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<front>
<journal-meta>
<journal-id journal-id-type="publisher">ACPD</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACPD</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7375</issn>
<publisher><publisher-name>Copernicus GmbH</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/acpd-10-28151-2010</article-id>
<title-group>
<article-title>A new method for retrieval of the extinction coefficient of water clouds by using the tail of the CALIOP signal</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Li</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hu</surname>
<given-names>Y.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Huang</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Stamnes</surname>
<given-names>K.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yi</surname>
<given-names>Y.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Key Laboratory for Semi-Arid Climate Change of the Ministry of Education College of Atmospheric Sciences, Lanzhou University, Lanzhou, 730000, China</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Dept. of Physics and Engineering, Stevens Institute of Tech., Hoboken, NJ, USA</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Climate Science Branch, NASA Langley Research Center, Hampton, VA, USA</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>Science Systems and Applications Inc., Hampton, VA 23666, USA</addr-line>
</aff>
<pub-date pub-type="epub">
<day>17</day>
<month>11</month>
<year>2010</year>
</pub-date>
<volume>10</volume>
<issue>11</issue>
<fpage>28151</fpage>
<lpage>28181</lpage>
<permissions>
<license xlink:type="simple">
<license-p>This is an open-access article ditributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.</license-p>
</license>
</permissions>
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<self-uri xlink:href="http://www.atmos-chem-phys-discuss.net/10/28151/2010/acpd-10-28151-2010.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys-discuss.net/10/28151/2010/acpd-10-28151-2010.pdf</self-uri>
<abstract>
<p>A method is developed based on Cloud-Aerosol Lidar and Infrared Pathfinder Satellite Observations (CALIPSO) level 1
attenuated backscatter profile data for deriving the mean extinction coefficient of water droplets close to cloud top.
The method is applicable to low level (cloud top &lt; 2 km), opaque water clouds in which the lidar signal is completely
attenuated beyond about 100 m of penetration into the cloud. The photo multiplier tubes (PMTs) of 532 nm detectors
(parallel and perpendicular polarizations) of Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) both exhibit
 a non-ideal recovery of the lidar signal after striking a strongly backscattering target (such as water cloud or surface).
  Therefore, the effects of any transient responses of CALIOP on the attenuated backscatter profile of the water cloud must first
   be removed in order to obtain a reliable (validated) attenuated backscatter profile. Then, the slope of the exponential decay
   of the validated water cloud attenuated backscatter profile, and the multiple scattering factor are used for deriving the mean
   extinction coefficient of low-level water cloud droplets close to cloud top. This novel method was evaluated and compared with
   the previous method by combining the cloud effective radius (3.7 μm) reported by MODIS with the lidar depolarization ratios
    measured by CALIPSO to estimate the mean extinction coefficient. Statistical results show that the extinction coefficients
    derived by the new method based on CALIOP alone agree reasonably well with those obtained in the previous study using combined
    CALIOP and MODIS data. Their mean absolute relative difference in extinction coefficient is about 13.4%. An important advantage
    of the new method is that it can be used to derive the extinction coefficient also during night time, and it is also applicable
    when multi-layered clouds are present. Overall, the global mean cloud water extinction coefficients during different seasons
    range from 26.17 to 29.46 km&lt;sup&gt;−1&lt;/sup&gt;, and the differences between day and night time all are small (about 1 km&lt;sup&gt;−1&lt;/sup&gt;). However, the
    global mean layer-integrated depolarization ratios of water cloud during different seasons range from 0.2 to 0.23, and the
     differences between day and night also are small, about 0.01.</p>
</abstract>
<counts><page-count count="31"/></counts>
</article-meta>
</front>
<body/>
<back>
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