2015
DOI: 10.1016/j.epsl.2014.10.043
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Mantle temperature as a control on the time scale of thermal evolution of extensional basins

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Cited by 20 publications
(21 citation statements)
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“…We define a strong and a weak lower crust, respectively, following Schmalholz et al (2009), where the weak lower crust is based on the experimentally derived properties of diabase (Afonso & Ranalli, 2004), and the strong lower crust is the Columbia diabase from Mackwell et al (1998; see Table 1 of the supporting information). The upper crust is wet quartzite (Ranalli, 1995), and a combined diffusion/dislocation creep dry olivine flow law based on Karato and Wu (1993) is assumed for both the lithosphere and asthenosphere (see Petersen et al, 2015). While the parameter values are based on limited experimental evidence, the important point is that the difference in lower crustal strength is six orders of magnitude between the strong and weak case (Schmalholz et al, 2009).…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…We define a strong and a weak lower crust, respectively, following Schmalholz et al (2009), where the weak lower crust is based on the experimentally derived properties of diabase (Afonso & Ranalli, 2004), and the strong lower crust is the Columbia diabase from Mackwell et al (1998; see Table 1 of the supporting information). The upper crust is wet quartzite (Ranalli, 1995), and a combined diffusion/dislocation creep dry olivine flow law based on Karato and Wu (1993) is assumed for both the lithosphere and asthenosphere (see Petersen et al, 2015). While the parameter values are based on limited experimental evidence, the important point is that the difference in lower crustal strength is six orders of magnitude between the strong and weak case (Schmalholz et al, 2009).…”
Section: Methodsmentioning
confidence: 99%
“…To calculate this duration we use the model time taken to generate 8 km of igneous crust. Therefore, to explore the combined effects of the rate of extension and crustal rheology we will focus on a mantle potential temperature of 1; 350 C ( Figure 5), which is close to that required to match the global trend of oceanic subsidence (Petersen et al, 2015). Therefore, to explore the combined effects of the rate of extension and crustal rheology we will focus on a mantle potential temperature of 1; 350 C ( Figure 5), which is close to that required to match the global trend of oceanic subsidence (Petersen et al, 2015).…”
Section: 1002/2017gc007326mentioning
confidence: 99%
“…The resulting linear system is solved iteratively, using a Gauss-Seidel scheme (Press et al, 1992) combined with multigrid (Tackley, 2008). This allows for high numerical efficiency and resolution (Petersen et al, 2010;Petersen et al, 2015).…”
Section: Dpicmentioning
confidence: 99%
“…During the last decade, a variety of numerical codes have been developed and 2D numerical modeling became a standard tool to investigate rift processes [e.g. Nagel and Buck, 2004;Lavier and Manatschal, 2006;Pérez-Gussinyé et al, 2006;Buiter et al, 2008;Gueydan et al, 2008;van Wijk et al, 2008;Jammes et al, 2010;Rosenbaum et al, 2010;Wallner and Schmeling, 2010;Huet et al, 2011;Huismans and Beaumont, 2011;Rey et al, 2011;Armitage et al, 2012;Beaumont and Ings, 2012;Choi and Buck, 2012;Chen et al, 2013;Chenin and Beaumont, 2013;Gueydan and Précigout, 2013;Watremez et al, 2013;Brune et al, 2014;Liao and Gerya, 2014;Clift et al, 2015;Petersen et al, 2015;Sharples et al, 2015]. The major limiting factor when conducting 3D numerical models is the model resolution.…”
Section: Modeling Approachesmentioning
confidence: 99%