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<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">
  <front>
    <journal-meta><journal-id journal-id-type="publisher">ACP</journal-id><journal-title-group>
    <journal-title>Atmospheric Chemistry and Physics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1680-7324</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/acp-20-12853-2020</article-id><title-group><article-title>Using machine learning to derive cloud condensation nuclei number concentrations from commonly available measurements</article-title><alt-title>Machine learning derivation of CCN</alt-title>
      </title-group><?xmltex \runningtitle{Machine learning derivation of CCN}?><?xmltex \runningauthor{A.~A.~Nair and F.~Yu}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes">
          <name><surname>Nair</surname><given-names>Arshad Arjunan</given-names></name>
          <email>aanair@albany.edu</email>
        <ext-link>https://orcid.org/0000-0003-2530-7757</ext-link></contrib>
        <contrib contrib-type="author" corresp="no">
          <name><surname>Yu</surname><given-names>Fangqun</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-8862-4835</ext-link></contrib>
        <aff id="aff1"><institution>Atmospheric Sciences Research Center, State University of New York, Albany, New York 12203, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Arshad Arjunan Nair (aanair@albany.edu)</corresp></author-notes><pub-date><day>5</day><month>November</month><year>2020</year></pub-date>
      
      <volume>20</volume>
      <issue>21</issue>
      <fpage>12853</fpage><lpage>12869</lpage>
      <history>
        <date date-type="received"><day>27</day><month>May</month><year>2020</year></date>
           <date date-type="rev-request"><day>10</day><month>June</month><year>2020</year></date>
           <date date-type="rev-recd"><day>23</day><month>August</month><year>2020</year></date>
           <date date-type="accepted"><day>30</day><month>September</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2020 </copyright-statement>
        <copyright-year>2020</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e86">Cloud condensation nuclei (CCN) number concentrations are an important aspect of aerosol–cloud interactions and the subsequent climate effects; however, their measurements are very limited. We use a machine learning tool, random decision forests, to develop a random forest regression model (RFRM) to derive CCN at 0.4 % supersaturation ([CCN0.4]) from commonly available measurements. The RFRM is trained on the long-term simulations in a global size-resolved particle microphysics model. Using atmospheric state and composition variables as predictors, through associations of their variabilities, the RFRM is able to learn the underlying dependence of [CCN0.4] on these predictors, which are as follows: eight fractions of PM<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, secondary organic aerosol (SOA), black carbon (BC), primary organic carbon (POC), dust, and salt), seven gaseous species (<inline-formula><mml:math id="M5" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M8" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M9" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:math></inline-formula>, isoprene, and monoterpene), and four meteorological variables (temperature (<italic>T</italic>), relative humidity (RH), precipitation, and solar radiation). The RFRM is highly robust: it has a median mean fractional bias (MFB) of <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.4</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">96.33</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the derived [CCN0.4] within a good agreement range of <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">60</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>&lt;</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>&lt;</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">60</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> and strong correlation of Kendall's <inline-formula><mml:math id="M13" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> coefficient <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.88</mml:mn></mml:mrow></mml:math></inline-formula>. The RFRM demonstrates its robustness over 4 orders of magnitude of [CCN0.4] over varying spatial (such as continental to oceanic, clean to polluted, and near-surface to upper troposphere) and temporal (from the hourly to the decadal) scales. At the Atmospheric Radiation Measurement Southern Great Plains observatory (ARM SGP) in Lamont, Oklahoma, United States, long-term measurements for PM<inline-formula><mml:math id="M15" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciation (<inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and organic carbon (OC)), <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <italic>T</italic>, and RH, as well as [CCN0.4] are available. We modify, optimize, and retrain the developed RFRM to make predictions from <inline-formula><mml:math id="M22" display="inline"><mml:mn mathvariant="normal">19</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M23" display="inline"><mml:mn mathvariant="normal">9</mml:mn></mml:math></inline-formula> of these available predictors. This retrained RFRM (RFRM-ShortVars) shows a reduction in performance due to the unavailability and sparsity of measurements (predictors); it captures the [CCN0.4] variability and magnitude at SGP with <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">67.02</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the derived values in the good agreement range. This work shows the potential of using the more commonly available measurements of PM<inline-formula><mml:math id="M25" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciation to alleviate the sparsity of CCN number concentrations' measurements.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e380">Minute particles suspended in the atmosphere prove to be the most nontrivial sources of uncertainty (variability across modeling efforts) in our understanding of climate change <xref ref-type="bibr" rid="bib1.bibx23" id="paren.1"/>. These particles or aerosols, or rather CCN (cloud condensation nuclei: aerosols capable of being imbibed in clouds and modifying their properties), have direct and indirect sources. They can be directly emitted into the atmosphere as sea salt, primary inorganic particulates such as dust and carbon, or primary organic particulates. Aqueous chemistry can modify the chemical species in the cloud droplet, which on evaporation will result in an aerosol size distribution capable of acting as CCN at lower RH <xref ref-type="bibr" rid="bib1.bibx20" id="paren.2"/>. In the air, emissions of <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>/</mml:mo><mml:mi mathvariant="normal">DMS</mml:mi></mml:mrow></mml:math></inline-formula> (dimethyl sulfide), <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and organics can undergo gas-phase (photo-)chemistry to form condensible vapors that may take part in new particle formation (nucleation) that converts gas to particles; this process is an important source of aerosols, especially from anthropogenic sources, and subsequent growth contributes up to 50 % or more of global CCN <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx57" id="paren.3"><named-content content-type="pre">e.g.,</named-content></xref>.</p>
      <p id="d1e420"><?xmltex \hack{\newpage}?>Of the uncertainty in the effective radiativ<?pagebreak page12854?>e forcing (ERF) in global climate models associated with aerosols, the aerosol indirect effect primarily through aerosol–cloud interactions (aci) is predominant <xref ref-type="bibr" rid="bib1.bibx23" id="paren.4"/>: ERF<inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi/><mml:mi mathvariant="normal">aci</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.2</mml:mn><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mtext>to</mml:mtext><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. These aerosol–cloud interactions are mediated by CCN that affect cloud micro- and macrophysics primarily through their interaction with water vapor to modify cloud droplet size and number. There are various such indirect effects: the first indirect effect <xref ref-type="bibr" rid="bib1.bibx50" id="paren.5"/>, the second indirect effect <xref ref-type="bibr" rid="bib1.bibx1" id="paren.6"/>, and others such as effects on cloud formation and precipitation dynamics <xref ref-type="bibr" rid="bib1.bibx45" id="paren.7"><named-content content-type="post">and the references therein</named-content></xref>, which affect the atmospheric energy balance.</p>
      <p id="d1e478">The numerous physical and chemical effects of and on CCN and their nonlinear interactions as detailed above provide a glimpse into the complexities and challenges associated with developing a valid physical description of aerosol processes in global climate models. A major problem is the accurate characterization of CCN number concentrations ([CCN]) in the atmosphere and quantification of their effects on Earth’s radiative budget. Extensive measurements of [CCN] would help in this regard, towards reducing the uncertainties in modeling aerosol–cloud interactions. Unfortunately, these are sparse; there are some in situ measurements available during short campaigns and for a few sites from networks such as the Atmospheric Radiation Measurement Climate Research Facility (ARM), the Aerosol, Clouds and Trace Gases Research Infrastructure (ACTRIS), and the Global Atmosphere Watch (GAW), while satellite inference of [CCN] is not yet robust, suffering from missing data and coarse resolution. In contrast, particle mass concentration and speciation have been routinely measured in a large number of networks, such as the Interagency Monitoring of Protected Visual Environments (IMPROVE), the Chemical Speciation Network (CSN/STN), and the Clean Air Status and Trends Network (CASTNET) in the United States; the Campaign on Atmospheric Aerosol Research network of China (CARE-China); the National Air Quality Monitoring Programme (NAMP) in India; and AirBase and the EMEP (European Monitoring and Evaluation Programme) networks in the European Union, with some of the earliest measurements from the 1980s.</p>
      <p id="d1e481">We investigate the possibility of using machine learning techniques to obtain CCN number concentrations from these measurements. Machine learning is a statistical learning branch of artificial intelligence where computers learn without being explicitly programmed to generalize from knowledge acquired by being trained on a huge number of specific scenarios. The development and use of machine learning to develop predictive models has been burgeoning over the last couple of decades, with recent applications in the atmospheric sciences such as in atmospheric new particle formation <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx61" id="paren.8"><named-content content-type="pre">e.g.,</named-content></xref>, mixing state <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx21" id="paren.9"><named-content content-type="pre">e.g.,</named-content></xref>, air quality <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx15" id="paren.10"><named-content content-type="pre">e.g.,</named-content></xref>, remote sensing <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx31 bib1.bibx38" id="paren.11"><named-content content-type="pre">e.g.,</named-content></xref>, and other aspects <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx25" id="paren.12"><named-content content-type="pre">e.g.,</named-content></xref>. These and other studies show the power of machine learning as a tool to account for the high nonlinearities in the associations between atmospheric states and compositions towards predictive modeling.</p>
      <p id="d1e510">The goal of the present study is to explore the possibility of deriving the number concentrations of CCN at 0.4 % supersaturation ([CCN0.4]) through more ubiquitous measurements of atmospheric state and composition. For this, we develop a random forest regression model (RFRM). The machine learning model is trained on 30 years' (1989–2018) simulations from a chemical transport model incorporating a size-resolved particle microphysics model. The expectation is that the RFRM is able to learn the associations between atmospheric state and composition predictors and the [CCN0.4] (outcome).</p>
      <p id="d1e513">The remainder of this paper is organized as follows: Sect. <xref ref-type="sec" rid="Ch1.S2"/> details the data, techniques, and statistical performance metrics used in this study; Sect. <xref ref-type="sec" rid="Ch1.S3"/> details the development of the RFRM, validation of its performance, and evaluation with empirical data; Sect. <xref ref-type="sec" rid="Ch1.S4"/> summarizes the major findings of this study; and Sect. <xref ref-type="sec" rid="Ch1.S4.SS1"/> discusses some of the implications of this work and the avenues it opens up.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>GEOS-Chem-APM model (GCAPM)</title>
      <p id="d1e539">GEOS-Chem is a global 3D chemical transport model (CTM) driven by assimilated meteorological observations from the Goddard Earth Observing System (GEOS) of the NASA Global Modeling and Assimilation Office (GMAO). Several research groups develop and use this model, which contains numerous state-of-the-art modules treating emissions <xref ref-type="bibr" rid="bib1.bibx52 bib1.bibx27" id="paren.13"/> and various chemical and aerosol processes <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx10 bib1.bibx30 bib1.bibx34 bib1.bibx39 bib1.bibx41" id="paren.14"><named-content content-type="pre">e.g.,</named-content></xref> for solving a variety of atmospheric composition research problems. The ISORROPIA II scheme <xref ref-type="bibr" rid="bib1.bibx12" id="paren.15"/> is used to calculate the thermodynamic equilibrium of inorganic aerosols. Secondary organic aerosol formation and aging are based on the mechanisms developed by <xref ref-type="bibr" rid="bib1.bibx41" id="text.16"/> and <xref ref-type="bibr" rid="bib1.bibx56" id="text.17"/>. MEGAN v2.1 (Model of Emissions of Gases and Aerosols from Nature; <xref ref-type="bibr" rid="bib1.bibx16" id="altparen.18"/>) implements biogenic emissions and GFED4 (Global Fire Emissions Database; <xref ref-type="bibr" rid="bib1.bibx14" id="altparen.19"/>) implements biomass burning emissions in GEOS-Chem.</p>
      <p id="d1e566">The present study uses GEOS-Chem version 10-01 with the implementation of the Advanced Particle Microphysics (APM) package <xref ref-type="bibr" rid="bib1.bibx57" id="paren.20"/>, henceforth referred to as GCAPM. The APM model has the following features of relevance towards accurate simulation of CCN<?pagebreak page12855?> number concentrations: (1) 40 bins to represent secondary particles with a high size resolution for the size range important for growth of nucleated particles to CCN sizes <xref ref-type="bibr" rid="bib1.bibx57" id="paren.21"/>; (2) a state-of-the-art ternary ion-mediated nucleation (TIMN) mechanism <xref ref-type="bibr" rid="bib1.bibx60" id="paren.22"/> and temperature-dependent organic nucleation parameterization <xref ref-type="bibr" rid="bib1.bibx59" id="paren.23"/>; (3) calculation of <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> condensation and the successive oxidation aging of secondary organic gases (SOGs) and explicit kinetic condensation of low-volatility SOGs onto particles <xref ref-type="bibr" rid="bib1.bibx56" id="paren.24"/>; (4) contributions of nitrate and ammonium via equilibrium uptake and semi-volatile organics through partitioning to particle growth considered <xref ref-type="bibr" rid="bib1.bibx56" id="paren.25"/>. CCN number concentrations simulated by GCAPM have previously been shown to agree well with measurements <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx56 bib1.bibx58" id="paren.26"/>.</p>
      <p id="d1e607">The horizontal resolution of GCAPM in this study is 2<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M32" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, with 47 vertical layers (14 layers from the surface to 2 km above the surface). The period of global simulation is 30 years from 1989 to 2018. For 47 sites spread across the globe, co-located
GCAPM data are output at the half-hourly time step for all model layers in the troposphere. In the present application, we use those at six selected vertical heights: surface, <inline-formula><mml:math id="M34" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 1, <inline-formula><mml:math id="M35" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 2, <inline-formula><mml:math id="M36" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 4, <inline-formula><mml:math id="M37" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 6, and <inline-formula><mml:math id="M38" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 8 km.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Random forest regression modeling</title>
      <p id="d1e679">In the present study, we choose to use the random forest (RF) technique <xref ref-type="bibr" rid="bib1.bibx5" id="paren.27"/> from the large suite of machine learning techniques, for the following reasons: (a) our objective of predicting (regressing) values of [CCN0.4], (b) the ease of physical interpretability of RF models, (c) ease of implementation, and (d) the ability to tune this supervised machine learning, which is learning by example.</p>
      <p id="d1e685">A random forest <xref ref-type="bibr" rid="bib1.bibx5" id="paren.28"/> is an ensemble of decision trees. A decision tree <xref ref-type="bibr" rid="bib1.bibx6" id="paren.29"/> is a supervised machine learning algorithm that recursively splits the data into subsets based on the input variables that best split the data into homogeneous sets. This is a top-down “greedy” approach called recursive binary splitting. Decision trees are easy to visualize, are not influenced by missing data or outliers, and are nonparametric. They can, however, overfit on the data. Random forest modeling is an ensemble technique of growing numerous decision trees from subsets (bags) of the training data and then using all the decision trees to make an aggregated (typically mean) prediction. This approach corrects for the overfitting of single decision trees. Additionally, the bootstrap aggregating <xref ref-type="bibr" rid="bib1.bibx4" id="paren.30"><named-content content-type="pre">bagging;</named-content></xref> allows for model validation during training, by evaluating each component tree of the random forest with the out-of-bag training examples (training data that were not subsetted in growing the decision tree). Random forest models are advantageous due to the component decision trees being able to resolve complex nonlinear relationships between predictor variables regardless of their interdependencies or cross correlations and the outcome to be predicted. Further, they are relatively easier to visualize and interpret as compared to black-box neural network or deep-learning methods. For the purpose of predictions, random forest models are one of the most accurate machine learning models with the ability to be trained fast due to the parallelizability of the growth of decision trees. For these reasons, random forest is our chosen machine learning tool.</p>
      <p id="d1e699">We utilize a fast implementation <xref ref-type="bibr" rid="bib1.bibx55" id="paren.31"/> of random forest models <xref ref-type="bibr" rid="bib1.bibx5" id="paren.32"/> in R <xref ref-type="bibr" rid="bib1.bibx42" id="paren.33"/> trained on the GCAPM modeled [CCN0.4] detailed in Sect. <xref ref-type="sec" rid="Ch1.S2.SS1"/>. Further details of model development and applications are in Sect. <xref ref-type="sec" rid="Ch1.S3.SS1"/>.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Statistical estimators of model performance</title>
      <p id="d1e723">In this study, we use the Kendall rank correlation coefficient (<inline-formula><mml:math id="M39" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula>) and mean fractional bias (MFB) as statistical estimators of correlation and deviation, respectively. These statistical parameters are more robust (as discussed later in this section) than the conventionally used Pearson product-moment correlation coefficient (<inline-formula><mml:math id="M40" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>) and mean normalized error (MNE) (or similar parameters).</p>
      <p id="d1e740">Pearson product-moment correlation coefficient (<inline-formula><mml:math id="M41" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>) is as follows:
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M42" display="block"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>C</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>C</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msqrt><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>C</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:msqrt><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mrow><mml:msup><mml:mi>C</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          And the Kendall rank correlation coefficient (<inline-formula><mml:math id="M43" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula>) is as follows:
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M44" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9.0}{9.0}\selectfont$\displaystyle}?><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="normal">sign</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>C</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="normal">sign</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>C</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msqrt><mml:mrow><mml:mfenced close=")" open="("><mml:mstyle scriptlevel="+1"><mml:mtable class="substack"><mml:mtr><mml:mtd><mml:mi>n</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">2</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mstyle></mml:mfenced><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:msubsup><mml:mi>t</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi>t</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:msqrt><mml:msqrt><mml:mrow><mml:mfenced close=")" open="("><mml:mstyle scriptlevel="+1"><mml:mtable class="substack"><mml:mtr><mml:mtd><mml:mi>n</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn mathvariant="normal">2</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mstyle></mml:mfenced><mml:mo>-</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:msubsup><mml:mi>t</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>t</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M45" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the sample size, <inline-formula><mml:math id="M46" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> is the value, <inline-formula><mml:math id="M47" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> is the number of ties in the <inline-formula><mml:math id="M48" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>th group of ties, and <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msup><mml:mo>]</mml:mo><mml:mi mathvariant="normal">m</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> denotes modeled and <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msup><mml:mo>]</mml:mo><mml:mi mathvariant="normal">o</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> denotes observed values.</p>
      <p id="d1e1146">As noted in <xref ref-type="bibr" rid="bib1.bibx35" id="text.34"/>:<disp-quote>
  <p id="d1e1153">In the use of Pearson's <inline-formula><mml:math id="M51" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula> are the following assumptions: (1) continuous measurements with pairwise complete observations for the two samples being compared (2) absence of outliers (3) Gaussian distribution of values (4) linearity between the two distributions, with minimal and homogenous variation about the linear fit (homoscedasticity).</p>
  <p id="d1e1163">Kendall's <inline-formula><mml:math id="M52" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> is a nonparametric rank correlation coefficient that is not constrained by the assumptions in the use of Pearson's <inline-formula><mml:math id="M53" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>. This parameter is also intuitive and simpler to interpret due to (a) the maximum possible value of <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicative of complete concordance and the minimum possible value of <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicative of complete discordance and (b) the ratio of concordance to discordance being <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx37" id="paren.35"/>.</p>
</disp-quote></p>
      <p id="d1e1233">MNE and MFB are defined as
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M57" display="block"><mml:mtable rowspacing="0.2ex" class="split" columnspacing="1em" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mtext>MNE</mml:mtext></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mfenced close="|" open="|"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup></mml:mrow><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="normal">and</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mtext>MFB</mml:mtext><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mfenced open="(" close=")"><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:mfenced close=")" open="("><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>C</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">o</mml:mi></mml:msubsup></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          where <inline-formula><mml:math id="M58" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the sample size, <inline-formula><mml:math id="M59" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> is the value, <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msup><mml:mo>]</mml:mo><mml:mi mathvariant="normal">m</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> denotes modeled and <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msup><mml:mo>]</mml:mo><mml:mi mathvariant="normal">o</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> denotes observed values, and <inline-formula><mml:math id="M62" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is the <inline-formula><mml:math id="M63" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>th of their <inline-formula><mml:math id="M64" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> pairs.</p>
      <p id="d1e1438">As noted in <xref ref-type="bibr" rid="bib1.bibx35" id="text.36"/>:<disp-quote>
  <p id="d1e1445">In the use of MNE, it is assumed that observed values are true values and not just estimates. MNE can easily blow up to <inline-formula><mml:math id="M65" display="inline"><mml:mi mathvariant="normal">∞</mml:mi></mml:math></inline-formula> when observed values are very small. Further, positive bias is weighted more than negative bias. Related parameters such as Normalised Mean Bias and Error (NMB and NME) also suffer from these deficiencies. Mean Fractional Bias (MFB) is not limited by the issues in the use of MNE. As a measure of deviation, Mean Fractional Bias (MFB), ranging from <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:mo>[</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, is symmetric about 0 and also not skewed by extreme differences in the compared values.</p>
</disp-quote></p>
      <p id="d1e1476">The following quantitative ranges are provided (arbitrarily) to qualitatively describe the degree of correlation: (1) poor agreement – <inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.2</mml:mn></mml:mrow></mml:math></inline-formula>; (2) fair agreement – <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.2</mml:mn><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.4</mml:mn></mml:mrow></mml:math></inline-formula>; (3) moderate agreement – <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.4</mml:mn><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>; (4) good agreement – <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>); and (5) excellent agreement – <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.8</mml:mn><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula>. Additionally, it is defined (arbitrarily; factor of 1.86 deviation) that there is good agreement between derived and expected values when the MFB is within [<inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>,</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>].</p>
      <p id="d1e1572">Statistical analyses are performed using R: a freely available language and environment for statistical computing and graphics <xref ref-type="bibr" rid="bib1.bibx42" id="paren.37"/> and with the aid of the “Kendall” <xref ref-type="bibr" rid="bib1.bibx32" id="paren.38"/> and    “pcaPP” <xref ref-type="bibr" rid="bib1.bibx11" id="paren.39"/> packages.</p>
</sec>
<?pagebreak page12856?><sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Observational data</title>
      <p id="d1e1592">For validation of the developed RFRM, we use in situ measurements of atmospheric state and composition as inputs to the RFRM and compare the output [CCN0.4] with its measurements. The U.S. Department of Energy's (DOE) ARM Southern Great Plains (SGP) Central Facility located in Lamont, Oklahoma (<inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:mn mathvariant="normal">36</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">36</mml:mn><mml:mo>′</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">18</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> N, <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mn mathvariant="normal">97</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">29</mml:mn><mml:mo>′</mml:mo></mml:msup><mml:msup><mml:mn mathvariant="normal">6</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> W; <inline-formula><mml:math id="M75" display="inline"><mml:mn mathvariant="normal">318</mml:mn></mml:math></inline-formula> m; Fig. <xref ref-type="fig" rid="Ch1.F1"/>) was established with the mission statement of “provid[ing] the climate research community with strategically located in situ and remote-sensing observatories designed to improve the understanding and representation, in climate and earth system models, of clouds and aerosols as well as their interactions and coupling with the Earth's surface”. We use data from this facility, which has the longest record of [CCN0.4] at the hourly resolution.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e1656">The ARM SGP site in Lamont, Oklahoma, USA, with marked locations of the instruments. Legend: meteorology – temperature and relative humidity measurements from the ARM Surface Meteorology Systems (MET) <xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx7" id="paren.40"/>; ACSM – Aerodyne Aerosol Chemical Speciation Monitor <xref ref-type="bibr" rid="bib1.bibx36" id="paren.41"/>; [<inline-formula><mml:math id="M76" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>] – concentrations of <inline-formula><mml:math id="M77" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measured by the ARM Aerosol Observing System <xref ref-type="bibr" rid="bib1.bibx17" id="paren.42"><named-content content-type="pre">AOS;</named-content></xref>; CCNc – cloud condensation nuclei particle counter (CCNc) <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx47 bib1.bibx48 bib1.bibx18" id="paren.43"/>. This image is adapted from satellite imagery © 2020 Maxar Technologies, USDA Farm Service Agency obtained through the Google Maps Static API.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f01.png"/>

        </fig>

<sec id="Ch1.S2.SS4.SSS1">
  <label>2.4.1</label><title>[CCN0.4] measurements</title>
      <p id="d1e1709">[CCN0.4] measurements at this SGP site have been made from 2007 to the present using a cloud condensation nuclei particle counter (CCNc) developed by <xref ref-type="bibr" rid="bib1.bibx44" id="text.44"/> with technical details in <xref ref-type="bibr" rid="bib1.bibx51" id="text.45"/>. The CCNc is a continuous-flow thermal-gradient diffusion chamber for measuring aerosols that can act as CCN. To measure these, aerosol is drawn into a column, where well-controlled and quasi-uniform centerline supersaturation is created. Through software controls, the temperature gradient and flow rate are modified to vary (0.1 %–3 %) supersaturations and obtain CCN spectra. Water vapor condenses on CCN in the sampled air to form droplets, just as cloud drops form in the atmosphere; these activated droplets are counted and sized by an optical particle counter (OPC).</p>
      <p id="d1e1718">We integrate the quality-checked data <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx47 bib1.bibx48 bib1.bibx18" id="paren.46"/> made publicly available through ARM from co-located instruments at the SGP site to form a long-term record of [CCN0.4] as in Fig. <xref ref-type="fig" rid="Ch1.F2"/> and for later analysis and validation of the RFRM.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e1728">Hourly [CCN0.4] measurements at Lamont, Oklahoma, from 2007 to 2020. The orange circles show the data for [CCN0.4] measured here. The purple circles show the data for [CCN0.4] derived from [CCN0.2–0.6] according to the method described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS4.SSS2"/>.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f02.png"/>

          </fig>

<?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page12857?><sec id="Ch1.S2.SS4.SSS2">
  <label>2.4.2</label><title>Filling the [CCN0.4] measurement gaps</title>
      <p id="d1e1750">The temporal range of available observations for [CCN0.4] at the SGP site is 19 May 2007 17:00:00 to  29 January 2020 23:00:00. For this period of 111 319 h, there is only <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">42</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> data completeness. To improve the data coverage, we examine the possibility of using [CCN] for other reported supersaturation ratios (0.2 %–0.6 %).</p>
      <p id="d1e1766">In a sneak preview of the efficacy of random forest for regression, we train random forest models that output [CCN0.4] from [CCN0.2–0.6]. These models are listed in Table <xref ref-type="table" rid="Ch1.T1"/>, with the notation rf_n, where n denotes the supersaturations used as input (for instance, rf_356 indicates [CCN0.3], [CCN0.5], and [CCN0.6] were used as inputs to derive [CCN0.4]). The approach works exceptionally well and shows the potential for application with other datasets to fill in such gaps as well as to perform sanity checks on available data. As reported in Table <xref ref-type="table" rid="Ch1.T1"/>, there is high correlation (Kendall's <inline-formula><mml:math id="M79" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula>) and minimal deviation (interquartile range of mean fractional bias (IQR(MFB)) between random forest derived [CCN0.4] and measured [CCN0.4], when simultaneous data for [CCN0.4] are available.</p>
      <p id="d1e1780">Using this approach, we fill in the missing observations and improve data completeness from <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">42</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">66</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, an increase of <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">54</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, for [CCN0.4] during this period (see Fig. <xref ref-type="fig" rid="Ch1.F2"/>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1828">Evaluation metrics of the random forest models developed to derive [CCN0.4] from other supersaturations.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">RF model</oasis:entry>
         <oasis:entry colname="col2">IQR(MFB)</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M83" display="inline"><mml:mi mathvariant="bold-italic">τ</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">rf_2356</oasis:entry>
         <oasis:entry colname="col2">0.05</oasis:entry>
         <oasis:entry colname="col3">0.93</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_235</oasis:entry>
         <oasis:entry colname="col2">0.06</oasis:entry>
         <oasis:entry colname="col3">0.92</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_256</oasis:entry>
         <oasis:entry colname="col2">0.08</oasis:entry>
         <oasis:entry colname="col3">0.91</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_236</oasis:entry>
         <oasis:entry colname="col2">0.09</oasis:entry>
         <oasis:entry colname="col3">0.91</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_356</oasis:entry>
         <oasis:entry colname="col2">0.10</oasis:entry>
         <oasis:entry colname="col3">0.90</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_25</oasis:entry>
         <oasis:entry colname="col2">0.11</oasis:entry>
         <oasis:entry colname="col3">0.88</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_26</oasis:entry>
         <oasis:entry colname="col2">0.11</oasis:entry>
         <oasis:entry colname="col3">0.89</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_35</oasis:entry>
         <oasis:entry colname="col2">0.11</oasis:entry>
         <oasis:entry colname="col3">0.88</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_56</oasis:entry>
         <oasis:entry colname="col2">0.11</oasis:entry>
         <oasis:entry colname="col3">0.89</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_36</oasis:entry>
         <oasis:entry colname="col2">0.15</oasis:entry>
         <oasis:entry colname="col3">0.87</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">rf_23</oasis:entry>
         <oasis:entry colname="col2">0.25</oasis:entry>
         <oasis:entry colname="col3">0.74</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS4.SSS3">
  <label>2.4.3</label><title>Atmospheric state and composition measurements</title>
      <p id="d1e2006">Meteorological data are sourced from the ARM Surface Meteorology Systems (MET) <xref ref-type="bibr" rid="bib1.bibx19" id="paren.47"/> with technical details in <xref ref-type="bibr" rid="bib1.bibx43" id="text.48"/>. We use the ARM Best Estimate Data Products (ARMBEATM; <xref ref-type="bibr" rid="bib1.bibx7" id="altparen.49"/>) derived from <xref ref-type="bibr" rid="bib1.bibx19" id="text.50"/> when available (1994–2016).</p>
      <p id="d1e2021">Trace gas concentrations are obtained from the ARM Aerosol Observing System (AOS; <xref ref-type="bibr" rid="bib1.bibx17" id="altparen.51"/>) with technical details in <xref ref-type="bibr" rid="bib1.bibx24" id="text.52"/>. Unfortunately, at the SGP site, measurements <xref ref-type="bibr" rid="bib1.bibx49" id="paren.53"/> are available only for <inline-formula><mml:math id="M84" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> from 2016 to the present. To compensate for this, we use data from the United States Environmental Protection Agency (EPA) Air Quality System (AQS) made publicly available at <uri>https://www.epa.gov/air-data</uri> (last access: 20 August 2020) from monitors in the vicinity (<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> km) of the SGP site.</p>
      <p id="d1e2062">Real-time aerosol mass loadings and their chemical composition measurements have been made from 2010 to the present using an Aerodyne aerosol chemical speciation monitor (ACSM; <xref ref-type="bibr" rid="bib1.bibx36" id="altparen.54"/>) with technical details in <xref ref-type="bibr" rid="bib1.bibx54" id="text.55"/>. We use the aerosol chemical speciation data <xref ref-type="bibr" rid="bib1.bibx53 bib1.bibx29 bib1.bibx2" id="paren.56"/>, which are publicly available through ARM.</p>
      <p id="d1e2074">For observation–model simultaneity, all data (atmospheric state, composition, and [CCN0.4]) are integrated to the hourly resolution with their geometric mean.</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>RFRM: training, testing, and optimizing</title>
      <p id="d1e2094">The GCAPM output for 47 sites across the globe, for six selected vertical levels from surface to <inline-formula><mml:math id="M86" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 8 km and for 30 years (1989–2018) at the half-hour time step (<inline-formula><mml:math id="M87" display="inline"><mml:mo lspace="0mm">≈</mml:mo></mml:math></inline-formula> 150 million rows, i.e., sets of predictors and [CCN0.4]) is considered in training the RFRM. The predictors of importance in controlling [CCN0.4] are listed in Table <xref ref-type="table" rid="Ch1.T2"/>. The RFRM is trained on a subset of this data. First, the ARM SGP site is ignored; this is to establish a completely independent analysis with available observational data in Sect. <xref ref-type="sec" rid="Ch1.S3.SS2.SSS2"/>. The remaining GCAPM data for 46 sites and six vertical levels each are partitioned into training (<inline-formula><mml:math id="M88" display="inline"><mml:mo lspace="0mm">≈</mml:mo></mml:math></inline-formula> 101 million rows) and testing sets (<inline-formula><mml:math id="M89" display="inline"><mml:mo lspace="0mm">≈</mml:mo></mml:math></inline-formula> 44 million rows) in a <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mn mathvariant="normal">7</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> ratio. Due to the large number of training and testing examples, these sets are reduced to a 1 % random<?pagebreak page12858?> subset; it is ensured to be representative, with almost identical statistical properties, of the training datasets (Fig. <xref ref-type="fig" rid="Ch1.F3"/>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e2147">Selected atmospheric state and composition variables as RFRM predictors for [CCN0.4].</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">Meteorological </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Temperature</oasis:entry>
         <oasis:entry colname="col2">Precipitation</oasis:entry>
         <oasis:entry colname="col3">RH</oasis:entry>
         <oasis:entry colname="col4">Solar radiation</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">Chemical species </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M91" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M92" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M93" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">OH</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M94" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Isoprene</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M95" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M96" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Monoterpene</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">PM<inline-formula><mml:math id="M98" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciated mass fraction </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M99" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M100" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M101" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">BC</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M102" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">POC</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M103" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">SOA</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M104" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">Dust</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M105" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">Salt</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e2407">Scaled Gaussian kernel density estimate for [CCN0.4] for the training set (dark purple) and each of its subsets (10 %: light purple; 1 %: light orange; 0.1 %: dark orange). The distributions are almost identical. A 1 % randomly sampled subset is used to train the RFRM.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f03.png"/>

        </fig>

      <p id="d1e2417">Once the data have been selected to train the RFRM, we tune the hyperparameters, which govern the training of the machine learning model. The default implementation of <xref ref-type="bibr" rid="bib1.bibx55" id="text.57"/> comes with reasonable (balancing speed and accuracy) choices for these. Based on literature review <xref ref-type="bibr" rid="bib1.bibx40" id="paren.58"><named-content content-type="post">and references therein</named-content></xref> as well as our preliminary examination of RFRMs with varying hyperparameters, we identify the following as most important to optimize: <italic>numtrees</italic> – number of trees in the forest; <italic>mtry</italic> – the minimum number of variables to consider for each split; and <italic>min.node.size</italic> – the minimum node size, i.e., the minimum size of homogeneous data to prevent overfitting. By setting the minimum number of training examples in the terminal nodes of the component trees of the RF, the individual tree depth is controlled, which further mitigates the overfitting associated with decision tree algorithms (discussed in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>). The default hyperparameter values in <xref ref-type="bibr" rid="bib1.bibx55" id="text.59"/> are as follows: <italic>numtrees</italic> <inline-formula><mml:math id="M106" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 500, <italic>mtry</italic> <inline-formula><mml:math id="M107" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> rounded-down square root of the number of variables, and <italic>min.node.size</italic> <inline-formula><mml:math id="M108" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 5. We verify whether these hyperparameter choices are optimal by performing a grid search of the hyperparameters and training multiple random forest models and not just examining their performance with the training set but also additionally with the test set. By evaluating the RFRMs with the test set (data that the machine learning algorithm was not exposed to during its training), additional mitigation of possible overfitting is achieved. Figures <xref ref-type="fig" rid="Ch1.F4"/> and <xref ref-type="fig" rid="Ch1.F5"/> show the results of this exercise.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e2480">RFRM evaluation through OOB error (green), <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> (orange), and IQR(MFB) (purple) with varying hyperparameters. The hyperparameters are (from top to bottom): <italic>numtrees</italic>, <italic>mtry</italic>, and <italic>min.node.size</italic>. Default hyperparameters for each trained model are as follows: <italic>numtrees</italic> <inline-formula><mml:math id="M110" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 500, <italic>mtry</italic> <inline-formula><mml:math id="M111" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4, and <italic>min.node.size</italic> <inline-formula><mml:math id="M112" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 5 – also shown with the vertical black dotted lines when the corresponding default value has been varied.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f04.png"/>

        </fig>

      <p id="d1e2540">Figure <xref ref-type="fig" rid="Ch1.F4"/> has nine panels, as follows from top to bottom:
<list list-type="bullet"><list-item>
      <p id="d1e2547">the top three are for varying number of trees in the random forest: <italic>numtrees</italic> from 1 (a single decision tree) to 1800, through the default choice of 500 (marked with vertical black dotted line);</p></list-item><list-item>
      <p id="d1e2554">the middle three are for varying number of variables considered at each split point: <italic>mtry</italic> from 1 to 19, through the default choice of 4 (marked with vertical black dotted line); and</p></list-item><list-item>
      <p id="d1e2561">the bottom three are for varying minimum size of the terminal nodes: <italic>min.node.size</italic> from 1 to 10, through the default choice of 5 (marked with vertical black dotted line).</p></list-item></list></p>
      <p id="d1e2567">From left to right, the panels are as follows:
<list list-type="bullet"><list-item>
      <p id="d1e2572">the left three (green) show the overall out-of-bag error, i.e., the mean square error for the entire random forest computed using the complement of the bootstrapped data used to train each tree;</p></list-item><list-item>
      <p id="d1e2576">the middle three (orange) show the <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values indicating the explained variance by the random forest; and</p></list-item><list-item>
      <p id="d1e2591">the right three (purple) show the interquartile range of the mean fractional bias of the random forest model when applied to the test set.</p></list-item></list></p>
      <p id="d1e2594">A single decision tree (left-most point in each of the top three panels of Fig. <xref ref-type="fig" rid="Ch1.F4"/>) is able to explain the variance (<inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.81</mml:mn></mml:mrow></mml:math></inline-formula>) in [CCN0.4] through the predictors' variabilities and has an interquartile range in the MFB (which has a median of <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.004</mml:mn></mml:mrow></mml:math></inline-formula>: not pictured as the symmetry of MFB means the median <inline-formula><mml:math id="M116" display="inline"><mml:mo>→</mml:mo></mml:math></inline-formula> 0) of 0.41, which corresponds to a deviation of <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mo>±</mml:mo><mml:mn mathvariant="normal">20</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>. However, this is drastically improved when moving beyond a simple decision tree to even a small ensemble of 30 trees (<inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>≈</mml:mo></mml:mrow></mml:math></inline-formula> 0.91; IQR(MFB) <inline-formula><mml:math id="M119" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 0.27), which plateaus (within a range of <inline-formula><mml:math id="M120" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.0005) after <inline-formula><mml:math id="M121" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 500 trees. The out-of-bag (OOB) error shows a similar trend. Growing a random forest of 500 trees with a <italic>min.node.size</italic> of 5, we see the effect of varying <italic>mtry</italic> in the middle three panels. Instead, keeping the <italic>mtry</italic> fixed at the default value of 4; the rounded<?pagebreak page12859?> down square root of the 19 predictor variables and the random forest performance metrics with varying <italic>min.node.size</italic> are shown in the bottom three panels. Figure <xref ref-type="fig" rid="Ch1.F4"/> thus shows the possibility of improving the random forest derivation of [CCN0.4] by changing the default choices of <xref ref-type="bibr" rid="bib1.bibx55" id="text.60"/> for this specific work. It must be kept in mind that a reasonable cutoff, beyond which there is imperceptible gain in performance at increased computational cost, should be considered.</p>
      <p id="d1e2700">The results shown in Fig. <xref ref-type="fig" rid="Ch1.F4"/> motivate a zoomed-in hyperparameter grid search to choose the optimal (accurate and fast) RFRM. Figure <xref ref-type="fig" rid="Ch1.F5"/> shows this for the best-performing random forest models with <italic>numtrees</italic> ranging from 600 to 1400, <italic>mtry</italic> from 6 to 18, and <italic>min.node.size</italic> from 3 to 6. While there is variability, it must be noted that the <inline-formula><mml:math id="M122" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axes range over 2 %, 0.2 %, and 2 % of the values of OOB error, <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and IQR(MFB), respectively. While, indeed, considering a larger (<italic>numtrees</italic>) forest is beneficial, considering the cost-to-benefit ratio, the hyperparameters we choose are a maximum number of 800 trees in the forest, 12 (<italic>mtry</italic>) variables  randomly chosen at each split, a minimum node size of 3 as the only control on tree depth, and the splitting rule as the minimization of variance. With these hyperparameters, the random forest has IQR(MFB), <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>, and OOB error of <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">100.34</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">99.93</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">100.56</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the best-performing model for each hyperparameter, respectively.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>What the model learns</title>
      <p id="d1e2800">We train the optimized RFRM using the 19 predictors listed in Table <xref ref-type="table" rid="Ch1.T2"/> as predictors of [CCN0.4]; these are as follows: eight fractions of PM<inline-formula><mml:math id="M128" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> (ammonium, sulfate, nitrate, secondary organic aerosol (SOA), black carbon (BC), primary organic carbon (POC), dust, and salt), seven gaseous species (nitrogen oxides (<inline-formula><mml:math id="M129" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), ammonia (<inline-formula><mml:math id="M130" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), ozone (<inline-formula><mml:math id="M131" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), sulfur dioxide (<inline-formula><mml:math id="M132" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), hydroxyl radical (<inline-formula><mml:math id="M133" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:math></inline-formula>), isoprene, and monoterpene), and four meteorological variables (temperature, relative humidity (RH), precipitation, and solar radiation).</p>
      <p id="d1e2867">Figure <xref ref-type="fig" rid="Ch1.F6"/> shows the importance of each predictor in determining the CCN0.4 number concentration in the above-trained RFRM. This importance measure is obtained by randomly permuting values of each predictor to break the association with CCN0.4. Also, the model is fed a pseudo-predictor of randomly generated white noise, labeled “Random” in Fig. <xref ref-type="fig" rid="Ch1.F6"/>. Most important are component mass fractions of PM<inline-formula><mml:math id="M134" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, especially its inorganic fraction (ammonium, sulfate, and nitrate), <inline-formula><mml:math id="M135" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, the other PM<inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> fractions excluding the salt and dust fractions, <inline-formula><mml:math id="M137" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M138" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>. The Random predictor is least important, contributing imperceptibly to the [CCN0.4] prediction.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e2940">RFRM evaluation through OOB error <bold>(a)</bold>, <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> <bold>(b)</bold>, and IQR(MFB) <bold>(c)</bold> with varying hyperparameters selected from the best balanced (accuracy and computational expense) ranges in Fig. <xref ref-type="fig" rid="Ch1.F4"/>.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f05.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e2974">Importance (in decreasing order) of each predictor in the RFRM derivation of [CCN0.4].</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f06.png"/>

        </fig>

      <p id="d1e2983">To quantify the importance of each of the 19 predictors, we do the following: (1) RFRM-Blind – train RFRMs without considering one variable at a time; (2)<?pagebreak page12860?> RFRM-Random – randomize each predictor variable and input into the RFRM. These exercises will provide a more robust, as well as more intuitive measure of the importance of each predictor by analyzing and comparing the deviation in predicted [CCN0.4] compared to the baseline optimized RFRM (hereafter, RFRM-AllVars). Table <xref ref-type="table" rid="Ch1.T3"/> shows the median <inline-formula><mml:math id="M140" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> median absolute deviation of MFB for each such trained RFRM-Blind and RFRM-Random evaluated with the test dataset, with the values for the baseline RFRM-AllVars at the bottom. For the MFB, its median absolute deviation (and even IQR(MFB)) is a stronger indicator of the performance than the median, due to the symmetry of MFB. Examining the median absolute deviation of the MFB, the “Blind” approach shows that the ammonium (PM<inline-formula><mml:math id="M141" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M142" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), sulfate (PM<inline-formula><mml:math id="M143" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M144" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), and secondary organic (PM<inline-formula><mml:math id="M145" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>SOA) fractions of PM<inline-formula><mml:math id="M146" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> are most important (in increasing order) in determining [CCN0.4]. The Blind approach may, however, underestimate the importance of a predictor due to possible correlations with other predictors, as seen in Fig. <xref ref-type="fig" rid="Ch1.F7"/>. These cross correlations could mean the implicit participation of a predictor despite its absence in training the RFRM. To overcome this limitation, in the Random approach, the trained RFRM-AllVars is then input randomized predictors (one at a time) from the testing dataset. This breaks the association of each predictor with the outcome ([CCN0.4]) as well as with other predictors. The resulting change (if any) in the RFRM-AllVars would show the importance of the specific predictor. RFRM-Random for each predictor shows that all predictors (except solar radiation) are important, with the most important being PM<inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>SOA, PM<inline-formula><mml:math id="M148" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M149" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and PM<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M151" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e3105">Mean fractional bias (MFB) of each random forest regression model (RFRM). RFRM-Blind refers to the RFRM trained ignoring the particular predictor. RFRM-Random refers to the randomization of the particular predictor before input into RFRM-AllVars. RFRM-AllVars (at the bottom of the table) is the baseline model where no variable is omitted or randomized. Values are median<inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>±</mml:mo><mml:mspace width="0.25em" linebreak="nobreak"/></mml:mrow></mml:math></inline-formula>median absolute deviation of MFB.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Predictor</oasis:entry>
         <oasis:entry colname="col2">RFRM-Blind</oasis:entry>
         <oasis:entry colname="col3">RFRM-Random</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M153" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M154" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">SOA</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.056</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.261</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.120</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.888</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M157" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M158" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.051</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.238</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.133</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.493</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M161" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M162" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.214</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.079</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.345</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Temperature</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.050</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.221</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.109</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.333</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M167" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.049</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.215</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.059</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.296</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M170" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M171" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">BC</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.211</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.094</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.263</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M174" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M175" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">SALT</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.224</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.054</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.256</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M178" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M179" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">POC</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.211</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.082</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.246</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M182" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.212</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.056</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.239</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M185" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.043</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.058</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.223</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M188" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M189" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.208</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.059</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.223</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PM<inline-formula><mml:math id="M192" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula><inline-formula><mml:math id="M193" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">DUST</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.211</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.056</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.221</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Relative humidity</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.040</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.208</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.047</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.221</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M198" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.046</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.052</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.218</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M201" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Monoterpene</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.045</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.048</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.213</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M204" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">Isoprene</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.046</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.211</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M207" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">OH</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.208</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.048</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.211</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Precipitation</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.046</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.210</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Solar radiation</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.208</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.045</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RFRM-AllVars</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?pagebreak page12861?><p id="d1e3990">Table <xref ref-type="table" rid="Ch1.T3"/> thus shows the importance of each predictor towards determining [CCN0.4] in decreasing order, which complements the results in Fig. <xref ref-type="fig" rid="Ch1.F6"/> that shows the out-of-bag increase in mean square error upon the permutation of a specific predictor. We modify the approach in <xref ref-type="bibr" rid="bib1.bibx55" id="text.61"/> (a) to leverage the advantages of the MFB; (b) to account for any implicit correlations between the data used to train (bagged) and evaluate (out-of-bag) the RFRM by using the unseen testing dataset; and (c) to dissociate the effects of cross correlations between predictors. The results of this modified evaluation of the RFRM are in Table <xref ref-type="table" rid="Ch1.T3"/>. These exercises to probe into the working of the RFRM show that all of the predictors were deemed necessary to capture [CCN0.4] magnitude and variability. The most important predictors are the PM<inline-formula><mml:math id="M215" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciated components, gases including <inline-formula><mml:math id="M216" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M217" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M218" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula>, and temperature and relative humidity.</p>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Comparison with GCAPM [CCN0.4]</title>
      <p id="d1e4064">We examine the RFRM in further detail with the subset of data excluded for testing, i.e., for the sites that RFRM-AllVars has not been exposed to during its training. Figure <xref ref-type="fig" rid="Ch1.F8"/>a shows RFRM-AllVars derived [CCN0.4] against that simulated by GCAPM for all of the testing dataset. RFRM-AllVars predicted [CCN0.4] values are highly correlated with expected values from GCAPM, with a correlation of <inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.88</mml:mn></mml:mrow></mml:math></inline-formula> and highest density along the dashed black line in Fig. <xref ref-type="fig" rid="Ch1.F8"/>a denoting MFB <inline-formula><mml:math id="M220" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0 or complete agreement. The dashed blue and red lines denote <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>&lt;</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>&lt;</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">99.69</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the values are within this factor of 3 times deviation. The dotted lighter blue and red lines denote <inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>&lt;</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>&lt;</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">96.33</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the values are within this range of good agreement between derived and expected [CCN0.4] values.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><label>Figure 7</label><caption><p id="d1e4159">Kendall rank correlation (<inline-formula><mml:math id="M225" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula>) for the 19 predictors and [CCN0.4] in the RFRM training dataset (<inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">101</mml:mn></mml:mrow></mml:math></inline-formula> million rows). The boxes show corresponding <inline-formula><mml:math id="M227" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> value according to color scale. Boxes are divided vertically to represent <inline-formula><mml:math id="M228" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> for each selected model height: surface, <inline-formula><mml:math id="M229" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 1, <inline-formula><mml:math id="M230" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 2, <inline-formula><mml:math id="M231" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 4, <inline-formula><mml:math id="M232" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 6, and <inline-formula><mml:math id="M233" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 8 km.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f07.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><label>Figure 8</label><caption><p id="d1e4237">Binned scatterplot of RFRM versus GCAPM simulated [CCN0.4]. Color bar shows the counts of points in each hexagonal bin. Bins with low counts (<inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of maximum count: <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the data) are shaded gray. The lines indicate MFB of <inline-formula><mml:math id="M236" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> (black; perfect agreement), <inline-formula><mml:math id="M237" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (darker red), <inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (darker blue), <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> (lighter red), and <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> (lighter blue).</p></caption>
            <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f08.png"/>

          </fig>

      <p id="d1e4321">Overall, the RFRM is able to derive [CCN0.4] with a median (median-absolute-deviation) MFB of <inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.4</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">21</mml:mn><mml:mo>)</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>. A comparison to expected [CCN0.4] values from GCAPM in Fig. <xref ref-type="fig" rid="Ch1.F9"/> (a) by means of the MFB shows the robustness of RFRM-AllVars in greater detail. The highest density of MFBs is on or around 0, reiterating how well RFRM-AllVars predictions of [CCN0.4] compares to GCAPM simulated values.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><label>Figure 9</label><caption><p id="d1e4345">Mean fractional bias (MFB) of RFRM derived [CCN0.4] compared to expected values from GCAPM in the testing dataset (441 756 values). Histogram shows the counts of the pairs by MFB. The lines indicate perfect agreement (black), MFB of <inline-formula><mml:math id="M242" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (dashed red), and MFB of <inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (dashed blue). The dotted lines indicate MFB of <inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> (dotted red) and <inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> (dotted blue).</p></caption>
            <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f09.png"/>

          </fig>

      <p id="d1e4394">Figure <xref ref-type="fig" rid="Ch1.F8"/>a is faceted by height in Fig. <xref ref-type="fig" rid="Ch1.F8"/>b. Across the various heights, with varied [CCN0.4] ranges, RFRM-AllVars performs robustly with <inline-formula><mml:math id="M246" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>. Its robustness across varied [CCN0.4] ranges is further shown in Fig. <xref ref-type="fig" rid="Ch1.F9"/>b, where Fig. <xref ref-type="fig" rid="Ch1.F9"/>a is faceted by the deciles of the GCAPM simulated [CCN0.4]. RFRM-AllVars performs well over 4 orders of magnitude of [CCN0.4] from <inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">0</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M248" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.7</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">4</mml:mn></mml:msup><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Comparisons for the SGP site</title>
      <p id="d1e4467">We also examine the temporal trends of [CCN0.4] for the SGP site (the surface <inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> model grid box), which was completely excluded from the RFRM training. Figure <xref ref-type="fig" rid="Ch1.F10"/> shows the weekly-aggregated time series from 1989 to 2018 for (a) GCAPM simulated and (b) RFRM-AllVars derived [CCN0.4]. Also shown in Fig. <xref ref-type="fig" rid="Ch1.F10"/>d is the comparison, using MFB, of the derived [CCN0.4] of RFRM-AllVars versus the GCAPM [CCN0.4] values. The RFRM performs well, being able to capture weekly variations with good correlation (<inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.68</mml:mn></mml:mrow></mml:math></inline-formula>) and low deviation (<inline-formula><mml:math id="M251" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">99.87</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> within the good agreement range of <inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10"><?xmltex \currentcnt{10}?><label>Figure 10</label><caption><p id="d1e4537">Time series (weekly-aggregated) for the surface <inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> GCAPM grid box containing the SGP site – <bold>(a)</bold> GCAPM simulated, <bold>(b)</bold> RFRM-AllVars, and <bold>(c)</bold> RFRM-ShortVars derived [CCN0.4] – and the mean fractional bias (MFB) of <bold>(d)</bold>  RFRM-AllVars and <bold>(e)</bold> RFRM-ShortVars. Dotted lines show the good agreement range of <inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f10.png"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS2.SSSx1" specific-use="unnumbered">
  <title>RFRM application: measured predictors as input</title>
      <p id="d1e4603">As detailed in Sect. <xref ref-type="sec" rid="Ch1.S2.SS4"/>, there are numerous observations of atmospheric state and composition for the SGP site that can be utilized to validate the RFRM with empirical data. In an ideal situation, continuous, long-term, high-quality measurements for all the inputs to the RFRM (the predictor variables listed in Table <xref ref-type="table" rid="Ch1.T2"/>) would have aided in this analysis. However, due to the sparsity and absence of measurements of certain predictors, we are limited to the available factors listed in Table <xref ref-type="table" rid="Ch1.T4"/>. These are shown in Fig. <xref ref-type="fig" rid="Ch1.F11"/>, with the speciated PM<inline-formula><mml:math id="M255" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> predictors in Fig. <xref ref-type="fig" rid="Ch1.F11"/>a, the trace gas measurements in Fig. <xref ref-type="fig" rid="Ch1.F11"/>b, and the meteorological variables in Fig. <xref ref-type="fig" rid="Ch1.F11"/>c.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><label>Figure 11</label><caption><p id="d1e4632">Time series (daily-aggregated) for predictors at the ARM SGP site: <bold>(a)</bold> PM<inline-formula><mml:math id="M256" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciation; <bold>(b)</bold> trace gas; and <bold>(c)</bold> meteorological measurements.</p></caption>
            <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f11.png"/>

          </fig>

      <p id="d1e4659">Thus, with a reduction from <inline-formula><mml:math id="M257" display="inline"><mml:mn mathvariant="normal">19</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M258" display="inline"><mml:mn mathvariant="normal">9</mml:mn></mml:math></inline-formula> predictor variables, we retrain the RFRM to use only these as inputs to derive [CCN0.4]. The RFRM optimization is carried out as described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>; the RFRM hyperparameters are <inline-formula><mml:math id="M259" display="inline"><mml:mrow><mml:mtext mathvariant="italic">numtrees</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M260" display="inline"><mml:mrow><mml:mtext mathvariant="italic">mtry</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:mtext mathvariant="italic">min.node.size</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> and use the nine predictors listed in Table <xref ref-type="table" rid="Ch1.T4"/> to derive [CCN0.4]. This retrained RFRM (henceforth, RFRM-ShortVars) is evaluated using the testing dataset; with median (median-absolute-deviation) MFB deteriorating from <inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.044</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0.209</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.184</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0.382</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M264" display="inline"><mml:mn mathvariant="normal">96.33</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mn mathvariant="normal">80.30</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the derived [CCN0.4] values in the good agreement range, and correlation reducing from <inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.88</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M267" display="inline"><mml:mn mathvariant="normal">0.79</mml:mn></mml:math></inline-formula>. While RFRM-ShortVars is less<?pagebreak page12862?> robust compared to RFRM-AllVars, the statistical estimators of model performance are still high for RFRM-ShortVars.</p>
      <p id="d1e4785">Specifically for the SGP site, Fig. <xref ref-type="fig" rid="Ch1.F10"/>c and e show the weekly-aggregated RFRM-ShortVars derived [CCN0.4] and its comparison with the GCAPM [CCN0.4] values, respectively. RFRM-ShortVars performs well, being able to capture these variations with good correlation (<inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.66</mml:mn></mml:mrow></mml:math></inline-formula>) and low deviation (<inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">98.72</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> within the good agreement range).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><?xmltex \currentcnt{4}?><label>Table 4</label><caption><p id="d1e4819">RFRM predictors for [CCN0.4] as listed in Table <xref ref-type="table" rid="Ch1.T2"/>. Italicized text shows those predictors determined (in Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>) to not strongly impact RFRM prediction of [CCN0.4]. Bold text shows the absence of their hourly measurements.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">Meteorological </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Temperature</oasis:entry>
         <oasis:entry colname="col2"><italic>Precipitation</italic></oasis:entry>
         <oasis:entry colname="col3">RH</oasis:entry>
         <oasis:entry colname="col4"><italic>Solar radiation</italic></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">Chemical species </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M279" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M280" display="inline"><mml:mrow><mml:mo mathvariant="bold">[</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">NH</mml:mi><mml:mn mathvariant="bold-italic">3</mml:mn></mml:msub><mml:mo mathvariant="bold">]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><bold>
                      <italic>[OH]</italic>
                    </bold></oasis:entry>
         <oasis:entry colname="col4"><bold>
                      <italic>[Isoprene]</italic>
                    </bold></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M281" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M282" display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4"><bold>
                      <italic>[Monoterpene]</italic>
                    </bold></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="center">PM<inline-formula><mml:math id="M283" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciated mass fraction </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M284" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M285" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M286" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><bold>BC</bold></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M287" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">POC</mml:mi></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M288" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M289" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">SOA</mml:mi></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M290" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><bold>
                      <italic>Dust</italic>
                    </bold></oasis:entry>
         <oasis:entry colname="col4"><bold>
                      <italic>Salt</italic>
                    </bold><inline-formula><mml:math id="M291" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e4826">Note: <inline-formula><mml:math id="M270" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> measurements for PM<inline-formula><mml:math id="M271" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M272" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">POC</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M273" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">SOA</mml:mi></mml:mrow></mml:math></inline-formula> are reported as PM<inline-formula><mml:math id="M274" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M275" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">OC</mml:mi></mml:mrow></mml:math></inline-formula> (total organic carbon). <inline-formula><mml:math id="M276" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> For PM<inline-formula><mml:math id="M277" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> salt, PM<inline-formula><mml:math id="M278" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> chloride measurements are available but subject to a large percent of missing data.</p></table-wrap-foot></table-wrap>

      <p id="d1e5168">Using measurements of the nine predictor variables at the SGP site for 2010–2020, we use the developed RFRM-ShortVars to derive [CCN0.4]. Compared to [CCN0.4] measurements, the RFRM performs well, with <inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.36</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">67</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>. We note that filling the measurement gaps (per Sect. <xref ref-type="sec" rid="Ch1.S2.SS4.SSS2"/>) could contribute to this observed decrease in RFRM performance (from RFRM-AllVars <inline-formula><mml:math id="M295" display="inline"><mml:mo>→</mml:mo></mml:math></inline-formula> RFRM-ShortVars). However, this contribution is minimal: when comparing the RFRM-ShortVars-derived [CCN0.4] with measurements excluding the filled-in [CCN0.4], Kendall's <inline-formula><mml:math id="M296" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> correlation increased from <inline-formula><mml:math id="M297" display="inline"><mml:mn mathvariant="normal">0.36</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math id="M298" display="inline"><mml:mn mathvariant="normal">0.42</mml:mn></mml:math></inline-formula> and the percentage within the good-agreement range from <inline-formula><mml:math id="M299" display="inline"><mml:mrow><mml:mn mathvariant="normal">67.02</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:mn mathvariant="normal">69.34</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, with the sample size <inline-formula><mml:math id="M301" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> reducing from <inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:mn mathvariant="normal">39</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">811</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M303" display="inline"><mml:mrow><mml:mn mathvariant="normal">29</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mn mathvariant="normal">047</mml:mn></mml:mrow></mml:math></inline-formula>. The deteriorated performance is mainly due to the reduction in necessary predictors to the available ones; the uncertainties associated with the measurements themselves may compound this. Regardless, the variability from diurnal to decadal scales is captured by the RFRM (top-left panel in Fig. <xref ref-type="fig" rid="Ch1.F12"/>a) when compared to the measurements (bottom-left panel in Fig. <xref ref-type="fig" rid="Ch1.F12"/>a) of [CCN0.4]. For reference, in Fig. <xref ref-type="fig" rid="Ch1.F12"/>a the top-right and bottom-right panels are the same as in Fig. <xref ref-type="fig" rid="Ch1.F10"/>c and a, respectively, but for this period of measurements.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><label>Figure 12</label><caption><p id="d1e5305"><bold>(a)</bold> Time series (daily-aggregated) for [CCN0.4] derived by RFRM-ShortVars (top two) and ORF (middle two), compared to SGP measured (bottom-left) and GCAPM-simulated (bottom-right). <bold>(b)</bold> Performance comparison of the models in quantifying [CCN0.4] compared to its measured values for the SGP site: left – GCAPM; center – RFRM-ShortVars with measurements of predictors as input; right – RFRM-ShortVars with GCAPM-simulated predictors as input. The summary performance metrics are <inline-formula><mml:math id="M304" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula>: Kendall's rank correlation coefficient and %-Agree: the percentage of pairwise model–observation compared values within the good-agreement range defined as <inline-formula><mml:math id="M305" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn><mml:mo>&lt;</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>&lt;</mml:mo><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>.</p></caption>
            <?xmltex \igopts{width=503.61378pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f12.png"/>

          </fig>

</sec>
<?pagebreak page12863?><sec id="Ch1.S3.SS2.SSSx2" specific-use="unnumbered">
  <title>Performance comparison of RFRM and GCAPM</title>
      <p id="d1e5352">Figure <xref ref-type="fig" rid="Ch1.F12"/>b compares GCAPM and RFRM performance in quantifying [CCN0.4] for SGP with respect to its measurements corresponding to Fig. <xref ref-type="fig" rid="Ch1.F12"/>a. In the left-hand panel, GCAPM simulated [CCN0.4] shows fair correlation (<inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.27</mml:mn></mml:mrow></mml:math></inline-formula>) with SGP measurements and 65 % within the good-agreement range. The general tendency is overestimation (<inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:mtext>median MFB</mml:mtext><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula>), seen as higher density above the perfect agreement line (dashed black). RFRM-ShortVars derives [CCN0.4] (Fig. <xref ref-type="fig" rid="Ch1.F12"/>b: center) to a greater degree of agreement than GCAPM does, with <inline-formula><mml:math id="M308" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula> % and <inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">75</mml:mn></mml:mrow></mml:math></inline-formula> % with <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M311" display="inline"><mml:mrow><mml:mtext>median MFB</mml:mtext><mml:mo>≈</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> indicating a slight tendency to underestimate.</p>
      <p id="d1e5438">It is to be recalled that the GCAPM [CCN0.4] is more reflective of regional tendencies, simulating [CCN0.4] for a <inline-formula><mml:math id="M312" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">2.5</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grid box around the SGP site. The RFRM is trained on GCAPM, from where the associations were learned between atmospheric state and composition variables and [CCN0.4], thus implicitly imbibing the effect of physical and chemical processes that control particle number concentrations. That RFRM-ShortVars-derived [CCN0.4] is better representative is a demonstration that these processes are well-represented within GCAPM. Leveraging this aspect as well as utilizing localized conditions (actual measurements) of atmospheric state and composition, the RFRM performs significantly better than GCAPM. These results and the ability to capture the variability of [CCN0.4] across temporal scales demonstrate the derivation of [CCN0.4] through the more commonly available measurements of meteorology: atmospheric chemical species including speciation of particulate matter.</p>
      <p id="d1e5460">The right-hand panel of Fig. <xref ref-type="fig" rid="Ch1.F12"/>b shows how RFRM-ShortVars performs when using GCAPM simulated values of the input predictor variables.  <inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.24</mml:mn></mml:mrow></mml:math></inline-formula> and 71 % with <inline-formula><mml:math id="M314" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> indicates that the RFRM model performance is comparable to GCAPM for the SGP site in alignment with our observations in Sect. <xref ref-type="sec" rid="Ch1.S3.SS2.SSS1"/>. This is encouraging towards further development of this machine learning approach for potential application in Earth system models (ESMs). The random forest technique discussed here has two key virtues: (1) its computational advantages as discussed in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/> and (2) its learning from a state-of-the-science chemical transport model coupled with size-resolved microphysics. In ESMs, where the demand for computational efficiency results in using simplified bulk microphysical treatment, the RFRM can provide a more accurate representation of particle numbers, especially those that mediate aerosol–cloud interactions, while remaining computationally efficient.</p>
</sec>
<sec id="Ch1.S3.SS2.SSSx3" specific-use="unnumbered">
  <title>RFRM trained using measurements</title>
      <p id="d1e5503">Development of the machine learning model generally requires a large number of training examples; however, we also investigate the possibility of developing an RFRM with<?pagebreak page12864?> the measurement data alone. The RFRM optimization is carried out as described in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>; this RFRM trained on actual measurements at SGP has <inline-formula><mml:math id="M315" display="inline"><mml:mrow><mml:mtext mathvariant="italic">numtrees </mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1000</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M316" display="inline"><mml:mrow><mml:mtext mathvariant="italic">mtry</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M317" display="inline"><mml:mrow><mml:mtext mathvariant="italic">min.node.size</mml:mtext><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula>. Compared to the RFRM trained on GCAPM simulated data (<inline-formula><mml:math id="M318" display="inline"><mml:mo lspace="0mm">≈</mml:mo></mml:math></inline-formula> 150 million training examples), such an RFRM has only <inline-formula><mml:math id="M319" display="inline"><mml:mo>≈</mml:mo></mml:math></inline-formula> 34 000 training examples for the SGP site. We train such an RFRM, henceforth denoted as ORF (observation-based random forest regression model), and examine its performance.</p>
      <p id="d1e5559">In comparison with SGP measured [CCN0.4], ORF shows correlation of <inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.53</mml:mn></mml:mrow></mml:math></inline-formula> and good agreement with <inline-formula><mml:math id="M321" display="inline"><mml:mrow><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">81.22</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of its derived [CCN0.4] values. The time series (daily-aggregated) of ORF-derived [CCN0.4] is shown in Fig. <xref ref-type="fig" rid="Ch1.F12"/>a, with measured predictors as input to the RFRM in the middle-left panel and GCAPM predictors as input to the RFRM in the middle-right panel. In Fig. <xref ref-type="fig" rid="Ch1.F13"/>b ORF-derived [CCN0.4] is compared to hourly measurements. ORF appears to perform better than RFRM-ShortVars from the summary statistics. However, it is unable to capture the range of variations in magnitude (middle-left panel in Fig. <xref ref-type="fig" rid="Ch1.F12"/>a). Similar results are observed (Figs. <xref ref-type="fig" rid="Ch1.F13"/>d and  <xref ref-type="fig" rid="Ch1.F12"/>a middle-right) when ORF is applied to GCAPM simulated data. This exercise of developing an observation-based RFRM is, however, not technically justifiable due to the small number of training examples and applicability to only the SGP site. Regardless, this exercise provides insight into whether considering only 9 out of the 19 required predictor variables is sufficient for RFRM-ShortVars, an examination of which suggests the affirmative. Further, this exercise is insightful in demonstrating the unlikelihood of missing any important predictor in the RFRM, providing an additional check on the importance of the RFRM predictors, and the potential utility of this machine learning approach being trained directly, without a physicochemically informed model, on atmospheric state and composition measurements to derive [CCN0.4].</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><?xmltex \currentcnt{13}?><label>Figure 13</label><caption><p id="d1e5600">Mean fractional bias (MFB) of the random forest derived [CCN0.4] compared to expected values. <bold>(a, b)</bold> Comparison with measured [CCN0.4]. <bold>(c, d)</bold> Comparison with GCAPM simulated [CCN0.4]. The histograms show the pairwise counts (total is inset top-left in each panel) by MFB. The lines indicate MFB of <inline-formula><mml:math id="M322" display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula> (black), <inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (dashed red), <inline-formula><mml:math id="M324" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> (dashed blue), <inline-formula><mml:math id="M325" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> (dotted red), and <inline-formula><mml:math id="M326" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> (dotted blue). The percentage of RFRM derived values in good (<inline-formula><mml:math id="M327" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) and fair (<inline-formula><mml:math id="M328" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) agreement are shown close to the <inline-formula><mml:math id="M329" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M330" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> MFB lines, respectively.</p></caption>
            <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/12853/2020/acp-20-12853-2020-f13.png"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Summary</title>
      <p id="d1e5725">We develop an RFRM to predict the number concentrations of cloud condensation nuclei at 0.4 % supersaturation ([CCN0.4]) from atmospheric state and composition variables. This RFRM, trained on 30-year simulations by a chemical transport model (GEOS-Chem) with a detailed microphysics scheme (APM), is able to predict [CCN0.4] values. The RFRM learns that the PM<inline-formula><mml:math id="M331" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> fractions (except salt and dust) and gases such as <inline-formula><mml:math id="M332" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M333" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the most important determinants of [CCN0.4]. The RFRM is robust in its derivation of [CCN0.4], with a median (median-absolute-deviation) mean fractional bias of <inline-formula><mml:math id="M334" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.4</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">21</mml:mn><mml:mo>)</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M335" display="inline"><mml:mrow><mml:mn mathvariant="normal">96.33</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the derived values within the good agreement range (<inline-formula><mml:math id="M336" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:mtext>MFB</mml:mtext><mml:mo>|</mml:mo><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.6</mml:mn></mml:mrow></mml:math></inline-formula>) and strong correlation of Kendall's <inline-formula><mml:math id="M337" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.88</mml:mn></mml:mrow></mml:math></inline-formula> for various locations around the globe, at various altitudes in the troposphere, and across a varied range of [CCN0.4] magnitudes. We also demonstrate the application of this technique for deriving [CCN0.4] from measurements of [CCN] at other supersaturations. For a location in the Southern Great Plains region of the United States, using real measurements as input to the RFRM demonstrates its applicability. To use the measurement data as input to the RFRM required its tweaking to account for unavailable<?pagebreak page12865?> measurements for certain predictors. The truncated RFRM performs robustly despite these adjustments: median (median-absolute-deviation) MFB of <inline-formula><mml:math id="M338" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">18</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">38</mml:mn><mml:mo>)</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M339" display="inline"><mml:mrow><mml:mn mathvariant="normal">80.30</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the derived [CCN0.4] in good agreement and strong correlation of Kendall's <inline-formula><mml:math id="M340" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.79</mml:mn></mml:mrow></mml:math></inline-formula>. Specifically for the ARM SGP site, using measured predictors as input to the RFRM and comparison with measured [CCN0.4], the median (median-absolute-deviation) MFB is <inline-formula><mml:math id="M341" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">61</mml:mn><mml:mo>)</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> with <inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:mn mathvariant="normal">67.02</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> of the derived [CCN0.4] in good agreement and Kendall's correlation coefficient <inline-formula><mml:math id="M343" display="inline"><mml:mrow><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>≈</mml:mo><mml:mn mathvariant="normal">0.36</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Further discussion and outlook</title>
      <p id="d1e5908">There are a number of limitations in the application of the present study to augment empirical measurements of [CCN]. These are as follows:
<list list-type="bullet"><list-item>
      <?pagebreak page12866?><p id="d1e5913">The RFRM is trained on GCAPM, with the assumption that the physical and chemical processes that relate the “predictor” variables to the [CCN0.4] outcome are accurate. Previous studies show that GCAPM performs reasonably when compared to observations, but uncertainties in both model and observation may contribute to uncertainties in the RFRM derivation.</p></list-item><list-item>
      <p id="d1e5917">Co-located and simultaneous (with [CCN0.4] measurements) measurements of the required predictor variables were available only for certain predictors. We had to retrain the RFRM to account for these constraints, which sacrificed its accuracy in deriving [CCN0.4]. Other issues with measurements arise from the limitations of their accuracy, precision, and detection limits. Further sources of error are the utilization of predictor measurements from nearby (but not co-located) monitors to fill in significant gaps in the required data for the SGP site.</p></list-item><list-item>
      <p id="d1e5921">Random forest was the machine learning tool of choice due to its parallelizability and high degree of accuracy. There are, however, other tools such as XGBoost (a choice for many winners of machine learning competitions) or regression neural networks. These, among others, could offer improved [CCN0.4] derivation. A cursory examination for the present study, however, showed no significant improvement at the cost of much higher computational expense.</p></list-item><list-item>
      <p id="d1e5925">To overcome some of the gaps in the [CCN0.4] measurement data from the SGP site, we proposed and implemented a derivation of [CCN0.4] from [CCN] measurements at other supersaturations using the random forest technique. While this derivation was confirmed to be exceptionally good, this is an approximation.</p></list-item><list-item>
      <p id="d1e5929">Development of an observation-based RFRM is presented in this study. However, it can be significantly improved with more observations for the SGP site, and generalizable if trained with observations from numerous other sites. This was presently not possible.</p></list-item></list></p>
      <p id="d1e5932">Despite the caveats associated with this work, this proof of concept shows promise for wide-ranging development and deployment. This machine learning approach can provide improved representation of cloud condensation nuclei numbers:
<list list-type="bullet"><list-item>
      <p id="d1e5937">in locations where their direct measurements are limited, but measurements of other atmospheric state and composition variables are available. Typically, since measurements of PM<inline-formula><mml:math id="M344" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> speciation, trace gases, and meteorology are easier than those of [CCN0.4], there are longer and more widely (spatially) distributed in<?pagebreak page12867?> situ measurement records, especially through air quality monitoring networks. The developed RFRM can derive [CCN0.4] from these ubiquitous measurements to complement [CCN0.4] measurements when available and fill in the gaps in their absence.</p></list-item><list-item>
      <p id="d1e5950">in Earth system models:
<list list-type="bullet"><list-item>
      <p id="d1e5955">by providing a more accurate alternative to bulk microphysical parameterizations</p></list-item><list-item>
      <p id="d1e5959">by providing a computationally less intensive alternative to explicit bin-resolving microphysics models.</p></list-item></list></p></list-item></list></p>
      <p id="d1e5962">This work is an initial step towards fast and accurate derivation of [CCN0.4], in the absence of its measurements, constrained by empirical data for other measurements of atmospheric state and composition. This work demonstrates the possible applications of machine learning tools in handling the complex, nonlinear, ordinal, and large amounts of data in the atmospheric sciences.</p>
</sec>
</sec>

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

      <p id="d1e5971">Data for training the RFRM are generated by GEOS-Chem, a grass-roots open-access model available at git://git.as.harvard.edu/bmy/GEOS-Chem (<xref ref-type="bibr" rid="bib1.bibx3" id="altparen.62"/>, last access: 20 August 2020). Model training and analysis of predictions in this study are though the free software environment for statistical computing and graphics R (<uri>https://www.r-project.org/</uri>, <xref ref-type="bibr" rid="bib1.bibx42" id="altparen.63"/>) and facilitated mainly by the “ranger” package (<uri>https://cran.r-project.org/web/packages/ranger/index.html</uri>, <xref ref-type="bibr" rid="bib1.bibx55" id="altparen.64"/>). Data were obtained from the Atmospheric Radiation Measurement (ARM) user facility, a U.S. Department of Energy (DOE) Office of Science User Facility managed by the Biological and Environmental Research program, which is publicly available at the ARM Discovery Data Portal at <uri>https://www.archive.arm.gov/discovery/</uri> (<xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx7 bib1.bibx36 bib1.bibx17 bib1.bibx46 bib1.bibx47 bib1.bibx48 bib1.bibx18" id="altparen.65"/>, last access: 20 August 2020) and the EPA AirData Portal at <uri>https://www.epa.gov/air-data/</uri> (last access: 20 August 2020).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e6002">AAN and FY were jointly responsible for conceptualization, data curation, formal analysis, investigation, methodology, project administration, resources, software, validation, visualization, writing of the original draft, and review and editing of the paper. In addition, FY carried out funding acquisition and supervision.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e6008">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e6014">We thank the DOE ARM SGP Research Facility and EPA Air Quality Analysis Group data teams for the operation and maintenance of instruments, quality checks, and making these measurement data publicly available.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e6019">This research has been supported by the National Science Foundation, Division of Atmospheric and Geospace Sciences (grant no. AGS-1550816), the National Aeronautics and Space Administration (grant no. NNX17AG35G), and the New York State Energy Research and Development Authority (grant no. 137487).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e6025">This paper was edited by Gordon McFiggans and reviewed by two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bibx1"><label>Albrecht(1989)</label><?label Albrecht_1989?><mixed-citation>Albrecht, B. A.: Aerosols, Cloud Microphysics, and Fractional Cloudiness,
Science, 245, 1227–1230, <ext-link xlink:href="https://doi.org/10.1126/science.245.4923.1227" ext-link-type="DOI">10.1126/science.245.4923.1227</ext-link>, 1989.</mixed-citation></ref>
      <ref id="bib1.bibx2"><label>Behrens et al.(1990)</label><?label acsmBehrens1990?><mixed-citation>Behrens, B., Salwen, C., Springston, S., and Watson, T.: ARM: AOS: aerosol
chemical speciation monitor, <ext-link xlink:href="https://doi.org/10.5439/1046180" ext-link-type="DOI">10.5439/1046180</ext-link>, 1990.</mixed-citation></ref>
      <ref id="bib1.bibx3"><label>Bey et al.(2001)</label><?label Bey_2001?><mixed-citation>Bey, I., Jacob, D. J., Yantosca, R. M., Logan, J. A., Field, B. D., Fiore,
A. M., Li, Q., Liu, H. Y., Mickley, L. J., and Schultz, M. G.: Global
modeling of tropospheric chemistry with assimilated meteorology: Model
description and evaluation, J. Geophys. Res.-Atmos.,
106, 23073–23095, <ext-link xlink:href="https://doi.org/10.1029/2001JD000807" ext-link-type="DOI">10.1029/2001JD000807</ext-link>, 2001.</mixed-citation></ref>
      <ref id="bib1.bibx4"><label>Breiman(1996)</label><?label Breiman_1996?><mixed-citation>Breiman, L.: Bagging predictors, Mach. Learn., 24, 123–140,
<ext-link xlink:href="https://doi.org/10.1007/bf00058655" ext-link-type="DOI">10.1007/bf00058655</ext-link>, 1996.</mixed-citation></ref>
      <ref id="bib1.bibx5"><label>Breiman(2001)</label><?label Breiman_2001?><mixed-citation>Breiman, L.: Random forests, Mach. Learn., 45, 5–32,
<ext-link xlink:href="https://doi.org/10.1023/A:1010933404324" ext-link-type="DOI">10.1023/A:1010933404324</ext-link>, 2001.</mixed-citation></ref>
      <ref id="bib1.bibx6"><label>Breiman et al.(1984)</label><?label Breiman_1984?><mixed-citation>Breiman, L., Friedman, J. H., Olshen, R. A., and Stone, C. J.: Classification
And Regression Trees, Routledge, <ext-link xlink:href="https://doi.org/10.1201/9781315139470" ext-link-type="DOI">10.1201/9781315139470</ext-link>, 1984.</mixed-citation></ref>
      <ref id="bib1.bibx7"><label>Chen and Xie(1994)</label><?label Chen1994?><mixed-citation>Chen, X. and Xie, S.: ARM: ARMBE: Atmospheric measurements,
<ext-link xlink:href="https://doi.org/10.5439/1095313" ext-link-type="DOI">10.5439/1095313</ext-link>, 1994.</mixed-citation></ref>
      <ref id="bib1.bibx8"><label>Christopoulos et al.(2018)</label><?label Christopoulos_2018?><mixed-citation>Christopoulos, C. D., Garimella, S., Zawadowicz, M. A., Möhler, O., and
Cziczo, D. J.: A machine learning approach to aerosol classification for
single-particle mass spectrometry, Atmos. Meas. Tech., 11,
5687–5699, <ext-link xlink:href="https://doi.org/10.5194/amt-11-5687-2018" ext-link-type="DOI">10.5194/amt-11-5687-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx9"><label>Dou and Yang(2018)</label><?label Dou_2018?><mixed-citation>Dou, X. and Yang, Y.: Comprehensive evaluation of machine learning techniques
for estimating the responses of carbon fluxes to climatic forces in different
terrestrial ecosystems, Atmosphere, 9, 83, <ext-link xlink:href="https://doi.org/10.3390/atmos9030083" ext-link-type="DOI">10.3390/atmos9030083</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx10"><label>Evans and Jacob(2005)</label><?label Evans_2005?><mixed-citation>Evans, M. and Jacob, D. J.: Impact of new laboratory studies of N<inline-formula><mml:math id="M345" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O<inline-formula><mml:math id="M346" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:math></inline-formula> hydrolysis
on global model budgets of tropospheric nitrogen oxides, ozone, and OH,
Geophys. Res. Lett., 32, L09813, <ext-link xlink:href="https://doi.org/10.1029/2005GL022469" ext-link-type="DOI">10.1029/2005GL022469</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx11"><label>Filzmoser et al.(2018)</label><?label RpcaPP?><mixed-citation>Filzmoser, P., Fritz, H., and Kalcher, K.: pcaPP: Robust PCA by Projection
Pursuit, available at: <uri>https://CRAN.R-project.org/package=pcaPP</uri> (last access: 20 August 2020), r package
version 1.9-73, 2018.</mixed-citation></ref>
      <?pagebreak page12868?><ref id="bib1.bibx12"><label>Fountoukis and Nenes(2007)</label><?label Fountoukis_2007?><mixed-citation>Fountoukis, C. and Nenes, A.: ISORROPIA II: a computationally efficient thermodynamic equilibrium model for K<inline-formula><mml:math id="M347" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>–Ca<inline-formula><mml:math id="M348" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–Mg<inline-formula><mml:math id="M349" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–NH<inline-formula><mml:math id="M350" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–Na<inline-formula><mml:math id="M351" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>–SO<inline-formula><mml:math id="M352" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="normal">−</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>–NO<inline-formula><mml:math id="M353" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mi mathvariant="normal">−</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>–Cl<inline-formula><mml:math id="M354" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">−</mml:mi></mml:msup></mml:math></inline-formula>–H<inline-formula><mml:math id="M355" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O aerosols, Atmos. Chem. Phys., 7, 4639–4659, <ext-link xlink:href="https://doi.org/10.5194/acp-7-4639-2007" ext-link-type="DOI">10.5194/acp-7-4639-2007</ext-link>, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx13"><label>Fuchs et al.(2018)</label><?label Fuchs_2018?><mixed-citation>Fuchs, J., Cermak, J., and Andersen, H.: Building a cloud in the southeast
Atlantic: understanding low-cloud controls based on satellite observations
with machine learning, Atmos. Chem. Phys., 18,
16537–16552, <ext-link xlink:href="https://doi.org/10.5194/acp-18-16537-2018" ext-link-type="DOI">10.5194/acp-18-16537-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx14"><label>Giglio et al.(2013)</label><?label Giglio_2013?><mixed-citation>Giglio, L., Randerson, J. T., and van der Werf, G. R.: Analysis of daily,
monthly, and annual burned area using the fourth-generation global fire
emissions database (GFED4), J. Geophys. Res.-Biogeo., 118, 317–328, <ext-link xlink:href="https://doi.org/10.1002/jgrg.20042" ext-link-type="DOI">10.1002/jgrg.20042</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx15"><label>Grange et al.(2018)</label><?label Grange_2018?><mixed-citation>Grange, S. K., Carslaw, D. C., Lewis, A. C., Boleti, E., and Hueglin, C.:
Random forest meteorological normalisation models for Swiss <inline-formula><mml:math id="M356" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">PM</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
trend analysis, Atmos. Chem. Phys., 18, 6223–6239,
<ext-link xlink:href="https://doi.org/10.5194/acp-18-6223-2018" ext-link-type="DOI">10.5194/acp-18-6223-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx16"><label>Guenther et al.(2012)</label><?label Guenther_2012?><mixed-citation>Guenther, A. B., Jiang, X., Heald, C. L., Sakulyanontvittaya, T., Duhl, T.,
Emmons, L. K., and Wang, X.: The Model of Emissions of Gases and Aerosols
from Nature version 2.1 (MEGAN2.1): an extended and updated framework for
modeling biogenic emissions, Geosci. Model Dev., 5, 1471–1492,
<ext-link xlink:href="https://doi.org/10.5194/gmd-5-1471-2012" ext-link-type="DOI">10.5194/gmd-5-1471-2012</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx17"><label>Hageman et al.(1996)</label><?label Hageman1996?><mixed-citation>Hageman, D., Behrens, B., Smith, S., Uin, J., Salwen, C., Koontz, A.,
Jefferson, A., Watson, T., Sedlacek, A., Kuang, C., Dubey, M., Springston,
S., and Senum, G.: ARM: Aerosol Observing System (AOS): aerosol data, 1-min,
Mentor-QC Applied, <ext-link xlink:href="https://doi.org/10.5439/1025259" ext-link-type="DOI">10.5439/1025259</ext-link>, 1996.</mixed-citation></ref>
      <ref id="bib1.bibx18"><label>Hageman et al.(2017)</label><?label osti_1150249?><mixed-citation>Hageman, D., Behrens, B., Smith, S., Uin, J., Salwen, C., Koontz, A.,
Jefferson, A., Watson, T., Sedlacek, A., Kuang, C., Dubey, M., Springston,
S., and Senum, G.: ARM: Aerosol Observing System (AOS): cloud condensation
nuclei data, <ext-link xlink:href="https://doi.org/10.5439/1150249" ext-link-type="DOI">10.5439/1150249</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx19"><label>Holdridge and Kyrouac(1993)</label><?label Holdridge1993?><mixed-citation>Holdridge, D. and Kyrouac, J.: ARM: ARM-standard Meteorological Instrumentation
at Surface,   <ext-link xlink:href="https://doi.org/10.5439/1025220" ext-link-type="DOI">10.5439/1025220</ext-link>, 1993.</mixed-citation></ref>
      <ref id="bib1.bibx20"><label>Hoppel et al.(1994)</label><?label Hoppel_1994?><mixed-citation>Hoppel, W. A., Frick, G. M., Fitzgerald, J. W., and Wattle, B. J.: A Cloud
Chamber Study of the Effect That Nonprecipitating Water Clouds Have on the
Aerosol Size Distribution, Aerosol Sci. Technol., 20, 1–30,
<ext-link xlink:href="https://doi.org/10.1080/02786829408959660" ext-link-type="DOI">10.1080/02786829408959660</ext-link>, 1994.</mixed-citation></ref>
      <ref id="bib1.bibx21"><label>Hughes et al.(2018)</label><?label Hughes_2018?><mixed-citation>Hughes, M., Kodros, J., Pierce, J., West, M., and Riemer, N.: Machine Learning
to Predict the Global Distribution of Aerosol Mixing State Metrics,
Atmosphere, 9, 15, <ext-link xlink:href="https://doi.org/10.3390/atmos9010015" ext-link-type="DOI">10.3390/atmos9010015</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx22"><label>Huttunen et al.(2016)</label><?label Huttunen_2016?><mixed-citation>Huttunen, J., Kokkola, H., Mielonen, T., Mononen, M. E. J., Lipponen, A.,
Reunanen, J., Lindfors, A. V., Mikkonen, S., Lehtinen, K. E. J., Kouremeti,
N., Bais, A., Niska, H., and Arola, A.: Retrieval of aerosol optical depth
from surface solar radiation measurements using machine learning algorithms,
non-linear regression and a radiative transfer-based look-up table,
Atmos. Chem. Phys., 16, 8181–8191,
<ext-link xlink:href="https://doi.org/10.5194/acp-16-8181-2016" ext-link-type="DOI">10.5194/acp-16-8181-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx23"><label>IPCC AR5(2013)</label><?label IPCC_2013?><mixed-citation>
IPCC AR5: Climate Change 2013: The Physical Science Basis. Contribution of
Working Group I to the Fifth Assessment Report of the Intergovernmental Panel
on Climate Change, Cambridge University Press, Cambridge, United Kingdom and
New York, NY, USA, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx24"><label>Jefferson(2011)</label><?label Jefferson2011?><mixed-citation>Jefferson, A.: Aerosol Observing System (AOS) Handbook, Tech. rep., DOE
Office of Science Atmospheric Radiation Measurement (ARM) Program,
<ext-link xlink:href="https://doi.org/10.2172/1020729" ext-link-type="DOI">10.2172/1020729</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx25"><label>Jin et al.(2019)</label><?label Jin_2019?><mixed-citation>Jin, J., Lin, H. X., Segers, A., Xie, Y., and Heemink, A.: Machine learning for
observation bias correction with application to dust storm data assimilation,
Atmos. Chem. Phys., 19, 10009–10026,
<ext-link xlink:href="https://doi.org/10.5194/acp-19-10009-2019" ext-link-type="DOI">10.5194/acp-19-10009-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx26"><label>Joutsensaari et al.(2018)</label><?label Joutsensaari_2018?><mixed-citation>Joutsensaari, J., Ozon, M., Nieminen, T., Mikkonen, S., Lähivaara, T.,
Decesari, S., Facchini, M. C., Laaksonen, A., and Lehtinen, K. E. J.:
Identification of new particle formation events with deep learning,
Atmos. Chem. Phys., 18, 9597–9615,
<ext-link xlink:href="https://doi.org/10.5194/acp-18-9597-2018" ext-link-type="DOI">10.5194/acp-18-9597-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx27"><label>Keller et al.(2014)</label><?label Keller_2014?><mixed-citation>Keller, C. A., Long, M. S., Yantosca, R. M., Da Silva, A. M., Pawson, S., and
Jacob, D. J.: HEMCO v1.0: a versatile, ESMF-compliant component for
calculating emissions in atmospheric models, Geosci. Model Dev.,
7, 1409–1417, <ext-link xlink:href="https://doi.org/10.5194/gmd-7-1409-2014" ext-link-type="DOI">10.5194/gmd-7-1409-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bibx28"><label>Kendall(1970)</label><?label Kendall_1970?><mixed-citation>
Kendall, M.: Rank Correlation Methods, Theory and applications of rank
order-statistics, Griffin,  London,  202 pp., 1970.</mixed-citation></ref>
      <ref id="bib1.bibx29"><label>Kulkarni(2019)</label><?label acsmKulkarni2019?><mixed-citation>Kulkarni, G.: aosacsm.b1, <ext-link xlink:href="https://doi.org/10.5439/1558768" ext-link-type="DOI">10.5439/1558768</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx30"><label>Martin et al.(2003)</label><?label Martin_2003?><mixed-citation>Martin, R. V., Jacob, D. J., Yantosca, R. M., Chin, M., and Ginoux, P.: Global
and regional decreases in tropospheric oxidants from photochemical effects of
aerosols, J. Geophys. Res.-Atmos., 108, 4097,
<ext-link xlink:href="https://doi.org/10.1029/2002jd002622" ext-link-type="DOI">10.1029/2002jd002622</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bibx31"><label>Mauceri et al.(2019)</label><?label Mauceri_2019?><mixed-citation>Mauceri, S., Kindel, B., Massie, S., and Pilewskie, P.: Neural network for
aerosol retrieval from hyperspectral imagery, Atmos. Meas.
Tech., 12, 6017–6036, <ext-link xlink:href="https://doi.org/10.5194/amt-12-6017-2019" ext-link-type="DOI">10.5194/amt-12-6017-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx32"><label>McLeod(2011)</label><?label RKendall?><mixed-citation>McLeod, A.: Kendall: Kendall rank correlation and Mann-Kendall trend test,
available at: <uri>https://CRAN.R-project.org/package=Kendall</uri>  (last access: 20 August 2020), r package version
2.2, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx33"><label>Merikanto et al.(2009)</label><?label Merikanto_2009?><mixed-citation>Merikanto, J., Spracklen, D. V., Mann, G. W., Pickering, S. J., and Carslaw,
K. S.: Impact of nucleation on global CCN, Atmos. Chem.
Phys., 9, 8601–8616, <ext-link xlink:href="https://doi.org/10.5194/acp-9-8601-2009" ext-link-type="DOI">10.5194/acp-9-8601-2009</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx34"><label>Murray et al.(2012)</label><?label Murray_2012?><mixed-citation>Murray, L. T., Jacob, D. J., Logan, J. A., Hudman, R. C., and Koshak, W. J.:
Optimized regional and interannual variability of lightning in a global
chemical transport model constrained by LIS/OTD satellite data, J.
Geophys. Res.-Atmos., 117, D20307, <ext-link xlink:href="https://doi.org/10.1029/2012jd017934" ext-link-type="DOI">10.1029/2012jd017934</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx35"><label>Nair et al.(2019)</label><?label Nair_2019?><mixed-citation>Nair, A. A., Yu, F., and Luo, G.: Spatioseasonal Variations of Atmospheric
Ammonia Concentrations Over the United States: Comprehensive
Model-Observation Comparison, J. Geophys. Res.-Atmos.,
124, 6571–6582, <ext-link xlink:href="https://doi.org/10.1029/2018JD030057" ext-link-type="DOI">10.1029/2018JD030057</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx36"><label>Ng et al.(2011)</label><?label Ng2011?><mixed-citation>Ng, N. L., Herndon, S. C., Trimborn, A., Canagaratna, M. R., Croteau, P. L.,
Onasch, T. B., Sueper, D., Worsnop, D. R., Zhang, Q., Sun, Y. L., and Jayne,
J. T.: An Aerosol Chemical Speciation Monitor (ACSM) for Routine Monitoring
of the Composition and Mass Concentrations of Ambient Aerosol, Aerosol
Sci. Technol., 45, 780–794, <ext-link xlink:href="https://doi.org/10.1080/02786826.2011.560211" ext-link-type="DOI">10.1080/02786826.2011.560211</ext-link>,
2011.</mixed-citation></ref>
      <ref id="bib1.bibx37"><label>Noether(1981)</label><?label Noether1981?><mixed-citation>Noether, G. E.: Why Kendall Tau?, Teaching Statistics, 3, 41–43,
<ext-link xlink:href="https://doi.org/10.1111/j.1467-9639.1981.tb00422.x" ext-link-type="DOI">10.1111/j.1467-9639.1981.tb00422.x</ext-link>, 1981.</mixed-citation></ref>
      <?pagebreak page12869?><ref id="bib1.bibx38"><label>Okamura et al.(2017)</label><?label Okamura_2017?><mixed-citation>Okamura, R., Iwabuchi, H., and Schmidt, K. S.: Feasibility study of multi-pixel
retrieval of optical thickness and droplet effective radius of inhomogeneous
clouds using deep learning, Atmos. Meas. Tech., 10,
4747–4759, <ext-link xlink:href="https://doi.org/10.5194/amt-10-4747-2017" ext-link-type="DOI">10.5194/amt-10-4747-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx39"><label>Park(2004)</label><?label Park_2004?><mixed-citation>Park, R. J.: Natural and transboundary pollution influences on
sulfate-nitrate-ammonium aerosols in the United States: Implications for
policy, J. Geophys. Res., 109, D15204, <ext-link xlink:href="https://doi.org/10.1029/2003jd004473" ext-link-type="DOI">10.1029/2003jd004473</ext-link>,
2004.</mixed-citation></ref>
      <ref id="bib1.bibx40"><label>Probst et al.(2019)</label><?label Probst_2019?><mixed-citation>Probst, P., Wright, M. N., and Boulesteix, A.-L.: Hyperparameters and tuning
strategies for random forest, Wiley Interdisciplinary Reviews: Data Mining
and Knowledge Discovery, 9, e1301, <ext-link xlink:href="https://doi.org/10.1002/widm.1301" ext-link-type="DOI">10.1002/widm.1301</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bibx41"><label>Pye and Seinfeld(2010)</label><?label Pye_2010?><mixed-citation>Pye, H. O. T. and Seinfeld, J. H.: A global perspective on aerosol from
low-volatility organic compounds, Atmos. Chem. Phys., 10,
4377–4401, <ext-link xlink:href="https://doi.org/10.5194/acp-10-4377-2010" ext-link-type="DOI">10.5194/acp-10-4377-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bibx42"><label>R Core Team(2020)</label><?label RCore_2020?><mixed-citation>R Core Team: R: A Language and Environment for Statistical Computing, R
Foundation for Statistical Computing, Vienna, Austria,
available at: <uri>https://www.R-project.org/</uri>  (last access: 20 August 2020), 2020.</mixed-citation></ref>
      <ref id="bib1.bibx43"><label>Ritsche(2011)</label><?label Ritsche2011?><mixed-citation>Ritsche, M.: ARM Surface Meteorology Systems Instrument Handbook, Tech. rep.,
Office of Scientific and Technical Information (OSTI),
<ext-link xlink:href="https://doi.org/10.2172/1007926" ext-link-type="DOI">10.2172/1007926</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx44"><label>Roberts and Nenes(2005)</label><?label RobertNenes2004?><mixed-citation>Roberts, G. C. and Nenes, A.: A Continuous-Flow Streamwise Thermal-Gradient CCN
Chamber for Atmospheric Measurements, Aerosol Sci. Technol., 39,
206–221, <ext-link xlink:href="https://doi.org/10.1080/027868290913988" ext-link-type="DOI">10.1080/027868290913988</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bibx45"><label>Seinfeld et al.(2016)</label><?label Seinfeld_2016?><mixed-citation>Seinfeld, J. H., Bretherton, C., Carslaw, K. S., Coe, H., DeMott, P. J.,
Dunlea, E. J., Feingold, G., Ghan, S., Guenther, A. B., Kahn, R., Kraucunas,
I., Kreidenweis, S. M., Molina, M. J., Nenes, A., Penner, J. E., Prather,
K. A., Ramanathan, V., Ramaswamy, V., Rasch, P. J., Ravishankara, A. R.,
Rosenfeld, D., Stephens, G., and Wood, R.: Improving our fundamental
understanding of the role of aerosol-cloud interactions in the climate
system, P. Natl. Acad. Sci. USA, 113, 5781–5790,
<ext-link xlink:href="https://doi.org/10.1073/pnas.1514043113" ext-link-type="DOI">10.1073/pnas.1514043113</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx46"><label>Shi and Flynn(2007)</label><?label osti_1095312?><mixed-citation>Shi, Y. and Flynn, C.: ARM: Aerosol Observing System (AOS): cloud condensation
nuclei data, averaged,  <ext-link xlink:href="https://doi.org/10.5439/1095312" ext-link-type="DOI">10.5439/1095312</ext-link>, 2007.</mixed-citation></ref>
      <ref id="bib1.bibx47"><label>Smith et al.(2011a)</label><?label osti_1256093?><mixed-citation>Smith, S., Salwen, C., Uin, J., Senum, G., Springston, S., and Jefferson, A.:
ARM: AOS: Cloud Condensation Nuclei Counter, <ext-link xlink:href="https://doi.org/10.5439/1256093" ext-link-type="DOI">10.5439/1256093</ext-link>,
2011a.</mixed-citation></ref>
      <ref id="bib1.bibx48"><label>Smith et al.(2011b)</label><?label osti_1342133?><mixed-citation>Smith, S., Salwen, C., Uin, J., Senum, G., Springston, S., and Jefferson, A.:
ARM: AOS: Cloud Condensation Nuclei Counter (Single Column), averaged,
<ext-link xlink:href="https://doi.org/10.5439/1342133" ext-link-type="DOI">10.5439/1342133</ext-link>, 2011b.</mixed-citation></ref>
      <ref id="bib1.bibx49"><label>Springston(2012)</label><?label Springston2012?><mixed-citation>Springston, S.: ARM: AOS: Sulfur Dioxide Analyzer,  <ext-link xlink:href="https://doi.org/10.5439/1095586" ext-link-type="DOI">10.5439/1095586</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bibx50"><label>Twomey(1977)</label><?label Twomey_1977?><mixed-citation>Twomey, S. A.: The Influence of Pollution on the Shortwave Albedo of Clouds,
J. Atmos. Sci., 34, 1149–1152,
<ext-link xlink:href="https://doi.org/10.1175/1520-0469(1977)034&lt;1149:TIOPOT&gt;2.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(1977)034&lt;1149:TIOPOT&gt;2.0.CO;2</ext-link>, 1977.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bibx51"><label>Uin(2016)</label><?label Uin2016?><mixed-citation>Uin, J.: Cloud Condensation Nuclei Particle Counter (CCN) Instrument
Handbook, Tech. rep., DOE Office of Science Atmospheric Radiation Measurement
(ARM) Program, <ext-link xlink:href="https://doi.org/10.2172/1251411" ext-link-type="DOI">10.2172/1251411</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bibx52"><label>van Donkelaar et al.(2008)</label><?label vanDonkelaar_2008?><mixed-citation>van Donkelaar, A., Martin, R. V., Leaitch, W. R., Macdonald, A. M., Walker,
T. W., Streets, D. G., Zhang, Q., Dunlea, E. J., Jimenez, J. L., Dibb, J. E.,
Huey, L. G., Weber, R., and Andreae, M. O.: Analysis of aircraft and
satellite measurements from the Intercontinental Chemical Transport
Experiment (INTEX-B) to quantify long-range transport of East Asian sulfur
to Canada, Atmos. Chem. Phys., 8, 2999–3014,
<ext-link xlink:href="https://doi.org/10.5194/acp-8-2999-2008" ext-link-type="DOI">10.5194/acp-8-2999-2008</ext-link>, 2008.</mixed-citation></ref>
      <ref id="bib1.bibx53"><label>Watson et al.(2018)</label><?label acsmosti_1455055?><mixed-citation>Watson, T., Aiken, A., Zhang, Q., Croteau, P., Onasch, T., Williams, L., and
Flynn, C. F.: First ARM Aerosol Chemical Speciation Monitor Users' Meeting
Report, Tech. rep., DOE Office of Science Atmospheric Radiation Measurement
(ARM) Program, <ext-link xlink:href="https://doi.org/10.2172/1455055" ext-link-type="DOI">10.2172/1455055</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx54"><label>Watson(2017)</label><?label acsmosti_1375336?><mixed-citation>Watson, T. B.: Aerosol Chemical Speciation Monitor (ACSM) Instrument
Handbook, Tech. rep., DOE Office of Science Atmospheric Radiation Measurement
(ARM) Program, <ext-link xlink:href="https://doi.org/10.2172/1375336" ext-link-type="DOI">10.2172/1375336</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx55"><label>Wright and Ziegler(2017)</label><?label Wright_2017?><mixed-citation>Wright, M. N. and Ziegler, A.: ranger: A Fast Implementation of Random Forests
for High Dimensional Data in C<inline-formula><mml:math id="M357" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula> and R, J. Stat. Softw., 77, 1,
<ext-link xlink:href="https://doi.org/10.18637/jss.v077.i01" ext-link-type="DOI">10.18637/jss.v077.i01</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx56"><label>Yu(2011)</label><?label Yu_2011?><mixed-citation>Yu, F.: A secondary organic aerosol formation model considering successive
oxidation aging and kinetic condensation of organic compounds: global scale
implications, Atmos. Chem. Phys., 11, 1083–1099,
<ext-link xlink:href="https://doi.org/10.5194/acp-11-1083-2011" ext-link-type="DOI">10.5194/acp-11-1083-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bibx57"><label>Yu and Luo(2009)</label><?label YuLuo2009?><mixed-citation>Yu, F. and Luo, G.: Simulation of particle size distribution with a global
aerosol model: contribution of nucleation to aerosol and CCN number
concentrations, Atmos. Chem. Phys., 9, 7691–7710,
<ext-link xlink:href="https://doi.org/10.5194/acp-9-7691-2009" ext-link-type="DOI">10.5194/acp-9-7691-2009</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bibx58"><label>Yu et al.(2013)</label><?label Yu_2013?><mixed-citation>Yu, F., Ma, X., and Luo, G.: Anthropogenic contribution to cloud condensation
nuclei and the first aerosol indirect climate effect, Environ. Res.
Lett., 8, 024029, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/8/2/024029" ext-link-type="DOI">10.1088/1748-9326/8/2/024029</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bibx59"><label>Yu et al.(2017)</label><?label Yu_2017?><mixed-citation>Yu, F., Luo, G., Nadykto, A. B., and Herb, J.: Impact of temperature dependence
on the possible contribution of organics to new particle formation in the
atmosphere, Atmos. Chem. Phys., 17, 4997–5005,
<ext-link xlink:href="https://doi.org/10.5194/acp-17-4997-2017" ext-link-type="DOI">10.5194/acp-17-4997-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bibx60"><label>Yu et al.(2018)</label><?label Yu_2018TIMN?><mixed-citation>Yu, F., Nadykto, A. B., Herb, J., Luo, G., Nazarenko, K. M., and Uvarova,
L. A.: H<inline-formula><mml:math id="M358" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="bold">2</mml:mn></mml:msub></mml:math></inline-formula>SO<inline-formula><mml:math id="M359" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="bold">4</mml:mn></mml:msub></mml:math></inline-formula>-H<inline-formula><mml:math id="M360" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="bold">2</mml:mn></mml:msub></mml:math></inline-formula>O-NH<inline-formula><mml:math id="M361" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="bold">3</mml:mn></mml:msub></mml:math></inline-formula> ternary
ion-mediated nucleation (TIMN): Kinetic-based model and comparison with CLOUD
measurements, Atmos. Chem. Phys., 18, 17451–17474,
<ext-link xlink:href="https://doi.org/10.5194/acp-2018-396" ext-link-type="DOI">10.5194/acp-2018-396</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bibx61"><label>Zaidan et al.(2018)</label><?label Zaidan_2018?><mixed-citation>Zaidan, M. A., Haapasilta, V., Relan, R., Junninen, H., Aalto, P. P., Kulmala,
M., Laurson, L., and Foster, A. S.: Predicting atmospheric particle formation
days by Bayesian classification of the time series features, Tellus B, 70, 1–10,
<ext-link xlink:href="https://doi.org/10.1080/16000889.2018.1530031" ext-link-type="DOI">10.1080/16000889.2018.1530031</ext-link>, 2018.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>Using machine learning to derive cloud condensation nuclei number concentrations from commonly available measurements</article-title-html>
<abstract-html><p>Cloud condensation nuclei (CCN) number concentrations are an important aspect of aerosol–cloud interactions and the subsequent climate effects; however, their measurements are very limited. We use a machine learning tool, random decision forests, to develop a random forest regression model (RFRM) to derive CCN at 0.4&thinsp;% supersaturation ([CCN0.4]) from commonly available measurements. The RFRM is trained on the long-term simulations in a global size-resolved particle microphysics model. Using atmospheric state and composition variables as predictors, through associations of their variabilities, the RFRM is able to learn the underlying dependence of [CCN0.4] on these predictors, which are as follows: eight fractions of PM<sub>2.5</sub> (NH<sub>4</sub>, SO<sub>4</sub>, NO<sub>3</sub>, secondary organic aerosol (SOA), black carbon (BC), primary organic carbon (POC), dust, and salt), seven gaseous species (NO<sub><i>x</i></sub>, NH<sub>3</sub>, O<sub>3</sub>, SO<sub>2</sub>, OH, isoprene, and monoterpene), and four meteorological variables (temperature (<i>T</i>), relative humidity (RH), precipitation, and solar radiation). The RFRM is highly robust: it has a median mean fractional bias (MFB) of 4.4 <i>%</i> with  ≈ 96.33 <i>%</i> of the derived [CCN0.4] within a good agreement range of −60 <i>%</i> &lt; MFB &lt; +60 <i>%</i> and strong correlation of Kendall's <i>τ</i> coefficient  ≈ 0.88. The RFRM demonstrates its robustness over 4 orders of magnitude of [CCN0.4] over varying spatial (such as continental to oceanic, clean to polluted, and near-surface to upper troposphere) and temporal (from the hourly to the decadal) scales. At the Atmospheric Radiation Measurement Southern Great Plains observatory (ARM SGP) in Lamont, Oklahoma, United States, long-term measurements for PM<sub>2.5</sub> speciation (NH<sub>4</sub>, SO<sub>4</sub>, NO<sub>3</sub>, and organic carbon (OC)), NO<sub><i>x</i></sub>, O<sub>3</sub>, SO<sub>2</sub>, <i>T</i>, and RH, as well as [CCN0.4] are available. We modify, optimize, and retrain the developed RFRM to make predictions from 19 to 9 of these available predictors. This retrained RFRM (RFRM-ShortVars) shows a reduction in performance due to the unavailability and sparsity of measurements (predictors); it captures the [CCN0.4] variability and magnitude at SGP with  ≈ 67.02 <i>%</i> of the derived values in the good agreement range. This work shows the potential of using the more commonly available measurements of PM<sub>2.5</sub> speciation to alleviate the sparsity of CCN number concentrations' measurements.</p></abstract-html>
<ref-html id="bib1.bib1"><label>Albrecht(1989)</label><mixed-citation>
Albrecht, B. A.: Aerosols, Cloud Microphysics, and Fractional Cloudiness,
Science, 245, 1227–1230, <a href="https://doi.org/10.1126/science.245.4923.1227" target="_blank">https://doi.org/10.1126/science.245.4923.1227</a>, 1989.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>Behrens et al.(1990)</label><mixed-citation>
Behrens, B., Salwen, C., Springston, S., and Watson, T.: ARM: AOS: aerosol
chemical speciation monitor, <a href="https://doi.org/10.5439/1046180" target="_blank">https://doi.org/10.5439/1046180</a>, 1990.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>Bey et al.(2001)</label><mixed-citation>
Bey, I., Jacob, D. J., Yantosca, R. M., Logan, J. A., Field, B. D., Fiore,
A. M., Li, Q., Liu, H. Y., Mickley, L. J., and Schultz, M. G.: Global
modeling of tropospheric chemistry with assimilated meteorology: Model
description and evaluation, J. Geophys. Res.-Atmos.,
106, 23073–23095, <a href="https://doi.org/10.1029/2001JD000807" target="_blank">https://doi.org/10.1029/2001JD000807</a>, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>Breiman(1996)</label><mixed-citation>
Breiman, L.: Bagging predictors, Mach. Learn., 24, 123–140,
<a href="https://doi.org/10.1007/bf00058655" target="_blank">https://doi.org/10.1007/bf00058655</a>, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>Breiman(2001)</label><mixed-citation>
Breiman, L.: Random forests, Mach. Learn., 45, 5–32,
<a href="https://doi.org/10.1023/A:1010933404324" target="_blank">https://doi.org/10.1023/A:1010933404324</a>, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>Breiman et al.(1984)</label><mixed-citation>
Breiman, L., Friedman, J. H., Olshen, R. A., and Stone, C. J.: Classification
And Regression Trees, Routledge, <a href="https://doi.org/10.1201/9781315139470" target="_blank">https://doi.org/10.1201/9781315139470</a>, 1984.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>Chen and Xie(1994)</label><mixed-citation>
Chen, X. and Xie, S.: ARM: ARMBE: Atmospheric measurements,
<a href="https://doi.org/10.5439/1095313" target="_blank">https://doi.org/10.5439/1095313</a>, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>Christopoulos et al.(2018)</label><mixed-citation>
Christopoulos, C. D., Garimella, S., Zawadowicz, M. A., Möhler, O., and
Cziczo, D. J.: A machine learning approach to aerosol classification for
single-particle mass spectrometry, Atmos. Meas. Tech., 11,
5687–5699, <a href="https://doi.org/10.5194/amt-11-5687-2018" target="_blank">https://doi.org/10.5194/amt-11-5687-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>Dou and Yang(2018)</label><mixed-citation>
Dou, X. and Yang, Y.: Comprehensive evaluation of machine learning techniques
for estimating the responses of carbon fluxes to climatic forces in different
terrestrial ecosystems, Atmosphere, 9, 83, <a href="https://doi.org/10.3390/atmos9030083" target="_blank">https://doi.org/10.3390/atmos9030083</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>Evans and Jacob(2005)</label><mixed-citation>
Evans, M. and Jacob, D. J.: Impact of new laboratory studies of N<sub>2</sub>O<sub>5</sub> hydrolysis
on global model budgets of tropospheric nitrogen oxides, ozone, and OH,
Geophys. Res. Lett., 32, L09813, <a href="https://doi.org/10.1029/2005GL022469" target="_blank">https://doi.org/10.1029/2005GL022469</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>Filzmoser et al.(2018)</label><mixed-citation>
Filzmoser, P., Fritz, H., and Kalcher, K.: pcaPP: Robust PCA by Projection
Pursuit, available at: <a href="https://CRAN.R-project.org/package=pcaPP" target="_blank"/> (last access: 20 August 2020), r package
version 1.9-73, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>Fountoukis and Nenes(2007)</label><mixed-citation>
Fountoukis, C. and Nenes, A.: ISORROPIA II: a computationally efficient thermodynamic equilibrium model for K<sup>+</sup>–Ca<sub>2</sub><sup>+</sup>–Mg<sub>2</sub><sup>+</sup>–NH<sub>4</sub><sup>+</sup>–Na<sup>+</sup>–SO<sub>4</sub><sup>2−</sup>–NO<sub>3</sub><sup>−</sup>–Cl<sup>−</sup>–H<sub>2</sub>O aerosols, Atmos. Chem. Phys., 7, 4639–4659, <a href="https://doi.org/10.5194/acp-7-4639-2007" target="_blank">https://doi.org/10.5194/acp-7-4639-2007</a>, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>Fuchs et al.(2018)</label><mixed-citation>
Fuchs, J., Cermak, J., and Andersen, H.: Building a cloud in the southeast
Atlantic: understanding low-cloud controls based on satellite observations
with machine learning, Atmos. Chem. Phys., 18,
16537–16552, <a href="https://doi.org/10.5194/acp-18-16537-2018" target="_blank">https://doi.org/10.5194/acp-18-16537-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>Giglio et al.(2013)</label><mixed-citation>
Giglio, L., Randerson, J. T., and van der Werf, G. R.: Analysis of daily,
monthly, and annual burned area using the fourth-generation global fire
emissions database (GFED4), J. Geophys. Res.-Biogeo., 118, 317–328, <a href="https://doi.org/10.1002/jgrg.20042" target="_blank">https://doi.org/10.1002/jgrg.20042</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>Grange et al.(2018)</label><mixed-citation>
Grange, S. K., Carslaw, D. C., Lewis, A. C., Boleti, E., and Hueglin, C.:
Random forest meteorological normalisation models for Swiss PM<sub>10</sub>
trend analysis, Atmos. Chem. Phys., 18, 6223–6239,
<a href="https://doi.org/10.5194/acp-18-6223-2018" target="_blank">https://doi.org/10.5194/acp-18-6223-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>Guenther et al.(2012)</label><mixed-citation>
Guenther, A. B., Jiang, X., Heald, C. L., Sakulyanontvittaya, T., Duhl, T.,
Emmons, L. K., and Wang, X.: The Model of Emissions of Gases and Aerosols
from Nature version 2.1 (MEGAN2.1): an extended and updated framework for
modeling biogenic emissions, Geosci. Model Dev., 5, 1471–1492,
<a href="https://doi.org/10.5194/gmd-5-1471-2012" target="_blank">https://doi.org/10.5194/gmd-5-1471-2012</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>Hageman et al.(1996)</label><mixed-citation>
Hageman, D., Behrens, B., Smith, S., Uin, J., Salwen, C., Koontz, A.,
Jefferson, A., Watson, T., Sedlacek, A., Kuang, C., Dubey, M., Springston,
S., and Senum, G.: ARM: Aerosol Observing System (AOS): aerosol data, 1-min,
Mentor-QC Applied, <a href="https://doi.org/10.5439/1025259" target="_blank">https://doi.org/10.5439/1025259</a>, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>Hageman et al.(2017)</label><mixed-citation>
Hageman, D., Behrens, B., Smith, S., Uin, J., Salwen, C., Koontz, A.,
Jefferson, A., Watson, T., Sedlacek, A., Kuang, C., Dubey, M., Springston,
S., and Senum, G.: ARM: Aerosol Observing System (AOS): cloud condensation
nuclei data, <a href="https://doi.org/10.5439/1150249" target="_blank">https://doi.org/10.5439/1150249</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>Holdridge and Kyrouac(1993)</label><mixed-citation>
Holdridge, D. and Kyrouac, J.: ARM: ARM-standard Meteorological Instrumentation
at Surface,   <a href="https://doi.org/10.5439/1025220" target="_blank">https://doi.org/10.5439/1025220</a>, 1993.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>Hoppel et al.(1994)</label><mixed-citation>
Hoppel, W. A., Frick, G. M., Fitzgerald, J. W., and Wattle, B. J.: A Cloud
Chamber Study of the Effect That Nonprecipitating Water Clouds Have on the
Aerosol Size Distribution, Aerosol Sci. Technol., 20, 1–30,
<a href="https://doi.org/10.1080/02786829408959660" target="_blank">https://doi.org/10.1080/02786829408959660</a>, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>Hughes et al.(2018)</label><mixed-citation>
Hughes, M., Kodros, J., Pierce, J., West, M., and Riemer, N.: Machine Learning
to Predict the Global Distribution of Aerosol Mixing State Metrics,
Atmosphere, 9, 15, <a href="https://doi.org/10.3390/atmos9010015" target="_blank">https://doi.org/10.3390/atmos9010015</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>Huttunen et al.(2016)</label><mixed-citation>
Huttunen, J., Kokkola, H., Mielonen, T., Mononen, M. E. J., Lipponen, A.,
Reunanen, J., Lindfors, A. V., Mikkonen, S., Lehtinen, K. E. J., Kouremeti,
N., Bais, A., Niska, H., and Arola, A.: Retrieval of aerosol optical depth
from surface solar radiation measurements using machine learning algorithms,
non-linear regression and a radiative transfer-based look-up table,
Atmos. Chem. Phys., 16, 8181–8191,
<a href="https://doi.org/10.5194/acp-16-8181-2016" target="_blank">https://doi.org/10.5194/acp-16-8181-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>IPCC AR5(2013)</label><mixed-citation>
IPCC AR5: Climate Change 2013: The Physical Science Basis. Contribution of
Working Group I to the Fifth Assessment Report of the Intergovernmental Panel
on Climate Change, Cambridge University Press, Cambridge, United Kingdom and
New York, NY, USA, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>Jefferson(2011)</label><mixed-citation>
Jefferson, A.: Aerosol Observing System (AOS) Handbook, Tech. rep., DOE
Office of Science Atmospheric Radiation Measurement (ARM) Program,
<a href="https://doi.org/10.2172/1020729" target="_blank">https://doi.org/10.2172/1020729</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>Jin et al.(2019)</label><mixed-citation>
Jin, J., Lin, H. X., Segers, A., Xie, Y., and Heemink, A.: Machine learning for
observation bias correction with application to dust storm data assimilation,
Atmos. Chem. Phys., 19, 10009–10026,
<a href="https://doi.org/10.5194/acp-19-10009-2019" target="_blank">https://doi.org/10.5194/acp-19-10009-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>Joutsensaari et al.(2018)</label><mixed-citation>
Joutsensaari, J., Ozon, M., Nieminen, T., Mikkonen, S., Lähivaara, T.,
Decesari, S., Facchini, M. C., Laaksonen, A., and Lehtinen, K. E. J.:
Identification of new particle formation events with deep learning,
Atmos. Chem. Phys., 18, 9597–9615,
<a href="https://doi.org/10.5194/acp-18-9597-2018" target="_blank">https://doi.org/10.5194/acp-18-9597-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>Keller et al.(2014)</label><mixed-citation>
Keller, C. A., Long, M. S., Yantosca, R. M., Da Silva, A. M., Pawson, S., and
Jacob, D. J.: HEMCO v1.0: a versatile, ESMF-compliant component for
calculating emissions in atmospheric models, Geosci. Model Dev.,
7, 1409–1417, <a href="https://doi.org/10.5194/gmd-7-1409-2014" target="_blank">https://doi.org/10.5194/gmd-7-1409-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>Kendall(1970)</label><mixed-citation>
Kendall, M.: Rank Correlation Methods, Theory and applications of rank
order-statistics, Griffin,  London,  202 pp., 1970.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>Kulkarni(2019)</label><mixed-citation>
Kulkarni, G.: aosacsm.b1, <a href="https://doi.org/10.5439/1558768" target="_blank">https://doi.org/10.5439/1558768</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>Martin et al.(2003)</label><mixed-citation>
Martin, R. V., Jacob, D. J., Yantosca, R. M., Chin, M., and Ginoux, P.: Global
and regional decreases in tropospheric oxidants from photochemical effects of
aerosols, J. Geophys. Res.-Atmos., 108, 4097,
<a href="https://doi.org/10.1029/2002jd002622" target="_blank">https://doi.org/10.1029/2002jd002622</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>Mauceri et al.(2019)</label><mixed-citation>
Mauceri, S., Kindel, B., Massie, S., and Pilewskie, P.: Neural network for
aerosol retrieval from hyperspectral imagery, Atmos. Meas.
Tech., 12, 6017–6036, <a href="https://doi.org/10.5194/amt-12-6017-2019" target="_blank">https://doi.org/10.5194/amt-12-6017-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>McLeod(2011)</label><mixed-citation>
McLeod, A.: Kendall: Kendall rank correlation and Mann-Kendall trend test,
available at: <a href="https://CRAN.R-project.org/package=Kendall" target="_blank"/>  (last access: 20 August 2020), r package version
2.2, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>Merikanto et al.(2009)</label><mixed-citation>
Merikanto, J., Spracklen, D. V., Mann, G. W., Pickering, S. J., and Carslaw,
K. S.: Impact of nucleation on global CCN, Atmos. Chem.
Phys., 9, 8601–8616, <a href="https://doi.org/10.5194/acp-9-8601-2009" target="_blank">https://doi.org/10.5194/acp-9-8601-2009</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>Murray et al.(2012)</label><mixed-citation>
Murray, L. T., Jacob, D. J., Logan, J. A., Hudman, R. C., and Koshak, W. J.:
Optimized regional and interannual variability of lightning in a global
chemical transport model constrained by LIS/OTD satellite data, J.
Geophys. Res.-Atmos., 117, D20307, <a href="https://doi.org/10.1029/2012jd017934" target="_blank">https://doi.org/10.1029/2012jd017934</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>Nair et al.(2019)</label><mixed-citation>
Nair, A. A., Yu, F., and Luo, G.: Spatioseasonal Variations of Atmospheric
Ammonia Concentrations Over the United States: Comprehensive
Model-Observation Comparison, J. Geophys. Res.-Atmos.,
124, 6571–6582, <a href="https://doi.org/10.1029/2018JD030057" target="_blank">https://doi.org/10.1029/2018JD030057</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>Ng et al.(2011)</label><mixed-citation>
Ng, N. L., Herndon, S. C., Trimborn, A., Canagaratna, M. R., Croteau, P. L.,
Onasch, T. B., Sueper, D., Worsnop, D. R., Zhang, Q., Sun, Y. L., and Jayne,
J. T.: An Aerosol Chemical Speciation Monitor (ACSM) for Routine Monitoring
of the Composition and Mass Concentrations of Ambient Aerosol, Aerosol
Sci. Technol., 45, 780–794, <a href="https://doi.org/10.1080/02786826.2011.560211" target="_blank">https://doi.org/10.1080/02786826.2011.560211</a>,
2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>Noether(1981)</label><mixed-citation>
Noether, G. E.: Why Kendall Tau?, Teaching Statistics, 3, 41–43,
<a href="https://doi.org/10.1111/j.1467-9639.1981.tb00422.x" target="_blank">https://doi.org/10.1111/j.1467-9639.1981.tb00422.x</a>, 1981.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>Okamura et al.(2017)</label><mixed-citation>
Okamura, R., Iwabuchi, H., and Schmidt, K. S.: Feasibility study of multi-pixel
retrieval of optical thickness and droplet effective radius of inhomogeneous
clouds using deep learning, Atmos. Meas. Tech., 10,
4747–4759, <a href="https://doi.org/10.5194/amt-10-4747-2017" target="_blank">https://doi.org/10.5194/amt-10-4747-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>Park(2004)</label><mixed-citation>
Park, R. J.: Natural and transboundary pollution influences on
sulfate-nitrate-ammonium aerosols in the United States: Implications for
policy, J. Geophys. Res., 109, D15204, <a href="https://doi.org/10.1029/2003jd004473" target="_blank">https://doi.org/10.1029/2003jd004473</a>,
2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>Probst et al.(2019)</label><mixed-citation>
Probst, P., Wright, M. N., and Boulesteix, A.-L.: Hyperparameters and tuning
strategies for random forest, Wiley Interdisciplinary Reviews: Data Mining
and Knowledge Discovery, 9, e1301, <a href="https://doi.org/10.1002/widm.1301" target="_blank">https://doi.org/10.1002/widm.1301</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>Pye and Seinfeld(2010)</label><mixed-citation>
Pye, H. O. T. and Seinfeld, J. H.: A global perspective on aerosol from
low-volatility organic compounds, Atmos. Chem. Phys., 10,
4377–4401, <a href="https://doi.org/10.5194/acp-10-4377-2010" target="_blank">https://doi.org/10.5194/acp-10-4377-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>R Core Team(2020)</label><mixed-citation>
R Core Team: R: A Language and Environment for Statistical Computing, R
Foundation for Statistical Computing, Vienna, Austria,
available at: <a href="https://www.R-project.org/" target="_blank"/>  (last access: 20 August 2020), 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>Ritsche(2011)</label><mixed-citation>
Ritsche, M.: ARM Surface Meteorology Systems Instrument Handbook, Tech. rep.,
Office of Scientific and Technical Information (OSTI),
<a href="https://doi.org/10.2172/1007926" target="_blank">https://doi.org/10.2172/1007926</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>Roberts and Nenes(2005)</label><mixed-citation>
Roberts, G. C. and Nenes, A.: A Continuous-Flow Streamwise Thermal-Gradient CCN
Chamber for Atmospheric Measurements, Aerosol Sci. Technol., 39,
206–221, <a href="https://doi.org/10.1080/027868290913988" target="_blank">https://doi.org/10.1080/027868290913988</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>Seinfeld et al.(2016)</label><mixed-citation>
Seinfeld, J. H., Bretherton, C., Carslaw, K. S., Coe, H., DeMott, P. J.,
Dunlea, E. J., Feingold, G., Ghan, S., Guenther, A. B., Kahn, R., Kraucunas,
I., Kreidenweis, S. M., Molina, M. J., Nenes, A., Penner, J. E., Prather,
K. A., Ramanathan, V., Ramaswamy, V., Rasch, P. J., Ravishankara, A. R.,
Rosenfeld, D., Stephens, G., and Wood, R.: Improving our fundamental
understanding of the role of aerosol-cloud interactions in the climate
system, P. Natl. Acad. Sci. USA, 113, 5781–5790,
<a href="https://doi.org/10.1073/pnas.1514043113" target="_blank">https://doi.org/10.1073/pnas.1514043113</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>Shi and Flynn(2007)</label><mixed-citation>
Shi, Y. and Flynn, C.: ARM: Aerosol Observing System (AOS): cloud condensation
nuclei data, averaged,  <a href="https://doi.org/10.5439/1095312" target="_blank">https://doi.org/10.5439/1095312</a>, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>Smith et al.(2011a)</label><mixed-citation>
Smith, S., Salwen, C., Uin, J., Senum, G., Springston, S., and Jefferson, A.:
ARM: AOS: Cloud Condensation Nuclei Counter, <a href="https://doi.org/10.5439/1256093" target="_blank">https://doi.org/10.5439/1256093</a>,
2011a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>Smith et al.(2011b)</label><mixed-citation>
Smith, S., Salwen, C., Uin, J., Senum, G., Springston, S., and Jefferson, A.:
ARM: AOS: Cloud Condensation Nuclei Counter (Single Column), averaged,
<a href="https://doi.org/10.5439/1342133" target="_blank">https://doi.org/10.5439/1342133</a>, 2011b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>Springston(2012)</label><mixed-citation>
Springston, S.: ARM: AOS: Sulfur Dioxide Analyzer,  <a href="https://doi.org/10.5439/1095586" target="_blank">https://doi.org/10.5439/1095586</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>Twomey(1977)</label><mixed-citation>
Twomey, S. A.: The Influence of Pollution on the Shortwave Albedo of Clouds,
J. Atmos. Sci., 34, 1149–1152,
<a href="https://doi.org/10.1175/1520-0469(1977)034&lt;1149:TIOPOT&gt;2.0.CO;2" target="_blank">https://doi.org/10.1175/1520-0469(1977)034&lt;1149:TIOPOT&gt;2.0.CO;2</a>, 1977.

</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>Uin(2016)</label><mixed-citation>
Uin, J.: Cloud Condensation Nuclei Particle Counter (CCN) Instrument
Handbook, Tech. rep., DOE Office of Science Atmospheric Radiation Measurement
(ARM) Program, <a href="https://doi.org/10.2172/1251411" target="_blank">https://doi.org/10.2172/1251411</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>van Donkelaar et al.(2008)</label><mixed-citation>
van Donkelaar, A., Martin, R. V., Leaitch, W. R., Macdonald, A. M., Walker,
T. W., Streets, D. G., Zhang, Q., Dunlea, E. J., Jimenez, J. L., Dibb, J. E.,
Huey, L. G., Weber, R., and Andreae, M. O.: Analysis of aircraft and
satellite measurements from the Intercontinental Chemical Transport
Experiment (INTEX-B) to quantify long-range transport of East Asian sulfur
to Canada, Atmos. Chem. Phys., 8, 2999–3014,
<a href="https://doi.org/10.5194/acp-8-2999-2008" target="_blank">https://doi.org/10.5194/acp-8-2999-2008</a>, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>Watson et al.(2018)</label><mixed-citation>
Watson, T., Aiken, A., Zhang, Q., Croteau, P., Onasch, T., Williams, L., and
Flynn, C. F.: First ARM Aerosol Chemical Speciation Monitor Users' Meeting
Report, Tech. rep., DOE Office of Science Atmospheric Radiation Measurement
(ARM) Program, <a href="https://doi.org/10.2172/1455055" target="_blank">https://doi.org/10.2172/1455055</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>Watson(2017)</label><mixed-citation>
Watson, T. B.: Aerosol Chemical Speciation Monitor (ACSM) Instrument
Handbook, Tech. rep., DOE Office of Science Atmospheric Radiation Measurement
(ARM) Program, <a href="https://doi.org/10.2172/1375336" target="_blank">https://doi.org/10.2172/1375336</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>Wright and Ziegler(2017)</label><mixed-citation>
Wright, M. N. and Ziegler, A.: ranger: A Fast Implementation of Random Forests
for High Dimensional Data in C+ +  and R, J. Stat. Softw., 77, 1,
<a href="https://doi.org/10.18637/jss.v077.i01" target="_blank">https://doi.org/10.18637/jss.v077.i01</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>Yu(2011)</label><mixed-citation>
Yu, F.: A secondary organic aerosol formation model considering successive
oxidation aging and kinetic condensation of organic compounds: global scale
implications, Atmos. Chem. Phys., 11, 1083–1099,
<a href="https://doi.org/10.5194/acp-11-1083-2011" target="_blank">https://doi.org/10.5194/acp-11-1083-2011</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>Yu and Luo(2009)</label><mixed-citation>
Yu, F. and Luo, G.: Simulation of particle size distribution with a global
aerosol model: contribution of nucleation to aerosol and CCN number
concentrations, Atmos. Chem. Phys., 9, 7691–7710,
<a href="https://doi.org/10.5194/acp-9-7691-2009" target="_blank">https://doi.org/10.5194/acp-9-7691-2009</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>Yu et al.(2013)</label><mixed-citation>
Yu, F., Ma, X., and Luo, G.: Anthropogenic contribution to cloud condensation
nuclei and the first aerosol indirect climate effect, Environ. Res.
Lett., 8, 024029, <a href="https://doi.org/10.1088/1748-9326/8/2/024029" target="_blank">https://doi.org/10.1088/1748-9326/8/2/024029</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>Yu et al.(2017)</label><mixed-citation>
Yu, F., Luo, G., Nadykto, A. B., and Herb, J.: Impact of temperature dependence
on the possible contribution of organics to new particle formation in the
atmosphere, Atmos. Chem. Phys., 17, 4997–5005,
<a href="https://doi.org/10.5194/acp-17-4997-2017" target="_blank">https://doi.org/10.5194/acp-17-4997-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>Yu et al.(2018)</label><mixed-citation>
Yu, F., Nadykto, A. B., Herb, J., Luo, G., Nazarenko, K. M., and Uvarova,
L. A.: H<sub>2</sub>SO<sub>4</sub>-H<sub>2</sub>O-NH<sub>3</sub> ternary
ion-mediated nucleation (TIMN): Kinetic-based model and comparison with CLOUD
measurements, Atmos. Chem. Phys., 18, 17451–17474,
<a href="https://doi.org/10.5194/acp-2018-396" target="_blank">https://doi.org/10.5194/acp-2018-396</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>Zaidan et al.(2018)</label><mixed-citation>
Zaidan, M. A., Haapasilta, V., Relan, R., Junninen, H., Aalto, P. P., Kulmala,
M., Laurson, L., and Foster, A. S.: Predicting atmospheric particle formation
days by Bayesian classification of the time series features, Tellus B, 70, 1–10,
<a href="https://doi.org/10.1080/16000889.2018.1530031" target="_blank">https://doi.org/10.1080/16000889.2018.1530031</a>, 2018.
</mixed-citation></ref-html>--></article>
