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Causality in Time Series - ClopiNet

Causality in Time Series - ClopiNet

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Causal analysis of fMRIv(t). In fMRI experiments the exogenous <strong>in</strong>puts v(t) mostly reflect experimental controland often have the form of a simple <strong>in</strong>dicator function that can represent, for <strong>in</strong>stance,the presence or absence of a visual stimulus. The vector-functions f and g can generallybe non-l<strong>in</strong>ear.The state-space formalism allows representation of a very large class of stochasticprocesses. Specifically, it allows representation of both so-called ‘black-box’ models,<strong>in</strong> which parameters are treated as means to adjust the fit to the data without reflect<strong>in</strong>gphysically mean<strong>in</strong>gful quantities, and ‘grey-box’ models, <strong>in</strong> which the adjustable parametersdo have a physical or physiological (<strong>in</strong> the case of the bra<strong>in</strong>) <strong>in</strong>terpretation. Aprom<strong>in</strong>ent example of a black-box model <strong>in</strong> econometric time-series analysis and systemsidentification is the (discrete) Vector Autoregressive Mov<strong>in</strong>g Average model withexogenous <strong>in</strong>puts (VARMAX model) def<strong>in</strong>ed as (Ljung, 1999; Re<strong>in</strong>sel, 1997):F (B)y t = G (B)v t + L(B)e t ⇔∑︀ pi=0 F iy t−i = ∑︀ sj=0G j v t− j + ∑︀ qk=0 L ke t−k(13)Here, the backshift operator B is def<strong>in</strong>ed, for any η t as B i η t = η t−i and F, G and Lare polynomials <strong>in</strong> the backshift operator, such that e.g. F (B) = ∑︀ pi=0 F iB i and p, sand q are the dynamic orders of the VARMAX(p,s,q) model. The m<strong>in</strong>imal constra<strong>in</strong>tson (13) to make it identifiable are F 0 = L 0 = I, which yields the standard VARMAXrepresentation. The VARMAX model and its various reductions (by use of only oneor two of the polynomials, e.g. VAR, VARX or VARMA models) have played a largerole <strong>in</strong> time-series prediction and WAGS <strong>in</strong>fluence model<strong>in</strong>g. Thus, <strong>in</strong> the context ofstate space models it is important to consider that the VARMAX model form can beequivalently formulated <strong>in</strong> a discrete l<strong>in</strong>ear state space form:x k+1 = Ax k + Bv k + Ke ky k = Cx k + Dv k + e k(14)In turn the discrete l<strong>in</strong>ear state space form can be explicitly accommodated by the cont<strong>in</strong>uousgeneral state-space framework <strong>in</strong> (12) when we def<strong>in</strong>e:f (x(t),v(t),Θ) ≃ Fx(t) +Gv(t)g(x(t),v(t),Θ) ≃ Hx(t) + Dv(t)ω(t) = ˜Kε(t)Θ = {︁ F,G, H, D, ˜K,Σ e}︁ (15)Aga<strong>in</strong>, the exact relations between the discrete and cont<strong>in</strong>uous state space parametermatrices can be derived analytically by explicit <strong>in</strong>tegration over time (Ljung, 1999).And, as discussed above, wherever discrete data is used to model cont<strong>in</strong>uous <strong>in</strong>fluencerelations the problems of temporal aggregation and alias<strong>in</strong>g have to be taken <strong>in</strong>to account.Although analytic solutions for the discretely sampled cont<strong>in</strong>uous l<strong>in</strong>ear systemsexist, the discretization of the nonl<strong>in</strong>ear stochastic model (12) does not have a uniqueglobal solution. However, physiological models of neuronal population dynamics andhemodynamics are formulated <strong>in</strong> cont<strong>in</strong>uous time and are mostly nonl<strong>in</strong>ear while fMRIdata is <strong>in</strong>herently discrete with low sampl<strong>in</strong>g frequencies. Therefore, it is the discretizationof the nonl<strong>in</strong>ear dynamical stochastic models that is especially relevant to causal87

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