Hill Ryan M, Reina Rivero Gonzalo, Tyler Ashley J, Schofield Holly, Doyle Cody, Osborne James, Bobela David, Rier Lukas, Gibson Joseph, Tanner Zoe, Boto Elena, Bowtell Richard, Brookes Matthew J, Shah Vishal, Holmes Niall
Sir Peter Mansfield Imaging Centre, School of Physics and Astronomy, University of Nottingham, Nottingham, United Kingdom.
Cerca Magnetics Limited, Nottingham, United Kingdom.
Imaging Neurosci (Camb). 2025 Apr 8;3. doi: 10.1162/imag_a_00535. eCollection 2025.
Optically-pumped magnetometers (OPMs) are compact and lightweight sensors that can measure magnetic fields generated by current flow in neuronal assemblies in the brain. Such sensors enable construction of magnetoencephalography (MEG) instrumentation, with significant advantages over conventional MEG devices, including adaptability to head size, enhanced movement tolerance, lower complexity, and improved data quality. However, realising the potential of OPMs depends on our ability to perform system calibration-which means finding sensor locations, orientations, and the relationship between the sensor output and magnetic field (termed sensor gain). Such calibration is complex in OPM-MEG since, for example, OPM placement can change from subject to subject (unlike in conventional MEG where sensor locations/orientations are fixed). Here, we present two methods for calibration, both based on generating well-characterised magnetic fields across a sensor array. Our first device (the HALO) is a head mounted system that generates dipole-like fields from a set of coils. Our second (the matrix coil (MC)) generates fields using coils embedded in the walls of a magnetically shielded room. Our results show that both methods offer an accurate means to calibrate an OPM array (e.g., sensor locations within 2 mm of the ground truth) and that the calibrations produced by the two methods agree strongly with each other: reconstructed positions, orientations, and gains differ on average by 2.0 mm; 1.2° and 1.3% between HALO and MC. When applied to data from human MEG experiments, both methods offer improved signal-to-noise ratio after beamforming, suggesting that they give calibration parameters closer to the ground truth than presumed physical sensor coordinates and orientations. Both techniques are practical and easy to integrate into real-world MEG applications. This advances the field significantly closer to the routine use of OPMs for MEG recording.
光泵磁力仪(OPM)是紧凑轻便的传感器,能够测量大脑中神经元集合体电流流动所产生的磁场。此类传感器可用于构建脑磁图(MEG)仪器,相较于传统MEG设备具有显著优势,包括适应头部尺寸、增强运动耐受性、降低复杂性以及提高数据质量。然而,要实现OPM的潜力,取决于我们进行系统校准的能力,这意味着要确定传感器的位置、方向以及传感器输出与磁场之间的关系(称为传感器增益)。在OPM - MEG中,这种校准很复杂,例如,OPM的放置因受试者而异(与传统MEG中传感器位置/方向固定不同)。在此,我们提出两种校准方法,均基于在传感器阵列上生成特征明确的磁场。我们的第一种设备(HALO)是头戴式系统,通过一组线圈产生类似偶极子的场。我们的第二种设备(矩阵线圈(MC))利用嵌入磁屏蔽室壁中的线圈产生场。我们的结果表明,这两种方法都提供了一种准确校准OPM阵列的手段(例如,传感器位置与真实值相差在2毫米以内),并且两种方法产生的校准结果彼此高度一致:HALO和MC之间重建的位置、方向和增益平均相差2.0毫米、1.2°和1.3%。当应用于人类MEG实验数据时,两种方法在波束形成后均提供了更高的信噪比,这表明它们给出的校准参数比假定的物理传感器坐标和方向更接近真实值。这两种技术都很实用,易于集成到实际的MEG应用中。这使该领域在将OPM用于MEG记录的常规应用方面向前迈进了一大步。