Forward and Inverse Modeling of EEG and MEG data · Forward and Inverse Modeling of EEG and MEG...
Transcript of Forward and Inverse Modeling of EEG and MEG data · Forward and Inverse Modeling of EEG and MEG...
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Forward and Inverse Modeling of EEG and MEG data
Robert Oostenveld Donders Institute, Radboud University, Nijmegen, NL NatMEG, Karolinska Institute, Stockholm, SE
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Biophysical source modelling: overview
inverse model
forward model
physiological source electrical current
observed potential or field
body tissue volume conductor
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Overview
Motivation and background Forward modeling
Source model Volume conductor model
Inverse modeling
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What produces the electric current
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Equivalent current dipoles
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Overview
Motivation and background Forward modeling
Source model Volume conductor model
Inverse modeling
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Volume conductor
described electrical properties of tissue describes geometrical model of the head describes how the currents flow, not where they originate from same volume conductor for EEG as for MEG, but also for tDCS, tACS, TMS, …
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Volume conductor
Computational methods for volume conduction problem that allow for realistic geometries BEM Boundary Element Method FEM Finite Element Method FDM Finite Difference Method
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Volume conductor: Boundary Element Method
Each compartment is homogenous isotropic
Important tissues skin skull brain (CSF)
Triangulated surfaces describe boundaries
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Volume conductor: Boundary Element Method
Construction of geometry segmentation in different tissue types extract surface description downsample to reasonable number of triangles
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Volume conductor: Boundary Element Method
Construction of geometry segmentation in different tissue types extract surface description downsample to reasonable number of triangles
Computation of model independent of source model only one lengthy computation fast during application to real data
Can also include more complex geometrical details ventricles holes in skull
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Volume conductor: Finite Element Method
Tesselation of 3D volume in tetraeders or hexaheders
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Volume conductor: Finite Element Method
tetraeders hexaheders
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Volume conductor: Finite Element Method
Tesselation of 3D volume in tetraeders or hexaheders
Each element can have its own conductivity FEM is the most accurate numerical method but
computationally quite expensive
Geometrical processing not as simple as BEM
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Volume conductor: Finite Difference Method
Easy to compute Not very usefull in practice
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Volume conductor: Finite Difference Method
(V1-V0)/R1 + (V2-V0)/R2 + (V3-V0)/R3 + (V4-V0)/R4 = 0
I1 + I2 + I3 + I4 = 0 V = I*R
ΔV1/R1 + ΔV2 /R2 + ΔV3 /R3 + ΔV4 /R4 = 0
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Volume conductor: Finite Difference Method
Unknown potential Vi at each node Linear equation for each node
approx. 100x100x100 = 1.000.000 linear equations just as many unknown potentials
Add a source/sink sum of currents is zero for all nodes, except sum of current is I+ for a certain node sum of current is I- for another node
Solve for unknown potential
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EEG volume conduction
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EEG volume conduction
Potential difference between electrodes corresponds to current flowing through skin
Only tiny fraction of current passes through skull Therefore the model should describe the skull and
skin as accurately as possible
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MEG volume conduction
MEG measures magnetic field over the scalp Magnetic field itself is not distorted by skull Magnetic field from ECDs but also from the
volume currents Only tiny fraction of current passes through skull,
therefore the model can ignore the skull and skin
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MEG volume conduction compared to EEG
EEG is measurement on scalp potential difference due to volume currents
MEG field not affected by head
- magnetic field due to primary current (source) - magnetic field due to secondary (volume) currents
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Overview
Motivation and background Forward modeling
Source model Volume conductor model EEG versus MEG
Inverse modeling
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Biophysical source modelling: overview
inverse model
forward model
physiological source electrical current
observed potential or field
body tissue volume conductor
![Page 24: Forward and Inverse Modeling of EEG and MEG data · Forward and Inverse Modeling of EEG and MEG data Robert Oostenveld Donders Institute, Radboud University, Nijmegen, NL NatMEG,](https://reader034.fdocuments.us/reader034/viewer/2022052009/601e0b42e8f0791520176d9a/html5/thumbnails/24.jpg)
Inverse localization: demo
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Inverse methods
Single and multiple dipole models Minimize error between model and measured potential/field
Distributed source models
Perfect fit of model to the measured potential/field Additional constraint on source smoothness, power or amplitude
Spatial filtering
Scan the whole brain with a single dipole and compute the filter output at every location
Beamforming (e.g. LCMV, SAM, DICS) Multiple Signal Classification (MUSIC)