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<blockquote><A NAME="921"> </A><IMG WIDTH=360 HEIGHT=154 ALIGN=BOTTOM ALT="figure1018" SRC="img4.gif" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/img4.gif"><BR>
<STRONG>Figure:</STRONG> <A NAME="figarspikes_surr"> </A>
A surrogate time series that has the same single time probability
distribution and the same autocorrelation function as the sequence in
Fig. <A HREF="node1.html#figarspikes" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node1.html#figarspikes">1</A>. The bursts are fully explained by these two
properties.<BR>
</blockquote>
<P>
<P>
In the case of the time series in Fig. <A HREF="node1.html#figarspikes" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node1.html#figarspikes">1</A>, there is no
additional structure since it has been generated by the rule
<BR><IMG WIDTH=500 HEIGHT=19 ALIGN=BOTTOM ALT="equation1019" SRC="img5.gif" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/img5.gif"><BR>
where <IMG WIDTH=30 HEIGHT=24 ALIGN=MIDDLE ALT="tex2html_wrap_inline1912" SRC="img6.gif" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/img6.gif"> are Gaussian independent increments and <IMG WIDTH=10 HEIGHT=7 ALIGN=BOTTOM ALT="tex2html_wrap_inline1914" SRC="img7.gif" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/img7.gif"> is chosen
so that the data have unit variance.<A NAME="tex2html3" HREF="footnode.html#41" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/footnode.html#41"><IMG ALIGN=BOTTOM ALT="gif" SRC="foot_motif.gif" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/foot_motif.gif"></A>
This means that the strong nonlinearity that generates the bursts is due to the
distorted measurement that enhances ordinary fluctuations, generated by linear
stochastic dynamics.
<P>
In order to systematically exclude simple explanations for time series
observations, this paper will discuss formal statistical tests for
nonlinearity. We will formulate suitable null hypotheses for the underlying
process or for the observed structures themselves. In the former case, null
hypotheses will be extensions of the statement that the data were generated by
a Gaussian linear stochastic processes. The latter situation may occur when it
is difficult to properly define a class of possibly underlying processes but we
want to check if a particular set of observables gives a complete account of
the statistics of the data. We will attempt to reject a null hypothesis by
comparing the value of a nonlinear parameter taken on by the data with its
probability distribution. Since only exceptional cases allow for the exact or
asymptotic derivation of this distribution unless strong additional assumptions
are made, we have to estimate it by a Monte Carlo resampling technique. This
procedure is known in the nonlinear time series literature as the method of
<EM>surrogate data</EM>, see Refs. [<A HREF="node36.html#theiler1" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node36.html#theiler1">6</A>, <A HREF="node36.html#theiler-sfi" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node36.html#theiler-sfi">7</A>, <A HREF="node36.html#fields" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node36.html#fields">8</A>]. Most of the
body of this paper will be concerned with the problem of generating an
appropriate Monte Carlo sample for a given null hypothesis.
<P>
We will also dwell on the proper interpretation of the outcome of such a test.
Formally speaking, this is totally straightforward: A rejection at a given
significance level means that if the null hypothesis is true, there is certain
small probability to still see the structure we detected. Non-rejection means
even less: either the null hypothesis is true, or the discriminating statistics
we are using fails to have power against the alternative realised in the
data. However, one is often tempted to go beyond this simple reasoning and
speculate either on the nature of the nonlinearity or non-stationarity that
lead to the rejection, or on the reason for the failure to reject.
<P>
Since the actual quantification of nonlinearity turns out to be the easiest --
or in any case the least dangerous -- part of the problem, we will discuss it
first. In principle, any nonlinear parameter can be employed for this purpose.
They may however differ dramatically in their ability to detect different kinds
of structures. Unfortunately, selecting the most suitable parameter has to be
done without making use of the data since that would render the test incorrect:
If the measure of nonlinearity has been optimised formally or informally with
respect to the data, a fair comparison with surrogates is no longer
possible. Only information that is shared by data and surrogates, that is, for
example, linear correlations, may be considered for guidance. If multiple data
sets are available, one could use some sequences for the selection of the
nonlinearity parameter and others for the actual test. Otherwise, it is
advantageous to use one of the parameter free methods that can be set up with
very little detailed knowledge of the data.
<P>
Since we want to advocate to routinely use a nonlinearity test whenever
nonlinear methods are planned to be applied, we feel that it is important to
make a practical implementation of such a test easily accessible. Therefore,
one branch of the TISEAN free software package [<A HREF="node36.html#tisean" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node36.html#tisean">9</A>] is devoted to
surrogate data testing. Appendix <A HREF="node32.html#appA" tppabs="http://www.mpipks-dresden.mpg.de/~tisean/TISEAN_2.0/docs/surropaper/node32.html#appA">A</A> will discuss the implementational
aspects necessary to understand what the programs in the package do.
<P>
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<P><ADDRESS>
<I>Thomas Schreiber <BR>
Mon Aug 30 17:31:48 CEST 1999</I>
</ADDRESS>
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