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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-18-9225-2018</article-id><title-group><article-title>Multi-species inversion and IAGOS airborne data for a better constraint of
continental-scale fluxes</article-title><alt-title>Multi-species inversion and IAGOS airborne data</alt-title>
      </title-group><?xmltex \runningtitle{Multi-species inversion and IAGOS airborne data}?><?xmltex \runningauthor{F. Boschetti et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Boschetti</surname><given-names>Fabio</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Thouret</surname><given-names>Valerie</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Maenhout</surname><given-names>Greet Janssens</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9335-0709</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Totsche</surname><given-names>Kai Uwe</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2692-213X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Marshall</surname><given-names>Julia</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2648-128X</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Gerbig</surname><given-names>Christoph</given-names></name>
          <email>cgerbig@bgc-jena.mpg.de</email>
        <ext-link>https://orcid.org/0000-0002-1112-8603</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department Biogeochemical Systems, Max Plank Institute for Biogeochemistry, Jena, 07745, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Laboratoire d'Aerologie, CNRS and Universite' Paul Sabatier, Toulouse, 31400, France</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>European Commission Joint Research Centre, Institute for Environment and Sustainability, Ispra, 21027, Italy</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Friedrich Schiller University, Jena, 07743, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Christoph Gerbig (cgerbig@bgc-jena.mpg.de)</corresp></author-notes><pub-date><day>3</day><month>July</month><year>2018</year></pub-date>
      
      <volume>18</volume>
      <issue>13</issue>
      <fpage>9225</fpage><lpage>9241</lpage>
      <history>
        <date date-type="received"><day>26</day><month>January</month><year>2017</year></date>
           <date date-type="rev-request"><day>1</day><month>March</month><year>2017</year></date>
           <date date-type="rev-recd"><day>11</day><month>January</month><year>2018</year></date>
           <date date-type="accepted"><day>15</day><month>April</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</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>
    <p id="d1e146">Airborne measurements of CO<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, and CH<inline-formula><mml:math id="M2" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>
proposed in the context of IAGOS (In-service Aircraft for a Global Observing
System) will provide profiles from take-off and landing of airliners in the
vicinity of major metropolitan areas useful for constraining sources and
sinks. A proposed improvement of the top-down method to constrain sources
and sinks is the use of a multispecies inversion. Different species such as
CO<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO have partially overlapping emission patterns for given
fuel-combustion-related sectors, and thus share part of the uncertainties
related both to the a priori knowledge of emissions and to model–data
mismatch error. We use a regional modelling framework consisting of the
Lagrangian particle dispersion model STILT (Stochastic Time-Inverted
Lagrangian Transport) combined with the high-resolution (10 km <inline-formula><mml:math id="M4" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10 km)
EDGARv4.3 (Emission Database for Global Atmospheric Research) emission
inventory, differentiated by emission sector and fuel type for CO<inline-formula><mml:math id="M5" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO,
and CH<inline-formula><mml:math id="M6" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>, and combined with the VPRM (Vegetation Photosynthesis and
Respiration Model) for biospheric fluxes of CO<inline-formula><mml:math id="M7" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. Applying the modelling
framework to synthetic IAGOS profile observations, we evaluate the benefits
of using correlations between different species' uncertainties on the
performance of the atmospheric inversion. The available IAGOS CO
observations are used to validate the modelling framework. Prior uncertainty
values are conservatively assumed to be 20 %, for CO<inline-formula><mml:math id="M8" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and 50 % for
CO and CH<inline-formula><mml:math id="M9" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>, while those for GEE (gross ecosystem exchange) and
respiration are derived from existing literature. Uncertainty reduction for
different species is evaluated in a domain encircling 50 % of the profile
observations' surface influence over Europe. We found that our modelling
framework reproduces the CO observations with an average correlation of
0.56, but simulates lower mixing ratios by a factor of 2.8, reflecting a low
bias in the emission inventory. Mean uncertainty reduction achieved for
CO<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> fossil fuel emissions is roughly 38 %; for photosynthesis and
respiration flux it is 41 and 44 % respectively. For CO and CH<inline-formula><mml:math id="M11" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>
the uncertainty reduction is roughly 63 and 67 % respectively.
Considering correlation between different species, posterior uncertainty can
be reduced by up to 23 %; such a reduction depends on the assumed error
structure of the prior and on the considered time frame. The study suggests a
significant uncertainty constraint on regional emissions using multi-species
inversions of IAGOS in situ observations.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\allowdisplaybreaks}?>
<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e256">As widely recognized at the international level, there is a need for
reduction in anthropogenic emissions (IPCC, 2014). This however implies the
necessity for reliable climate predictions from atmospheric models in order
to allow policymakers to make informed decisions. Unfortunately, current
climate predictions are hampered by excessive uncertainties; for example
intercomparisons of different models show important differences in their
predictions as shown in Friedlingstein et al. (2006). This makes it difficult
to assess the better environmental policies to implement. Because most
biogenic<?pagebreak page9226?> fluxes in Europe are influenced by human activities, with 22 %
of Europe's land dedicated to agriculture (FAO, 2013) and 45 % covered by
forests, of which 80 % is managed for wood supply (UNECE, FAO, 2011),
understanding and managing these biogenic fluxes must also be a component of
any policy to reduce anthropogenic emissions.</p>
      <p id="d1e259">A commonly used approach to estimate carbon budgets by teasing apart sources
and sinks in a given spatial domain is the atmospheric Bayesian inversion.
Atmospheric inversions combine prior knowledge from emission inventories with
atmospheric observations acting as a top-down constraint to produce better
posterior knowledge. As the main goal of this study is to assess the benefit
of inter-species correlations in reducing the uncertainty of the posterior
state space, we are particularly interested in the effects of such
correlations on the uncertainty reduction, defined as the difference between
prior and posterior uncertainty normalized by the prior. The vast majority of
published papers on atmospheric inversions investigate the budget of a single
species, usually a long-lived greenhouse gas like CO<inline-formula><mml:math id="M12" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> (e.g.
Rödenbeck et al., 2003) or CH<inline-formula><mml:math id="M13" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> (e.g. Hein et al., 1997; Bousquet et
al., 2006), but the technique can also be applied to active species like CO
(Bergamaschi et al., 2000). Note that carbon dioxide is a special case as
atmospheric CO<inline-formula><mml:math id="M14" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> mixing ratios result from a combination of strong
anthropogenic sources with strong sources and sinks from biospheric
processes, calling for a separation of anthropogenic fluxes from biospheric
fluxes. One way to achieve such a separation is to measure CO alongside
CO<inline-formula><mml:math id="M15" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and use CO as a proxy for CO<inline-formula><mml:math id="M16" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> anthropogenic emissions. Several
studies have made use the correlations among different species. One of the
first examples is the work from Enting et al. (1995) on CO<inline-formula><mml:math id="M17" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and
<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">13</mml:mn></mml:msup></mml:math></inline-formula>CO<inline-formula><mml:math id="M19" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, while Brioude et al. (2012) attempted to derive a CO<inline-formula><mml:math id="M20" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
emission inventory without a prior emission estimate, instead using
inventories of CO, NO<inline-formula><mml:math id="M21" display="inline"><mml:msub><mml:mi/><mml:mi>y</mml:mi></mml:msub></mml:math></inline-formula>, and SO<inline-formula><mml:math id="M22" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. Similarly, Peischl et al. (2013)
made use of CO and CO<inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> inventories to help quantifying sources of
CH<inline-formula><mml:math id="M24" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> in the Los Angeles basin. The ability to measure multiple species
has proved useful, also in remote sensing. For example, Pandey et al. (2015)
made use of simultaneously retrieved CO<inline-formula><mml:math id="M25" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CH<inline-formula><mml:math id="M26" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> total column to
reduce scattering effect. Further examples of studies making use of
co-emitted species can be found in atmospheric chemistry (Konovalov et al.,
2014; Berezin et al., 2013; Pison et al., 2009). More focused on exploiting
inter-species correlation to reduce uncertainty in Bayesian inversion, Palmer
et al. (2006) made use of CO<inline-formula><mml:math id="M27" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>–CO correlations to improve inversion
using data from the TRACE-P aircraft mission, while Wang et al. (2009)
employed a similar method using satellite data, obtaining a reduction in the
flux error of a CO<inline-formula><mml:math id="M28" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> inversion.</p>
      <p id="d1e417">So far the lion's share of the studies investigating atmospheric inversions
make use of both continuous in situ and flask measurements from ground-based
observational networks of tall towers (e.g. Kadygrov et al., 2015;
Sasakawa et al., 2010).
However, as profiles collected from aircraft easily exceed the height of
towers, airborne data may also offer an interesting option. This alternative was tested in some recent studies that made
use of aircraft profiles alone or in combination with other data sources
(e.g. Brioude et al., 2013; Gourdji et al., 2012). Methods to maximize the
cost-effectiveness of airborne data are the use of unmanned aircraft
(drones) and commercial airliners. The latter, in particular, allow for
collecting data on a regular basis without requiring a particularly small or
light sensor. The most important projects making use of commercial airliners
are CONTRAIL (Comprehensive Observation Network for Trace Gases; Machida et al.,
2008) and MOZAIC/IAGOS (Measurements of Ozone and water vapour by in-service
AIrbus aircraft/In-service Aircraft for a Global Observing System; Marenco et al., 1998; Petzold et al., 2015). Both projects have been running for more
than 2 decades and have produced extensive datasets that have proven to be
important in the fields of atmospheric modelling and satellite calibration
and validation (Zbinden et al., 2013; Sawa et al., 2012). Regarding
carbonaceous species, CONTRAIL has so far collected CO<inline-formula><mml:math id="M29" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> mixing
ratio measurement, while IAGOS is focused on CO. In the next years the
IAGOS fleet will simultaneously provide CO, CO<inline-formula><mml:math id="M30" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and CH<inline-formula><mml:math id="M31" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>
atmospheric concentration measurements (Filges et al., 2015), enabling the use of
multi-species synergy in modelling applications. This synergy follows the
fact that the collocated measurements share the same atmospheric transport
and have partially correlated emission uncertainties.</p>
      <p id="d1e447">This paper is focused on investigating the benefits
of such a multi-species inversion on uncertainty reduction in comparison with a single-species
inversion. To achieve this goal, we set up a synthetic experiment utilizing
the measurement times and locations collected from the IAGOS projects in the
year 2011. The present paper is intended to pave the way for future studies
making use of multi-species IAGOS datasets when they become available. A
receptor-oriented framework was set up to derive flux interactions between
the atmosphere and the biosphere using IAGOS data. The modelling framework is
composed of a Lagrangian particle dispersion model (LPDM, specifically the
STILT model), a diagnostic biosphere–atmosphere exchange model (the VPRM
model), gridded emission inventories, global tracer transport model output
that provides the tracer boundary conditions for the regional domain, and a
Bayesian inversion scheme. The present work is based on the modelling
framework used in Boschetti et al. (2015) and builds upon that by adding other
species, and using a formal Bayesian inversion. A multi-species inversion
was carried out in order to exploit the correlations in uncertainties
between CO<inline-formula><mml:math id="M32" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, and CH<inline-formula><mml:math id="M33" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>, specifically in their respective
uncertainties in a priori anthropogenic emissions and in model
representation error. The aim of this multi-species inversion is to provide
better estimates of anthropogenic emissions, and, in the case of CO<inline-formula><mml:math id="M34" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>,
to better separate the biospheric from anthropogenic contributions. This
paper is structured as follows: a short description of the different
components of the modelling framework is given in Sect. 2;<?pagebreak page9227?> in Sect. 3 we
present and discuss our results; Sect. 4 gives the conclusions.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p id="d1e481">Specific emission sectors accounted for in the state vector and
aggregated categories as used in Fig. 8.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Adj IPCC</oasis:entry>
         <oasis:entry colname="col3">Description</oasis:entry>
         <oasis:entry colname="col4">Aggregated</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">1a1a</oasis:entry>
         <oasis:entry colname="col3">power generation</oasis:entry>
         <oasis:entry colname="col4">energy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">1a1bcr</oasis:entry>
         <oasis:entry colname="col3">other transformation non-energy use</oasis:entry>
         <oasis:entry colname="col4">energy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">1b1</oasis:entry>
         <oasis:entry colname="col3">solid fuel production</oasis:entry>
         <oasis:entry colname="col4">energy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">1b2abc</oasis:entry>
         <oasis:entry colname="col3">gas flaring</oasis:entry>
         <oasis:entry colname="col4">energy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">5</oasis:entry>
         <oasis:entry colname="col2">1b2ac</oasis:entry>
         <oasis:entry colname="col3">oil prod., distribution, and flaring</oasis:entry>
         <oasis:entry colname="col4">energy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">6</oasis:entry>
         <oasis:entry colname="col2">1b2b</oasis:entry>
         <oasis:entry colname="col3">gas production and distribution</oasis:entry>
         <oasis:entry colname="col4">energy</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">7</oasis:entry>
         <oasis:entry colname="col2">1a3a<inline-formula><mml:math id="M35" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1c1</oasis:entry>
         <oasis:entry colname="col3">international and domestic aviation</oasis:entry>
         <oasis:entry colname="col4">transport</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">8</oasis:entry>
         <oasis:entry colname="col2">1a3b</oasis:entry>
         <oasis:entry colname="col3">road transport</oasis:entry>
         <oasis:entry colname="col4">transport</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">9</oasis:entry>
         <oasis:entry colname="col2">1a3ce</oasis:entry>
         <oasis:entry colname="col3">non-road ground transport</oasis:entry>
         <oasis:entry colname="col4">transport</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">10</oasis:entry>
         <oasis:entry colname="col2">1a3d<inline-formula><mml:math id="M36" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1c2</oasis:entry>
         <oasis:entry colname="col3">inland waterways and shipping</oasis:entry>
         <oasis:entry colname="col4">transport</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">11</oasis:entry>
         <oasis:entry colname="col2">1a2<inline-formula><mml:math id="M37" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>6cd</oasis:entry>
         <oasis:entry colname="col3">industrial combustion (non-power)</oasis:entry>
         <oasis:entry colname="col4">industry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">12</oasis:entry>
         <oasis:entry colname="col2">2a</oasis:entry>
         <oasis:entry colname="col3">cement and lime production</oasis:entry>
         <oasis:entry colname="col4">industry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">13</oasis:entry>
         <oasis:entry colname="col2">2befg <inline-formula><mml:math id="M38" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 3</oasis:entry>
         <oasis:entry colname="col3">chemical industry and solvents</oasis:entry>
         <oasis:entry colname="col4">industry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">14</oasis:entry>
         <oasis:entry colname="col2">2c</oasis:entry>
         <oasis:entry colname="col3">metal industry emission</oasis:entry>
         <oasis:entry colname="col4">industry</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">15</oasis:entry>
         <oasis:entry colname="col2">1a4</oasis:entry>
         <oasis:entry colname="col3">buildings</oasis:entry>
         <oasis:entry colname="col4">buildings</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">16</oasis:entry>
         <oasis:entry colname="col2">4a</oasis:entry>
         <oasis:entry colname="col3">enteric fermentation in agriculture</oasis:entry>
         <oasis:entry colname="col4">agriculture</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">17</oasis:entry>
         <oasis:entry colname="col2">4b</oasis:entry>
         <oasis:entry colname="col3">manure management</oasis:entry>
         <oasis:entry colname="col4">agriculture</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">18</oasis:entry>
         <oasis:entry colname="col2">4c</oasis:entry>
         <oasis:entry colname="col3">rice cultivation</oasis:entry>
         <oasis:entry colname="col4">agriculture</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">19</oasis:entry>
         <oasis:entry colname="col2">4f</oasis:entry>
         <oasis:entry colname="col3">agricultural waste burning</oasis:entry>
         <oasis:entry colname="col4">agriculture</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">20</oasis:entry>
         <oasis:entry colname="col2">6a</oasis:entry>
         <oasis:entry colname="col3">solid waste disposal in landfills</oasis:entry>
         <oasis:entry colname="col4">waste</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">21</oasis:entry>
         <oasis:entry colname="col2">6b</oasis:entry>
         <oasis:entry colname="col3">wastewater treatment</oasis:entry>
         <oasis:entry colname="col4">waste</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">22</oasis:entry>
         <oasis:entry colname="col2">7a</oasis:entry>
         <oasis:entry colname="col3">fossil fuel fires</oasis:entry>
         <oasis:entry colname="col4">FF_fuels</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2">
  <title>Material and methods</title>
<sec id="Ch1.S2.SS1">
  <title>Modelling framework</title>
      <p id="d1e890">Before describing the different models composing the modelling framework, we
introduce some specific terminology to reduce ambiguity in Sect. 2.1.1–2.1.6. Quantities that can be observed are termed
“species” or “trace gases”, corresponding
in this case to total CO<inline-formula><mml:math id="M39" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, and CH<inline-formula><mml:math id="M40" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. These three species are
simulated using five “modelled species”, namely CO<inline-formula><mml:math id="M41" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> from fossil fuels, CO<inline-formula><mml:math id="M42" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> related
to GEE (gross ecosystem exchange), CO<inline-formula><mml:math id="M43" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> related to respiration, CO, and CH<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. Modelled
species related to anthropogenic emissions are modelled as the sum of
contributions from different “emission sectors” (Table 1) and“fuel types” (Table 2); for further
differentiation, anthropogenic and biospheric contributions are split
into monthly contributions. Simulated fluxes specific for different modelled
species, emission sectors, fuel types, and months of the year are called
“flux categories”. In this section, a brief description of the different
models that make up the modelling framework is given. For more detailed
information, see Boschetti et al. (2015).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><caption><p id="d1e951">Specific fuel types accounted for in the state vector and
aggregated categories as used in Fig. 8.</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>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Fuel type</oasis:entry>
         <oasis:entry colname="col3">Aggregated</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">fuel type</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">brown coal</oasis:entry>
         <oasis:entry colname="col3">coal</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">hard coal</oasis:entry>
         <oasis:entry colname="col3">coal</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">peat</oasis:entry>
         <oasis:entry colname="col3">coal</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">gas derivatives</oasis:entry>
         <oasis:entry colname="col3">gas</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">5</oasis:entry>
         <oasis:entry colname="col2">natural gas</oasis:entry>
         <oasis:entry colname="col3">gas</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">6</oasis:entry>
         <oasis:entry colname="col2">heavy oil</oasis:entry>
         <oasis:entry colname="col3">oil</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">7</oasis:entry>
         <oasis:entry colname="col2">light oil</oasis:entry>
         <oasis:entry colname="col3">oil</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">8</oasis:entry>
         <oasis:entry colname="col2">solid waste</oasis:entry>
         <oasis:entry colname="col3">waste</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">9</oasis:entry>
         <oasis:entry colname="col2">venting and flaring</oasis:entry>
         <oasis:entry colname="col3">oil</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">10</oasis:entry>
         <oasis:entry colname="col2">other<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">other</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">11</oasis:entry>
         <oasis:entry colname="col2">gas biofuels</oasis:entry>
         <oasis:entry colname="col3">bio</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">12</oasis:entry>
         <oasis:entry colname="col2">liquid biofuels</oasis:entry>
         <oasis:entry colname="col3">bio</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">13</oasis:entry>
         <oasis:entry colname="col2">solid biofuels</oasis:entry>
         <oasis:entry colname="col3">bio</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e954"><inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> The category “other” is derived by summing the contribution from those
processes in which it is difficult to establish the specific fuel responsible
for the emissions.</p></table-wrap-foot></table-wrap>

<sec id="Ch1.S2.SS1.SSS1">
  <title>Vertical profile input data</title>
      <p id="d1e1174">In this study the modelled profiles have identical structure to those
collected from the IAGOS fleet of commercial airliners. More precisely, the
spatial and temporal coordinates of different observations will be used as
input for the modelling framework, whereas the observed values of atmospheric
mixing ratios of CO and meteorological parameters themselves will play a
role in calibrating the modelling framework.</p>
      <p id="d1e1177">Central for this work is the concept of the mixed layer (ML), the lower part
of the troposphere in which trace gases are well mixed due to turbulent
convection in the timescale of an hour or less, and in which the effect of
regional surface–atmosphere fluxes is the strongest. As input to the
inversion we use the enhancement of the species' mixing ratio within the
mixed layer relative to that in the free troposphere (FT), similar to the
approach described in Boschetti et al. (2015). This mixed layer enhancement best
reflects the influence of regional fluxes. To compute this, we take the
average mixing ratio within the mixed layer and subtract the value taken at
2 km above the mixed layer top (<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, i.e. well within the free
troposphere. The <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a very important parameter in atmospheric
modelling, and accounts for most of the transport uncertainty in the vertical
domain. In fact, when assuming that the mixed layer is the part of the
troposphere in which trace gases are well mixed due to turbulent convection,
given a certain amount of trace gas in the ML, its mixing ratio will depend
strongly on its depth <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. More precisely, even if the model has
correctly reproduced the amount of trace gas in the real mixed layer, if the
modelled <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is lower (higher) than the actual one, then the simulated ML
mixing ratio will be higher (lower) than it actually should be. In the
present study, modelled <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is corrected according to Boschetti et al. (2015,
Sect. 2.2.1)</p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <title>Transport–flux coupling</title>
      <p id="d1e1243">The modelling framework is composed of a regional transport model (STILT),
the EDGAR (Emission Database for Global Atmospheric Research) emission
inventory to model anthropogenic emissions, VPRM (Vegetation Photosynthesis
and Respiration Model) to model emissions from the biosphere, and output from
global transport models for lateral boundary conditions for the different
modelled species. The expressions “anthropogenic emissions” and “fossil fuel
emissions” are considered synonymous in this paper and are used to indicate
the sum of fossil fuel and biofuel emissions, without including
contributions from LULUCF (Land Use, Land-Use Change and Forestry).</p>
      <p id="d1e1246">For regional transport we make use of the LPDM STILT (Stochastic
Time-Inverted Lagrangian Transport; Lin et al., 2003) to derive the sensitivity of
the atmospheric mixing ratio measurement to upstream surface–atmosphere
fluxes, so-called “footprints”. Briefly, for each measurement location and
time (also called receptor point), the model releases an ensemble of virtual
particles that are driven back in time using wind fields from ECMWF and
turbulence as stochastic process; the residence time within the lower half
of the mixed layer is used to determine the potential contribution from
surface fluxes, and the cumulative sum of these contributions determines the
footprint that identifies the part of the domain with a certain influence
on a single receptor point. To represent the mixed layer enhancements, the
footprints for receptors within the boundary layer are averaged, and the
footprint for the free tropospheric receptor is subtracted from this,
resulting in a footprint for the mixed layer enhancements.  This footprint is
then matrix-multiplied with an emission map from an emission inventory,
resulting in a simulated mixing ratio enhancement corresponding to the
regional contribution at the measurement location.</p>
      <p id="d1e1249">A detailed description of STILT is given in Lin et al. (2003) and Gerbig et
al. (2003). We use STILT coupled with emission models for both anthropogenic
(EDGAR) and biosphere (VPRM) fluxes on a regional domain that covers most of
Europe (33 to 72<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <inline-formula><mml:math id="M53" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>15 to 35<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) with a spatial
resolution of <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for latitude and <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">12</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for longitude,
roughly corresponding to 10 km. The MACC reanalysis (Inness et al., 2013,
downloaded from <uri>http://www.ecmwf.int</uri>, last access: 23 June 2016) was
used for lateral boundary conditions for CO mixing ratios, whereas for
CO<inline-formula><mml:math id="M59" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CH<inline-formula><mml:math id="M60" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> we used output from the Jena CarboScope (Rödenbeck
et al., 2003; CO<inline-formula><mml:math id="M61" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> data available from
<uri>www.bgc-jena.mpg.de/CarboScope/</uri>, last access: 10 February 2016), which
are based on forward simulations of global-inversion optimized fluxes with
the TM3<?pagebreak page9228?> transport model (Heimann and Körner, 2003). TM3 fields have lower
resolution, but they are chosen for their consistency with measurements from
the ground-based network. In addition, spatial resolution is of relatively
minor importance for the contribution from the lateral boundary as it is far
away from the measurement locations.</p>
      <p id="d1e1351"><?xmltex \hack{\newpage}?>For fossil fuel emissions, we use a model based on the EDGAR v4.3.1 emission
inventory (European Commission, 2016) modified
following the same approach taken for COFFEE (CO<inline-formula><mml:math id="M62" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> release and Oxygen
uptake from Fossil Fuel Emission Estimate; Steinbach et al., 2011; Vardag et
al., 2015). More precisely, to obtain hourly resolved emissions from the
original EDGAR annual fluxes for different emission categories we add
specific temporal activity factors (Denier van der Gon et al., 2011) to
account for differences in emissions due to seasonal, weekly, and daily
cycles. In addition, the different emission categories are further split into
contributions from different fuel types from British Petroleum's Statistical
Review of World Energy 2014 (BP, 2014). The World Energy Outlook from IEA as
alternative source of information was not chosen, as the report from BP was
available earlier (April 2015 vs. November of the following year). This allows for taking into
account changes in emissions between different years. Such an emission model
provides hourly resolved fluxes for each fossil fuel flux category with a
spatial resolution of roughly 10 km on our regional European domain. For
each of the three anthropogenic modelled species (CO<inline-formula><mml:math id="M63" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, and
CH<inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, different emission maps are used as input. Temporal profiles are
then applied to these sector- and fuel-specific emission maps. To also take
into account the contribution from the biosphere we use VPRM. VPRM simulates
realistic patterns at small spatial (10 km <inline-formula><mml:math id="M65" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10 km) and temporal
(hourly) scales and is used here to provide the a priori fluxes for
biosphere–atmosphere exchange of CO<inline-formula><mml:math id="M66" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. This model is described in detail
in Mahadevan et al. (2008).</p>
      <?pagebreak page9229?><p id="d1e1402">STILT transport is driven by meteorological fields from the ECMWF IFS (12 h forecasts twice daily at 3-hourly temporal resolution), which have a
spatial resolution of 0.25<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> with 61 vertical levels. In the following,
we will refer to the STILT/EDGAR/VPRM/MACC/TM3 combination of transport,
simulated fluxes and advected boundary conditions as merely “STILT” for
simplicity.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS3">
  <title>Bayesian inversion</title>
      <p id="d1e1421">Atmospheric inversions provide an estimate of the distribution of sources
and sinks over the domain's surface from available concentration
measurements (top-down approach). This can be formalized in the
following linear relation:
              <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M68" display="block"><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="bold">K</mml:mi><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ε</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where the <inline-formula><mml:math id="M69" display="inline"><mml:mi mathvariant="bold-italic">y</mml:mi></mml:math></inline-formula> vector contains the <inline-formula><mml:math id="M70" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> observations, and <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="bold">K</mml:mi></mml:math></inline-formula> is
the Jacobian matrix that relates the observations with the state vector
<inline-formula><mml:math id="M72" display="inline"><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:math></inline-formula>. In the present study the focus will be on
surface–atmosphere gas exchanges due to biospheric processes and
anthropogenic emissions. So the observations are trace gas mixing ratios at
different times and locations, <inline-formula><mml:math id="M73" display="inline"><mml:mi mathvariant="bold">K</mml:mi></mml:math></inline-formula> is the product of a transport
operator <inline-formula><mml:math id="M74" display="inline"><mml:mi mathvariant="bold">H</mml:mi></mml:math></inline-formula> that maps flux sensitivities at different times and
locations with a set of gridded fluxes <inline-formula><mml:math id="M75" display="inline"><mml:mi mathvariant="bold">F</mml:mi></mml:math></inline-formula> for the categories of
interest, while the state vector <inline-formula><mml:math id="M76" display="inline"><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:math></inline-formula> contains the <inline-formula><mml:math id="M77" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> scaling
factors for the flux categories of interest. <inline-formula><mml:math id="M78" display="inline"><mml:mi mathvariant="bold">H</mml:mi></mml:math></inline-formula> has
<inline-formula><mml:math id="M79" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> rows and a number of columns equal to <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi>t</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi>s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> respectively the number of pixels in the emission model
along the <inline-formula><mml:math id="M81" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M82" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axes, the number of (hourly) simulations in the whole
year of interest, and the number of state vector elements, resulting in a
huge matrix. As the matrix <inline-formula><mml:math id="M83" display="inline"><mml:mi mathvariant="bold">F</mml:mi></mml:math></inline-formula> describes the different simulated
gridded fluxes, it is comparably large and has <inline-formula><mml:math id="M84" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula> rows and <inline-formula><mml:math id="M85" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> columns. By
considering <inline-formula><mml:math id="M86" display="inline"><mml:mi mathvariant="bold">K</mml:mi></mml:math></inline-formula> as the result of the product of these two large
matrices, it is possible to limit its dimensions to only <inline-formula><mml:math id="M87" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> rows and <inline-formula><mml:math id="M88" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula>
columns; this allows for simplifying the critical task of relating
observation with simulated fluxes of the categories of interest. The state
vector accounts for specific emission sectors (Table 1) and fuel types
(Table 2) for each one of the three modelled species from the EDGAR emission
model, plus gross fluxes (gross ecosystem exchange, GEE, and respiration,
<inline-formula><mml:math id="M89" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>) modelled by VPRM for five different vegetation classes. For both
anthropogenic and biospheric fluxes the temporal resolution of the state
vector is monthly. The number of state vector elements per month amounts to
69 scaling factors for the different fuel- and sector-specific anthropogenic
emissions for each species, and 10 scaling factors for biosphere–atmosphere
exchange (respiration and photosynthesis for each of the five vegetation
classes), so in total 217 scaling factors per month, or 2604 scaling factors
for the full year. To avoid large memory requirements for <inline-formula><mml:math id="M90" display="inline"><mml:mi mathvariant="bold">H</mml:mi></mml:math></inline-formula> and
<inline-formula><mml:math id="M91" display="inline"><mml:mi mathvariant="bold">F</mml:mi></mml:math></inline-formula> matrices, their product is directly computed within the STILT
code. The random error
<inline-formula><mml:math id="M92" display="inline"><mml:mi mathvariant="italic">ε</mml:mi></mml:math></inline-formula> accounts for measurement error related to
uncertainty in the observation and to model–data mismatch resulting from
model uncertainty.</p>
      <p id="d1e1645">Bayesian inversion combines observations (IAGOS profiles) with a priori
information (scaling factors and their a priori uncertainties) to
reconstruct the most probable state vector. Optimum posterior estimates of
the scaling factors are obtained by minimizing the following cost function
<inline-formula><mml:math id="M93" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> (Rodgers, 2000):

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M94" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>J</mml:mi><mml:mfenced close=")" open="("><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:mfenced></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="bold">K</mml:mi><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:mrow></mml:mfenced><mml:mi>T</mml:mi></mml:msup><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="bold">K</mml:mi><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mi>T</mml:mi></mml:msup></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where the first and the second term are the observational constraint and the
prior constraint term respectively. The prior scaling factors for the fluxes
of the different tracers are set equal to one. <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
is the error covariance matrix for the mismatch between simulated and
observed mole fractions (model–data mismatch) and accounts for instrumental
uncertainty, uncertainty related to the transport model, and other sources of
uncertainty like boundary conditions and flux aggregation not accounted for
through the state vector adjustment. <inline-formula><mml:math id="M96" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
error covariance matrix for the prior scaling factor; its implementation
requires a different approach for biospheric and anthropogenic fluxes. The
detailed error structure for model–data mismatch and prior uncertainty is
described in the Sect. 2.1.4. Minimizing the cost function results in an
optimal posterior estimate of the state vector <inline-formula><mml:math id="M97" display="inline"><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:math></inline-formula> that is
consistent with both the measurements and the prior model estimates:
              <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M98" display="block"><mml:mrow><mml:mover accent="true"><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mi mathvariant="bold">K</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mi mathvariant="bold">K</mml:mi><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">K</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mi mathvariant="bold-italic">y</mml:mi><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The error covariance matrix of the optimal posterior state (the posterior
uncertainty) is given by
              <disp-formula id="Ch1.E4" content-type="numbered"><mml:math id="M99" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msup><mml:mi mathvariant="bold">K</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mi mathvariant="bold">K</mml:mi><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Note that this quantity depends on neither the prior fluxes nor the measured
mixing ratios, but only on their respective uncertainties and on the
transport matrix <inline-formula><mml:math id="M100" display="inline"><mml:mi mathvariant="bold">K</mml:mi></mml:math></inline-formula>. In this study, the inverse of the matrices was
calculated using the R function “solve'` from the base package of R
version 3.0.0 (<uri>http://www.r-project.org/</uri>, last access: 30 April 2013).</p>
      <p id="d1e1938">The targeted quantities of this study are the aggregated emissions over a
specific area at a specific timescale (e.g. month); those quantities can be
derived from the prior and posterior state through a spatiotemporal
aggregation operator <inline-formula><mml:math id="M101" display="inline"><mml:mi mathvariant="bold">A</mml:mi></mml:math></inline-formula> that allows for the conversion of scaling
factors into physically representative quantities. As the pseudo-observations
are clustered around a single location (Frankfurt), it is very likely that the fluxes over the whole European domain are not constrained. Therefore, as a spatial aggregation scale we chose an area from
which fluxes have a significant contribution to the observations made at
Frankfurt. For this we compute the temporally accumulated footprint values
(cf. Sect. 2.1.2) for the whole year 2011, and select those spatial pixels
that correspond to 50 % of the total (spatially integrated) footprint
(Fig. 1). Note that by using this aggregation<?pagebreak page9230?> scale we assume perfectly known
distribution within a given flux category that can result in aggregation
error, especially with respect to biogenic fluxes, that are not as well known
as anthropogenic fluxes. However, the chosen domain of aggregation is quite
small, and the total anthropogenic fluxes are divided according to species,
emission categories, fuel types, and months. This results in 69 degrees of
freedom per month for each anthropogenic species and 10 degrees of freedom
per month for the biospheric fluxes; for this reason we expect the
aggregation error not to be a particularly important source of uncertainty.
The prior and posterior uncertainty of these targeted quantities
(<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is obtained by applying
the aggregation operator to the respective uncertainty covariances:

                  <disp-formula id="Ch1.E5" content-type="numbered"><mml:math id="M104" display="block"><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mi mathvariant="bold">A</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mi mathvariant="bold">A</mml:mi></mml:mrow></mml:msqrt><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mtext>and</mml:mtext><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mi mathvariant="bold">A</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub><mml:mi mathvariant="bold">A</mml:mi></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

            Different versions of the aggregation operator were created for this:
emissions categories are aggregated according to different fuel types (coal,
oil, gas, bio, waste, and other) and according to emission sectors (energy,
transport, industry, buildings, agriculture, waste, and fossil fuel fires). Note
that only these aggregated fluxes are optimized, not the individual gridded
fluxes of the emission inventories.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p id="d1e2034">Cumulative sum of the ML footprints for all the flights into or out
of Frankfurt airport (FRA) in the year 2011. The grey line delineates the
50 % footprint.</p></caption>
            <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f01.png"/>

          </fig>

      <p id="d1e2044">To quantitatively assess the information provided by the inversion, the
reduction of uncertainty in the posterior compared to the prior estimate is
a useful measure. The uncertainty reduction (UR) is defined as
              <disp-formula id="Ch1.E6" content-type="numbered"><mml:math id="M105" display="block"><mml:mrow><mml:mi mathvariant="normal">UR</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The uncertainty reduction ranges from 0 (posterior as large as the prior
uncertainty) to 1 (posterior negligible compared to the prior uncertainty).</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S2.SS1.SSS4">
  <title>Prior error structure</title>
      <p id="d1e2084">As in this study a multi-species inversion with CO, CO<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and CH<inline-formula><mml:math id="M107" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> is
envisioned, we have the chance to exploit the correlations in the
uncertainties of the different trace gases related to both a priori fluxes
and model–data mismatch. This is particularly true for CO and CO<inline-formula><mml:math id="M108" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
because they share a larger part of the emission sources, which implies
correlations in the respective uncertainties. In the multi-species
inversion, such information is stored in the areas of the error covariance
matrices that describe covariance between different modelled species
(off-diagonal “blocks” in Fig. 2b for <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and Fig. 3b for <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>. In the single-species
inversions, said covariance is set to zero, corresponding to a situation
where the different species are completely independent of one another.
Conversely, the measurement uncertainty is stored in the main diagonal of
the <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Fig. 3d).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e2152">Prior error correlation matrix <bold>(a)</bold> used in the multi-species
inversion, and the respective components for modelled species <bold>(b)</bold>, emission
sectors <bold>(c)</bold>, and fuel types <bold>(d)</bold>. Matrix <bold>(a)</bold> is the element-wise product of
matrices <bold>(b)</bold>, <bold>(c)</bold>, and <bold>(d)</bold>. Each matrix has the same dimensions (2604 <inline-formula><mml:math id="M112" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2604)
reflecting the length of the state vector. The matrices are shown for only
1 month here, for illustration. The grey lines indicate subsets of the
flux categories according to different modelled species (blocks), ordered
as follows from top to bottom and from left to right: anthropogenic
CO<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, CH<inline-formula><mml:math id="M114" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>, GEE, and respiration. In the single-species
inversion, the correlation values in the off-diagonal blocks of
matrix <bold>(b)</bold>
are set to zero. In the complete matrix, correlation between fluxes from
different months is also set to zero.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f02.png"/>

          </fig>

      <p id="d1e2215">We used a single year (2011) dataset restricted to the vertical profiles
centred at the Frankfurt airport (FRA) and restricted to daytime during
well-mixed atmospheric conditions (10:30 to 17:30 CET). The dataset contains
1098<?pagebreak page9231?> pseudo-observations, 366 for each of the three observable species,
whereas the state vector contains the scaling factors for 2604 flux
categories, each equal to one in the prior.</p>
      <p id="d1e2218">The prior error covariance matrix can be expressed as follows:
              <disp-formula id="Ch1.E7" content-type="numbered"><mml:math id="M115" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the prior error correlation matrix
(Fig. 2a) and <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a prior rescaling
matrix described in Sect. 2.1.5 (Fig. 4a). First we describe how
<inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is generated. The prior error correlation
matrix is a square matrix of rank 2604, reflecting the length of the state
vector, and results from the product of three components (Fig. 2b, c, and d) accounting for correlations between flux categories according to the
modelled species, emission sectors, and fuel types respectively. In four
different instances, a correlation of 0.7 is applied:
<list list-type="order"><list-item>
      <p id="d1e2281">between different anthropogenic modelled species;</p></list-item><list-item>
      <p id="d1e2285">between GEE and respiration;</p></list-item><list-item>
      <p id="d1e2289">between different emission sectors;</p></list-item><list-item>
      <p id="d1e2293">between different fuel types.</p></list-item></list>
Such a correlation implies that the explained variance for each constraint,
everything else being equal, is roughly 50 % (0.7 to the square equals
0.49), with the rest remaining independent. In addition, the correlation
between fossil-fuel-related and biosphere-related scaling factors is zero,
and the same holds for fluxes of different months, indicating complete
independence from one another. In this study, we assume a certain annual
total domain-wide flux uncertainty, and then break it down by sectors,
fuels, and months by inflating the error. By assuming no correlation between
different months we ensure maximum flexibility in the system to retrieve
month-to-month changes based on the observations. We assume correlation
between months is possible, but it has not been investigated here. It is
unclear how good the seasonal variation in emissions from the inventories
actually is; so in order to not rely too much on these we chose zero
correlation. Investigating the effects of different correlation set-ups for
the seasonal cycle could be the focus of future research.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS5">
  <title>Prior error scaling</title>
      <p id="d1e2303">After having specified the prior error correlation matrix
<inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, we now describe how we rescale it to obtain
<inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; for this task we rewrite Eq. (7) as

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M121" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub><mml:mo>=</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>=</mml:mo><mml:mfenced close=")" open="("><mml:mtable class="array" columnalign="center center"><mml:mtr><mml:mtd><mml:mtable class="array" columnalign="center center center"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">11</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">12</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">13</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">21</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">22</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">23</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">31</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">32</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mn mathvariant="normal">33</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mtd><mml:mtd><mml:mtable class="array" columnalign="center"><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtable class="array" columnalign="center center center"><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mn mathvariant="normal">0</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/></mml:mrow></mml:mtd><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mtd><mml:mtd><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">bio</mml:mi></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E8"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mfenced close=")" open="("><mml:mtable class="array" columnalign="center center"><mml:mtr><mml:mtd><mml:mtable class="array" columnalign="center center center"><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mtd><mml:mtd><mml:mtable class="array" columnalign="center"><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtable class="array" columnalign="center center center"><mml:mtr><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd><mml:mtd><mml:mn mathvariant="normal">0</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mtd><mml:mtd><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">bio</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where each <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is a subset of the fossil fuel part of
<inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (block) as shown in Fig. 2, and each <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is defined as
              <disp-formula id="Ch1.E9" content-type="numbered"><mml:math id="M125" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="bold">A</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:mi>T</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="bold">A</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>j</mml:mi></mml:munder><mml:msub><mml:mi>A</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:msqrt><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold">A</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is the aggregation operator for annual fluxes over the
full domain, and <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the corresponding relative prior
uncertainty, assuming the values specified in Table 3 for different cases.
Case 1 is considered as the default case, with prior uncertainty values
conservatively assumed to be 20 % for CO<inline-formula><mml:math id="M128" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and 50 % for CO and
CH<inline-formula><mml:math id="M129" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. Conversely, <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">bio</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> covers the biosphere part
of <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and for <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:mo>∑</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
for <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">bio</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> we use a prior uncertainty of 0.54 GtC y<inline-formula><mml:math id="M134" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, as
derived in Kountouris et al. (2018) for the VPRM model. The biospheric part
of the prior error covariance matrix assumes no correlation with the fossil
fuel species.</p>
      <p id="d1e2911">The posterior of each Bayesian inversion depends on its specific prior. As
the multi- and single-species inversions have different prior uncertainty
structures, the uncertainty reduction for targeted quantities cannot be
directly compared (Eq. 4). To be able to compare the two inversions, we
require that the a priori aggregated uncertainty of the targeted quantities
remains the same, and distribute it differently each time; the prior
rescaling matrix <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is needed for this
task. The benefits were tested for observations taken in different months
and for three different error structures in the prior uncertainty. As a
priori aggregated uncertainty we use a percentage of the aggregated modelled
emissions for fossil fuels across the whole year. Table 3 shows the
percentage values used for different cases.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><caption><p id="d1e2928">Relative uncertainty of the prior fluxes aggregated domain-wide and
annually for the different cases.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">CO<inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">CO</oasis:entry>
         <oasis:entry colname="col4">CH<inline-formula><mml:math id="M137" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Case 1</oasis:entry>
         <oasis:entry colname="col2">20 %</oasis:entry>
         <oasis:entry colname="col3">50 %</oasis:entry>
         <oasis:entry colname="col4">50 %</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Case 2</oasis:entry>
         <oasis:entry colname="col2">10 %</oasis:entry>
         <oasis:entry colname="col3">50 %</oasis:entry>
         <oasis:entry colname="col4">50 %</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Case 3</oasis:entry>
         <oasis:entry colname="col2">10 %</oasis:entry>
         <oasis:entry colname="col3">25 %</oasis:entry>
         <oasis:entry colname="col4">25 %</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS1.SSS6">
  <title>Model–data mismatch error structure</title>
      <p id="d1e3032">In an atmospheric inversion, the model–data mismatch from every uncertainty
source (such as measurement uncertainty, transport model uncertainty,
spatial representation error due to limited model resolution, and boundary
condition inaccuracies) needs to be taken into account. In our<?pagebreak page9232?> inversion
scheme, we parameterize both the transport model uncertainty and the
measurement uncertainty, with the latter playing a minor role. The
model–data mismatch covariance matrix (<inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>
is constructed according to the following equation:
              <disp-formula id="Ch1.E10" content-type="numbered"><mml:math id="M139" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="bold">s</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">tran</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">meas</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> accounts for correlations between different
observed species (Fig. 3b), <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">C</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> accounts for the
temporal correlation (Fig. 3c), <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">tran</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the total transport error, and
<inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">meas</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:math></inline-formula> accounts for all of the
non-transport-related errors like spatial representation error and lateral
boundary conditions (Fig. 3d).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p id="d1e3138">Model–data mismatch correlation matrix <bold>(a)</bold> used in the
multi-species inversion, species correlation matrix <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(b)</bold>, temporal
correlation matrix <inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(c)</bold>, and squared measurement uncertainty <bold>(d)</bold>. Note
that the measurement uncertainty is expressed in ppm for CO<inline-formula><mml:math id="M146" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and ppb
for CO and CH<inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. Each matrix has the same dimensions (1098 <inline-formula><mml:math id="M148" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1098)
reflecting the length of the observation vector, but here only the data of
July are plotted to increase visibility. The grey lines indicate different
species in the observation vector (blocks), ordered as follows from top to
bottom and from left to right: total CO<inline-formula><mml:math id="M149" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, and CH<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. In the
single-species inversion, the correlation value in the off-diagonal
blocks
of matrix <bold>(b)</bold> is set to zero. The structure in <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi>s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in <bold>(c)</bold> is a result of
the uneven temporal distribution of the observations within the month.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f03.png"/>

          </fig>

      <p id="d1e3243">The assumed measurement uncertainty is 1 ppm for CO<inline-formula><mml:math id="M152" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, 20 ppb for CO, and
20 ppb for CH<inline-formula><mml:math id="M153" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>, while <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">tran</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is time dependent and
assumed to be proportional to the modelled enhancement due to regional
fluxes. The assumed measurement uncertainty is higher than the expected
instrument precision because it also includes in addition the uncertainties
related to spatial representation and lateral boundary conditions.
<inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">tran</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is characterized as follows by different components
in the vertical and horizontal domain:
              <disp-formula id="Ch1.E11" content-type="numbered"><mml:math id="M156" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">tran</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">enh</mml:mi><mml:msqrt><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:msqrt><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where enh indicates the modelled enhancement, and both the horizontal transport
error <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and the vertical transport
error <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are characterized as
percentage error; <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is assumed to be
50 %, while <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is a profile-specific
relative error with a mean value of about 10 %. The vertical transport
error accounts for the fact that the shallower the mixed layer is, the more
difficult it is to model the atmosphere. We assume that after <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> correction
the remaining error is of the order of 50 m (related to the vertical
resolution of the profile data), so the relative error <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mrow><mml:mi mathvariant="normal">tran</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi mathvariant="normal">v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is assumed to be the ratio of 50 m to the modelled
<inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; in this way we obtain an error that gets larger the shallower the
mixed layer is. For the horizontal component, an uncertainty of 50 % is a
conservative estimate based on Lin and Gerbig (2005), where the horizontal
transport error is found to be 5.9 ppm for CO<inline-formula><mml:math id="M164" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. This, combined with
about 10 ppm of drawdown in the mixed layer relative to the free
troposphere, gives something like 50 % error in the regional flux signal.
The vertical component is so much smaller in percentage since the simulated
mixing ratios are already corrected for mismatch between modelled and
observed <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e3457">In the multi-species inversion, the transport error correlation across
species is 0.7 (Fig. 3b), while in the single-species inversion this is set
to zero. Time correlation is assumed to decay exponentially with an
exponential constant of 12 h. The between-species correlation for
model–data mismatch related to transport uncertainty reflects the fact that
species are partially co-emitted and share the same atmospheric transport
(and its related uncertainty).</p>
</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Synthetic experiment</title>
<sec id="Ch1.S2.SS2.SSSx1" specific-use="unnumbered">
  <title>Pseudo-data generation</title>
      <p id="d1e3472">As explained in the introduction, in situ measurements are not available for
all of the three trace gases of interest, but only for CO. For this reason
this paper aims to evaluate the benefits of a multi-species inversion over a
corresponding single-species inversion by performing a synthetic experiment, using
pseudo-observations derived by perturbation of the model outputs based on a
priori state vector values. More precisely, the pseudo-observation vector is
obtained by matrix multiplication between the Jacobian matrix <inline-formula><mml:math id="M166" display="inline"><mml:mi mathvariant="bold">K</mml:mi></mml:math></inline-formula> and
what we assume to be the true state vector. The true state vector itself is
obtained by using the sum of the prior state vector (all values equal to
one) and a random realization of the prior error, truncated to avoid
negative state vector values. In detail, the error realization is obtained
by multiplying a randomly generated, normally distributed vector with the
prior error covariance matrix. This ensures that such a realization has the
same error correlation as the prior uncertainty. Where the<?pagebreak page9233?> result of such
matrix-vector product is negative, the same operation is performed
recursively until all elements of the state vector are positive.  This ensures
that the difference between the true and prior state vector has the same
error correlation structure as described by the prior error covariance
matrix.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e3484">The final rescaling matrix <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(a)</bold> and the prior
error covariance matrix <inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(b)</bold>. Note that <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be
defined as the element-wise ratio of <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> to C<inline-formula><mml:math id="M171" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:math></inline-formula>.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f04.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e3555">Mean daily enhancement of mixed layer vs. free tropospheric mole
fractions. Modelled mixing ratios are shown as black lines, while the
observed CO is shown as a blue line. Note that the modelled values for CO have
been multiplied by a factor of 2.8, corresponding to the mean ratio between
observed and modelled CO enhancements, to match the observed values.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f05.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results and discussion</title>
      <p id="d1e3572">Before evaluating the performance of the inversion scheme in reducing the
uncertainty of the state space, a closer look at the ability of the modelling
framework to reproduce the enhancements is necessary. Unfortunately, this
can be done only for CO as actual measurements are not available for the
other species. Figure 5 shows the mean daily enhancement of the three fossil
fuel species for both observations and model outputs using prior emissions.
A common feature of the three trace gases is that lower values tend to occur
during summer time due to better mixing of the atmosphere. Conversely,
enhancement values tend to be higher during winter, reflecting the more
stratified atmosphere of the cold months.</p>
      <p id="d1e3575">In Fig. 5 the modelled CO plot was multiplied by a factor of 2.8,
corresponding to the mean ratio between observed and modelled CO
enhancements, similar to what was found in Boschetti et al. (2015). Mixing ratio
values are highly variable, but the model provides a good indication of the
temporal variation of the ML enhancement; the squared correlation
coefficient between observed and modelled CO enhancements is 0.62, while the
standard deviation of corrected model and observation residuals is 85 ppb;
note that by not accounting for the <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> correction, such values would be
0.56 and 87 ppb respectively. The median of the mixing ratio enhancement for
the three trace gases is 2.8 ppm for CO<inline-formula><mml:math id="M173" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, 18.6 ppb for CO, and 26.6 ppb
for CH<inline-formula><mml:math id="M174" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. For CO<inline-formula><mml:math id="M175" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> this seasonal difference is enhanced due to the
simultaneous presence of both anthropogenic and biogenic emissions. During
summer, values are slightly negative due to strong photosynthesis fluxes from
growing vegetation from the active combined with deeper vertical mixing.
Negative values arise in 31 % of the cases predominantly during the warmer
months, implying that during the growing period uptake by photosynthesis
dominates over release from combustion and respiration. Both CO and CH<inline-formula><mml:math id="M176" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>
experience higher values during winter due to the shallow mixed layer
usually associated with cold temperatures, and lower values during summer as
higher temperatures cause the mixed layer to reach higher altitudes;
differences related to seasonal domestic heating and transportation may also
play a role. In addition, enhancement for both species is occasionally
negative, most likely owing to advection of polluted air masses in the free
troposphere. An alternative explanation is that strong winds at lower
heights can disperse the emissions in the boundary layer and create a
situation in which the mixing ratio in the FT is higher than in the ML.</p>
      <p id="d1e3625">Figure 6 shows the prior and posterior error covariance matrices for the
base multi-species inversion. Note that CO<inline-formula><mml:math id="M177" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> from anthropogenic
emissions is assumed to be independent from biogenic emissions; therefore
prior error correlation between these categories is zero. The posterior
error covariance matrix for the multi-species inversion (Fig. 6b) shows
lower values corresponding to an average uncertainty reduction of 23 %
across all state vector elements, while the posterior error covariance
matrix for the single-species inversion (not shown) is characterized by a
mean uncertainty reduction of 20 %. This result implies that the
multi-species inversion improves the uncertainty reduction by roughly
15 %. Negative values in the posterior error correlation matrix are to be
expected because different categories are bound together by correlations and
therefore are not free to vary independently.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e3639">Prior error covariance matrix <bold>(a)</bold> and corresponding posterior
error covariance matrix <bold>(b)</bold>.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f06.png"/>

      </fig>

      <p id="d1e3655">Figures 7 and 8 show a priori, a posteriori, and “true” fluxes related to
different aggregated fuel types and to different emission categories as
described in Tables 1 and 2 for the months of July and December. Figure 8
also shows the biospheric contribution (as absolute values) scaled down by a
factor of 10. As is to be expected, the biospheric contributions show strong
differences according to the seasonal cycle, while anthropogenic emissions
remain rather stable. However, it is worth pointing out that while the
fossil fuel prior is similar for both months, the assumed truth can be
rather different due the random assignment of the prior error realization.
In most cases, the posterior adapts and is therefore closer to the truth
than the prior; the posterior uncertainty is also visibly reduced, as
expected. Regarding the different tracers, CO<inline-formula><mml:math id="M178" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO show a somewhat
similar pattern indicating a partial overlap in dominating emission
categories while CH<inline-formula><mml:math id="M179" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> is dominated by different contributions in both
fuel types and emission categories.</p>
      <p id="d1e3676">Our modelling framework is currently not well suited to account for
unreported sources of CH<inline-formula><mml:math id="M180" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> due to the lack of information about natural
gas and oil production operations, or from recent and old mining areas.
Many recent studies have discussed the problem, mainly referring to shale
basins exploited via hydraulic fracturing in the USA (e.g. Kort et al., 2016;
Karion et al., 2015; Lyon et al., 2015). For example, Karion et al. (2015)
concludes that EDGAR<?pagebreak page9234?> underestimates methane emissions associated with oil
and gas industry by a factor of 5 in the USA. However, the situation over the
European continent may be quite different. In a review about risk assessment
of shale gas development in the UK, Prpich et al. (2015) reports that the European
Union is generally much more cautious about unconventional oil and gas
sources, while a recent study on a methane plume over the North Sea (Cain et
al., 2017) concluded that the bulk signature of said plume originated from
on-shore coal mines and power stations in the Yorkshire area.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e3690">Prior, posterior, and true (pseudo-data) fluxes in physical units
aggregated for different fuel types. Note that as the true fluxes are the
result of a random perturbation of the prior, they do not describe an actual
situation in the physical world. So, for example, the fact that the true
value of CH<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> fluxes in July is lower than the same value in December
should not be surprising.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f07.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e3710">Prior, posterior, and true (pseudo-data) fluxes in physical units
aggregated for different emission sectors for CO<inline-formula><mml:math id="M182" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> <bold>(a)</bold>,
CO <bold>(b)</bold>, and CH<inline-formula><mml:math id="M183" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> <bold>(c)</bold>. Absolute values of
biosphere–atmosphere exchange fluxes of CO<inline-formula><mml:math id="M184" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> are included in
<bold>(a)</bold>, but scaled down by a factor of 10. Note that as the true fluxes
are the result of a random perturbation of the prior, they do not describe an
actual situation in the physical world. So, for example, the fact that the
true value of CO for transport in July is higher than the same value in
December should not be surprising.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f08.png"/>

      </fig>

      <p id="d1e3759">In general, the absence of some emission sources in an inventory is
equivalent to the assumption of having point sources not included in the
emission map, but still contributing to the measurements. The inversion
scheme would typically react to this by assigning such point sources in some
other sectors to another fuel type. As a result, the posterior enhancements would
be biased low in proximity of those point sources, and (slightly) biased high
for influences from other regions with the same sector or fuel type. This
issue should definitely be considered in future study making use of actual
CO, CO<inline-formula><mml:math id="M185" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and CH<inline-formula><mml:math id="M186" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> observations from IAGOS but has limited effects on
this paper, as our main focus is on the benefits of inter-species
correlation on the posterior uncertainty in a synthetic
experiment.</p>
      <p id="d1e3781">Note that our modelling framework does not allow for simulating CO biogenic
fluxes during the growing season. Warm days in summer correspond to large
amount of biogenic volatile organic compounds (VOCs) being emitted from
vegetation, producing CO at non-negligible levels. According to Hudman et
al. (2008), anthropogenic emissions account for only 31 % of CO emissions
in the USA during summer. Conversely, according to estimates from EDGAR,<?pagebreak page9235?> CO
anthropogenic emissions during summer are about 18 % of the annual
anthropogenic emissions. Combining these two results, one could conclude that
CO production from biogenic sources accounts for roughly 42 % of total
annual CO emissions.</p>
      <p id="d1e3784">CO<inline-formula><mml:math id="M187" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO are dominated by combustion sectors (Fig. 8). The most
important emission sectors for CO<inline-formula><mml:math id="M188" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> are energy, industry, transport, and
building, each contributing 7–10 in July and 6–14 MtC month<inline-formula><mml:math id="M189" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in
December. Dominant fuels (Fig. 7) for CO<inline-formula><mml:math id="M190" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> are coal, gas, and oil, whose
prior fluxes (pseudo-data) have a magnitude of 6–11 Megatons of carbon per
year (MtC month<inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in July and 8–14 MtC month<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in December.
For CO the most important emission sector is heating of buildings during winter, contributing a
flux of 0.19 MtC month<inline-formula><mml:math id="M193" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Contributions from industry and transport dominate during summer, with magnitudes of 0.04 and 0.05 MtC month<inline-formula><mml:math id="M194" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
respectively. The dominant fuel for CO is biofuel with 0.19 MtC month<inline-formula><mml:math id="M195" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
emissions during winter. The secondary industrial and transport contributions
originate in summer from oil and biofuels with a magnitude of
0.06–0.08 MtC month<inline-formula><mml:math id="M196" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and from agricultural waste burning with a
magnitude of 0.06–0.11 MtC month<inline-formula><mml:math id="M197" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p>
      <p id="d1e3914">Contrary to CO<inline-formula><mml:math id="M198" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO, CH<inline-formula><mml:math id="M199" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> is determined by non-combustion
sectors, more specifically by a contribution of 0.15 MtC month<inline-formula><mml:math id="M200" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> flux
from agriculture (manure management and rice cultivation) in July with
secondary contributions from waste and energy with a magnitude of roughly
0.06–0.08 MtC month<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in both July and December. Other non-combustion
sectors, in particular wastewater treatment and landfills contribute to a
total of 0.16–0.24 MtC month<inline-formula><mml:math id="M202" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> of emissions. These non-combustion
sectors contribute to less than 20 % of total CO<inline-formula><mml:math id="M203" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions, with
1.13 MtC month<inline-formula><mml:math id="M204" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from the cement and lime industry and less than 20 %
of the total CO emissions (0.03 MtC month<inline-formula><mml:math id="M205" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from the metal industry).</p>
      <p id="d1e4005">The contribution to CO<inline-formula><mml:math id="M206" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> from biospheric primary production (a sink for
atmospheric CO<inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is about 100 MtC month<inline-formula><mml:math id="M208" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in July, which drops to
almost zero in December, while respiration values are 50 MtC month<inline-formula><mml:math id="M209" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in
July and roughly 15 MtC month<inline-formula><mml:math id="M210" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in December.</p>
      <p id="d1e4065">As further assessment of the inversion performance, we tested the ability of
the inversion scheme to capture the truth compared with a perturbed version
of the prior. Such perturbed version is obtained by adding a random
distribution with mean and standard deviation equal one to the prior state
space, similar to how the truth is obtained. For each simulated species we
calculated the total annual fluxes for prior, posterior, truth, and
perturbed prior. From these total fluxes we then derive the overall residual
between prior and truth, posterior and truth, and perturbed prior and truth.
It is clear from Table 4 that while the overall bias between posterior and
truth is lower than the prior–truth bias, the bias between perturbed prior
and truth is much higher, implying that the performance of the inversion is
not an artifact of the pseudo-data generation. In addition, it was found
that the truth–posterior bias of the multi-species inversion is mostly
slightly lower compared to the single-species inversion. The difference is
between <inline-formula><mml:math id="M211" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.2 and 7.6 %, according to the simulated species, with an
overall value of 0.3 %.</p>
      <p id="d1e4075">Improper characterization of the error correlation may result in systematic
bias in the posterior estimate. As mentioned in Sect. 2.1.6, inter-species
correlation, the correlation between different fuel types and the
correlation between different emission sectors in
<inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, is assumed equal to 0.7 (Sect. 2.1.4). To
assess how well the system will reproduce the true fluxes with incorrectly
specified correlations, a series of experiments was performed in which the
inter-species correlation in <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="italic">ε</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> remains
equal to 0.7, while the three correlation coefficients in
<inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold">S</mml:mi><mml:mi mathvariant="normal">prior</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> assume different values ranging from 0.1 to
0.9. Table 5 shows the residuals between total annual posterior fluxes and
total annual true fluxes for the five simulated species, derived similarly
as for Table 4. We found that for all species the uncertainty reduction
increases with correlation. More precisely, from correlation 0.1 to 0.9, the
annual uncertainty reduction for anthropogenic CO<inline-formula><mml:math id="M215" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> increases from
26.6 to 51.7 %, while the increase is lower for GEE (from 72.4 to
73.1 %) and respiration (from 39.3 to 41.3 %) because the biospheric
fluxes are independent from other species. For CO, the uncertainty reduction
increases from 60.7 (with correlation 0.1) to 66.4 % (with correlation
0.9). The annual uncertainty reduction for CH<inline-formula><mml:math id="M216" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> increases from 60.5
to 67.5 %.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><caption><p id="d1e4133">Overall bias for different species between the prior and both
posterior and perturbed prior. The percentage values in parentheses are
the corresponding prior–truth bias.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.90}[.90]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Prior–truth</oasis:entry>
         <oasis:entry colname="col3">Posterior–truth</oasis:entry>
         <oasis:entry colname="col4">Pert. prior–truth</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(MtC y<inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">(MtC y<inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">(MtC y<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">CO<inline-formula><mml:math id="M220" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> FF</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M221" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>14.2</oasis:entry>
         <oasis:entry colname="col3">1.5 (<inline-formula><mml:math id="M222" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>111 %)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M223" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>8.8 (<inline-formula><mml:math id="M224" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>38 %)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CO</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M225" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.95</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M226" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.29 (<inline-formula><mml:math id="M227" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>69 %)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M228" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.08 (<inline-formula><mml:math id="M229" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>13 %)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CH<inline-formula><mml:math id="M230" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">0.36</oasis:entry>
         <oasis:entry colname="col3">0.11 (<inline-formula><mml:math id="M231" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>68 %)</oasis:entry>
         <oasis:entry colname="col4">0.84 (<inline-formula><mml:math id="M232" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>133 %)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GEE</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M233" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>81.8</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M234" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>17.9 (<inline-formula><mml:math id="M235" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>78 %)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M236" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>116.8 (<inline-formula><mml:math id="M237" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>43 %)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Respiration</oasis:entry>
         <oasis:entry colname="col2">39.5</oasis:entry>
         <oasis:entry colname="col3">20.6 (<inline-formula><mml:math id="M238" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>48 %)</oasis:entry>
         <oasis:entry colname="col4">62.2 (<inline-formula><mml:math id="M239" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>58 %)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><caption><p id="d1e4439">Residuals between total annual posterior fluxes (post) and total
annual true fluxes (truth) for the five simulated species (in MtC y<inline-formula><mml:math id="M240" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and different inter-species correlation values
in the prior error covariance matrix (first column). The corresponding
posterior uncertainty was added for each post–truth value.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Correlation</oasis:entry>
         <oasis:entry colname="col2">Post–truth CO<inline-formula><mml:math id="M241" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> FF</oasis:entry>
         <oasis:entry colname="col3">Post–truth CO</oasis:entry>
         <oasis:entry colname="col4">Post–truth CH<inline-formula><mml:math id="M242" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">Post–truth GEE</oasis:entry>
         <oasis:entry colname="col6">Post–truth respiration</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">0.1</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M243" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>6.3 <inline-formula><mml:math id="M244" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 16.4</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M245" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M246" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M247" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.1 <inline-formula><mml:math id="M248" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M249" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.5 <inline-formula><mml:math id="M250" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.6</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M251" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>19.0 <inline-formula><mml:math id="M252" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 27.5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M253" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4<inline-formula><mml:math id="M254" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4 <inline-formula><mml:math id="M255" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 16.1</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M256" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M257" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.0 <inline-formula><mml:math id="M258" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M259" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.6 <inline-formula><mml:math id="M260" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.5</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M261" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>19.2 <inline-formula><mml:math id="M262" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 27.4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.3</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M263" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.7 <inline-formula><mml:math id="M264" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 15.9</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M265" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M266" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.0 <inline-formula><mml:math id="M267" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M268" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.6 <inline-formula><mml:math id="M269" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.4</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M270" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>19.5 <inline-formula><mml:math id="M271" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 27.3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.4</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M272" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.3 <inline-formula><mml:math id="M273" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 15.6</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M274" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M275" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.0 <inline-formula><mml:math id="M276" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.3</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M277" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.5 <inline-formula><mml:math id="M278" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.4</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M279" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>19.7 <inline-formula><mml:math id="M280" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 27.3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.5</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M281" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.1 <inline-formula><mml:math id="M282" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 15.2</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M283" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M284" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.0 <inline-formula><mml:math id="M285" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M286" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.4 <inline-formula><mml:math id="M287" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.3</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M288" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20.0 <inline-formula><mml:math id="M289" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 27.2</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.6</oasis:entry>
         <oasis:entry colname="col2">0.8 <inline-formula><mml:math id="M290" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 14.6</oasis:entry>
         <oasis:entry colname="col3">0.3 <inline-formula><mml:math id="M291" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.1 <inline-formula><mml:math id="M292" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M293" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>18.2 <inline-formula><mml:math id="M294" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.2</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M295" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20.3 <inline-formula><mml:math id="M296" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 27.1</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.7</oasis:entry>
         <oasis:entry colname="col2">1.5 <inline-formula><mml:math id="M297" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 13.7</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M298" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M299" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.1 <inline-formula><mml:math id="M300" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M301" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>17.9 <inline-formula><mml:math id="M302" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.2</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M303" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20.6 <inline-formula><mml:math id="M304" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 26.9</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.8</oasis:entry>
         <oasis:entry colname="col2">1.9 <inline-formula><mml:math id="M305" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 12.4</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M306" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.3 <inline-formula><mml:math id="M307" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.2 <inline-formula><mml:math id="M308" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M309" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>17.6 <inline-formula><mml:math id="M310" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.1</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M311" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20.9 <inline-formula><mml:math id="M312" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 26.8</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">0.9</oasis:entry>
         <oasis:entry colname="col2">1.5 <inline-formula><mml:math id="M313" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 10.4</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M314" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.4 <inline-formula><mml:math id="M315" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col4">0.3 <inline-formula><mml:math id="M316" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M317" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>17.3 <inline-formula><mml:math id="M318" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 23.0</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M319" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>21.1 <inline-formula><mml:math id="M320" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 26.5</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?pagebreak page9236?><p id="d1e5230">In addition, the posterior–truth biases are always lower than the
prior–truth biases. The posterior uncertainty values (1<inline-formula><mml:math id="M321" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>) are usually
larger then the corresponding bias values as expected, except for CO and for
CH<inline-formula><mml:math id="M322" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> with prior correlations equal to 0.9. Thus the posterior is not
significantly different from the truth. Conversely, the prior (not shown) is
significantly different from the prior in the majority of cases for fossil
fuel fluxes, and in some cases also for biogenic fluxes. The effect of
assuming the incorrect error correlations appears to be in general small,
possibly implying a relative robustness of our methods. Following this
result, the fact that CH<inline-formula><mml:math id="M323" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> is only partially co-emitted with CO<inline-formula><mml:math id="M324" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
and CO should not affect the inversion in a strong way. For all of the
experiments, the residuals between true and posterior fluxes are lower than
residuals between true and prior fluxes for each of the simulated species;
the difference between the cases with maximum and minimum residuals is
around 4.2 %. In addition, we found that the posterior aggregated fluxes
in the nine experiments are not significantly different from each other,
implying that the system is fairly robust against errors in the assumed
inter-species correlation.</p>
      <p id="d1e5267">Before investigating the benefits of correlations between different tracers,
it is worthwhile to evaluate the uncertainty reduction in the monthly
budgets for all five modelled species (Fig. 9, based on targeted spatial
domain in Fig. 1). The first thing to note is that for all of the five trace
gases the posterior uncertainty is lower than the prior one, as it should
be. In addition, prior uncertainty varies through the year, reflecting
modulation in emission fluxes obtained by adding activity factors to
describe the seasonal, weekly, and daily cycle.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p id="d1e5272">Comparison between prior and posterior monthly uncertainties for
the five tracers. The posterior uncertainty is plotted for both the
multi-species inversion, accounting for inter-species correlations, and the
single-species inversion, in which all of the species are independent. Both
prior and posterior uncertainty are expressed in physical units. The spike
in the prior methane uncertainty estimate for the month of March depends on
the emission inventory and is related to the cycle of agricultural
activities.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f09.png"/>

      </fig>

      <p id="d1e5282">Prior uncertainty assumes values around 0.4–0.6 MtC month<inline-formula><mml:math id="M325" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for
CO<inline-formula><mml:math id="M326" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, 5–15 ktC month<inline-formula><mml:math id="M327" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CO, and 15 ktC month<inline-formula><mml:math id="M328" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for
CH<inline-formula><mml:math id="M329" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. For GEE the prior uncertainty is between 0.3 and
46.7 MtC month<inline-formula><mml:math id="M330" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and for respiration it is 5.1–19.0 MtC month<inline-formula><mml:math id="M331" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.
Posterior uncertainty for CO<inline-formula><mml:math id="M332" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> is 0.24–0.38 MtC month<inline-formula><mml:math id="M333" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for fossil
fuel emissions, 0.3–9.9 MtC month<inline-formula><mml:math id="M334" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for GEE, and 3.1–10.4 MtC month<inline-formula><mml:math id="M335" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for respiration, while it has a range of
3.3–4.7 for CO and 2.7–7.0 ktC month<inline-formula><mml:math id="M336" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for CH<inline-formula><mml:math id="M337" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. Mean
uncertainty reduction of the monthly values is 38 % for fossil fuel
emissions of CO<inline-formula><mml:math id="M338" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, 41 % for GEE, and roughly 45 % for respiration,
63 % for CO, and about 67 % for CH<inline-formula><mml:math id="M339" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. It is worth pointing out that
such values are higher than the mean uncertainty reduction in the scaling
factors (23 %); this happens because the most representative emission
sectors are those influencing the observations the most and thus are also
the most constrained.</p>
      <p id="d1e5449">In addition, note that in this case, the posterior uncertainties for single-
and multi-species inversions are similar for the modelled species, with the
exception of the CO<inline-formula><mml:math id="M340" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> anthropogenic contributions. To generalize this
last result, we tested the benefit of a multi-species inversion for the
different cases of prior uncertainty values shown in Table 3. As an
indicator for the benefit of including correlation between different
species, we use the ratio between posterior uncertainty of the multi-species
inversion and the posterior uncertainty of the corresponding single-species
inversion. A value of 1 means that there is no benefit from adding an
inter-species correlation to the inversion, while values greater than 1
mean that a multi-species inversion is even less constrained than a
single-species one. We expect this indicator to be less than 1, meaning
that inter-species correlations actually improve the constraint power of the
inversion. As before, we consider here the uncertainties of the retrieved
budgets for the 50 % footprint, where the surface influence is strongest
(Fig. 1). Values of this uncertainty ratio for the different trace gases as
function of month are shown in Fig. 10 for the different cases listed in
Table 3. The benefit of including inter-species<?pagebreak page9237?> correlations shown in Fig. 10 does not depend on different manifestations of the true fluxes, but only
on the posterior uncertainty of the multi- and single-species inversions.</p>
      <p id="d1e5461">All of the species experience a reduction in the posterior uncertainty ratio
due to the addition of inter-species correlation; said reduction is up to
20 % for fossil fuel CO<inline-formula><mml:math id="M341" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and up to 10 % for the other species; in
addition, anthropogenic CO<inline-formula><mml:math id="M342" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> is more sensitive to the prior relative
error values than CO and CH<inline-formula><mml:math id="M343" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. As the uncertainty of GEE and respiration
is not modified, they show little to no variation for different cases (Fig. 10).
There is a dependence of the benefit of the multi-species inversion over the
single-species inversion on the prior uncertainty values (differences
between Cases 1–3), with the largest difference for fossil fuel emissions of
CO<inline-formula><mml:math id="M344" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>. Interestingly for Case 2 with reduced prior uncertainty for fossil
fuel CO<inline-formula><mml:math id="M345" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions the benefit nearly doubles over the default case
(Case 1). Also reducing the prior uncertainties of CO and CH<inline-formula><mml:math id="M346" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> emissions
(Case 3) more or less compensates for this increase in benefit. The reason
for both of these results is probably to be found in Eq. (8). In fact,
changing the prior uncertainty in CO<inline-formula><mml:math id="M347" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions means to also change
the off-diagonal blocks linking the different species together. However, by
reducing the anthropogenic CO<inline-formula><mml:math id="M348" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> uncertainty from 20 to 10 % (Case
2), the diagonal block for CO<inline-formula><mml:math id="M349" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> in the prior uncertainty changes by a
factor of 4, while the off-diagonal blocks change only by a factor of 2.
This effectively ties the emissions of CO<inline-formula><mml:math id="M350" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> tighter to the emissions of
the other species, resulting in greater benefit from a multi-species inversion over a
single-species inversion. Conversely, when all prior uncertainties are
reduced by a factor of 2 (Case 3), both diagonal and off-diagonal blocks are
reduced by a factor of 4. This explains why Case 1 and Case 3 show similar
benefit values. Note that the assumed prior uncertainties for the default
case (Case 1) are quite conservative; therefore lower uncertainties were
chosen for Cases 2 and 3. While the absolute benefit of adding inter-species
correlation is not a game-changer, it is worth pointing out that such
improvement also comes with only slightly greater computational effort than
multiple independent single-species inversions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10"><caption><p id="d1e5557">Benefit of a multi-species inversion over the corresponding
single-species inversion (dotted line) per different species per months of
the year. The benefit has been tested for the three different cases of
Table 3. Note that CO<inline-formula><mml:math id="M351" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> refers to fossil fuel emissions only, and RESP
and GEE refers to the biospheric fluxes. Note that “unc.” stands for uncertainty.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f10.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11"><caption><p id="d1e5577">Benefit of a multi-species inversion over the corresponding
single-species inversion (dotted line) per different species and month. The
benefit has been tested for a “normal” inversion featuring both prior and
model–data mismatch (mdm) correlation between different species (black) or only
one of these two components (red and orange). Results refer to Case 1 of
Table 3 (black line of Fig. 10). Values derived from Palmer et al. (2006) for
the month of March are indicated with a diamond. Note that “unc.” stands for uncertainty.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/9225/2018/acp-18-9225-2018-f11.png"/>

      </fig>

      <p id="d1e5587">In order to assess the contribution of inter-species correlation in the prior
uncertainty vs. that of model–data mismatch uncertainty, Fig. 11 also shows
the resulting posterior uncertainty ratios for Case 1 (Table 3) from
inversions only using prior or model–data mismatch correlation. For the
anthropogenic component of CO<inline-formula><mml:math id="M352" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, the greatest constraint is given by the
prior correlation, while for GEE, respiration, and CH<inline-formula><mml:math id="M353" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> the strongest
contribution is from the model–data mismatch correlation. In the case of CO,
the inter-species correlations for different components are dominant for
different months of the year. What makes CO sensitive to<?pagebreak page9238?> different
correlation structures during different seasons is CO enhancement showing a
stronger seasonal cycle compared to, for example, the fossil fuel component
of the CO<inline-formula><mml:math id="M354" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> enhancement, with average values of around 150 ppb (25 ppm
for CO<inline-formula><mml:math id="M355" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for January and around 9 ppb (4 ppm for CO<inline-formula><mml:math id="M356" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> for July.
This results in a much weaker constraint on the CO emissions from the CO
observations during summer, but there is still some constraint through the
other species such as CO<inline-formula><mml:math id="M357" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> via the a priori correlation in the emissions.</p>
      <p id="d1e5651">Palmer et al. (2006; in the following referred to as P06) studied the importance
of inter-species correlation to improve inverse analysis using airborne data
from the TRACE-P mission conducted in March/April 2001 over the western
region of the Pacific Ocean. P06 derived a prior error correlation lower
than 0.2 by analysing the uncertainty of emission factors from an
Asia-specific emission inventory (Streets, 2003), which is significantly
smaller than the correlation of 0.7 assumed in the present study. P06 deemed
CO<inline-formula><mml:math id="M358" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>–CO prior correlation greater than 0.5 to be unrealistic for the
emissions in Asia, which is mostly associated with the uncertainty in
emission factors for CO of 67 % for fossil fuel emissions and 240 % for
biofuel emissions in China (P06 Table 1). However, for the European region
used in the present paper we argue that values around 0.7 are appropriate.
The resulting uncertainty in the CO<inline-formula><mml:math id="M359" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>–CO ratio, diagnosed from the prior
error covariance matrix used in this study, is about 50 % for both biofuel
and fossil fuel emissions in Europe, which we regard as reasonable. To
compare results from P06 with those from the present study, ratios of
posterior uncertainties resulting from inversions using correlations between
CO<inline-formula><mml:math id="M360" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO of 0.7 in the prior uncertainties and to those using no
correlations have been extracted from Fig. 7 in P06 and are also shown as
orange diamonds in Fig. 11. It is easy to see that for anthropogenic
CO<inline-formula><mml:math id="M361" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, the value derived from P06 is higher than in our study, while the
two values are very similar for CO. Similarly, posterior uncertainty ratios
using model–data mismatch correlations of 0.7 between CO<inline-formula><mml:math id="M362" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and CO are
derived from Fig. 8 of P06 and are shown as red diamonds. In this case, the
value derived from P06 is slightly lower than in our study for anthropogenic
CO<inline-formula><mml:math id="M363" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, while the two are again very similar for CO.</p>
      <p id="d1e5709">From this comparison we can see that the estimates of the benefit of
including inter-species correlation in atmospheric inversions in P06 and in
this paper are of the same order of magnitude for anthropogenic CO<inline-formula><mml:math id="M364" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and
almost identical for CO, suggesting a general continuity of results.</p>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e5728">The present paper presents a synthetic experiment aiming to evaluate the
effects of exploiting correlations between different trace gases in an
atmospheric inversion. We quantitatively described the capability of the
modelling framework to reproduce observations, the performance of the
inversion scheme in reducing the uncertainty of the different trace gases,
and the benefits of multi-species inversions compared to corresponding
single-species inversions. We also describe a method to re-scale different
prior uncertainty covariance matrices so that the corresponding posterior
uncertainties are actually comparable.</p>
      <p id="d1e5731">Where possible, we compared model outputs with available observations.
Such comparison, possible only for CO, showed a good degree of agreement
between the model and observations with an overall correlation of roughly
0.75; modelled values for CO enhancement underestimate the observed ones by a
factor of roughly 2.8, compatible with what was found in Boschetti (2015).
It is found that posterior uncertainty is much lower than the prior for all
of the five simulated species. The mean uncertainty reduction for CO<inline-formula><mml:math id="M365" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
emissions from fossil fuels is roughly 38 %, for GEE it is around
41 %,
while for respiration it is roughly 44 %. For CO and CH<inline-formula><mml:math id="M366" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> the
uncertainty reduction is about 63 and 67 % respectively. Finally, we
described quantitatively the benefit of using multi-species inversions by
exploiting correlations in different chemical species. It is found that
considering correlations between different trace gases can reduce the
posterior uncertainty by up to about 20 % for monthly fluxes.<?pagebreak page9239?> These
benefits are however dependent on the error structure of the prior
uncertainty.</p>
      <p id="d1e5752">The present paper paves the way for future studies using simultaneous
measurements of different trace gases. This will be especially important in
the context of the upcoming routine measurements of CO<inline-formula><mml:math id="M367" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, CO, and
CH<inline-formula><mml:math id="M368" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> vertical profiles within IAGOS. As IAGOS makes use of commercial
airliners, such profiles will be collected in the vicinity of major
international airports, and hence in the vicinity of major metropolitan
areas, where many different human activities take place simultaneously. In
such a context, any improvement in the constraint of atmospheric inversions
will be particularly useful. A possible improvement in this analysis would
be to evaluate the effects of different correlation factors specific to
different pairs of anthropogenic species, fuels, and emission sectors.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p id="d1e5777">IAGOS and MOZAIC data for carbon monixide mole fraction
measurements are available at the IAGOS data base under
<uri>http://iagos.sedoo.fr/portal.html</uri> (last access: 14 November 2016).</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e5786">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e5792">The research leading to these results was supported by the European
Community's Seventh Framework Programme ([FP7/2007-2013]) under grant
agreement no. 312311 (IGAS).</p><p id="d1e5794">The authors acknowledge the strong support of the European Commission,
Airbus, and the airlines (Lufthansa, Air France, Austrian, Air Namibia,
Cathay Pacific, Iberia, and China Airlines so far) who carry the MOZAIC or
IAGOS equipment and have performed maintenance since 1994. In its last 10 years
of operations, MOZAIC has been funded by INSU-CNRS (France),
Météo-France, Université Paul Sabatier (Toulouse, France), and
Forschungszentrum Jülich (FZJ, Jülich, Germany).
IAGOS has been additionally funded by the EU projects IAGOS-DS and IAGOS-ERI. The MOZAIC–IAGOS database is supports by Aeris (CNES AND INSU-CNRS).<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Martyn Chipperfield<?xmltex \hack{\newline}?>
Reviewed by: three anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Multi-species inversion and IAGOS airborne data for a better constraint of continental-scale fluxes</article-title-html>
<abstract-html><p>Airborne measurements of CO<sub>2</sub>, CO, and CH<sub>4</sub>
proposed in the context of IAGOS (In-service Aircraft for a Global Observing
System) will provide profiles from take-off and landing of airliners in the
vicinity of major metropolitan areas useful for constraining sources and
sinks. A proposed improvement of the top-down method to constrain sources
and sinks is the use of a multispecies inversion. Different species such as
CO<sub>2</sub> and CO have partially overlapping emission patterns for given
fuel-combustion-related sectors, and thus share part of the uncertainties
related both to the a priori knowledge of emissions and to model–data
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Lagrangian particle dispersion model STILT (Stochastic Time-Inverted
Lagrangian Transport) combined with the high-resolution (10 km  ×  10 km)
EDGARv4.3 (Emission Database for Global Atmospheric Research) emission
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and CH<sub>4</sub>, and combined with the VPRM (Vegetation Photosynthesis and
Respiration Model) for biospheric fluxes of CO<sub>2</sub>. Applying the modelling
framework to synthetic IAGOS profile observations, we evaluate the benefits
of using correlations between different species' uncertainties on the
performance of the atmospheric inversion. The available IAGOS CO
observations are used to validate the modelling framework. Prior uncertainty
values are conservatively assumed to be 20 %, for CO<sub>2</sub> and 50 % for
CO and CH<sub>4</sub>, while those for GEE (gross ecosystem exchange) and
respiration are derived from existing literature. Uncertainty reduction for
different species is evaluated in a domain encircling 50 % of the profile
observations' surface influence over Europe. We found that our modelling
framework reproduces the CO observations with an average correlation of
0.56, but simulates lower mixing ratios by a factor of 2.8, reflecting a low
bias in the emission inventory. Mean uncertainty reduction achieved for
CO<sub>2</sub> fossil fuel emissions is roughly 38 %; for photosynthesis and
respiration flux it is 41 and 44 % respectively. For CO and CH<sub>4</sub>
the uncertainty reduction is roughly 63 and 67 % respectively.
Considering correlation between different species, posterior uncertainty can
be reduced by up to 23 %; such a reduction depends on the assumed error
structure of the prior and on the considered time frame. The study suggests a
significant uncertainty constraint on regional emissions using multi-species
inversions of IAGOS in situ observations.</p></abstract-html>
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