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<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics</journal_title>
		<journal_url>www.atmos-chem-phys.net</journal_url>
		<issn>1680-7316</issn>
		<eissn>1680-7324</eissn>
		<volume_number>7</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2007</publication_year>
	</journal>
	<doi>10.5194/acp-7-495-2007</doi>
	<article_url>http://www.atmos-chem-phys.net/7/495/2007/</article_url>
	<abstract_html>http://www.atmos-chem-phys.net/7/495/2007/acp-7-495-2007.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys.net/7/495/2007/acp-7-495-2007.pdf</fulltext_pdf>
	<start_page>495</start_page>
	<end_page>509</end_page>
	<publication_date>2007-01-26</publication_date>
	<article_title content_type="html">Investigations of the photochemical isotope equilibrium between O&lt;sub&gt;2&lt;/sub&gt;, CO&lt;sub&gt;2&lt;/sub&gt; and O&lt;sub&gt;3&lt;/sub&gt;</article_title>
	<authors>
		<author numeration="1" affiliations="1,2">
			<name>R. Shaheen</name>
			<email>robina.shaheen@mpi-hd.mpg.de</email>
		</author>
		<author numeration="2" affiliations="1,3">
			<name>C. Janssen</name>
		</author>
		<author numeration="3" affiliations="1,4">
			<name>T. Röckmann</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Max-Planck-Institute for Nuclear Physics, Division of Atmospheric Physics, 69117 Heidelberg, Germany</affiliation>
		<affiliation numeration="2" content_type="html">University of California San Diego, Department of Chemistry, La Jolla, USA</affiliation>
		<affiliation numeration="3" content_type="html">Laboratoire de Physique Moléculaire pour l&apos;Atmosphère et l&apos;Astrophysique, Université Pierre et Marie Curie/CNRS, 75252 Paris, France</affiliation>
		<affiliation numeration="4" content_type="html">Institute for  Marine and Atmospheric Research Utrecht, Utrecht University, The Netherlands</affiliation>
	</affiliations>
	<abstract content_type="html">Contrary to tropospheric CO&lt;sub&gt;2&lt;/sub&gt; whose oxygen isotopic composition follows a
standard mass dependent relationship, i.e. &amp;delta;&lt;sup&gt;17&lt;/sup&gt;O~0.5&amp;delta;&lt;sup&gt;18&lt;/sup&gt;O, 
stratospheric CO&lt;sub&gt;2&lt;/sub&gt; is preferentially enriched in &lt;sup&gt;17&lt;/sup&gt;O,
leading to a strikingly different relation: &amp;delta;&lt;sup&gt;17&lt;/sup&gt;O~1.7&amp;delta;&lt;sup&gt;18&lt;/sup&gt;O. It has 
been shown repeatedly that the isotope anomaly is
inherited from O&lt;sub&gt;3&lt;/sub&gt; via photolytically produced O(&lt;sup&gt;1&lt;/sup&gt;D) that undergoes
isotope exchange with CO&lt;sub&gt;2&lt;/sub&gt; and the anomaly may well serve as a tracer of
stratospheric chemistry if details of the exchange mechanism are understood.
We have studied the photochemical isotope equilibrium in UV-irradiated
O&lt;sub&gt;2&lt;/sub&gt;-CO&lt;sub&gt;2&lt;/sub&gt; and O&lt;sub&gt;3&lt;/sub&gt;-CO&lt;sub&gt;2&lt;/sub&gt; mixtures to quantify the transfer of
the anomaly from O&lt;sub&gt;3&lt;/sub&gt; to CO&lt;sub&gt;2&lt;/sub&gt; at room temperature. By following the
time evolution of the oxygen isotopic compositions of CO&lt;sub&gt;2&lt;/sub&gt; and O&lt;sub&gt;2&lt;/sub&gt; under
varying initial isotopic compositions of both, O&lt;sub&gt;2&lt;/sub&gt;/O&lt;sub&gt;3&lt;/sub&gt; and CO&lt;sub&gt;2&lt;/sub&gt;, the
isotope equilibria between the two reservoirs were determined. A very strong
dependence of the isotope equilibrium on the O&lt;sub&gt;2&lt;/sub&gt;/CO&lt;sub&gt;2&lt;/sub&gt;-ratio was
established. Equilibrium enrichments of &lt;sup&gt;17&lt;/sup&gt;O and &lt;sup&gt;18&lt;/sup&gt;O in CO&lt;sub&gt;2&lt;/sub&gt; relative to
O&lt;sub&gt;2&lt;/sub&gt; diminish with increasing CO&lt;sub&gt;2&lt;/sub&gt; content, and this reduction in the
equilibrium enrichments does not follow a standard mass dependent relation.
When molecular oxygen exceeds the amount of CO&lt;sub&gt;2&lt;/sub&gt; by a factor of about 20,
&lt;sup&gt;17&lt;/sup&gt;O and &lt;sup&gt;18&lt;/sup&gt;O in equilibrated CO&lt;sub&gt;2&lt;/sub&gt; are enriched by (142&amp;plusmn;4)&amp;permil;
and (146&amp;plusmn;4)&amp;permil;, respectively, at room temperature and at a
pressure of 225 hPa, independent of the initial isotopic
compositions of CO&lt;sub&gt;2&lt;/sub&gt; and O&lt;sub&gt;2&lt;/sub&gt; or O&lt;sub&gt;3&lt;/sub&gt;. From these findings we derive
a simple and general relation between the starting isotopic compositions and
amounts of O&lt;sub&gt;2&lt;/sub&gt; and CO&lt;sub&gt;2&lt;/sub&gt; and the observed slope in a three oxygen
isotope diagram. Predictions from this relation are compared with published
laboratory and atmospheric data.</abstract>
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</article>

