Molecular Imaging & X-Nuclei
Cancer/Spectroscopy/Molecular Imaging/Pre-Clinical Tuesday, 18 May 2021

Oral Session - Molecular Imaging & X-Nuclei
Cancer/Spectroscopy/Molecular Imaging/Pre-Clinical
Tuesday, 18 May 2021 12:00 - 14:00
  • Deuterium Echo-Planar Spectroscopic Imaging (DEPSI) to Dynamically Monitor Deuterated Glucose in the Liver at 7T
    Kyung Min Nam1, Ayhan Gursan1, Alex Bhogal1, Jannie Wijnen1, Dennis Klomp1, Jeanine Prompers1, and Arjan D. Hendriks1
    1University of Medical Center Utrecht, Utrecht, Netherlands
    Deuterium Echo-Planar Spectroscopic Imaging (DEPSI) is proposed as a way to increase the spatial and temporal resolution of 7T deuterium metabolic imaging (DMI). The sensitivity was high enough to monitor in-vivo liver glucose metabolism with 20 mm3 resolution and a scan time of < 10min.
    Fig. 4: 3D DEPSI scans of the liver, acquired respectively two hours (A and C) and 3 hours (B and D) after intake of deuterated glucose (glucose). In the MRI-DMI overlays (A and B), the liver contours are highlighted. Selected voxels in the liver (C and D) show both the glucose peak (blue marker) and the water peak (orange marker). It can be seen that the glucose peak decreases over time. Note that the glucose signal in the stomach (A, blue marker) can also be detected and that it is much higher 2 hours after intake than 3 hours after intake (B).
    Fig. 3: 3D DEPSI datasets of the human liver at natural abundance, acquired with Hamming weighting (A) and without Hamming weighting (B). The left panels show overlays of the 1H MRI images (Dixon) and the 2H spectra. The right panel highlights 6 voxels located in the liver. The average SNR of the deuterated water signal in the ROI (white box) is 2.4 times higher for the Hamming weighted DEPSI acquisition.
  • Deuterium metabolic imaging (DMI) of glucose metabolism in pregnant preeclamptic mice at 15.2 tesla.
    Stefan Markovic1, Tangi Roussel2, Michal Neeman3, and Lucio Frydman1
    1Department of Chemical and Biological Physics, Weizmann Institute of Science, Rehovot, Israel, 2Center for Magnetic Resonance in Biology and Medicine, Marseille, France, 3Department of Biological Regulation, Weizmann Institute of Science, Rehovot, Israel
    The fate of 2H6,6’-glucose in pregnant controls and preeclamptic mice was followed by Deuterium Metabolic Imaging. Lactate was produced in placentas and fetal organs, and its levels were elevated and washed out more slowly in the case of preeclamptic pregnancies.
    DMI data collected at the indicated stages following the intravenous administration of 2H6,6’-glucose to a preeclamptic pregnant mouse. Metabolic maps of 2H6,6’-glucose (A) and its metabolic products 2H3,3’-lactate (B) and 2H-water (C) are here shown for illustration purposes. The anatomical 1H image on top of which all 2H data are shown is depicted in (D). Time traces for all metabolites (E) and a zoom into lactate traces (F) are shown for the entire time series.
    2H MRS and MRSI spectra arising after intravenous administration of 2H6,6’-glucose to pregnant preeclamptic and control mice. The columns A and C present non-localized spectra from the 2H MRS and organ-specific 2H spectra localized from the MRSI data (B, D) at similar post-injection time-points. Signals for 2H6,6’-glucose and its metabolic products water and lactate are indicated by letters G, W and L respectively.
  • Hyperpolarized [2-13C]Pyruvate Molecular Imaging with Whole Brain Coverage
    Yaewon Kim1, Brian T. Chung1, Jeremy W. Gordon1, Adam W. Autry1, Chou T. Tan2, Chris Suszczynski2, Susan M. Chang3, Yan Li1, Duan Xu1, and Daniel B. Vigneron1,3
    1Department of Radiology and Biomedical Imaging, University of California, San Francisco, CA, United States, 2ISOTEC Stable Isotope Division, MilliporeSigma, Merck KGaA, Miamisburg, OH, United States, 3Department of Neurological Surgery, University of California, San Francisco, CA, United States
    A new method for hyperpolarized [2-13C]pyruvate MRI with volumetric and dynamic EPI of the human brain with metabolite-specific in-plane resolution was developed and applied in healthy volunteers to investigate both TCA and glycolytic metabolism in the same acquisition.
    Figure 1. The 4D dynamics of hyperpolarized [2-13C]pyruvate, [5-13C]glutamate, [2-13C]lactate (downfield peak), and [2-13C]lactate (upfield peak) in the healthy human brain. The displayed images were obtained after denoising using a patch-based denoising method. The first 10 timeframes, acquired with a temporal resolution of 3 s, are displayed. The upper window level was adjusted to 20% of the maximum intensity voxel for pyruvate and to 100% for lactate and glutamate.
    Figure 3. Representative AUC images of [2-13C]pyruvate, [5-13C]glutamate, and Σ[2-13C]lactate signals summed over 20 timeframes with 1H anatomical images from a healthy brain volunteer.
  • Clinical translation of simultaneous metabolic and perfusion imaging with hyperpolarized [1-13C]pyruvate and [13C, 15N2]urea
    Hecong Qin1,2, Shuyu Tang1, Andrew Riselli1, Robert A. Bok1, Romelyn Delos Santos1, Mark Van Criekinge1, Jeremy W. Gordon1, Rahul Aggarwal3, Evelyn Escobar1, Rui Chen4, Chunxin Tracy Zhang5, Gregory Goddard5, Albert Chen4, Galen Reed4, Ruscitto M. Daniel5, Renuka Sriram1, James Slater1, Peder E.Z. Larson1,2, Daniel B. Vigneron1,2, and John Kurhanewicz1,2
    1Radiology and Biomedical Imaging, University of California, San Francisco, San Francisco, CA, United States, 2Graduate Program in Bioengineering, UC Berkeley – UCSF, San Francisco, CA, United States, 3Medicine, University of California, San Francisco, San Francisco, CA, United States, 4GE Healthcare, Waukesha, WI, United States, 5GE Research, Niskayuna, NY, United States
    We developed a formulation and standard operating procedure that can reproducibly generate sterile hyperpolarized 13C pyruvate and urea solutions for human injection, as well as a novel imaging approach for simultaneous metabolic and perfusion imaging. 
    Figure 1. Imaging mechanism: hyperpolarized 13C pyruvate and urea are intravenously injected in a single bolus, then leave the vasculature and enter exocellular space. Pyruvate can enter the cell and be metabolized into lactate, alanine, or CO2/bicarbonate, evaluating multiple metabolic fluxes, whereas urea is predominately extracellular and metabolic inactive, serving as a perfusion contrast agent. (Ktrans, vascular transfer constant; MCT, monocarboxylate transporter; LDH, lactate dehydrogenase; ALT, alanine transaminase; PDH, pyruvate dehydrogenase).
    Figure 5. A balanced steady-state free precession (bSSFP) sequence for hyperpolarized (HP) 13C urea (A, highlighted area indicates readout duration) produced superior image qualities (SNR, resolution, sharpness) than a single shot spiral gradient echo (GRE) sequence (B). (C): Representative images of sum HP 13C signal of a healthy rat overlaid on T2 weight images: flip angels of lactate, alanine, pyruvate, and urea are 30°, 30°, 8°, ± 25°; 2.5 × 2.5 × 21mm spatial resolution; 4.2s temporal resolution. (D) HP signal dynamics in the aorta and kidneys of a healthy rat.
  • High-resolution 3D Phosphorus Metabolic Imaging of the Human Brain at 7T using SPICE
    Hannes Michel Wiesner1, Rong Guo2,3, Yudu Li2,3, Yibo Zhao2,3, Zhi-Pei Liang2,3, Xiao-Hong Zhu1, and Wei Chen1
    1CMRR, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 2Beckman Institute for Advanced Science and Technology, University of Illinois at Urbana-Champaign, Urbana, IL, United States, 3Departments of Electrical and Computer Engineering, University of Illinois at Urbana-Champaign, Urbana, IL, United States
    We demonstrated the feasibility and potential of the SPICE approach for obtaining high-fidelity 3D 31P MRSI of the human brain at 7T.
    Figure 2 Representative in vivo human brain 31P CSI results from 3D dataset before (A) and after (B) using the SPICE denoising method. The data were acquired using Siemens CSI sequence with the following parameters: TR = 300 ms; TE = 0.35 ms; FOV = 220´220´200; Matrix = 24×24×12; Resolution (nominal) = 9.1×9.1×16 mm3; Average (weighted) = 10; bandwidth = 5000 Hz; vector size = 1024; scan time = 32 min. The red lines outline the brain edge and the left panels show the representative in vivo 31P spectra taken from 4 voxels within the black box as shown on the left panels.
    Figure 1 Representative phantom 31P CSI results from 3D dataset before (A) and after (B) using the SPICE denoising method and Siemens CSI sequence and parameters: TR = 200 ms; TE = 1.6 ms; FOV = 240×240×80; Matrix = 12×12×4; Resolution = 20×20×20 mm3; Average = 4; bandwidth = 5000 Hz; vector size = 800; scan time = 8 min.
  • Assessment of sensitivity, resolution, and quantification of Synomag-D labeled dendritic cells with magnetic particle imaging
    Julia J Gevaert1,2, Corby Fink3,4, Jimmy D Dikeakos3, Gregory A Dekaban3,4, and Paula J Foster1,2
    1Department of Medical Biophysics, University of Western Ontario, London, ON, Canada, 2Cellular and Molecular Imaging Group, Robarts Research Institute, London, ON, Canada, 3Department of Microbiology and Immunology, University of Western Ontario, London, ON, Canada, 4Biotherapeutics Research Laboratory, Robarts Research Institute, London, ON, Canada
    DCs labeled with Synomag-D and TAs demonstrated a cellular sensitivity of 6k cells with 1min 2D images. Vivotrax labeled DCs revealed extracellular iron and clumping of iron, which was pronounced with TAs. Signal from 250k and 25k cells could be resolved at a distance of 2cm with 3D imaging.
    Figure 4: In-vivo cellular sensitivity and resolution of DCs. 25k and 250k cells injected subcutaneously 2cm (A) and 5cm apart (F). Signal from 25k cells is hidden within the signal from 250k cells, with indistinct peaks from the corresponding signal intensity profile (B). Signals are resolved using 3D imaging (35 projections) after window leveling to the lower signal (C). MRI confirms signal voids from 25k (D) and 250k cells (E). Signal from 250k, liver/gut, and 25k is seen with 2D (G) and 3D (H) images.
    Figure 2: Cellular detection limits of DCs labeled with Vivotrax and Synomag-D with and without TAs. Images are of a single sample scanned at a time. No TAs limits detection of Synomag-D to 25k cells. 12k and 6k cell samples were not detectable (black X). With TAs, 6000 cells are visible for both Vivotrax and Synomag-D. 500k samples using TAs for labelling were not prepared (gray squares). Extracellular iron contributes to overestimation of signal with Vivotrax. More signal is detected using Vivotrax with TAs than with without TAs.
  • First in vivo detection of carnosine using CEST
    Solène Bardin1,2, Michele Lecis1,3, Davide Boido1,2, Fawzi Boumezbeur1,2, and Luisa Ciobanu1,2
    1NeuroSpin, CEA, Gif-sur-Yvette, France, 2Paris-Saclay University, Saclay, France, 3Technical University of Munich, Munich, Germany
    Accelerated CEST acquisitions using a linescan sequence coupled with an ultra-high magnetic field allows, for the first time, the detection of carnosine in vivo.
    Figure 3. (A) Anatomical image of the lower-leg muscle showing the voxels used for linescan and 1H-MRS (B) LASER spectrum (TE/TR=25/2000ms, 3*1.8*1.5mm3) and the carnosine signal fitted using LCModel (C) Low resolution Z-spectrum (D) Low (blue) and high (red) resolution Z-spectra showing Cr / PCr peaks (E) Zoom showing the Car and APT peaks from two different rats. All peaks were detected with a significance p-value < 0.001, except for the APT peak for rat 2 (p = 0.017). Full circles: rat 1, Empty circles: rat 2.
    Figure 1. The “peak finder” is an algorithm that automatically detects peaks and assesses their significance. The original data (A) are flipped for peak detection (B). A baseline is estimated for each peak using Gaussian Processes (GP) and a chi-square value χ2data is calculated (C). The code randomly generates pseudo-experiments assuming a Gaussian distribution around the baseline with a variance in accordance with the confidence interval returned by the GP (D). The fraction of simulated curves with χ2pseudo < χ2data is taken as p-value of the detected peak. The output is shown in (E).
  • Quantitative Sodium MRI of the Human Kidney at 7T Applying Respiratory Sorting
    Anna K. Scheipers1, Johanna Lott1, Armin M. Nagel1,2, Peter Bachert1, Mark E. Ladd1, and Tanja Platt1
    1Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2University Hospital Erlangen, Institute of Radiology, Friedrich‐Alexander‐Universität Erlangen‐Nürnberg (FAU), Erlangen, Germany
    Different corrections were applied to 23Na MR images of a phantom and of the human kidney and were invested regarding their influence on a reliable quantification of the sodium concentration. Motion sorted B1+ correction was shown to be feasible with the applied setup for 23Na MRI at 7T.
    Fig. 3: Quantitative 23Na concentration in the human kidney at 7T in all directions for not respiratory sorted data, inhaled and exhaled state. Slices in each direction were chosen to have the kidneys visible (transversal: 38, coronal: 53, saggital: 33, for a 80×80×80 matrix).
    Fig. 2: Phantom (a) and in-vivo (b) data in all directions. First column shows the not respiratory sorted data corrected with the unsorted B1+ map, second column shows the inhaled state data corrected with the inhale sorted B1+ map, third and fourth column show the exhaled state data corrected with the exhale sorted B1+ map and the unsorted B1+ map respectively. Slices in each direction were chosen to have the kidneys visible (transversal: 38, coronal: 53, saggital: 33, for a 80×80×80 matrix).
  • Quantitative sodium and diffusion imaging of mild traumatic brain injury: regional analysis findings
    Anna M Chen1, Teresa Gerhalter1, Seena Dehkharghani1,2, Rosemary Peralta1, Fatemeh Adlparvar1, James S Babb1, Tamara Bushnik3, Jonathan M Silver4, Brian S Im3, Stephen P Wall5, Ryan Brown1,6, Steven Baete1,6, Ivan I Kirov1,2,6, and Guillaume Madelin1
    1Center for Biomedical Imaging, Department of Radiology, New York University Grossman School of Medicine, New York, NY, United States, 2Department of Neurology, New York University Grossman School of Medicine, New York, NY, United States, 3Department of Rehabilitation Medicine, New York University Grossman School of Medicine, New York, NY, United States, 4Department of Psychiatry, New York University Grossman School of Medicine, New York, NY, United States, 5Ronald O. Perelman Department of Emergency Medicine, New York University Grossman School of Medicine, New York, NY, United States, 6Center for Advanced Imaging Innovation and Research, Department of Radiology, New York University Grossman School of Medicine, New York, NY, United States
    Mean TSC was lower in mild TBI than in controls across 12 brain regions, but only the caudate reached statistical significance. Significant FA differences only occurred in frontal WM, while none were detected for ADC. TSC changes existed in mild TBI and occurred with similar frequency as FA.
    Figure 2: Example of multimodal image segmentation and registration. A) Top: During the 1H session, apparent diffusion coefficient (ADC) and fractional anisotropy (FA) maps were obtained. Bottom: During the 23Na session, total sodium concentration maps (TSC) and low-resolution MPRAGE images for registration were acquired. B) ROIs were obtained from the high-resolution MPRAGE, then registered to the TSC using the low-resolution MPRAGE and to the diffusion maps using the diffusion-b0 image.
    Figure 3: Boxplots of TSC, ADC, and FA distributions in mTBI and control (CTL) groups. Boxplots exclude the three oldest mTBI patients who lacked age-matched controls. FWM FA and caudate TSC were lower in mTBI patients compared to controls (MW, ♦: p<0.05). Note that nine out of 12 ROIs revealed lower median TSC values in mTBI patients compared to controls. gWM: global WM; CC: corpus callosum; BCC: body of CC; GCC: genu of CC; SCC: splenium of CC; CR: corona radiata; FWM: frontal WM; PWM: posterior WM; gcGM: global cortical GM; CA: caudate; PA: pallidus; PU: putamen; TH: thalamus.
  • Optimized simultaneous 3D proton MRF and sodium MRI
    Zidan Yu1,2, Olga Dergahyova1, Daniel K. Sodickson1,2, Guillaume Madelin1,2, and Martijn A. Cloos3,4
    1Center for Biomedical Imaging, Department of Radiology, New York University School of Medicine, New York, NY, United States, 2Vilcek Institute of Graduate Biomedical Sciences, NYU Langone Health, New York, NY, United States, 3Centre for Advanced Imaging, The University of Queensland, Brisbane, Australia, 4ARC Training Centre for Innovation in Biomedical Imaging Technology, The University of Queensland, Brisbane, Australia
    In this work, we present an optimized 3D technique that can simultaneously acquire quantitative 1H density, T1, T2, B1+ maps and a 23Na image of the whole head in a reasonable scan time (~20 min).
    Figure 4: In-vivo results. Sodium images are shown in the first row, which has 3 mm3 isotropic resolution. Proton T1,T2, B1+ maps from the three directions are shown beneath the sodium images.
    Figure 1: Sequence diagram of the 3D simultaneous technique. The bars on top show the sodium excitations with constant flip angle and the proton MRF train with various flip angles. The details of the sequence for different segments are shown in the corresponding cards on the bottom.
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Digital Poster Session - Molecular Imaging & X-Nuclei: Applications
Cancer/Spectroscopy/Molecular Imaging/Pre-Clinical
Tuesday, 18 May 2021 13:00 - 14:00
  • Quadrupole moment splittings observed in 7T deuterium magnetic resonance spectra of skeletal muscle
    Ayhan Gursan1, Martijn Froeling1, Arjan D. Hendriks1, Dimitri Welting1, Dennis W.J. Klomp1, and Jeanine J. Prompers1
    1Department of Radiology, University Medical Center Utrecht, Utrecht, Netherlands
    Anisotropic motional averaging in skeletal muscle leads to deuterium quadrupole moment splittings of the HDO signal, the size of which depends on the angle between the muscle fibers and B0.
    Figure 1. Natural abundance DMRSI data in the right lower leg positioned parallel with B0. (A) Coronal T1w image. The white rectangle indicates the slice shown in panels B and C. Transversal T1w image with (B) segmentation of Tibialis Anterior (TA), Soleus (SOL) and Gastrocnemius Medialis (GM) muscles, and (C) overlaid with DMRSI data. Spectra from selected voxels in TA (D), SOL (E) and GM (F), as indicated in panel C, showing the signal from HDO at 4.7 ppm (x-axis range: 0-10 ppm = 457 Hz).
    Figure 3. Natural abundance DMRSI data in the right lower leg positioned at an angle of approximately 45° with respect to B0. (A) Sagittal T1w image. The white rectangle indicates the slice shown in panels B and C (cropped in AP direction to size of open part of rectangle). Transversal T1w image with (B) segmentation of TA, SOL and GM muscles, and (C) overlaid with DMRSI data. Spectra from selected voxels in TA (D), SOL (E) and GM (F), as indicated in panel C, showing the signal from HDO at 4.7 ppm (x-axis range: 0-10 ppm = 457 Hz).
  • Brain Metabolic Heterogeneity Revealed by Inorganic Phosphate (Pi):  The Puzzling Line Broadening and Splitting of Pi Magnetic Resonance at 7T
    Jimin Ren1,2, Craig R Malloy1,2, and Dean Sherry1,2
    1Advanced Imaging Research Center, UT Southwestern Medical Center, Dallas, TX, United States, 2Department of Radiology, UT Southwestern Medical Center, Dallas, TX, United States
    We presented solid evidence of large Pi line-broadening and splitting observed in human brain by 31P MRS at 7T. The effect may reflect pH heterogeneity in different brain tissues and/or cell types with distinct metabolism. 
    Fig1. 7T 31P MR spectrum acquired from the occipital-parietal region of a 30 years old female using a partial volume coil. Note that the intracellular Pi signal is split into two separate peaks with 0.1 ppm difference in chemical shift.
    Fig 3. 7T 31P MR spectrum averaged over eight healthy subjects. The data were acquired from the posterior brain using a partial volume coil. Note that the nearly symmetric line-broadening at Pi in reference to PCr (blue trace).
  • Monitoring liver glucose uptake and metabolism with dynamic 3D deuterium metabolic imaging at 7T
    Ayhan Gursan1, Arjan D. Hendriks1, Dimitri Welting1, Dennis W.J. Klomp1, and Jeanine J. Prompers1
    1Department of Radiology, University Medical Center Utrecht, Utrecht, Netherlands
    Dynamic 3D deuterium metabolic imaging with oral administration of deuterated glucose allows non-invasive and spatially resolved assessment of the dynamics of hepatic glucose uptake and metabolism.

    Figure 1. 3D DMI measurements at baseline and 0-130 min after oral administration of [6,6’-2H2]glucose (scan 1). (A) Overlay of last DMI data set (130 min) on transversal Dixon water image, with equal scaling of all spectra. (B-D) DMI spectra at baseline and up to 130 min after intake of deuterated glucose from voxels in the anterior (B) and posterior (C) side of the liver and the stomach (D).

    Figure 3. 3D DMI measurements 68-205 min after oral administration of [6,6’-2H2]glucose (scan 2). (A) Overlay of a DMI data set (160 min after intake) on transversal Dixon water image, with equal scaling of all spectra. (B-D) DMI spectra recorded from 68-205 min after intake of deuterated glucose from voxels in the anterior (B) and posterior (C) side of the liver and the stomach (D).

  • Precision and Reliability of Metabolite Quantification of 31P MRS at 7T
    Jia Xu1, Rolf F. Schulte2, William R. Kearney1, and Vincent A. Magnotta1,3,4
    1Radiology, University of Iowa, Iowa City, IA, United States, 2GE Global Research, Munich, Germany, 3Psychiatry, University of Iowa, Iowa City, IA, United States, 4Biomedical Engineering, University of Iowa, Iowa City, IA, United States
    The peak integration by simple summation of the magnitude spectrum is the most sensitive and robust 31P MRS quantification method to detect small ATP concentration changes. The test-retest repeatability of in-vivo ATP quantification is less than 3%. 
    Figure 3. Interscan test-retest repeatability of PCr, α-ATP, β-ATP, and γ-ATP peaks from quantitative, non-localized 31P MRS of 7 human subjects. The corresponding CVs estimated by Monte Carlo Simulation are shown in hatched bars. The dashed horizon line represents a 5% threshold.
    Figure 2. Comparison of Trueness (RMSE), linearity (R2), and relative uncertainty (CV) of α-ATP, β-ATP, γ-ATP, and PCr peaks quantified by HSVD, AMARES, conventional peak integration, lineshape fitting, and simple summation. The RMSE, R2, and CV values are normalized to (0, 1) range so that the reference point (center) represents the worst performance (0) and the circle represents the best performance (1). The normalized RMSE, R2, and CV values of α-ATP, β-ATP, γ-ATP, and PCr peaks are distributed evenly along the angular axes (circle).
  • 31P dual-band pulse for selective refocusing of phosphomonoesters and phosphodiesters at low B1+ and low SAR
    Zahra Shams1, Evita C. Wiegers1, Wybe J.M. van der Kemp1, Dennis W.J. Klomp1, and Jannie P. Wijnen1
    1Department of radiology, University Medical Center Utrecht, Utrecht, Netherlands
    We designed a dual-band pulse to selectively refocus PME and PDE spins. The dual band pulse, with B1+ < 15µT, uses almost 3 times less power compared to a single band pulse, making this an attractive option for multi-echo 31P body MRSI  in cancer.
    Figure 3. The spectra acquired in vivo from a pulse acquire and a spin echo acquisition with the dual band pulse aimed to hit the PDE and PME spin groups from the entire head, where B0 shimming is optimized over the yellow box. All MR spectra were displayed using a 10‐Hz Lorentzian line‐broadening filter. Note the well refocused signals of PME and PDE.
    Figure 2. Spectra acquired from a phantom with a spin echo (A) and a pulse acquire (B) acquisition. The dual band pulse at the frequency offset 3 resulted in a full refocusing of the three peaks of PE, PC and GPC. All MR spectra were displayed using a 10‐Hz Lorentzian line‐broadening filter. The yellow box is the shim box.
  • Multi-Centre patients receiving lithium treatment for bipolar disorder: 7Li-MRI optimization using a physiologically representative phantom
    Karthik Chary1, Franck Mauconduit2, Fiona Smith1, Marie Chupin3, Emmanuelle Gourieux2,3, Laura Pelizzari4, Karen Kettless5, Kristoffer Brendstrup-Brix6, Eva Mezger7, Daniel Keeser7, Olaf Dietrich8, Tim Wesemann9, Philipp Ritter10, Annett Werner9, Letizia Squarcina11, Paolo Brambilla11,12, Frank Bellivier13, Fawzi Boumezbeur2, David Cousins1,14, and Pete Thelwall1
    1Translational and Clinical Research Institute, Newcastle Magnetic Resonance Centre, Newcastle University, Newcastle upon Tyne, United Kingdom, 2NeuroSpin, CEA, CNRS, Paris-Saclay University, Gif-sur-Yvette, France, 3CATI, Institut du Cerveau et de la Moëlle Epinière, Paris, France, 4IRCCS, Fondazione Don Carlo Gnocchi ONLUS, Milan, Italy, 5Siemens Healthcare A/S & Siemens Healthcare GmbH, Copenhagen, Denmark, 6Neurobiology Research Unit (NRU) at Copenhagen University Hospital Rigshospitalet, Copenhagen, Denmark, 7Department of Psychiatry and Psychotherapy, University Hospital, LMU University, Munich, Germany, 8Department of Radiology, University Hospital, LMU Munich, Munich, Germany, 9Institute and Clinic of Diagnostic and Interventional Neuroradiology, University Hospital, Carl Gustav Carus, Dresden, Germany, 10Department of Psychiatry, University Hospital Carl Gustav Carus, Technische Universität Dresden, Dresden, Germany, 11Department of Pathophysiology and Transplantation, University of Milan, Milan, Italy, 12Department of Neurosciences and Mental Health, Fondazione IRCCS Ca' Granda Ospedale Maggiore Policlinico, Milan, Italy, 13INSERM UMRS-1144, AP-HP, Saint-Louis - Lariboisière – F. Widal Hospitals, Paris, France, 14Regional Affective Disorders Service, Cumbria, Northumberland, Tyne and Wear NHS Foundation Trust, Newcastle Upon Tyne, United Kingdom
    We demonstrated good agreement between modelling and phantom acquisitions to maximize 7Li-MRI signal amplitude which showed minimal inter-site variation in signal-to-noise to facilitate multi-centre studies of lithium treatment in bipolar disorder.
    Figure 2. Modelling vs phantom validation. A) SNR was computed on magnitude images using an identically positioned ROI (red block) on a signal and pure noise image according to the NEMA standard method. Parameters: TR=6.5 ms, TE=3.0 ms, NSA=217, recon matrix=32x32x7, recon voxel size=21.88x21.88x25 mm3, acquisition time=5 min. The Philips bSFFP sequence incorporated an elliptical shutter. B) Slight variation in the profile of the bSSFP signal amplitude versus flip angle was observed when comparing the theoretical modelling to the phantom tests.
    Figure 3. Pilot in vivo acquisitions. T1w images displayed for anatomical reference (A-C), 7Li-MRI images showing the 7Li distribution in the brain (D-F). The 7Li-MRI in vivo images acquired from three different test patients showed signal variations across multiple sites. The Philips data was interpolated to 21.88x21.88x25 mm3.
  • Simultaneous acquisition of 1H/19F/23Na/31P MR imaging in Phantom at 3T using a quadruple-nuclear RF coil system
    Nan Li1,2, Xing Yang1,2, Feng Du1,2, Kang Yan3, Bei Liu3, Yiping Du3, Chunsheng Yang4,5, Zhi Zhang4,5, Li Chen4,5, Fang Chen4,5, Xiaoliang Zhang6, Xin Liu1,2, Hairong Zheng1,2, and Ye Li1,2
    1Lauterbur Imaging Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China;, shenzhen, China, 2Key Laboratory for Magnetic Resonance and Multimodality Imaging of Guangdong Province, Shenzhen, China, Shenzhen, China, 3Institute for Medical Imaging Technology, School of Biomedical Engineering, Shanghai Jiao Tong University, Shanghai, China., Shanghai, China, 4State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Wuhan Center for Magnetic Resonance, Innovation Academy for Precision Measurement Science and Technology, the Chinese Academy of Sciences, Wuhan 430071, China;, Wuhan, China, 5University of Chinese Academy of Science, Beijing 100049, China, Wuhan, China, 6Department of Biomedical Engineering, State University of New York at Buffalo, NY, United States, Buffalo, NY, United States
     Imaging tests were performed to demonstrate the feasibility of synchronized 1H / 19F / 23Na/ 31P MR imaging at 3T by using developed quadruple-nuclear RF coil. The imaging approach combined with triple-tuned 19F / 23Na/ 31P receive coil also indicated the improved SNR.
    Fig. 3. (a)-(b): The 1H/19F/23Na/31P MR measured images obtained with the specific phantom. (a) only scanned by using the quadruple-nuclear RF coil. (b) Combined the quadruple-nuclear coil and triple tuned local 19F/23Na/31P receive coil. (c)-(d): SNR maps for the 1H/19F/23Na/31P imaging. (c) Without the local triple-tuned RF coils. (d) Combined with the local triple-tuned 19F/23Na/31P receive RF coils. The position of the local receive RF coil was indicated by the white dotted-line, and the SNR of the region indicated by the red arrow is significantly improved.
    Fig. 4. (a)-(b): The 1H/19F/23Na/31P MR measured images obtained with the independent nuclide test phantom. (a) only scanned by using the quadruple-nuclear RF coil. (b) Combined the quadruple-nuclear coil and triple tuned local 19F/23Na/31P receive coil. (c)-(d): SNR maps for the 1H/19F/23Na/31P imaging. (c) Without the local triple-tuned RF coils. (d) Combined with the local triple-tuned 19F/23Na/31P receive RF coils. The position of the local receive RF coil was indicated by the white dotted-line, and the SNR of the region indicated by the red arrow is significantly improved.
  • Sodium NMR relaxation times of human skin as potential biomarkers for Type 2 Diabetes Mellitus
    Daria V Fomina1,2, Elnur G Sadykhov3, Petra Hanson4,5, Christopher J Philp1, Harpal S Randeva4,5, J Paul O'Hare4,5, Olga S Pavlova3,6, Nikolay V Anisimov6, Alexander M Makurenkov3, Yury A Pirogov3, Thomas M Barber4,5, Thomas Meersmann1, and Galina E Pavlovskaya1,2
    1SPMIC, School of Medicine, University of Nottingham, Nottingham, United Kingdom, 2NIHR Nottingham Biomedical Research Centre, University of Nottingham, Nottingham, United Kingdom, 3Faculty of Physics, Lomonosov Moscow State University, Moscow, Russian Federation, 4Warwick Medical School, University of Warwick, Coventry, United Kingdom, 5Warwickshire Institute for the Study of Diabetes Endocrinology and Metabolism, University Hospitals Coventry and Warwickshire, Coventry, United Kingdom, 6Faculty of Fundamental Medicine, Lomonosov Moscow State University, Moscow, Russian Federation
    Investigation of 23Na NMR relaxation times, T2short and T2long, in human skin samples from control and T2DM patients using 23Na MRS at 9.4T has shown a significant elongation of T2long in T2DM patients that might indicate to disease specific skin structure changes.
    Figure 2. Sodium T2short and T2long obtained from bi-exponential fitting of CPMG (a) for samples collected from the foot/leg and abdomen from control patients and (b) for all samples from control and diabetic patients (samples from foot/leg and abdomen from control patients are presented together in one control group). ***P-value<0.001.
    Figure 1. Sodium CPMG echo integrals of the foot/leg skin samples from control (green) and diabetic (red) patients as a function of echo time (TE). Squares represent experimental data; solid lines correspond to the calculated fitting function.
  • Accuracy of quantified 23Na MRI in ischemic Stroke with varying undersampling Factors and CNN Postprocessing
    Anne Adlung1, Nadia Karina Paschke1, Alena-Kathrin Golla1,2, Dominik Bauer1,2, Sherif Mohamed3, Melina Samartzi4, Marc Fatar4, Eva Neumaier Probst3, Frank Gerrit Zöllner1,2, and Lothar Rudi Schad1
    1Computer Assisted Clinical Medicine, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 2Mannheim Institute for Intelligent System in Medicine, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 3Department of Neuroradiology, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 4Department of Neurology, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany
    This study investigates factors of k-space undersampling for which CNN postprocessing is able to improve 23Na MRI data and results indicate that it could enable the significant reduction of 23Na MRI data acquisition time.

    Figure 2: One representative image slice of one test case

    Top: Quantified FI, RI (S = 5) and the CNN output image with L2 and LGDL. Bottom: Corresponding TSC error maps within the whole brain.

    Figure 1: Representative image slice of one patient in its different versions. Full image (FI) and reduced images (RI) with varying factors S (2, 4, 5 10), and the corresponding CNN out images for L2 and LGDL.
  • 23Na MRI of mild traumatic brain injury: linear regression analysis reveals decreased total sodium concentration
    TERESA GERHALTER1, Anna M. Chen1, Seena Dehkharghani1, Rosermary Peralta1, Fatemeh Adlparvar1, James S. Babb1, Tamara Bushnik2, Jonathan M. Silver3, Brian S. Im2, Stephen P. Wall4, Ryan Brown1, Guillaume Madelin1, and Ivan Kirov1
    1Center for Biomedical Imaging, Department of Radiology, New York University Grossman School of Medicine, NEW YORK, NY, United States, 2Department of Rehabilitation Medicine, New York University Grossman School of Medicine, NEW YORK, NY, United States, 3Department of Psychiatry, New York University Grossman School of Medicine, NEW YORK, NY, United States, 4Ronald O. Perelman Department of Emergency Medicine, New York University Grossman School of Medicine, NEW YORK, NY, United States
    Using linear regression analysis, total sodium concentrations (TSC) in global white and grey matter were reduced in mild traumatic brain injury patients (at one month after injury) compared to healthy controls. TSC correlated with cognitive testing.
    Figure 2: Boxplots of TSC in mTBI and control (CTL) from linear regression analysis. Boxplots show the 1st, 2nd (median), and 3rd quartiles (box), ±95% (whiskers), and means (*) of the TSC distributions of the controls and mTBI patients for global grey and white matter (GM, WM, respectively) using linear regression. The boxplots excluded the three elder mTBI patients who lacked an age-matched control. Note that TSC in the GM and WM was decreased in mTBI when compared to controls (age-adjusted analysis of covariance, ♦: p<0.05).
    Table 2: Correlations between clinical and TSC measures. Direct and partial Spearman correlations (r) and p-values are presented for the association of TSC with the scores from the Brief Test of Adult Cognition by Telephone (BTACT) and Rivermead Post-Concussion Symptoms Questionnaire (RPQ) without (direct) and with (partial) adjustment for the elapsed time from injury to imaging, respectively. Only statistically significant correlations are shown (p<0.05).
  • Evaluation of different References for the Quantification of Tissue Sodium Concentration in Patients with ischemic Stroke
    Anne Adlung1, Sherif Mohamed2, Nadia Karina Paschke1, Mara Berger1, Melina Samartzi3, Marc Fatar3, Achim Gass4, Eva Neumaier Probst2, and Lothar Rudi Schad1
    1Computer Assisted Clinical Medicine, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 2Department of Neuroradiology, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 3Department of Neurology, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 4Heidelberg University, Mannheim, Germany
    Aim was to evaluate the reliability of internal vs. external references for quantification of tissue sodium concentration. 49 patients with ischemic stroke were examined. Results indicated high similarity between both reference types.
    Figure 2: One representative 23Na MRi slice from one patient with the ROI segmentation for the different quantification methods A: vials, B: CSF, and C: VH.
    Figure 3: Top row: TSC map from 23Na MRI of one patient and one exemplary slice with quantification based on A: reference vials, B: cerebral spinal fluid, C: vitreous humor. Bottom row: corresponding error maps of D: absolute TSC difference between A and B and E: absolute TSC difference between A and C
  • Sodium TQ signal of amino acids and α-lactalbumin in comparison to bovine serum albumin
    Dennis Kleimaier1, Simon Reichert1, Victor Schepkin2, and Lothar R. Schad1
    1Computer Assisted Clinical Medicine, Heidelberg University, Mannheim, Germany, 2National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL, United States
    Glutamic acid, arginine, and lysine as well as the small sized protein α-LA resulted only in a significant reduction in the sodium relaxation times without a detectable sodium TQ signal. In contrast, a BSA concentration of 3% w/v was already sufficient to yield a well detected sodium TQ signal.
    Fig.4: a) Dependence of the longitudinal and the transverse relaxation times on the BSA concentration. In the samples with a BSA concentration of 0% and 1% w/v, no sodium TQ signal was observed. Consequently, the TQTPPI FID was only fitted by a mono-exponential SQ signal decay. B) Dependence of the sodium TQ signal on the BSA concentration. The sodium TQ signal increased almost linearly with the BSA concentration. c) Zoomed TQTPPI spectra for different BSA concentrations.
    Fig.2: TQTPPI FID fit results of the samples containing amino acids or α-LA. The TQ SNR of each sample was less than three and thus the TQ term in the TQTPPI FID fit function was omitted. Hence, the TQTPPI FID fit function consisted only of a mono-exponential SQ signal decay. Exemplary TQTPPI spectra of these samples are shown in Fig.3.
  • Measuring CMRO2 in Brain Subcortical Structures Using Dynamic 17O-MRI
    Hao Song1, Burak Akin1, Johannes Fischer1, Ali Caglar Özen1,2, Stefan Schumann3, and Michael Bock1,2
    1Dept. of Radiology, Medical Physics, Medical Center University of Freiburg, Faculty of Medicine, University of Freiburg, Freiburg, Germany, 2German Consortium for Translational Cancer Research (DKTK), Partner Site Freiburg, Freiburg, Germany, 3Dept. of Anesthesiology and Critical Care, Medical Center University of Freiburg, Faculty of Medicine, University of Freiburg, Freiburg, Germany
    The CMRO2 values were determined in brain subcortical structures including thalamus, dorsal striatum, caudate nucleus and insula cortex using dynamic 17O-MRI. Our results show the feasibility of measuring local CMRO2 in brain subcortical structures using 17O-MRI at 3T.
    Figure 1. Co-registered masks of ROIs including thalamus (a), dorsal striatum (b), caudate nucleus (c) and insula (d) superimposed on the averaged 17O MR images.
    Figure 2. Dynamic H217O concentration (CH217O) in all examined ROIs. Blue dashed lines indicate the 17O2 inhalation time period.
  • MRI visualization of neurogenesis with ferritin and eGFP gene reporters in the intact and post-ischemic rat brain
    Marina Y Khodanovich1, Andrey E Akulov2, Tatyana V Anan’ina1, Elena P Krutenkova1, and Anna V Naumova3
    1Research Institute of Biology and Biophysics, Tomsk State University, Tomsk, Russian Federation, 2Institute of Cytology and Genetics, Novosibirsk, Russian Federation, 3Radiology, University of Washington, Seattle, WA, United States
    Ferritin and eGFP expression under doublecortin promoter caused 20% decrease in T2* intensity in the neurogenic (signal comes from the mature and young neurons) and ischemic (signal from macrophages) zones in the rat brain.
    Figure 2. Representative T2 and T2*-weighted images of the rat brain after MCAO surgery in the day 28 after injection of viral vectors or PBS. Immunofluorescent staining was done for ferritin (FerrH) and activated microglia/macrophages (CD68). eGFP signal was read at the fluorescent microscope with a wavelength of 488 nm. Areas of ischemic lesion were delineated on T2-weighted and propagated to T2*-weighed and to the histological images. Green arrows point to areas of the transgene expression near SVZ outside of ischemic lesion.
    Figure 3. Prussian Blue histological staining for detection of iron accumulation in the zone near lateral ventricle and SVZ (top row) and in the ischemic lesion zone (bottom row). Green arrows point to the cells with iron accumulation in the zone near the SVZ; red arrows point to the cells with iron accumulation in the ischemic lesion. Scale bar corresponds to 50 µm.
  • Treatment-induced changes in 2H-labeled lactate measured by 2H magnetic resonance spectroscopy are associated with apoptotic cell death
    Josephine L Tan1,2, Daniel Djayakarsana1,2, Hanzhi Wang1,2, Rachel W Chan2, Colleen Bailey1,2, and Angus Z Lau1,2
    1Medical Biophysics, University of Toronto, Toronto, ON, Canada, 2Physical Sciences, Sunnybrook Research Institute, Toronto, ON, Canada
    Significant decreases in 2H-labeled lactate signal were detected by deuterium magnetic resonance spectroscopy in acute myeloid leukemia cells 48 hours after cisplatin treatment, and significantly correlated with apoptotic cell death and extracellular lactate concentration.
    (a) Experimental setup consisting of three AML sample tubes lying on top of the 2H coil (green circle), with overlaid 2H spectra. (b) Single voxel 2H spectra for the untreated (U) and cisplatin-treated samples (T24 and T48) two hours after injection of [6,6’-2H2]glucose. (c) Time course of 2H-labeled species 10 minutes after injection of [6,6’-2H2]glucose. Error bars are the standard deviation across 6 samples. Stars indicate a statistically significance difference between T48 and U, and T48 and T24 (p<0.05)
    Representative TUNEL and H&E stained sections (10x and 200x magnification) from untreated and cisplatin-treated cell pellets, which were fixed in formalin for at least 96 hours after scanning. Formalin fixation may have caused pellet size shrinkage.
  • Three-compartment modeling for dynamic theragnostic agent enhanced MRI for Quantitative Analysis of NASH progression
    Asaduddin Muhammad1, Wonsik Jung2, Sangyong Jon2, and Sung-Hong Park1
    1Bio and Brain Engineering, Korea Advanced Institute of Science and Technology, Daejeon, Korea, Republic of, 2Biological science, Korea Advanced Institute of Science and Technology, Daejeon, Korea, Republic of
    We developed three compartment model to quantify NASH progression through the use of theragnostic drugs and proper kinetic modelling. In particular, parameter k22 linearly correlates with NASH progression. This can be used to prevent further progression into liver disease such as cirrhosis.
    Figure 1. Two different models tested (Top row) accounting for different circulation characteristic. Result of fitting (bottom row) using the two different models
    Figure 3 representative k21 and k22 parameter maps from each mice group. all maps from respective parameter shares the same colorbar range.
  • Dynamic Oxygen-17 MRI with Model-Based Approach for Mapping Cerebral Metabolic Rate of Oxygen in Mouse Brain at 9.4 T
    Yuning Gu1, Huiyun Gao2, Kihwan Kim1, Yunmei Wang2, and Xin Yu1,3
    1Biomedical Engineering, Case Western Reserve University, Cleveland, OH, United States, 2Medicine, Case Western Reserve University, Cleveland, OH, United States, 3Radiology, Case Western Reserve University, Cleveland, OH, United States
    We developed a model-based approach for CMRO2 mapping in the post-stroke mouse brain with 1.6-mm nominal resolution at 9.4 T.  The method showed ~50% reduced CMRO2 in the infarct core.
    Figure 3. In vivo results. A. TTC staining of the post-stroke mouse brain. B. CMRO2 maps overlayed on T2-weighted image. C. Histogram of CMRO2 values in the ipsilateral and contralateral hemisphere.
    Figure 1. Intermediate results in the simulation study at high SNR. A. The entire cost function (blue line) and the error from data consistency term (red line) in each iteration. B. Intermediate CMRO2 mapping results in each iteration.
  • Liver parenchymal change after stereotactic radiotherapy for hepatocellular carcinoma using DWI  and  MRE
    Yoshie Omiya1, Utaroh Motosugi2, Hiroyuki Morisaka1, and Hiroshi Onishi1
    1University of Yamanashi, Yamanashi, Japan, 2Kofu-Kyoritsu Hospital, Yamanashi, Japan
    Stereotactic body radiotherapy (SBRT) is a treatment option for patients with hepatocellular carcinoma (HCC). We evaluated the liver parenchymal changes after SBRT using liver stiffness with MRE and the apparent diffusion coefficient values with DWI. They were significantly elevated.
    Figure2. Box plots show of the liver stiffness and ADC values in the area receiving high dose and low dose of stereotactic body radiotherapy (SBRT). Liver stiffness and ADC values were significantly increased in both areas after SBRT. Exclude cases where ROI cannot be obtained sufficiently.
    Figure3. Case1: 79-year-old man with HCC at S6. The dose of SBRT was 50Gy/25Fr (PTV-95). The liver stiffnesses after SBRT were higher than those before SBRT in both area receiving >30Gy and area receiving <15Gy.
  • Deuterium Metabolic Imaging of the human brain at 9.4 T: Coil design and dynamic glucose uptake
    Loreen Ruhm1,2, Nikolai Avdievitch1, Theresia Ziegs1,2, Armin M. Nagel3,4, Henk M. De Feyter5, Robin A. de Graaf5, and Anke Henning1,6
    1High-Field MR Center, Max Planck Institute for Biological Cybernetics, Tuebingen, Germany, 2IMPRS for Cognitive and Systems Neuroscience, Eberhard-Karls University, Tuebingen, Germany, 3Institute of Radiology, University Hospital Erlangen, Erlangen, Germany, 4Division of Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 5Radiology and Biomedical Imaging, Yale University, New Haven, CT, United States, 6Advanced Imaging Research Center, UT Southwestern Medical Center, Dallas, TX, United States
    We present first DMI data of the human brain at B0 = 9.4T with a high spatial resolution acquired at a Siemens whole body scanner with a dedicated coil design. We investigated the dynamic uptake of [6,6’-2H]-glucose after oral administration in different brain areas.
    Fig. 5: 2H images for different times of one volunteer for water, glucose and Glx with and without referencing to a baseline water measurement (A). Zero-filling to twice the original resolution was applied. In (B), signals for different voxels are shown for water, glucose and Glx for the same volunteer. The colors of the frame label the corresponding metabolic images in (A). (C) shows data from four different volunteers (different colors) for water, glucose, Glx and lipid/lactate for summed voxels over different regions of the head.
    Fig. 2: The results for three volunteers of a whole brain FID measurement after the oral administration of deuterated glucose for four resonances (A). The temporal resolution of the measurement is 2 minutes. In (B), several spectra from volunteer 3 are shown at different time points. The time points are labeled with different colors.
  • Low field 19F imaging of perfluoroctylbromide: eliminating chemical shift effects and minimizing scalar coupling signal loss
    Javad Parsa1 and Andrew Webb1
    1Leiden University Medical Center, Leiden, Netherlands
    Low field MRI can be used to acquire 19F images with very high efficiency even for contrast agents with multiple resonances and scalar coupling, achieving very close to the theoretical SNR limit. 
    Figure 1. (left) Photograph of the solenoid coil which can be switched between 1H and 19F using a mechanical switch (arrow). (centre) Photograph of the phantom placed in the centre of the coil. (right) Schematic of the phantom with vials filled with water (blue), fomblin (orange) and a single tube of PFOB (red).
    Figure 2. (left) S11 plots of the 1H and 19F switched-mode RF coil. (center) Spin-echo 1H image from the phantom, (right) Corrsponding spin-echo 19F image.
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Digital Poster Session - Molecular Imaging & X-Nuclei: Developments
Cancer/Spectroscopy/Molecular Imaging/Pre-Clinical
Tuesday, 18 May 2021 13:00 - 14:00
  • Triple-quantum-filtered Sodium MRI at 7T: Optimization of the Enhanced SISTINA Sequence Using FLORET k-space Trajectories
    Qingping Chen1,2,3, Wieland A. Worthoff1, and N. Jon Shah1,2,4,5
    1Institute of Neuroscience and Medicine 4, INM-4, Forschungszentrum Jülich, Germany, 2Department of Neurology, RWTH Aachen University, Aachen, Germany, 3Department of Biomedical Engineering, The University of Melbourne, Parkville, Australia, 4Institute of Neuroscience and Medicine 11, INM-11, JARA, Forschungszentrum Jülich, Germany, 5JARA - BRAIN - Translational Medicine, Aachen, Germany
    The optimization of the triple-quantum-filtered sodium MRI sequence - enhanced SISTINA with FLORET improves the UTE image quality, while maintaining the multiple-quantum-filtered image quality and introducing randomness for potential application of compressed-sensing acceleration.
    Figure 2: Sequence diagrams of (A) conventional enhanced SISTINA with DISCOBALL UTE and MGRE MQC readout, and (B) optimized enhanced SISTINA with FLORET UTE and MQC readouts. Three hard RF pulses with flip angle α123=90°, preparation time τ=10ms, evolution time δ=50us. 12-step phase cycling scheme is applied to separate SQ- and TQ-weighted signal. Rewinder gradients are applied immediately after every readout to avoid the effect of residual magnetization on high-order coherences. Spoilers are used to dephase the residual transversal magnetization after the last MQC readout.
    Figure 4: The first-echo UTE, SQ, and TQ images after B0 and B1 correction obtained from three measurements depicted in Table 1. (Left) UTE, (middle) SQ, and (right) TQ images of (A) conventional enhanced SISTINA, (B) enhanced SISTINA with FLORET UTE readouts and MGRE MQC readouts, and (C) optimized enhanced SISTINA with FLORET UTE and FLORET MQC readouts. (D) the image differences of UTE, SQ, and TQ images: (left) the UTE image difference between the second and third measurements; (middle) the SQ and (right) TQ image differences between the first and second measurements.
  • Development of an add-on 23Na MRI platform for an existing 1H MRI scanner using a crossband repeater: Proof-of-concept
    Michiru Kajiwara1, Tomoyuki Haishi2,3, and Yasuhiko Terada1
    1Institute of Applied Physics, University of Tsukuba, Tsukuba, Japan, 2Department of Radiological Sciences, School of Health Sciences at Narita, International University of Health and Welfar, Narita, Japan, 3MRTechnology Inc., Tsukuba, Japan
    We have developed and demonstrated the feasibility of an add-on crossband repeater platform that enables 23Na-MRI by simply inserting it into an existing 1H-MRI system.
    Fig. 1 Add-on 23Na MRI platform equipped with the 1.5T 1H system. (a) Schematic overview of the system. (b) 1.5T magnet. (c) 1H transmit/receive coil without the RF shield. (d) 23Na transmit/received coil without the RF shield. (e) 1H pick-up coil. (f) Crossband convertor.
    Fig. 5 Demonstration of 1H/23Na imaging. (a) Saturated saline and water phantom. (b) Live mouse. (c) SNR measured in phantom and in vivo studies. (d,e) 1H-MRI and 23Na-MRI for (d) phantom and (e) live mouse. The red and blue squares indicate the noise and signal areas evaluated for the SNR measurement, respectively.
  • High-Resolution Sodium Imaging Using Anatomical and Sparsity Constraints for Denoising and Recovery of Novel Features
    Yibo Zhao1,2, Rong Guo1,2, Yudu Li1,2, Keith R. Thulborn3, and Zhi-Pei Liang1,2
    1Department of Electrical and Computer Engineering, University of Illinois, Urbana-Champaign, Urbana, IL, United States, 2Beckman Institute for Advanced Science and Technology, University of Illinois, Urbana-Champaign, Urbana, IL, United States, 3Center for Magnetic Resonance Research, University of Illinois at Chicago, Chicago, IL, United States
    A novel method is proposed for reconstruction of high-resolution sodium images from noisy, limited k-space data. The proposed method has been validated using both simulated and clinical data by comparison to conventional results.
    Figure 1. Illustration of the proposed reconstruction method. Tissue-based structural information from high-quality proton images is incorporated into the reconstruction of normal image features using a motion-compensated GS model. Sodium-dependent novel features (e.g., lesions) are reconstructed from the residues using a sparse model.
    Figure 3. Phantom and healthy subject results. (A) Phantom 1H reference image, 23Na FFT and proposed reconstruction, with corresponding calibration curves. Note that both curves are linear, but the FFT reconstruction had much larger standard deviation (5.3%) than the proposed method (2.8%). (B) Images from two healthy subjects. Note the marked improvement in image quality by the proposed method. (C) Regional TSC values obtained using the proposed method, which were consistent across different brain regions and subjects, demonstrating the reproducibility of the proposed method.
  • Three Dimensional Sodium Magnetic Resonance Fingerprinting using Irreducible Spherical Tensor Operator Simulations
    Fabian J. Kratzer1, Sebastian Flassbeck1,2,3, Sebastian Schmitter1,4, Tobias Wilferth5, Arthur W. Magill1, Benjamin R. Knowles1, Tanja Platt1, Peter Bachert1, Mark E. Ladd1, and Armin M. Nagel1,5
    1Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Center for Advanded Imaging Innovation and Research, New York University, New York, NY, United States, 3Center for Biomedical Imaging, Dept. of Radiology, New York University, New York, NY, United States, 4Physikalisch Technische Bundesanstalt (PTB), Braunschweig and Berlin, Germany, 5Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen (FAU), Erlangen, Germany
    A 3D 23Na-MRF technique for simultaneous quantification of T1, T2s*, T2l*, T2* and ΔB0 of is presented, which is based on irreducible spherical tensor operator simulations. Successful parameter quantification in a phantom is demonstrated.

    Fig.3: Phantom measurements of the transverse relaxation acquired with MRF (top) and the reference method (bottom). Here, both a mono- and a biexponential FID were fitted to multi-echo GRE images (FA=90°;TR=200ms;TE: 32 samples in [0.35,54.6]ms;Tacq=1h47min). The red masks in the T2l* and T2s* maps indicate pixels that were determined to relax monoexponentially (biexponentially in T2* maps). For the reference measurement, this distinction was determined by the goodness of the fit R2, whereas MRF determined this differentiation intrinsically in the dictionary matching step.

    Fig.2: Measurements of T1 and ΔB0 in a phantom with 23Na-MRF (top) and the references methods (bottom). The measurement time of 23Na-MRF was 1h4min. Furthermore, the 1st frame of the MRF data after compression into the new basis (23Na image) and a spin density (SD) image are shown. The T1 reference was acquired via fitting a monoexponential model to the data of an IR sequence with varying inversion time (FA=90°,TR=290ms;TI = [4,20,40,70,100,130,170,200,250]ms,Tacq=5h48min). ΔB0 was determined via a phase difference measurement (FA=45°;TR=25ms;TE=[0.55,5.55]ms,Tacq=7min).
  • New tuHDC BST-BT Ceramics with Optimal Permittivity Greatly Improve B1 efficiency and SNR at Room Temperature for 17O MRSI Application at 10.5T
    Hannes Michel Wiesner1, Xiao-Hong Zhu1, Maryam Sarkarat2, Xin Li1, Matt Waks1, Michael T. Lanagan2, Qing X. Yang3, and Wei Chen1
    1CMRR, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 2Department of Engineering, Pennsylvania State College of Engineering, University Park, PA, United States, 3CNMRR, Department of Neurosurgery, Penn State University, Hershey, PA, United States
    The newly developed BST-BT ceramics enabled unprecedented (> 4 times) improvements in RF transmission efficiency, reception sensitivity and SNR for room temperature 17O MRSI applications at 10.5T. 
    Figure 1 Temperature dependence of dielectric constant (A) and loss (B) measured in the BST-BT uHDC disks at three measurement frequencies.
    Figure 3 Representative B1+ maps in axial orientation (left panels) and B1+ profiles along the vertical dashed lines acquired under (A) control without the uHDC disks, (B) with one uHDC disk and (C) two stacked disks. The ratio images between (D) one uHDC disk versus control and (E) two stacked disks versus control. The yellow rings represent the 15-cm 17O RF coil.
  • A Dedicated RF Coil System for 19F MRI of Myocardial Infarction at a 3 T Clinical MRI System
    Ali Caglar Özen1,2, Felix Spreter1, Timo Heidt3, Constantin von zur Mühlen3, and Michael Bock1
    1Deptartment of Radiology, Medical Physics, University Medical Center Freiburg, University of Freiburg, Freiburg, Germany, 2German Consortium for Translational Cancer Research Partner Site Freiburg, German Cancer Research Center (DKFZ), Heidelberg, Germany, 3Department of Cardiology and Angiology I, UHZ, University Medical Center and Faculty of Medicine, University of Freiburg, Freiburg, Germany
    A detachable Tx array of as low as 5 independent loop coils can be used to generate a homogeneous B1+ field within the heart of an adult pig. In combination with an optimized Rx coil array that conforms to the special geometry of a pig supine position high SNR can be achieved.
    Fig. 1: Schematic and layout of the dedicated 19F MRI RF coil system. Printed circuit boards of the Tx and Rx coil elements are shown on the left hand side. Sij curves, circuit diagrams and the component values can be found in https://github.com/alibaz/F19Coils
    Fig. 4: S matrix of the 6 channel anterior part of the 19F MRI coil system measured with phantom and in vivo loading. In the phantom Sii<-20dB and Sij<-16 dB, and in the animal an Sii<-14dB and Sij<-18 dB was achieved.
  • Fast Fluorine Spectroscopic Imaging with pseudo-spiral k-space sampling
    Muhammed Yildirim1,2, Patrick Scholtz2, Markus Schütz2, Xenia Kovalyk2, Edwin Heijman2,3, Rolf Lamerichs3, Holger Grüll2, and Esin Ozturk Isik1
    1Computational Imaging Lab, Institute Of Biomedical Engineering, Bogazici University, Istanbul, Turkey, 2Institute of Diagnostic and Interventional Radiology, Faculty of Medicine and University Hospital of Cologne, University of Cologne, Cologne, Germany, 3Philip Research Labs, Eindhoven, Netherlands
    Following a long period of dismissal, 19F spectroscopic imaging strikes back with BaSSI, a balanced sequence with spiral k-space trajectory. The sequence records a sensitivity of 63 μmol-1min-1/2; which is 25% better than the 3D-balanced-UTE-SSFP sequence , the golden standard of 19F MRI.
    Detection sensitivity and image quality comparison of balanced spiral spectroscopic imaging and 3D balanced UTE SSFP using a 0.1μl sample of PFOB. The spectroscopic imaging sequence is capable of detecting the sample with NSA=1, whereas the imaging sequence starts picking up the signal with higher NSA's. In terms of image quality, spectroscopic imaging shows significantly less spreading than its imaging counterpart, offering accurate localization of the target.

    a) all phase-encoded spectroscopic imaging sequence with balanced gradients. Encoding can be done in 2D or 3D.

    b) pseudo-spiral k-space sampling scheme in 2D. 3D encoding is done by stacking 2D trajectories.

  • Comparison of low rank compressed sensing with non-uniform undersampled non-linear FID fitting for time efficient 23Na TQTPPI measurements
    Simon Reichert1, Dennis Kleimaier1, and Lothar Schad1
    1Computer Assisted Clinical Medicine, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany
    Low rank reconstruction and a fit of the undersampled data (NUSF) were implemented and quantitatively compared for simulated and measured 23Na TQTPPI data. In both cases, the measurement time can be reduced by a factor of 5 without significantly decreasing the accuracy.
    a) The TQTPPI pulse sequence consisted of three 90° pulses and an additional 180° refocusing pulse. In every phase step both the evolution time and a phase are incremented. b) A fully sampled TQTPPI FID and the corresponding NUS TQTPPI FID are shown. The undersampling pattern was sinusoidal Poisson gap sampling c) A Fourier transformation leads to a sparse spectrum consisting of SQ and TQ signals. The Fourier transform of the NUS FID shows an increased noise level and reduced SQ and TQ signals. The spectrum and FID can be recovered using CS.
    Variation of undersampling factor in the range of 2 to 16 using simulated data. The parameters were: ATQ/ASQ=10%, SNR=70, T2S=39ms and T2F=10ms. a), b) and c) show ATQ/ASQ, T2S and T2F, respectively. The deviation to ground truth was less than 5% for undersampling factors up to 5. For T2S there is a small offset for NUSF.
  • Interleaved 31P MRS and 1H dual-echo GRE B0 map pulse sequence for 7T Terra scanners
    Jabrane Karkouri1 and Christopher T. Rodgers1
    1Wolfson Brain Imaging Center, University of Cambridge, Cambridge, United Kingdom
    In this abstract, we demonstrate a framework for interleaving 1H imaging and 31P spectroscopy on the Siemens 7T Terra platform. We show how this can be done and demonstrate the concept with interleaved B0 map acquisition with 31P-MRS on a phantom and the quadriceps of a healthy volunteer.
    Figure 2: Interleaving sequence working scheme and in-house built circuit for safety testing
    Figure 5: In vivo B0 map image of the thigh of a healthy volunteer at[CTR1] 7 T, 1H spectrum and interleaved 31P spectrum.
  • Three-Dimensional Sodium MRI Using A Rotation of Spiral Disc (RSD) Trajectory
    Kwan-Jin Jung1 and Brad Sutton1,2
    1Beckman Institute for Advanced Science and Technology, University of Illinois at Urbana-Champaign, Urbana, IL, United States, 2Electrical & Computer Engineering, University of Illinois at Urbana-Champaign, Urbana, IL, United States
    Sodium MRI is challenging due to its low sensitivity and short T2 and hence a three-dimensional sequence with a spiral trajectory has been applied. The spiral trajectory was shortened in the TPI method by accelerating the span at the k-space origin using a radial start and then transiting into a spiral trajectory. This popular TPI method, however, requires a very high gradient slew rate when the 3D cone approaches the polar pole. This drawback has been resolved by rotating a two-dimensional disc filled with interleaved TPI trajectories. This method achieved the faster sweeping of TPI as well as a uniform gradient slew rate over the sphere sampling. We are reporting some artifacts in TPI-based scans not only in our study but also in other studies.
    Figure 2. Trajectories of the proposed RSD scheme. (A) The disc, filled with the interleaved TPI trajectories shown in Fig. 1A, is rotated along the x-axis to form a sphere. (B) A half-filled sphere with TPI discs.
    Figure 3. Sodium phantom images on 3 orthogonal slices. The red numbers on the larger bottles count the bright rings of the annular pattern in each bottle. The dotted yellow rectangle includes the smaller tubes with the center dark spot.
  • Conserving low amplitude resonances in tensor rank truncation for image enhancement of spectroscopic imaging data.
    Alan J. Wright1, Richard Mair1,2,3, Anastasia Tsyben1, and Kevin M. Brindle1,3,4
    1CRUK Cambridge Institute, University of Cambridge, Cambridge, United Kingdom, 2Department of Clinical Neurosciences, University of Cambridge, Cambridge, United Kingdom, 3Cancer Research UK Major Centre-Cambridge, University of Cambridge, Cambridge, United Kingdom, 4Department of Biochemistry, University of Cambridge, Cambridge, United Kingdom
    Tensor decomposition can be used for denoising magnetic resonance spectroscopic imaging (MRSI) data. A condition for selection of rank order is proposed that removes only noise from the reconstructed data and preserves signals from low amplitude resonances. 
    Figure 3. A) Metabolite amplitudes of the first 13C MRSI dataset: top row - acquired data; lower row - TRI de-noised data (core rank: 7x6x7). A T2-weighted image shows the positions of the brain, tumour and a [13C]urea phantom. Relative amplitudes are indicated by the colour bar, except for [1-13C]pyruvate, which is decreased ten-fold. B) As for (A), but for the second dataset (core rank 3x3x3). C) The first three fibers in the spectral dimension of the tensor decomposition in (B), shown as spectra.
    Figure 1. A) Carbon-13 MRSI spectra from the head of a rat with an orthotopically implanted patient-derived glioblastoma xenograft. Rows 7 to 10, columns 13 to 22 and chemical shifts 209 ppm to 141 ppm are shown. Spectra were baseline corrected and line broadened to 25 Hz. B) The same data but reconstructed with a core tensor size of 7x6x7 and processed similarly. C) The residual of the acquired data minus the TRI data with no line broadening or baseline correction.
  • Variable Temporal Resolution Cartesian Sampling for Cell Tracking MRI
    Mark Armstrong1, Felix Freppon2, Enrica Wilken2, Max Masthoff2, Cornelius Faber2, and Dan Xiao1
    1University of Windsor, Windsor, ON, Canada, 2Universität Münster, Münster, Germany
    A Cartesian sampling scheme for dynamic MRI is presented. Both the high temporal resolution images and fully sampled image are acquired. The undersampling ratio can be flexibly chosen retrospectively, providing a unique advantage when experimental conditions cannot be predetermined.
    Figure 3. In vivo cell tracking experiments (a) reconstructed with fully sampled k-space. (b) was reconstructed with 21% k-space data, retrospectively selected from (a). (c) was the time frame following (b) reconstructed with the same undersampling ratio. The red circle highlights a location where the cell is not visible in (a), but visible in (b), and had exited the slice in (c). A few other cells that are visible in (b) and (c), but not in (a), are highlighted in green.
    The cartesian sampling scheme illustration. A fully sampled k-space (a) can be retrospectively undersampled at different ratios, such as (b) and (c).
  • Single Loop Tri-frequency Surface Coil Design for 1H MRI and Interleaved Dynamic 2H and 17O MRS Applications at Ultrahigh Field of 16.4T
    Parker John Bresnahan Jenkins1, Guangle Zhang1, Wei Zhu1, Xiao-Hong Zhu1, and Wei Chen1
    1Center for Magnetic Resonance Research, University of Minnesota, Minneapolis, MN, United States
    A novel tri-frequency surface coil based on traditional loop design utilizing active tuning circuitry was developed and validated for 1H, 2H, and 17O MR applications at 16.4T. It shows a potential for temporally efficient interleaved metabolic imaging.
    Figure 5. (a) 1H axial images acquired with 2D GEMS sequence. (b) Left: the 2H signal of Control scan and that of interleaved 2H- 17O scans (nt=20). Right: the 17O signal of the Control scan and that of interleaved 2H- 17O scans (nt=100). (c) Top: 20 deuterium spectra from interleaved 2H- 17O scans (nt=1×20); Bottom: 20 oxygen-17 spectra from interleaved 2H- 17O scans (nt=5×20).
    Figure 1. Schematic circuit diagram of the triple-tuned coil design. For 1H (no DC), modulate C2 and C5 to tune and match to 698MHz. For 2H (no DC) tune and match C2 and C5 to 107MHz. For 17O, make sure setup for 2H is established, apply DC and modulate C3 and C4 to tune and match to 94MHz.
  • Parametric VARied Saturation (PaVARS) for enhanced CEST characterization of human brain at 3T
    Zhensen Chen1, Yishi Wang2, Le He1, Hanyu Wei1, Yibing Chen3, and Xiaolei Song1
    1Center for Biomedical Imaging Research, School of Medicine, Tsinghua University, Beijing, China, 2Philips Healthcare, Beijing, China, 3School of Information Science and Technology, Northwest University, Xi'an, China
    A new CEST saturation preparation and readout scheme that allows discrimination of fast and slow exchange species was proposed, implemented and tested at 3TMR scanner for human brain imaging.
    Fig.3. PaVARS CEST images and signal evolution for healthy human brain at 3T. A, B and C are MTRasym images at 3.5ppm, Amide signal and NOE signal using LD quantification, respectively. Images from the 5 modules of PaVARS and the first principal component of the five modules are shown. D: T2w FLARE image showing the drawn ROI of putamen, caudate and globus pallidus. E shows the five PaVARS Zspectra and the corresponding Lorentzian fitted lines and the zoomed residual (LD) spectra. F plots the LD signal changes as sat. module #, with the error bar indicating standard deviation across subjects.
    Fig.2. Phantom experiments of PaVARS CEST profile for three different metabolites, from left to right: Glu., pCr. and Cr. The upper row was obtained with constant B1 =2uT, while the bottom row was obtained with an alternating B1 of 0.6uT and 2.8uT. As seen, PaVARS allows a unique profile for Glu., pCr. and Cr., despite that pCr. and Cr. both contain guanidinium amine protons and the Glutamate amine resonances at similar offset frequency.
  • Towards a Probabilistic Neurochemical atlas via parcellated approach using ZOOM MRSI
    Nicholas Farley1, Jaiyta Sood1, Antonia Susjnar2, Sean Lane3, Mark Chiew4, Michael Albert Thomas5, and Uzay Emir1,2
    1School of Health Sciences, Purdue University, West Lafayette, IN, United States, 2Weldon School of Biomedical Engineering, Purdue University, West Lafayette, IN, United States, 3Department of Psychological Sciences, Purdue University, West Lafayette, IN, United States, 4Welcome Center for Integrative Neuroimaging, University of Oxford, Oxford, United Kingdom, 5Department of Radiology, University of California Los Angeles, Los Angeles, CA, United States
    Quantify the test-retest reliability of ZOOM MRSI via measuring molecular contrast stability within the posterior cingulate and cerebellum.  This is performed over two independent scan sessions and results demonstrate the efficacy of this MRSI technique.
    Figure 4: Group-average normalized metabolite maps overlaid on Montreal Neurological Institute-152
    Figure 1: Single-subject normalized metabolite maps overlaid on the Montreal Neurological Institute-152 template
  • MRI contrast agent for myocardial infarction based on novel manganese-based nanoparticles
    Chengbin He1, Xiaoxuan Zhou1, Cailing Pu1, Jingle Fei1, Yan Wu1, and Hongjie Hu1
    1Department of Radiology, Sir Run Run Shaw Hospital (SRRSH), Zhejiang University School of Medicine, Hangzhou, China
    Our study found that BHMNP had high T1 relaxation rate and high signal intensity in the myocardial infarction area. In addition, BHMNP has the potential for clinical transformation due to its simple synthesis, good biocompatibility and biodegradability.

    a. MRI images of mice injected with BHM;

    b. TTC and HE staining;

    c. CNR curves of BHM and Omniscan.

    a.The particle size of BHM was about 67 nm.

    b.The particles were regular and uniform spheres under transmission electron microscope

  • MR detection of gas microbubbles via hyperCEST: a path toward a dual modality contrast agent
    Christian T McHugh1, Phillip G Durham2, Michele Kelley1, Paul A Dayton3, and Rosa T Branca1
    1Physics & Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, NC, United States, 2Pharmacoengineering and Molecular Pharmaceutics, University of North Carolina at Chapel Hill, Chapel Hill, NC, United States, 3Biomedical Engineering, University of North Carolina at Chapel Hill, Chapel Hill, NC, United States
    Gas microbubbles have the potential to be a dual modality contrast agent for US and MRI, but the MR detection sensitivity to microbubbles must improve. Here we show that microbubbles, at clinically relevant doses, can be detected by using hyperCEST.
    Figure 2. Zoom-in of experimental Z-spectra around the gas-phase peak. Z-spectra for (A, 340 fM) small and (B, 40 fM) medium MBs at different B1 strengths. Z spectra obtained with a constant B1 (5 μT) at different gas-volume concentrations with (C) small, (D) medium, and (E) large MBs. (F) Z-spectra of MBs with different sizes at a constant concentration of 400 fM. Signal loss increases with B1 as well as with gas-volume concentration. HyperCEST efficiency is maximized for MBs with a 2 μm diameter.
    Figure 1. Simulations of MBs hyperCEST contrast. MB samples are characterized by the gas-volume concentration (μL/L) and average diameter (μm). These characteristics are directly related to the exchange rate and participation rate of 129Xe. Using the FHC solution, signal loss at different B1 strengths is shown. Signal loss generally increases with B1 and gas-volume concentration. The MB size must be optimized, and MBs lose efficiency as hyperCEST agents at sizes in excess of 2 μm.
  • Kartogenin and synthetic melanin nanoparticle loaded hydrogel scaffold for cartilage regeneration and monitored by quantitative MRI
    Chuyao Chen1, Shaoshan Huang2, Zelong Chen1, Chenggong Yan1, Yingjie Mei3, Yikai Xu1, and Rui Guo2
    1Medical Imaging Center, Nanfang Hospital, Southern Medical University, Guangzhou, China, 2Key Laboratory of Biomaterials of Guangdong Higher Education Institutes, Guangdong Provincial Engineering and Technological Research Centre for Drug Carrier Development, Department of Biomedical Engineering, Jinan University, Guangzhou, China, 3Philips Healthcare, Guangzhou, China
    A KGN/SMNP loaded cell-therapy theranostic hydrogel scaffold for cartilage repair was developed in our study.
    Figure 2 A. MR water-selective cartilage scan (3D_WATSc) for neocartilage assessment at 3,6, 9, and 12 weeks after surgery (Left: No-treated group, Right: Treated group). B. Quantitative R1 relaxometry rate of the different hydrogels measured by T1 mapping scan in vivo. C. Macroscopic and histological observations of cartilage harvested during weeks 6 and 12 (white box: degenerated cartilage).
    Figure 1 A. Schematic illustration of the experimental protocol. B. Structural observation and MRI characterization of hydrogels. C. T1-weigted MRI images and quantitative R1 relaxometry rate of SMNP-KGN hydrogel at various concentrations.
  • Glycogen Synthesis and Glucose Utilization at 3T using Localized Spectroscopy and Chemical Shift Imaging
    Shun Kishimoto1, Jeffrey R Brender1, Jeeva Munasinghe2, Martin Lizak2, Yu Saito1, Kota Yamashita1, Otowa Yasunori1, Kazu Yamamoto1, James Mitchell1, and Murali C. Krishna1
    1NIH/NCI, Bethesda,, MD, United States, 2NIH/NINDS, Bethesda,, MD, United States
    Glycogen metabolism and glucose utilization in mice can be followed in brain tissue semi-quantitatively by proton localized MRS using standard 3T preclinical imaging systems.
    (A) Time lapse CSI images of a normal mouse brain after the injection of 50 mg unlabeled glucose. FOV 20 mm x 20 mm x 6 mm, Tr=2 s, 512 spectral FID points. Data is shown in magnitude mode without averaging. (B) Kinetics of the peak at 5.2 ppm (C) Contour map of the 5.2 ppm peak
    Dose dependence of (A) glycogen and (B) glucose kinetics for 0, 25, and 50 mg doses by following the peaks indicated in (C)
  • In vivo hijacking local activated macrophages for targeted theranostics of epilepsy with nanomedicines
    Lin Lin1,2, Xiaodan Chen3, and Pu-Yeh Wu4
    1Fujian Medical University Union Hosptial, Fuzhou, China, 2Fudan University Huashan Hospital, Shanghai, China, 3Fujian Cancer Hospital, Fuzhou, China, 4GE Healthcare, Beijing, China
    In vivo hijacking local activated macrophages for targeted  epilepsy theranostics
    MR maging of the epileptogenic region to evaluate the targeting capability of BMC NPs.
    In vivo assessments of BMC NPs on hypoxia attenuation, cell apoptosis, and neuron protection.