Abstract

Small, commercially-available Optically Pumped Magnetometers (OPMs) can be used to construct a wearable Magnetoencephalography (MEG) system that allows large head movements to be made during recording. The small dynamic range of these sensors however means that movement in the residual static magnetic field found inside typical Magnetically Shielded Rooms (MSRs) can saturate the sensor outputs, rendering the data unusable. This problem can be ameliorated by using a set of electromagnetic coils to attenuate the spatially-varying remnant field. Here, an array of bi-planar coils, which produce an open and accessible scanning environment, was designed and constructed. The coils were designed using a harmonic minimisation method previously used for gradient coil design in Magnetic Resonance Imaging (MRI). Six coils were constructed to null Bx, By and Bz as well as the three dominant field gradients dBx/dz, dBy/dz and dBz/dz. The coils produce homogeneous (within ±5%) fields or field gradients over a volume of 40 × 40 × 40 cm3. This volume is sufficient to contain an array of OPMs, mounted in a 3D-printed scanner-cast, during basic and natural movements. Automated control of the coils using reference sensor measurements allows reduction of the largest component of the static field (Bx) from 21.8 ± 0.2 nT to 0.47 ± 0.08 nT. The largest gradient (dBx/dz) was reduced from 7.4 nT/m to 0.55 nT/m. High precision optical tracking allowed experiments involving controlled and measured head movements, which revealed that a rotation of the scanner-cast by ±34° and translation of ±9.7 cm of the OPMs in this field generated only a 1 nT magnetic field variation across the OPM array, when field nulling was applied. This variation could be further reduced to 0.04 nT by linear regression of field variations that were correlated with the measured motion parameters. To demonstrate the effectiveness of the bi-planar coil field cancellation system in a real MEG experiment, a novel measurement of retinotopy was investigated, where the stimulus remains fixed and head movements made by the subject shift the visual presentation to the lower left or right quadrants of the field of view. Left and right visual field stimulation produced the expected responses in the opposing hemisphere. This simple demonstration shows that the bi-planar coil system allows accurate OPM-MEG recordings to be made on an unrestrained subject.

Highlights

  • Magnetoencephalography (MEG) is a method for non-invasively mapping electrophysiological activity in the human brain (Cohen, 1968)

  • We demonstrate the extensive range of subject head motions that can be tolerated whilst maintaining operation of the Optically Pumped Magnetometers (OPMs), and show that residual magnetic artefacts in the resulting data can be markedly reduced by linear regression of head motion parameters that are measured using an infra-red camera system

  • The variation of the field or field gradient relative to the value at the centre of the coils was evaluated and contoured as a measure of the homogeneity of the fields generated by the coils

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Summary

Introduction

Magnetoencephalography (MEG) is a method for non-invasively mapping electrophysiological activity in the human brain (Cohen, 1968). It produces images of brain function with high spatiotemporal resolution by measuring the magnetic fields generated outside the head by neuronal currents in the brain. The unnatural environment of current MEG scanners does not allow easy application of naturalistic stimuli. It can pose problems in recording from subject groups, such as patients or infants, who find it hard to keep their heads still relative to the MEG sensors. Several valuable approaches for compensating for head movement within the confines of the conventional MEG helmet have been developed (Nenonen et al, 2012; Taulu et al, 2005; Wehner et al, 2008), large gross motion (e.g. motion of the head away from the helmet) remains a significant problem due to loss of signal, which cannot be compensated in post processing

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