Winter William R, Nunez Paul L, Ding Jian, Srinivasan Ramesh
Department of Biomedical Engineering, Tulane University, New Orleans, LA, USA.
Stat Med. 2007 Sep 20;26(21):3946-57. doi: 10.1002/sim.2978.
We analyzed models of volume conduction and magnetic field spread to account for aspects of spatial structure in electroencephalographic (EEG) and magnetoencephalographic (MEG) coherence. The head volume conduction model consisted of three confocal ellipsoids, representing three layers (brain, skull, and scalp) with different tissue conductivities, while the magnetic field model follows from the Biot-Savart law in a spherically symmetric medium. Source models were constructed based on magnetic resonance imaging data from three subjects, approximating neocortical current source distributions as dipoles oriented perpendicular to the local cortical surface. Assuming that every source is uncorrelated to every other source, coherence between sensors due to volume conduction and field-spread effects was estimated. Spatial properties of the model coherences were then compared with simultaneously recorded spontaneous EEG and MEG. In both models and experimental data, EEG and MEG coherence was elevated between closely spaced channels. At very large channel separations, the field-spread effect on MEG coherence appears smaller than the volume conduction effect on EEG coherence. In EEG coherence studies, surface Laplacian methods can be used to remove volume conduction effects. With single-coil magnetometers, MEG coherences are free of field effects only for sensor pairs separated by more than 20 cm. Model coherences resemble most high-frequency (e.g. >20 Hz) data; volume conduction and field-spread effects are independent of frequency, suggesting mostly uncorrelated sources in these bands. High-frequency EEG and MEG coherence can evidently serve as an estimate of coherence effects due to volume conduction and field effects, when source and head models are not available for individual subjects.
我们分析了容积传导和磁场传播模型,以解释脑电图(EEG)和脑磁图(MEG)相干性中的空间结构方面。头部容积传导模型由三个共焦椭球体组成,代表具有不同组织电导率的三层(大脑、颅骨和头皮),而磁场模型则基于球对称介质中的毕奥 - 萨伐尔定律。源模型是根据来自三名受试者的磁共振成像数据构建的,将新皮质电流源分布近似为垂直于局部皮质表面定向的偶极子。假设每个源与其他每个源不相关,估计了由于容积传导和场传播效应导致的传感器之间的相干性。然后将模型相干性的空间特性与同时记录的自发EEG和MEG进行比较。在模型和实验数据中,紧密间隔的通道之间的EEG和MEG相干性都有所提高。在非常大的通道间距下,磁场传播对MEG相干性的影响似乎小于容积传导对EEG相干性的影响。在EEG相干性研究中,表面拉普拉斯方法可用于消除容积传导效应。对于单线圈磁力计,只有当传感器对之间的距离超过20厘米时,MEG相干性才不受场效应的影响。模型相干性与大多数高频(例如>20 Hz)数据相似;容积传导和场传播效应与频率无关,这表明在这些频段中源大多不相关。当无法获得个体受试者的源模型和头部模型时,高频EEG和MEG相干性显然可作为由于容积传导和场效应导致的相干性效应的估计。
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