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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-3-102-1996</article-id>
<title-group>
<article-title>Renormalization group theory of earthquakes</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Saleur</surname>
<given-names>H.</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>Sammis</surname>
<given-names>C. G.</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>Sornette</surname>
<given-names>D.</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 and Astronomy, University of Southern California, Los Angeles, CA 90089-0740, USA</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Packard Fellow</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Department of Earth Sciences, University of Southern California, Los Angeles, CA 90089-0740, USA</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>Laboratoire de Physique de la Matière Condensée, CNRS URA 190, Université des Sciences, B. P. 70, Parc Valrose, 06108 Nice Cedex 2, France</addr-line>
</aff>
<pub-date pub-type="epub">
<day>30</day>
<month>06</month>
<year>1996</year>
</pub-date>
<volume>3</volume>
<issue>2</issue>
<fpage>102</fpage>
<lpage>109</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 1996 H. Saleur et al.</copyright-statement>
<copyright-year>1996</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/3/102/1996/npg-3-102-1996.html">This article is available from https://npg.copernicus.org/articles/3/102/1996/npg-3-102-1996.html</self-uri>
<self-uri xlink:href="https://npg.copernicus.org/articles/3/102/1996/npg-3-102-1996.pdf">The full text article is available as a PDF file from https://npg.copernicus.org/articles/3/102/1996/npg-3-102-1996.pdf</self-uri>
<abstract>
<p>We  study theoretically  the physical 
origin of  the
          proposed &lt;I&gt;discrete&lt;/I&gt; scale invariance  of earthquake
processes, at
          the   origin  of  the  &lt;I&gt;universal&lt;/I&gt;  log-periodic 
corrections  to
          scaling,  recently  discovered  in  regional  seismic 
activity
          (Sornette and Sammis  (1995)). The discrete  scaling
symmetries
          which may be present at  smaller scales&lt;B&gt; &lt;/B&gt;are shown
to be  robust
          on a  global scale  with respect  to  disorder.
Furthermore,  a
          single complex  exponent is sufficient  in practice to 
capture
          the essential properties of the leading  correction to
scaling,
          whose real  part may be renormalized  by disorder,  and
thus be
          specific  to the  system. We then  propose a  new&lt;B&gt;
&lt;/B&gt;mechanism for
          discrete  scale  invariance,  based  on  the&lt;B&gt;
&lt;/B&gt;interplay  between
          dynamics and disorder. The existence of  non-linear
corrections
          to the  renormalization group flow  implies that an 
earthquake
          is not an isolated &quot;critical  point&quot;, but is accompanied

by an
          embedded  set of  &quot;critical  points&quot;,  its foreshocks 
and  any
          subsequent shocks for which it may be a foreshock.</p>
</abstract>
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