correlation sum

{{One source|date=November 2007}}

In chaos theory, the correlation sum is the estimator of the correlation integral, which reflects the mean probability that the states at two different times are close:

:C(\varepsilon) = \frac{1}{N^2} \sum_{\stackrel{i,j=1}{i \neq j}}^N \Theta(\varepsilon - \| \vec{x}(i) - \vec{x}(j)\|), \quad \vec{x}(i) \in \mathbb{R}^m,

where N is the number of considered states \vec{x}(i), \varepsilon is a threshold distance, \| \cdot \| a norm (e.g. Euclidean norm) and \Theta( \cdot ) the Heaviside step function. If only a time series is available, the phase space can be reconstructed by using a time delay embedding (see Takens' theorem):

:\vec{x}(i) = (u(i), u(i+\tau), \ldots, u(i+\tau(m-1)),

where u(i) is the time series, m the embedding dimension and \tau the time delay.

The correlation sum is used to estimate the correlation dimension.

See also

References

  • {{cite journal | author=P. Grassberger and I. Procaccia | title=Measuring the strangeness of strange attractors | journal=Physica | year=1983 | volume=9D| issue=1–2 | pages=189–208 | doi=10.1016/0167-2789(83)90298-1|bibcode = 1983PhyD....9..189G }}

Category:Chaos theory

Category:Dynamical systems

Category:Dimension theory

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