EEG and Brain Connectivity: A Tutorial - Bio-Medical Instruments, Inc.
EEG and Brain Connectivity: A Tutorial - Bio-Medical Instruments, Inc.
EEG and Brain Connectivity: A Tutorial - Bio-Medical Instruments, Inc.
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Mathematical <strong>and</strong> statistical st<strong>and</strong>ardization of <strong>EEG</strong> coherence are<br />
best understood using a h<strong>and</strong> held calculator <strong>and</strong> then by simulation of the<br />
<strong>EEG</strong>.<br />
Coherence arises from Joseph Fourier’s 1805 fundamental inequality<br />
where by the ratio of the cross-spectrum/product of auto-spectrum < 1.<br />
Coherence is inherently a statistical estimate of coupling or association<br />
between two time series <strong>and</strong> is in essence the correlation over trials or<br />
repeated measures. As mentioned previously, the critical concept is “phase<br />
consistency”, i.e., when the phase relationship between two time series is<br />
constant over trials than coherence = 1.<br />
7- How Does One Compute Coherence?<br />
The first step in the calculation of the coherence spectrum is to<br />
describe the activity of each raw time-series in the frequency domain by the<br />
“auto-spectrum” which is a measure of the amount of energy or “activity” at<br />
different frequencies. The second step is to compute the “cross-spectrum”<br />
which is the energy in a frequency b<strong>and</strong> that is in common to the two<br />
different raw data time-series. The third step is to compute coherence<br />
which is a normalization of the cross-spectrum as the ratio of the autospectra<br />
<strong>and</strong> cross-spectra. To summarize:<br />
1- Compute the auto-spectra of channels X <strong>and</strong> Y based on the “atoms” of<br />
the spectrum<br />
2- Compute the cross-spectra of X <strong>and</strong> Y from the “atoms” of the spectrum<br />
3- Compute Coherence as the ratio of the auto-spectra <strong>and</strong> cross-spectra<br />
8- First Compute the auto-spectra of channels X <strong>and</strong> Y based on the<br />
“atoms” of the spectrum<br />
Joseph Fourier in his thesis of 1805, benefiting from almost a century<br />
of failed attempts, finally correctly showed that any complex time-series can<br />
be decomposed into elemental “atoms” of individual frequencies (sine <strong>and</strong><br />
cosine <strong>and</strong> linear operations). Fourier defined the autospectrum as the<br />
amount of energy present at a specific frequency b<strong>and</strong>. He showed that the<br />
autospectrum can be computed by multiplying each point of the raw data by<br />
a series of cosines, <strong>and</strong> independently again by a series of sines, for the<br />
frequency of interest. The average product of the raw-data <strong>and</strong> cosine is<br />
known as the cosine coefficient of the finite discrete Fourier transform, <strong>and</strong><br />
that for the sine <strong>and</strong> the raw data as a sine coefficient. The relative<br />
contributions of each frequency are expressed by these cosine <strong>and</strong> sine<br />
(finite discrete Fourier) coefficients. The cosine <strong>and</strong> sine coefficients