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Separating Horn Output from Base Leakage

Note that Fig.3.16 indicates the existence of fixed and angle-dependent components in the measured impulse responses. An iterative algorithm was developed to model the two components separately [477].

Let $ M=256$ denote the number of impulse-response samples in each measured impulse response,and let $ N=25$ denote the number of angles (-180:15:180) at which impulse-response measurements were taken. We denote the $ M\times N$ impulse-response matrix by $ {\mathbf{h}}$. Each column of $ {\mathbf{h}}$ is an impulse response at some horn angle. (Figure 3.16 can be interpreted as a plot of the transpose of $ {\mathbf{h}}$.)

We model $ {\mathbf{h}}$ as

$\displaystyle {\mathbf{h}}=$   $\displaystyle \mbox{${\bm \alpha}$}$$\displaystyle +$   $\displaystyle \mbox{${\bm \gamma}$}$$\displaystyle \cdot$   diag$\displaystyle (z^{-\tau_i}) + {\mathbf{e}}
$

where $ \tau_i$ is the arrival-time delay, in samples, for the horn output in the $ i$th row (the delays clearly visible in Fig.3.16 as a function of angle). These arrival times are estimated as the location of the peak in the cross-correlation between the $ i$th impulse response and the same impulse response after converting it to