Eduardo Mart�nez Montes Neurophysics Department Cuban

Shared by: Nns35oeE
Categories
Tags
-
Stats
views:
16
posted:
12/5/2011
language:
English
pages:
22
Document Sample
scope of work template
							Source Localization for the EEG
and MEG




 Eduardo Martínez Montes

 Neurophysics Department
Cuban Neuroscience Center
EEG/MEG    Inverse Problem             BET
           of the EEG/MEG


               Prior Information
                or Constraints




  Anatomical                   Mathematical
           EEG generators




EEG reflects the electrical activity of neuronal
 masses, with spatial and temporal
 synchrony.

Primary Current Density (PCD). Macroscopic
  temporal and spatial average of current
  density produced by Postsinaptic Potentials.
   PCD
               Direct Problem         EEG/MEG




                 Main difficulties
    . Geometry . Inhomogeneity . Anisotropy

Model for the head                   Espherical
. Piece-wise                          Geometry
   isotropic
 and homogeneous                     Realistic
                                      Geometry
               Direct Problem
     POTENTIAL                    LEAD FIELD
Maxwell equations +         Reciprocity Theorem =
Boundary conditions +       Fredholm Eq. 1st type
2nd Green Identity =
                            V (re )   k (re , r)  j(r)d 3r
Fredholm Eq. 2nd type
                                      Rc


Drawbacks                   k -> lead field
. Prior Model for DCP       Drawbacks
. Sensitivity to            . Sensitivity to conductivity
   conductivity ratios         ratios

                   Nunez, 1981;   Riera and Fuentes, 1998
EEG/MEG            Inverse Problem                             PCD
                   of the EEG/MEG

                  V (re )   k (re , r)  j(r)d 3r
                            Rc



Continuum:          v  rs , t    K  rs , rg   j  rg , t  d 3rg
 Drawback: The IP has analytical solution only for unrealistically simple
 head geometries and prior assumptions.

Discrete:         v Ns  Nt = K Ns 3 N g  j3 N g  Nt + e Ns  Nt
 Drawback: The problem is highly underdetermined (Ns<<Ng), with an
 ill-conditioned system matrix K that makes the solution very sensible
 to small measurement noise errors.
              Different Approaches
                                                  BESA
   Dipolar - local minima, ad hoc number         CURRY
              of dipoles, spread act.             MUSIC

                                           Regularization
   Distributed - non-uniq., ill-cond.,     . Minimum Norm
                  point sources             . Weighted MN,
                                          FOCUSS, RWMN
                                            . LORETA
                                           Bayesian Approach
                                            . BMA
                                           Others
                                            . LAURA, EPIFOCUS
Christoph et al., 2004
                                            . Beamformer
What’s wrong with IS methods?
1- Ghost Sources:




2- Bias in the estimation of deep sources:
           New methodology

 Based on Bayesian Approach
 Aims to reduce the appearance of ghost sources
 Aims to overcome the bias on the estimation of
  the deep sources.


     Bayesian Model Averaging (BMA)


                                Trujillo et al., 2004.
 MN Methods: Tikhonov vs Bayes
                              v = K  j+e
               Tikhonov
             Regularization                         Bayes



                          Bayesian
                           Model
                                                 P  j v   P  v j  P  j



                                e    N  0,  I 
                                             2         j        
                                                            N 0,       2
                                                                            L L
                                                                             T       1
                                                                                          
j
     j
         
ˆ  min v  K  j 2   L  j 2             ˆ  max P  j v 
                                              j
                                                            j
                                                                                
            Why Bayes?

 Offers a natural way for introducing prior
  information in terms of probabilities
 It is easy to construct very complicated
  models from much simpler ones
            Bayesian Framework:
                 First Level
 Given:                          Infer:

                                    P  v j, M k  P  j M k 
                 P  j v, M k  
                                           Pv Mk 
Model   Mk
 +               P  v M k    P  v j, M k  P  j, M k  dj
Data    v
                         j
                             
                 ˆ  max P  j v, M 
                 jk                k         
                 ˆ  E  j v, M 
                 jk           k
          Why Bayes Again?


   It accounts for uncertainty about model
    form by weighting the conditional posterior
    densities according to the posterior
    probabilities of each model.
          Model Uncertainty:
Model 1          ˆ
                 j1

Model 2          ˆ
                 j2            DATA



Model N          ˆ
                 jN
         Bayesian Framework:
            Second Level
                                   N
Given:           P  j v    P  j v, M k   P  M k v 
                                   k 1

                                            k Bk 0                PMk 
                 P Mk v 
Model   M1                                                  ; k 
                                           N
                                                                   P M0 
                                B
             A
             v                                     r   r0
                                          r 0
             e
             r   B  P v M  P v M 
                  k0                       k                  0
             a
             g   ˆ  max  P  j v  
                 j
             i             j
Model M N    n
                                                             
                       N

  +          g      max P  j v , M k   P  M k v 
                               j
                       k 1
Data v                                         N
                 ˆ  E  j v   E  j v, M   P  M v 
                 j                     k        k
                                           k 1
     Models and Dimensionality:
            N
E  j v    E  j v, M k   P  M k v 
                        
           k 1


                                             M1
                                                  M k 1
                                             M2

                                             M3   M k 2



     For 69 compartments
                   20
         N 10                                              MN
                                             Mk
Simulations
Previous Studies about Visual
  Steady-State responses:
 A strong source has been reported in the primary
  visual cortex located in the medial region of the
  occipital hemispheric pole.
 A second frontal source has also been observed
  and has been associated with the
  electroretinogram.
 Some authors have predicted the activation of the
  thalamus, but it has not been yet detected with
  none of the inverse methods available.
   Visual Steady-State Response

 BMA:




 BESA:
LORETA
              Conclusions:
 A new Bayesian inverse solution method based on
  model averaging is proposed
 The new method shows less blurring and
  significantly less ghost sources than previous
  approaches
 The new approach shows that the EEG might
  contain enough information for estimating deep
  sources even in the presence of cortical ones.
        Ongoing Research:
 Extension of the methodology to include
  spatial-temporal constraints
 Use connectivity constraints for solving the
  EEG/MEG inverse problem
 Estimation of causal models using the
  anatomical connectivity as prior
  information
                             References
   Nunez P., (1981) Electrics Fields of the Brain. New York: Oxford Univ. Press.
   Riera JJ, Fuentes ME (1998). Electric lead field for a piecewise homogeneous
    volume conductor model of the head. IEEE Trans Biomed Eng 45:746 –753.
   Christoph M. Michel, Micah M. Murray, Göran Lantz, Sara Gonzalez, Laurent
    Spinelli, Rolando Grave de Peralta, (2004). EEG source imaging. Clinical
    Neurophysiology, 115, 2195–2222.
   N.J. Trujillo-Barreto, L. Melie-García, E. Cuspineda, E. Martínez, P.A. Valdés-
    Sosa. Bayesian Inference and Model Averaging in EEG/MEG Imaging
    [abstract]. Presented at the 9th International Conference on Functional Mapping of
    the Human Brain, June 19-22, 2003, New York, NY. Available on CD-Rom in
    NeuroImage, Vol. 19, No. 2.
   N.J. Trujillo-Barreto, E. Palmero, L. Melie, E. Martinez. MCMC for Bayesian
    Model Averaging in EEG/MEG Imaging [abstract]. Presented at the 9th
    International Conference on Functional Mapping of the Human Brain, June 19-22,
    2003, New York, NY. Available on CD-Rom in NeuroImage, Vol. 19, No. 2.
   N.J. Trujillo-Barreto, E. Aubert-Vázquez, P.A. Valdés-Sosa, (2004). Bayesian
    Model Averaging in EEG/MEG imaging. NeuroImage, 21: 1300–1319.

						
Related docs
Other docs by Nns35oeE
Nombre de la asignatura:
Views: 12  |  Downloads: 0
INDICE - Excel 9
Views: 35  |  Downloads: 0
????????????
Views: 1  |  Downloads: 0
Registro - Excel
Views: 296  |  Downloads: 0
CB 24
Views: 94  |  Downloads: 0
ANXO 10 LISTA CHEQUEO VIG FIJ
Views: 134  |  Downloads: 0
Comercio Internacional - PowerPoint
Views: 720  |  Downloads: 0
chp7 Hypercalcemie Hypocalcemie Osteomalacie
Views: 70  |  Downloads: 0