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<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics Discussions</journal_title>
		<journal_url>www.atmos-chem-phys-discuss.net</journal_url>
		<issn>1680-7367</issn>
		<eissn>1680-7375</eissn>
		<volume_number>8</volume_number>
		<issue_number>3</issue_number>
		<publication_year>2008</publication_year>
	</journal>
	<doi>10.5194/acpd-8-8881-2008</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/8/8881/2008/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/8/8881/2008/acpd-8-8881-2008.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/8/8881/2008/acpd-8-8881-2008.pdf</fulltext_pdf>
	<start_page>8881</start_page>
	<end_page>8912</end_page>
	<publication_date>2008-05-19</publication_date>
	<article_title content_type="html">Absolute rate constant and O(&lt;sup&gt;3&lt;/sup&gt;P) yield for the O(&lt;sup&gt;1&lt;/sup&gt;D)+N&lt;sub&gt;2&lt;/sub&gt;O reaction in the temperature range 227 K to 719 K</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>S. Vranckx</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>J. Peeters</name>
		</author>
		<author numeration="3" affiliations="1">
			<name>S. A. Carl</name>
			<email>shaun.carl@chem.kuleuven.be</email>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">University of Leuven, Department of Chemistry, 200F Celestijnenlaan, 3001 Leuven, Belgium</affiliation>
	</affiliations>
	<abstract content_type="html">We have determined, in the temperature range 227 K to 719 K, the absolute
rate constant for the reaction O(&lt;sup&gt;1&lt;/sup&gt;D)+N&lt;sub&gt;2&lt;/sub&gt;O &amp;rarr; products and, in
the temperature range 248 K to 600 K, the fraction of the reaction that
yields O(&lt;sup&gt;3&lt;/sup&gt;P). Both the rate constants and product yields were
determined using a recently-developed chemiluminescence technique for
monitoring O(&lt;sup&gt;1&lt;/sup&gt;D) that allows for higher precision determinations for
both rate constants, and, particularly, O(&lt;sup&gt;3&lt;/sup&gt;P) yields, than do other
methods. We found the rate constant, &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;R1&lt;/sub&gt;, to be essentially independent
of temperature between 400 K and 227 K, having a value of
(1.37&amp;plusmn;0.09)&amp;times;10&lt;sup&gt;&amp;minus;10&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. For temperatures greater than 450 K a
marked decrease in value was observed, with a rate constant of only
(0.94&amp;plusmn;0.11)&amp;times;10&lt;sup&gt;&amp;minus;10&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt; at 719 K. The rate constants determined
over the 227 K&amp;ndash;400 K range show very low scatter and are significantly
greater, by 20% at room temperature and by 15% at 227 K, than the
current recommended values. The fraction of O(&lt;sup&gt;3&lt;/sup&gt;P) produced in this
reaction was determined to be 0.002&amp;plusmn;0.002 at 250 K rising steadily to
0.010&amp;plusmn;0.004 at 600 K, thus the channel producing O(&lt;sup&gt;3&lt;/sup&gt;P) can be
entirely neglected in atmospheric kinetic modeling calculations. A further
result of this study is an expression of the relative quantum yields as a
function of temperature for the chemiluminescence reactions (&lt;i&gt;k&lt;/i&gt;&lt;sub&gt;CL1&lt;/sub&gt;) C&lt;sub&gt;2&lt;/sub&gt;H+O(&lt;sup&gt;1&lt;/sup&gt;D) &amp;rarr; CH(A)+CO and (&lt;i&gt;k&lt;/i&gt;&lt;sub&gt;CL2&lt;/sub&gt;) C&lt;sub&gt;2&lt;/sub&gt;H+O(&lt;sup&gt;3&lt;/sup&gt;P) &amp;rarr; CH(A)+CO,
both followed by CH(A) &amp;rarr; CH(X)+hν,
as &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;CL1&lt;/sub&gt;(T)/&lt;i&gt;k&lt;/i&gt;&lt;sub&gt;CL2&lt;/sub&gt;(T)=(32.8&lt;i&gt;T&lt;/i&gt;&amp;minus;3050)/(6.29&lt;i&gt;T&lt;/i&gt;+398).</abstract>
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</article>

