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EEG’s Rosetta stone: _ Identifying _ phase-coupling & metastability in the brain

The Human Brain and Behavior Laboratory. EEG’s Rosetta stone: _ Identifying _ phase-coupling & metastability in the brain. http://www.ccs.fau.edu/hbbl.html. Emmanuelle Tognoli 06/07/2007. ?. Which oscillation is a good model to study general principles of coordinated brain states?.

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EEG’s Rosetta stone: _ Identifying _ phase-coupling & metastability in the brain

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  1. The Human Brain and Behavior Laboratory EEG’s Rosetta stone:_Identifying _phase-coupling & metastabilityin the brain http://www.ccs.fau.edu/hbbl.html Emmanuelle Tognoli 06/07/2007 ?

  2. Which oscillation is a good model to study general principles of coordinated brain states?

  3. The Freeman~Kelso Dialogue:“…my evidence in the past 18 years for sustained synchrony (never antiphasic), for spatial phase gradients in intracranial EEGs from high-density arrays,  and for phase cones with phase velocities corresponding to intracortical axonal propagation velocities as evidence for state transitions.”

  4. Inspiration I: spend time to contemplate the states

  5. Question 1: antiphase coordination in scalp EEG? Indeed by the plenty (too many): Phase locking?

  6. Question 2: …and what about inphase? One source and volume conduction? Two sources coordinated inphase?

  7. f = dw - a sinf - 2b sin (2f) + Qxt One source, two? (or more) Question 1: antiphase coordination in scalp EEG? A priori, it is difficult to distinguish tangential patterns formed by a single source from pairs of radial patterns due to coordinated sources (inverse problem) Question 2: …and what about inphase? Inphase patterns cannot be directly studied neither. Distinguishing single from multiple sources will often require to address the problem of volume conduction(inverse problem) 2p p 0 Let us safely move to the case of broken symmetry for now.

  8. Question 3: phase-locking viewed from a certain angle…Broken symmetry (BS) BS examples rarer/briefer than [0,p]:-reflects true EEG synchrony with its “natural duration” (same typical length/recurrence for real inphase and antiphase)?-broken symmetry is intrinsically less stable? Desynchronization (decoupling, phase scattering) Questions of outstanding importance:-how long does coordination in the brain persists (how many cycles)?-special physiological significance of inphase & antiphase?-can two areas present stability at different phases depending on context or will a given pair of areas always be coordinated with the same angle? Major frequency change for all 3 sites Return to “intrinsic” frequencies?

  9. Summary 1: Identifying phase-locking in real time scalp EEG: direct method Is there antiphase coordination in scalp EEG?Probably. We observed a variety of relative phases. While we cannot directly distinguish tangential patterns from antiphase coordination (yet), there is no reason to observe BS coordination patterns around p, then a black hole atop p suppressing antiphase. Is there a preferential representation of inphase and antiphase (attractors) in scalp EEG?Difficult to say. Raw EEG shows ample phase concentration inphase and antiphase (inflated by spurious synchrony). Because of the volume conduction bias, it is impossible to quantify relative occurrence of broken-symmetry and inphase/antiphase Physiologically, significance of inphase (spatial summation, potentiation) antiphase? (Kelso & Tognoli, 2007)

  10. Question 4: Where is the true antiphase? Forward models The same volume conduction effect that emphasizes spurious antiphase synchrony also attenuates real antiphase synchrony.

  11. Question 5: scalp amplitude modulation by phase misalignment in the volume conductor. E1 E2 S1 S2 E1=0.95*S1+0.6*S2 E2=0.95*S2+0.6*S1 S1 S2 p→0: distant sources p→0.60: close sources p→0.95: id sources E1=0.95*S1+p*S2 E2=0.95*S2+p*S1 Both source P2P amplitude of 2

  12. The hidden truth about real antiphase coordination (Amplitude-wise) The Freeman~Kelso Dialogue:“…my evidence in the past 18 years for sustained synchrony (never antiphasic), for spatial phase gradients in intracranial EEGs from high-density arrays,  and for phase cones with phase velocities corresponding to intracortical axonal propagation velocities as evidence for state transitions.” Contribution of real antiphase to neural cell assemblies is less noticeable: - amplitude reduction (volume conduction) is proportionate to phase misalignment - at antiphase: maximal attenuation - increases with spatial proximity(macroscale-mesoscale)-at distance zero (symmetry in amplitude), is completely cancelled

  13. Trouble ahead in Question 6: apparent relative phase E1=0.95*S1+0.6*S2 E2=0.95*S2+0.6*S1 Red source half amplitude antiphase 90°

  14. Summary 2: forward models of coordinated states Scalp amplitudes are not faithfulScalp amplitudes are affected by relative phase between the sources. Inphase is inflated. Intermediate phases are diversely modulated. Antiphase has maximal attenuation.This modulation is a function of volume conduction (in part: distance) Most scalp relative phases are not faithfulOnly sources that are inphase systematically transfer into scalp patterns inphase. Intermediate phases converge to inphase. Antiphase may suffer drastic amplitude reduction but remains faithful for a range of parameter. In cases of unequal amplitudes of the sources though, eventually it shifts to inphase.This modulation is a function of volume conduction & amplitude asymmetry.

  15. Inspiration II: look at the edges of the state

  16. Question 7: Transitions, transients and intermittency: amplitude Dwell time Escape time Escape time State Transition Transition

  17. AMPLITUDE MODULATION Local patterns of phase cancellation due to volume conductor Intermittency Dynamics of phase misalignment REMIND SOMETHING?

  18. p Question 8: Dephasing: transitions, transients and intermittency Scalp frequencies of unlocked regimes are not faithfulDuring transitions/transients/intermittent regimes, scalp frequencies undulate around their true value (dynamics of relative phase shift seen in state). Undershoot at inphase and overshoot at antiphase. E1=0.95*S1+0.6*S2 E2=0.95*S2+0.6*S1

  19. Question 9: and what next… when another area enters the ballet “Coordination in the brain is like a Balanchine ballet. Neural groups briefly couple, some join as others leave, new groups form and dissolve, creating fleeting dynamical coordination patterns of mind that are always meaningful but don’t stick around for very long.” Kelso & Engstrøm (2006) The Complementary Nature. Recruitment of new neural groups is accompanied by shift in space of preexisting pattern. Or in other words transition in spacedoes not imply the replacement of the current pattern by a new pattern. Waltz of the patterns over the scalp depends on instantaneous polarities (movement toward or away) & amplitudes (distance shift). (it was Inspiration III)

  20. Summary 3: forward models of transitions/intermittency Scalp amplitudes are dynamically modulated at transitionAt transition, scalp signals loose the coupling of the source but maintain the coupling of VC. Frequencies split apart but amplitudes may stay correlated (with typical signature max-inphase min-antiphase). Scalp frequencies and phases are dynamically modulated at transition Relative phase’s dwelling increases with volume conduction. Dwelling is also prolonged but less recurrent with smaller dw(different time scale; rp concentration not affected) Frequencies undulate around their true value for small VCs. For higher VCs and amplitude difference, scalp signal above the weak source looses its own frequency and undulate around the frequency of the strong source. Persisting areas’ scalp topographies glide with incoming/outgoing areas Smooth spatial transition is not pertinent (sufficient) to call for the dissolution of a pair of coupled areas. 21

  21. Significance

  22. Question 1: antiphase coordination in the scalp EEG? A priori, it is difficult to distinguish tangential patterns formed by a single source from pairs of radial patterns due to coordinated sources (inverse problem) Brain Coordination? Question 2: …and what about inphase? Inphase patterns cannot be directly studied neither. Distinguishing single from multiple sources will often require to address the problem of volume conduction(inverse problem) Time has come to address the separation of true and spurious synchrony

  23. An experiment compares EEG coherence between task A and B.Tasks engage the same networks, with the same coupling, same amplitudes, same duration… except that B recruits the left intraparietal sulcus which is not active in task A.This situation is sufficient to elicit significant change in coherence. Bias example 1 B A

  24. Bias example 2 An experiment compares EEG coherence between task A and B.Tasks engaged the same networks, with the same coupling, same amplitudes, same duration… except that B disengages the fusiform gyrus.Oh yes! even this can affect synchrony. A B

  25. Procedures and recipes

  26. STRATEGY: Understand the multitude of objects (patterns) that constitute the real-time EEG.Identify their occurrence, rules of succession Sequencing approach (genome):- start identifying patterns in simple cases (where superposition is understandable)- identify succession probability (pattern … is frequently followed by pattern…)- characterize their task dependence (a step toward behavioral/cognitive significance) Selective modeling:- detect primary & secondary indices-mathematical reconstruction of sources’ coordination dynamics + +

  27. Selective modeling: how much data concerned? Frequency stabilization is the primary sign of phase locking Even less represent the activity for which this electrode pair is at maximum Even less are modulated by the task under investigation Metastability?

  28. Modeling: what do we know about the sources? Coordination Variable: rpE E2: AE2: amplitude at location 1 fE2: frequency at location 1 fE2: phase at location 1 E1: AE1: amplitude at location 1 fE1:frequency at location 1 fE1: phase at location 1 • Approximations of volume conductor • Standard values in the literature (e.g. distance). • Non specific VC values can be derived directly from the data over long periods of time (distribution of relative phase), • Specific values could probably be modeled from phase-dependent distribution of amplitude attenuation. AE1, fE1, fE1 =f(AS1, fS1, AS2,fS2, VC) AE2, fE2, fE2=f(AS1, fS1, AS2,fS2, VC) fS1fS2? S2: AS2: amplitude at location 1 fS2: frequency at location 1 fS2: phase at location 1 S1: AS1: amplitude at location 1 fS1:frequency at location 1 fS1: phase at location 1 Coordination Variable: rpS

  29. Phase coordination’s decision tree (v.1): primary & secondary indices Real coupling State at relative phase ≠ [0, p] No new source growth Real coupling antiphase (terminated) Transition shows drifting frequencies Real coupling antiphase (ongoing) New area grows amplitude (rotates) State antiphase Both maxima decay, replaced by VC from other sources No frequency drift before source dies out Tangential source Radial source Spatial discontinuity not resolved Real coupling antiphase Close sources State inphase Spatial discontinuity resolved Amplitudes different Real coupling Real coupling inphase Amplitudes similar Off zero (BS) Metastable regime Dwell near inphase Phase attraction by volume conductor Centered at zero Frequencies with no notable ratio relationship Metastable regime Dwell near antiphase Phase attraction by volume conductor Frequencies in odds of Arnold’s tongue (exact antiphase conjunction)

  30. The end ~beginning

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