<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "https://jats.nlm.nih.gov/nlm-dtd/publishing/3.0/journalpublishing3.dtd">
<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" dtd-version="3.0" xml:lang="en">
<front>
<journal-meta>
<journal-id journal-id-type="publisher">NPG</journal-id>
<journal-title-group>
<journal-title>Nonlinear Processes in Geophysics</journal-title>
<abbrev-journal-title abbrev-type="publisher">NPG</abbrev-journal-title>
<abbrev-journal-title abbrev-type="nlm-ta">Nonlin. Processes Geophys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1607-7946</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/npg-10-131-2003</article-id>
<title-group>
<article-title>Resonant-to-nonresonant transition in electrostatic ion-cyclotron wave phase velocity</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Carroll III</surname>
<given-names>J. J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Koepke</surname>
<given-names>M. E.</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>Zintl</surname>
<given-names>M. W.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gavrishchaka</surname>
<given-names>V.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Department of Physics, West Virginia University, Morgantown, WV 26506-6315, USA</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>present address: Eastern Michigan University, Ypsilanti, MI 48197, USA</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>present address: SARA, Inc., Huntington Beach, CA 92649, USA</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>Science Applications International Corp., McLean, VA 22102, USA</addr-line>
</aff>
<pub-date pub-type="epub">
<day>30</day>
<month>04</month>
<year>2003</year>
</pub-date>
<volume>10</volume>
<issue>1/2</issue>
<fpage>131</fpage>
<lpage>138</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2003 J. J. Carroll III et al.</copyright-statement>
<copyright-year>2003</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution-NonCommercial-ShareAlike 2.5 Generic License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by-nc-sa/2.5/">https://creativecommons.org/licenses/by-nc-sa/2.5/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://npg.copernicus.org/articles/10/131/2003/npg-10-131-2003.html">This article is available from https://npg.copernicus.org/articles/10/131/2003/npg-10-131-2003.html</self-uri>
<self-uri xlink:href="https://npg.copernicus.org/articles/10/131/2003/npg-10-131-2003.pdf">The full text article is available as a PDF file from https://npg.copernicus.org/articles/10/131/2003/npg-10-131-2003.pdf</self-uri>
<abstract>
<p>Because of the
      implications for plasmas in the laboratory and in space, attention has
      been drawn to inhomogeneous energy-density driven (IEDD) waves that are
      sustained by velocity-shear-induced inhomogeneity in cross-field plasma
      flow. These waves have a frequency &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;r&lt;/sub&gt;
      in the lab frame within an order of magnitude of the ion gyrofrequency &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;ci&lt;/sub&gt;,
      propagate nearly perpendicular to the magnetic field (k&lt;sub&gt;z&lt;/sub&gt; /k&lt;font face=&quot;Symbol&quot;&gt;&lt;sub&gt;^&lt;/sub&gt;&lt;/font&gt;
      &amp;lt;&amp;lt; 1), and can be Landau resonant (0 &amp;lt; &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;1&lt;/sub&gt;/k&lt;sub&gt;z&lt;/sub&gt;
      &amp;lt; &lt;font face=&quot;Symbol&quot;&gt;n&lt;/font&gt;&lt;sub&gt;d&lt;/sub&gt;) with a parallel drifting
      electron population (drift speed &lt;font face=&quot;Symbol&quot;&gt;n&lt;/font&gt;&lt;sub&gt;d&lt;/sub&gt;),
      where subscripts &lt;i&gt;1&lt;/i&gt; and &lt;i&gt;r&lt;/i&gt; indicate frequency in the frame of
      flowing ions and in the lab frame, respectively, and k&lt;sub&gt;z&lt;/sub&gt; is the
      parallel component of the wavevector. A transition in phase velocity from
      0 &amp;lt; &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;1&lt;/sub&gt;/k&lt;sub&gt;z&lt;/sub&gt; &amp;lt; &lt;font face=&quot;Symbol&quot;&gt;n&lt;/font&gt;&lt;sub&gt;d&lt;/sub&gt;
      to 0 &amp;gt; &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;1&lt;/sub&gt;/k&lt;sub&gt;z&lt;/sub&gt; &amp;gt; &lt;font face=&quot;Symbol&quot;&gt;n&lt;/font&gt;&lt;sub&gt;d&lt;/sub&gt;
      for a pair of IEDD eigenmodes is observed as the degree of in-homogeneity
      in the transverse &lt;b&gt;&lt;i&gt;E × B&lt;/i&gt;&lt;/b&gt; flow is increased in a magnetized
      plasma column. For weaker velocity shear, both eigenmodes are dissipative,
      i.e. in Landau resonance, with k&lt;sub&gt;z&lt;/sub&gt; &lt;font face=&quot;Symbol&quot;&gt;n&lt;/font&gt;&lt;sub&gt;d&lt;/sub&gt;
      &amp;gt; 0. For stronger shear, both eigenmodes become reactive, with one&apos;s
      wavevector component k&lt;sub&gt;z&lt;/sub&gt; remaining parallel, but with &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;1&lt;/sub&gt;/k&lt;sub&gt;z&lt;/sub&gt;
      &amp;gt; &lt;font face=&quot;Symbol&quot;&gt;n&lt;/font&gt;&lt;sub&gt;d&lt;/sub&gt; , and the other&apos;s
      wavevector component k&lt;sub&gt;z&lt;/sub&gt; becoming anti-parallel, so that 0 &amp;gt; &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;1&lt;/sub&gt;/k&lt;sub&gt;z&lt;/sub&gt;
      . For both eigenmodes, the transition (1) involves a small frequency shift
      and (2) does not involve a sign change in the wave energy density, which
      is proportional to &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;r&lt;/sub&gt; &lt;font face=&quot;Symbol&quot;&gt;v&lt;/font&gt;&lt;sub&gt;1&lt;/sub&gt;,
      both of which are previously unrecognized aspects of inhomogeneous
      energy-density driven waves.</p>
</abstract>
<counts><page-count count="8"/></counts>
</article-meta>
</front>
<body/>
<back>
</back>
</article>