Abstract

BackgroundThe magnetoencephalograms (MEGs) are mainly due to the source currents. However, there is a significant contribution to MEGs from the volume currents. The structure of the anatomical surfaces, e.g., gray and white matter, could severely influence the flow of volume currents in a head model. This, in turn, will also influence the MEGs and the inverse source localizations. This was examined in detail with three different human head models.MethodsThree finite element head models constructed from segmented MR images of an adult male subject were used for this study. These models were: (1) Model 1: full model with eleven tissues that included detailed structure of the scalp, hard and soft skull bone, CSF, gray and white matter and other prominent tissues, (2) the Model 2 was derived from the Model 1 in which the conductivity of gray matter was set equal to the white matter, i.e., a ten tissuetype model, (3) the Model 3 consisted of scalp, hard skull bone, CSF, gray and white matter, i.e., a five tissue-type model. The lead fields and MEGs due to dipolar sources in the motor cortex were computed for all three models. The dipolar sources were oriented normal to the cortical surface and had a dipole moment of 100 μA meter. The inverse source localizations were performed with an exhaustive search pattern in the motor cortex area. A set of 100 trial inverse runs was made covering the 3 cm cube motor cortex area in a random fashion. The Model 1 was used as a reference model.ResultsThe reference model (Model 1), as expected, performed best in localizing the sources in the motor cortex area. The Model 3 performed the worst. The mean source localization errors (MLEs) of the Model 3 were larger than the Model 1 or 2. The contour plots of the magnetic fields on top of the head were also different for all three models. The magnetic fields due to source currents were larger in magnitude as compared to the magnetic fields of volume currents.DiscussionThese results indicate that the complexity of head models strongly influences the MEGs and the inverse source localizations. A more complex head model performs better in inverse source localizations as compared to a model with lesser tissue surfaces.

Highlights

  • The magnetoencephalograms (MEGs) are mainly due to the source currents

  • The location of the positive and negative peaks for the volume currents is diametrically opposite of the source currents magnetic field plot

  • This is expected because the returning volume currents flow opposite to the direction of the MEG source currents

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Summary

Methods

Model constructions Our model building details have been described earlier [1]. For the sake of completeness, these details are included here. A five tissuetype FEM model of the head has been used earlier for efficient computations of the lead fields [4,5] and for analyzing the effects of tissue conductivities on MEG forward and inverse simulations [6]. The major tissues in this model are: scalp, hard skull, CSF, gray and white matter This model was developed by replacing the other tissues in each slice with the nearby tissues. The lead fields at 145 MEG coil positions were computed for all three models due to dipolar sources in the motor cortex area. Due to the addition of the noise, the simulated MEGs for the reference Model were very different from the lead fields as well as from the magnetic field of the source current. Postprocessing and visualizations were done using the Matlab software, version 7.1 (Mathworks, Inc., Natick, MA)

Results
Discussion
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