Signal Modelling for Quantitative MRI
Acq/Recon/Analysis Wednesday, 19 May 2021

Oral Session - Signal Modelling for Quantitative MRI
Acq/Recon/Analysis
Wednesday, 19 May 2021 14:00 - 16:00
  • Probing restricted diffusion and water exchange with free gradient waveforms: Addressing the need for a compartment model
    Arthur Chakwizira1, Filip Szczepankiewicz2, Linda Knutsson1,3, and Markus Nilsson2
    1Department of Medical Radiation Physics, Lund University, Lund, Sweden, 2Department of Diagnostic Radiology, Lund University, Lund, Sweden, 3Russell H. Morgan Department of Radiology and Radiological Science, Johns Hopkins University School of Medicine, Baltimore, MD, United States

    We have proposed a general theory for describing restricted diffusion and water exchange for any gradient waveform, b-value and diffusion encoding time. We validated the model by numerical simulations that show good agreement with ground truth.

    Figure 3: Contrast and goodness of fit for different combinations of restriction and exchange. Panel (a) shows that the proposed model describes that data well in all simulated cases. (b) Exchange rate and cell size estimates are in good agreement with simulation. (c) Changes in exchange rate for a fixed size do not erroneously manifest in our model as a change in size. This demonstrates the independent contributions of restriction and exchange to the signal as captured by our model.
    Figure 4: Demonstration of the robustness of the developed theory to ultrahigh b-values and long encoding times. Panel (a) shows a good agreement between model and simulation for all considered b-values. Panels (b) and (c) show that the theory produces stable estimates of size and exchange over the entire range of simulates b-values and encoding times.
  • Identifying microstructural changes in diffusion MRI models; How to break parameter degeneracies
    Hossein Rafipoor1, Saad Jbabdi1, Ludovica Griffanti1,2, and Michiel Cottaar1
    1Wellcome Centre for Integrative Neuroimaging (WIN), Nuffield Department of Clinical Neurosciences (NDCN), University of Oxford, Oxford, United Kingdom, 2Wellcome Centre for Integrative Neuroimaging (WIN), Department of Psychiatry, University of Oxford, Oxford, United Kingdom

    We have developed a general Bayesian framework for inference on parameter changes from changes in the data. This allows us to employ more complex models to study changes. We applied this framework to study microstructural changes in white matter hyperintensities compared to a normal tissue. 

    Figure 1. Illustration of the inversion-free inference. Although the model is not invertible (each oval in parameter space (left) corresponds to a single point in measurement space (right)) we can still infer the true underlying parameter change by comparing actual change in measurements (black arrow) to the expected change as a result of particular changes in parameters (red and green arrows).
    Figure 5. A) Posterior probability maps P(s|y, Δy) of change in the parameters of NODDI for the WMH dataset. The maps show that change in sex can explain the differences between WMH and normal tissue in deep white matter. On the other hand, the null model explains the data in periventricular WMHs. The rest of the parameters did not explain differences between NAWM and WMH. B) Parcellation of the WMHs based on the best model that can explain the change. C) Estimated amount of change in sex, which shows the amount of change is higher in deep white matter.
  • Sensitivity of cortical kurtosis measurement to diffusion time in KINSA modeling assessed with Connectome scanner diffusion MRI
    Tianjia Zhu1,2, Qiyuan Tian3,4, Susie Huang3,4, and Hao Huang1,5
    1Department of Radiology, Children's Hospital of Philadelphia, Philadelphia, PA, United States, 2Department of Bioengineering, University of Pennsylvania, Philadelphia, PA, United States, 3Department of Radiology, Harvard Medical School, Boston, MA, United States, 4Massachusetts General Hospital, Boston, MA, United States, 5Department of Radiology, University of Pennsylvania, Philadelphia, PA, United States
    We have demonstrated the sensitivity of cortical kurtosis measurement to diffusion time formulated in Kurtosis-based Imaging of Neurite and Soma Architecture (KINSA) modeling using both with Connectome scanner dMRI and simulation studies.
    Fig 2. Both somas and neurites contribute to mean kurtosis in the cerebral cortex and total kurtosis as well as Ksc,v, Knc,v are sensitive to diffusion time. Both soma Ksc,v=(1-fec)fisKsc, (green lines) and neurite Knc,v=(1-fec)(1-fis)Knc, (blue lines) contribute to total intracellular kurtosis K across diffusion times and various soma volume fractions. As demonstrated by the vertical purple dashed lines, Ksc,v+Knc,v=K as expected for 25ms in the case fec=0.
    Fig 4. Cortical mean kurtosis(MK) is sensitive to diffusion time in in-vivo data. Left: Significant total MK change across relevant diffusion times 16-31ms for both subjects. Right: Bar plot for MK values in ROIs chosen for the frontal, temporal, thalamus also quantitatively shown significant MK drop.
  • Inhomogeneous Magnetization Transfer (ihMT): theoretical characterization of T1D-filtering and experimental validation
    Andreea Hertanu1,2, Lucas Soustelle1,2, Arnaud Le Troter1,2, Julie Buron1,2,3, Julie Le Priellec3, Victor N. D. Carvalho1,2,4, Myriam Cayre3, Pascale Durbec3, Gopal Varma5, David C. Alsop5, Olivier M. Girard1,2, and Guillaume Duhamel1,2
    1Aix Marseille Univ, CNRS, CRMBM, Marseille, France, 2APHM, Hôpital Universitaire Timone, CEMEREM, Marseille, France, 3Aix Marseille Univ, CNRS, IBDM, Marseille, France, 4Aix Marseille Univ, CNRS, ICR, Marseille, France, 5Division of MR Research, Radiology, Beth Israel Deaconess Medical Center, Harvard Medical School, Boston, MA, United States
    Filtering the short T1D components contributing to the ihMT signal leads to an increase in the experimental WM/GM relative contrast. A minimum of two T1D components must be considered in the theoretical model to predict this experimental observation.
    Figure 3: Simulated ihMTR(T1D) curves with various Δt values for (a, b) WM and GM respectively, using the single-T1D model. The 2% line represents the detectability threshold, arbitrarily chosen. (c, d) ihMTR(T1D) simulated for WM and GM, using the bi-T1D model. The long T1D component was fixed at 6.0 ms for WM and 5.8 ms for GM, and the short component was varied in the [10 µs; 1 ms] range. (e) Experimental ihMTR templates corresponding to different levels about the bregma.
    Figure 4: ihMTR(T1D) curves corresponding to the subtractions between the non-filtered and the filtered configurations for (a) WM and (b) GM. Only CM-Δt0.8 was able to isolate a detectable signal within a finite range of T1D values (100 µs - 1 ms). (c) Experimental subtracted ihMTR maps template at different bregma levels.
  • A computational fluid dynamics framework to generate digital reference objects for perfusion imaging
    Ulin Nuha Abdul Qohar1, Erik Andreas Hanson1, Steven Sourbron2, and Antonella Zanna Munthe-Kaas1
    1Mathematics, University of Bergen, Bergen, Norway, 2University of Sheffield, Sheffield, United Kingdom
    CFD generated perfusion MRI data was used for evaluation and comparison of tracer kinetic models. The proposed framework provides suitable ground truth data as a digital reference data to study the elusive problem of model bias in more deeply than was previously possible. 
    Simulated CA flow in the vascular system after bolus injection. The flow patterns exhibit a natural behaviour with a flow from the arterial network roots feeding the whole vasculature, spreading to the capillaries and a washout through the veins. The images were captured at 6, 8, 10, 15, 20, 25, 35, 50, 70 and 100 second respectively (from left to right).
    Plasma flow (PF) estimation results using four tracer kinetic models in 11 ROIs. The MS model is systematically underestimating PF, but generate the best estimation among the four models in terms of absolute values. The remaining models are, in general, overestimating PF and generate close to identical values, except for ROI 2. This reveals that the 2-compartment models are over-parameterized and not suited for estimations in our CA flow phantom. The proposed flow model only accounts for blood circulation in the intravascular structures.
  • On the variability of single-point MPF mapping in the human brain using different Variable Flip Angle T1 mapping protocols
    Lucas Soustelle1,2, Thomas Troalen3, Andreea Hertanu1,2, Maxime Guye1,2, Jean-Philippe Ranjeva1,2, Guillaume Duhamel1,2, and Olivier M. Girard1,2
    1Aix Marseille Univ, CNRS, CRMBM, Marseille, France, 2APHM, Hôpital Universitaire Timone, CEMEREM, Marseille, France, 3Siemens Healthcare SAS, Saint-Denis, France
    Fast MPF mapping has shown great promises for the evaluation of myelin-related studies while allowing for acceptable scan times. Here we show how the input T1 map of the single-point method inherently biases MPF values, and that T1 should be jointly estimated in SP-quantitative MT applications.
    Figure 2: Representative axial slices of T1 (upper row) and MPF (lower row) maps from VFA protocols A to E.
    Figure 1: Simulated difference (ΔT1) between input T1 (1000 ms) and estimated T1 by the VFA method as a function of the pulse width for an SPGR sequence without MT effects (orange) or perfect spoiling (yellow), SPGR with MT and realistic spoiling (blue), and SPGR with CSMT pulses with MT and realistic spoiling at reference FA of 30° (purple) and 90° (green). Simulated bias related to protocols A to E are reported. SPGR-CSMT estimations were performed with a pulse duration superior to 1-ms as spectral overlapping was found suitably limited to not disrupt the on-resonance component.
  • Rapid approximate Bayesian $$$T_2$$$ analysis under Rician noise using deep initialization
    Jonathan Doucette1,2, Christian Kames1,2, Christoph Birkl3, and Alexander Rauscher1,2,4,5
    1UBC MRI Research Centre, Vancouver, BC, Canada, 2Physics & Astronomy, University of British Columbia, Vancouver, BC, Canada, 3Neuroradiology, Medical University of Innsbruck, Innsbruck, Austria, 4Radiology, University of British Columbia, Vancouver, BC, Canada, 5Pediatrics, University of British Columbia, Vancouver, BC, Canada
    We demonstrate that rapid $$$T_2$$$ analysis under Rician noise assumptions is possible using a methodology which utilizes a deep learned initial guess for a subsequent maximum likelihood estimation procedure. Generalization to out-of-distribution datasets demonstrated.
    Figure 3: Representative slices of MWF maps resulting from parameter inference using DECAES, MLE, and CVAE. Both CVAE and MLE are able to produce high quality MWF maps for all datasets, despite being trained only on simulated data. In dataset #3, DECAES fails to properly estimate the MWF when using the default refocusing control angle. This can be manually corrected (adjacent), but no such issue occurs for CVAE or MLE which estimate the refocusing control angle directly.
    Table 2: Mean absolute error values over inferred $$$\hat{\theta}$$$ for each method. CVAE ($$$n$$$) indicates that $$$\hat{\theta}$$$ is an average over $$$n$$$ samples $$$\hat{\theta}\sim\hat{P}(\theta\,|\,\hat{Y})$$$ from the approximate CVAE posterior $$$\hat{P}$$$.
  • The variability of MR axon radii estimates in the human white matter
    Jelle Veraart1, Erika P. Raven1, Luke J. Edwards2, Nikolaus Weiskopf2,3, and Derek K. Jones4,5
    1Center for Biomedical Imaging, NYU Grossman School of Medicine, New York, NY, United States, 2Max Planck Institute for Human Cognitive and Brain Sciences, Leipzig, Germany, 3Felix Bloch Institute for Solid State Physics, Leipzig University, Leipzig, Germany, 4School of Psychology, Cardiff University, Cardiff, United Kingdom, 5Mary MacKillop Institute for Health Research, Australian Catholic University, Melbourne, Australia

    The non-invasive quantification of the axon diameter in the human white matter using diffusion MRI is feasible, yet limited to the larger axons. The technique yields a reproducible and sensitive metric, with strong inter- and along-tract variability in the human white matter. 

    Figure 4: The trend of the effective MR radius r [μm] along the tract (posterior to anterior or inferior to superior) for each individual measurements (5 subjects and 2 repetitions) are shown in shaded lines. In addition, we show the average (solid) and 95% confidence intervals (dashed).
    Figure 2: (top) The distribution of MR axon radii [μm]. (bottom) The average MR axon radii for each individual subject (markers) is shown for all scan scan sessions.
  • Characterization of B1+ Field Variation at 3 Tesla in 373 Healthy Brains over the Lifespan
    Thomas MacLennan1, Peter Seres1, Julia Rickard1, Emily Stolz1, Christian Beaulieu1, and Alan H. Wilman1
    1Biomedical Engineering, University of Alberta, Edmonton, AB, Canada
    After transforming 373 brain $$$B_1^+$$$ maps acquired at 3T to a standard space, $$$B_1^+$$$ was found to be similar across subjects with a whole brain mean CoV of 3.65%. Slight variations were found due to brain size, shape, head orientation, CSF volume, and Tx power calibration.
    Figure 1: (a-c) show the mean, normalized $$$B_1^+$$$ ($$$nB_1^+$$$ ) map of all 373 subjects in MNI space in axial, sagittal and coronal views. Note that the scale is normalized by the nominal $$$B_1^+$$$ field strength. Images (d-f) show the coefficient of variation (CoV) map in axial, sagittal and coronal views calculated from all 373 subjects.
    Figure 2: Mean normalized $$$B_1^+$$$ calculated bilaterally for several regions of interest in MNI space. Frontal regions tend to have smaller $$$B_1^+$$$, while central regions have larger $$$B_1^+$$$. The central mark on each box represents the median and the left and right edges represent the 25th and 75th percentiles, respectively. Maximum and minimum, excluding outliers, are marked by the whiskers with all data points scattered across the boxes.
  • Predicting disability from structural and functional coupling in multiple sclerosis
    Ceren Tozlu1, Keith Jamison1, Susan Gauthier1,2,3, and Amy Kuceyeski1
    1Department of Radiology, Weill Cornell Medicine, New York, NY, United States, 2Judith Jaffe Multiple Sclerosis Center, Weill Cornell Medicine, New York, NY, United States, 3Department of Neurology, Weill Cornell Medicine, New York, NY, United States
    The structural connectivity degree as well as the structural and functional connectome coupling are important predictors of disability in multiple sclerosis. Damage to SC, particularly in the right parsorbitalis, thalamus, and parahippocampal is a hallmark of disability in MS.
    Figure 1: The relative Wilcoxon rank-sum test statistics that were computed to compare a) SC degree, b) SC degree, and c) SC-FC coupling between impaired vs not-impaired people with MS. Higher relative statistic value indicates that the variable in this region was greater in the impaired people with MS as compared to not-impaired people with MS.
    Figure 2: The prediction accuracy of the models that included a) SC degree, b) FC degree, c) concatenation of SC and FC degree, and d) SC-FC coupling in classifying people with MS by impairment level. * indicates significant differences in AUC, corrected p < 0.05.
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Digital Poster Session - Modelling: Diffusion, Kinetics & More
Acq/Recon/Analysis
Wednesday, 19 May 2021 15:00 - 16:00
  • The effects of basis sets on magnetic resonance spectroscopy quantification for stock PRESS sequences, a simulation study
    Karl Landheer1, Martin Gajdošík1, and Christoph Juchem1,2
    1Biomedical Engineering, Columbia University, New York City, NY, United States, 2Radiology, Columbia University, New York City, NY, United States
    The effect that using a realistic basis set (i.e., simulation which involves proper shaped RF pulses and timings) versus a basis set at the same echo but different exact details is investigated here via simulation with realistic PRESS spectra.
    Figure 2: The synthesized GE spectra at the three different echo times along with the fits for the four different basis sets. The synthesized spectra are given in black, the fit in red and the residual in grey. Perfect fits can be observed with the GE basis, as expected, since these particular spectra were synthesized from the GE basis, while non-perfect fits were obtained with the other three basis sets. Similar results were obtained for the synthesized Philips and Siemens spectra (results not shown).
    Figure 1: The synthesized spectra for TE = 30 ms, A, TE = 80 ms, B, and TE = 144 ms, C, across the three different vendor implementations of PRESS with blue depicting the Siemens implementation, red depicting the GE implementation and black depicting the Philips implementation. Spectra have been normalized to account for differences in voxel profile due to different pulses (i.e., different transition widths).
  • Reproducibility of Semi-LASER Localized Correlated Spectroscopic Imaging Using Concentric Ring Echo-Planar Trajectories
    Andres Saucedo1, Manoj Kumar Sarma1, Uzay Emir2, James Sayre1, Paul M Macey3, and Michael Albert Thomas1
    1Radiological Sciences, UCLA Geffen School of Medicine, Los Angeles, CA, United States, 2School of Health Sciences, Purdue University, West Lafayette, IN, United States, 3UCLA School of Nursing, Los Angeles, CA, United States

    Test-retest reproducibility of a novel 5D COSI-CONCEPT sequence was validated using a GE Braino on two different 3T MRI scanners. The phantom was scanned on different days and we observed excellent coefficients of variance (CV) and intra-class correlation coefficients for all 6 metabolites

     

    Fig. 2: (Top) Three-plane localization of the volume-of-interest (VOI) in the brain phantom. The VOI size was 10.5cm × 10.5cm × 7.5cm and the field-of-view (FOV) for spectroscopic imaging was 24cm × 24cm × 12cm along the left-to-right (L-R), anterior-to-posterior (A-P) and foot-to-head (F-H) directions, respectively. Sixteen voxels (red square) within the VOI were quantified. (Bottom) Axial NAA maps acquired along the F-H dimension within the FOV. Signal from five slices was measurable within the VOI, which had an extent of 7.5 cm along F-H.

    Fig. 3: Multi-voxel contour plots of COSY spectra from the central slice of the brain phantom. Sixteen voxels within a 4 x 4 region (red square) inside the volume-of-interest (VOI) were quantified using peak integration to compute metabolite ratios for the reproducibility analysis.
  • Linear-combination modeling of GABA-edited MEGA-PRESS at 3T: Evaluating different modeling strategies
    Helge Jörn Zöllner1,2, Sofie Tapper1,2, Steve C. N. Hui1,2, Peter B. Barker1,2, Richard A. E. Edden1,2, and Georg Oeltzschner1,2
    1Russell H. Morgan Department of Radiology and Radiological Science, The Johns Hopkins University School of Medicine, Baltimore, MD, United States, 2F. M. Kirby Research Center for Functional Brain Imaging, Kennedy Krieger Institute, Baltimore, MD, United States
    This study investigates various modeling strategies for quantifying GABA-edited spectra using LCM. Fit residuals and CV distributions of GABA+/tCr imply that a dedicated basis function for co-edited 3 ppm signals is favorable.
    (A) Distribution of the GABA+/tCr. Boxplot, smoothed distribution, and mean +- SD for all MM3co models (color-coded) and knot spacings. The coefficient of variation (SD/mean x 100) is depicted in the second row. (B) Summary of the CV analysis with the five key findings.
    A) Co-edited MM3co model implementations – Overview of the six model implementations based on the 3 ppm co-edited MM basis function MM3co (B) Combinations of modeling strategies – Overview of the possible combinations of fit range, spline knot spacing ,and MM3co model.
  • Are Cramér-Rao Lower Bounds an Accurate Estimate for Standard Deviations in Magnetic Resonance Spectroscopy?
    Karl Landheer1 and Christoph Juchem1,2
    1Biomedical Engineering, Columbia University, New York City, NY, United States, 2Radiology, Columbia University, New York City, NY, United States
    Cramér-Rao Lower Bounds have become the routine method to approximate standard deviations for MRS. It was shown that this is an appropriate approximation when the model characterizes the data, but not when the model deviates from the data.
    Figure 4: The true CRLBs (red) and estimated CRLBs (black) divided by the standard deviations calculated through MC simulations for the estimated amplitudes for the 18 metabolites and the macromolecules signal across 5 different noise factors (NF = 1 to 16) in the case where the model properly characterizes the data. The circles, squares and stars represent Gb = 3 Hz2, 8 Hz2, and 20 Hz2, respectively. The breakdown SNR is reached when the true CRLB divided by standard deviation (red) is greater than 1. Similar results were obtained for the other four estimated parameters.
    Figure 5: The true CRLBs (red) and estimated CRLBs (black) divided by the standard deviations calculated through MC simulations for the estimated amplitudes for the 18 metabolites and the macromolecules signal across 5 different noise factors (NF 1 to 16) in the case where the model does not properly characterize the data. The circles, squares and stars represent Gb = 3 Hz2, 8 Hz2, and 20 Hz2, respectively. The breakdown SNR is reached when the true CRLB/SD (red) is consistently greater than 1. Similar results were obtained for the other four estimated parameters.
  • The effects of cutting/zero-filling and linebroadening on quantification of magnetic resonance spectra via maximum-likelihood estimation
    Karl Landheer1 and Christoph Juchem1,2
    1Biomedical Engineering, Columbia University, New York City, NY, United States, 2Radiology, Columbia University, New York City, NY, United States
    Cutting/zero-filling and linebroadening are routinely employed prior to quantification, however they should be avoided as they do not improve precision and invalidate the assumptions used to calculate Cramér-Rao Lower Bounds (CRLB).
    Table 1: The standard deviation and CRLB for the 18 measured metabolites and macromolecules (MM) across the three different pipelines. Note that for no preprocessing the CRLB is an excellent proxy for standard deviation for all metabolites, while there is an artificial reduction of CRLBs for the two preprocessing steps. Furthermore, the exponential line broadening results in a reduction in precision on most metabolites. Note that these CRLBs are in the same units of standard deviation (i.e., au), it is not relative CRLBs (%) as is typically presented in MRS.
    Figure 4: The effect cutting/zero-filling, A, and exponential linebroadening, B, has on the autocorrelation function of a simulated white Gaussian noise spectrum. In both cases as the effect of the processing steps is increased the autocorrelation of the noise spectrum deviates further from its assumed shape of $$$\delta(f)$$$. Cut/zero-fill factor = 2/4/8 means that the entire time domain signal except for the first half/quarter/eighth has been artificially set to zero.
  • ComBat Empirical Bayes Model Supersedes Naive Methods for Statistical Harmonization of Multi-Site 1H MR Spectroscopy
    Lasya P Sreepada1,2, Sam H Jiang1, Huijun Vicky Liao1, Katherine M Breedlove1, Eduardo Coello1, and Alexander P Lin1
    1Radiology, Center for Clinical Spectroscopy, Brigham and Women's Hospital and Harvard Medical School, Boston, MA, United States, 2Radiology, Center for Biomedical Image Computing and Analytics, Perelman School of Medicine, University of Pennsylvania, Philadelphia, PA, United States
    Basic harmonization increased within-site variance and was not able to bring metabolite means closer together or remove significant site effects. ComBat successfully estimated and removed significant site effects, verified ANOVA and Tukey HSD tests.
    ComBat Harmonization: Box plots illustrating the means and significance with * or p-values (A) before harmonization and (B) after harmonization in all 4 sites, for (i) tNAA (ii) tCr (iii) Glx; (C) Visualization of Site effects that are removed by ComBat.
    (A) Voxel placement of PCG within the brain (B) LCModel output showing the processed spectrum in one subject at SITE 1. The selected scan passed all the manual QA measures and had an FWHM of 8 after pre-processing, the lowest in our dataset.
  • Assessment of Higher-Order SVD Rank Reduction Denoising on Dynamic Hyperpolarized [13C]pyruvate Metabolic Imaging Data on Patients with Glioma
    Sana Vaziri1, Adam Autry1, Yaewon Kim1, Hsin-Yu Chen1, Jeremy W Gordon1, Marisa LaFontaine1, Jasmine Graham1, Janine Lupo1, Jennifer Clarke2, Javier Villanueva-Meyer1, Nancy Ann Oberheim Bush3, Duan Xu1, Susan M Chang2, Peder EZ Larson1, Daniel B Vigneron1,4, and Yan Li1
    1Department of Radiology and Biomedical Imaging, University of California, San Francisco, San Francisco, CA, United States, 2Department of Neurological Surgery, University of California, San Francisco, San Francisco, CA, United States, 3Department of Neurology, University of California, San Francisco, San Francisco, CA, United States, 4Department of Bioengineering and Therapeutic Science, University of California, San Francisco, San Francisco, CA, United States
    An evaluation of two higher-order singular value decomposition denioising techniques is presented on hyperpolarized [13C]pyruvate metabolic images acquired on patients with glioma. Methods are evaluated using simulations and patient data. After denoising, an increase in SNR is observed. 
    SNR maps for area-under-the-curve (AUC) lactate images (obtained by summing images over all 20 time points) after applying kPL error mask. Both denoising methods (c, d) recover more voxels than the artificially noise-added data (b) and are comparable to the originally acquired data (a). The GLHOSVD-denoised SNR map better agrees with the originally acquired data.
    Representative slices of (a) acquired, (b) noise-added lactate signal. (c) and (d) show the denoised images after applying TD and GLHOSVD to the noise-added images from (b).
  • A Bayesian Approach for T2* Mapping with Built-in Parameter Estimation
    Shuai Huang1, James J. Lah1, Jason W. Allen1, and Deqiang Qiu1
    1Emory University, Atlanta, GA, United States
    T2* mapping is performed from undersampled measurements using a Bayesian approach where the parameters are automatically and adaptively estimated. It is more efficient and outperforms state-of-the-art regularization-based approaches, especially in the low-sampling-rate regime.
    Figure 1: The factor graph of the proposed nonlinear AMP framework for T2* mapping, the circle represents the variable node, and the black square represents the factor node.
    Figure 3: Sampling rate = 10%. The recovered T2* map, proton density and their corresponding relative error images using different approaches.
  • Denoising Induced Iterative Reconstruction for Fast $$$T_{1\rho}$$$ Parameter Mapping
    Qingyong Zhu1, Yuanyuan Liu2, Zhuo-Xu Cui1, Ziwen Ke1, and Dong Liang1,2
    1Research Center for Medical AI, SIAT, Chinese Academy of Sciences, Shenzhen, China, 2Paul C. Lauterbur Research Center for Biomedical Imaging, SIAT, Chinese Academy of Sciences, Shenzhen, China
    A novel iterative denoising-reconstruction scheme is proposed and can help effectively accelearte $$$T_{1\rho}$$$ parameter mapping with high quality.
    Figure 2. The parameter maps obtained all methods with SR=16.47$$$\%$$$, 25.00$$$\%$$$ and 33.15$$$\%$$$.
    Figure 1. The reconstruction results of all comparison methods at TSL=1ms and TSL= 80ms with SR= 25.00$$$\%$$$.
  • Discrimination of tumor texture based on MRI radiomic features: is there a volume threshold? A phantom study.
    Linda Bianchini1, João Santinha2,3, Francesca Botta4, Daniela Origgi4, Marta Cremonesi4, and Alessandro Lascialfari1
    1University of Pavia, Pavia, Italy, 2Champalimaud Center for the Unknown, Lisbon, Portugal, 3Instituto Superior Técnico, Lisbon, Portugal, 4European Institute of Oncology IRCCS, Milan, Italy
    A study on T2-weighted MR images of a radiomic phantom mimicking pelvic tumors shows that the texture discriminative power of radiomic features depends on tumor volume, with most features losing this property below 1 cm3 at 1.5 T.
    Figure 2. Discrimination of textures 1 and 2 on scanner A. The plot shows the number of times a feature is able to discriminate texture 1 and 2 if extracted from original and filtered images acquired on scanner A, as a function on the VOI size. Due to the selection of features with ICC>0.9, not all the features were extracted from all the available image types (10 in total: original + 9 filtered images), so the maximum count a feature could reach is indicated next to the feature name on y axis.
    Figure 1. Identified VOIs and textures. Three phantom inserts were chosen as representative of three textures, from a finer texture (1) to a coarser one (3), through a medium texture (2). The volumes of the selected VOIs were: 29.8 cm3 (red), 20.7 cm3 (green), 13.3 cm3 (blue), 7.4 cm3 (yellow), 3.3 cm3 (pink), and 0.8 cm3 (cyan).
  • Fitting kinetic rate constants in metabolite-specific bSSFP hyperpolarized [1-13C]pyruvate MRI
    Sule Sahin1,2, Shuyu Tang3, Manushka Vaidya2, and Peder E.Z. Larson2
    1Graduate Program in Bioengineering, University of California, Berkeley and University of California, San Francisco, Berkeley, CA, United States, 2Radiology, University of California, San Francisco, San Francisco, CA, United States, 3HeartVista, Inc., Los Altos, CA, United States
    A model was developed for hyperpolarized [1-13C]pyruvate studies where lactate was acquired with a bSSFP sequence. This model was shown to fit in vivo data of these bSSFP acquisitions better than using a GRE fitting method. 
    Figure 1: Flow chart describing the “lactate-bSSFP” and “GRE-all” experiments. The novelty in this work is the bSSFP rate constant fitting (green square).
    Figure 4: For all three types of in vivo data, an example of a lactate image acquired in the “lactate-bSSFP” experiment and the corresponding localizers. The kidney ROI for healthy rats and the tumor ROI for mouse prostate and human studies are outlined in blue. The signal from the ROI was averaged to get the time courses. The plots show “GRE-all” time courses fit using the GRE fitting and the “lactate-bSSFP” experiment time courses fit with the bSSFP fitting.
  • Time dependence of flow compensated intravoxel incoherent motion in tumor
    Oscar Jalnefjord1,2, Louise Rosenqvist1, Mikael Montelius1, Lukas Lundholm1, Eva Forssell-Aronsson1,2, and Maria Ljungberg1,2
    1Department of Radiation Physics, University of Gothenburg, Gothenburg, Sweden, 2Department of Medical Physics and Biomedical Engineering, Sahlgrenska University Hospital, Gothenburg, Sweden
    The results of this study show an encoding-time dependence of IVIM parameters in tumor when using a combination of flow-compensated and non-flow-compensated diffusions-encoding.
    Figure 1. Pulse sequence used to produce flow-compensated (dashed line) and non-flow-compensated (solid line) diffusion encoding. The delays marked in red and blue were increased/decreased to vary the encoding time (T). The sum of the red and blue delays was kept constant to achieve a fixed echo time
    Figure 4. Signal vs. b-value for different encoding times. The signal was averaged over voxels where assuming the ballistic regime provided a better fit to data than assuming the diffusive regime, using data from the shortest encoding time (T = 25 ms). The rationale behind this is that only these voxels were assumed to possibly show an encoding-time dependence, given that other voxels already were in the diffusive regime
  • Comparison of compartmental models of diffusion MRI for assessing myocardial microstructure
    Mohsen Farzi1, Irvin Teh1, Darryl McClymont2, Hannah Whittington2, Craig A. Lygate2, and Jürgen E. Schneider1
    1Cardiovascular & Metabolic Medicine, University of Leeds, Leeds, United Kingdom, 2Cardiovascular Medicine, University of Oxford, Oxford, United Kingdom
    We propose a novel two-compartment model of diffusion to quantify cardiomyocyte radius, volume fraction, and dispersion. The intra- and extra-cellular space were modelled using a cylinder with Bingham distributed axes and an oblate tensor.

    Figure 1. Intracellular and extracellular compartment models.

    Table 1. Mean [STD] of Biophysical Parameters on a Slab from the Left Ventricle Wall. The 𝜶2 and 𝜶3 are the dispersion about the primary eigenvector in the sheetlet plane and sheetlet-normal plane. Reported physiological range from literature for intracellular, extracellular and vessels volume fractions are 65.0±3.6, 31.2±5.8, and 7.7±2.2 percent 8. Myocyte radii along the short and long axes are 6.0±0.7 and 15.3±1.0 𝜇m 7. Assuming a circular cross-section, the radius is 9.5±0.5 𝜇m 7.
  • Time Dependency of the Continuous-Time Random-Walk Diffusion Model at Long Diffusion Times in the Human Brain
    Guangyu Dan1,2, Yuxin Zhang3,4, Zheng Zhong1,2, Kaibao Sun1, Muge Karaman1,2, Diego Hernando3,4, and Xiaohong Joe Zhou1,2,5
    1Center for MR Research, University of Illinois at Chicago, Chicago, IL, United States, 2Department of Bioengineering, University of Illinois at Chicago, Chicago, IL, United States, 3Department of Medical Physics, University of Wisconsin-Madison, Madison, WI, United States, 4Department of Radiology, School of Medicine and Public Health, University of Wisconsin-Madison, Madison, WI, United States, 5Departments of Radiology and Neurosurgery, University of Illinois at Chicago, Chicago, IL, United States
    We have shown that parameters of a continuous-time random-walk diffusion model are highly dependent on diffusion time in the human brain tissue at long time regime.
    Figure 2. Diffusion parameter maps based on D, αQDI, αT-FROC, and τ at different TM values in row a), b), c), and d), respectively.
    Figure 1. A diffusion phase diagram with respect to temporal fractional derivative α, and spatial fractional derivative β. Two special cases (β = 2, and 2α = β) in this study were marked with dash lines. Note that the circled point corresponds to Gaussian diffusion.
  • A kinetic model to quantify 2-hydroxyglutarate when using hyperpolarized [1-13C]α-ketoglutarate to detect mutant IDH1 in low grade gliomas
    Manushka V. Vaidya1, Donghyun Hong1, Sule Sahin1, Georgios Batsios1, Pavithra Viswanath1, Sabrina M. Ronen1, and Peder E.Z. Larson1
    1Department of Radiology, University of California San Francisco, San Francisco, CA, United States
    For hyperpolarized studies using C1aKG, 2HG was detected separately from natural abundance peak of C5aKG using a kinetic modeling framework. The computed metabolic conversion rates of C1aKG to either 2HG or glutamate could be used to monitor treatment response for low grade gliomas.
    Figure 1: Three-site model used in the kinetic model. The model considers unidirectional conversion of hyperpolarized substrate [1-13C]aKG to either [1-13C] 2HG or [1-13C] glutamate.
    Figure 3: Fits for dataset 1 using the overlapped fitting method. Experimentally measured substrate (A), measured product signal (B), and computed fits (C, D) are shown. For the cell lysate data, separate 2HG measurement (B) was possible. A larger amount of 2HG was detected when C5aKG+2HG was used as input (C) than the case when C5aKG alone (D) was inputted in the model. Fits for C5aKG (red) and 2HG (yellow) are derived for the best summed fit (purple) w.r.t the measured input signal (blue).
  • A direct link between the DKI model and the sub-diffusion process
    Qianqian Yang1 and Viktor Vegh2,3
    1Queensland University of Technology, Brisbane, Australia, 2The University of Queensland, Brisbane, Australia, 3Centre for Innovation in Biomedical Imaging Technology, Brisbane, Australia
    We derived a direct mathematical link between DKI and anomalous sub-diffusion models and provided a new alternative and explicit way to compute kurtosis, leading to superior grey-white matter contrast compared to traditional DKI metric. 
    Figure 3. Comparison of diffusivity and kurtosis estimated from (a) the sub-diffusion and (b) DKI models. Top row: axial view; bottom row: mid-sagittal view. $$$D^*$$$ and $$$K^*$$$ have been computed based on sub-diffusion model parameters $$$D_{SUB}$$$ and $$$\beta$$$; $$$D_{DKI}$$$ and $$$K_{DKI}$$$ have been estimated by fitting the standard DKI model to the data.
    Figure 2. Link between sub-diffusion and DKI models: (a) plot of the natural logarithm of the sub-diffusion model and its approximations. Mono-exponential (MONO) and DKI are the first- and second-order approximations of the sub-diffusion model, respectively; (b) relationship between kurtosis $$$K^*$$$ and $$$\beta$$$; (c) relationship between the ratio $$$D^*/D_{SUB}$$$ and $$$\beta$$$. $$$D^*$$$ and $$$K^*$$$ are the diffusivity and kurtosis computed from sub-diffusion model parameters $$$D_{SUB}$$$ and $$$\beta$$$.
  • Elaborating and Testing Activity MRI [aMRI] Diffusion Modeling
    Brendan Moloney1, Xin Li1, Eric M. Baker1, and Charles S. Springer1
    1Advanced Imaging Research Center, Oregon Health & Science University, Portland, OR, United States
    Activity MRI [aMRI] simulates diffusion-weighted data with three metabolic and cytometric tissue properties: kio (s-1), the mean steady-state cellular water efflux rate constant [measuring cellular metabolic activity], r, the cell density (cells/μL), and V (pL), the average cell volume.

    Figure 3. The light gray curves comprise samples of an aMRI library of >4000 simulated SDE b-space decays. Experimental data from murine colorectal tumor (circles),7 human prostate lesion (stars) and NA tissue (triangles), brain GM (diamonds), and bladder (squares) single voxels are shown. Different aMRI model kio, r, and V parameter sets produce the colored library simulated curves matching the disparate data. More importantly, the model parameters for each curve are in generally good agreement with measures from independent ex vivo studies of these tissues (Figure 4).


    Figure 1. Simulated SDE decay curves showing the dependence on each of the aMRI parameters: the mean cellular water efflux rate constant kio (a), the cell density r (b), and the mean cell volume V (c), while the other two are held constant. Thus, for (a) r = 1,200,000 cells/μL, V = 0.54 pL, for (b) kio = 39 s-1, V = 0.54 pL, and for (c) kio = 39 s-1, r = 1,200,000 cells/μL. In these semi-log plots, all decays are curved [non‑Gaussian] except those for pure water: r = 0 in (b), and V = 0 in (c).
  • The effect of inversion time on a two-compartment SMT and NODDI: an in vivo study
    Dominika Ciupek1, Maryam Afzali2, Fabian Bogusz1, Marco Pizzolato3,4, Derek K. Jones2, and Tomasz Pięciak1,5
    1AGH University of Science and Technology, Kraków, Poland, 2Cardiff University Brain Research Imaging Centre (CUBRIC), School of Psychology, Cardiff University, Cardiff, United Kingdom, 3Department of Applied Mathematics and Computer Science, Technical University of Denmark, Kongens Lyngby, Denmark, 4Signal Processing Lab (LTS5), École polytechnique fédérale de Lausanne (EPFL), Lausanne, Switzerland, 5LPI, ETSI Telecomunicación, Universidad de Valladolid, Valladolid, Spain
    Most of the metrics of biophysical models are very sensitive to changes in TI values, therefore they can be used to analyse the brain microstructure only for high TIs.
    Figure 1: Visual representation of SMT (intracellular volume fraction $$$v_{in}$$$ and intrinsic diffusivity $$$\lambda \ [\mathrm{mm}^2/\mathrm{s}]$$$) and NODDI (orientation dispersion index $$$OD$$$, intracellular volume fraction $$$v_{ic}$$$ and isotropic volume fraction $$$v_{iso}$$$) parameters under different inversion times.

    Figure 2: Mean values and first and third quartiles for SMT (intracellular volume fraction $$$v_{in}$$$ and intrinsic diffusivity $$$\lambda \ [\mathrm{mm}^2/\mathrm{s}]$$$) and NODDI (mean orientation of Watson distribution $$$\mu = (\theta, \phi) \ [\mathrm{rad}]$$$, orientation dispersion index $$$OD$$$, intracellular volume fraction $$$v_{ic}$$$ and isotropic volume fraction $$$v_{iso}$$$) over regions-of-interests and changes in TI. WM - white matter, GM - grey matter, CSF - cerebrospinal fluid.

  • Implications of a constant tissue-trace constraint on the two-compartment free water model
    Jordan A. Chad1,2, Ofer Pasternak3, and J. Jean Chen1,2
    1Department of Medical Biophysics, University of Toronto, Toronto, ON, Canada, 2Rotman Research Institute, Baycrest Health Sciences, Toronto, ON, Canada, 3Brigham and Women's Hospital, Harvard Medical School, Boston, MA, United States
    A constant tissue-trace constraint on the two-compartment free-water model allots all variation in isotropic diffusivity to the free water compartment, which is found to be more linearly aligned with quadratic variations in diffusivity.
    Figure 1. Reproduction of the “tissue compartment” results of a single-shell free-water study of aging white matter, simulated using the constant tissue-trace constraint. Metrics derived from the tissue compartment, as per Eq. 6, represent variation in the shape of the tissue tensor while the size remains constant, since all isotropic variations are allotted to the free water compartment. For a biological interpretation of these results, see ref. 6.
    Figure 2. Reproduction of the “free water compartment” results of a single-shell free-water study of aging white matter, simulated using the constant tissue-trace constraint. The constant tissue-trace relationship between f and MD (Eq. 3) is nonlinear, so the linear correlation coefficients exhibited by f and MD differ. If MD better follows a quadratic distribution, as is thought to be the case in aging, f follows a distribution that can be better approximated by a line.
  • Towards an Unbiased Brain Template of Fiber Orientation Distribution Using Multimodal Registration
    Jinglei Lv1, Rui Zeng1, and Fernando Calamante1
    1School of Biomedical Engineering, The University of Sydney, Sydney, Australia
    We propose a multimodal registration method to generate an unbiased template of fiber orientation distribution, which significantly improves the spatial specificity of near-cortex white matter and subcortex with low registration error.
    Fig.1. Method and Experiment design. (A)-(C) illustrates the multimodal registration and template generation. The transformation generated with multimodal images is applied to the FOD data, which are then averaged to generate each FOD template. (D) illustrates the population FOD template generation based on single modality FOD-based registration.
    Fig.2 FOD templates generated from 50 HCP subjects with 4 methods shown in Fig.1. The FOD butterfly patterns (overlaid on the L0 term of the FOD expansion, which corresponds to the total apparent fiber density). The white boxes highlight the FODs with crossing-fibers and near-cortex white matter.
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Digital Poster Session - Modelling Signals Throughout the Body
Acq/Recon/Analysis
Wednesday, 19 May 2021 15:00 - 16:00
  • Mechanism and quantitative assessment of saturation transfer for water-based detection of the aliphatic protons in carbohydrate polymers
    Yang Zhou1, Peter van Zijl2,3, Jiadi Xu2,3, and Nirbhay N. Yadav2,3
    1Institute of Biomedical and Health Engineering, Shenzhen Institutes of Advanced Technology, Shenzhen, China, 2The Russell H. Morgan Department of Radiology, The Johns Hopkins University School of Medicine, Baltimore, MD, United States, 3F.M. Kirby Research Center for Functional Brain Imaging, Kennedy Krieger Institute, Baltimore, MD, United States
    The analytical solution for rNOE based magnetization transfer in CEST experiments is derived and then successfully validated for polycarbohydrates through both numerical simulations and experimental data from glycogen in different solvents and as a function of pH. 
    Figure 1. The pH dependence of NMR and Z-spectral intensities for oyster glycogen (100 mM glucose units) in 95% D2O/5% H2O. (a) 1D NMR spectra at different pH. (b) Z-spectra at three pH values (4s continuous RF irradiation, B1 = 0.4 µT). (c) Lorentzian fitted peak intensities (S/S0) at +1.2, +0.6 and -1.0 ppm as a function of pH. (d) GlycoNOE (-1 ppm) intensity as a function of B1 (16s continuous RF) at two pH values. The curve was fitted using Eq. 1.
    Figure 2. Numerical simulations agree with the analytical results. (a, d) Numerically simulated Z-spectra for different hydroxyl exchange rates. (b, d) The dependence of the numerically simulated glycoNOE (black circles) intensities on B1 field strengthis in agreement with that using the analytical solution (red line, using Eq. 1). (c, f) Values for the enhancement factor (e) for numerically and analytically simulated data are the same.
  • Improving the Bloch Fitting Method for the Analysis of acidoCEST MRI
    Tianzhe Li1, Aikaterini Kotrotsou1, Shu Zhang1, Kyle Jones1, and Mark Pagel1
    1Cancer Systems Imaging, UT MD Anderson Cancer Center, Houston, TX, United States
    Our Bloch-fitting algorithm can quantify the changes of kex of iopamidol amide protons with sample pH levels and temperatures. We have confirmed that including experimentally measured information can increase the accuracy of the fitting results.
    Figure 3. Bloch fitted kex with different fitting conditions for the 5.6 ppm amide proton in 25 mM iopamidol solutions with different T1 values. The analyzed spectra were acquired at 37 °C with a saturation power of 3.0 μT and a saturation time of 6.0 sec.
    Figure 4. The computation time for the Bloch-fitting process with different fitting conditions. For each fitting condition, the computation time presented includes data for the fitting of the spectra of twenty-four 25 mM iopamidol samples scanned at five temperatures (i.e. 120 spectra per fitting condition).
  • Time resynchronization of data obtained during cardiovascular MRI combined with catheterization using biophysical cardiac modeling
    Maria Gusseva1,2, Daniel Alexander Castellanos3, Mohamed Abdelghafar Hussein4,5, Joshua Greer 4, Gerald Greil4, Surendranath Veeram Reddy4, Dominique Chapelle1,2, Tarique Hussain4, and Radomir Chabiniok1,2,4,6
    1Inria, Palaiseau, France, 2LMS, Ecole Polytechnique, Palaiseau, France, 3Department of Cardiology, Boston Children’s Hospital, Boston, MA, United States, 4Division of Pediatric Cardiology, UT Southwestern Medical Center Dallas, Dallas, TX, United States, 5Pediatric department, Kafrelsheikh University, Kafr Elsheikh, Egypt, 6Department of Mathematics, Czech Technical University in Prague, Faculty of Nuclear Sciences and Physical Engineering, Prague, Czech Republic
    Patient-specific biophysical heart modeling was employed to resynchronize the intraventricular pressure and volume data acquired during combined cardiovascular MRI and catheterization procedure. Such model-filtered P-V loops allowed better clinical interpretation of iCMR exam.
    Figure 1: Left: Single-heart cavity model coupled with the circulation system via system of diodes and a two-stage Windkessel. Right: Example of acquired and processed CMR and pressure data of LV rTOF patient #1.
  • Realistic diffusion tensor cardiovascular magnetic resonance simulations in a histology-based substrate: The effect of membrane permeability
    Jan N Rose1, Ignasi Alemany1, Andrew D Scott2,3, and Denis J Doorly1
    1Department of Aeronautics, Imperial College London, London, United Kingdom, 2Cardiovascular Magnetic Resonance unit, Royal Brompton Hospital, London, United Kingdom, 3National Heart and Lung Institute, Imperial College London, London, United Kingdom
    We extend our existing, histology-based Monte Carlo random walk simulations of DT-CMR with a model for permeable cell membranes. Results show that values of FA move closer towards in-vivo expectations when considering permeability.
    2D illustration of the virtual histology-based geometry used in the simulations. Myocytes are triangular meshes (polyhedra). The extra-cellular volume fraction is 22%.
    FA and MD values for two extreme permeability cases ($$$\kappa$$$=0 and 0.05μm/ms). All simulations have been computed considering a STEAM sequence with increasing $$$\Delta$$$ and constant gradient strength and duration. Parameters: $$$N_p$$$=104 walkers, $$$D_\text{ICS}$$$=1.5µm2/ms and $$$D_\text{ECS}$$$=3µm2/ms.
  • Packing hierarchical structures in myocardial tissue to synthesise a realistic substrate
    Jan N Rose1, Andrew D Scott2,3, and Denis J Doorly1
    1Department of Aeronautics, Imperial College London, London, United Kingdom, 2Cardiovascular Magnetic Resonance unit, Royal Brompton Hospital, London, United Kingdom, 3National Heart and Lung Institute, Imperial College London, London, United Kingdom
    We have developed an algorithm to pack cardiomyocytes of arbitrary polygonal shape into groups also of arbitrary shape, known as sheetlets, found in the myocardium. Using the method, we synthesise an imaging voxel replicating histological specimen geometric properties.
    (Top) Sheetlet segmented from histological images. (Bottom) Synthesised sheetlet after completion of the packing algorithm and after removing ghost cells, which leave distinct pockets of ECS between myocytes. The sheetlet outline was used as the target region and myocytes were created to match cell geometries from histology.
    Illustration of the presented packing algorithm. Bounding circles are used to quickly reject objects from intersection computation. Objects in grey are the buffer zone and "ghost cells", which will be removed at the end of the simulation, leaving the myocyte objects.
  • Neurovascular coupling in the cerebellum: reconstructing the neurophysiological basis of different cerebellar fMRI responses.
    Anita Monteverdi1,2, Giuseppe Gagliano2, Stefano Casali2, Fulvia Palesi1,2, Claudia AM Gandini Wheeler-Kingshott 1,2,3, Lisa Mapelli2, and Egidio D'Angelo1,2
    1Brain Connectivity Center Research Department, IRCCS Mondino Foundation, Pavia, Italy, 2Brain and Behavioral Sciences, University of Pavia, Pavia, Italy, 3Queen Square MS Centre, Department of Neuroinflammation, UCL Queen Square Institute of Neurology, Faculty of Brain Sciences, University College London, London, United Kingdom
    Our results show for the first time the region-specificity and frequency-dependency of the neurovascular coupling in the cerebellar cortex, combining vascular time-lapse bright-field imaging, electrophysiological investigations ex vivo, and computational models of neuronal activity. 
    Fig.1| Cerebellar vermis and hemisphere showed different fMRI signals in humans in vivo1,2. In order to explore the neurophysiological basis of such difference we characterized capillary responses ex-vivo in vermis lobule V and hemisphere lobule VI in acute mouse cerebellar slices (left: vascular organization of these regions) and recorded neuronal activity with an HD-MEA (right: LFP signals recorded from the granular layer). Then, we validated a biophysical realistic model with the electrophysiological data and used it to dissect the neuronal contribution to the NVC.
    Fig. 2| Capillary dilation differed between cerebellar vermis and hemisphere in response to mossy fibers stimulation, and vascular responses did not show linear trends while increasing the input frequency. Granular layer neuronal responses recorded as Local Field Potentials (N2a-N2b peaks) differed in cerebellar vermis and hemisphere, and the N2b peak presented a non-linear frequency dependent trend. Importantly N2b peak is informative of N-methyl-D-aspartate receptors (NMDA) activation and the NMDAR-NO pathway is known to regulate cerebellar neurovascular coupling3.
  • Simulations of the BOLD Non-Linearity Based on a Viscoelastic Model for Capillary and Vein Compliance
    Joerg Peter Pfannmoeller1, Grant Addison Hartung1, Xiaojun Cheng2, Avery Berman1, David Boas2, and Jonathan Rizzo Polimeni1
    1Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States, 2Neurophotonics Center, Boston University, Boston, MA, United States
    We extended an existing framework of BOLD modeling based on biophysical simulations to incorporate viscoelastic properties of individual blood vessels and tissue, and use it to examine BOLD response nonlinearities to short-duration stimuli.
    Fig.1 Realistic VAN model of mouse cortex. (A) Anatomical reconstruction of full vascular network (600 micron cube). Arteries (red), capillaries (green), veins (blue). The inputs and outputs to the network are indicated in magenta. The boundary conditions must be computed to emulate the behavior within the VAN as if it were connected to large feeding arteries and draining veins as it is in the brain. (B) The distribution of Young’s elasticity modulus indicating the characteristic difference between pial veins and the intra cortical diving veins and capillaries (logarithmic scale).
    Fig.2 Determination of boundary conditions using a whole-brain stylistic VAN. (A) Vascular network for mouse brain (diving artery:vein ratio 1:3; arteries red, capillaries green, veins blue). Cyan indicates the path used for analysis, the area representing the realistic VAN is shaded, magenta dots show the VAN boundary nodes. (B) Pressure and (C) blood volume along the path in (A) for baseline and active conditions for short and long-duration stimuli. Magenta lines indicate the boundary nodes in (A). (D) Pressure increases at the boundary nodes for different stimulus durations.
  • Established a rat model of discogenic low back pain for evaluating the paravertebral muscle functional magnetic resonance changes
    Luo Bao fa1, Huang Yi long1, Yang Kai wen1, Nie Li sha2, and He Bo1
    1The First Affiliated Hospital of Kunming Medical University, kunming, China, 2GE Healthcare, MR Research China, Beijing, Beijing, China
     It is feasible to construct DLBP rat model by X-ray guided puncture of intervertebral disc, and the T2 value changes earlier than R2*in the early stage of DLBP.
    Figure.2 Behavioral assay,1,7,14 and 30 days after operation. ( A ) Gait disturbance score: There was no significant difference among the three groups;(B and C) Hot-Plate and acetone assay: Compared with the normal group and sham group, the DLBP group showed a decreased in pain and temperature threshold; (D,E and F) Grip force and tail suspension assay: The DLBP group showed reduced grip and struggle time and increased bending time due to axial pain in the waist and back (#P < 0.05).
    Figure.4 MRI T2 mapping (A and B) and BOLD (C and D),1 month after operation. Compared with the normal group and sham group, the T2 values of the L4/5 and L5/6 multifidus and erector spinae in the DLBP group were increased. There was no significant difference in R2*values of multifidus , erector spinae and psoas major among the three groups (#P < 0.05) .
  • Modelling Depth-Dependent VASO and BOLD Signal Changes in Human Primary Motor Cortex
    Atena Akbari1, Saskia Bollmann1, and Markus Barth1,2,3
    1Centre for Advanced Imaging, The University of Queensland, Brisbane, Australia, 2School of Information Technology and Electrical Engineering, Brisbane, Australia, 3ARC Training Centre for Innovation in Biomedical Imaging Technology, Brisbane, Australia
    Using a cortical vascular model, we simulated the depth-dependent BOLD and VASO signal change in human primary motor cortex. 
    Figure 2. The first row shows the pattern of the CBV change across the layers used in our simulation. Rows 2 to 5 show the BOLD and VASO simulated profiles. Profiles with RMSE 20% higher than the minimum RMSE are plotted as the shaded area. In all figures the horizontal axes show the relative cortical depth, vertical axes show the percentage of signal change, solid lines represent imaging data, dotted lines represent simulated responses, and error bars show the standard error of the mean.
    Figure 1. A) Schematic representation of the modelled primary motor cortex centred on two adjacent principal veins of groups 3 and 4 (V3, V4) with artery to vein ratio of 2-1. B) Baseline blood volume in intracortical vessels and the laminar network (i.e. arterioles, capillaries, and venules) in the modelled area.
  • A Comparison on the Estimated Stiffness and Signal-to-Noise Ratio of Magnetic Resonance Elastography Images Acquired at 3T and 7T
    Yuan Le1, Andrew J. Fagan1, Jun Chen1, Eric G. Stinson2, Joel P. Felmlee1, Matthew C. Murphy1, Kevin J. Glaser1, Arvin Arani1, Phillip J. Rossman1, Stephan Kannengiesser3, Bradley D. Bolster, Jr.2, John Huston, III1, and Richard L. Ehman1
    1Radiology, Mayo Clinic, Rochester, MN, United States, 2Siemens Medical Solutions USA, Inc., Malvern, PA, United States, 3Siemens Healthcare GmbH, Erlangen, Germany
    By comparing the MRE images acquired using a PVC phantom at 7T vs. 3T, we found that the signal-to-noise ratio and the octahedral shear strain based SNR were much higher, or close to double, at 7T compared with 3T. The stiffness values were very close between the two field strengths.
    Figure 3. Wave images, curl maps and stiffness maps at 7T and 3T.
    Figure 1. PVC head phantom and the setup of the MRE test.
  • Towards direct neuronal-current MRI: a novel statistical processing technique for measurements in the presence of system imperfections.
    Chiara Coletti1, Sebastian Domsch1, Frans Vos1, and Sebastian Weingärtner1
    1Imaging Physics, TU Delft, Delft, Netherlands
    • - Direct neuro-current MRI shows high susceptibility to B0 and B1+ inhomogeneities.
    • - The proposed data-processing for neuro-current MRI time series, achieves higher sensitivity and is less susceptible to system imperfections than previous approaches.
    Representative activation maps for the two processing methods, NEMO and SVarM, for different levels of B0 and B1+ inhomogeneities. On the right, corresponding plots of Dice score and surviving pixels ration (mean ± std). On the top, ground truth activation map, obtained from BOLD fMRI experiments, and representative B0 and B1+ field maps.
    Simulated neuro-current time series with (a) or without (b) concomitant neural activation. Time courses (mean ± std) after each step of data processing. NEMO consists of a regression and high-pass filtering step to remove low frequency confounds (d), a rectification step converting variance differences in mean shifts (e) and extraction of the peak magnitude in the frequency spectrum at the task frequency (f). SVarM uses GLM regression to remove low frequency confounds (h), then pools the data into ON and OFF groups and tests the difference in their variance with Levene’s test (i-j).
  • UNIform COmbined RecoNstruction (UNICORN) for 7T Clinical Fat-Suppressed TSE Imaging of the Human Knee
    Xiaowei Zou1, Venkata V Chebrolu2, and Nakul Gupta3
    1Siemens Medical Solutions USA Inc., Houston, TX, United States, 2Siemens Medical Solutions USA Inc., Rochester, MN, United States, 3Department of Radiology, Houston Methodist Research Institute, Houston, TX, United States
    UNICORN is a promising method to improve uniformity and contrast of 7T clinical fat-suppressed TSE images of the human knee.
    Figure 2: Exemplary images of the original and UNICORN+B1 images of RRx1 to RRx8 of (A) FA = 126o and (B) FA = 163o. Each image was automatically windowed individually.
    Figure 1: Quantitative ROI analysis and qualitative clinical evaluation for the eight different UNICORN settings RRx1 to RRx8 of FA = 126o (top) and FA = 163o (bottom). Each setting reconstructed three image series: original without UNICORN and B1 filtering (original, red), UNICORN without B1 filtering (UNICORN, green), and UNICORN with B1 filtering (UNICORN+B1, blue).
  • Correcting Signal Intensity Bias in 19F MR Imaging of Inflammation by Statistical Modelling
    Ludger Starke1, Thoralf Niendorf1, and Sonia Waiczies1
    1Berlin Ultrahigh Field Facility (B.U.F.F.), Max Delbrück Center for Molecular Medicine in the Helmholtz Association, Berlin, Germany
    Labeling cells with 19F NPs enables localization of inflammation and monitoring of cell therapy. Systematic overestimation of signal intensities has been observed. We propose a statistical model which successfully removes this bias and improves the reliability of quantitative 19F MRI.
    Example in vivo dataset. Estimation bias including moving average for individual voxels (A) and averaged over signal features (B). The area of markers is proportional to the number of voxels in the feature. (C) Example slice from the same 3D dataset. 19F-NPs are taken up by inflammatory cells, which then accumulate at sites of inflammation. The first row shows 19F-MR signal intensity for test data after RNBC (measured) and with model based bias correction (corrected), as well as the reference data. The second line shows estimation bias computed by comparison of test and reference data.
    (A) Rician noise with known noise level is used for the forward model. (B) The true signal intensities are assumed to be drawn from a positively skewed probability distribution. Here a log-normal prior is shown. The measured data is thus drawn from a marginal distribution computed by integrating the product of forward model and prior distribution. The right shift of probability mass for signal levels above the detection threshold leads to the observed overestimation. (C) Posterior distributions for two measured signal levels. The posterior mean gives the corrected signal
  • Automated 3D modeling and analysis of cerebral small vessels with MR angiography at 7 Tesla
    Zhixin Li1,2,3, Yue Wu1,2,3, Dongbiao Sun1,2,3, Jing An4, Qingle Kong5, Rong Xue1,2,3, Yan Zhuo1,2,3, and Zihao Zhang1,2,3
    1State Key Laboratory of Brain and Cognitive Science, Institute of Biophysics, Chinese Academy of Sciences, Beijing, China, 2The Innovation Center of Excellence on Brain Science, Chinese Academy of Sciences, Beijing, China, 3University of Chinese Academy of Sciences, Beijing, China, 4Siemens Shenzhen Magnetic Resonance Ltd., Shenzhen, China, 5MR Collaboration, Siemens Healthcare Ltd, Beijing, China
    A comprehensive framework was proposed to overcome the challenges in the automated modeling of 3D cerebral small vessels with 7T TOF-MRA. The vasculature and quantification of LSA were obtained in an automated way, which facilitate related radiological studies in the future.
    Figure 1. The 3D vasculature from 7T TOF-MRA obtained by our progressive method.
    Figure 2. Comparison between the segmentation results of our method and U-NET. (a) Origin image. (b) Ground truth. (c) Result of U-NET. (d) Result of our method.
  • Impact of ASL modelling strategies on cerebral blood flow and reactivity assessment
    Joana Pinto1, Nicholas P. Blockley2, James W. Harkin3, and Daniel P. Bulte1
    1Institute of Biomedical Engineering, Department of Engineering Science, University of Oxford, Oxford, United Kingdom, 2School of Life Sciences, University of Nottingham, Nottingham, United Kingdom, 3Respiratory Medicine Department, School of Medicine, University of Nottingham, Nottingham, United Kingdom
    Our results highlight the importance of multiple-PLD ASL strategies for accurate CBF and CVR quantification. Furthermore, when using this strategy, the modelling options used significantly impact CBF quantification, regardless of the condition studied. 
    Figure 1. Orthogonal representations of CBF, BAT, and aCBV maps of one subject for the different modelling strategies and conditions (air and hypercapnia). aCBV maps are only obtained when using strategies where the macrovascular component is modelled (Mart). MartMnodisp - model with macrovascular component but without dispersion, MartMdisp - model with macrovascular and dispersion components, MnoartMnodisp - model without macrovascular and dispersion components, MnoartMdisp - model with dispersion but without macrovascular component.
    Figure 2. Regional analysis of the different haemodynamic parameters (CBF, BAT and aBV; rows) with the different modelling strategies (colors, correspondence detailed in Figure 1 legend) and conditions (columns). Statistically significant results are highlighted with * (p>0.05, corrected for multiple comparisons).
  • Improving the predictive power of The Virtual Brain in healthy and neurodegenerative diseases with cerebro-cerebellar loops integration.
    Anita Monteverdi1,2, Fulvia Palesi1,2, Claudia AM Gandini Wheeler-Kingshott 1,2,3, and Egidio D'Angelo1,2
    1Brain Connectivity Center Research Department, IRCCS Mondino Foundation, Pavia, Italy, 2Brain and Behavioral Sciences, University of Pavia, Pavia, Italy, 3NMR Research Unit, Queen Square MS Centre, Department of Neuroinflammation, UCL Queen Square Institute of Neurology, Faculty of Brain Sciences, UCL, London, United Kingdom
    The integration of cerebro-cerebellar connections in The Virtual Brain increases its ability to predict subject-specific brain dynamics both in healthy and in pathological conditions, i.e. Alzheimer’s disease and Frontotemporal Spectrum Disorder.
    Fig.1| The Virtual Brain (TVB) simulation was performed in three different conditions: healthy (HC), Alzheimer’s disease (AD) and Frontotemporal Spectrum Disorder (FTSD). For each group a randomly chosen subject is reported as an example. Each row shows structural connectivity (SC), experimental functional connectivity (expFC) and simulated functional connectivity (simFC) obtained with three different networks: whole-brain, cortical subnetwork (CORTEX) and embedded cerebro-cerebellar subnetwork (CORTEXCRBL).
    Fig.2| Boxplot of Pearson correlation coefficient (PCC) between experimental and simulated functional connectivity for all groups (healthy, HC Alzheimer’s disease, AD Frontotemporal Spectrum Disorder, FTSD) and networks. PCC values obtained integrating cerebro-cerebellar connections (CORTEXCRBL) are higher than PCC values obtained with the other networks (WHOLEBRAIN and CORTEX) both in healthy and pathological conditions.
  • Hemodynamic simulations reveal changes in ascending venules leads to enhanced venous CBV response to arterial dilation.
    Grant Hartung1, Joerg Pfannmoeller1, Avery J. L. Berman1, and Jonathan R. Polimeni1
    1Athinoula A. Martinos Center for Biomedical Imaging, Boston, MA, United States
    We adapted realistic models of cortical microvasculature to alter the topology of the vascular network and performed dynamical simulations of blood flow and volume changes following neural activity. We find that the topology changes cause qualitatively different blood volume responses.
    Figure 1. Visualization of A) the first network and B) the other three networks both (Left Column) before and (Right Column) after the anatomical swapping of arteries and veins. Not only was the labeling swapped but the diameter spectra were also reassigned so that the newly assigned arteries have the same diameter distribution as the previous arteries and similarly the veins share the diameter spectra of the original veins. C) This topological matching is also reflected by plotting the diameter spectra of the arteries, capillaries, and veins from before and after swapping the anatomy.
    Figure 4. Visualization of the cerebral blood volume (CBV) time course for all 4 VANs. The dilation in the experimental group (3:1 ratio) is significantly higher than the control counterpart in each case.
  • Pre-processing of high-resolution gradient-echo images for laminar fMRI applications
    Patricia Pais-Roldan1, Seong Dae Yun1, and Jon N Shah1
    1Forschungszentrum Juelich, Juelich, Germany
    Sophisticated pre-processing with added voxel-wise regression of the phase signal from the pre-processed magnitude increases the accuracy of GE signals, allowing whole-brain, high-resolution GE-sequences to be exploited in the resting-state laminar fMRI field.
    Figure 2. Signal amplitude and independence in resting-state data. a) The image shows the location of nine voxels crossing the cortical ribbon (“cross-cortex line”) that were used in the successive analysis. b) Power of low-frequency fluctuations at different points of the cross-cortex line calculated for ten different pre-processing pipelines. c) Mean homogeneity, assessed as correlation and coherence between pairs of voxels in the cross-cortex-line. Error bars represent standard error of the mean. Different letters indicate significantly different groups.
    Figure 3. Identification of evoked responses. a) Line activation profiles, calculated as the mean beta-value across 20 lines (see inset on the bottom left), for two task-fMRI scans involving either motor-only (M) or motor and sensory processing induced by touch (M+T), computed after pre-processing with ten different pipelines. The dashed lines indicate the intensity of the mean functional image. b) ROIs selected for group analysis. c) The GM to CSF ratio of the t-statistic. Asterisks indicate significant differences between pre-processing pipelines (p<0.05).
  • Improved signal integrity in multi-echo fMRI through locally low-rank tensor regularization
    Nolan K Meyer1, Daehun Kang2, MyungHo In2, John Huston2, Yunhong Shu2, Matt A Bernstein2, and Joshua D Trzasko2
    1Mayo Clinic Graduate School of Biomedical Sciences, Rochester, MN, United States, 2Radiology, Mayo Clinic, Rochester, MN, United States
    Locally low-rank regularization methods are extended to denoise multi-echo resting-state functional MRI data, yielding substantial increases in temporal signal to noise ratio and robustly improved network connectivity mapping.
    Figure 1. Group mean atlased tSNR, identically viewed and windowed (rows 1-2), and masked to grey matter (rows 3-5). Control images shown in rows 1/4; LLR-denoised images, rows 2/5. For control data, global, masked, and default mode, auditory, and sensorimotor network seed mean and standard deviation tSNRs were 180.98 ± 17.19, 181.75 ± 18.40, 132.28 ± 7.29, 236.79 ± 28.67, and 246.87 ± 41.24 respectively; for LLR data, 454.10 ± 62.76, 436.63 ± 66.58, 237.83 ± 27.87, 498.25 ± 71.02, and 576.57 ± 161.65.
    Figure 5. Group-level sensorimotor network connectivity statistical map. Left column shows control data; right column, LLR-denoised data. Shown for each variant and threshold are volumes (volSC) of the seed-containing cluster (blue arrows). Clusters are thresholded in volume to 40 voxels. Top row has maps thresholded to $$$p=1\times{10}^{-3}$$$; bottom row, $$$p=2.55\times{10}^{-4}$$$ (reduction to $$$25.5\%$$$ of baseline) for LLR-denoised data to replicate volSC of control. LLR-denoised data show a $$$98.58\%$$$ increase in volSC at $$$p=1\times{10}^{-3}$$$.
  • Comparison of Region-Wise and Voxel-Wise Diffusion Signal Harmonisation via Z-scoring and ComBat
    Stefan Winzeck1,2, Maíra Siqueira Pinto3, Virginia F. J. Newcombe2, Ben Glocker1, David K. Menon2, and Marta M. Correia4
    1BioMedIA, Department of Computing, Imperial College London, London, United Kingdom, 2Division of Anaesthesia, Department of Medicine, University of Cambridge, Cambridge, United Kingdom, 3Universitair Ziekenhuis Antwerpen, Antwerp, Belgium, 4MRC Cognition and Brain Sciences Unit, University of Cambridge, Cambridge, United Kingdom
    Z-scoring and ComBat could both reduce variation in FA and MD derived from different scanning protocols. The signal harmonisations on a regional or voxel-wise level were equally successful when DWI data were processed identically.
    Figure1. Harmonisation of FA and MD on ROI-wise level via Z-scoring or ComBat was equally effective. While Z-scoring projected diffusion metrics independently (here to reference scheme 30x2), ComBat adjusted signal across all acquisition schemes.
    Table 1. Coefficient of Variation of JHU ROI Means Before and After Data Harmonisation. All CV values displayed as mean [min, max] in %.