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The Effect of Head Model Simplification on Beamformer Source Localization

Beamformers are a widely-used tool in brain analysis with magnetoencephalography (MEG) and electroencephalography (EEG). For the construction of the beamformer filters realistic head volume conductor modeling is necessary for accurately computing the EEG and MEG leadfields, i.e., for solving the EEG...

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Autores principales: Neugebauer, Frank, Möddel, Gabriel, Rampp, Stefan, Burger, Martin, Wolters, Carsten H.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Frontiers Media S.A. 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5701642/
https://www.ncbi.nlm.nih.gov/pubmed/29209157
http://dx.doi.org/10.3389/fnins.2017.00625
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author Neugebauer, Frank
Möddel, Gabriel
Rampp, Stefan
Burger, Martin
Wolters, Carsten H.
author_facet Neugebauer, Frank
Möddel, Gabriel
Rampp, Stefan
Burger, Martin
Wolters, Carsten H.
author_sort Neugebauer, Frank
collection PubMed
description Beamformers are a widely-used tool in brain analysis with magnetoencephalography (MEG) and electroencephalography (EEG). For the construction of the beamformer filters realistic head volume conductor modeling is necessary for accurately computing the EEG and MEG leadfields, i.e., for solving the EEG and MEG forward problem. In this work, we investigate the influence of including realistic head tissue compartments into a finite element method (FEM) model on the beamformer's localization ability. Specifically, we investigate the effect of including cerebrospinal fluid, gray matter, and white matter distinction, as well as segmenting the skull bone into compacta and spongiosa, and modeling white matter anisotropy. We simulate an interictal epileptic measurement with white sensor noise. Beamformer filters are constructed with unit gain, unit array gain, and unit noise gain constraint. Beamformer source positions are determined by evaluating power and excess sample kurtosis (g(2)) of the source-waveforms at all source space nodes. For both modalities, we see a strong effect of modeling the cerebrospinal fluid and white and gray matter. Depending on the source position, both effects can each be in the magnitude of centimeters, rendering their modeling necessary for successful localization. Precise skull modeling mainly effected the EEG up to a few millimeters, while both modalities could profit from modeling white matter anisotropy to a smaller extent of 5–10 mm. The unit noise gain or neural activity index beamformer behaves similarly to the array gain beamformer when noise strength is sufficiently high. Variance localization seems more robust against modeling errors than kurtosis.
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spelling pubmed-57016422017-12-05 The Effect of Head Model Simplification on Beamformer Source Localization Neugebauer, Frank Möddel, Gabriel Rampp, Stefan Burger, Martin Wolters, Carsten H. Front Neurosci Neuroscience Beamformers are a widely-used tool in brain analysis with magnetoencephalography (MEG) and electroencephalography (EEG). For the construction of the beamformer filters realistic head volume conductor modeling is necessary for accurately computing the EEG and MEG leadfields, i.e., for solving the EEG and MEG forward problem. In this work, we investigate the influence of including realistic head tissue compartments into a finite element method (FEM) model on the beamformer's localization ability. Specifically, we investigate the effect of including cerebrospinal fluid, gray matter, and white matter distinction, as well as segmenting the skull bone into compacta and spongiosa, and modeling white matter anisotropy. We simulate an interictal epileptic measurement with white sensor noise. Beamformer filters are constructed with unit gain, unit array gain, and unit noise gain constraint. Beamformer source positions are determined by evaluating power and excess sample kurtosis (g(2)) of the source-waveforms at all source space nodes. For both modalities, we see a strong effect of modeling the cerebrospinal fluid and white and gray matter. Depending on the source position, both effects can each be in the magnitude of centimeters, rendering their modeling necessary for successful localization. Precise skull modeling mainly effected the EEG up to a few millimeters, while both modalities could profit from modeling white matter anisotropy to a smaller extent of 5–10 mm. The unit noise gain or neural activity index beamformer behaves similarly to the array gain beamformer when noise strength is sufficiently high. Variance localization seems more robust against modeling errors than kurtosis. Frontiers Media S.A. 2017-11-09 /pmc/articles/PMC5701642/ /pubmed/29209157 http://dx.doi.org/10.3389/fnins.2017.00625 Text en Copyright © 2017 Neugebauer, Möddel, Rampp, Burger and Wolters. http://creativecommons.org/licenses/by/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
spellingShingle Neuroscience
Neugebauer, Frank
Möddel, Gabriel
Rampp, Stefan
Burger, Martin
Wolters, Carsten H.
The Effect of Head Model Simplification on Beamformer Source Localization
title The Effect of Head Model Simplification on Beamformer Source Localization
title_full The Effect of Head Model Simplification on Beamformer Source Localization
title_fullStr The Effect of Head Model Simplification on Beamformer Source Localization
title_full_unstemmed The Effect of Head Model Simplification on Beamformer Source Localization
title_short The Effect of Head Model Simplification on Beamformer Source Localization
title_sort effect of head model simplification on beamformer source localization
topic Neuroscience
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5701642/
https://www.ncbi.nlm.nih.gov/pubmed/29209157
http://dx.doi.org/10.3389/fnins.2017.00625
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