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<!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" article-type="research-article"><?xmltex \bartext{Measurement report}?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">ACP</journal-id><journal-title-group>
    <journal-title>Atmospheric Chemistry and Physics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1680-7324</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/acp-23-5699-2023</article-id><title-group><article-title>Measurement Report: Wintertime new particle <?xmltex \hack{\break}?> formation in the rural area of the North China Plain – influencing factors and possible formation mechanism</article-title><alt-title>Wintertime new particle formation in the rural area of the North China Plain</alt-title>
      </title-group><?xmltex \runningtitle{Wintertime new particle formation in the rural area of the North China Plain}?><?xmltex \runningauthor{J.~Hong et al.}?>
      <contrib-group>
        <contrib contrib-type="author" equal-contrib="yes" corresp="yes" rid="aff1 aff2">
          <name><surname>Hong</surname><given-names>Juan</given-names></name>
          <email>juanhong0108@jnu.edu.cn</email>
        </contrib>
        <contrib contrib-type="author" equal-contrib="yes" corresp="no" rid="aff1 aff2">
          <name><surname>Tang</surname><given-names>Min</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Wang</surname><given-names>Qiaoqiao</given-names></name>
          <email>qwang@jnu.edu.cn</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Ma</surname><given-names>Nan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Zhu</surname><given-names>Shaowen</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Zhang</surname><given-names>Shaobin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Pan</surname><given-names>Xihao</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Xie</surname><given-names>Linhong</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Li</surname><given-names>Guo</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0350-9879</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Kuhn</surname><given-names>Uwe</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <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>Tao</surname><given-names>Jiangchuan</given-names></name>
          
        <ext-link>https://orcid.org/0009-0007-7118-8070</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Kuang</surname><given-names>Ye</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4813-9784</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>He</surname><given-names>Yao</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Xu</surname><given-names>Wanyun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Cai</surname><given-names>Runlong</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Zhou</surname><given-names>Yaqing</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Wang</surname><given-names>Zhibin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Zhou</surname><given-names>Guangsheng</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yuan</surname><given-names>Bin</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3041-0329</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Cheng</surname><given-names>Yafang</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4912-9879</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Su</surname><given-names>Hang</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4889-1669</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Institute for Environmental and Climate Research, Jinan University, Guangzhou, Guangdong 511443, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Guangdong–Hong Kong–Macau Joint Laboratory of Collaborative Innovation for Environmental Quality, Guangzhou, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Multiphase Chemistry Department, Max Planck Institute for Chemistry, 55128 Mainz, Germany</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>School of Atmospheric Sciences, Joint International Research
Laboratory of Atmospheric and Earth System Sciences, Nanjing University,
Nanjing, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Hebei Gucheng, Agrometeorology, National Observation and Research
Station, <?xmltex \hack{\break}?> Chinese Academy of Meteorological Sciences, Beijing 100081, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Institute for Atmospheric and Earth System Research/Physics, Faculty of Science, <?xmltex \hack{\break}?> University of Helsinki, Helsinki 00014, Finland</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>College of Environmental and Resource Sciences, Zhejiang University, Zhejiang Provincial Key Laboratory of Organic Pollution Process and Control, Hangzhou 310058, China</institution>
        </aff><author-comment content-type="econtrib"><p>These authors contributed equally to this work.</p></author-comment>
      </contrib-group>
      <author-notes><corresp id="corr1">Juan Hong (juanhong0108@jnu.edu.cn) and Qiaoqiao Wang (qwang@jnu.edu.cn)</corresp></author-notes><pub-date><day>22</day><month>May</month><year>2023</year></pub-date>
      
      <volume>23</volume>
      <issue>10</issue>
      <fpage>5699</fpage><lpage>5713</lpage>
      <history>
        <date date-type="received"><day>16</day><month>November</month><year>2022</year></date>
           <date date-type="rev-request"><day>15</day><month>December</month><year>2022</year></date>
           <date date-type="rev-recd"><day>12</day><month>April</month><year>2023</year></date>
           <date date-type="accepted"><day>27</day><month>April</month><year>2023</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2023 </copyright-statement>
        <copyright-year>2023</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e326">The high concentration of fine particles and gaseous pollutants makes polluted areas, such as the urban setting of North China Plain (NCP) of China, a different environment for new particle formation (NPF) compared to many clean regions. Such conditions also hold for other polluted environments in this region (for instance, the rural area of NCP), yet the underlying mechanisms for NPF remain less understood, owing to the limited observations of particles in the sub<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm range. Comprehensive measurements, particularly covering the particle number size distribution down to 1.3 nm, were conducted at a rural background site of Gucheng (GC) in the North China Plain (NCP) from 12 November to 24 December 2018. In total, five NPF events during the 39 effective days of measurements for the campaign were identified, with the mean particle nucleation rate (<inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and growth rate (GR<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">1.3</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">2.4</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula>) being 22.0 cm<inline-formula><mml:math id="M4" 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> s<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 3.9 nm h<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively. During these 5 d, NPF concurrently occurred at an urban site in Beijing. Sharing similar sources and transport paths of air masses arriving at our site to that of urban Beijing, we hypothesize that NPF events during these days in this region might be a regional phenomenon. The simultaneous occurrence of NPF in both places implies that H<inline-formula><mml:math id="M7" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M8" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>-amine nucleation, concluded for urban Beijing there, could probably be the dominating mechanism for NPF at our rural site. The higher concentration of sulfuric acid during many non-event days compared to that of event days indicates that the content of sulfuric acid may not necessarily lead to NPF events under current atmosphere. Only when the condensation sink or coagulation sink was significantly lowered, atmospheric NPF occurred, implying that condensation sinks (CSs) and coagulation sinks (CoagSs) are the dominating factors controlling the occurrence of NPF for the present rural environment of the NCP, which is quite similar to the feature seen in urban Beijing.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National Natural Science Foundation of China</funding-source>
<award-id>42175117</award-id>
<award-id>41907182</award-id>
<award-id>41877303</award-id>
<award-id>91644218</award-id>
</award-group>
<award-group id="gs2">
<funding-source>Central Universities in China</funding-source>
<award-id>21621105</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

<?pagebreak page5700?><sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e428">Atmospheric new particle formation (NPF) is a major source of the global
particles in terms of number concentration and size distribution (Kulmala et al., 2004) and is considered to contribute up to half of the global cloud condensation nuclei (CCN) budget in the lower troposphere (Spracklen et al., 2006; Dunne et al., 2016). In general, NPF consists of two consecutive processes, namely (a) the formation or nucleation of molecular clusters by low-volatile gaseous substances and (b) their subsequent growth to detectable sizes or even larger – at which sizes these particles may act as CCN or contribute to the particle mass concentration (Kulmala et al., 2000; Zhang et al., 2012).</p>
      <p id="d1e431">Numerous laboratory measurements and field studies have shown that sulfuric
acid molecules (H<inline-formula><mml:math id="M9" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>) are one of the key precursors to forming
molecular clusters for nucleation (Nieminen et al., 2010; Sipilä et al., 2010; Kirkby et al., 2011; Riccobono et al., 2014; Stolzenburg et al., 2020). However, these H<inline-formula><mml:math id="M11" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M12" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> clusters relevant to atmospheric nucleation are typically quite small (i.e., with diameters below 1.5 nm), making the detection efficiency of traditional instruments specific for NPF unsatisfactory (Kulmala, 2013). This led to large uncertainties in the measured formation rate of newly formed particles and thus precise measurements of these clusters or particles down to sub<inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm were required. Recently, progress such as the use of a particle size magnifier (PSM; Vanhanen et al., 2011; Xiao et al., 2015), a neutral cluster and air ion spectrometer (NAIS; Mirme and Mirme, 2013), and a chemical ionization–atmospheric pressure interface time-of-flight mass spectrometer (CI-APi-TOF; Jokinen et al., 2012) have made it possible to directly measure the number concentration of clusters in the 1–3 nm size range. Benefitting from these novel techniques, observations have found that the growth of H<inline-formula><mml:math id="M14" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M15" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> clusters would be significantly promoted after being stabilized by other precursors like amines, ammonia, or iodine species (Berndt et al., 2010; Kirkby et al., 2011; Almeida et al., 2013; Riccobono et al., 2014; Kürten et al., 2016; Sipilä et al., 2010). Furthermore, oxidation products from volatile organic compounds (for instance, highly oxidized organic compounds) were suggested to be important contributors to atmospheric nucleation (Ehn et al., 2014; Bianchi et al., 2016; Kirkby et al., 2016; Tröstl et al., 2016).</p>
      <p id="d1e499">The North China Plain (NCP) of China has been suffering heavily from the
highly complex air pollution for decades (Ma et al., 2016; Shen et al., 2018a, b; Zhang et al., 2020), owing to the high emissions or formation of different pollutants such as SO<inline-formula><mml:math id="M16" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, NH<inline-formula><mml:math id="M17" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, volatile organic compounds (VOCs), and fine particles from various sources (Guo et al., 2014; Zhang et al., 2015). Due to the high concentration of pre-existing particles, previous studies considered that, in the NCP, less NPF would occur, as the newly formed particles would be scavenged much faster before growing. By contrast, atmospheric NPF was still frequently observed in this region (Chu et al., 2019; Deng et al., 2020; Cai et al., 2021b), occurring more often than theoretically predicted (Kulmala et al., 2014) and indicating that the underlying mechanisms for NPF in this area might be different, meaning that those mechanisms previously found for other environments might not be completely applicable. The higher concentration of these gaseous precursors makes this region a unique condition for NPF compared to relatively clean environments (Kulmama et al., 2016; Yu et al., 2017; Wang et al., 2017), further supporting the hypothesis of different formation mechanisms and thereby distinct features of NPF events in this region. These doubts concerning NPF in the NCP, however, still remain to be elucidated due to limitations of comprehensive measurements, particularly for rural areas of the NCP, where observations regarding NPF were even more rare.</p>
      <p id="d1e520">In addition, with respect to those existing studies concerning NPF in the
NCP, they mainly focused on the measurements of particles beyond 3 nm. Without applicable instruments, observations of new particles down to sub<inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> m were still quite limited (Fang et al., 2020; Zhou et al., 2020), causing large uncertainties in the measured characteristics of NPF for the current region. To fill the gap of the measurements of particles or clusters in the size range of 1–3 nm and further advance our understanding of NPF in this region, particularly in the rural area of NCP, we conducted a comprehensive measurement campaign at a rural background site in the NCP from 12 November to 24 December 2018. By obtaining the particle number size distribution over a wide diameter range (1.3 nm–10 <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m), we aimed to investigate the characteristics of NPF events at the rural site in NCP
during wintertime, find out which factors govern the occurring of NPF compared to other regions of NCP such as the urban areas, and explore the
potential mechanisms for NPF in this area.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Experiment</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Field measurements site</title>
      <p id="d1e556">The measurements were conducted at Gucheng (GC) site (39<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>09<inline-formula><mml:math id="M21" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>01.1<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 115<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>44<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>02.6<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> E), situated at an Ecological and Agricultural Meteorology Station (39<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>09<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> N, 115<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>44<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> E) of the Chinese Academy of Meteorological Sciences from 12 November to 24 December 2018. The station is located in Dingxing county, Baoding city, Hebei province, China (as seen in Fig. 1), and surrounded by agricultural fields and sporadically distributed villages. Being far from the urban and industrial emission areas, this site can be treated as a representative regional site in the northern part of NCP. More details about this site can be found in Lin et al. (2009) and Shen et al. (2018a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e658"><bold>(a, b)</bold> The geographical location of the site (red
dot and circled; © Google Maps) where our field measurements were carried out. <bold>(c)</bold> The measurement containers in which the
sampling instruments were set up.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/5699/2023/acp-23-5699-2023-f01.jpg"/>

        </fig>

<?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page5701?><sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Measurements</title>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Particle number size distribution (PNSD) measurement</title>
      <p id="d1e689">The aerosol sampling inlet was located on the rooftop of a measurement
container, where room temperature was maintained at 22<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> C (Fig. 1c).
The aerosol was sampled via a low-flow PM<inline-formula><mml:math id="M31" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> cyclone inlet, passed through a Nafion dryer, and directed to different instruments through stainless steel or conductive black tubing using an isokinetic flow splitter. The particle number size distribution (PNSD) of the aerosol particles with
diameters from 10 to 10 000 nm was measured by using a scanning mobility
particle sizer (SMPS; TSI 3938) and an aerodynamic particle sizer (APS; TSI 3321) at a time resolution of around 5 min. The SMPS consisted of an electrostatic classifier (TSI 3080) and a condensation particle counter (CPC; TSI 3772).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><?xmltex \opttitle{Sub$-3$\,nm particle number concentration measurement}?><title>Sub<inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm particle number concentration measurement</title>
      <p id="d1e729">Sub<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm particles were measured with an Airmodus A11 nano condensation nucleus counter system (nCNC), consisting of a particle size magnifier
(PSM; A10) and a butanol condensation particle counter (CPC; A20; Vanhanen et al., 2011). The Airmodus PSM uses diethylene glycol as the working fluid to activate and grow nano-sized particles. Specifically, the PSM was operated under the scanning mode so that the diethylene glycol flow varied between 0.1 and 1.3 L min<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Thus, the number size distribution of five different size bins (i.e., 1.3–1.4, 1.4–1.6, 1.6–1.9, 1.9–2.4, and 2.4–3.7 nm) was obtained. Owing to the data quality, only the data of the former four size bins were used in this study. During this campaign, the duration of each scan was completed within around 240 s.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><?xmltex \opttitle{Pollutant gases, PM${}_{{2.5}}$, and meteorological parameter measurement}?><title>Pollutant gases, PM<inline-formula><mml:math id="M35" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, and meteorological parameter measurement</title>
      <p id="d1e772">The concentration of trace gases, including SO<inline-formula><mml:math id="M36" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, O<inline-formula><mml:math id="M37" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, CO, and NO<inline-formula><mml:math id="M38" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>, was measured continuously during this campaign using different Thermo Fisher analyzers (43i-TLE, 49i, 48i, and 42i), respectively, at a time resolution of 1 min. The concentration of oxygenated volatile organic compounds (OVOCs) was measured with an iodide-adduct long time-of-flight
chemical ionization mass spectrometer (I-CIMS; Aerodyne Research Inc., USA) at a time resolution of 10–30 s for the current study.</p>
      <p id="d1e802">In addition, ambient meteorological conditions, such as wind speed, wind
direction, temperature, relative humidity,<?pagebreak page5702?> and solar radiation, were also
regularly measured in another building, which is located about 20 m to the southwest of the container, at the same observational site.</p>
      <p id="d1e805">Furthermore, in order to investigate the influence of the origins and
transport paths of air parcels to the local atmospheric compositions during
NPF events, 72 h back-trajectories of air masses arriving at 100 m a.g.l. (above ground level) at our GC site were analyzed using the HYbrid Single-Particle Lagrangian Integrated Trajectory (HYSPLIT) model for the classified event days.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Data processing</title>
<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><?xmltex \opttitle{Formation rate ($J_{{D_{\mathrm{p}}}}$) and growth rate~(GR)}?><title>Formation rate (<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) and growth rate (GR)</title>
      <p id="d1e840"><inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> defines the formation rate of atmospheric particles at a certain diameter (<inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and can be calculated, according to Kulmala et al. (2012), as follows:
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M42" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{8.9}{8.9}\selectfont$\displaystyle}?><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:msub><mml:mi>N</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">CoagS</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:msub><mml:mi mathvariant="normal">GR</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>×</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:msub><?xmltex \hack{$\egroup}?><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M43" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> is the particle number concentration between the diameter
dp<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and dp<inline-formula><mml:math id="M45" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> (denoted as <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), CoagS is the coagulation sink of particles, and GR is the particle growth rate out of the selected size bin.</p>
      <p id="d1e1014">In our study, we used two independent methods to calculate GR. One is the
maximum concentration method (Kulmala et al., 2012), which is mainly for the PSM data. The other is based on the variation in the geometric mean diameters of the particle number size distribution, which is derived by fitting the PNSD into two or three log-normal modes using an automatic algorithm (DO-FIT model; Hussein et al., 2005), which is mainly for SMPS data.
              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M47" display="block"><mml:mrow><mml:mi mathvariant="normal">GR</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="normal">ddp</mml:mi><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:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">dp</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="normal">dp</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">dp</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where dp<inline-formula><mml:math id="M48" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> and dp<inline-formula><mml:math id="M49" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> were particle diameters at time <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, respectively.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Condensation sink (CS) and coagulation sink (CoagS)</title>
      <p id="d1e1130">The CS describes how fast the low-volatility molecules condense onto pre-existing aerosols and can be expressed as follows (Kulmala et al., 2012):
              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M52" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9.5}{9.5}\selectfont$\displaystyle}?><mml:mi mathvariant="normal">CS</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>D</mml:mi><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mrow><mml:msub><mml:mi mathvariant="normal">dp</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">dp</mml:mi></mml:mrow></mml:msub><mml:mi mathvariant="normal">dp</mml:mi><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">dp</mml:mi></mml:msub><mml:mi mathvariant="normal">ddp</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:mi>D</mml:mi><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi mathvariant="normal">dp</mml:mi></mml:munder><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">dp</mml:mi></mml:mrow></mml:msub><mml:mi mathvariant="normal">dp</mml:mi><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">dp</mml:mi></mml:msub><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M53" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> is the diffusion coefficient of the condensing vapor, which is usually referred to sulfuric acid, and <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">dp</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the mass flux transition correction factor.</p>
      <p id="d1e1237"><?xmltex \hack{\newpage}?>The CoagS represents how fast the freshly formed particles are lost to pre-existing particles through coagulation and can be calculated as follows:
              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M55" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9.1}{9.1}\selectfont$\displaystyle}?><mml:msub><mml:mi mathvariant="normal">CoagS</mml:mi><mml:mi mathvariant="normal">dp</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo movablelimits="false">∫</mml:mo><mml:mi>K</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mi>n</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mi mathvariant="normal">ddp</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>≅</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:msup><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="normal">dp</mml:mi></mml:mrow><mml:mrow><mml:msup><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="normal">max</mml:mi></mml:mrow></mml:munderover><mml:mi>K</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mi>N</mml:mi><mml:msup><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>′</mml:mo></mml:msup><?xmltex \hack{$\egroup}?><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>,</mml:mo><mml:msup><mml:mi mathvariant="normal">dp</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the collision efficiency between
particles at the diameter from dp to dp<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <label>2.3.3</label><title>Sulfuric acid proxy (SA proxy)</title>
      <p id="d1e1375">Sulfuric acid (SA) was considered to be one of the key precursors responsible for particle nucleation in the atmosphere. However, no direct measurement for the concentration of SA was available in current study. We therefore used a proxy variable to substitute the concentration of SA, as SA is mainly produced by the oxidation of SO<inline-formula><mml:math id="M58" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> by OH radicals, which can be approximated by the UV-B intensity (Petäjä et al., 2009). Thus, the proxy concentration of SA can be calculated, by Lu et al. (2019), as follows:
              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M59" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">SA</mml:mi><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mi mathvariant="normal">proxy</mml:mi></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0013</mml:mn><mml:mo>⋅</mml:mo><mml:msup><mml:mi mathvariant="normal">UVB</mml:mi><mml:mn mathvariant="normal">0.13</mml:mn></mml:msup><mml:mo>⋅</mml:mo><mml:msup><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:mn mathvariant="normal">0.40</mml:mn></mml:msup><mml:mo>⋅</mml:mo><mml:msup><mml:mi mathvariant="normal">CS</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.17</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>⋅</mml:mo><mml:mfenced open="(" close=")"><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:mn mathvariant="normal">0.44</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="[" close="]"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">0.41</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
</sec>
<sec id="Ch1.S2.SS3.SSS4">
  <label>2.3.4</label><title>Classification of NPF event</title>
      <p id="d1e1475">The days of the NPF events were classified according to the method proposed by Dal Maso et al. (2005) and Kulmala et al. (2012), in which (i) a burst in the concentration of sub<inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm particles or clusters was observed, and (ii) these particles had a continuous growth over a time span of hours (e.g., usually more than 10 h). If no clear growth of these newly formed particles (sub<inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm particles) can be identified, then the day was classified as an undefined day. The days without both the burst of sub<inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm particles and their subsequent growth were considered to be non-event days.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1510">Time series of <bold>(a)</bold> wind speed and wind direction, <bold>(b)</bold> temperature (<inline-formula><mml:math id="M63" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>), and relative humidity (RH), <bold>(c)</bold> total particle surface and volume concentration calculated by using PNSD data, <bold>(d)</bold> measured PNSD in the size range of 10–800 nm, <bold>(e)</bold> particle number concentration in the range of 1.3 to 2.4 nm, and H<inline-formula><mml:math id="M64" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M65" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> proxy concentration during the entire measurement period (12 November–24 December 2018). The white portion indicates that no data were available due to instrument maintenance or power failure. Note that the white portion in the PNSD in the size range of 10–15 nm, indicating no available data, is due to technical problems with our SMPS system; therefore, data for that time period from a parallel SMPS covering sizes of 15–800 nm were used instead.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/5699/2023/acp-23-5699-2023-f02.png"/>

          </fig>

</sec>
<sec id="Ch1.S2.SS3.SSS5">
  <label>2.3.5</label><title>Indicator for the occurrence of NPF</title>
      <?pagebreak page5703?><p id="d1e1569">Previously, McMurry et al. (2005) proposed a dimensionless criterion, <inline-formula><mml:math id="M66" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula>, to predict the occurrence of NPF events in the atmosphere. After being validated in diverse atmospheric environments (Kuang et al., 2010; Cai et al., 2017), <inline-formula><mml:math id="M67" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> has been used to investigate the governing factors for NPF events under typical atmospheric conditions. Recently, Cai et al. (2021a) proposed a new indicator, <inline-formula><mml:math id="M68" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>, on the basis of <inline-formula><mml:math id="M69" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula>, which only considered H<inline-formula><mml:math id="M70" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M71" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> to be driving the growth. The new indicator was calculated by further taking into account the condensation of other species (for instance, amines) and has been suggested to be a good quantitative representation for the occurrence of NPF after comparing with <inline-formula><mml:math id="M72" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> for NPF events observed in urban Beijing (Deng et al., 2020). Detailed information for the calculation of <inline-formula><mml:math id="M73" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> can be found in Cai et al. (2021a).</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>General characteristics of NPF at GC site</title>
      <p id="d1e1650">Figure 2 shows the time series of meteorological parameters (Fig. 2a shows the wind speed and direction; Fig. 2b shows the temperature and relative humidity) and aerosol properties (Fig. 2c shows the total surface and volume concentration; Fig. 2d and e show the PNSD in the size range of 10 to 800 nm and particle number concentration in the range of 1.3 to 2.4 nm) during this field campaign. During our study, wind speed was typically quite low, with an average of 1.18 m s<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, indicating stagnant meteorological conditions for the limited dilution of air pollutants at the current site. The temperature and relative humidity (RH) show opposite diurnal variations over the observational period, with the highest temperature and lowest RH during daytime and vice versa during nighttime. The observed time series of the concentration of different trace gases during current study is shown in Fig. S1 in the Supplement. To be specific, the campaign-averaged concentration of CO, O<inline-formula><mml:math id="M75" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M76" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>, and SO<inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> was 1394, 7, 83, and 10 ppb, respectively.</p>
      <p id="d1e1692"><?xmltex \hack{\newpage}?>According to the PNSD and PSM data, 5 d, with 4 d having a significant burst of sub<inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm clusters (as shown in Fig. 2e), were classified as being NPF events occurring during the total experimental period. It has to be noted that, on the day of 18 November, though PSM data were not available due to technical issues, clear growth of nucleation mode particles with a typical banana-shaped PNSD was observed and lasted for more than 12 h. These particles under the growth of such a long time should not be from traffic emissions or transported particles. Therefore, it was also classified as an event day in our study. Considering all of these five NPF events, this corresponds to an NPF frequency of 12.8 %, which was lower than that at an urban site (i.e., Beijing) in the same region during the same season (Shen et al., 2018b found 25.8 %; Deng et al., 2020 found 51.4 %). Similar findings were also observed in Yue et al. (2009) and Wang et al. (2013) who found that NPF frequencies were higher at the Beijing urban site than at the corresponding regional background or rural site. Yue et al. (2009) and Wang et al. (2013) attributed this to the higher pollution level and correspondingly higher precursor content in the urban cities, leading to stronger NPF events there.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1708">A case of an NPF event on 7 December during this field campaign. Time series of <bold>(a)</bold> wind speed and wind directions and <bold>(b)</bold> the PNSD in the size range of 10–450 nm (the dotted white line represents the size with diameter at 25, 50, and 100 nm; black line represents the polynomial fit of the measured PNSD). <bold>(c)</bold> The particle number concentration of nucleation mode (9–25 nm) and CS. <bold>(d)</bold> The number concentration of sub<inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm clusters and predicted concentration of sulfuric acid.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/5699/2023/acp-23-5699-2023-f03.png"/>

        </fig>

      <p id="d1e1740">During our study, 6 d, with a slightly weak burst of sub<inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm particles, were identified as being undefined days, as their formation and growth
rate cannot be calculated accurately. For non-event days, we observed that,
during many<?pagebreak page5704?> of them, some nucleation mode particles with sizes above 10 nm did appear. However, we did not observe the burst of sub<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm clusters from the PSM measurements, and moreover, no clear growth of these particles can be identified. This indicates that these small particles are probably not from the nucleation of H<inline-formula><mml:math id="M82" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M83" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> with other species and their subsequent growth but more likely local emissions (traffic exhausts) or long-range transported particles.</p>
      <p id="d1e1781">Figure 3 shows a typical NPF event on 7 December as an example. Northwesterly
wind prevailed, with elevated wind speed starting from around 08:00 LT,
which was conducive to the diffusion of local pollutants, leading to a rapid
decrease in CS concurrently. At the same time, an obvious rise in the H<inline-formula><mml:math id="M84" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M85" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration was observed, coinciding with a strong burst
in the concentration of sub<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm clusters. Then, new particles with diameters larger than 10 nm, as shown in Fig. 3b, gradually formed by growth (exhibited as a visible banana shape in PNSD).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1815">Summaries of the parameters (average values) relevant for NPF events
during wintertime in China and other countries.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.84}[.84]?><oasis:tgroup cols="8">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Station</oasis:entry>
         <oasis:entry colname="col2">Period</oasis:entry>
         <oasis:entry colname="col3">Frequency</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M94" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">GR</oasis:entry>
         <oasis:entry colname="col6">CS</oasis:entry>
         <oasis:entry colname="col7">SA</oasis:entry>
         <oasis:entry colname="col8">Reference</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(cm<inline-formula><mml:math id="M95" 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> s<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col4">(nm h<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">(10<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col6">(10<inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:math></inline-formula> cm<inline-formula><mml:math id="M101" 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>)</oasis:entry>
         <oasis:entry colname="col7"/>
         <oasis:entry colname="col8"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">GC<inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">18 Nov 2018</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">3.15 (<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">4.3</oasis:entry>
         <oasis:entry colname="col6">4.7</oasis:entry>
         <oasis:entry colname="col7">12.5</oasis:entry>
         <oasis:entry colname="col8">This study</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GC<inline-formula><mml:math id="M104" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">6 Dec 2018</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">29.7 (<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">1.8</oasis:entry>
         <oasis:entry colname="col6">0.7</oasis:entry>
         <oasis:entry colname="col7">14.4</oasis:entry>
         <oasis:entry colname="col8">This study</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GC<inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">7 Dec 2018</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">30.4 (<inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">4.1</oasis:entry>
         <oasis:entry colname="col6">0.8</oasis:entry>
         <oasis:entry colname="col7">14.7</oasis:entry>
         <oasis:entry colname="col8">This study</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GC<inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8 Dec 2018</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">21.8 (<inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">8.1</oasis:entry>
         <oasis:entry colname="col6">2.7</oasis:entry>
         <oasis:entry colname="col7">13.5</oasis:entry>
         <oasis:entry colname="col8">This study</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GC<inline-formula><mml:math id="M110" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">23 Dec 2018</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">6.0 (<inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">1.2</oasis:entry>
         <oasis:entry colname="col6">1.6</oasis:entry>
         <oasis:entry colname="col7">14.3</oasis:entry>
         <oasis:entry colname="col8">This study</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GC<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula> (mean)</oasis:entry>
         <oasis:entry colname="col2">12 Nov–24 Dec 2018</oasis:entry>
         <oasis:entry colname="col3">12.8 %</oasis:entry>
         <oasis:entry colname="col4">22.0 (<inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">3.9</oasis:entry>
         <oasis:entry colname="col6">2.1</oasis:entry>
         <oasis:entry colname="col7">13.9</oasis:entry>
         <oasis:entry colname="col8">This study</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Thissio<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">UB</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Aug 2015–Aug 2016; Feb 2017–Feb 2018<inline-formula><mml:math id="M115" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">10.3 %</oasis:entry>
         <oasis:entry colname="col4">1.55 (<inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">3.48</oasis:entry>
         <oasis:entry colname="col6">0.79</oasis:entry>
         <oasis:entry colname="col7">6.33</oasis:entry>
         <oasis:entry colname="col8">Kalkavouras et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">New Delhi<inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">26 Oct–9 Nov 2002</oasis:entry>
         <oasis:entry colname="col3">53.3 %</oasis:entry>
         <oasis:entry colname="col4">7.3 (<inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">14.9</oasis:entry>
         <oasis:entry colname="col6">5.75</oasis:entry>
         <oasis:entry colname="col7">–</oasis:entry>
         <oasis:entry colname="col8">Mönkkönen et al. (2005)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Panyu<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Winter 2011</oasis:entry>
         <oasis:entry colname="col3">21.3 %</oasis:entry>
         <oasis:entry colname="col4">0.89 (<inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">5.1</oasis:entry>
         <oasis:entry colname="col6">5.5</oasis:entry>
         <oasis:entry colname="col7">–</oasis:entry>
         <oasis:entry colname="col8">Tan et al. (2016)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Shanghai<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">25 Nov 2013–25 Jan 2014</oasis:entry>
         <oasis:entry colname="col3">21 %</oasis:entry>
         <oasis:entry colname="col4">188 (<inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.34</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">11.4</oasis:entry>
         <oasis:entry colname="col6">6.0</oasis:entry>
         <oasis:entry colname="col7">37</oasis:entry>
         <oasis:entry colname="col8">Xiao et al. (2015)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Nanjing<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">18 Nov 2011–31 Mar 2012</oasis:entry>
         <oasis:entry colname="col3">20 %</oasis:entry>
         <oasis:entry colname="col4">33.2 (<inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">8.5</oasis:entry>
         <oasis:entry colname="col6">2.4</oasis:entry>
         <oasis:entry colname="col7">45.3</oasis:entry>
         <oasis:entry colname="col8">Herrmann et al. (2014)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hong Kong<inline-formula><mml:math id="M125" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">25 Oct–29 Nov 2010</oasis:entry>
         <oasis:entry colname="col3">34.3 %</oasis:entry>
         <oasis:entry colname="col4">2.94 (<inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">5.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">3.86</oasis:entry>
         <oasis:entry colname="col6">0.8–6.2</oasis:entry>
         <oasis:entry colname="col7">9.17</oasis:entry>
         <oasis:entry colname="col8">Guo et al. (2012)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Beijing<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">23 Jan–31 Mar 2018</oasis:entry>
         <oasis:entry colname="col3">51.5 %</oasis:entry>
         <oasis:entry colname="col4">38 (<inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">5.5</oasis:entry>
         <oasis:entry colname="col6">3.7</oasis:entry>
         <oasis:entry colname="col7">4.13</oasis:entry>
         <oasis:entry colname="col8">Chu et al. (2021)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ziyang<inline-formula><mml:math id="M129" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">5 Dec 2012–5 Jan 2013</oasis:entry>
         <oasis:entry colname="col3">23 %</oasis:entry>
         <oasis:entry colname="col4">5.2 (<inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">3.6</oasis:entry>
         <oasis:entry colname="col6">7.4</oasis:entry>
         <oasis:entry colname="col7">6.7</oasis:entry>
         <oasis:entry colname="col8">Chen et al. (2014)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Melpitz<inline-formula><mml:math id="M131" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Winter 2003–2006</oasis:entry>
         <oasis:entry colname="col3">3 %</oasis:entry>
         <oasis:entry colname="col4">0.7 (<inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">5.6</oasis:entry>
         <oasis:entry colname="col6">1.2</oasis:entry>
         <oasis:entry colname="col7">0.123</oasis:entry>
         <oasis:entry colname="col8">Hamed et al. (2010)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Melpitz<inline-formula><mml:math id="M133" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Winter 1996–1997</oasis:entry>
         <oasis:entry colname="col3">10 %</oasis:entry>
         <oasis:entry colname="col4">4.9 (<inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">4.1</oasis:entry>
         <oasis:entry colname="col6">0.9</oasis:entry>
         <oasis:entry colname="col7">0.259</oasis:entry>
         <oasis:entry colname="col8">Hamed et al. (2010)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Pingyuan<inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">3 Nov 2017–20 Jan 2018</oasis:entry>
         <oasis:entry colname="col3">39.2 %</oasis:entry>
         <oasis:entry colname="col4">164.2 (<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.6</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">3.9</oasis:entry>
         <oasis:entry colname="col6">1.9</oasis:entry>
         <oasis:entry colname="col7">2.45</oasis:entry>
         <oasis:entry colname="col8">Fang et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Xinken<inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">3 Oct–5 Nov 2004</oasis:entry>
         <oasis:entry colname="col3">25.9 %</oasis:entry>
         <oasis:entry colname="col4">0.5–5.4 (<inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">2.2–19.8</oasis:entry>
         <oasis:entry colname="col6">–</oasis:entry>
         <oasis:entry colname="col7">–</oasis:entry>
         <oasis:entry colname="col8">Liu et al. (2008)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Solapur<inline-formula><mml:math id="M139" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Oct 2018–Feb 2019</oasis:entry>
         <oasis:entry colname="col3">28.9 %</oasis:entry>
         <oasis:entry colname="col4">0.22–10.07 (<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">15</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">1.2–13.8</oasis:entry>
         <oasis:entry colname="col6">0.6–3</oasis:entry>
         <oasis:entry colname="col7">–</oasis:entry>
         <oasis:entry colname="col8">Varghese et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cyprus<inline-formula><mml:math id="M141" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">RB</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Jan–Feb 2018</oasis:entry>
         <oasis:entry colname="col3">69 %</oasis:entry>
         <oasis:entry colname="col4">16.4 (<inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">9.97</oasis:entry>
         <oasis:entry colname="col6">1.2</oasis:entry>
         <oasis:entry colname="col7">–</oasis:entry>
         <oasis:entry colname="col8">Baalbaki et al. (2021)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SEAS<inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">O</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Winter 2018</oasis:entry>
         <oasis:entry colname="col3">5 %</oasis:entry>
         <oasis:entry colname="col4">2.95 (<inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">14.35</oasis:entry>
         <oasis:entry colname="col6">4.5</oasis:entry>
         <oasis:entry colname="col7">–</oasis:entry>
         <oasis:entry colname="col8">Kompalli et al. (2020)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SMEAR II<inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">B</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">Winter 1996–2003</oasis:entry>
         <oasis:entry colname="col3">24.2 %</oasis:entry>
         <oasis:entry colname="col4">0.2–1.1 (<inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col5">0.29–3.7</oasis:entry>
         <oasis:entry colname="col6">0.05–0.35</oasis:entry>
         <oasis:entry colname="col7">0.53</oasis:entry>
         <oasis:entry colname="col8">Dal Maso et al. (2005)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table><?xmltex \begin{scaleboxenv}{.84}[.84]?><table-wrap-foot><p id="d1e1818"><?xmltex \hack{\vspace*{1mm}}?>SEAS is the southeastern Arabian Sea, <inline-formula><mml:math id="M87" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">R</mml:mi></mml:msup></mml:math></inline-formula> is the rural site, <inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">UB</mml:mi></mml:msup></mml:math></inline-formula> is the urban background site, <inline-formula><mml:math id="M89" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">RB</mml:mi></mml:msup></mml:math></inline-formula> is the rural background site, <inline-formula><mml:math id="M90" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">U</mml:mi></mml:msup></mml:math></inline-formula> is the urban site, <inline-formula><mml:math id="M91" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">B</mml:mi></mml:msup></mml:math></inline-formula> is the background site, <inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">O</mml:mi></mml:msup></mml:math></inline-formula> is the ocean site, <inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mo>*</mml:mo></mml:msup></mml:math></inline-formula> is only in wintertime, and “–” is no number.</p></table-wrap-foot><?xmltex \end{scaleboxenv}?><?xmltex \gdef\@currentlabel{1}?></table-wrap>

      <?pagebreak page5705?><p id="d1e3098">For all the identified NPF events, the formation rate of 1.3 nm (<inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) particles ranged from 6.0 to about 30.4 cm<inline-formula><mml:math id="M148" 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> s<inline-formula><mml:math id="M149" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, with an average value of 22.0 cm<inline-formula><mml:math id="M150" 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> s<inline-formula><mml:math id="M151" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at our GC site during the measurement period. Note that most atmospheric formation rates reported in China were based on the measured formation rates at relatively larger size, i.e., 3–10 nm, which are so-called “apparent” particle formation rates. In order to derive the formation rates of critical clusters from the apparent particle formation rates (Kulmala et al., 2017), the nuclei GR or GR at sub<inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm is needed but usually remains unclear. Therefore, we focused more on the formation rate of particles at sizes below 3 nm in the following discussion. In principle, the particle formation rate is inversely proportional to the CS, as the nucleation precursors or clusters would be scavenged more rapidly under higher CS conditions, leading to a slower nanoparticle formation with a lower <inline-formula><mml:math id="M153" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula>. However, as shown in Table 1, in spite of the higher CS, the particle formation rates at our site appear to be higher than those in clean environments. This kind of intensive NPF becomes more noticeable for those Chinese megacities, such as Shanghai, Beijing, and Nanjing, which have an even higher <inline-formula><mml:math id="M154" display="inline"><mml:mi>J</mml:mi></mml:math></inline-formula> and CS compared to that at our GC site. The most plausible explanation could be the higher abundance of nucleating precursors for NPF in those polluted atmospheres, which is indicated by the SA concentration that is either measured in urban Shanghai and Nanjing or calculated in our study. To be specific, the mean SA proxy concentration during NPF at our GC site was around <inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">7</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M156" 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>, which is a factor of around 30 higher than that at Hyytiälä in Finland (Nieminen et al., 2014). The SA concentration during NPF at Shanghai (Xiao et al., 2015) and Nanjing
(Herrmann et al., 2014) was even higher, at around <inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">7</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M158" 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>.</p>
      <p id="d1e3240">Although the formation rate of 1.3 nm particles is relatively high, the
newly formed particles at our GC site usually cannot grow into very large
particles within a short time, as indicated by their low GR. The average value of GR<inline-formula><mml:math id="M159" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">1.3</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">2.4</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> and GR<inline-formula><mml:math id="M160" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">9</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> at our site was 0.5 and 3.9 nm h<inline-formula><mml:math id="M161" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively, which is generally lower than many clean environments – GR<inline-formula><mml:math id="M162" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> of 0.9 nm h<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for Hyytiälä (Kulmala, 2013) and of 5.1 nm h<inline-formula><mml:math id="M164" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for Jungfraujoch (Boulon et al., 2010) – but similar to those at urban Beijing (Chu et al., 2021) and rural Pingyuan (Fang et al., 2020). This could be attributed to the high CS or CoagS at those polluted environments, as the growth of small particles is limited, which are more vulnerable to the coagulation scavenging. However, despite the high CoagS, the observed GR at Shanghai and Nanjing was still exceptionally high. This discrepancy suggests that, besides the high concentration of precursors (mainly H<inline-formula><mml:math id="M165" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M166" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>) in polluted environments, including both rural and urban sites, other precursors with different efficiencies for nanoparticle growth and other involving mechanisms (for instance, multiphase reactions) may all contribute to the nanoparticle growth but have yet to be elucidated.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Potential mechanisms for NPF events in the rural NCP</title>
      <p id="d1e3348">To further understand the dominating nucleation mechanism in the rural atmosphere of NCP in China, we plotted the measured formation rate of 1.3 nm
particles (<inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) against the simulated H<inline-formula><mml:math id="M168" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M169" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration and compared the results to previous studies conducted in different environments, as shown in Fig. 4. As illustrated by the significant correlation between the concentration of sulfuric acid and the particle formation rates, sulfuric acid is considered to be the driving species in the initial steps of NPF, as confirmed conventionally. However, the obtained <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>–H<inline-formula><mml:math id="M171" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M172" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> relationship for current environment appeared to deviate largely from those obtained by other studies. If only referring to the slope of the <inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>–H<inline-formula><mml:math id="M174" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M175" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> relationship, our results seem to approximate most to the ones measured by these CLOUD (the Cosmics Leaving OUtdoor Droplets chamber) experiments, based on the mechanism of H<inline-formula><mml:math id="M176" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M177" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>-DMA (dimethylamine) nucleation. However, without the direct measurements of other potential precursors, the molecules stabilizing H<inline-formula><mml:math id="M178" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M179" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> clustering still remain unclear.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e3478">The particle formation rate (<inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mn mathvariant="normal">1.3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) as a function of H<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M182" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration for our study and for urban Shanghai
(Yao et al., 2018), Beijing (Cai et al., 2021b), rural Pingyuan (Fang et al., 2020), and CLOUD measurements. The gray square, triangle, pentagram, and diamond represent CLOUD data for H<inline-formula><mml:math id="M183" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M184" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M185" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> H<inline-formula><mml:math id="M186" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O,
H<inline-formula><mml:math id="M187" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M188" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M189" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> H<inline-formula><mml:math id="M190" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O <inline-formula><mml:math id="M191" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> NH<inline-formula><mml:math id="M192" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, and H<inline-formula><mml:math id="M193" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M194" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M195" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> H<inline-formula><mml:math id="M196" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O <inline-formula><mml:math id="M197" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> DMA (Kirkby et al., 2011; Riccobono et al., 2014), where DMA represents dimethylamine.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/5699/2023/acp-23-5699-2023-f04.png"/>

        </fig>

      <p id="d1e3644">Comparing the particle formation rates reported in different environments in
China, our results were of a similar magnitude to that in Beijing (Cai et al., 2021b), an urban site in the NCP. It has to be noted that the Cai et al. (2021b) study was conducted during a much longer time and completely<?pagebreak page5706?> covered the measurement period of our study. More importantly, during the 5 d of events in our study, NPF concurrently occurred at their measurement site (Liu et al., 2020). Additionally, for these 5 event days, air masses arriving at our site followed similar transport paths to that in urban Beijing (see Fig. S2 in the Supplement for an example), as they both originated from Siberian areas, where the concentration of gaseous pollutants and particulate matter was typically quite low, through the northwest of the observational sites. Taking both sources of evidence, we hypothesize that NPF events during these days in this area might be a regional phenomenon that is sharing the same or a similar nucleation mechanism. Cai et al. (2021b) and Yan et al. (2021) further concluded that H<inline-formula><mml:math id="M198" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M199" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>-DMA was the dominating nucleation mechanism for urban Beijing, with additional support from the measured C2-amine concentration. Considering the similarities between these two sites, we speculated that the clustering of H<inline-formula><mml:math id="M200" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M201" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> with DMA may also dominate the nucleation process at our site during winter, though future work is needed to verify the current hypothesis.</p>
      <p id="d1e3684">On the other hand, we noticed that our results deviate significantly from
the measured formation rate at Pingyuan (Fang et al., 2020), which is another
rural site in the NCP. They concluded that neither H<inline-formula><mml:math id="M202" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M203" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>-NH<inline-formula><mml:math id="M204" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> nor H<inline-formula><mml:math id="M205" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M206" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>-DMA mechanisms could fully explain their observed particle formation rate but suggested that gaseous dicarboxylic acids were the dominating species for the initial step of H<inline-formula><mml:math id="M207" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M208" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> clustering under a diacid-rich environment. Being similar to the rural environment of NCP, we cannot completely rule out the contribution of dicarboxylic acids to the H<inline-formula><mml:math id="M209" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M210" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> stabilization. However, as illustrated in Fig. S4, the concentration of these four dicarboxylic acids during NPF events was in general lower than that during non-event days. Furthermore, during the daytime of events days when NPF was typically initiated, the signals of these diacids obtained from the I-CIMS did not show a clear increase, unlike sulfuric acid, but were rather elevated during the nighttime (see Fig. S5), which is obviously different to the case of Pingyuan. Hence, the involvement of diacids during the initial steps of nucleation under the current rural atmosphere might not hold. This statement does not necessarily mean that our previous inference was incorrect but, on the other hand, provides some hints that although NPF events in the NCP are regional, there might be no uniform theory but multiple mechanisms coexisting to explain its features, with the dominating one varying according to different emission patterns or meteorological conditions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e3771"><bold>(a)</bold> H<inline-formula><mml:math id="M211" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M212" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration as a function of the condensation sink during both event days and non-event days during our study. <bold>(b)</bold> The dimensionless indicator, <inline-formula><mml:math id="M213" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>, as a function of the condensational sink. For both panels, the triangles indicate data for event days, while the circles indicate data for non-event days. The color bar indicates the solar radiation <bold>(a)</bold> and H<inline-formula><mml:math id="M214" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M215" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> proxy concentration <bold>(b)</bold>.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/5699/2023/acp-23-5699-2023-f05.png"/>

        </fig>

</sec>
<?pagebreak page5707?><sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Governing factors for the occurrence of NPF in rural NCP</title>
      <p id="d1e3843">The high concentration of SO<inline-formula><mml:math id="M216" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, NH<inline-formula><mml:math id="M217" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M218" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>, and VOCs (Chu et al., 2019), as well as fine particles, makes the NCP of China a unique context for NPF compared to many other environments. In principle, the competition between how fast the newly formed clusters grow and how fast they are scavenged determines whether or not NPF will occur in the atmosphere. However, in the NCP, the concentration of SA was typically quite high, probably reaching its maximum rate to form clusters. Thus, CS or CoagS becomes the dominant factor controlling the occurrence of NPF. This was partly confirmed by existing observations; for instance, Cai et al. (2021b) found that H<inline-formula><mml:math id="M219" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M220" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> was high enough in urban Beijing but did not necessarily lead to the occurrence of NPF there. Their research pointed out that as long as CS or CoagS was below a certain threshold (Cai et al., 2017), NPF is very likely to occur.</p>
      <p id="d1e3891">Was this also true for the rural atmosphere in the NCP? By comparing with non-event days at our site (see Fig. 5a), we noticed that the H<inline-formula><mml:math id="M221" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M222" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>
level was not significantly higher (but sometimes even lower) than that during non-event days. In other words, the abundance of H<inline-formula><mml:math id="M223" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M224" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> did not always lead to NPF, and it was only when CS was significantly lowered that the event became more likely to occur. This strongly demonstrates the
similarity between our site with that of urban Beijing in that CS would be the limiting factor for the occurrence of NPF. However, we noticed that there were a very few cases (two cases) in which the CS was somewhat low, with the levels being quite close to that under those event days, yet NPF still did not occur. The most plausible explanation for this could be, on the one hand, the lowered H<inline-formula><mml:math id="M225" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M226" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration on these days (as shown in Fig. 5a) and, on the other hand, that the other nucleating species rather than H<inline-formula><mml:math id="M227" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M228" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> may not be always enough to initiate nucleation at this site.</p>
      <p id="d1e3967">As previously stated, the dimensionless criterion, <inline-formula><mml:math id="M229" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>, is a good
quantitative indicator to predict whether an NPF occurs or not during a
certain day. Thus, we plotted <inline-formula><mml:math id="M230" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> against the condensational sink for NPF days and other days under different H<inline-formula><mml:math id="M231" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M232" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> levels. Cai et al. (2021a) found that the larger the <inline-formula><mml:math id="M233" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> value, the higher frequency at which NPF events occurred for both urban Beijing and Shanghai, which was also clearly revealed by our results. On the one hand, as shown in Fig. 5b, the largest <inline-formula><mml:math id="M234" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> values were mostly observed for NPF days, confirming its feasibility in predicting the occurrence of NPF events. On the other hand, the obtained <inline-formula><mml:math id="M235" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> anti-correlated with CS quite well, while the influence from the available H<inline-formula><mml:math id="M236" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M237" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> was not obvious. This strongly suggests that CS was the dominating factor governing the appearance of NPF events in the current environment, which is highly consistent with the feature observed in Beijing.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e4045">Diurnal variation in <bold>(a)</bold> CO, <bold>(b)</bold> SO<inline-formula><mml:math id="M238" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, <bold>(c)</bold> NO<inline-formula><mml:math id="M239" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>, <bold>(d)</bold> O<inline-formula><mml:math id="M240" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, <bold>(e)</bold> PM<inline-formula><mml:math id="M241" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, <bold>(f)</bold> solar radiation (SR), <bold>(g)</bold> <inline-formula><mml:math id="M242" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>, <bold>(h)</bold> RH, <bold>(i)</bold> wind speed (WS), <bold>(j)</bold> number concentration of sub<inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm cluster, <bold>(k)</bold> CS, and <bold>(l)</bold> H<inline-formula><mml:math id="M244" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M245" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> proxy during the NPF and non-NPF days during this field campaign. These values were averaged over the 5 NPF days and 28 non-event days, respectively.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/23/5699/2023/acp-23-5699-2023-f06.png"/>

        </fig>

      <p id="d1e4164">Moreover, we found that the RH level under event days was generally lower than that on non-event days (see Fig. 6). This is similar to the cases for which NPF was observed in Beijing by Yue et al. (2009), who suggested that photochemical reactions were faster on sunny days with low RH. In addition to this, the ambient temperature during NPF was relatively lower than that on non-event days (Kirkby et al., 2011; Riccobono et al., 2014). Yan et al. (2021) considered that temperature can affect the stability of H<inline-formula><mml:math id="M246" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M247" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> clustering and thus influence NPF. Therefore, all of these factors could be the potential reasons increase or decrease the probability of NPF occurring in current rural areas. It has to be noted that all these features, including the reduced RH level in addition to ambient <inline-formula><mml:math id="M248" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> during event days, could be coincidental, with reduced CS over clean days, for instance, being a consequence of air masses originating from the north and bringing drier,<?pagebreak page5708?> colder, and cleaner air to the site. Therefore, current discussion in this regard becomes ambiguous and may be inclusive but should still be considered separately when larger datasets are available. In addition, we observed that the O<inline-formula><mml:math id="M249" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> concentration was clearly higher during event days, implying that other condensable vapors, for instance, organics that involve O<inline-formula><mml:math id="M250" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, among others, in forming HOM, might also be important to NPF in this region. Although these organic compounds formed through O<inline-formula><mml:math id="M251" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> oxidation (Mohr et al., 2019) may not necessarily participate in H<inline-formula><mml:math id="M252" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M253" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> clustering, they may contribute considerably to the growth of newly formed particles, which should not be ruled out in the study of NPF for this region and also need to be investigated in the future.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Summary and conclusions</title>
      <p id="d1e4247">Most previous studies dealing with NPF in China were mainly based on the measurements of particles at larger sizes, typically above 3 nm, whereas
the detection of particles at the sub<inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> nm range was quite limited. In our study, by coupling a PSM with a traditional SMPS, we were able to measure the particle number size distribution down to 1.3 nm during NPF events in the wintertime at a rural site on the NCP. Correspondingly, the formation rate of particles at 1.3 nm was obtained, widening the data pool concerning the feature of NPF for this region. At the current rural environment, a high level of H<inline-formula><mml:math id="M255" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M256" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> may not always initiate the occurrence of NPF. Only under the condition in which the CS was considerably low were NPF events more likely to take place. This feature is quite similar to that of the urban atmosphere of NCP, whereas NPF events were usually characterized by high formation rates, high CS, and high H<inline-formula><mml:math id="M257" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M258" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration. However, as our H<inline-formula><mml:math id="M259" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M260" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration was predicted from empirical parameters, we emphasize the need for caution regarding their particular associated uncertainties. Yang et al. (2021) demonstrated that the derived fitting parameters for the calculations of H<inline-formula><mml:math id="M261" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M262" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> proxy may vary from site to site and between different seasons. For instance, they considered that the products from the ozonolysis of alkenes were able to oxidize SO<inline-formula><mml:math id="M263" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> to form gaseous H<inline-formula><mml:math id="M264" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M265" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>. Moreover, they pointed out that H<inline-formula><mml:math id="M266" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M267" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> could be from primary emissions, such as<?pagebreak page5709?> vehicles or freshly emitted plumes. Sulfuric acid from these sources could account for 10 % of the total H<inline-formula><mml:math id="M268" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M269" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> in the atmosphere. These aspects were not comprehensively considered in our calculations, which could bring huge uncertainties or errors to the estimation. Thereby, direct measurements of the H<inline-formula><mml:math id="M270" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M271" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> concentration should be implemented in the future before deriving any further conclusions.</p>
</sec>

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

      <p id="d1e4421">The details of the data used in this work can be found at <ext-link xlink:href="https://doi.org/10.5281/zenodo.7326388" ext-link-type="DOI">10.5281/zenodo.7326388</ext-link> (Hong et al., 2022).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e4427">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-23-5699-2023-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-23-5699-2023-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e4436">JH collected the resources, wrote, and finalized the paper. MT analyzed the data, plotted the figures, and wrote the original draft. QW and NM planned the study, collected the resources, and reviewed the paper. SZhu, SZha, XP, LX, GL, and UK conducted the measurements. CY, JT, YK, YH, YZ, WX, GZ, BY, and ZW discussed the results. YC and HS contributed to fund acquisition.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e4442">At least one of the (co-)authors is a member of the editorial board of <italic>Atmospheric Chemistry and Physics</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e4451">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e4457">This work has been supported by the National Natural Science Foundation of China (grant nos. 42175117, 41907182, 41877303, and 91644218) and the National key R&amp;D Program of China (grant no. 2018YFC0213901), the Fundamental Research Funds for the Central Universities (grant no. 21621105), and Special Fund Project for Science and Technology Innovation Strategy of Guangdong Province (grant no. 2019B121205004).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e4463">This paper was edited by Birgit Wehner and reviewed by two anonymous referees.</p>
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