njit-etd2003-081 - New Jersey Institute of Technology
njit-etd2003-081 - New Jersey Institute of Technology njit-etd2003-081 - New Jersey Institute of Technology
87 3.10 Coherence Analysis Within the present framework, the dependence between two signals can be characterized by parameters, which assess the correlation between the signals. In the frequency domain it is customary to consider the magnitude squared of the correlation between the Fourier transforms of the two signals under consideration. For the bivariate point processes (N0 , N 1 ) this leads to [61][62] as a measure of the correlation between processes N 0 and N 1 . This quantity is called the coherence function [63], denoted by 1710 (f )1 2 , estimates of which provide a measure of the strength of correlation between N 0 and N1 as a function of frequency. The definition of the correlation corr{FN1(ω),FN0 (ω)} between the Fourier transforms of the two point processes N 0 and N 1 in terms of variance and covariance, given by the leads to the alternative definition for the coherence function between point processes N 0 and N 1 as Coherence functions provide a normative measure of linear association between two processes on a scale from 0 to 1, with 0 occurring in the case of independent processes [61][62]. Equation (3.84b) leads to an estimation procedure by substitution of the appropriate spectral estimates to give
RR similar manner to give: When computing the coherence using equation (3.85a), the important step is to compute the coherence by means of averaged estimates based on segments of the original signals. In other words, the signals x(t) and y(t) are broken up into N segments of equal length and the power spectra ( Pxx(ω) and PH (ω)) and cross spectrum ( Pxy(ω)) are estimated on the basis of averages taken from the individual spectra of the segments. To increase the number of individual spectra, which increases the accuracy, the segments may overlap. In addition, care must be taken to assure that the segments are long enough to obtain an accurate spectrum. Therefore, there is a compromise required in the choice of the segment length. It must be long enough to obtain accurate frequency resolution, but short enough to allow a sufficient number of segments in the average. In addition, each segment must be extracted using a time-domain window to control the sidelobes in the frequency domain. To make things more complicated, if too many
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87<br />
3.10 Coherence Analysis<br />
Within the present framework, the dependence between two signals can be characterized<br />
by parameters, which assess the correlation between the signals. In the frequency<br />
domain it is customary to consider the magnitude squared <strong>of</strong> the correlation between the<br />
Fourier transforms <strong>of</strong> the two signals under consideration. For the bivariate point<br />
processes (N0 , N 1 ) this leads to [61][62]<br />
as a measure <strong>of</strong> the correlation between processes N 0 and N 1 . This quantity is called<br />
the coherence function [63], denoted by 1710 (f )1 2<br />
, estimates <strong>of</strong> which provide a measure<br />
<strong>of</strong> the strength <strong>of</strong> correlation between N 0 and N1 as a function <strong>of</strong> frequency. The<br />
definition <strong>of</strong> the correlation corr{FN1(ω),FN0 (ω)} between the Fourier transforms <strong>of</strong> the<br />
two point processes N 0 and N 1 in terms <strong>of</strong> variance and covariance, given by the<br />
leads to the alternative definition for the coherence function between point processes N 0<br />
and N 1 as<br />
Coherence functions provide a normative measure <strong>of</strong> linear association between<br />
two processes on a scale from 0 to 1, with 0 occurring in the case <strong>of</strong> independent<br />
processes [61][62]. Equation (3.84b) leads to an estimation procedure by substitution <strong>of</strong><br />
the appropriate spectral estimates to give