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.