Abstract. Electroencephalography (EEG) and Magnetoencephalography (MEG) are two important methods for the functional imaging of the brain. For the case of the spherical homogeneous model, we elucidate the mathematical relations of these two methods. In particular, we derive and analyse three different representations for the electric and magnetic potentials, as well as the corresponding electric and magnetic induction fields, namely: integral representations involving the Green and the Neumann kernels, representations in terms of eigenfunction expansions, and closed form expressions. We show that the parts of the EEG and MEG fields in the interior of the brain that are due to the induction current are related via Kelvin's inversion transformation. We also derive closed form expressions for the interior and exterior vector potentials of the corresponding magnetic induction fields.
Introduction.Electrochemically generated neuronal currents in the brain give rise to a magnetic field, which in turn excites an induction current within the conductive brain tissue. This electromagnetic activity of the brain is recorded by measuring the electric potential on the scalp (EEG) and the magnetic induction field at distances 4-6 cm from the head (MEG). There exists an extensive literature on how to utilise the EEG and MEG recordings [13], [17] in order to determine the electric potential and the magnetic induction field outside the head. From the mathematical point of view, the two basic problems for EEG and MEG are the forward problem, namely find the interior and exterior fields in terms of the neuronal current and the inverse problem, namely find the neuronal current in terms of the electric potential or in terms of the magnetic field. The fact that neither of these inverse problems has a unique solution was known to Helmholtz in 1853. Nevertheless, complete quantitative results on the non-uniqueness of the inverse MEG problem were obtained only recently, in [9], [10] for the spherical model