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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-26-2871-2008</article-id>
<title-group>
<article-title>On a new process for cusp irregularity production</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Carlson</surname>
<given-names>H. C.</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>Oksavik</surname>
<given-names>K.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Moen</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Department of Physics, University of Oslo, Oslo, Norway</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Utah State University, CASS, Logan, UT, USA</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Arctic Geophysics, The University Centre in Svalbard, Longyearbyen, Norway</addr-line>
</aff>
<pub-date pub-type="epub">
<day>23</day>
<month>09</month>
<year>2008</year>
</pub-date>
<volume>26</volume>
<issue>9</issue>
<fpage>2871</fpage>
<lpage>2885</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2008 H. C. Carlson et al.</copyright-statement>
<copyright-year>2008</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>
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<abstract>
<p>Two plasma instability mechanisms were thought until 2007 to dominate the
formation of plasma irregularities in the F region high latitude and polar
ionosphere; the gradient-drift driven instability, and the velocity-shear
driven instability. The former mechanism was accepted as accounting for
plasma structuring in polar cap patches, the latter for plasma structuring
in polar cap sun aligned arcs. Recent work has established the need to
replace this view of the past two decades with a new patch plasma structuring
process (not a new mechanism), whereby shear-driven instabilities first
rapidly structure the entering plasma, after which gradient drift
instabilities build on these large &quot;seed&quot; irregularities. Correct modeling
of cusp and early polar cap patch structuring will not be accomplished
without allowing for this compound process. This compound process explains
several previously unexplained characteristics of cusp and early polar cap
patch irregularities. Here we introduce additional data, coincident in time
and space, to extend that work to smaller irregularity scale sizes and
relate it to the structured cusp current system.</p>
</abstract>
<counts><page-count count="15"/></counts>
</article-meta>
</front>
<body/>
<back>
<ref-list>
<title>References</title>
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</article>