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Causality in Time Series - ClopiNet

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Causal analysis of fMRIcharges (SWDs) spread through the bra<strong>in</strong>. fMRI was used to map the hemodynamicresponse throughout the bra<strong>in</strong> to seizure activity, where ictal and <strong>in</strong>terictal states werequantified by the simultaneously recorded EEG. Three structures were selected by theauthors as the crucial nodes <strong>in</strong> the network that generates and susta<strong>in</strong>s seizure activityand further analysed with i) DCM, ii) simple AR model<strong>in</strong>g of the fMRI signal andiii) AR model<strong>in</strong>g applied to neuronal state-variable estimates obta<strong>in</strong>ed with a hemodynamicdeconvolution step. By apply<strong>in</strong>g G-causality analysis to deconvolved fMRItime-series, the stochastic dynamics of the l<strong>in</strong>ear state-space model are augmented withthe complex biophysically motivated observation model <strong>in</strong> DCM. This step is crucialif the goal is to compare the dynamic connectivity models and draw conclusions onthe relative merits of l<strong>in</strong>ear stochastic models (explicitly estimat<strong>in</strong>g WAGS <strong>in</strong>fluence)and bil<strong>in</strong>ear determ<strong>in</strong>istic models. The results showed both AR analysis after deconvolutionand DCM analysis to be <strong>in</strong> accordance with the gold-standard iEEG analyses,identify<strong>in</strong>g the most pert<strong>in</strong>ent <strong>in</strong>fluence relations undisturbed by variations <strong>in</strong> HRF latencies.In contrast, the f<strong>in</strong>al result of simple AR model<strong>in</strong>g of the fMRI signal showedless correspondence with the gold standard, due to the confound<strong>in</strong>g effects of differenthemodynamic latencies which are not accounted for <strong>in</strong> the model.Two important lessons can be drawn from David et al.’s study and the ensu<strong>in</strong>gdiscussions (Bressler and Seth, 2010; Daunizeau et al., 2009a; David, 2009; Friston,2009b,a; Roebroeck et al., 2009a,b). First, it confirms aga<strong>in</strong> the distort<strong>in</strong>g effects ofhemodynamic processes on the temporal structure of fMRI signals and, more importantly,that the difference <strong>in</strong> hemodynamics <strong>in</strong> different parts of the bra<strong>in</strong> can form aconfound for dynamic bra<strong>in</strong> connectivity models (Roebroeck et al., 2005). Second,state-space models that embody observation models that connect latent neuronal dynamicsto observed fMRI signals have a potential to identify causal <strong>in</strong>fluence unbiasedby this confound. As a consequence, substantial recent methodological work has aimedat comb<strong>in</strong><strong>in</strong>g different models of latent neuronal dynamics with a form of a hemodynamicobservation model <strong>in</strong> order to provide an <strong>in</strong>version or filter<strong>in</strong>g algorithm for estimationof parameters and hidden state trajectories. Follow<strong>in</strong>g the orig<strong>in</strong>al formulationof DCM that provides a bil<strong>in</strong>ear ODE form for the hidden neuronal dynamics, attemptshave been made at explicit <strong>in</strong>tegration of hemodynamics convolution with stochasticdynamic models that are <strong>in</strong>terpretable <strong>in</strong> the framework of WAGS <strong>in</strong>fluence.For <strong>in</strong>stance <strong>in</strong> (Ryali et al., 2010), follow<strong>in</strong>g earlier work (Penny et al., 2005;Smith et al., 2009), a discrete state space model with a bi-l<strong>in</strong>ear vector autoregressivemodel to quantify dynamic neuronal state evolution and both <strong>in</strong>tr<strong>in</strong>sic and modulatory<strong>in</strong>teractions is proposed:x k = Ax k−1 + ∑︀ j=1 v j k B j x k−1 + Cv j k + ε kx m k = [︁ xk m, xm k−1 ,··· , ]︁xm k−L+1(20)y m k = βm Φx m k + em kHere, we <strong>in</strong>dex exogenous <strong>in</strong>puts with j and ROIs with m<strong>in</strong> superscripts. The entries<strong>in</strong> the autoregressive matrix A, exogenous <strong>in</strong>fluence matrix C and bi-l<strong>in</strong>ear matricesB j have the same <strong>in</strong>terpretation as <strong>in</strong> determ<strong>in</strong>istic DCM. The relation between93

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