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    <meta name="description" content="Application Domains - Inverse source problems in EEG"/>
    <meta name="dc.title" content="Application Domains - Inverse source problems in EEG"/>
    <meta name="dc.creator" content="Laurent Baratchart"/>
    <meta name="dc.creator" content="Kateryna Bashtova"/>
    <meta name="dc.creator" content="Juliette Leblond"/>
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    <meta name="dc.date" content="(SCHEME=ISO8601) 2013-01"/>
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	    Raweb 
	    2013</a> | <a href="http://www.inria.fr/en/teams/apics">Presentation of the Project-Team APICS</a> | <a href="http://team.inria.fr/apics/">APICS Web Site
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        <h2>Section: 
      Application Domains</h2>
        <h3 class="titre3">Inverse source problems in EEG</h3>
        <p class="participants"><span class="part">Participants</span> :
	Laurent Baratchart, Kateryna Bashtova, Juliette Leblond.</p>
        <p>This work is done in collaboration with Maureen Clerc and Théo Papadopoulo from the Athena Project-Team, and Jean-Paul Marmorat (Centre de mathématiques appliquées - CMA, École des Mines de Paris).</p>
        <p>Solving overdetermined Cauchy problems for the Laplace equation on a
spherical layer (in 3-D) in order to extrapolate
incomplete data (see Section <a title="Range of inverse problems" href="./uid11.html#uid12">
	3.2.1</a> ) is
a necessary
ingredient of the team's approach to inverse source problems, in particular
for applications to EEG since the latter involves propagating the
initial conditions through several layers of different conductivities,
from the boundary
down to the center of the domain where the
singularities (<i>i.e.</i> the sources) lie.
Then, once propagated
to the innermost sphere, it turns out that that traces of the
boundary data on 2-D cross sections (disks) coincide
with analytic functions in the slicing plane,
that has branched singularities inside the disk <a href="./bibliography.html#apics-2013-bid17">[3]</a> . These
singularities are
related to the actual location of the sources (namely, they reach in turn a
maximum in modulus when the plane contains one of the sources). Hence, we are
back to the 2-D framework of Section <a title="Approximation of boundary data" href="./uid17.html#uid22">
	3.3.3</a> 
where approximately recovering these singularities
can be performed using best rational approximation.
The goal is to produce a fast but already good enough
initial guess on the number
and location of the sources in order to run heavier
descent algorithms on the direct problem, which are more precise but
computationally costly, and often
fail to converge if not properly initialized.</p>
        <p>Numerical experiments give
very good results on simulated data and we are now engaged in the process
of handling
real experimental magneto-encephalographic data, see
also Sections <a title="&#10;        FindSources3D&#10;      " href="./uid52.html">
	5.6</a>  and <a title="Source recovery problems" href="./uid57.html">
	6.1</a> ,
in collaboration with the Athena team at Inria Sophia Antipolis,
neuroscience teams in partner-hospitals (la Timone, Marseille),
and the BESA company (Munich).
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