Diffusion MRI is successfully used to map white matter in the brain. In this work we develop a new clinically viable technique with particular focus on grey matter microstructure. To capture the heterogeneous morphology of grey matter, it is imperative to disentangle cylindrical and spherical geometries commonly attributed to neurites and neural soma. We achieve this by leveraging the latest advances in B-tensor encoding and deep learning techniques and present microstructural feature maps of neurites and neural soma in-vivo in the human brain.
B-tensor encoding is a diffusion MRI technique that enables us to distinguish between different types of tissue heterogeneity such as microscopic shape anisotropy and compartment size1,2. To disentangle different signal contributors, measurements using different gradient waveforms are combined3,4. The key observation here is that the signal obtained from spherical (isotropic) tensor encoding (STE) and from the spherical mean of linear tensor encoding (LTE) give strikingly different contrast in the brain using otherwise identical measurement parameters. Figure 1 demonstrates this contrast inversion, whereby in LTE the signal is higher in white matter and lower in grey matter, whereas in STE the signal is higher in grey matter and lower in white matter.
Previous work suggests that STE is sensitive to spherical compartments of vanishing diffusivity5, and that the presence of cell bodies influences LTE simulations and measurements6,7. In this work, we combine STE and LTE diffusion acquisitions and exploit contrast inversion to map microstructural markers of neurites and neural soma in grey matter. We use a deep-learning neural network to estimate four independent tissue parameters: neurite volume fraction and diffusivity, and neural soma volume fraction and diffusivity.
Data acquisition
Healthy volunteers were scanned on a 3T Siemens Prisma scanner using a 64-channel head coil. Isotropic 2 mm voxels were acquired with TE=94 ms and TR=9.2 s for both waveforms. B-values of [0, 500, 1000, 1500, 2000] s/mm2 were measured for STE, and b-values of [0, 1000, 2000, 3500, 5000] s/mm2 were measured for LTE, as higher b-values are achievable in LTE within the same TE. STE was designed using Maxwell-compensated optimisation8,9 and LTE was made using symmetric trapezoidal pulses.
Neural soma model
To map neural soma, we use a microstructural model similar to Ref. 10 consisting of three compartments: cylinders representing neurites, spheres representing neural soma, and extracellular space. In LTE, the signal depends on the direction of diffusion gradients and the orientation of microcompartments. To factor out this effect, we take the spherical mean over gradient directions11,12. The resulting mean signal for a given b-value is $$\frac{\bar{S}_{LTE}(b)}{S_0} = v_{sph}\exp(-b\lambda_{sph})+v_{cyl}\frac{\sqrt{\pi} \text{erf}(\sqrt{b\lambda})}{2\sqrt{b\lambda}}+v_{ext}\exp(-b\lambda_\perp^{ext})\frac{\sqrt{\pi}\text{erf}\big(\sqrt{b(\lambda_\parallel^{ext}-\lambda_\perp^{ext})}\big)}{2\sqrt{b(\lambda_\parallel^{ext}-\lambda_\perp^{ext})}}$$where $$$v_x$$$ are the volume fractions satisfying $$$v_{cyl}+v_{sph}+v_{ext}=1$$$ and erf is the error function. $$$\lambda_{sph}$$$ is the diffusivity of spherical compartments and $$$\lambda_{\parallel}^{ext}$$$, $$$\lambda_{\perp}^{ext}$$$ are the parallel and perpendicular diffusivities of extracellular space. We assume that the perpendicular diffusivity of cylinders is zero and the parallel diffusivity is the intrinsic neural diffusivity $$$\lambda$$$. In STE, diffusion weighting is isotropic and there is no dependence on compartment orientation. The signal is $$\frac{S_{STE}(b)}{S_0} = v_{sph}\exp(-b\lambda_{sph})+v_{cyl}\exp\big(-\frac{b}{3}\lambda\big)+v_{ext}\exp\big(-\frac{b}{3}(\lambda_\parallel^{ext}+2\lambda_\perp^{ext})\big)$$ where b is the trace of the diffusion weighting b-tensor. To reduce the number of free parameters, we model extracellular diffusivities $$$\lambda_\parallel^{ext}$$$ and $$$\lambda_\perp^{ext}$$$ using a tortuosity approximation10. We also assume that $$$\lambda_{sph}<\lambda$$$ due to compartment restriction.
Model parameter estimation
To estimate model parameters, a neural network of three fully connected layers with rectified linear unit activation functions was used. Training was done on a synthesised dataset using a mean square error loss criterion and a stochastic gradient descent optimiser. The model parameters in the training dataset were kept within biophysically plausible ranges, i.e. $$$v_{sph}\in[0,1]$$$, $$$\lambda\in[0,3]$$$ μm2/ms and $$$\lambda_{sph}\in[0,\lambda]$$$.
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