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  <front>
    <journal-meta>
<journal-id journal-id-type="publisher">ACPD</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACPD</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys. Discuss.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7375</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/acpd-15-23969-2015</article-id><title-group><article-title>Equatorial middle atmospheric chemical composition changes during
sudden stratospheric warming events</article-title>
      </title-group><?xmltex \runningtitle{Chemical composition during SSW}?><?xmltex \runningauthor{O. Nath and S.~Sridharan}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Nath</surname><given-names>O.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7116-2494</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Sridharan</surname><given-names>S.</given-names></name>
          <email>susridharan@narl.gov.in</email>
        <ext-link>https://orcid.org/0000-0002-0327-3085</ext-link></contrib>
        <aff id="aff1"><institution>National Atmospheric Research Laboratory, Department of Space, Gadanki 517 112,
India</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">S. Sridharan (susridharan@narl.gov.in)</corresp></author-notes><pub-date><day>4</day><month>September</month><year>2015</year></pub-date>
      
      <volume>15</volume>
      <issue>17</issue>
      <fpage>23969</fpage><lpage>23988</lpage>
      <history>
        <date date-type="received"><day>9</day><month>July</month><year>2015</year></date>
           <date date-type="accepted"><day>11</day><month>August</month><year>2015</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015.html">This article is available from https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015.html</self-uri>
<self-uri xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015.pdf</self-uri>


      <abstract>
    <p>Chemical composition data obtained from the Microwave Limb Sounder (MLS) and
Michelson Interferometer for Passive Atmospheric Sounding (MIPAS)
instruments onboard EOS-Aura and ENVISAT satellites are used to investigate
the variation of ozone (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), water vapor (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>) and methane
(<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) volume mixing ratios (VMRs) in the height range 20–60 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> over the
equatorial region during the sudden stratospheric warmings (SSWs) of 2004,
2009 and 2012, the occurrence of which are identified using the ERA
(European Center for Medium Range Weather Forecasting Reanalysis) Interim
temperature and zonal wind data sets. It is found that the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR shows
increment whereas <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR shows decrement during the SSW event and the
possible reasons for these changes in the VMRs are investigated. In the
upper stratosphere, the source of water vapor is oxidation of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> which
takes place either by hydroxyl (OH) or by atomic oxygen (O). However, the OH
VMR available for the year 2009 SSW event does not show any significant
variation. The decrease of zonal mean MLS temperature over the equator
during the SSW suggests that the rate of the reaction of ozone production
(<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>⟶</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">M</mml:mi></mml:mrow></mml:math></inline-formula>), which increases with decreasing temperature,
shifts the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> ratio towards <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> resulting in the decrease of
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> oxidation and consequent decrease in water vapor.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>Sudden stratospheric warming (SSW) is a high latitude wintertime phenomenon
which is characterized by a sudden enhancement in temperature by several
kelvins at 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> and above, followed by a deceleration and even sometimes,
reversal of the zonal westerly wind to easterly. Scherhag (1952) was the
first who detected a SSW by a radiosounding over Berlin. The SSWs occur in
winter when planetary waves interact with the background flow (Matsuno,
1971). Breaking and dissipation of westward propagating planetary waves at
stratospheric altitudes decelerate or even reverse the prevailing eastward
flow of the polar winter time stratosphere. The SSWs are often accompanied
by either a displacement of the polar vortex toward midlatitudes or an
elongation which results in splitting of the vortex into daughter vortices.
Though the SSW is a high latitude phenomenon, it influences the thermal
structure, circulation and distribution of minor constituents globally.
First observational case studies regarding stratospheric chemical
composition changes during the SSW were performed using in situ (Dutsch and
Braun, 1980) and SAGE I satellite measurements (Wanget et al., 1983). Due to
the availability of several satellite observations in the recent decades,
there have been many reports on chemical composition changes at
high-latitudes during the major SSW of 2004, 2006 and 2009 (Manney et al., 2008a, b, 2009;  Randel et al., 2006, 2009). Using Sounding of Atmosphere by
Broadband Emission radiometry (SABER) on board
Thermosphere-Ionosphere-Mesosphere Energetics and Coupling (TIMED) satellite
data sets, Siskind et al. (2007) observed elevation of stratopause and
a downward mesospheric transport of NO during the 2006 SSW event. Manney et al. (2009) investigated stratospheric chemistry of polar vortex during the
2009 and 2006 SSW events and they observed downward descent of CO, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> from mesosphere during the decay of vortex fragments.
Similarly, Salmi et al. (2011) also reported about the dowward transport of
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mtext mathvariant="italic">x</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula> from mesosphere to upper stratosphere, though the NO<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>
involved catalytic ozone production/depletion cycle was shown to be
ineffective in upper stratosphere. Using Global Ozone Monitoring by
Occultation of Stars (GOMOS) data sets, Sofieva et al. (2012) observed
strong horizontal mixing of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> with outside-vortex air and large
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> enhancement correlating with the temperature enhancment. Damiani
et al. (2014) also investigated a few chemical constituents (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,
ClO<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, HCl, ClO, CO, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mtext mathvariant="italic">x</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> etc.) over polar region for
a few SSW events. They found increment in ozone which could increase ClO and
hence <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">ClONO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> along with a decrease in HCl. In case of methane
(<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), they observed temporal evolution after the SSW events which they
attributed to ingression of mid-latitude air. Using ground based microwave
radiometer observations from 20 to 70 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> over Bern (Switzerland), Flury
et al. (2009) observed decrease of ozone and increase of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> during the
vortex breakdown period due to mixing of humid air from subtropical
mesosphere. Tschanz and Kampfer (2015) also observed increase of water vapor
over Sodankylä, Finland (67.4<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 26.6<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) derived
from the middle atmospheric water vapor radiometer (MIAWARA) measurements.</p>
      <p>There are only few studies over the equatorial region and low-latitudes on
chemical composition changes during the SSW events, although enhancement of
ozone mixing ratio has consistently been observed (Sridharan et al., 2012;
Nath et al., 2015). Sridharan et al. (2012) suggested that the enhancement
of the equatorial and low-latitude ozone during the SSW event could be due
to weakening of Brewer–Dobson circulation (BDC) responsible for transporting
ozone to higher latitudes due to decrease in planetary wave activity. In the
present study, changes in chemical composition in the upper stratosphere
over the equator during a few SSW events are investigated and an attempt is
made to give a feasible chemical interpretation about the observed
variations.</p>
</sec>
<sec id="Ch1.S2">
  <title>Data sets used</title>
<sec id="Ch1.S2.SS1">
  <?xmltex \opttitle{MLS data for the equatorial O${}_{{3}}$,
H${}_{{2}}$O VMR and temperature}?><title>MLS data for the equatorial O<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>,
H<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O VMR and temperature</title>
      <p>The Earth Observing System (EOS) Microwave Limb Sounder (MLS) is one of the
four instruments on the NASA's EOS Aura satellite, which is part of NASA's
A-train group of Earth observing satellites, launched on 15 July 2004
(Manney et al., 2005). The MLS makes measurements of atmospheric
composition, temperature, humidity and cloud ice globally both day and
night. It observes thermal microwave emission from Earth's “limb” (the edge
of the atmosphere) viewing forward along the Aura spacecraft flight
direction, scanning its view from the ground to <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>90</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> every
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>25</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">s</mml:mi></mml:math></inline-formula>. Aura is in a near-polar 705 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> altitude orbit. As
Earth rotates underneath it, the Aura orbit stays fixed relative to the sun
to give daily global coverage with <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>13</mml:mn></mml:mrow></mml:math></inline-formula> orbits per day. MLS is
giving data since August 2004. In this present study we used MLS Version 3
VMR data of ozone (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and temperature (<inline-formula><mml:math display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula>) for 2009 and 2012 SSWs and
water vapor (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>) during the SSWs of 2004, 2009 and 2012 to study their
variation in upper stratosphere. The MLS useful data range for <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR,
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR and <inline-formula><mml:math display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> are as follows for the pressure level range 261–0.02,
316–0.002 and 261–0.001 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> respectively. The data accuracy in the
height range considered for observation is 4–9 %.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <?xmltex \opttitle{MIPAS-ENVISAT data for CH${}_{{4}}$ VMR}?><title>MIPAS-ENVISAT data for CH<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula> VMR</title>
      <p>MIPAS (Michelson Interferometer for Passive Atmospheric Sounding) is
a limb-scanning Fourier infrared spectrometer on board the European
Environmental Satellite (ENVISAT);  more detailed characteristics regarding
the measurements bythis spaceborne instrument are given by Carli et al. (2004) and Raspollini et al. (2006). The sunsynchronous polar orbit provides
a global coverage with nearly 14 orbits per day at a horizontal resolution of
approximately 500 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>. More than 20 trace constituents are observed in the
upper troposphere and in the stratosphere. Currently, the MIPAS level-2
operational products are provided by the European Space Agency (ESA). These
products include the temperature, and the concentrations of
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>,<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">HNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. In its
original nominal measurement mode, MIPAS scanned the Earth limb at 17
tangent altitudes of 6, 9, …, 39, 42, 47, 52, 60, and 68 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>. The vertical
resolution is 3 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> for the 13 lower most tangent altitudes and increases to
8 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> at the upper end of the limb scan. MIPAS <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR data has been
compared with satellite instruments including ACE-FTS, HALOE, SOFIE and
SCIAMACHY (Laeng et al., 2015). Above 50 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> altitude, MIPAS methane mixing
ratios agree almost perfectly with ACE, and above 40–45 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> with SOFIE.
Between 30 and 40 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> excellent agreement with SCIAMACHY has been found. In
the lower stratosphere (below about 25–30 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>) MIPAS <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is biased high,
and the most likely esimate of this bias is 0.2 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula>. MIPAS data are
available for the years 2002–2012. In this study, methane volume mixing
ratio data have been taken from MIPAS-ENVISAT data source for the SSWs
occurred in 2004, 2009 and 2012.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>ECMWF ERA-Interim data for zonal wind and temperature</title>
      <p>ERA-Interim is the latest European Centre for Medium-Range Weather Forecasts
(ECMWF) global atmospheric reanalysis of the period 1979 to present
(Berrisford, 2009). This follows on from the ERA-15 and ERA-40 re-analysis
projects. The datasets include data on surface, PV, potential temperature
and pressure surfaces. The ECMWF has in the past produced three major
reanalyses: FGGE, ERA-15 and ERA-40. The last of these consisted of a set of
global analyses describing the state of the atmosphere and land and
ocean-wave conditions from mid-1957 to mid-2002. The ERA-Interim is an
“interim” reanalysis of the period 1989-present in preparation for the
next-generation extended reanalysis to replace ERA-40.</p>
      <p>In this present study, ERA-Interim data have been used for the observation
of zonal wind as well as temperature (grid <inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mn>1.5</mml:mn><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn>1.5</mml:mn><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>)
variations for the pressure levels 100–1 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> during the SSWs of 2004, 2009
and 2012.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>2011/12 winter and equatorial temperature and ozone</title>
      <p>Figure 1a and b shows the zonal mean of ERA- Interim temperature difference
between 90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and of ERA- Interim zonal wind
at 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N respectively for the pressure levels 100–1 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> and for
the duration 1 December 2011 to 18 February 2012. The SSW is normally
identified from the positive temperature between 90 and
60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N latitudes at 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>. Before day number 43, the temperature
difference is <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 to <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>20 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula>, which means that the temperature at
60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N is more than that at 90<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N indicating that the
normal cold winter is prevailing. A clear sudden enhancement in temperature
can be observed from day number 43 in the height range 10–1 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>. When the
warming starts the temperature difference becomes positive, as the polar
stratospheric temperature is increased by several kelvins. Here the
temperature difference between 90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N rises
upto 16 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula> (on day number 55) and it remains positive during day numbers
43–64, which indicates the duration of the SSW. When the SSW occurs, the
polar westerly wind gets decelerated up to 5 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and as it does not get
reversed to easterly, this event is considered only as a minor SSW. Figure 1c and e show the altitude profiles of MLS zonal mean of ozone (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) VMR
and temperature over the equator for the height region 20–60 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> for the
duration of 1 December 2011 to 18 February 2012. As the onset of SSW takes
place, <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR shows enhancement, whereas temperature and water vapor
decrease in the middle and upper stratosphere from day number 49. Though the
onset of SSW is marked on day number 43 at 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>, it may be noted that the
polar temperature starts to increase from day number 29 at higher heights
(<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn>10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>). Time mean removed zonal mean <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR and
temperature have been plotted in Fig. 1d and Fig. 1f respectively. It can be
observed from the figures that there is an increase in the time mean removed
ozone VMR by about 0.6 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> during day number 29–35, whereas the temperature
decreases by a value <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula> from day number 29.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>2008/09 winter and equatorial temperature and ozone</title>
      <p>Figure 2a and b shows the zonal mean of ERA-Interim temperature difference
between 90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and of ERA-Interim zonal wind at
60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N respectively for the pressure levels 100–1 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> for the time
period 1 December 2008 to 18 February 2009. The temperature
difference is around <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>10 to <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>15 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula> before the day number 52 and it becomes
positive from day number 52 in the height range 10–1 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> indicating the
onset of the SSW event. It reaches a maximum of 25.8 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula> on day number 54 and
the positive temperature difference (the SSW event) persists during the day
numbers 52–57. The zonal mean wind at 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N becomes westward on
day number 55 at and above 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> revealing that the SSW event is a major
one. Figure 2c and e show the altitude profiles of zonal mean of ozone (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>)
VMR and temperature over the equator obtained from MLS for the heights 20–60 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> for the duration of 1 December 2008–18 February 2009. For more clear
interpretation, Fig. 2d and f are plotted which show time mean removed zonal
mean ozone VMR and temperature. Day number 52 onwards, the time mean removed
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR increases, reaches a high value of around 0.8 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> and gradually
reduces after day number 60. The time mean removed temperature decreases
more to a maximum of <inline-formula><mml:math display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>9 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">K</mml:mi></mml:math></inline-formula> during day numbers 50–55. After day number 60, it
starts to become positive again.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Equatorial water vapor and methane during the 2008/09 SSW</title>
      <p>Figure 3a shows zonal mean temperature difference between 90 and
60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N for the pressure levels 10–1 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> for the time period 1 December 2008 to 18 February 2009 for reference. As shown earlier, the major
SSW event occurs during the day numbers 52–57. Figure 3b shows time mean
removed zonal mean <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR over the equator for the height range 20–60 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>. Above 40 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>, day number 35 onwards the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR starts to decrease
by small amount (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula>). As the day of onset approaches,
the time removed <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR decreases by an amount 0.5 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> and it
persists up to day number 62. The source of water vapor in this height
region (upper stratosphere) is oxidation of methane (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) (Dessler,
2000;  Seinfield and Pandis, 2006). For investigating the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> variation
during the time of observation, MIPAS onboard ENVISAT data are being
considered to show the time mean removed zonal mean <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR in Fig. 3c.
Above 3 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>, time removed <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR starts to increase from day number
35, reaches a value around 0.15 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> on day number 53. After day number 70,
the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR slowly reduces.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <title>Equatorial water vapor and methane during the 2011/12 SSW</title>
      <p>In the case of 2011/12 winter, the time mean removed zonal mean <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR are shown in Fig. 4 along with the state of zonal mean
temperature and zonal mean wind as reference. During this winter, a minor
SSW event occurs during the day numbers 43–64. However, SSW begins at higher
heights from day number 29 (Fig. 4a). Above 40 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>, the time mean removed
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR starts to decrease from day number 29 and reaches a value
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>0.48</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> around day number 45. After day number 70, the
value reduces. Time mean removed <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR begins to increase from
a value of 0.018 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> around day number 30 to a value of 0.15 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> around day
number 45. After day number 70, the value reduces. From these two cases, it
is apparent that the minor constituents respond to the temperature
variations above 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> rather than at 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>, which has been traditionally
used to identify the occurrence of SSW. The variations of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are not simply seasonal in nature, as they are quite different in
the two winters and their maximum or minimum VMR coincide with the SSW
event.</p>
</sec>
<sec id="Ch1.S3.SS5">
  <title>Equatorial water vapor and methane during the 2003/04 SSW</title>
      <p>To verify the consistencies of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>VMR variations
observed during the two SSW events of 2009 (major) and 2012 (minor), the
variations of the minor constituents, during the 2004 major SSW event are
also presented. In Fig. 5a zonal mean temperature difference is shown
between 90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N for the duration 1 December 2003–18 February 2004 for the identification of the SSW event. The onset of
the warming can be observed on day number 36 and the event persists up to
day number 44. Figure 5b and c show time mean removed zonal mean <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR over the equator for the same time period. The time mean
removed <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR shows a decrease from day number 32, reaches a value
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>0.7</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> around day number 40 and begins to decrease from
day number 60. The time mean removed <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR is also observed to
increase from day number 30 above 3 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula> and attain a maximum of
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn>0.17</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> on day number 41. Large values of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR
persist until day number 60. In this case study the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMRs
show consistent decrease and increase respectively in association with all
the SSW events considered here.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <title>Discussion and conclusions</title>
      <p>In the present study, changes in the VMRs of ozone (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), water vapor
(<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>) obtained from the MLS and VMR of methane (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) obtained from
MIPAS over the equator during the SSW events of 2004, 2009 and 2012 are
studied. The zonal mean temperature difference between 90 and
60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and zonal wind are used to identify the occurrences of the
SSW events. The ozone and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMRs show enhancement as the onset of SSW
occurs whereas <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR shows a decrease. The observed variation of
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR during the 2009 and 2012 SSW was verified with the
case study of the SSW occured in 2004 which shows similar type of results as
observed in case of 2009 and 2012. In the equatorial stratosphere ozone
production is due to photolysis of molecular oxygen. This ozone get
transported poleward due to BDC (Andrews et al., 1987). During normal time,
the <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentration is more in higher latitudes compared to that over
the equatorial and lower latitudes. During the SSW, the OVMR is found to
increase because of the weakening of BDC due to reduction in planetary wave
activity with the onset of warming. Sridharan et al. (2012) observed
enhancement of ozone during the major SSW of years 2006 and 2009 and
suggested as a reason for the enhancement of mesospheric semi-diurnal tide
which has been consistenly observed during the major SSW. Nath et al. (2015)
also observed increasing OVMR during the 2013 major SSW event. The <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>
VMR decreases in association with the warming at heights greater than 10 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">hPa</mml:mi></mml:math></inline-formula>. In the upper stratosphere, the main source of water vapor is the
oxidation of methane. Oxidation of methane can occur via two ways (Brasseur
and Solomon, 1995):

              <disp-formula specific-use="align"><mml:math display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">O</mml:mi><mml:msup><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:msup><mml:mi mathvariant="normal">D</mml:mi><mml:mo>)</mml:mo><mml:mo>⟶</mml:mo><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">OH</mml:mi></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">OH</mml:mi><mml:mo>⟶</mml:mo><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p>Atomic oxygen (O) production results in from the photolysis of <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>3.</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>

              <disp-formula id="Ch1.Ex3"><mml:math display="block"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mtext mathvariant="italic">h</mml:mtext><mml:mi mathvariant="italic">ν</mml:mi><mml:mo>⟶</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></disp-formula></p>
      <p>O produced in the above reaction can be in one of two electronic states:
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mi mathvariant="normal">P</mml:mi></mml:mrow></mml:math></inline-formula> (“triplet P”) or <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msup><mml:mi mathvariant="normal">D</mml:mi></mml:mrow></mml:math></inline-formula> (“singlet D”). O (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msup><mml:mi mathvariant="normal">D</mml:mi></mml:mrow></mml:math></inline-formula>) is rapidly
converted to O (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mi mathvariant="normal">P</mml:mi></mml:mrow></mml:math></inline-formula>) through collisions with molecules such as <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. So the abundance of more reactive O (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msup><mml:mi mathvariant="normal">D</mml:mi></mml:mrow></mml:math></inline-formula>) is much less
compared to that of less reactive O (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mi mathvariant="normal">P</mml:mi></mml:mrow></mml:math></inline-formula>) in stratosphere (Dessler,
2000). The ozone destruction rate and hence the ozone mixing ratio, are
strongly dependent on the mixing ratio of atomic oxygen O. The O mixing
ratio is determined by the O production (by <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> photolysis, insensitive
to temperature) and O destruction. The oxygen destruction occurs by the
reaction
          <disp-formula id="R1" content-type="numbered reaction"><mml:math display="block"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">M</mml:mi><mml:mo>⟶</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mi mathvariant="normal">M</mml:mi></mml:mrow></mml:math></disp-formula></p>
      <p>The rate of the reaction is <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mi mathvariant="normal">O</mml:mi><mml:msup><mml:mo>]</mml:mo><mml:mo>*</mml:mo></mml:msup><mml:mo>[</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mo>]</mml:mo><mml:mo>*</mml:mo></mml:msup><mml:mo>[</mml:mo><mml:mi mathvariant="normal">M</mml:mi><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:mo>[</mml:mo><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mo>]</mml:mo></mml:mrow></mml:math></inline-formula> sign
stands for concentration) where rate constant <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn>10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn>34</mml:mn></mml:mrow></mml:msup><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mo>(</mml:mo></mml:mrow></mml:math></inline-formula>T<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mn>300</mml:mn><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn>2.3</mml:mn></mml:mrow></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mn mathvariant="normal">6</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">molecules</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. This
three-body reaction is inversely dependent on temperature (Seinfield
and Pandis, 2006). A temperature increase as observed during the SSW
over higher latitudes results in a decrease of the reaction rate
constant of reaction (1) by a factor of approximately 2 which leads to
a significantly higher mixing ratio of atomic oxygen (O) and a smaller
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR (Flury et al., 2009). The decrease of temperature over
the equatorial latitudes during the SSW events probably shifts the
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> partitioning towards <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, resulting in higher
<inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR and lower atomic oxygen abundance. In the present study
variations of hydroxyl (OH) VMR (Fig. 6) over the equator observed by
MLS are shown only for the 2009 SSW event, as the MLS data are not
available for 2004 and 2012 SSW events. The time mean removed OH
VMR
shows a very little insignificant decrease of about
0.0001 <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">ppmv</mml:mi></mml:math></inline-formula> during day numbers 48–60 (Fig. 6b). Hence it can
be concluded that most probably the reduction of atomic oxygen
abundance affects the methane oxidation during the occurrence of SSW
events resulting in the decrease in water vapor mixing ratio.</p>
</sec>

      
      </body>
    <back><ack><title>Acknowledgements</title><p>The authors acknowledge the Aura-MLS team for providing valuable
chemical components datasets and making it available to the scientific
community. They are also thankful to ECMRWF for the temperature and
winds reanalysis data and MIPAS-ENVISAT for the methane volume mixing
ratio data used in the present study.</p></ack><ref-list>
    <title>References</title>

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  </ref-list><app-group content-type="float"><app><title/>

      <fig id="App1.Ch1.F1"><caption><p>Height profile of <bold>(a)</bold> ERA-Interim zonal mean temperature
difference between 90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(b)</bold> ERA-Interim
zonal mean wind at 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, zonal mean Aura-MLS <bold>(c)</bold> <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR, <bold>(e)</bold>
temperature and time mean removed zonal mean <bold>(d)</bold> <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR, <bold>(f)</bold>
temperature during 1 December 2011–18 February 2012. The dotted lines
represent the duration of the warming event.</p></caption>
      <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015-f01.png"/>

    </fig>

      <fig id="App1.Ch1.F2"><caption><p>Height profile of <bold>(a)</bold> ERA-Interim zonal mean temperature
difference between 90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, <bold>(b)</bold> ERA-Interim
zonal mean wind at 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, zonal mean Aura-MLS <bold>(c)</bold> <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR, <bold>(e)</bold>
temperature and time mean removed zonal mean <bold>(d)</bold> <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR, <bold>(f)</bold>
temperature during 1 December 2008–18 February 2009. The dotted lines
represent the duration of the warming event.</p></caption>
      <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015-f02.png"/>

    </fig>

      <fig id="App1.Ch1.F3"><caption><p><bold>(a)</bold> ERA-Interim zonal mean temperature difference between
90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and time mean removed zonal mean <bold>(b)</bold>
Aura-MLS <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR and <bold>(c)</bold> MIPAS-ENVISAT <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR over the equator
during 1 December 2008–18 February 2009.</p></caption>
      <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015-f03.png"/>

    </fig>

      <fig id="App1.Ch1.F4"><caption><p><bold>(a)</bold> ERA-Interim zonal mean temperature difference between
90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and time mean removed zonal mean <bold>(b)</bold>
Aura-MLS <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR and <bold>(c)</bold> MIPAS-ENVISAT <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR over the equator
during 1 December 2011–18 February 2012.</p></caption>
      <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015-f04.png"/>

    </fig>

      <fig id="App1.Ch1.F5"><caption><p><bold>(a)</bold> ERA-Interim zonal mean temperature difference between
90 and 60<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N and time mean removed zonal mean <bold>(b)</bold>
Aura-MLS <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> VMR and <bold>(c)</bold> MIPAS-ENVISAT <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> VMR over the equator
during 1 December 2003–18 February 2004.</p></caption>
      <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015-f05.png"/>

    </fig>

      <fig id="App1.Ch1.F6"><caption><p>Height–time cross section of Aura-MLS <bold>(a)</bold> zonal mean and <bold>(b)</bold> time
mean removed zonal mean OH over the equator for 1 December 2008–18 February 2009.</p></caption>
      <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/preprints/15/23969/2015/acpd-15-23969-2015-f06.png"/>

    </fig>

    </app></app-group></back>
    </article>
