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基于新型小波包分解与典型相关分析联用的单通道 EEG 和 fNIRS 运动伪迹校正。

Motion Artifacts Correction from Single-Channel EEG and fNIRS Signals Using Novel Wavelet Packet Decomposition in Combination with Canonical Correlation Analysis.

机构信息

Department of Electrical, Electronic and Systems Engineering, Universiti Kebangsaan Malaysia, Bangi 43600, Malaysia.

Department of Electrical Engineering, Qatar University, Doha 2713, Qatar.

出版信息

Sensors (Basel). 2022 Apr 21;22(9):3169. doi: 10.3390/s22093169.

DOI:10.3390/s22093169
PMID:35590859
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9102309/
Abstract

The electroencephalogram (EEG) and functional near-infrared spectroscopy (fNIRS) signals, highly non-stationary in nature, greatly suffers from motion artifacts while recorded using wearable sensors. Since successful detection of various neurological and neuromuscular disorders is greatly dependent upon clean EEG and fNIRS signals, it is a matter of utmost importance to remove/reduce motion artifacts from EEG and fNIRS signals using reliable and robust methods. In this regard, this paper proposes two robust methods: (i) Wavelet packet decomposition (WPD) and (ii) WPD in combination with canonical correlation analysis (WPD-CCA), for motion artifact correction from single-channel EEG and fNIRS signals. The efficacy of these proposed techniques is tested using a benchmark dataset and the performance of the proposed methods is measured using two well-established performance matrices: (i) difference in the signal to noise ratio ( ) and (ii) percentage reduction in motion artifacts ( ). The proposed WPD-based single-stage motion artifacts correction technique produces the highest average (29.44 dB) when db2 wavelet packet is incorporated whereas the greatest average (53.48%) is obtained using db1 wavelet packet for all the available 23 EEG recordings. Our proposed two-stage motion artifacts correction technique, i.e., the WPD-CCA method utilizing db1 wavelet packet has shown the best denoising performance producing an average and values of 30.76 dB and 59.51%, respectively, for all the EEG recordings. On the other hand, for the available 16 fNIRS recordings, the two-stage motion artifacts removal technique, i.e., WPD-CCA has produced the best average (16.55 dB, utilizing db1 wavelet packet) and largest average (41.40%, using fk8 wavelet packet). The highest average and using single-stage artifacts removal techniques (WPD) are found as 16.11 dB and 26.40%, respectively, for all the fNIRS signals using fk4 wavelet packet. In both EEG and fNIRS modalities, the percentage reduction in motion artifacts increases by 11.28% and 56.82%, respectively when two-stage WPD-CCA techniques are employed in comparison with the single-stage WPD method. In addition, the average also increases when WPD-CCA techniques are used instead of single-stage WPD for both EEG and fNIRS signals. The increment in both and values is a clear indication that two-stage WPD-CCA performs relatively better compared to single-stage WPD. The results reported using the proposed methods outperform most of the existing state-of-the-art techniques.

摘要

脑电图 (EEG) 和功能近红外光谱 (fNIRS) 信号本质上高度非平稳,在使用可穿戴传感器记录时会受到运动伪影的极大影响。由于各种神经和神经肌肉疾病的成功检测在很大程度上取决于干净的 EEG 和 fNIRS 信号,因此使用可靠和强大的方法从 EEG 和 fNIRS 信号中去除/减少运动伪影是至关重要的。在这方面,本文提出了两种强大的方法:(i)小波包分解(WPD)和(ii)WPD 与典型相关分析(WPD-CCA)的组合,用于从单通道 EEG 和 fNIRS 信号中校正运动伪影。使用基准数据集测试了这些建议技术的有效性,并使用两个成熟的性能矩阵测量了这些方法的性能:(i)信噪比的差异()和(ii)运动伪影减少的百分比()。当使用 db2 小波包时,基于 WPD 的单阶段运动伪影校正技术产生的最高平均(29.44 dB),而对于所有可用的 23 个 EEG 记录,使用 db1 小波包获得的最大平均(53.48%)。我们提出的两阶段运动伪影校正技术,即使用 db1 小波包的 WPD-CCA 方法,为所有 EEG 记录产生了最佳的去噪性能,产生平均和值分别为 30.76 dB 和 59.51%。另一方面,对于可用的 16 个 fNIRS 记录,两阶段运动伪影去除技术,即 WPD-CCA,使用 db1 小波包产生了最佳的平均(16.55 dB)和最大平均(41.40%,使用 fk8 小波包)。对于所有 fNIRS 信号,使用 fk4 小波包的单阶段伪影去除技术(WPD)产生的最高平均(16.11 dB)和最大平均(26.40%)。在 EEG 和 fNIRS 两种模式下,与单阶段 WPD 方法相比,使用两阶段 WPD-CCA 技术可分别将运动伪影减少 11.28%和 56.82%。此外,当使用 WPD-CCA 技术而不是单阶段 WPD 时,平均也会增加。和值的增加清楚地表明,两阶段 WPD-CCA 的性能相对优于单阶段 WPD。使用所提出的方法报告的结果优于大多数现有的最先进技术。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/bb9af0580348/sensors-22-03169-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/212e8dd4d617/sensors-22-03169-g001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/f95a7e0bd0e8/sensors-22-03169-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/bb9af0580348/sensors-22-03169-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/212e8dd4d617/sensors-22-03169-g001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/e01c00f93a9b/sensors-22-03169-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/ed55db022b89/sensors-22-03169-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/fa434adce46e/sensors-22-03169-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/f95a7e0bd0e8/sensors-22-03169-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f069/9102309/bb9af0580348/sensors-22-03169-g010.jpg

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