论文标题
头部建模误差对MEG的空间频率表示的影响
Effects of head modeling errors on the spatial frequency representation of MEG
论文作者
论文摘要
光学泵的磁力计(OPM) - 下一代磁摄影仪(MEG)传感器 - 可以直接放置在头部上,与更常用的超导量子干扰装置(SQUID)传感器不同,必须将其放置在几厘米远的地方。这允许捕获较高空间分辨率的信号,从而导致可能更准确的源定位。在本文中,我们表明,在无噪声和高的信噪比(SNR)中,大约$ \ geq 6 $ dB,边界元素方法(BEM)头导体模型(或等效地,当前模型不准确)导致信号和等效的电流(ECD)源置换时,封闭式介于传感器时会导致封闭的信号和等效性。这是正确的,尤其是在批量当前贡献很高的深层和表面的情况下。但是,在嘈杂的情况下,更高的SNR用于更紧密的传感器阵列可改善ECD拟合,并超过头部几何形状不准确的影响。这需要增加头部建模的重点以减少逆建模错误,尤其是当MEG的领域努力争取更紧密的传感器阵列和更清洁的信号。还提供了一种分析形式,以获得BEM头几何形状中小扰动的磁场误差。
Optically-pumped magnetometers (OPM) -- next-generation magnetoencephalography (MEG) sensors -- may be placed directly on the head, unlike the more commonly used superconducting quantum interference device (SQUID) sensors, which must be placed a few centimeters away. This allows for signals of higher spatial resolution to be captured, resulting in potentially more accurate source localization. In this paper, we show that in the noiseless and high signal-to-noise ratio (SNR) case of approximately $\geq 6$ dB, inaccuracies in boundary element method (BEM) head conductor models (or equivalently, inaccurate volume current models) lead to increased signal and equivalent current dipole (ECD) source localization inaccuracies when sensor arrays are placed closer to the head. This is true especially in the case of deep and superficial sources where volume current contributions are high. In the noisy case however, the higher SNR for closer sensor arrays allows for an improved ECD fit and outweighs the effects of head geometry inaccuracies. This calls for an increase in emphasis in head modeling to reduce inverse modeling errors, especially as the field of MEG strives for closer sensor arrays and cleaner signals. An analytical form to obtain the magnetic field errors for small perturbations in the BEM head geometry is also provided.