Spherical deconvolution for diffusion MRI requires a response function in order to accurately reconstruct the underlying voxel-wise fiber orientation distribution (FOD). Here, using 3D histologically-defined fiber orientation distributions and the corresponding diffusion signal, we derive the ground-truth fiber response functions. We show that there is significant variation in these response functions across the brain. We find that the current methods to estimate this function do not match the histological results, which leads to differences in fiber volume fractions. This is important because the wrong response function can amplify spurious peaks in the FOD and lead to inaccurate tractography.
Briefly, three ex vivo squirrel monkey brains were scanned on a Varian 9.4T scanner at 300um isotropic resolution. 100 diffusion directions were acquired at a b-value of 6,000 s/mm2. The brain was then sectioned, stained with a fluorescent dye, and imaged on an LSM710 Confocal microscope followed the procedures described in [4]. From the 3D confocal z-stack, the ground truth histological FOD was determined using 3D structure tensor analysis. Finally, using a multi-step registration method4, the diffusion MRI signal corresponding to these z-stacks can be obtained (Figure 1, top).
Normally, one estimates the FOD by deconvolving the signal with the response function:
$$S(\theta,\phi) = R(\theta) \otimes F(\theta,\phi)$$
however, here we ask “what is the true response function, given the signal and the FOD?” (Figure 1, bottom). This is done for 10 mosaic z-stacks (90 voxels), yielding 90 total response functions. We assess the variability in this function across the brain, and using MRTRix3 software, perform spherical deconvolution using our histological kernels, as well as two commonly implemented response function estimation procedures2,3.
however, here we ask “what is the true response function, given the signal and the FOD?” (Figure 1, bottom). This is done for 10 mosaic z-stacks (90 voxels), yielding 90 total response functions. We assess the variability in this function across the brain, and using MRTRix3 software, perform spherical deconvolution using our histological kernels, as well as two commonly implemented response function estimation procedures2,3.
Exemplar FODs, diffusion signals, and response functions are shown in Figure 1 (bottom). Performing similar procedures for all z-stacks yields individual kernels for all voxels. The average histological response function is shown in Figure 2 (A), along with the standard deviation (B) across all histological voxels. The kernels estimated using the 100 highest FA voxels2 (C) as well as an iterative estimation method3 (D) are also shown. The histologically-defined kernel lies somewhere between these two methods.
To highlight the variability in response functions across the brain, we show the average kernel from two different regions with single fiber populations. The average kernel estimated from Region #1 (fornix) kernel indicates more radial signal attenuation, and less axial attenuation, than the “flatter” kernel from Region #2 (corpus callosum). A multivariate analysis of variance indicates that the response functions from these two brain regions differs significantly between the groups (p=1.8E-4), and a two sample Komogorov-Smirnov test of distributions indicates that the average response function from Stack #1 is significantly different than that from Stack #2 (p=3.9E-9). Thus, the optimal kernel varies considerably across brain regions.
To show the differences in reconstruction when using these kernels (and the two commonly implemented methods), we display the estimated FODs for all four methods in Figure 4. The most obvious differences are the amplification of spurious peaks in those methods with “flat” kernels (Confocal stack #2 and Iterative Kernel), and the reduced prevalence of crossing fibers in the less “flat” kernels.
1. Anderson, AW. Measurement of fiber orientation distributions using high angular resolution diffusion imaging. Magn. Reson. Med., 54 (2005), pp. 1194-1206
2. Tournier, J.-D.; Calamante, F.; Gadian, D. G. & Connelly, A. Direct estimation of the fiber orientation density function from diffusion-weighted MRI data using spherical deconvolution. NeuroImage, 2004, 23, 1176-1185
3. Tournier, J.-D.; Calamante, F. & Connelly, A. Determination of the appropriate b-value and number of gradient directions for high-angular-resolution diffusion-weighted imaging. NMR Biomedicine, 2013, 26, 1775-1786
4. Schilling, K., Janve, V., Gao, Y., Stepniewska, I., Landman, B.A., Anderson, A.W., 2016. Comparison of 3D orientation distribution functions measured with confocal microscopy and diffusion MRI. Neuroimage 129, 185-197.