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<front>
<journal-meta>
<journal-id journal-id-type="publisher">ANGEO</journal-id>
<journal-title-group>
<journal-title>Annales Geophysicae</journal-title>
<abbrev-journal-title abbrev-type="publisher">ANGEO</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Ann. Geophys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1432-0576</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/angeo-31-1205-2013</article-id>
<title-group>
<article-title>On the electron temperature downstream of the solar wind termination shock</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Chashei</surname>
<given-names>I. V.</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>Fahr</surname>
<given-names>H. J.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Lebedev Physical Institute, Leninskii Prospect 53, 117924 Moscow, Russian Federation</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Argelander Institut für Astronomie, Astrophysics Department, University of Bonn, Auf dem Huegel 71, 53121 Bonn, Germany</addr-line>
</aff>
<pub-date pub-type="epub">
<day>09</day>
<month>07</month>
<year>2013</year>
</pub-date>
<volume>31</volume>
<issue>7</issue>
<fpage>1205</fpage>
<lpage>1212</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2013 I. V. Chashei</copyright-statement>
<copyright-year>2013</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://angeo.copernicus.org/articles/31/1205/2013/angeo-31-1205-2013.html">This article is available from https://angeo.copernicus.org/articles/31/1205/2013/angeo-31-1205-2013.html</self-uri>
<self-uri xlink:href="https://angeo.copernicus.org/articles/31/1205/2013/angeo-31-1205-2013.pdf">The full text article is available as a PDF file from https://angeo.copernicus.org/articles/31/1205/2013/angeo-31-1205-2013.pdf</self-uri>
<abstract>
<p>In this paper we study the temperatures of electrons convected with the
solar wind to large solar distances and finally transported over the solar
wind termination shock. Nearly nothing, unless at high energies in the
cosmic ray regime, is known about the thermodynamical behaviour of these
distant electrons from in~situ plasma observations. Hence it is tacitly
assumed these electrons, due to their adiabatic behaviour and vanishing heat
conduction or energization processes, have rapidly cooled off to very low
temperatures once they eventually arrive at the solar wind termination
shock (at about 100 AU). In this paper we show that such electrons, however,
at their passage over the termination shock due to the shock–electric field
action undergo an over-adiabatic heating and therefore appear on the
downstream side as a substantially heated plasma species. Looking
quantitatively into this heating process we find that solar wind electrons
achieve temperatures of the order of 2–4 &amp;times;  10&lt;sup&gt;6&lt;/sup&gt; K downstream of the
termination shock, depending on the upstream solar wind bulk velocity and
the shock compression ratio. Hence these electrons therewith play an
important dynamical role in structuring this shock and determining the
downstream plasma flow properties. Furthermore, they present an additional
ionization source for incoming neutral interstellar hydrogen and excite
X-ray emission. They also behave similar to cosmic ray electrons and extend
to some limited region upstream of the shock of the order of 0.1 AU by
spatial diffusion and thereby also modify the upstream solar wind
properties.</p>
</abstract>
<counts><page-count count="8"/></counts>
</article-meta>
</front>
<body/>
<back>
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</article>