2021
DOI: 10.31223/x5b05d
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Controls of the lithospheric thermal field of an ocean-continent subduction zone: the southern Central Andes

Abstract: In an ocean-continent subduction zone, the assessment of the lithospheric thermal state is essential to determine the controls of the deformation within the upper plate and the dip angle of the subducting lithosphere. In this study, we evaluate the degree of influence of both the configuration of the upper plate and variations of the subduction angle on the lithospheric thermal field of the southern Central Andes (29°–39°S). Here, the subduction angle increases from subhorizontal (5°) north of 33°S, to steep (… Show more

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Cited by 2 publications
(9 citation statements)
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“…Compressional deformation occurs in the transition zone between the flat and steep sectors of the slab, promoted by increased slab pull (steepening segment; red‐shaded area). The isotherms (Rodriguez Piceda, Scheck Wenderoth, Bott et al., 2021) are marked by dashed blue lines. Light‐gray lines show the interfaces of the model layers (Rodriguez Piceda, Scheck Wenderoth, Gomez Dacal et al., 2021).…”
Section: Discussionmentioning
confidence: 99%
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“…Compressional deformation occurs in the transition zone between the flat and steep sectors of the slab, promoted by increased slab pull (steepening segment; red‐shaded area). The isotherms (Rodriguez Piceda, Scheck Wenderoth, Bott et al., 2021) are marked by dashed blue lines. Light‐gray lines show the interfaces of the model layers (Rodriguez Piceda, Scheck Wenderoth, Gomez Dacal et al., 2021).…”
Section: Discussionmentioning
confidence: 99%
“…In an attempt to better quantify the efficiency of viscous creep, we also discuss the results in terms of the effective viscosity (η eff ). This parameter is expressed by a power‐law dependence of temperature and strain rate as (Burov, 2011): ηnormalenormalfnormalf=21normalnn31+normaln2normalnA1nε˙1n1exp()normalHnRT ${{\eta}}_{\mathrm{e}\mathrm{f}\mathrm{f}}=\frac{{2}^{\frac{1-\mathrm{n}}{\mathrm{n}}}}{{3}^{\frac{1+\mathrm{n}}{2\mathrm{n}}}}{\mathrm{A}}^{-\frac{1}{\mathrm{n}}}{\dot{\varepsilon }}^{\frac{1}{\mathrm{n}}-1}\mathrm{exp}\left(\frac{\mathrm{H}}{\mathrm{n}\mathrm{R}\mathrm{T}}\right)$ the material and temperature distributions used as input were derived from 3D lithospheric‐scale models of the SCA (Rodriguez Piceda, Scheck Wenderoth, Gomez Dacal et al., 2021; Rodriguez Piceda, Scheck Wenderoth, Bott et al., 2021) and described in more detail in Section 2.1.1. The specific mechanical properties assigned to the lithospheric units of the model are subsequently outlined in Section 2.1.2.…”
Section: Methodsmentioning
confidence: 99%
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