4.6 Article

Mountain building and mantle dynamics

期刊

TECTONICS
卷 32, 期 1, 页码 80-93

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AMER GEOPHYSICAL UNION
DOI: 10.1029/2012TC003176

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  1. NSF [EAR-0855546, EAR 0930046, 0643365]
  2. Directorate For Geosciences
  3. Division Of Earth Sciences [0855546] Funding Source: National Science Foundation
  4. Division Of Earth Sciences
  5. Directorate For Geosciences [0643365, 0809023] Funding Source: National Science Foundation

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Mountain building at convergent margins requires tectonic forces that can overcome frictional resistance along large-scale thrust faults and support the gravitational potential energy stored within the thickened crust of the orogen. A general, dynamic model for this process is still lacking. Here we propose that mountain belts can be classified between two end-members. First, those of slab pull type, where subduction is mainly confined to the upper mantle, and rollback trench motion lead to moderately thick crustal stacks, such as in the Mediterranean. Second, those of slab suction type, where whole-mantle convection cells (conveyor belts) lead to the more extreme expressions of orogeny, such as the largely thickened crust and high plateaus of present-day Tibet and the Altiplano. For the slab suction type, deep mantle convection produces the unique conditions to drag plates toward each other, irrespective of their nature and other boundary conditions. We support this hypothesis by analyzing the orogenic, volcanic, and convective history associated with the Tertiary formation of the Andes after similar to 40 Ma and Himalayas after collision at similar to 55 Ma. Based on mantle circulation modeling and tectonic reconstructions, we surmise that the forces necessary to sustain slab-suction mountain building in those orogens derive, after transient slab ponding, from the mantle drag induced upon slab penetration into the lower mantle, and from an associated surge of mantle upwelling beneath Africa. This process started at similar to 65-55 Ma for Tibet-Himalaya, when the Tethyan slab penetrated into the lower mantle, and similar to 10 Myr later in the Andes, when the Nazca slab did. This surge of mantle convection drags plates against each other, generating the necessary compressional forces to create and sustain these two orogenic belts. If our model is correct, the available geological records of orogeny can be used to decipher time-dependent mantle convection, with implications for the supercontinental cycle. Citation: Faccenna, C., T. W. Becker, C. P. Conrad, and L. Husson (2013), Mountain building and mantle dynamics, Tectonics, 32, 80-93, doi:10.1029/2012TC003176.

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