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# From wavelets to adaptive approximations: time-frequency parametrization of EEG

^{1}Laboratory of Medical Physics, Institute of Experimental Physics, Warsaw University, Warszawa, Poland

^{}Corresponding author.

## Abstract

This paper presents a summary of time-frequency analysis of the electrical activity of the brain (EEG). It covers in details two major steps: introduction of wavelets and adaptive approximations. Presented studies include time-frequency solutions to several standard research and clinical problems, encountered in analysis of evoked potentials, sleep EEG, epileptic activities, ERD/ERS and pharmaco-EEG. Based upon these results we conclude that the matching pursuit algorithm provides a unified parametrization of EEG, applicable in a variety of experimental and clinical setups. This conclusion is followed by a brief discussion of the current state of the mathematical and algorithmical aspects of adaptive time-frequency approximations of signals.

## EEG

The electroencephalogram (EEG), recorded from electrodes placed on the scalp, reflects the electrical activity of the brain.

First registered from human scalp in 1929 [1], until today EEG remains an important tool in neuroscience and clinical neurophysiology. For a long time it was the only objective parameter providing information on brain's *function*. Recently emerging dynamic imaging techniques like fMRI and PET offer a complementary information on brains functioning. Their drawbacks include significantly lower time resolution, high cost and invasiveness. Nevertheless, in spite of those drawbacks, they are often preferred for the straightforward interpretability. On the contrary, visual interpretation of EEG is a difficult, tedious and complicated task, requiring many years of experience. And even then it contains a significant subjective factor:

Every experienced electroencephalographer has his or her personal approach to EEG interpretation. (...) there is an element of science and element of art in a good EEG interpretation; it is the latter that defies standardization.

writes Prof. Ernst Niedermayer in the recent edition of a fundamental reference [2].

In spite of this discouraging opinion, application of various signal processing methods in this field is still very popular. First introduction of Fourier analysis to EEG is dated 1932 [3]. Since then spectral analysis has become a standard tool in this field. But until today, basically no other method gained a general acceptance – the few widely accepted and applied methods of EEG analysis still amount to [4]:

1. visual analysis of raw EEG traces,

2. Fourier estimation of spectral power in selected frequency bands,

3. description of evoked potentials, averaged in the time domain.

One of the reasons of this unsatisfactory situation is that among the variety of new methods, proposed each year for the analysis of EEG, very few have any direct relationship to the traditional, visual analysis. That means that their results usually cannot be directly related to the most valuable knowledge base of 70 years of experience, collected by means of the visual analysis of EEG. On the contrary, each new method needs to be evaluated from the scratch, in many laboratories and over many repeated studies, before it can be considered as a clinically usable parameter. And since there is a multitude of new methods being proposed, with few *a priori *hints for their possible performance, this process seems to be hardly convergent.

## Wavelets: the first step towards time-frequency analysis

EEG as a signal is extremely complex and reveals both rhythmical and transient features. Therefore, when orthogonal wavelets triggered in eighties the time-frequency revolution in signal processing, analysis of EEG was one of the fields where hopes for a more "morphological" description of signal arose.

First successful applications of wavelets addressed the issue of evoked potentials (EP). Event-related potentials are small changes of EEG activity in response to an external (evoked) or internal stimulus. They are usually an order of magnitude weaker than the on-going EEG activity, so traditionally they were observed only in time averages of stimulus-synchronized repetitions. Owing to the property of the time synchronization, they can be studied in the space of orthogonal wavelet coefficients. Figures Figures22,,33,,44 present the first wavelet study of evoked potentials [5]. Randomly chosen epochs of on-going EEG were statistically compared – in the space of wavelet coefficients – to those synchronized by an auditory stimulus. As a result, only 9 out of 512 coefficients were found to discriminate between those conditions. They were enough to reproduce the basic morphology of the average EP. Figure Figure44 presents reconstruction of single evoked potentials using those coefficients.

### Limitations of linear and quadratic time-frequency representations

Further attempts to apply wavelets to the analysis of on-going EEG activity encountered a major drawback. Representation of the signal, obtained from orthogonal wavelet representation, is not time-shift invariant. This property is illustrated in Figure Figure55.

This limitation is not present in the continuous wavelet transform, as well as several quadratic representations of signal's energy density in the time-frequency plane (c.f. [6] and Figure Figure8).8). However, in such case we loose the compact description offered by orthogonal wavelets – the representation is highly redundant. Another problem relates to the occurence of cross terms (Figure (Figure66).

*a*+

*b*)

^{2 }=

*a*

^{2 }+

*b*

^{2 }+ 2

*ab*. Wigner-De Ville transform (above) of a signal composed of two sine waves with compact and separated support (below). The structure appearing in the time coordinates

**...**

Both these problems can be solved (or at least significantly reduced) by the solution proposed in the next section.

## Adaptive approximations and matching pursuit

Given a set of functions (dictionary) *D *= {*g*_{1},*g*_{2}...*g*_{n}} such that ||*g*_{i}|| = 1, we can define an optimal *M*-approximation as an expansion, minimizing the error ε of an approximation of signal *f*(*t*) by *M* waveforms:

where {γ_{i}}_{i = 1..M } represents the indices of the chosen functions *g*_{γi}. Finding such an optimal approximation is an NP-hard problem. A suboptimal expansion can be found by means of an iterative procedure, such as the matching pursuit algorithm (MP) proposed by Mallat and Zhang [7].

In the first step of MP, the waveform *g*_{γ0} which best matches the signal *f*(*t*) is chosen. In each of the consecutive steps, the waveform *g*_{γn} is matched to the signal R^{n}*f*, which is the residual left after subtracting results of previous iterations:

Orthogonality of R^{n+1 }*f* and *g*_{γn} in each step implies energy conservation:

For a complete dictionary the procedure converges to *f*:

From this equation we can derive a time-frequency distribution of the signal's energy, that is free of cross-terms, by adding Wigner distributions of selected functions:

This magnitude is presented in Figure Figure7,7, calculated from MP decomposition of a simulated signal with known and simple content. We observe that most of the structures are represented compactly and with high resolution, except for the structure of changing frequency (linear chirp). It is represented by a series of structures of constant frequency, since in the applied Gabor dictionary (section 5) we have only constant frequency modulations. Section 7 presents an alternative approach to this issue.

**...**

Figure Figure88 presents estimates of the time-frequency density of the same signal's energy, obtained from: spectrograms with different window widths, continuous wavelet transform and smoothed pseudo Wigner-Ville distribution. Only in the last case representation of the chirp looks better than on the plot obtained from MP decomposition, but we must take into account that in this case the parameters of the kernel of the distribution were optimized for this particular signal.

Except for the lack of cross terms and high resolution, adaptive time-frequency parametrizations exhibit one more basic and important advantage over the continuous time-frequency representations. Unlike the maps from Figure Figure8,8, for all the structures presented in Figure Figure77 we have a priori the exact values of their time and frequency centers, widths, amplitudes and phases. This property will be thoroughly explored in the following studies.

## First application in EEG analysis: sleep spindles

The presence of sleep spindle should not be defined unless it is of at least 0.5 sec duration, i.e., one should be able to count 6 or 7 distinct waves within the half-second period. (...) The term should be used only to describe activity between 12 and 14 cps.

– says the definition from the basic reference [8] – "A manual of standardized terminology, techniques and scoring system for sleep stages in human subjects". It can be directly translated into the language of parameters of the structures fitted to the signal by the algorithm discussed in the previous section.

By choosing from the time-frequency atoms, fitted to EEG by the MP algorithm, those conforming to the above criteria, we obtain a detailed, automatic and high-resolution parametrization of the relevant structures, which correspond to sleep spindles [9,10]. Figures Figures1010 and and1111 present results of such a procedure carried out for several derivations of an overnight sleep EEG recording. This parametrization has proven to be consistent with visual detection, especially for the structures of higher amplitudes [11]. For lower amplitudes the algorithm detects also spindles elusive to a human expert.

**...**

Results presented in these figures conform also the previously observed effect of predominance of lower frequencies of sleep spindles in frontal derivations and higher frequencies in parietal derivations. We also notice that some frequencies on these plots are "prefereed", i.e. exhibit regular maxima in the histograms. But are they preferred by the brain or by the analysis algorithm? This question will be resolved in the next section.

## Discrete Gabor dictionary

Gabor functions (sine-modulated Gaussian functions) provide optimal joint time-frequency localization. A real Gabor function can be expressed as:

*N *is the size of the signal for which the dictionary is constructed, *K*(γ) is such that ||*g*_{γ}|| = 1. γ = {*u*,ω,*s*, } denotes parameters of the dictionary's functions (time-frequency atoms). These parameters generate a three-dimensional continuous space; this results in an infinite dictionary size. Therefore, in practical implementations, we use subsets of the possible dictionary's functions.

In the dictionary implemented originally by Mallat and Zhang in [7], parameters of these functions (time-frequency atoms) are chosen from dyadic sequences of integers. Their sampling is governed by an extra parameter – octave *j *(integer). Scale *s*, which corresponds to an atom's width in time, is derived from the dyadic sequence *s *= 2^{j}, 0 ≤ *j *≤ *L *(signal size *N *= 2^{L}). Parameters *u *and ω, which correspond to position in time and frequency, are sampled for each octave *j *with interval *s *= 2^{j}, or, if oversampling by *l *is introduced, with interval 2^{j-l}.

This specific wavelet-like structure of the dictionary is responsible for the fact that decomposition over such a dictionary "prefers" certain positions in frequency or time (Figures (Figures12,12, ,13).13). In those positions more atoms are available for decomposition due to the particular structure of the dictionary, i.e. scheme of subsampling the parameter space.

**...**

*a, b*) and white noise (

*c-f*) over dyadic (

*a, c, e*) and stochastic (

*b, d, f*) dictionaries. Histograms of frequency centers of atoms fitted by MP decomposition over dyadic dictionary to

**...**

### Stochastic dictionaries

In forming the dictionary used for MP decomposition, using any *fixed *scheme of subsampling the parameter space introduces statistical bias in the resulting parametrization. This bias becomes apparent only when statistics comes into play, like in parameterization of large amounts of data. Unbiased MP decompositions can be obtained by an analogue of Monte Carlo methods.

In [12] we proposed MP with stochastic dictionaries, where the parameters of a dictionary's atoms are randomized before each decomposition. A stochastic dictionary *D *is constructed for a given signal length *N *and chosen "resolutions"^{1 }in time, frequency and scale (Δ*t*, Δω and Δ*s*). The space of parameters *t*, ω and *s *is thereby divided into bricks of size Δ*t *by Δω by Δ*s *each, where ω (0,π). In each of those bricks, one time-frequency atom is chosen by drawing its parameters from flat distributions within the given ranges of continuous parameters.

Figures Figures1414 and and1515 present results for the same data as Figures Figures1010 and and11.11. These results, owing to the application of the above described stochastic dictionaries, are free from the statistical bias.

^{1}The resolution of the matching pursuit is hard to define in general, since the procedure is nonlinear and signal-dependent. It should be related to the distance between neighboring dictionary waveforms available for decomposition. In the described procedure, this distance does not exceed twice the value of the corresponding parameter (Δ*t*, Δω or Δ*s*).

## Pharmaco EEG

This section presents an application of the proposed methodology to the standard clinical problem of testing influence of sleep inducing drugs on the sleep EEG.

The effects of zolpidem, midazolam and placebo, administered at bed time, were studied in 7 paid volunteers. From each of the 21 all-night recordings (3 nights for each subject) we extracted artifact-free epochs from derivation C3-A2 of the 10–20 system. For the analysis of slow wave activity (SWA) we used data from stages III and IV and for sleep spindles only data from sleep stage II.

Figures Figures1616 and and1818 present the classical approach to the analysis of these data, that is averaging the spectral integrals in the above mentioned ranges, for each of the analyzed recordings.

**...**

Figures Figures1717 and and1919 present each of the structures, classified as sleep spindles (Figure (Figure17)17) or SWA (Figure (Figure19)19) as a dot in the frequency-amplitude plane. These structures were selected using not only the frequency information, as in the "classical" approach, but also information on time duration and amplitude from Table Table1.1. Total power carried by these structures, summed and normalized per time unit, is indicated on the right of each plot, together with the average number of occurrences per minute, average amplitude and frequency.

*V*and time duration

**...**

*V*and duration above half a second. Plots and descriptions organized as in Figure Figure1717

We observe that selective MP-based estimates of power are more sensitive to the effect of influence of both drugs than the spectral integrals. This sensitivity becomes crucial in two of the analyzed cases:

1. In the recording of patient ZCB09, which revealed a very low spindling activity (last row in Figures Figures1616 and and17),17), fluctuations in the background masked the power of sleep spindles to such an extent, that spectral integrals indicate a partially reverse trend, i.e. decrease of power of sleep spindles under the influence of midazolam. Selective estimates indicate the expected increase.

2. For patient ZCB08 (second row from the bottom) spectral integrals indicate increase of power of SWA (δ), while MP estimates reveal a decrease coherent with all the other cases.

Finally, as an example of an effect elusive to the classical methodology, these results indicate also a statistically significant decrease of the frequency of the slow wave activity. Further discussion and statistical evaluation of results can be found in [13].

Figure Figure2020 partially explains the increased sensitivity of the proposed approach as compared to the classical paradigm of band-limited spectral power integrals.

## Representation of changing frequency

Another interesting property of the stochastic time-frequency dictionaries, discussed in section 5.1, relates to the representation of structures of changing frequency. Such structures are absent in the dictionaries usually applied for the decomposition, and therefore are represented as a series od fixed-frequency Gabor functions (Figure 22 (f) and Figure 21 (b)).

*a*). In 3-dimensional plots on the left side energy is proportional to height, on flat pictures on the right – to the shades of gray. (

*b*) presents results of a single

**...**

**...**

However, by averaging several decompositions of the same signal in different realizations of smaller stochastic dictionaries, we obtain a more continuous representation like in Figures 22 (g) and Figure 21 (c). The representation is no more compact, but retains the general property of absence of cross terms.

## Event-related desynchronization and synchronization

Advantages of the MP algorithm with stochastic dictionaries can be also combined with the stochastic element present inherently in the data, like e.g. in the case of analyzing repetitions of event-related potentials. This relates especially to the non-phase locked activity, i.e. such that would not be enhanced in the stimulus-synchronized time averages. Its detection requires a different analysis technique, allowing for averaging signal's energy irrelevant of the phase^{2}. Classically it was achieved by squaring the values of signals, band-pass filtered in *a priori *chosen frequency bands, before averaging ([14], Figure Figure2323).

**...**

This methodology has several drawbacks, including tha arbitrary choice of frequency bands and limited sensitivity (c.f. Figure Figure20).20). Averaging the time-frequency densities of energy, obtained from the MP decomposition, allows for an instantaneous evaluation of the complete picture of changes in the time-frequency plane, with high resolution. Figure Figure2525 presents this picture for the same data as in Figure Figure23.23. Another study in Figure Figure2626 reveals clearly splitting of the alpha band in the upper and lower frequencies, with different behaviour related to the finger movement. This phenomenon would be very difficult to find using the classical methodology.

**...**

**...**

**...**

^{2}If we want to analyze phasic synchronization in higher frequencies, like e.g. gamma band around 40 Hz, the accuracy of the triger's determination would have to be *much *better than e.g. 1 ms, which is rather beyond the accuracy of determining e.g. the moment of a finger movement. But non-phasic effects should be visible in the presented approach.

## Epileptic seizures

Discussed advantages of time-frequency estimates of energy density, obtained from MP decomposition, allowed for identification of different dynamic states during evolution and propagation of epileptic seizures in [15].

Figure Figure2727 presents an example of time-frequency density of energy, calculated from the MP expansion of an intracranial recording of epileptic seizure. Sensitivity of the algorithm to the phase changes clearly distinguishes the initial less synchronized period of transitional rhytmic activity (starting near 15th second) from the organized rhytmic activity. In this period (starting about 30th second) all the harmonics, up to the Nyquist frequency, clearly follow the pattern of decreasing frequency. Such a clear representation of changing frequency was possible using the technique discussed in section 7.

## Problems

As presented in figure figure28,28, greedy MP algorithm in certain cases can fail to properly decompose signal containing even a simple combination of dictionary's functions. This counterexample was simulated especially for discussion of practical issues and as such may look scary, but on the other hand we never encountered such a failure in applications to real world signals. The trap in this case lies in the fact that both these structures have *exactly *the same phase, and it might be even dicussable if they should not be treated as one in the first approximation. If they were produced by two different biological generators, such a coincidence of phases would not be possible and they would be parametrized separately.

**...**

Other, more theoretical examples of MP failures are given in [16] and [17]. Some of these cases can be properly solved by the orthogonalized matching pursuit [18], at a cost of increased computational requirements and a possibility of introducing numerical instabilities [19]. Another modification of the MP algorithm, discussed in [20], relies on a modification of the similarity function used in each step to choosed the "best fit". Other works [21] indicate that global optimalization of the *l*^{1 }norm of expansion's coefficients might be the best choice [17], but, in spite of recent advances in linear programming, computational complexity is still very high.

Other problems, awaiting better solutions, include: efficient and (at the same time) bias-free implementations, robust estimation of resolution, proper addressing of the tradeoff between resolution (increasing dictionary size) and computation cost, and extension of the algorithm to the multichannel case. Such research will improve effectivity and understanding of mathematical foundations of these higly nonlinear procedures. However, current implementations and knowledge of algorithm's properties are already sufficient for large scale applications in EEG research and clinical practice. They may serve as a basis for a unification of parametrization and description of EEG.

Implementations of MP with stochastic dictionaries is available from http://brain.fuw.edu.pl/mp.

## Authors contributions

Parts of presented research, according to the quoted references, were coauthored by:

• Prof. Katarzyna J. Blinowska, head of the Laboratory of Medical Physics, Warsaw University, and my colleagues from the Lab: Józef Ginter Jr, Dobiesław Ircha, Jarosław Zygierewicz.

• Prof. Waldemar Szelenberger, Medical University of Warsaw

• Prof Ernest A. Bartnik, Inst. of Theoretical Physics, Warsaw University

• Prof. Piotr Franaszczuk, Johns Hopkins Medical University

• Prof. Gert Pfurtscheller and dr Christa Neuper, Graz Technical University

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- Adaptive time-frequency parametrization in pharmaco EEG.[J Neurosci Methods. 2002]
*Durka PJ, Szelenberger W, Blinowska KJ, Androsiuk W, Myszka M.**J Neurosci Methods. 2002 May 30; 117(1):65-71.* - Time-frequency analysis of brain electrical activity--adaptive approximations.[Methods Inf Med. 2004]
*Blinowska KJ, Durka PJ, Zygierewicz J.**Methods Inf Med. 2004; 43(1):70-3.* - Explicit parameterization of sleep EEG transients.[Comput Biol Med. 2007]
*Malinowska U, Durka PJ, Zygierewicz J, Szelenberger W, Wakarow A.**Comput Biol Med. 2007 Apr; 37(4):534-41. Epub 2006 Sep 22.* - Time-frequency microstructure and statistical significance of ERD and ERS.[Prog Brain Res. 2006]
*Durka PJ.**Prog Brain Res. 2006; 159:121-33.* - Computer analyses of EEG-sleep in the neonate: methodological considerations.[J Clin Neurophysiol. 1990]
*Scher MS, Sun M, Hatzilabrou GM, Greenberg NL, Cebulka G, Krieger D, Guthrie RD, Sclabassi RJ.**J Clin Neurophysiol. 1990 Jul; 7(3):417-41.*

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*V S Schönwald, Carvalho DZ, de Santa-Helena EL, Lemke N, L Gerhardt GJ.**BMC Neuroscience. 1389* - Extraction of single-trial cortical beta oscillatory activities in EEG signals using empirical mode decomposition[BioMedical Engineering OnLine. ]
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