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On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers

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 v...

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Autores principales: Iivanainen, Joonas, Zetter, Rasmus, Grön, Mikael, Hakkarainen, Karoliina, Parkkonen, Lauri
Formato: Online Artículo Texto
Lenguaje:English
Publicado: 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6536327/
https://www.ncbi.nlm.nih.gov/pubmed/30885786
http://dx.doi.org/10.1016/j.neuroimage.2019.03.022
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author Iivanainen, Joonas
Zetter, Rasmus
Grön, Mikael
Hakkarainen, Karoliina
Parkkonen, Lauri
author_facet Iivanainen, Joonas
Zetter, Rasmus
Grön, Mikael
Hakkarainen, Karoliina
Parkkonen, Lauri
author_sort Iivanainen, Joonas
collection PubMed
description 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.
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spelling pubmed-65363272019-07-01 On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers Iivanainen, Joonas Zetter, Rasmus Grön, Mikael Hakkarainen, Karoliina Parkkonen, Lauri Neuroimage Article 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. 2019-03-15 2019-07-01 /pmc/articles/PMC6536327/ /pubmed/30885786 http://dx.doi.org/10.1016/j.neuroimage.2019.03.022 Text en This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/bync-nd/4.0/).
spellingShingle Article
Iivanainen, Joonas
Zetter, Rasmus
Grön, Mikael
Hakkarainen, Karoliina
Parkkonen, Lauri
On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers
title On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers
title_full On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers
title_fullStr On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers
title_full_unstemmed On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers
title_short On-scalp MEG system utilizing an actively shielded array of optically-pumped magnetometers
title_sort on-scalp meg system utilizing an actively shielded array of optically-pumped magnetometers
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6536327/
https://www.ncbi.nlm.nih.gov/pubmed/30885786
http://dx.doi.org/10.1016/j.neuroimage.2019.03.022
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