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Investigations of Faraday Rotation Maps of Extended Radio Sources ...

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28 CHAPTER 1. INTRODUCTION<br />

where n is the dimension <strong>of</strong> θ and det V indicates the determinant. It is noteworthy<br />

that Eq. (1.88) is exact when y(µ xi , θ) depends linearly on the various θ i .<br />

The likelihood function can also be used as a power spectrum estimator since such<br />

an estimator has to minimise the variance. If one identifies the covariance matrix as<br />

defined by Eq. (1.60) and assuming the mean to be zero 〈y i 〉 = 0, the likelihood<br />

function changes<br />

L(θ; x) =<br />

[<br />

1<br />

(2π) N/2 (det C) 1/2 exp − 1 ]<br />

2 ∆T C −1 ∆ , (1.89)<br />

where C is the covariance matrix, which expresses the theoretical expectations and<br />

dependents on the model parameters, ∆ i are the data and N is the dimension <strong>of</strong> the<br />

covariance matrix.<br />

1.4.4 Structure <strong>of</strong> the Thesis<br />

The interpretation <strong>of</strong> the <strong>Faraday</strong> rotation data as being associated with an external<br />

<strong>Faraday</strong> screen has been challenged several times and is subject to a broad discussion.<br />

Therefore, Chapter 2 is devoted to this question. After being confident <strong>of</strong> the<br />

interpretation as <strong>Faraday</strong> rotation being external to the source, Chapter 3 describes<br />

the application <strong>of</strong> autocorrelation and power spectrum analysis to the <strong>Faraday</strong> rotation<br />

data. However, it was realised that the map making algorithm might produce artefacts<br />

related to the mentioned nπ-ambiguity influencing this analysis significantly. Therefore,<br />

in Chapter 4 a new RM map-making algorithm called Pacman is introduced<br />

and compared to the standard algorithms. Finally, motivated by the recent and great<br />

success <strong>of</strong> maximum likelihood methods in the determination <strong>of</strong> power spectra, this<br />

method is applied to <strong>Faraday</strong> rotation data in Chapter 5.

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