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@node Signal Processing
@chapter Signal Processing

This chapter describes the signal processing and fast Fourier
transform functions available in Octave.  Fast Fourier transforms are
computed with the @sc{fftw} or @sc{fftpack} libraries depending on how
Octave is built.

@c fft libinterp/corefcn/fft.cc
@anchor{XREFfft}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{y} =} fft (@var{x})
@deftypefnx {} {@var{y} =} fft (@var{x}, @var{n})
@deftypefnx {} {@var{y} =} fft (@var{x}, @var{n}, @var{dim})
Compute the discrete Fourier transform of @var{x} using
a Fast Fourier Transform (FFT) algorithm.

The FFT is calculated along the first non-singleton dimension of the
array.  Thus if @var{x} is a matrix, @code{fft (@var{x})} computes the
FFT for each column of @var{x}.

If called with two arguments, @var{n} is expected to be an integer
specifying the number of elements of @var{x} to use, or an empty
matrix to specify that its value should be ignored.  If @var{n} is
larger than the dimension along which the FFT is calculated, then
@var{x} is resized and padded with zeros.  Otherwise, if @var{n} is
smaller than the dimension along which the FFT is calculated, then
@var{x} is truncated.

If called with three arguments, @var{dim} is an integer specifying the
dimension of the matrix along which the FFT is performed.
@xseealso{@ref{XREFifft,,ifft}, @ref{XREFfft2,,fft2}, @ref{XREFfftn,,fftn}, @ref{XREFfftw,,fftw}}
@end deftypefn


@c ifft libinterp/corefcn/fft.cc
@anchor{XREFifft}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{x} =} ifft (@var{y})
@deftypefnx {} {@var{x} =} ifft (@var{y}, @var{n})
@deftypefnx {} {@var{x} =} ifft (@var{y}, @var{n}, @var{dim})
Compute the inverse discrete Fourier transform of @var{y}
using a Fast Fourier Transform (FFT) algorithm.

The inverse FFT is calculated along the first non-singleton dimension
of the array.  Thus if @var{y} is a matrix, @code{ifft (@var{y})} computes
the inverse FFT for each column of @var{y}.

If called with two arguments, @var{n} is expected to be an integer
specifying the number of elements of @var{y} to use, or an empty
matrix to specify that its value should be ignored.  If @var{n} is
larger than the dimension along which the inverse FFT is calculated, then
@var{y} is resized and padded with zeros.  Otherwise, if @var{n} is
smaller than the dimension along which the inverse FFT is calculated,
then @var{y} is truncated.

If called with three arguments, @var{dim} is an integer specifying the
dimension of the matrix along which the inverse FFT is performed.
@xseealso{@ref{XREFfft,,fft}, @ref{XREFifft2,,ifft2}, @ref{XREFifftn,,ifftn}, @ref{XREFfftw,,fftw}}
@end deftypefn


@c fft2 libinterp/corefcn/fft2.cc
@anchor{XREFfft2}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{B} =} fft2 (@var{A})
@deftypefnx {} {@var{B} =} fft2 (@var{A}, @var{m}, @var{n})
Compute the two-dimensional discrete Fourier transform of @var{A} using
a Fast Fourier Transform (FFT) algorithm.

The optional arguments @var{m} and @var{n} may be used specify the number of
rows and columns of @var{A} to use.  If either of these is larger than the
size of @var{A}, @var{A} is resized and padded with zeros.

If @var{A} is a multi-dimensional matrix, each two-dimensional sub-matrix
of @var{A} is treated separately.
@xseealso{@ref{XREFifft2,,ifft2}, @ref{XREFfft,,fft}, @ref{XREFfftn,,fftn}, @ref{XREFfftw,,fftw}}
@end deftypefn


@c ifft2 libinterp/corefcn/fft2.cc
@anchor{XREFifft2}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{A} =} ifft2 (@var{B})
@deftypefnx {} {@var{A} =} ifft2 (@var{B}, @var{m}, @var{n})
Compute the inverse two-dimensional discrete Fourier transform of @var{B}
using a Fast Fourier Transform (FFT) algorithm.

The optional arguments @var{m} and @var{n} may be used specify the number of
rows and columns of @var{B} to use.  If either of these is larger than the
size of @var{B}, @var{B} is resized and padded with zeros.

If @var{B} is a multi-dimensional matrix, each two-dimensional sub-matrix
of @var{B} is treated separately.
@xseealso{@ref{XREFfft2,,fft2}, @ref{XREFifft,,ifft}, @ref{XREFifftn,,ifftn}, @ref{XREFfftw,,fftw}}
@end deftypefn


@c fftn libinterp/corefcn/fftn.cc
@anchor{XREFfftn}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{B} =} fftn (@var{A})
@deftypefnx {} {@var{B} =} fftn (@var{A}, @var{size})
Compute the N-dimensional discrete Fourier transform of @var{A} using
a Fast Fourier Transform (FFT) algorithm.

The optional vector argument @var{size} may be used specify the dimensions
of the array to be used.  If an element of @var{size} is smaller than the
corresponding dimension of @var{A}, then the dimension of @var{A} is
truncated prior to performing the FFT@.  Otherwise, if an element of
@var{size} is larger than the corresponding dimension then @var{A} is
resized and padded with zeros.
@xseealso{@ref{XREFifftn,,ifftn}, @ref{XREFfft,,fft}, @ref{XREFfft2,,fft2}, @ref{XREFfftw,,fftw}}
@end deftypefn


@c ifftn libinterp/corefcn/fftn.cc
@anchor{XREFifftn}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{A} =} ifftn (@var{B})
@deftypefnx {} {@var{A} =} ifftn (@var{B}, @var{size})
Compute the inverse N-dimensional discrete Fourier transform of @var{B}
using a Fast Fourier Transform (FFT) algorithm.

The optional vector argument @var{size} may be used specify the dimensions
of the array to be used.  If an element of @var{size} is smaller than the
corresponding dimension of @var{B}, then the dimension of @var{B} is
truncated prior to performing the inverse FFT@.  Otherwise, if an element of
@var{size} is larger than the corresponding dimension then @var{B} is
resized and padded with zeros.
@xseealso{@ref{XREFfftn,,fftn}, @ref{XREFifft,,ifft}, @ref{XREFifft2,,ifft2}, @ref{XREFfftw,,fftw}}
@end deftypefn


Octave uses the @sc{fftw} libraries to perform FFT computations.  When Octave
starts up and initializes the @sc{fftw} libraries, they read a system wide
file (on a Unix system, it is typically @file{/etc/fftw/wisdom}) that
contains information useful to speed up FFT computations.  This
information is called the @emph{wisdom}.  The system-wide file allows
wisdom to be shared between all applications using the @sc{fftw} libraries.

Use the @code{fftw} function to generate and save wisdom.  Using the
utilities provided together with the @sc{fftw} libraries
(@command{fftw-wisdom} on Unix systems), you can even add wisdom
generated by Octave to the system-wide wisdom file.

@c fftw libinterp/dldfcn/fftw.cc
@anchor{XREFfftw}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{method} =} fftw ("planner")
@deftypefnx {} {} fftw ("planner", @var{method})
@deftypefnx {} {@var{wisdom} =} fftw ("dwisdom")
@deftypefnx {} {} fftw ("dwisdom", @var{wisdom})
@deftypefnx {} {@var{nthreads} =} fftw ("threads")
@deftypefnx {} {} fftw ("threads", @var{nthreads})

Manage @sc{fftw} wisdom data.

Wisdom data can be used to significantly accelerate the calculation of the
FFTs, but implies an initial cost in its calculation.  When the @sc{fftw}
libraries are initialized, they read a system wide wisdom file (typically in
@file{/etc/fftw/wisdom}), allowing wisdom to be shared between applications
other than Octave.  Alternatively, the @code{fftw} function can be used to
import wisdom.  For example,

@example
@var{wisdom} = fftw ("dwisdom")
@end example

@noindent
will save the existing wisdom used by Octave to the string @var{wisdom}.
This string can then be saved to a file and restored using the @code{save}
and @code{load} commands respectively.  This existing wisdom can be
re-imported as follows

@example
fftw ("dwisdom", @var{wisdom})
@end example

If @var{wisdom} is an empty string, then the wisdom used is cleared.

During the calculation of Fourier transforms further wisdom is generated.
The fashion in which this wisdom is generated is also controlled by
the @code{fftw} function.  There are five different manners in which the
wisdom can be treated:

@table @asis
@item @qcode{"estimate"}
Specifies that no run-time measurement of the optimal means of
calculating a particular is performed, and a simple heuristic is used
to pick a (probably sub-optimal) plan.  The advantage of this method is
that there is little or no overhead in the generation of the plan, which
is appropriate for a Fourier transform that will be calculated once.

@item @qcode{"measure"}
In this case a range of algorithms to perform the transform is considered
and the best is selected based on their execution time.

@item @qcode{"patient"}
Similar to @qcode{"measure"}, but a wider range of algorithms is
considered.

@item @qcode{"exhaustive"}
Like @qcode{"measure"}, but all possible algorithms that may be used to
treat the transform are considered.

@item @qcode{"hybrid"}
As run-time measurement of the algorithm can be expensive, this is a
compromise where @qcode{"measure"} is used for transforms up to the size
of 8192 and beyond that the @qcode{"estimate"} method is used.
@end table

The default method is @qcode{"estimate"}.  The current method can
be queried with

@example
@var{method} = fftw ("planner")
@end example

@noindent
or set by using

@example
fftw ("planner", @var{method})
@end example

Note that calculated wisdom will be lost when restarting Octave.  However,
the wisdom data can be reloaded if it is saved to a file as described
above.  Saved wisdom files should not be used on different platforms since
they will not be efficient and the point of calculating the wisdom is lost.

The number of threads used for computing the plans and executing the
transforms can be set with

@example
fftw ("threads", @var{NTHREADS})
@end example

Note that Octave must be compiled with multi-threaded @sc{fftw} support for
this feature.  By default, the number of (logical) processors available to the
current process or @var{3} is used (whichever is smaller).

@xseealso{@ref{XREFfft,,fft}, @ref{XREFifft,,ifft}, @ref{XREFfft2,,fft2}, @ref{XREFifft2,,ifft2}, @ref{XREFfftn,,fftn}, @ref{XREFifftn,,ifftn}}
@end deftypefn


@c fftconv scripts/signal/fftconv.m
@anchor{XREFfftconv}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{c} =} fftconv (@var{x}, @var{y})
@deftypefnx {} {@var{c} =} fftconv (@var{x}, @var{y}, @var{n})
Convolve two vectors using the FFT for computation.

@code{c = fftconv (@var{x}, @var{y})} returns a vector of length equal to
@code{length (@var{x}) + length (@var{y}) - 1}.  If @var{x} and @var{y}
are the coefficient vectors of two polynomials, the returned value is the
coefficient vector of the product polynomial.

The computation uses the FFT by calling the function @code{fftfilt}.  If
the optional argument @var{n} is specified, an N-point FFT is used.
@xseealso{@ref{XREFdeconv,,deconv}, @ref{XREFconv,,conv}, @ref{XREFconv2,,conv2}}
@end deftypefn


@c fftfilt scripts/signal/fftfilt.m
@anchor{XREFfftfilt}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{y} =} fftfilt (@var{b}, @var{x})
@deftypefnx {} {@var{y} =} fftfilt (@var{b}, @var{x}, @var{n})
Filter @var{x} with the FIR filter @var{b} using the FFT.

If @var{x} is a matrix, filter each column of the matrix.

Given the optional third argument, @var{n}, @code{fftfilt} uses the
overlap-add method to filter @var{x} with @var{b} using an N-point FFT@.
The FFT size must be an even power of 2 and must be greater than or equal to
the length of @var{b}.  If the specified @var{n} does not meet these
criteria, it is automatically adjusted to the nearest value that does.

@xseealso{@ref{XREFfilter,,filter}, @ref{XREFfilter2,,filter2}}
@end deftypefn


@c filter libinterp/corefcn/filter.cc
@anchor{XREFfilter}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{y} =} filter (@var{b}, @var{a}, @var{x})
@deftypefnx {} {[@var{y}, @var{sf}] =} filter (@var{b}, @var{a}, @var{x}, @var{si})
@deftypefnx {} {[@var{y}, @var{sf}] =} filter (@var{b}, @var{a}, @var{x}, [], @var{dim})
@deftypefnx {} {[@var{y}, @var{sf}] =} filter (@var{b}, @var{a}, @var{x}, @var{si}, @var{dim})
Apply a 1-D digital filter to the data @var{x}.

@code{filter} returns the solution to the following linear, time-invariant
difference equation:
@tex
$$
\sum_{k=0}^N a_{k+1} y_{n-k} = \sum_{k=0}^M b_{k+1} x_{n-k}, \qquad
 1 \le n \le P
$$
@end tex
@ifnottex
@c Set example in small font to prevent overfull line

@smallexample
@group
 N                   M
SUM a(k+1) y(n-k) = SUM b(k+1) x(n-k)    for 1<=n<=length(x)
k=0                 k=0
@end group
@end smallexample

@end ifnottex

@noindent
where
@ifnottex
N=length(a)-1 and M=length(b)-1.
@end ifnottex
@tex
$a \in \Re^{N-1}$, $b \in \Re^{M-1}$, and $x \in \Re^P$.
@end tex
The result is calculated over the first non-singleton dimension of @var{x}
or over @var{dim} if supplied.

An equivalent form of the equation is:
@tex
$$
y_n = -\sum_{k=1}^N c_{k+1} y_{n-k} + \sum_{k=0}^M d_{k+1} x_{n-k}, \qquad
 1 \le n \le P
$$
@end tex
@ifnottex
@c Set example in small font to prevent overfull line

@smallexample
@group
          N                   M
y(n) = - SUM c(k+1) y(n-k) + SUM d(k+1) x(n-k)  for 1<=n<=length(x)
         k=1                 k=0
@end group
@end smallexample

@end ifnottex

@noindent
where
@ifnottex
 c = a/a(1) and d = b/a(1).
@end ifnottex
@tex
$c = a/a_1$ and $d = b/a_1$.
@end tex

If the fourth argument @var{si} is provided, it is taken as the
initial state of the system and the final state is returned as
@var{sf}.  The state vector is a column vector whose length is
equal to the length of the longest coefficient vector minus one.
If @var{si} is not supplied, the initial state vector is set to all
zeros.

In terms of the Z Transform, @var{y} is the result of passing the
discrete-time signal @var{x} through a system characterized by the following
rational system function:
@tex
$$
H(z) = {\displaystyle\sum_{k=0}^M d_{k+1} z^{-k}
        \over 1 + \displaystyle\sum_{k+1}^N c_{k+1} z^{-k}}
$$
@end tex
@ifnottex

@example
@group
          M
         SUM d(k+1) z^(-k)
         k=0
H(z) = ---------------------
            N
       1 + SUM c(k+1) z^(-k)
           k=1
@end group
@end example

@end ifnottex
@xseealso{@ref{XREFfilter2,,filter2}, @ref{XREFfftfilt,,fftfilt}, @ref{XREFfreqz,,freqz}}
@end deftypefn


@c filter2 scripts/signal/filter2.m
@anchor{XREFfilter2}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{y} =} filter2 (@var{b}, @var{x})
@deftypefnx {} {@var{y} =} filter2 (@var{b}, @var{x}, @var{shape})
Apply the 2-D FIR filter @var{b} to @var{x}.

If the argument @var{shape} is specified, return an array of the desired
shape.  Possible values are:

@table @asis
@item @qcode{"full"}
pad @var{x} with zeros on all sides before filtering.

@item @qcode{"same"}
unpadded @var{x} (default)

@item @qcode{"valid"}
trim @var{x} after filtering so edge effects are no included.
@end table

Note this is just a variation on convolution, with the parameters reversed
and @var{b} rotated 180 degrees.
@xseealso{@ref{XREFconv2,,conv2}}
@end deftypefn


@c freqz scripts/signal/freqz.m
@anchor{XREFfreqz}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {[@var{h}, @var{w}] =} freqz (@var{b}, @var{a}, @var{n}, "whole")
@deftypefnx {} {[@var{h}, @var{w}] =} freqz (@var{b})
@deftypefnx {} {[@var{h}, @var{w}] =} freqz (@var{b}, @var{a})
@deftypefnx {} {[@var{h}, @var{w}] =} freqz (@var{b}, @var{a}, @var{n})
@deftypefnx {} {@var{h} =} freqz (@var{b}, @var{a}, @var{w})
@deftypefnx {} {[@var{h}, @var{w}] =} freqz (@dots{}, @var{Fs})
@deftypefnx {} {} freqz (@dots{})

Return the complex frequency response @var{h} of the rational IIR filter
whose numerator and denominator coefficients are @var{b} and @var{a},
respectively.

The response is evaluated at @var{n} angular frequencies between 0 and
@ifnottex
2*pi.
@end ifnottex
@tex
$2\pi$.
@end tex

@noindent
The output value @var{w} is a vector of the frequencies.

If @var{a} is omitted, the denominator is assumed to be 1 (this
corresponds to a simple FIR filter).

If @var{n} is omitted, a value of 512 is assumed.  For fastest computation,
@var{n} should factor into a small number of small primes.

If the fourth argument, @qcode{"whole"}, is omitted the response is
evaluated at frequencies between 0 and
@ifnottex
pi.
@end ifnottex
@tex
$\pi$.
@end tex

@code{freqz (@var{b}, @var{a}, @var{w})}

Evaluate the response at the specific frequencies in the vector @var{w}.
The values for @var{w} are measured in radians.

@code{[@dots{}] = freqz (@dots{}, @var{Fs})}

Return frequencies in Hz instead of radians assuming a sampling rate
@var{Fs}.  If you are evaluating the response at specific frequencies
@var{w}, those frequencies should be requested in Hz rather than radians.

@code{freqz (@dots{})}

Plot the magnitude and phase response of @var{h} rather than returning them.

@xseealso{@ref{XREFfreqz_plot,,freqz_plot}}
@end deftypefn


@c freqz_plot scripts/signal/freqz_plot.m
@anchor{XREFfreqz_plot}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {} freqz_plot (@var{w}, @var{h})
@deftypefnx {} {} freqz_plot (@var{w}, @var{h}, @var{freq_norm})
Plot the magnitude and phase response of @var{h}.

If the optional @var{freq_norm} argument is true, the frequency vector
@var{w} is in units of normalized radians.  If @var{freq_norm} is false, or
not given, then @var{w} is measured in Hertz.
@xseealso{@ref{XREFfreqz,,freqz}}
@end deftypefn


@c sinc scripts/signal/sinc.m
@anchor{XREFsinc}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{y} =} sinc (@var{x})
Compute the sinc function.

Return
@tex
$ \sin (\pi x)/(\pi x)$.
@end tex
@ifnottex
sin (pi*x) / (pi*x).
@end ifnottex
@end deftypefn


@c unwrap scripts/signal/unwrap.m
@anchor{XREFunwrap}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{b} =} unwrap (@var{x})
@deftypefnx {} {@var{b} =} unwrap (@var{x}, @var{tol})
@deftypefnx {} {@var{b} =} unwrap (@var{x}, @var{tol}, @var{dim})
Unwrap radian phases by adding or subtracting multiples of 2*pi as
appropriate to remove jumps greater than @var{tol}.

@var{tol} defaults to pi.

@code{unwrap} will work along the dimension @var{dim}.  If @var{dim}
is unspecified it defaults to the first non-singleton dimension.

@code{unwrap} ignores all non-finite input values (Inf, NaN, NA).

@end deftypefn


@c FIXME: someone needs to organize these ...

@c arch_fit scripts/signal/arch_fit.m
@anchor{XREFarch_fit}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {[@var{a}, @var{b}] =} arch_fit (@var{y}, @var{x}, @var{p}, @var{iter}, @var{gamma}, @var{a0}, @var{b0})
Fit an ARCH regression model to the time series @var{y} using the scoring
algorithm in @nospell{Engle's} original ARCH paper.

The model is

@example
@group
y(t) = b(1) * x(t,1) + @dots{} + b(k) * x(t,k) + e(t),
h(t) = a(1) + a(2) * e(t-1)^2 + @dots{} + a(p+1) * e(t-p)^2
@end group
@end example

@noindent
in which @math{e(t)} is @math{N(0, h(t))}, given a time-series vector
@var{y} up to time @math{t-1} and a matrix of (ordinary) regressors @var{x}
up to @math{t}.  The order of the regression of the residual variance is
specified by @var{p}.

If invoked as @code{arch_fit (@var{y}, @var{k}, @var{p})} with a positive
integer @var{k}, fit an ARCH(@var{k}, @var{p}) process, i.e., do the above
with the @math{t}-th row of @var{x} given by

@example
[1, y(t-1), @dots{}, y(t-k)]
@end example

Optionally, one can specify the number of iterations @var{iter}, the
updating factor @var{gamma}, and initial values @math{a0} and @math{b0}
for the scoring algorithm.
@end deftypefn


@c arch_rnd scripts/signal/arch_rnd.m
@anchor{XREFarch_rnd}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{y} =} arch_rnd (@var{a}, @var{b}, @var{t})
Simulate an ARCH sequence of length @var{t} with AR coefficients @var{b} and
CH coefficients @var{a}.

The result @math{y(t)} follows the model
@c Set example in small font to prevent overfull line

@smallexample
y(t) = b(1) + b(2) * y(t-1) + @dots{} + b(lb) * y(t-lb+1) + e(t),
@end smallexample

@noindent
where @math{e(t)}, given @var{y} up to time @math{t-1}, is
@math{N(0, h(t))}, with
@c Set example in small font to prevent overfull line

@smallexample
h(t) = a(1) + a(2) * e(t-1)^2 + @dots{} + a(la) * e(t-la+1)^2
@end smallexample
@end deftypefn


@c arch_test scripts/signal/arch_test.m
@anchor{XREFarch_test}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {[@var{pval}, @var{lm}] =} arch_test (@var{y}, @var{x}, @var{p})
For a linear regression model

@example
y = x * b + e
@end example

@noindent
perform a Lagrange Multiplier (LM) test of the null hypothesis of no
conditional heteroscedascity against the alternative of CH(@var{p}).

I.e., the model is

@example
y(t) = b(1) * x(t,1) + @dots{} + b(k) * x(t,k) + e(t),
@end example

@noindent
given @var{y} up to @math{t-1} and @var{x} up to @math{t},
@math{e}(t) is @math{N(0, h(t))} with

@example
h(t) = v + a(1) * e(t-1)^2 + @dots{} + a(p) * e(t-p)^2,
@end example

@noindent
and the null is @math{a(1)} == @dots{} == @math{a(p)} == 0.

If the second argument is a scalar integer, @math{k}, perform the same
test in a linear autoregression model of order @math{k}, i.e., with

@example
[1, y(t-1), @dots{}, y(t-@var{k})]
@end example

@noindent
as the @math{t}-th row of @var{x}.

Under the null, LM approximately has a chisquare distribution with
@var{p} degrees of freedom and @var{pval} is the @math{p}-value (1
minus the CDF of this distribution at LM) of the test.

If no output argument is given, the @math{p}-value is displayed.
@end deftypefn


@c arma_rnd scripts/signal/arma_rnd.m
@anchor{XREFarma_rnd}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{x} =} arma_rnd (@var{a}, @var{b}, @var{v}, @var{t}, @var{n})
Return a simulation of the ARMA model.

The ARMA model is defined by

@example
@group
x(n) = a(1) * x(n-1) + @dots{} + a(k) * x(n-k)
     + e(n) + b(1) * e(n-1) + @dots{} + b(l) * e(n-l)
@end group
@end example

@noindent
in which @var{k} is the length of vector @var{a}, @var{l} is the length of
vector @var{b} and @var{e} is Gaussian white noise with variance @var{v}.
The function returns a vector of length @var{t}.

The optional parameter @var{n} gives the number of dummy @var{x}(@var{i})
used for initialization, i.e., a sequence of length @var{t}+@var{n} is
generated and @var{x}(@var{n}+1:@var{t}+@var{n}) is returned.  If @var{n}
is omitted, @var{n} = 100 is used.
@end deftypefn


@c autoreg_matrix scripts/signal/autoreg_matrix.m
@anchor{XREFautoreg_matrix}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{x} =} autoreg_matrix (@var{y}, @var{k})
Given a time series (vector) @var{y}, return a matrix with ones in the first
column and the first @var{k} lagged values of @var{y} in the other columns.

In other words, for @var{t} > @var{k},
@code{[1, @var{y}(@var{t}-1), @dots{}, @var{y}(@var{t}-@var{k})]} is the
t-th row of the result.

The resulting matrix may be used as a regressor matrix in autoregressions.
@end deftypefn


@c bartlett scripts/signal/bartlett.m
@anchor{XREFbartlett}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{c} =} bartlett (@var{m})
Return the filter coefficients of a Bartlett (triangular) window of length
@var{m}.

For a definition of the Bartlett window see, e.g.,
@nospell{A.V. Oppenheim & R. W. Schafer},
@cite{Discrete-Time Signal Processing}.
@end deftypefn


@c blackman scripts/signal/blackman.m
@anchor{XREFblackman}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{c} =} blackman (@var{m})
@deftypefnx {} {@var{c} =} blackman (@var{m}, "periodic")
@deftypefnx {} {@var{c} =} blackman (@var{m}, "symmetric")
Return the filter coefficients of a @nospell{Blackman} window of length
@var{m}.

If the optional argument @qcode{"periodic"} is given, the periodic form
of the window is returned.  This is equivalent to the window of length
@var{m}+1 with the last coefficient removed.  The optional argument
@qcode{"symmetric"} is equivalent to not specifying a second argument.

For a definition of the @nospell{Blackman} window, see, e.g.,
@nospell{A.V. Oppenheim & R. W. Schafer},
@cite{Discrete-Time Signal Processing}.
@end deftypefn


@c detrend scripts/signal/detrend.m
@anchor{XREFdetrend}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{y} =} detrend (@var{x}, @var{p})
If @var{x} is a vector, @code{detrend (@var{x}, @var{p})} removes the
best fit of a polynomial of order @var{p} from the data @var{x}.

If @var{x} is a matrix, @code{detrend (@var{x}, @var{p})} does the same
for each column in @var{x}.

The second argument @var{p} is optional.  If it is not specified, a value of
1 is assumed.  This corresponds to removing a linear trend.

The order of the polynomial can also be given as a string, in which case
@var{p} must be either @qcode{"constant"} (corresponds to @code{@var{p}=0})
or @qcode{"linear"} (corresponds to @code{@var{p}=1}).
@xseealso{@ref{XREFpolyfit,,polyfit}}
@end deftypefn


@c diffpara scripts/signal/diffpara.m
@anchor{XREFdiffpara}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {[@var{d}, @var{dd}] =} diffpara (@var{x}, @var{a}, @var{b})
Return the estimator @var{d} for the differencing parameter of an
integrated time series.

The frequencies from @math{[2*pi*a/t, 2*pi*b/T]} are used for the
estimation.  If @var{b} is omitted, the interval
@math{[2*pi/T, 2*pi*a/T]} is used.  If both @var{b} and @var{a} are omitted
then @math{a = 0.5 * sqrt (T)} and @math{b = 1.5 * sqrt (T)} is used, where
@math{T} is the sample size.  If @var{x} is a matrix, the differencing
parameter of each column is estimated.

The estimators for all frequencies in the intervals described above is
returned in @var{dd}.

The value of @var{d} is simply the mean of @var{dd}.

Reference: @nospell{P.J. Brockwell & R.A. Davis}. @cite{Time Series:
Theory and Methods}. @nospell{Springer} 1987.
@end deftypefn


@c durbinlevinson scripts/signal/durbinlevinson.m
@anchor{XREFdurbinlevinson}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {[@var{newphi}, @var{newv}] =} durbinlevinson (@var{c}, @var{oldphi}, @var{oldv})
Perform one step of the @nospell{Durbin-Levinson} algorithm.

The vector @var{c} specifies the autocovariances
@code{[gamma_0, @dots{}, gamma_t]} from lag 0 to @var{t}, @var{oldphi}
specifies the coefficients based on @var{c}(@var{t}-1) and @var{oldv}
specifies the corresponding error.

If @var{oldphi} and @var{oldv} are omitted, all steps from 1 to @var{t} of
the algorithm are performed.
@end deftypefn


@c fftshift scripts/signal/fftshift.m
@anchor{XREFfftshift}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{y} =} fftshift (@var{x})
@deftypefnx {} {@var{y} =} fftshift (@var{x}, @var{dim})
Perform a shift of the vector @var{x}, for use with the @code{fft} and
@code{ifft} functions, in order to move the frequency 0 to the center of
the vector or matrix.

If @var{x} is a vector of @math{N} elements corresponding to @math{N} time
samples spaced by @nospell{@math{dt}}, then
@code{fftshift (fft (@var{x}))} corresponds to frequencies

@example
f = [ -(ceil((N-1)/2):-1:1), 0, (1:floor((N-1)/2)) ] * df
@end example

@noindent
where @nospell{@math{df = 1 / (N * dt)}}.

If @var{x} is a matrix, the same holds for rows and columns.  If @var{x}
is an array, then the same holds along each dimension.

The optional @var{dim} argument can be used to limit the dimension along
which the permutation occurs.
@xseealso{@ref{XREFifftshift,,ifftshift}}
@end deftypefn


@c ifftshift scripts/signal/ifftshift.m
@anchor{XREFifftshift}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{x} =} ifftshift (@var{y})
@deftypefnx {} {@var{x} =} ifftshift (@var{y}, @var{dim})
Undo the action of the @code{fftshift} function.

For even length @var{x}, @code{fftshift} is its own inverse, but odd lengths
differ slightly.
@xseealso{@ref{XREFfftshift,,fftshift}}
@end deftypefn


@c fractdiff scripts/signal/fractdiff.m
@anchor{XREFfractdiff}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{fd} =} fractdiff (@var{x}, @var{d})
Compute the fractional differences @math{(1-L)^d x} where @math{L}
denotes the lag-operator and @math{d} is greater than -1.
@end deftypefn


@c hamming scripts/signal/hamming.m
@anchor{XREFhamming}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{c} =} hamming (@var{m})
@deftypefnx {} {@var{c} =} hamming (@var{m}, "periodic")
@deftypefnx {} {@var{c} =} hamming (@var{m}, "symmetric")
Return the filter coefficients of a Hamming window of length @var{m}.

If the optional argument @qcode{"periodic"} is given, the periodic form
of the window is returned.  This is equivalent to the window of length
@var{m}+1 with the last coefficient removed.  The optional argument
@qcode{"symmetric"} is equivalent to not specifying a second argument.

For a definition of the Hamming window see, e.g.,
@nospell{A.V. Oppenheim & R. W. Schafer},
@cite{Discrete-Time Signal Processing}.
@end deftypefn


@c hanning scripts/signal/hanning.m
@anchor{XREFhanning}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{c} =} hanning (@var{m})
@deftypefnx {} {@var{c} =} hanning (@var{m}, "periodic")
@deftypefnx {} {@var{c} =} hanning (@var{m}, "symmetric")
Return the filter coefficients of a Hanning window of length @var{m}.

If the optional argument @qcode{"periodic"} is given, the periodic form
of the window is returned.  This is equivalent to the window of length
@var{m}+1 with the last coefficient removed.  The optional argument
@qcode{"symmetric"} is equivalent to not specifying a second argument.

For a definition of the Hanning window see, e.g.,
@nospell{A.V. Oppenheim & R. W. Schafer},
@cite{Discrete-Time Signal Processing}.
@end deftypefn


@c hurst scripts/signal/hurst.m
@anchor{XREFhurst}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{H} =} hurst (@var{x})
Estimate the Hurst parameter of sample @var{x} via the rescaled range
statistic.

If @var{x} is a matrix, the parameter is estimated for every column.
@end deftypefn


@c pchip scripts/polynomial/pchip.m
@anchor{XREFpchip}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{pp} =} pchip (@var{x}, @var{y})
@deftypefnx {} {@var{yi} =} pchip (@var{x}, @var{y}, @var{xi})
Return the Piecewise Cubic Hermite Interpolating Polynomial (pchip) of
points @var{x} and @var{y}.

If called with two arguments, return the piecewise polynomial @var{pp}
that may be used with @code{ppval} to evaluate the polynomial at specific
points.

When called with a third input argument, @code{pchip} evaluates the pchip
polynomial at the points @var{xi}.  The third calling form is equivalent to
@code{ppval (pchip (@var{x}, @var{y}), @var{xi})}.

The variable @var{x} must be a strictly monotonic vector (either increasing
or decreasing) of length @var{n}.

@var{y} can be either a vector or array.  If @var{y} is a vector then it
must be the same length @var{n} as @var{x}.  If @var{y} is an array then
the size of @var{y} must have the form
@tex
$$[s_1, s_2, \cdots, s_k, n]$$
@end tex
@ifnottex
@code{[@var{s1}, @var{s2}, @dots{}, @var{sk}, @var{n}]}
@end ifnottex
The array is reshaped internally to a matrix where the leading dimension is
given by
@tex
$$s_1 s_2 \cdots s_k$$
@end tex
@ifnottex
@code{@var{s1} * @var{s2} * @dots{} * @var{sk}}
@end ifnottex
and each row of this matrix is then treated separately.  Note that this is
exactly opposite to @code{interp1} but is done for @sc{matlab}
compatibility.

@xseealso{@ref{XREFspline,,spline}, @ref{XREFppval,,ppval}, @ref{XREFmkpp,,mkpp}, @ref{XREFunmkpp,,unmkpp}}
@end deftypefn


@c periodogram scripts/signal/periodogram.m
@anchor{XREFperiodogram}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {[@var{Pxx}, @var{w}] =} periodogram (@var{x})
@deftypefnx {} {[@var{Pxx}, @var{w}] =} periodogram (@var{x}, @var{win})
@deftypefnx {} {[@var{Pxx}, @var{w}] =} periodogram (@var{x}, @var{win}, @var{nfft})
@deftypefnx {} {[@var{Pxx}, @var{f}] =} periodogram (@var{x}, @var{win}, @var{nfft}, @var{Fs})
@deftypefnx {} {[@var{Pxx}, @var{f}] =} periodogram (@dots{}, "@var{range}")
@deftypefnx {} {} periodogram (@dots{})
Return the periodogram (Power Spectral Density) of @var{x}.

The possible inputs are:

@table @var
@item x

data vector.  If @var{x} is real-valued a one-sided spectrum is estimated.
If @var{x} is complex-valued, or @qcode{"@var{range}"} specifies
@qcode{"@nospell{twosided}"}, the full spectrum is estimated.

@item win
window weight data.  If window is empty or unspecified a default rectangular
window is used.  Otherwise, the window is applied to the signal
(@code{@var{x} .* @var{win}}) before computing the periodogram.  The window
data must be a vector of the same length as @var{x}.

@item nfft
number of frequency bins.  The default is 256 or the next higher power of
2 greater than the length of @var{x}
(@code{max (256, 2.^nextpow2 (length (x)))}).  If @var{nfft} is greater
than the length of the input then @var{x} will be zero-padded to the length
of @var{nfft}.

@item Fs
sampling rate.  The default is 1.

@item range
range of spectrum.  @qcode{"@nospell{onesided}"} computes spectrum from
[0:nfft/2+1].  @qcode{"@nospell{twosided}"} computes spectrum from
[0:nfft-1].
@end table

The optional second output @var{w} are the normalized angular frequencies.
For a one-sided calculation @var{w} is in the range [0, pi] if @var{nfft}
is even and [0, pi) if @var{nfft} is odd.  Similarly, for a two-sided
calculation @var{w} is in the range [0, 2*pi] or [0, 2*pi) depending on
@var{nfft}.

If a sampling frequency is specified, @var{Fs}, then the output frequencies
@var{f} will be in the range [0, @var{Fs}/2] or [0, @var{Fs}/2) for
one-sided calculations.  For two-sided calculations the range will be
[0, @var{Fs}).

When called with no outputs the periodogram is immediately plotted in the
current figure window.
@xseealso{@ref{XREFfft,,fft}}
@end deftypefn


@c sinetone scripts/signal/sinetone.m
@anchor{XREFsinetone}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{y} =} sinetone (@var{freq}, @var{rate}, @var{sec}, @var{ampl})
Return a sinetone of frequency @var{freq} with a length of @var{sec}
seconds at sampling rate @var{rate} and with amplitude @var{ampl}.

The arguments @var{freq} and @var{ampl} may be vectors of common size.

The defaults are @var{rate} = 8000, @var{sec} = 1, and @var{ampl} = 64.
@xseealso{@ref{XREFsinewave,,sinewave}}
@end deftypefn


@c sinewave scripts/signal/sinewave.m
@anchor{XREFsinewave}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{y} =} sinewave (@var{m}, @var{n}, @var{d})
Return an @var{m}-element vector with @var{i}-th element given by
@code{sin (2 * pi * (@var{i}+@var{d}-1) / @var{n})}.

The default value for @var{d} is 0 and the default value for @var{n} is
@var{m}.
@xseealso{@ref{XREFsinetone,,sinetone}}
@end deftypefn


@c spectral_adf scripts/signal/spectral_adf.m
@anchor{XREFspectral_adf}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{sde} =} spectral_adf (@var{c})
@deftypefnx {} {@var{sde} =} spectral_adf (@var{c}, @var{win})
@deftypefnx {} {@var{sde} =} spectral_adf (@var{c}, @var{win}, @var{b})
Return the spectral density estimator given a vector of autocovariances
@var{c}, window name @var{win}, and bandwidth, @var{b}.

The window name, e.g., @qcode{"triangle"} or @qcode{"rectangle"} is
used to search for a function called @code{@var{win}_lw}.

If @var{win} is omitted, the triangle window is used.

If @var{b} is omitted, @code{1 / sqrt (length (@var{x}))} is used.
@xseealso{@ref{XREFspectral_xdf,,spectral_xdf}}
@end deftypefn


@c spectral_xdf scripts/signal/spectral_xdf.m
@anchor{XREFspectral_xdf}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{sde} =} spectral_xdf (@var{x})
@deftypefnx {} {@var{sde} =} spectral_xdf (@var{x}, @var{win})
@deftypefnx {} {@var{sde} =} spectral_xdf (@var{x}, @var{win}, @var{b})
Return the spectral density estimator given a data vector @var{x}, window
name @var{win}, and bandwidth, @var{b}.

The window name, e.g., @qcode{"triangle"} or @qcode{"rectangle"} is used to
search for a function called @code{@var{win}_sw}.

If @var{win} is omitted, the triangle window is used.

If @var{b} is omitted, @code{1 / sqrt (length (@var{x}))} is used.
@xseealso{@ref{XREFspectral_adf,,spectral_adf}}
@end deftypefn


@c spencer scripts/signal/spencer.m
@anchor{XREFspencer}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{savg} =} spencer (@var{x})
Return @nospell{Spencer's} 15-point moving average of each column of
@var{x}.
@end deftypefn


@c stft scripts/signal/stft.m
@anchor{XREFstft}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn  {} {@var{y} =} stft (@var{x})
@deftypefnx {} {@var{y} =} stft (@var{x}, @var{win_size})
@deftypefnx {} {@var{y} =} stft (@var{x}, @var{win_size}, @var{inc})
@deftypefnx {} {@var{y} =} stft (@var{x}, @var{win_size}, @var{inc}, @var{num_coef})
@deftypefnx {} {@var{y} =} stft (@var{x}, @var{win_size}, @var{inc}, @var{num_coef}, @var{win_type})
@deftypefnx {} {[@var{y}, @var{c}] =} stft (@dots{})
Compute the short-time Fourier transform of the vector @var{x} with
@var{num_coef} coefficients by applying a window of @var{win_size} data
points and an increment of @var{inc} points.

Before computing the Fourier transform, one of the following windows
is applied:

@table @asis
@item @qcode{"hanning"}
win_type = 1

@item @qcode{"hamming"}
win_type = 2

@item @qcode{"rectangle"}
win_type = 3
@end table

The window names can be passed as strings or by the @var{win_type} number.

The following defaults are used for unspecified arguments:
@var{win_size} = 80, @var{inc} = 24, @var{num_coef} = 64, and
@var{win_type} = 1.

@code{@var{y} = stft (@var{x}, @dots{})} returns the absolute values of the
Fourier coefficients according to the @var{num_coef} positive frequencies.

@code{[@var{y}, @var{c}] = stft (@var{x}, @dots{})} returns the entire
STFT-matrix @var{y} and a 3-element vector @var{c} containing the window
size, increment, and window type, which is needed by the @code{synthesis}
function.
@xseealso{@ref{XREFsynthesis,,synthesis}}
@end deftypefn


@c synthesis scripts/signal/synthesis.m
@anchor{XREFsynthesis}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {@var{x} =} synthesis (@var{y}, @var{c})
Compute a signal from its short-time Fourier transform @var{y} and a
3-element vector @var{c} specifying window size, increment, and window type.

The values @var{y} and @var{c} can be derived by

@example
[@var{y}, @var{c}] = stft (@var{x} , @dots{})
@end example
@xseealso{@ref{XREFstft,,stft}}
@end deftypefn


@c yulewalker scripts/signal/yulewalker.m
@anchor{XREFyulewalker}
@html
<span style="display:block; margin-top:-4.5ex;">&nbsp;</span>
@end html


@deftypefn {} {[@var{a}, @var{v}] =} yulewalker (@var{c})
Fit an AR (p)-model with Yule-Walker estimates given a vector @var{c} of
autocovariances @code{[gamma_0, @dots{}, gamma_p]}.

Returns the AR coefficients, @var{a}, and the variance of white noise,
@var{v}.
@end deftypefn

