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In-vivo Neural Soma Imaging Using B-tensor Encoding and Deep Learning
Noemi G. Gyori1,2, Christopher A. Clark2, Iulius Dragonu3, Daniel C. Alexander1, and Enrico Kaden1

1Centre for Medical Image Computing, University College London, London, United Kingdom, 2Great Ormond Street Institute of Child Health, University College London, London, United Kingdom, 3Siemens Healthcare Ltd, Frimley, United Kingdom

Synopsis

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.

Introduction

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.

Methods

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 $$$\lambda_{sph}\in[0,\lambda]$$$.

Results and Discussion

To check that the trained neural network can recover model parameters, a test dataset was evaluated. Figure 2 shows that parameters are estimated with reasonable accuracy. For imaging grey matter, we suggest that cylindrical and spherical compartments are markers for neurites and neural soma and show parameter maps of compartment volume fractions and diffusivities (Figure 3). As expected, neurite volume fraction is high in white matter and low in grey matter. The maps also show high volume fraction of spherical compartments in both the cerebellar and cerebral cortex, which in agreement with well-known neuroanatomy presumably reflects neural soma in grey matter. In Figure 4, we demonstrate that these methods are robust for clinically viable acquisition times. We compare maps from a full dataset (~40 minutes) with maps using one third of the acquired gradient directions (~14 minutes). Similar results are found for five further subjects (not shown).

Conclusion

This work demonstrates that cylindrical and spherical compartments can be disentangled using B-tensor encoding. These geometries putatively reflect neurites and neural soma in brain grey matter. The density of neural soma may be used as a novel biomarker for neurodegenerative diseases such as Alzheimer’s and Parkinson's disease. Data was obtained on a clinical system using realistic measurement times that could be shortened to as low as five minutes with multiband EPI13. With deep learning, model parameters can be estimated in seconds, and hence the methods described here can easily be translated to everyday clinical use.

Acknowledgements

The authors thank the London Interdisciplinary Bioscience PhD Consortium and the following grants for funding: BBSRC BB/M009513/1, UK EPSRC EP/M020533/1, EP/N018702/1 and EU H2020 634541-2. We also thank Filip Szczepankiewicz and Markus Nilsson for sharing their free-waveform diffusion EPI sequence.

References

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[7] Palombo, M., Shemesh, N., Ianus, A., Alexander, D. C., Zhang, H. (2018b), Abundance of cell bodies can explain the stick model’s failure in grey matter at high b-value. ISMRM 2018, Paris, France.

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[9] Szczepankiewicz, F., Nilsson, M. (2018), Maxwell-compensated waveform design for asymmetric diffusion encoding, ISMRM 2018, Paris, France.

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Figures

Figure 1. Normalised signal at b-value=2000 s/mm2 using linear tensor encoding (LTE) averaged over gradient directions (top), and spherical tensor encoding (STE) (bottom). 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. This is especially apparent in the cerebellum.

Figure 2. Estimated cylinder volume fraction and diffusivity and sphere volume fraction and diffusivity using a synthetic dataset at SNR=25. In grey matter we use cylinders as markers for neurites and spheres as markers for neural soma. For each boxplot, the shown parameter was fixed, with the other parameters uniformly distributed. This shows that microscopic compartments in grey matter can be recovered with reasonable accuracy using B-tensor encoding and deep learning.

Figure 3. Volume fraction and diffusivity of microscopic compartments in brain grey matter. We estimate cylindrical compartments related to neurites, spherical compartments related to neural soma and derive values for extracellular space. The estimated microstructural parameters are unconfounded by orientation heterogeneity in tissue. The volume fraction of neural soma may be used as a novel biomarker in clinical assessment, for example to identify neural loss in Alzheimer’s disease or to characterise disorders of neurodevelopment.

Figure 4. Imaging microcompartments in grey matter can be achieved for clinically viable acquisition times. Here we reduce a full dataset (~40-minute acquisition time) by removing two thirds of the measured gradient directions (~14-minute acquisition time) and show the respective maps to demonstrate the robustness of the method. With the addition of multiband acceleration, grey matter can be imaged in under 5 minutes.

Proc. Intl. Soc. Mag. Reson. Med. 27 (2019)
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