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For the same voxel or region, we also measure the temporal coherence of its fluctuations to other voxels or regions, based on exceeding a given threshold, Θ, for zero lag correlation, establishing functional connectivity between pairs of neuronal populations.
For zero lag, there are three lagged products.
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The correlogram of squared residuals was computed for five lags (Table 11).
After pushing the lag time for three lags, the endogeneity disappears, yet the mediation capacity of arbitral institutes still does not pass the significance test.
Indulgently accepting the stationarity assumption, the pairwise Granger test statistically accredits a certain interconnection between the respective series only on a short run, with the causality direction from avca toward ava (probability of null hypothesis = 0.0881) for one lag, and converse, from ava toward avca (probability of null hypothesis = 0.0943) for two lags.
Then, significant autocorrelations at the 99% level were plotted on a map of the world for three lags: 0, 1, and 2 quarters.
The term (Q -1) is subtracted from the upper bound due to the unavoidable overlap between the Q difference co-arrays for the zero lag.
The optimal lag period was 13 17 years for average intensity and 15-years for cumulative exposure; however results for both zero lags and 15-year lags were presented.
In common with other miners' studies (Tomasek et al, 1993; Darby et al, 1995a), a 5-year lag was used to calculate the cumulative exposure to radon for all sites of cancer other than leukaemia and a zero lag for leukaemia.
The estimated numbers of excess cancers attributable to CT scans for these three lag periods were 608, 402, and 209, respectively.
†Unit increase is 10 μg/m for PM10, ozone, NO2, and SO2 and 0.1 mg/m for CO. ‡Represents the cumulative effect over lag 1-72 hours, estimated by summing regression coefficients for the five lag terms.
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