tfrunter.tex

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% This is part of the TFTB Reference Manual.% Copyright (C) 1996 CNRS (France) and Rice University (US).% See the file refguide.tex for copying conditions.\markright{tfrunter}\hspace*{-1.6cm}{\Large \bf tfrunter}\vspace*{-.4cm}\hspace*{-1.6cm}\rule[0in]{16.5cm}{.02cm}\vspace*{.2cm}{\bf \large \fontfamily{cmss}\selectfont Purpose}\\\hspace*{1.5cm}\begin{minipage}[t]{13.5cm}Unterberger time-frequency distribution, active or passive form.\end{minipage}\vspace*{.5cm}{\bf \large \fontfamily{cmss}\selectfont Synopsis}\\\hspace*{1.5cm}\begin{minipage}[t]{13.5cm}\begin{verbatim}[tfr,t,f] = tfrunter(x)[tfr,t,f] = tfrunter(x,t)[tfr,t,f] = tfrunter(x,t,form)[tfr,t,f] = tfrunter(x,t,form,fmin,fmax)[tfr,t,f] = tfrunter(x,t,form,fmin,fmax,N)[tfr,t,f] = tfrunter(x,t,form,fmin,fmax,N,trace)\end{verbatim}\end{minipage}\vspace*{.5cm}{\bf \large \fontfamily{cmss}\selectfont Description}\\\hspace*{1.5cm}\begin{minipage}[t]{13.5cm}        {\ty tfrunter} generates the auto- or cross-Unterberger        distribution (active or passive form). The expression of the activeUnterberger distribution writes\begin{eqnarray*}U^{(a)}_x(t,a)=\frac{1}{|a|}\ \int_0^{+\infty} (1+\frac{1}{\alpha^2})\X\left(\frac{\alpha}{a}\right)\  X^*\left(\frac{1}{\alpha a}\right)\e^{j2\pi (\alpha-1/\alpha)\frac{t}{a}}\ d\alpha,       \end{eqnarray*}whereas the passive Unterberger distribution writes\begin{eqnarray*}U^{(p)}_x(t,a)=\frac{1}{|a|} \int_0^{+\infty} \frac{2}{\alpha}\X\left(\frac{\alpha}{a}\right)\ X^*\left(\frac{1}{\alpha a}\right)\e^{j2\pi (\alpha-\frac{1}{\alpha})\frac{t}{a}}\ d\alpha.       \end{eqnarray*}\hspace*{-.5cm}\begin{tabular*}{14cm}{p{1.5cm} p{8.5cm} c}Name & Description & Default value\\\hline        {\ty x} & signal (in time) to be analyzed. If {\ty x=[x1 x2]}, {\ty tfrunter}            computes the cross-Unterberger distribution {\ty (Nx=length(x))}\\        {\ty t} & time instant(s) on which the {\ty tfr} is evaluated & {\ty (1:Nx)}\\        {\ty form} & {\ty 'A'} for active, {\ty 'P'} for passive			Unterberger distribution     & {\ty 'A'}\\        {\ty fmin, fmax} & respectively lower and upper frequency bounds of            the analyzed signal. These parameters fix the equivalent            frequency bandwidth (expressed in Hz). When unspecified, you           have to enter them at the command line from the plot of the           spectrum. {\ty fmin} and {\ty fmax} must be $>${\ty 0} and $\leq${\ty 0.5}\\        {\ty N} & number of analyzed voices & auto\footnote{This value,	determined from {\ty fmin} and {\ty fmax}, is the 	next-power-of-two of the minimum value checking the non-overlapping	condition in the fast Mellin transform.}\\\hline\end{tabular*}\end{minipage} %\newpage\hspace*{1.5cm}\begin{minipage}[t]{13.5cm}\hspace*{-.5cm}\begin{tabular*}{14cm}{p{1.5cm} p{8.5cm} c}Name & Description & Default value\\\hline        {\ty trace} & if nonzero, the progression of the algorithm is shown                                                & {\ty 0}\\        \hline {\ty tfr} & time-frequency matrix containing the coefficients of the            decomposition (abscissa correspond to uniformly sampled           time, and ordinates correspond to a geometrically sampled            frequency). First row of {\ty tfr} corresponds to the lowest            frequency. \\        {\ty f} & vector of normalized frequencies (geometrically sampled            from {\ty fmin} to {\ty fmax})\\\hline\end{tabular*}\vspace*{.2cm}When called without output arguments, {\ty tfrunter} runs {\ty tfrqview}.\end{minipage}\vspace*{1cm}{\bf \large \fontfamily{cmss}\selectfont Example}\begin{verbatim}         sig=altes(64,0.1,0.45);          tfrunter(sig);\end{verbatim}\vspace*{.5cm}{\bf \large \fontfamily{cmss}\selectfont See Also}\\\hspace*{1.5cm}\begin{minipage}[t]{13.5cm}all the {\ty tfr*} functions.\end{minipage}\vspace*{.5cm}{\bf \large \fontfamily{cmss}\selectfont References}\\\hspace*{1.5cm}\begin{minipage}[t]{13.5cm}[1] A. Unterberger ``The Calculus of Pseudo-Differential Operators of FuchsType'' Comm. in Part. Diff. Eq., Vol. 9, pp. 1179-1236, 1984.\\[2] P. Flandrin, P. Gon鏰lv鑣 ``Geometry of Affine Time-FrequencyDistributions'' Applied and Computational Harmonic Analysis, Vol. 3,pp. 10-39, January 1996.\end{minipage}

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