2000
DOI: 10.1029/2000jb900032
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Modeling mountain building and the seismic cycle in the Himalaya of Nepal

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Cited by 339 publications
(324 citation statements)
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“…The disequilibrium induced by the very high level of the Ivrea Body, imbricated within the upper crust, is compensated to some degree by the presence of low-density sediments (d = 2.4) in the overlying Po plain. The rheological parameters have been fixed using laboratory experiments of deformation (Kirby and Kronenberg 1987;Cloetingh and Burov 1996) as well as comparison with other tectonic numerical models (e.g., Chéry et al 1990;Hassani and Chéry 1996;Burov et al 1999;Cattin and Avouac 2000). The analyses of the different models tested show that modifications of these parameters within realistic ranges do not alter the major patterns of the stress/strain states.…”
Section: D Crustal Cross-section Finite Element Modelingmentioning
confidence: 99%
“…The disequilibrium induced by the very high level of the Ivrea Body, imbricated within the upper crust, is compensated to some degree by the presence of low-density sediments (d = 2.4) in the overlying Po plain. The rheological parameters have been fixed using laboratory experiments of deformation (Kirby and Kronenberg 1987;Cloetingh and Burov 1996) as well as comparison with other tectonic numerical models (e.g., Chéry et al 1990;Hassani and Chéry 1996;Burov et al 1999;Cattin and Avouac 2000). The analyses of the different models tested show that modifications of these parameters within realistic ranges do not alter the major patterns of the stress/strain states.…”
Section: D Crustal Cross-section Finite Element Modelingmentioning
confidence: 99%
“…Modellers commonly use generic viscosity contrasts or laboratory-derived flow laws under the assumption that they can be extrapolated over several orders of magnitude to geological conditions (e.g. Cattin and Avouac, 2000). An olivine-controlled rheology is commonly assumed for the upper mantle (Jackson, 2002), whereas the ductile parts of the crust are modelled using power-law creep equations describing crystal -plastic flow of quartz or feldspar (Bos and Spiers, 2002).…”
Section: Introductionmentioning
confidence: 99%
“…The MHT reaches the surface at the MFT (Nakata 1989) (Fig. 3), and the MHT is actually locked at the surface and roots about 100 km to the north of the MFT into a subhorizontal shear zone, which is probably thermally enhanced ductile flow (Cattin and Avouac 2000). Therefore, we set a receiver fault similar to the MHT and calculated the Coulomb stress change on that.…”
Section: Normal Fault Systems Riskmentioning
confidence: 99%