• Deutsch

University Logo

  • Home
  • Search
  • Browse
  • Submit
  • Sitemap
Schließen

Refine

Has Fulltext

  • no (15)

Author

  • Sobolev, Stephan Vladimir (12)
  • Baes, Marzieh (4)
  • Haberland, Christian (3)
  • Kind, Rainer (3)
  • Asch, Günter (2)
  • Bock, Günter (2)
  • Bribach, Jens (2)
  • Giese, Peter (2)
  • Grunewald, Steffen (2)
  • Mechie, James (2)
+ more

Year of publication

  • 2019 (2)
  • 2018 (1)
  • 2017 (2)
  • 2016 (1)
  • 2015 (3)
  • 2012 (1)
  • 2006 (2)
  • 2004 (1)
  • 2000 (1)
  • 1999 (1)
+ more

Document Type

  • Article (15)

Language

  • English (15)

Is part of the Bibliography

  • yes (15)

Keywords

  • Dead Sea Transform (2)
  • tectonophysics (2)
  • Central Andes (1)
  • Deformation (1)
  • Geodynamic modelling (1)
  • Gravity modelling (1)
  • LLSVPs (1)
  • Lithospheric structure (1)
  • Numerical modelling (1)
  • S receiver functions (1)
+ more

Institute

  • Institut für Geowissenschaften (15)

15 search hits

  • 1 to 10
  • BibTeX
  • CSV
  • RIS
  • XML
  • 10
  • 20
  • 50
  • 100

Sort by

  • Year
  • Year
  • Title
  • Title
  • Author
  • Author
Subduction and collision processes in the Central Andes constrained by converted seismic phases (2000)
Yuan, X. H ; Sobolev, Stephan Vladimir ; Kind, Rainer ; Oncken, Onno ; Bock, Günter ; Asch, Günter ; Schurr, B. ; Gräber, F. ; Rudloff, Alexander ; Hanka, W. ; Wylegalla, Kurt ; Tibi, R. ; Haberland, Christian ; Rietbrock, Andreas ; Giese, Peter ; Wigger, Peter ; Rower, P. ; Zandt, G. ; Beck, S. ; Wallace, T. ; Pardo, M. ; Comte, D.
Survival of LLSVPs for billions of years in a vigorously convecting mantle: Replenishment and destruction of chemical anomaly (2015)
Mulyukova, Elvira ; Steinberger, Bernhard ; Dabrowski, Marcin ; Sobolev, Stephan Vladimir
We study segregation of the subducted oceanic crust (OC) at the core-mantle boundary and its ability to accumulate and form large thermochemical piles (such as the seismically observed Large Low Shear Velocity Provinces (LLSVPs)). Our high-resolution numerical simulations of thermochemical mantle convection suggest that the longevity of LLSVPs for up to three billion years, and possibly longer, can be ensured by a balance in the rate of segregation of high-density OC material to the core-mantle boundary (CMB) and the rate of its entrainment away from the CMB by mantle upwellings. For a range of parameters tested in this study, a large-scale compositional anomaly forms at the CMB, similar in shape and size to the LLSVPs. Neutrally buoyant thermochemical piles formed by mechanical stirringwhere thermally induced negative density anomaly is balanced by the presence of a fraction of dense anomalous materialbest resemble the geometry of LLSVPs. Such neutrally buoyant piles tend to emerge and survive for at least 3Gyr in simulations with quite different parameters. We conclude that for a plausible range of values of density anomaly of OC material in the lower mantleit is likely that it segregates to the CMB, gets mechanically mixed with the ambient material, and forms neutrally buoyant large-scale compositional anomalies similar in shape to the LLSVPs.
Seismic reflection image revealing offset of Andean subduction-zone earthquake locations into oceanic mantle (1999)
Oncken, Onno ; Luschen, Ewald ; Mechie, James ; Sobolev, Stephan Vladimir ; Schulze, Albrecht ; Gaedicke, Christoph ; Grunewald, Steffen ; Bribach, Jens ; Asch, Günter ; Giese, Peter ; Wigger, Peter ; Schmitz, Michael ; Lueth, Stefan ; Scheuber, Ekkehard ; Haberland, Christian ; Rietbrock, Andreas ; Götze, Hans-Jürgen ; Brasse, Heinrich ; Patzwahl, Regina ; Chong, Guillermo ; Wilke, Hans-Gerhard ; Gonzalez, Gabriel ; Jensen, Arturo ; Araneda, Manuel ; Vieytes, Hugo ; Behn, Gerardo ; Martinez, Eloy
Low-buoyancy thermochemical plumes resolve controversy of classical mantle plume concept (2015)
Dannberg, Juliane ; Sobolev, Stephan Vladimir
The Earth's biggest magmatic events are believed to originate from massive melting when hot mantle plumes rising from the lowermost mantle reach the base of the lithosphere. Classical models predict large plume heads that cause kilometre-scale surface uplift, and narrow (100 km radius) plume tails that remain in the mantle after the plume head spreads below the lithosphere. However, in many cases, such uplifts and narrow plume tails are not observed. Here using numerical models, we show that the issue can be resolved if major mantle plumes contain up to 15-20% of recycled oceanic crust in a form of dense eclogite, which drastically decreases their buoyancy and makes it depth dependent. We demonstrate that, despite their low buoyancy, large enough thermochemical plumes can rise through the whole mantle causing only negligible surface uplift. Their tails are bulky (4200 km radius) and remain in the upper mantle for 100 millions of years.
Thermomechanical model reconciles contradictory geophysical observations at the Dead Sea Basin (2012)
Petrunin, Alexey G. ; Rioseco, Ernesto Meneses ; Sobolev, Stephan Vladimir ; Weber, Michael H.
The Dead Sea Transform (DST) comprises a boundary between the African and Arabian plates. During the last 15-20 m.y. more than 100 km of left lateral transform displacement has been accumulated on the DST and about 10 km thick Dead Sea Basin (DSB) was formed in the central part of the DST. Widespread igneous activity since some 20 Ma ago and especially in the last 5 m.y., thin (60-80 km) lithosphere constrained by seismic data and absence of seismicity below the Moho, seem to be quite natural for this tectonically active plate boundary. However, surface heat flow values of less than 50-60 mW/m(2) and deep seismicity in the lower crust (deeper than 20 km) reported for this region are apparently inconsistent with the tectonic settings specific for an active continental plate boundary and with the crustal structure of the DSB. To address these inconsistencies which comprise what we call the "DST heat-flow paradox," we have developed a numerical model that assumes an erosion of initially thick and cold lithosphere just before or during the active faulting at the DST. The optimal initial conditions for the model are defined using transient thermal analysis. From the results of our numerical experiments we conclude that the entire set of observations for the DSB can be explained within the classical pull-apart model assuming that the lithosphere has been thermally eroded at about 20 Ma and the uppermost mantle in the region have relatively weak rheology consistent with experimental data for wet olivine or pyroxenite.
The crustal structure of the Dead Sea Transform (2004)
Weber, Michael H. ; Abu-Ayyash, Khalil ; Abueladas, Abdel-Rahman ; Agnon, Amotz ; Al-Amoush, H. ; Babeyko, Andrey Y. ; Bartov, Yosef ; Baumann, M. ; Ben-Avraham, Zvi ; Bock, Günter ; Bribach, Jens ; El-Kelani, R. ; Forster, A. ; Förster, Hans-Jürgen ; Frieslander, U. ; Garfunkel, Zvi ; Grunewald, Steffen ; Gotze, Hans-Jürgen ; Haak, Volker ; Haberland, Christian ; Hassouneh, Mohammed ; Helwig, S. ; Hofstetter, Alfons ; Jackel, K. H. ; Kesten, Dagmar ; Kind, Rainer ; Maercklin, Nils ; Mechie, James ; Mohsen, Amjad ; Neubauer, F. M. ; Oberhänsli, Roland ; Qabbani, I. ; Ritter, O. ; Rumpker, G. ; Rybakov, M. ; Ryberg, Trond ; Scherbaum, Frank ; Schmidt, J. ; Schulze, A. ; Sobolev, Stephan Vladimir ; Stiller, M. ; Th
To address one of the central questions of plate tectonics-How do large transform systems work and what are their typical features?-seismic investigations across the Dead Sea Transform (DST), the boundary between the African and Arabian plates in the Middle East, were conducted for the first time. A major component of these investigations was a combined reflection/ refraction survey across the territories of Palestine, Israel and Jordan. The main results of this study are: (1) The seismic basement is offset by 3-5 km under the DST, (2) The DST cuts through the entire crust, broadening in the lower crust, (3) Strong lower crustal reflectors are imaged only on one side of the DST, (4) The seismic velocity sections show a steady increase in the depth of the crust-mantle transition (Moho) from 26 km at the Mediterranean to 39 km under the Jordan highlands, with only a small but visible, asymmetric topography of the Moho under the DST. These observations can be linked to the left-lateral movement of 105 km of the two plates in the last 17 Myr, accompanied by strong deformation within a narrow zone cutting through the entire crust. Comparing the DST and the San Andreas Fault (SAF) system, a strong asymmetry in subhorizontal lower crustal reflectors and a deep reaching deformation zone both occur around the DST and the SAF. The fact that such lower crustal reflectors and deep deformation zones are observed in such different transform systems suggests that these structures are possibly fundamental features of large transform plate boundaries
Plate tectonics on the Earth triggered by plume-induced subduction initiation (2015)
Gerya, Taras V. ; Stern, Robert J. ; Baes, Marzieh ; Sobolev, Stephan Vladimir ; Whattam, Scott A.
Scientific theories of how subduction and plate tectonics began on Earth-and what the tectonic structure of Earth was before this-remain enigmatic and contentious(1). Understanding viable scenarios for the onset of subduction and plate tectonics(2,3) is hampered by the fact that subduction initiation processes must have been markedly different before the onset of global plate tectonics because most present-day subduction initiation mechanisms require acting plate forces and existing zones of lithospheric weakness, which are both consequences of plate tectonics(4). However, plume-induced subduction initiation(5-9) could have started the first subduction zone without the help of plate tectonics. Here, we test this mechanism using high-resolution three-dimensional numerical thermomechanical modelling. We demonstrate that three key physical factors combine to trigger self-sustained subduction: (1) a strong, negatively buoyant oceanic lithosphere; (2) focused magmatic weakening and thinning of lithosphere above the plume; and (3) lubrication of the slab interface by hydrated crust. We also show that plume-induced subduction could only have been feasible in the hotter early Earth for old oceanic plates. In contrast, younger plates favoured episodic lithospheric drips rather than self-sustained subduction and global plate tectonics.
Modeling Seismic Cycles of Great Megathrust Earthquakes Across the Scales With Focus at Postseismic Phase (2017)
Sobolev, Stephan Vladimir ; Muldashev, Iskander A.
Mantle Flow as a Trigger for Subduction Initiation: A Missing Element of the Wilson Cycle Concept (2017)
Baes, Marzieh ; Sobolev, Stephan Vladimir
The classical Wilson Cycle concept, describing repeated opening and closing of ocean basins, hypothesizes spontaneous conversion of passive continental margins into subduction zones. This process, however, is impeded by the high strength of passive margins, and it has never occurred in Cenozoic times. Here using thermomechanical models, we show that additional forcing, provided by mantle flow, which is induced by neighboring subduction zones and midmantle slab remnants, can convert a passive margin into a subduction zone. Models suggest that this is a long-term process, thus explaining the lack of Cenozoic examples. We speculate that new subduction zones may form in the next few tens of millions of years along the Argentine passive margin and the U.S. East Coast. Mantle suction force can similarly trigger subduction initiation along large oceanic fracture zones. We propose that new subduction zones will preferentially originate where subduction zones were active in the past, thus explaining the remarkable colocation of subduction zones during at least the last 400 Myr.
3-D thermo-mechanical modeling of plume-induced subduction initiation (2016)
Baes, Marzieh ; Gerya, T. ; Sobolev, Stephan Vladimir
Here, we study the 3-D subduction initiation process induced by the interaction between a hot thermochemical mantle plume and oceanic lithosphere using thermo-mechanical viscoplastic finite difference marker-in-cell models. Our numerical modeling results show that self-sustaining subduction is induced by plume-lithosphere interaction when the plume is sufficiently buoyant, the oceanic lithosphere is sufficiently old and the plate is weak enough to allow the buoyant plume to. pass through it. Subduction initiation occurs following penetration of the lithosphere by the hot plume and the downward displacement of broken, nearly circular segments of lithosphere (proto-slabs) as a result of partially molten plume rocks overriding the proto-slabs. Our experiments show four different deformation regimes in response to plume-lithosphere interaction: a) self-sustaining subduction initiation, in which subduction becomes self-sustaining; b) frozen subduction initiation, in which subduction stops at shallow depths; c) slab break-off, in which the subducting circular slab breaks off soon after formation; and d) plume underplating, in which the plume does not pass through the lithosphere and instead spreads beneath it (i.e., failed subduction initiation). These regimes depend on several parameters, such as the size, composition, and temperature of the plume, the brittle/plastic strength and age of the oceanic lithosphere, and the presence/absence of lithospheric heterogeneities. The results show that subduction initiates and becomes self-sustaining when the lithosphere is older than 10 Myr and the non dimensional ratio of the plume buoyancy force and lithospheric strength above the plume is higher than approximately 2. The outcomes of our numerical experiments are applicable for subduction initiation in the modern and Precambrian Earth and for the origin of plume-related corona structures on Venus. (C) 2016 Elsevier B.V. All rights reserved.
  • 1 to 10

OPUS4 Logo  KOBV Logo  OAI Logo  DINI Zertifikat 2007  OA Netzwerk Logo

    • Publication server
    • University Bibliography
    • University Library
    • Policy
    • Contact
    • Imprint
    • Privacy Policy
    • Accessibility

    Login