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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-23-6647-2023</article-id><title-group><article-title>Implications of differences between recent anthropogenic aerosol
emission inventories for diagnosed AOD and radiative forcing from 1990 to 2019</article-title><alt-title>Implications of differences between recent anthropogenic aerosol emission inventories</alt-title>
      </title-group><?xmltex \runningtitle{Implications of differences between recent anthropogenic aerosol emission inventories}?><?xmltex \runningauthor{M.~T.~Lund et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Lund</surname><given-names>Marianne Tronstad</given-names></name>
          <email>m.t.lund@cicero.oslo.no</email>
        <ext-link>https://orcid.org/0000-0001-9911-4160</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Myhre</surname><given-names>Gunnar</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4309-476X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Skeie</surname><given-names>Ragnhild Bieltvedt</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1246-4446</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Samset</surname><given-names>Bjørn Hallvard</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8013-1833</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Klimont</surname><given-names>Zbigniew</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>CICERO Center for International Climate Research, Oslo, Norway</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Pollution Management Research Group, International Institute for Applied Systems Analysis (IIASA), Laxenburg, Austria</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Marianne Tronstad Lund (m.t.lund@cicero.oslo.no)</corresp></author-notes><pub-date><day>19</day><month>June</month><year>2023</year></pub-date>
      
      <volume>23</volume>
      <issue>12</issue>
      <fpage>6647</fpage><lpage>6662</lpage>
      <history>
        <date date-type="received"><day>9</day><month>September</month><year>2022</year></date>
           <date date-type="rev-request"><day>4</day><month>October</month><year>2022</year></date>
           <date date-type="rev-recd"><day>17</day><month>February</month><year>2023</year></date>
           <date date-type="accepted"><day>30</day><month>April</month><year>2023</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2023 </copyright-statement>
        <copyright-year>2023</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/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e125">This study focuses on implications of differences between recent global emissions inventories for simulated trends in anthropogenic aerosol abundances and radiative forcing (RF) over the 1990–2019 period. We use the ECLIPSE version 6 (ECLv6) and CEDS year 2021 release (CEDS21) as input to the chemical transport model OsloCTM3 and compare the resulting aerosol evolution to corresponding results derived with the first CEDS release, as well as to observed trends in regional and global aerosol optical depth (AOD). Using CEDS21 and ECLv6 results in a 3 % and 6 % lower global mean AOD compared to CEDS in 2014, primarily driven by differences over China and India, where the area average AOD is up to 30 % lower. These differences are considerably larger than the satellite-derived interannual variability in AOD. A negative linear trend over 2005–2017 in global AOD following changes in anthropogenic emissions is found with all three inventories but is markedly stronger with CEDS21 and ECLv6. Furthermore, we confirm that the model better captures the sign and strength of the observed AOD trend over China with CEDS21 and ECLv6 compared to using CEDS, while the opposite is the case for South Asia. We estimate a net global mean aerosol-induced RF in 2014 relative to 1990 of 0.08 W m<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CEDS21 and 0.12 W m<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for ECLv6, compared to 0.03 W m<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> with CEDS. Using CEDS21, we also estimate the RF in 2019 relative to 1990 to be 0.10 W m<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, reflecting the continuing decreasing trend in aerosol loads post-2014. Our results facilitate more rigorous comparison between existing and upcoming studies of climate and health effects of aerosols using different emission inventories.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>Norges Forskningsråd</funding-source>
<award-id>248834</award-id>
<award-id>314997</award-id>
<award-id>324182</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="d1e185">Human activities have led to a substantial increase in atmospheric
abundances of aerosols relative to pre-industrial conditions. While
increasing emissions of greenhouse gases is the dominant driver of recent
global warming, aerosols play a key role in shaping regional and global
climate through their interactions with radiation and clouds. The Sixth Assessment Report (AR6) of the
Intergovernmental Panel on Climate Change (IPCC) estimates that changes in
atmospheric aerosols have contributed an effective radiative forcing (ERF)
of <inline-formula><mml:math id="M5" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.3 W m<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> over the industrial era (1750–2014), albeit with a
wide uncertainty range of <inline-formula><mml:math id="M7" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.0 to <inline-formula><mml:math id="M8" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.6 W m<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Forster et al.,
2021).</p>
      <p id="d1e233">Over recent decades, anthropogenic emissions of aerosols and their precursor
gases have changed rapidly, with substantial spatiotemporal heterogeneity,
particularly in Asia. Following decades of rapid economic growth in China,
the combustion of coal, other fossil fuels, and biofuels increased
considerably, resulting in the region becoming the dominant source of air
pollution emissions. However, since the adoption of national action
plans targeting particulate matter levels (i.e., Air Pollution Prevention and
Control in 2013 (SCPRC, 2013) and Winning the Blue Sky Defense
Battle in 2018; SCPRC, 2018), emissions of sulfur dioxide
(<inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and then nitrogen oxide (<inline-formula><mml:math id="M11" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) in China have declined rapidly<?pagebreak page6648?> (Klimont et al., 2013, 2017; Tong et al., 2020; Zheng et
al., 2018). Recent studies suggest that black carbon (BC) emissions are
also declining (Kanaya et al., 2020; Zheng et al., 2018). A strong growth in
emissions of <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and other pollutants has been seen in South Asia
(Kurokawa and Ohara, 2020), resulting, according to
studies, in India overtaking China as the dominant emitter of <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
(Li et al., 2017). These contrasting trends have given rise to a
distinct dipole pattern of increasing and declining aerosol optical depth
over South and East Asia, respectively, visible in satellite data
(Samset et al., 2019). Such rapid changes are likely to affect the
climate of the regions, as aerosols have been shown to have a notable
influence on regional temperature and precipitation, including extremes
(e.g., Bollasina et al., 2011; Hegerl et al., 2019; Marvel et al., 2020;
Samset et al., 2018; Sillmann et al., 2013), with different responses to
scattering and absorbing aerosols. However, the exact nature and magnitude
of such climate implications need to be better quantified (Persad
et al., 2022).</p>
      <p id="d1e280">Robust quantification of the impacts of aerosols requires reliable and
consistent estimates of anthropogenic emissions. However, currently there
exist substantial differences, in both magnitudes and trends, between
available emission inventories (e.g., Crippa et al., 2018; Elguindi et
al., 2020; Smith et al., 2022). Emission inventories are quantifications of
contributions from various industrial processes or other anthropogenic
activities to the rate of emissions of various compounds to the atmosphere.
They generally combine bottom-up information such as reported economic
activities with direct observations and process modeling and are used
extensively in essentially all efforts to quantify climate and air quality
implications of human activities. While the overall scientific uncertainty
on aerosol-induced global mean radiative forcing (RF) is larger than the
estimated regional changes, the uncertainty also varies over recent
decades depending on the overall level of emissions and their location
relative to cloud decks and other climate features (Bellouin et al.,
2020; Regayre et al., 2014; Samset et al., 2019; Szopa et al., 2021). Hence,
understanding both the inherent inventory differences and the implications
of these for downstream calculations and modeled quantities such as aerosol
optical depths and radiative forcing is crucial.</p>
      <p id="d1e283">As an example, a critical issue that has recently been highlighted is a
notable underestimation of the decline in Chinese emissions of <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M15" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and overestimation of carbonaceous aerosol emissions in Asia and
Africa in the Community Emissions Data System (CEDS) developed for the sixth
cycle of the Coupled Model Intercomparison Project (CMIP6)
(Szopa et al., 2021).
Recent work has shown that results from the CMIP6 experiments fail to fully
capture the observed recent trends in aerosol optical depth (AOD) in Asia
(Cherian and Quaas, 2020; Ramachandran et al., 2022; Su et al., 2021;
Wang et al., 2021), with the discrepancy largely attributed to the
misrepresentation of emissions in the region in the last decade of the
historical CMIP6 period. Other studies demonstrate that the poor
representation of observed aerosol trends can propagate to further
uncertainties in attribution of aerosol-induced impacts, such as the East
Asian monsoon (Wang et al., 2022) and health impacts
(Cheng et al., 2021). In addition to CMIP6, the CEDS emissions
have also been used in individual model studies of historical aerosol
evolution, radiative forcing, sector attribution, and air quality
assessments (e.g., Bauer et al., 2020; Chowdhury et al., 2022; Lund et
al., 2018, 2020; Paulot et al., 2018). Moreover, uncertainties
and biases in the baseline historical inventory may influence scenario-based
assessments of near-term future regional climate risk.</p>
      <p id="d1e309">Since the initial parts of the CMIP6 exercise, the CEDS inventory has
undergone several revisions. The most recent version from 2021, covering the
period up to 2019, exhibits several key differences compared to the initial
release – for some species all the way back to the early 2000s. More
specifically, emissions of BC, OC, and <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are all substantially lower in the
update, in global totals and, particularly, in Asia, and the decreasing
trend in Chinese <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is more pronounced. However, the implications of
these differences in input data for simulated anthropogenic aerosol
distributions, globally and regionally, and the resulting radiative forcing
have not been fully quantified and cannot be directly extrapolated.
Furthermore, as the update to CEDS came too late for uptake in IPCC AR6, it
is pertinent to ask if the influence of these emission inventory differences
affected the assessed evolution of atmospheric aerosol trends and subsequent
climate implications.</p>
      <p id="d1e334">Here, we present an investigation of the implications of known differences
in recent emission inventories for quantified aerosol burdens, optical depth,
and radiative forcing, over the period 1990–2019. Using the chemical
transport model OsloCTM3, we perform simulations with the CEDS21 emission
inventory and compare it to previously published results derived from the
original CEDS release (Lund et al., 2018, 2019). We also
perform simulations with a third recent global inventory, the Evaluating the Climate and Air Quality Impacts of Short-Lived Pollutants (ECLIPSE)
version 6b, where emissions are similar in evolution but generally even
lower than in CEDS21, especially in the most recent period. We explore the
differences in the simulated evolution of global and regional anthropogenic
aerosol loads between experiments using the different inventories, comparing
optical depth to remote sensing observations, and quantify the resulting
radiative forcing. Our aims are to document the model's ability to represent
recent observed aerosol trends and to quantify the implications of
differences in inventories available to the community for downstream
diagnosed quantities critical for assessing the air quality and climate
implications of anthropogenic aerosol.</p>
</sec>
<?pagebreak page6649?><sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
      <p id="d1e345">Atmospheric concentrations of aerosols are simulated with the global
chemical transport model OsloCTM3 (Lund et al., 2018; Søvde et al.,
2012). The model is driven by meteorological data from the European Centre
for Medium-Range Weather Forecast (ECMWF) OpenIFS model updated every 3 h and is run in a 2.25<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M19" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.25<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> horizontal
resolution, with 60 vertical levels (the uppermost centered at 0.1 hPa).
OsloCTM3 treats tropospheric and stratospheric chemistry, as well as modules
for carbonaceous, secondary organic, sulfate, ammonium nitrate, sea salt, and
dust aerosols. Aerosols are scavenged by convective and large-scale rain
(ice and liquid phase), with rainfall calculated from ECMWF data for
convective activity, cloud fraction, and rainfall. Dry deposition applies
prescribed deposition velocities for different land cover types. For further
details we refer to Lund et al. (2018) and Søvde et al. (2012).</p>
      <p id="d1e373">The aerosol optical depth (AOD) and instantaneous top-of-atmosphere
radiative forcing due to aerosol–radiation interactions (RFari) are
calculated offline using a multi-stream model with the discrete ordinate
method DISORT (Myhre et al., 2013; Stamnes et al., 1988). The same
radiative transfer model is also used to estimate the radiative forcing of
aerosol–cloud interactions (RFaci) (earlier denoted the cloud albedo effect
or Twomey effect). To account for the change in cloud droplet concentration
resulting from anthropogenic aerosols, which alter the cloud effective
radius and thus the optical properties of the clouds, the approach from
Quaas et al. (2006) is used. Briefly, this approach is
based on a statistical relationship between cloud droplet number
concentrations and fine-mode AOD derived from satellite data from the
MODerate Resolution Imaging Spectroradiometer (MODIS).</p>
      <p id="d1e376">Modeled AOD is compared with retrievals from the MODIS instrument on the
Aqua satellite, which is available for the period 2003–2020
(MOD08, 2018). We use the combined Dark Target and Deep Blue AOD
at 550 nm, release version MOD08 M3 v6.1, downloaded
from NASA's Giovanni interface. The MODIS Terra AOD is also available for the
same period and is, for most years, around 10 % lower than MODIS Aqua on
a global average. However, based on previous evaluations of the MODIS AOD and a
reported drift in the Terra data (Levy et al., 2010; Sherman et al.,
2017), we choose to use MODIS Aqua for the model comparison in the current
study. Temporal trends in the simulated and observed AOD are estimated on
a global mean and grid point basis by linear least-square fitting and defined
as statistically significant (from no trend) when the linear Pearson
correlation coefficient is significant at the 0.05 level. To minimize the
influence of individual years, e.g., with higher biomass burning influence,
we calculate a set of trends removing one year at a time from the sample
and then take the average of this set of coefficients. Interannual
variability is estimated on a grid point basis as the standard deviation of
the residual when subtracting a 10-year boxcar average (with mirrored data
around the end points). We also compare modeled AOD with ground-based
measurements from the AErosol RObotic NETwork (AERONET)
(Holben et al., 1998) version 3 level-2.0
retrievals at 500 nm. The comparison uses all available data from all months
and stations for a given year, with modeled AOD linearly interpolated to the
latitude and longitude of each station.</p>
      <p id="d1e379">Five different time series of simulated aerosol distributions covering the
1990–2019 period are included in this analysis, using three different
emission inventories and either fixed or actual (i.e., corresponding to the
emission year) meteorology. The fixed meteorology runs form the basis for
investigating differences in simulated anthropogenic aerosol and
corresponding RF, while the latter is used in the comparison with observed
AOD. Table 1 provides a summary of the experiments.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e386">Summary of experiments used in the study.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Name</oasis:entry>
         <oasis:entry colname="col2">Description</oasis:entry>
         <oasis:entry colname="col3">Years simulated</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">CEDS</oasis:entry>
         <oasis:entry colname="col2">CEDS v2016 emissions, fixed meteorology</oasis:entry>
         <oasis:entry colname="col3">1990, 1995, 2000, 2005, 2010, 2014</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CEDS21</oasis:entry>
         <oasis:entry colname="col2">CEDS v2021 emissions, fixed meteorology</oasis:entry>
         <oasis:entry colname="col3">1990, 1995, 2000, 2005, 2010, 2014, 2016, 2018, 2019</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ECLv6</oasis:entry>
         <oasis:entry colname="col2">ECLIPSEv6b emissions, fixed meteorology</oasis:entry>
         <oasis:entry colname="col3">1990, 1995, 2000, 2005, 2010, 2014, 2016</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CEDSmet</oasis:entry>
         <oasis:entry colname="col2">CEDS v2017 emissions until 2014 and SSP2-4.5</oasis:entry>
         <oasis:entry colname="col3">1990–2017</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">for 2015–2017, running meteorology</oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CEDS21met</oasis:entry>
         <oasis:entry colname="col2">CEDS v2021 emissions, running meteorology</oasis:entry>
         <oasis:entry colname="col3">2001–2017</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><?xmltex \gdef\@currentlabel{1}?></table-wrap>

      <p id="d1e489">Two sets of fixed meteorology simulations are performed using anthropogenic
emissions from CEDS version 2021 (O'Rourke et
al., 2021) (CEDS21) and ECLIPSEv6b (ECLv6) inventories.
The ECLv6 emissions are developed with the Greenhouse Gas–Air Pollution
Interactions and Synergies (GAINS) model (Amann et al., 2011). Version 6b
(IIASA, 2022) consists of gridded aerosol and reactive gas emissions
in 5-year intervals over the period 1990–2015, as well as emissions for
2008, 2009, 2014, and 2016. The Community Emissions Data System (CEDS)
inventory has provided a gridded inventory of anthropogenic greenhouse gas,
reactive gases, and aerosols since 1750 (Hoesly et al., 2018). In
the first release, the most recent year was 2014, while the 2021 release
covers the period until 2019. Simulations are performed for 1990, 1995,
2000, 2005, 2010, 2014, and 2016 emissions, as well as the years 2018 and 2019
for CEDS21. Results from the current study are compared with previously
published results from simulations over 1990 to 2014 performed with the
first release of the CEDS emissions (Lund et al., 2018) and three of the Shared Socioeconomic Pathway (SSP)
scenarios (SSP1-1.9, SSP2-4.5, and SSP3-7.0) from 2015 to 2100 (here we use
data for 2020 and 2030) (Lund et al., 2019). These
three scenarios broadly span the range of aerosol and precursor emissions
projected in the SSPs. In line with the experimental design in
Lund et al. (2018), we use the year 2010
meteorological data, and each simulation is run for 1 year, with 6 months'
spin-up. All three time series use biomass burning emissions from
van Marle et al. (2017) from
1990 to 2014 and the Global Fire Emissions Database version 4 (GFED4,
Randerson et al., 2017) thereafter. We note that
van Marle et al.'s (2017)
emissions are also based on GFED. Other natural emissions (dust and sea salt
aerosols, precursor gases from the ocean, soil, and vegetation) are fixed at
the year 2010 levels.</p>
      <p id="d1e492">For the comparison with MODIS data, we use a time series of OsloCTM3
simulations with CEDS emissions and actual meteorology covering the period
1990–2017 (the last 3 years use Shared Socioeconomic Pathway (SSP)
2-4.5 emissions<?pagebreak page6650?> (Fricko et al., 2017) linearly interpolated
between 2015 and 2020) (hereafter CEDSmet). These simulations were originally
performed for phase III of the AeroCom project (e.g., Gliß et al.,
2021). For the present study, we also produce an updated version covering
the 2001–2017 period using CEDS version 2021 emissions (hereafter
CEDS21met). While differences in emissions also exist in the years prior, we restrict
the use of resources by only going back to the start of the MODIS record,
covering the period when the differences are most pronounced. In these
simulations, the other natural aerosol emissions also vary following the
meteorological year.</p>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
      <p id="d1e503">Here we first document the differences in simulated global and regional
aerosol abundances and trends arising from the spread between emission
inventories. We then investigate how AOD diagnosed from experiments using
old and new emission estimates compare with observed AOD. Finally, we
present updated estimates of radiative forcing relative to 1990.</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Influence of emission inventory differences on simulated aerosol
distributions</title>
      <p id="d1e513">Figure 1 shows global total emissions of <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, BC, OC, <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, ammonium
(<inline-formula><mml:math id="M23" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), and non-methane volatile organic compound (NMVOC) over the
1990–2019 period in the inventories used here. The differences are
particularly pronounced after 2005. Both ECLv6 and CEDS21 show substantially
lower emissions of most species during this period, relative to CEDS. In
2014, the largest relative differences between CEDS21 and CEDS are in BC and
OC emissions, where CEDS21 is 20 %–30 % lower. For <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M25" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and NMVOC,
the corresponding number is approximately 10 %. ECLv6 is generally lower
than both CEDS inventories, particularly for <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and NMVOC, by about
30 %. While not used in this study, we also note that similar differences
have also been found between CEDS and two other recent global inventories,
the Emissions Database for Global Atmospheric Research (EDGAR) version 5
(Crippa et al., 2020) and Hemispheric Transport of Air Pollution
(HTAP) version 3 (Crippa et al., 2022).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e585">Global total anthropogenic emissions of <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, BC, OC, <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and NMVOC in the CEDS21, ECLv6, and CEDS inventories for the period 1990 to the most recent inventory year (2019, 2016, and 2014, respectively). Dotted lines show emissions from the SSP2-4.5 scenario, linearly interpolated from 2015 to 2019.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/6647/2023/acp-23-6647-2023-f01.png"/>

        </fig>

      <?pagebreak page6651?><p id="d1e627">Important geographical distinctions underlie these global differences, as
demonstrated in Fig. S1 for selected main source regions. While a
comprehensive investigation of causes for the inventory differences is
beyond the scope of the present study, and can be difficult due to the
number of underlying assumptions, input data, and revisions, we discuss some
key features here. All three inventories rely on the energy statistical data
from the International Energy Agency (IEA); however, there are differences in
assumptions about emission rates, implementation of policies, and data on
non-energy sources. The ECLv6 estimates include explicit representation of
air quality policies and their implementation efficiency, drawing on
national information and, if not available, extrapolation of trends
considering capacity replacement (e.g., new vehicles, newly built power
plant capacity) and emission performance of these new technologies. The
result is, among other things, estimated faster decline of <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
emissions from power and industry (in turn in total emissions) in China over
recent years than in CEDS (Fig. S1a, d). This decline has also  been confirmed
in Zheng et al. (2018). CEDS21 made a
correction to CEDS, mirroring the estimates in the GAINS model for ECLv6. In
South Asia, dominated by India, ECLv6 and CEDS21 show a  difference similar
to CEDS emissions in <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, representing the use of updated emission
characteristics for coal power plants. India has had a slower economic
growth and less heavy industry than China. While some policies aimed at
controlling <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from transport have been introduced, the limited polices in
the power and industry sector have resulted in increasing Indian <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
and <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> emissions, but the growth has been slower than that in China in the
2000s. For BC and OC (Fig. S1b, c), the largest inventory differences are
found in East Asia, mainly China, owing to differences in estimates of
emissions from coal use in industries, with ECLv6 applying the lowest emission
factors, and from open burning of municipal waste. For the latter category,
CEDS has originally relied on the rather high estimates of waste generation
and share of generated waste that is burnt (using Wiedinmyer et al., 2014), while ECLv6 used
independently estimated generation rates (Gómez-Sanabria et al.,
2022). The declining BC trends in East Asia, as shown in ECLv6 and CEDS21,
have been supported by measurements (e.g.,
Kanaya et al., 2020). Estimates for some species, e.g., <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, are often
based on very similar sources of information, as, apart from in Europe and
North America, these have received less attention from policymakers and
measurement (emissions) communities. Consequently, estimates are similar
across all inventories at the aggregated regional level (Fig. S1e). Aside
from East and South Asia, the overall temporal evolution is generally
similar in the main source regions across inventories, although magnitudes
can differ.</p>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>Global and regional aerosol burdens in 2014</title>
      <p id="d1e727">The differences between inventories are substantial enough to influence
simulated aerosol burdens (i.e., column-integrated aerosol mass, in mg m<inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> at the global mean level. For 2014, i.e., the most recent common
year for all three emission inventories, we estimate 4 % and 8 % lower
global mean burdens of total BC when using CEDS21 and ECLv6 (6 % and
11 % if considering aerosols only from fossil fuel and biofuel
combustion), respectively, compared to CEDS (Table S1). For primary organic
aerosol (POA), the corresponding numbers are 11 % and 13 % (30 % and
40 %), while the global mean total sulfate burden is 8 % and 15 % lower
with CEDS21 and ECLv6. Smaller reductions of the order of 3 %–4 % are also
seen in the global mean SOA burden. Biogenic VOC emissions, the main source
of SOA, are the same in all simulations. However, the SOA abundance is
affected by the lower emissions of anthropogenic VOCs in both CEDS21 and
ECLv6 than in CEDS (Fig. 1), as well as by the lower amount of POAs, which serve
as substrates for SOA formation.</p>
      <p id="d1e745">For all these aerosol species, the burden differences are consistently
the largest over East Asia, followed by South Asia, and larger for ECLv6 than
for CEDS21. Figure 2 shows the absolute regional mean burden (with corresponding
relative changes given in Fig. S3). Regions considered are East Asia (EAS),
South Asia (SAS), sub-Saharan Africa (SAF), North America (NAM), South
America (SAM), North Africa and the Middle East (NAF), Europe (EUR),
Southeast Asia (SEA), and Russia (RBU) (see also Fig. S2). For EAS, the new
simulated burden of BC and POA is 30 %–40 % lower, depending on inventory,
compared to simulations using CEDS, following 50 %–60 % lower BC and OC
emissions. The 40 %–50 % lower <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions translate to a 20 %–30 %
lower regional sulfate burden in our simulations. A similar relationship
between emission and burden differences is simulated for SAS, where the
burdens of BC, POA, and sulfate are 6 %, 27 %, and 30 % lower,
respectively, in experiments with ECLv6 than with CEDS. Lower burdens of
sulfate and POA are simulated for all other regions as well and in
particular over NAF with ECLv6. In some regions, like SAM, NAF, and SAF, the
new inventories estimate 20 %–30 % lower BC emissions than CEDS; however,
due to the lower absolute magnitudes, the simulated burden differences are
small compared to other aerosols. We note that regional burdens can be
influenced by long-range transport and thus affected by inventory
differences outside the main source region. We also note that we find
differences in surface concentrations between simulations that are broadly
similar to the burden changes. While beyond the scope of the present study,
this may have implications for assessments of air-pollution-related health
impacts.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e761">Absolute difference in the regional mean burden of the key anthropogenic aerosol species between simulations with CEDS21 and CEDS (upper bar) and ECLv6 and CEDS (lower bar). Regions are the same as in Lund et al. (2019): EAS, East Asia; SAS, South Asia; SAF, sub-Saharan Africa; NAM, North America; SAM, South America; NAF, North Africa and the Middle East; EUR, Europe; SEA, South East Asia; and RBU, Russia.</p></caption>
            <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/6647/2023/acp-23-6647-2023-f02.png"/>

          </fig>

      <p id="d1e771">The only species that is globally more abundant in simulations with the two
new inventories is nitrate. There is considerable regional heterogeneity,
where the burden is lower compared to the CEDS experiments in South Asia and
on the US east coast but higher in the US Midwest; parts of Africa and South
America; and, especially, over East Asia (Figs. 2 and S3). While absolute
differences are small in many regions compared to other species, the net
effect is nevertheless a 15 % and 24 % higher global mean nitrate burden
with CEDS21 and ECLv6, respectively, compared to using CEDS emissions.
Changes in the atmospheric nitrate distribution result from a complex
interplay between differences in emissions of <inline-formula><mml:math id="M40" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.
Studies have also shown that<?pagebreak page6652?> nitrate formation can be influenced by
background concentrations of VOCs (e.g.,
Womack et al., 2019) We find the largest absolute difference in nitrate in
EAS and SAS, however, of opposite sign. In EAS, emissions of <inline-formula><mml:math id="M43" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M44" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are both lower in ECLv6 and CEDS21 than in CEDS, whereas <inline-formula><mml:math id="M45" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
emissions are higher (Figs. 1 and S1). This results in lower chemical
competition for available sulfate and, in turn, enhanced formation of
nitrate aerosol. In SAS, <inline-formula><mml:math id="M46" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are all lower in the
two new inventories than in CEDS, as is the nitrate burden. Differences in
concentrations of VOCs in the simulations with different inventories is a
further complicating factor. Studies have suggested that nitrate formation
can be more sensitive to changes in VOCs than <inline-formula><mml:math id="M49" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; however, this is highly
site specific (Yang et
al., 2022). Further delineating the role of individual factors in nitrate
differences would require simulations beyond what is available for the
current study. The potential for an increasing relative role of nitrate in
air pollution and climate in a world with concurrent declines in <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
and <inline-formula><mml:math id="M51" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> emissions but little in <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> has also been discussed in previous
studies (e.g., Bauer et al., 2007; Bellouin et al., 2011; Zhai et al.,
2021). However, while more studies have focused on local air pollution
impacts of nitrate and associated mitigation strategies, nitrate is still
missing from many global climate models. Moreover, when included, the model
diversity in simulated distributions is large (Bian et al., 2017). Our results
suggest that uncertainties in emissions and choice of inventory can
contribute to spread in simulated nitrate aerosols and confound the
comparison of conclusions across modeling studies. Moreover, the complexity
of the nitrate response demonstrates that the impact of inventory
differences on simulated aerosols cannot be understood from scaling with the
changes in individual emissions but requires explicit modeling.</p>
      <p id="d1e919">To place the range in estimates between simulations with different
inventories into more context, we compare the differences in simulated
aerosol burdens in 2014 to the difference in burdens over the 5-year period
from 2014 to 2019 using CEDS21. Both globally and regionally, the spread in
burdens between simulations with different inventories and the 2014–2019
burden changes are of the same order of magnitude. In other words, at least
in this case, the changes resulting from inventory differences are as large
as those due to the recent overall change in anthropogenic emissions.</p>
      <p id="d1e922">Combined, these burden differences translate to a 3 % and 6 % lower
global annual mean AOD with CEDS21 and ECLv6, respectively, compared to
CEDS in 2014 in our simulations. As expected, the differences are most
pronounced over China and India (Fig. S4), where we estimate a 20 % and
30 % lower regional mean AOD in 2014 using the two new emission
inventories, respectively, compared to using CEDS. For context, Fig. S4 also
shows the interannual variability in AOD from MODIS Aqua (see Sect. 2): in
these regions the differences between inventories are markedly larger than
what can be expected from natural year-to-year variations.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>Global and regional AOD 1990–2019</title>
      <p id="d1e933">Next, we take a closer look at differences in the simulated temporal trend,
focusing on total AOD. Figure 3 shows the global and regional mean AOD from
1990 to 2019. Also shown is the linear trend from 2005 to 2017 for each of
the time series. This period overlaps with the availability of remotely
sensed AOD measurements, discussed in Sect. 3.1.3, as well as the most
pronounced differences in the inventories. However, as there is a certain extent of
inventory differences prior to 2005, we also provide corresponding linear
trends over the full 1990–2017 period in Table S2.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e938">Global and regional mean total AOD simulated with emissions from the CEDS21, ECLv6, and CEDS inventories. In the case of CEDS, the time series is extended from 2014 to 2017 using SSP2-4.5 emissions. Dashed lines show the linear 2005–2017 trend, defined as statistically significant from no trend when the linear Pearson correlation coefficient is significant at the 0.05 level. To reduce any influence of individual, outlier years on the trends, we calculate a set of trends removing one year at a time from the sample and show the average. Significance is given in the parenthesis. If a dash is given, individual trends from the sample differed from each other in terms of significance.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/6647/2023/acp-23-6647-2023-f03.png"/>

          </fig>

      <p id="d1e947">The simulated AOD is consistently lower when using CEDS21 and ECLv6
emissions compared to CEDS over the full period studied, with increasing
divergence over time, especially after 2005. We estimate a significant (at
the 0.05 level – see Sect. 2) negative linear trend in the global mean AOD of
<inline-formula><mml:math id="M53" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.005 and <inline-formula><mml:math id="M54" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.006 per decade in simulations with CEDS21 and ECLv6,
respectively. This trend strengthens when extended to 2019 based on
simulations with CEDS21. A negative global trend is also found when using
the first CEDS release; however, it is smaller and not significant over the
period 2005–2014. Extending the time series to 2017 by assuming that
emissions follow SSP2-4.5 after 2014 (see Sect. 2), as in Fig. 3, the
negative trend strengthens and switches to significant as per our
definition, but it remains weaker than for the other two inventories.
Considering the full period, we estimate a significant negative trend in
simulations with CEDS21 and ECLv6 but no trend when using<?pagebreak page6653?> CEDS (Table S2).
This long-term decline in the total AOD is primarily driven by the decline in
sulfate AOD, following the emission decline after the introduction of air
quality policies, first in the US and Europe, then in China, and the
collapse of the Soviet Union (e.g., Aas et al., 2019). Over
the full period, we simulate increasing trends in BC and nitrate AOD,
significant at the 0.05 level, with all three inventories (not shown);
however, their contributions to the total AOD are much smaller than that of
sulfate. Robust evidence of a declining influence of aerosols on climate
since 1990 was recently found from observables (Quaas et al., 2022). Our model
simulations capture this overall trend, and the findings reinforce the role
of changes in anthropogenic emission, particularly since 2005. Furthermore,
we suggest that if using the original CEDS emissions, models may have failed
to capture this trend. We note that biomass burning emissions also change
over time in our simulations, but we do not find any significant trend in the AOD of
biomass aerosols (BC and POA) on the global mean scale over this period.
We do note that years of high biomass burning activity, such as in 2019 where
GFED4 emissions are 25 % higher than in 2018, can lead to marked jumps in
simulated AOD. We have limited possible influence of such years on the
linear trend calculated (see Sect. 2).</p>
      <p id="d1e965">Regionally, we simulate significant declining trends in AOD over 2005–2017
for EUR and NAM, with this trend extending back to 1990 (Table S2), as
expected. This is also consistent with surface observations for both AOD and
atmospheric sulfur and is in agreement with other models (Mortier et al.,
2020; Aas et al., 2019); we capture the decline regardless of which
emission inventory is used. In both regions, and across simulations with all
three scenarios, we find a decline in the AOD of BC, OA, and sulfate but an
increasing trend in nitrate AOD. Over RBU, we also simulate a
significant<?pagebreak page6654?> decline in the area average AOD over the full 1990–2017 period but
a flatter evolution when considering only 2005–2017. However, the results
are  also similar with all three scenarios here. In parts of the RBU region,
GFED4 shows an increase in emissions over the latter period, resulting in a
positive trend in the AOD of biomass aerosols from 2005. On the African
continent, we simulate a negative, albeit weak, trend in AOD over the
2005–2017 period for SAF. In contrast, the trend over the full period is
positive. Anthropogenic emissions in SAF have increased (Fig. S1), although
less steeply than in Asia, and we find significant increases in the AOD of
all the anthropogenic species with all inventories from 1990 to 2017.
However, from 2005 onwards, there has been a decreasing trend in GFED4
emissions, following a reduction in the burned area of savannas
(Wu et al., 2021). Biomass burning aerosols contribute
relatively more to the total AOD here than in the Northern Hemisphere regions
and hence impose a stronger effect on the area average trend. A similar
pattern is seen for SAM, while for SEA, another biomass-burning-influenced
region, we find less clear trends. While diagnosed trends in the total AOD in
these regions are mostly of a similar sign across simulations with the three
inventories, we find that the trend in sulfate AOD diverges between model
runs using CEDS or CEDS21 (positive trend) and ECLv6 (negative trend) in SAF
and NAF, pointing to a need to better understand the drivers of emission
changes in these regions and homogenize between inventories. As expected,
the key differences between simulations with different inventories arise
over Asia. Simulations with both CEDS21 and ECLv6 show a significant
decreasing trend in the total AOD over EAS between 2005 and 2017. While a
decline is found using CEDS, it is much weaker and not significant.
Moreover, differences between inventories affect the sign of the simulated
trend when considering the full period, owing primarily to the spread in
estimated sulfate AOD. For SAS, we simulate a consistent positive trend, but
ranging from 0.01 per decade with ECLv6 to 0.03 per decade with CEDS, with
increasing divergence in AOD over time. Similar magnitude differences
between the sets of experiments exist for the AOD of all anthropogenic
aerosols in this region.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS3">
  <label>3.1.3</label><title>Comparison with observed AOD</title>
      <p id="d1e976">To explore whether the model captures observed global and regional trends
better with the CEDS21 emissions than with CEDS, we compare simulated AOD to
MODIS Aqua retrievals and ground-based AERONET measurement. For this
evaluation, we also use simulations where the model is driven by meteorology
for the respective years, referred to as CEDSmet and CEDS21met (see Sect. 2), for more realistic comparison with the observations. Using both these,
we also estimate negative linear trends in the simulated global mean AOD from
2005 to 2017, strengthening from <inline-formula><mml:math id="M55" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.001 per decade in CEDSmet to <inline-formula><mml:math id="M56" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.003 per
decade in CEDS21met. These are, however, weaker than the trends derived from
the fixed meteorology simulations in Sect. 3.1.2 (Fig. 3) and not
significant at the 0.05 level, demonstrating the notable influence of
variability in meteorology and natural aerosols, masking trends due to
changes in anthropogenic emissions. This influence is particularly visible
for the area average AOD for SAF and NAF, where the diagnosed trend is
positive but non-significant in these simulations, in contrast to the
negative trend found in simulations with fixed meteorology above. The
negative trend over SAM is also not significant at the at the 0.05 level in
these runs. For other focus regions, results are similar between fixed and
actual meteorology runs, and significant trends arise over the natural
variability.</p>
      <p id="d1e993">Figure 4a shows the annual global mean simulated AOD from 1990 to 2017 and
the MODIS Aqua AOD from 2003 to 2019. Dashed lines show the linear 2005–2017
trends. Figure 4b–d show the spatially explicit trends. We first note that
the magnitude of the simulated global mean AOD is lower than that derived from
MODIS Aqua by around 20 %. However, the overall geographical pattern of
observed AOD is captured by the model (Fig. S5). Furthermore, the AOD
simulated by the OsloCTM3 is within, although in the lower range, the
spread in AOD between the CMIP and AeroCom models (Vogel et al.,
2022). As also shown by Vogel et al. (2022), there can be a notable
spread in AOD derived from different satellite products. They found a 13 %
standard deviation range in the global mean AOD between eight satellite
products, with MODIS retrievals in the upper end. Although again in the lower
range, the OsloCTM3 AOD falls within the full range of the satellite-derived
annual mean AOD. Overall, this suggests a reasonable OsloCTM3 performance in
terms of magnitude and distribution.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e998"><bold>(a)</bold> Global annual mean AOD from MODIS Aqua and the OsloCTM3 over the 1990–2019 period. Note that data north and south of 70<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> are excluded here due to the limited MODIS Aqua coverage. Dashed lines show a linear trend from 2005 to 2017. <bold>(b–d)</bold> Spatially resolved linear trends in observed and simulated AOD. Hatching indicates where the linear trend is significantly different from 0 at the 0.05 level.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/6647/2023/acp-23-6647-2023-f04.png"/>

          </fig>

      <?pagebreak page6655?><p id="d1e1022"><?xmltex \hack{\newpage}?>In terms of temporal evolution, MODIS Aqua data indicate a very weak
positive linear trend of 0.001 per decade in the global mean AOD over the
2005–2017 period (0.004 per decade when extending the data to 2019). We do
not, however, find this trend to be significant. MODIS data are influenced by
substantial year-to-year variability, in particular after 2010, which was
also pointed out by Vogel et al. (2022). Regions with significant
positive observed AOD trends include parts of the ocean in the Southern
Hemisphere (Fig. 4b). Here, sea salt aerosols could be causing the increase.
However, Quaas et al. (2022)
recently showed that this positive trend is not clear in Multi-angle Imaging
SpectroRadiometer (MISR) data. While we are focused on the
anthropogenically influenced regions in the present analysis, we briefly
note that the magnitude of the trends over the Southern Hemisphere oceanic
regions is also not captured by the model (Fig. 4c–d). We also simulate
weaker trends in the boreal regions of North America and Russia
contributing to the model–observation difference.</p>
      <p id="d1e1026">Over the main anthropogenic emission source regions, there are significant
observed declines in AOD over East Asia, the US, and Europe (Fig. 4b). These
trends have been confirmed by both ground-based and remote sensing
observations of AOD and other variables (Gui et al., 2021; Moseid et al.,
2020; Paulot et al., 2018; Quaas et al., 2022). For NAM and EUR, we
calculate an area average negative observed trend of <inline-formula><mml:math id="M58" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.006 and <inline-formula><mml:math id="M59" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.009,
respectively, from MODIS Aqua. This is of the same sign but weaker than the
trend simulated with both emission inventories. For the latter, this
contrasts with findings by Mortier et al. (2020), where models in general were found to underestimate the observed
decrease in AOD seen in surface observations. Over EAS, where the influence
of inventory differences is most pronounced, a significant negative observed
trend of <inline-formula><mml:math id="M60" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.044 per decade is calculated. This is in very close agreement
with the <inline-formula><mml:math id="M61" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.40 per decade AOD trend simulated with CEDS21, while
simulations with CEDS do not show a significant trend. Hence, the model is
clearly able to better represent observed trends with the updated inventory.
This is further confirmed in Fig. 5, where we show 5-year average
deviations from the period 2003–2017 in both MODIS Aqua and simulated AOD.
Using CEDS21 results in marked improvements compared to observed AOD trends
over China, both for the first and most recent full 5-year periods. However,
the opposite tendency is found for AOD over SAS. Here observations suggest a
significant positive trend of 0.04 per decade. The diagnosed trends are also
positive in simulations using both inventories but somewhat weaker,
especially when switching from CEDS to CEDS21 (and even more so when using
EClv6 emissions – Fig. 3). Figure 5 suggests that this discrepancy arises in
the more recent decade. Furthermore, simulated AOD and underlying
emissions suggest a leveling off in recent years, which is not seen from
MODIS Aqua. Whether this is due to inaccurate representation of the
evolution of anthropogenic emissions in the inventories or  poor model representation of other aerosols such as dust from
agricultural soils and urban areas (e.g., construction, non-exhaust transport
emissions) is however not clear from this analysis. We note that the model
underestimates the magnitude of AOD observed by MODIS Aqua in both EAS and
SAS. To the extent that the MODIS is accurate, this could support the
latter. This type of dust is suggested to give an important contribution to
the particulate matter load (e.g., Chen et al., 2019; Xia et al., 2022)
but is still missing from many global models. Other contributing factors
include the representation of processes related to aerosol transport and
scavenging. Finally, we also note that the 5-year deviations in Fig. 5 show
quite some variability over the Middle East, with both positive and negative
deviations from the baseline period. While anthropogenic emissions in this
region increase steadily over the period (by 13 %–40 % depending on species)
in the inventories used in the present study, the strong influence from dust
emissions in this region likely dominates the temporal variability.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e1059">Evolution of AOD over South and East Asia and the Middle East over the period 2003–2020. All panels show 5-year average deviations from the period 2003–2017, except the rightmost MODIS Aqua panel, which shows the 3-year average deviation (same baseline). The top row shows retrievals from MODIS Aqua; the two bottom rows show model calculations with OsloCTM3 based on the CEDS and CEDS21 emission inventories.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/6647/2023/acp-23-6647-2023-f05.png"/>

          </fig>

      <p id="d1e1068">A previous OsloCTM3 study by Lund et al. (2018)
found an improved agreement between the year 2010 ground-based AERONET
observations and model output, including over Asia, when switching from
CMIP5 and ECLIPSEv5 emissions to CEDS, the latter having higher emissions.
This seemingly contradicts expectations following the now-known biases in
this first release of CEDS. Here we repeat the comparison with AERONET but
for the year 2014. Resulting scatter-density plots are given in Fig. S6. The
normalized mean bias (NMB) compared to AERONET ranges from <inline-formula><mml:math id="M62" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>21 to <inline-formula><mml:math id="M63" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>29 % in
the simulations with fixed and actual meteorology. We find higher bias and
lower correlation when switching from the original CEDS release to CEDS21
and ECLv6. Hence, while the model is better able to represent observed
recent aerosol trends over East Asia with newer emission inventories, these
results point to other issues that may have been concealed by too high
anthropogenic emissions. Dust and atmospheric processing, as discussed
above, are again possible contributing factors.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Impact of inventory differences on estimated anthropogenic
aerosol RF</title>
      <p id="d1e1094">Finally, we quantify the aerosol-induced RF from the three sets of
experiments. Figure 6a shows the RFari, RFaci, and net aerosol radiative
forcing (RFnet, RFari plus RFaci) relative to 1990 for the three sets of
experiments. The net RF of changes in anthropogenic (and biomass burning)
aerosol has been positive since 1990, except for 1995 and 2005, where a small
negative forcing is estimated. As shown in Fig. 1, global anthropogenic
<inline-formula><mml:math id="M64" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions show a peak in 2005, and the biomass burning emissions are
relatively high. This positive global mean net RF is determined mainly by
the balance between a positive forcing over the northern extratropics,
dominated by aerosol–radiation interactions, and a negative forcing over
Asia and parts of South America and Africa<?pagebreak page6656?> with stronger contributions from
aerosol–cloud interactions (Fig. S7).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e1110"><bold>(a)</bold> Global mean RFari and RFaci (top) and RFnet (RFari <inline-formula><mml:math id="M65" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> RFaci) (bottom) relative to 1990 from simulations using the CEDS, CEDS21, and ECLv6 emission inventories. The vertical bars to the right show the range in RFnet in 2020 and 2030 (relative to 1990) estimated with the SSP1-1.9 and SSP3-7.0 emissions (adapted from Lund et al., 2019). <bold>(b)</bold> Regional mean RFnet, RFari, and RFaci in 2014 relative to 1990 in simulations with the CEDS, CEDS21, and ECLv6 inventories.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/6647/2023/acp-23-6647-2023-f06.png"/>

        </fig>

      <p id="d1e1131">In 2014, we estimate a global mean RFnet of 0.03 W m<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CEDS, 0.08 W m<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CEDS21, and 0.12 W m<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for ECLv6 relative to 1990, of
which the RFari constitutes 0.07, 0.09, and 0.10 W m<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively. We note that our framework only captures the cloud
albedo effect and not radiative effects of any changes in cloud lifetimes
that may arise through the influence of aerosols (i.e., we calculate RF, not
ERF). Our RFari estimate using CEDS emissions is similar to the multi-model
mean RFari of 0.05 W m<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> derived for the 1990–2015 period using ECLIPSE
version 5 emissions by Myhre et al. (2017). The same study estimated a model mean RFnet of 0.1 W m<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> but
with a significant intermodel spread from close to 0 to more than 0.2 W m<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. This spread is larger than the difference between estimates with
different inventories in the present analysis. Nevertheless, the differences
in emissions between CEDS and CEDS21 (ECLv6) translate to a factor 3 (5)
stronger RFnet in our calculations.</p>
      <p id="d1e1220">Figure 6b shows regional mean RF, including the balance between RFari and
RFaci. Following the significant decline in AOD over EUR and NAM, the
dominant contributions to positive RF are found here, followed by Russia.
There is however little difference between simulations with the three
inventories. In contrast, the net RF over EAS switches signs from negative in
simulations with CEDS to positive when using CEDS21 or ECLv6 due to the observed
decline in emissions now captured. While negative in all three sets of
experiments, the net RF over SAS is 40 % (20 %) weaker when ECLv6
(CEDS21) emissions are used compared to CEDS. This results from a 50 %
(20 %) lower net area average AOD change between 1990 and 2014 compared
to simulations with CEDS.</p>
      <p id="d1e1223">The CEDS21 inventory extends to 2019 compared to 2014 in CEDS. The global
mean net RF over this 5-year period is estimated to be 0.10 W m<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
driven primarily by a further positive forcing over China in line with the
continued decline in <inline-formula><mml:math id="M74" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions following the implementation of measures
targeting improved air quality. Over India, the forcing in 2019 relative to
2014 remains negative but weaker than during the preceding period, while
over Europe and western Russia, the RF is low, suggesting little further
recent emission changes. We note however that this is a short period, and
results should be interpreted with that in mind. Using a selection of the
SSP scenarios, Lund et al. (2019) extended simulations from 2014 CEDS
emissions and quantified the projected aerosol-induced RF. The orange
hatched bars in Fig. 6 show the range in RFnet in 2020 and 2030 (relative to
1990) estimated with SSP1-1.9, SSP2-4.5, and SSP3-7.0 in that study. The
RFnet in 2019 estimated with CEDS21 here is close to the lower end of the
bar, i.e., the RFnet projected under SSP3-7.0. However, prior to this higher
biomass burning year, there are indications that the RFnet from simulations
with CEDS21 tracked closer to SSP2-4.5 or an even lower emission pathway.</p>
      <p id="d1e1249">The dipole pattern of aerosol changes, and resulting RF, over India versus
China that can be seen in observations and is expected to impose regional
climate impacts was first highlighted by Samset et al. (2019).
Using emissions from CEDS and SSP1-1.9, SSP2-4.5, and SSP3-7.0, combined with
a<?pagebreak page6657?> radiative kernel approach, that study estimated a range of 2014–2030
aerosol (<inline-formula><mml:math id="M75" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and BC) net RF of <inline-formula><mml:math id="M76" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.0 (SSP1-1.9) to 0.82 W m<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (SSP2-4.5) over India and 0.06 (SSP2-4.5) to 1.10 W m<inline-formula><mml:math id="M78" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (SSP3-7.0) over China. Part of this range can be attributed to poor
knowledge of current, and hence also future, regional emissions (Samset et
al., 2019). In the present study, we estimate regionally averaged RFnet in
2019 relative to 2014 of <inline-formula><mml:math id="M79" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.09 and 0.22 W m<inline-formula><mml:math id="M80" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> over India and
China, respectively. For China, this recent RFnet is about 20 % of the
previously estimated difference between high and low future aerosol emission
scenarios in 2030 (SSP2-4.5 and SSP3-7.0). Missing or incorrectly captured
past emission trends can therefore markedly affect assessments of projected
near-term aerosol-induced climate impacts, as they depend on a well-constrained starting point.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e1323">We have investigated the impact of differences between recent global
emission inventories available to the aerosol and climate modeling
community on simulated anthropogenic aerosol abundances and associated
radiative forcing from 1990 to 2019. Simulations with the chemical
transport model OsloCTM3 and the CEDS emission inventory, developed for the
sixth cycle of the IPCC, have been compared with corresponding results using
two newer inventories: the CEDS 2021 update (CEDS21) and the ECLIPSE version 6b (ECLv6). Our objective was to evaluate the model performance considering
revisions to the emissions input data, partly done to correct known regional
biases, and to investigate the implications of inventory differences for
downstream diagnosed quantities critical for assessing the air quality and
climate effects of anthropogenic aerosol.</p>
      <p id="d1e1326">We have found that, apart from nitrate, simulations with the CEDS21 (ECLv6)
inventory give lower global mean aerosol burdens than corresponding runs
with CEDS, ranging from 4 % (6 %) for BC to approx. 10 % (15 %) for
sulfate and POA in 2014 (the most recent historical year common for all
scenarios). Differences are consistently most pronounced over East Asia,
followed by South Asia, where they are of the order of 30 %–60 % depending
on species and scenario. Differences in the underlying anthropogenic
emissions arise from different assumptions about emission rates; data on
non-energy sources; and, importantly, representation of air quality policies
and their implementation efficiency. In our model, the global mean fine-mode
nitrate burden is 15 % (24 %) higher with CEDS21 (ECLv6) relative to
CEDS but with regional heterogeneity in the sign of the difference. Overall, we
estimate a 3 % (6 %) lower total AOD with CEDS21 (ECLv6)
compared to CEDS in 2014. The difference reaches approx. 20 % and 30 %
over East and South Asia.</p>
      <p id="d1e1329">Over East Asia, we diagnose a significant negative linear trend in the total area average AOD from 2005 to 2017 of <inline-formula><mml:math id="M81" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.03 per decade in simulations using
the ECLv6 emissions. In contrast, we find no significant trend in
corresponding experiments with CEDS. Importantly, we find that the model is
better able to capture the trend observed by MODIS Aqua with both new
inventories. In all three sets of simulations, we estimate a significant
positive linear AOD trend over South Asia. The simulated trend is, however,
weaker than that derived from MODIS Aqua, and this gap increases when
switching from CEDS to the CEDS21 and ECLv6 inventories. We also
underestimate the magnitude of observed AOD in the region, at least compared
to this specific satellite product. Recent emission trends are less well
constrained by observations in India than, e.g., in China. The extent to which
the model–observation difference arises from the input of anthropogenic
emissions or could be influenced by poor model representation of other
aerosol sources or atmospheric<?pagebreak page6658?> processes is not clear from the present
analysis. For other regions considered, there is generally agreement in the
sign of the simulated area average AOD trend between the three sets of
simulations, although the magnitude can differ, in particular for the AOD of
individual species. For instance, there is an increasing (over time)
divergence in the sulfate AOD over Africa between simulations using CEDS and
ECLv6. Over most regions, nitrate AOD increases; however, nitrate
contributes relatively less to the total AOD than sulfate and OA.</p>
      <p id="d1e1339">Using offline radiative transfer calculations, we estimate a global mean net
aerosol RF in 2014 relative to 1990 of 0.03 W m<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CEDS, 0.08 W m<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CEDS21, and 0.12 W m<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for ECLv6. Regionally, the sign
of the net aerosol-induced RF switched from negative to positive when
replacing CEDS emissions with CEDS21 or ECLv6 in our study. Hence, the
failure to capture recent observed emission trends in China may have
resulted in the wrong sign in estimates of the regional effect on the energy
balance over recent decades. Over South Asia, the area average net RF is up
to 40 % lower in simulations with the updated inventories compared to
CEDS.</p>
      <p id="d1e1379">While the focus of the present study is on anthropogenic aerosols, our
comparison with observed AOD reveals potential issues related to the
representation of natural aerosols or other processes in the OsloCTM3. In
particular, the model does not capture the strength of the positive AOD
trend observed over high-latitude North America and Russia, likely due to an
increase in biomass burning aerosols. For individual years, we also find a
larger underestimation in AOD compared to AERONET measurements when
switching from CEDS to the lower CEDS21 and ECLv6 emissions, despite better
representation of some key regional observed trends. Further studies are
required to investigate this in more detail.</p>
      <p id="d1e1382">Anthropogenic aerosols are changing rapidly, particularly in Asia, with
potentially large but insufficiently quantified implications for regional
climate. We have demonstrated that differences between recent emission
inventories translate to notable differences in global and regional trends
in anthropogenic aerosol distributions and in turn in estimates of
radiative forcing. Although additional studies are required to fully
quantify the broader implications for aerosol-induced climate and health
impacts, our results facilitate comparisons between existing and upcoming
studies, using different emission inventories, of anthropogenic aerosols and
their effects.</p>
</sec>

      
      </body>
    <back><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e1390">The OsloCTM3 is available from <uri>https://github.com/NordicESMhub/OsloCTM3</uri> (Søvde et al., 2023).</p>
  </notes><?xmltex \hack{\newpage}?><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1400">Model data underlying the paper figures are available from
<ext-link xlink:href="https://doi.org/10.6084/m9.figshare.20254764" ext-link-type="DOI">10.6084/m9.figshare.20254764</ext-link> (Lund et al., 2023). AERONET data are downloaded from <uri>https://aeronet.gsfc.nasa.gov/cgi-bin/webtool_aod_v3</uri> (AERONET, 2023), MODIS data from <uri>https://giovanni.gsfc.nasa.gov/giovanni/#service=TmAvMp&amp;starttime=&amp;endtime=&amp;data=MYD08_M3_6_1_AOD_550_Dark_Target_Deep_Blue_Combined_Mean_Mean&amp;variableFacets=dataFieldDiscipline:Aerosols;dataFieldMeasurement:Aerosol Optical Depth;dataProductPlatformInstrument:MODIS-Aqua;</uri> (see also Platnick et al., 2015),  CEDS21 emissions from  <ext-link xlink:href="https://doi.org/10.5281/zenodo.4509372" ext-link-type="DOI">10.5281/zenodo.4509372</ext-link> (O'Rourke et al., 2021), and GFED4 emissions from <uri>https://doi.org/10.3334/ORNLDAAC/1293</uri> (Randerson et al. 2017).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e1418">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-23-6647-2023-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-23-6647-2023-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1427">MTL led the study design, analysis, and writing. The OsloCTM3 model
experiments were performed by MTL and RBS. GM performed the radiative
transfer modeling, and BHS contributed to graphics and MODIS
analysis. All authors contributed to the discussions and writing.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1433">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="d1e1439">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1445">The authors acknowledge the
UNINETT Sigma2 – the National Infrastructure for High-Performance Computing
and Data Storage in Norway – resources (grant no. NN9188K).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e1450">This research has been supported by the Norges Forskningsråd (grant nos. 248834, 314997, and 324182).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1456">This paper was edited by Qiang Zhang and reviewed by two anonymous referees.</p>
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