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P. Schmoldt, PhD - MTNet - DIAS

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11. Summary and conclusions<br />

high misfits associated with impedance tensor decomposition for every direction indicate<br />

invalidity of a 2D approximation for this region. Thus, further investigation was focussed<br />

on the Tajo Basin subsurface using the novel inversion approaches developed in the course<br />

of this thesis to cope with the issue of oblique geoelectric strike directions in the basin’s<br />

crust and mantle regions. In addition, extensive isotropic 2D and 3D inversions were<br />

conducted to further enhance knowledge about the geological setting.<br />

The final Tajo Basin subsurface model is the synthesis of results from the different inversion<br />

approaches. Crustal structures in the model were determined through isotropic<br />

2D inversion of a dataset decomposed according to the crustal geoelectric strike direction<br />

with the period range limited to crustal penetration depths. Owing to inadequacy<br />

of isotropic 2D and anisotropic 1D inversion results, and uncertainties associated with<br />

the anisotropic 2D inversion results, mantle structures were mostly deduced from the 3D<br />

inversion model. Most striking features of models for the Tajo Basin crust are:<br />

282<br />

• A well-defined difference in terms of electric resistivity of the crust between the<br />

southern and northern parts of the Tajo Basin. The interface between the two regions<br />

coincides with a significant change in seismic velocity determined in a seismic<br />

tomography study. The southern region exhibits high electric resistivities and<br />

high seismic velocities, whereas the northern region comprises relatively low electric<br />

resistivities and low seismic velocities. Based on the correlation of the seismic<br />

velocity model with the border between the so-called ‘Variscan Spain’ and ‘Alpine<br />

Spain’ regions for most of the Iberian Peninsula, the southern high resistivity –<br />

high velocity region was inferred to be associated with Precambrian and Palaeozoic<br />

rocks of the Variscan Iberian Massif, whereas the northern region was attributed<br />

to the domain that underwent significant Alpine deformation. Alpine deformation<br />

of the northern Tajo Basin region is related to collisions of the Iberian Peninsula<br />

with the rest of Eurasia and Africa during Late Mesozoic and Cenozoic times that<br />

resulted in the orogeny of the Pyrenees and Betic Mountain chains. It is concluded<br />

that the difference of the Alpine Spain and Variscan Spain region in terms of electric<br />

resistivity values is due to compositional differences with additional temperature effects.<br />

The Precambrian and Palaeozoic rocks of the Iberian Massif, constituting the<br />

majority of the Variscan Spain region, are significantly older than the Alpine Spain<br />

region (Mesozoic and Cenozoic material). Thus, the Variscan Spain region has undergone<br />

a respectively longer cooling, a situation similar to cratonic regions when<br />

compared with surrounding mobile belts. Compositional differences may therein<br />

involve a higher amount of resistive olivine, pyroxene, garnet components for the<br />

Variscan Spain region in contrast to the higher amount of metallic elements as well<br />

as graphite and sulphide bearing oxides in the Alpine Spain region (cf. Sec. 5.2.1).<br />

Further, higher conductivity may be indicative of an enhanced connectivity of the<br />

conducting phases in the Alpine Spain region. The enhanced connectivity may originate<br />

from deformation events during the more recent Alpine orogeny in contrast<br />

to the relatively undeformed Iberian Massif. However, additional studies about the

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