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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" article-type="research-article"><?xmltex \bartext{Research article}?>
  <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-22-15963-2022</article-id><title-group><article-title>Satellite observations of seasonality and long-term trends in cirrus cloud properties over Europe: investigation of possible aviation impacts</article-title><alt-title>Seasonality and long-term trends in cirrus cloud properties​​​​​​​</alt-title>
      </title-group><?xmltex \runningtitle{Seasonality and long-term trends in cirrus cloud properties​​​​​​​}?><?xmltex \runningauthor{Q. Li and S. Groß}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes">
          <name><surname>Li</surname><given-names>Qiang</given-names></name>
          <email>qiang.li@dlr.de</email>
        <ext-link>https://orcid.org/0000-0003-1951-8144</ext-link></contrib>
        <contrib contrib-type="author" corresp="no">
          <name><surname>Groß</surname><given-names>Silke</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7467-9269</ext-link></contrib>
        <aff id="aff1"><institution>Deutsches Zentrum für Luft- und Raumfahrt, Institut für Physik der Atmosphäre,<?xmltex \hack{\break}?> 82234 Oberpfaffenhofen, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Qiang Li (qiang.li@dlr.de)</corresp></author-notes><pub-date><day>20</day><month>December</month><year>2022</year></pub-date>
      
      <volume>22</volume>
      <issue>24</issue>
      <fpage>15963</fpage><lpage>15980</lpage>
      <history>
        <date date-type="received"><day>12</day><month>July</month><year>2022</year></date>
           <date date-type="rev-request"><day>20</day><month>July</month><year>2022</year></date>
           <date date-type="rev-recd"><day>21</day><month>November</month><year>2022</year></date>
           <date date-type="accepted"><day>22</day><month>November</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Qiang Li</copyright-statement>
        <copyright-year>2022</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/22/15963/2022/acp-22-15963-2022.html">This article is available from https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e90">Linear contrails and contrail cirrus induced by global aviation have long been known to contribute to climate change by warming the atmosphere. Besides increasing global cirrus cloudiness, aviation may also alter the properties of natural cirrus clouds by soot emissions which lead to more heterogeneous freezing. During the first COVID-19 lockdown in Europe, changes in the properties and occurrence of cirrus clouds were determined with the lidar measurements of CALIPSO, which are presumed to be caused by the corresponding reduction in civil aviation. In the 10 years before the COVID-19 outbreak, however, aviation grew strongly in terms of CO<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions and flight densities in Europe. In this study, 10-year lidar measurements with CALIPSO are analysed to determine the seasonality and long-term trends in cirrus clouds as well as their correlations with the ambient temperatures and air traffic. The results show that there is a distinct seasonal cycle in the occurrence rates (ORs) and particle linear depolarization ratio (PLDR) of cirrus clouds. In addition, cirrus clouds appear within a broader altitude range in winter than in summer and they are characterized by larger OR and PLDR values in winter than in summer. The monthly medians of PLDR as well as their deseasonalized time series in the 10-year period before COVID-19 both show positive trends, which are statistically significant according to the Mann–Kendall (MK) significance test. However, the ORs of cirrus clouds show a negative trend, which might be connected with the background meteorological conditions. Since the cirrus PLDR strongly depends on the ambient temperatures, the contributions induced by temperature are further removed from the cirrus PLDR with a simple linear regression model. The derived residuals show significant positive trends according to the MK test. To compare the cirrus PLDR and air traffic (with the CO<inline-formula><mml:math id="M2" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation as a proxy), the deseasonalization of both datasets were previously conducted since the seasonal cycles in both are not consistent. The deseasonalized time series determined for the cirrus PLDR and CO<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation both show increasing trends and their correlation coefficient is <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.54</mml:mn></mml:mrow></mml:math></inline-formula> at the confidence level above 99.5 %. Finally, comparisons between the cirrus PLDR and aviation in every season were made and revealed a strong correlation in other seasons than in summer.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e141">Aviation affects the Earth's radiation budget through a combination of aviation emissions of CO<inline-formula><mml:math id="M5" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and non-CO<inline-formula><mml:math id="M6" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> effects which have a warming effect on the atmosphere <xref ref-type="bibr" rid="bib1.bibx37" id="paren.1"/>. Linear contrails and contrail cirrus induced by water vapour and soot emissions from air traffic in the upper atmosphere are expected to contribute a large part of the climate impact of aviation <xref ref-type="bibr" rid="bib1.bibx8" id="paren.2"><named-content content-type="pre">e.g.</named-content></xref>. Due to their climate impact and their suitability for monitoring the mitigation of aviation, numerous experimental and theoretical efforts have been carried out in the past few years to understand contrails and to determine their effect on climate by calculating radiative forcing <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx74 bib1.bibx8 bib1.bibx16 bib1.bibx58 bib1.bibx30 bib1.bibx29 bib1.bibx4 bib1.bibx59 bib1.bibx60" id="paren.3"><named-content content-type="pre">e.g.</named-content></xref>. However, aviation emissions and the resulting contrail formation interact with the atmosphere through a complex manner which is still not fully understood.</p>
      <p id="d1e175">Cirrus clouds, composed of ice crystals with a variety of forms and shapes, usually appear in the upper atmosphere above <inline-formula><mml:math id="M7" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 6 km. They have long been recognized, as studies reveal that cirrus clouds permanently cover on average 30 % of the Earth's surface with up to 70 % coverage over the tropics and they have a large impact on the Earth's radiation balance and climate evolution <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx77 bib1.bibx81 bib1.bibx52 bib1.bibx55 bib1.bibx47" id="paren.4"/>. Cirrus clouds influence the radiation balance by trapping the outgoing long-wave radiation from the ground and underlying atmosphere (warming) and reflecting the incoming short-wave solar radiation back into space (cooling). The contribution of these two opposite effects depends on the cloud microphysical, thermal, and optical properties, which include cloud heights, temperatures, and the shape and orientation of ice crystals <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx84 bib1.bibx83 bib1.bibx64 bib1.bibx9" id="paren.5"><named-content content-type="pre">e.g.</named-content></xref>. Overall, cirrus clouds are assumed to have a net warming effect on the climate system, unlike the low and midlevel clouds <xref ref-type="bibr" rid="bib1.bibx10" id="paren.6"/>.</p>
      <p id="d1e196">Midlatitude cirrus clouds are of particular interest and have been intensively studied thanks to the high number of observation sites as well as campaign-based observations <xref ref-type="bibr" rid="bib1.bibx75 bib1.bibx76" id="paren.7"><named-content content-type="pre">e.g.</named-content></xref> at these latitudes. Nevertheless, midlatitude cirrus clouds are induced and affected by various weather patterns and interact with the atmospheric dynamics, which lead to difficulties in their representation in global and regional climate models <xref ref-type="bibr" rid="bib1.bibx6" id="paren.8"/>. Furthermore, midlatitude cirrus clouds can be strongly influenced by the frequent air traffic. Besides increasing global cirrus cloudiness <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx43 bib1.bibx66" id="paren.9"/>, aviation-induced contrails and contrail cirrus also alter the optical and microphysical properties of natural cirrus clouds <xref ref-type="bibr" rid="bib1.bibx69 bib1.bibx72 bib1.bibx38" id="paren.10"><named-content content-type="pre">e.g.</named-content></xref>. Studies reveal that the effect of contrails and cirrus clouds on our climate is growing significantly, which is, however, still challenging the atmosphere community to parameterize their overall effect well <xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx37" id="paren.11"/>.</p>
      <p id="d1e218">The radiative effects of cirrus clouds strongly depend on their microphysical properties, e.g. particle number concentration, size, and shape <xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx21" id="paren.12"><named-content content-type="pre">e.g.</named-content></xref>, which are further influenced by the ambient conditions (e.g. temperature and supersaturation) and the nucleation mode <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx32 bib1.bibx65 bib1.bibx72" id="paren.13"/>. Hence, an accurate estimate of ice crystal shape and orientation is very important for the calculation of radiative transfer. In the past few decades, both laboratory experiments and field observations reveal a high variety of habit diagrams of atmospheric ice crystals which are closely correlated with temperature and ice supersaturation <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx3 bib1.bibx35 bib1.bibx36" id="paren.14"/>. In natural clouds, however, ice crystals encounter varying temperature and humidity and may grow into irregular forms <xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx34" id="paren.15"/>. Furthermore, the dependence of ice crystal habits on temperature is also governed by mass transport (including convection and advection) and the region of origin of the particles <xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx71" id="paren.16"><named-content content-type="pre">e.g.</named-content></xref>.</p>
      <p id="d1e241">It is well known that light scattered by atmospheric ice crystals may exhibit different polarization states from incident light. Computation of the geometric ray tracing technique reveals that changes in polarization states depend on the internal ray paths and, more precisely, increase with increasing hexagonal axis ratio (<inline-formula><mml:math id="M8" display="inline"><mml:mo lspace="0mm">=</mml:mo></mml:math></inline-formula> length over width) <xref ref-type="bibr" rid="bib1.bibx67" id="paren.17"><named-content content-type="pre">e.g.</named-content></xref>. The particle linear depolarization ratio (PLDR) is a well-defined parameter for evaluating this effect and is widely used to retrieve information on ice crystal habits, i.e. particle phase, shape, and orientation. In traditional lidar applications, PLDR is defined as the ratio of power from both polarization components perpendicular and parallel to the transmitted laser source and can be calculated using Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>):
          <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M9" display="block"><mml:mrow><mml:mi mathvariant="normal">PLDR</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mo>⊥</mml:mo></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mo>∥</mml:mo></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mo>⊥</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mo>∥</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula> are the perpendicular and parallel components of the backscatter coefficients retrieved from the ice crystals in clouds, respectively. The light backscattered by spherical particles exhibits the same orientation of polarization as the incident light, while the polarization changes when the light is backscattered by non-spherical particles such as cirrus ice crystals <xref ref-type="bibr" rid="bib1.bibx54 bib1.bibx14 bib1.bibx53 bib1.bibx72" id="paren.18"/>. As a well-established technique, polarization lidar has been widely used to provide information on aerosol profiling and to distinguish between different types of aerosols <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx68 bib1.bibx17 bib1.bibx19 bib1.bibx20" id="paren.19"/>. Further, this technique is also applied to unambiguously determine the cloud phase <xref ref-type="bibr" rid="bib1.bibx7" id="paren.20"><named-content content-type="pre">e.g.</named-content></xref> and to study ice cloud properties <xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx51 bib1.bibx1 bib1.bibx18 bib1.bibx72" id="paren.21"><named-content content-type="pre">e.g.</named-content></xref>. PLDR is mainly determined by ice crystal shapes that are a function of temperature, supersaturation (humidity), and potentially the availability of ice nuclei during ice formation <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx3 bib1.bibx56 bib1.bibx28" id="paren.22"><named-content content-type="pre">e.g.</named-content></xref>. In addition, the shapes of ice crystals are strongly influenced by the internal cloud dynamics, lifetime duration, and stage <xref ref-type="bibr" rid="bib1.bibx36" id="paren.23"><named-content content-type="post">and references therein</named-content></xref>. PLDR is a suitable parameter used to retrieve information on ice crystal shape and hence to trace the aviation effects on clouds. Previous studies show that persistent contrails and contrail cirrus are characterized by higher values of PLDR than natural cirrus clouds <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx44 bib1.bibx48 bib1.bibx27" id="paren.24"/>. In addition, <xref ref-type="bibr" rid="bib1.bibx72" id="text.25"/> reported that cirrus clouds with enhanced PLDR values were found to be incidental to significantly lower supersaturations inside the clouds indicating more frequent heterogeneous freezing. They also carried out a backward-trajectory analysis and found that the affected ice clouds appear within areas under the influence of high aviation emissions. Under soot emissions, ice nucleation took place at lower supersaturation, which influences the form and size of ice crystals and further alters their optical properties <xref ref-type="bibr" rid="bib1.bibx72" id="paren.26"/>. During the first COVID-19 lockdown in Europe starting from mid-March 2020, civil air traffic was significantly reduced by up to 88 % in April 2020 compared to the previous year <xref ref-type="bibr" rid="bib1.bibx38" id="paren.27"><named-content content-type="pre">e.g.</named-content></xref>. Based on the analysis of lidar measurements with CALIPSO, a significant reduction in the cirrus PLDR was found in both March and April 2020 compared to the corresponding periods in the previous 6 years <xref ref-type="bibr" rid="bib1.bibx38" id="paren.28"/>. It is known, however, that global air traffic has been growing in the past few decades in terms of number of flights and CO<inline-formula><mml:math id="M12" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation before the COVID-19 pandemic, which, of course, is considered a smaller change in air traffic compared to that caused by the COVID-19 lockdown (see Fig. <xref ref-type="fig" rid="Ch1.F1"/> for the evolution of civil aviation in 42 European countries and regions in the 11 years from 2010 to 2020). In this study, we extend the analyses of <xref ref-type="bibr" rid="bib1.bibx38" id="text.29"/> and study the possible impact of aviation on the microphysical properties of cirrus clouds in terms of seasonality and long-term trend in the occurrence rate (OR) and PLDR of cirrus clouds.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e368">Number of flights and the corresponding CO<inline-formula><mml:math id="M13" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from air traffic in different months over Europe (a total of 42 countries and regions) in 11 years during 2010–2020. The seasonal cycle in air traffic shows more flights (as well as CO<inline-formula><mml:math id="M14" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions) in summer than in winter. The number of flights increased by about 1.30 % yr<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, whereas the CO<inline-formula><mml:math id="M16" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions increased by about 3.16 % yr<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the last 10 years in Europe before the COVID-19 outbreak. During the COVID-19 pandemic, however, civil aviation in Europe was significantly reduced from March 2020 with only a partial recovery in summer 2020 and further reduction afterwards. Furthermore, we also note that there was in fact a slight decrease in the first 3 years from 2010 to 2013, especially in winter and early spring. The plots are reproduced based on the European flight historic data from the European Organisation for the Safety of Air Navigation (EUROCONTROL, <uri>https://www.eurocontrol.int/covid19</uri>, last access: 9 February 2022).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f01.png"/>

      </fig>

      <p id="d1e432">In Sect. 2 we outline the CALIPSO data and methods. Section 3 describes our results concerning seasonal variations and long-term trends in cirrus cloud properties and occurrence based on 10-year lidar measurements from March 2010 to February 2020. The dependence of the cirrus cloud properties on the corresponding ambient temperatures as well as aviation is determined and discussed in Sect. 4. Our conclusions are summarized in Sect. 5.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
      <p id="d1e443">In this study, we focus on the same research area as <xref ref-type="bibr" rid="bib1.bibx38" id="text.30"/>, i.e. the midlatitude regions from 35 to 60<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and from the Atlantic Ocean (15<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) to central Europe (15<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) (for the sake of simplicity, we refer to this research area as “Europe” in the rest of this paper). The measurements of cirrus clouds used here were conducted with the CALIOP (Cloud-Aerosol Lidar with Orthogonal Polarization) lidar, which is carried aboard the CALIPSO satellite within the A-Train constellation in a sun-synchronous polar orbit <xref ref-type="bibr" rid="bib1.bibx80 bib1.bibx62" id="paren.31"/>. CALIOP is a dual-wavelength elastic backscatter lidar at 532 and 1064 nm and is polarization-sensitive at 532 nm <xref ref-type="bibr" rid="bib1.bibx78 bib1.bibx26" id="paren.32"/>. The main datasets used here are the Level 2 5 km Cloud Profile Products of CALIOP which provide information on scientific parameters such as PLDR, temperature (derived from the GEOS-5 data), ice water content (derived from the CALIOP retrieved extinction by ice cloud particles), etc.</p>
      <p id="d1e483">CALIOP is able to observe altitude-resolved profiles of backscatter intensity from numerous geophysical entities including clouds, aerosol layers, regions of clear air, and the returns from the Earth's surface. In this study, however, we are only interested in the cirrus ice clouds. We hence use the vertical feature mask (VFM) developed by the CALIPSO team to distinguish cirrus clouds from other entities including aerosols as well as from non-cirrus clouds <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx41 bib1.bibx25 bib1.bibx49 bib1.bibx73 bib1.bibx79" id="paren.33"><named-content content-type="pre">e.g.</named-content></xref>. Furthermore, the archived data of CALIOP are classified into day- and night-time. The daytime observations are affected by solar illumination, which may lead to a reduction in the signal-to-noise ratio and hence make them more difficult to interpret. However, there is an aviation fingerprint with two maxima of flight densities during morning eastbound and afternoon westbound air traffic in the North Atlantic air traffic corridor, the research area we are focusing on in this study <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx58" id="paren.34"><named-content content-type="pre">e.g.</named-content></xref>. This implies that aviation effects on cirrus clouds are expected to be stronger during daytime than night-time. Therefore, both day- and night-time observations will be analysed here to study the influence of air traffic on cirrus to the fullest extent. For a detailed description of the CALIOP data, readers are referred to <xref ref-type="bibr" rid="bib1.bibx38" id="text.35"/> and references therein.</p>
      <p id="d1e499">Being a nadir-pointing lidar, CALIOP collects data only along the ground track of the CALIPSO satellite. CALIPSO flies 3–4 times each day over this area and therefore <inline-formula><mml:math id="M21" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 100 tracks of observations each month were collected during 2010–2020. Furthermore, this research area covers a large fraction of the North Atlantic flight corridor connecting central Europe with North America where the generation of contrail-induced cirrus clouds and the impact of aviation on cirrus clouds have been intensively studied <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx58 bib1.bibx75 bib1.bibx72 bib1.bibx59 bib1.bibx38" id="paren.36"><named-content content-type="pre">e.g.</named-content></xref>.</p>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
      <p id="d1e522">The cirrus morphologies and ORs as well as the high degree of variability in their microphysical properties depend greatly on the substantial differences in meteorological conditions. Hence, we first compare the evolution of the general meteorological conditions along the entire altitude range from 6 to 13 km including temperature, relative humidity with respect to ice (RHi), as well as vertical updraft and wind velocity covering our research area during 2010–2020. These parameters are directly derived from global ERA5 reanalysis data, produced by ECMWF with the Copernicus Climate Change Service <xref ref-type="bibr" rid="bib1.bibx22" id="paren.37"/>, and their monthly values are shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>. The vertical bars in the upper panels stand for all the data points of air temperature and RHi, and in the lower panels, for vertical updraft and wind velocity. The blue circles show the medians of each quantity in different months and the red lines are best-fitting lines using a simple linear regression model (i.e. least squares fit of a first-degree polynomial to data) for all four quantities. The derived slopes are hence considered as the long-term trends in each quantity. First, there is a clear seasonal cycle in the air temperatures and a higher degree of variability in temperatures can be seen in winter than in summer. Further, extremely low temperatures with medians below <inline-formula><mml:math id="M22" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 <inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C are seen in January and February 2012, which are indicative of the cold spell in early 2012 in Europe starting from 24 January and lasting for about 3 weeks <xref ref-type="bibr" rid="bib1.bibx11" id="paren.38"/>. The influence of the extreme lower temperatures on the properties of cirrus clouds will be discussed below. Air temperatures show in median values an increasing trend of 0.0941 <inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C yr<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> with the confidence level at 90.0 %. In addition, the year-to-year variabilities of air temperatures in different months show that temperatures increased more significantly in winter than in summer (an increasing trend of 0.0098 <inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C yr<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in summer and 0.1183 <inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C yr<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in winter). The seasonal cycle in RHi, however, is not as significant as in air temperatures. For the long-term evolution, RHi shows a small decrease in median values with a trend of <inline-formula><mml:math id="M30" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.0557 % yr<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at the confidence level of only 25.5 %. In addition, the maxima of the monthly RHi values show a decreasing trend of <inline-formula><mml:math id="M32" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.2431 % yr<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (81.1 % confidence level), whereas their minima show an increasing trend of 0.9125 % yr<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (99.8 % confidence level); i.e. the range of the RHi distribution became narrower in the last 11 years, especially during the period from 2010 to the end of 2017. We mentioned earlier that the vertical updrafts play a crucial role in the formation of cirrus clouds. However, monthly mean values of vertical updrafts determined from ERA5 reanalysis data are highly smoothed and can only provide a climatological reference for the background. This is also the case for wind velocity. Figure <xref ref-type="fig" rid="Ch1.F2"/> (lower panel) shows in general a small decrease in vertical updrafts (negative values for upwards) and a small decrease in wind velocity with the confidence level at 53.7 % and 35.6 %, respectively. In a nutshell, the meteorological and dynamical conditions over Europe in the last 11 years provide us with a general picture of the background, which is generally stable during the period we focus on. With this information in mind, we can further study the seasonal variations and long-term trends in cirrus cloud occurrence and properties.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e668">Monthly variations in air temperature, relative humidity with respect to ice (RHi), vertical updraft, and wind velocity in the background at altitudes from 6 to 13 km, derived from ERA5 reanalysis data for 11 years from 2010 to 2020 over the European area (i.e. the research area in this study, lat: 35–60<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, long: 15<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W to 15<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E). The vertical bars show the value ranges for temperatures and RHi, respectively, in panels <bold>(a)</bold> and <bold>(b)</bold>, and for vertical updraft and wind, respectively, in panels <bold>(c)</bold> and <bold>(d)</bold>. The blue circles show the medians of each quantity in different months and the red lines are the best-fitting lines using the simple linear regression to data for all of them.</p></caption>
        <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f02.png"/>

      </fig>

<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Seasonal variations of cirrus clouds</title>
      <p id="d1e724">We first present the distribution of cirrus PLDR in each month from January 2010 to December 2020 in Fig. <xref ref-type="fig" rid="Ch1.F3"/>. This is derived from the observations at the typical altitudes in which cirrus clouds form from 6 to 13 km and at temperatures between <inline-formula><mml:math id="M38" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>75 and <inline-formula><mml:math id="M39" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>38 <inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. Please note that typical cruising altitudes of aircraft over the North Atlantic and Europe lie between 8.8 and 12.5 km. However, aviation emissions over the mainland take place also at lower altitudes during ascent and descent from and to the airports. In order to compare the distribution of cirrus PLDR in different months, the number densities of scatter point data are normalized and visualized with different colour codes with the maximum number density indicated by 1 for each month. February 2016 with no observations available is marked in blank. Figure <xref ref-type="fig" rid="Ch1.F3"/> provides a general climatology of the PLDR distributions in Europe with the majority of PLDR (<inline-formula><mml:math id="M41" display="inline"><mml:mo lspace="0mm">&gt;</mml:mo></mml:math></inline-formula> 60 % of the maxima) falling within the range from 0.2 to 0.55. There are clear seasonal cycles as expected in PLDR, which becomes more remarkable for those falling within the smaller range of PLDR. In addition, there are clear reductions in PLDR during the period of COVID-19 from March to December 2020 compared to the corresponding months in the previous years, which is consistent with previous studies <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx76" id="paren.39"/> and will be discussed in detail below. Furthermore, the reductions in the cirrus PLDR are more remarkable for the measurements made in the daytime. The ORs of cirrus cloud during the period of COVID-19 also show a reduction, which has been reported recently <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx50 bib1.bibx38" id="paren.40"><named-content content-type="pre">e.g.</named-content></xref>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e772">Number densities of the cirrus PLDR distribution normalized for each month from January 2010 to December 2020. The data are derived from the observations at the typical cirrus heights from 6 to 13 km and at temperatures between <inline-formula><mml:math id="M42" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>75 and <inline-formula><mml:math id="M43" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>38 <inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. The colour codes are used to visualize the relative number densities of scatter point data, with the maximum number density indicated by 1 in the colour bar.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e806">Distributions of the occurrence rate (OR) and PLDR of cirrus clouds in each 1 km altitude bin. Both parameters follow a seasonal cycle: cirrus clouds in winter are characterized by larger values of PLDR and higher ORs than in summer. Furthermore, cirrus clouds appear within the full altitude range from 6 to 13 km in the winter months but only within the altitudes from <inline-formula><mml:math id="M45" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 9 to 12.5 km in summer.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f04.png"/>

        </fig>

      <p id="d1e823">We next turn to the seasonality in cirrus cloud occurrence and PLDR in more detail. Figure <xref ref-type="fig" rid="Ch1.F4"/> shows the cirrus OR and PLDR in different months (see the legend on the plot with descriptive labels) for each 1 km altitude bin from 6 to 13 km. They are derived from both day- and night-time lidar measurements of CALIPSO within the typical altitude range of cirrus clouds at temperatures between <inline-formula><mml:math id="M46" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>75 and <inline-formula><mml:math id="M47" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>38 <inline-formula><mml:math id="M48" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C over the last 10 years before COVID-19, i.e. from March 2010 to February 2020. The data with cirrus OR smaller than 0.1 % are neglected for plotting PLDR in the right panel. The profiles of cirrus OR along altitudes show that cirrus clouds mainly occurred in the height range from 9 to 11 km (with OR <inline-formula><mml:math id="M49" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 3 % in every month). The cirrus occurrence follows a significant seasonal cycle in all the altitude bins. The maxima of cirrus OR, up to 11 %, are found in the winter months, precisely in January or February below 10 km and in December above 10 km, respectively, and the minima of OR appear in July along altitudes. In addition, there is a stronger seasonality in the lower altitudes, with the cirrus OR in winter more than 10 times larger than in summer. Please note that this study concentrates on the aviation effects on cirrus clouds and thus the measurements of cirrus clouds due to deep convection are excluded when applying the CALIPSO VFM, which leads to a decrease in the cirrus ORs, especially in summer. Furthermore, cirrus clouds in the winter months appear within the full altitude range from 6 to 13 km while in summer only from 9 to 12.5 km for the data with OR <inline-formula><mml:math id="M50" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 1 % considered. For the PLDR values of cirrus clouds shown in the right panel, they also follow a distinct seasonal cycle in which cirrus clouds are characterized by larger PLDR values in winter than in summer in each altitude bin and the difference of PLDR in different months can be as large as 0.06 (<inline-formula><mml:math id="M51" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 15 %). The distributions of cirrus PLDR along altitudes show a clear increase with altitudes in each month and the difference in the medians of PLDR in each month can be as large as more than 0.1 <xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx38" id="paren.41"/>.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Long-term trend of cirrus cloud properties with significance test</title>
      <p id="d1e885">In Fig. <xref ref-type="fig" rid="Ch1.F5"/> (upper panel) we present the medians of cirrus PLDR in every month derived from both day- and night-time observations from 2010 to 2020 that covers the period of the COVID-19 pandemic in 2020. We can see that the cirrus PLDR shows clear reductions during the period of COVID-19 starting from March 2020 compared with the corresponding months in the previous years (shown with squares in grey in the upper panel of Fig. <xref ref-type="fig" rid="Ch1.F5"/>). The same findings on the changes in the cirrus cloud properties and occurrence in March and April 2020 compared to the previous years have been reported by <xref ref-type="bibr" rid="bib1.bibx38" id="text.42"/> as well as in early summer 2020 during the BLUESKY campaign by <xref ref-type="bibr" rid="bib1.bibx76" id="text.43"/>. Hence, in this study only observations before the COVID-19 outbreak are considered for further analysis. In order to calculate the long-term trends in the cirrus PLDR, we apply two methods in this study, i.e. the ordinary least square (OLS) estimator and Theil–Sen estimator (TSE) (<xref ref-type="bibr" rid="bib1.bibx70 bib1.bibx61" id="altparen.44"/>). The OLS estimator is a commonly used method to estimate the unknown parameters in a linear regression model by minimizing the sum of the squares of the differences between the observed dependent variables (here PLDR) and those predicted by the linear function of the independent variable (time in months). However, OLS is strongly affected by the presence of outliers in the time series, thus making the estimation less efficient. The TSE method is a nonparametric estimation technique by calculating all the slopes between pairs of points and choosing the median as the estimation of the regression slope. Compared to OLS, TSE is a robust linear regression against outliers since it uses medians instead of means. The calculated long-term trends (i.e. slopes) and the regressed linear fits with both methods are shown on the plot. We mentioned earlier that the aviation densities in Europe grew more strongly from 2013 (see Fig. <xref ref-type="fig" rid="Ch1.F1"/>). We hence further calculate the trends for the observations during a shorter period from March 2013 to February 2020 and the corresponding results are also presented in Fig. <xref ref-type="fig" rid="Ch1.F5"/>. First, the PLDR values show an increasing trend with a slope of 0.77 <inline-formula><mml:math id="M52" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 1.02 <inline-formula><mml:math id="M54" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> with both methods, respectively, in the 10 years before the COVID-19 outbreak. We note the exceptions that cirrus clouds are characterized by extremely large values of PLDR in January and February 2012, which might be connected with the cold spell in Europe in early 2012 <xref ref-type="bibr" rid="bib1.bibx11" id="paren.45"><named-content content-type="pre">e.g.</named-content></xref>. We further compare the occurrence heights of cirrus clouds in January and February 2012 with other years and find that they are higher in distribution than other years. Conversely, the extremely low values of PLDR in July 2012 are correlated with the much lower occurrence heights of cirrus clouds in July 2012 than in other years. The interpretations for the results are based on the altitude dependence of the cirrus PLDR that is presented in Fig. <xref ref-type="fig" rid="Ch1.F4"/> and also reported in previous studies <xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx38" id="paren.46"><named-content content-type="pre">e.g.</named-content></xref>. For the subsequent analysis the extreme values are considered as outliers and removed. The interpolated data are then analysed with both OLS and TSE methods and the derived slopes are 0.87 <inline-formula><mml:math id="M57" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 0.97 <inline-formula><mml:math id="M59" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively. These exercises imply that the TSE method is more efficient for the data analysed here. Compared with the changes in aviation, we find that the PLDR values generally increase following the increasing aviation densities. This is consistent with the previous studies showing that cirrus clouds with enhanced PLDR values form in areas of high aviation emissions or vice versa <xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx38" id="paren.47"><named-content content-type="pre">e.g.</named-content></xref>. Furthermore, larger trends are expected and derived as well from observations in a shorter period from March 2013 with a slope of 1.18 <inline-formula><mml:math id="M62" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 1.51 <inline-formula><mml:math id="M64" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> with both methods, respectively. The same analyses are extended to the observations made only during daytime (not shown here), and the corresponding results show slightly larger trends of 0.93 <inline-formula><mml:math id="M67" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and 1.09 <inline-formula><mml:math id="M69" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> with both OLS and TSE, respectively, than the results derived from the combined day- and night-time observations. All the results of long-term trends with the medians of total PLDR values are summarized in Tables <xref ref-type="table" rid="Ch1.T1"/> and <xref ref-type="table" rid="Ch1.T2"/>. The comparison indicates that aviation exerts a stronger influence on cirrus clouds in the daytime than at night since there is an aviation fingerprint with two maxima during morning eastbound and afternoon westbound air traffic in the North Atlantic flight corridor covering the area in this study <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx58" id="paren.48"><named-content content-type="pre">e.g.</named-content></xref>.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e1138"><bold>(a)</bold> Medians of cirrus PLDR in different months from March 2010 to February 2020 shown in grey lines and during the COVID-19 pandemic starting from March 2020 shown in squares. The results are derived from both day- and night-time lidar measurements of CALIPSO. Both OLS and TSE methods are applied to determine the long-term trends (i.e. slopes) of the cirrus PLDR (medians) and the results are indicated on the plot (see text for details). <bold>(b)</bold> The long-term trends determined from the deseasonalized time series of cirrus PLDR (medians).</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f05.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1155">Long-term trends of monthly values of particle linear depolarization ratio (PLDR) within the typical cirrus altitude range from 6 to 13 km derived from both day- and night-time data during the period from March 2010 to February 2020: Comparison between two methods of the ordinary least square (OLS) estimator and the Theil–Sen estimator (TSE), including the Mann–Kendall (MK) significance test.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Median</oasis:entry>
         <oasis:entry colname="col3">OR of cirrus</oasis:entry>
         <oasis:entry colname="col4">Trend</oasis:entry>
         <oasis:entry colname="col5">Trend</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M72" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M73" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(%)</oasis:entry>
         <oasis:entry colname="col4">(yr<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, OLS)</oasis:entry>
         <oasis:entry colname="col5">(yr<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, TSE)</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">PLDR (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">0.3701</oasis:entry>
         <oasis:entry colname="col3">4.3679</oasis:entry>
         <oasis:entry colname="col4">0.7732 <inline-formula><mml:math id="M76" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">1.0170 <inline-formula><mml:math id="M78" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7">0.0079</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Deseasonalized PLDR (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">0.4703 <inline-formula><mml:math id="M80" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.6676 <inline-formula><mml:math id="M82" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M84" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PLDR (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">0.3714</oasis:entry>
         <oasis:entry colname="col3">4.4451</oasis:entry>
         <oasis:entry colname="col4">1.1754 <inline-formula><mml:math id="M85" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M86" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">1.5084 <inline-formula><mml:math id="M87" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7">0.0258</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Deseasonalized PLDR (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">0.5572 <inline-formula><mml:math id="M89" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M90" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">0.7197 <inline-formula><mml:math id="M91" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M93" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e1519">Same as Table <xref ref-type="table" rid="Ch1.T1"/>, but for the results derived from only daytime data during the period from March 2010 to February 2020.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Median</oasis:entry>
         <oasis:entry colname="col3">OR of cirrus</oasis:entry>
         <oasis:entry colname="col4">Trend</oasis:entry>
         <oasis:entry colname="col5">Trend</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M94" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M95" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(%)</oasis:entry>
         <oasis:entry colname="col4">(yr<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, OLS)</oasis:entry>
         <oasis:entry colname="col5">(yr<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, TSE)</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">PLDR (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">0.4084</oasis:entry>
         <oasis:entry colname="col3">3.6335</oasis:entry>
         <oasis:entry colname="col4">0.9301 <inline-formula><mml:math id="M98" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">1.0946 <inline-formula><mml:math id="M100" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M102" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Deseasonalized PLDR (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">0.8325 <inline-formula><mml:math id="M103" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M104" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">1.0210 <inline-formula><mml:math id="M105" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M106" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M107" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PLDR (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">0.4106</oasis:entry>
         <oasis:entry colname="col3">3.6335</oasis:entry>
         <oasis:entry colname="col4">1.1073 <inline-formula><mml:math id="M108" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">1.3548 <inline-formula><mml:math id="M110" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M111" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M112" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Deseasonalized PLDR (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">0.9082 <inline-formula><mml:math id="M113" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M114" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">1.0483 <inline-formula><mml:math id="M115" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">1</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M117" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1893">We mentioned in the previous subsection that cirrus cloud properties (PLDR) and ORs are dominated by seasonal cycles. Spectral analysis with Fourier transform is carried out on the time series of PLDR (not shown here), and the periodogram of PLDR with a dominant peak of power at the point of the 12-month cycle indicates a conspicuous seasonality (aka annual cycle). This repeating cycle of seasonality may obscure the long-term trend in the data that we want to determine. We therefore deseasonalize the data by computing the monthly climatological mean values, subtracting them from each monthly record and finally adding the total mean of PLDR. The deseasonalized values of PLDR are shown in the lower panel of Fig. <xref ref-type="fig" rid="Ch1.F5"/>. The detection of seasonal anomalies of extremely large PLDR values in winter and extremely small PLDR values in summer are easy, but the opponent cases are not. With the deseasonalization process, an outlier of February 2018 is detected which, however, will not bias the calculation by using the TSE method. The results of long-term trends again calculated with both OLS and TSE methods and the regressed linear fits are also shown in Fig. <xref ref-type="fig" rid="Ch1.F5"/> (lower panel). The deseasonalized PLDR values show a long-term trend of 0.67 <inline-formula><mml:math id="M118" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (with TSE) and 0.72 <inline-formula><mml:math id="M121" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (with TSE) for the combined day- and night-time observations in the period from March 2010 to February 2020 and during a shorter period from March 2013 to February 2020, respectively.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e1966">Long-term trends of monthly occurrence rate (OR) of cirrus clouds at the typical cirrus altitude range from 6 to 13 km derived from both day- and night-time data during the period from March 2010 to February 2020 with the Theil–Sen estimator (TSE) method including the Mann–Kendall (MK) significance test.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Median</oasis:entry>
         <oasis:entry colname="col3">Trend</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M124" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M125" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(%)</oasis:entry>
         <oasis:entry colname="col3">(% yr<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, TSE)</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">OR (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">4.2660</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M128" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.0017</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.9910</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M129" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.0113</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Deseasonalized OR (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">4.4578</oasis:entry>
         <oasis:entry colname="col3">-0.0121</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.4466</oasis:entry>
         <oasis:entry colname="col6">-0.7610</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">OR (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">4.3701</oasis:entry>
         <oasis:entry colname="col3">-0.0795</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.1962</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M130" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>1.2923</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Deseasonalized OR (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">4.4515</oasis:entry>
         <oasis:entry colname="col3">-0.0916</oasis:entry>
         <oasis:entry colname="col4">1</oasis:entry>
         <oasis:entry colname="col5">0.0098</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M131" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.5844</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4" specific-use="star"><?xmltex \currentcnt{4}?><label>Table 4</label><caption><p id="d1e2178">Long-term trends of monthly occurrence height (OH) of cirrus clouds at the typical cirrus altitude range from 6 to 13 km derived from both day- and night-time data during the period from March 2010 to February 2020 with the Theil–Sen estimator (TSE) method including the Mann–Kendall (MK) significance test.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Median</oasis:entry>
         <oasis:entry colname="col3">Trend</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M132" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M133" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(km)</oasis:entry>
         <oasis:entry colname="col3">(km yr<inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, TSE)</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"/>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">OH (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">10.06</oasis:entry>
         <oasis:entry colname="col3">0.0238</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.1202</oasis:entry>
         <oasis:entry colname="col6">1.5541</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Deseasonalized OH (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">9.95</oasis:entry>
         <oasis:entry colname="col3">0.0309</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">0.1022</oasis:entry>
         <oasis:entry colname="col6">1.6345</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">OH (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">10.06</oasis:entry>
         <oasis:entry colname="col3">0.0447</oasis:entry>
         <oasis:entry colname="col4">1</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M136" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
         <oasis:entry colname="col6">4.2646</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Deseasonalized OH (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2">9.96</oasis:entry>
         <oasis:entry colname="col3">0.0508</oasis:entry>
         <oasis:entry colname="col4">1</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M137" display="inline"><mml:mo>&lt;</mml:mo></mml:math></inline-formula> 0.001</oasis:entry>
         <oasis:entry colname="col6">5.1694</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2375">The significance tests of the derived trends in the cirrus PLDR and their deseasonalized time series are carried out applying the Mann–Kendall (MK) test <xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx31" id="paren.49"/>. It is a rank-based nonparametric method that has been widely used to statistically assess whether there is a monotonic trend in a time series of environmental and hydrological data <xref ref-type="bibr" rid="bib1.bibx82" id="paren.50"><named-content content-type="pre">e.g.</named-content></xref> (see Appendix B). The overall results of the MK test for the long-term trends in PLDR at a significance level of <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> % are presented in Tables <xref ref-type="table" rid="Ch1.T1"/> and <xref ref-type="table" rid="Ch1.T2"/> for all the observations (including day- and night-time) and for only the daytime observations, respectively. Here, the <inline-formula><mml:math id="M139" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value returned from a MK test is a measure of the probability of rejecting or retaining the null hypothesis H0 stating that the data are independently distributed with no trend. <inline-formula><mml:math id="M140" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula> is a logical value (0 or 1) used to give the test decision: <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates a rejection of the null hypothesis (i.e. no trend) and <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> indicates a failure to reject it at the 5 % significance level. From the results of the MK test, it is striking that significantly increasing trends (all with <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mi>h</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) exist in the monthly values of PLDR and their deseasonalized values in the period from March 2010 to February 2020 as well as during a shorter period from March 2013 to February 2020.</p>
      <p id="d1e2454">We next turn to the determination of trend in the OR of cirrus clouds. Again, we analyse the observations of cirrus clouds at the altitudes from 6 to 13 km and at the temperatures from <inline-formula><mml:math id="M144" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>75 to <inline-formula><mml:math id="M145" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>38 <inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. The corresponding results are shown in Fig. <xref ref-type="fig" rid="Ch1.F6"/> (upper panel). Clearly, a strong seasonal cycle also exists in the OR with a monthly mean value of up to 8 % in the winter months and as low as 1 % in summer. Following the same procedure, the deseasonalization of cirrus OR was carried out and the corresponding results are shown in the lower panel of Fig. <xref ref-type="fig" rid="Ch1.F6"/>. The long-term trends are calculated with the TSE method and the linear fits are overplotted in Fig. <xref ref-type="fig" rid="Ch1.F6"/> showing negative values; i.e. the cirrus ORs decrease with time in the 10 years before COVID-19. However, the significance tests with the MK test show that only a significant trend of <inline-formula><mml:math id="M147" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.0916 % yr<inline-formula><mml:math id="M148" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> exists in the deseasonalized OR for the period from March 2013 to February 2020. The derived long-term trends in the cirrus ORs are summarized in Table 3 along with their median values and the results of the significance test. Nevertheless, the decreasing cirrus OR can be traced back to the changes in the meteorological conditions, i.e. with increasing temperatures and decreasing humidity, during this 10-year period (see Fig. <xref ref-type="fig" rid="Ch1.F2"/>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e2510">Long-term variations in monthly occurrence rate (OR) of cirrus clouds in the period 2010–2020 as well as the linear fitting for the values in the periods from March 2010 to February 2020 (in red) and from March 2013 to February 2020 (in blue). The ORs of cirrus clouds during the COVID-19 pandemic are shown in black for comparison. The corresponding trends (i.e. the slopes) are indicated on the plot: panel <bold>(a)</bold> for the derived monthly OR from all the data including day- and night-time; panel <bold>(b)</bold> for the deseasonalized time series of OR.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f06.png"/>

        </fig>

      <p id="d1e2525">We presented earlier that PLDR generally increases with altitude. We hence determine the occurrence heights of cirrus clouds and their monthly means are shown in Fig. <xref ref-type="fig" rid="Ch1.F7"/>. The occurrence heights of cirrus also follow a distinct seasonal cycle with larger values in the summer months than in winter, which indicates that cirrus clouds in winter occur at the full altitude range from 6 to 13 km but in summer only at higher altitudes. The same procedures to calculate the long-term trends with the TSE method were carried out and the corresponding results are shown in Fig. <xref ref-type="fig" rid="Ch1.F7"/>. It is striking that the occurrence heights of cirrus clouds show a trend of 0.0238 km yr<inline-formula><mml:math id="M149" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (0.0447 km yr<inline-formula><mml:math id="M150" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) during the full period from March 2010 to February 2020 (a shorter period from March 2013 to February 2020). After deseasonalizing the data, we reach a long-term trend of 0.0309 km yr<inline-formula><mml:math id="M151" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (0.0508 km yr<inline-formula><mml:math id="M152" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) for the full period (a shorter period). Table 4 shows the summary of the derived long-term trends in the occurrence heights of cirrus clouds and the corresponding significance test. Importantly, the trends in the deseasonalized values of cirrus occurrence heights are statistically significant according to the results of the MK test. These findings are consistent with the upward shift of the aircraft cruising altitudes in the last years due to the fact that aircraft flying higher leads to less fuel burn and hence less CO<inline-formula><mml:math id="M153" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions (<ext-link xlink:href="https://www.eurocontrol.int/publication/eurocontrol-data-snapshot-21-aircraft-flying-higher-more-efficiently-and-sustainably">https://www.eurocontrol.int/publication/eurocontrol-data-snapshot-21-aircraft-flying-higher-more-efficiently-and-sustainably</ext-link>, last access: 27 October 2022). In contrast to this, however, an upward displacement of air traffic may lead to the increase in the contrail coverage <xref ref-type="bibr" rid="bib1.bibx12" id="paren.51"><named-content content-type="pre">e.g.</named-content></xref>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e2600">Same as Fig. <xref ref-type="fig" rid="Ch1.F6"/>, but for the long-trend variations of the occurrence heights of cirrus clouds for both day- and night-time observations during the period from March 2010 to February 2020.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f07.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Correlation with the ambient temperatures</title>
      <p id="d1e2627">It is reported that temperatures and other meteorological parameters play a decisive role in the formation and maintenance of cirrus clouds <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx71" id="paren.52"><named-content content-type="pre">e.g.</named-content></xref>. Given the scope of this study, we only discuss the contributions of temperature to the cirrus cloud properties. We first compare the relationship between the cirrus PLDR and the corresponding ambient temperatures in clouds. The temperatures used for this analysis are derived from the GEOS-5 (Goddard Earth Observing System, version 5) model data product provided to the CALIPSO by the GMAO (Global Modeling and Assimilation Office) data assimilation system. The comparisons between both quantities show that the dependence of the cirrus PLDR on the ambient temperatures has clearly different variations separated at a temperature threshold of <inline-formula><mml:math id="M154" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M155" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 <inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. At temperatures below <inline-formula><mml:math id="M157" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 <inline-formula><mml:math id="M158" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, the PLDR values are roughly negatively correlated with the ambient temperatures. At temperatures warmer than <inline-formula><mml:math id="M159" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 <inline-formula><mml:math id="M160" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, however, PLDR shows no clear correlation with the ambient temperatures, with the majority of values falling within the range from <inline-formula><mml:math id="M161" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 0.23 to 0.45. The same relationship was determined also from the monthly data in April from 2014 to 2020 by <xref ref-type="bibr" rid="bib1.bibx38" id="text.53"/> (see their Fig. 7). For all the data in total, the PLDR values show a negative correlation with the corresponding ambient temperatures.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e2703"><bold>(a)</bold> The grey circles stand for the correlation between the monthly medians of cirrus PLDR and the corresponding ambient temperatures, and the black line for the linear fitting line derived from all data points. <bold>(b, c)</bold> The monthly medians of cirrus PLDR during the period from March 2010 to February 2020 are shown in grey and the regressed values with the first-degree polynomial are shown in blue <bold>(b)</bold>; the residuals after removing the regressed values from the monthly medians of PLDR are shown in grey and the linear fitting line with the Theil–Sen estimator (TSE) method is shown in red, with the long-term trend of 0.54 <inline-formula><mml:math id="M162" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M164" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> indicated on the plots <bold>(c)</bold>.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f08.png"/>

        </fig>

      <p id="d1e2755">We further calculate the medians of cirrus PLDR in each month from March 2010 to February 2020 as well as the medians of ambient temperatures in cirrus clouds and the corresponding results are presented in the left panel of Fig. <xref ref-type="fig" rid="Ch1.F8"/>. The scatter plots clearly show that the cirrus PLDR values increase following the decreasing ambient temperatures with a correlation coefficient <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.76</mml:mn></mml:mrow></mml:math></inline-formula>, which is statistically significant (<inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.0001</mml:mn></mml:mrow></mml:math></inline-formula>). Due to the strong influence of the ambient temperatures on the properties of cirrus clouds, an appropriate method is needed to eliminate the parts in cirrus PLDR induced by temperatures. In this study, a regression model based on linear dependence is applied to isolate the temperature-induced parts:
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M167" display="block"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">th</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>b</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>b</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>⋅</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where the variable <inline-formula><mml:math id="M168" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> stands for the ambient temperature and <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">th</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the theoretical value of PLDR regressed from temperatures. After regression analyses, the absolute deviation <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi></mml:mrow></mml:math></inline-formula> (i.e. the residual) of the observational data <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from the corresponding <inline-formula><mml:math id="M172" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">th</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be calculated by
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M173" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">obs</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">th</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          Using the derived <inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi></mml:mrow></mml:math></inline-formula>, linear trends can further be determined using a simple linear regression model:
            <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M175" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi><mml:mo>=</mml:mo><mml:mi>d</mml:mi><mml:mo>+</mml:mo><mml:mi>m</mml:mi><mml:mo>⋅</mml:mo><mml:mi mathvariant="normal">time</mml:mi></mml:mrow></mml:math></disp-formula>
          where “time” stands for each month, season, or year for which data are available. For this study, a linear trend coefficient (slope) <inline-formula><mml:math id="M176" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> can be determined from the monthly values of PLDR medians using Eq. (<xref ref-type="disp-formula" rid="Ch1.E4"/>).</p>
      <p id="d1e2937">Applying the linear dependence by Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) as well as Eq. (<xref ref-type="disp-formula" rid="Ch1.E4"/>), we derive the regressed PLDR values and the residuals (see the right panels of Fig. <xref ref-type="fig" rid="Ch1.F8"/>). The long-term trend in the residuals is calculated with the TSE method showing an increase of 0.54 <inline-formula><mml:math id="M177" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M178" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M179" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, which is above the 90 % confidence level according to the MK test with <inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0582</mml:mn></mml:mrow></mml:math></inline-formula>. For a comparison, we also determine the regressed values according to the quadratic and cubic dependence, which, however, show no major difference from the results based on the linear dependence. The same analyses were also carried out on the daytime observations resulting in a long-term trend of 0.69 <inline-formula><mml:math id="M181" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M182" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the residuals of PLDR, which is statistically significant with <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.001</mml:mn></mml:mrow></mml:math></inline-formula>. We should note that the dependence of the cirrus PLDR on the ambient temperatures to the full extent is not linear but shows different characteristics in different temperature range (roughly separated at <inline-formula><mml:math id="M185" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M186" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 <inline-formula><mml:math id="M187" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C). However, the monthly mean values of both quantities along the full altitudes of cirrus clouds can still provide a climatological relationship between them. After removing the temperature-induced parts in the cirrus PLDR, the residuals still show an increasing trend over this period, which are presumed to be due to other factors than the meteorological conditions.</p>
      <p id="d1e3057">We discussed earlier that the occurrence heights of cirrus clouds show on average an increase over this period which, in general, corresponds to a decrease in temperatures in clouds. The altitude dependence of temperatures is assumed based on the fact that the tropopause heights are roughly 1.2 km higher than the peak of the cirrus occurrence heights (i.e. the most probable altitudes at which cirrus clouds occurred) and both parameters are highly correlated including their seasonal cycles and trends.</p>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Correlation with the air traffic densities over Europe</title>
      <p id="d1e3068">Using the airborne lidar measurements during the ML-CIRRUS campaign in 2014 <xref ref-type="bibr" rid="bib1.bibx75" id="paren.54"/>, <xref ref-type="bibr" rid="bib1.bibx72" id="text.55"/> concentrated on the specific clouds and found lower supersaturation in the cirrus clouds with enhanced PLDR which were traced back to be forming in areas of high aviation emissions. Recently, <xref ref-type="bibr" rid="bib1.bibx38" id="text.56"/> analysed the satellite data of CALIPSO which cover the European area (i.e. the same research area as the current study) and found that strong reductions in air traffic in Europe caused by the COVID-19 pandemic led to significant changes in cirrus cloud properties in terms of PLDR. In this study, we further study the impact of the increasing air traffic on the cirrus clouds in a longer period of 10 years before COVID-19. We described that the air traffic densities in the 42 European countries and regions (see Fig. <xref ref-type="fig" rid="Ch1.F1"/>) show a clear seasonal cycle which is, however, roughly anticorrelated with the seasonality in the cirrus PLDR. To directly compare them, we first deseasonalize both datasets (here considering CO<inline-formula><mml:math id="M188" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions as a proxy of air traffic densities) and the results are shown in Fig. <xref ref-type="fig" rid="Ch1.F9"/>. Please note that both the number of flights and the CO<inline-formula><mml:math id="M189" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation are available and analysed here. The results derived from both datasets are consistent. Hence, we will only concentrate on the effect of CO<inline-formula><mml:math id="M190" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation. According to the description above, the outliers in the deseasonalized PLDR have been removed and further interpolated (see Fig. <xref ref-type="fig" rid="Ch1.F5"/>). Furthermore, the annual mean variations of the deseasonalized PLDR are derived using a 12-point moving average smooth (shown in black in Fig. <xref ref-type="fig" rid="Ch1.F9"/>). We can see that the unexpected extreme values of PLDR might significantly change the deseasonalized dataset. The low values of the deseasonalized PLDR in the second half of 2010 and the first half of 2018 are presumed to be due to lower values of PLDR in August and November 2010 as well as February–March 2018 compared to the corresponding months in other years, respectively, which are correlated with the lower occurring heights of cirrus as discussed above (see Fig. <xref ref-type="fig" rid="Ch1.F7"/>). Besides the anomalies, an increasing trend can conspicuously be recognized in both parameters, especially during the period from January 2013 to February 2020. The correlation coefficients between them for a full period from January 2010 to February 2020 are <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.54</mml:mn></mml:mrow></mml:math></inline-formula>, respectively. Larger values of the correlation coefficients (<inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.58</mml:mn></mml:mrow></mml:math></inline-formula>) are also derived for a shorter period from January 2013 to February 2020. The confidence levels for all the cases are above 99.5 %.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e3157">Comparison between the deseasonalized time series of cirrus PLDR (in blue) and the corresponding deseasonalized CO<inline-formula><mml:math id="M194" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation in Europe (in green). The annual mean variations of the deseasonalized PLDR are overplotted with a 12-point moving average smooth (in black). The correlation coefficients between both parameters for a full period as well as for a shorter period from January 2013 are calculated and indicated on the plot, which are all at the confidence level above 99.5 %.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f09.png"/>

        </fig>

<?xmltex \hack{\newpage}?><?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e3179">Long-term trends in cirrus PLDR in different seasons and their correlations with the corresponding CO<inline-formula><mml:math id="M195" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation in Europe. There are increasing trends in PLDR as well as CO<inline-formula><mml:math id="M196" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation in all seasons in the 10 years before COVID-19. The correlation analysis between both parameters shows a strong correlation in winter, spring, and autumn, but a weak correlation in summer.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/15963/2022/acp-22-15963-2022-f10.png"/>

        </fig>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><?xmltex \currentcnt{5}?><label>Table 5</label><caption><p id="d1e3209">Correlation coefficients between the monthly PLDR values of cirrus clouds within the altitude from 6 to 13 km and corresponding CO<inline-formula><mml:math id="M197" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation as well as number of flights in Europe in different seasons.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.97}[.97]?><oasis:tgroup cols="5">
     <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:colspec colnum="5" colname="col5" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Season</oasis:entry>
         <oasis:entry colname="col2">Winter (DJF)</oasis:entry>
         <oasis:entry colname="col3">Spring (MAM)</oasis:entry>
         <oasis:entry colname="col4">Summer (JJA)</oasis:entry>
         <oasis:entry colname="col5">Autumn (SON)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">CO<inline-formula><mml:math id="M198" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.18</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.3211</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.30</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.1345</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M204" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.4247</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M205" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.49</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0098</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CO<inline-formula><mml:math id="M207" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.57</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0047</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.46</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0354</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.8216</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.61</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0034</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Number of flights (Mar 2010–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M216" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.1624</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M218" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.37</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0573</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M220" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5802</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.40</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M223" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0373</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Number of flights (Mar 2013–Feb 2020)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.49</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0170</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.60</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0039</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9376</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.53</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.0125</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <p id="d1e3703">With the general relationship between the cirrus PLDR and air traffic in the 10-year period in mind, we may further concentrate on their correlations in different seasons. To illustrate the seasonal variations of the relationships between the cirrus PLDR and air traffic, we show the comparison between both parameters in different seasons (winter: December–February, but only January and February for 2010; spring: March–May; summer: June–August; autumn: September–November) in Fig. <xref ref-type="fig" rid="Ch1.F10"/>. First, the cirrus PLDR values in all the seasons show increasing trends in the 10 years before COVID-19. The trend in summer, however, is much smaller (10 times smaller) than those in other seasons. Strong reductions in air traffic due to the COVID-19 pandemic starting from March 2020 led to corresponding reductions in the cirrus PLDR in the spring, summer, and autumn of 2020, but a slight increase in the winter of 2020 (including December 2019) <xref ref-type="bibr" rid="bib1.bibx38" id="paren.57"/>. The calculated correlation coefficients between both parameters are all positive, but the confidence levels are above 95 % only for summer and autumn. We also calculate the correlation coefficients excluding the COVID-19 period, i.e. for winter from 2010 to 2020 and for other seasons from 2010 to 2019, showing the confidence levels above 95 % only for autumn. Finally, we perform the same calculations of correlation coefficients on the monthly PLDR and corresponding CO<inline-formula><mml:math id="M232" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation in different seasons excluding the COVID-19 period and the results along with the corresponding <inline-formula><mml:math id="M233" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values at the 95 % confidence level are listed in Table <xref ref-type="table" rid="Ch1.T5"/>.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e3739">Motivated by the work of <xref ref-type="bibr" rid="bib1.bibx38" id="text.58"/>, who presented the changes in cirrus cloud properties and occurrence caused by the reduced air traffic during the COVID-19 pandemic, we carry out in the current study further analyses of 10-year lidar measurements of cirrus clouds with CALIPSO before the COVID-19 outbreak. Over this period, aviation grew strongly in terms of CO<inline-formula><mml:math id="M234" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions and flight densities in Europe, especially from 2013 to early 2020.</p>
      <p id="d1e3754">The results show that cirrus clouds follow a distinct seasonal cycle in their appearance including occurrence rate (OR) and occurrence height (OH) as well as in the particle linear depolarization ratio (PLDR). Cirrus clouds in the winter months occurred within a broader altitude range from 6 to 13 km than in summer (only from 9 to 12.5 km) and their OR in winter can be more than 10 times larger than that in summer. Further, the seasonal cycles in cirrus OR are recognized along the entire altitudes where cirrus clouds form and it seems that they are more remarkable in the lower altitudes. The PLDR values of cirrus clouds show the majority of the data falling within the range from 0.2 to 0.55. Cirrus clouds are characterized by larger values of PLDR in winter than in summer. In addition, the PLDR values show generally a clear increase along the altitudes in each month, which is consistent with previous studies <xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx38" id="paren.59"><named-content content-type="pre">e.g.</named-content></xref>.</p>
      <p id="d1e3762">The medians of PLDR in each month were first calculated from the measurements from 2010 to 2020 and they show a significant reduction during the COVID-19 pandemic starting from March 2020 which are presumed to be caused by the reduced air traffic <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx76" id="paren.60"/>. The long-term evolution of the cirrus PLDR before COVID-19 shows an increasing trend with a slope of 1.02 <inline-formula><mml:math id="M235" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M236" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M237" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (1.51 <inline-formula><mml:math id="M238" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M239" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M240" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) in the period from March 2010 to February 2020 (from March 2013 to February 2020) based on the calculation with the Theil–Sen Estimator (TSE) method. The derived trends are both above the 95 % confidence level according to the Mann–Kendall (MK) significance test. The long-term trend of PLDR (a slope of 1.09 <inline-formula><mml:math id="M241" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M242" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M243" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) was also derived from the daytime observations showing a slightly larger value than the result determined from both day- and night-time observations. Since the cirrus cloud occurrence and PLDR are dominated by seasonal cycles, we further deseasonalized the time series of monthly medians of PLDR. The deseasonalized PLDR values show a long-term trend of 0.67 <inline-formula><mml:math id="M244" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M245" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M246" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (with TSE) at the 99.5 % confidence level. The cirrus ORs as well as the deseasonalized values, however, both show a small negative trend over this period, which is presumed to be connected with the background meteorological conditions. Furthermore, there are strong increasing trends in the cirrus occurrence heights as well as in their deseasonalized values, which is very striking since the findings correspond to the upward shift of the aircraft cruising altitudes in the last years.</p>
      <p id="d1e3894">To study the potential reasons for the trends detected in cirrus clouds, we first compare the relationship between the cirrus PLDR and the corresponding ambient temperatures from all the data, which show a negative correlation at temperatures below <inline-formula><mml:math id="M247" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>50 <inline-formula><mml:math id="M248" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and no clear correlation above that. For the monthly medians, however, a significant linear correlation was reached between both parameters with a correlation coefficient of <inline-formula><mml:math id="M249" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>0.76. We hence regressed PLDR with a simple linear regression model because of the strong dependence of PLDR on the ambient temperatures and removed the temperature-induced contributions from the cirrus PLDR. The derived residuals reveal an increasing trend of 0.54 <inline-formula><mml:math id="M250" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M251" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M252" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> above the 90 % confidence level according to the MK test, which should be induced by other factors than temperatures. Before we carry out the comparison between the cirrus PLDR and the corresponding aviation, we should first deseasonalize both datasets since they follow totally different seasonal cycles (roughly anticorrelated). In general, there is a conspicuous increasing trend in the deseasonalized time series of PLDR as well as the corresponding CO<inline-formula><mml:math id="M253" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation, especially in the period from January 2013 to February 2020. The close correlation between them shows a correlation coefficient of 0.25 (0.58) in the full period from January 2010 to February 2020 (from January 2013 to February 2020), which are above the 99.5 % confidence level. We further compared the relationship between the cirrus PLDR and the corresponding CO<inline-formula><mml:math id="M254" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from aviation in different seasons. Concentrating on the data before the COVID-19 outbreak, we calculated the correlation coefficients between both parameters based on their monthly values in different seasons and found a strong correlation in winter, spring, and autumn, but a weak correlation in summer.</p>
</sec>

      
      </body>
    <back><app-group>

<app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title>Ordinary least squares (OLS) estimator and Theil–Sen estimator (TSE)</title>
      <p id="d1e3981">The OLS estimator is a common technique for estimating coefficients of linear regression equations which describe the relationship between one or more independent quantitative variables and a dependent variable (simple or multiple linear regression). The OLS estimator chooses the coefficients by minimizing the sum of the squares of the differences between the observed dependent variables and the predicted values by a linear regression function of the independent variable. The OLS estimator is highly biased by the outliers in the time series. The presence of outliers shifts the distribution of errors away from a normal distribution resulting in heavy tails due to greater standard error than expected.</p>
      <p id="d1e3984">The TSE (or Theil–Sen regression or Sen tau method) is a nonparametric estimation technique for estimating a linear trend (i.e. only for one-variable regression), which uses median instead of mean. Hence, this estimator is not sensitive to outliers. The idea behind the estimator is simple. The slopes <inline-formula><mml:math id="M255" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> between all pairwise sets of observations are computed and the medians of all these slopes are chosen as the estimate of the regression slope.</p>
      <p id="d1e3994">The simple linear regression model based on the observations (<inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) is <inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">β</mml:mi><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, 2, …, <inline-formula><mml:math id="M259" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>, where <inline-formula><mml:math id="M260" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> is the dependent variable, <inline-formula><mml:math id="M261" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> is the independent variable, <inline-formula><mml:math id="M262" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M263" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula> are intercept and slope parameters, respectively, and <inline-formula><mml:math id="M264" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula> is the error term. The Theil–Sen slope estimate is obtained by taking the median of all
          <disp-formula id="App1.Ch1.S1.E5" content-type="numbered"><label>A1</label><mml:math id="M265" display="block"><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>≤</mml:mo><mml:mi>i</mml:mi><mml:mo>≤</mml:mo><mml:mi>j</mml:mi><mml:mo>≤</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:math></inline-formula>. The intercept <inline-formula><mml:math id="M267" display="inline"><mml:mi>b</mml:mi></mml:math></inline-formula> is obtained by taking the median of all the differences (<inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>s</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>).</p>
</app>

<app id="App1.Ch1.S2">
  <?xmltex \currentcnt{B}?><label>Appendix B</label><title>Mann–Kendall test</title>
      <p id="d1e4206">The Mann-Kendall (MK) trend test <xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx31" id="paren.61"/> is a nonparametric test (i.e. no underlying assumption made about the distribution of the data) widely used to statistically assess whether there is a monotonic increasing or decreasing trend in a time series of climatologic and hydrologic data, even if there is a seasonal component in the time series. The null hypothesis, H0, states that the data are independently distributed with no trend. The alternative hypothesis, H1, is that the data follow a monotonic trend. According to the test, each data value of the time series with <inline-formula><mml:math id="M269" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> data points is compared with all subsequent data values. The statistic <inline-formula><mml:math id="M270" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is incremented by 1, if a data value from a later time period is higher than a data value sampled earlier, otherwise <inline-formula><mml:math id="M271" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is decremented by 1; i.e. the MK test statistic <inline-formula><mml:math id="M272" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is calculated by
          <disp-formula id="App1.Ch1.S2.E6" content-type="numbered"><label>B1</label><mml:math id="M273" display="block"><mml:mrow><mml:mi>S</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:mrow><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:munderover><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><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:mi mathvariant="normal">sign</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M274" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M275" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the values of sequence <inline-formula><mml:math id="M276" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M277" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>; <inline-formula><mml:math id="M278" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the length of the time series and
          <disp-formula id="App1.Ch1.S2.E7" content-type="numbered"><label>B2</label><mml:math id="M279" display="block"><mml:mrow><mml:mi mathvariant="normal">sign</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced close="" open="{"><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if  </mml:mtext><mml:mi>x</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if  </mml:mtext><mml:mi>x</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if  </mml:mtext><mml:mi>x</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></disp-formula>
        <xref ref-type="bibr" rid="bib1.bibx42" id="text.62"/> and <xref ref-type="bibr" rid="bib1.bibx31" id="text.63"/> have documented that the statistic <inline-formula><mml:math id="M280" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is approximately normally distributed when <inline-formula><mml:math id="M281" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula>. The mean of <inline-formula><mml:math id="M282" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is <inline-formula><mml:math id="M283" display="inline"><mml:mrow><mml:mi>E</mml:mi><mml:mo>(</mml:mo><mml:mi>S</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> and the variance <inline-formula><mml:math id="M284" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of <inline-formula><mml:math id="M285" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is defined by
          <disp-formula id="App1.Ch1.S2.E8" content-type="numbered"><label>B3</label><mml:math id="M286" display="block"><mml:mrow><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>n</mml:mi><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>n</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>m</mml:mi></mml:msubsup><mml:msub><mml:mi>T</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi>T</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">5</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mn mathvariant="normal">18</mml:mn></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
        where <inline-formula><mml:math id="M287" display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula> is the number of the groups of tied ranks and <inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the number of data points in the <inline-formula><mml:math id="M289" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula>th tied group. The standardized test statistic <inline-formula><mml:math id="M290" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is computed by
          <disp-formula id="App1.Ch1.S2.E9" content-type="numbered"><label>B4</label><mml:math id="M291" display="block"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="array" columnalign="left left"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi>S</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi mathvariant="italic">σ</mml:mi></mml:mfrac></mml:mstyle></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if  </mml:mtext><mml:mi>S</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if  </mml:mtext><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="false"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi>S</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi mathvariant="italic">σ</mml:mi></mml:mfrac></mml:mstyle></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if  </mml:mtext><mml:mi>S</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e4707">A positive (negative) value of the statistic <inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> indicates that the data show an increase (decrease) with time. Given a significance level <inline-formula><mml:math id="M293" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, the null hypothesis is rejected (i.e. there is a statistically significant trend in the time series) if the absolute value of <inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is larger than the theoretical value <inline-formula><mml:math id="M295" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (for two-tailed test) or <inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (for one-tailed test), indicating that a significant trend exists in the time series. Here <inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> denotes the <inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mn mathvariant="normal">100</mml:mn><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>)th percentile of the standard normal distribution and can be obtained from the standard normal <inline-formula><mml:math id="M299" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> table. In this study a confidence level <inline-formula><mml:math id="M300" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> is used. At the significance level <inline-formula><mml:math id="M301" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> %, the null hypothesis is rejected if <inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:mo>|</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">MK</mml:mi></mml:msub><mml:mo>|</mml:mo><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.96</mml:mn></mml:mrow></mml:math></inline-formula>.</p>
</app>
  </app-group><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e4874">Data description and example codes for handling the VFM data are available at <uri>https://www-calipso.larc.nasa.gov/resources/calipso_users_guide/data_summaries/vfm/</uri> (last access: 27 September 2021, <xref ref-type="bibr" rid="bib1.bibx45" id="altparen.64"/>). The MATLAB codes for drawing the plots in this paper can be made available upon request.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e4886">The CALIPSO data, including VFM used in this study, can be obtained via <uri>https://subset.larc.nasa.gov/calipso/login.php</uri> (last access: 27 September 2021, login required, <xref ref-type="bibr" rid="bib1.bibx46" id="altparen.65"/>). ECMWF ERA5 data can be freely accessed from <uri>https://www.ecmwf.int/en/forecasts/datasets/reanalysis-datasets/era5</uri> (last access: 13 December 2022, <xref ref-type="bibr" rid="bib1.bibx22" id="altparen.66"/>). The reanalysed data of cirrus parameters can be made available upon request.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e4904">QL collected and analysed the data and wrote the manuscript with help from SG. Both authors discussed the results and findings and contributed to finalizing the manuscript.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e4910">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e4916">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e4922">We thank the NASA Langley Research Center Atmospheric Science Data Center (ASDC) and CALIPSO science team for making the data available for research. Furthermore, we acknowledge ECMWF for providing the ERA5 data from the Copernicus Climate Change Service (C3S) Climate Data Store.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e4927">This research has been supported by the DLR internal funding within the MABAK project.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>The article processing charges for this open-access <?xmltex \notforhtml{\newline}?>publication were covered by the German Aerospace Center (DLR).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e4938">This paper was edited by Matthias Tesche and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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