# Comparative study of nonlinear properties of EEG signals of normal persons and epileptic patients

- Md Nurujjaman
^{1}Email author, - Ramesh Narayanan
^{1, 2}and - AN Sekar Iyengar
^{1}

**3**:6

https://doi.org/10.1186/1753-4631-3-6

© Nurujjaman et al; licensee BioMed Central Ltd. 2009

**Received: **04 December 2008

**Accepted: **20 July 2009

**Published: **20 July 2009

## Abstract

### Background

Investigation of the functioning of the brain in living systems has been a major effort amongst scientists and medical practitioners. Amongst the various disorder of the brain, epilepsy has drawn the most attention because this disorder can affect the quality of life of a person. In this paper we have reinvestigated the EEGs for normal and epileptic patients using surrogate analysis, probability distribution function and Hurst exponent.

### Results

Using random shuffled surrogate analysis, we have obtained some of the nonlinear features that was obtained by Andrzejak *et al*. [Phys Rev E 2001, 64:061907], for the epileptic patients during seizure. Probability distribution function shows that the activity of an epileptic brain is nongaussian in nature. Hurst exponent has been shown to be useful to characterize a normal and an epileptic brain and it shows that the epileptic brain is long term anticorrelated whereas, the normal brain is more or less stochastic. Among all the techniques, used here, Hurst exponent is found very useful for characterization different cases.

### Conclusion

In this article, differences in characteristics for normal subjects with eyes open and closed, epileptic subjects during seizure and seizure free intervals have been shown mainly using Hurst exponent. The H shows that the brain activity of a normal man is uncorrelated in nature whereas, epileptic brain activity shows long range anticorrelation.

## Background

The brain is a highly complex and vital organ of a human body whose neurons interact with the local as well as the remote ones in a very complicated way [1–4]. These interactions evolve as the spatio-temporal electro magnetic field of the brain, and are recorded as Electroencephalogram (EEG) [1, 4–6]. Though the detail link between EEGs and the underlying physiology is not well understood, the former is widely used for detection and prediction of epilepsy, localization of epileptic zone and characterization of the pre and post-ictal [1, 6, 7] using linear and nonlinear analysis techniques [1, 6–11]. Though mainly nonlinear methods have been applied to predict the onset of epileptic seizure and localizing epileptic regions, limited progress has been achieved so far [11]. Even some negative results have also been reported like linear measures are better than nonlinear measures [12, 13], seizure is not a low dimensional process [14], it lacks determinism [8, 15, 16], etc. Hence finding proper analysis techniques is also one of the main issues and experts try out different analysis tools for characterizing the normal and diseased brain states, especially the epileptic brain.

In 2001, Ralph G. Andrzejak, *et al*. and later some other authors [17, 18] have analyzed five sets of EEG signals [19] each set containing 100 epochs to study the determinism in the brain dynamics for five different physiological and pathological conditions. Sets A and B are for normal persons with eyes open and closed respectively and recorded extracranially. Sets C and D were recorded intracranially from the hippocampal formation which was nonepiletogenic of the opposite hemisphere of the brain and from within the epileptogenic zone of an epileptic patient during seizure free intervals respectively. Set E was recorded intracranially from the epileptic zone during seizure. The details of the experiments and the conditions have been described in Ref [1]. R.G. Andrzejak, *et al*. [1] had shown that the normal healthy subject with eyes closed and open shows stochastic behavior using amplitude adjusted Fourier transform surrogate analysis where discriminating statistics were the effective correlation dimension and nonlinear prediction error whereas, using delay vector variance discriminating statistics, significant nonlinear determinism was shown in the same subject [17]. So two conflicting results were obtained for the same subject using nonlinear methods. In the case of epileptic patients during seizure and seizure free intervals, determinism was shown using two different methods [1, 17] though other studies show lack of determinism for different epileptic patients during seizure [12, 15, 16, 20].

On the other hand, characterization of EEGs by scaling properties of the signal is also a major area of research interest [8–10, 21–27]. Power spectral exponent has been used to characterize the different subjects with different physiological conditions [8, 9, 24, 25] and the same exponent has also been used to estimate the correlation dimension (*D*_{
corr
}) [8]. Fractal dimension and hurst exponent have also been used to characterize the EEGs [26, 27]. Hence a number of experts prefer scaling properties to characterize EEG for different physiological and pathological conditions [8].

In this paper, we have reinvestigated the EEG data studied in Refs. [1, 17, 18] by random shuffled surrogate analysis using *D*_{
corr
}as discriminating statistics in order to find determinism in the signal [28–30] and the results have been compared with earlier analyses [1, 17]. Probability distribution function shows a difference between normal and epileptic brain states and this has been discussed in latter Section. Finally, we have quantified the five different physiological brain states by Hurst exponent (H) which has been estimated using *R*/*S* analysis [31].

## Results and discussion

### Surrogate analysis

Surrogate analysis determines the dynamics in the time series: whether it is governed by stochastic or deterministic process [28–30].

*D*

_{ corr }which gives us a measure of the complexity has been estimated for both the original and the surrogate data of the data sets A, B, C, D, and E respectively. Fig 1(a) shows that the

*D*

_{ corr }increases with the same trend for both the original [Fig 1(b)] and the surrogate data [Fig 1(c)] for the normal persons with eyes open [Set A]. A similar trend is observed in the case of the persons with eyes closed, i.e., for Set B [Fig 2(a)]. This shows that the brain activity of a normal person is stochastic in nature agreeing with the analysis by Andrzejak,

*et al*. [1]. For an epileptic patient we found a different behavior during seizure free intervals and during seizure activity. The EEG signals, at seizure free state, recorded both from the hippocampal formation of the opposite hemisphere of the brain [Fig 2(b) Set C] and within the epileptogenic zone [Fig 2(c) Set D] show almost same trend in the increase in

*D*

_{ corr }for the surrogate data as well as for original data, except for a small separation at higher embedding dimensions, which may be due to a high dimensionality of the system. During seizure activity [Fig 2(d) Set E],

*D*

_{ corr }saturates with embedding dimension indicating low dimensional deterministic dynamics and these results agrees well with previous analyses [1, 17]. For sets A-D, as there is no saturation in

*D*

_{ corr }at higher embedding dimension [Fig 1(a) and Figs 2(b)–(d)] and hence it is difficult to estimate actual

*D*

_{ corr }. In Ref [1]

*D*

_{ corr }was computed based on quasiscaling regions, but such an estimation is very much dependent on the variations of the time-frequency-energy characteristics rather than any nonlinear dynamics. Hence this may be inadequate to characterize epilepsy or diseased brain states for clinical application [33].

### Probability distribution functions

### Hurst exponent

*R*/

*S*). This method was proposed by Hurst and well established by Mandelbrot, and Wallis [31]. For a given set of data series,

*R*/

*S*is defined as [31, 34]:

*S*

^{2}(

*n*), and n are respectively the mean, variance, and time lag of the signal. The expected value of the

*R*/

*S*scales like

*cn*

^{ H }as

*n*→ ∞, where H is called the Hurst exponent, and can be estimated from the slope of typical plot vs lag (n). For a given signal, we divided the data into nonoverlapping blocks of equal length and

*R*/

*S*has been calculated using the Equation 1 and the average value of

*R*/

*S*has been plotted as a function of lag in a log - log plot as shown in Fig 4 and estimated H from the slope of the curve. For random data

*H*= 0.5, while

*H*> 0.5 for the data with long range correlations, and

*H*< 0.5 indicates the presence of long-range anticorrelation or antipersistency in the data.

*H*>) with an error bar of 100 epochs for all the five EEG data sets (viz. A-E) have been shown in Fig 5. The solid box and black dot show the <

*H*> for sets A and B respectively. For a normal person with eyes open (set A), the average H (<

*H*>) ≈ 0.47 whereas, for the data set B, i.e., for a normal person with his eyes closed, <

*H*> ≈ 0.41. The <

*H*> ≈ 0.5 for a normal man with eyes open indicates that the signals are uncorrelated over long time scales signifying stochasticity of the normal brain. But with eyes closed state, decreases in H (<

*H*> ≈ 0.41) may be due to the imposition of some extra constraint, which may influence the system towards an antipersistent state. The <

*H*> for epileptic patients are shown by up triangle for set C; star for set D; and down triangle for set E respectively. <

*H*> ≈ 0.34 and 0.29 for the EEGs recorded at the hippocampal formation and epileptic zone for the seizure free intervals of epileptic patients respectively and during seizure (data set E), we get the lowest H (<

*H*> ≈ 0.19). The H for epileptic patient during seizure and seizure free intervals show anticorrelation which may be due to epileptiform discharges during seizure free intervals indicating that a large discharge is always followed by a small one. The physiology behind the epileptiform discharge is due to the chronic dysfunction or "defect" in the epileptic brain, i.e., the epileptic brain is not normal even during seizure free time [35]. Though the hippocampus was nonepileptogenic for these subjects, its H is still less than a normal person which may be due to its participation in secondary, nonautonomous epileptic processes initiated by the epileptic zone [1]. The wide dispersion in H for the EEG recorded from the epileptic zone in seizure free intervals (star) indicates that the epileptiform discharges are intermittent probably due to the chronic presence of abnormal epileptogenic tissues [36, 37]. EEG recording during seizure may not be economical and hence it may be better to locate epileptic zone by recording EEG during seizure free intervals. These analyses show the possibility of detecting the onset of the seizure state from the time dependent Hurst exponent estimated during the transition from normal to seizure state [35]. Fig 6 shows the Hurst exponents for all the epochs of five different sets that have been discussed above.

## Conclusion

In this paper we have reinvestigated the EEG data of normal and epileptic subjects to get an insight into the brain dynamics at different imposed and diseased conditions using RS surrogate analysis, PDF and H exponents. From these analysis we have found that RS and PDF may be useful to find a broad difference between normal and epileptic subjects but not helpful for constrained and seizure free intervals. Whereas, using H exponent, we have obtained differences in characteristics for normal subjects with eyes open and closed, and epileptic subjects during seizure and seizure free interval. The H shows that the brain activity of a normal man is uncorrelated in nature whereas, epileptic brains show long range anticorrelation.

## Declarations

### Acknowledgements

We gratefully acknowledge the use of TISEAN package for the estimation of the correlation dimension.

## Authors’ Affiliations

## References

- Andrzejak RG, Lehnertz K, Mormann F, Rieke C, David P, Christian EE: Indications of nonlinear deterministic and finite dimensional structures in time series of brain electrical activity: dependence on recording region and brain state. Phys Rev E. 2001, 64: 061907-10.1103/PhysRevE.64.061907.View ArticleADSGoogle Scholar
- Diambra L, Malta CP: BRCA1 protein products: functional motifs. Phys Rev E. 1999, 59: 929-10.1103/PhysRevE.59.929.View ArticleADSGoogle Scholar
- Rombouts SARB, Keunen RWM, Stam CJ: Investigation of nonlinear structure in multichannel EEG. Phys Letts A. 1995, 202: 352-10.1016/0375-9601(95)00335-Z.View ArticleADSGoogle Scholar
- Dafilis MP, David TJL, Cadusch PJ: Robust chaos in a model of the electroencephalogram: Implications for brain dynamics. Chaos. 2001, 11: 474-10.1063/1.1394193.View ArticleADSMATHGoogle Scholar
- Robinson PA, Rennie CJ, Rowe DL: Dynamics of large-scale brain activity in normal arousal states and epileptic seizures. Phys Rev E. 2002, 65: 041924-10.1103/PhysRevE.65.041924.View ArticleADSGoogle Scholar
- Stam CJ: Nonlinear dynamical analysis of EEG and MEG: Review of an emerging field. Clinical Neurophysiology. 2005, 116: 2266-2301. 10.1016/j.clinph.2005.06.011.View ArticleGoogle Scholar
- Pradhan N, Sadasivan PK: Relevence of surrogate-data testing in electroencephalograms. Phys Rev E. 1996, 53: 2684-10.1103/PhysRevE.53.2684.View ArticleADSGoogle Scholar
- Krakovská A, Štolc SJ: Spectral decay vs. correlation dimension of EEG. Neurocomputing. 2008, 71: 2978-10.1016/j.neucom.2007.06.007.View ArticleGoogle Scholar
- Pereda E, Gamundi A, Rial R, Gonzalez J: Non-linear behaviour of human EEG: fractal exponent versus correlation dimension in awake and sleep stages. Neurosci Lett. 1998, 250: 91-10.1016/S0304-3940(98)00435-2.View ArticleGoogle Scholar
- Pereda E, Gamundi A, Nicolau MC, Rial R, Gonzalez J: Interhemispheric differences in awake and sleep human EEG: a comparison between nonlinear and spectral measures. Neurosci Lett. 1999, 263: 37-10.1016/S0304-3940(99)00104-4.View ArticleGoogle Scholar
- Hughes JR: Progress in predicting seizure episodes with nonlinear methods. Epilepsy & Behavior. 2008, 12: 128-10.1016/j.yebeh.2007.08.004.View ArticleGoogle Scholar
- Mormann F, Kreuz T, Rieke C, Andrzejak RG, Kraskov A, David P, Christian Elger E, Lehnertza K: On the predictability of epileptic seizures. Clin Neurophysiol. 2005, 116: 569-10.1016/j.clinph.2004.08.025.View ArticleGoogle Scholar
- Jerger KK, Theoden NI, Joseph TF, Timothy S, Pecora L, Steven WL, Steven SJ: Early seizure detection. J Clin Neurophysiol. 2001, 18: 259-10.1097/00004691-200105000-00005.View ArticleGoogle Scholar
- Lopes da Silva FH, Blanes W, Kalitzin SN, Parra J, Suffczynski P, Velis DN: Dynamical diseases of brain systems: different routes to epileptic seizures. IEEE Trans Biomed Eng. 2003, 50: 540-10.1109/TBME.2003.810703.View ArticleGoogle Scholar
- Slutzky MW, Cvitanovic P, Mogul DJ: Deterministic chaos and noise in three in vitro hippocampal models of epilepsy. Ann Biomed Eng. 2001, 29: 607-10.1114/1.1380419.View ArticleGoogle Scholar
- Savit R, Li D, Zhou W, I D: Understanding dynamic state changes in temporal lobe epilepsy. J Clin Neurophysiol. 2001, 18: 246-10.1097/00004691-200105000-00004.View ArticleGoogle Scholar
- Gautama T, Mandic DP, Hulle MMV: Indications of nonlinear structures in brain electrical activity. Phys Rev E. 2003, 67: 046204-10.1103/PhysRevE.67.046204.View ArticleADSGoogle Scholar
- Harikrishnan K, Misra R, Ambika G, Kembhavi A: A non-subjective approach to the GP algorithm for analysing noisy time series. Physica D. 2006, 215: 137-10.1016/j.physd.2006.01.027.View ArticleADSMathSciNetMATHGoogle Scholar
- EEG time series download page. [http://www.meb.uni-bonn.de/epileptologie/cms/front_content.php?idcat=193]
- Pijn JP, Velis DN, Heyden van der MJ, DeGoede J, van Veelen CW, Lopes da Silva FH: Nonlinear dynamics of epileptic seizures on basis of intracranial EEG recordings. Brain Topogr. 1997, 9: 249-10.1007/BF01464480.View ArticleGoogle Scholar
- Shen Y, Olbricha E, Achermann P, Meier P: Dimensional complexity and spectral properties of the human sleep EEG. Clinical Neurophysiology. 2003, 114: 199-10.1016/S1388-2457(02)00338-3.View ArticleGoogle Scholar
- Lee JS, Yang BH, Lee JH, Choi JH, Choi IG, Kim SB: Detrended fluctuation analysis of resting EEG in depressed outpatients and healthy controls. Clinical Neurophysiology. 2007, 118: 2489-10.1016/j.clinph.2007.08.001.View ArticleGoogle Scholar
- Kannathal N, Acharya UR, Lim C, Sadasivan PK: Characterization of EEG-A comparative study. Computer Methods and Programs in Biomedicine. 2005, 80: 17-10.1016/j.cmpb.2005.06.005.View ArticleGoogle Scholar
- Freeman WJ, Holmes MD, Burke BC, Vanhatalo S: Spatial spectra of scalp EEG and EMG from awake humans. Clinical Neurophysiology. 2003, 114: 1053-10.1016/S1388-2457(03)00045-2.View ArticleGoogle Scholar
- Robinson PA, Rennie CJ, Wright JJ, Bahramali H, Gordon E, Rowe DL: Prediction of electroencephalographic spectra from neurophysiology. Phys Rev E. 2001, 63: 021903-10.1103/PhysRevE.63.021903.View ArticleADSGoogle Scholar
- Nikolic D, Moca VV, Singera W, Muresan RC: Properties of multivariate data investigated by fractal dimensionality. Journal of Neuroscience Methods. 2008, 172: 27-10.1016/j.jneumeth.2008.04.007.View ArticleGoogle Scholar
- Natarajan K, Acharya R, Alias F, Tiboleng T, Puthusserypady SK: Nonlinear analysis of EEG signals at different mental states. BioMedical Engineering OnLine. 2004, 3: 7-10.1186/1475-925X-3-7.View ArticleGoogle Scholar
- Theiler J, Eubank S, Longtin A, Galdrikian B, Farmer D: Testing for nonlinearity in time series: the method of surrogate data. Physica D. 1992, 58: 77-10.1016/0167-2789(92)90102-S.View ArticleADSMATHGoogle Scholar
- Nakamura T, Small M: Applying the method of Small-Shuffle surrogate data: Testing for dynamics in fluctuating data with trends. International Journal of Bifurcations and Chaos. 2006, 16: 3581-10.1142/S0218127406016999.View ArticleMATHGoogle Scholar
- Small M, Tse CK: Detecting determinism in time series: The method of surrogate data. IEEE Transactions on circuits and systems-I. 2003, 50: 663-10.1109/TCSI.2003.811020.View ArticleMathSciNetGoogle Scholar
- van Milligen BP, Pedrosa MA, Balbín R, Hidalgo C, Newman DE, Sánchez E, Frances M, García-Cortés I, Bleuel J, Endler M, Riccardi C, Davies S, Matthews GF, Latten A, Klinger T: Self-similarity of the plasma edge fluctuations. Phys Plasmas. 1998, 5: 3632-10.1063/1.873081.View ArticleADSGoogle Scholar
- Dori G, Fishman S, Ben-Haim SA: The correlation dimension of rat hearts in an experimentally controlled environment. Chaos. 2000, 10: 257-10.1063/1.166471.View ArticleADSGoogle Scholar
- Harrison MAF, Osorio I, Frei MG, Asuri S, Lai YC: Correlation dimension and integral do not predict epileptic seizures. Chaos. 2005, 15: 033106-10.1063/1.1935138.View ArticleADSGoogle Scholar
- Nurujjaman M, Iyengar ANS: Realization of SOC behavior in a dc glow discharge plasma. Phys Letts A. 2007, 360: 717-10.1016/j.physleta.2006.09.005.View ArticleADSGoogle Scholar
- Cajueiro DO, Tabak BM: The Hurst exponent over time: testing the assertion that emerging markets are becoming more efficient. Physica A. 2004, 336: 521-10.1016/j.physa.2003.12.031.View ArticleADSMathSciNetGoogle Scholar
- Schwartzkroin PA: Progress in Epilepsy Research: Origins of the Epileptic State 38 (8): 853–858 (1997). Epilepsia. 1997, 38: 853-10.1111/j.1528-1157.1997.tb01250.x.View ArticleGoogle Scholar
- Bromfield EB: Epileptiform Discharges. [http://emedicine.medscape.com/article/1138880-overview]

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