Diffusion: Encoding & Estimation
Diffusion/Perfusion Tuesday, 18 May 2021

Oral Session - Diffusion: Encoding & Estimation
Diffusion/Perfusion
Tuesday, 18 May 2021 18:00 - 20:00
  • How do we know we measure tissue parameters, not the prior?
    Santiago Coelho1, Els Fieremans1, and Dmitry S. Novikov1
    1Center for Biomedical Imaging and Center for Advanced Imaging Innovation and Research (CAI$^2$R), Department of Radiology, New York University School of Medicine, New York, NY, United States
    We develop a theory to analyze how much the prior distributions affect parameter estimates in supervised data driven regressions. Theory is validated numerically and on white matter Standard Model in vivo.
    Root mean squared error in the training data as a function of the SNR in the measurements. For high SNR the regression method needs a higher order than linear to do an optimal fit. Since the model is nonlinear and the analytical inversion requires a logarithm, as we increase the SNR, polynomials become suboptimal. For low SNR all regressions perform equally well, and their behaviour is represented by the theory.
    Standard deviation of three regression methods for each parameter in the SM. As Eq. 2 shows, for high SNR the variance reaches the values in the training while for low SNR it tends to 0. Maps for f estimated for the high SNR data (right) and different levels of artificially decreased SNR (values are an average over a WM ROI). Even though the noise increases from right to left, the standard deviation of the values decreases (WM ROI). The corresponding SNR values are highlighted, the trend observed is similar. Additionally, the mean values get closer to the expected value of the prior used.
  • Gradient waveform design for cross-term-compensated diffusion MRI: Demonstration of tensor-valued encoding in phantom and simulations
    Filip Szczepankiewicz1 and Jens Sjölund2
    1Clinical Sciences Lund, Lund University, Lund, Sweden, 2Department of Information Technology, Uppsala University, Uppsala, Sweden
    We propose a novel gradient waveform design for diffusion MRI that removes background gradient cross-terms. We demonstrate that the approach improves accuracy for tensor-valued diffusion encoding.
    Figure 3 - A water phantom with a folded surface demonstrates the effect of stationary background gradients. In addition to image distortions, background gradients cause signal variation when waveforms are rotated, causing a positive bias in FA (true value is zero in pure water). Direction encoded color-maps, brightness scaled by FA$$$\in[0.0~0.4]$$$, show prominent coross-term effects for conventional waveforms (high FA), compared to cross-term compensated waveforms, which appear more robust to background gradients (low FA). Violin plots show FA distributions in the slice.
    Figure 3 - A water phantom with a folded surface demonstrates the effect of stationary background gradients. In addition to image distortions, background gradients cause signal variation when waveforms are rotated, causing a positive bias in FA (true value is zero in pure water). Direction encoded color-maps, brightness scaled by FA$$$\in[0.0~0.4]$$$, show prominent coross-term effects for conventional waveforms (high FA), compared to cross-term compensated waveforms, which appear more robust to background gradients (low FA). Violin plots show FA distributions in the slice.
  • Improved unsupervised physics-informed deep learning for intravoxel-incoherent motion modeling
    Misha P. T. Kaandorp1,2,3, Sebastiano Barbieri4, Remy Klaassen5, Hanneke W.M. van Laarhoven5, Hans Crezee6, Peter T. While2,3, Aart J. Nederveen1, and Oliver J. Gurney-Champion1
    1Department of Radiology and Nuclear Medicine, Amsterdam UMC, Amsterdam, Netherlands, 2Department of Radiology and Nuclear Medicine, St. Olav's University Hospital, Trondheim, Norway, 3Department of Circulation and Medical Imaging, NTNU: Norwegian University of Science and Technology, Trondheim, Norway, 4Centre for Big Data Research in Health, UNSW, Sydney, Australia, 5Department of Medical Oncology, Amsterdam UMC, Amsterdam, Netherlands, 6Department of Radiation Oncology, Amsterdam UMC, Amsterdam, Netherlands
    We implemented an improved physics-informed deep neural network approach for IVIM fitting. In simulations, our method outperformed state-of-the-art fitting approaches, and in patients with pancreatic cancer, it detected the most significant parameter changes during chemoradiotherapy.
    Figure 3: IVIM parameter maps (D, f, D*) of the least-squares, Bayesian and IVIM-NEToptim approaches to IVIM fitting of a PDAC patient before receiving CRT. The red ROI represents the PDAC. The least-squares and Bayesian approaches appear noisy, whereas IVIM-NEToptim shows less noisy and more detailed parameter maps.
    Figure 1: Representation of the PI-DNN with different hyperparameter options. Here, the input signal, consisting of the measured DWI signal, is fed forward either through (A) a parallel network design or (B) the original single fully-connected network design. The blue crossed circles indicate random dropout. The output layer is constrained with either absolute or sigmoid activation functions. Subsequently, the network predicts the IVIM signal which is used to compute the loss function.
  • Training Data Distribution Significantly Impacts the Estimation of Tissue Microstructure with Machine Learning
    Noemi G. Gyori1,2, Marco Palombo1, Christopher A. Clark2, Hui Zhang1, and Daniel C. Alexander1
    1Centre for Medical Image Computing, University College London, London, United Kingdom, 2Great Ormond Street Institute of Child Health, University College London, London, United Kingdom
    We demonstrate that training on the observed parameter-combination distribution may be advantageous for detecting small variations in healthy tissue, whereas for detecting atypical tissue abnormalities sampling from a uniform training data distribution may be favourable. 
    Figure 2. Panel (A): Different training data distribution strategies: (i) uniform distribution, (ii) in-vivo parameter combinations from traditional model fitting, (iii) in-vivo white matter parameter combinations and (iv) in-vivo grey matter parameter combinations. Panel (B): RMS errors of vcyl estimates (top) and λcyl estimates (bottom) at different parameter combinations. Panel (C): Parameter maps estimated from each training data distribution. Panel (D): Difference between parameter maps in panel (C) and parameter maps from traditional model fitting in Figure 1.
    Figure 4. The bias in parameter estimates for (i) the uniform training data distribution and for (ii) the in-vivo parameter distribution. The arrows start from the ground truth of each parameter combination and end at the estimates. Red arrows mark the tissue abnormalities shown in Figure 3. In (ii), the red contours show the training data density. Multiple regions of the parameter space act as “sinks” towards which estimates of nearby parameters are biased.
  • On the use of neural networks to fit high-dimensional microstructure models
    João Pedro de Almeida Martins1,2, Markus Nilsson1, Björn Lampinen3, Marco Palombo4, Carl-Fredrik Westin5,6, and Filip Szczepankiewicz1,5,6
    1Department of Clinical Sciences, Radiology, Lund University, Lund, Sweden, 2Department of Radiology and Nuclear Medicine, St. Olav's University Hospital, Trondheim, Norway, 3Department of Clinical Sciences, Medical Radiation Physics, Lund University, Lund, Sweden, 4Centre for Medical Image Computing and Dept of Computer Science, University College London, London, United Kingdom, 5Radiology, Brigham and Women’s Hospital, Boston, MA, United States, 6Harvard Medical School, Boston, MA, United States
    We found that neural networks can vastly accelerate the fitting of high-dimensional microstructural models but cannot by themselves reduce the requirements on the acquisition protocol or correct for the degeneracy of the parameter estimation problem.
    Figure 2. Deploying trained networks on previously unseen synthetic and in vivo data provides anatomically plausible parameter maps in under 10 s. The parameter maps corresponding to the synthetic dataset (second column) are compared to the corresponding ground-truth labels (first column), with difference maps being shown in the third column. Parameter maps obtained from applying a trained network on in vivo brain data are displayed in the fourth column.
    Figure 5. Sensitivity of different acquisition protocols to 10% parameter modulations. The matrices display the relation between an induced parameter change and the observed response. When a single parameter on the y-axis is modulated by 10%, the response can be read in all other parameters along the x-axis. An ideal network would report a diagonal matrix with the value 10% on the diagonal, and zero otherwise. Protocol A appears sensitive in all parameters, whereas Protocols B and C lack sensitivity to DΔ;Z and DI;S, respectively.
  • b-M1-Optimized Waveforms for Improved Stability of Quantitative Intravoxel Incoherent Motion DWI
    Gregory Simchick1,2, Ruiqi Geng1,2, Yuxin Zhang1,2, and Diego Hernando1,2,3
    1Radiology, University of Wisconsin-Madison, Madison, WI, United States, 2Medical Physics, University of Wisconsin-Madison, Madison, WI, United States, 3Biomedical Engineering, University of Wisconsin-Madison, Madison, WI, United States
    b-M1-optimized waveforms were designed in order to obtain intravoxel incoherent motion (IVIM) mapping of the liver with improved stability in comparison to conventional monopolar waveforms.
    Figure 5: Representative parametric maps of D (first row), Vb (second row), and F (third row) for the monopolar and ten-point b-M1-optimized data samplings for two subjects. Reduced variability in the estimates in the right lobe of the liver is observed for the estimates obtained using the b-M1-optimized sampling in comparison to the monopolar sampling. For the monopolar sampling, Subject 2 demonstrates areas of instability in the fitting (yellow arrows), whereas the b-M1-optimized sampling demonstrates stability.
    Figure 2: b-M1-optimized waveforms associated with the Cramer-Rao lower bound (CRLB) b-M1-optimized data sampling (Figure 1b). Waveforms were designed by combining a monopolar gradient waveform with the M1-nulled gradient waveform, which allows for the simultaneous control of b and M1.9 Of these ten waveforms or data points in the b-M1-optimized sampling, numbers 1, 2, 5, 8, and 9 provide the optimal solution to Eq. (2) for a five-point b-M1-optimized sampling, and the addition of number 6 provides a six-point b-M1-optimized sampling.
  • Resolving the underlying sources of diffusion kurtosis in focal ischemia by Correlation Tensor MRI
    Rita Alves1, Rafael Neto Henriques1, Sune Nørhøj Jespersen2,3, and Noam Shemesh1
    1Champalimaud Research, Champalimaud Centre for the Unknown, Lisbon, Portugal, 2Center of Functionally Integrative Neuroscience (CFIN) and MINDLab, Department of Clinical Medicine, Aarhus University, Aarhus, Denmark, 3Department of Physics and Astronomy, Aarhus University, Aarhus, Denmark
    We provide a first characterization of non-Gaussian kurtosis sources in stroke via correlation tensor imaging (CTI). The CTI contrasts enhanced the sensitivity and specificity of the underlying ischemic alterations at 3 h post onset.
    Fig.2 – Ex vivo CTI kurtosis measures for a representative slice of brain specimens from the 3 h post-stroke (A) and sham (B) animal groups. From left to right: panels A and B show the total kurtosis (KT), anisotropic kurtosis (Kaniso), isotropic kurtosis (Kiso) and intracompartmental kurtosis (Kintra). KT and Kintra reveal to have elevated contribution in both white and gray matter in the ipsilesional hemisphere, where the infarct core is located.
    Fig.3 – Specificity analysis after ANOVA (multiple comparisons) across different regions of interest (ROIs). Different kurtosis sources are plotted along rows and each plot contains the respective kurtosis source measure for the L1, R1 and counter control animal group ipsilateral hemisphere, consecutively. Each column refers to only GM and only WM, respectively (p < 0.05).
  • Enforcing positivity constraints in Q-space Trajectory Imaging (QTI) allows for reduced scan time
    Deneb Boito1,2, Magnus Herberthson3, Tom Dela Haije4, and Evren Özarslan1,2
    1Department of Biomedical Engineering, Linköping University, Linköping, Sweden, 2Center for Medical Image Science and Visualization, Linköping University, Linköping, Sweden, 3Department of Mathematics, Linköping University, Linköping, Sweden, 4Department of Computer Science, University of Copenhagen, Copenhagen, Denmark
    Our results demonstrate the robustness of the QTI-derived parameters to data under-sampling when relevant positivity conditions are employed. The constrained estimation framework of QTI+ could make the technique feasible in clinical settings.
    Figure 3. Scalar maps obtained by employing the QTI+ estimation on the full, p81, p56, and p39 protocols. Note how a large part of the information available in the full and p81 protocols is retained, when the p56 and p39 protocols were employed. The bars on the last row show the mean absolute deviation of the maps from their ground truth values (maps computed on the full dataset) for the three protocols. These plots highlight the resilience to downsampling achieved by imposing positivity constraints.
    Figure 5. (a) $$$\mu FA$$$ maps obtained by fitting the QTI model with WLLS(ss) and emplying QTI+ on the four protocols. The fits performed with both methods on the full protocol are used as reference. (b) Difference between the reference $$$ \mu FA$$$ maps and those estimated with both methods on the three protocols. (c) Histograms showing the distribution of $$$ \mu FA$$$ values for the three protocols.
  • Random matrix theory denoising minimizes cross-scanner,-protocol variability and maximizes repeatability of higher-order diffusion metrics
    Benjamin Ades-Aron1, Santiago Coelho1, Jelle Veraart1, Gregory Lemberskiy1, Genevieve Barroll1, Steven Baete1, Timothy Shepherd1, Dmitry S. Novikov1, and Els Fieremans1
    1Radiology, NYU School of Medicine, New York, NY, United States
    This study measures intra-scan, cross-scan, and cross-protocol variability, then evaluates the role of denoising using MPPCA (magnitude) and RMT (reconstruction from raw data) on the precision of estimating conventional DTI and higher-order diffusion metrics.
    Coefficients of Variation over an ROI of the posterior limb of the internal capsule for rotational invariants, DTI parameters, and DKI parameters, averaged over all subjects. P1 v. P2 and S1 v. S2 measure scan-rescan variation. TE=92 v. TE=128 measure the effect of varying the echo time, CV for Prisma 1 and Prisma 2 scan vs. Prisma 3 scan were averaged. P v. S measure inter-scan variation, where scans Skyra 1 and Skyra 2 scan vs. Prisma 3 scan (with matched echo times) were averaged. Rescaling to the voxel level by $$$1/\sqrt{N voxels}$$$ yields CV ~ 1%.
    Voxel-wiseVoxelwise coefficients of variation are shown for MD, MK, and FA for scan-rescan data on the Prisma and the Skyra. Generally, theThe CVs are at 5-10% level on a voxelwise basis in whiter matter and higher in gray matter.
  • A time-efficient OGSE sequence with spiral readout for an improved depiction of diffusion dispersion
    Eric Seth Michael1, Franciszek Hennel1, and Klaas Paul Pruessmann1
    1Institute for Biomedical Engineering, ETH Zurich and University of Zurich, Zurich, Switzerland
    A diffusion imaging methodology combining enhanced sensitivity OGSE waveforms with spiral readouts provided an improved depiction of diffusion dispersion in the in-vivo human brain. The findings suggest the relationship is better resolved at higher b-values.
    Figure 5. Diffusion dispersion rate (Λ) maps of a single slice from each subject (different rows) for all b-values (different columns), for OGSE shapes without flow compensation. All sampled frequencies for each respective b-value are accounted for in computation. Voxels with negative Λ are masked. The underlying contrast is similar for all b-values but stabilizes as the b-value increases (going from left to right), as fewer pixels exhibit spurious intensities.
    Figure 1. Comparison of OGSE gradient waveforms and power spectra. All plots are in arbitrary units, and the gradient plots show effective shapes including the inversion by the refocusing RF pulse. Power spectra are pictured for a standard OGSE shape with a half-period gap (A), a reduced gap OGSE shape2 (B), and a further modification to the latter producing FC (C). Note that the power spectra of (B) and (C) have higher peaks and smaller side lobes than that of (A). Also, the zero frequency peak of power spectrum (B) is eliminated in (C) by extending the innermost gradient lobes of (C) by TFC.
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Digital Poster Session - Diffusion: Encoding, Estimation & Machine Learning
Diffusion/Perfusion
Tuesday, 18 May 2021 19:00 - 20:00
  • Quantification of multiple diffusion metrics from asymmetric balanced SSFP frequency profiles using neural networks
    Florian Birk1, Felix Glang1, Christoph Birkl2, Klaus Scheffler1,3, and Rahel Heule1,3
    1High Field Magnetic Resonance, Max Planck Institute for Biological Cybernetics, Tübingen, Germany, 2Department of Neuroradiology, Medical University of Innsbruck, Innsbruck, Austria, 3Department of Biomedical Magnetic Resonance, University of Tübingen, Tübingen, Germany
    Neural networks proved ability to learn complex dependencies between phase-cycled bSSFP and DTI data. Direct multi-parametric mapping from bSSFP profiles to diffusion metrics provided promising results for MD, FA, and the angle ϴ of the principal diffusion eigenvector relative to B0.
    Figure 1. Scheme of the neural network multi-parametric mapping pipeline. Real and imaginary parts of the 12-point bSSFP phase-cycling data are fed voxelwise as input into the NN (green box). For each voxel, a 3x3 window of nearest neighbors in the axial plane is extracted leading to 216 input features. WM asymmetries in the magnitude profile are shown for a representative ROI in corpus callosum (orange box). The trained NNs enable voxelwise predictions of four diffusion metrics: MD, FA, azimuth (Φ) and inclination (ϴ) (blue box).
    Figure 3. NN predictions (middle) are depicted for a representative axial slice of a testing subject not included into NN training in comparison to reference data (left) obtained with standard SE-EPI-based DTI fitting. On the right, the corresponding relative uncertainty maps of the NN are shown.
  • Rotation-Equivariant Deep Learning for Diffusion MRI
    Philip Müller1, Vladimir Golkov1, Valentina Tomassini2, and Daniel Cremers1
    1Computer Vision Group, Technical University of Munich, Munich, Germany, 2D’Annunzio University, Chieti–Pescara, Italy
    We propose neural networks equivariant under rotations and translations for diffusion MRI (dMRI) data and therefore generalize prior work to the 6D space of dMRI scans. Our model outperforms non-rotation-equivariant models by a notable margin and requires fewer training samples.
    Segmentation of multiple-sclerosis lesions in six scans from the validation set. (a) Ground truth of one example slice per scan, (b) predictions for that slice using our equivariant model, (c) predictions for that slice using the non-rotation-equivariant reference model with 3D convolutional layers, (e) ROC curves of all models on the full scans, (f) precision-recall curves of all models on the full scans. While our equivariant model is very certain (yellow areas) at most positions, the non-rotation-equivariant model has large areas of high uncertainty (purple areas).
    Segmentation of multiple-sclerosis lesions in a scan from the validation set (not used for training) using our equivariant (top) and the non-rotation-equivariant (bottom) model, both trained on reduced subsets of the training set (from left to right) with the ground truth segmentation in the left column. While our equivariant model achieves quite accurate segmentations when trained on 26.3% of the training scans, the segmentations of the non-rotation-equivariant model only start getting accurate when trained on 65.8% of the set, indicating better generalization of our model.
  • Improved image quality with Deep learning based denoising of diffusion MRI data
    Radhika Madhavan1, Jaemin Shin2, Nastaren Abad1, Luca Marinelli1, J Kevin DeMarco3, Robert Y Shih3, Vincent B Ho3, Suchandrima Banerjee4, and Thomas K Foo1
    1GE Global Research, Niskayuna, NY, United States, 2GE Healthcare, New York, NY, United States, 3Walter Reed National Military Medical Center and Uniformed Services University of the Health Sciences, Bethesda, MD, United States, 4GE Healthcare, Menlo Park, CA, United States
    Diffusion MRI often suffers from low signal-to-noise ratio, especially for high b-values. This work proposes a deep learning based denoising method to address this limitation, allowing the use of high b-values as well as higher spatial resolution.
    Figure 1: Diffusion weighted images for an example healthy volunteer showing improved SNR (separability of gray and white matter compartments in b-values >=2000 s/mm2) without spatial smoothing across multiple intensities of DL-based denoising.
    Figure 3: DL-based denoising improved differentiation across signal compartments while preserving quantitative tensor-based metrics. (A-C) Histogram analysis demonstrating distribution of FA values in whole brain CSF, Gray matter (GM) and WM. Quantitative diffusion metrics were compared across two level of DL denoising (50% and 75%). Results were consistent across both volunteers and across acquisitions. (D) FA values across 50 WM regions remain unchanged demonstrating that DL-based denoising maintains tensor-based quantitative metrics.
  • Deep learning based denoising for high b-value high resolution diffusion imaging
    Seema S Bhat1, Pavan Poojar2, Hanumantharaju M C3, and Sairam Geethanath1,2
    1Medical Imaging Research center, Dayananda sagar college of engineering, Bangalore, India, 2Columbia University in the City of New York, Newyork, NY, United States, 3Department of Electronic and Communications, BMS Institute of Technology and Management, Bangalore, India
    Deep learning  based denoising of high b-value DWI was done in this work and we achieved PSNR (>32dB) for noise simulated DWI and image entropy(>7.17) for prospective DWI. Denoising can reduce acquisition time and increase resolution with smaller slice thickness.
    Figure 5: First column shows high b-value prospective DWI with slice thickness 2 mm, NEX=1, 2. More noise in test images can be observed with reduction in slice thickness. Last column shows their denoised counterparts. Noisy & denoised parts are magnified (highlighted with red and yellow squares) in second & third columns. Significant noise reduction and increase in entropy measures can be noted.
    Figure 2: Visualization of Openneuro high b-value DWI denoising: First column (second row onwards) shows input images with Rician noise at σ =0.01,0.03 and 0.05 respectively. Last column shows denoised images. Noisy & denoised parts are magnified (highlighted with red and yellow squares respectively) in second & third columns. Significant reduction in noise can be observed in the denoised version.
  • Microstructural White Matter Segmentation in Mild Traumatic Brain Injury Patients using DTI and a Deep 2D-UNet Ensemble
    Brian McCrindle1,2, Nicholas Simard1,2, Ethan Samson2,3, Ethan Danielli 2,3, Thomas E. Doyle1,3,4, and Michael D. Noseworthy1,2,3
    1Electrical and Computer Engineering, McMaster University, Hamilton, ON, Canada, 2Imaging Research Center, St. Joseph's Healthcare, Hamilton, ON, Canada, 3School of Biomedical Engineering, McMaster University, Hamilton, ON, Canada, 4Vector Institute, Toronto, ON, Canada
    We develop a deep ensemble-based 2D-UNet framework for brain microstructural white matter damage segmentation. We show that ensembles perform the most reliably in out-of-distribution conditions even with minimal training data.
    Example of an unseen slice fed into the ensemble model. (a) Normalized Axial FA Slice. (b) Z-Scoring label. (c – e) Model predictions for 2D-UNets with Resnet101, Vgg19, InceptionV4 Encoders with Dice scores 0.69, 0.69, 0.70 respectively. (f) Ensemble Predictive Uncertainty. (g) Ensemble Prediction. (h) Ensemble Prediction with “Optimal” Threshold and a Dice Score of 0.71.
    Dice-Score vs Threshold for all models with and without TTA. The ensemble performs most reliably over the threshold range.
  • Deep learning-based DWI Denoising method that suppressed the "instability" problem
    Hayato Nozaki1,2, Yasuhiko Tachibana3, Yujiro Otsuka4, Wataru Uchida1,2, Yuya Saito1, Koji Kamagata1, and Shigeki Aoki1
    1Department of Radiology, Graduate School of Medicine, Juntendo University, Tokyo, Japan, 2Graduate School of Human Health Sciences, Tokyo Metropolitan University, Tokyo, Japan, 3Department of Molecular Imaging and Theranostics National Institute of Radiological Sciences National Institutes for Quantum and Radiological Science and Technology, Chiba, Japan, 4Miliman, Tokyo, Japan
    The deep learning-based method which can effectively denoise DWI images almost without risked to output outliers due to the instability problem in deep learning was developed and evaluated.

    Figure 1. Outline of the neural network architecture.

    The output value has small risk to become an outlier because it is generated by the combination of the weighted averages for the neighboring pixels in the original image. The loss to be minimized consists of both the mean absolute error between the output and the target images and the Euclid distance between the derived diffusion tensors for efficient optimization.

    Figure 4. The results of the ROI-based analysis.

    dNR was closer to NEX8 than NEX1 in most regions and parameter maps, and some significant differences between NEX1 and NEX8 were resolved in between dNR and NEX8. However, dNR was far from NEX8 than NEX1 in some combinations of the region and the parameter. Especially, in the regions of deep white matter and periventricular white matter in ODI, the difference compared to NEX8 was significant in dNR and not in NEX1.

  • Accelerating Brain Diffusion Tensor Imaging using Neural Networks: A Comparison of three Neural Networks
    Yuhao Yan1,2 and Zheng Chang1,2
    1Medical Physics Graduate Program, Duke University, Durham, NC, United States, 2Department of Radiation Oncology, Duke University, Durham, NC, United States
    Neural networks can accelerate brain DTI. Cascade-net out-performed U-net and PD-net, obtaining comparable image quality as compared with the reference reconstructed from the full k-space data on reconstruction of DTI images, ADC maps and FA maps.
    Figure 3. Illustration of DTI images, ADC maps, FA maps and colored FA maps of a selected slice, from top to bottom row. Each column from left to right are reference images reconstructed from full k-space data, images reconstructed from zero-filled under-sampled k-space data, images reconstructed from under-sampled k-space data using U-net, PD-net and Cascade-net.
    Figure 1.a. Structure of U-net.1,4 The number of filters in each layer is a quarter of the original structure. Zero-padding is adapted to maintain the size of images in convolutions. 1.b. Structure of PD-net.5 In this work, the activation function PReLU non-linearity in the original structure was substituted by ReLU non-linearity for consistency with U-net and Cascade-net.1 1.c. Structure of Cascade-net.2 The number of filters was set as 48 in this work, which was 64 in the original structure.1
  • Accelerating Diffusion Tensor Imaging of the Rat Brain using Deep Learning
    Ali Bilgin1,2,3,4, Loi Do1, Phillip A Martin2, Ethan Lockhart4, Adam S Bernstein1, Chidi Ugonna1, Laurel Dieckhaus1, Courtney Comrie1, Elizabeth B Hutchinson1, Nan-Kuei Chen1, Gene E Alexander5,6, Carol A Barnes5,7,8, and Theodore P Trouard1,3,5
    1Biomedical Engineering, University of Arizona, Tucson, AZ, United States, 2Electrical and Computer Engineering, University of Arizona, Tucson, AZ, United States, 3Medical Imaging, University of Arizona, Tucson, AZ, United States, 4Program in Applied Mathematics, University of Arizona, Tucson, AZ, United States, 5Evelyn F. McKnight Brain Institute, University of Arizona, Tucson, AZ, United States, 6Departments of Psychology and Psychiatry, University of Arizona, Tucson, AZ, United States, 7Division of Neural System, Memory & Aging, University of Arizona, Tucson, AZ, United States, 8Departments of Psychology, Neurology and Neuroscience, University of Arizona, Tucson, AZ, United States
    Deep learning enables calculation of diffusion tensor metrics with up to ten-fold reduction in scan time when imaging the rat brain.
    Figure1: (a) In conventional DTI, acquired DWIs are first used to estimate the diffusion tensor. The resulting tensor is used to compute the DTI metrics. (b) In proposed DL-DTI, the acquired DWIs are first used to predict DWIs that were not acquired. The acquired and predicted DWIs are used together for estimating the diffusion tensor. The diffusion tensor is then used to compute the DTI metrics.
    Figure 3: Comparison of DTI metrics. Directionally Encoded Color (DEC), Fractional Anisotropy (FA), Mean Diffusivity (MD), Axial Diffusivity (AD), and Radial Diffusivity (RD) maps are shown for a reference (N=64) dataset together with the same metrics obtained using the conventional DTI (Figure 1(a)) and DL-DTI (Figure 1(b)) approaches using a varying number of input DWIs. The metrics obtained from DL-DTI correspond well to those obtained using the reference dataset even at high acceleration rates.
  • Automatic Detection of Nyquist Ghosts in Whole-Body Diffusion Weighted MRI Using Deep Learning
    Alistair Lamb1, Anna Barnes2, Stuart A Taylor2, and Hui Zhang3
    1Department of Medical Phyics and Biomedical Engineering, University College London, London, United Kingdom, 2Centre for Medical Imaging, University College London, London, United Kingdom, 3Centre for Medical Image Computing, University College London, London, United Kingdom
    A supervised deep-learning approach to detect the presence of Nyquist ghosts in axial DWI slices of the abdomen is proposed with intent for use in improving the reproducibility of quantitative ADC measurements in the body. A test accuracy of 81.5% was achieved.
    Figure 5: The percentage accuracy of the classifier on test data for each of the 11 cross-validation iterations is shown, for both the network trained on DWI slices with intensity values windowed between 0-25, and for the network trained without windowing. The mean accuracy and corresponding standard deviation across all 11 iterations is also shown for both cases.
    Figure 5: The percentage of slices containing Nyquist ghosts is shown for each pair of subjects. For each subject pair, the percentage for the constituent subjects are also shown, labelled with the subject number. The mean (44.2%) across all subject pairs is given, along with the standard deviation (5.3%) which is much lower than that of slices containing Nyquist Ghosting in individual subjects, as shown in Figure 2.
  • SRDTI: Deep learning-based super-resolution for diffusion tensor MRI
    Qiyuan Tian1,2, Ziyu Li3, Qiuyun Fan1,2, Chanon Ngamsombat1, Yuxin Hu4, Congyu Liao1,2, Fuyixue Wang1,2, Kawin Setsompop1,2, Jonathan R Polimeni1,2, Berkin Bilgic1,2, and Susie Y Huang1,2
    1Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Boston, MA, United States, 2Harvard Medical School, Boston, MA, United States, 3Department of Biomedical Engineering, Tsinghua University, Beijing, China, 4Department of Electrical Engineering, Stanford University, Stanford, CA, United States
    •  
    1. 1. Proposed a deep learning-based super-resolution method for DTI.
    1. 2. Employed a very deep convolutional neural network, residual learning, and multi-contrast imaging.
    • 3. High-quality results similar to high-resolution ground truth and superior to those from image interpolation.
    Figure 3. Direction-encoded fractional anisotropy maps. Fractional anisotropy maps color encoded by the primary eigenvector (red: left–right; green: anterior–posterior; blue: superior–inferior) derived from the diffusion tensors fitted using interpolated data (a, b), SRDTI super-resolution data (c), and ground-truth high-resolution data (d) along axial, coronal and sagittal directions, showing regions-of-interest in the internal capsule (i, ii), cerebral cortex (iii, iv) and pons (v, vi), respectively.
    Figure 2. Image results. b=0 images (row a) and diffusion-weighted images (DWIs) (row c) along one direction of the six optimized diffusion-encoding directions (i.e., [0.91, 0.416, 0]) from interpolated data (i, ii) (interpolated data using cubic spline is the input to SRDTI), SRDTI output data (iii), ground-truth high-resolution data (iv), and their residuals comparing to the ground-truth high-resolution images (rows b, d). A region-of-interest in the deep white matter (yellow boxes) is displayed in enlarged views (rows, b, d, column iv).
  • Inferring Diffusion Tensors on Unregistered Cardiac DWI Using a Residual CNN and Implicitly Modelled Data Prior
    Jonathan Weine1, Robbert J. H. van Gorkum1, Christian T. Stoeck1, Valery Vishnevskiy1, Thomas Joyce1, and Sebastian Kozerke1
    1Institute for Biomedical Engineering, University and ETH Zurich, Zürich, Switzerland
    We present a feasibility study of training a residual CNN on simulated data to infer diffusion tensors from unregistered free breathing single-shot 2nd order motion-compensated diffusion-weighted SE-EPI data. Improvement in resulting parameter maps at myocardial borders is demonstrated.

    Figure 1: Architecture design of the proposed residual CNN. Input is 144 stacked diffusion-weighted magnitude images, normalized to the mean LV intensity of the first image. The final output 6 channels represents the tensor entries. Convolutional layers (blue) have a $$$3\times3\times N$$$ kernel and ReLU activation. The residual blocks (green) consist of the parallel paths with different kernel sizes. The outputs are concatenated and reduced 1 convolution layer to match the input channels. The output of a residual block is added to the skip connection and fed to the next block.


    Figure 2: Illustration of the simulated training data and visual comparison to real in vivo data. (a) Animation of single averages for each linear diffusion-weighting and (b) example of the correspondingly simulated and LV-masked training dataset. The red contours show a dilated LV-mask in which the inference on the unregistered data is performed. (c-d) Maps of mean MD, FA as well as an artificial lesion map resulting serving as ground truth of the simulated dataset.
  • Learning the relationship between human brain tissue microstructure and diffusion MRI data
    Emmanuelle Weber1, Christoph Leuze1, Daniel A. N. Barbosa1, Gustavo Chau Loo Kung1, Kalanit Grill-Spector1, and Jennifer A. McNab1
    1Stanford, Stanford, CA, United States
    Feasibility study of a machine learning direct prediction of tissue microstructure from raw diffusion MRI data. We attempted to predict the well-understood main fiber orientation from both simulated and dMRI-3D histology dataset.
    Figure 1: Deep learning framework aiming at predicting the microstructural features from raw diffusion MRI (dMRI) data using histology images as ground truth. Example of prediction of main fiber orientation from previously acquired data on human thalamus.
    Figure 2: Summary of the whole pipeline that enables to predict a single simulated fiber orientation using deep learning. A) Normalized dMRI signal from an B) infinitely long rotating cylinder as a function of the C) PGSE sequence b values for different gradient orientation. D) This signal is then fed to a neural network to predict the E) orientation of the cylinder given by the spherical angles theta and phi.
  • Patch-CNN-DTI: Data-efficient high-fidelity tensor recovery from 6 direction diffusion weighted imaging.
    Tobias Goodwin-Allcock1, Ting Gong1, Robert Gray2, Parashkev Nachev2, and Hui Zhang1
    1Centre for Medical Image Computing (CMIC), UCL, London, United Kingdom, 2High-Dimensional Neurology, University College London Queen Square Institute of Neurology, London, United Kingdom
    Proposed Patch-CNN-DTI as a method for estimating accurate diffusion tensors from as few as 6 diffusion-weighted images (DWI) with only one training subject, which outperforms conventional fitting with twice the number of DWIs.
    Figure 2) Top are the FA weighted colour maps of the primary direction of diffusion. The motor tract, highlighted in yellow, is enlarged at the bottom where the primary directions of diffusion are illustrated as colour encoded sticks. The sticks are masked such that only WM voxels remain, determined by FA>0.2. Estimations from Patch-CNN are visually more similar to the GT for both RGB colourmap and sticks.
    Figure 4) Boxplots computed over the medians of errors for each of the 4 testing subjects. For (a,c,d) the median error is computed across all of the brain voxels at each subject. For (b) median error is computed for each subject across voxels for which the primary direction of diffusion is well defined, where the linearity coefficient9>0.6.
  • Rapid Multi-slice STEAM Diffusion Imaging with a Prepared Gradient Echo Echoplanar Sequence
    David C Alsop1,2, Manuel Taso1,2, and Arnaud Guidon3
    1Radiology, Beth Israel Deaconess Medical Center, Boston, MA, United States, 2Radiology, Harvard Medical School, Boston, MA, United States, 3Global MR applications and workflow, GE Healthcare, Boston, MA, United States
    We propose a non-selective preparation of a conventional gradient echo echoplanar sequence that enables the rapid acquisition of many slices. Initial application to the brain readily enabled up to 32 slice acquisition within a single TR.
    Figure 1. Schematic diagram of the nonselective STEAM prepared multislice echoplanar sequence.
    Figure 2: Example multi-slice b=1000 diffusion weighted images after correction for differential slice delays by geometric averaging.
  • Multi-band in Diffusion MRI: Can we go too fast?
    Arun Venkataraman1, Benjamin Risk2, Deqian Qiu3,4, Jianhui Zhong1,5, and Zhengwu Zhang6
    1Physics and Astronomy, University of Rochester, Rochester, NY, United States, 2Biostatistics and Bioinformatics, Emory University, Atlanta, GA, United States, 3Radiology and Imaging Sciences, Emory University School of Medicine, Atlanta, GA, United States, 4Biomedical Engineering, Emory University, Atlanta, GA, United States, 5Imaging Sciences, University of Rochester Medical Center, Rochester, NY, United States, 6Biostatistics and Computational Biology, University of Rochester Medical Center, Rochester, NY, United States
    In this study, we found that slice and phase acceleration lead to increased noise amplification. This leads to worse DTI fitting and instability of tractography that is preferentially seen in the frontal areas, with relative sparing of the occipital areas.
    Figure 2 g-factor calculated for all accelerated acquisitions, red line indicates g-factor of 1, which represents the SNR of the unaccelerated (S1P1) dMRI acquisiton. p-values indicated by asterisks and were calculated using a paired t-test, in this figure, all p < 0.0001 (****).
  • A unified framework for estimating diffusion kurtosis tensors with multiple prior information
    Li Guo1,2,3, Lyu Jian2,3, Yingjie Mei4, Mingyong Gao1, Yanqiu Feng2,3, and Xinyuan Zhang2,3,5
    1Department of MRI, The First People’s Hospital of Foshan (Affiliated Foshan Hospital of Sun Yat-sen University), Foshan, China, 2School of Biomedical Engineering, Southern Medical University, Guangzhou, China, 3Guangdong Provincial Key Laboratory of Medical Image Processing, Southern Medical University, Guangzhou, China, 4Philips Healthcare, Guangzhou, China, 5Guangdong-Hong Kong-Macao Greater Bay Area Center for Brain Science and Brain-Inspired Intelligence, Guangzhou, China
    The unified framework that integrates multiple prior information including nonlocal structural self-similarity, local spatial smoothness, physical relevance of DKI model, and noise characteristic of magnitude diffusion images can improve the accuracy of DKI tensor estimation.
    Figure 3. FA, MD, MK, noise SD (σ) maps and their corresponding error maps of the M1NCM-based methods, using the simulated data with unstationary noise level of 0.02. The error maps show the absolute difference between the reference parameters and the estimated parameters. The RMSE of each parameter map is shown in the right bottom of its error map. The unit of the MD is ×10-3 mm2/s.
    Figure 1. RMSE comparisons of FA, MD, MK maps estimated with the UVNLM-NLS, UVNLM-CWLLS, M1NCM, M1NCM-NSS, M1NCM-LSS, M1NCM-NSS-LSS, and M1NCM-NSS-LSS-PR algorithms, using the simulated datasets with stationary and fixed noise levels of 0.02-0.09.
  • Influence of electrocardiogram signal triggering on filter exchange imaging
    Julian Rauch1,2, Dominik Ludwig1,2, Frederik B. Laun3, and Tristan A. Kuder1
    1Division of Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Faculty of Physics and Astronomy, Heidelberg University, Heidelberg, Germany, 3Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Erlangen, Germany
    The signal stability of AXR measurements is slightly improved when suppressing pulsation-induced variations by ECG triggering. However, pulsation does not seem to be the main source of signal variations.
    Figure 1: Schematic representation of a filter exchange imaging (FEXI) sequence using two pulsed gradient spin echo (PGSE) blocks. The first gradient pair used as the FEXI filter is followed by a varying mixing time during which the magnetization is longitudinally stored while transversal components are dephased. Before and after the second and third radiofrequency pulse, respectively, gradients to choose the right echo path are applied. The second gradient pair is a standard diffusion weighting. This block is followed by an echo planar imaging (EPI) readout.
    Figure 2: Comparison of the standard deviations σ resulting from the different trigger experiments. No diffusion weighting was applied (b = 0 s/mm2). The three used orthogonal diffusion encoding directions (2/3, 2/3, 1/3), (1/3, 2/3, 2/3) and (2/3, 1/3, 2/3) are depicted in blue, red and black, respectively.
  • Improved parameter estimation for non-Gaussian IVIM using an unbiased vector non-local means
    Lyu Jian1,2, Xinyuan Zhang1,2,3, Yingjie Mei4, and Li Guo1,2,5
    1School of Biomedical Engineering, Southern Medical University, Guangzhou, China, 2Guangdong Provincial Key Laboratory of Medical Image Processing, Southern Medical University, Guangzhou, China, 3Guangdong-Hong Kong-Macao Greater Bay Area Center for Brain Science and Brain-Inspired Intelligence, Guangzhou, China, 4Philips Healthcare, Guangzhou, China, 5Department of MRI, The First People’s Hospital of Foshan (Affiliated Foshan Hospital of Sun Yat-sen University), Foshan, China
    To improve the accuracy and precision of parameter estimation for NG-IVIM, we propose to use an unbiased vector non-local means (UVNLM) filter to denoise and correct the noise bias before NG-IVIM model fitting.
    Fig. 4. f, D*, Dapp, Kapp maps and their corresponding error maps of the proposed UVNLM-NLS method. The error maps show the absolute difference between the reference parameters and the estimated parameters.
    Fig. 1. RMSE comparisons of f, D*, Dapp, Kapp maps estimated with the conventional NLS, the PCA-NLS, the proposed UVNLM-NLS method.
  • Evaluation of quantitative MRI parameters reproducibility across a major scanner upgrade: spinal cord diffusion weighted (DW) imaging
    Ratthaporn Boonsuth1, Marco Battiston1, Francesco Grussu1,2, Marios Yiannakas1, Torben Schneider3, Rebecca Samson1, Ferran Prados1,4,5, and Claudia A. M. Gandini Wheeler-Kingshott1,6,7
    1NMR research Unit, Queen Square MS Centre, Department of Neuroinflammation, UCL Queen Square Institute of Neurology, London, United Kingdom, 2Radiomics Group, Vall d’Hebron Institute of Oncology, Vall d’Hebron Barcelona Hospital Campus, Barcelona, Spain, 3Philips Healthcare, Guildford, Surrey, United Kingdom, 4Centre for Medical Image Computing, Medical Physics and Biomedical Engineering, University College London, London, United Kingdom, 5E-Heath Centre, Universitat Oberta de Catalunya, Barcelona, Spain, 6Department of Brain & Behavioural Sciences, University of Pavia, Pavia, Italy, 7Department of Brain Connectivity Centre Research Department, IRCCS Mondino Foundation, Pavia, Italy
    The diffusion-derived metrics are reproducible, with no significant differences between pre- and post-upgrade in spinal cord, white matter, and grey matter. Following a major scanner upgrade at a single site, diffusion measurements were found not to differ substantially
    Figure 1. Bland–Altman plots of four diffusion metrics for 3 different ROIs, namely whole spinal cord area, white matter, and grey matter. The x and y-axes represent, respectively, average, and mean differences between pre- and post-upgrade. The blue lines show the mean of the differences, while the pairs of dotted red lines denote the 95% confidence intervals.
    Figure 2. Parametric maps for fractional anisotropy (FA), mean diffusity (MD), mean kurtosis (MK) and neurite density index (NDI) from a single subject obtained pre- and post-upgrade.
  • High-resolution microstructural imaging in the human hippocampus with b-tensor encoding and zoomed imaging
    Jiyoon Yoo1, Leevi Kerkelä1, Patrick W. Hales1, Kiran K. Seunarine1, Iulius Dragonu2, Enrico Kaden1, and Christopher A. Clark1
    1UCL Great Ormond Street Institute of Child Health, London, United Kingdom, 2Siemens Healthcare Ltd, Frimley, United Kingdom
    All-in-one sequence for microstructural imaging in the hippocampus, providing high-resolution images for localisation of hippocampal subregions and fitting of standard and advanced diffusion models.
    Figure 3. Derived microstructural maps and parameters. From top to bottom: Mean diffusivity (MD) from diffusion kurtosis fit, fractional anisotropy (FA) calculated from diffusion kurtosis fit, microscopic fractional anisotropy (μFA) from QTI, normalised size variance (CMD) from QTI. STD=standard deviation.
    Figure 4. (A) Mean diffusion-weighted LTE image at b-value of 1000 s/mm2 shows contrast within the hippocampal subregions. Subregions were manually segmented for subiculum (blue), Cornu Ammonis (CA) regions CA1-3 (red) and CA4 with dentate gyrus (DG, yellow). (B) Microstructural parameters were calculated in each subregion; Subiculum, CA1-3 and CA4/DG.
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Digital Poster Session - Diffusion: Encoding & Estimation
Diffusion/Perfusion
Tuesday, 18 May 2021 19:00 - 20:00
  • Benefits of arbitrary gradient waveform design for diffusion encoding
    Kevin Moulin1,2,3, Mike Loecher1,2, Matthew J Middione1,2, and Daniel B Ennis1,2,3
    1Department of Radiology, Stanford University, Stanford, CA, United States, 2Department of Radiology, Veterans Administration Health Care System, Palo Alto, CA, United States, 3Cardiovascular Institute, Stanford University, Stanford, CA, United States
    ARB waveforms can precisely meet their design constraints defined in the numerical optimization while their conversion to TRAP waveforms lead to higher residual gradient moments. For symmetric design, ARB waveforms offer higher b-value than TRAP’s while better mitigating PNS.  
    Figure 2: Asymmetric motion compensated (M1=M2=0) arbitrary (ARB) waveform optimally designed with GrOpt (blue) and the corresponding trapezoidal (TRAP) implementation before (red) and after (green) balancing. Temporal evolution of the zero (M0), first (M1) and second (M2) order gradient moments are represented for each waveform. ARB has the lowest residual moments, followed by balanced TRAP, then unbalanced TRAP.
    Figure 4: Symmetric motion compensated trapezoidal (TRAP) waveforms (M1=M2=0) with SRlimit=50mT/m/s (blue) and SRmax=200mT/m/s (red) are compared to an arbitrary (ARB) cubic ramp-up waveform (green). For this scanner setup the best cubic ramp-up shape parameter was obtained for a=1.5x10-3. The temporal evolution of the b-value as well as the peripheral nerve stimulation (PNS) plots are represented for each waveform. As marked by the red dashed line, a PNS ≥1 indicates potential stimulation.
  • Gradient waveforms for comprehensive sampling of the frequency and "shape" dimensions in b(ω)-encoded diffusion MRI
    Hong Jiang1 and Daniel Topgaard1
    1Physical Chemistry, Lund University, Lund, Sweden
    The proposed family of gradient waveforms enables comprehensive sampling of both the frequency and shape dimensions of diffusion encoding as required for detailed characterization of restrictions and anisotropy in heterogeneous materials such as brain tissues.
    Figure 2. Experimental (markers) and fitted (lines) “powder-averaged”18 signal S/S0 vs. b-value. (a) Two-compartment phantom with pure water and a concentrated solution of magnesium nitrate give rise to two isotropic Gaussian (ω-independent) components. (b) Polydomain lamellar liquid crystal giving Gaussian axial and radial diffusivities, DA and DR, as estimated with a “Pake” model fit12. (c) Sediment of yeast cells with intra- and extracellular compartments, the latter exhibiting restricted (ω-dependent) diffusion.
    Figure 1. Gradient waveforms gi(t) with duration τ for comprehensive sampling of the 2D space of root-mean-square frequency ωrms and normalized anisotropy bΔ (“shape”) of the tensor-valued diffusion encoding spectrum b(ω) with elements bij(ω). The q-vector trajectories shown for the bΔ= 0 case are derived from magic-angle spinning (MAS) and double rotation (DORn). Superquadric tensor glyphs29 along the vertical axis indicate the special values bΔ = –1/2, 0, 1/2, and 1. The waveforms are scaled to give identical b-values.
  • Tissue microstructure by ellipsoidal tensor encoding with independently varying spectral anisotropy and tuning
    Samo Lasic1,2 and Henrik Lundell1
    1Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital Hvidovre, Copenhagen, Denmark, 2Random Walk Imaging, Lund, Sweden
    Ellipsoidal tensor encoding with independent control of spectral anisotropy and tuning yields distinctly different signal signatures for compartments with different anisotropic time-dependent diffusion.
    Figure 1: Tuned ellipsoidal tensor encodings with varying spectral anisotropy featuring more encoding power at low frequencies (LF-ETE) or high frequencies (HF-ETE) along z-axis. While the trace spectra is similar for LF-ETE and HF-ETE, the power distribution across different directions is markedly different. Color coding is based on the RGB-weights given by projections of the encoding power in the three bands with crossover frequencies determined by $$$D(\omega)$$$ for a sphere with $$$D_0^2R^{-4}=8000 \,\mathrm{s}^{-2}$$$ reaching 1/3 and 2/3 of the asymptotic value.
    Figure 3: Directional spread of signals (normalized STD, $$$\sigma_\mathrm{S}/\bar{S}$$$) as a function of compartment size for cylindrical, ellipsoidal and stick-like restrictions. HF-ETE (solid blue lines) and LF-ETE (dashed red lines) for Watson orientation distributions with varying order parameters (OP). Location of the minima is independent of OP. For cylindrical restrictions, the minima occur only with the HF-ETE, while for stick-like restrictions, the minima occur only with the LF-ETE. For ellipsoidal restrictions we have minima with both LF-ETE and HF-ETE.
  • A Novel Fast Quantitative Parameter Distribution Estimator Applied to Diffusion Tensor Distribution Imaging
    Anders Garpebring1
    1Radiation Sciences, div. Radiation Physics, Umeå University, Umeå, Sweden
    Non-parametric diffusion tensor distribution estimation is very computationally expensive and can require several hours of processing for a single 3D volume. This work shows that this time can be reduced to minutes or even seconds.
    Figure 1. A comparison between a high quality reference mean axial diffusivity map (left column) and mean axial diffusivity maps obtained using the REF and FAST methods. The label in the upper left corner shows the estimation method used and the numbers indicate number of b-tensors / number of averaged estimates. The number in the lower left corner shows the normalized mean absolute error between the image in the left column and the current image.
    Figure 3. The time required to estimate one sample for the REF and FAST methods. Note that this time scales linearly with the number of samples. I.e. if 25 estimates are averaged as for some of the maps in Figure 1 and 2 the time in the table needs to be multiplied by 25.
  • Quantifying the Repeatability of Microstructural Measures Derived from Free Gradient Waveforms
    Kristin Koller1, Chantal MW Tax1,2, Dmitri Sastin1,3,4, and Derek K Jones1,5
    1Cardiff University Brain Research Imaging Centre, Cardiff, United Kingdom, 2Image Sciences Institute, University Medical Center Utrecht, Utrecht, Netherlands, 3Department of Neurosurgery, University Hospital of Wales, Cardiff, United Kingdom, 4BRAIN Biomedical Research Unit, Health & Care Research Wales, Cardiff, United Kingdom, 5Mary MacKillop Institute for Health Research, Australian Catholic University, Melbourne, Australia
    High test-retest repeatability of microscopic FA (μFA) and isotropic and anisotropic diffusional variance (MKi and MKa) derived from free gradient waveforms is demonstrated in a cohort of 6 participants scanned 5 times on an ultra-high gradient MRI scanner.
    Fig. 3. Summary statistical maps for each participant averaged across all sessions. μFA. As expected, the bright voxels are highest in dense white matter regions. Bright voxels in SD and COV maps show more variability in regions contaminated with cerebrospinal fluid such as the ventricles, and low variability in white matter regions. MKi. Bright voxels located in areas of isotropic diffusion such as CSF in the ventricles. MKa Bright voxels demonstrate regions of strong anisotropic diffusion.
    Fig. 2A. Voxel-wise whole brain white matter Pearson correlations are presented between individual time points for μFA white matter skeletons. Voxels pooled across all subjects for each map, r = Pearson correlation coefficient, p<.0001 for all plots. Univariate histograms on the diagonal show distributions of voxels of μFA across all voxels. Calculation of metrics in session 2 of one subject was not robust and thus excluded.
  • Adequate mixing time for double diffusion encoding in normal brain structures and brain tumors
    Kentaro Akazawa1, Koji Sakai1, Tomoaki Kitaguchi1, Tomonori Toyotsuji1, Thorsten Feiweier 2, Hiroshi Imai3, and Kei Yamada1
    1Radiology, Kyoto Prefectural University of Medicine, Kyoto, Japan, 2Siemens Healthcare GmbH, Erlangen, Germany, 3Siemens Healthcare K.K., Shinagawa, Japan
    A relatively short mixing time of 30 msec for double diffusion encoding is likely adequate to evaluate the microscopic fractional anisotropy not only in the normal brain structures, but also in pathologically abnormal areas such as brain tumors.
    The scatter plots of relative signal intensities in the enhanced lesions in brain tumors, the normal thalamus, the normal white matters, and the lateral ventricle. The horizontal and vertical axes are relative signal intensities from the parallel directions and from the anti-parallel directions, respectively. There were significantly correlated in all areas (p < 0.001).
    The scatter plots of relative signal intensities in the enhanced lesions, the normal thalamus, the normal white matters, and the lateral ventricle. The horizontal and vertical axes are relative signal intensities from the collinear directions which are the averages of the parallel and anti-parallel directions, and from the orthogonal directions, respectively. There were significantly correlated in all areas (p < 0.001). The slopes of the thalamus and white matter seemed to be different from those in figure 2.
  • Intra-compartmental kurtosis biases tensor-valued multidimensional diffusion
    Rafael Neto Henriques1, Sune Nørhøj Jespersen2,3, and Noam Shemesh1
    1Champalimaud Research, Champalimaud Centre for the Unknown, Lisbon, Portugal, 2Center of Functionally Integrative Neuroscience (CFIN) and MINDLab, Clinical Institute, Aarhus University, Aarhus, Denmark, 3Department of Physics and Astronomy, Aarhus University, Aarhus, Denmark
    Correation Tensor Imaging revealed that positive sources of intra-compartmental kurtosis bias tensor-valued MDE estimates even in the absence of detectable diffusion time dependence. A regime in which tensor-valued methods can accurately estimate anisotropic kurtosis is identified.
    Fig.4 – Kurtosis estimates of a representative rat brain coronal slice: A) CTI kurtosis estimates; B) Tensor-valued kurtosis estimates obtained by fitting Eq. 2 to all acquired data (TV(all)); C) Tensor-valued kurtosis estimates obtained by fitting Eq. 2 to only the data acquired with b1=b2 and parallel/perpendicular gradient directions (TV(sel)).
    Fig.5 – Scatter plots of tensor-valued vs CTI kurtosis estimates: A) Tensor-valued kurtosis estimates obtained by fitting Eq. 2 to all acquired data (TV(all)) vs CTI estimates; B) Tensor-valued kurtosis estimates obtained by fitting Eq. 2 to DDE data acquired with b1=b2 (TV(sel)) vs CTI estimates. The points in the scatter plots are color-coded according to CTI’s Kintra estimates.
  • Towards more robust and reproducible Diffusion Kurtosis Imaging
    Rafael N Henriques1, Sune N. Jespersen2,3, Derek K. Jones4,5, and Jelle Veraart6
    1Champalimaud Research, Champalimaud Centre for the Unknown, Lisbon, Portugal, 2Department of Clinical Medicine, Aarhus University, Aarhus, Denmark, 3Department of Physics and Astronomy, Aarhus University, Aarhus, Denmark, 4School of Psychology, Cardiff University, Cardiff, United Kingdom, 5Mary MacKillop Institute for Health Research, Australian Catholic University, Melbourne, Australia, 6Center for Biomedical Imaging, NYU Grossman School of Medicine, New York, NY, United States
    Our novel regularized DKI estimator improves the robustness and reproducibility of the kurtosis metrics and results in parameter maps with enhanced quality and contrast; thereby promoting the wider use of DKI in clinical research and potentially diagnostics
    Figure 4: The $$$\bar{K}$$$ maps for the various data set are shown for the ordinary and regularized NLS in the top and middle row, respectively. Moreover, we show the map of the predicted mean kurtosis $$$\hat{K}$$$ (bottom row) to illustrate the similarity in contrast.
    Figure 2: The tract-averaged $$$\bar{K}$$$ using various fitting strategies and $$$\hat{K}$$$ (bottom row) for the test (filled marker) and retest data (open marker) each subject (labeled by marker shape). The graphs on the right column show the same data, but windowed differently for enhanced contrast. Seven major white matter tracts were evaluated: genu and splenium of the corpus callosum (GCC and SCC), corticospinal tract (CST), arcuate fasciculus (AF), inferior fronto-occipital fasciculus (IFO), Superior Longitudinal Fasciculus (SLF) and optic radiation (OR).
  • The diffusion time dependence of MAP-MRI parameters in the human brain
    Alexandru V Avram1,2, Qiyuan Tian3, Qiuyun Fan3, Susie Y Huang3,4, and Peter J Basser1
    1Eunice Kennedy Shriver National Institute of Child Health and Human Development, National Institutes of Health, Bethesda, MD, United States, 2Center for Neuroscience and Regenerative Medicine, The Henry Jackson Foundation, Bethesda, MD, United States, 3Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, MA, United States, 4Harvard-MIT Division of Health Sciences and Technology, Massachusetts Institute of Technology, Cambridge, MA, United States
    We measure mean apparent diffusion propagators (MAP) in the human brain using different diffusion times. We estimate the time-scaling parameters of two important propagator parameters in order to describe anomalous diffusion processes in fractal-like tissue environments.
    Figure 4: Time-scaling MRI parameters derived from in vivo MAP-MRI data with different diffusion times quantify anomalous diffusion in live brain tissues. The random walk dimension, dw, and the spectral dimension, ds, are dynamic exponents that describe the diffusion process in a fractal-like medium, while the fractal dimension, df, describes the scaling of the mass of the environment with distance.
    Figure 1: Diffusion time dependence of MAP-MRI scalar parameters. Generally, the tissue contrast in Propagator Anisotropy (PA) and Non-Gaussianity (NG) images increases with diffusion time; meanwhile, both the Return-to-axis probability (RTAP) and the Return-to-origin-probability (RTOP) decrease with diffusion time throughout the parenchyma, especially in gray matter.
  • Investigating the relationship between diffusion MRI signal cumulants and hepatocyte microstructure at fixed diffusion time
    Francesco Grussu1, Kinga Bernatowicz1, Ignasi Barba2, and Raquel Perez-Lopez1,3
    1Radiomics Group, Vall d'Hebron Institute of Oncology, Vall d'Hebron Barcelona Hospital Campus, Barcelona, Spain, 2NMR Lab, Vall d'Hebron Institute of Oncology, Vall d'Hebron Barcelona Hospital Campus, Barcelona, Spain, 3Department of Radiology, Hospital Universitari Vall d'Hebron, Barcelona, Spain
    We investigate in simulations the feasibility of estimating hepatocyte size and diffusivity from diffusion signal cumulants (apparent diffusivity and kurtosis) at fixed diffusion time. The task appears to be feasible with realistic liver SNR levels.
    Figure 4: example of interpolation of the experimental D0(D,K) and L(D,K) observations for a SNR at b = 0 of 20. Top: observations for Δ = 50 ms and bmax = 1500 s mm–2 (A, to the left: D0(D,K); B, to the right: L(D,K)). Bottom: radial basis function interpolation and extrapolation to the whole (D,K) domain (C, to the left: D0(D,K); D, to the right: L(D,K)).
    Figure 1: example of synthetic hepatic cells considered in this study. From left to right: different cell realisations obtained by independent perturbations of regular prisms with the same base shape. From top to bottom: different base shapes (square, pentagonal and hexagonal). L corresponds to the inter-base distance.
  • Application of DKI and IVIM in staging of hepatic fibrosis
    YANLI JIANG1, Jie Zou1, FengXian Fan1, Yuping Bai1, Jing Zhang1, and Shaoyu Wang2
    1Department of Magnetic Resonance, LanZhou University Second Hospital, LanZhou, China, 2MR Scientific Marketing, Siemens Healthineers, Shanghai, China
    Our study evaluated the relationship between IVIM-DKI diffusion models and clinical-pathologic to assess their diagnostic accuracy for staging of hepatic fibrosis. We recommended the DKI model in MRI to stage the hepatic fibrosis.
    Figure 1. Examples of placement of regions of interest (ROIs) on MD map(a), MK map(b), D map (d), PD map (e), f map(f)
    Figure 2. The Pearson rank correlation analysis shows a negative correlation between the MD values and the Fibroscan (r=-0.452 , P=0.016)
  • Single-shot measurement of sub-millisecond, time-dependent diffusion using optimized, unequal pulse spacings in a static field gradient
    Teddy Xuke Cai1,2, Nathan Hu Williamson1,3, Velencia Witherspoon1, Rea Ravin1,4, and Peter Basser1
    1Section on Quantitative Imaging and Tissue Sciences, Eunice Kennedy Shriver National Institute of Child Health and Human Development, Bethesda, MD, United States, 2Wellcome Centre for Integrative Neuroimaging, University of Oxford, Oxford, United Kingdom, 3National Institute of General Medical Sciences, Bethesda, MD, United States, 4Celoptics, Inc., Rockville, MD, United States
    Instantaneous diffusivity curves from 50 – 500 microseconds are recovered in 1 minute using a static gradient, time-incremented echo train acquisition (SG-TIETA) framework. Measured curves on yeast suspensions are consistent with the expected behavior for micron length-scale structures.
    SG-TIETA decays and inverted $$$\textbf{X}$$$ for D6, yeast, and water. (a) Decays analyzed as described in the text. Err. bars = $$$\pm1$$$ SD for, in legend order, $$$38, 3, 4, 25$$$ repetitions truncated at $$$n = 34, 17, 17, 15$$$, respectively. (b) $$$\textbf{X}$$$ solutions. Inversion parameters were identical to Fig. 2 other than $$$\Delta t(k)$$$ for D6. Again, $$$D_0$$$ and $$$D_\infty$$$ (dashed lines) were given as initial $$$\textbf{X}$$$ guesses. Zoomed plot compares experimental results to the presented theoretical short-time $$$D_{\mathrm{inst}}(t)$$$.
    Example SG-TIETA sequence. (a) Timings: $$$m_j = \{1, 3, 1, 2, 1\}$$$, $$$\tau = 4\delta$$$, and $$$\delta = 14\; \mu$$$s $$$= 1$$$ dash. $$$\pi$$$-pulses occur at $$$t_n$$$ and echoes form at $$$T_n$$$. Magenta line indicates timing behavior: $$$T_n = t_{n} + h_n$$$, where $$$h_n$$$ is the $$$|F(t)|/\gamma g$$$ "height" at $$$t_n$$$, given recursively by $$$h_1 = \tau$$$ and $$$h_{n} = 2\tau + m_n\delta -h_{n-1}$$$ for $$$n > 1$$$. (b) Direct echo $$$F(t)$$$ drawn along with other coherence pathways that refocus (red, dash-dot) or do not refocus (gray, dotted).
  • Automated Surface-Based Segmentation of Deep Grey Matter Brain Regions Based Solely on Diffusion Tensor Images
    Graham Little1 and Christian Beaulieu1
    1Biomedical Engineering, University of Alberta, Edmonton, AB, Canada
    An automatic surface-based deep grey matter segmentation method was developed that works directly on brain diffusion images. As a demonstration, the method yielded unique non-linear trajectories of diffusion metrics in deep grey matter regions in  healthy people aged 6-90 years. 
    Figure 3. Deep grey matter segmentations derived from workflow in Figure 2 displayed for three subjects spanning a large age range. Segmentations are displayed in 3D as well as on a single axial slice of the mean b1000 diffusion weighted image and FA map. Even with substantial subject variability in brain shape, reasonably accurate cortical segmentations were generated for each region
    Figure 2. Segmentation workflow of deep GM structure based solely on DTI. (A) Initial segmentations registered from an atlas are (B) converted into surfaces. (C) The caudate and thalamus are deformed to an edge on the FA map or nearest ventricle edge (purple). (D) The globus pallidus (GP) is deformed on the mean b1000 image. The putamen is deformed on the FA map preventing deformation into the GP. A correction to the GP is applied on the FA map. (E) Visualization of final deep GM segmentations.
  • Investigating time dependent diffusion, microscopic anisotropy and T2 effects in the mouse heart
    Henrik Lundell1, Samo Lasič1,2, Filip Szczepankiewicz3,4,5, Beata Wereszczyńska6, Matthew Budde7, Erica Dall'Armellina6, Nadira Yuldasheva6, Jürgen E. Schneider6, and Irvin Teh6
    1Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital Hvidovre, Hvidovre, Denmark, 2Random Walk Imaging, Lund, Sweden, 3Clinical Sciences, Lund University, Lund, Sweden, 4Harvard Medical School, Boston, MA, United States, 5Brigham and Women's Hospital, Boston, MA, United States, 6Leeds Institute of Cardiovascular and Metabolic Medicine, University of Leeds, Leeds, United Kingdom, 7Department of Neurosurgery, Medical College of Wisconsin, Milwaukee, WI, United States
    We suggest a battery of MDE measurements that probe diffusivity and microscopic anisotropy at different diffusion and echo times. We show a clear effect of time-dependent diffusion but a smaller effect from transversal relaxation.
    Microscopic fractional anisotropy (µFA) calculated from pairs of STE and tuned LTE for the long τ and TE (top left), short τ and long TE (top center) and short τ and short TE. ROI mean and standard deviation from the 3 maps are shown below.
    Mean diffusivity (MD) maps calculated form the initial slope of the different LTE and TE configurations. Maps are ordered with increasing high frequency spectral content (see figure 1) towards the right.
  • Data-driven separation of MRI signal components for tissue characterization
    Sofie Rahbek1, Kristoffer H. Madsen2,3, Henrik Lundell2, Faisal Mahmood4,5, and Lars G. Hanson1,2
    1Department of Health Technology, Technical University of Denmark, Kgs. Lyngby, Denmark, 2Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital Hvidovre, Hvidovre, Denmark, 3Department of Applied Mathematics and Computer Science, Technical University of Denmark, Kgs. Lyngby, Denmark, 4Laboratory of Radiation Physics, Odense University Hospital, Odense, Denmark, 5Department of Clinical Research, University of Southern Denmark, Odense, Denmark
    We propose a novel monotonous slope non-negative matrix factorization for extraction of tissue-related signal components from high-dimensional MRI data. Applications of the method are demonstrated using both diffusion-weighted and relaxometry data.
    (a): Example of a measured image of the monkey brain. (b): The signal components, W, from the msNMF. (c): The associated normalized mixture maps, H, labelled by the frame colors. A logarithmic color scale is used for the yellow component. Maps are given for both data sets and the right column shows the difference between the two (Short diffusion time subtracted from long diffusion time). The thin and thick black arrows mark the conspicuous visual cortex and cerebellum, respectively.
    Result of the msNMF for the relaxometry data of rat spinal cord. (a): The signal components, W. (b): The associated mixture maps, H, indicated by the frame and label colors. Each column of images shows the maps for a specific rat (one from each group).
  • Multi-tissue log-domain intensity and inhomogeneity normalisation for quantitative apparent fibre density
    Thijs Dhollander1,2, Rami Tabbara2, Jonas Rosnarho-Tornstrand3,4, J-Donald Tournier3,4, David Raffelt2, and Alan Connelly2
    1Developmental Imaging, Murdoch Children's Research Institute, Melbourne, Australia, 2Florey Institute of Neuroscience and Mental Health, University of Melbourne, Melbourne, Australia, 3Centre for the Developing Brain, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 4Department of Biomedical Engineering, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom
    We describe a bias field correction and intensity normalisation method that leverages information from multi-tissue constrained spherical deconvolution results, in the log-domain. It outperforms a previously proposed approach that did not operate in the log-domain.
    Fig.5: The relative error (as a percentage) between the total signal from the resulting corrected phantom obtained from both methods (Raffelt et al.[7] and the log-domain method in this work) and the original phantom (unaffected by bias fields). The relative error is averaged across results for all 10 bias fields and overlaid with a WM image of the phantom for reference. The method by Raffelt et al.[7] struggles mostly at the extremities (low and high) of the bias field value range; i.e., deep in the brain and at the edge. At the bottom of the mask, errors exceed 20% (up to 35% in some voxels).
    Fig.4: The relative error (expressed as a percentage) between the total signal from the resulting corrected phantom obtained from both methods (Raffelt et al.[7] and the log-domain method in this work) and the original phantom (unaffected by bias fields). The relative error is averaged over the entire brain mask and shown separately for each of the 10 "ground truth" bias fields. The log-domain method proposed in this work appears to consistently outperform the method by Raffelt et al.[7], as evidenced by lower relative errors after intensity and inhomogeneity normalisation.
  • dMRIPrep: a robust preprocessing pipeline for diffusion MRI
    Michael J Joseph1, Derek Pisner2, Adam Richie-Halford3, Garikoitz Lerma-Usabiaga4, Salim Mansour1, James D Kent5, Anisha Keshavan3, Matthew Cieslak6, Erin W Dickie1, Sebastian Tourbier7, Aristotle N Voineskos1, Theodore D Satterthwaite6, Russell A Poldrack8, Jelle Veraart9, Ariel Rokem10, and Oscar Esteban7
    1The Centre for Addiction and Mental Health, Toronto, ON, Canada, 2Department of Psychology, University of Texas at Austin, Austin, TX, United States, 3eScience Institute, The University of Washington, Seattle, WA, United States, 4Basque Center on Cognition, Brain and Language, Donostia - San Sebastian, Spain, 5Neuroscience Program, University of Iowa, Iowa City, IA, United States, 6Perelman School of Medicine, University of Pennsylvania, Philadelphia, PA, United States, 7Lausanne University Hospital and University of Lausanne, Lausanne, Switzerland, 8Department of Psychology, Stanford University, Stanford, CA, United States, 9NYU Grossman School of Medicine, New York City, NY, United States, 10Department of Psychology, The University of Washington, Seattle, WA, United States
    We present dMRIPrep, a preprocessing pipeline for dMRI that reliably and consistently performs on diverse data acquired in different studies. Inspired by fMRIPrep and its wide uptake, it leverages and expands the NiPreps community framework.
    A reliable pipeline for the preprocessing of dMRI.
    dMRIPrep produces visual reports that allow quality-control of the results while serving as a scaffold for understanding the pipeline.
  • Sensitivity to WM injury in SLE assessed by diffusion MRI: influence of field strength, acquisition approach and post-processing strategy
    Evgenios N. Kornaropoulos1,2, Stefan Winzeck2,3, Theodor Rumetshofer1, Anna Wikstrom1, Linda Knutsson4,5, Marta Correia6, Pia Sundgren1,7,8, and Markus Nilsson1
    1Diagnostic Radiology, Lund University, Lund, Sweden, 2Division of Anaesthesia, University of Cambridge, Cambridge, United Kingdom, 3Department of Computing, Imperial College London, London, United Kingdom, 4Department of Medical Radiation Physics, Lund University, Lund, Sweden, 5Russell H. Morgan Department of Radiology and Radiological Science, Johns Hopkins University, Baltimore, MD, United States, 6MRC Cognition and Brain Sciences Unit, University of Cambridge, Cambridge, United Kingdom, 7Lund University BioImaging Center, Lund University, Lund, Sweden, 8Department of Medical Imaging and Physiology, Skane University Hospital, Lund, Sweden
    We found that, in terms of detecting groupwise WM changes, DTI is preferrable to DKI, 3T yields slightly better results than 7T, Eddy is a more effective post-processing step than Gibbs and LPCA, while smoothing the data is detrimental.
    Evaluation of diffusion strategy deriving the diffusion feature (x-axis) with highest Cohen’s d (Equation1, y-axis). The mean and standard deviation of each diffusion parameter, derived by either 3T-DTI or 3T-DKI or 7T-DTI, were examined and denoted by the letters “M” and “S” respectively (e.g. MFA for FA). The LPCA and Gibbs and Eddy pipeline was applied in each case. No smoothing was applied. The box-and-whisker plot captures variation among tracts.
    Evaluation of tracts' segmentation. The six tracts (left and right fornix, left and right inferior cerebellar peduncle, left and right superior cerebellar peduncle) that exceeded the value of 0.19, were excluded for further analysis. A list with all abbreviations for the studied nerve tracts can be found at the github page of TractSeg ( https://github.com/MIC-DKFZ/TractSeg ).
  • Reducing Noise in Complex-Valued Multi-Channel Diffusion-Weighted Data via Optimal Shrinkage of Singular Values
    Khoi Minh Huynh1,2, Wei-Tang Chang2, and Pew-Thian Yap1,2
    1Biomedical Engineering, UNC Chapel Hill, Chapel Hill, NC, United States, 2Department of Radiology and Biomedical Research Imaging Center (BRIC), UNC Chapel Hill, Chapel Hill, NC, United States
    We show that denoising on complex-valued data, rather than the magnitude data, is a more effective means of improving diffusion-weighted images, microstructure quantification, fiber orientation estimation, and tractography.
    Fig. 1. Effects on Diffusion-Weighted Images. Images for different b-values from the the original noisy dataset and after denoising with dwidenoise, VST-Mag, and OS-SVD.
    Fig.3. Effects on Orientation Estimation and Tractography. OS-SVD improves estimation of the fiber orientation distribution function (fODF) and eventually tractography.
  • Model Based Denoising of Diffusion MRI Reduces Bias in Tensor Derived Parameters and Connectivity Measures
    Nastaren Abad1, Luca Marinelli1, Radhika Madhavan1, and Tom K.F Foo1
    1General Electric Global Research, Niskayuna, NY, United States
    Model based denoising was used to explore accelerated sampling by evaluating bias developed in qualitative and quantitative end points. Experimental results highlight superior performance, compared to ground truth, in noise and bias reduction in metrics and structure preservation.
    Figure 1. Examples of diffusion-weighted images with and without denoising, highlighting that signal components can be individually separated with improved conspicuity, and without spatial regularization or blurring. All images are scaled to the non-denoised b=500 s/mm2 data.
    Figure 2. Qualitative assessment of denoising indicates retention of spatial features such as striatal cell bodies connecting the caudate and putamen through the internal capsule (red arrow).