prior, while negative values indicate a decrease.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f08.png"/>

        </fig>

      <p id="d2e2603">The monthly mean formaldehyde columns for 2020, derived from the prior simulation, posterior simulations constrained by the OMPS and TROPOMI observations, and satellite observations from OMPS and TROPOMI, are presented for China (a), NCP (b), YRD (c), PRD (d), and SCB (e) in Fig. <xref ref-type="fig" rid="F7"/>. At the national scale, the overall changes resulting from assimilation are relatively modest, with the main adjustments occurring in summer and early autumn. The OMPS-driven posterior results show increases relative to the prior in June–July, whereas the TROPOMI-assimilated results exhibit decreases in July–August compared to the prior. These discrepancies may be attributed to differences between the satellite products in their responses to biogenic emissions and photochemical processes under high-temperature and high-radiation conditions <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx95" id="paren.102"/>.</p>
      <p id="d2e2611">Figure <xref ref-type="fig" rid="F8"/>a presents the increments between the posterior and prior simulations over the four regions when assimilating OMPS or TROPOMI observations, respectively. In the NCP, the posterior results constrained by both OMPS and TROPOMI show consistent increases in May–June, suggesting that the prior inventory may have underestimated the contributions from active photochemical production and anthropogenic emissions during summer <xref ref-type="bibr" rid="bib1.bibx98" id="paren.103"/>. In the YRD and PRD, stronger consistency is observed in the cold season (January–March and October–December), with both posterior results showing decreases, which is consistent with reduced anthropogenic activity and lower formaldehyde production rates under wintertime conditions. The SCB exhibits more distinct characteristics, with OMPS and TROPOMI assimilation results consistently showing decreases in the second half of the year, particularly pronounced in June, July, and October. This pattern suggests that the prior emissions in this region were overestimated. Previous studies have highlighted that the large uncertainties in biogenic emissions in the SCB are critical factors influencing the accuracy of NMVOC emissions and simulations  <xref ref-type="bibr" rid="bib1.bibx67" id="paren.104"/>.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Impact of formaldehyde assimilation on ozone surface concentration</title>
      <p id="d2e2631">The spatial distributions of observed MDA8 ozone at ground stations (a.1–a.4), together with the prior (b.1–b.4) and posterior simulations based on OMPS and TROPOMI assimilation (c.1–c.4, d.1–d.4), are shown in Fig. <xref ref-type="fig" rid="F9"/>. As shown in panels (b.1–b.4), pronounced ozone hotspots are observed in NCP (February, May, and August), YRD (May and August), PRD (May, August, and November), and SCB (May and August). This is very similar to the observations shown in panels (a.1–a.4). It indicates that the prior simulation captures the general patterns of ozone hotspots reasonably well, but notable biases remain. For example, ozone is clearly overestimated in PRD during February, May, and August, while underestimated in SCB during May and August. After assimilation with OMPS or TROPOMI, the posterior MDA8 ozone simulations retain the overall hotspot distribution, but the direction and magnitude of changes vary by region. For instance, in August, ozone concentrations increase in NCP and PRD with OMPS assimilation but decrease with TROPOMI assimilation. In February, both assimilation results decrease in YRD, although the decrease is more pronounced in the TROPOMI-based results. Moreover, many regional changes are difficult to discern visually from the spatial maps alone, highlighting the necessity of using statistical metrics to quantitatively assess ozone variations.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e2638">Spatial distributions of surface ozone concentrations in February, May, August, and November 2020. Panels <bold>(a.1)</bold>–<bold>(a.4)</bold> show ground-based observations, panels <bold>(b.1)</bold>–<bold>(b.4)</bold> show prior simulations, panels <bold>(c.1)</bold>–<bold>(c.4)</bold> show posterior simulations constrained by assimilating OMPS formaldehyde observations, and panels <bold>(d.1)</bold>–<bold>(d.4)</bold> show posterior simulations constrained by assimilating TROPOMI formaldehyde observations.</p></caption>
          <graphic xlink:href="https://acp.copernicus.org/articles/26/33/2026/acp-26-33-2026-f09.png"/>

        </fig>

      <p id="d2e2672">The RMSE values between the simulated MDA8 ozone and the ground-based observations are calculated. To better visualize the assimilation benefits, the RMSE variation either assimilating the TROPOMI or assimilating the OMPS in the four key regions are also shown in Fig. <xref ref-type="fig" rid="F8"/>b. Larger decreases in RMSE (darker blue) indicate more significant improvements, with the posterior ozone being closer to ground-based observations; conversely, larger increases in RMSE (darker red) indicate degraded performance, with the posterior ozone diverging further from the observations. In those inconsistent cases where the OMPS and TROPOMI posterior increments exhibit opposite signs (i.e., one increases while the other decreases), ozone simulation improvement is not guaranteed. For instance, in NCP during January-April and July, in YRD during June and September, and in PRD during April, May, August, and September, one assimilation leads to improvement while the other indicates deterioration. Moreover, in several additional months both posteriors even show degradation, making it difficult to effectively evaluate the improvement in posterior ozone simulations. By contrast, ozone simulation improvements are clearly observed in consistent cases where the OMPS- and TROPOMI-constrained posteriors exhibit the same sign (i.e., both reductions in <inline-formula><mml:math id="M132" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSE). In NCP, substantial improvements are observed in May and June, with the largest RMSE decrease in June, in agreement with the high-consistency pattern shown in Fig. <xref ref-type="fig" rid="F8"/>a. In YRD and PRD, RMSE decreases by more than 30 % in December, representing the most significant improvement; in addition, PRD also shows clear improvements in January and October. These improvement months all correspond to periods of high consistency. In SCB, RMSE also decreases markedly during high-consistency months, including January, June, July, and September–December.</p>
      <p id="d2e2687">To further quantify ozone simulation improvements in consistent regions, statistics were performed for the months classified as consistent. Considering the similarity in monthly behavior between YRD and PRD, the two regions were combined in the analysis. The results indicate that the consistent regions include NCP in May–June, YRD/PRD in January–March and October–December, and SCB in January and June–December. Within these regions, except for March and November in YRD/PRD and August in SCB, all other months show ozone simulation improvements. Overall, 13 out of the 16 consistent months exhibit improvements, accounting for 81.25 %, with an average RMSE reduction of 24.7 %. This result suggests that constraining NMVOC emissions through formaldehyde assimilation not only substantially improves formaldehyde simulations, but also exerts a positive impact on ozone simulations, with particularly significant improvements in regions and months characterized by high consistency.</p>
      <p id="d2e2690">To more robustly substantiate this conclusion, it is necessary to examine whether similar features can also be identified in 2019. In that year, OMPS and TROPOMI satellite observations were assimilated independently to constrain NMVOC emissions. The posterior-prior increments from the OMPS- and TROPOMI-driven assimilations, together with the changes in MDA8 ozone <inline-formula><mml:math id="M133" display="inline"><mml:mi mathvariant="normal">Δ</mml:mi></mml:math></inline-formula>RMSE, are presented in Fig. S6 of the Supplement. In NCP, March, May, and June are identified as consistent months, during which the ozone RMSE values decrease, with the most pronounced improvement occurring in June. In YRD, the consistent months are February, October, and November, where the ozone improvements are relatively limited but nevertheless show better agreement with ground-based observations. In PRD, the consistent months include January, February, and June–December; with the exception of August, September, and November, the ozone RMSE decreases in the other months, with notable improvements in June and July. In SCB, the two posterior datasets exhibit the highest level of consistency in 2019, with synchronous increases and decreases throughout the year. Ozone simulations in this region show better performance in all months except March and April, with particularly large improvements in June, July, and September–November, when the RMSE decreases by an average of 25.74 %.</p>
      <p id="d2e2700">Across the four regions, 27 months are classified as consistent in 2019. Of these, 22 months exhibit improved ozone simulations, which corresponds to 81.48 % of all consistent months, with both assimilations producing MDA8 ozone values closer to ground-based observations. This proportion differs from that of 2020 by only 0.23 %, providing further evidence that ozone improvements are particularly significant in the months defined as consistent across the four regions.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Summary and conclusion</title>
      <p id="d2e2712">In this study, satellite-based formaldehyde retrievals from OMPS and TROPOMI were assimilated to constrain NMVOC emissions over China in 2020. The results demonstrate that assimilation corrects systematic biases in prior emission inventories and improves the simulation of formaldehyde columns and surface ozone in general. More importantly, by analyzing the consistency of posterior results via assimilating different formaldehyde products across regions and months, this work establishes a methodological framework to further assess the reliability of emission estimates with multiple satellite constraints.</p>
      <p id="d2e2715">At the national scale, the OMPS- and TROPOMI-constrained posterior NMVOC emissions are broadly consistent across most months, with decreases in January–February and October–December and increases in March-May. The winter–spring decreases likely reflect overestimation of heating emissions in the prior inventory under reduced heating demand, whereas the spring increases are attributable to enhanced biogenic activity with rising temperatures. By contrast, notable discrepancies emerge in June–September – dominated by July–August – likely linked to strong convection, high humidity, and elevated cloud/aerosol loading that differentially affect retrievals. These discrepancies result in annual totals of 40.82 Tg (OMPS) and 34.83 Tg (TROPOMI), compared with 39.26 Tg in the prior. Regionally, NCP indicates prior underestimation in May–June consistently but pronounced divergences in July–September; YRD and PRD show warm-season inconsistencies but consistent cold-season decreases, suggesting wintertime overestimation in the prior inventory; SCB features substantial summer decreases (exceeding 20 %, particularly in June–July) alongside consistent winter decreases, while several spring months also point to possible prior overestimation.</p>
      <p id="d2e2718">Both the prior and the posterior simulations capture the spatial distribution of the formaldehyde columns well. When comparing the prior simulation and the posterior simulation constrained by OMPS with TROPOMI satellite observations, the prior already shows strong correlations, but further improvements are achieved after OMPS assimilation. The <inline-formula><mml:math id="M134" 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> increases from 0.870 to 0.897 at the national scale and from 0.774 to 0.812 in NCP; in YRD, the increase is larger, from 0.882 to 0.918; while the largest improvements are observed in PRD and SCB, with increases of about 0.05. Meanwhile, RMSE and MAE decrease in all regions except NCP. In NCP, the simulations improve in the low-to-middle value ranges, but overestimations remain in the high-value range, likely due to the large uncertainties introduced by OMPS instrumental errors.</p>
      <p id="d2e2732">For ozone, comparison with surface MDA8 observations highlights significant improvements in high-consistency regions. In NCP, RMSE reductions are most pronounced in June, consistent with the strong emission and formaldehyde adjustments in this period. In YRD and PRD, December RMSE reductions exceed 30 %, while additional improvements are found in PRD during January and October. In SCB, assimilation leads to persistent improvements from January through December, with notable reductions in June–July and the late autumn months. Overall, ozone improvements are observed in 13 of the 16 consistent months, which represent 81.25 % of the total, with an average RMSE reduction of 24.7 %.</p>
      <p id="d2e2736">To further test the robustness of our approach, OMPS and TROPOMI satellite observations were independently assimilated to constrain NMVOC emissions for 2019 (Fig. S4). The spatial distribution of formaldehyde hotspots is similar to 2020 but with overall higher formaldehyde columns. At the regional scale, most consistent months between OMPS- and TROPOMI-constrained results indicate that the prior inventory underestimates emissions in NCP and overestimates them in YRD, PRD, and SCB. Importantly, 22 of the 27 consistent months (81.48 %) show reduced ozone RMSE, with the largest improvements in SCB, confirming that consistent cases are strongly associated with enhanced ozone simulation performance. These findings also lend greater confidence to the optimized NMVOC emissions during the consistent months in these regions.</p>
      <p id="d2e2739">Future efforts should reassess assimilation performance with updated emission inventories and incorporate source-specific uncertainties, assigning different uncertainties to anthropogenic, biogenic, and biomass burning sectors, in order to better constrain their respective emissions. Moreover, because no independent validation data such as aircraft or FTIR measurements were available over China in 2020, future studies could further evaluate the assimilation results once such observational datasets become accessible.</p>
</sec>

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

      <p id="d2e2747">The 4DEnVar emission inversion system is in the Python environment and is archived on Zenodo. (<ext-link xlink:href="https://doi.org/10.5281/zenodo.14633919" ext-link-type="DOI">10.5281/zenodo.14633919</ext-link>; <xref ref-type="bibr" rid="bib1.bibx106" id="altparen.105"/>). OMPS-N20 Level 2 NM formaldehyde Total Column swath orbital Version 1 product (<ext-link xlink:href="https://doi.org/10.5067/CIYXT9A4I2F4" ext-link-type="DOI">10.5067/CIYXT9A4I2F4</ext-link>, <xref ref-type="bibr" rid="bib1.bibx1" id="altparen.106"/>). Sentinel-5P TROPOMI Level 2 Tropospheric formaldehyde Version 2 product (<ext-link xlink:href="https://doi.org/10.5270/S5P-vg1i7t0" ext-link-type="DOI">10.5270/S5P-vg1i7t0</ext-link>, <xref ref-type="bibr" rid="bib1.bibx19" id="altparen.107"/>). OMI/Aura formaldehyde Total Column Daily L2 Global Version 3 product (<ext-link xlink:href="https://doi.org/10.5067/Aura/OMI/DATA2016" ext-link-type="DOI">10.5067/Aura/OMI/DATA2016</ext-link>, <xref ref-type="bibr" rid="bib1.bibx13" id="altparen.108"/>). National Urban Air Quality Real-time Publishing Platform of the China National Environmental Monitoring Center (CNEMC, <uri>https://air.cnemc.cn:18007/</uri>, last access: 15 May 2024).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d2e2778">The supplement related to this article is available online at <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-26-33-2026-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-26-33-2026-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e2787">JJ conceived the study and designed the emission inversion method. JJ wrote the code of the emission inversion. CX carried out the analysis and evaluation. KL, YQ, JX, ZC, HXL and HL provided useful comments on the paper. CX and JJ prepared the manuscript with contributions from all other co-authors.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e2793">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="d2e2799">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. The authors bear the ultimate responsibility for providing appropriate place names. 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="d2e2805">We thank for the technical support of the National Large Scientific and Technological Infrastructure “Earth System Numerical Simulation Facility” (<uri>https://cstr.cn/31134.02.EL</uri>, last access: 23 December 2025).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e2813">This study was supported by the National Key Research and Development Program of China [grant number 2022YFE0136100], the National Natural Science Foundation of China [grant number 42475150], and the Postgraduate Research &amp; Practice Innovation Program of Jiangsu Province [grant number KYCX24_1528].</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e2819">This paper was edited by Andreas Richter and reviewed by two anonymous referees.</p>
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