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P. Schmoldt, PhD - MTNet - DIAS

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List of Figures<br />

xiv<br />

10.31.RMS misfit for different Tajo Basin subsurface models used to investigate<br />

the electric resistivity of the lithospheric-mantle and the depth of the<br />

lithosphere–asthenosphere boundary . . . . . . . . . . . . . . . . . . . . 270<br />

10.32.Misfit distribution for XY apparent resistivity data of the PICASSO Phase<br />

I stations and periods for a selection of Tajo Basin subsurface models . . 271<br />

10.33.Comparison of the isotropic 3D inversion result of PICASSO Phase I station<br />

responses in the Tajo Basin and a seismic tomography transect extracted<br />

from the global P-wave velocity model of Amaru [2007] . . . . . 272<br />

10.34.Location of the southern Tajo Basin mid-crustal high conductivity anomaly<br />

in the isotropic 3D inversion model . . . . . . . . . . . . . . . . . . . . . 273<br />

A.1. Geological evolution of the Iberian Peninsula in terms of past and presentday<br />

stress fields . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 288<br />

A.2. Geological evolution of the Iberian Peninsula in terms of past and presentday<br />

stress fields (continued) . . . . . . . . . . . . . . . . . . . . . . . . . 289<br />

A.3. Issues in conjunction with using the true crustal electric resistivity distribution<br />

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 292<br />

A.4. Isotropic 2D inversion results for the 3D-mantle profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 296<br />

A.5. Isotropic 2D inversion results for the 04-centre profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 297<br />

A.6. Isotropic 2D inversion results for the 07-centre profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 298<br />

A.7. Isotropic 2D inversion results for the 10-centre profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 299<br />

A.8. Isotropic 2D inversion results for the 3D-crust profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 300<br />

A.9. Isotropic 2D inversion results for the G-centre profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 301<br />

A.10.Isotropic 2D inversion results for the J-centre profile on top of the synthetic<br />

3D model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 302<br />

A.11.Result of anisotropic 2D inversion for the 3D-mantle profile with stations<br />

pic001 - pic020 on top of the synthetic 3D model . . . . . . . . . . . . . 304<br />

A.12.Result of anisotropic 2D inversion for the 3D-crust profile with stations<br />

pic001 - pic020 on top of the synthetic 3D model using resistivity gradient<br />

regularisation and an increased smoothing parameter (τ = 6) . . . . . . . 305<br />

A.13.Result of anisotropic 2D inversion for the 3D-crust profile with stations<br />

pic001 - pic020 on top of the synthetic 3D model using resistivity laplacian<br />

regularisation and a lower smoothing parameter (τ = 1) . . . . . . . 306<br />

A.14.Result of anisotropic 2D inversion for the 3D-crust profile with stations<br />

pic001 - pic020 on top of the synthetic 3D model using resistivity gradient<br />

regularisation and a lower smoothing parameter (τ = 1) . . . . . . . . . . 307

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