The mixture models could be used as a second stage to analyze the SPMs resulting from a first stage of a univariate temporal FMRI analysis (Woolrich et al., 2001). This is the same two-stage approach used when using the commonly used random field theory of Worsley et al. (1992) and is also the same approach that Everitt and Bullmore (1999); Hartvig (2000) take with the mixture models they consider.
The result of a univariate temporal analysis is effectively the parameter estimate, , of the correlation with the assumed response at each voxel . We might consider using as the observations, , for our mixture models. However, this carries over none of the uncertainty in the estimation of from the univariate temporal analysis. Hence, we use instead the normalised version:
We now need to specify for all classes. For this we propose to use a similar approach to Hartvig and Jensen (2000), who uses three classes: activation, deactivation and non-activation. The non-activating class is modelled as a Normal distribution:
Note that we sometimes find it useful for the interpretation of parameters to reparameterise a Gamma distribution in terms of its mean, , and variance, . See the appendix for this transformation.
The hyperpriors to be used on the component parameters are non-informative, disperse priors. However, we do place a restriction on the mode of the activation and deactivation Gamma classes. The mode of the activation class is constrained to be greater than the mean of the non-activation class, and the mode of the deactivation class is constrained to be less than the mean of the non-activation class. This encodes a sensible prior belief about the expected shape of the activation and deactivation distributions with respect to the non-activation. The mode of a Gamma distribution is given in equation 27.