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Imaging the relationship of axon diameter and myelination in macaque and human brain
Ting Gong1, Chiara Maffei1, Evan Dann1, Hong-Hsi Lee1, Hansol Lee1, Susie Y. Huang1, Suzanne N. Haber2,3, and Anastasia Yendiki1
1Martinos Center for Biomedical Imaging, Massachusetts General Hospital and Harvard Medical School, Boston, MA, United States, 2Department of Pharmacology and Physiology, University of Rochester, Rochester, NY, United States, 3McLean Hospital, Belmont, MA, United States

Synopsis

Keywords: White Matter, Microstructure

Motivation: Axon diameter and myelination are essential for conduction of action potentials and therefore related to brain function. However, the relationships between them in white matter (WM) across different species are not well understood.

Goal(s): To investigate the relationship between axon diameter and myelination in human and macaque brain WM.

Approach: We estimate axon diameter and myelin water fraction (MWF), and derive fiber g-ratio, using macaque and human brain data acquired on a preclinical scanner.

Results: Microstructure parameters exhibit consistent patterns across WM tracts and species. Regions with smaller axons tend to have higher packing density and MWF; fiber g-ratio is relatively stable.

Impact: The weak correlations between dMRI measures and MWF suggest they can provide complementary information about fiber morphology. The regional variations of these microstructure measures will be baseline for investigating changes in abnormal tissue conditions such as demyelination and axonal loss.

Introduction

Axon diameter and myelin thickness are closely related to the conduction velocity of action potentials in the nervous system1. Imaging them non-invasively is thus valuable for studying brain microstructure and function. Recent studies using ultra-high gradient strength diffusion MRI have demonstrated improved estimation of axon diameter across WM tracts2–7, while myelin-sensitive imaging has been established with several methods8. However, the relationships between axon diameter and myelination across the brain have not been investigated. Presence of myelin is an important assumption in most axon diameter models, therefore establishing their relationships in normal myelinated tissue is important for interpreting changes in conditions such as demyelination and axonal loss. In this study, we estimate axon diameter, myelin water fraction (MWF)9 and fiber g-ratio10 and investigate their correlations across the brain in ex vivo macaque and human brain samples.

Methods

Data acquisition. We scanned two fixed macaque brains and one human brain tissue slab on a small-bore 4.7 T Bruker BioSpin MRI system. For axon diameter estimation, we collected DWIs using a two-shot 3D EPI sequence at 0.5 mm isotropic resolution and TE/TR = 52-55/500ms. The diffusion gradients width and separation were fixed at δ/Δ=11/15ms for 8 b-values at 1, 2.5, 5, 7.5, 11.1, 18.1, 25 and 43 ms/πœ‡m2, reaching the Gmax= 660 mT/m of the system; 12 (b<=7.5 ms/πœ‡m2) or 32 gradient directions were uniformly sampled over the hemisphere with one b=0 image for each b-shell. For MWF estimation, we collected multi-slice multi-echo images using the CPMG sequence with slice selective RF pulses and 0.5 mm isotropic resolution. 20 echo times from 8-160 ms with an equal echo spacing of 8 ms and TR of 3000 ms were used for the macaque samples; 40 echo times from 5-200ms with an equal spacing of 5ms and TR of 2000 ms were used for the human tissue.

Axon diameter imaging. We use a four-compartment tissue model with the spherical mean technique11, which models intra-axonal space as cylinders of equal radii4,7,12, extra-axonal space as a diffusion tensor, free water as an isotropic tensor, and immobile water in ex vivo tissue as a dot compartment2,13. We fix only the free-water diffusivity to the value of ex vivo tissue at room temperature (2 πœ‡m2/ms), and we assume that the intrinsic diffusivity is equal to intra-axonal and extra-cellular parallel diffusivity. The tissue parameters we estimate from the data are $$$θ= (𝑓_{π‘–π‘Ž},𝑑_π‘Ž,𝐷_βˆ₯^{π‘–π‘Ž}, 𝐷_⊥^{𝑒𝑐}, 𝑓_{𝑐𝑠𝑓}, 𝑓_{π‘‘π‘œπ‘‘})$$$.
We use a two-stage Markov Chain Monte Carlo (MCMC) method with Gaussian noise model to sample the posterior probability of modelling parameters. Compared to fixing the diffusivity $$$𝐷_βˆ₯^{π‘–π‘Ž}$$$ to the same values, typically 0.6 πœ‡m2/ms for ex vivo tissue7, we find that fitting all parameters improves the quality of fitting, as quantified by the Bayes factor. This however introduces a higher uncertainty of estimated $$$𝑓_{π‘–π‘Ž}$$$ and $$$𝑑_π‘Ž$$$, as quantified by the standard deviations of MCMC samples. We follow a two-stage approach: 1. Sampling probabilities of all 6 parameters and 2. Fixing $$$𝐷_βˆ₯^{π‘–π‘Ž}$$$ and $$$𝐷_⊥^{𝑒𝑐}$$$ to posterior means and sampling only the distributions of other parameters for each voxel. The second MCMC gives roughly the same likelihood of measurements and lower uncertainty of $$$𝑓_{π‘–π‘Ž}$$$ and $$$𝑑_π‘Ž$$$ than the first run.

MWF and g-ratio. We estimate the T2 spectrum from the multi-echo T2-weighted images using non-negative least squares14 with calibration for B1 field inhomogeneity15. From the T2 spectrum, we calculate MWF as the signal fraction for 6ms<T2<15 ms for the macaque samples and 6ms<T2<30 ms for the human sample. We calculate the aggregate g-ratio10 by calibrating MWF to myelin volume fraction16 and combining it with estimated $$$𝑓_{π‘–π‘Ž}$$$ from dMRI data.

Results

We demonstrate the high quality of fit of the four-compartment model (Figure 1). The variability of axon diameter, intra-axonal signal fraction, MWF and g-ratio are shown for the human tissue slab (Figure 2) and macaque brain sample (Figure 3). Variation of parameter estimates among WM regions is consistent between the human and macaque samples (Figure 4).
Axon diameter is negatively correlated with intra-axonal signal fraction and MWF across tracts and species, such that smaller axons give rise to higher axonal density and myelin concentration. The intra-axonal signal fraction is correlated positively with MWF across tracts, while such correlations are inconsistent across voxels within a tract. The aggregate g-ratio is relatively stable and independent of axon diameter (Figure 5).

Discussions & Conclusion

Diffusion MRI can provide distinct estimates of axon diameter and axonal fraction, supported by consistent regional variability between species. The weak correlations between dMRI metrics and MWF suggest they can provide complementary information about fiber geometry.

Acknowledgements

This work is supported by the National Institute of Neurological Disorders and Stroke (R01-NS119911), the National Institute of Mental Health (R01-MH045573, P50-MH106435), and the National Institute of Biomedical Imaging and Bioengineering (R01-EB021265, U01-EB026996).

References

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13. Panagiotaki E, Schneider T, Siow B, Hall MG, Lythgoe MF, Alexander DC. Compartment models of the diffusion MR signal in brain white matter: A taxonomy and comparison. Neuroimage. 2012;59(3):2241-2254. doi:10.1016/j.neuroimage.2011.09.081

14. Doucette J, Kames C, Rauscher A. DECAES - DEcomposition and Component Analysis of Exponential Signals. Z Med Phys. 2020;30(4):271-278. doi:10.1016/J.ZEMEDI.2020.04.001

15. Prasloski T, Mädler B, Xiang QS, MacKay A, Jones C. Applications of stimulated echo correction to multicomponent T2 analysis. Magn Reson Med. 2012;67(6):1803-1814. doi:10.1002/MRM.23157

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Figures

Figure 1. Quality of fit for axon diameter imaging. The spherical mean signal decay versus b-value and distribution of MCMC samples are shown from a WM voxel in (A) the human and (b) a macaque brain sample. The human sample has higher dot signal fraction, possibly due to longer fixation time than the macaque samples. With our imaging protocol, the resolution limits17 for axon diameter estimation are 1.27 and 1.86 πœ‡m for parallel and dispersed axons considering intrinsic diffusivity D0 = 0.4 πœ‡m2/ms and noise level $$$σ = 0.02$$$ as suggested by the samples.

Figure 2. Distributions of microstructure parameters within tract segments of the human sample. The whole left hemisphere was scanned for fiber tractography before blocking a tissue slab for microstructure imaging; the tissue slab scan was registered to the hemisphere scan to define tract segments in the slab: superior longitudinal fasciculus (SLF), anterior commissure (AC), uncinate fasciculus (UF), and internal capsule fibers projecting to superior frontal, inferior frontal, and anterior prefrontal cortex (IC1-3).

Figure 3. Maps and distributions of parameters in whole macaque brain sample. As most axon diameter studies have focused on the corpus callosum (CC), we show boxplots of parameters in the CC tract segments (C). Agreeing with histological studies, axon diameters in the CC body (motor and somatosensory) are higher than CC genu and splenium while axonal fraction is lower. We also found high diameter in the CC rostrum agreeing with a previous in vivo human study18.

Figure 4. Cross-species comparison of microstructure parameters. Tract ROIs in the macaque brains were extracted from the left hemispheres containing parts of SLF, anterior limb of IC (ALIC), AC and UF to match the human slab. The parameter distributions suggest consistent variations of microstructure parameters across WM regions between species. The UF tract segment is near the intersection with the extreme capsule, which is sometimes defined as inferior fronto-occipital fasciculus (IFOF) and has been shown to have larger axons than the SLF in a previous in vivo study18.

Figure 5. Correlations of parameters by considering voxels in each CC tract in Figure 3 (A) and considering voxels in all the tracts in Figure 4 for each brain/slab sample (B). The consistent negative correlations between axon diameter and intra-axonal fractions within CC tracts and across tracts agree with histological findings suggesting smaller axons of higher packing density in tissue. Similar tendencies of estimates were shown in a previous study even when considering water exchange19.

Proc. Intl. Soc. Mag. Reson. Med. 32 (2024)
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DOI: https://doi.org/10.58530/2024/2039