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<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:creator>Frederick Pollitz</dc:creator>
  <dc:date>2019</dc:date>
  <dc:description>&lt;p&gt;&lt;span&gt;In tectonically active regions, post-earthquake motions are generally shaped by a combination of continued fault slippage (afterslip) on a timescale of days to months and viscoelastic relaxation of the&amp;nbsp;lower crust&amp;nbsp;and&amp;nbsp;upper mantle&amp;nbsp;on a timescale of days to years. Transient crustal motions have been observed following numerous magnitude &amp;gt;~7 earthquakes in various&amp;nbsp;tectonic settings: continental&amp;nbsp;rift zones&amp;nbsp;(Basin and Range), continental&amp;nbsp;plate boundary&amp;nbsp;zones (San Andreas fault corridor; Alaska; Turkey),&amp;nbsp;subduction zones&amp;nbsp;(Japan, Chile, Sumatra), ongoing&amp;nbsp;continental collision&amp;nbsp;zones (Arabia; Tibet), and mid-ocean rifting zones (Iceland). When afterslip can be discriminated from viscoelastic relaxation and when temporal coverage of the postseismic measurements is broad (i.e.,&amp;nbsp;geodetic surveys&amp;nbsp;of at least several years duration are available), a wide spectrum of relaxation timescales are usually identified. Current temporal resolution and modeling approaches (e.g., Burgers body analog) allow identification of transient (Kelvin) and steady-state (Maxwell) viscosities that are operable in the short-term and long-term, respectively. I compile results from 40 studies of post-earthquake motions, augmented by ten studies of contemporary surface loading or unloading, that illuminate current estimates of transient and steady-state viscosity of the lower crust and/or uppermost mantle. Lower crust viscosity estimates range from&amp;nbsp;&lt;/span&gt;&lt;i&gt;~&lt;/i&gt;&lt;span&gt;10&lt;/span&gt;&lt;sup&gt;18&lt;/sup&gt;&lt;span&gt;&amp;nbsp;to 10&lt;/span&gt;&lt;sup&gt;21&lt;/sup&gt;&lt;span&gt;&amp;nbsp;Pa s, with most estimates near the upper end except in areas of overthickened crust. Mantle lithosphere and&amp;nbsp;asthenosphere&amp;nbsp;viscosity estimates are particularly abundant and yield a picture of transient viscosity ranging from ~10&lt;/span&gt;&lt;sup&gt;16&lt;/sup&gt;&lt;span&gt;&amp;nbsp;to 10&lt;/span&gt;&lt;sup&gt;19&lt;/sup&gt;&lt;span&gt;&amp;nbsp;Pa s and steady-state viscosity ranging from ~10&lt;/span&gt;&lt;sup&gt;18&lt;/sup&gt;&lt;span&gt;&amp;nbsp;to 10&lt;/span&gt;&lt;sup&gt;21&lt;/sup&gt;&lt;span&gt; Pa s. To first order, both transient and steady-state viscosities are well correlated with regional heat flow, and steady-state viscosities are comparable with temperature and strain-rate dependent rock viscosities from laboratory-based flow laws.&lt;/span&gt;&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1016/j.pepi.2019.106271</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Elsevier</dc:publisher>
  <dc:title>Lithosphere and shallow asthenosphere rheology from observations of post-earthquake relaxation</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>