<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0"><?xmltex \makeatother\@nolinetrue\makeatletter?>
  <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-20-11747-2020</article-id><title-group><article-title>Sources and sinks driving sulfuric acid concentrations in contrasting environments: implications on proxy calculations</article-title><alt-title>Sources and sinks of atmospheric sulfuric acid</alt-title>
      </title-group><?xmltex \runningtitle{Sources and sinks of atmospheric sulfuric acid}?><?xmltex \runningauthor{L.~Dada~et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Dada</surname><given-names>Lubna</given-names></name>
          <email>lubna.dada@helsinki.fi</email>
        <ext-link>https://orcid.org/0000-0003-1105-9043</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff3">
          <name><surname>Ylivinkka</surname><given-names>Ilona</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5591-4876</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Baalbaki</surname><given-names>Rima</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4480-2107</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Li</surname><given-names>Chang</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Guo</surname><given-names>Yishuo</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Yan</surname><given-names>Chao</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5735-9597</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Yao</surname><given-names>Lei</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2680-1629</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Sarnela</surname><given-names>Nina</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1874-3235</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Jokinen</surname><given-names>Tuija</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1280-1396</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Daellenbach</surname><given-names>Kaspar R.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1246-6396</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Yin</surname><given-names>Rujing</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5776-3592</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Deng</surname><given-names>Chenjuan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Chu</surname><given-names>Biwu</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7548-5669</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff5">
          <name><surname>Nieminen</surname><given-names>Tuomo</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2713-715X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Wang</surname><given-names>Yonghong</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2498-9143</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Lin</surname><given-names>Zhuohui</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Thakur</surname><given-names>Roseline C.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3238-4171</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Kontkanen</surname><given-names>Jenni</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-5373-3537</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Stolzenburg</surname><given-names>Dominik</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1014-1360</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Sipilä</surname><given-names>Mikko</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff6 aff7">
          <name><surname>Hussein</surname><given-names>Tareq</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Paasonen</surname><given-names>Pauli</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4625-9590</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Bianchi</surname><given-names>Federico</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2996-3604</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Salma</surname><given-names>Imre</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8319-1647</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9">
          <name><surname>Weidinger</surname><given-names>Tamás</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7500-6579</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff10">
          <name><surname>Pikridas</surname><given-names>Michael</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8131-2369</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff10">
          <name><surname>Sciare</surname><given-names>Jean</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Jiang</surname><given-names>Jingkun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Liu</surname><given-names>Yongchun</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6758-2151</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Petäjä</surname><given-names>Tuukka</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1881-9044</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Kerminen</surname><given-names>Veli-Matti</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0706-669X</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Kulmala</surname><given-names>Markku</given-names></name>
          <email>markku.kulmala@helsinki.fi</email>
        <ext-link>https://orcid.org/0000-0003-3464-7825</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Aerosol and Haze Laboratory, Beijing Advanced Innovation Center for Soft Matter Science and Engineering, <?xmltex \hack{\break}?>Beijing University of Chemical Technology, 100029 Beijing, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Institute for Atmospheric and Earth System Research INAR/Physics, Faculty of Science, University of Helsinki, <?xmltex \hack{\break}?>00014 Helsinki, Finland</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>SMEAR II station, University of Helsinki, 35500 Korkeakoski, Finland</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>State Key Joint Laboratory of Environment Simulation and Pollution Control, School of Environment, <?xmltex \hack{\break}?>Tsinghua University, 100084 Beijing, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Institute for Atmospheric and Earth System Research INAR/Forest Sciences, Faculty of Agriculture and Forestry, <?xmltex \hack{\break}?>University of Helsinki, 00014, Helsinki, Finland</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Department of Physics, The University of Jordan, Amman 11942, Jordan</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Department Material Analysis and Indoor Chemistry, Fraunhofer WKI, 38108 Braunschweig, Germany</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>Institute of Chemistry, Eötvös University, P.O. Box 32, 1518 Budapest, Hungary</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>Department of Meteorology, Eötvös University, P.O. Box 32, 1518 Budapest, Hungary</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>The Cyprus Institute, Climate &amp; Atmosphere Research Centre (CARE-C), <?xmltex \hack{\break}?>20 Konstantinou Kavafi Street, 2121 Nicosia, Cyprus</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Lubna Dada (lubna.dada@helsinki.fi) and Markku Kulmala (markku.kulmala@helsinki.fi)</corresp></author-notes><pub-date><day>19</day><month>October</month><year>2020</year></pub-date>
      
      <volume>20</volume>
      <issue>20</issue>
      <fpage>11747</fpage><lpage>11766</lpage>
      <history>
        <date date-type="received"><day>18</day><month>February</month><year>2020</year></date>
           <date date-type="accepted"><day>25</day><month>August</month><year>2020</year></date>
           <date date-type="rev-recd"><day>15</day><month>July</month><year>2020</year></date>
           <date date-type="rev-request"><day>10</day><month>March</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2020 </copyright-statement>
        <copyright-year>2020</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e439">Sulfuric acid has been shown to be a key driver for new particle formation and subsequent growth in various environments, mainly due to its low
volatility. However, direct measurements of gas-phase sulfuric acid are oftentimes not available, and the current sulfuric acid proxies cannot
predict, for example, its nighttime concentrations or result in significant discrepancies with measured values. Here, we define the sources and sinks
of sulfuric acid in different environments and derive a new physical proxy for sulfuric acid to be utilized in locations and during periods when
it is not measured. We used <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measurements from four different locations: Hyytiälä, Finland; Agia Marina, Cyprus; Budapest,
Hungary; and Beijing, China, representing semi-pristine boreal forest, rural environment in the Mediterranean area, urban environment and heavily
polluted megacity, respectively. The new proxy takes into account the formation of sulfuric acid from <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> via OH oxidation and other
oxidation pathways, specifically via stabilized Criegee intermediates. The sulfuric acid sinks included in the proxy are its condensation
sink (CS) and atmospheric clustering starting from <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> dimer formation. Indeed, we found that the observed sulfuric acid
concentration can be explained by the proposed sources and sinks with similar coefficients in the four contrasting environments where we have tested
it. Thus, the new proxy is a more flexible and an important improvement over previous proxies. Following the recommendations in this paper, a
proxy for a specific location can be derived.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<?pagebreak page11748?><sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e494">Atmospheric new particle formation (NPF) events and their subsequent growth have been observed as taking place almost everywhere in the world (Kulmala
et al., 2004; Kerminen et al., 2018). Many of these observations are based on continuous measurements, and some include more than a year of measurement
data (Nieminen et al., 2018). The importance of NPF events on the global aerosol budget and cloud condensation nuclei formation has been well
established (Spracklen et al., 2008, 2010; Merikanto et al., 2009; Kerminen et al., 2012; Gordon et al., 2017). Recently, the contribution of NPF to
haze formation, which was still controversial, is being investigated in an increasing number of studies from Chinese megacities (Guo et al., 2014; Kulmala et al., 2020).</p>
      <p id="d1e497">Sulfuric acid (<inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), which has a very low saturation vapor pressure and strong hydrogen bonding capability (Zhang et al., 2011), has
been found to be the major precursor of atmospheric NPF (Weber et al., 1996; Kulmala et al., 2004; Sihto et al., 2006; Sipilä et al., 2010; Erupe
et al., 2011; Lehtipalo et al., 2018; Ma et al., 2019) and is often used in global models for simulating the occurrence and intensity of new particle
formation events (Dunne et al., 2016). However, atmospheric measurements of gas-phase sulfuric acid are rare, mainly due to its low concentration
(10<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:math></inline-formula>–10<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">7</mml:mn></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">molecules</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> or below) that can only be measured using state-of-the-art instruments (Mikkonen et al., 2011), such as
the chemical ionization atmospheric-pressure interface time-of-flight spectrometer (CI-APi-ToF) (Eisele and Tanner, 1993; Jokinen et al.,
2012). Therefore, a physically and chemically sound proxy is needed to estimate <inline-formula><mml:math id="M8" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations in various environments where NPF
events are observed, but <inline-formula><mml:math id="M9" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations are not continuously measured.</p>
      <p id="d1e584">Due to its important participation in clustering and thus in the NPF process, several studies have tried to produce proxies for <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in
order to fill gaps in data. For example, Petäjä et al. (2009) developed an approximation of gas-phase <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in
Hyytiälä, southern Finland, using its source from reactions between <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and OH radicals and its loss by condensation onto
preexisting particles (condensation sink, CS). Later, Mikkonen et al. (2011) developed <inline-formula><mml:math id="M13" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> proxies based on measurements at six urban,
rural and forest areas in European and North American sites. Proxies developed by Mikkonen et al. (2011) suggested that the sulfuric acid
concentration depends mostly on the available radiation and <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration, with little influence by CS. However, Lu et al. (2019), who
developed a daytime proxy based on measurements in Beijing, China, suggested the need for taking the CS into account when approximating gaseous
<inline-formula><mml:math id="M15" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, especially in areas where the condensational sink can be relatively high. The proxy developed by Lu et al. (2019) takes into
consideration the formation pathways of <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> via OH radicals from both the conventional photolysis of <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and from the
photolysis of HONO, as well as the loss of <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> via CS. Besides the previously developed proxies, an additional proxy is still needed
for representing nighttime periods that were not considered previously.</p>
      <p id="d1e717">Here, we derive a new proxy that takes into account the production of gaseous sulfuric acid from <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> with oxidation by OH and stabilized
Criegee intermediates (Mauldin et al., 2012) reactions, and its losses onto preexisting aerosol particles (condensation sink) and due to molecular
cluster formation. In order to evaluate our hypothesized sources and sinks and derive the proxy equations, we utilize measurements from four different
locations: (1) Hyytiälä, Finland; (2) Agia Marina, Cyprus; (3) Budapest, Hungary; and (4) Beijing, China, representing a semi-pristine boreal
forest environment, rural environment in the Mediterranean area, urban environment, and heavily polluted megacity, respectively. To evaluate the
predictive power of the derived proxies, the equations are further tested on independent data sets. We compare the coefficients of production
and losses in each environment in order to understand the prevailing mechanism of the <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget in each of the studied
environments. As a result of this investigation, a well-defined sulfuric acid concentration can be derived for multiple areas around the world and
even extended during times when it was not measured (gap filling, forecast, prediction, estimation, etc.).</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Measurement locations, observations and instrumentation</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Locations</title>
<sec id="Ch1.S2.SS1.SSS1">
  <label>2.1.1</label><?xmltex \opttitle{Semi-pristine boreal forest environment: Hyyti\"{a}l\"{a}, Finland}?><title>Semi-pristine boreal forest environment: Hyytiälä, Finland</title>
      <p id="d1e770">Measurements were conducted at the SMEAR II-station (Station for Measuring Ecosystem–Atmosphere Relations), located in Hyytiälä
(61.1<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 24.17<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 181 <inline-formula><mml:math id="M23" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>; Hari and Kulmala, 2005), southern Finland. Here we used measurements from 18 August 2016
to 5 June 2017 and from 8 March 2018 to 28 February 2019. The data from 2016, 2018 and 2019 were used as a training data set for developing the proxy
equation, while the data from 2017 were used for testing the predictive power of the developed proxy. A summary for all locations and the instrumentation used
is given in Tables S1 (training data sets) and S2 (testing data sets) in the Supplement.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS2">
  <label>2.1.2</label><title>Rural background site: Agia Marina, Cyprus</title>
      <p id="d1e820">Measurements were conducted at the Cyprus Atmospheric Observatory (CAO) (35.03<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 33.05<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 532 <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>), a rural
background site located close to Agia Marina Xyliatou village, between 22 February and 3 March 2018. For more details, see, e.g., Pikridas
et al. (2018). The data set from this location is used solely as a training data set.</p>
</sec>
<?pagebreak page11749?><sec id="Ch1.S2.SS1.SSS3">
  <label>2.1.3</label><title>Semi-urban site: Helsinki, Finland</title>
      <p id="d1e870">Measurements were conducted at the SMEAR III-station, located in Helsinki (60.20<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 24.96<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 25 <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>). For more
details about the location see, e.g., Hussein et al. (2008). Here, we measured from 1 to 16 July 2019 as a testing data set.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS4">
  <label>2.1.4</label><title>Urban location: Budapest, Hungary</title>
      <p id="d1e920">The measurements took place at the Budapest platform for Aerosol Research Training (BpART) Research Laboratory (47.47<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 19.06<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E;
115 <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>) of the Eötvös University situated on the bank of the Danube between 21 March and 17 April 2018. The site represents a
well-mixed average atmosphere of the city center (Salma et al., 2016a). The data set from this location is used solely as a training data set.</p>
</sec>
<sec id="Ch1.S2.SS1.SSS5">
  <label>2.1.5</label><title>Polluted megacity: Beijing, China</title>
      <p id="d1e971">Here, observations performed at the west campus of Beijing University of Chemical Technology (39.94<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 116.30<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) between 15 March
and 15 June 2019 were used as a training data set, while observations from 8 September to 15 October 2019 were used as a testing data
set. The sampling took place from outside the window on the fifth floor of a university building adjacent to a busy street. For more details, see, e.g., Lu et al. (2019) and Zhou et al. (2020).</p>
</sec>
<sec id="Ch1.S2.SS1.SSS6">
  <label>2.1.6</label><title>Near an oil refinery in an industrial area: Kilpilahti, Finland</title>
      <p id="d1e1000">The measurement took place at Nyby measurement station (60.31<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 25.50<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) between 7 and 29 June 2012. The site is within
1.5 <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> of the Neste Oyj oil refinery and Kilpilahti industrial area. For more information on the site, please see Sarnela et al. (2015). The
data set from this location is used solely as a testing data set.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Instrumentation</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Trace gases</title>
      <p id="d1e1045">A summary for all locations and instrumentation is given in Tables S1 and S2. Measurements of different variables within the same location are
performed at the same platform unless specified otherwise. In all locations, the sulfuric acid concentrations were measured using a Chemical
ionization atmospheric pressure interface time-of-flight spectrometer (CI-APi-ToF) (Eisele and Tanner, 1993; Jokinen et al., 2012) with
<inline-formula><mml:math id="M38" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> as a reagent ion and analyzed using a tofTools package based on MATLAB software (Junninen et al., 2010). In all locations, the
CI-APi-ToF instruments were calibrated in a similar way prior to the campaign using the method presented by Kurten et al. (2012) to ensure the results
from different sites are comparable. In Hyytiälä, the sulfuric acid concentrations were measured at the tower 35 <inline-formula><mml:math id="M39" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">g</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula> In
Helsinki, the sulfuric acid concentrations were measured from the fourth-floor window (<inline-formula><mml:math id="M40" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 12 <inline-formula><mml:math id="M41" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">g</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>) of the university building
adjacent (<inline-formula><mml:math id="M42" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 200 <inline-formula><mml:math id="M43" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) to the SMEAR III station.</p>
      <p id="d1e1126">In Hyytiälä and Beijing, the <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M45" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations were
measured using an <inline-formula><mml:math id="M46" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> analyzer (Model 43i, Thermo, USA) with a detection limit of 0.1 <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">ppbv</mml:mi></mml:mrow></mml:math></inline-formula> and a <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> analyzer (Model 49i,
Thermo, USA), respectively. In Hyytiälä, the trace gas concentrations were measured at the tower 16.8 <inline-formula><mml:math id="M49" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">g</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula> In Agia Marina, <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is monitored using Ecotech Instrument (9850). In Helsinki, the
<inline-formula><mml:math id="M51" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations were monitored at a 32 <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> tower at the SMEAR III station using UV fluorescence (Horiba APSA 360). Concentrations of <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in Budapest were
measured by UV fluorescence (Ysselbach 43C) with a time resolution of 1 <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:math></inline-formula> at a station of the National Air Quality Network located
1.7 <inline-formula><mml:math id="M55" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> in the upwind-prevailing direction from the BpART site. It was shown earlier that the hourly average <inline-formula><mml:math id="M56" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations (see
Fig. S1 in the Supplement) in central Budapest are ordinarily distributed without large spatial gradients (Salma and Németh, 2019; Mikkonen
et al., 2020). In Kilpilahti, <inline-formula><mml:math id="M57" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations were measured using a Thermo Scientific™ Model 43i <inline-formula><mml:math id="M58" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> Analyzer at
Neste Oil refinery. Trace gases measured during the short campaign periods in Agia Marina and Budapest are representative of yearly concentrations in
respective locations when compared to longer-term measurements at the same site (Salma et al., 2016b; Baalbaki, 2020; Mikkonen et al., 2020).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Particle number size distribution</title>
      <p id="d1e1302">The condensation sink (CS) was calculated using the method proposed by Kulmala et al. (2012) from number size distribution measurements. In
Hyytiälä, the particle number size distribution was measured using a twin differential mobility particle sizer (DMPS) (Aalto et al., 2001). In
Agia Marina, the particle number size distribution between 2 and 800 <inline-formula><mml:math id="M59" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula> was reconstructed from two instruments: an Airel NAIS (Neutral cluster
and Air Ion Spectrometer, 2–20 <inline-formula><mml:math id="M60" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula>) and TSI SMPS (Scanning Mobility Particle Sizer, 20–800 <inline-formula><mml:math id="M61" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula>). In Helsinki, a twin-DMPS system
(diameter 3–950 <inline-formula><mml:math id="M62" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula>) was used to monitor the particle number size distribution. In Budapest, the particle number size distribution was
measured by a flow-switching type DMPS in a diameter range from 6 to 1000 <inline-formula><mml:math id="M63" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula> in the dry state of particles (RH <inline-formula><mml:math id="M64" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 30 %) in 30 channels
with a time resolution of 8 <inline-formula><mml:math id="M65" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">min</mml:mi></mml:mrow></mml:math></inline-formula> (Salma et al., 2016a). In Beijing, the particle number size distribution between 3 and 850 <inline-formula><mml:math id="M66" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula> was
measured using a Particle Size Distribution System (PSD, Liu et al., 2016). Condensation sink obtained at Kilpilahti was acquired from particle number
size distribution measured using a DMPS (6–1000 <inline-formula><mml:math id="M67" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula>). Despite having a diurnal cycle, condensation sink values obtained during the short
campaign periods in Agia Marina and Budapest are representative of yearly concentrations in those respective locations<?pagebreak page11750?> when compared to longer-term
measurements at the same site (Salma et al., 2016b; Baalbaki, 2020).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Radiation</title>
      <p id="d1e1385">In Hyytiälä, Global radiation (GlobRad) was measured using a SK08 solar pyranometer until 24 August 2017 and after that using a EQ08-S solar
pyranometer. The measurements were relocated from 18 m height to 37 m height on 14 February 2017. Global Radiation from the Agia Marina is monitored
using a weather station (Campbell Scientific Europe). In Helsinki, the global radiation is measured using Kipp and Zonen CNR1 at 31 <inline-formula><mml:math id="M68" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">g</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula>
in the SMEAR III station. In Budapest, global radiation was measured by an SMP3 pyranometer (Kipp and Zonen, the Netherlands) on the roof of the
building complex with a time resolution of 1 <inline-formula><mml:math id="M69" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">min</mml:mi></mml:mrow></mml:math></inline-formula>. Its operation was checked by comparing the measured data with those obtained from regular
radiation measurements performed by a CMP11 pyranometer (Kipp and Zonen, the Netherlands) at the Hungarian Meteorological Service (HMS) at a distance
of 10 <inline-formula><mml:math id="M70" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>. The annual mean GlobRad ratio and SD of the 1 h values for the BpART and HMS stations were 1.03 <inline-formula><mml:math id="M71" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.23 for
GlobRad <inline-formula><mml:math id="M72" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 100 <inline-formula><mml:math id="M73" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, which changed to 1.01 <inline-formula><mml:math id="M74" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.05 when considering clear sky conditions. In Beijing, GlobRad intensity from 285
to 2800 <inline-formula><mml:math id="M75" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula> was measured at the rooftop of the five-floor building using a CMP11 pyranometer (Kipp and Zonen, Delft, the Netherlands). The
radiometer was maintained weekly to ensure the orientation was horizontal and clean. In order to do the fitting for the nighttime data, zero values were
replaced by the detection limit of the instrument, assumed to be half the minimum measured radiation. In Kilpilahti, no global radiation measurements
were available, so we relied on radiation data measured at the SMEAR III station, which is around 32 <inline-formula><mml:math id="M76" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> from the measurement site.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS4">
  <label>2.2.4</label><title>Alkenes</title>
      <p id="d1e1488">Volatile organic compounds (VOCs) were measured with a proton transfer reaction quadrupole mass spectrometer (PTR-MS, Ionicon Analytik GmbH) in
Hyytiälä. Ambient mixing ratios are measured every third hour from several different measurement heights. In this study, we use monoterpene
concentration from 16.8 <inline-formula><mml:math id="M77" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> height. The instrument is calibrated regularly with standard gas (Apel-Riemer Environmental, Inc.) (Taipale et al.,
2008). The same instrumentation was used to measure monoterpene concentrations in Kilpilahti every 1 h.</p>
      <p id="d1e1499">In Beijing, VOCs were measured using single-photon ionization time-of-flight mass spectrometer (SPI-MS 3000R, Hexin Mass Spectrometry) with unit mass
resolution (UMR) (Gao et al., 2013). The alkenes included here are butylene, butadiene, isoprene, pentene and
hexene. As the instrument cannot distinguish conformers, the pentene and hexene could also be cyclopentene and cyclohexene. Correlation coefficients
between the different variables used in our study (training data sets) in all four locations are shown in Figs. S2–S6 in the Supplement.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS5">
  <label>2.2.5</label><title>Meteorological parameters</title>
      <p id="d1e1511">Temperature (<inline-formula><mml:math id="M78" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>) and relative humidity (RH) in Hyytiälä were measured at 16.8 <inline-formula><mml:math id="M79" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> using four-wire PT-100 sensors and relative humidity
sensors (Rotronic Hygromet MP102H with Hygroclip HC2-S3, Rotronic AG, Bassersdorf, Switzerland), respectively. In Agia Marina, <inline-formula><mml:math id="M80" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> and RH were
measured using a weather station (Campbell Scientific Europe). <inline-formula><mml:math id="M81" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> and RH were measured at the Physicum rooftop 26 <inline-formula><mml:math id="M82" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">a</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">g</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">l</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></inline-formula> and 220 <inline-formula><mml:math id="M83" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>
northeast from SMEAR III using a Pentronics PT100 sensor and Vaisala HMP243 transmitter, respectively. In Budapest, <inline-formula><mml:math id="M84" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> and RH were measured using temperature probe and a Vaisala HMP45D humidity transmitter at the Hungarian Meteorological Service (HMS) within a 10 <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula> radius from the BpArt station. In
Beijing, meteorological parameters are monitored by a Vaisala weather station data acquisition system (AWS310).</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Derivation of the new proxy</title>
      <p id="d1e1598">We applied the following equation to describe the time-evolution of gas-phase sulfuric acid concentration:
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M86" display="block"><mml:mtable rowspacing="0.2ex" class="split" columnspacing="1em" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:mfenced><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced open="[" close="]"><mml:mtext>Alkene</mml:mtext></mml:mfenced><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        Here, <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> represents the
coefficient of <inline-formula><mml:math id="M88" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> production term due to the well-known <inline-formula><mml:math id="M89" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M90" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:math></inline-formula>  reaction (Petäjä
et al., 2009) and <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the coefficient of <inline-formula><mml:math id="M92" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> production via stabilized Criegee intermediates (sCI) produced by the ozonolysis of
alkenes (Mauldin et al., 2012). We use available monoterpene concentration (MT) here as a proxy for alkenes in Hyytiälä as they are the
dominating species in the boreal forest environment (Hakola et al., 2012; Hellén et al., 2018; Rinne et al., 2005). For Beijing, we use urban-dominating aromatic alkenes. As no VOC measurements are performed in either Agia Marina or Budapest, we evaluate the proxy without the stabilized
Criegee intermediates source term. It is important to note here that the coefficient for sCI is a “bulk” term and that it varies from place to place due
to the differences in sCI structures and different production efficiency from different alkene species (Novelli et al., 2017; Sipilä et al.,
2014). The third term in Eq. (1) represents the loss of <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> onto preexisting aerosol particles, known as condensation sink (CS) and is
calculated by multiplying the CS calculated for sulfuric acid with the concentration of sulfuric acid monomer. The fourth term in Eq. (1) is defined
as the square of sulfuric acid concentration multiplied by clustering coefficient <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. The square of sulfuric acid represents the collision of
two sulfuric acid monomers forming a sulfuric acid dimer, which was found to be the first step of atmospheric cluster<?pagebreak page11751?> formation (Yao et al.,
2018). Therefore, this term takes into account the additional loss of <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> due to cluster formation not included in the term containing
CS. This is necessary because CS is only inferred from size distribution measurements at maximum down to 1.5 <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula>, i.e., not containing any
cluster concentrations and hence losses onto these clusters. This term is written in the form of sulfuric acid dimer production, which seems to be
the first step of cluster formation once stabilized by bases (Kulmala et al., 2013; Almeida et al., 2013; Yao et al., 2018).</p>
      <p id="d1e1847">Since measuring the OH concentration is challenging, we first replaced it with the UVB radiation intensity, which has been shown to be a good proxy
for the OH concentration (Berresheim et al., 2002; Lu et al., 2019; Rohrer and Berresheim, 2006). Unfortunately, UVB was not measured in all the field
studies considered here. Alternatively, GlobRad, a commonly measured quantity, tends to correlate well with UVB and can generally replace it, as used
previously by Petäjä et al. (2009). We confirmed the strong correlation between UVB radiation and global radiation in two locations,
Hyytiälä and Beijing (Fig. S7–S8 in the Supplement). Accordingly, the coefficient <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> here replaces the coefficient of <inline-formula><mml:math id="M98" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
production <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> terms (Eq. 2). We proceed here using only GlobRad in the proxy to be consistent with the two other locations where UVB was
not measured (Agia Marina and Budapest).
          <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M100" display="block"><mml:mtable class="split" columnspacing="1em" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mtext>GlobRad</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced open="[" close="]"><mml:mtext>Alkene</mml:mtext></mml:mfenced><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        By assuming a steady state between <inline-formula><mml:math id="M101" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> production and loss, the <inline-formula><mml:math id="M102" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration can be solved directly from Eq. (2).
          <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M103" display="block"><mml:mtable rowspacing="0.2ex" class="split" columnspacing="1em" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="[" close="]"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mtext>GlobRad</mml:mtext><mml:mo>+</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced open="[" close="]"><mml:mtext>Alkene</mml:mtext></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:msup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        In order to evaluate the importance of each of the source terms in determining the change in sulfuric acid concentration, we refitted the data after
excluding the stabilized Criegee intermediates source pathway, as shown in Eq. (4).
          <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M104" display="block"><mml:mtable rowspacing="0.2ex" class="split" columnspacing="1em" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mtext>GlobRad</mml:mtext><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        In order to evaluate the importance of each of the sink terms in determining the sulfuric acid concentration, we refitted the data after excluding
the loss of sulfuric acid via the cluster formation pathway using Eq. (5).
          <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M105" display="block"><mml:mtable class="split" columnspacing="1em" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mtext>GlobRad</mml:mtext><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced close="]" open="["><mml:mtext>Alkene</mml:mtext></mml:mfenced><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        We also refitted the data using the simple proxy proposed by Petäjä et al. (2009), by excluding the formation of sulfuric acid via stabilized
Criegee intermediates source pathway and loss of sulfuric acid via the cluster formation pathway using Eq. (6).
          <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M106" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mtext>GlobRad</mml:mtext><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>
        We then evaluated our new proposed proxy by comparing it to the
original Petäjä et al. (2009) proxy using Eq. (7) and to Mikkonen et al. (2011) using Eq. (8) below (which corresponds to Eq. 11 in Mikkonen et al., 2011). The calculation of the scaled reaction constant <inline-formula><mml:math id="M107" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> used in Eq. (8) is given in Sect. 1 in the Supplement.

              <disp-formula specific-use="align" content-type="numbered"><mml:math id="M108" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mo>[</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mn mathvariant="normal">1.4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup><mml:mo>⋅</mml:mo><mml:msup><mml:mtext>GlobRad</mml:mtext><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>[</mml:mo><mml:mtext>GlobRad</mml:mtext><mml:mo>]</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E7"><mml:mtd><mml:mtext>7</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mo>=</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mn mathvariant="normal">8.21</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mi>k</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mtext>GlobRad</mml:mtext><mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">0.62</mml:mn></mml:msup></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E8"><mml:mtd><mml:mtext>8</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></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:mtext>CS</mml:mtext><mml:mo>⋅</mml:mo><mml:mtext>RH</mml:mtext></mml:mrow></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.13</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

          The equations derived for each of the sites can be found in Table 1. The fitting coefficients were obtained by minimizing the sum of the squared
logarithm of the ratio between the proxy values and measured sulfuric acid concentration using the method described by Lagarias et al. (1998), a
built-in function <italic>fminsearch</italic> of MATLAB, giving the optimal values for the coefficients. The data were subject to 10 000 bootstrap resamples
when getting each of the <inline-formula><mml:math id="M109" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> values as a measure of accuracy in terms of bias, variance, confidence intervals or prediction error (Efron and
Tibshirani, 1994). We accounted for the systematic uncertainty in <inline-formula><mml:math id="M110" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and predictor variables. For every bootstrap fit, we assumed both
<inline-formula><mml:math id="M111" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and all predictor variables to be affected by independent systematic errors between their lower and upper accuracy limits. More
details on the bootstrap resampling method and uncertainty introduction can be found in the Supplement. The 25th percentile and
75th percentiles of the coefficients are shown for all locations together with the median <inline-formula><mml:math id="M112" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> values in Table 2. The median <inline-formula><mml:math id="M113" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> values from the
bootstrap resamples were used in the equations for deriving sulfuric acid concentrations at each site. Figures S2–S6 present the correlation matrix
between the different variables participating in <inline-formula><mml:math id="M114" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> formation and loss in all locations (training data sets). The goodness of the fit and the
probability of overfitting or under-fitting was evaluated using the Akaike Information Criterion (AIC; Fig. S9 in the Supplement), which<?pagebreak page11752?> also compares the
proxies given in Eqs. (2), (4), (5) and (6). The criterion uses the sample size (number of points), the number of parameters (terms in the equation) and
the sum of the squared estimate of errors (SSE, i.e., deviations predicted from actual empirical values of data) to estimate the quality of each model, relative
to each of the other models, and thus provides means for model selection (McElreath, 2018).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e2667">Equations for sulfuric acid proxy derivation at each of the measurement locations.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.98}[.98]?><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msub><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mtext>boreal</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4.2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4.2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">4.2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">8.6</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>⋅</mml:mo><mml:mtext>GlobRad</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">6.1</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">29</mml:mn></mml:mrow></mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced open="[" close="]"><mml:mtext>Alkene</mml:mtext></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula><?xmltex \hack{\hfill\break}?></oasis:entry>
         <oasis:entry colname="col2">(9)</oasis:entry>
       <?xmltex \interline{[9pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mtext>rural</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="[" close="]"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>(</mml:mo><mml:mn mathvariant="normal">9.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>⋅</mml:mo><mml:mtext>GlobRad</mml:mtext><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula><?xmltex \hack{\hfill\break}?></oasis:entry>
         <oasis:entry colname="col2">(10)</oasis:entry>
       <?xmltex \interline{[9pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mtext>urban</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">9.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">9.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">9.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1.6</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>⋅</mml:mo><mml:mtext>GlobRad</mml:mtext><mml:mo>)</mml:mo></mml:mrow></mml:mfenced><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula><?xmltex \hack{\hfill\break}?></oasis:entry>
         <oasis:entry colname="col2">(11)</oasis:entry>
       <?xmltex \interline{[9pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mtext>megacity</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mtext>CS</mml:mtext><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">7.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mrow><mml:mn mathvariant="normal">2.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup><mml:mo>⋅</mml:mo><mml:mtext>GlobRad</mml:mtext><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">29</mml:mn></mml:mrow></mml:msup><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced close="]" open="["><mml:mtext>Alkene</mml:mtext></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">(12)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e3321">Coefficients used in the proxy equation in all four environments. Numbers in parentheses represent the 25th and 75th percentiles of bootstrapped data (including outliers). See Sect. 2 in the Supplement for more details.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <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:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Location</oasis:entry>
         <oasis:entry colname="col2">GlobRad (<inline-formula><mml:math id="M119" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (10<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M122" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">W</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (10<inline-formula><mml:math id="M124" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">29</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M125" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mn mathvariant="normal">6</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (10<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M128" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Hyytiälä</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M129" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 0</oasis:entry>
         <oasis:entry colname="col3">0.85 (0.60–1.21)</oasis:entry>
         <oasis:entry colname="col4">6.10 (4.27–8.57)</oasis:entry>
         <oasis:entry colname="col5">4.26 (2.98–5.99)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Agia Marina</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M130" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 50</oasis:entry>
         <oasis:entry colname="col3">0.92 (0.64–1.34)</oasis:entry>
         <oasis:entry colname="col4">NA</oasis:entry>
         <oasis:entry colname="col5">2.21 (1.27–3.79)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Budapest</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M131" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 50</oasis:entry>
         <oasis:entry colname="col3">0.16 (0.09–0.27)</oasis:entry>
         <oasis:entry colname="col4">NA</oasis:entry>
         <oasis:entry colname="col5">9.80 (9.79–9.81)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Beijing</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M132" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 0</oasis:entry>
         <oasis:entry colname="col3">1.94 (1.12–3.50)</oasis:entry>
         <oasis:entry colname="col4">1.45 (0.93–2.26)</oasis:entry>
         <oasis:entry colname="col5">7.0</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e3324">NA: not available</p></table-wrap-foot></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e3614">Sulfuric acid proxy concentration as a function of measured sulfuric acid. Observation at SMEAR II station, Hyytiälä, Finland. The observed concentrations from the training data set are measured for 2016–2019 using CI-APi-ToF and are 3 <inline-formula><mml:math id="M133" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:math></inline-formula> medians, resulting in a total of 1860 data points. In <bold>(a)</bold>, the full Eq. (2) is used, in <bold>(b)</bold> the equation without the stabilized Criegee intermediates source (Eq. 4) is used, in <bold>(c)</bold> the equation without the cluster sink term (Eq. 5) is used, and in <bold>(d)</bold> the equation without the stabilized Criegee intermediates source and the cluster sink term (Eq. 6) is used. The “fit” refers to the fitting between the measured and the proxy-calculated sulfuric acid concentration (<inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
        <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f01.png"/>

      </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e3679">The diurnal variation of sulfuric acid proxy concentrations using different fits and observed concentrations at SMEAR II in Hyytiälä, Finland. Median values are shown. Fits 1, 2, 3 and 4 correspond to Eqs. (2) and (4), (5), and (6), respectively. The Petäjä fit shown is applied using the coefficients reported in Petäjä et al. (2009) (Eq. 7). The Mikkonen fit shown is applied using the coefficients reported in Mikkonen et al. (2011) (Eq. 8).</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results and discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><?xmltex \opttitle{The sulfuric acid proxy for Hyyti\"{a}l\"{a} SMEAR~II station}?><title>The sulfuric acid proxy for Hyytiälä SMEAR II station</title>
      <p id="d1e3704">Figure 1a shows the scatterplot between the observed <inline-formula><mml:math id="M135" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations and that derived by the proxy using the full Eq. (2). The
correlation coefficient was 0.84 (1860 data points). The data were related to 3 <inline-formula><mml:math id="M136" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:math></inline-formula> medians, as the monoterpene concentration was measured only
every third hour. In Fig. 1b–d, the proxy is refitted after removing one of the source or sink terms (Eqs. 4–6), in order to evaluate the
sensitivity of the proxy to each of the terms and to show the improvement of the proxy using the additional source and sink (Fig. 1a) in comparison to
the simple proxy that was used by Petäjä et al. (2009) (Fig. 1d). Our results show that the integration of additional terms of
<inline-formula><mml:math id="M137" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> formation (i.e., the stabilized Criegee Intermediates) and loss (atmospheric cluster formation) gives the new proxy the ability to
accurately capture the diurnal variation of the <inline-formula><mml:math id="M138" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration, demonstrating a clear improvement over the earlier physical proxy
(Petäjä et al., 2009).</p>
      <p id="d1e3763">In Fig. 1b, the corresponding data are shown without the alkene term (Eq. 4). The correlation is substantially weaker (0.74) than with the full
equation. Even more importantly, we cannot estimate the contribution of the alkene term to the sulfuric acid concentration (Fig. 2 – Fit 2) as the
fit also results in an unphysical coefficient for cluster formation (Kürten et al., 2015) and the fit fails to capture the diurnal pattern during
dark hours after 16:00 LT (Fig. 2 – Fit 2). When fitting the data without the cluster source term
(Eq. 5), the correlation coefficient is high (Fig. 1c), yet the goodness of the fit is not as good as when the cluster source term is taken into
account (Table S4 in the Supplement – Fig. S9). Furthermore, we derived an additional proxy equation using CS corrected for hygroscopic growth
(Laakso et al., 2004) to be used when calculating a more robust proxy for Hyytiälä. The details, equation and results are shown in Figs. S10–S12 in the Supplement.</p>
      <p id="d1e3766">Note that we opted for deriving a bulk proxy (daytime and nighttime together) instead of two independent proxies, one for daytime and one for
nighttime separately. Our results show that one bulk equation is able to explain the Hyytiälä sulfuric acid daytime and nighttime sources
accurately. Additionally, separating the bulk equation into two distinct equations results in bias towards the pattern of one of the predictor
variables. For instance, the <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> value during daytime follows the cycle of global radiation, while that of <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> follows the cycle of
alkenes. Therefore, in order to accurately reflect the continuum of source and sink terms throughout the day, we decided on the bulk
proxy. Additionally, one bulk equation was able to predict sulfuric acid concentrations during daytime and nighttime with high accuracy (slope of
<inline-formula><mml:math id="M141" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1), as further discussed in Sect. 4.5.</p>
      <p id="d1e3799">The fit was able to reproduce the sulfuric acid concentration in such a clean environment without the cluster term (Fig. 2 – Fit 3), perhaps due to
low concentrations of bases participating in clustering in Hyytiälä (Jen et al., 2014). Finally, the corresponding data without both the
alkene source term and cluster formation source term (Eq. 6, Fig. 1d) shows a weaker correlation between the measured and modeled sulfuric acid
concentration (0.70), but more importantly it deviates far from the <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line during both daytime and nighttime (Fig. 2 – Fit 4). It is important
to note here that when deriving the Petäjä proxy (Petäjä et al. 2009), the model relied on summer data between April and June 2007,
which could explain the misfit with the current data from Hyytiälä that spans the whole year. See also Figs. S13 and S14 in the Supplement
for scatterplots comparing the measured sulfuric acid concentrations of the training data set with Petäjä et al. (2009) and Mikkonen
et al. (2011), respectively. In general, using all four terms in Eq. (2) shows improvement over all other combinations (Eqs. 4–6), not only in terms of
correlation coefficients and accurate diurnal cycle between measured and calculated concentrations of sulfuric acid as shown in Figs. 1 and 2 but
also by showing a better goodness of the fit as shown in Table S4 and Fig. S9 when using the AIC statistical method. The final equation for the boreal
forest environment can be found in Table 1, Eq. (9).</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Sulfuric acid proxy at a rural site: Agia Marina, Cyprus</title>
      <p id="d1e3822">Since there were no direct measurements of alkenes in Agia Marina, we had to exclude the formation of <inline-formula><mml:math id="M143" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the oxidation by sCI from
the proxy, and therefore we derived only the daytime <inline-formula><mml:math id="M144" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> proxy concentration. The correlation between the measured and proxy
concentration of <inline-formula><mml:math id="M145" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> was 0.88 (96 data points), which shows that the chosen predictors were able to largely explain the measured sulfuric acid
concentration (Fig. 3). However, the slope deviates from the 1-to-1 line, which could be attributed to the additional formation mechanisms that
we could not include with the current data. However, the addition of the cluster loss mechanism shows a noticeable improvement over the simple proxy
in Fig. 3b (<inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.80</mml:mn></mml:mrow></mml:math></inline-formula>). The cluster loss term starts to become more important in this rural environment in comparison to the boreal forest, which could
be due to a higher concentration of stabilizing bases in Agia Marina compared with Hyytiälä. Although both fits of Eqs. (4) and (6) show
similar diurnal patterns (Fig. 4, Fits 2 and 4), the loss term due to <inline-formula><mml:math id="M147" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> cluster formation improved the precision of the new<?pagebreak page11753?> proxy
(Fig. 3). According to the statistical AIC method, the goodness of the fit improved from 70 to 33, with and without the clustering term, as shown in Fig. S9. Also, even without the alkene term, the newly derived coefficients improved the proxy in comparison to
Petäjä et al. (2009) and Mikkonen et al. (2011), as shown in Figs. 4, S13 and S14. The final equation for the rural site can be found in
Table 1, Eq. (10).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e3903">Sulfuric acid proxy concentration as a function of measured sulfuric acid. Observation at Agia Marina, Cyprus, excluding the alkene term. The observed numbers concentrations are measured during February–March 2018 using CI-APi-ToF and are hourly medians resulting in a total of 96 data points. Sulfuric acid proxy concentration as a function of measured sulfuric acid. In <bold>(a)</bold>, the equation without the stabilized Criegee intermediates source (Eq. 4) is used, and in <bold>(b)</bold> the equation with neither the stabilized Criegee intermediates source nor the cluster sink term (Eq. 6) is used. The “fit” refers to the fitting between the measured and the proxy-calculated sulfuric acid concentration (<inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e3953">The diurnal variation of sulfuric acid proxies and observed concentrations in Agia Marina, Cyprus. Hourly median values are shown. Fits 2 and 4 correspond to Eqs. (4) and (6), respectively (see also Fig. 3a and b, respectively). The Petäjä fit shown is applied using the coefficients reported in Petäjä et al. (2009) (Eq. 7). The Mikkonen fit shown is applied using the coefficients reported in Mikkonen et al. (2011) (Eq. 8).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f04.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>Proxy for urban environment: Budapest, Hungary</title>
      <p id="d1e3970">Next we try to understand the mechanisms of sulfuric acid formation and losses in an even more complex environment, i.e., urban Budapest (Figs. 5
and 6). Since there were no direct measurements of alkenes there or of its proxies, such as monoterpenes, or anthropogenic volatile organic
compounds, we derived the sulfuric acid proxy excluding the formation due to stabilized Criegee intermediates pathway, as in Eq. (4). In comparison to
the simple proxy (Fig. 5b; <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.49</mml:mn></mml:mrow></mml:math></inline-formula>; 263 data points), the correlation between the measured and proxy concentration of <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> improved
with the addition of the loss term due to cluster formation, <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.59</mml:mn></mml:mrow></mml:math></inline-formula> (Fig. 5a). The correlation between measured and modeled values of sulfuric
acid became weaker in Budapest in comparison to Hyytiälä and Agia Marina, which could be attributed to a more complex environment, and
additional pathways of sulfuric acid formation and losses. Additionally, we observed a sudden <inline-formula><mml:math id="M152" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration change in the middle of the
campaign, possibly due to sudden change in local meteorology and air mass transport, which could also explain the weaker correlation (See Fig. S1). The
loss term due to <inline-formula><mml:math id="M153" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> dimerization improved the precision of the new proxy in comparison to the simple model, as well as the
Petäjä et al. (2009) or the Mikkonen et al. (2011) derivation, as shown in Figs. 6, S13 and S14. We think that the overestimation in the
Petäjä proxy is because of its dependence on the <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mtext>CS</mml:mtext></mml:mrow></mml:math></inline-formula> ratio. The proxy is originally derived in Hyytiälä, and when
we apply the same coefficients to Budapest it gives a higher estimated concentration when compared to the measured one since the <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mtext>CS</mml:mtext></mml:mrow></mml:math></inline-formula> ratio is
smaller in Budapest (Fig. 9). Although the proxy developed by Mikkonen et al. (2011) has been shown to work in varying environments, it clearly
overestimates the sulfuric acid concentration in Budapest for perhaps the same reasons (its dependence on the <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mtext>CS</mml:mtext></mml:mrow></mml:math></inline-formula> ratio). It is
also visible from Figs. 5 and 6 that the addition of the dimerization term was capable of better capturing the lower <inline-formula><mml:math id="M157" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
concentrations in comparison to fitting the data without the dimerization term. In comparison to both Hyytiälä and Agia Marina, the
coefficient associated with dimerization in Budapest is slightly higher, which can be attributed to the availability of a possibly facilitated
clustering due to higher abundance of stabilizing bases such as amines and ammonia (discussed in Sect. 4.6). The final equation for the urban
environment can be found in Table 1, Eq. (11).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e4107">Sulfuric acid proxy as a function of measured sulfuric acid at Budapest station, excluding the alkene term. The observed numbers are measured during spring 2018 using CI-APi-ToF and are 1 h medians coinciding with the measurement of trace gases and global radiation every hour resulting in a total of 263 data points. In <bold>(a)</bold>, the equation without the stabilized Criegee Intermediates source (Eq. 4) was used, and in <bold>(b)</bold> the equation with neither the stabilized Criegee intermediates source nor the cluster sink term (Eq. 6) was used. The “fit” refers to the fitting between the measured and the proxy-calculated sulfuric acid concentration (<inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f05.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e4157">The diurnal variation of sulfuric acid proxies and measured concentrations in Budapest. Hourly median values are shown. Fits 2 and 4 correspond to Eqs. (4) and (6), respectively. The Petäjä fit shown is applied using the coefficients reported in Petäjä et al. (2009) (Eq. 7). The Mikkonen fit shown is applied using the coefficients reported in Mikkonen et al. (2011) (Eq. 8).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f06.png"/>

        </fig>

</sec>
<sec id="Ch1.S4.SS4">
  <label>4.4</label><title>Proxy for megacity: Beijing, China</title>
      <p id="d1e4174">In megacities, in our case Beijing, the sulfuric acid concentration is particularly high during nighttime, which confirms the need for determining
the contribution of sources other than OH (radiation) to its formation. Our observations<?pagebreak page11754?> emphasize the contribution of the alkene pathway, as without
considering this route we would not replicate morning hours correctly. During daytime, there is enhanced dimerization and cluster formation due to the
abundance of stabilizing bases (Yao et al., 2018). We assessed the derivation of the proxy equation first using daytime data and nighttime data
separately and found that such a separation results in an unphysical <inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> value since clustering in Beijing happens mostly during daytime (Zhou
et al., 2020). This obstacle was also observed when deriving a bulk equation. To overcome it, we set an upper limit for the <inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> value at
7 <inline-formula><mml:math id="M161" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M162" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> obtained from the fitting of daytime data (GlobRad <inline-formula><mml:math id="M163" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 50 <inline-formula><mml:math id="M164" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>). The reason for such an observation is that, in
such a complex environment, sulfuric acid might originate from sources other than the ones we accounted for in our calculation, especially during
nighttime, e.g., through the hydrolysis of <inline-formula><mml:math id="M165" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> formed from non-photochemical processes (Yao et al., 2020). The alkenes or volatile organic compounds during daytime are different from those during nighttime and might vary between seasons, which
could be attributed to a different fleet composition during those times or the biogenic activity (Yang et al., 2019). However, the derived Eq. (12)
(derived from spring data) is able to predict the daytime and nighttime sulfuric acid concentrations during summer and autumn (See more in
Sect. 4.5).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><label>Figure 7</label><caption><p id="d1e4253"><bold>(a)</bold> Sulfuric acid proxy concentration as a function of measured sulfuric acid. Observation at Beijing, China. The observed concentrations of the training data set were measured in 2019 using CI-APi-ToF and are 1 h medians, resulting in a total of 877 data points. In <bold>(a)</bold>, the full Eq. (2) is used, in <bold>(b)</bold> the equation without the stabilized Criegee intermediates source (Eq. 4) is used, in <bold>(c)</bold> the equation without the cluster sink term (Eq. 5) is used, and in <bold>(d)</bold> the equation without the stabilized Criegee intermediates source or the cluster sink term (Eq. 6) was used. Coefficients shown on top of the subplots relate to the daytime values. The “fit” refers to the fitting between the measured and the proxy-calculated sulfuric acid concentration (<inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f07.png"/>

        </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F8"><?xmltex \currentcnt{8}?><label>Figure 8</label><caption><p id="d1e4311">The diurnal variation of sulfuric acid proxy concentrations using different fits and observed concentrations at Beijing, China. Median values are shown. Fits 1, 2, 3 and 4 correspond to Eqs. (2) and (4), (5), and (6), respectively. The Petäjä fit shown is applied using the coefficients reported in Petäjä et al. (2009) (Eq. 7). The Mikkonen fit shown is applied using the coefficients reported in Mikkonen et al. (2011) (Eq. 8).</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f08.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><label>Figure 9</label><caption><p id="d1e4323">Characteristic predictor variables and <inline-formula><mml:math id="M167" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations in different environments. <inline-formula><mml:math id="M168" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and alkene data are available from the boreal forest (Hyytiälä) and megacity (Beijing) environments. This figure could be used in order to choose the equation and coefficients for calculating sulfuric acid proxy at a new location. The alkenes in the boreal environment are monoterpenes (e.g., alpha-pinene) and in the megacity are anthropogenic volatile organic compounds (butylene, butadiene, isoprene, pentene and hexene). The concentrations are displayed as violin plots, which are a combination of boxplot and a kernel distribution function on each side of the boxplots. The white circles define the median of the distribution and the edges on the inner grey boxes refer to the 25th and 75th percentiles, respectively. Whole day data are shown for Hyytiälä and Beijing, while daytime data are shown (GlobRad <inline-formula><mml:math id="M169" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 50 <inline-formula><mml:math id="M170" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) for Agia Marina and Budapest. Daytime data (GlobRad <inline-formula><mml:math id="M171" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 50 <inline-formula><mml:math id="M172" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>) are shown in Fig. S15 in the Supplement. The correlations between the different variables at each site are shown in Figs. S2–S6.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f09.png"/>

        </fig>

      <?pagebreak page11755?><p id="d1e4402">In Fig. 7, we see an improvement of the new proxy (Eq. 2) in comparison to the simple proxy (Eq. 6) derived by Petäjä et al. (2009) as the
former takes into the account the additional sources and sinks of <inline-formula><mml:math id="M173" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> that were not considered in previous works (see also
Fig. S9). Introducing the alkene production term improved the accuracy of the <inline-formula><mml:math id="M174" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration during both daytime and nighttime
(Figs. 7 and 8), which supports our assumption that <inline-formula><mml:math id="M175" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> formation during nighttime is driven by stabilized Criegee intermediates. In
Fig. 7b we show the proxy without the alkene term is unable to capture the nighttime concentrations. In Fig. 8, we see the importance of all sources
and sinks predicted for sulfuric acid, as Fit 1 (Eq. 2) best predicts the measured sulfuric acid concentration. Additionally, according to the
statistical AIC method, using the full equation has the least probability of inaccuracy and error in estimating the sulfuric acid concentration
(Fig. S9). Moreover, it is clear that the addition of the cluster sink term in the megacity environment is required due to its large contribution as a
sink for <inline-formula><mml:math id="M176" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, especially due to higher concentrations of stabilizing molecules; the cluster mode (sub-3 <inline-formula><mml:math id="M177" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">nm</mml:mi></mml:mrow></mml:math></inline-formula>) particle
concentration is the highest in Chinese megacities (Zhou et al., 2020). The final equation for the megacity can be found in Table 1, Eq. (12).</p>
</sec>
<sec id="Ch1.S4.SS5">
  <label>4.5</label><title>Predictive power of proxy equations</title>
      <p id="d1e4486">Each of the proxies of the boreal forest environment, the rural background and the megacity were tested for predictive power on independent data sets using
extended data sets from the same location or using measurements from locations with similar characteristics. The sulfuric acid concentrations at each
of these locations is modeled using the equation (with median <inline-formula><mml:math id="M178" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> per source/sink term) relevant to the site and compared to the measured
concentrations. The derivation of the sulfuric acid concentrations using 10 000 combinations of <inline-formula><mml:math id="M179" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> values, as well as the error in the predictions,
are shown in the Supplement. Note that the testing data sets are not subject to any bootstrap resampling or uncertainty additions but
are instead used as is for testing the predictive power of the suggested proxy.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><label>Figure 10</label><caption><p id="d1e4505">Sulfuric acid concentrations modeled as a function of measured sulfuric acid using testing data sets. The colored data points refer to the modeled (predicted) concentrations, and the dashed blue line refers to the fit (<inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>⋅</mml:mo><mml:mtext>log</mml:mtext><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>b</mml:mi></mml:mrow></mml:math></inline-formula>) of the aforementioned data points. The black squares are the median modeled concentrations in logarithmically spaced measured sulfuric acid bins, and their lower and upper whiskers correspond to 25th and 75th percentiles of the predicted concentrations. <bold>(a)</bold> Hyytiälä SMEAR II station: the concentrations shown are 3 <inline-formula><mml:math id="M181" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">h</mml:mi></mml:mrow></mml:math></inline-formula> medians coinciding with the alkene measurements every 3 h, resulting in a total of 257 data points. The modeled concentrations are derived using Eq. (9). <bold>(b)</bold> Helsinki SMEAR III station: the concentrations shown are 1 h medians, resulting in a total of 416 data points. The modeled concentrations are derived using Eq. (10). <bold>(c)</bold> Beijing: the concentrations shown are 1 h medians resulting in a total of 268 data points. The modeled concentrations are derived using Eq. (12). <bold>(d)</bold> Kilpilahti: the concentrations shown are 1 h medians resulting in 114 data points. The modeled concentrations are derived using Eq. (9).</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f10.png"/>

        </fig>

<sec id="Ch1.S4.SS5.SSS1">
  <label>4.5.1</label><?xmltex \opttitle{Boreal forest environment: Hyyti\"{a}l\"{a}}?><title>Boreal forest environment: Hyytiälä</title>
      <p id="d1e4576">For testing the predictive power of the boreal forest proxy (Eq. 9), we use an independent testing data set from the same location measured from
1 January to 5 June 2017. Results show that the modeled sulfuric acid concentrations correlate well (<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>) with the measured sulfuric
concentrations, with a slope of 0.997 for the testing data set (Figs. 10a and<?pagebreak page11756?> S16 in the Supplement). Moreover, we tested the four fits on the testing
data set, i.e., the full Eq. (2), the equation without the stabilized Criegee intermediates source (Eq. 4), the equation without the cluster sink term
(Eq. 5), and the equation with neither the stabilized Criegee intermediates source nor the cluster sink term (Eq. 6), and found that Fit 1 (Eq. 4)
best defines the measured sulfuric acid concentration in comparison to the rest of the equations (Fig. S17 in the Supplement). The diurnal cycle is
also accurately described by Eq. (4), which captures both nighttime and daytime values (Fig. S18 in the Supplement).</p>
</sec>
<sec id="Ch1.S4.SS5.SSS2">
  <label>4.5.2</label><title>Semi-urban location: Helsinki</title>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><label>Figure 11</label><caption><p id="d1e4602">Fraction contribution of each source and sink term to the change in <inline-formula><mml:math id="M183" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration. Figure 11 is complementary to Table 3. The boreal, rural, urban and megacity labels refer to the Hyytiälä, Agia Marina, Budapest and Beijing sites, respectively. Note that the fraction of the alkene term contribution is not zero for the rural or urban sites but is due to unavailable alkene data from these sites. In <bold>(a)</bold> we show all day medians for Hyytiälä and Beijing, and in <bold>(b)</bold> we show daytime medians for all sites.</p></caption>
            <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f11.png"/>

          </fig>

      <p id="d1e4633">For testing the predictive power of the rural background site proxy (Eq. 10), we use an independent testing data set from a semi-urban location in
Helsinki, Finland, measured from 1 to 16 July 2019 during daytime (GlobRad <inline-formula><mml:math id="M184" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 50 <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>). The rural background site Eq. (10) is used as
the condensation sink, and <inline-formula><mml:math id="M186" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations in the testing location are within the interquartile span of the Agia Marina measurements
(Fig. 9, Table S3 in the Supplement). Results show that although the modeled sulfuric acid concentrations do not correlate as well as in other
locations (<inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.44</mml:mn></mml:mrow></mml:math></inline-formula>), the bias could be attributed to the missing source (alkene) in the original equation (Fig. 10b). Indeed, looking at the binned
data, we find that at within each concentration bin the modeled sulfuric acid concentrations tend to span the <inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line. Actually, the discrepancy between
the measured and the modeled concentration is smaller than the model prediction error (Fig. S19 in the Supplement). Note that the model prediction
error is estimated as the interquartile range of the modeled <inline-formula><mml:math id="M189" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration of a single point in time arising from the uncertainty
in <inline-formula><mml:math id="M190" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> values. For the rural background site, we also found that the diurnal cycle is better described when introducing the additional clustering sink
term (Fig. S20 in the Supplement).</p>
</sec>
<sec id="Ch1.S4.SS5.SSS3">
  <label>4.5.3</label><title>Megacity: Beijing</title>
      <p id="d1e4724">For testing the predictive power of the megacity proxy (Eq. 12), we use an independent testing data set from the same location (Beijing) measured from
1 September to 15 October 2019. Results show that the modeled sulfuric acid concentrations correlate well (<inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.83</mml:mn></mml:mrow></mml:math></inline-formula>) with the measured
sulfuric concentrations, with a slope of <inline-formula><mml:math id="M192" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1.1 for the testing data set (Fig. 10c). Also for this site, we tested the four fits on the testing
data set, i.e., the full Eq. (2), the equation without the stabilized Criegee intermediates source (Eq. 4), the equation without the cluster sink term
(Eq. 5), and the equation with neither the stabilized Criegee intermediates source nor the cluster sink term (Eq. 6), and found that Fit 1 (Eq. 4)
best defines the measured sulfuric acid concentration in comparison to the rest of the equations (Fig. S22 in the Supplement).<?pagebreak page11757?> The diurnal cycle is
also described by Eq. (4), which captures both nighttime and daytime (Fig. S23 in the Supplement).</p>
</sec>
<sec id="Ch1.S4.SS5.SSS4">
  <label>4.5.4</label><title>Industrial area: Kilpilahti</title>
      <p id="d1e4754">Finally, we tested the predictive power of our developed proxy on a data set measured at an industrial area in close proximity to an oil
refinery. Interestingly, the median CS at the location lies within the interquartile range of the CS measured in Hyytiälä and that measured in
Agia Marina (Table S3, Fig. 9). The <inline-formula><mml:math id="M193" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations at the measurement site are higher than in both Hyytiälä and Agia Marina but are
smaller than the ones reported in Budapest. Additionally, we observed alkene concentrations at Kilpilahti that are within the range of those
monitored in Hyytiälä attributed to the green belt in the area (Sarnela et al., 2015). Accordingly, we test the proxy Eq. (9) on the
Kilpilahti data set. Our results show that Eq. (9) is able to predict the sulfuric acid concentrations in Kilpilahti with a high correlation
coefficient (<inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.74</mml:mn></mml:mrow></mml:math></inline-formula>) (Fig. 10d). Similar to other locations, the Fit 1 (Eq. 4) best describes the sources and sinks at the location (Fig. S25). The
discrepancy between the measured and the modeled concentration is smaller than the model prediction error for less than 50 % of the data points
only (Fig. S24 in the Supplement). This observation is consistent with the diurnal cycle (Fig. S26 in the Supplement). During certain<?pagebreak page11758?> mornings
(04:00–08:00 LT), when the measured sulfuric concentrations are particularly high, the model was unable to predict the concentrations
accurately. These high concentrations were attributed to air masses coming from the oil refinery (Sarnela et al., 2015). Indeed, our proxy was not
able to explain these morning peaks using biogenic alkenes, however, in such an industrial area, anthropogenic sources could play a role in
determining the magnitude of sulfuric acid concentrations. With the condensation sink being rather low (median <inline-formula><mml:math id="M195" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.005 <inline-formula><mml:math id="M196" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), the
impact of direct <inline-formula><mml:math id="M197" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions cannot be ruled out either.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e4820">Fraction of each source and sink term for the change in <inline-formula><mml:math id="M198" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration. Median of bootstrap resampling results and their 25th and 75th percentiles are shown.</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" colsep="1"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right" colsep="1"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">GlobRad (<inline-formula><mml:math id="M199" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry namest="col3" nameend="col4" align="center">Source terms </oasis:entry>
         <oasis:entry namest="col5" nameend="col6" align="center">Sink terms </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> Glob<inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:mi mathvariant="normal">A</mml:mi></mml:mrow></mml:mfenced><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mtext>CS</mml:mtext><mml:mfenced close="]" open="["><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Hyytiälä</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M207" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 0</oasis:entry>
         <oasis:entry colname="col3">0.34</oasis:entry>
         <oasis:entry colname="col4">0.16</oasis:entry>
         <oasis:entry colname="col5">0.16</oasis:entry>
         <oasis:entry colname="col6">0.34</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(0.10–0.44)</oasis:entry>
         <oasis:entry colname="col4">(0.08–0.40)</oasis:entry>
         <oasis:entry colname="col5">(0.08–0.26)</oasis:entry>
         <oasis:entry colname="col6">(0.24–0.42)</oasis:entry>
       <?xmltex \interline{[6pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Agia Marina</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M208" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 50</oasis:entry>
         <oasis:entry colname="col3">0.5</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.24</oasis:entry>
         <oasis:entry colname="col6">0.26</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">(0.19–0.29)</oasis:entry>
         <oasis:entry colname="col6">(0.21–0.31)</oasis:entry>
       <?xmltex \interline{[6pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Budapest</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M209" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 50</oasis:entry>
         <oasis:entry colname="col3">0.5</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.26</oasis:entry>
         <oasis:entry colname="col6">0.24</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">(0.18–0.31)</oasis:entry>
         <oasis:entry colname="col6">(0.19–0.32)</oasis:entry>
       <?xmltex \interline{[6pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Beijing</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M210" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 0</oasis:entry>
         <oasis:entry colname="col3">0.28</oasis:entry>
         <oasis:entry colname="col4">0.22</oasis:entry>
         <oasis:entry colname="col5">0.29</oasis:entry>
         <oasis:entry colname="col6">0.21</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(2 <inline-formula><mml:math id="M211" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msup></mml:math></inline-formula>–0.41)</oasis:entry>
         <oasis:entry colname="col4">(0.09 – 0.50)</oasis:entry>
         <oasis:entry colname="col5">(0.19 – 0.39)</oasis:entry>
         <oasis:entry colname="col6">(0.11 – 0.31)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><label>Figure 12</label><caption><p id="d1e5225"><bold>(a)</bold> Monthly variation of each source and sink term fraction contribution to the change in <inline-formula><mml:math id="M213" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in Hyytiälä within the training data set 2016–2019. <bold>(b)</bold> Monthly variation of each source and sink term to the change in <inline-formula><mml:math id="M214" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in Beijing within the training and testing data sets in 2019; the data outside the training and testing data sets have missing measured sulfuric acid concentrations, thus proxy concentrations were used in obtaining this figure. <bold>(c)</bold> Diurnal variation of each source and sink term to the change in <inline-formula><mml:math id="M215" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in Hyytiälä within the training data set. <bold>(d)</bold> Diurnal variation of each source and sink term to the change in <inline-formula><mml:math id="M216" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration in Beijing within the training and testing data sets.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/11747/2020/acp-20-11747-2020-f12.png"/>

          </fig>

</sec>
</sec>
<?pagebreak page11759?><sec id="Ch1.S4.SS6">
  <label>4.6</label><?xmltex \opttitle{Sensitivity of the proxy to the {$\protect\chem{H_{{2}}SO_{{4}}}$} sources and sinks}?><title>Sensitivity of the proxy to the <inline-formula><mml:math id="M217" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sources and sinks</title>
      <p id="d1e5336">The variations of coefficients related to Eq. (3) can be used to get insights into the general chemical behavior under current atmospheric conditions,
as well as into the mechanisms of sulfuric acid formation and losses in various environments. The contribution of different terms in different
locations seem to vary significantly. The new loss term taking into account clustering starting from dimer formation needs to be taken into account in
all the environments in daytime. On the other hand, without alkene term it is in practice impossible to get nighttime concentrations correct.</p>
      <p id="d1e5339"><?xmltex \hack{\newpage}?>In Table 2, we have presented the fitted coefficients (Eq. 3) for all our sites, whereas the contributions of the different terms in the balance
equation are given during daytime in Fig. 11 and Table 3. The contribution of the various source and sink terms to the change of <inline-formula><mml:math id="M218" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
concentrations are determined using Eq. (2). The median-derived <inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> values, together with the measured <inline-formula><mml:math id="M222" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,
CS, trace gases and GlobRad per site, were used to calculate each of the terms. Source term 1 refers to <inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M224" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> GlobRad <inline-formula><mml:math id="M225" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> [<inline-formula><mml:math id="M226" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>], source
term 2 refers to <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M228" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> [O<inline-formula><mml:math id="M229" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>] <inline-formula><mml:math id="M230" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> [Alkene] <inline-formula><mml:math id="M231" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> [<inline-formula><mml:math id="M232" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>], sink term 3 refers to <inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M234" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> [<inline-formula><mml:math id="M235" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>]<inline-formula><mml:math id="M236" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> and sink term 4 refers
to CS <inline-formula><mml:math id="M237" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> [<inline-formula><mml:math id="M238" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>]. The contribution of each term is then calculated as the median or percentiles of the normalized term to the sum of all
terms. The variability of the coefficients (Ta<?pagebreak page11760?>ble 2), as well as the relative contributions of each term to the change in sulfuric acid concentration
(Table 3), could give valuable information on the mechanisms resulting in sulfuric acid formation and losses. At steady state (Eq. 2), the sources
and sinks are in balance with each other during both daytime and nighttime, but there were clear differences in the individual contributions. For
instance, a variation in <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> could be due to variations in OH sources and sinks. Although in urban locations OH sinks are expected to be higher
and therefore <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to be lower, additional sources of OH are available in such locations, for example HONO (Zhang et al., 2019). The alkene and Criegee
intermediates terms was found to be an important <inline-formula><mml:math id="M241" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> source (Figs. 1, 2, 7 and 8), as without it we are not able predict night or morning
concentrations of <inline-formula><mml:math id="M242" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> properly. The alkene source term contributed up to almost 100 % of the <inline-formula><mml:math id="M243" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> sources during
nighttime in Beijing and up to 90 % of the sources during nighttime in Hyytiälä (Fig. 12). The Criegee intermediates term showed its
importance mostly when global radiation is low, not only in nighttime but also during winter (Fig. 12) in both Hyytiälä and Beijing. It is
important to note here that Criegee intermediates vary between locations, and they also form in different yield percentages from different alkenes
(Novelli et al., 2017; Sipilä et al., 2014). These stabilized Criegee intermediates also react differently under different environmental
conditions.</p>
      <p id="d1e5636">The CS term had the highest contribution to the total sink in Hyytiälä. Its contribution decreased when moving towards more polluted
environments (Fig. 11) to become regardless of the relatively high condensation sink in Megacities, smaller in Beijing than that of the cluster sink
term (Laakso et al., 2006; Monkkonen et al., 2004, 2005; Yao et al., 2018). This observation might be attributed to decreased effectiveness of
condensation sink in more polluted environments (Kulmala et al., 2017), but also to increased contribution of the clustering sink term in such
environments where the<?pagebreak page11761?> concentration of stabilizing bases is highest, particularly in daytime (Yao et al., 2018; Yan et al., 2018). It should be noted
that measurements of ammonia and similar bases are rare, so their exact contribution is difficult to estimate. The cluster term is found to contribute
most during spring daytime in Hyytiälä (Fig. 12a and c), which is the time window during which clustering and thus new
particle formation events happen (Dada et al., 2017, 2018). The same is observed for Beijing, where the clustering term contributed up to 70 % of
the total sink terms during daytime (Fig. 12d), especially during summer when the CS is lowest (Deng et al., 2020).</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions and recommendations</title>
      <p id="d1e5649">Sulfuric acid is a key gas-phase compound linked to secondary aerosol production in the atmosphere. The concentration of sulfuric acid in the gas
phase is governed by several sources and sinks. In this paper we defined the sources and sinks of <inline-formula><mml:math id="M244" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and derived a physically and
chemically sound proxy for the sulfuric acid concentration using measurements at four different locations, including a boreal forest environment
(Hyytiälä, Finland), a rural Mediterranean site (Agia Marina, Cyprus), an urban area (Budapest, Hungary) and a megacity (Beijing, China). When describing the change in gas-phase sulfuric acid concentration, we took into account two source terms: (1) photochemical oxidation of sulfur dioxide and (2) sulfuric acid
originating from alkene and ozone reactions and the associated stabilized Criegee intermediates pathway. For the sink terms, we considered (3) the loss rate to
the preexisting aerosol described by condensation sink and (4) the loss rate of sulfuric acid monomer due to the clustering process.</p>
      <p id="d1e5668">In general, the variation in the environmental conditions and the difference in concentrations of air pollutants affects the coefficients derived, and
therefore it is important to derive location-specific coefficients. The derived coefficients give insights into the general chemical behavior and into
the mechanisms of sulfuric acid formation and losses in various environments. As there are improvements from previously derived proxies, without the alkene
<inline-formula><mml:math id="M245" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> formation pathway, it is in practice impossible to get nighttime concentrations. On the other hand, the additional loss term taking
into account clustering starting from dimer formation needs to be taken into account in all the environments, especially those<?pagebreak page11762?> with higher cluster
formation probabilities due to availability of stabilizing bases.</p>
      <p id="d1e5687">The coefficients derived do not differ substantially between the different locations. The proxy could therefore be used at locations with no prior
<inline-formula><mml:math id="M246" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measurements, provided that the environmental conditions are approximately similar to those in one of the four sites described
here. More specifically, the proxies could be utilized to derive long-term data sets for <inline-formula><mml:math id="M247" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations, which would be essential
in performing various kinds of trend analyses. In order to derive the long term sulfuric acid concentrations, we recommend deriving in-house
coefficients in cases where sulfuric acid concentrations are directly measured rather than using the ones from already-derived studies. The choice of
equation depends on the availability of the data on site. In cases where alkenes or their proxies are measured and sulfuric acid is measured, derivation of
the coefficients should be based on Eq. (2). In cases where neither alkenes nor their proxies are measured but sulfuric acid is measured, the coefficients
and therefore the proxy for daytime only can be derived using Eq. (4). In cases where sulfuric acid is not measured, one can calculate the sulfuric acid
proxy using Eqs. (2) or (4), depending on whether the alkene data are available or not, respectively, using the coefficients suggested in Table 1
that are relevant to the site of interest. In order to make the best choice for the coefficients, Fig. 9 can be followed in order to decide which
description fits the location of interest best. For example, in cases where the condensation sink is between 2 <inline-formula><mml:math id="M248" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M249" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
6 <inline-formula><mml:math id="M250" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M251" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M252" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and the <inline-formula><mml:math id="M253" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration is lower than 2 <inline-formula><mml:math id="M254" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M255" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">9</mml:mn></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M256" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">molecules</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>,
coefficients of Hyytiälä or the boreal forest are to be used.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e5823">The data used in the paper are available from the first author at
lubna.dada@helsinki.fi. The plug and play MATLAB code used to calculate a location-specific <inline-formula><mml:math id="M257" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> proxy using the coefficients derived in this paper can be found at <ext-link xlink:href="https://doi.org/10.5281/zenodo.4048329" ext-link-type="DOI">10.5281/zenodo.4048329</ext-link> (Dada, 2020).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e5845">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-20-11747-2020-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-20-11747-2020-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e5854">MK came up with the idea. LD, IY, CL and RB analyzed the data. YG, CD, RY, CY, LY, JJ, YL, BC, ZL and YW performed the measurements in
Beijing and preprocessed the raw data. NS, TJ, MS and TP performed the measurements in Hyytiälä and preprocessed the raw data. LD, TN, JK,
KRD, DS, TH, PP, FB, VMK and MK provided useful discussion and ideas. IS, TW, RB and TJ performed the measurements in Budapest and preprocessed the raw
data. MP, JS, RB and TJ performed the measurements in Agia Marina and preprocessed the raw data. RCT, TJ and MS performed the sulfuric acid measurements
in Helsinki and preprocessed the raw data. LD and KRD introduced the error and bootstrap resampling analyses. LD, VMK and MK wrote the
manuscript. All co-authors contributed to reviewing the manuscript and to the discussions related to it.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e5860">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e5866">We thank Veronika Varga and Zoltán Németh of the Eötvös University for their help in the experimental work in
Budapest, Kimmo Neitola and Tiia Laurila for their help at Agia Marina, and Lauriane Quéléver and Tuuli Lehmusjärvi for
their help in setting up the sulfuric acid measurement in Helsinki. This publication has been produced within the framework of the EMME-CARE
project, which has received funding from the European Union's Horizon 2020 Research and Innovation Programme (under grant agreement no. 856612) and
the Government of Cyprus. The sole responsibility of this publication lies with the author. The European Union is not responsible for any use that may
be made of the information contained therein.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e5871">This project has received funding from the National Natural Science Foundation of China (project no. 41877306), the
National Key R&amp;D Program of China (grant no. 2017YFC0209503), and the National Research, Development and Innovation Office, Hungary (grant nos. K116788
and K132254). This research has been supported by the European Research Council under the following programs: ATM-GTP (grant no. 742206), CHAPAs (grant no. 850614), EMME-CARE (grant no. 856612), ACTRIS PPP (grant no. 739530), ACTRIS-2 (grant no. 654109), and GASPARCON (grant no. 714621). It has also been supported by the Academy of Finland (grant nos. 307331, 316114, 311932, and 296628).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e5877">This paper was edited by Kari Lehtinen and reviewed by Santtu Mikkonen and one anonymous referee.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><?label 1?><mixed-citation>Aalto, P., Hameri, K., Becker, E., Weber, R., Salm, J., Makela, J. M., Hoell, C., O'Dowd, C. D., Karlsson, H., Hansson, H. C., Vakeva, M., Koponen, I. K., Buzorius, G., and Kulmala, M.:
Physical characterization of aerosol particles during nucleation events,
Tellus B,
53, 344–358, <ext-link xlink:href="https://doi.org/10.1034/j.1600-0889.2001.530403.x" ext-link-type="DOI">10.1034/j.1600-0889.2001.530403.x</ext-link>, 2001.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><?label 2?><mixed-citation>Almeida, J., Schobesberger, S., Kurten, A., Ortega, I. K., Kupiainen-Maatta, O., Praplan, A. P., Adamov, A., Amorim, A., Bianchi, F., Breitenlechner, M., David, A., Dommen, J., Donahue, N. M., Downard, A., Dunne, E., Duplissy, J., Ehrhart, S., Flagan, R. C., Franchin, A., Guida, R., Hakala, J., Hansel, A., Heinritzi, M., Henschel, H., Jokinen, T., Junninen, H., Kajos, M., Kangasluoma, J., Keskinen, H., Kupc, A., Kurten, T., Kvashin, A. N., Laaksonen, A., Lehtipalo, K., Leiminger, M., Leppa, J., Loukonen, V., Makhmutov, V., Mathot, S., McGrath, M. J., Nieminen, T., Olenius, T., Onnela, A., Petaja, T., Riccobono, F.<?pagebreak page11763?>, Riipinen, I., Rissanen, M., Rondo, L., Ruuskanen, T., Santos, F. D., Sarnela, N., Schallhart, S., Schnitzhofer, R., Seinfeld, J. H., Simon, M., Sipila, M., Stozhkov, Y., Stratmann, F., Tome, A., Trostl, J., Tsagkogeorgas, G., Vaattovaara, P., Viisanen, Y., Virtanen, A., Vrtala, A., Wagner, P. E., Weingartner, E., Wex, H., Williamson, C., Wimmer, D., Ye, P. L., Yli-Juuti, T., Carslaw, K. S., Kulmala, M., Curtius, J., Baltensperger, U., Worsnop, D. R., Vehkamaki, H., and Kirkby, J.:
Molecular understanding of sulphuric acid-amine particle nucleation in the atmosphere,
Nature,
502, 359–363, <ext-link xlink:href="https://doi.org/10.1038/nature12663" ext-link-type="DOI">10.1038/nature12663</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><?label 3?><mixed-citation>
Baalbaki, R., Pikridas M., Jokinen T., Dada L., Ahonen L., Lehtipalo K., Petäjä T., Sciare J., and Kulmala M.:
Towards understanding the mechanisms of new particle formation in the Eastern Mediterranean,
in preparation, 2020.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><?label 4?><mixed-citation>Berresheim, H., Elste, T., Tremmel, H. G., Allen, A. G., Hansson, H. C., Rosman, K., Dal Maso, M., Makela, J. M., Kulmala, M., and O'Dowd, C. D.:
Gas-aerosol relationships of <inline-formula><mml:math id="M258" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M259" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">MSA</mml:mi></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M260" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:math></inline-formula>: Observations in the coastal marine boundary layer at Mace Head, Ireland,
J. Geophys. Res.-Atmos.,
107, 8100, <ext-link xlink:href="https://doi.org/10.1029/2000jd000229" ext-link-type="DOI">10.1029/2000jd000229</ext-link>, 2002.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><?label 1?><mixed-citation>Dada, L.: Sulfuric acid proxy calculation using coefficients derived from four contrasting environments, Zenodo, <ext-link xlink:href="https://doi.org/10.5281/zenodo.4048329" ext-link-type="DOI">10.5281/zenodo.4048329</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><?label 5?><mixed-citation>Dada, L., Paasonen, P., Nieminen, T., Buenrostro Mazon, S., Kontkanen, J., Peräkylä, O., Lehtipalo, K., Hussein, T., Petäjä, T., Kerminen, V.-M., Bäck, J., and Kulmala, M.: Long-term analysis of clear-sky new particle formation events and nonevents in Hyytiälä, Atmos. Chem. Phys., 17, 6227–6241, <ext-link xlink:href="https://doi.org/10.5194/acp-17-6227-2017" ext-link-type="DOI">10.5194/acp-17-6227-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><?label 6?><mixed-citation>Dada, L., Chellapermal, R., Buenrostro Mazon, S., Paasonen, P., Lampilahti, J., Manninen, H. E., Junninen, H., Petäjä, T., Kerminen, V.-M., and Kulmala, M.: Refined classification and characterization of atmospheric new-particle formation events using air ions, Atmos. Chem. Phys., 18, 17883–17893, <ext-link xlink:href="https://doi.org/10.5194/acp-18-17883-2018" ext-link-type="DOI">10.5194/acp-18-17883-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><?label 7?><mixed-citation>Deng, C., Fu, Y., Dada, L., Yan, C., Cai, R., Yang, D., Zhou, Y., Yin, R., Lu, Y., Li, X., Qiao, X., Fan, X., Nie, W., Kontkanen, J., Kangasluoma, J., Chu, B., Ding, A., Kerminen, V.-M., Paasonen, P., Worsnop, D. R., Bianchi, F., Liu, Y., Zheng, J., Wang, L., Kulmala, M., and Jiang, J.:
Seasonal Characteristics of New Particle Formation and Growth in Urban Beijing,
Environ. Sci. Technol., 54, 8547–8557, <ext-link xlink:href="https://doi.org/10.1021/acs.est.0c00808" ext-link-type="DOI">10.1021/acs.est.0c00808</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><?label 8?><mixed-citation>Dunne, E. M., Gordon, H., Kurten, A., Almeida, J., Duplissy, J., Williamson, C., Ortega, I. K., Pringle, K. J., Adamov, A., Baltensperger, U., Barmet, P., Benduhn, F., Bianchi, F., Breitenlechner, M., Clarke, A., Curtius, J., Dommen, J., Donahue, N. M., Ehrhart, S., Flagan, R. C., Franchin, A., Guida, R., Hakala, J., Hansel, A., Heinritzi, M., Jokinen, T., Kangasluoma, J., Kirkby, J., Kulmala, M., Kupc, A., Lawler, M. J., Lehtipalo, K., Makhmutov, V., Mann, G., Mathot, S., Merikanto, J., Miettinen, P., Nenes, A., Onnela, A., Rap, A., Reddington, C. L. S., Riccobono, F., Richards, N. A. D., Rissanen, M. P., Rondo, L., Sarnela, N., Schobesberger, S., Sengupta, K., Simon, M., Sipilaa, M., Smith, J. N., Stozkhov, Y., Tome, A., Trostl, J., Wagner, P. E., Wimmer, D., Winkler, P. M., Worsnop, D. R., and Carslaw, K. S.:
Global atmospheric particle formation from CERN CLOUD measurements,
Science,
354, 1119–1124, <ext-link xlink:href="https://doi.org/10.1126/science.aaf2649" ext-link-type="DOI">10.1126/science.aaf2649</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><?label 9?><mixed-citation>
Efron, B. and Tibshirani, R. J.:
An introduction to the bootstrap,
CRC Press, 29 West 35th Street
New York, NY 10001, USA, 1994.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><?label 10?><mixed-citation>Eisele, F. L. and Tanner, D. J.:
Measurement of the Gas-Phase Concentration of <inline-formula><mml:math id="M261" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and Methane Sulfonic-Acid and Estimates of <inline-formula><mml:math id="M262" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> Production and Loss in the Atmosphere,
J. Geophys. Res.-Atmos.,
98, 9001–9010, <ext-link xlink:href="https://doi.org/10.1029/93jd00031" ext-link-type="DOI">10.1029/93jd00031</ext-link>, 1993.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><?label 11?><mixed-citation>Erupe, M. E., Viggiano, A. A., and Lee, S.-H.: The effect of trimethylamine on atmospheric nucleation involving H2SO4, Atmos. Chem. Phys., 11, 4767–4775, <ext-link xlink:href="https://doi.org/10.5194/acp-11-4767-2011" ext-link-type="DOI">10.5194/acp-11-4767-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><?label 12?><mixed-citation>Gao, W., Tan, G., Hong, Y., Li, M., Nian, H., Guo, C., Huang, Z., Fu, Z., Dong, J., Xu, X., Cheng, P., and Zhou, Z.:
Development of portable single photon ionization time-of-flight mass spectrometer combined with membrane inlet,
Int. J. Mass Spectrom.,
334, 8–12, <ext-link xlink:href="https://doi.org/10.1016/j.ijms.2012.09.003" ext-link-type="DOI">10.1016/j.ijms.2012.09.003</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><?label 13?><mixed-citation>Gordon, H., Kirkby, J., Baltensperger, U., Bianchi, F., Breitenlechner, M., Curtius, J., Dias, A., Dommen, J., Donahue, N. M., Dunne, E. M., Duplissy, J., Ehrhart, S., Flagan, R. C., Frege, C., Fuchs, C., Hansel, A., Hoyle, C. R., Kulmala, M., Kurten, A., Lehtipalo, K., Makhmutov, V., Molteni, U., Rissanen, M. P., Stozkhov, Y., Trostl, J., Tsagkogeorgas, G., Wagner, R., Williamson, C., Wimmer, D., Winkler, P. M., Yan, C., and Carslaw, K. S.:
Causes and importance of new particle formation in the present-day and preindustrial atmospheres,
J. Geophys. Res.-Atmos.,
122, 8739–8760, <ext-link xlink:href="https://doi.org/10.1002/2017jd026844" ext-link-type="DOI">10.1002/2017jd026844</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><?label 14?><mixed-citation>Guo, S., Hu, M., Zamora, M. L., Peng, J., Shang, D., Zheng, J., Du, Z., Wu, Z., Shao, M., Zeng, L., Molina, M. J., and Zhang, R.:
Elucidating severe urban haze formation in China,
P. Natl. Acad. Sci. USA,
111, 17373–17378, <ext-link xlink:href="https://doi.org/10.1073/pnas.1419604111" ext-link-type="DOI">10.1073/pnas.1419604111</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><?label 15?><mixed-citation>Hakola, H., Hellén, H., Hemmilä, M., Rinne, J., and Kulmala, M.: In situ measurements of volatile organic compounds in a boreal forest, Atmos. Chem. Phys., 12, 11665–11678, <ext-link xlink:href="https://doi.org/10.5194/acp-12-11665-2012" ext-link-type="DOI">10.5194/acp-12-11665-2012</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><?label 16?><mixed-citation>
Hari, P. and Kulmala, M.:
Station for measuring ecosystem-atmosphere relations (SMEAR II),
Boreal Environ. Res.,
10, 315–322, 2005.</mixed-citation></ref>
      <ref id="bib1.bib18"><label>18</label><?label 17?><mixed-citation>Hellén, H., Praplan, A. P., Tykkä, T., Ylivinkka, I., Vakkari, V., Bäck, J., Petäjä, T., Kulmala, M., and Hakola, H.: Long-term measurements of volatile organic compounds highlight the importance of sesquiterpenes for the atmospheric chemistry of a boreal forest, Atmos. Chem. Phys., 18, 13839–13863, <ext-link xlink:href="https://doi.org/10.5194/acp-18-13839-2018" ext-link-type="DOI">10.5194/acp-18-13839-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><?label 18?><mixed-citation>
Hussein, T., Martikainen, J., Junninen, H., Sogacheva, L., Wagner, R., Dal Maso, M., Riipinen, I., Aalto, P. P., and Kulmala, M.:
Observation of regional new particle formation in the urban atmosphere,
Tellus B,
60, 509–521, 2008.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><?label 19?><mixed-citation>
Jen, C. N., McMurry, P. H., and Hanson, D. R.:
Stabilization of sulfuric acid dimers by ammonia, methylamine, dimethylamine, and trimethylamine,
J. Geophys. Res.-Atmos.,
119, 7502–7514, 2014.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><?label 20?><mixed-citation>Jokinen, T., Sipilä, M., Junninen, H., Ehn, M., Lönn, G., Hakala, J., Petäjä, T., Mauldin III, R. L., Kulmala, M., and Worsnop, D. R.: Atmospheric sulphuric acid and neutral cluster measurements using CI-APi-TOF, Atmos. Chem. Phys., 12, 4117–4125, <ext-link xlink:href="https://doi.org/10.5194/acp-12-4117-2012" ext-link-type="DOI">10.5194/acp-12-4117-2012</ext-link>, 2012.</mixed-citation></ref>
      <?pagebreak page11764?><ref id="bib1.bib22"><label>22</label><?label 21?><mixed-citation>Junninen, H., Ehn, M., Petäjä, T., Luosujärvi, L., Kotiaho, T., Kostiainen, R., Rohner, U., Gonin, M., Fuhrer, K., Kulmala, M., and Worsnop, D. R.: A high-resolution mass spectrometer to measure atmospheric ion composition, Atmos. Meas. Tech., 3, 1039–1053, <ext-link xlink:href="https://doi.org/10.5194/amt-3-1039-2010" ext-link-type="DOI">10.5194/amt-3-1039-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><?label 22?><mixed-citation>Kerminen, V.-M., Paramonov, M., Anttila, T., Riipinen, I., Fountoukis, C., Korhonen, H., Asmi, E., Laakso, L., Lihavainen, H., Swietlicki, E., Svenningsson, B., Asmi, A., Pandis, S. N., Kulmala, M., and Petäjä, T.: Cloud condensation nuclei production associated with atmospheric nucleation: a synthesis based on existing literature and new results, Atmos. Chem. Phys., 12, 12037–12059, <ext-link xlink:href="https://doi.org/10.5194/acp-12-12037-2012" ext-link-type="DOI">10.5194/acp-12-12037-2012</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><?label 23?><mixed-citation>Kerminen, V.-M., Chen, X., Vakkari, V., Petäjä, T., Kulmala, M., and Bianchi, F.:
Atmospheric new particle formation and growth: review of field observations,
Environ. Res. Lett.,
13, 103003, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/aadf3c" ext-link-type="DOI">10.1088/1748-9326/aadf3c</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><?label 24?><mixed-citation>Kulmala, M., Vehkamäki, H., Petäjä, T., Dal Maso, M., Lauri, A., Kerminen, V.-M., Birmili, W., and McMurry, P. H.:
Formation and growth rates of ultrafine atmospheric particles: a review of observations,
J. Aerosol Sci.,
35, 143–176, <ext-link xlink:href="https://doi.org/10.1016/j.jaerosci.2003.10.003" ext-link-type="DOI">10.1016/j.jaerosci.2003.10.003</ext-link>, 2004.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><?label 25?><mixed-citation>Kulmala, M., Petaja, T., Nieminen, T., Sipila, M., Manninen, H. E., Lehtipalo, K., Dal Maso, M., Aalto, P. P., Junninen, H., Paasonen, P., Riipinen, I., Lehtinen, K. E. J., Laaksonen, A., and Kerminen, V. M.:
Measurement of the nucleation of atmospheric aerosol particles,
Nat. Protoc.,
7, 1651–1667, <ext-link xlink:href="https://doi.org/10.1038/nprot.2012.091" ext-link-type="DOI">10.1038/nprot.2012.091</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><?label 26?><mixed-citation>Kulmala, M., Kontkanen, J., Junninen, H., Lehtipalo, K., Manninen, H. E., Nieminen, T., Petaja, T., Sipila, M., Schobesberger, S., Rantala, P., Franchin, A., Jokinen, T., Jarvinen, E., Aijala, M., Kangasluoma, J., Hakala, J., Aalto, P. P., Paasonen, P., Mikkila, J., Vanhanen, J., Aalto, J., Hakola, H., Makkonen, U., Ruuskanen, T., Mauldin, R. L., Duplissy, J., Vehkamaki, H., Back, J., Kortelainen, A., Riipinen, I., Kurten, T., Johnston, M. V., Smith, J. N., Ehn, M., Mentel, T. F., Lehtinen, K. E. J., Laaksonen, A., Kerminen, V. M., and Worsnop, D. R.:
Direct Observations of Atmospheric Aerosol Nucleation,
Science,
339, 943–946, <ext-link xlink:href="https://doi.org/10.1126/science.1227385" ext-link-type="DOI">10.1126/science.1227385</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><?label 27?><mixed-citation>Kulmala, M., Kerminen, V. M., Petaja, T., Ding, A. J., and Wang, L.:
Atmospheric gas-to-particle conversion: why NPF events are observed in megacities?,
Faraday Discuss.,
200, 271–288, <ext-link xlink:href="https://doi.org/10.1039/c6fd00257a" ext-link-type="DOI">10.1039/c6fd00257a</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><?label 1?><mixed-citation>Kulmala, M., Dada, L., Dällenbach, K., Yan, C., Stolzenburg, D., Kontkanen, J., Ezhova, E., Hakala, S., Tuovinen, S., Kokkonen, T., Kurppa, M., Cai, R., Zhou, Y., Yin, R., Baalbaki, R., Chan, T., Chu, B., Deng, C., Fu, Y., Ge, M., He, H., Heikkinen, L., Junninen, H., Nei, W., Rusanen, A., Vakkari, V., Wang, Y., Wang, L., yao, l., Zheng, J., Kujansuu, J., Kangasluoma, J., Petäjä, T., Paasonen, P., Järvi, L., Worsnop, D., Ding, A., Liu, Y., Jiang, J., Bianchi, F., Yang, G., Liu, Y., Lu, Y., and Kerminen, V.-M.: Is reducing new particle formation a plausible solution to mitigate particulate air pollution in Beijing and other Chinese megacities?, Faraday Discuss., <ext-link xlink:href="https://doi.org/10.1039/D0FD00078G" ext-link-type="DOI">10.1039/D0FD00078G</ext-link>, accepted, 2020.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><?label 28?><mixed-citation>Kurten, A., Rondo, L., Ehrhart, S., and Curtius, J.:
Calibration of a chemical ionization mass spectrometer for the measurement of gaseous sulfuric acid,
Phys. Chem. A,
116, 6375–6386, <ext-link xlink:href="https://doi.org/10.1021/jp212123n" ext-link-type="DOI">10.1021/jp212123n</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib31"><label>31</label><?label 29?><mixed-citation>Kürten, A., Williamson, C., Almeida, J., Kirkby, J., and Curtius, J.: On the derivation of particle nucleation rates from experimental formation rates, Atmos. Chem. Phys., 15, 4063–4075, <ext-link xlink:href="https://doi.org/10.5194/acp-15-4063-2015" ext-link-type="DOI">10.5194/acp-15-4063-2015</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib32"><label>32</label><?label 30?><mixed-citation>Laakso, L., Petäjä, T., Lehtinen, K. E. J., Kulmala, M., Paatero, J., Hőrrak, U., Tammet, H., and Joutsensaari, J.: Ion production rate in a boreal forest based on ion, particle and radiation measurements, Atmos. Chem. Phys., 4, 1933–1943, <ext-link xlink:href="https://doi.org/10.5194/acp-4-1933-2004" ext-link-type="DOI">10.5194/acp-4-1933-2004</ext-link>, 2004.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><?label 31?><mixed-citation>Laakso, L., Koponen, I. K., Monkkonen, P., Kulmala, M., Kerminen, V. M., Wehner, B., Wiedensohler, A., Wu, Z. J., and Hu, M.:
Aerosol particles in the developing world; A comparison between New Delhi in India and Beijing in China,
Water Air Soil Poll.,
173, 5–20, <ext-link xlink:href="https://doi.org/10.1007/s11270-005-9018-5" ext-link-type="DOI">10.1007/s11270-005-9018-5</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib34"><label>34</label><?label 32?><mixed-citation>Lagarias, J. C., Reeds, J. A., Wright, M. H., and Wright, P. E.:
Convergence Properties of the Nelder–Mead Simplex Method in Low Dimensions,
SIAM J. Optimiz.,
9, 112–147, <ext-link xlink:href="https://doi.org/10.1137/s1052623496303470" ext-link-type="DOI">10.1137/s1052623496303470</ext-link>, 1998.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><?label 33?><mixed-citation>Lehtipalo, K., Yan, C., Dada, L., Bianchi, F., Xiao, M., Wagner, R., Stolzenburg, D., Ahonen, L. R., Amorim, A., Baccarini, A., Bauer, P. S., Baumgartner, B., Bergen, A., Bernhammer, A.-K., Breitenlechner, M., Brilke, S., Buchholz, A., Mazon, S. B., Chen, D., Chen, X., Dias, A., Dommen, J., Draper, D. C., Duplissy, J., Ehn, M., Finkenzeller, H., Fischer, L., Frege, C., Fuchs, C., Garmash, O., Gordon, H., Hakala, J., He, X., Heikkinen, L., Heinritzi, M., Helm, J. C., Hofbauer, V., Hoyle, C. R., Jokinen, T., Kangasluoma, J., Kerminen, V.-M., Kim, C., Kirkby, J., Kontkanen, J., Kürten, A., Lawler, M. J., Mai, H., Mathot, S., Mauldin, R. L., Molteni, U., Nichman, L., Nie, W., Nieminen, T., Ojdanic, A., Onnela, A., Passananti, M., Petäjä, T., Piel, F., Pospisilova, V., Quéléver, L. L. J., Rissanen, M. P., Rose, C., Sarnela, N., Schallhart, S., Schuchmann, S., Sengupta, K., Simon, M., Sipilä, M., Tauber, C., Tomé, A., Tröstl, J., Väisänen, O., Vogel, A. L., Volkamer, R., Wagner, A. C., Wang, M., Weitz, L., Wimmer, D., Ye, P., Ylisirniö, A., Zha, Q., Carslaw, K. S., Curtius, J., Donahue, N. M., Flagan, R. C., Hansel, A., Riipinen, I., Virtanen, A., Winkler, P. M., Baltensperger, U., Kulmala, M., and Worsnop, D. R.:
Multicomponent new particle formation from sulfuric acid, ammonia, and biogenic vapors,
Sci. Adv.,
4, eaau5363, <ext-link xlink:href="https://doi.org/10.1126/sciadv.aau5363" ext-link-type="DOI">10.1126/sciadv.aau5363</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><?label 34?><mixed-citation>Liu, J., Jiang, J., Zhang, Q., Deng, J., and Hao, J.:
A spectrometer for measuring particle size distributions in the range of 3 nm to 10 <inline-formula><mml:math id="M263" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>,
Front. Env. Sci. Eng.,
10, 63–72, <ext-link xlink:href="https://doi.org/10.1007/s11783-014-0754-x" ext-link-type="DOI">10.1007/s11783-014-0754-x</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><?label 35?><mixed-citation>Lu, Y., Yan, C., Fu, Y., Chen, Y., Liu, Y., Yang, G., Wang, Y., Bianchi, F., Chu, B., Zhou, Y., Yin, R., Baalbaki, R., Garmash, O., Deng, C., Wang, W., Liu, Y., Petäjä, T., Kerminen, V.-M., Jiang, J., Kulmala, M., and Wang, L.: A proxy for atmospheric daytime gaseous sulfuric acid concentration in urban Beijing, Atmos. Chem. Phys., 19, 1971–1983, <ext-link xlink:href="https://doi.org/10.5194/acp-19-1971-2019" ext-link-type="DOI">10.5194/acp-19-1971-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><?label 36?><mixed-citation>Ma, F., Xie, H.-B., Elm, J., Shen, J., Chen, J., and Vehkamäki, H.:
Piperazine Enhancing Sulfuric Acid-Based New Particle Formation: Implications for the Atmospheric Fate of Piperazine,
Environ. Sci. Technol.,
53, 8785–8795, <ext-link xlink:href="https://doi.org/10.1021/acs.est.9b02117" ext-link-type="DOI">10.1021/acs.est.9b02117</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><?label 37?><mixed-citation>Mauldin, R. L., Berndt, T., Sipila, M., Paasonen, P., Petaja, T., Kim, S., Kurten, T., Stratmann, F., Kerminen, V. M., and Kulmal<?pagebreak page11765?>a, M.:
A new atmospherically relevant oxidant of sulphur dioxide,
Nature,
488, 193–196, <ext-link xlink:href="https://doi.org/10.1038/nature11278" ext-link-type="DOI">10.1038/nature11278</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib40"><label>40</label><?label 38?><mixed-citation>
McElreath, R.:
Statistical rethinking: A Bayesian course with examples in R and Stan,
Chapman and Hall/CRC, Taylor &amp; Francis Group
6000 Broken Sound Parkway NW, Suite 300
Boca Raton, FL 33487-2742, USA, 2018.</mixed-citation></ref>
      <ref id="bib1.bib41"><label>41</label><?label 39?><mixed-citation>Merikanto, J., Spracklen, D. V., Mann, G. W., Pickering, S. J., and Carslaw, K. S.: Impact of nucleation on global CCN, Atmos. Chem. Phys., 9, 8601–8616, <ext-link xlink:href="https://doi.org/10.5194/acp-9-8601-2009" ext-link-type="DOI">10.5194/acp-9-8601-2009</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib42"><label>42</label><?label 40?><mixed-citation>Mikkonen, S., Romakkaniemi, S., Smith, J. N., Korhonen, H., Petäjä, T., Plass-Duelmer, C., Boy, M., McMurry, P. H., Lehtinen, K. E. J., Joutsensaari, J., Hamed, A., Mauldin III, R. L., Birmili, W., Spindler, G., Arnold, F., Kulmala, M., and Laaksonen, A.: A statistical proxy for sulphuric acid concentration, Atmos. Chem. Phys., 11, 11319–11334, <ext-link xlink:href="https://doi.org/10.5194/acp-11-11319-2011" ext-link-type="DOI">10.5194/acp-11-11319-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib43"><label>43</label><?label 41?><mixed-citation>Mikkonen, S., Németh, Z., Varga, V., Weidinger, T., Leinonen, V., Yli-Juuti, T., and Salma, I.: Decennial time trends and diurnal patterns of particle number concentrations in a Central European city between 2008 and 2018, Atmos. Chem. Phys. Discuss., <ext-link xlink:href="https://doi.org/10.5194/acp-2020-305" ext-link-type="DOI">10.5194/acp-2020-305</ext-link>, in review, 2020.</mixed-citation></ref>
      <ref id="bib1.bib44"><label>44</label><?label 42?><mixed-citation>Monkkonen, P., Koponen, I. K., Lehtinen, K. E. J., Uma, R., Srinivasan, D., Hameri, K., and Kulmala, M.:
Death of nucleation and Aitken mode particles: observations at extreme atmospheric conditions and their theoretical explanation,
J. Aerosol Sci.,
35, 781–787, <ext-link xlink:href="https://doi.org/10.1016/j.jaerosci.2003.12.004" ext-link-type="DOI">10.1016/j.jaerosci.2003.12.004</ext-link>, 2004.</mixed-citation></ref>
      <ref id="bib1.bib45"><label>45</label><?label 43?><mixed-citation>Mönkkönen, P., Koponen, I. K., Lehtinen, K. E. J., Hämeri, K., Uma, R., and Kulmala, M.: Measurements in a highly polluted Asian mega city: observations of aerosol number size distribution, modal parameters and nucleation events, Atmos. Chem. Phys., 5, 57–66, <ext-link xlink:href="https://doi.org/10.5194/acp-5-57-2005" ext-link-type="DOI">10.5194/acp-5-57-2005</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bib46"><label>46</label><?label 44?><mixed-citation>Nieminen, T., Kerminen, V.-M., Petäjä, T., Aalto, P. P., Arshinov, M., Asmi, E., Baltensperger, U., Beddows, D. C. S., Beukes, J. P., Collins, D., Ding, A., Harrison, R. M., Henzing, B., Hooda, R., Hu, M., Hőrrak, U., Kivekäs, N., Komsaare, K., Krejci, R., Kristensson, A., Laakso, L., Laaksonen, A., Leaitch, W. R., Lihavainen, H., Mihalopoulos, N., Németh, Z., Nie, W., O'Dowd, C., Salma, I., Sellegri, K., Svenningsson, B., Swietlicki, E., Tunved, P., Ulevicius, V., Vakkari, V., Vana, M., Wiedensohler, A., Wu, Z., Virtanen, A., and Kulmala, M.: Global analysis of continental boundary layer new particle formation based on long-term measurements, Atmos. Chem. Phys., 18, 14737–14756, <ext-link xlink:href="https://doi.org/10.5194/acp-18-14737-2018" ext-link-type="DOI">10.5194/acp-18-14737-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib47"><label>47</label><?label 45?><mixed-citation>Novelli, A., Hens, K., Tatum Ernest, C., Martinez, M., Nölscher, A. C., Sinha, V., Paasonen, P., Petäjä, T., Sipilä, M., Elste, T., Plass-Dülmer, C., Phillips, G. J., Kubistin, D., Williams, J., Vereecken, L., Lelieveld, J., and Harder, H.: Estimating the atmospheric concentration of Criegee intermediates and their possible interference in a FAGE-LIF instrument, Atmos. Chem. Phys., 17, 7807–7826, <ext-link xlink:href="https://doi.org/10.5194/acp-17-7807-2017" ext-link-type="DOI">10.5194/acp-17-7807-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib48"><label>48</label><?label 46?><mixed-citation>Petäjä, T., Mauldin, III, R. L., Kosciuch, E., McGrath, J., Nieminen, T., Paasonen, P., Boy, M., Adamov, A., Kotiaho, T., and Kulmala, M.: Sulfuric acid and OH concentrations in a boreal forest site, Atmos. Chem. Phys., 9, 7435–7448, <ext-link xlink:href="https://doi.org/10.5194/acp-9-7435-2009" ext-link-type="DOI">10.5194/acp-9-7435-2009</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib49"><label>49</label><?label 47?><mixed-citation>Pikridas, M., Vrekoussis, M., Sciare, J., Kleanthous, S., Vasiliadou, E., Kizas, C., Savvides, C., and Mihalopoulos, N.:
Spatial and temporal (short and long-term) variability of submicron, fine and sub-10 <inline-formula><mml:math id="M264" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> particulate matter (<inline-formula><mml:math id="M265" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M266" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M267" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) in Cyprus,
Atmos. Environ.,
191, 79–93, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2018.07.048" ext-link-type="DOI">10.1016/j.atmosenv.2018.07.048</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib50"><label>50</label><?label 48?><mixed-citation>
Rinne, J., Ruuskanen, T. M., Reissell, A., Taipale, R., Hakola, H., and Kulmala, M.:
On-line PTR-MS measurements of atmospheric concentrations of volatile organic compounds in a European boreal forest ecosystem,
Boreal Environ. Res.,
10, 425–436, 2005.</mixed-citation></ref>
      <ref id="bib1.bib51"><label>51</label><?label 49?><mixed-citation>Rohrer, F. and Berresheim, H.:
Strong correlation between levels of tropospheric hydroxyl radicals and solar ultraviolet radiation,
Nature,
442, 184–187, <ext-link xlink:href="https://doi.org/10.1038/nature04924" ext-link-type="DOI">10.1038/nature04924</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib52"><label>52</label><?label 52?><mixed-citation>Salma, I. and Németh, Z.: Dynamic and timing properties of new aerosol particle formation and consecutive growth events, Atmos. Chem. Phys., 19, 5835–5852, <ext-link xlink:href="https://doi.org/10.5194/acp-19-5835-2019" ext-link-type="DOI">10.5194/acp-19-5835-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib53"><label>53</label><?label 50?><mixed-citation>Salma, I., Németh, Z., Kerminen, V.-M., Aalto, P., Nieminen, T., Weidinger, T., Molnár, Á., Imre, K., and Kulmala, M.: Regional effect on urban atmospheric nucleation, Atmos. Chem. Phys., 16, 8715–8728, <ext-link xlink:href="https://doi.org/10.5194/acp-16-8715-2016" ext-link-type="DOI">10.5194/acp-16-8715-2016</ext-link>, 2016a.</mixed-citation></ref>
      <ref id="bib1.bib54"><label>54</label><?label 51?><mixed-citation>Salma, I., Németh, Z., Weidinger, T., Kovács, B., and Kristóf, G.: Measurement, growth types and shrinkage of newly formed aerosol particles at an urban research platform, Atmos. Chem. Phys., 16, 7837–7851, <ext-link xlink:href="https://doi.org/10.5194/acp-16-7837-2016" ext-link-type="DOI">10.5194/acp-16-7837-2016</ext-link>, 2016b.</mixed-citation></ref>
      <ref id="bib1.bib55"><label>55</label><?label 53?><mixed-citation>Sarnela, N., Jokinen, T., Nieminen, T., Lehtipalo, K., Junninen, H., Kangasluoma, J., Hakala, J., Taipale, R., Schobesberger, S., Sipila, M., Larnimaa, K., Westerholm, H., Heijari, J., Kerminen, V. M., Petaja, T., and Kulmala, M.:
Sulphuric acid and aerosol particle production in the vicinity of an oil refinery,
Atmos. Environ.,
119, 156–166, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2015.08.033" ext-link-type="DOI">10.1016/j.atmosenv.2015.08.033</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib56"><label>56</label><?label 54?><mixed-citation>Sihto, S.-L., Kulmala, M., Kerminen, V.-M., Dal Maso, M., Petäjä, T., Riipinen, I., Korhonen, H., Arnold, F., Janson, R., Boy, M., Laaksonen, A., and Lehtinen, K. E. J.: Atmospheric sulphuric acid and aerosol formation: implications from atmospheric measurements for nucleation and early growth mechanisms, Atmos. Chem. Phys., 6, 4079–4091, <ext-link xlink:href="https://doi.org/10.5194/acp-6-4079-2006" ext-link-type="DOI">10.5194/acp-6-4079-2006</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib57"><label>57</label><?label 55?><mixed-citation>Sipilä, M., Berndt, T., Petäjä, T., Brus, D., Vanhanen, J., Stratmann, F., Patokoski, J., Mauldin, R. L., Hyvärinen, A.-P., Lihavainen, H., and Kulmala, M.:
The Role of Sulfuric Acid in Atmospheric Nucleation,
Science,
327, 1243–1246, <ext-link xlink:href="https://doi.org/10.1126/science.1180315" ext-link-type="DOI">10.1126/science.1180315</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib58"><label>58</label><?label 56?><mixed-citation>Sipilä, M., Jokinen, T., Berndt, T., Richters, S., Makkonen, R., Donahue, N. M., Mauldin III, R. L., Kurtén, T., Paasonen, P., Sarnela, N., Ehn, M., Junninen, H., Rissanen, M. P., Thornton, J., Stratmann, F., Herrmann, H., Worsnop, D. R., Kulmala, M., Kerminen, V.-M., and Petäjä, T.: Reactivity of stabilized Criegee intermediates (sCIs) from isoprene and monoterpene ozonolysis toward <inline-formula><mml:math id="M268" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and organic acids, Atmos. Chem. Phys., 14, 12143–12153, <ext-link xlink:href="https://doi.org/10.5194/acp-14-12143-2014" ext-link-type="DOI">10.5194/acp-14-12143-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib59"><label>59</label><?label 57?><mixed-citation>Spracklen, D. V., Carslaw, K. S., Kulmala, M., Kerminen, V. M., Sihto, S. L., Riipinen, I., Merikanto, J., Mann, G. W., Chipperfield, M. P., and Wiedensohler, A.:
Contribution of particle formation to global cloud condensation nuclei concentrations,
Geophy. Res. Lett.,
35, L06808, <ext-link xlink:href="https://doi.org/10.1029/2007GL033038" ext-link-type="DOI">10.1029/2007GL033038</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bib60"><label>60</label><?label 58?><mixed-citation>Spracklen, D. V., Carslaw, K. S., Merikanto, J., Mann, G. W., Reddington, C. L., Pickering, S., Ogren, J. A., Andrews, E<?pagebreak page11766?>., Baltensperger, U., Weingartner, E., Boy, M., Kulmala, M., Laakso, L., Lihavainen, H., Kivekäs, N., Komppula, M., Mihalopoulos, N., Kouvarakis, G., Jennings, S. G., O'Dowd, C., Birmili, W., Wiedensohler, A., Weller, R., Gras, J., Laj, P., Sellegri, K., Bonn, B., Krejci, R., Laaksonen, A., Hamed, A., Minikin, A., Harrison, R. M., Talbot, R., and Sun, J.: Explaining global surface aerosol number concentrations in terms of primary emissions and particle formation, Atmos. Chem. Phys., 10, 4775–4793, <ext-link xlink:href="https://doi.org/10.5194/acp-10-4775-2010" ext-link-type="DOI">10.5194/acp-10-4775-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib61"><label>61</label><?label 59?><mixed-citation>Taipale, R., Ruuskanen, T. M., Rinne, J., Kajos, M. K., Hakola, H., Pohja, T., and Kulmala, M.: Technical Note: Quantitative long-term measurements of VOC concentrations by PTR-MS – measurement, calibration, and volume mixing ratio calculation methods, Atmos. Chem. Phys., 8, 6681–6698, <ext-link xlink:href="https://doi.org/10.5194/acp-8-6681-2008" ext-link-type="DOI">10.5194/acp-8-6681-2008</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bib62"><label>62</label><?label 60?><mixed-citation>Weber, R. J., Marti, J. J., McMurry, P. H., Eisele, F. L., Tanner, D. J., and Jefferson, A.:
Measured Atmospheric New Particle Formation Rates: Implications For Nucleation Mechanisms,
Chem. Eng. Commun.,
151, 53–64, <ext-link xlink:href="https://doi.org/10.1080/00986449608936541" ext-link-type="DOI">10.1080/00986449608936541</ext-link>, 1996.</mixed-citation></ref>
      <ref id="bib1.bib63"><label>63</label><?label 61?><mixed-citation>Yan, C., Dada, L., Rose, C., Jokinen, T., Nie, W., Schobesberger, S., Junninen, H., Lehtipalo, K., Sarnela, N., Makkonen, U., Garmash, O., Wang, Y., Zha, Q., Paasonen, P., Bianchi, F., Sipilä, M., Ehn, M., Petäjä, T., Kerminen, V.-M., Worsnop, D. R., and Kulmala, M.: The role of <inline-formula><mml:math id="M269" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> anion clusters in ion-induced aerosol nucleation mechanisms in the boreal forest, Atmos. Chem. Phys., 18, 13231–13243, <ext-link xlink:href="https://doi.org/10.5194/acp-18-13231-2018" ext-link-type="DOI">10.5194/acp-18-13231-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib64"><label>64</label><?label 62?><mixed-citation>Yang, D., Zhang, S., Niu, T., Wang, Y., Xu, H., Zhang, K. M., and Wu, Y.: High-resolution mapping of vehicle emissions of atmospheric pollutants based on large-scale, real-world traffic datasets, Atmos. Chem. Phys., 19, 8831–8843, <ext-link xlink:href="https://doi.org/10.5194/acp-19-8831-2019" ext-link-type="DOI">10.5194/acp-19-8831-2019</ext-link>, 2019.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib65"><label>65</label><?label 63?><mixed-citation>Yao, L., Garmash, O., Bianchi, F., Zheng, J., Yan, C., Kontkanen, J., Junninen, H., Mazon, S. B., Ehn, M., Paasonen, P., Sipilä, M., Wang, M., Wang, X., Xiao, S., Chen, H., Lu, Y., Zhang, B., Wang, D., Fu, Q., Geng, F., Li, L., Wang, H., Qiao, L., Yang, X., Chen, J., Kerminen, V.-M., Petäjä, T., Worsnop, D. R., Kulmala, M., and Wang, L.:
Atmospheric new particle formation from sulfuric acid and amines in a Chinese megacity,
Science,
361, 278–281, <ext-link xlink:href="https://doi.org/10.1126/science.aao4839" ext-link-type="DOI">10.1126/science.aao4839</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib66"><label>66</label><?label 64?><mixed-citation>Yao, L., Fan, X., Yan, C., Kurtén, T., Daellenbach, K. R., Wang, Y., Guo, Y., Li, C., Dada, L., Cai, J., Jun, T. Y., Zha, Q., Du, W., Yu, M., Zheng, F., Zhou, Y., Chan, T., Shen, J., Kujansuu, J. T., Kangasluoma, J., Jiang, J., Li, H., Wang, L., Worsnop, D. R., He, H., Petäjä, T., Kerminen, V.-M., Liu, Y., Chu, B., Kulmala, M., and Bianchi, F.:
Unprecedented ambient sulphur trioxide (<inline-formula><mml:math id="M270" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) detection: possible formation mechanism and atmospheric implications,
Environ. Sci. Technol. Lett.,
accepted, 2020.</mixed-citation></ref>
      <ref id="bib1.bib67"><label>67</label><?label 65?><mixed-citation>
Zhang, R., Khalizov, A., Wang, L., Hu, M., and Xu, W.:
Nucleation and growth of nanoparticles in the atmosphere,
Chem. Rev.,
112, 1957–2011, 2011.</mixed-citation></ref>
      <ref id="bib1.bib68"><label>68</label><?label 66?><mixed-citation>Zhang, W., Tong, S., Ge, M., An, J., Shi, Z., Hou, S., Xia, K., Qu, Y., Zhang, H., Chu, B., Sun, Y., and He, H.:
Variations and sources of nitrous acid (HONO) during a severe pollution episode in Beijing in winter 2016,
Sci. Total Environ.,
648, 253–262, <ext-link xlink:href="https://doi.org/10.1016/j.scitotenv.2018.08.133" ext-link-type="DOI">10.1016/j.scitotenv.2018.08.133</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib69"><label>69</label><?label 67?><mixed-citation>Zhou, Y., Dada, L., Liu, Y., Fu, Y., Kangasluoma, J., Chan, T., Yan, C., Chu, B., Daellenbach, K. R., Bianchi, F., Kokkonen, T. V., Liu, Y., Kujansuu, J., Kerminen, V.-M., Petäjä, T., Wang, L., Jiang, J., and Kulmala, M.: Variation of size-segregated particle number concentrations in wintertime Beijing, Atmos. Chem. Phys., 20, 1201–1216, <ext-link xlink:href="https://doi.org/10.5194/acp-20-1201-2020" ext-link-type="DOI">10.5194/acp-20-1201-2020</ext-link>, 2020.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Sources and sinks driving sulfuric acid concentrations in contrasting environments: implications on proxy calculations</article-title-html>
<abstract-html><p>Sulfuric acid has been shown to be a key driver for new particle formation and subsequent growth in various environments, mainly due to its low
volatility. However, direct measurements of gas-phase sulfuric acid are oftentimes not available, and the current sulfuric acid proxies cannot
predict, for example, its nighttime concentrations or result in significant discrepancies with measured values. Here, we define the sources and sinks
of sulfuric acid in different environments and derive a new physical proxy for sulfuric acid to be utilized in locations and during periods when
it is not measured. We used H<sub>2</sub>SO<sub>4</sub> measurements from four different locations: Hyytiälä, Finland; Agia Marina, Cyprus; Budapest,
Hungary; and Beijing, China, representing semi-pristine boreal forest, rural environment in the Mediterranean area, urban environment and heavily
polluted megacity, respectively. The new proxy takes into account the formation of sulfuric acid from SO<sub>2</sub> via OH oxidation and other
oxidation pathways, specifically via stabilized Criegee intermediates. The sulfuric acid sinks included in the proxy are its condensation
sink (CS) and atmospheric clustering starting from H<sub>2</sub>SO<sub>4</sub> dimer formation. Indeed, we found that the observed sulfuric acid
concentration can be explained by the proposed sources and sinks with similar coefficients in the four contrasting environments where we have tested
it. Thus, the new proxy is a more flexible and an important improvement over previous proxies. Following the recommendations in this paper, a
proxy for a specific location can be derived.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Aalto, P., Hameri, K., Becker, E., Weber, R., Salm, J., Makela, J. M., Hoell, C., O'Dowd, C. D., Karlsson, H., Hansson, H. C., Vakeva, M., Koponen, I. K., Buzorius, G., and Kulmala, M.:
Physical characterization of aerosol particles during nucleation events,
Tellus B,
53, 344–358, <a href="https://doi.org/10.1034/j.1600-0889.2001.530403.x" target="_blank">https://doi.org/10.1034/j.1600-0889.2001.530403.x</a>, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Almeida, J., Schobesberger, S., Kurten, A., Ortega, I. K., Kupiainen-Maatta, O., Praplan, A. P., Adamov, A., Amorim, A., Bianchi, F., Breitenlechner, M., David, A., Dommen, J., Donahue, N. M., Downard, A., Dunne, E., Duplissy, J., Ehrhart, S., Flagan, R. C., Franchin, A., Guida, R., Hakala, J., Hansel, A., Heinritzi, M., Henschel, H., Jokinen, T., Junninen, H., Kajos, M., Kangasluoma, J., Keskinen, H., Kupc, A., Kurten, T., Kvashin, A. N., Laaksonen, A., Lehtipalo, K., Leiminger, M., Leppa, J., Loukonen, V., Makhmutov, V., Mathot, S., McGrath, M. J., Nieminen, T., Olenius, T., Onnela, A., Petaja, T., Riccobono, F., Riipinen, I., Rissanen, M., Rondo, L., Ruuskanen, T., Santos, F. D., Sarnela, N., Schallhart, S., Schnitzhofer, R., Seinfeld, J. H., Simon, M., Sipila, M., Stozhkov, Y., Stratmann, F., Tome, A., Trostl, J., Tsagkogeorgas, G., Vaattovaara, P., Viisanen, Y., Virtanen, A., Vrtala, A., Wagner, P. E., Weingartner, E., Wex, H., Williamson, C., Wimmer, D., Ye, P. L., Yli-Juuti, T., Carslaw, K. S., Kulmala, M., Curtius, J., Baltensperger, U., Worsnop, D. R., Vehkamaki, H., and Kirkby, J.:
Molecular understanding of sulphuric acid-amine particle nucleation in the atmosphere,
Nature,
502, 359–363, <a href="https://doi.org/10.1038/nature12663" target="_blank">https://doi.org/10.1038/nature12663</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Baalbaki, R., Pikridas M., Jokinen T., Dada L., Ahonen L., Lehtipalo K., Petäjä T., Sciare J., and Kulmala M.:
Towards understanding the mechanisms of new particle formation in the Eastern Mediterranean,
in preparation, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Berresheim, H., Elste, T., Tremmel, H. G., Allen, A. G., Hansson, H. C., Rosman, K., Dal Maso, M., Makela, J. M., Kulmala, M., and O'Dowd, C. D.:
Gas-aerosol relationships of H<sub>2</sub>SO<sub>4</sub>, MSA, and OH: Observations in the coastal marine boundary layer at Mace Head, Ireland,
J. Geophys. Res.-Atmos.,
107, 8100, <a href="https://doi.org/10.1029/2000jd000229" target="_blank">https://doi.org/10.1029/2000jd000229</a>, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Dada, L.: Sulfuric acid proxy calculation using coefficients derived from four contrasting environments, Zenodo, <a href="https://doi.org/10.5281/zenodo.4048329" target="_blank">https://doi.org/10.5281/zenodo.4048329</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Dada, L., Paasonen, P., Nieminen, T., Buenrostro Mazon, S., Kontkanen, J., Peräkylä, O., Lehtipalo, K., Hussein, T., Petäjä, T., Kerminen, V.-M., Bäck, J., and Kulmala, M.: Long-term analysis of clear-sky new particle formation events and nonevents in Hyytiälä, Atmos. Chem. Phys., 17, 6227–6241, <a href="https://doi.org/10.5194/acp-17-6227-2017" target="_blank">https://doi.org/10.5194/acp-17-6227-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Dada, L., Chellapermal, R., Buenrostro Mazon, S., Paasonen, P., Lampilahti, J., Manninen, H. E., Junninen, H., Petäjä, T., Kerminen, V.-M., and Kulmala, M.: Refined classification and characterization of atmospheric new-particle formation events using air ions, Atmos. Chem. Phys., 18, 17883–17893, <a href="https://doi.org/10.5194/acp-18-17883-2018" target="_blank">https://doi.org/10.5194/acp-18-17883-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
Deng, C., Fu, Y., Dada, L., Yan, C., Cai, R., Yang, D., Zhou, Y., Yin, R., Lu, Y., Li, X., Qiao, X., Fan, X., Nie, W., Kontkanen, J., Kangasluoma, J., Chu, B., Ding, A., Kerminen, V.-M., Paasonen, P., Worsnop, D. R., Bianchi, F., Liu, Y., Zheng, J., Wang, L., Kulmala, M., and Jiang, J.:
Seasonal Characteristics of New Particle Formation and Growth in Urban Beijing,
Environ. Sci. Technol., 54, 8547–8557, <a href="https://doi.org/10.1021/acs.est.0c00808" target="_blank">https://doi.org/10.1021/acs.est.0c00808</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Dunne, E. M., Gordon, H., Kurten, A., Almeida, J., Duplissy, J., Williamson, C., Ortega, I. K., Pringle, K. J., Adamov, A., Baltensperger, U., Barmet, P., Benduhn, F., Bianchi, F., Breitenlechner, M., Clarke, A., Curtius, J., Dommen, J., Donahue, N. M., Ehrhart, S., Flagan, R. C., Franchin, A., Guida, R., Hakala, J., Hansel, A., Heinritzi, M., Jokinen, T., Kangasluoma, J., Kirkby, J., Kulmala, M., Kupc, A., Lawler, M. J., Lehtipalo, K., Makhmutov, V., Mann, G., Mathot, S., Merikanto, J., Miettinen, P., Nenes, A., Onnela, A., Rap, A., Reddington, C. L. S., Riccobono, F., Richards, N. A. D., Rissanen, M. P., Rondo, L., Sarnela, N., Schobesberger, S., Sengupta, K., Simon, M., Sipilaa, M., Smith, J. N., Stozkhov, Y., Tome, A., Trostl, J., Wagner, P. E., Wimmer, D., Winkler, P. M., Worsnop, D. R., and Carslaw, K. S.:
Global atmospheric particle formation from CERN CLOUD measurements,
Science,
354, 1119–1124, <a href="https://doi.org/10.1126/science.aaf2649" target="_blank">https://doi.org/10.1126/science.aaf2649</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Efron, B. and Tibshirani, R. J.:
An introduction to the bootstrap,
CRC Press, 29 West 35th Street
New York, NY 10001, USA, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>
Eisele, F. L. and Tanner, D. J.:
Measurement of the Gas-Phase Concentration of H<sub>2</sub>SO<sub>4</sub> and Methane Sulfonic-Acid and Estimates of H<sub>2</sub>SO<sub>4</sub> Production and Loss in the Atmosphere,
J. Geophys. Res.-Atmos.,
98, 9001–9010, <a href="https://doi.org/10.1029/93jd00031" target="_blank">https://doi.org/10.1029/93jd00031</a>, 1993.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>
Erupe, M. E., Viggiano, A. A., and Lee, S.-H.: The effect of trimethylamine on atmospheric nucleation involving H2SO4, Atmos. Chem. Phys., 11, 4767–4775, <a href="https://doi.org/10.5194/acp-11-4767-2011" target="_blank">https://doi.org/10.5194/acp-11-4767-2011</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Gao, W., Tan, G., Hong, Y., Li, M., Nian, H., Guo, C., Huang, Z., Fu, Z., Dong, J., Xu, X., Cheng, P., and Zhou, Z.:
Development of portable single photon ionization time-of-flight mass spectrometer combined with membrane inlet,
Int. J. Mass Spectrom.,
334, 8–12, <a href="https://doi.org/10.1016/j.ijms.2012.09.003" target="_blank">https://doi.org/10.1016/j.ijms.2012.09.003</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>
Gordon, H., Kirkby, J., Baltensperger, U., Bianchi, F., Breitenlechner, M., Curtius, J., Dias, A., Dommen, J., Donahue, N. M., Dunne, E. M., Duplissy, J., Ehrhart, S., Flagan, R. C., Frege, C., Fuchs, C., Hansel, A., Hoyle, C. R., Kulmala, M., Kurten, A., Lehtipalo, K., Makhmutov, V., Molteni, U., Rissanen, M. P., Stozkhov, Y., Trostl, J., Tsagkogeorgas, G., Wagner, R., Williamson, C., Wimmer, D., Winkler, P. M., Yan, C., and Carslaw, K. S.:
Causes and importance of new particle formation in the present-day and preindustrial atmospheres,
J. Geophys. Res.-Atmos.,
122, 8739–8760, <a href="https://doi.org/10.1002/2017jd026844" target="_blank">https://doi.org/10.1002/2017jd026844</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>
Guo, S., Hu, M., Zamora, M. L., Peng, J., Shang, D., Zheng, J., Du, Z., Wu, Z., Shao, M., Zeng, L., Molina, M. J., and Zhang, R.:
Elucidating severe urban haze formation in China,
P. Natl. Acad. Sci. USA,
111, 17373–17378, <a href="https://doi.org/10.1073/pnas.1419604111" target="_blank">https://doi.org/10.1073/pnas.1419604111</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>
Hakola, H., Hellén, H., Hemmilä, M., Rinne, J., and Kulmala, M.: In situ measurements of volatile organic compounds in a boreal forest, Atmos. Chem. Phys., 12, 11665–11678, <a href="https://doi.org/10.5194/acp-12-11665-2012" target="_blank">https://doi.org/10.5194/acp-12-11665-2012</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>
Hari, P. and Kulmala, M.:
Station for measuring ecosystem-atmosphere relations (SMEAR II),
Boreal Environ. Res.,
10, 315–322, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation>
Hellén, H., Praplan, A. P., Tykkä, T., Ylivinkka, I., Vakkari, V., Bäck, J., Petäjä, T., Kulmala, M., and Hakola, H.: Long-term measurements of volatile organic compounds highlight the importance of sesquiterpenes for the atmospheric chemistry of a boreal forest, Atmos. Chem. Phys., 18, 13839–13863, <a href="https://doi.org/10.5194/acp-18-13839-2018" target="_blank">https://doi.org/10.5194/acp-18-13839-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation>
Hussein, T., Martikainen, J., Junninen, H., Sogacheva, L., Wagner, R., Dal Maso, M., Riipinen, I., Aalto, P. P., and Kulmala, M.:
Observation of regional new particle formation in the urban atmosphere,
Tellus B,
60, 509–521, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation>
Jen, C. N., McMurry, P. H., and Hanson, D. R.:
Stabilization of sulfuric acid dimers by ammonia, methylamine, dimethylamine, and trimethylamine,
J. Geophys. Res.-Atmos.,
119, 7502–7514, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation>
Jokinen, T., Sipilä, M., Junninen, H., Ehn, M., Lönn, G., Hakala, J., Petäjä, T., Mauldin III, R. L., Kulmala, M., and Worsnop, D. R.: Atmospheric sulphuric acid and neutral cluster measurements using CI-APi-TOF, Atmos. Chem. Phys., 12, 4117–4125, <a href="https://doi.org/10.5194/acp-12-4117-2012" target="_blank">https://doi.org/10.5194/acp-12-4117-2012</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation>
Junninen, H., Ehn, M., Petäjä, T., Luosujärvi, L., Kotiaho, T., Kostiainen, R., Rohner, U., Gonin, M., Fuhrer, K., Kulmala, M., and Worsnop, D. R.: A high-resolution mass spectrometer to measure atmospheric ion composition, Atmos. Meas. Tech., 3, 1039–1053, <a href="https://doi.org/10.5194/amt-3-1039-2010" target="_blank">https://doi.org/10.5194/amt-3-1039-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation>
Kerminen, V.-M., Paramonov, M., Anttila, T., Riipinen, I., Fountoukis, C., Korhonen, H., Asmi, E., Laakso, L., Lihavainen, H., Swietlicki, E., Svenningsson, B., Asmi, A., Pandis, S. N., Kulmala, M., and Petäjä, T.: Cloud condensation nuclei production associated with atmospheric nucleation: a synthesis based on existing literature and new results, Atmos. Chem. Phys., 12, 12037–12059, <a href="https://doi.org/10.5194/acp-12-12037-2012" target="_blank">https://doi.org/10.5194/acp-12-12037-2012</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation>
Kerminen, V.-M., Chen, X., Vakkari, V., Petäjä, T., Kulmala, M., and Bianchi, F.:
Atmospheric new particle formation and growth: review of field observations,
Environ. Res. Lett.,
13, 103003, <a href="https://doi.org/10.1088/1748-9326/aadf3c" target="_blank">https://doi.org/10.1088/1748-9326/aadf3c</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation>
Kulmala, M., Vehkamäki, H., Petäjä, T., Dal Maso, M., Lauri, A., Kerminen, V.-M., Birmili, W., and McMurry, P. H.:
Formation and growth rates of ultrafine atmospheric particles: a review of observations,
J. Aerosol Sci.,
35, 143–176, <a href="https://doi.org/10.1016/j.jaerosci.2003.10.003" target="_blank">https://doi.org/10.1016/j.jaerosci.2003.10.003</a>, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>
Kulmala, M., Petaja, T., Nieminen, T., Sipila, M., Manninen, H. E., Lehtipalo, K., Dal Maso, M., Aalto, P. P., Junninen, H., Paasonen, P., Riipinen, I., Lehtinen, K. E. J., Laaksonen, A., and Kerminen, V. M.:
Measurement of the nucleation of atmospheric aerosol particles,
Nat. Protoc.,
7, 1651–1667, <a href="https://doi.org/10.1038/nprot.2012.091" target="_blank">https://doi.org/10.1038/nprot.2012.091</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation>
Kulmala, M., Kontkanen, J., Junninen, H., Lehtipalo, K., Manninen, H. E., Nieminen, T., Petaja, T., Sipila, M., Schobesberger, S., Rantala, P., Franchin, A., Jokinen, T., Jarvinen, E., Aijala, M., Kangasluoma, J., Hakala, J., Aalto, P. P., Paasonen, P., Mikkila, J., Vanhanen, J., Aalto, J., Hakola, H., Makkonen, U., Ruuskanen, T., Mauldin, R. L., Duplissy, J., Vehkamaki, H., Back, J., Kortelainen, A., Riipinen, I., Kurten, T., Johnston, M. V., Smith, J. N., Ehn, M., Mentel, T. F., Lehtinen, K. E. J., Laaksonen, A., Kerminen, V. M., and Worsnop, D. R.:
Direct Observations of Atmospheric Aerosol Nucleation,
Science,
339, 943–946, <a href="https://doi.org/10.1126/science.1227385" target="_blank">https://doi.org/10.1126/science.1227385</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation>
Kulmala, M., Kerminen, V. M., Petaja, T., Ding, A. J., and Wang, L.:
Atmospheric gas-to-particle conversion: why NPF events are observed in megacities?,
Faraday Discuss.,
200, 271–288, <a href="https://doi.org/10.1039/c6fd00257a" target="_blank">https://doi.org/10.1039/c6fd00257a</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation>
Kulmala, M., Dada, L., Dällenbach, K., Yan, C., Stolzenburg, D., Kontkanen, J., Ezhova, E., Hakala, S., Tuovinen, S., Kokkonen, T., Kurppa, M., Cai, R., Zhou, Y., Yin, R., Baalbaki, R., Chan, T., Chu, B., Deng, C., Fu, Y., Ge, M., He, H., Heikkinen, L., Junninen, H., Nei, W., Rusanen, A., Vakkari, V., Wang, Y., Wang, L., yao, l., Zheng, J., Kujansuu, J., Kangasluoma, J., Petäjä, T., Paasonen, P., Järvi, L., Worsnop, D., Ding, A., Liu, Y., Jiang, J., Bianchi, F., Yang, G., Liu, Y., Lu, Y., and Kerminen, V.-M.: Is reducing new particle formation a plausible solution to mitigate particulate air pollution in Beijing and other Chinese megacities?, Faraday Discuss., <a href="https://doi.org/10.1039/D0FD00078G" target="_blank">https://doi.org/10.1039/D0FD00078G</a>, accepted, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation>
Kurten, A., Rondo, L., Ehrhart, S., and Curtius, J.:
Calibration of a chemical ionization mass spectrometer for the measurement of gaseous sulfuric acid,
Phys. Chem. A,
116, 6375–6386, <a href="https://doi.org/10.1021/jp212123n" target="_blank">https://doi.org/10.1021/jp212123n</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation>
Kürten, A., Williamson, C., Almeida, J., Kirkby, J., and Curtius, J.: On the derivation of particle nucleation rates from experimental formation rates, Atmos. Chem. Phys., 15, 4063–4075, <a href="https://doi.org/10.5194/acp-15-4063-2015" target="_blank">https://doi.org/10.5194/acp-15-4063-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation>
Laakso, L., Petäjä, T., Lehtinen, K. E. J., Kulmala, M., Paatero, J., Hőrrak, U., Tammet, H., and Joutsensaari, J.: Ion production rate in a boreal forest based on ion, particle and radiation measurements, Atmos. Chem. Phys., 4, 1933–1943, <a href="https://doi.org/10.5194/acp-4-1933-2004" target="_blank">https://doi.org/10.5194/acp-4-1933-2004</a>, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation>
Laakso, L., Koponen, I. K., Monkkonen, P., Kulmala, M., Kerminen, V. M., Wehner, B., Wiedensohler, A., Wu, Z. J., and Hu, M.:
Aerosol particles in the developing world; A comparison between New Delhi in India and Beijing in China,
Water Air Soil Poll.,
173, 5–20, <a href="https://doi.org/10.1007/s11270-005-9018-5" target="_blank">https://doi.org/10.1007/s11270-005-9018-5</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation>
Lagarias, J. C., Reeds, J. A., Wright, M. H., and Wright, P. E.:
Convergence Properties of the Nelder–Mead Simplex Method in Low Dimensions,
SIAM J. Optimiz.,
9, 112–147, <a href="https://doi.org/10.1137/s1052623496303470" target="_blank">https://doi.org/10.1137/s1052623496303470</a>, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation>
Lehtipalo, K., Yan, C., Dada, L., Bianchi, F., Xiao, M., Wagner, R., Stolzenburg, D., Ahonen, L. R., Amorim, A., Baccarini, A., Bauer, P. S., Baumgartner, B., Bergen, A., Bernhammer, A.-K., Breitenlechner, M., Brilke, S., Buchholz, A., Mazon, S. B., Chen, D., Chen, X., Dias, A., Dommen, J., Draper, D. C., Duplissy, J., Ehn, M., Finkenzeller, H., Fischer, L., Frege, C., Fuchs, C., Garmash, O., Gordon, H., Hakala, J., He, X., Heikkinen, L., Heinritzi, M., Helm, J. C., Hofbauer, V., Hoyle, C. R., Jokinen, T., Kangasluoma, J., Kerminen, V.-M., Kim, C., Kirkby, J., Kontkanen, J., Kürten, A., Lawler, M. J., Mai, H., Mathot, S., Mauldin, R. L., Molteni, U., Nichman, L., Nie, W., Nieminen, T., Ojdanic, A., Onnela, A., Passananti, M., Petäjä, T., Piel, F., Pospisilova, V., Quéléver, L. L. J., Rissanen, M. P., Rose, C., Sarnela, N., Schallhart, S., Schuchmann, S., Sengupta, K., Simon, M., Sipilä, M., Tauber, C., Tomé, A., Tröstl, J., Väisänen, O., Vogel, A. L., Volkamer, R., Wagner, A. C., Wang, M., Weitz, L., Wimmer, D., Ye, P., Ylisirniö, A., Zha, Q., Carslaw, K. S., Curtius, J., Donahue, N. M., Flagan, R. C., Hansel, A., Riipinen, I., Virtanen, A., Winkler, P. M., Baltensperger, U., Kulmala, M., and Worsnop, D. R.:
Multicomponent new particle formation from sulfuric acid, ammonia, and biogenic vapors,
Sci. Adv.,
4, eaau5363, <a href="https://doi.org/10.1126/sciadv.aau5363" target="_blank">https://doi.org/10.1126/sciadv.aau5363</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation>
Liu, J., Jiang, J., Zhang, Q., Deng, J., and Hao, J.:
A spectrometer for measuring particle size distributions in the range of 3&thinsp;nm to 10&thinsp;µm,
Front. Env. Sci. Eng.,
10, 63–72, <a href="https://doi.org/10.1007/s11783-014-0754-x" target="_blank">https://doi.org/10.1007/s11783-014-0754-x</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation>
Lu, Y., Yan, C., Fu, Y., Chen, Y., Liu, Y., Yang, G., Wang, Y., Bianchi, F., Chu, B., Zhou, Y., Yin, R., Baalbaki, R., Garmash, O., Deng, C., Wang, W., Liu, Y., Petäjä, T., Kerminen, V.-M., Jiang, J., Kulmala, M., and Wang, L.: A proxy for atmospheric daytime gaseous sulfuric acid concentration in urban Beijing, Atmos. Chem. Phys., 19, 1971–1983, <a href="https://doi.org/10.5194/acp-19-1971-2019" target="_blank">https://doi.org/10.5194/acp-19-1971-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>
Ma, F., Xie, H.-B., Elm, J., Shen, J., Chen, J., and Vehkamäki, H.:
Piperazine Enhancing Sulfuric Acid-Based New Particle Formation: Implications for the Atmospheric Fate of Piperazine,
Environ. Sci. Technol.,
53, 8785–8795, <a href="https://doi.org/10.1021/acs.est.9b02117" target="_blank">https://doi.org/10.1021/acs.est.9b02117</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>
Mauldin, R. L., Berndt, T., Sipila, M., Paasonen, P., Petaja, T., Kim, S., Kurten, T., Stratmann, F., Kerminen, V. M., and Kulmala, M.:
A new atmospherically relevant oxidant of sulphur dioxide,
Nature,
488, 193–196, <a href="https://doi.org/10.1038/nature11278" target="_blank">https://doi.org/10.1038/nature11278</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>40</label><mixed-citation>
McElreath, R.:
Statistical rethinking: A Bayesian course with examples in R and Stan,
Chapman and Hall/CRC, Taylor &amp; Francis Group
6000 Broken Sound Parkway NW, Suite 300
Boca Raton, FL 33487-2742, USA, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>41</label><mixed-citation>
Merikanto, J., Spracklen, D. V., Mann, G. W., Pickering, S. J., and Carslaw, K. S.: Impact of nucleation on global CCN, Atmos. Chem. Phys., 9, 8601–8616, <a href="https://doi.org/10.5194/acp-9-8601-2009" target="_blank">https://doi.org/10.5194/acp-9-8601-2009</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>42</label><mixed-citation>
Mikkonen, S., Romakkaniemi, S., Smith, J. N., Korhonen, H., Petäjä, T., Plass-Duelmer, C., Boy, M., McMurry, P. H., Lehtinen, K. E. J., Joutsensaari, J., Hamed, A., Mauldin III, R. L., Birmili, W., Spindler, G., Arnold, F., Kulmala, M., and Laaksonen, A.: A statistical proxy for sulphuric acid concentration, Atmos. Chem. Phys., 11, 11319–11334, <a href="https://doi.org/10.5194/acp-11-11319-2011" target="_blank">https://doi.org/10.5194/acp-11-11319-2011</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>43</label><mixed-citation>
Mikkonen, S., Németh, Z., Varga, V., Weidinger, T., Leinonen, V., Yli-Juuti, T., and Salma, I.: Decennial time trends and diurnal patterns of particle number concentrations in a Central European city between 2008 and 2018, Atmos. Chem. Phys. Discuss., <a href="https://doi.org/10.5194/acp-2020-305" target="_blank">https://doi.org/10.5194/acp-2020-305</a>, in review, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>44</label><mixed-citation>
Monkkonen, P., Koponen, I. K., Lehtinen, K. E. J., Uma, R., Srinivasan, D., Hameri, K., and Kulmala, M.:
Death of nucleation and Aitken mode particles: observations at extreme atmospheric conditions and their theoretical explanation,
J. Aerosol Sci.,
35, 781–787, <a href="https://doi.org/10.1016/j.jaerosci.2003.12.004" target="_blank">https://doi.org/10.1016/j.jaerosci.2003.12.004</a>, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>45</label><mixed-citation>
Mönkkönen, P., Koponen, I. K., Lehtinen, K. E. J., Hämeri, K., Uma, R., and Kulmala, M.: Measurements in a highly polluted Asian mega city: observations of aerosol number size distribution, modal parameters and nucleation events, Atmos. Chem. Phys., 5, 57–66, <a href="https://doi.org/10.5194/acp-5-57-2005" target="_blank">https://doi.org/10.5194/acp-5-57-2005</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>46</label><mixed-citation>
Nieminen, T., Kerminen, V.-M., Petäjä, T., Aalto, P. P., Arshinov, M., Asmi, E., Baltensperger, U., Beddows, D. C. S., Beukes, J. P., Collins, D., Ding, A., Harrison, R. M., Henzing, B., Hooda, R., Hu, M., Hőrrak, U., Kivekäs, N., Komsaare, K., Krejci, R., Kristensson, A., Laakso, L., Laaksonen, A., Leaitch, W. R., Lihavainen, H., Mihalopoulos, N., Németh, Z., Nie, W., O'Dowd, C., Salma, I., Sellegri, K., Svenningsson, B., Swietlicki, E., Tunved, P., Ulevicius, V., Vakkari, V., Vana, M., Wiedensohler, A., Wu, Z., Virtanen, A., and Kulmala, M.: Global analysis of continental boundary layer new particle formation based on long-term measurements, Atmos. Chem. Phys., 18, 14737–14756, <a href="https://doi.org/10.5194/acp-18-14737-2018" target="_blank">https://doi.org/10.5194/acp-18-14737-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>47</label><mixed-citation>
Novelli, A., Hens, K., Tatum Ernest, C., Martinez, M., Nölscher, A. C., Sinha, V., Paasonen, P., Petäjä, T., Sipilä, M., Elste, T., Plass-Dülmer, C., Phillips, G. J., Kubistin, D., Williams, J., Vereecken, L., Lelieveld, J., and Harder, H.: Estimating the atmospheric concentration of Criegee intermediates and their possible interference in a FAGE-LIF instrument, Atmos. Chem. Phys., 17, 7807–7826, <a href="https://doi.org/10.5194/acp-17-7807-2017" target="_blank">https://doi.org/10.5194/acp-17-7807-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>48</label><mixed-citation>
Petäjä, T., Mauldin, III, R. L., Kosciuch, E., McGrath, J., Nieminen, T., Paasonen, P., Boy, M., Adamov, A., Kotiaho, T., and Kulmala, M.: Sulfuric acid and OH concentrations in a boreal forest site, Atmos. Chem. Phys., 9, 7435–7448, <a href="https://doi.org/10.5194/acp-9-7435-2009" target="_blank">https://doi.org/10.5194/acp-9-7435-2009</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>49</label><mixed-citation>
Pikridas, M., Vrekoussis, M., Sciare, J., Kleanthous, S., Vasiliadou, E., Kizas, C., Savvides, C., and Mihalopoulos, N.:
Spatial and temporal (short and long-term) variability of submicron, fine and sub-10&thinsp;µm particulate matter (PM<sub>1</sub>, PM<sub>2.5</sub>, PM<sub>10</sub>) in Cyprus,
Atmos. Environ.,
191, 79–93, <a href="https://doi.org/10.1016/j.atmosenv.2018.07.048" target="_blank">https://doi.org/10.1016/j.atmosenv.2018.07.048</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>50</label><mixed-citation>
Rinne, J., Ruuskanen, T. M., Reissell, A., Taipale, R., Hakola, H., and Kulmala, M.:
On-line PTR-MS measurements of atmospheric concentrations of volatile organic compounds in a European boreal forest ecosystem,
Boreal Environ. Res.,
10, 425–436, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>51</label><mixed-citation>
Rohrer, F. and Berresheim, H.:
Strong correlation between levels of tropospheric hydroxyl radicals and solar ultraviolet radiation,
Nature,
442, 184–187, <a href="https://doi.org/10.1038/nature04924" target="_blank">https://doi.org/10.1038/nature04924</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>52</label><mixed-citation>
Salma, I. and Németh, Z.: Dynamic and timing properties of new aerosol particle formation and consecutive growth events, Atmos. Chem. Phys., 19, 5835–5852, <a href="https://doi.org/10.5194/acp-19-5835-2019" target="_blank">https://doi.org/10.5194/acp-19-5835-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>53</label><mixed-citation>
Salma, I., Németh, Z., Kerminen, V.-M., Aalto, P., Nieminen, T., Weidinger, T., Molnár, Á., Imre, K., and Kulmala, M.: Regional effect on urban atmospheric nucleation, Atmos. Chem. Phys., 16, 8715–8728, <a href="https://doi.org/10.5194/acp-16-8715-2016" target="_blank">https://doi.org/10.5194/acp-16-8715-2016</a>, 2016a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>54</label><mixed-citation>
Salma, I., Németh, Z., Weidinger, T., Kovács, B., and Kristóf, G.: Measurement, growth types and shrinkage of newly formed aerosol particles at an urban research platform, Atmos. Chem. Phys., 16, 7837–7851, <a href="https://doi.org/10.5194/acp-16-7837-2016" target="_blank">https://doi.org/10.5194/acp-16-7837-2016</a>, 2016b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>55</label><mixed-citation>
Sarnela, N., Jokinen, T., Nieminen, T., Lehtipalo, K., Junninen, H., Kangasluoma, J., Hakala, J., Taipale, R., Schobesberger, S., Sipila, M., Larnimaa, K., Westerholm, H., Heijari, J., Kerminen, V. M., Petaja, T., and Kulmala, M.:
Sulphuric acid and aerosol particle production in the vicinity of an oil refinery,
Atmos. Environ.,
119, 156–166, <a href="https://doi.org/10.1016/j.atmosenv.2015.08.033" target="_blank">https://doi.org/10.1016/j.atmosenv.2015.08.033</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>56</label><mixed-citation>
Sihto, S.-L., Kulmala, M., Kerminen, V.-M., Dal Maso, M., Petäjä, T., Riipinen, I., Korhonen, H., Arnold, F., Janson, R., Boy, M., Laaksonen, A., and Lehtinen, K. E. J.: Atmospheric sulphuric acid and aerosol formation: implications from atmospheric measurements for nucleation and early growth mechanisms, Atmos. Chem. Phys., 6, 4079–4091, <a href="https://doi.org/10.5194/acp-6-4079-2006" target="_blank">https://doi.org/10.5194/acp-6-4079-2006</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>57</label><mixed-citation>
Sipilä, M., Berndt, T., Petäjä, T., Brus, D., Vanhanen, J., Stratmann, F., Patokoski, J., Mauldin, R. L., Hyvärinen, A.-P., Lihavainen, H., and Kulmala, M.:
The Role of Sulfuric Acid in Atmospheric Nucleation,
Science,
327, 1243–1246, <a href="https://doi.org/10.1126/science.1180315" target="_blank">https://doi.org/10.1126/science.1180315</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>58</label><mixed-citation>
Sipilä, M., Jokinen, T., Berndt, T., Richters, S., Makkonen, R., Donahue, N. M., Mauldin III, R. L., Kurtén, T., Paasonen, P., Sarnela, N., Ehn, M., Junninen, H., Rissanen, M. P., Thornton, J., Stratmann, F., Herrmann, H., Worsnop, D. R., Kulmala, M., Kerminen, V.-M., and Petäjä, T.: Reactivity of stabilized Criegee intermediates (sCIs) from isoprene and monoterpene ozonolysis toward SO<sub>2</sub> and organic acids, Atmos. Chem. Phys., 14, 12143–12153, <a href="https://doi.org/10.5194/acp-14-12143-2014" target="_blank">https://doi.org/10.5194/acp-14-12143-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>59</label><mixed-citation>
Spracklen, D. V., Carslaw, K. S., Kulmala, M., Kerminen, V. M., Sihto, S. L., Riipinen, I., Merikanto, J., Mann, G. W., Chipperfield, M. P., and Wiedensohler, A.:
Contribution of particle formation to global cloud condensation nuclei concentrations,
Geophy. Res. Lett.,
35, L06808, <a href="https://doi.org/10.1029/2007GL033038" target="_blank">https://doi.org/10.1029/2007GL033038</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>60</label><mixed-citation>
Spracklen, D. V., Carslaw, K. S., Merikanto, J., Mann, G. W., Reddington, C. L., Pickering, S., Ogren, J. A., Andrews, E., Baltensperger, U., Weingartner, E., Boy, M., Kulmala, M., Laakso, L., Lihavainen, H., Kivekäs, N., Komppula, M., Mihalopoulos, N., Kouvarakis, G., Jennings, S. G., O'Dowd, C., Birmili, W., Wiedensohler, A., Weller, R., Gras, J., Laj, P., Sellegri, K., Bonn, B., Krejci, R., Laaksonen, A., Hamed, A., Minikin, A., Harrison, R. M., Talbot, R., and Sun, J.: Explaining global surface aerosol number concentrations in terms of primary emissions and particle formation, Atmos. Chem. Phys., 10, 4775–4793, <a href="https://doi.org/10.5194/acp-10-4775-2010" target="_blank">https://doi.org/10.5194/acp-10-4775-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>61</label><mixed-citation>
Taipale, R., Ruuskanen, T. M., Rinne, J., Kajos, M. K., Hakola, H., Pohja, T., and Kulmala, M.: Technical Note: Quantitative long-term measurements of VOC concentrations by PTR-MS – measurement, calibration, and volume mixing ratio calculation methods, Atmos. Chem. Phys., 8, 6681–6698, <a href="https://doi.org/10.5194/acp-8-6681-2008" target="_blank">https://doi.org/10.5194/acp-8-6681-2008</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib62"><label>62</label><mixed-citation>
Weber, R. J., Marti, J. J., McMurry, P. H., Eisele, F. L., Tanner, D. J., and Jefferson, A.:
Measured Atmospheric New Particle Formation Rates: Implications For Nucleation Mechanisms,
Chem. Eng. Commun.,
151, 53–64, <a href="https://doi.org/10.1080/00986449608936541" target="_blank">https://doi.org/10.1080/00986449608936541</a>, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib63"><label>63</label><mixed-citation>
Yan, C., Dada, L., Rose, C., Jokinen, T., Nie, W., Schobesberger, S., Junninen, H., Lehtipalo, K., Sarnela, N., Makkonen, U., Garmash, O., Wang, Y., Zha, Q., Paasonen, P., Bianchi, F., Sipilä, M., Ehn, M., Petäjä, T., Kerminen, V.-M., Worsnop, D. R., and Kulmala, M.: The role of H<sub>2</sub>SO<sub>4</sub> − NH<sub>3</sub> anion clusters in ion-induced aerosol nucleation mechanisms in the boreal forest, Atmos. Chem. Phys., 18, 13231–13243, <a href="https://doi.org/10.5194/acp-18-13231-2018" target="_blank">https://doi.org/10.5194/acp-18-13231-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib64"><label>64</label><mixed-citation>
Yang, D., Zhang, S., Niu, T., Wang, Y., Xu, H., Zhang, K. M., and Wu, Y.: High-resolution mapping of vehicle emissions of atmospheric pollutants based on large-scale, real-world traffic datasets, Atmos. Chem. Phys., 19, 8831–8843, <a href="https://doi.org/10.5194/acp-19-8831-2019" target="_blank">https://doi.org/10.5194/acp-19-8831-2019</a>, 2019.

</mixed-citation></ref-html>
<ref-html id="bib1.bib65"><label>65</label><mixed-citation>
Yao, L., Garmash, O., Bianchi, F., Zheng, J., Yan, C., Kontkanen, J., Junninen, H., Mazon, S. B., Ehn, M., Paasonen, P., Sipilä, M., Wang, M., Wang, X., Xiao, S., Chen, H., Lu, Y., Zhang, B., Wang, D., Fu, Q., Geng, F., Li, L., Wang, H., Qiao, L., Yang, X., Chen, J., Kerminen, V.-M., Petäjä, T., Worsnop, D. R., Kulmala, M., and Wang, L.:
Atmospheric new particle formation from sulfuric acid and amines in a Chinese megacity,
Science,
361, 278–281, <a href="https://doi.org/10.1126/science.aao4839" target="_blank">https://doi.org/10.1126/science.aao4839</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib66"><label>66</label><mixed-citation>
Yao, L., Fan, X., Yan, C., Kurtén, T., Daellenbach, K. R., Wang, Y., Guo, Y., Li, C., Dada, L., Cai, J., Jun, T. Y., Zha, Q., Du, W., Yu, M., Zheng, F., Zhou, Y., Chan, T., Shen, J., Kujansuu, J. T., Kangasluoma, J., Jiang, J., Li, H., Wang, L., Worsnop, D. R., He, H., Petäjä, T., Kerminen, V.-M., Liu, Y., Chu, B., Kulmala, M., and Bianchi, F.:
Unprecedented ambient sulphur trioxide (SO<sub>3</sub>) detection: possible formation mechanism and atmospheric implications,
Environ. Sci. Technol. Lett.,
accepted, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib67"><label>67</label><mixed-citation>
Zhang, R., Khalizov, A., Wang, L., Hu, M., and Xu, W.:
Nucleation and growth of nanoparticles in the atmosphere,
Chem. Rev.,
112, 1957–2011, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib68"><label>68</label><mixed-citation>
Zhang, W., Tong, S., Ge, M., An, J., Shi, Z., Hou, S., Xia, K., Qu, Y., Zhang, H., Chu, B., Sun, Y., and He, H.:
Variations and sources of nitrous acid (HONO) during a severe pollution episode in Beijing in winter 2016,
Sci. Total Environ.,
648, 253–262, <a href="https://doi.org/10.1016/j.scitotenv.2018.08.133" target="_blank">https://doi.org/10.1016/j.scitotenv.2018.08.133</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib69"><label>69</label><mixed-citation>
Zhou, Y., Dada, L., Liu, Y., Fu, Y., Kangasluoma, J., Chan, T., Yan, C., Chu, B., Daellenbach, K. R., Bianchi, F., Kokkonen, T. V., Liu, Y., Kujansuu, J., Kerminen, V.-M., Petäjä, T., Wang, L., Jiang, J., and Kulmala, M.: Variation of size-segregated particle number concentrations in wintertime Beijing, Atmos. Chem. Phys., 20, 1201–1216, <a href="https://doi.org/10.5194/acp-20-1201-2020" target="_blank">https://doi.org/10.5194/acp-20-1201-2020</a>, 2020.
</mixed-citation></ref-html>--></article>
