Syncing to home.
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55
main.tex
55
main.tex
@@ -610,16 +610,16 @@ This effect is more pronounced for lower $\fc$ of the lowpass filter and is
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presumably caused by the attenuation of high-frequency components in the
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signal, which are more prominent in the noise component $\noc(t)$ than in the
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song component $\soc(t)$. The effect also appears relatively consistent across
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different species, although small variations based on different song structures
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and distributions exist~(Fig.\,\ref{fig:rect-lp}e). In summary, the standard
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deviation of $\env(t)$ has never been observed to transition into a saturation
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regime for larger $\sca$ but rather continues to increase proportionally to
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$\sca$ for all tested $\fc$, in both the noiseless and the noisy case and
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across different species. Consequently, the combination of rectification and
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lowpass filtering does not contribute to intensity invariance. However, this
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transformation pair does improve the SNR of $\env(t)$ relative to $\filt(t)$
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and thus provides subsequent processing stages with a more robust input
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representation and higher input SNR.
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different species, although small variations exist~(Fig.\,\ref{fig:rect-lp}e)
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that are presumably based on different song structures and frequency spectra.
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In summary, the standard deviation of $\env(t)$ has never been observed to
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transition into a saturation regime for larger $\sca$ but rather continues to
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increase proportionally to $\sca$ for all tested $\fc$, in both the noiseless
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and the noisy case and across different species. Consequently, the combination
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of rectification and lowpass filtering does not contribute to intensity
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invariance. However, this transformation pair does improve the SNR of $\env(t)$
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relative to $\filt(t)$ and thus provides subsequent processing stages with a
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more robust input representation and higher input SNR.
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\begin{figure}[!ht]
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\centering
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@@ -880,7 +880,21 @@ the SNR of $\adapt(t)$ are much less understood and likely relate to properties
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of the signal, whereas the SNR of $f(t)$ depends on the choice of $\Theta$ and
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can be more directly manipulated by the system.
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Finally,
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Finally, the effects of thresholding and temporal averaging must be seen in the
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context of the previous transformation pair of logarithmic compression and
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adaptation.
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Finally, the question remains whether the intensity-invariant output $\adapt(t)$
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of the previous transformation pair allows feature
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Finally, the output $\adapt(t)$ of the previous transformation
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pair~(Fig.\,\ref{fig:log-hp}cd) can be related to the input $\adapt(t)$ of the
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current transformation pair by plotting the values of $f(t)$ over the standard
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deviation of input $\adapt(t)$ instead of
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$\sca$~(Fig.\,\ref{fig:thresh-lp_single}f). This is relevant because, unlike
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$\sca$, the standard deviation of $\adapt(t)$ is capped to a maximum value of
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around 10\,dB by the previous transformation pair~(Fig.\,\ref{fig:log-hp}cd)
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\begin{figure}[!ht]
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\centering
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@@ -904,14 +918,17 @@ Finally,
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same $\adapt(t)$ from \textbf{a} but with different
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$\Theta$.
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\textbf{Right}:~Average value $\mu_f$ of $f(t)$ for each
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$\Theta$ from \textbf{b\,-\,d}, once for the noisy case
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(solid lines) and once for the noiseless case (dotted
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lines). Dots indicate $95\,\%$ curve span (noisy case).
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\textbf{e}:~$\mu_f$ over a range of $\sca$.
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\textbf{f}:~$\mu_f$ over the standard deviation of noisy
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input $\adapt$ corresponding to the values of $\sca$ shown
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in \textbf{e}.
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% Why plot noiseless case over SD of noisy input? Omit?
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$\Theta$ from \textbf{b\,-\,d}. Dots indicate $95\,\%$
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curve span (noisy case).
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\textbf{e}:~$\mu_f$ over a range of $\sca$, once for the
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noisy case (solid lines) and once for the noiseless case
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(dotted lines).
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\textbf{f}:~Noisy case: $\mu_f$ over the standard
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deviation of input $\adapt$ corresponding to the values of
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$\sca$ shown in \textbf{e}. Shaded area indicates standard
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deviations that would be capped in the output $\adapt(t)$
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of the previous transformation pair (see
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Fig.\,\ref{fig:log-hp}cd).
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}
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\label{fig:thresh-lp_single}
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\end{figure}
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