Sir Peter Mansfield Imaging Centre, School of Physics and Astronomy, University of Nottingham, University Park, Nottingham, NG7 2RD, UK; Department of Physics, Loughborough University, Leicestershire, LE11 3TU, UK.
Sir Peter Mansfield Imaging Centre, School of Physics and Astronomy, University of Nottingham, University Park, Nottingham, NG7 2RD, UK.
Neuroimage. 2018 Jun;173:188-198. doi: 10.1016/j.neuroimage.2018.02.034. Epub 2018 Feb 25.
Motion artefacts (MAs) are induced within EEG data collected simultaneously with fMRI when the subject's head rotates relative to the magnetic field. The effects of these artefacts have generally been ameliorated by removing periods of data during which large artefact voltages appear in the EEG traces. However, even when combined with other standard post-processing methods, this strategy does not remove smaller MAs which can dominate the neuronal signals of interest. A number of methods are therefore being developed to characterise the MA by measuring reference signals and then using these in artefact correction. These methods generally assume that the head and EEG cap, plus any attached sensors, form a rigid body which can be characterised by a standard set of six motion parameters. Here we investigate the motion of the head/EEG cap system to provide a better understanding of MAs. We focus on the reference layer artefact subtraction (RLAS) approach, as this allows measurement of a separate reference signal for each electrode that is being used to measure brain activity. Through a series of experiments on phantoms and subjects, we find that movement of the EEG cap relative to the phantom and skin on the forehead is relatively small and that this non-rigid body movement does not appear to cause considerable discrepancy in artefacts between the scalp and reference signals. However, differences in the amplitude of these signals is observed which may be due to differences in geometry of the system from which the reference signals are measured compared with the brain signals. In addition, we find that there is non-rigid body movement of the skull and skin which produces an additional MA component for a head shake, which is not present for a head nod. This results in a large discrepancy in the amplitude and temporal profile of the MA measured on the scalp and reference layer, reducing the efficacy of MA correction based on the reference signals. Together our data suggest that the efficacy of the correction of MA using any reference-based system is likely to differ for different types of head movement with head shake being the hardest to correct. This provides new information to inform the development of hardware and post-processing methods for removing MAs from EEG data acquired simultaneously with fMRI data.
运动伪影(MA)是当受试者的头部相对于磁场旋转时,在同时采集的 fMRI 数据中产生的 EEG 数据中的伪影。通常通过在 EEG 迹线上出现大的伪影电压的时间段内删除数据来减轻这些伪影的影响。然而,即使与其他标准后处理方法结合使用,这种策略也不能去除较小的 MA,这些 MA 可能会主导感兴趣的神经元信号。因此,正在开发许多方法来通过测量参考信号来对 MA 进行特征化,然后在纠正伪影中使用这些信号。这些方法通常假设头部和 EEG 帽,以及任何附加的传感器,形成一个刚体,可以用一组标准的六个运动参数来描述。在这里,我们研究头部/EEG 帽系统的运动,以更好地理解 MA。我们专注于参考层伪影减法(RLAS)方法,因为它允许为每个正在用于测量大脑活动的电极测量单独的参考信号。通过对幻影和受试者进行一系列实验,我们发现 EEG 帽相对于幻影和前额皮肤的运动相对较小,并且这种非刚体运动似乎不会导致头皮和参考信号之间的伪影出现相当大的差异。然而,观察到这些信号的幅度存在差异,这可能是由于与大脑信号相比,参考信号所测量的系统的几何形状存在差异。此外,我们发现头骨和皮肤存在非刚体运动,这会为头部晃动产生额外的 MA 分量,而对于头部点头则不存在。这导致头皮和参考层上测量的 MA 的幅度和时间分布存在很大差异,从而降低了基于参考信号的 MA 校正的效果。总的来说,我们的数据表明,使用任何基于参考的系统校正 MA 的效果可能因头部运动的类型而异,头部晃动最难校正。这为开发从同时采集的 fMRI 数据中去除 EEG 数据中的 MA 的硬件和后处理方法提供了新的信息。