Vorwerk Johannes, Cho Jae-Hyun, Rampp Stefan, Hamer Hajo, Knösche Thomas R, Wolters Carsten H
Institut für Biomagnetismus und Biosignalanalyse, Westfälische Wilhelms-Universität, Münster, Germany.
Max Planck Institute for Human Cognitive and Brain Sciences, Leipzig, Germany.
Neuroimage. 2014 Oct 15;100:590-607. doi: 10.1016/j.neuroimage.2014.06.040. Epub 2014 Jun 25.
For accurate EEG/MEG source analysis it is necessary to model the head volume conductor as realistic as possible. This includes the distinction of the different conductive compartments in the human head. In this study, we investigated the influence of modeling/not modeling the conductive compartments skull spongiosa, skull compacta, cerebrospinal fluid (CSF), gray matter, and white matter and of the inclusion of white matter anisotropy on the EEG/MEG forward solution. Therefore, we created a highly realistic 6-compartment head model with white matter anisotropy and used a state-of-the-art finite element approach. Starting from a 3-compartment scenario (skin, skull, and brain), we subsequently refined our head model by distinguishing one further of the above-mentioned compartments. For each of the generated five head models, we measured the effect on the signal topography and signal magnitude both in relation to a highly resolved reference model and to the model generated in the previous refinement step. We evaluated the results of these simulations using a variety of visualization methods, allowing us to gain a general overview of effect strength, of the most important source parameters triggering these effects, and of the most affected brain regions. Thereby, starting from the 3-compartment approach, we identified the most important additional refinement steps in head volume conductor modeling. We were able to show that the inclusion of the highly conductive CSF compartment, whose conductivity value is well known, has the strongest influence on both signal topography and magnitude in both modalities. We found the effect of gray/white matter distinction to be nearly as big as that of the CSF inclusion, and for both of these steps we identified a clear pattern in the spatial distribution of effects. In comparison to these two steps, the introduction of white matter anisotropy led to a clearly weaker, but still strong, effect. Finally, the distinction between skull spongiosa and compacta caused the weakest effects in both modalities when using an optimized conductivity value for the homogenized compartment. We conclude that it is highly recommendable to include the CSF and distinguish between gray and white matter in head volume conductor modeling. Especially for the MEG, the modeling of skull spongiosa and compacta might be neglected due to the weak effects; the simplification of not modeling white matter anisotropy is admissible considering the complexity and current limitations of the underlying modeling approach.
为了进行准确的脑电图/脑磁图源分析,有必要尽可能逼真地对头容积导体进行建模。这包括区分人类头部不同的导电腔室。在本研究中,我们调查了对头容积导体中的海绵状颅骨、致密颅骨、脑脊液(CSF)、灰质和白质导电腔室进行建模/不建模以及纳入白质各向异性对脑电图/脑磁图正向解的影响。因此,我们创建了一个具有白质各向异性的高度逼真的六腔室头部模型,并使用了先进的有限元方法。从三腔室模型(皮肤、颅骨和大脑)开始,我们随后通过区分上述另一个腔室来细化我们的头部模型。对于生成的五个头部模型中的每一个,我们测量了相对于高分辨率参考模型以及上一步细化生成的模型对信号地形图和信号幅度的影响。我们使用各种可视化方法评估了这些模拟结果,使我们能够全面了解影响强度、触发这些影响的最重要源参数以及受影响最严重的脑区。由此,从三腔室方法开始,我们确定了头容积导体建模中最重要的额外细化步骤。我们能够表明,纳入电导率值已知的高导电性脑脊液腔室对两种模式下的信号地形图和幅度都有最强的影响。我们发现灰质/白质区分的影响几乎与纳入脑脊液的影响一样大,并且对于这两个步骤,我们都在影响的空间分布中确定了清晰的模式。与这两个步骤相比,引入白质各向异性导致的影响明显较弱,但仍然很大。最后,当对均质化腔室使用优化的电导率值时,海绵状颅骨和致密颅骨之间的区分在两种模式下产生的影响最弱。我们得出结论,在头容积导体建模中纳入脑脊液并区分灰质和白质是非常值得推荐的。特别是对于脑磁图,由于影响较弱,海绵状颅骨和致密颅骨的建模可能会被忽略;考虑到基础建模方法的复杂性和当前局限性,不模拟白质各向异性的简化是可以接受的。