<?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>Paul J. Wallace</dc:contributor>
  <dc:contributor>Matthew W. Loewen</dc:contributor>
  <dc:contributor>Don Swanson</dc:contributor>
  <dc:contributor>Adam J R Kent</dc:contributor>
  <dc:creator>Robin M Tuohy</dc:creator>
  <dc:date>2016</dc:date>
  <dc:description>&lt;div class="abstract svAbstract " data-etype="ab"&gt;
&lt;p id="sp0005"&gt;Concentrations of H&lt;sub&gt;2&lt;/sub&gt;O and CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;in olivine-hosted melt inclusions can be used to estimate crystallization depths for the olivine host. However, the original dissolved CO&lt;sub&gt;2&lt;/sub&gt;concentration of melt inclusions at the time of trapping can be difficult to measure directly because in many cases substantial CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;is transferred to shrinkage bubbles that form during post-entrapment cooling and crystallization. To investigate this problem, we heated olivine from the 1959 Kīlauea Iki and 1960 Kapoho (Hawai&amp;lsquo;i) eruptions in a 1-atm furnace to temperatures above the melt inclusion trapping temperature to redissolve the CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;in shrinkage bubbles. The measured CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;concentrations of the experimentally rehomogenized inclusions (⩽590 ppm for Kīlauea Iki [n=10]; ⩽880 ppm for Kapoho, with one inclusion at 1863 ppm [n=38]) overlap with values for naturally quenched inclusions from the same samples, but experimentally rehomogenized inclusions have higher within-sample median CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;values than naturally quenched inclusions, indicating at least partial dissolution of CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;from the vapor bubble during heating. Comparison of our data with predictions from modeling of vapor bubble formation and published Raman data on the density of CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;in the vapor bubbles suggests that 55-85% of the dissolved CO&lt;sub&gt;2&lt;/sub&gt;&amp;nbsp;in the melt inclusions at the time of trapping was lost to post-entrapment shrinkage bubbles. Our results combined with the Raman data demonstrate that olivine from the early part of the Kīlauea Iki eruption crystallized at &amp;lt;6 km depth, with the majority of olivine in the 1-3 km depth range. These depths are consistent with the interpretation that the Kīlauea Iki magma was supplied from Kīlauea&amp;rsquo;s summit magma reservoir (&amp;sim;2-5 km depth). In contrast, olivine from Kapoho, which was the rift zone extension of the Kīlauea Iki eruption, crystallized over a much wider range of depths (&amp;sim;1-16 km). The wider depth range requires magma transport during the Kapoho eruption from deep beneath the summit region and/or from deep beneath Kīlauea&amp;rsquo;s east rift zone. The deeply derived olivine crystals and their host magma mixed with stored, more evolved magma in the rift zone, and the mixture was later erupted at Kapoho.&lt;/p&gt;
&lt;/div&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1016/j.gca.2016.04.020</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Geochemical Society</dc:publisher>
  <dc:title>Magma transport and olivine crystallization depths in Kīlauea’s East Rift Zone inferred from experimentally rehomogenized melt inclusions</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>