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Author Lev Vinnik, Sergey Oreshin, Larissa Makeyeva, Dmitriy Peregoudov, Elena Kozlovskaya, Elena Kozlovskaya, Helle Pedersen, Jaroslava Plomerova, Ulrich Achauer, Eduard Kissling, Irina Sanina, Teppo Jämsen, Hanna Silvennoinen, Catherine Pequegnat, Riitta Hurskainen, Robert Guiguet, Helmut Hausmann, Petr Jedlicka, Igor Aleshin, Ekaterina Bourova, Reynir Bodvarsson, Evald Brückl, Tuna Eken, Pekka Heikkinen, Gregory Houseman, Helge Johnsen, Elena Kremenetskaya, Kari Komminaho, Helena Munzarova, Roland Roberts, Bohuslav Ruzek, Hossein Shomali, Johannes Schweitzer, Artem Shaumyan, Ludek Vecsey, Sergei Volosov doi  openurl
  Title Anisotropic lithosphere under the Fennoscandian shield from P receiver functions and SKS waveforms of the POLENET/LAPNET array Type Journal
  Year (down) 2014 Publication Tectonophysics Abbreviated Journal  
  Volume 628 Issue Pages 45-54  
  Keywords Asthenosphere Lithosphere Mantle flow Receiver functions Seismic anisotropy Shear-wave splitting  
  Abstract Seismic azimuthal anisotropy is the key evidence of the past and present strains in the upper mantle. The standard analysis of shear-wave splitting with the SKS techniques is useful in mapping lateral variations but it is insensitive to depth of anisotropy and to variations of anisotropy with depth. To retrieve the depth localized anisotropy under the Fennoscandian shield, we inverted P-wave receiver functions of the POLENET/LAPNET array in northern Finland jointly with SKS recordings. Shear-wave anisotropy of ~2.5% with the fast direction of 40°–60° in a depth range from the Moho to ~110km is a robust result of the inversion. The obtained direction is nearly normal to the azimuth of the maximum horizontal compressional stress in the lithosphere, but a recent origin of this anisotropy is in doubt. This anisotropy may be frozen since the Precambrian, but it shows no clear relation with the trends of the Precambrian tectonics. The upper anisotropic layer accounts for ~40% of shear-wave splitting in SKS, and to explain the rest another anisotropic layer is required. The top of the second layer with a practically similar fast direction is found at a depth of 200–240km. This direction is close to the current APM direction of the lithosphere with implication that the inferred anisotropy may be related with the current plate motion, and the anisotropic layer belongs to the asthenosphere. The bottom of this layer is uncertain, but it is at least 320km deep. In a depth range from 160km to 200–240km the fast anisotropy direction is 110–150°. Origin of this direction is unclear.  
  Programme 1021  
  Campaign  
  Address  
  Corporate Author Thesis  
  Publisher Place of Publication Editor  
  Language Summary Language Original Title  
  Series Editor Series Title Abbreviated Series Title  
  Series Volume Series Issue Edition  
  ISSN 0040-1951 ISBN Medium  
  Area Expedition Conference  
  Notes Approved yes  
  Call Number Serial 8169  
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