The function
p(
D∣
s) measures how well the existence of pathway
s is supported by the tensors
D derived from diffusion measurements. The pathway score aggregates local terms multiplicatively, i.e.,
for the
n-nodes that define the pathway
s with diffusion tensors
Di and tangent vectors
ti. The local score for the diffusion data given the pathway tangent vector is computed using a Bingham distribution (Cook, Alexander, & Parker,
2004; Kaden, Knösche, & Anwander,
2007; Mardia & Jupp,
2000),
where
v1,
v2, and
v3 are the three ordered eigenvectors of the
ith diffusion tensor,
Di;
C(
σ3,
σ2) is a normalizing constant so that the function integrates to one over the sphere; and
σi is the decay rate in the direction of the eigenvector,
vi. The two decay rate parameters are determined by summing two dispersion parameters that are based on (a) uncertainty in the data (
σm) and (b) the ellipsoid shape (
σi*). That is,
σi =
σm +
σi*.
We calculate one dispersion parameter (
σm) from repeated measures of the principal direction of diffusion or PDD (
v1). The repeatability of the data sets a lower bound on fiber direction uncertainty. We estimate
σm using a bootstrap procedure (Efron,
1979): a tensor is fit to 1000 permutations of the raw DWI. The bootstrap procedure estimates the mean PDD and the dispersion about that mean. Other bootstrap procedures, such as the wild bootstrap (Liu,
1988), can be used if the DWI data lacks an adequate number of repetitions (Whitcher, Tuch, & L.,
2005). We summarize the bootstrapped dispersion,
σm, using the Watson distribution on the 3D sphere (Mardia & Jupp,
2000; Schwartzman, Dougherty, & Taylor,
2005). The Watson distribution is identical to a Bingham distribution with radial symmetry, i.e., when
σ2 =
σ3.
The bootstrap sometimes produces an unreasonably low dispersion parameter. Hence, we set a minimum dispersion to 4°—the mean dispersion of all brain voxels with a high linearity index (
CL > 0.4) in all of our data sets. The linearity index is a measure of anisotropy (Peled, Gudbjartsson, Westin, Kikinis, & Jolesz,
1998) and is the positive difference between the largest two eigenvalues of the diffusion tensor divided by the sum of its eigenvalues. In our algorithm, increasing the linearity criterion does not change the minimum dispersion value; decreasing the linearity criterion increases the minimum dispersion to a value larger than 4°. The precise value of this parameter is not critical to the performance of ConTrack.
We derive a second dispersion term, σi*, from the diffusion shape. This dispersion term is necessary because the PDD of an oblate or nearly isotropic diffusion ellipsoid might be highly reliable, yet such voxels clearly have high fiber direction uncertainty. Reliable measurements of oblate and spherical ellipsoids occur when voxels include many crossing fibers, such as where the tapetum interdigitates with the inferior longitudinal fasciculus.
A user-specified function relates ordered tensor eigenvalues (
λi) to the shape dispersion term.
The value δ is a dispersion factor calculated from CL the tensor linearity index, and a user parameter η, discussed below.
The constant, 100°, is maximum total dispersion. A perfect spherical tensor, where σm = 4° and λ1 = λ2 = λ3, would have a uniform distribution about the sphere (σ2 = σ3 = 54°).
The constant 0.015 is chosen so that δ varies between the maximum added dispersion and zero within ∼0.15 units of CL. Adjusting these constants did not alter the results significantly.
Four examples of local distribution functions are shown in
Figure 4. When the linearity index is small, the shape of the tensor adds significant uncertainty to the local distribution function. This uncertainty may be concentrated along one axis for more oblate-shaped ellipsoids or distributed uniformly across the sphere for more spherical ellipsoids. When the ellipsoid has a very high linearity index (i.e., a prolate ellipsoid), the total fiber direction uncertainty equals the bootstrap dispersion estimate.