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<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-19-611-2012</article-id>
<title-group>
<article-title>Complete synchronization of chaotic atmospheric models by connecting only a subset of state space</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hiemstra</surname>
<given-names>P. H.</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>Fujiwara</surname>
<given-names>N.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Selten</surname>
<given-names>F. M.</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>Kurths</surname>
<given-names>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>Royal Netherlands Meteorological Institute (KNMI), P.O. Box 201, 3730 AE, De Bilt, The Netherlands</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Potsdam Institute for Climate Impact Research (PIK), P.O. Box 60 12 03, 14412 Potsdam, Germany</addr-line>
</aff>
<pub-date pub-type="epub">
<day>12</day>
<month>11</month>
<year>2012</year>
</pub-date>
<volume>19</volume>
<issue>6</issue>
<fpage>611</fpage>
<lpage>621</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2012 P. H. Hiemstra et al.</copyright-statement>
<copyright-year>2012</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://npg.copernicus.org/articles/19/611/2012/npg-19-611-2012.html">This article is available from https://npg.copernicus.org/articles/19/611/2012/npg-19-611-2012.html</self-uri>
<self-uri xlink:href="https://npg.copernicus.org/articles/19/611/2012/npg-19-611-2012.pdf">The full text article is available as a PDF file from https://npg.copernicus.org/articles/19/611/2012/npg-19-611-2012.pdf</self-uri>
<abstract>
<p>Connected chaotic systems can, under some circumstances, synchronize their states with an exchange
of matter and energy between the systems. This is the case for toy models like the Lorenz 63, and more complex models.
In this study we perform synchronization experiments with two connected quasi-geostrophic (QG) models of the atmosphere
with 1449 degrees of freedom. The purpose is to determine whether connecting only a subset of the model state space can
still lead to complete synchronization (CS). In addition, we evaluated whether empirical orthogonal functions (EOF)
form efficient basis functions for synchronization in order to limit the number of connections. In this paper,
we show that only the intermediate spectral wavenumbers (5–12) need to be connected in order to achieve CS.
In addition, the minimum connection timescale needed for CS is 7.3 days. Both the connection subset and the connection timescale,
or strength, are consistent with the time and spatial scales of the baroclinic instabilities in the model. This is in line with
the fact that the baroclinic instabilities are the largest source of divergence between the two connected models.
Using the Lorenz 63 model, we show that EOFs are nearly optimal basis functions for synchronization. The QG model
results show that the minimum number of EOFs that need to be connected for CS is a factor of three smaller than
when connecting the original state variables.</p>
</abstract>
<counts><page-count count="11"/></counts>
</article-meta>
</front>
<body/>
<back>
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</article>