Causality in Time Series - ClopiNet
Causality in Time Series - ClopiNet
Causality in Time Series - ClopiNet
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Robust Statistics for <strong>Causality</strong>Granger, <strong>in</strong> his 1969 paper, suggests that ‘<strong>in</strong>stantaneous’ (i.e. covariate) effects beignored and only the temporal structure be used. Whether or not we accept <strong>in</strong>stantaneouscausality depends on prior knowledge: <strong>in</strong> the case of EEG, the mix<strong>in</strong>g matrixcannot have any physical ‘causal’ explanation even if it is sparse. Without additionala priori assumptions, either we <strong>in</strong>fer causality on unseen and presumably <strong>in</strong>teract<strong>in</strong>ghidden variables (mixed output form, the case of EEG/MEG) or we assume a a noncausalmixed <strong>in</strong>novations <strong>in</strong>put. Note also that the zero-lag system appears to be causalbut can be written <strong>in</strong> a form which suggest the opposite difference causal <strong>in</strong>fluence(hence it is sometimes termed ‘spurious causality’). In short, s<strong>in</strong>ce <strong>in</strong>stantaneous <strong>in</strong>teraction<strong>in</strong> the Gaussian case cannot be resolved causally purely <strong>in</strong> terms of predictionand conditional <strong>in</strong>formation (as <strong>in</strong>tended by Wiener and Granger), it is proposed thatsuch <strong>in</strong>teractions be accounted for but not given causal <strong>in</strong>terpretation (as <strong>in</strong> ‘strong’Granger non-causality) .There are at least four dist<strong>in</strong>ct overall approaches to deal<strong>in</strong>g with alias<strong>in</strong>g effects<strong>in</strong> time series causality. 1) is to make prior assumptions about covariance matrices andlimit <strong>in</strong>ference to doma<strong>in</strong> relevant and <strong>in</strong>terpretable posteriors, as <strong>in</strong> Bernanke et al.(2005) <strong>in</strong> economics and Valdes-Sosa et al. (2005) <strong>in</strong> neuroscience. 2) to allow forunconstra<strong>in</strong>ed graphical causal model type <strong>in</strong>ference among covariate <strong>in</strong>novations, byeither assum<strong>in</strong>g Gaussianity or non-Gaussianity, the latter allow<strong>in</strong>g for stronger causal<strong>in</strong>ferences (see Moneta et al. (2011) <strong>in</strong> this volume). One possible drawback of thisapproach is that DAG-type <strong>in</strong>ference, at least <strong>in</strong> the Gaussian case <strong>in</strong> which there isso-called ’Markov equivalence’ among candidate graphs, is non-unique. 3) a physically<strong>in</strong>terpretable mixed output or co-variate <strong>in</strong>novations is assumed and the <strong>in</strong>ferredsparsity structure (or the <strong>in</strong>tersection thereof over the nonzero lag coefficient matrices)as the connection graph. Popescu (2008) implemented such an approach by us<strong>in</strong>g them<strong>in</strong>imum description length pr<strong>in</strong>ciple to provide a universal prior over rational-valuedcoefficients, and was able to recover structure <strong>in</strong> the majority of simulated co-variate<strong>in</strong>novations processes of arbitrary sparsity. This approach is computationally laborious,as it is NP and non-convex, and moreover a system that is sparse <strong>in</strong> one form (covariate<strong>in</strong>novations or mixed-ouput) is not necessarily sparse <strong>in</strong> another equivalent SVARform. Moreover completely dense SVAR systems may be non-causal (<strong>in</strong> the strongGC sense). 4) <strong>Causality</strong> is not <strong>in</strong>terpreted as a b<strong>in</strong>ary value, but rather direction of<strong>in</strong>teraction is determ<strong>in</strong>ed as a cont<strong>in</strong>uous valued statistic, and one which is theoreticallyrobust to covariate <strong>in</strong>novations or mixtures. This is the pr<strong>in</strong>ciple of the recently<strong>in</strong>troduced phase slope <strong>in</strong>dex (PSI), which belongs to a class of methods based on spectraldecomposition and partition of coherency. Although auto-regressive, spectral andimpulse response convolution are theoretically equivalent representation of l<strong>in</strong>ear dynamics,they do differ numerically and spectral representations afford direct access tophase estimates which are crucial to the <strong>in</strong>terpretation of lead and lag as it relates tocausal <strong>in</strong>fluence. These methods are reviewed <strong>in</strong> the next section.49