2012
DOI: 10.1088/0266-5611/28/5/055018
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Source localization using rational approximation on plane sections

Abstract: In functional neuroimaging, a crucial problem is to localize active sources within the brain non-invasively, from knowledge of electromagnetic measurements outside the head. Identification of point sources from boundary measurements is an ill-posed inverse problem. In the case of electroencephalography (EEG), measurements are only available at electrode positions, the number of sources is not known in advance and the medium within the head is inhomogeneous. This paper presents a new method for EEG source local… Show more

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Cited by 21 publications
(29 citation statements)
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“…Observe further that similar deconvolution issues also appear in automatic control (on the boundary of domains of dimension 2, however), concerning harmonic identification in frequency domain [5]. For dipolar point sources, we review some identifiability results related to the EEG inverse problem [9], that we also formulate as observability properties. Algorithmical and numerical aspects are described, most of them requiring (best constrained quadratic) optimization techniques.…”
Section: Introductionmentioning
confidence: 94%
See 1 more Smart Citation
“…Observe further that similar deconvolution issues also appear in automatic control (on the boundary of domains of dimension 2, however), concerning harmonic identification in frequency domain [5]. For dipolar point sources, we review some identifiability results related to the EEG inverse problem [9], that we also formulate as observability properties. Algorithmical and numerical aspects are described, most of them requiring (best constrained quadratic) optimization techniques.…”
Section: Introductionmentioning
confidence: 94%
“…Spherical head models are classically considered and supposed to be made of 3 spherical homogeneous layers [9]. Put then Ω = B for the unit ball and ∂Ω = S for the unit sphere.…”
Section: Eeg Inverse Source Problemmentioning
confidence: 99%
“…In view of recovering the location X d of the dipole, and since the field is known on circles, we adapt and apply the ideas of [1] to our context (see also the references there and [4] for other localization procedures). The key observation is that the denominator of Equation (1) is not polluted by the moment of the dipole, together with the fact that it can be linked to the pole of some rational function whose definition only relies on the data available on each of the 9 circles.…”
Section: Magnetic Dipole Localizationmentioning
confidence: 99%
“…We conducted experiments using Matlab, with several locations X d and moments M d . For each configuration, we built our data using Equation (1). The parameters values are realistic: R = 111 mm and the sections heights are h 1 = 0 mm, h 2 = 15 mm, h 3 = 30 mm.…”
Section: Numerical Simulations With Synthetic Datamentioning
confidence: 99%
“…To prove the first equality, we appeal to another type of approximation, namely, meromorphic approximation in L 2 -norm on T , for which asymptotics of the error and the poles are obtained below. This type of approximation turns out to be useful in certain inverse source problems [9,34,16]. Observe that |T | 1/p−1/2 h 2,T ≤ h p,T ≤ |T | 1/p h T for any p ∈ (2, ∞) and any bounded function h on T by Hölder inequality, where · p,T is the usual p-norm on T with respect to ds and |T | is the arclength of T .…”
Section: C\kmentioning
confidence: 99%