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P. Schmoldt, PhD - MTNet - DIAS

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10. Data inversion<br />

Depth (km)<br />

S<br />

0<br />

50<br />

100<br />

150<br />

Campo de Montiel M.P. Loranca Basin N<br />

pic020<br />

pic019<br />

pic017<br />

pic015<br />

pic013<br />

pic011<br />

200<br />

200<br />

-100 -50 0 50 100<br />

Distance from centre of profile (km)<br />

pic009<br />

pic007<br />

pic005<br />

pic004<br />

pic003<br />

pic002<br />

pic001<br />

0<br />

50<br />

100<br />

150<br />

3D MT inversion<br />

Tajo Basin<br />

Resistivity log 10(Wm)<br />

0 0.8 1.6 2.4 3.2<br />

36ON A.D.<br />

N<br />

100 km<br />

Seismic tomography<br />

Betics Tajo Basin<br />

dP-wave velocity<br />

-2.5% +2.5%<br />

Fig. 10.33.: Comparison of the isotropic 3D inversion result of PICASSO Phase I station responses in the Tajo Basin (left) and a<br />

seismic tomography transect extracted from the global P-wave velocity model of Amaru [2007] (bottom-right); similar seismic results<br />

are obtained by Hoernle et al. [1995], Bijwaard et al. [1998], and Villaseñor et al. [2007] for the same region (cf. Chap. 7). Location<br />

of the PICASSO Phase I stations and course of the profile on top of the inversion mesh are shown on the top-right of this figure,<br />

next to a map of the Iberian Peninsula in which the PICASSO Phase I profile in the Tajo Basin is indicated by a red line. Geological<br />

regions, based on the USGS EnVision map for Europe (Figure 9.1), are shown on the top of the MT inversion model (M.P: Manchega<br />

Plain). The location of the MT inversion model in respect to the seismic transect is indicated by the dashed black lines on top of the<br />

seismic model. The dotted green line indicates the upper range of the low velocity region beneath the Tajo Basin (plotted on top of<br />

the seismic as well as on the MT model). Yellow lines represent potential fluid migration paths that may originate from dehydration<br />

of the subducting slab beneath Alboran Domain (A.D.) and Betics (indicated by high velocity feature in the seismic inset) and intrude<br />

into the lithosphere beneath the Tajo Basin; see text for details. White dashed and dotted-dashed lines on top of the MT inversion<br />

model indicate inferred approximate location of the crust-mantle and the lithosphere–asthenosphere boundary (LAB), respectively (cf.<br />

Chapter 7 and Section 8.3.3). Structure at crustal depth are not strongly constrained because the focus of this isotropic 3D inversion<br />

was on investigating mantle structures, whereas characteristics of sublithospheric regions are not strongly constrained by the inversion<br />

due to the low signal-to-noise ratio of related impedance estimates (the location of these weakly constrained regions are indicated by<br />

shaded areas); see text for further details.<br />

vides useful insights about the source of the high conductivity – low velocity anomaly in<br />

the middle and lower crust beneath the Campo de Montiel region (feature ‘f’ in Figure<br />

10.6). In the 3D inversion result, the crustal anomaly is modelled to the west of stations<br />

pic015 – pic019 at a depth of approximately 10 – 25 km (cf. Fig. 10.34), which is in<br />

excellent agreement with induction arrow directions (Figure 10.12) and results of the ambient<br />

noise tomography study by Villaseñor et al. [2007] (Figs. 7.21 and 10.11). Hence,<br />

3D inversion is supporting previous conclusions that this high conductivity anomaly is a<br />

relatively small-scale feature and correlated with the low seismic velocity anomaly; see<br />

Section 10.1.5 for a discussion of this feature.<br />

272<br />

100<br />

300<br />

500<br />

41 O N<br />

100<br />

300<br />

500<br />

Depth (km)

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