Previously,
parameterised HRFs limited to epochs of boxcar designs have been
modelled in a Bayesian framework using
MCMC (21,25). In this work we introduced a
novel half-cosine parameterisation of the HRF, and implemented it
in a framework allowing for general stimulation types (boxcar,
single-event). We imposed no spatial regularisation of the
signal to allow an investigation of what can be inferred at
each voxel. Whilst the HRF signal model is voxel-wise, it is worth
emphasising that the noise model used at the same time is fully
spatio-temporal.
The use of the half-cosine parameterised form produces easily
interpretable parameters, which is useful for the specification of
priors and for interpreting the results. The parameters which
represent the size of the initial dip and post undershoot
crucially had an ARD prior. An ARD prior will force to zero those
parameters that are not supported by the model and the data. This
allows us to identify whether or not the data supports the
existence of these HRF features on a voxel-wise basis.
One of the results on the HRF characterisation suggested that
there is a negative correlation between activation height and HRF
time to peak. The idea that activation height is negatively
correlated with the HRF time to peak, was also found
in (25) for boxcar designs only. However,
we need to be careful. The apparent causality
between activation height and time to peak is just as likely to be
indirect, and merely reflect that for voxels with low activation
heights, the uncertainty in the time to peak is larger and hence
we get a spread of estimated posterior mean time to peaks around
the true value. This is demonstrated in
figure 15 with the marginal
posterior distribution for a strongly activating voxel having a
much tighter distribution than the weakly activating voxel (both
from the visual boxcar stimulus). There is another possibility. We
may have voxels passing the threshold which are not pure responses
to the stimuli. This ``confound activation'' may be structured
noise partially correlated with the assumed response by chance, or
response/stimulus related confounds such as motion artefact. These
``confound activations'' will have apparent
HRF shapes spread across a wide range. These could have been avoided by
being more restrictive with the HRF shape, however, without knowing the
exact shape of the true HRF response a priori, we might then have
missed some of the true response to the stimulus.
Figure 16 is a schematic
suggesting how the activation height--time to peak ()
scatter plot maybe made up of all three of these effects. There is
no clear way with the current model to distinguish between these
effects.
Figure 15:
Marginal posterior distribution of the time to peak,
, for the visual boxcar stimulation for (a) a voxel with
large activation, (b) a voxel with small
activation.
Figure 16:
Schematic suggesting how the activation height--time to
peak scatter plot maybe made up three different effects (1) The
``true activation'' is negatively correlated. (2) The uncertainty
in the ``true activation'' increases with smaller activation
height. (3) There are voxels with ``confound activation'' passing
the threshold. This may be structured noise randomly correlated
with the assumed response, or response/stimulus related confounds
such as motion artefact -- these ``confound activations'' will
have apparent HRF shapes spread across a wide range.
There is no clear way with the current model
to distinguish between these effects.
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