Recognition of Emotional States Using Multiscale Information Analysis of High Frequency EEG Oscillations
Abstract
:1. Introduction
2. Materials and Methods
2.1. Database
2.1.1. Signals
2.1.2. Labels
2.2. Methods.
2.2.1. Data Preprocessing
2.2.2. Multiscale EEG Complexity in the Time Domain
- First, set different time scale τ from 1 to s.
- xi is divided into non-overlapping windows of equal length M.
- Above all, it is called coarse graining, and SE was then calculated for each coarse-graining time series in different scale factors.
- When all SE for time scale τ from 1 to s are calculated, the MSE(τ) series was the multiscale entropy of the original time series.
- Obtain the MSE curve for all samples (32 channels, 20-second, m = 2, and r = 0.15) of each subject.
- Make a classification on each scale and find the range of scales that have higher accuracy.
- Calculate the area under the MSE curve of higher accuracy range as MECI.
2.2.3. Multiscale Analysis Methods in Frequency Domain
Empirical Mode Decomposition and Ensemble Empirical Mode Decomposition
- Obtain the upper envelope Ui and lower envelope Li of the original signal xi.
- Then, calculate the mean envelope Mi of the upper and lower envelope.
- Middle signal is obtained by subtracting the mean envelope from the original signals.
- Determine whether the middle signal satisfies the IMF-conditions.
- a)
- Throughout the data segment, the number of extreme points and the number of zero crossing points must be equal or not more than 1.
- b)
- The mean envelope of the upper and lower envelope at any data segments is 0, which means the upper and lower envelope is asymmetry.
- If Mi satisfied the conditions, the IMF = Mi and the new original data is obtained by subtracting the IMF from xi. Repeat step a to step d. If Mi does not satisfy the conditions, the Mi is the new original data and repeat step a to step d.
- Lastly, we get several IMFs j = 1, 2, 3, …, m and a remaining signal ri.
- The first, white noise of finite amplitude is added to the original.
- EMD is used to calculate IMFs.
- Repeat step a and b many times.
- When n-th noise is added, we calculate the average IMFs.
Comparison of EMD and EEMD
- Clean signals: they have no EOG artifacts, baseline drift, head movement artifacts, or other obvious artifacts.
- EOG affected signals: they have clear EOG artifacts and head movement artifacts, but no baseline drift.
- Baseline signals: they are low-frequency baselines.
EEMD Enhanced Energy and Entropy
- (1)
- Decompose the EEG signals of all samples (32 channels, 20-second, noise ratio = 0.1 and ensemble 100 times) into several IMFs with a different frequency scale using EEMD.
- (2)
- Compute the Energy and Entropy of each IMF.
- a)
- EnergyWhen applying EEMD on EEG signals, EOG artifacts are not removed. We did not use the normalized energy of the IMF in this study.
- b)
- Sample EntropySample entropy is a modification of approximate entropy [36]. We have an and use a time interval to reconstruct series . The length of sequence is m. The distance function of two sequences is . For a given embedding dimension m, tolerance r and number of data points N, SE is expressed as:The tolerance level r is usually set to a percentage of the standard deviation of the normalized data. For our case, we selected 0.15.
- c)
- Fuzzy EntropyFuzzy entropy [38] is the entropy of a fuzzy set, which loosely represents the information of uncertainty.For an , we reconstruct series with length m:The distance function of two sequences is . Given n and r, calculate the similarity degree through a fuzzy function .Define the function asis got similarly. Lastly, the of the series is shown below.
- d)
- Renyi EntropyThere is an and that adopts n values with probabilities .The Renyi entropy [22] of order α, where and , is defined as:We used the gaussian kernel to obtain the probability density function before calculating RE.
- (3)
- Accumulate the IMFs one by one and compute the energy and entropy of combined IMFs.
2.2.4. Support Vector Machine
2.2.5. Statistical Methods
3. Results
3.1. Distinguishability of Emotional States in Four Dimensions Based on Time-Frequency Analysis
3.2. Multiscale EEG Complexity Analysis in the Time Domain
3.3. Multiscale Information Analysis in Frequency Domain Based on EEMD
3.3.1. EEMD Enhanced Energy Analysis Based on the High Frequency EEG Oscillations
3.3.2. EEMD Enhanced Entropy Analysis Based on the High Frequency EEG Oscillations
3.4. Comparison between Different Brain Regions
3.5. Comparison of Multiscale Information Analysis Methods with Classical Methods
4. Discussion
- The classification accuracy of four-dimensional emotion recognition is associated with the high frequency oscillations (51–100 Hz) of EEG than the low frequency oscillations (0.3–49 Hz).
- The frontal and temporal regions play much more important roles in emotion recognition than other regions.
- The performance of MIA methods is better than classical methods like energy based on DWT, FD, and SE.
Author Contributions
Funding
Conflicts of Interest
References
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Components | Frequency Range (Hz) | Accuracy of Four Dimensional Emotions (%) | Correlation (IMF2) | Energy Ratio (IMF2) |
---|---|---|---|---|
IMF1 | (64, 256) | 43.96 ± 7.16 | 0.6932 | 7.1156 |
IMF2 | (32, 128) | 53.88 ± 11.04 | 1.0000 | 1.0000 |
IMF3 | (16, 64) | 46.20 ± 8.87 | 0.5447 | 0.4945 |
IMF4 | (8, 32) | 43.05 ± 7.74 | 0.1290 | 0.4511 |
IMF1-2 | (32, 256) | 52.81 ± 9.74 | 0.9510 | 0.6111 |
IMF1-3 | (16, 256) | 47.86 ± 7.92 | 0.8333 | 0.1751 |
IMF1-4 | (8, 256) | 47.55 ± 9.22 | 0.6600 | 0.0857 |
IMF2-3 | (16, 128) | 48.10 ± 9.66 | 0.7722 | 0.2251 |
IMF2-4 | (8, 128) | 47.32 ± 10.16 | 0.5704 | 0.1038 |
Methods | Features | Accuracy of Four Dimensional Emotions (%) | Accuracy of Four Dimensional Emotions Based on Combined Features (%) |
---|---|---|---|
Classical Methods | FD | 39.51 ± 8.07 | 43.98 ± 8.88 |
SE | 42.42 ± 9.00 | ||
Energy of Beta | 44.56 ± 8.49 | ||
Energy of Gamma | 45.65 ± 10.00 | ||
MIA Methods | MECI | 53.46 ± 9.68 | 62.01 ± 10.27 |
EEMD enhanced Energy | 53.62 ± 10.80 | ||
EEMD enhance FE | 53.70 ± 8.18 |
Methods | Evaluations | HVHA | HVLA | LVHA | LVLA | Average |
---|---|---|---|---|---|---|
Classical Methods | Precision | 44.97% | 46.85% | 40.16% | 43.24% | 43.81% |
Recall/Sensitivity | 58.77% | 40.52% | 38.59% | 29.56% | 41.86% | |
Specificity | 49.14% | 78.59% | 72.34% | 81.93% | 70.50% | |
Accuracy | —— | —— | —— | —— | 43.98% | |
MIA Methods | Precision | 61.48% | 60.56% | 64.00% | 62.08% | 62.03% |
Recall/Sensitivity | 71.37% | 54.03% | 64.43% | 52.19% | 60.51% | |
Specificity | 70.99% | 87.26% | 84.78% | 88.17% | 82.80% | |
Accuracy | —— | —— | —— | —— | 62.01% |
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Gao, Z.; Cui, X.; Wan, W.; Gu, Z. Recognition of Emotional States Using Multiscale Information Analysis of High Frequency EEG Oscillations. Entropy 2019, 21, 609. https://doi.org/10.3390/e21060609
Gao Z, Cui X, Wan W, Gu Z. Recognition of Emotional States Using Multiscale Information Analysis of High Frequency EEG Oscillations. Entropy. 2019; 21(6):609. https://doi.org/10.3390/e21060609
Chicago/Turabian StyleGao, Zhilin, Xingran Cui, Wang Wan, and Zhongze Gu. 2019. "Recognition of Emotional States Using Multiscale Information Analysis of High Frequency EEG Oscillations" Entropy 21, no. 6: 609. https://doi.org/10.3390/e21060609
APA StyleGao, Z., Cui, X., Wan, W., & Gu, Z. (2019). Recognition of Emotional States Using Multiscale Information Analysis of High Frequency EEG Oscillations. Entropy, 21(6), 609. https://doi.org/10.3390/e21060609