<?xml version='1.0' encoding='utf-8'?>
<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:contributor>C. L. Lichtenberg</dc:contributor>
  <dc:contributor>P. Spudis</dc:contributor>
  <dc:contributor>R. Bonner</dc:contributor>
  <dc:contributor>W. Ort</dc:contributor>
  <dc:contributor>E. Malaret</dc:contributor>
  <dc:contributor>M. Robinson</dc:contributor>
  <dc:contributor>E.M. Shoemaker</dc:contributor>
  <dc:creator>Stewart Nozette</dc:creator>
  <dc:date>1996</dc:date>
  <dc:description>&lt;div id="abstracts"&gt;&lt;div class="core-container"&gt;&lt;div&gt;During the Clementine 1 mission, a bistatic radar experiment measured the magnitude and polarization of the radar echo versus bistatic angle, β, for selected lunar areas. Observations of the lunar south pole yield a same-sense polarization enhancement around β = 0. Analysis shows that the observed enhancement is localized to the permanently shadowed regions of the lunar south pole. Radar observations of periodically solar-illuminated lunar surfaces, including the north pole, yielded no such enhancement. A probable explanation for these differences is the presence of low-loss volume scatterers, such as water ice, in the permanently shadowed region at the south pole.&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1126/science.274.5292.1495</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>American Association for the Advancement of Science</dc:publisher>
  <dc:title>The Clementine bistatic radar experiment</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>