Department of Neuroscience and Biomedical Engineering, Aalto University School of Science, FI-00076, Aalto, Finland.
Department of Neuroscience and Biomedical Engineering, Aalto University School of Science, FI-00076, Aalto, Finland.
Neuroimage. 2019 Jul 1;194:244-258. doi: 10.1016/j.neuroimage.2019.03.022. Epub 2019 Mar 15.
The spatial resolution of magnetoencephalography (MEG) can be increased from that of conventional SQUID-based systems by employing on-scalp sensor arrays of e.g. optically-pumped magnetometers (OPMs). However, OPMs reach sufficient sensitivity for neuromagnetic measurements only when operated in a very low absolute magnetic field of few nanoteslas or less, usually not reached in a typical magnetically shielded room constructed for SQUID-based MEG. Moreover, field drifts affect the calibration of OPMs. Static and dynamic suppression of interfering fields is thus necessary for good-quality neuromagnetic measurements with OPMs. Here, we describe an on-scalp MEG system that utilizes OPMs and external compensation coils that provide static and dynamic shielding against ambient fields. In a conventional two-layer magnetically shielded room, our coil system reduced the maximum remanent DC-field component within an 8-channel OPM array from 70 to less than 1 nT, enabling the sensors to operate in the sensitive spin exchange relaxation-free regime. When compensating field drifts below 4 Hz, a low-frequency shielding factor of 22 dB was achieved, which reduced the peak-to-peak drift from 1.3 to 0.4 nT and thereby the standard deviation of the sensor calibration from 1.7% to 0.5%. Without band-limiting the field that was compensated, a low-frequency shielding factor of 43 dB was achieved. We validated the system by measuring brain responses to electric stimulation of the median nerve. With dynamic shielding and digital interference suppression methods, single-trial somatosensory evoked responses could be detected. Our results advance the deployment of OPM-based on-scalp MEG in lighter magnetic shields.
脑磁图(MEG)的空间分辨率可以通过使用头皮传感器阵列(例如光泵磁强计(OPM))来提高,这些传感器阵列的空间分辨率比传统的 SQUID 系统更高。然而,只有在非常低的绝对磁场(几纳特或更低)下,OPM 才能达到足够的神经磁测量灵敏度,而通常在为 SQUID 基 MEG 构建的典型磁屏蔽室内无法达到该磁场。此外,磁场漂移会影响 OPM 的校准。因此,为了用 OPM 进行高质量的神经磁测量,需要对干扰场进行静态和动态抑制。在这里,我们描述了一种利用 OPM 和外部补偿线圈的头皮 MEG 系统,该系统可提供针对环境场的静态和动态屏蔽。在传统的双层磁屏蔽室内,我们的线圈系统将 8 通道 OPM 阵列内的最大剩余直流磁场分量从 70 减少到小于 1 纳特,使传感器能够在敏感的自旋交换弛豫自由状态下工作。在补偿低于 4 Hz 的磁场漂移时,实现了 22 dB 的低频屏蔽系数,将峰值到峰值漂移从 1.3 减少到 0.4 纳特,从而将传感器校准的标准偏差从 1.7%减少到 0.5%。在不限制补偿的磁场的情况下,实现了 43 dB 的低频屏蔽系数。我们通过测量正中神经电刺激引起的脑反应来验证该系统。通过动态屏蔽和数字干扰抑制方法,可以检测到单次体感诱发电位。我们的结果推进了基于 OPM 的头皮 MEG 在更轻的磁屏蔽中的部署。