Estimating the efficiency of the Granger causality method for detecting unidirectional coupling in the presence of common low frequency interference
Received 23 May 2017
2017, Vol. 13, No. 3, pp. 349-362
Author(s): Kornilov M. V., Sysoev I. V.
External low-frequency interference (including interference with a pronounced main frequency)
is a common problem in measurements of complex signals, which can affect results of coupling
estimation. Since it is impossible to completely remove the interference without affecting the
signal itself, the question arises: what distorts the results of coupling estimation to a lesser
extent: filtering the interference or ignoring it?
The Granger causality (GC) method is one of the most popular approaches to the detection of
directional coupling from observed signals. GC uses predictive empirical models, mostly, linear
and nonlinear autoregressive models (recurrence maps). Since the method is highly parametric,
its success depends primarily on the parameters of the models and on the properties of the
signals. Therefore, the method has to be adapted to the data. In physiology and climatology,
most signals have a pronounced time scale, so one of the most important problems is that of
adapting the Granger causality method to signals with a selected time scale.
The purpose of this paper is to formulate recommendations for using the Granger causality
method for signals with a pronounced temporal scale in the presence of common low-frequency
interference. In this paper, we restrict our attention to the case of testing for unilateral coupling
and use the recommendations and criteria, developed earlier, for the effectiveness of the method.
The sensitivity and specificity of the method are estimated based on surrogate time series. The
testing is performed using reference systems of nonlinear dynamics and radiophysics.
It is shown that the loss of sensitivity and specificity of the method decrease nonlinearly with
increasing amplitude of the total interference. This dependence varies for different parameters of
the method. If the power of interference is several per cent of the signal power, the best results
can be achieved by an appropriate choice of parameters of the method rather than by filtering
the interference. At a higher noise power, filtering is preferable.
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