Nonlinear properties of multistable states of intracranial EEG

Poster No:

1339 

Submission Type:

Abstract Submission 

Authors:

Ying Wang1, Min Li2, Ronaldo García Reyes3, Jorge Bosch-Bayard4, Maria Bringas-Vega1, Ludovico Minati1, Pedro Valdes-Sosa1

Institutions:

1University of Electronic Science and Technology of China, Chengdu, China, 2Hangzhou Dianzi University, Hangzhou, China, 3Cuban Center for Neurocience, La Habana, Cuba, 4Universidad Autónoma de Madrid, Madrid, Spain

First Author:

Ying Wang  
University of Electronic Science and Technology of China
Chengdu, China

Co-Author(s):

Min Li  
Hangzhou Dianzi University
Hangzhou, China
Ronaldo García Reyes  
Cuban Center for Neurocience
La Habana, Cuba
Jorge Bosch-Bayard  
Universidad Autónoma de Madrid
Madrid, Spain
Maria Bringas-Vega  
University of Electronic Science and Technology of China
Chengdu, China
Ludovico Minati  
University of Electronic Science and Technology of China
Chengdu, China
Pedro Valdes-Sosa  
University of Electronic Science and Technology of China
Chengdu, China

Introduction:

Multistability, the presence of multiple stable states (attractors) in dynamical systems, is crucial in neuroscience, especially for EEG studies[1–5]. It reflects transitions between distinct modes of brain activity. Linear models, with their single global attractor, fail to capture these complex multistable dynamics.
Threshold autoregressive (TAR) models [6,7] have been used for neural dynamics [8]. While TAR approximates attractors using piecewise linear models, it struggles with threshold determination in high-dimensional systems and often requires multiple models per attractor. Parametric nonlinear AR (NAR) such as NARMAX [9] depend heavily on order selection and parameter fitting, making them unrobust for complex, high-dimensional data with unknown structure.
Nonparametric approaches, such as nonparametric NAR (NNAR) with Nadaraya-Watson estimators, overcome these limitations by directly modeling dynamics from data, with bandwidth as the only key parameter [10,8]. Although NNAR effectively captures phenomena such as spiking wave limit cycles, their performance declines in multistable systems due to the inherent variability in attractors' intrinsic dimensions and scales. A global bandwidth fails to account for local properties, leading to poor representation of dynamics. And Implicit multistability is not conducive to interpretability.
To address these challenges, we propose a nonlinear clustering-based approach inspired by microstates[11]. By clustering states in high-dimensional embedding spaces, we enable localized modeling within each cluster, improving accuracy and interpretability. This method captures each attractor's local features and provides a robust framework for understanding their domains of attraction. Additionally, our findings align with frequency domain nonlinear characteristics identified by the HOXiAlpha (Higher Order XiAlpha) model[12].

Methods:

We applied Gaussian Mixture Modeling (GMM) to high-dimensional iEEG embeddings to identify clusters corresponding to distinct attractor states. Nonparametric NAR was applied within each cluster to estimate local nonlinear dynamics. The embedding dimension was optimized using AICc (Corrected Akaike information criteria) from linear AR model, while the number of clusters was guided by established bistability in EEG [1–3]. The CNAR (cluster NAR) model iteratively refines cluster assignments and model parameters using an Expectation-Maximization (EM) algorithm. We validated the approach on 1772 channels of sEEG and ECoG recordings from 106 patients [13]. Spectral dynamics of the reconstructed time series were evaluated using higher-order spectrum-bicoherence, to identify phase coupling and nonlinear frequency interactions in the full model and within each attractor.

Results:

The CNAR model successfully partitioned the state space into distinct clusters, each representing a localized dynamical regime. Simulated time series accurately replicated the temporal structure and nonlinear interactions observed in the original data, including the harmonic contributions of individual attractors. Bicoherence revealed robust phase coupling, with significant bicoherence peaks indicative of nonlinear frequency interactions specific to each attractor. The spectra and bicoherence of the limit cycle corresponding to the alpha process we spilite with our previous study with HOXiAlpha model. PCA projections showed well-preserved attractor-like geometry structures.
Supporting Image: ohbm_fig1.png
Supporting Image: ohbm_fig2.png
 

Conclusions:

The CNAR model provides a powerful framework for characterizing multistability in iEEG data, offering both interpretability and precision in modeling complex nonlinear dynamics. Its ability to simulate realistic time series and uncover higher-order spectral interactions makes it a valuable tool for advancing our understanding of brain dynamics. This approach has potential applications in clinical and cognitive neuroscience, particularly for investigating pathophysiological conditions characterized by disrupted multistability.

Modeling and Analysis Methods:

EEG/MEG Modeling and Analysis 1
Methods Development 2
Task-Independent and Resting-State Analysis

Keywords:

Computational Neuroscience
Data analysis
Electroencephaolography (EEG)
Machine Learning
Modeling
Other - Multistability

1|2Indicates the priority used for review

Abstract Information

By submitting your proposal, you grant permission for the Organization for Human Brain Mapping (OHBM) to distribute your work in any format, including video, audio print and electronic text through OHBM OnDemand, social media channels, the OHBM website, or other electronic publications and media.

I accept

The Open Science Special Interest Group (OSSIG) is introducing a reproducibility challenge for OHBM 2025. This new initiative aims to enhance the reproducibility of scientific results and foster collaborations between labs. Teams will consist of a “source” party and a “reproducing” party, and will be evaluated on the success of their replication, the openness of the source work, and additional deliverables. Click here for more information. Propose your OHBM abstract(s) as source work for future OHBM meetings by selecting one of the following options:

I am submitting this abstract as an original work to be reproduced. I am available to be the “source party” in an upcoming team and consent to have this work listed on the OSSIG website. I agree to be contacted by OSSIG regarding the challenge and may share data used in this abstract with another team.

Please indicate below if your study was a "resting state" or "task-activation” study.

Resting state
Task-activation
Other

Healthy subjects only or patients (note that patient studies may also involve healthy subjects):

Healthy subjects

Was this research conducted in the United States?

No

Were any human subjects research approved by the relevant Institutional Review Board or ethics panel? NOTE: Any human subjects studies without IRB approval will be automatically rejected.

Yes

Were any animal research approved by the relevant IACUC or other animal research panel? NOTE: Any animal studies without IACUC approval will be automatically rejected.

Not applicable

Please indicate which methods were used in your research:

EEG/ERP
Computational modeling
Other, Please specify  -   ECoG and sEEG

Provide references using APA citation style.

[1] F Freyer, K Aquino, P A Robinson, et al. Bistability and non-gaussian fluctuations in spontaneous cortical activity[J]. Journal of Neuroscience, Society for Neuroscience, 2009, 29(26): 8512–8524.
[2] F Freyer, J A Roberts, R Becker, et al. Biophysical Mechanisms of Multistability in Resting-State Cortical Rhythms[J]. Journal of Neuroscience, Society for Neuroscience, 2011, 31(17): 6353–6361.
[3] F Freyer, J A Roberts, P Ritter, et al. A Canonical Model of Multistability and Scale-Invariance in Biological Systems[J]. BEHRENS T. PLoS Computational Biology, 2012, 8(8): e1002634.
[4] M I Rabinovich, M A Zaks, P Varona. Sequential dynamics of complex networks in mind: consciousness and creativity[J]. Physics Reports, 2020, 883: 1–32.
[5] F Hancock, F E Rosas, A I Luppi, et al. Metastability demystified — the foundational past, the pragmatic present and the promising future[J]. Nature Reviews Neuroscience, 2024.
[6] H Tong, K S Lim. Threshold Autoregression, Limit Cycles and Cyclical Data[J]. Journal of the Royal Statistical Society. Series B (Methodological), [Royal Statistical Society, Wiley], 1980, 42(3): 245–292.
[7] L Breiman. Hinging hyperplanes for regression, classification, and function approximation[J]. IEEE Transactions on Information Theory, 1993, 39(3): 999–1013.
[8] P Valdés-Sosa, J Bosch, J Jiménez, et al. The statistical identification of nonlinear brain dynamics: A progress report[G]//Non linear Dynamic and Brain Funcioning. 1999: 278–284.
[9] S A Billings. Nonlinear System Identification: NARMAX Methods in the Time, Frequency, and Spatio-Temporal Domains[M]. 第1版. Wiley, 2013.
[10] J L Hernández, P A Valdés, P Vila. EEG spike and wave modelled by a stochastic limit cycle[J]. NeuroReport, 1996, 7(13): 2246.
[11] R D Pascual-Marqui, K Kochi, T Kinoshita. On the relation between EEG microstates and cross-spectra[J]. 2022.
[12] Y Wang, M Li, J F Bosch-Bayard, et al. The EEG xi (aperiodic) spectral component, but not the alpha rhythm, is linear and gaussian[C]//The Organization for Human Brain Mapping (OHBM) 2023 Annual Meeting. 2023: 4438.
[13] B Frauscher, N Von Ellenrieder, R Zelmann, et al. Atlas of the normal intracranial electroencephalogram: neurophysiological awake activity in different cortical areas[J]. Brain, 2018, 141(4): 1130–1144.

UNESCO Institute of Statistics and World Bank Waiver Form

I attest that I currently live, work, or study in a country on the UNESCO Institute of Statistics and World Bank List of Low and Middle Income Countries list provided.

No