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Field recordings of transcranial magnetic stimulation in human brain postmortem models.
Quesada, Charles; Fauchon, Camille; Pommier, Benjamin; Bergandi, Florian; Peyron, Roland; Mertens, Patrick; Garcia-Larrea, Luis.
Afiliação
  • Quesada C; NeuroPain Team, Centre de Recherche en Neurosciences de Lyon (CRNL), Inserm U1028, CNRS UMR5292, UJM & UCBL, Lyon, France.
  • Fauchon C; Physiotherapy Department, Sciences of Rehabilitation Institute (ISTR), University Claude Bernard Lyon 1, Lyon, France.
  • Pommier B; NeuroPain Team, Centre de Recherche en Neurosciences de Lyon (CRNL), Inserm U1028, CNRS UMR5292, UJM & UCBL, Lyon, France.
  • Bergandi F; NeuroPain Team, Centre de Recherche en Neurosciences de Lyon (CRNL), Inserm U1028, CNRS UMR5292, UJM & UCBL, Lyon, France.
  • Peyron R; University of Medecine Jacques Lisfranc, Anatomy Laboratory, UJM, Saint-Etienne, France.
  • Mertens P; NeuroPain Team, Centre de Recherche en Neurosciences de Lyon (CRNL), Inserm U1028, CNRS UMR5292, UJM & UCBL, Lyon, France.
  • Garcia-Larrea L; Neurological Department & CETD, University Hospital, CHU Saint-Etienne, Saint-Etienne, France.
Pain Rep ; 9(2): e1134, 2024 Apr.
Article em En | MEDLINE | ID: mdl-38375090
ABSTRACT

Introduction:

The ability of repetitive transcranial magnetic stimulation (rTMS) to deliver a magnetic field (MF) in deep brain targets is debated and poorly documented.

Objective:

To quantify the decay of MF in the human brain.

Methods:

Magnetic field was generated by single pulses of TMS delivered at maximum intensity using a flat or angulated coil. Magnetic field was recorded by a 3D-magnetic probe. Decay was measured in the air using both coils and in the head of 10 postmortem human heads with the flat coil being positioned tangential to the scalp. Magnetic field decay was interpreted as a function of distance to the coil for 6 potential brain targets of noninvasive brain stimulation the primary motor cortex (M1, mean depth 28.5 mm), dorsolateral prefrontal cortex (DLPFC 28 mm), secondary somatosensory cortex (S2 35.5 mm), posterior and anterior insulae (PI 38.5 mm; AI 43.5 mm), and midcingulate cortex (MCC 57.5 mm).

Results:

In air, the maximal MF intensities at coil center were 0.88 and 0.77 T for the flat and angulated coils, respectively. The maximal intracranial MF intensity in the cadaver model was 0.34 T, with a ∼50% decay at 15 mm and a ∼75% MF decay at 30 mm. The decay of the MF in air was similar for the flat coil and significantly less attenuated with the angulated coil (a ∼50% decay at 20 mm and a ∼75% MF decay at 45 mm).

Conclusions:

Transcranial magnetic stimulation coil MFs decay in brain structures similarly as in air, attenuation with distance being significantly lower with angulated coils. Reaching brain targets deeper than 20 mm such as the insula or Antérior Cingulate Cortex seems feasible only when using angulated coils. The abacus of MF attenuation provided here can be used to adjust modalities of deep brain stimulation with rTMS in future research protocols.
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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article