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Letter

Nature 440, 324-328 (16 March 2006) | doi:10.1038/nature04608; Received 13 October 2005; Accepted 24 January 2006

A mechanism to thin the continental lithosphere at magma-poor margins

Luc L. Lavier1 & Gianreto Manatschal2

  1. University of Texas Institute for Geophysics, Jackson School of Geosciences, Austin, Texas 78759, USA
  2. CGS-EOST, Université Louis Pasteur, 1 rue Blessig, F-67084 Strasbourg, France

Correspondence to: Luc L. Lavier1 Correspondence and requests for materials should be addressed to L.L.L. (Email: luc@ig.utexas.edu).

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Where continental plates break apart, slip along multiple normal faults provides the required space for the Earth's crust to thin and subside1. After initial rifting, however, the displacement on normal faults observed at the sea floor seems not to match the inferred extension2. Here we show that crustal thinning can be accomplished in such extensional environments by a system of conjugate concave downward faults instead of multiple normal faults. Our model predicts that these concave faults accumulate large amounts of extension and form a very thin crust (< 10 km) by exhumation of mid-crustal and mantle material. This transitional crust is capped by sub-horizontal detachment surfaces over distances exceeding 100 km with little visible deformation. Our rift model is based on numerical experiments constrained by geological and geophysical observations from the Alpine Tethys and Iberia/Newfoundland margins3, 4, 5, 6, 7, 8, 9. Furthermore, we suggest that the observed transition from broadly distributed and symmetric extension to localized and asymmetric rifting is directly controlled by the existence of a strong gabbroic lower crust. The presence of such lower crustal gabbros is well constrained for the Alpine Tethys system4, 9. Initial decoupling of upper crustal deformation from lower crustal and mantle deformation by progressive weakening of the middle crust is an essential requirement to reproduce the observed rift evolution. This is achieved in our models by the formation of weak ductile shear zones.

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