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<article language="en">
	<journal>
		<journal_title>Nonlinear Processes  in Geophysics</journal_title>
		<journal_url>www.nonlin-processes-geophys.net</journal_url>
		<issn>1023-5809</issn>
		<eissn>1607-7946</eissn>
		<volume_number>9</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2002</publication_year>
	</journal>
	<doi>10.5194/npg-9-101-2002</doi>
	<article_url>http://www.nonlin-processes-geophys.net/9/101/2002/</article_url>
	<abstract_html>http://www.nonlin-processes-geophys.net/9/101/2002/npg-9-101-2002.html</abstract_html>
	<fulltext_pdf>http://www.nonlin-processes-geophys.net/9/101/2002/npg-9-101-2002.pdf</fulltext_pdf>
	<start_page>101</start_page>
	<end_page>109</end_page>
	<publication_date>0000-00-00</publication_date>
	<article_title content_type="html">Modeling stretched solitary waves along magnetic field lines</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>L. Muschietti</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>I. Roth</name>
		</author>
		<author numeration="3" affiliations="1">
			<name>C. W. Carlson</name>
		</author>
		<author numeration="4" affiliations="1">
			<name>M. Berthomier</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Space Sciences Laboratory, University of California, Berkeley, USA</affiliation>
	</affiliations>
	<abstract content_type="html">A model is presented
      for a new type of fast solitary waves which is observed in downward
      current regions of the auroral zone. The three-dimensional, coherent
      structures are electrostatic, have a positive potential, and move along
      the magnetic field lines with speeds on the order of the electron drift.
      Their parallel potential profile is flattened and cannot fit to the
      Gaussian shape used in previous work. We develop a detailed BGK model
      which includes a flattened potential and an assumed cylindrical symmetry
      around a centric magnetic field line. The model envisions concentric
      shells of trapped electrons slowly drifting azimuthally while bouncing
      back and forth in the parallel direction. The electron dynamics is
      analysed in terms of three basic motions that occur on different time
      scales characterized by the cyclotron frequency &lt;font face=&quot;Symbol&quot;&gt;W&lt;/font&gt;&lt;sub&gt;e&lt;/sub&gt;
      , the bounce frequency &lt;font face=&quot;Symbol&quot;&gt;w&lt;/font&gt;&lt;sub&gt;b&lt;/sub&gt; , and the
      azimuthal drift frequency &lt;font face=&quot;Symbol&quot;&gt;w&lt;sub&gt;g&lt;/sub&gt;&lt;/font&gt;. The
      ordering &lt;font face=&quot;Symbol&quot;&gt;W&lt;/font&gt;&lt;sub&gt;e&lt;/sub&gt; &amp;gt;&amp;gt; &lt;font face=&quot;Symbol&quot;&gt;w&lt;/font&gt;&lt;sub&gt;b
      &amp;gt;&amp;gt;&lt;/sub&gt; &lt;font face=&quot;Symbol&quot;&gt;w&lt;sub&gt;g&lt;/sub&gt;&lt;/font&gt; is required.
      Self-consistent distribution functions are calculated in terms of
      approximate constants of motion. Constraints on the parameters
      characterizing the amplitude and shape of the stretched solitary wave are
      discussed.</abstract>
	<references>
	</references>
</article>

