Syncing to home.

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j-hartling
2026-05-05 18:19:09 +02:00
parent 05e808ba30
commit a48457d967
9 changed files with 189 additions and 151 deletions

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