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<front>
<journal-meta>
<journal-id journal-id-type="publisher">AMTD</journal-id>
<journal-title-group>
<journal-title>Atmospheric Measurement Techniques Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">AMTD</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1867-8610</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/amtd-4-1853-2011</article-id>
<title-group>
<article-title>A sublimation technique for high-precision measurements of &amp;delta;&lt;sup&gt;13&lt;/sup&gt;CO&lt;sub&gt;2&lt;/sub&gt; and mixing ratios of CO&lt;sub&gt;2&lt;/sub&gt; and N&lt;sub&gt;2&lt;/sub&gt;O from air trapped in ice cores</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Schmitt</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>Schneider</surname>
<given-names>R.</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>Fischer</surname>
<given-names>H.</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-group><aff id="aff1">
<label>1</label>
<addr-line>Climate and Environmental Physics, Physics Institute, &amp; Oeschger Centre for Climate Change Research, University of Bern, Sidlerstrasse 5, 3012 Bern, Switzerland</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Alfred Wegener Institute for Polar and Marine Research, Bremerhaven, Germany</addr-line>
</aff>
<pub-date pub-type="epub">
<day>16</day>
<month>03</month>
<year>2011</year>
</pub-date>
<volume>4</volume>
<issue>2</issue>
<fpage>1853</fpage>
<lpage>1892</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-meas-tech-discuss.net/4/1853/2011/amtd-4-1853-2011.pdf">The full text article is available as a PDF file from http://www.atmos-meas-tech-discuss.net/4/1853/2011/amtd-4-1853-2011.pdf</self-uri>
<abstract>
<p>In order to provide high precision stable carbon isotope ratios (&amp;delta;&lt;sup&gt;13&lt;/sup&gt;CO&lt;sub&gt;2&lt;/sub&gt; 
or &amp;delta;&lt;sup&gt;13&lt;/sup&gt;C on CO&lt;sub&gt;2&lt;/sub&gt;) from small bubble and
clathrate ice core samples we developed a new method based on vacuum
sublimation extraction of the CO&lt;sub&gt;2&lt;/sub&gt; and gas chromatography-isotope ratio
mass spectrometry (GC-IRMS). In a first step the trapped air is
quantitatively released from ~30 g of ice and CO&lt;sub&gt;2&lt;/sub&gt; together with
N&lt;sub&gt;2&lt;/sub&gt;O are separated from the bulk air components and stored in a
miniature glass tube. In an off-line step, the extracted sample is
introduced into a helium carrier flow using a minimised tube cracker device.
Prior to measurement, N&lt;sub&gt;2&lt;/sub&gt;O and organic sample contaminants are gas
chromatographically separated from CO&lt;sub&gt;2&lt;/sub&gt;. Pulses of a CO&lt;sub&gt;2&lt;/sub&gt;/N&lt;sub&gt;2&lt;/sub&gt;O
mixture are admitted to the tube cracker and follow the path of the sample
through the system. This allows an identical treatment and comparison of
sample and standard peaks. The ability of the method to reproduce &amp;delta;&lt;sup&gt;13&lt;/sup&gt;C from bubble and clathrate ice is verified on different ice cores.
We achieve reproducibilities for bubble ice between 0.05&amp;permil; and 0.07&amp;permil; and for
clathrate ice between 0.05&amp;permil; and 0.09&amp;permil; (dependent on the ice core used). A
comparison of our data with measurements on bubble ice from the same ice
core but using a mechanic extraction device shows no significant systematic
offset. In addition to &amp;delta;&lt;sup&gt;13&lt;/sup&gt;C, the CO&lt;sub&gt;2&lt;/sub&gt; and N&lt;sub&gt;2&lt;/sub&gt;O mixing
ratios can be volumetrically derived with a precision of 2 ppmv and 8 ppbv,
respectively.</p>
</abstract>
<counts><page-count count="40"/></counts>
</article-meta>
</front>
<body/>
<back>
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