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Estimation of causal direction from time series in the presence of mixed and colored noise G. Nolte Fraunhofer FIRST, Berlin EEG Typical Properties of Data > 10 minutes measurement > 100 samples/sec 19-128 channels Some millions of


  1. Estimation of causal direction from time series in the presence of mixed and colored noise G. Nolte Fraunhofer FIRST, Berlin

  2. EEG Typical Properties of Data > 10 minutes measurement > 100 samples/sec 19-128 channels ⇒ Some millions of data points

  3. 1. Divide data into epochs (e.g. of 1 sec) 2. Make an analysis in each epoch and average over epochs

  4. The Problem of volume conduction T 1 T 2 T 1 << T 2

  5. z i ( f , k ) Data: Channel Epoch Frequency 1 K ∑ = ∗ S ( f ) z ( f , k ) z ( f , k ) Cross-spectrum: ij i j K = k 1 S ( f ) = ij C ( f ) Coherency: ij S ( f ) S ( f ) ii jj

  6. Independent sources do not contribute to the imaginary part of the cross-spectrum = + S ( f ) Re( S ( f )) i Im( S 12 f ( )) 12 12   P 0 0   1  0 P 0    = 2 T S L L           0 0 P    M

  7. PISA Imaginary parts sPCA Interaction MOCA independent PSI

  8. Granger causality   1 E x   = 1 F log E   → E y x   2 y ˆ = − G F F → → x y y x ˆ G G = ˆ std ( G )

  9. Motivation • Many measurements like EEG/MEG/fMRI are extremely noisy Mixtures of independent sources: Additive noise: Do we estimate fake direction? Do we estimate wrong direction? Channel B Channel A Channel B Channel A Noise Source 2 Source 1 Noise Source

  10. Channel B Channel A Granger Causality Noise Source

  11. Phase Slope Index (PSI)(ψ) Observations: A Independent sources do not contribute to the imaginary part of the cross-spectrum B Slope of phase of cross-spectrum indicates direction

  12. B Slope of phase-spectrum indicates temporal ordering Data Decomposition

  13. Combining A and B: Average of Phase-Slope such that it is insensitive to mixtures Nolte, et.al., Phys Rev Let., 2008

  14.   . 95 0   = A ( 1 )   . 95 . 5   White Noise Source 2 Source 1

  15. Simulation: (1- γ ) true flow + γ mixed noise Comparison with Granger Causality γ Only No Only No Noise Noise Noise Noise

  16. “I know that I don’t know anything” Sokrates No Only Noise Noise

  17. • correct: +1 point Challenge • wrong: -10 points • “I don ‘t know”: 0 points Granger causality Phase Slope Index Correct wrong Total points Correct wrong Total points 736 100 -264 638 6 578 wrong correct correct wrong correct wrong I don’t know correct wrong correct wrong correct wrong

  18. What matters: Simulated challenge data: • problem is generic (details are open to discussion) • evidence is weighted

  19. Nonlinearity of order k Granger Causality

  20. Nonlinearity of order k PSI

  21. FAQ Question Answer Nonlinear systems? alright with exceptions In general; it possible but difficult to construct counterexamples Direct vs. indirect ? partialing (rarely) possible PSI is (trivially) correct, Bidirectional flux? (impossible to resolve completely) Not in the presence of noise, Estimate delay? Results are really binary

  22. Alpha rhythm, Eyes closed, 88 subjects

  23. Surrogate Data to test for artefacts of volume conduction  ( ) = Data x ( t ) x ( t ), , x ( t )  1 n   = s ( t ) W x ( t ) 1. Demix with ICA = v ( t ) s ( t ) 1 1 2. Delay i.th component = + v ( t ) s ( t T ) 2 2 by (i - 1) * T = + v ( t ) s ( t 2 T ) 3 3    − = 1 x ( t ) W v ( t ) 3. Remix surr

  24. Granger Causality, Data vs. Surrogates

  25. Phase Slope Index, Data vs. Surrogates

  26. Summary • Imaginary parts of cross-spectra is not affected by non-interacting sources ⇒ valuable quantity to study interactions • Direction with “Phase Slope Index” (PSI) • Surrogates with ICA

  27. Thanks to Stefan Haufe Mark Hallett Andreas Ziehe Ou Bai Vadim Nikulin Lewis Wheaton Nicole Krämer Masao Matsuhashi Alois Schlögl Zoltan Mari Frank C. Meinecke Sherry Vorbach Florin Popescu Klaus-Robert Müller Tom Brismar Arne Ewald Forooz Shahbazi Laura Marzetti Gian Luca Romani

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