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<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>William L. Ellsworth</dc:contributor>
  <dc:contributor>Justin L. Rubinstein</dc:contributor>
  <dc:creator>Fred F. Pollitz</dc:creator>
  <dc:date>2015</dc:date>
  <dc:description>&lt;p&gt;&lt;span&gt;A series of near-surface chemical explosions conducted at the San Andreas Fault Observatory at Depth (SAFOD) were recorded by high-frequency downhole receiver arrays in separate experiments in November 2003 and May 2005. The 2003 experiment involved &amp;sim;100&amp;thinsp;&amp;thinsp;kg shots detonated along a 46-km-long line (Hole&amp;ndash;Ryberg line) centered on SAFOD and recorded by 32 three-component geophones in the pilot hole between 0.8 and 2.0&amp;nbsp;km depth. The 2005 experiment involved &amp;sim;36&amp;thinsp;&amp;thinsp;kg shots detonated at Parkfield Area Seismic Observatory (PASO) stations (at &amp;sim;1&amp;ndash;8&amp;thinsp;&amp;thinsp;km offset) recorded by 80 three-component geophones in the main hole between the surface and 2.4&amp;nbsp;km depth. These data sample the downgoing seismic wavefield and constrain the shallow velocity and attenuation structure, as well as the first-order characteristics of the source. Using forward modeling on a velocity structure designed for the near field, both observed&amp;nbsp;&lt;/span&gt;&lt;i&gt;P&lt;/i&gt;&lt;span&gt;- and&amp;nbsp;&lt;/span&gt;&lt;i&gt;S&lt;/i&gt;&lt;span&gt;-wave energy for the PASO shots are identified with the travel times expected for direct and/or reflected phases. Larger-offset recordings from shots along the Hole&amp;ndash;Ryberg line reveal substantial&amp;nbsp;&lt;/span&gt;&lt;i&gt;SV&lt;/i&gt;&lt;span&gt;&amp;nbsp;and&amp;nbsp;&lt;/span&gt;&lt;i&gt;SH&lt;/i&gt;&lt;span&gt;&amp;nbsp;energy, especially southwest of SAFOD from the source as indicated by&amp;nbsp;&lt;/span&gt;&lt;i&gt;P&lt;/i&gt;&lt;span&gt;-to-&lt;/span&gt;&lt;i&gt;S&lt;/i&gt;&lt;span&gt;&amp;nbsp;amplitude ratios. The generated&amp;nbsp;&lt;/span&gt;&lt;i&gt;SV&lt;/i&gt;&lt;span&gt;&amp;nbsp;energy is interpreted to arise chiefly from&amp;nbsp;&lt;/span&gt;&lt;i&gt;P&lt;/i&gt;&lt;span&gt;-to-&lt;/span&gt;&lt;i&gt;S&lt;/i&gt;&lt;span&gt;&amp;nbsp;conversions at subhorizontal discontinuities. This provides a simple mechanism for often-observed low&amp;nbsp;&lt;/span&gt;&lt;i&gt;P&lt;/i&gt;&lt;span&gt;-to-&lt;/span&gt;&lt;i&gt;S&lt;/i&gt;&lt;span&gt;&amp;nbsp;amplitude ratios from nuclear explosions in the far field, as originating from strong near-field wave conversions.&lt;/span&gt;&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1785/0120140242</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Seismological Society of Amercia</dc:publisher>
  <dc:title>Interpretation of &lt;i&gt;S&lt;/i&gt; waves generated by near-surface chemical explosions at SAFOD</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>