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P. Schmoldt, PhD - MTNet - DIAS

P. Schmoldt, PhD - MTNet - DIAS

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8.2. Generating synthetic 3D model data<br />

Fig. 8.3.: Subsurface model with orthogonal geoelectric strike directions at crust and mantle depths. Constructed to derive an optimised<br />

1D or 2D inversion approach that provides an optimal recovery of the resistivity distribution at mantle depth for such a case of oblique<br />

strike directions in crust and mantle. The approximate location of the projected PICASSO Phase I profile is indicated by the dashed<br />

line.<br />

impedance values of each station, i.e. a variance of 10 −21 . This step is required to permit<br />

subsequent calculations, which otherwise would fail due to attempted divisions by zero.<br />

Performance of the different approaches for datasets with higher noise levels is studied at<br />

a later stage of this investigation. From those files with minuscule uncertainty levels two<br />

different types of datasets are created, i.e ‘rotated’ and ‘decomposed’, which are used for<br />

anisotropic and isotropic inversion processes, respectively (see Sec. 8.3).<br />

Creation of the first dataset type simply involves rotating of data from all stations to<br />

N45W and N45E using a script by Xavier Garcia (personal communication, 2008). Note<br />

that N45W and N45E represent the respective strike directions of crust and mantle, and<br />

that TE and TM modes are swapped for datasets with a difference of rotation by 90 degrees.<br />

For these rotated datasets, diagonal elements of the impedance tensor are in general<br />

non-zero and are used for the novel anisotropic inversion approach.<br />

The second type of data (decomposed) is created using the program strike by Mc-<br />

Neice and Jones [2001], based on the theory by Groom and Bailey [1989] (Sec. 4.4.4),<br />

commonly used to provide datasets suitable for isotropic 2D inversion. Therein, two<br />

datasets are generated that are adequate for the strike directions at either crustal or mantle<br />

depth, i.e. N45E and N45W, respectively. For these decomposed datasets, the diagonal<br />

elements of the impedance tensor (Zxx and Zyy) are considered insignificant and are not<br />

used during isotropic 2D inversion.<br />

Prior to inversion of forward responses from the synthetic 3D model, data are analysed<br />

to identify characteristics of the responses which help to understand applicability of the<br />

different inversion approaches. First the response data are visualised using maps of four<br />

different periods (periods are used as a depths proxy, cf. Section 6.3.1), in which North<br />

is located towards the top left (Fig. 8.6); figures are rotated anticlockwise by 45 degrees<br />

173

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