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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>9</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2009</publication_year>
	</journal>
	<doi>10.5194/acpd-9-6597-2009</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/9/6597/2009/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/9/6597/2009/acpd-9-6597-2009.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/9/6597/2009/acpd-9-6597-2009.pdf</fulltext_pdf>
	<start_page>6597</start_page>
	<end_page>6615</end_page>
	<publication_date>2009-03-10</publication_date>
	<article_title content_type="html">Spatio-temporal observations of tertiary ozone maximum</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>V. F. Sofieva</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>E. Kyrölä</name>
		</author>
		<author numeration="3" affiliations="1">
			<name>P. T. Verronen</name>
		</author>
		<author numeration="4" affiliations="1">
			<name>A. Seppälä</name>
		</author>
		<author numeration="5" affiliations="1">
			<name>J. Tamminen</name>
		</author>
		<author numeration="6" affiliations="2">
			<name>D. R. Marsh</name>
		</author>
		<author numeration="7" affiliations="2">
			<name>A. K. Smith</name>
		</author>
		<author numeration="8" affiliations="3">
			<name>J.-L. Bertaux</name>
		</author>
		<author numeration="9" affiliations="3">
			<name>A. Hauchecorne</name>
		</author>
		<author numeration="10" affiliations="3">
			<name>F. Dalaudier</name>
		</author>
		<author numeration="11" affiliations="4">
			<name>D. Fussen</name>
		</author>
		<author numeration="12" affiliations="4">
			<name>F. Vanhellemont</name>
		</author>
		<author numeration="13" affiliations="5">
			<name>O. Fanton d&apos;Andon</name>
		</author>
		<author numeration="14" affiliations="5">
			<name>G. Barrot</name>
		</author>
		<author numeration="15" affiliations="5">
			<name>M. Guirlet</name>
		</author>
		<author numeration="16" affiliations="6">
			<name>T. Fehr</name>
		</author>
		<author numeration="17" affiliations="6">
			<name>L. Saavedra</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Earth observation, Finnish Meteorological Institute, Helsinki, Finland</affiliation>
		<affiliation numeration="2" content_type="html">Atmospheric Chemistry Division, National Center for Atmospheric Research, Boulder, Colorado, USA</affiliation>
		<affiliation numeration="3" content_type="html">Service d&apos;Aeronomie du CNRS, Verrières-le-Buisson Cedex, France</affiliation>
		<affiliation numeration="4" content_type="html">Institut d&apos;Aeronomie Spatiale de Belgique, Brussels, Belgium</affiliation>
		<affiliation numeration="5" content_type="html">ACRI-ST, France</affiliation>
		<affiliation numeration="6" content_type="html">ESRIN/ESA, Italy</affiliation>
	</affiliations>
	<abstract content_type="html">We present spatio-temporal distributions of tertiary ozone maximum (TOM),
based on GOMOS (Global Ozone Monitoring by Occultation of Stars) ozone
measurements in 2002–2006. The tertiary ozone maximum is typically observed
in the high-latitude winter mesosphere at altitude ~72 km. Although
the explanation for this phenomenon has been found recently – low
concentrations of odd-hydrogen cause the subsequent decrease in odd-oxygen
losses – models have had significant deviations from existing observations
until recently. Good coverage of polar night regions by GOMOS data has
allowed for the first time obtaining spatial and temporal observational
distributions of night-time ozone mixing ratio in the mesosphere.
&lt;br&gt;&lt;br&gt;
The distributions obtained from GOMOS data have specific features, which are
variable from year to year. In particular, due to a long lifetime of ozone
in polar night conditions, the downward transport of polar air by the
meridional circulation is clearly observed in the tertiary ozone maximum
time series. Although the maximum tertiary ozone mixing ratio is achieved
close to the polar night terminator (as predicted by the theory), TOM can be
observed also at very high latitudes, not only in the beginning and at the
end, but also in the middle of winter. We have compared the observational
spatio-temporal distributions of tertiary ozone maximum with that obtained
using WACCM (Whole Atmosphere Community Climate Model) and found that the
specific features are reproduced satisfactorily by the model.
&lt;br&gt;&lt;br&gt;
Since ozone in the mesosphere is very sensitive to HO&lt;sub&gt;x&lt;/sub&gt; concentrations,
energetic particle precipitation can significantly modify the shape of the
ozone profiles. In particular, GOMOS observations have shown that the
tertiary ozone maximum was temporarily destroyed during the January 2005 and
December 2006 solar proton events as a result of the HO&lt;sub&gt;x&lt;/sub&gt; enhancement
from the increased ionization.</abstract>
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</article>

