<?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>S.V. Rasskazov</dc:contributor>
  <dc:contributor>I.S. Brandt</dc:contributor>
  <dc:contributor>A.V. Ivanov</dc:contributor>
  <dc:contributor>Michael J. Kunk</dc:contributor>
  <dc:creator>Stephen B. Brandt</dc:creator>
  <dc:date>1997</dc:date>
  <dc:description>&lt;p&gt;&lt;span&gt;Results of two routine&amp;nbsp;&lt;/span&gt;&lt;sup&gt;40&lt;/sup&gt;&lt;span&gt;Ar/&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar stepwise heating experiments on a biotite and a basanite are interpreted in terms of Fick's and Arrhenius' laws. Both patterns represent a saddle-shaped&amp;nbsp;&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar release. Argon isotope spectra are suggested to be controlled by the activation energy of diffusion&amp;nbsp;&lt;/span&gt;&lt;i&gt;E&lt;/i&gt;&lt;span&gt;&amp;nbsp;and the frequency factor&amp;nbsp;&lt;/span&gt;&lt;i&gt;D&lt;sub&gt;o&lt;/sub&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;&lt;/i&gt;&lt;span&gt;. The activation energy of&amp;nbsp;&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar is lower than the one of&amp;nbsp;&lt;/span&gt;&lt;sup&gt;40&lt;/sup&gt;&lt;span&gt;Ar. This results in a preferable release of&amp;nbsp;&lt;/span&gt;&lt;sup&gt;40&lt;/sup&gt;&lt;span&gt;Ar relatively to&amp;nbsp;&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar at high-temperature steps and an increasing high-temperature wing in the saddle-shaped age spectrum. At low temperatures, considerable losses and irregularities in release of mainly&amp;nbsp;&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar are observed, which cause the decreasing low-temperature wing in the “saddle”. The suggestion of argon losses (mainly of&amp;nbsp;&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar) from a loose, “unstable” zone of the mineral structures becomes justified. The&amp;nbsp;&lt;/span&gt;&lt;i&gt;n&lt;/i&gt;&lt;span&gt;-irradiation of the samples and the shift of&amp;nbsp;&lt;/span&gt;&lt;i&gt;E&lt;/i&gt;&lt;span&gt;&amp;nbsp;of&amp;nbsp;&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar towards lower values seems to explain the saddle-shaped age-spectra often encountered in&amp;nbsp;&lt;/span&gt;&lt;sup&gt;40&lt;/sup&gt;&lt;span&gt;Ar/&lt;/span&gt;&lt;sup&gt;39&lt;/sup&gt;&lt;span&gt;Ar-geochronometry.&lt;/span&gt;&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1080/10256019708234052</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Taylor &amp; Francis</dc:publisher>
  <dc:title>The inverse problem of argon diffusion from minerals: Determination of kinetic parameters from stepwise-heating experiments</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>