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Grenoble|images|parole|signal|automatique|laboratoire

Blind source separation and

electroencephalography analysis

a geometrical approach

Persyval days 2017

Florent Bouchard,

J´erˆome Malick, Marco Congedo

Laboratoire Gipsa-lab, UMR 5216, CNRS, UGA 11 rue des math´ematiques 38420 Grenoble, France

[email protected]

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Context

Our approach: geometrical modeling of the problem

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Context

Our approach: geometrical modeling of the problem

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Electroencephalography (EEG)

I recording of the electrical activity on the scalp resulting from the electrical activity of the brain

I applications:

• brain research

• diagnosis- epilepsy, sleep disorders,...

• neurofeedback- modulate its own brain activity

• brain computer interface- video games, assistance to disabled persons

I interests:

• low cost • non-invasive

• very good temporal resolution

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Electroencephalography (EEG)

I recorded activity generated by electrical source dipoles inside the brain

simultaneous activation of colons of neurons

electrodes

source dipoles

I source signals are mixed while propagating through the brain,

skull and scalp [Nunez and Srinivasan, 2006]

I recorded signals x(t)∈Rn follow the mixing process:

x(t) =As(t), • s(t)∈Rp, source signals

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Blind source separation (BSS)

I retrieve the source signals s(t) and the mixing processA from the observations x(t) [Comon and Jutten, 2010] only assume that source signals are statistically independent

I use K matrices Ck containing the statistics ofx(t): I elementi, j: statistical link between electrodesiandj

I inS++

n , set of symmetric positive definite (SPD) matrices

I matrices Sk containing the statistics of s(t)are diagonal

{Ck} ··· k {Sk} ··· k D++ n S++ n • • • • Ck • • • • • • • • Sk

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Approximate joint diagonalization (AJD)

I Given {Ck}, find an invertible matrixB ∈Rn×n such that

BCkBT are as much diagonal as possible

I estimated source signals are s˜(t) =Bx(t)

I for K >2, no closed form solution- iterative optimization algorithm

{Ck} {BCkBT} ··· k AJD ··· k

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Context

Our approach: geometrical modeling of the problem

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Approximate joint diagonalization (AJD)

I from a geometrical point of view:

S++ n D++ n • • • • • • • • Ck BCkBT • •

I we want change the basis in order to get the matricesCk as

“close” as possible to D++

n

we need the notion of “distance” of a matrix on S++

n to the

subsetD++

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Approximate joint diagonalization (AJD)

S++ n D++ n • BCkBT • Λk(B) • e Λk(B) I “distance” from BCkBT toD++n : • a divergenced(·,·)on S++ n

similar to a distance, less properties

• a diagonal matrixΛk(B)in D++n

I given d(·,·), the natural choice forΛk(B) is [Alyani et al., 2016]

Λk(B) = argmin

Λ∈D++ n

d(BCkBT,Λ)

I the joint diagonalizer B is defined as

argmin

B

X

k

wkd(BCkBT,Λk(B))

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Approximate joint diagonalization (AJD)

I Frobenius distance: least-squares criterion

AJD in [Cardoso and Souloumiac, 1993]

δ2F(C,Λ) =kC−Λk2

F Λ = ddiag(C)

I Kullback-Leibler divergence: from statistics and signal processing

dKL(P, S) = tr(P−1S−In)−log det(P−1S)

• left measure - log-likelihood criterion AJD in [Pham, 2000]

dlKL(C,Λ) =dKL(Λ, C) Λ = ddiag(C)

• right measure

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Approximate joint diagonalization (AJD)

I natural Riemannian distance: geodesical distance onS++

n [Bhatia, 2009] δ2R(C,Λ) = log(Λ −1/2CΛ−1/2) 2 F log(C −1Λ) = 0

I Bhattacharyya distance: closely related to the natural Riemannian distance, numerically cheaper [Sra, 2013]

δB2(C,Λ) = 4 log det((C+ Λ)/2)

det(C)1/2det(Λ)1/2 2 ddiag (C+ Λ)

−1

= Λ−1

I Wasserstein distance: from optimal transport [Villani, 2008]

δW2(C,Λ) = tr 1 2(C+ Λ)−(Λ 1/2CΛ1/2)1/2 ddiag (Λ1/2CΛ1/2)1/2= Λ

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Context

Our approach: geometrical modeling of the problem

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Numerical experiment

I recording of an epileptic patient - 19 electrodes, sampling rate 128Hz

I goal: retrieve the source corresponding to the 3 peak-slow wave complexes 0 1 2 3 4 5 Fp1 Fp2 F3 F4 Cz Pz O1 O2 t(s) Nasion Inion Cz Fz Fp1 Fp2 F3 F4 Pz O1 O2 F7 F8 C3 C4 T3 T4 P3 P4 T5 T6

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Numerical experiment

0 1 2 3 4 5 F lKL rKL R B W t(s) F lKL rKL R B W 0 0.2 0.4 0.6 0.8

Left: waveforms of the estimated source corresponding to the peak-slow wave complexes for all divergences considered

Right: spatial distributions of the estimated source on the scalp for all divergences considered

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Conclusions and perspectives

I different criteria give different information →combine them

I try different combinations of divergence / target matrices

I study the theoretical properties of the criteria

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Thank you for your attention !

I PhD: October 2015 - September 2018

I Publications:

• F. Bouchard, L. Korczowski, J. Malick, M. Congedo.Approximate joint diagonalization within the Riemannian geometry framework. 24th European Signal Processing Conference (EUSIPCO-2016).

• F. Bouchard, J. Malick, M. Congedo.Approximate joint diagonalization according to the natural Riemannian distance. 13th International Conference on Latent Variable Analysis and Signal Separation (LVA/ICA-2017)

• F. Bouchard, P. Rodrigues, J. Malick, M. Congedo.R´eduction de dimension pour la s´eparation aveugle de sources. Submitted to GRETSI 2017.

• F. Bouchard, J. Malick, M. Congedo.Riemannian optimization and approximate joint diagonalization for blind source separation. Submitted to IEEE Transactions on signal processing.

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Alyani, K., Congedo, M., and Moakher, M. (2016).

Diagonality measures of Hermitian positive-definite matrices with application to the approximate joint diagonalization problem.

Linear Algebra and its Applications.

Bhatia, R. (2009). Positive definite matrices.

Princeton University Press.

Cardoso, J.-F. and Souloumiac, A. (1993).

Blind beamforming for non Gaussian signals.

IEE Proceedings-F, 140(6):362–370.

Comon, P. and Jutten, C. (2010).

Handbook of Blind Source Separation: Independent Component Analysis and Applications.

Academic Press, 1st edition.

Nunez, P. L. and Srinivasan, R. (2006).

Electric fields of the brain: the neurophysics of EEG.

Oxford University Press, USA.

Pham, D.-T. (2000).

Joint approximate diagonalization of positive definite Hermitian matrices.

SIAM J. Matrix Anal. Appl., 22(4):1136–1152.

Sra, S. (2013).

Positive definite matrices and the S-divergence.

arXiv preprint arXiv:1110.1773.

Villani, C. (2008).

Optimal transport: old and new, volume 338.

References

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