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1391 | The Coax Dipole Antenna: a flexible, low SAR dipole antenna for body imaging at 7 Tesla. | |
Carel C. van Leeuwen1, Bart R.E. Steensma1, Dennis W.J. Klomp1, Cornelis A.T. van den Berg1, and Alexander J.E. Raaijmakers1,2 | ||
1University Medical Center Utrecht, Utrecht, Netherlands, 2Biomedical Engineering, Eindhoven University of Technology, Eindhoven, Netherlands |
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A coax cable dipole antenna with gaps in the shield supports flat current profiles on the outside of the shield. A simulation study is performed to further optimize the design of this flexible so-called ‘coax dipole antenna’. MR thermometry measurements are performed using a single antenna and a homogeneous phantom. The coax dipole antenna causes 18% lower peak heating than a fractionated dipole antenna. An array of eight coax dipole antennas is used to generate T2-weighted images and B1 maps of the prostate of three volunteers, where the coax dipoles achieve the same B1 as an array of fractionated dipoles. |
1392 | Bailey splitter/combiner for RF shimming/Rx coil combination | |
Yue Zhu1,2, John C Gore1,2,3,4, and Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University, Nashville, TN, United States, 3Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 4Electrical and Computer Engineering, Vanderbilt University, Nashville, TN, United States |
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We designed a continuously adjustable Bailey splitter/combiner with a sliding mechanism. This device has a good input matching of < -18dB and a low insertion loss of about -0.5dB. The sliding mechanism allowed easy handling and precise adjustments. The resistor free design eliminated the potential safety concern from the previous Ratio Adjustable Power Splitter circuits. We obtained good agreements between predicted and measured transmit field maps with the Bailey splitter/combiner. |
1393 | Performance of flexible coaxial transmission line resonator coils vs. stranded wire coils at 3 T | |
Raphaela Czerny1, Michael Obermann1, and Elmar Laistler1 | ||
1High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria |
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As flexible form-fitting RF coils can provide enhanced receive sensitivity in MRI, various coil design approaches have been studied recently, including coaxial and stranded wire coil elements. While stranded wire coils are electrically identical to conventional rigid copper loop coils, coaxial transmission line resonators are self-resonant and do not require additional components along the conductor. The goal of this work was to compare flexible receive-only stranded wire coils and coaxial coils in terms of Q-factors, inter-element coupling, noise correlation, and SNR. |
1394 | High Impedance Loop coil Design for improved EM Decoupling in Multichannel Coil arrays | |
Sirihaas Gaddipati1 and Xiaoliang zhang2 | ||
1University at Buffalo, Buffalo, NY, United States, 2Biomedical Engineering, University at Buffalo, Buffalo, NY, United States |
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In traditional magnetic resonance imaging (MRI) design, ideal coil overlapping is used to minimize coupling between nearest-neighbor coils, and low input impedance preamplifiers are used to isolate the relatively weak coupling. Modern-day MR systems use phased array coils constructed out of low impedance resonant loops. Inside such arrays, electrodynamic interactions between elements must be carefully balanced[1]. However, to make the complex sensitivities of phased-array coils sufficiently distinct in parallel spatially-encoded MRI, needed an overlapping between coils. This electromechanical balancing act becomes increasingly difficult as the number of receive elements grows for optimal performance, leading to geometrical puzzles of profound complexity. |
1395 | An Improved Power Handling Active Transmit/Receive Switch for Low Field MRI using Reed Relays | |
Don Straney1, Clarissa Zimmerman Cooley1,2, and Matthew S Rosen1,2,3 | ||
1Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States, 2Harvard Medical School, Boston, MA, United States, 3Department of Physics, Harvard University, Cambridge, MA, United States |
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An active transmit/receive (T/R) switch based on reed relays shows promise in overcoming the previous limitations at low field of both passive and active T/R switches. We aim to provide a design for other low-field researchers to use which handles a wide range of frequencies (DC to 3.4 Mhz) and power levels (<1 mW to 2 kW pulsed) in a simple, low-parts-count device which is easy to reproduce. |
1396 | Use of High - Permittivity Pads to enhance SNR and Transmit Efficiency in the Chest at 7T | |
Giuseppe Carluccio1,2 and Christopher Michael Collins1,3 | ||
1Radiology, Center for Advanced Imaging Innovation and Research (CAI2R), New York, NY, United States, 2Radiology, Bernard and Irene Schwartz Center for Biomedical Imaging, New York, NY, United States, 3Bernard and Irene Schwartz Center for Biomedical Imaging, New York, NY, United States |
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High-Permittivity materials have been recently used to shape the B1 field distribution to enhance SNR and transmit efficiency. So far, these materials have been mainly applied to increase SNR in the head. In this work, through numerical simulations, we explore the possibility to use high-permittivity pads to improve the signal in the chest. The pads are positioned between the model of the coils (8 TEM transmit coils and 24 receive loops) and of the human body. Our simulations show that some improvement can be obtained by adding the pads to the coils. |
1397 | Introducing the Double-Folded Dipole to enhance the Excitation Efficiency at 7T Ultra-High Field MRI | |
Sam-Luca J.D. Hansen1, Markus W. May1, Mirsad Mahmutovic1, Manisha Shrestha1, Anpreet Ghotra1, Matthäus Poniatowski1, and Boris Keil1 | ||
1Institute of Medical Physics and Radiation Protection, TH Mittelhessen University of Applied Sciences, Gießen, Germany |
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We demonstrated a highly efficient B1+to-SAR dipole antenna for ultrahigh-field MRI which consists of a double-folded ladder structure. The antenna was simulated and bench tested. The antenna has a high impedance which provides low mutual coupling between other antenna elements. Ultimately, this characteristic possibly allows to construct antenna array for pTx. |
1398 | Non-Uniform Dielectric Substrate (NODES) Antenna Design for Cardiac Imaging at 7T | |
Alireza Sadeghi-Tarakameh1, Bahram Khalichi2, Xiaoping Wu1, Gregory J. Metzger1, and Yigitcan Eryaman3 | ||
1Center for Magnetic Resonance Research (CMRR), University of Minnesota, Minneapolis, MN, United States, 2Department of Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey, 3University of Minnesota, Minneapolis, MN, United States |
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Utilizing receive and transmit array coils with improved SNR/SAR performance is crucial to realizing the full potential of ultra-high field (UHF) MRI. In this work, we optimize a previously introduced antenna (NODES) to improve its SNR and SAR performances for 7T cardiac MRI applications. |
1399 | Parametric Coil Optimization via Global Optimization | |
Jose EC Serralles1, Elfar Adalsteinsson2,3, Lawrence L Wald4, and Luca Daniel1 | ||
1Computational Prototyping Group (CPG), Research Laboratory of Electronics (RLE), Department of Electrical Engineering and Computer Science (EECS), Massachusetts Institute of Technology (MIT), Cambridge, MA, United States, 2Department of Electrical Engineering and Computer Science (EECS), Massachusetts Institute of Technology (MIT), Cambridge, MA, United States, 3Institute for Medical Engineering and Science (IMES), Massachusetts Institute of Technology (MIT), Cambridge, MA, United States, 4Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Harvard Medical School, Boston, MA, United States |
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Algorithmic design of coil arrays in MRI is typically considered desirable but computationally intractable. In this work, we demonstrate that it is in fact feasible to programmatically optimize over the design of a coil array to achieve a metric-of-interest, such as slice homogeneity in the transmit field. We build on previous work by employing global optimizers in several of the key steps in the optimization procedure. We demonstrate the effectiveness of this approach via a couple of numerical examples. |
1400 | MR imaging with a standard electro-optical modulator: Initial results | |
Paul Nobre1, Gwenaël Gaborit2,3, Raphaël Sablong1, Lionel Duvillaret3, and Olivier Beuf1 | ||
1Univ. Lyon, INSA-Lyon, Université Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS, UMR 5220, U1206, Villeurbanne, France, 2Université de Savoie, IMEP-LAHC, UMR 5130, Le Bourget-du-Lac, France, 3KAPTEOS, Sainte-Hélène-du-Lac, France |
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The large majority of receiver clinical MR coil are using cables between the resonant coil and Connector plug. To remove possible induced currents on the cable’s shield, circuits such as RF traps are distributed along the cable. This is done to ensure patients’ safety during the exam. RF-traps are difficult to miniaturize and are not fit for inner coils such as endoluminal coils. Optical fibers would be a smart option to get rid of this critical drawback but this requires electro-optical conversion devices. This abstract presents the first images obtained at 7T with an electro-optical conversion based on Pockel’s effect. |
1401 | Correcting meander-line surface coil fields for large-area near-surface imaging | |
Gary Zabow1, Stephen Dodd2, and Alan Koretsky2 | ||
1Applied Physics Division, National Institute of Standards and Technology (NIST), Boulder, CO, United States, 2NINDS, National Institutes of Health (NIH), Bethesda, MD, United States |
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Planar meander-line coils have been proposed as ideal surface coils because they should, theoretically, create highly uniform fields over planes of essentially unlimited area. Experimentally, however, field uniformity of planar meander-line coils is often worse, not better, than even simple loop surface coils. This presentation shows why existing predictions of meander-line coil fields and imaging performance are misinterpreted and how coil geometries can be simply corrected to better match theory. In particular, it is shown how a single extra turn of wire can increase field uniformity by at least an order of magnitude, allowing for uniform, large-area near-surface imaging. |
1402 | UVC Based Wireless Patient Bore Disinfection Utilizing Scanner RF Transmission | |
Devavrat Likhite1, Rob Amerling1, Leon Lee1, and Saban Kurucay1 | ||
1GE Healthcare, Waukesha, WI, United States |
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In the recent times, cleaning protocols after every patient, regular disinfection of medical equipment and use of single-use devices have become a common practice. MRI equipment has been one of the most difficult imaging modalities to clean. Here, we present a simple technique that uses UV light to disinfect the MRI system, without the use of any external power or connecting cables. This technique uses the power from the MRI system and thereby provides a simple and wire-free UV disinfection solution that does not need external electrical source. |
1403 | Smart Metamaterials for 3T MRI | |
Dennis Philipp1, Endri Stoja2, Simon Konstandin1, Robin Wilke1, Diego Betancourt2, Thomas Bertuch2, Juergen Jenne1,3, Reiner Umathum1,3, and Matthias Guenther1,4 | ||
1Fraunhofer MEVIS, Bremen, Germany, 2Fraunhofer FHR, Wachtberg, Germany, 3German Cancer Research Center DKFZ, Heidelberg, Germany, 4MR Imaging and Spectroscopy, Faculty 01, University of Bremen, Bremen, Germany |
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Smart metasurfaces, special two-dimensional metamaterial devices, have a huge potential to drastically improve imaging efficiency in MRI and are a promising tool to overcome some of the limitations which are hampering technological advances in the field. The design, simulation, and experimental verification of thin, smart, non-linear metasurfaces is presented, which yield an up to eightfold enhanced signal-to-noise ratio in 3T MRI. The smart metasurface is a system of two inductively coupled structures, one of which has a non-linear, incident power-dependent behavior. On-bench characterization and MRI scans with a homogeneous phantom and a kiwi fruit prove the functionality and working principle. |
1404 | High dielectric sheet to reduce electric fields in Self-decoupled radiofrequency coils for magnetic resonance imaging | |
Aditya Ashok Bhosale1 and Xiaoliang Zhang1 | ||
1Biomedical Engineering, State University of New York, Buffalo, Buffalo, NY, United States |
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Self-decoupled radiofrequency coils reduce the electromagnetic coupling between the coil elements and eliminate the use of complex decoupling technologies. The use of a small value capacitor (Cmode) in a self-decoupled coil helps in eliminating the coupling between coil elements but causes a large electric field across the Cmode capacitor1.which may potentially cause a safety problem during imaging. In this study, we propose the use of a high dielectric sheet to reduce the electric field across the capacitor and thereby reducing the higher SAR in the subject. |
1405 | Lightweight metasurface pads for passive RF shimming in 3T abdominal imaging | |
Tania del Socorro Vergara Gomez1,2, Marc Dubois1,2,3, Pierre Jomin2, Megdouda Benamara3, Djamel Berrahou3, Elodie Georget3, Tryfon Antonakakis3, David Bendahan1, Frank Kober1, Stefan Enoch2, and Redha Abdeddaim2 | ||
1Aix Marseille Univ, CNRS, CRMBM, Marseille, France, 2Aix Marseille Univ, CNRS, Centrale Marseille, Institut Fresnel, Marseille, France, 3Multiwave Imaging, Marseille, France |
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Abdominal imaging at 3T suffers from B1+ inhomogeneities due to radiofrequency (RF) wavelength reduction. High permittivity dielectric pads have been introduced as suitable solution to this problem. Such pads can require up to a few kilograms of ceramic powder usually dispersed in water. This could be detrimental to patient comfort during examination. Here we present a new approach based on thin, lightweight and flexible metasurface pads. The pads are shown to improve transmit and receive efficiency together with SNR in vitro. |
1406 | Passive Tunable RF Leakage Canceller for Simultaneous Transmit and Receive (STAR) RF Coils at 1.5T Imaging | |
Zachary Colwell1, Djaudat Idiyatullin2, Lance DelaBarre2, Thomas Vaughan3, Michael Garwood2, and Sung-Min Sohn1 | ||
1School of Biological and Health Systems Engineering, Arizona State University, Tempe, AZ, United States, 2Center for Magnetic Resonance Research, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 3Zuckerman Institute, Columbia University, New York, NY, United States |
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Simultaneous Transmit and Receive (STAR) requires high decoupling between the RF transmitter and receiver. Current methods for this include, but are not limited to: geometric isolation, active RF leakage cancellation and metamaterial decoupling. The presented method uses a passive, four-port, tunable canceller circuit to achieve upwards of 40 dB of isolation between a quadrature transmit coil pair and the single receiving coil for a 1.5T system. |
1407 | Gallium nitride MOSFETs enable transmit-receive switching in less than 100ns | |
Christoph Michael Schildknecht1, Markus Weiger1, Romain Froidevaux1, and Klaas Paul Pruessmann1 | ||
1Institute for Biomedical Engineering, ETH Zurich and University of Zurich, Zürich, Switzerland |
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For short-T2 MRI measurements, fast T/R switches that can handle high RF power are of paramount importance. In this work, we present a T/R switch based on GaN MOSFETs that switches in tens of nanoseconds and can handle a peak power of more than 1000W. |
1408 | Galvanically Isolated RF Switches for Low Field MRI | |
Mike Twieg1 | ||
1Hyperfine Research, Guilford, CT, United States |
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RF switches occupy many roles in MRI RF systems, including spoiling, damping, transmit/receive (T/R) switches, digital tuners, and crossbar switches. For high field MRI, PIN diodes are the switching device of choice, but at low field strength FETs are attractive. However, implementing the typical drive circuitry for the switch is difficult at lower frequencies. Here we describe a novel drive circuit suitable for a broad frequency range. It does not rely on any ferrous materials, or any high frequency oscillating circuits, and is thus suitable for use on the coil. |
1409 | UWB antenna system fidelity investigation for wireless MRI | |
Wonje Lee1, Fraser Robb2, John Pauly3, Shreyas Vasanawala1, and Greig Scott3 | ||
1Pediatric Radiology, Stanford University, Palo Alto, CA, United States, 2GE Healthcare, Aurora, OH, United States, 3Electrical Engineering, Stanford University, Palo Alto, CA, United States |
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We assess the effect of UWB antenna arrangement within a simulated bore environment that includes a pediatric human phantom using system fidelity factor calculations for wireless data link integrity |
1410 | Flexible Tunable Capacitor: A Variable Capacitor for Tuning Flexible/Thermoformed MRI Coils | |
Julian Adolfo Maravilla1, Karthik Gopalan1, Ana Claudia Arias1, and Michael Lustig1 | ||
1EECS, UC Berkeley, Berkeley, CA, United States |
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Recent advances in coil design and fabrication have allowed for flexible and thermoformed coil arrays. However, the weak solder joints and rigid design of traditional variable capacitors used with these coils greatly limit their flexibility. Here, we propose the Flexible Tunable Capacitor (FTC), a high-Q, flexible, easily tunable variable capacitor. This design uses an array of small low-loss parallel plate capacitors adjustable with small step sizes by exploiting series and parallel combinations. This work proposes a basic design that offers a wide range of capacitor values (0.5 pF to 7 pF) suitable for 3T and 7T coils. |
1411 | Rapid high power transmit-receive switching using a timed cascade of PIN diodes | |
Christoph Michael Schildknecht1, Markus Weiger1, Romain Froidevaux1, and Klaas Paul Pruessmann1 | ||
1Institute for Biomedical Engineering, ETH Zurich and University of Zurich, Zürich, Switzerland |
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For imaging of short-T2 samples often very short excitation pulses are desired, which requires high peak RF power. In this work, a transmit-receive switch is presented that can handle 18kW peak RF power and switches its state in less than 1µs. The novel design uses a timed cascade of anti-parallel PIN diode pairs to achieve this performance. |
1412 | Analysis of preamplifier decoupling effect in MRI coil array with electromagnetic field and RF circuit co-simulation | |
Ming lu1,2, Bei Zhang3, John C. Gore1,2, and Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Vanderbilt University Medical Center, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University Medical Center, Nashville, TN, United States, 3Advanced Imaging Research Center, University of Texas Southwestern Medical Center, Dallas, TX, United States |
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Preamplifier decoupling is a standard way of suppressing inter-element inductive coupling in MRI receive arrays. A well-known method to evaluate and optimize RF coils before practical fabrication is to use circuit-level and electromagnetic (EM) field-level simulations. However, to be best of our knowledge, currently there is not a solid method to evaluate the preamp decoupling effect with circuitry and EM field analysis. In this work, we used RF circuit and EM co-simulation4 to evaluate the preamplifier decoupling effect and tested it on the conventional coil (LIC) and the recently introduced high impedance coil (HIC). |
1413 | Should coaxial coils be operated at their self-resonance? A simulation study | |
Sigrun Roat1, Andre Kuehne2, Lena Nohava1,3, and Elmar Laistler1 | ||
1High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria, 2MRI.TOOLS GmbH, Berlin, Germany, 3CEA, CNRS, Inserm, BioMaps (Laboratoire d'Imagerie Biomédicale Multimodale Paris Saclay), Université Paris-Saclay, Orsay, France |
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Flexible RF coils gained large interest in recent years. One possibility to achieve flexibility is using transmission line resonator-type coils made from coaxial cable. These self-resonant structures can be constructed without lumped elements along the loop enhancing flexibility. No consensus has been reached yet whether these coils should be driven at their respective self-resonance. To investigate this question, we have performed a simulation study investigating 11 different setups at 3 frequencies each |
1414 | Conformal design of radio-frequency head coil for ultra-high field MRI | |
Tiago Martins1, Tales Santini1, Jacob Berardinelli1, Anthony DeFranco1, and Tamer S Ibrahim1 | ||
1University of Pittsburgh, Pittsburgh, PA, United States |
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In this work, we explore a conformal Tic Tac Toe (TTT) head coil design for ultra-high field MRI. By conforming the antennas to the human head, we can extract better homogeneity allowing for better radiofrequency shimming. The comparison between the traditional TTT design and the conformal TTT design shows expanded coverage, reduction of the coefficient of variation by 0.4% and same intensity for the 16-channel version. The conformal designs are extremely flexible as its advantages can be explored for different configurations and sizes. |
1415 | Safety and imaging performance of 2-channel RF shimming for fetal MRI at 3T | |
Filiz Yetisir1, Esra Abaci Turk1,2, P. Ellen Grant1,2,3, Elfar Adalsteinsson4,5, and Lawrence L. Wald3,5,6 | ||
1Fetal-Neonatal Neuroimaging and Developmental Science Center, Boston Children's Hospital, Boston, MA, United States, 2Department of Pediatrics, Harvard Medical School, Boston, MA, United States, 3Department of Radiology, Harvard Medical School, Boston, MA, United States, 4Department of Electrical Engineering and Computer Science, Massachusetts Institute of Technology, Cambridge, MA, United States, 5Harvard-MIT Division of Health Science and Technology, Massachusetts Institute of Technology, Cambridge, MA, United States, 6Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States |
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3T MRI provides increased SNR but poses technical challenges for fetal imaging such as increased field inhomogeneity and SAR. RF shimming can address some of these challenges but also adds safety considerations. Using a diverse set of 5 numerical pregnant body models generated from patient MRI datasets, we found that 2-channel RF shimming can improve transmit field amplitude and uniformity by up to 19% and 36% respectively without increasing maternal or fetal SAR. The biggest difference in SAR and transmit field patterns was observed between the supine models and the left lateral model. |
1416 | Stabilization of bias field on 3D MPRAGE at 7T with dielectric pads and 3D-based B1+ scaling | |
Giske Opheim1, Vincent O. Boer2, Esben Thade Petersen2,3, Martin Prener1, Olaf B. Paulson1,4, and Jan Ole Pedersen5 | ||
1Neurobiology Research Unit, Dept. of Neurology, Copenhagen University Hospital Rigshospitalet, Copenhagen, Denmark, 2Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Hvidovre, Denmark, 3Section for Magnetic Resonance, DTU Health Tech, Technical University of Denmark, Kgs. Lyngby, Denmark, 4Faculty of Health and Medical Sciences, University of Copenhagen, Copenhagen, Denmark, 5Philips Healhtcare, Copenhagen, Denmark |
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7T MRI has several cases of demonstrated clinical yield, but is challenged by spatial B1 inhomogeneity. Bias fields in structural images may be acceptable for visual and computational analysis, and can to some extent be accounted for by bias-field corrections. However, this is significantly complicated since the characteristics of the bias field often varies between patients. By analyzing stability of bias fields in 3D MPRAGE images, we compared two dielectric pad setups and the impact of 3D-based B1+ scaling, i.e., optimization of the RF gain. We found increased stability by using large pads and 3D-based B1+ scaling in combination. |
1417 | The impact of B1+ on the optimisation of high-resolution ASL acquisitions at 7T | |
Sriranga Kashyap1, Roy A. M. Haast2, Thomas F. Kirk3, An T. Vu4,5, Denizhan Kurban1, Ron Hellenbrand1, Christopher J. Wiggins6, Alard Roebroeck1, Ali R. Khan2, David A. Feinberg1,7,8, Benedikt A. Poser1, and Dimo Ivanov1 | ||
1Department of Cognitive Neuroscience, Maastricht University, Maastricht, Netherlands, 2Centre for Functional and Metabolic Mapping, Western University, London, ON, Canada, 3University of Oxford, Oxford, United Kingdom, 4University of California, San Francisco, CA, United States, 5San Francisco Veteran Affairs Health Care System, San Francisco, CA, United States, 6Scannexus B.V., Maastricht, Netherlands, 7Advanced MRI Technologies, Sebastopol, CA, United States, 8Helen Wills Neuroscience Institute, University of California, Berkeley, CA, United States |
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In this 7T study, we examined potential causes of apparent absence of perfusion in the right inferior temporal lobe, by (i) assessing the B1+ distributions on two 1Tx/32Rx head-coils to rule out a hardware source, and (ii) optimising the spatial positioning of dielectric pads to achieve a more symmetric B1+ field. We observed that using an optimised dielectric pad positioning allows for a near whole-brain symmetric B1+, thereby, ensuring the adiabatic condition for the inversion pulse is fulfilled, resulting in the robust measurement of perfusion in the right temporal lobes. |
1418 | Is it feasible to Make More Effective Use of Finite RF Power Resources in pTx Systems Using a Coupling Matrix? | |
Stephen E. Ogier1, Shaihan Malik1, and Joseph Hajnal1,2 | ||
1Biomedical Engineering Department, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 2Centre for the Developing Brain, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom |
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Parallel transmit using equal numbers of RF power amplifiers and coil elements has emerged as a common way to improve the homogeneity of the transmit field through RF shimming. When performing RF shimming, in many cases the magnitude of the transmit field is limited by the maximum power limit of a single RF amplifier. We propose networks that can be used to share power between transmit channels, increasing the maximum transmit field. These networks are shown to provide substantial flexibility in RF power allocation for certain conditions on the relative phases of the channels. |
1419 | Design of transmit array coils by minimizing the modal reflected power values and increasing B1+ efficiency | |
Ehsan Kazemivalipour1,2, Giorgio Bonmassar3, Laleh Golestanirad4,5, and Ergin Atalar1,2 | ||
1Electrical and Electronics Engineering Department, Bilkent University, Ankara, Turkey, 2National Magnetic Resonance Research Center (UMRAM), Bilkent University, Ankara, Turkey, 3AA. Martinos Center, Massachusetts General Hospital (MGH), Harvard Medical School, Boston, MA, United States, 4Department of Radiology, Feinberg School of Medicine, Northwestern University, Chicago, IL, United States, 5Department of Biomedical Engineering, McCormick School of Engineering, Northwestern University, Evanston, IL, United States |
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The vast majority of RF coil design techniques are based on reducing the coupling level to increase the coils' power efficiency. The assessment of scattering (S) parameters plays a crucial role in these techniques. However, just by checking S-parameters, we cannot be sure that the coil's accepted power generates a field with useful characteristics. Here, we propose to perform the co-simulation on transmit array coils and replace unknown capacitors with power sources. Extraction of the field profiles of the coil's lumped ports/elements could provide the opportunity to involve the field-dependent parameters in the minimization procedure of finding the coil's capacitors. |
1420 | Brain perfusion imaging using pseudo-continuous arterial spin labelling MRI: impact of RF coil shimming of the labelling region | |
Sofia Guterres1, Ana Rodrigues Fouto1, Nuno André Silva2, Pedro Vilela3, and Patrícia Figueiredo1 | ||
1Institute for Systems and Robotics - Lisboa and Department of Bioengineering, Instituto Superior Técnico, Universidade de Lisboa, Lisboa, Portugal, 2Hospital da Luz Learning Health, Lisboa, Portugal, 3Hospital da Luz, Lisboa, Portugal |
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The labelling efficiency of pCASL perfusion imaging sequences can be hampered by B0 field inhomogeneities. We assessed the impact of shimming the labelling region using a commercial RF coil with dedicated shiming channels in the neck, on data acquired from healthy volunteers. Brain perfusion was quantified, as well as the labelling efficiency (based on B0 fieldmaps and numerical simulations). Simulation experiments show that labelling efficiency significantly depends on B0 field inhomogeneity. In vivo experiments, however, showed subtle inhomogeneity reduction within the arteries in the labelling region, yielding no significant improvements in pCASL labelling efficiency or the respective perfusion signal. |
1421 | The Impact of Quasi-Transverse Electric Modes Excited by Dipole Antennas on Transmit Field in In Vivo Ultrahigh Field MRI | |
Daniel Wenz1,2 and Rolf Gruetter1,3 | ||
1CIBM Center for Biomedical Imaging, Lausanne, Switzerland, 2Animal Imaging and Technology, Ecole Polytechnique Federale de Lausanne (EPFL), Lausanne, Switzerland, 3Laboratory of Functional and Metabolic Imaging (LIFMET), Ecole Polytechnique Federale de Lausanne (EPFL), Lausanne, Switzerland |
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This work investigates quasi-transverse electric modes which can be excited within rectangular dielectric blocks which are often used to shorten dipole antennas for MRI at 7T. In simulations we studied different parameters which can affect the performance of a dielectrically-shortened dipole antenna. We showed that an optimal geometry for the case when the block and the sample are physically separated differs significantly from the case when perfect direct contact is achieved. Two prototypes were built and used in an in vivo MRI experiments involving one subject showing how different dielectric modes can affect the image quality. |
1422 | A Novel High Density 32-channel Sleeve Antenna Receiver Array for the Human Head Imaging at 10.5 T | |
Myung Kyun Woo1, Lance DelaBarre1, Matt Waks1, Russell Lagore1, Jeromy Thotland1, Uk-Su Choi2, Andrea Grant1, Steve Jungst1, Nader Tavaf1, Yigitcan Eryaman1, Kamil Ugurbil1, and Gregor Adriany1 | ||
1Center for Magnetic Resonance Research, Minneapolis, MN, United States, 2Center for Information and Neural Networks, Osaka, Japan |
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We designed an elliptically arranged novel 32-channel Sleeve antenna receiver array for human whole brain imaging at 10.5 tesla. To demonstrate the signal-to-noise ratio (SNR) performance of this array, we evaluated and compared it with a standard 32-channel loop receiver array. |
1423 | Combining Loops and Dipoles to Increase the Signal-to-Noise Ratio in Human Brain MRI at 7T: How to Shorten a Dipole Antenna? | |
Thomas Dardano1, Rolf Gruetter1,2, and Daniel Wenz2,3 | ||
1Laboratory of Functional and Metabolic Imaging (LIFMET), Ecole Polytechnique Federale de Lausanne (EPFL), Lausanne, Switzerland, 2CIBM Center for Biomedical Imaging, Lausanne, Switzerland, 3Animal Imaging and Technology, Ecole Polytechnique Federale de Lausanne (EPFL), Lausanne, Switzerland |
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Dipole antennas can be used in multi-channel loop/dipole arrays to boost the signal-to-noise ratio in MRI at 7T (f=300MHz). For this purpose, dipole antennas need to be physically shorter. In this work we conducted electromagnetic field simulations and phantom experiments at 7T to compare the performance of an inductively-shortened dipole antenna with a dielectrically-shortened dipole antenna in a loop/dipole combination. We evaluated the performance of both designs in different loading conditions and we found that the dielectrically-shortened dipole antenna performed in a very robust manner providing apparent receive field gains when compared with its inductively-shortened counterpart. |
1424 | Optimization of a massive-element self-decoupled transmit array for 7T head imaging | |
Ming Lu1,2, John C. Gore1,2, and Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University Medical Center, Nashville, TN, United States |
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At high fields, B1 inhomogeneity is one of the major challenges that limit imaging performance. Parallel transmission with an array of coils is a recognized solution to B1 inhomogeneity. The self-decoupled coil is attractive in Tx array design since it exhibits intrinsic inter-element isolation that may ease the coil fabrication, and allows the dipole mode as well as loop mode. In this work, we evaluated a series of self-decoupled coils in terms of these parameters and aimed to provide guidance for the practical building of a high-performance self-decoupled Tx array. |
1425 | High-density 72-channel head array at 7Tesla | |
Mark Gosselink1, Tijl van der Velden1, Hans Hoogduin1, Martijn Froeling1, and Dennis W. J. Klomp1 | ||
1University Medical Center Utrecht, Utrecht, Netherlands |
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A 64 channel head coil receiver is presented that operates with low noise coupling inside a continuously tuned 8-channel transceiver coil. When used as a 72-channel receiver the setup outperforms the default 32 channel receiver array in acceleration, demonstrated by high-resolution MPRAGE images of the human brain. |
1426 | A 30-element transmit array for 7 Tesla brain imaging with array compressed parallel transmission | |
Charlotte Sappo1,2, Gary R Drake1,3, Xinqiang Yan1,3, and William A Grissom1,2,3,4 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 3Radiology, Vanderbilt University, Nashville, TN, United States, 4Electrical and Computer Engineering, Vanderbilt University, Nashville, TN, United States |
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A dense array is desirable for ultra-high field in parallel transmission to better mitigate B1+ field inhomogeneities and control specific absorption rate. Most ultra-high field scanners are limited by the existing number of transmit channels. This limitation can be overcome using array-compressed parallel transmission (acpTx) which enables a small number of channels to drive a large number of coils. This work describes the construction of a 30-loop head transmit array using a mixed overlapped and self-decoupled design with a widely-used commercial 32-channel receive insert for human imaging applications. |
1427 | SNR of Flexible Versus Rigid Coil Arrays for Knee MRI | |
Jeremiah Hess1, Marianne Black2, Feliks Kogan2, and Brian Hargreaves1,2,3 | ||
1Department of Bioengineering, Stanford University, Stanford, CA, United States, 2Department of Radiology, Stanford University, Stanford, CA, United States, 3Department of Electrical Engineering, Stanford University, Stanford, CA, United States |
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Flexible extremity coil-arrays for knee imaging in MRI can improve coil positioning and comfort to patients in the scanner and wrap tightly around the knee, placing coil elements close to anatomy of interest. Despite this, flex coils have not been widely adapted due to perceived superiority of the SNR of transmit-receive coils. In this study, we analyzed the SNR of flex coil-arrays versus a rigid coil-array in phantom and in vivo to determine which coil-arrays had improved SNR. Preliminary results suggest that flexible coil-arrays show comparable or increased SNR and generally more uniform SNR over rigid coil-arrays. |
1428 | Reduction of coupling and noise by ultrahigh dielectric constant (uHDC) materials for phase array coil at 3T | |
Navid PourramzanGandji1, Christopher T. Sica2, Gary W. Yang3, Hannes Wiesner4, Soo Han Soon4, Xiao-Hong Zhu4, Michael Lanagan5, Wei Chen4, and Qing X. Yang1 | ||
1Neurosurgery, Pennsylvania State University, Hershey, PA, United States, 2Radiology, Pennsylvania State University, Hershey, PA, United States, 3Pennsylvania State University, Hershey, PA, United States, 4Center for Magnetic Resonance Research, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 5Materials Science and Engineering, Pennsylvania State University, State College, PA, United States |
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Prior work has examined the effects of uHDC material upon phased array coils. Several beneficial effects have been observed: reduction of per-channel noise and inter-channel noise correlations, and enhancement of SNR. Due to the high dielectric constant the electric field will be confined to the dielectric material, which leads to a reduction of the primary noise source, the conservative electric field. As a result the non-conservative field becomes more dominant within the sample, with a resulting increase of B1 field intensity and more substantial SNR enhancement. |
1429 | A novel characterization method of HTS non-linear electrical properties using MRI | |
Aimé Labbé1, Isabelle Saniour1, Rose-Marie Dubuisson1, Jean-Christophe Ginefri1, Luc Darrasse1, and Marie Poirier-Quinot1 | ||
1Université Paris-Saclay, CEA, CNRS, Inserm, BioMaps, Orsay, France |
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Decoupling is a major technological challenge of High-Temperature Superconducting (HTS) surface coils. A promising strategy is to exploit nonlinearities in the HTS coil electric response to achieve decoupling. In this work, we present a new characterization method allowing the evaluation of these nonlinearities using MRI. We first present the theoretical model behind this approach; we then proceed to use it on 3D images of a water phantom in the vicinity of a copper coil and then a HTS coil to validate the model through the extraction of the quality factor Q, compared to the one measured by alternative methods. |
1430 | Robot Assisted Dynamic Ankle Joint Imaging with a Wearable 4-Channel High Impedance Coil at 1.5T MRI | |
Matthäus Poniatowski1, Ilan Elias2, Mirsad Mahmutovic1, Gurinder Multani1, Sam-Luca J.D. Hansen1, Markus W. May1, Alexander M. König3, Jens H. Figiel3, Andreas H. Mahnken3, and Boris Keil1 | ||
1Institute of Medical Physics and Radiation Protection, TH Mittelhessen University of Applied Sciences, Gießen, Germany, 2Motionrad GmbH, Berlin, Germany, 3Department of Diagnostic and Interventional Radiology, Philipps-University Marburg, Marburg, Germany |
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Limitations of conventional MRI include its lack of ability to observe controlled joint motion and biomechanics in real-time. Although clinically evident, many injuries, instabilities, and dysfunctions of the musculoskeletal system are frequently not depicted on conventional static MRI. To enable dynamic MRI for joints, an in-bore motion-assisted device and a wearable coil array was designed, constructed, and validated. The combination of robotic assisted joint motion, a tight-fitting coil array that does not restrict the joint's range of motion, and accelerated imaging enabled dynamic MRI of the ankle. |
1571 | Design and evaluation of a 2-Tx 24-Rx coil for 5T knee MR imaging | |
Shao Che1, Junjun Qin1, Shihong Han1, and Ye Li2 | ||
1United Imaging Healthcare, Shanghai, China, 2Lauterbur Imaging Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Science, Shanghai, China |
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Musculoskeletal imaging is one widely used MR application with advantages in exquisite details of anatomic structure, rich contrast options for various soft tissues and high diagnostic accuracy [1]. The SNR gain of high field MRI can further help extending such applications as magnetic resonance knee imaging. A 2-channel birdcage transmit and 24-channel loop array receive coil is designed and evaluated on the novel whole body 5T MRI scanner (United Imaging Healthcare, Shanghai, China, abbreviated as UIH below). The imaging performance is compared with a 3T scanner and the results are discussed. |
1572 | In-vivo human brain imaging at 5 T using a 48 channel Tx-Rx array | |
Ye Li1,2, Zidong Wei1,2,3, Shihong Han3, Shuheng Zhang3, Qiang He3, Xiaoliang Zhang4, Xin Liu1,2, and Hairong Zheng1,2 | ||
1Lauterbur Imaging Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, 2Key Laboratory for Magnetic Resonance and Multimodality Imaging of Guangdong Province, Shenzhen, China, 3United Imaging Healthcare, Shanghai, China, 4Department of Biomedical Engineering, State University of New York at Buffalo, NY, NY, United States |
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Intermediate field strength between 3 T and 7 T may provide significant signal-to-noise ratio improvement but with less radio frequency challenges. In this work in-vivo human brain images including anatomic images, angiography images and susceptibility weighted images have been acquired at a prototype 5 T whole body scanner using a 48 channel Tx-Rx array, and compared with those at 3 T commercial scanner. Significant signal-to-noise ratio improvement of 5 T has been shown while image homogeneity is still acceptable. |
1573 | An 8-channel transmit loop array for body imaging at 5T | |
Fuyi Fang1, Wei Luo1, Jingxia Gong1, Rongxing Zhang1, Zidong Wei2, and Ye Li2 | ||
1United Imaging Healthcare, Shanghai, China, 2Lauterbur Imaging Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China |
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In this study, an 8-channel (8ch) loop and a 2-channel (2ch) birdcage in 5T frequency are built and compared. Basic electrical characteristics, engineering issues in implementation, transmitting efficiency, perturbation sensitivity, B1+ uniformity and local SAR are compared between these two coils. Measurement result of the B1+ distribution in torso region with these coils are obtained from a whole body 5T MRI scanner.
|
1574 | Robust decoupling of a 7 Tesla 8-channel loop array for head and cervical spinal cord imaging | |
Bei Zhang1, Abbas Zaki2, Daniel Lowrance2, Ivan Dimitrov1,3, Binu Thomas1, Andreas Pfrommer4, and Anke Henning1,4 | ||
1Advanced Imaging Research Center, University of Texas Southwestern Medical Center, Dallas, TX, United States, 2Erik Jonsson School of Engineering and Computer Science at The University of Texas at Dallas, Richardson, TX, United States, 3Philips Healthcare, Gainesville, FL, United States, 4Max Planck Institute for Biological Cybernetics, Tuebingen, Germany |
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With the guidance of our in-house analytical modeling tool that was developed originally for minimizing both electrical coupling and magnetic coupling , we designed a 7T 8-channel T/R array with robust decoupling performance for both head and cervical spinal cord imaging, and our 7T 8 channel array demonstrated robust decoupling performance for both head and cervical spine cord imaging in both simulations and experiments. |
1575 | Effect on SAR and Transmit Efficiency by Geometrical Configuration of RF Transmit Head Coil for 7 T MRI | |
Youngdae Cho1 and Hyoungsuk Yoo1 | ||
1Electronic Engineering, Hanyang University, Seoul, Korea, Republic of |
||
As the risk of RF heating in UHF MRI due to high specific absorption rate (SAR), recent work to design the coil focused to reduce SAR. In this study, the impact of the geometrical shape of the multi-channel RF head coil on the transmit efficiency (TE) and SAR efficiency (SE) was analyzed. Four different configurations of the head coil were simulated. it is evident from the results that a coil configuration similar to the head shape is required to optimize the TE and SE simultaneously. |
1576 | A dipole antenna array with “flipped” high dielectric constant (HDC) material for improved SNR at 10.5 Tesla | |
Myung Kyun Woo1, Lance DelaBarre1, Russell Lagore1, Steve Jungst1, Michael T Lanagan2, Thane Bonnett2, Qing X Yang2, Riccardo Lattanzi3, Kamil Ugurbil1, and Gregor Adriany1 | ||
1Center for Magnetic Resonance Research, Minneapolis, MN, United States, 2Penn state University, Centre County, PA, United States, 3Radiology at NYU Grossman School of Medicine, New York University, New York, NY, United States |
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In the previous work, we evaluated the transmit performance of 10.5 T RF coils composed of dipole antennas and high dielectric constant (HDC) ceramic materials with a “Normal” (Dipole - HDC - Sample) and a counterintuitive “Flipped” geometry (HDC – Dipole - Sample) positioning. Now we evaluated the receive performance of such an array structure with these setups both in simulations and experiments. The “flipped” setup showed notable periphery SNR improvement and suggest some promise for the UHF receiver arrays. |
1577 | Development of a Dedicated Mono-surface 16-Element Transceiver Dipole Antenna Array for Parallel Transmission Cardiac MRI in Pigs at 7 Tesla | |
Ibrahim A. Elabyad1, Maxim Terekhov1, Michael Hock1, David Lohr1, and Laura M. Schreiber1 | ||
1Chair of Molecular and Cellular Imaging, Comprehensive Heart Failure Center (CHFC), University Hospital Wuerzburg, Wuerzburg, Germany |
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To improve parallel imaging performance for cardiac MRI in pigs at 7T, a dedicated transceiver 16-element antisymmetric dipole antenna array was developed and tested. EMF-simulations were performed with the antisymmetric dipole array loaded with a dedicated pig thorax-shaped phantom. Imaging performance of the dipole array was validated through MR-measurements in a pig phantom and an 85kg pig cadaver. The dipole array demonstrated a threefold improvement in coefficient-of-variation of the measured FA maps after $$${B_1^+}$$$-shimming using the vendor integrated pTx-platform. Parallel imaging with acceleration factor up to R=4 was possible while maintaining a mean g-factor of 1.13 within the pig heart. |
1578 | Design of a 19-Channel hybrid array system for Foot/Ankle Imaging at 7T | |
Aditya Ashok Bhosale1, Leslie L Ying1, and Xiaoliang Zhang1 | ||
1Biomedical Engineering, University at Buffalo, Buffalo, NY, United States |
||
Microstrips are being used in MR applications due to their unique properties such as reduced radiation loss, high frequency capability, and reduced perturbation of sample loading to the RF coil compared to conventional coils. In this study, we propose a 19-channel hybrid array consisting of 14 Microstrips and 5 loop coils placed on the foot/ankle phantom to cover maximum area of the subject at 7T. |
1579 | A 28-channel decoupled Tic-Tac-Toe transmit radiofrequency coil for 7T MRI | |
Tales Santini1, Anthony DeFranco1, Tiago Martins1, Andrea Sajewski1, Howard J. Aizenstein1, and Tamer S. Ibrahim1 | ||
1University of Pittsburgh, Pittsburgh, PA, United States |
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In this work, we investigated the potential of the smaller sizes of the Tic-Tac-Toe transmit coil elements, comparing the newly developed uncoupled configuration with the traditional coupled version of this RF coil design. Simulations with 14 Tic-Tac-Toe panels showed excellent levels of transmit field homogeneity at 7T (coefficient of variation = 12.6%, average = 0.28µT for 1W) while maintaining low levels of SAR (SAR efficiency = 1.41 µT/√(W/Kg)). The simulations were validated with phantom experiments. Future work includes the assembling of the 28-channel transmit coil and the investigation of the optimal power splitting strategy. |
1580 | A Comparative Study Highlighting a Novel UHF MRI Volume Body Coil Design | |
Sayim Gokyar1, Henning U. Voss1, Victor Taracila2, Fraser J. L. Robb2, Douglas J. Ballon1, and Simone Angela Winkler1 | ||
1Radiology, Weill Cornell Medicine, New York, NY, United States, 2General Electric Healthcare, Aurora, OH, United States |
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We designed a novel 2D cylindrical high-pass ladder (c-HPL) volume body coil by adding a second dimension in S-I direction to the 1D birdcage concept, given that the latter fails at 7T body dimensions. We compared its performance to the (non-functional) 1D birdcage and transverse electromagnetic (TEM) designs. In silico results showed improved B1 homogeneity (inhomogeneity of 15.9%) with lower specific absorption rate (SAR) and better SAR efficiency (0.743 μT/W∙√kg). The proposed architecture is a promising candidate for UHF MRI applications where the current lack of a built-in body coil hinders the modality from gaining full clinical acceptance/approval. |
1581 | Asymmetric ring birdcage coil for volume excitation | |
Hideta Habara1 and Shinichiro Suzuki1 | ||
1Healthcare Business Unit, Hitachi, Ltd., Tokyo, Japan |
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Design of asymmetric ring diameter birdcage volume coil has been studied by electromagnetic filed simulations. Even if the diameter of the front and the rear rings of the birdcage coil is changed to some extent with respect to the cylindrical RF shield, the uniformity in the Z direction can be maintained by changing the width of the front and rear rings. Increasing the gap between the ring and the RF shield has an advantage in efficiency even applied on one side of the ring. |
1582 | Toward Enhanced Transmit Performance of Rectangular Dielectric Resonator Antenna Arrays for 7-T MRI Using Loop/Dipole Coupling Scheme | |
Daniel Wenz1,2 | ||
1CIBM Center for Biomedical Imaging, Lausanne, Switzerland, 2Animal Imaging and Technology, Ecole Polytechnique Federale de Lausanne (EPFL), Lausanne, Switzerland |
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This study investigates a loop-dipole coupling scheme as a new approach to excite orthogonal dielectric modes in a rectangular dielectric resonator antenna for MRI at 7T. A rectangular dielectric resonator antenna was simulated, built and its performance was evaluated in phantom experiments using two coupling schemes: dipole-only and loop-dipole. It was found that the loop-dipole coupling scheme can substantially enhance not only transmit performance of a single element, but also of an array of rectangular dielectric resonator antennas (transmit field efficiency gain of 35%). |
1583 | Development of a Microstrip Tx Coil Module for 7T MRI | |
Andrea N Sajewski1, Tales Santini1, Matthew Saich1, Tiago Martins1, and Tamer S Ibrahim1 | ||
1University of Pittsburgh, Pittsburgh, PA, United States |
||
A 7T microstrip RF coil was designed based on the Tic-Tac-Toe (TTT) concept that has previously shown homogeneity and load-insensitivity. Simulations were performed to compare B1+ distributions between the microstrip TTT and standard TTT coils. A 4-channel microstrip coil was assembled and B1+ maps were acquired at 7T. Nearly equivalent B1+ distributions were observed, indicating the potential for using a highly dense microstrip array to provide excellent homogeneity and reduction of SAR while enabling unique designs, such as conforming to the anatomy of interest. |
1584 | New commercial 8Tx/16RX array for Clinical 7T Cardiac MRI: initial experience | |
Maxim Terekhov1, David Lohr1, Theresa Reiter2, Ibrahim A. Elabyad1, Michael Hock1, and Laura M. Schreiber1 | ||
1Chair of Molecular and Cellular Imaging, University Hospital Würzburg, Comprehensive Heart Failure Center, Wuerzburg, Germany, 2Department of Internal Medicine I, Cardiology, University Hospital Würzburg, Wuerzburg, Germany |
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7T cardiac MRI is a novel field with the potential to increase the physical sensitivity and diagnostic value of the clinical cardiac images. Multiple elements transmit/receive phased array coils in combination with parallel transmit RF-technology allow for an improvement of the image quality at ultra-high-field (B0≥7T) field strength. In this work, we present initial experience with a new commercial 8Tx/16Rx thorax array coil operating in a “pTX-Compatibility Mode” of the scanner for cardiac MRI at 7T. |
1585 | High power RF amplifier for UHF MRI with configurable number of channels | |
Jifeng Chen1,2, Ye Li1, Han Zhang2, Bin Cao2, Xin Liu1, Hairong Zheng1, and Xu Chu2 | ||
1Lauterbur Imaging Research Center, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, 2United Imaging Healthcare, Shanghai, China |
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Increasing magnetic field strength can improve signal-to-noise ratio (SNR) of MRI [1] and it requires higher power capability and fidelity from RF Power Amplifier (RFPA). Meanwhile, to reduce B1 inhomogeneity at high field usually requires multi-channel parallel transmission (pTx) technique. In this study, we present a method to design RFPA with high power capability and output linearity, and with configurable number of transmit channels so as to meet different RF coil and load requirements. |
1586 | Quadrature Tx/Rx wireless coil for targeted breast MRI at 1.5 T | |
Viktor Puchnin1, Anna Hurshkainen1, Anton Nikulin2, Georgiy Solomakha1, Anna Andreychenko1,3, and Alena Shchelokova1 | ||
1Department of Physics and Engineering, ITMO University, St. Petersburg, Russian Federation, 2Institut Langevin, ESPCI Paris, CNRS, PSL University, Paris, France, 3Research and Practical Clinical Center for Diagnostics and Telemedicine Technologies of the Moscow Health Care Department, Moscow, Russian Federation |
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We demonstrate for the first-time a quadrature transceive wireless coil for 1.5T targeted breast MRI. The proposed concept features two volumetric resonators: metamaterial-inspired structure and Helmholtz coil. These coils are electromagnetically coupled to the body birdcage coil and interact with its magnetic field’s components, thus boosting body coil transmit efficiency, SAR efficiency, and receive performance for the targeted area of the human breast. |
1587 | Circularly polarized coil for 1.5 T MRI RF harvesting | |
Pavel Seregin1, Georgiy Solomakha1, Egor Kretov2, Oleg Burmistrov1, and Alexey Slobozhanyuk1 | ||
1The Department of Physics and Engineering, ITMO University, Saint Petersburg, Russian Federation, 2Max Delbruck Center for Molecular Medicine in the Helmholtz Association, Berlin, Germany |
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The concept of the wireless power supply for the MRI coils demands high efficiency in a restricted volume. To meet these requirements, we investigated the possibility of harvesting the energy from the B1 field of a 1.5 T MRI scanner using a new volumetric coil design. We performed a series of experiments with the different positions of the proposed coil within the scanners bore and estimated the accepted power levels during the different types of MR pulse sequences. |
1588 | Development of Microstrip Coils Integrated with High Dielectric Constant (HDC) Material to Improve B1 Field and Performance of 1H MR imaging at 7T | |
Soo Han Soon1,2, Matt Waks1, Xiao-Hong Zhu1, Hannes M. Wiesner1, Navid P. Gandji3, Qing X. Yang3, Michael T. Lanagan4, and Wei Chen1 | ||
1CMRR, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 2Biomedical Engineering, University of Minnesota, Minneapolis, MN, United States, 3CNMRR, Department of Neurosurgery, Penn State University, Hershey, PA, United States, 4Department of Engineering, Penn State University, Hershey, PA, United States |
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The development of ultra-high-field (UHF) magnetic resonance imaging (MRI) and spectroscopy imaging (MRSI) technologies improves sensitivity and spatial resolution for biomedical and clinical applications. However, the limited inherent signal-to-noise ratio (SNR) is still challenging, especially for pushing spatiotemporal resolution even at UHF. Previous studies have shown that high dielectric constant (HDC) materials could provide a new RF engineering solution for the challenge. In this study, we introduce a novel microstrip transmission line (MTL) transceiver array that uses HDC material as substrate, and significantly improves the RF transmission (B1+) and reception (B1-) fields and SNR for 1H imaging application at 7T. |
1589 | A 2D High-Pass Ladder RF Coil Architecture for UHF MRI | |
Sayim Gokyar1, Henning U. Voss1, Victor Taracila2, Fraser J. L. Robb2, Michael Bernico3, Douglas Kelley3, Douglas J. Ballon1, and Simone Angela Winkler1 | ||
1Radiology, Weill Cornell Medicine, New York, NY, United States, 2General Electric Healthcare, Aurora, OH, United States, 3General Electric Healthcare Technologies, Waukesha, WI, United States |
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We propose a two-dimensional cylindrical high-pass ladder (2D c-HPL) volume coil architecture as a new class of radiofrequency coils to be used for 7T Body MR imaging. As a first simplified experimental proof-of-concept we show feasibility in a head sized coil. In silico results show 45% more homogeneous B1 field distribution with 25% lower specific absorption rate compared to a similar size birdcage coil. Experimental results are in good agreement with theory and numerical simulations. The proposed architecture shows promise to solve the longstanding open challenge of volume coil B1+ inhomogeneity in UHF MRI applications. |
1590 | Performance comparison of using an external 16-channel transmit array vs. using 16 elements of a 32-channel receive array as transceivers at 10.5 T | |
Bei Zhang1, Gregor Adriany2, Navid Pourramzan Gandji3, Qing X. Yang3, Brian Rutt4, Jeramie Radder2, Lance DelaBarre2, Myung Kyun Woo2, Kamil Ugurbil2, and Riccardo Lattanzi5,6 | ||
1Advanced Imaging Research Center, UT Southwestern Medical Center, Dallas, TX, United States, 2Center for Magnetic Resonance Research, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 3Department of Radiology, Pennsylvania State College of Medicine, Hershey, PA, United States, 4Department of Radiology, Stanford University, Stanford, CA, United States, 5Center for Advanced Imaging Innovation and Research (CAI2R) and Bernard and Irene Schwartz Center for Biomedical Imaging, Department of Radiology, New York University School of Medicine, New York, NY, United States, 6The Vilcek Institute at NYU Langone Health, New York, NY, United States |
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Shielding effects associated with surrounding the receive array with an external transmit (Tx) array could decrease the signal-to-noise ratio (SNR) at 10.5 T. Two Tx approaches were compared: using 16 receive elements as transceivers vs. using a 16-channel external transmit array. For both cases, the effect of using high-permittivity material (HPM) was evaluated. Our simulation results showed that performance was larger for the transceivers and further increased with HPM. This suggests that the additional complexity associated with constructing a multi-element transceiver array compared to using an external transmitter could be justified for 10.5T imaging by the expected gain in performance. |
1591 | Ultra-Flexible, High-Resolution, 60-Channel RF Coil for Supine Breast Imaging | |
Jana Vincent1,2,3, Clyve Konrad Follante1, Ersin Bayram4, Lloyd Estkowski5, Ty Cashen6, Mark Giancola1, Victor Taracila1, Yun-Jeong Stickle1, Lalit Rai1, Venkata Malasani1, Nicole Wake7,8, Vichiry Yan1, Robert Stormont9, Joseph Rispoli2,10, and Fraser Robb1 | ||
1GE Healthcare Coils, Aurora, OH, United States, 2Weldon School of Biomedical Engineering, Purdue University, West Lafayette, IN, United States, 3Basic Medical Sciences, Purdue University, West Lafayette, IN, United States, 4Global MR Applications & Workflow, GE Healthcare, Houston, TX, United States, 5Global MR Applications & Workflow, GE Healthcare, Waukesha, WI, United States, 6Global MR Applications and Workflow, GE Healthcare, Madison, WI, United States, 7Albert Einstein College of Medicine, Montefiore Medical Center, Bronx, NY, United States, 8Center for Advanced Imaging Innovation and Research, Department of Radiology, NYU School of Medicine, New York, NY, United States, 9GE Healthcare, Waukesha, WI, United States, 10School of Electrical & Computer Engineering, Purdue University, West Lafayette, IN, United States |
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Typically, breast MR scans are performed prone; however, there are advantages to supine imaging. Here we present the first 60-channel, high-resolution, flexible breast coil. The coil can be run with the embedded posterior coil for a total of 90-channels in the FOV. In addition to better image quality, with such a high channel count, an acceleration of up to 5 by 2 was possible. Due to the structured shape, breast tissue was kept in place for the duration of the scan and women with cup sizes up to a DD could be accommodated. Straps provide adjustments for smaller bust sizes. |
1592 | A Continuously Adjustable 32-Ch Head Coil Array for MRI at 3T | |
Yunsuo Duan1, Jiacheng Wang2, Feng Liu1, Rachel Marsh1, and Thomas J. Vaughan3 | ||
1MR Research, Department of Psychiatry, NYSPI and Columbia University, New York, NY, United States, 2Department of Electrical Engineering, New York University, New York, NY, United States, 3ZMBBI, Columbia University, New York, NY, United States |
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Close fitting is extremely crucial for RF coil arrays in order to maximize sensitivity. It is impossible to closely fit for all subjects of various head sizes using rigid head coil arrays. We presented a novel design of partially flexible 32-channel coil array to address the issue. The inner dimensions of the coil array can be smoothly adjusted from 180mmx220mm to 220mmx 260 mm, which fit for almost all head sizes of adult human subjects. The experiment results showed high imaging quality within the adjustable ranges. The coil array is highly practical for both research and clinical settings. |
1593 | A Quadrature Birdcage/47Rx Coil Array for Acceleration Images on 3 T MRI | |
Jo Lee1,2, Sen Jia1,2, Liu Liu3, Xiaoliang Zhang4, and Ye Li1,2 | ||
1Paul C. Lauterbur Research Center for Biomedical Imaging, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, 2Shenzhen Key Laboratory for MRI, Shenzhen, China, 3United Imaging Healthcare, Shanghai, China, 4Department of Biomedical Engineering, State University of New York, Buffalo, NY, United States |
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We designed and built a quadrature-birdcage/ 47Rx head coil array for accelerated images on 3 T MRI. A 32-channel commercial head coil was used as a comparison. The inverse g-factor images and accelerated anatomical images both show that the 47-channel head coil has better acceleration ability. EPI images and cerebrovascular images further verified that the 47-channel head coil is capable of human’s brain studies. |
1594 | A dedicated coil for cerebellar fMRI | |
Nikos Priovoulos1, Thomas Roos1, Ozlem Ipek2, Ettore Meliado3, Richard Nkrumah2, Dennis Klomp3, and Wietske van der Zwaag1 | ||
1Spinoza Center, Amsterdam, Netherlands, 2King’s College London, London, United Kingdom, 3University Medical Center Utrecht, Utrecht, Netherlands |
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The function of human cerebellum is underexplored in vivo, due to its small size and its placement at the bottom of the brain where transmit fields are suboptimal at 7Tesla. Here, we combined 2 dense coil arrays of 16 small surface receive elements each with a transmit array of 3 antennas elements. Our results show improved B1+ and SNR close to the surface as well as g-factor gains compared to a whole-head commercial coil. This resulted in large gains in the surface (< 3.5cm) in the spatial extent of the BOLD activation, at the cost of increased signal inhomogeneity. |
1595 | A novel multi-turn histology RF coil design for micro-histological slide imaging | |
Byung-Pan Song1,2, Sung-Jun Yoon1, Hyeong-Seop Kim1,2, Kyoung-Nam Kim3, and Seung-Kyun Lee1,2,4,5 | ||
1Department of Biomedical Engineering, Sungkyunkwan University, Suwon, Korea, Republic of, 2Department of Intelligent Precision Healthcare Convergence, Sungkyunkwan University, Suwon, Korea, Republic of, 3Department of Biomedical Engineering, Gachon University, Incheon, Korea, Republic of, 4Department of Physics, Sungkyunkwan University, Suwon, Korea, Republic of, 5IBS Center for Neuroscience Imaging Research, Suwon, Korea, Republic of |
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MR microscopy can provide high-resolution measurement of MR properties of biological and artificial tissues that can be compared with optical imaging. In such experiments, low signal-to-noise ratios (SNR) of a common clinical RF coil with a low filling factor will be a challenge. So, we propose a novel, multi-turn histology coil for imaging microscopic tissue histology slices with substantially higher SNR in clinical MRI scanner compared to the previous design for microscopy tissue imaging. |
1596 | How far Should Coil Coverage be Extended to Reach Optimum Simultaneous Multi-Slice Acceleration in Cardiac MRI? | |
Anpreet Ghotra1, Sam-Luca JD Hansen1, Robin Etzel1, Mirsad Mahmutovic1, Alina Scholz1, Nicolas Kutscha1, Matthäus Poniatowski1, Markus W May1, Choukri Mekkaoui2, and Boris Keil1 | ||
1Institute of Medical Physics and Radiation Protection, TH Mittelhessen University of Applied Sciences, Giessen, Germany, 2Harvard Medical School, Massachusetts General Hospital, Department of Radiology, A.A. Martinos Center for Biomedical Imaging, Boston, MA, United States |
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Even with commonly used k-space subsampling acceleration methods, cardiac MRI still suffers from relatively slow acquisition speed which imposes limitations in spatial and temporal resolution and volumetric coverage when imaging the moving heart. The recently introduced simultaneous multi-slice (SMS) acceleration technique offers the potential to acquire multiple slices which can substantially increase myocardial coverage without compromising in-plane spatial resolution. However, to disentangle the collapsed slices, array coils must provide enough sensitivity variation along the slice direction. Therefore, in this simulation study, we evaluated the coverage of the cardiac array coil to maximize SMS encoding performance. |
1597 | A novel 16 channel flexible coil for highly accelerated upper-airway MRI | |
Wahidul Alam1, Rushdi Zahid Rusho1, Scott Reineke2, Madavan Raja2, Stanley Kruger3, Joseph M. Reinhardt1, Junjie Liu4, Douglas Van Daele5, and Sajan Goud Lingala1,2 | ||
1Roy J Carver Department of Biomedical Engineering, University of Iowa, iowa city, IA, United States, 2ScanMed LLC, Omaha, NE, United States, 3Department of Radiology, University of Iowa, iowa city, IA, United States, 4Department of Neurology, University of Iowa, iowa city, IA, United States, 5Department of Otolaryngology, University of Iowa, iowa city, IA, United States |
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We develop a novel custom airway coil that offers significant boost in signal sensitivity in several regions of the upper-airway such as tongue, soft-palate, pharynx, glottis. Our coil is designed to be flexible for easy conformation to the subjects face/neck anatomy. With the proposed coil, we demonstrate robust parallel MRI performance up to R=4-5 fold for static imaging with 1-D under-sampling, and highly accelerated dynamic imaging (up to R~27 fold) of swallowing, and airway shaping due to variations in breathing. |
1598 | Signal-to-noise of thermal versus hyperpolarized MRI as a function of field strength and receive coil temperature | |
Mohammed M. Albannay1, Charles McGrath1, Alexander Jaffray1, and Sebastian Kozerke1 | ||
1University and ETH Zurich, Institute for Biomedical Engineering, Zurich, Switzerland |
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In this work SNR of thermal and hyperpolarized MRI is simulated based on first principles. It is demonstrated that detection of hyperpolarized nuclei is more favourable at lower field strengths (e.g. 0.75T) where prolonged T2* values and reduced readout bandwidth lead to higher SNR compared to standard clinical field strengths. Moreover, SNR benefits of receive coil cooling are experimentally studied on a clinical 3T Philips Achieva scanner that has been ramped down to a field strength of 0.75T. |
1599 | Performance comparison of a 10 cm single-gap vs. double-gap coaxial coil used as a transceiver for 7T MRI | |
Lena Nohava1,2, Andre Kuehne3, Elmar Laistler1, and Sigrun Roat1 | ||
1High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria, 2BioMaps (Laboratoire d'Imagerie Biomédicale Multimodale Paris Saclay), Université Paris-Saclay, CEA, CNRS, Inserm, Orsay, France, 3MRI.TOOLS GmbH, Berlin, Germany |
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In this work, we investigated the performance differences between a flexible single-gap coaxial coil operated far above self-resonance and a double-gap coaxial coil operated on self-resonance at 7T. Based on electromagnetic simulations and MRI results it is demonstrated that in the single-gap design the current distribution on the outside of the coaxial shield is strongly inhomogeneous. This leads to a strong dependence of the Tx performance on the coil orientation relative to B0. In contrast, the double-gap design results in homogeneous current distribution and orientation-independent Tx performance. |
1600 | Additive manufacturing of MRI coils by printing and electroplating a conductive polymer | |
Christoph Michael Schildknecht1 and Klaas Paul Pruessmann1 | ||
1Institute for Biomedical Engineering, ETH Zurich and University of Zurich, Zürich, Switzerland |
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In this work, additive manufacturing of MRI coils by selectively electroplating a conductive polymer is demonstrated, enabling the fabrication of complex coil geometries with high accuracy and reproducibility. Using a low-cost multi-material FDM 3D printer, deposition of insulating and conductive elements has been achieved in a single process, followed by straightforward electroplating. The proposed approach is demonstrated by an example of a wrist coil, including in-vivo imaging at 3T. |
1601 | Novel antenna array for ultra-high field MR-PET | |
Chang-Hoon Choi1, Suk-Min Hong1, Jörg Felder1, Lutz Tellmann1, Jürgen Scheins1, Elena Rota Kops1, Christoph Lerche1, and N. Jon Shah1,2,3,4 | ||
1INM-4, Forschungszentrum Juelich, Juelich, Germany, 2JARA-BRAIN-Translational Medicine, Aachen, Germany, 3Department of Neurology, RWTH Aachen University, Aachen, Germany, 4INM-11, Forschungszentrum Juelich, Juelich, Germany |
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Hybrid MR-PET is a powerful imaging technique that capitalised on the advantages of both modalities. However, to optimise these capabilities, the MRI antenna, which is located inside the effective PET detection area, needs to be operated without compromising any aspects of system performance or image quality compared to the stand-alone instrumentation. Here, we report a novel J-pole antenna array concept which is gamma radiation transparent. Furthermore, this unique feature provides advantages in MR-only applications by reducing the coupling effect between cables and the antenna elements and by lowering the potential specific absorption rate burden. |
1602 | Decomposition of the incomplete volume-surface integral equation matrices for MR coil simulations | |
Ilias Giannakopoulos1, Georgy Dmitrievich Guryev2, Jose Enrique Cruz Serralles2, Ioannis Georgakis1, Luca Daniel2, Jacob White2, and Riccardo Lattanzi1,3,4 | ||
1Center for Advanced Imaging Innovation and Research (CAI2R), Department of Radiology, New York University Grossman School of Medicine, New York, NY, United States, 2Department of Electrical & Computer Engineering, Massachusetts Institute of Technology, Cambridge, MA, United States, 3The Bernard and Irene Schwartz Center for Biomedical Imaging (CBI), Department of Radiology, New York University Grossman School of Medicine, New York, NY, United States, 4Vilcek Institute of Graduate Biomedical Sciences, New York University Grossman School of Medicine, New York, NY, United States |
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The volume-surface integral equation (VSIE) method is used for rapid and accurate simulations of electromagnetic fields in magnetic resonance imaging. For the case of a 7T array and a numerical head phantom, we constructed the VSIE coupling matrix that models the interactions between the coil and the scatterer. We reshaped the columns of the matrix as incomplete 3D tensors. We investigated how the low rank properties of these tensors, could be exploited to compress the coupling matrix, by expressing the tensors in their canonical form. We showed that an excellent compression could be achieved with an error lower than 2%. |
1603 | Flexible Body Coil for Vertical Field MRI using Loop/CRC RF Coil Array | |
Yosuke Otake1, Takeshi Taniguchi1, Hideta Habara1, Christophor Napier2, Errol Brissett2, Shawn Etheridge2, Masayoshi Dohata1, and Kazuyuki Kato1 | ||
1Healthcare Business Unit, Hitachi, Ltd., Tokyo, Japan, 2Hitachi Healthcare Americas, Twinsburg, OH, United States |
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To improving the SNR and the usability in the vertical field MRI(Open MRI), a flexible body(spine/torso) coil has been developed. The coil consists of loop/CRC hybrid multi-channel array (LCA). The performance of the coil was evaluated in phantom experiment at 1.2T vertical field MRI. The SNR of the coil using LCA was 46% better than a conventional body coil. This technique will contribute to improve the performance of the vertical field MRI. |
1604 | Design of an over-overlapped wearable 3T pelvic phased array using a capacitor-terminated coaxial coil | |
Ming Lu1,2, Junzhong Xu1,2, Sandeep S. Arora3, John C. Gore1,2, and Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Vanderbilt University Medical Center, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University Medical Center, Nashville, TN, United States, 3Department of Radiology and Biomedical Imaging, Yale University School of Medicine, New Haven, CT, United States |
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Prostate cancer is one of the leading causes of cancer death among men in the US. MRI is a useful tool to assess the presence and extent of prostate cancer, and diagnostic accuracy relies on acquiring images with high SNR. We aimed to improve the performance of such arrays by using flexible coaxial coil technology and an over-overlapping layout to increase the number of coil elements without sacrificing coil size. |
1605 | An Integrated Radio-Frequency/Wireless (iRFW) Coil Design for Wireless Q-Spoiling During MR Imaging | |
Jonathan Cuthbertson1,2, Trong-Kha Truong1,2, Jasmine Chen1,2, Fraser Robb3, Allen W. Song1,2, and Dean Darnell1,2 | ||
1Medical Physics Graduate Program, Duke University, Durham, NC, United States, 2Brain Imaging Analysis Center, Duke University, Durham, NC, United States, 3GE Healthcare, Aurora, OH, United States |
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The integrated RF/wireless coil design allows for simultaneous MR image acquisition and wireless data transfer with the same coil element in order to reduce the number of wired connections in the scanner. Here, we use this coil design to wirelessly transmit the scanner trigger signal to perform the Q-spoiling required for MR imaging. Proof-of-concept experiments in a phantom showed that this coil design was able to accurately and reliably transmit the scanner trigger from the adjacent console room to a WiFi-enabled module in the scanner bore, while having minimal impact on the image SNR or wireless performance. |
1606 | Universally Sized, High-Resolution and ASSET Optimized AIR Cervical Coils Combined with a 48-Channel Head Coil for 3T MRI | |
Yun-Jeong Stickle1, Clyve Konrad Follante1, Mark Giancola1, David Anderson1, Fraser Robb1, Thomas Stickle1, Robert Stormont2, Holly Blahnik2, Ho-Joon Lee3, Young Han Lee4, and Darryl B. Sneag5 | ||
1GE Healthcare Coils, Aurora, OH, United States, 2GE Healthcare, Waukesha, WI, United States, 3Haeundae Paik Hospital, Busan, Korea, Republic of, 4Severance hospital, Yonsei University, Seoul, Korea, Republic of, 5Hospital for Special Surgery, New York, NY, United States |
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Conventional high density phased-array head/neck coils are designed to tightly conform to head/neck region to increase SNR and accommodate higher acceleration, which in turn limits space and their use for larger patients. This study shows results for two different universally sized AIR (Adaptive Imaging Receive) neck/cervical spine coils combined with a 48-Channel head coil to provide higher SNR and improved acceleration compared to a conventional coil. 3T MRI setups to image the head/neck, carotids and cervical spine were designed and constructed. Phantom measurements and high-resolution in vivo imaging were performed to demonstrate design performance. |
1607 | Development of a multiplexed ERETIC-RF array coil for quantitative whole brain 3D-MR spectroscopic imaging (MRSI) | |
Bijaya Thapa1,2, Bernhard Strasser1,2, Xianqi Li1,2, Jason Stockman1,2, Azma Mareyam1, Boris Keil3, Zhe Wang4, Stefan Carp1,2, Yulin V. Chang4, Lawrence Wald1,2, Philipp Hoecht Hoecht5, and Ovidiu Andronesi1,2 | ||
1Dept. of Radiology, MGH, A. A. Martinos Center for Biomedical Imaging, Charlestown, MA, United States, 2Harvard Medical School, Boston, MA, United States, 3Mittelhessen University of Applied Science, Giessen, Germany, 4Siemens Medical Solutions USA, Charlestown, MA, United States, 5Siemens Healthcare, Erlangen, Germany |
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An Electronic REference To access In vivo Concentrations (ERETIC) to absolutely quantify the brain metabolites for 3D-MRSI using an array coil was developed. The challenge of ERETIC for large receive arrays is that the addition of many ERETIC channels might negatively impact B0 and B1 homogeneity and increase the unwanted channel cross-talk. Here we investigated whether the number of ERETIC channels can be reduced below the number of RF receive elements. We also developed a unique method to coil combine the ERETIC and receive array signal. Metabolite concentration maps obtained with ERETIC were compared to internal water reference method. |
1608 | New approach to Improve Sensitivity of Implantable NMR microprobe through Electrical Modelization | |
José Antonio BERNARDO1, Abel Rangel Trejo1, Lucas Werling2, Wilfried Uhring2, Luc Hebrard2, Youssef Zaim Wadghiri3, Christian Gontrand4, and Latifa Antonio Fakri-bouchet5 | ||
1Univ Lyon, CNRS, Université Claude Bernard Lyon 1, Institut des Sciences Analytiques, UMR 5280, Villeurbanne, France, 2Icube Laboratory, UMR –CNRS 7357, Université de Strasbourg, Strasbourg, France, 3Grossman School of Medicine, New York University, New York, NY, United States, 4INL(Institut des nanotechnologies de Lyon), INSA (Institut National des Sciences Appliquées) Lyon, CNRS, Université Claude Bernard Lyon1, Villeurbanne Cedex, France, 5Univ Lyon, CNRS, Université Claude Bernard Lyon 1, Institut des Sciences Analytiques, UMR 5280, INSA Lyon (Institut National des Sciences Appliquées), Villeurbanne, France |
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In this study, we propose an original modelling platform 3D-TLE (Transmission Line Extractor) to determine NMR coil and microcoil performance from their geometry. Each part of our microcoil (region of interest \((ROI \sim 2µL-3µL))\), active part, Transmission Line (TL), micro-wire connection (underpass-vias) and the substrate is modelled by an electrical circuit and each contribution to the equivalent resistance is quantified. Our platform allows predicting the optimized microcoil geometry related to expected performances in terms of \(Q-factor\) and the signal-to-noise ratio \((SNR)\). |
1609 | Exploring parallel imaging performance for prostate imaging at 7T using a 72-channel receive array | |
Tijl van der Velden1, Mark Gosselink1, Ingmar Voogt2, Martijn Froeling1, Hans Hoogduin1, Dennis Klomp1, Bart Steensma1, and Alexander Raaijmakers1,3 | ||
1UMC Utrecht, Utrecht, Netherlands, 2Wavetronica, Utrecht, Netherlands, 3Biomedical Engineering, Eindhoven University of Technology, Eindhoven, Netherlands |
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In this study we investigate the parallel imaging performance of a 72 channel body array for 7 tesla. G-factor maps and T2w prostate images have been acquired in a healthy volunteer. Accelerations of 3x3 and 4x1 are feasible without detrimental g-factor penalties. |
1610 | Coaxial coil modules as building blocks of individually arranged receive-only coil arrays | |
Michael Obermann1, Sigrun Roat1, and Elmar Laistler1 | ||
1High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria |
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Close form-fitting and adaptation of the RF coil array to the target anatomy are key for obtaining high SNR. We combine ultra-flexible coaxial coils with a modular setup to achieve form-fitting by coil flexibility and adaptive coverage of the assembled array through modularity. In this work, the robustness of the coil characteristics upon reconfiguration of three modules in different array arrangements, was investigated and demonstrated its feasibility without compromise in coil performance. |
2279 | Using deep neural networks to predict RF heating of implanted conductive leads exclusively from implant trajectory and RF coil features | |
Jasmine Vu1,2, Bach T Nguyen2, Bhumi Bhusal2, Justin Baraboo1,2, Joshua Rosenow3, Ulas Bagci 2, Molly G Bright1,4, and Laleh Golestanirad1,2 | ||
1Biomedical Engineering, McCormick School of Engineering, Northwestern University, Evanston, IL, United States, 2Radiology, Feinberg School of Medicine, Northwestern University, Chicago, IL, United States, 3Neurosurgery, Feinberg School of Medicine, Northwestern University, Chicago, IL, United States, 4Physical Therapy and Human Movement Sciences, Feinberg School of Medicine, Northwestern University, Chicago, IL, United States |
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Safety risks associated with radiofrequency (RF) heating of tissue around implanted leads limit MRI accessibility for patients with active electronic implants such as those with deep brain stimulation (DBS) devices. RF heating is highly sensitive to the trajectory of the implanted lead, and full-wave electromagnetic simulations are currently the standard method for quantifying RF heating, requiring extensive computational resources and simulation time. Here, we present a promising, fast approach for predicting trajectory-specific maximum local specific absorption rate (SAR) in the tissue around tips of implanted lead models using deep learning. |
2280 | RF-Induced Heating of Medical Devices in an Open Bore MRI | |
Seoggwan Kim1, Amy Kester1, Alan R. Leewood1, and David C. Gross1 | ||
1MED Institute Inc., West Lafayette, IN, United States |
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The goal of this study was to develop a computational model that can accurately predict the radiofrequency (RF) induced temperature rise of medical devices in a 1.2T (49 MHz) Hitachi Oasis open bore system for the purpose of MRI labeling according to ASTM F2503. A comparison of experimental and analytical temperature rise of calibration rods, a stent, and a knee implant within a gel phantom was conducted. Simulations of RF heating of the stent and knee implant within the Duke virtual human model were compared for the 1.2T Hitachi Oasis open bore and 1.5T Siemens Avanto closed bore MRI systems. |
2281 | RF Impedance of MR-Conditional Pacemaker Leads when Connected to Implantable Pulse Generators from Different MR-Conditional Systems | |
David Prutchi1, Jason Meyers1, and Ramez Shehada2 | ||
1Impulse Dynamics (USA) Inc., Marlton, NJ, United States, 2Medical Technology Laboratories, La Mirada, CA, United States |
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RF-induced heating of an active implantable medical device (AIMD) composed of a pulse generator (IPG) and leads depends on the transmission line impedance of the lead and its proximal-end termination by the impedance of the IPG. We demonstrate that the RF impedance of IPGs is minimal relative to that of the leads, which dominates the overall impedance of the implantable system. Accordingly, mixed hybrid systems composed of MR-Conditional leads and any MR-conditional IPG are expected to have a comparable overall impedance and consequently produce the same RF-induced heating as their corresponding original systems specified by the manufacturers. |
2282 | Importance of Pacemaker Lead Preconditioning for MR Safety In-Vitro Studies | |
David Prutchi1, Jason Meyers1, and Ramez Shehada2 | ||
1Impulse Dynamics (USA) Inc., Marlton, NJ, United States, 2Medical Technology Laboratories, La Mirada, CA, United States |
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This study investigates the change in the RF filtering characteristics of the leads of active implantable medical devices (AIMDs) as body fluids seep into the leads during the initial post-implant period. Our findings indicate that the RF characteristics change dramatically with fluid absorption, making it necessary to precondition the leads by soaking in isotonic saline solution to simulate the in-vivo scenario when conducting in-vitro MR safety testing. Furthermore, leads designed with RF-attenuating lumped inductances must consider the effect of fluid absorption on changing the peak RF attenuation frequency. |
2283 | Radio-Frequency Induced Heating of Hip and Knee Implants in the Cylindrical and Planar Systems | |
Kyoko Fujimoto1, Tayeb A Zaidi1, Dave Lampman2, Josha W Guag1, Shawn Etheridge2, Hideta Habara3, and Sunder S Rajan1 | ||
1Center for Devices and Radiological Health, US Food and Drug Administration, Silver Spring, MD, United States, 2Hitachi Healthcare Americas, Twinsburg, OH, United States, 3Healthcare Business Unit, Hitachi, Ltd., Tokyo, Japan |
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Radio-Frequency (RF) induced thermal injury is a common adverse event reported to US Food and Drug Administration. RF-induced heating risk depends on the interaction of implantable medical devices with electric field distribution in the MRI systems. A study showed that RF-induced heating of a neuromodulation device was much lower in the planar system compared to the cylindrical system. In this study, the hip and knee implants were studied in an anatomical human model at a 1.2T planar system and a 1.5T cylindrical system. |
2284 | Validation of a new 64MHz RF exposure system for testing medical implants for RF-induced heating according to ASTM-F2182 and ISO/TS 10974 | |
Finya Ketelsen1,2, Kevin Kröninger2, and Gregor Schaefers1,3 | ||
1MRI-STaR - Magnetic Resonance Institute for Safety, Technology and Research GmbH, Gelsenkirchen, Germany, 2TU Dortmund University, Dortmund, Germany, 3MR:comp GmbH, Testing Services for MR Safety & Compatibility, Gelsenkirchen, Germany |
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To determine the RF-induced heating of implants, it is necessary, that the RF field source used for testing fulfills several requirements. This study introduced the validation of a new developed linear exposure system for testing. The results for E-Field distributions from numerical simulations are validated experimentally by measuring these E-field distributions. Furthermore, the temperature rise at the 100mm titanium rod is compared with the target values form ISO/TS 10974 Annex I. The system fulfills the requirements and is suitable for testing active and passive implants for RF-induced heating according to ASTM F2182 and ISO/TS 10974. |
2285 | MRI in patients with a cerebral aneurysm clip; Guideline in the Netherlands | |
Mark BM Hofman1, Cristina Lavini2, Albert van der Zwan3, Carola van Pul4, Sara H Muller5, Mette K Stam6, Marinette van der Graaf7, Carla Kloeze8, Bastiaan J van Nierop9, Wouter Teeuwisse10, Peter Kappert11, Evie EM Kolsteren12, Kristie Venhorst12, and Joost PA Kuijer13 | ||
1Radiology and Nuclear Medicine, Amsterdam UMC, Vrije Universiteit, Amsterdam, Netherlands, 2Radiology and Nuclear Medicine, Amsterdam UMC location AMC, Amsterdam, Netherlands, 3, Neurology and Neurosurgery, UMC Utrecht Brain Center, Utrecht, Netherlands, 4Maxima Medical Centre, Eindhoven, Netherlands, 5Antoni van Leeuwenhoek Hospital, Amsterdam, Netherlands, 6Radiology, LUMC, Leiden, Netherlands, 7Imaging, Radboud UMC, Nijmegen, Netherlands, 8Catharina Hospital, Eindhoven, Netherlands, 9Radiology and Nuclear Medicine, University Medical Centre Utrecht, Utrecht, Netherlands, 10CJ Gorter Center for High Field MRI, LUMC, Leiden, Netherlands, 11Radiology, UMCG, Groningen, Netherlands, 12Knowledge Institute Medical Specialists, Utrecht, Netherlands, 13Radiology and Nuclear Medicine, Amsterdam UMC, Vrije Universiteit Amsterdam, Amsterdam, Netherlands |
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The Dutch Association of Medical Specialists wrote a guideline for MR safety experts for an MRI examination in a patient with a cerebral aneurysm clip for known and unknown clip types. Risk stratification for unknown clip types was based on a survey in the Netherlands that identified time frames and locations of ferromagnetic clip use. |
2286 | Pediatric Patient Positioning Can Reduce Local-SAR at the Pacemaker Lead-tip During MRI Exams | |
Jessica A. Martinez1 and Daniel B. Ennis1,2,3 | ||
1Department of Radiology, Stanford University, Stanford, CA, United States, 2Cardiovascular Institute, Stanford University, Stanford, CA, United States, 3Maternal & Child Health Research Institute, Stanford University, Stanford, CA, United States |
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Pediatric patients with cardiac implantable electronic devices (CIEDs) are generally contraindicated for MRI exams. Previous work in the adult population suggests that RF heating strongly depends on the patient’s position and orientation within the MRI scanner. The objective of this work was to evaluate in silico several pediatric patient-positions within the MRI scanner as methods to reduce RF-heating. |
2287 | RF safety simulation of 128-channel EEG net on a 29-month-old whole-body model at 3T | |
Hongbae Jeong1,2 and Giorgio Bonmassar1,2 | ||
1Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States, 2Department of Radiology, Massachusetts General Hospital/Harvard Medical School, Boston, MA, United States |
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In this study, RF heating of an EEG on a 29-month-old whole-body voxel model in a 3T MRI was studied with numerical simulation using Sim4Life. 128-channel EEG leads and electrodes were drawn on the head of the 29-month-old voxel model, and the position of the EEG electrodes was estimated from the 3D scan of the EEG net. The 10gSARmax and the SARhead were assessed in the model with and without the EEG net in birdcage transmit body coil at 3T. In both cases, estimated results of SAR were well-below the RF safety limit in the international standard. |
2288 | Experimental validation of simulated implant heating induced by switched gradient fields | |
Rüdiger Brühl1, Thomas Schwenteck1, Bernd Ittermann1, Fabio Baruffaldi2, Alessandro Arduino3, Umberto Zanovello3, Luca Zilberti3, Mario Chiampi3, and Oriano Bottauscio3 | ||
1Physikalisch-Technische Bundesanstalt (PTB), Berlin, Germany, 2IRCCS Istituto Ortopedico Rizzoli, Bologna, Italy, 3Istituto Nazionale di Ricerca Metrologica (INRIM), Torino, Italy |
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Switching MR gradients induce eddy-currents in metallic implants. Gradient-aggressive MR sequences were used on a commercial 3 T scanner to heat orthopaedic prostheses ex vivo. Heating experiments are presented, and the measured temperature evolution is compared with corresponding numerical results. Numerical simulations have been successfully validated for five MR sequences at different implant position and orientations in the gradient field. |
2289 | Numerical Simulation study on the effects of intentionally inhomogeneous E-field distributions on RF-induced heating of implants | |
Vincent Hammersen1, Finya Ketelsen1, Andreas Rennings2, and Gregor Schaefers1,3 | ||
1MRI-STaR Magnetic Resonance Institute for Safety Technology and Research GmbH, Gelsenkirchen, Germany, 2General and Theoretical Electrical Engineering (ATE), University of Duisburg-Essen, Duisburg, Germany, 3MR:comp GmbH, Gelsenkirchen, Germany |
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RF-induced heating of implants is strongly dependent on the E-Field magnitude at the test location, which is why a universal ±1dB and ±20° phase shift target field value limit is applied. We used numerical simulation to vary the exposing E-Fields, while keeping a constant average E-field magnitude at the test location. Strong deviations in heating development could be observed. In a second step we added phase shifts between exposition sources. The results suggest that, in addition to the limits, the exact field distribution especially the E-field directions should also be taken into account in critical inhomogeneous cases. |
2290 | Lead electromagnetic models for RF-induced heating in multi-electrode cortical implants | |
Mubashir Hussain1 and Gregor Schaefers1,2 | ||
1Magnetic Resonance Institute for Safety, Technology and Research GmbH, Gelsenkirchen, Germany, 2MR:comp GmbH, Testing Services for MR Safety & Compatibility, Gelsenkirchen, Germany |
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This work focus on estimating the RF-induced deposited power at the multi-electrode array of cortical implant (CorTec GmbH, Germany) by means of lead electromagnetic models (LEM). To develop the LEM for such a complex structure, we computed the transfer function for each of the electrode and generated a set of artificial tangential electric fields for validation of the LEM. The transfer functions and the tangential electric fields along the leads are then used to develop the LEM which can estimate the deposited power at the electrode array for an arbitrary lead pathway. |
2291 | Numerical Modelling of a Close-fitting 8-channel Transceiver Head Coil and EEG Electrodes for Safety Validation at 7T | |
Paul Mcelhinney1, Sarah Allwood-Spiers2, Gavin Paterson1, Marios Philiastides1, and Shajan Gunamony1 | ||
1University of Glasgow, Glasgow, United Kingdom, 2NHS Greater Glasgow and Clyde, Glasgow, United Kingdom |
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Simultaneous use of EEG and fMRI at high fields (UHF, ≥7T) offers the dual benefits of a high spatial resolution as well as the ability to study dynamic brain processes. A close fitting coil design has been built for this purpose, having open access to the subject and the EEG hardware while maintaining excellent performance characteristics. We present here the results from computer simulations of the head coil, including the EEG cap using human body models for safety validation and optimization of the design. |
2292 | MRI in patients with a prosthetic heart valve, annuloplasty ring or mitra clip; Guideline in the Netherlands | |
Mark BM Hofman1, Carla Kloeze2, Bastiaan J van Nierop3, Sara H Muller4, Joost PA Kuijer1, Kristie Venhorst5, Cristina Lavini6, Mette K Stam7, Carola van Pul8, Wouter Teeuwisse9, Marco JW Gotte10, Peter Kappert11, Evie EM Kolsteren5, and Marinette van der Graaf12 | ||
1Radiology and Nuclear Medicine, Amsterdam UMC, Vrije Universiteit Amsterdam, Amsterdam, Netherlands, 2Catharina Hospital, Eindhoven, Netherlands, 3Radiology and Nuclear Medicine, University Medical Centre Utrecht, Utrecht, Netherlands, 4Antoni van Leeuwenhoek Hospital, Amsterdam, Netherlands, 5Knowledge Institute Medical Specialists, Utrecht, Netherlands, 6Radiology and Nuclear Medicine, Amsterdam UMC location AMC, Amsterdam, Netherlands, 7Radiology, LUMC, Leiden, Netherlands, 8Maxima Medical Centre, Eindhoven, Netherlands, 9CJ Gorter Center for High Field MRI, LUMC, Leiden, Netherlands, 10Cardiology, Amsterdam UMC, Vrije Universiteit Amsterdam, Amsterdam, Netherlands, 11Radiology, UMCG, Groningen, Netherlands, 12Imaging, Radboud UMC, Nijmegen, Netherlands |
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Can a patient with a prosthetic heart valve, annuloplasty ring or a mitra clip undergo an MRI examination? The Dutch Association of Medical Specialists (FMS) wrote a guideline, using searches of guidelines, literature, implant databases, and incident databases. The recommendation is: scan the patient with a prosthetic heart valve, annuloplasty ring or mitra clip with an 1.5T or 3T whole body MRI system with a horizontal closed bore superconducting magnet without further restrictions. |
2293 | Comparing RF Heating Based on SAR vs. B1+RMS MRI Conditional Labeling | |
Negin Behzadian1 and Shiloh Sison2 | ||
1Research and Development, Abbott, Sylmar, CA, United States, 2Research and Development, Abbott, Sunnyvale, CA, United States |
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MRI RF heating can cause thermal damage to biological tissues, especially in patients with leaded implantable devices, by concentrating power deposition at the implant-tissue interface. With the emergence of B1+RMS as a more precise RF exposure metric than SAR, implantable device manufacturers have begun MR conditional labeling to fixed B1+RMS levels, in addition to SAR labeling. Our study characterizes the relationship between RF heating per SAR vs. B1+RMS-based scaling methods in the context of 3T Normal Operating and First Level Controlled Mode MRI exposure. |
2294 | Quantification of safety and image quality in low field MRI in the presence of medical implants. | |
Camille D.E. Van Speybroeck1, Wouter M. Teeuwisse1, Tom O'Reilly1, Paul M. Arnold2, and Andrew G. Webb1 | ||
1G.J. Gorter Center for High Field MRI, Leiden University Medical Center, Leiden, Netherlands, 2Neurosurgery, Carle Foundation Hospital, Urbana, IL, United States |
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Very little quantitative data exist on safety aspects of medical implants in low field MRI systems. Protocols for clinical scanners must be adjusted due to differences in bore size and B0 direction. We present measured and simulated data on magnetically induced displacement forces, image artifacts and SAR on a 50 mT portable MRI system. Results show that some implants must be considered MR unsafe even at 50 mT, that image artifacts are less compared to 3 T even with much lower gradient strengths, and SAR limits can be breached if using very short pulses and inter-echo times in TSE sequences. |
2295 | A Single Setup Approach for the MRI-based Measurement and Validation of the Transfer Function of Elongated Medical Implants | |
Peter Stijnman1,2, Arcan Erturk3, Cornelis van den Berg1, and Alexander Raaijmakers1,2 | ||
1Computational Imaging, UMC Utrecht, Utrecht, Netherlands, 2Biomedical Engineering, Eindhoven University of Technology, Eindhoven, Netherlands, 3Medtronic, Minneapolis, MN, United States |
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A new method to validate the transfer function (TF) of linear implants was developed, using an independent RF transmitter. A simulation study was performed exploring different methods to change the incident electric field, local transmit coils positioned at various locations is most effective for the validation. A benefit is the constant position of the leap tip and the temperature probe. We performed a TF measurement and validation study for three leads. The simulated incident electric fields of the local transmit coils and the measured TF were used to predict tip heating, verified by temperature probe measurements showing excellent agreement ($$$R^2\geq0.977$$$). |
2296 | Analysis on 1.5T MR clinical scan time of patients from multiple imaging centers | |
Yuqing Wan1, Nathan Ooms2, Paul Nguyen1, and Guangqiang (Jay) Jiang1 | ||
1Axonics Modulation Technologies, Irvine, CA, United States, 2Purdue University, West Lafayette, IN, United States |
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This study reported magnetic resonance imaging (MRI) examination duration of 974 patients collected from two imaging sites. Statistical scan time analysis was performed, and distributions were obtained for different scan regions. Scan time disparities were found between the two imaging sites due to the sequence selections and configuration, which may impact imaging cost and image quality. The clinical examination duration data provides useful information for implant device manufacturers to define practical MRI conditions that improve the patients’ overall MR experience. |
2297 | An anthropomorphic phantom for deep brain stimulation MRI safety investigations | |
Benson Yang1,2, Fred Tam1, Benjamin Davidson3, Clement Hamani3,4, Nir Lipsman1,3,4, Chih-hung Chen2, and Simon J Graham1,5 | ||
1Physical Sciences, Sunnybrook Research Institute, Toronto, ON, Canada, 2Electrical and Computer Engineering, McMaster University, Hamilton, ON, Canada, 3Division of Neurosurgery, Sunnybrook Health Sciences Centre, Toronto, ON, Canada, 4Harquail Centre for Neuromodulation, Sunnybrook Research Institute, Toronto, ON, Canada, 5Department of Medical Biophysics, University of Toronto, Toronto, ON, Canada |
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Magnetic resonance imaging of deep brain stimulation (DBS) patients remains a safety concern at higher magnetic fields strengths. Phantoms play an important role in validating and estimating patient safety conditions. However, conventional phantoms are typically simple homogeneous structures that limit the ability to replicate DBS surgical implant procedures. In this work, a new phantom structure is proposed with more human-like realism and compartments to enable improved replication of DBS device placement geometries. Preliminary radiofrequency heating results demonstrate significant differences in temperature elevations when the phantom is assembled in a heterogeneous and homogeneous configuration. |
2298 | Compact 3T MRI for patients with implanted devices: Software tool to display MR fields at a specified location | |
Lydia Jean Bardwell Speltz1,2, Yunhong Shu2, Myung-Ho In2, Nolan Meyer1,2, Erin Gray2, Diana Lanners2, Yihe Hua3, Robert E Watson2, John Huston III2, Thomas KF Foo3, and Matt A Bernstein2 | ||
1Mayo Clinic Graduate School of Biomedical Sciences, Mayo Clinic, Rochester, MN, United States, 2Department of Radiology, Mayo Clinic, Rochester, MN, United States, 3GE Global Research, Niskayuna, NY, United States |
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Many implanted devices are labeled MR Conditional, meaning specific, labeled conditions must be met to ensure safe scanning. We developed a software tool for use with a high-performance, compact 3T (C3T) scanner that verifies relevant MR conditions can be met at the location of the device (e.g., abdomen), even if those conditions are exceeded at the level of the anatomy being scanned (e.g., brain). MR parameters assessed include main magnetic field strength, gradient slew rate, RF amplitude (B1+2), and dB/dz. The limited extent of the fields with C3T suggests high-performance exams can sometimes be obtained without compromising patient safety. |
2299 | Patient specific parallel transmit pulses are patient position dependent while safety models are fixed: safety implications | |
Emre Kopanoglu1 | ||
1CUBRIC, School of Psychology, Cardiff University, Cardiff, United Kingdom |
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Pulses designed using patient-specific B1+-maps are inherently patient position dependent, while safety models (available on scanners) used for local SAR supervision are not. The effect of this positional mismatch on SAR estimation was investigated for 1-/2-/3-/4-/5-spoke pulses. The results showed substantial underestimation of local SAR: the actual local SAR at off-centre positions was observed to be up to 4.6-fold higher compared to the peak estimated using a centred model. This behaviour was worse for more spokes and consistent across slices between cerebellum and crown. Using multiple distributed models reduced the likelihood of SAR underestimation, but at the cost of over-restrictiveness. |
2300 | Assessing the In-Vivo RF Heating Effects of Short-Duration B1+RMS in MRI Sequences | |
Negin Behzadian1 and Shiloh Sison2 | ||
1Research and Development, Abbott, Sylmar, CA, United States, 2Research and Development, Abbott, Sunnyvale, CA, United States |
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Exposure to the RF energy of an MRI shall be limited to prevent potential harm to biological tissues. Whole-body SAR, averaged over any 6-minute interval, shall be limited to 2W/kg and 4W/kg under the limits of Normal and First Level Controlled Operating Mode, respectively, and is further restricted to twice the operating mode limit over any 10-second period. Our study investigates whether similar short-duration assessments are necessary for the alternative RF exposure metric of B1+RMS, in the context of RF heating safety of cardiac protocols with leaded cardiac implants. |
2301 | Validation of SAR Management Procedure for Dynamic pTx RF Waveforms Using a Self-Built Coil at 7 Tesla | |
Sydney Nicole Williams1, Sarah Allwood-Spiers2, Paul McElhinney1, Yuehui Tao3, John E. Foster2, Shajan Gunamony1,4, and David A. Porter1 | ||
1Imaging Centre of Excellence, University of Glasgow, Glasgow, United Kingdom, 2MRI Physics, NHS Greater Glasgow & Clyde, Glasgow, United Kingdom, 3Siemens Healthcare Ltd., Glasgow, United Kingdom, 4MR CoilTech Limited, Glasgow, United Kingdom |
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Parallel transmit (pTx) can reduce B1+ field inhomogeneity present at 7T, but needs additional consideration for specific absorption rate (SAR) monitoring due to the superimposed electromagnetic fields. For self-built pTx coils, validation includes comparing electromagnetic field simulations with experimental B1+ maps and thermometry, previously presented for static pTx in a self-built 8Tx/32Rx coil. We present full-waveform pTx validation with two further tests: comparison of measured and prescribed RF waveforms, and calculation of local SAR with virtual observation points (VOPs) for all pTx pulses with comparison to scanner predictions and measurements. After validation, dynamic pTx is performed in vivo. |
2302 | Individualized and accurate SAR characterization method based on an equivalent circuit model in MRI system | |
Weiman Jiang1, Fan Yang1, and Kun Wang1 | ||
1GE Healthcare, Beijing, China |
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This work proposed a novel SAR characterization method based on an equivalent circuit model and the circuit’s frequency response analysis. Comparing to well recognized pulse energy method defined in NEMA MS 8, this method doesn’t need the flux loop fixed on transmit coil. Meanwhile, it can monitor SAR accurately. The Root Mean Square (RMS) error and maximum error of the novel method relative to the method in NEMA MS 8 are 4.96% and 9.47% respectively. This method could avoid design complexity of integrating the flux loop and has potential to be easily realized in most MRI scanners. |
2303 | A local SAR compression algorithm with improved compression, speed and flexibility | |
Stephan Orzada1, Thomas M. Fiedler1, Harald H. Quick2,3, and Mark E. Ladd1,2,4,5 | ||
1Medical Physics in Radiology (E020), German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Erwin L. Hahn Institute for MRI, University Duisburg-Essen, Essen, Germany, 3High-Field and Hybrid MR Imaging, University Hospital Essen, Essen, Germany, 4Faculty of Physics and Astronomy, University of Heidelberg, Heidelberg, Germany, 5Faculty of Medicine, University of Heidelberg, Heidelberg, Germany |
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For parallel transmit systems, control of local SAR is very important to ensure safety. For pulse calculation and online supervision, compression of the SAR matrices is used to reduce calculation effort. The original clustering method by Eichfelder et al. was later outperformed by a method proposed by Lee et al. We propose an enhancement to Lee’s algorithm that further increases compression efficiency, speed and flexibility by iteratively reducing the overestimation. |
2304 | Validation of a Temperature Prediction Workflow for Imaging Complete Deep Brain Stimulation Systems | |
Alireza Sadeghi-Tarakameh1, Nur Izzati Huda Zulkarnain1, Noam Harel1, and Yigitcan Eryaman1 | ||
1Center for Magnetic Resonance Research (CMRR), University of Minnesota, Minneapolis, MN, United States |
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We validate a previously proposed temperature prediction workflow for a complete DBS Systems undergoing MRI. Accuracy of the workflow is investigated for different termination conditions using an extension cable and an implantable pulse generator (IPG) device. The workflow accurately predicted the temperature time-course during the MRI scan for different trajectories and terminations. |
2305 | Radiofrequency peak B1+ Survey of commercial 3T MR Systems | |
Xin Huang1, Vick Chen1, and Shiloh Sison1 | ||
1Abbott Laboratories, Sunnyvale, CA, United States |
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To determine the appropriate peak B1+ field levels, an RF peak B1+ survey is performed on commercial 3T MR systems loaded with ASTM phantom filled with saline. The peak B1+ averaged over center slab inside the 3T commercial MR systems can be as high as 27 µT. The 3T MRI safety assessment should include values up to this level. |
2306 | Impact of 1.5T SAR Limits on the MRI Scan Time for Implantable Devices | |
Yuqing Wan1, Nathan Ooms2, Paul Nguyen1, and Guangqiang (Jay) Jiang1 | ||
1Axonics Modulation Technologies, Irvine, CA, United States, 2Purdue University, West Lafayette, IN, United States |
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Implant device manufacturers often specify a RF exposure limit based on specific absorption rate (SAR) or B1+rms and a continuous active scan time in the device magnetic resonance imaging (MRI) labelling. Due to the restriction of the labeled SAR, MR sequence parameters may need to be adjusted to reduce RF power, resulting in prolonged scan time. The patient examination duration may be extended by up to 67% when compared to standard protocols. The overall session may be further prolonged due to additional wait time requirements from certain implanted devices, which can result in great inconvenience and extra cost to patients. |
2307 | RF safety and image quality testing of deep brain stimulation electrodes with 3T MRI | |
Gaurav Verma1, Paul Min2, MyungHo In2, Jungho Cha3, Akbar Alipour1, Charlotte Elorette4, Lazar Fleysher5, Priti Balchandani1, Helen Mayberg3, and Ki Sueng Choi3 | ||
1Radiology, Icahn School of Medicine at Mount Sinai, New York, NY, United States, 2Radiology, Mayo Clinic, Rochester, MN, United States, 3Center for Advanced Circuit Therapeutics, Icahn School of Medicine at Mount Sinai, New York, NY, United States, 4Neuroscience, Icahn School of Medicine at Mount Sinai, New York, NY, United States, 5Diagnostic, Molecular and Interventional Radiology, Icahn School of Medicine at Mount Sinai, New York, NY, United States |
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Radio frequency (RF) safety and image quality testing was performed in the presence of deep brain stimulation (DBS) electrodes using gel acrylamide phantoms and two 3T MRI scanners. Two electrodes, (Abbott and Medtronic) were tested with sequences including GRE, T1-weighted magnetization-prepared rapid gradient echo (MPRAGE), and T2-weighted turbo spin-echo (TSE). Safety testing showed low heating when electrodes were aligned along the B0 field (Z-axis) of the magnet, but higher heating when the electrodes were angled to the main field. Image quality testing showed smaller ferromagnetic susceptibility artifacts when electrode was parallel with B0 field and normal to transmit field. |
2308 | Improved compression of SAR matrices by a reformulation of the generalized virtual observation point compression scheme | |
Vincent Gras1 and Nicolas Boulant1 | ||
1DRF/Joliot/Neurospin, CEA - Université Paris Saclay, Gif sur Yvette, France |
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Parallel transmission to date is the most promising technology to tackle the RF field inhomogeneity problem in MRI at ultra-high field. The Virtual Observation Point compression technique was a cornerstone in the field to reduce drastically the number of SAR matrices to handle in exam supervision and RF pulse design. After its original discovery, it was further improved to boost the compression. This work describes a reformulation of the problem which simplifies substantially the numerical search and allows reducing further the number of matrices by a factor ~5 or more. |
2309 | Stand-Alone Hardware SAR Monitor based on low cost Electronic Standard Components | |
Marcus Prier1,2, Max Joris Hubmann1,2, Enrico Pannicke1,2, and Oliver Speck1,2 | ||
1Otto-von-Guericke University, Magdeburg, Germany, 2Research Campus STIMULATE, Magdeburg, Germany |
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A low cost, stand-alone RF power monitor was developed that fulfills the requirements given in the standard 60601-2-33 and is based on electrical standard components. It consists of two dual directional couplers, two RMS envelope filters and a microcontroller. A fixed power limit can be programmed or patient dependent power limits can be communicated from a host computer. Evaluation measurements show power measurement and RFPA blanking switching times accuracies with an error less than 1%. A sampling rate of 130kSamples/s indicates usability for relatively short or moderate complex shaped RF waveforms. |
2310 | Is a Local Tx Coil sufficient for Guidewire Safety in MRI? | |
Felipe Godinez1,2, Greig Scott3, Joseph V Hajnal1,2, and Shaihan J Malik1,2 | ||
1Biomedical Engineering Department, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 2Centre for the Developing Brain, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 3Department of Electrical Engineering, Stanford, Stanford, CA, United States |
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Imaging guidewires in MRI is known to have heating hazards associated. In this work we show initial data that supports the use of local Tx coils over whole body coils for the safe imaging of standard guidewires with MRI. This was tested in vitro using parallel transmit (PTx) techniques to generate a scenario for a proper comparison between the two coil types. It was found that a local Tx coil produces less heating at the guidewire tip, than a body coil under comparable conditions. |
2311 | Input Impedance Comparison of MR-Conditional Cardiac Implantable Pulse Generators at the 1.5T MR Frequency of 63.87 MHz | |
Jason Meyers1, David Prutchi1, and Ramez Shehada2 | ||
1Impulse Dynamics (USA) Inc., Marlton, NJ, United States, 2Medical Technology Laboratories, La Mirada, CA, United States |
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The MR environment poses a tissue heating hazard to patients with cardiac IPGs (implantable pulse generators), such as pacemakers and defibrillators, due to RF currents circulating in the loop formed by the IPG, a transvenous lead, and the tissue. Heating will be limited by the impedance of this loop at the MR frequency (63.87 MHz for 1.5T). The IPG input impedance (a portion of this loop) was measured in six MR-Conditional IPG’s. All have a comparable, low impedance, suggesting that device manufacturers are not intentionally adding impedance and that some interchangeability may be possible without changing RF-induced heating. |
2312 | Computational simulations of heating in the vicinity of an 8-contact depth EEG electrode: the impact of model simplification | |
Hassan B Hawsawi1,2, Ozlem Ipek3,4, David W Carmichael5,6, and Louis Lemieux1 | ||
1Clinical and Experimental Epilepsy, University College London, London, United Kingdom, 2Administration of Medical Physics, King Abdullah Medical City, Makkah, Saudi Arabia, 3King’s College London, London, United Kingdom, 4CIBM-AIT, Ecole Polytechnique Federale de Lausanne, Lausanne, Switzerland, 5Department of Biomedical Engineering, King’s College London, London, United Kingdom, 6Developmental Imaging and Biophysics Section, UCL Great Ormond Street Institute of Child Health, London, United Kingdom |
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Electromagnetic (EM) simulations offer the possibility of assessing RF-induced heating around intracranial EEG (icEEG) electrodes across a variety of placement scenarios in a shorter time than experimental phantom-based temperature measurements. However, given the sub-millimetric dimensions of the wires and contacts the range of spatial scales spans many orders of magnitude, leading to high computational demands. In this study, we assessed the effect of model simplification for a typical 8-contact depth EEG electrode on the estimated heating patterns. |
2313 | Safety Considerations in Neuroimaging of Neonatal and Pediatric Patients Using Portable Low Field MRI | |
Mark Smith1, Harry Hu2, Ram Krishnamurthy1, John Pitts3, and Mai-Lan Ho1 | ||
1Nationwide Children's Hospital, Columbus, OH, United States, 2Hyperfine, Dublin, OH, United States, 3Hyperfine, Cleveland, OH, United States |
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In 2020, a portable 64mT ultra-low field MRI system designed for point of care bedside use received 510K clearance (Hyperfine, Guilford, CT). Our pediatric institution (Nationwide Children’s Hospital) has acquired one of these systems to meet neuroimaging needs for critically ill NICU or PICU patients who cannot tolerate transport to the MRI department. Prior to scanning patients, safety testing for displacement and heating was conducted on monitoring hardware that will be connected to the patient during the bedside MRI. The monitoring hardware was found safe to stay connected to the patient during the bedside MRI. |
2314 | Influence of E-Field Homogeneity and Drift for Testing Medical Implants for RF-induced heating at 64MHz according to ASTM-F2182 and ISO/TS 10974 | |
Finya Ketelsen1,2, Vincent Hammersen1, Kevin Kröninger2, and Gregor Schaefers1,3 | ||
1MRI-STaR - Magnetic Resonance Institute for Safety, Technology and Research GmbH, Gelsenkirchen, Germany, 2TU Dortmund University, Dortmund, Germany, 3MR:comp GmbH, Testing Services for MR Safety & Compatibility, Gelsenkirchen, Germany |
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Medical implants of all kind must be tested for RF-induced heating to determine their MR safety and compatibility. Test conditions concerning E-field homogeneity and E-field drift during assessment time are defined in ISO/TS 10974 and ASTM-F2182. This study evaluates the influence of E-field drift and E-field homogeneity on RF-heating. It shows that both effects can lead to a temperature underestimation. Even for small implants whose volume is in a homogenous area within ±1dB, this underestimation can occur. System instability and implant size and position can further increase the underestimation of RF-induced heating and should be carefully considered. |
2315 | Parallel-transmit coil dimensions affect SAR sensitivity to motion at 7T. | |
Alix Plumley1, Philip Schmid1, and Emre Kopanoglu1 | ||
1Cardiff University Brain Research Imaging Centre, Cardiff, United Kingdom |
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Subject motion in parallel-transmit (pTx) causes channels’ electric field interference patterns to change, influencing SAR distributions. This can cause safety limits to be exceeded when SAR-constrained pulses are designed for one position. Here, we consider effects of pTx coil dimensions on SAR sensitivity to motion by simulating 6 differently-sized coil models, and evaluating SAR at 19 displaced positions. Our results agree with those previously reported for the similar-sized coil, but SAR sensitivity was generally lower for larger coils, and higher for smaller coils, with maximum motion-induced local-SAR increase of 3.8-fold and 1.6-fold for the smallest and largest coil models, respectively. |
2316 | Safety evaluation with respect to RF-induced heating of a new setup for Transcranial Electric Stimulation during MRI | |
Fróði Gregersen1,2,3,4, Cihan Göksu2,5, Gregor Schaefers6,7, Rong Xue4,8,9, Axel Thielscher1,2, and Lars Hanson1,2 | ||
1Section for Magnetic Resonance, DTU Health Tech, Technical University of Denmark, Kgs Lyngby, Denmark, 2Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital, Amager and Hvidovre, Denmark, 3Sino-Danish Center for Education and Research, Aarhus, Denmark, 4University of Chinese Academic of Sciences, Beijing, China, 5High-Field Magnetic Resonance Center, Max-Planck-Institute for Biological Cybernetic, Tübingen, Germany, 6MRI-STaR-Magnetic Resonance Institute for Safety, Technology and Research GmbH, Gelsenkirchen, Germany, 7MR:comp GmbH, MR Safety Testing Laboratory, Gelsenkirchen, Germany, 8State Key Laboratory of Brain and Cognitive Science, Beijing MRI Center for Brain Research, Institute of Biophysics, Chinese Academy of Sciences, Beijing, China, 9Beijing Institute for Brain Disorders, Beijing, China |
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Combining transcranial electrical stimulation (TES) with MRI offers various interesting research opportunities, but also introduces safety concerns. Coupling between the RF field and highly conductive TES leads can lead to skin burns. These safety issues are usually mitigated with the use of safety resistors and controlled lead paths that reduce the power absorbed by the leads. However, these methods introduce practical limitations for combined TES/MRI experiments, such as limited stimulation currents and cable stray fields corrupting MR current density imaging. We overcome these limitations by using low-conductivity silicone-rubber as TES leads. Simulations and temperature measurements are used for safety assessment. |
2317 | Unloaded RF transmit coil B1+ maps do not correlate with SAR hotspots | |
Xin Chen1 and Michael Steckner1 | ||
1Canon Medical Research USA Inc., Mayfield Village, OH, United States |
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MRI vendors have been asked to provide B1+ contour plots of unloaded whole body transmit coils in order to show technologists/radiographers where not position a patient for SAR hotspot/RF burn avoidance purposes. Two flaws with this strategy are demonstrated by modeling Duke at the abdominal landmark in the centered and off-set position: 1) B1+ maps correlate poorly to SAR hotspots, 2) loaded B1+ maps are significantly different relative to unloaded B1+ maps. Knowledge of the birdcage coil end-ring position in conjunction with spacing pads will improve RF burn safety outcomes. |
2477 | Device and simulation workflow for validating cardiac magneto-stimulation thresholds in porcine models | |
Valerie Klein1,2, Mathias Davids1,2,3, Donald Straney2, Livia Vendramini2, Lothar R. Schad1, Maaike van den Boomen2,3,4, Christopher Nguyen2,3,4, Lawrence L. Wald2,3,5, and Bastien Guerin2,3 | ||
1Computer Assisted Clinical Medicine, Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany, 2A. A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Charlestown, MA, United States, 3Harvard Medical School, Boston, MA, United States, 4Cardiovascular Research Center, Cardiology Division, Massachusetts General Hospital, Charlestown, MA, United States, 5Harvard-MIT Division of Health Sciences and Technology, Cambridge, MA, United States |
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We developed a magnetic stimulator to measure cardiac stimulation (CS) thresholds of time-varying magnetic fields in pigs. The stimulator consists of a high-power capacitor bank (C=110 µF) discharging into a pancake coil. We will use the measured thresholds to validate a previously developed CS simulation framework that combines electromagnetic field simulations with electrophysiological models of excitable cardiac fibers. We generate whole-body porcine voxel models from multi-bed MRI Dixon and CINE acquisitions to reproduce the anatomy and posture of the animals in our simulations. Carefully validated CS simulations may eventually be useful in setting cardiac safety limits for MRI gradient applications. |
2478 | Are interventionalists prone to nerve stimulation during MR interventions? PNS simulation study with posable human body models | |
Feng Jia1, Sebastian Littin1, Philipp Amrein1, Maximilian Frederik Russe1, and Maxim Zaitsev1,2 | ||
1Department of Radiology, Medical Physics, University of Freiburg, Faculty of Medicine, Freiburg, Germany, 2High Field MR Center Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria |
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TODO Simulation of peripheral nerve stimulation of MRI gradient coils for an interventional radiologist. |
2479 | Electric Field Calculation and PNS Prediction for Head and Body Gradient Coils | |
Koray Ertan1,2, Trevor Wade3,4, Andrew Alejski4, Charles A McKenzie3, Paolo Decuzzi2, Brian Rutt1, and Peter B Roemer5 | ||
1Department of Radiology, Stanford University, Stanford, CA, United States, 2Laboratory of Nanotechnology for Precision Medicine, Italian Institute of Technology, Genoa, Italy, 3Department of Medical Biophysics, Western University, London, ON, Canada, 4Robarts Research Institute, Western University, London, ON, Canada, 5Roemer Consulting, Lutz, FL, United States |
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Computationally efficient methods are presented which allow calculation of switched-gradient-induced electric field distributions on realistically sized body model with uniform interior properties (compatible with regulatory IEC standards). Electric fields were calculated for three classes of gradient coils (asymmetric head, symmetric head and body gradients) using 100-member male and female body model populations; these were then used to estimate population-mean PNS parameters which were validated against experimental PNS measurements, showing high accuracy. Our computationally efficient methods can calculate whole-body E-field distributions in seconds with updates for different gradient designs in tens of milliseconds, providing an important tool for PNS-constrained gradient design. |
2480 | Peripheral Nerve Stimulation limits with fast narrow and broad-band pulses | |
Joseba Alonso1,2, Daniel Grau2,3, Juan Pablo Rigla3, Eduardo Pallás1,2, José Miguel Algarín1,2, José Borreguero1,2, Rubén Bosch1,2, Guillermo Comazzi1,2, Elena Díaz3, Fernando Galve1,2, José Manuel González3, Carlos Gramage1,2, Rubén Pellicer1,2, Alfonso Ríos3, and José María Benlloch1,2 | ||
1Spanish National Research Council (CSIC), Valencia, Spain, 2Universitat Politècnica de València, Valencia, Spain, 3Tesoro Imaging S.L., Valencia, Spain |
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We present an apparatus for PNS threshold determination on a subject's limb, capable of narrow and broad-band magnetic excitation with pulse characteristic times down to 40 us. From measurements on 51 volunteers, we observe that PNS limits coincide for sinusoidal and triangular excitations, and are slightly lower for trapezoidal pulses. We measure significant correlations of PNS sensitivity with arm size and body weight, and none with height or gender. We confirm thresholds increase significantly for short trains also in these fast timescales. Finally, we propose our versatile low-cost system for fast offline determination of a subject's limits prior to scanning. |
2481 | Design and Electric Field Analyses of a Shorter and Wider Asymmetric Gradient Coil for Whole Body MRI Scanners: A Comparison with a Symmetric Design | |
Afis Ajala1, Yihe Hua1, Desmond Teck Beng Yeo1, Mark Vermilyea1, and Thomas Foo1 | ||
1GE Global Research, Niskayuna, NY, United States |
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A unique approach to providing a more open, less claustrophobic whole-body MRI is presented. A design for an asymmetric gradient coil moves the region of interest (ROI) towards one end of the gradient coil, shortening the gradient coil length from the isocenter to the patient opening. This results in a stepped configuration where the patient-bore diameter outside of the imaging ROI is substantially wider compared to using a conventional symmetric gradient coil design. The stepped patient bore has previously been used in head-only gradient systems where the greater openness has resulted in increased patient comfort and reduced claustrophobia. |
2482 | Thermal simulations for a high power diffusion weighting MR gradient coil | |
Philipp Amrein1, Feng Jia1, Sebastian Littin1, and Maxim Zaitsev1 | ||
1Dept.of Radiology, Medical Physics, University Medical Center Freiburg, Freiburg, Germany |
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In the context of the development of a high power MR diffusion probe for the human breast, a computer model for thermal simulation was created that allows evaluation of different duty cycles and current strengths. The proposed method includes simulating constant effective currents rather than time resolved pulse sequences. This allows reasonable computational effort to analyze the heating effects for a given diffusion weighting sequence on a given gradient system. The simulated results show reasonable agreement with experimental data. |
2483 | Induced heating of compact cryogen-free superconducting magnet during field-cycling insert coil operation | |
Matthew A. McCready1, William B. Handler1, and Blaine A. Chronik1 | ||
1Physics and Astronomy, Western University, London, ON, Canada |
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Delta relaxation enhanced magnetic resonance (dreMR) is a field-shifting quantitative molecular imaging method. The dreMR method is expected to produce higher contrast images at low-fields. Our low-field magnet has a small bore and may interact more strongly with the dreMR system causing a quench. No investigation of induced heating within the bore has been carried out for dreMR. Here, we investigate this interaction with our 0.5T superconducting magnet and find that dreMR pulse sequences do not cause significant heating in the magnet. We therefore state that dreMR is safe to carry out in such systems without quenching the magnet. |
2484 | Evaluation of a Novel Acoustic Noise Shield for PET-MR | |
Chen Lin1, LeRoy H Stecker1, Brittany L Benson1, Craig A Hildestad2, Shengzhen Tao1, and Robert A Pooley1 | ||
1Radiology, Mayo Clinic, Jacksonville, FL, United States, 2Mayo Clinic, Jacksonville, FL, United States |
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A novel acoustic noise shield constructed of clear acrylic has been developed and evaluated. The results suggest that: 1) it is effective for MR acoustic noise reduction, 2) PET image quality exceeds ACR accreditation testing standards with the proposed acoustic shield in use, showing its compatibility with PET imaging, 3) there is a small impact on PET SUV which can be compensated with attenuation correction, and 4) it does not cause claustrophobia. |
2485 | Acoustic evaluation of carbon fiber RF shield structure for a 3T head-only imaging system | |
Matthew Tarasek1, Tom Foo1, Mark Vermilyea1, Desmond Yeo1, Isabelle Jansen1, Eric Budesheim 1, and Keith Park1 | ||
1GE Global Research, Niskayuna, NY, United States |
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In this work we evaluate the MRI acoustic changes brought about by modifying the RF shield structure in a head-only (MAGNUS) 3T imaging system. Specifically, we use a standardized acoustic measurement protocol to compare sound pressure levels (SPL) in a fiberglass patient-bore structure to a similar newly developed carbon fiber reinforced polymer (CFRP) structure. Results indicate that a modification of the structural properties of the patient-bore structure properties can provide SPL reduction for MR imaging applications, and is likely due to the different modulus of elasticity between the two materials. |
2486 | MRSaiFE: towards the real-time prediction of tissue heating in MRI - a feasibility study | |
Simone Angela Winkler1, Elizaveta Motovilova1, Sayim Gökyar1, Isabelle Saniour1, Fraser Robb2, and Akshay Chaudhari3 | ||
1Department of Radiology, Weill Cornell Medicine, New York, NY, United States, 2GE Healthcare, Aurora, OH, United States, 3Stanford University, Stanford, CA, United States |
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A crucial safety concern for UHF MRI is the significant RF power deposition in the body in the form of local specific absorption rate (SAR) hotspots, leading to dangerous tissue heating/damage. This work is a proof-of-concept demonstration of an artificial intelligence (AI) based real-time MRI safety prediction software (MRSaiFE) facilitating safe generation of 3T and 7T images by means of accurate local SAR-monitoring at sub-W/kg levels. This feasibility study demonstrates that SAR patterns can be predicted with a root-mean-square error (RMSE) of <11% along with a structural similarity (SSIM) level of >84% for both field strengths. |
2487 | Motion and Pose Variability of SAR Estimation with Parallel Transmission at 7T | |
Amer Ajanovic1, Joseph V Hajnal1,2, Raphael Tomi-Tricot1,3, and Shaihan Malik1 | ||
1Biomedical Engineering Department, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 2Centre for the Developing Brain, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 3MR Research Collaborations, Siemens Healthcare Limited, Frimley, United Kingdom |
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Contemporary safety assessment for parallel transmit (pTx) MRI relies on computationally expensive electromagnetic (EM) simulations; hence, safety evaluations rely on the use of small numbers of models. The effect of patient movement inside the coil on patient safety is, therefore, difficult to capture. In this work we compare 'within-scan' variability with the alternative scenario in which a subject’s head is positioned arbitrarily within the coil, but that this position is different to the one used for the SAR estimation model; we refer to this as ‘pose’ variability. |
2488 | Robustness of pTx safety concepts to varying subjects and subject positions | |
Johannes Petzold1, Bernd Ittermann1, and Frank Seifert1 | ||
1Physikalisch-Technische Bundesanstalt (PTB), Braunschweig and Berlin, Germany |
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This simulation study compares two concepts ensuring IEC-compliant SAR values for parallel transmission (pTx) in respect to their robustness against subject- and position-changes: 1) direct SAR assessment (SL) and 2) an amplitude limit for all pTx channels (AL). For the example case of a 3T pTx body coil, SL resulted in ten-fold the allowed SAR in one model for the same excitation vector that obeys IEC limits in another model. For AL, less than twice the SAR was found in this case. AL allows for a lower safety factor, therefore, resulting in a higher mean(B1+) compared to SL. |
2489 | Radiofrequency safety evaluation and management of the Australian MRI-Linac system | |
Mingyan Li1, Ewald Weber1, Aurelien Destruel2, Feng Liu1, and Stuart Crozier1 | ||
1School of Information Technology and Electrical Engineering, The University of Queensland, Australia, Australia, 2Center for Magnetic Resonance in Biology and Medicine, Aix-Marseille University, MARSEILLE, France |
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The Australian MRI-Linac system has a split magnet with wide opening, which offers treatment flexibility with different patient positioning. However, the versatile patient setup and individual physique differences also lead to uncertainty for specific absorption rate (SAR) management. In particular, a standing patient may have body regions close to radiofrequency (RF) coil rungs, which may lead to high local SAR. In this work, numerical simulations were employed to investigate the SAR distribution while a human model was in different treatment positions and thus give safety management suggestions. A standard whole-body RF coil was also simulated as a reference. |
2490 | Electromagnetic simulation analysis of an RF burn injury case occurred at the elbow-bore wall contact point | |
Minghui Tang1, Kiyoi Okamoto2, and Toru Yamamoto1 | ||
1Faculty of Health Sciences, Hokkaido University, Sapporo, Japan, 2Graduate School of Health Sciences, Hokkaido University, Sapporo, Japan |
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RF burn injuries occasionally occur at the contact points of skin and the bore wall, albeit out of common belief of hazardous loop forming. To investigate the mechanism of the RF burn injury occurred by the bore wall contact, we modeled an elbow-bore wall contact case on an electromagnetic analysis software by using the computable human phantom. The simulated SAR at the contact point varied up to 480% depending on the patient position in a scanner. This tendency was in accordance with the simulated electric field distribution in the scanner which is dominantly determined by the RF transmission coil. |
2491 | A Novel Specific Absorption Rate Prediction Framework Using Multi-Task Feedback Generative Adversarial Learning: Application to 10.5 T Head MRI | |
Jinyoung Kim1, Alireza Sadeghi-Tarakameh1, Angel Torrado-Carvajal2,3, and Yigitcan Eryaman1 | ||
1Center for Magnetic Resonance Research, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 2Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital and Harvard Medical School, Boston, MA, United States, 3Medical Image Analysis and Biometry Laboratory, Universidad Rey Juan Carlos, Madrid, Spain |
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In this study, we propose a novel local SAR prediction framework based on deep learning. To this end, we introduce multi-task feedback adversarial learning to simultaneously predict local SAR distribution and its peak SAR value. The proposed model learns a mapping between simulated B1+ magnitude/tissue property maps and local SAR provided by EM simulations. Given query inputs with the properly trained model, the generator produces the local SAR distribution slice by slice, and the local SAR peak estimator predicts the upper bound of local SAR values. Validation results show that the proposed model may allow online subject-specific local SAR prediction. |
2492 | Realistic model of the 3T Siemens Connectom birdcage coil and its validation | |
Mikhail Kozlov1, Kerrin J. Pine1, and Nikolaus Weiskopf1,2 | ||
1Max Planck Institute for Human Cognitive and Brain Sciences, Leipzig, Germany, 2Felix Bloch Institute for Solid State Physics, Leipzig, Germany |
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We devised a numerical model of a 123.2MHz 32-rung high-pass whole-body birdcage coil of the Siemens 3T Connectom scanner. The model was developed based on realistic geometrical data for most of coil elements and a reverse engineering approach. Our simulations suggest that RF exposure at level of 3.2W/kg head SAR may result in higher than 20W/kg of SAR10g in the Connectom scanner; (ii) B1+ mapping alone cannot be used for validation of numerical model of whole-body birdcage coil, (iii) developed RF-circuit and 3D-EM co-simulation approach with reverse engineering resulted in a reasonable agreement between simulations and measurements in human subject. |
2493 | GPU accelerated calculations of the scattered RF-field due to a dielectric update without extensive pre-calculated data. | |
Peter Stijnman1, Bart Steensma1, Cornelis van den Berg1, and Alexander Raaijmakers1,2 | ||
1Computational Imaging, UMC Utrecht, Utrecht, Netherlands, 2Biomedical Engineering, Eindhoven University of Technology, Eindhoven, Netherlands |
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Previous work showed that the scattered RF-fields created by dielectric pads and medical implants can quickly be calculated. The method requires an extensive offline calculation stage and a lot of memory. We propose an extension to the method that removes these two problems by using a volume integral equation solver. This allows us to do the entire calculation on a GPU for more acceleration. The resulting scattered electric fields have a maximum difference of 3.2% with respect to FDTD, while currently being a 106 times faster. Eventually, we want to use this method for patient-specific implant RF-safety assessment. |
2494 | RF Safety Assessment of High Permittivity Dielectric Pads - Impact of Material Insulation | |
Wyger Brink1, Rob Remis2, and Andrew Webb3 | ||
1Leiden University Medical Center, Leiden, Netherlands, 2Circuits and Systems, dept. of Microelectronics, Delft University of Technology, Delft, Netherlands, 3C.J. Gorter Center, dept. of Radiology, Leiden University Medical Center, Leiden, Netherlands |
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High permittivity dielectric pads are known to be effective for tailoring the RF field and improving image quality in high field MRI systems. Despite the number of studies reporting benign SAR effects, their safety remains a concern and should be evaluated on an application-specific basis using RF simulations. In this work we demonstrate the impact of insulation material on the RF safety of high permittivity pads, using both RF simulations as well as phantom experiments. |
2495 | Advances in Caterpillar Traps: A Highly Flexible, Distributed System of Toroid Cable Traps | |
Ekin Karasan1, Alison Hammerschmidt1, Victor Taracila2, Fraser Robb2, and Michael Lustig1 | ||
1University of California, Berkeley, CA, United States, 2GE Healthcare, Coils, Aurora, OH, United States |
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Conducting wires within the scanner may interact with the transmit field causing high shield currents and posing safety hazards. Closely spaced RF traps are used to mitigate common-mode currents. However, these bulky and rigid traps hinder the flexibility of the cable. We previously proposed caterpillar traps: a distributed system of smaller, flexible toroids covering the full length of the cable. Their potential to attenuate shield currents while being flexed was demonstrated. This work makes several improvements to the manufacturing process to reduce time and cost and improve usability. Furthermore, we present results from experiments to evaluate their performance and robustness. |
2496 | LCCC Balun for RF Coil | |
Xinqiang Yan1,2 and John C. Gore1,2 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radilogical Science, Vanderbilt University Medical Center, Nashville, TN, United States |
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We introduced a novel LCCC lumped-element balun to suppress the unwanted common-mode current in RF coils and RF systems. Unlike the 4-element Lattice balun consisting of two capacitors and two inductors (LCCL), this design has 3 capacitors and only 1 inductor. With fewer inductors (previous lumped-element baluns need at least 2 inductors), this LCCC balun can further be miniaturized and has lower insertion loss. |
2497 | Signal-to-noise-ratio gain and in vivo application of a 13C cryo-coil for hyperpolarized MRSI | |
Luca Nagel1, Geoffrey J. Topping1, and Franz Schilling1 | ||
1Department of Nuclear Medicine, Technical University of Munich, School of Medicine, Klinikum rechts der Isar, Munich, Germany |
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Cryogenically cooled transmit/receive radiofrequency coils (cryocoils) improve the signal-to-noise ratio (SNR) compared to conventional RF coils by minimizing thermal coil noise. The SNR of a cryoprobe, a surface coil at room temperature and a volume coil was assessed using chemical shift imaging of a 13C-urea phantom. Using the cryocoil an SNR improvement up to a factor of 10 compared to conventional coils was observed. In addition, a proof-of-concept in vivo experiment using the 13C-cryocoil for detection of the metabolic turnover of hyperpolarized 13C-pyruvate was successfully performed. |
2498 | Ultra-Flexible 8-Channel Receive Array for 13C Imaging | |
Vitaliy Zhurbenko1, Juan Diego Sánchez Heredia1, Wenjun Wang1, and Jan Henrik Ardenkjær-Larsen1 | ||
1Technical University of Denmark, Kgs. Lyngby, Denmark |
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Imaging of low-abundance nuclei could benefit from close proximity detecting coils. Close proximity is conveniently achieved using flexible arrays, which conform to the shape of the subject. In this work, a design of an 8-element ultra-flexible array for 13C imaging is presented. Each array element includes a low-noise preamplifier with 13C/1H active and passive decoupling, as well as high-power pulse protection circuits. The array is lightweight and easy to handle. The design approach is directly scalable to larger size arrays. |
2499 | Metamaterial Liner RF Head Coil for 23Na and 1H at 4.7 T | |
Adam Maunder1, Ashwin Iyer2, and Nicola De Zanche1 | ||
1Oncology, Medical Physics, Cross Cancer Institute, University of Alberta, Edmonton, AB, Canada, 2Electrical and Computer ENgineering, University of Alberta, Edmonton, AB, Canada |
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Well-established and emerging methods of 23Na sodium imaging in the brain benefit from high field strength, but require imaging sequences that are constrained by specific absorption rate (SAR) limits. Additionally, concurrent proton imaging is desirable for complementary anatomical/structural information. Here, we present a novel metamaterial liner-based MR coil for 23Na/1H imaging at 4.7 T, consisting of longitudinally-spaced rings that alter the effective electromagnetic properties between the liner and outer RF shield (waveguide boundary). In simulation, the metamaterial liner was found to produce lower local 10g averaged SAR for the same mean transmit field relative to a conventional birdcage coil. |
2500 | 1H, 31P, 23Na, and 13C imaging and spectroscopy with a multi-tunable double-coil assembly | |
Viktor Puchnin1, Viacheslav Ivanov1, Mikhail Gulyaev2, and Mikhail Zubkov1 | ||
1Department of Physics and Engineering, ITMO University, Saint-Petersburg, Russian Federation, 2Faculty of Fundamental Medicine, Lomonosov Moscow State University, Moscow, Russian Federation |
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The RF-coils of small-animal scanners often limit the range of accessible nuclei to single- or double-nuclear scanning. Here, a multi-tuneable RF-coil design is investigated. The design comprises a butterfly-type RF-coil for 1H, and a multi-tuneable coil for X-nucleus imaging. The coil assembly is tested in a 7 T scanner. 1H and X-nucleus field maps show good matching between the simulation and experiment. Imaging and spectroscopy experiments provide well-resolved images as well as distinctive spectral peaks corresponding to the phantom compounds. The presented imaging method with single coil assembly is considered a promising expansion of heteronuclear imaging. |
2501 | SNR and B1+ Field Homogeneity of a Koch Fractal Geometry RF Surface Coil for 23Na-MRI | |
Cameron Nowikow1, Paul Polak1, Norman B. Konyer2, Natalia Nikolova3, and Michael D. Noseworthy1,2,3 | ||
1School of Biomedical Engineering, McMaster University, Hamilton, ON, Canada, 2Imaging Research Centre, St. Joseph's Healthcare, Hamilton, ON, Canada, 3Electrical and Computer Engineering, McMaster University, Hamilton, ON, Canada |
||
There is an intrinsic lack of SNR in 23Na-MRI images compared to that of proton-based MRI. It is possible that RF coil geometry can affect the acquired images' SNR. This abstract is an investigation into the B1+ field characteristics of a Koch snowflake fractal RF surface coil to see if the produced field is more homogeneous than that of a standard circular surface coil which could lead to higher SNR in the resultant 23Na images. It was found that the circular geometry produced a more homogeneous field, along with higher SNR than the fractal coil. |
2502 | Towards a cryogenic RF coil array for 13C human head imaging: first experience | |
Wenjun Wang1, Juan Diego Sánchez Heredia2, Vitaliy Zhurbenko1, and Jan Henrik Ardenkjær Larsen2 | ||
1Department of Electrical Engineering, Technical University of Denmark, Kongens Lyngby, Denmark, 2Department of Health Technology, Technical University of Denmark, Kongens Lyngby, Denmark |
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A cryogenic coil and a dedicated cryostat for 13C human head imaging is developed. A 1.90-fold SNR enhancement over a room temperature coil is observed experimentally. To verify the retention of SNR enhancement in arrays, a 4-channel cryogenic coil array and another cryostat are also developed. The superior performance to a room-temperature array is confirmed experimentally. |
2503 | Quantitative Comparison of 31P MRS Imaging Performances between 7T and 10.5T Human Scanners Using a Loop-dipole 31P-1H Probe | |
Xin Li1, Hannes M. Wiesner1, Matt Waks1, Xiao-Hong Zhu1, and Wei Chen1 | ||
1Center for magnetic Resonance Research (CMRR), Department of Radiology, University of Minnesota, Minneapolis, MN, United States |
||
In vivo 31P MRS imaging (MRSI) is important for studying cerebral energy metabolism, intracellular NAD and redox ratio. However, it is challenging to achieve high spatiotemporal resolution owing to limited 31P sensitivity and low phosphorus metabolites concentration. We had demonstrated that ultrahigh field (UHF) could significantly improve the 31P-MRS sensitivity and spectral resolution. In this study, we designed and constructed a loop-dipole 31P-1H probe, which could operate at 7T and 10.5T for quantitative comparison of 31P MRSI signal-to-noise ratio (SNR) between the two fields. We found that the apparent SNR at 10.5T was significantly higher than that of 7T. |
2504 | A nested dual-tuned proton-sodium loop-array transceiver coil on a 9.4T whole-body MRI system | |
Zhe Wang1, Fangrong Zong2, Cheng Fang1, Wenhui Yang3,4, Shasha Yue1, Yan Hou2, Zehui Li2, Tianyu Xie2, Kun Zhang2, Yan Zhuo1,4,5, Xiaohong Joe Zhou6, Xiaoliang Zhang7, and Rong Xue1,4,8 | ||
1State Key Laboratory of Brain and Cognitive Science, Beijing MRI Center for Brain Research, Institute of Biophysics, Chinese Academy of Sciences, Beijing, China, 2Institute of Biophysics, Chinese Academy of Sciences, Beijing, China, 3Institute of Electrical Engineering Chinese Academy of Sciences, Beijing, China, 4University of Chinese Academy of Sciences, Beijing, China, 5CAS Center for Excellence in Brain Science and Intelligence Technology, Chinese Academy of Sciences, Beijing, China, 6Center for MR Research and Departments of Radiology, Neurosurgery and Bioengineering, University of Illinois at Chicago, Chicago, IL, United States, 7Department of Biomedical Engineering, State University of New York at Buffalo, Buffalo, NY, United States, 8Beijing Institute of Brain Disorders, Beijing, China |
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In this study, a nested dual-tuned proton-sodium multi-channel loop-array transceiver coil was designed and constructed for 9.4T MRI, which could provide images for both proton and sodium at the same location. This coil adopts nested structure, which contains 8-channel transceiver loop elements respectively, and each loop is equipped with an independent transmit/receive circuit. The coil array was simulated for B1 field distribution and was further tested on a 9.4T whole-body MRI platform with home-built spectrometer. Proton and sodium images on a water phantom were successfully collected on this system with high quality. |
2505 | Flexible 32-Channel 13C MRI Head Array: An EEG-Lookalike Design Approach | |
Juan Diego Sánchez Heredia1, Wenjun Wang1,2, Vitaliy Zhurbenko2, and Jan Henrik Ardenkjær-Larsen1 | ||
1Department of Health Technology, Technical University of Denmark (DTU), Kgs. Lyngby, Denmark, 2Department of Electrical Engineering, Technical University of Denmark (DTU), Kgs. Lyngby, Denmark |
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We propose a design concept for flexible human head coil arrays applicable to a wide frequency range. Electrically, the design relies on high decoupling obtained through a controlled high mismatched connection to the low-impedance preamplifiers. Mechanically, the array is built into a neoprene EEG cap, and made of regular-copper flexible wire. The array layout is designed to have an axis to stretch along, therefore allowing tight fit to a variety of human-head sizes. A 32-channel prototype for 13C at 3T (32.1 MHz) is presented and evaluated, showing SNR performance superior to a 13C-dedicated volume coil. |
2506 | 9.4 T Double-Tuned 13C/1H Human Head Array Using a Combination of Surface Loops and Dipole Antennas. | |
Nikolai Avdievich1, Georgiy Solomakha2, Loreen Ruhm1, Anke Henning1,3, and Klaus Scheffler1 | ||
1High-field Magnetic Resonance, Max Planck Institute for Bilogical Cybernetics, Tübingen, Germany, 2Physics and Engineering, ITMO University, St. Petersburg, Russian Federation, 3Advanced Imaging Research Center, University of Texas Southwestern Medical Center, Dallas, TX, United States |
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Dipole antennas have been successfully utilized at ultra-high fields (UHF, >7 T) for human body and head imaging. Combining X-nuclei surface loops and 1H dipoles can substantially simplify the design of a double-tuned UHF human head coil. In this work, we developed and constructed a novel 13C/1H human head 9.4 T array coil consisting of eight 13C surface loops and eight 1H folded-end dipoles surrounding the head. We showed that coupling between loops and dipoles can be minimized by placing four 1H traps into each 13C loop. The new coil demonstrated an improved 1H longitudinal coverage and reasonable Tx efficiency. |
2507 | Analysis of common-mode rejection ability and Insertion Loss of Dual band Lattice Balun with non-ideal components | |
Yue Zhu1,2 and Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University, Nashville, TN, United States |
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A dual band Lattice balun was proposed previously, which holds the promise of removing common mode current for both frequencies in dual-tuned MRI coils with a single interfacing unit. However, the previously fabricated unit had a considerable insertion loss at the proton Larmor frequency. In this work, we analyzed how each lumped element will affect this device's performance and optimized the circuit performance based on the analysis. |
2508 | Interleaved nine-leg birdcages for simultaneous geometric decoupling from a double tuned planar array | |
Joseph Busher1, Chenhao Sun2, Travis Carrell1, Edith Valle2, Steven M. Wright1,2, and Mary McDougall1,2 | ||
1Biomedical Engineering, Texas A&M University, College Station, TX, United States, 2Electrical and Computer Engineering, Texas A&M University, College Station, TX, United States |
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This work describes two interleaved nine-leg linear birdcages for geometric decoupling from a double-tuned planar array for 1H and 23Na at 4.7T. An asymmetric design was chosen to create aligned fields to simultaneously decouple the receive array from the two transmit birdcages. This straightforward design provides sufficient decoupling from coils in all six positions in the final array configuration and enables multinuclear multichannel imaging experiments. |
2509 | Flexible 8-Channel Array for Hyperpolarized 13C at 3T (32.1 MHz), with Nearly Identical 23Na (33.8 MHz) Sensitivity Profiles | |
Juan Diego Sánchez Heredia1, Wenjun Wang1,2, James T. Grist3,4,5, Esben Søvsø Szocska Hansen6, Christoffer Laustsen6, Vitaliy Zhurbenko2, and Jan Henrik Ardenkjær-Larsen1 | ||
1Department of Health Technology, Technical University of Denmark (DTU), Kgs. Lyngby, Denmark, 2Department of Electrical Engineering, Technical University of Denmark (DTU), Kgs. Lyngby, Denmark, 3Department of Physiology, Anatomy and Genetics, University of Oxford, Oxford, United Kingdom, 4Oxford Centre for Magnetic Resonance, University of Oxford, Oxford, United Kingdom, 5Department of Radiology, The Churchill Hospital, Oxford University Hospitals NHS Trust, Oxford, United Kingdom, 6The MR Research Center, Department of Clinical Medicine, Aarhus University, Aarhus, Denmark |
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We describe the design of a flexible coil array tuned optimally for 13C MRI at 3T (32.1 MHz), but with the coil coupling coefficients matched to be nearly identical at the 13C and 23Na (33.8 MHz) frequencies. In this way, the array provides the means to obtain accurate sensitivity profiles for hyperpolarized 13C imaging from the high 23Na naturally present in biological tissue. We show the feasibility of this approach, and compare the performance to other 13C coils, showing that the 13C SNR provided by this array is not compromised despite the modification to equalize the 13C and 23Na profiles. |
2510 | Increased B1+ efficiency of a dipole antenna compared to a loop coil for 31P-MRS at 7T: simulations and cardiac MRSI data | |
Jabrane Karkouri1, Saba Shirvani1, Tiger Zhang1, Dennis Klomp2, Martijn Lunenburg3, Ladislav Valkovic4, and Christopher T. Rodgers1 | ||
1Wolfson Brain Imaging Center, University of Cambridge, Cambridge, United Kingdom, 2Department of Radiology, University Medical Center Utrecht, Utrecht, Netherlands, 3Tesla Dynamic Coils, Zaltbommel, Netherlands, 4Oxford Centre for Clinical Magnetic Resonance Research, University of Oxford, Oxford, United Kingdom |
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We evaluated the performance of two RF coil configurations for ultra-high field (7T) 31P-MRS applications in the body. We tested: (A) a dipole Tx/Rx + loop Rx coil vs (B) a quadrature dual-loop Tx/Rx coil. We assessed their relative performance by EM modelling simulations and through phantom and in vivo cardiac scans. Both simulations and experimental verifications indicate that there is notable improvement in terms of B1+ efficiency for the dipole+loop combination compared to quadrature loops. We extrapolate these preliminary findings to predict the performance of the dipole+loop combination if driven at 35kW total like our previous whole-body birdcage coil. |
2511 | Optimized Single-loop Coil with 3D-shaped Design for Simultaneous fMRI and Optical Imaging in Rodent | |
Wen-Ju Pan1, Lei Zhou1, Gloria Perrin Clavijo1, Vahid Khalilzad Sharghi1, and Shella Keilholz1 | ||
1Biomedical Engineering, Emory University/Georgia Institute of Technology, Atlanta, GA, United States |
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Single loop coil was optimized in 3D shape to fitting rodent bran geometry and designed in slim and large center opening to meet the requirement of simultaneous fMRI and optical imaging. Relative to conventional 2D flat loop, the proposed 3D design may allow setting a loop coil closer to rat cerebral hemispheres and save more overhead space for optical imaging configuration than a 2D flat coil while keeping B1 perpendicular to B0. Our 3D-shape modification exhibited significant improvement in overall SNR and signal homogeneity especially in cortical areas and center brain in T2-weighted images, EPI and field maps. |
2512 | Inductively coupled small-diameter volume coils insertable to the knee coil at 7T for MR microscopy | |
Tomohisa Okada1, Shinya Handa2, Bill Ding2, Shin-ichi Urayama1, Koji Fujimoto1, Atsushi Shima3, Takashi Ayaki4, Nobukatsu Sawamoto3, Ryosuke Takahashi4, Hirotaka Onoe1, Tadashi Isa1, and Labros Petropoulos2 | ||
1Human Brain Research Center, Kyoto University, Kyoto, Japan, 2Quality Electrodynamics, Mayfield Village, OH, United States, 3Department of Human Health Sciences, Kyoto University, Kyoto, Japan, 4Department of Neurology, Kyoto University, Kyoto, Japan |
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MR imaging is frequently correlated to histopathology of specimen, and their high-resolution imaging is required. However, it is not usually feasible using the whole-body human MR scanner. We implemented inductively coupled small diameter coils insertable to the knee coil at 7T without modification of the coil interface. Up to isotropic 50 μm imaging was successfully conducted, and fine details of the specimen could be visualized using the same sequence for in vivo scans. The proposed coils are easy to use and will facilitate investigation of image-histopathology correlation. |
2513 | A Simple, Multi-purpose Coil for Improved Mouse Brain Image Quality and Coverage at 3-T MRI | |
Kuan-Hung Cho1, Po-Hsun He1, Hsuan-Han Chiang1, Ming-Jye Chen1, Ezequiel Farrher2, Nadim Jon Shah2,3, Chang-Hoon Choi2, and Li-Wei Kuo1,4 | ||
1Institute of Biomedical Engineering and Nanomedicine, National Health Research Institutes, Miaoli County, Taiwan, 2Institute of Neuroscience and Medicine – 4, Forschungszentrum Juelich, Juelich, Germany, 3Department of Neurology, Faculty of Medicine, RWTH Aachen University, Aachen, Germany, 4Institute of Medical Device and Imaging, National Taiwan University College of Medicine, Taipei, Taiwan |
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For mouse brain imaging, determining the size of a loop coil is a trade-off between SNR and imaging coverage. Here, we propose a multi-purpose coil arrangement incorporating a small loop coil and a position-adjustable add-on saddle coil to enhance the imaging coverage of anatomical images and improve the SNR in the regions distant to the surface coil. The result shows the imaging coverage can be adjustable for targeting different brain regions and demonstrated this design concept in mouse brain imaging experiments. |
2514 | Development of a multi-turn double helix dipole coil for magnetic resonance microimaging of chemically-fixed human embryos at 7T. | |
Yuto Murakami1 and Yasuhiko Terada1 | ||
1University of Tsukuba, Tsukuba, Japan |
||
A double helix dipole (DHD) coil, consisting of two tilted solenoid coils, exhibits the high signal-to-noise ratio (SNR) close to that of an equivalent solenoid whose SNR is almost three times larger than a saddle coil. However, its application to high-field MRI is challenging because of the high inductance. Here, we proposed a new DHD coil design with division capacitors that enables high-field MRI application. As proof-of-concept, we designed a 6-turn DHD coil for MR microimaging of a chemically-fixed human embryo specimen at 7T, and showed that the proposed DHD has nearly twice the SNR of an equivalent saddle coil. |
2515 | Wirelessly controlled stand-alone automatic RF tuning and matching system for preclinical imaging at 7T | |
Sri Kirthi Kandala1 and SungMin Sohn2 | ||
1Biomedical Engineering, Arizona State Universirty, Tempe, AZ, United States, 2Biomedical engineering, Arizona State University, Tempe, AZ, United States |
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Impedance matching of RF coils during MR imaging is crucial to improve SNR and would enhance power transfer efficiency for transmit coil reducing wastage of RF power. This work focuses on presenting a stand-alone system with wireless Automatic Tuning and Matching system (ATM) for transmit (Tx)-only and receive (Rx)-only coils separately. We present separate Tx-only and Rx-only coils with high power and low power ATMs respectively along with a self-triggering circuit for Rx coil decoupling while high power Tx signal is active. |
2516 | Imaging performance of a multi-channel non-human primate coil | |
Daniel Papp1, Urs Schüffelgen2, Mo Shahdloo2, Sebastian W Rieger1,3, Aaron T Hess4, Matthew Rushworth2, and Stuart Clare1 | ||
1Wellcome Centre for Integrative Neuroimaging, FMRIB, Nuffield Department of Clinical Neurosciences, University of Oxford, Oxford, United Kingdom, 2Wellcome Centre for Integrative Neuroimaging, Department of Experimental Psychology, University of Oxford, Oxford, United Kingdom, 3Wellcome Centre for Integrative Neuroimaging, OHBA, Department of Psychiatry, University of Oxford, Oxford, United Kingdom, 4British Heart Foundation Centre of Research Excellence, Department of Cardiovascular Medicine, University of Oxford, Oxford, United Kingdom |
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A 15-channel array coil has been developed for our centre by a coil manufacturer for the purposes of awake behaving macaque fMRI. Here, we evaluated the imaging performance in vivo and on phantoms. Compared to a 4 channel flexible coil, we found significant improvements in SNR and tSNR both in vivo and in phantom studies. Furthermore, we demonstrate the feasibility of multiband and in-plane accelerated acquisitions, up to a multiband factor of 6 with in-plane acceleration of 2. |
3085 | Gradient Characterization for High Performance Gradients | |
Nastaren Abad1, Afis Ajala1, Yihe Hua1, and Tom K.F Foo1 | ||
1General Electric Global Research, Niskayuna, NY, United States |
||
Impulse response function (IRF) harvesting is a powerful technique for gradient characterization. In this study a field monitoring system was utilized to characterize a head-only, high-performance gradient coil (MAGNUS), enabling expansion of the spatial response pattern into higher order spherical harmonics. The predictive power of IRF-estimated waveforms and field evolution is demonstrated by comparing to nominal and active field monitored approaches for arbitrary gradient waveforms. The calculated modulation function indicated good correspondence for arbitrary waveforms and k-space trajectories varying with slew rate, amplitudes and number of interleaves. |
3086 | Measuring the Gradient Impulse Response Function (GIRF) for UTE Imaging on an MR-Linac | |
Rosie Goodburn1, Tom Bruijnen2, Wajiha Bano1, Uwe Oelfke1, and Andreas Wetscherek1 | ||
1Radiotherapy and Imaging, The Institute of Cancer Research, London, United Kingdom, 2Department of Radiotherapy, University Medical Center Utrecht, Utrecht, Netherlands |
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Synthetic CT (sCT) is a key component of adaptive MR-guided radiotherapy. Generation of thoracic sCT is challenging and benefits from ultrashort echo-time (UTE) imaging that provides contrast in short-T2* tissues such as bone and lung. However, UTE imaging is susceptible to artifacts caused by eddy currents and gradient delays. In this work, we measured the gradient impulse response function (GIRF) of an MR-Linac with standard scanner hardware and used it to retrospectively correct k-space trajectories. Images reconstructed with GIRF and gradient-delay corrected trajectories exhibited higher image quality, including reduced halo artifacts, blurring, destructive phase artifacts, and improved uniformity and contrast. |
3087 | Phantom-based high-resolution measurement of the gradient system transfer function | |
Hannah Scholten1, Manuel Stich2, and Herbert Köstler1 | ||
1Department of Diagnostic and Interventional Radiology, University of Würzburg, Würzburg, Germany, 2Siemens Healthcare, Erlangen, Germany |
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The gradient system transfer function (GSTF) constitutes a comprehensive tool for correcting k-space trajectory distortions due to gradient infidelities. We developed a new phantom-based measurement approach that allows determining the GSTF with a high frequency resolution without relying on long readout durations. Our first results include self- and B0 cross-terms with high SNR and resolutions below 10 Hz, resolving the true width of several resonances. The high resolution enables us to capture long-lasting eddy current effects, which is especially promising for the application of GSTF-based correction methods in, for example, diffusion-weighted imaging. |
3088 | Calibration of Concomitant Field Compensation using Phase Contrast MRI | |
Thomas K.F. Foo1, Louis Frigo2, Myung-Ho In3, Nastaren Abad1, Vincent B Ho4, and Matt A Bernstein3 | ||
1GE Research, Niskayuna, NY, United States, 2GE Healthcare, Waukesha, WI, United States, 3Mayo Clinic, Rochester, MN, United States, 4Uniformed Services University of the Health Sciences, Bethesda, MD, United States |
||
A phase contrast pulse sequence was modified to use a single-sided bipolar encoding to calibrate the transverse gradient offsets for asymmetric gradient coils. The phase difference approach cancels the concomitant gradient field effects from all gradient waveforms except for the bipolar gradient waveforms. By fitting the measured phase offset in the phase difference images to the applied bipolar gradient amplitudes, the gradient offset value can be calculated. This was used for pre-emphasis compensation for the zeroth and first order concomitant gradient fields. |
3089 | Direct Comparison of Gradient Modulation Transfer Functions and Acoustic Noise Spectra of the same MRI at High- (3T) and Lower-Field (0.75T) | |
Hannes Dillinger1, Sebastian Kozerke1, and Christian Guenthner1 | ||
1Institute for Biomedical Engineering, University and ETH Zurich, Zurich, Switzerland |
||
In this work, gradient fidelity is compared between high-field (3T) and lower-field (0.75T) configurations on the same MRI system by measuring the Gradient Modulation Transfer Function (GMTF) and audio noise spectra. Results demonstrate that at lower field mechanical resonances are reduced, leading to improved gradient fidelity and reduction of audio noise levels of up to 70%. Furthermore, it is shown that spectral peaks in the audio spectrum can be related to resonances in the GMTF, which suggests mechanical resonances can be identified using the audio spectrum. |
3090 | PSF-based reconstruction for removal of artifacts caused by misalignment between a silent gradient insert and the body gradients | |
Edwin Versteeg1, Dennis W.J. Klomp1, and Jeroen C.W. Siero1,2 | ||
1Radiology, University Medical Center Utrecht, Utrecht, Netherlands, 2Spinoza centre for neuroimaging Amsterdam, Amsterdam, Netherlands |
||
A silent gradient axis driven at 20 kHz can reduce sound in MR-sequences. This silent gradient axis consists of a separate coil that is positioned on the patient table and operated in synergy with the whole-body gradients. The positioning of this coil with respect to the whole-body gradients is prone to operator errors which leads to image artifacts. In this work, we show that this misalignment can be characterized and corrected by measuring the point spread function (PSF) of the silent gradient axis. Using this method, a significant reduction in ghosting artifacts was observed in phantom experiments. |
3091 | Eddy current correction for field probes mounted in a head coil | |
Jennifer Nussbaum1, Maria Engel1, and Klaas Paul Pruessmann1 | ||
1Institute for Biomedical Engineering, ETH Zurich and University of Zurich, Zurich, Switzerland |
||
Concurrent acquisition of dynamic fields has become a prominent way to correct for field imperfections. However, when using field probes in close proximity to a head coil, the field measurement can be corrupted by eddy currents on the head coil that are induced by the gradient fields. In this work, we provide a one-time calibration solution to correct for this issue. |
3092 | Design and Implementation of High Switching Frequency Gradient Power Amplifier Using eGaN Devices | |
Soheil Taraghinia1, Volkan Acikel2, Reza Babaloo1,3, and Ergin Atalar1,3 | ||
1UMRAM, Bilkent University, Ankara, Turkey, 2Aselsan A.S., Ankara, Turkey, 3Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey |
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In this work, a switching H-bridge gradient power amplifier utilizing eGaN devices is implemented. A single-stage 150 V/ 50 A full-bridge GPA for an insert gradient array system at 1 MHz effective switching frequency is fabricated and tested. Pulse width modulation signals are generated digitally using a Virtex 7 family FPGA board. A single-stage LC low pass filter is designed to attenuate the ripple current. |
3093 | Droop compensation of gradient current waveforms in gradient array systems | |
Reza Babaloo1,2, Soheil Taraghinia2, and Ergin Atalar1,2 | ||
1Department of Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey, 2National Magnetic Resonance Research Center (UMRAM), Ankara, Turkey |
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Providing accurate gradient currents is challenging due to the nonlinearity of the gradient system arising from gradient power amplifiers and power supply stages which causes droop in the output currents. This work introduces a nonlinear model for the gradient array system by using the state-space averaging technique and the nonlinear inversion of the model compensates for droop. The feasibility of the method is depicted by simulation and experimental results. The proposed method can provide desired currents by lower voltages which results in minimizing the needed power. It is also possible to use small capacitors to lower the cost of system. |
3094 | Fast and quiet MPRAGE using a silent gradient axis at 7T – subject experience and qualitative image assessment | |
Sarah M Jacobs1, Edwin Versteeg1, Leonie NC Visser2, Anja G van der Kolk1,3, Dennis WJ Klomp1, and Jeroen CW Siero1,4 | ||
1Department of Radiology and Nuclear Medicine, University Medical Center Utrecht, Utrecht, Netherlands, 2Alzheimer Center Amsterdam, Department of Neurology, Amsterdam Neuroscience, Vrije Universiteit Amsterdam, Amsterdam UMC, Amsterdam, Netherlands, 3Department of Radiology, the Netherlands Cancer Institute, Amsterdam, Netherlands, 4Spinoza Centre for Neuroimaging Amsterdam, Amsterdam, Netherlands |
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Acoustic noise can negatively impact patients from anxiety and communication problems to transient and permanent hearing loss. In this pilot study we used a silent gradient axis that is switched at the inaudible frequency of 20 kHz with a silent readout module implemented in an MPRAGE sequence, and investigated subject experience and image quality of fast and quiet anatomical brain imaging at 7T. Here we show preliminary evidence that our silent gradient axis with silent readout module incorporated into a T1-weighted MPRAGE sequence is perceived more quiet and positive and delivers images of largely acceptable quality. |
3095 | Gradient induced electric field within a shoulder cut-out gradient coil built for head and neck imaging. | |
Arjama A Halder1,2, Eric J Lessard1,2, William B Handler1, and Blaine A Chronik1,2 | ||
1xMR Labs, Physics and Astronomy, London, ON, Canada, 2Medical Biophysics, Western University, London, ON, Canada |
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This abstract aims to investigate the electromagnetic environment within a high-performance shoulder cut-out gradient coil designed to be used as a part of an all-in-one platform for head and neck imaging applications. The results achieved in this abstract and future measurements that will be performed with this coil will allow the quantification for gradient induced electric field effects experienced by patients and ensure that the coil is within the expected PNS limits. |
3096 | Approaching order of magnitude increase of gradient strength: Non-linear breast gradient coil for diffusion encoding | |
Sebastian Littin1, Tristan A. Kuder2, Feng Jia1, Arthur Magill2, Philipp Amrein1, Frederik B. Laun3, Sebastian Bicklehaupt4, Mathias Davids5,6,7, Valerie Klein5,7, Mark E. Ladd2, and Maxim Zaitsev1,8 | ||
1Department of Radiology, Medical Physics, University Freiburg, Faculty of Medicin, Freiburg, Germany, 2Medical Physics in Radiology, German Cancer Research Center, Heidelberg, Germany, 3Department of Radiology, MR Physics, University Medical Center Erlangen, Erlangen, Germany, 4Department of Radiology, University Medical Center Erlangen, Erlangen, Germany, 5Department of Radiology, A. A. Martinos Center for Biomedical Imaging, Charlestown, MA, United States, 6Harvard Medical School, Boston, MA, United States, 7Computer Assisted Clinical Medicine, Heidelberg University, Medical Faculty Mannheim, Heidelberg, Germany, 8High Field MR Center Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria |
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Local gradient coils allow for enhanced performance in terms of both gradient amplitude and switching rate. We recently presented the concept of a single channel non-linear breast gradient coil. Here we show results of the characterization, safety assessment and initial diffusion encoded images from phantom experiments of the prototype coil. Is an order of magnitude increase of gradient strength for diffusion weighting feasible using local gradient coils? |
3097 | Towards a More Power Efficient Two-Channel Biplanar Z-Gradient Coil Design Using Target Field Method | |
Haile Baye Kassahun1, Sadeq S Alsharafi1, Ahmed M Badawi1, and AbdEl-Monem M El-Sharkawy1 | ||
1Systems and Biomedical Engineering, Cairo University, Cairo, Egypt |
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A two-channel biplanar Z-gradient coil design is introduced by dividing the conventional coil surface into two sections radially. The corresponding lower and upper sections are driven by the same current strength but in opposite directions. Coils were designed using the Fourier series expansion (target field) method. For the same target field, the dissipated power of the two-channel biplanar Z-gradient coil was lower than that of the conventional coil (with corresponding dimensions) by at least 25% thereby reducing the ohmic losses. In the future, the benefit of using multi-channel bi-planar gradient coils may be further investigated. |
3098 | Design of Biplanar Matrix Z2 Nonlinear Gradient Coil with An Open Structure for O-Space imaging | |
Congcong Liu1,2, Shi Su1, Ye Li1,2, Xin Liu1,2, Hairong Zheng1,2, Dong Liang1,2,3, and Haifeng Wang1,2 | ||
1Paul C. Lauterbur Research Center for Biomedical Imaging, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, 2Shenzhen College of Advanced Technology, University of Chinese Academy of Sciences, Shenzhen, China, 3Research Center for Medical AI, Shenzhen Institute of Advanced Technology,Chinese Academy of Sciences, Shenzhen, China |
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In this work, a novel biplanar matrix Z2 nonlinear gradient coil with an open structure has been designed, which could be employed in open spatial low-field MRI system, and an efficient encoding strategy for O-Space imaging was proposed in combination with the proposed biplanar matrix nonlinear gradient coil, which has the potential to shift the center placements (CP’s) in nonlinear gradient imaging without an external linear gradient field. The biplanar Z2 encoding field generated by a nonlinear gradient element consisting of curve segments was optimized and implemented to show the feasibility of this proposed biplanar matrix coil and encoding approach. |
3099 | MRI Hybrid Gradient Coil Equipped with a Programmable Z-Array and Conventional X- and Y- Elements | |
Manouchehr Takrimi1 and Ergin Atalar1,2 | ||
1UMRAM, Bilkent University, Ankara, Turkey, 2Department of Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey |
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A novel hybrid gradient coil consisting of two conventional actively shielded x/y gradient coils and a programmable active-shield z-gradient array coil is introduced and simulated. The proposed hybrid gradient coil can dynamically provide the required magnetic profile based on diverse applications in MRI. This is achieved by using a set of independent power amplifiers that feed the conventional coils and the array elements. To show the flexibility, three magnetic profiles are simulated: (a) a conventional profile; (b) a profile with twice z-gradient intensity and a shifted FOV; (c) a profile with quadruple z-gradient intensity when the active-shield is reverse fed. |
3100 | Mechanical Tilt-Induced Gradient Fields for Low-Field Spokes-and-Hub Permanent Magnet MR Imagers | |
Irene Kuang1, Jason Stockmann2,3, Elfar Adalsteinsson1,4, and Jacob White1 | ||
1Electrical Engineering and Computer Science, Massachusetts Institute of Technology, Cambridge, MA, United States, 2A. A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States, 3Harvard Medical School, Boston, MA, United States, 4Institute for Medical Engineering and Science, Massachusetts Institute of Technology, Cambridge, MA, United States |
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As recently demonstrated by Cooley et al., for Halbach-array based permanent-magnet MR imagers, time-varying encoding fields can be generated mechanically, by rotating the entire array. In this paper we show that in spokes-and-hub based permanent magnet imagers, time-varying encoding fields can also be generated mechanically, but with much smaller motions. In particular, we show that a quarter-degree magnet tilt, along an easily precessed axis, can produce a spatially-discriminating field gradient. We demonstrate the spatial discrimation using both simulation and measurements from our recently-presented prototype imager. |
3101 | Systematic, Linear Algebra-based Dimensional Analysis of Gradient Inductance Scaling with Coil Radius | |
Matt A Bernstein1 and Seung-Kyun Lee2 | ||
1Radiology, Mayo Clinic, Rochester, MN, United States, 2Biomedical Engineering, Sungkyunkwan University, Suwon, Korea, Republic of |
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Applying systematic dimensional analysis based linear algebraic methods, we derive the important scaling relation for MR gradient design: gradient coil inductance L scales as the square gradient efficiency (measured in T/m/A) and the fifth power of radius. The inclusion of "turns" as a unit in the dimensional matrix produces the result uniquely, greatly simplifying the analysis. |
3102 | Acceleration of magnetic field calculation of permanent magnet arrays for their optimizations | |
Ting-Ou Liang1, Yi-Dan Chen2, Shao Ying Huang2, and Erping Li1 | ||
1Zhejiang University, Hangzhou, China, 2Singapore University of Technology and Design, Singapore, Singapore |
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Two current-model-based approaches are presented to accelerate the calculation of the magnetic field of permanent-magnet-array(PMA) that consists of magnet blocks. It enables a speedy convergence of optimization of a PMA design that is a key component of the popular body-part-dedicated portable MRI in the recent years. This method can be extended to magnet of other shapes. Both Halbach(60blocks) and sparse Inward-Outward ring-pair-PMA(1,200 blocks) are used as examples to demonstrate the speed and accuracy of the algorithm. The best acceleration is 78.92% and 77.94%calculation-time reduction compared to the conventional nested for-loops, and 99.81% and 99.91%reduction compared to FEM-based commercial software. |
3103 | Design and Development of a Hybrid Helmholtz Coil System for Production of Low Magnetic Field System (up to 7 mT) | |
Yenal Gokpek1 and Ozkan Doganay1 | ||
1Institute of Health Sciences, Ege University, IZMIR, Turkey |
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In this study, the design and construction of a hybrid Helmholtz coil system and numerical modelling were investigated for production of homogeneous magnetic field over a volume of interest that consist of cylindrical geometry (h=700mm, r=90mm). The 4‑coil system was constructed and tested by two commercially available low power DC power supplies. The magnetic field created by the 4‑coil system was found to be B=2.5182±0.0035mT over the volume of interest. We found that the simulated and measured magnetic fields are in good agreement (R=0.9759, p<0.05). |
3104 | D-T2 Distribution Obtained Using CPMG-only Sequence Compared with Traditional SE-CPMG Sequence on the Single-sided NMR Device | |
Ziyi Pan1, Jieying Zhang1, Hai Luo2, Weiqian Wang2, Xiao Chen2, Ziyue Wu2, and Hua Guo1 | ||
1Center for Biomedical Imaging Research, Department of Biomedical Engineering, School of Medicine, Tsinghua University, Beijing, China, 2Marvel Stone Healthcare, Wuxi, Jiangsu, China |
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Two-dimension (2D) diffusion-relaxation (D-T2) correlation measured by a low-cost, portable single-sided NMR system can separate fat and water in biological tissues (for example for liver steatosis detection). Diffusion-editing CPMG sequence is commonly used for such measurement. Recently, a novel approach is proposed to measure the D-T2 correlation using the simplest CPMG-only sequence. The CPMG-only sequence is less sensitive to motion, and can extend to systems with more imperfect magnetic and radiofrequency fields. This work compares the proposed CPMG-only sequence with the traditional diffusion-editing SE-CPMG sequence. Results show the SE-CPMG and CPMG-only sequences can achieve comparable performance on water-fat separation. |
3105 | In-vivo B0 shimming of the liver using a local array of shim coils in combination with 2nd order spherical harmonics at 7T | |
Lieke van den Wildenberg1, Quincy van Houtum1, Wybe van der Kemp1, Catalina Arteaga de Castro1, Alex Bhogal1, Paul Chang2, Sahar Nassirpour2, and Dennis Klomp1 | ||
1Radiology Department, UMC Utrecht, Utrecht, Netherlands, 2MR Shim GmbH, Reutlingen, Germany |
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Maximizing shim performance, particularly for larger organs such as the liver, is crucial at ultra-high field MRI due to the increased sensitivity to B0 field inhomogeneity. The conventional shimming in most MRI systems at ultra-high field, provides insufficient correction. However, by combining the available 2nd order spherical harmonic fields with an external array of 16 local shim coils, the magnetic field homogeneity in the liver is improved by as much as 44%. |
3106 | “RF transparent” local B0 shim coil | |
Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radilogical Science, Vanderbilt University Medical Center, Nashville, TN, United States |
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Multiple coils shimming technology has been demonstrated as a promising approach to reduce the B0 inhomogeneity in MRI. However, strong coupling arises when local DC coils are placed close to the imaging area and RF coils. To solve this problem, we proposed a novel local DC shim coil that has little effect on the RF coils, which we called "RF transparent" DC coil. This concept was validated by EM simulation, bench test, and MR experiments. The RF transparent concept will bring much more freedoms to DC coil design (such as many turn and irregular shaped). |
3107 | Shim Coils Tailored for Correction of B0 Inhomogeneity in the Human Brain (SCOTCH) at Ultra High Field | |
Bruno Pinho-Meneses1, Jason Stockmann2,3, Edouard Chazel1, Paul-François Gapais1, Eric Giacomini1, Franck Mauconduit1, Alexandre Vignaud1, Michel Luong4, and Alexis Amadon1 | ||
1Université Paris-Saclay, CEA, CNRS, BAOBAB, NeuroSpin, Gif-sur-Yvette, France, 2Athinoula A. Martinos Center for Biomedical Imaging, Charlestown, MA, United States, 3Harvard Medical School, Boston, MA, United States, 4Université Paris-Saclay, CEA, Institut de Recherche sur les Lois Fondamentales de l'Univers, Gif-sur-Yvette, France |
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A Singular Value Decomposition based Multi-Coil Array for B0 shimming of the human brain was designed from a database of 100 δB0 fieldmaps. An optimized 2-layer 36-channel MCA design was obtained and constructed. The system was characterized and measured fieldmaps were used for comparison to expected performance from ideal simulated fields. The static whole-brain and dynamic slice-wise shimming was validated in-vivo and assessed with GRE and EPI acquisitions at 7 Tesla. |
3108 | Designing a high-density combined RF/B0 shim coil for imaging the brain at 7T | |
Paul Chang1, Sahar Nassirpour1, Kaizad Rustomji2, Elodie Georget2, Ingmar Voogt3, Aidin Haghnejad3, Evita Wiegers4, Jannie Wijnen4, and Dennis Klomp4 | ||
1MR Shim GmbH, Reutlingen, Germany, 2Multiwave Imaging, Marseille, France, 3WaveTronica, Utrecht, Netherlands, 4UMC Utrecht, Utrecht, Netherlands |
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Increased B0 inhomogeneity at ultra-high fields continues to pose a challenge for many MR applications. Local arrays of shim coils offer a complimentary way of reducing the local inhomogeneities. In this study, practical design considerations for a combined RF/B0 shim 7T head coil were assessed. Numerical simulations were used to find the optimal size and distance of the shim coils relative to Rx loops. These results were then verified in a bench test. Finally, having these considerations in mind, it was shown that by optimizing the arrangement of the shim coils improved B0 homogeneity can be achieved. |
3109 | Shielded coaxial cable coils for transmit, receive and B0 shimming in a 7T neck array | |
Vincent O. Boer1, Jan Ole Pedersen2, Hørður Andreasen3, Sadri Güler1,4, Vitaliy Zhurbenko3, Jason Stockmann5, Irena Zivkovic6, and Esben Thade Petersen1,4 | ||
1Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital, Hvidovre, Denmark, 2Philips Healthcare, Copenhagen, Denmark, 3Department of Electrical Engineering, Technical University of Denmark, Kongens Lyngby, Denmark, 4Section for Magnetic Resonance, DTU Health Tech, Technical University of Denmark, Kongens Lyngby, Denmark, 5Athinoula A Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Charlestown, MA, United States, 6Electrical Engineering department, Technical University of Eindhoven, Eindhoven, Netherlands |
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Shielded coaxial RF coils show very low coupling between elements, and are ideal for building transmit-receive arrays. In this work we extended a 6 element transceive array with B0 shim capabilities. |
3110 | Improving MRI Near Metal with Local B0 Shimming using a Unified Shim-RF Coil (UNIC): First Case Study, Hip Prosthesis in Phantom. | |
Fardad Michael Serry1, Junzhou Chen1,2, Anthony G Christodoulou1,2, Yuheng Huang1,2, Fei Han3, Won Bae4,5, Christine Chung4,5, Richard Handlin1, John Stager1, Matthew Dausch1, Yubin Cai1, Yujie Shan1, Yucen Liu1, Yibin Xie1, Xiaoming Bi3, Rohan Dharmakumar1,2, Zhaoyang Fan1,6, Debiao Li1,2, Hsin-Jung Yang1, and Hui Han1 | ||
1Biomedical Imaging Research Institute, Cedars-Sinai Medical Center, Los Angeles, CA, United States, 2Department of Bioengineering, UCLA, Los Angeles, CA, United States, 3Siemens Medical Solutions USA, Inc., Los Angeles, CA, United States, 4University of California, San Diego, San Diego, CA, United States, 5VA Medical Center, San Diego, CA, United States, 6University of Southern California Department of Radiology, Los Angeles, CA, United States |
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Metal artifact image degradation can interfere with tissue status assessment. Metal artifact reduction pulse sequences, mainly spin-echo based, and scanner B0-shimming can mitigate the artifacts. We have tested in a metal hip prosthesis phantom improving shimming locally with a novel technology that integrates separate but co-planar RF receive and shim arrays, expanding the freedom to position shim coils and shape B0, independently of the RF coil geometry and pulse sequence. Metal-induced signal-void artifact was reduced in GRE scans, revealing up to 50% additional area around the prosthesis. The sequence-agnostic technology may help improve MRI near metal prostheses and interventional devices. |
3111 | Shimming-Toolbox: An open-source software package for performing realtime B0 shimming experiments | |
Alexandre D'Astous1, Ryan Topfer1, Gaspard Cereza1, Eva Alonso-Ortiz1, Lincoln Craven-Brightman2, Jason Stockmann2,3, and Julien Cohen-Adad1,4 | ||
1NeuroPoly Lab, Institute of Biomedical Engineering, Ecole Polytechnique, Montreal, QC, Canada, 2Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States, 3Harvard Medical School, Boston, MA, United States, 4Functional Neuroimaging Unit, Centre de recherche de l'Institut universitaire de gériatrie de Montréal, Montreal, QC, Canada |
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As MRI static fields get increasingly stronger, reducing $$$B_0$$$ inhomogeneities becomes more important but also challenging. When standard active shimming on commercial systems is insufficient for researchers’ needs, alternative approaches such as external shim or hybrid AC/DC coils can be used. However, in order to perform advanced shimming experiments, a proper software ecosystem is required and there is currently no open-source solution for transparent and reproducible shimming experiments. Here we introduce the Shimming Toolbox (https://shimming-toolbox.org), an open-source software package for performing and prototyping static, dynamic and realtime $$$B_0$$$ shimming experiments. |
3112 | Magnetic fields produced by simple coils inside finite-length cylindrical passive shields with end-caps | |
Richard W. Bowtell1, Michael Packer 2, Peter Hobson 2, James Leggett1, Niall Holmes1, Paul Glover 1, Matthew Brookes1, and Mark Fromhold2 | ||
1Sir Peter Mansfield Imaging Centre, University of Nottingham, Nottingham, United Kingdom, 2School of Physics and Astronomy, University of Nottingham, Nottingham, United Kingdom |
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Cylindrical shields formed from material of high permeability are commonly used in providing low-magnetic field environments for experimental research. Cylindrical coils are often sited inside such shields to produce controlled patterns of field variation, but interaction of the coils with the mu-metal distorts the fields. Here we show how to analytically calculate the fields that are produced by simple coils inside a finite-length, cylindrical mu-metal shield with end-caps, and report experimental measurements on two different coils (loop and saddle), demonstrating excellent agreement with the theory. Optimal spacings of Helmholtz-type coils inside finite-length shields are also derived using the analytic expressions. |
3113 | Hardware developed for phase and frequency locking of interleaved MRI and DMI studies | |
Terence W. Nixon1, Yanning Liu1, Henk M. DeFeyter1, Scott McIntyre1, and Robin A. de Graaf1 | ||
1Yale University, New Haven, CT, United States |
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Deuterium metabolic imaging (DMI) is a powerful new method to supplement the anatomical and functional information of MRI with a metabolic component. A reduction in overall scan time by interleaving MRI and DMI is clinically relevant, whereas research applications can benefit from complimentary information obtained through interleaved acquisition. Because most MR scanners only allow acquisition of one frequency, additional hardware is required to enable interleaved acquisition. Here we present hardware for the upconversion of 2H data into the 1H receive path and present a solution to achieve effective phase and frequency locking. |
3114 | Simultaneous transmit/receive for Bloch-Siegert encoding: a feasibility study | |
Baosong Wu1, Sajad Hosseinnezhadian2, Yonghyun Ha2, Kartiga Selvaganesan2, Charles Rogers III2, Kasey Hancock2, Gigi Galiana2, and R. Todd Constable2 | ||
1Department of Radiology and Biomedical Imaging, Yale School of Medicine, NEW HAVEN, CT, United States, 2Department of Radiology and Biomedical Imaging, Yale School of Medicine, New Haven, CT, United States |
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This work presents the feasibility of Bloch-Siegert (BS) frequency encoding for magnetic resonance (MR) applications requiring a simultaneous transmit and receive system. RF frequency encoding technique is referred to receiving MR signal while existing one offset-field radiation, which can be considered as a radio frequency interference(RFI). A prototype was built demonstrating first MR experiment and preliminary data using this method. Our system is currently a research technology with the goal of generating a low-field and point-of-care medical imaging system using novel RF encoding. |
3115 | RF sinc pulse distortion compensation using multiple square pulses at 1 MHz. | |
Yonghyun Ha1, Kartiga Selvaganesan1, Baosong Wu1, Kasey Hancock1, Charles Rogers III1, Sajad Hosseinnezhadian1, Gigi Galiana1, and R. Todd Constable1 | ||
1Department of Radiology and Biomedical Imaging, Yale School of Medicine, New Haven, CT, United States |
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The response times of RF coils in MRI are long when operating at low B0 field, making it difficult to achieve the desired pulse shape in the coil. Compensation pulses are shown that were optimized using a series of square pulses. Both the duration and amplitude of the compensation elements were calculated with Q-factor which was calculated from the ring-down time measured using a sniffer coil. The SNRs of the echo signal acquired using compensated pulse was compared with those of signal obtained with uncompensated pulses and showed significant improvements of 51.5%. |
3116 | Automatic 3D B1 field mapping using 3D printer and digital oscilloscope for gradient-free MRI system | |
Yonghyun Ha1, Kartiga Selvaganesan1, Sajad Hosseinnezhadian1, Baosong Wu1, Kasey Hancock1, Gigi Galiana1, and R. Todd Constable1 | ||
1Department of Radiology and Biomedical Imaging, Yale School of Medicine, New Haven, CT, United States |
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For gradient-free RF spatial encoding, MR image based B1 mapping methods cannot be used due to the absence of gradient coils. However, it is important to get a B1 map particularly if Bloch-Siegert shift encoding is used. In this work, a method to automatically measure the amplitude of B1 field is introduced. Three perpendicular pickup loops were used to measure the B1 field in three orthogonal axes simultaneously. The position of the pickup loops was controlled by 3D printer, and the peak-to-peak voltage of the coupled signal was automatically saved using PC oscilloscope. |
3117 | Inhomogeneity and ramping effects in field-cycled quantitative molecular MRI | |
Matthew A. McCready1, William B. Handler1, Francisco Martinez2,3, Timothy J. Scholl2,3, and Blaine A. Chronik1,2 | ||
1Physics and Astronomy, Western University, London, ON, Canada, 2Medical Biophysics, Western University, London, ON, Canada, 3Robarts Research Institute, Western University, London, ON, Canada |
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Delta relaxation enhanced magnetic resonance (dreMR) is a field-shifting quantitative molecular imaging method. The dreMR method may be used to produce images with signal proportional to concentration of contrast agents with longitudinal relaxivity dispersion. Here we find that field inhomogeneities and ramping periods, which were previously ignored, cause significant errors in dreMR images. These errors include apparent non-zero signal from dispersion-free tissue, and apparent change in signal due to contrast agents. We show that these effects can be mitigated by use of an improved homogeneity design method, and increased slew rates. |
3118 | Very low field MRI for brain imaging | |
Samson Lecurieux Lafayette1 and Claude Fermon1 | ||
1SPEC - CEA Saclay - Université Paris Saclay, Saclay, France |
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Classic high field MRI is a powerful tool in healthcare. However, it is an expensive and complex installation and it might be useful to supply a less convenient device adapted to a lot of usage not requiring high field potential. We have developed a very low field MRI working at between 1mT and 10mT. Main static field is providing by a water-cooled resistive magnet. In order to achieve an iso spatial resolution of 2mm in a reasonably short time of acquisition, we have worked on adapted sequences including compressed sensing and optimized detection with parallel acquisition. |
3119 | Comparison of SNR between a low-field (0.26T) Tabletop-MRI and a clinical high-field (3T) scanner | |
Robert Kowal1, Enrico Pannicke2, Marcus Prier1, Ralf Vick2, Georg Rose3, and Oliver Speck1 | ||
1Department of Biomedical Magnetic Resonance, Otto von Guericke University, Magdeburg, Germany, 2Chair of Electromagnetic Compatibility, Otto von Guericke University, Magdeburg, Germany, 3Chair in Healthcare Telematics and Medical Engineering, Otto von Guericke University, Magdeburg, Germany |
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The SNR-performance of a low-field (0.26T) Tabletop-MRI-system was experimentally compared to a high-field (3T) clinical scanner. The SNR of simple FID sequences were evaluated for RF-units with identical coil and sample geometries as well as T/R-switch designs. The SNR was calculated from time signals and put into perspective to compute the relative SNR-performance of the Tabletop-system which was measured at 11.3%. Additional compensations for several differing experimental conditions were carried out. The full comparison suggests limiting factors in the equivalent measurement in the clinical scanner which can result in more SNR loss than expected. |
3120 | Initial Experience of Body Imaging at 5T | |
Zhenhua Shen1, Xuchen Zhu1, Shihong Han1, Fuyi Fang1, Wei Luo1, Shao Che1, Zidong Wei1, Jinguang Zong1, Yongquan Ye2, Bo Li1, Shuheng Zhang1, Anthony Vu2, Weiguo Zhang2, and Guobin Li1 | ||
1United Imaging Healthcare, Shanghai, China, 2UIH America, Inc., Houston, TX, United States |
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For the first time, routine clinical body imaging with large FOV on a whole-body 5T MRI system is demonstrated. With multi-channel RF parallel transmission hardware architecture and static RF shimming techniques, the uniformity of the RF transmission field is shown to be well controlled for imaging quality guarantee. Preliminary results show great promise for body imaging at 5T. |
3121 | A sample temperature control system for post mortem MRI | |
Sebastian Walter Rieger1, Karla Miller1, Peter Jezzard1, and Wenchuan Wu1 | ||
1Wellcome Centre for Integrative Neuroimaging, University of Oxford, Oxford, United Kingdom |
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In post mortem MRI, the absence of body temperature autoregulation can lead to significant local heating in the sample from RF absorption and heat from the environment. This can interfere with scanning (such as diffusion measurements) and in unfixed samples, accelerate tissue decomposition. In this work, a temperature control system is presented which enables prolonged scanning of post mortem samples at a stable temperature while preserving tissue. |
3122 | Compact MRI bioreactor for real-time monitoring 3D printed tissue-engineered constructs. | |
Jean-Lynce GNANAGO1,2,3,4,5,6, Tony GERGES1,2,3,4,5,6, Laura Chastagnier1,2,4,6,7,8,9,10, Emma Petiot2,4,6,7,8,9,10, Vincent SEMET1,2,4,5,6, Philippe Lombard1,2,3,4,5,6, Christophe Marquette1,2,4,6,7,8,9,10, Michel Cabrera1,2,3,4,5,6, and Simon Auguste Lambert1,2,3,4,5,6 | ||
1Université Claude Bernard Lyon 1, VILLEURBANNE, France, 2INSA LYON, VILLEURBANNE, France, 3Ecole Centrale Lyon, Ecully, France, 4CNRS, VILLEURBANNE, France, 5AMPERE UMR 5005, VILLEURBANNE, France, 6Université de Lyon, VILLEURBANNE, France, 73d.FAB, VILLEURBANNE, France, 8CPE Lyon, VILLEURBANNE, France, 9ICBMS, VILLEURBANNE, France, 10UMR 5246, VILLEURBANNE, France |
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Tissue engineering for regenerative medecine is a growing field which faces structural and functional challenges at different scales. Real-time quantitative 3D characterization of tissues both in vitro and in vivo would help biologists assessing their methods. Magnetic Resonance Imaging (MRI) offers the possibility to perform such characterization non-invasively. We propose here a 7T MRI coil integrated within a perfusion tissue engineering bioreactor to perform tissue assessments throughout its growth. The MRI bioreactor is built using 3D printing and plastronics. This works resulted in a successful observation of a bioprinted tissue with a 75 µm in plane resolution. |
3123 | Characterization of 3AM diffusion MRI phantoms via microscopy, and phase-contrast micro-CT | |
Farah Mushtaha1,2, Tristan K. Kuehn1,3, Omar El-Deeb4, Seyed A. Rohani3, Luke W. Helpard3, Hanif Ladak2,3,5, Amanda Moehring6, Corey A. Baron1,2,3,7, and Ali R. Khan1,2,3,7 | ||
1Robarts Research Institute, London, ON, Canada, 2Medical Biophysics, Schulich School of Medicine and Dentistry, Western University, London, ON, Canada, 3School of Biomedical Engineering, Western University, London, ON, Canada, 4Neuroscience, Western University, London, ON, Canada, 5Department of Electrical and Computer Engineering, Western University, London, ON, Canada, 6Biology, Western University, London, ON, Canada, 7The Brain and Mind Institute, Western University, London, ON, Canada |
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Validating diffusion MRI (dMRI) representations and models of brain tissue is challenging because there is no reference ground-truth for in vivo scans. We investigate the microstructural characteristics of 3D printed axon-mimetic (3AM) phantoms as a dMRI validation tool using fluorescence microscopy and phase-contrast micro computed tomography (micro-CT). Both microscopy and micro-CT yielded pore diameters of ~ 8 μm. We constructed a 2-compartment microstructural model using microscopy and micro-CT data to simulate 3AM dMRI scans, and compared the observed metrics from in-vivo scans and simulation data. |
3124 | A phantom system for evaluating the effect of lipid and iron composition on qMRI parameters | |
Rona Shaharabani1, Shir Filo1, Oshrat Shtangel1, and Aviv Mezer1 | ||
1The Edmond and Lily Safra Center for Brain Science, The Hebrew University of Jerusalem, Jerusalem, Israel, Jerusalem, Israel |
||
Neurodegenerative diseases such as Alzheimer, Parkinson, and Multiple sclerosis are often linked to abnormal changes in lipids and iron. Lipids are the main components of any membrane, including myelin, and iron is an essential brain’s trophic. The interaction of lipids and iron with water protons is considered to be a major contributor to the brain’s MRI signals. Here we examine the combined effects of the iron and lipid compositions on quantitative MRI parameters using a novel phantom system. We quantitatively characterize the R2* dependence on lipid and iron concentrations. |
3325 | Single Half-Cylinder B0 Shim Coil for the Knee | |
Mingdong Fan1, Sugandima Nishadi Weragoda1, Benjamin Cheung1, Michael Martens1, Labros Petropoulos2, Xiaoyu Yang2, Shinya Handa2, Noah Deetz2, Hiroyuki Fujita2, and Robert Brown1 | ||
1Case Western Reserve University, Cleveland, OH, United States, 2Quality Electrodynamics, Mayfield, OH, United States |
||
The void under the knee of a supine patient leads to localized B0 magnetic field distortions due to air-tissue susceptibility differences. To cancel this local artifact, low-order harmonic shims are inadequate, but a single local shim coil can produce higher harmonic suppression. A half-cylinder version wrapped on the outside of the RF coil has been constructed and used to obtain in vivo data consistent with the magnetic field simulations. The detailed results support the possibility of an effective knee shimming approach. |
3326 | B0 Susceptibility-Induced Geometric Image Distortion at Low-Field for Magnetic Resonance Imaging in Radiation Therapy | |
Manuel Schneider1, Sylvain Doussin1, Dieter Ritter1, and Martin Requardt1 | ||
1Siemens Healthcare GmbH, Erlangen, Germany |
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Our main purpose was to quantify geometric image distortion due to reduced susceptibility at 0.55T compared to 1.5T. Therefore, Bloch simulations of a digital phantom and a 2D GRE sequence were performed. The simulations at both field strengths were calculated twice: once without considering B0 susceptibility, and once considering B0 susceptibility artefacts. Additionally, 3D T2 SPACE images with high readout bandwidth as well as echo-planar diffusion-weighted images were obtained and compared in n=3 volunteers. Less geometric distortion due to B0 susceptibility artefacts was observed at 0.55T compared to higher field strengths. |
3327 | Hybrid Active and Passive Local Shimming (HAPLS) for Two-region Magnetic Resonance Imaging (MRI) | |
Zhi Hua Ren1, Jason P. Stockmann2,3, Andrew Dewdney4, and Ray F. Lee1 | ||
1Zuckerman Institute, Columbia University, New York, NY, United States, 2Harvard Medical School, Boston, MA, United States, 3Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Boston, MA, United States, 4Siemens Healthcare GmbH, Erlangen, Germany |
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When the bilateral regions of intersest are far off isocenter like in case of shoulders or for brains of two people to be scanned simultaneously, the image quality often suffers from non-optimal spherical harmonic based shimming routine and higher field inhomogeneity in large off-isocenter regions. To address these challenges, a hybrid active and passive local shimming (HAPLS) technique is proposed to shim two isolated areas in one field of view (FOV) simultaneously. Both the simulation and experimental results validated that HAPLS can complementarily address the bifocal and high-order inhomogeneities in the two-region MRI. |
3328 | Characterization of 3rd order shim system of human 7T MRI system demonstrates the need of real shim field calibration | |
Mahrshi Jani1, Ivan Dimitrov1, Bei Zhang1, Binu Thomas1, and Anke henning1 | ||
1Advance Imaging Research Center, UT Southwestern Medical Center, Dallas, TX, United States |
||
To perform magnetic resonance imaging (MRI) and magnetic resonance spectroscopy (MRS)in high and ultra-high field homogeneity of field (B0) is required to improve image quality and obtainable metabolic information form MRI scan. In this work we present, real shim field calibration to improve homogeneity of B0 field. The vendor implemented B0 shim system consists of one 0th order, three 1st order, five 2nd order and seven 3rd order shim coils. The proposed calibration to be implemented in existing stand-alone Philips system and further application software shall be developed to integrate latest algorithms and methods to B0 shimming. |
3329 | The Spherical Harmonic Rating: A Metric for B0 Shim System Performance Assessment | |
Bruno Pinho-Meneses1 and Alexis Amadon1 | ||
1Université Paris-Saclay, CEA, CNRS, BAOBAB, NeuroSpin, Gif-sur-Yvette, France |
||
Different B0 shim system designs are tested on two distinct fieldmap databases for assessment of commonly employed metrics for evaluation of B0 inhomogeneity mitigation. We verify that those metrics might not always be the best choice for performance analysis, as, for a same shim system, they may provide hardly comparable values across sites. We then propose a novel, simple and robust metric for shim system analysis, the Spherical Harmonic Rating, which is shown to provide consistent performance across sites, providing an equivalency of the shim system to a Spherical Harmonics basis. |
3330 | On-coil B0 shimming with a flexible coaxial coil element at 3 T | |
Bernhard Gruber1,2, Maxim Zaitsev1, and Elmar Laistler1 | ||
1High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria, 2Department of Radiology, A.A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Harvard Medical School, Charlestown, MA, United States |
||
The combination of highly flexible RF coils and on-coil shimming is an interesting concept, in particular for applications in body parts that have strong inter-patient variability, such as breast, thorax or abdomen. The well-known AC/DC approach on rigid standard loop coils involves many bulky RF chokes and would therefore not be suitable for flexible coil elements. In the presented approach coaxial coils are used instead, where no segmenting capacitors and correspondingly no RF chokes are required. We demonstrate that this conceptual design shows good RF performance and the created magnetic fields for shimming are in good agreement with analytical calculations. |
3331 | Open-Source Gradient Impulse Response Function (GIRF) calibration measurements and their impact in Spiral acquisition | |
Tiago Timoteo Fernandes1, Andreia S Gaspar1, Andreia C. Freitas1, Nuno A. da Silva2, and Rita G Nunes1 | ||
1Institute for Systems and Robotics - Lisboa and Department of Bioengineering, IST-UL, Lisbon, Portugal, 2Hospital da Luz Learning Health, Lisbon, Portugal |
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A major challenge in MRI, particularly when aiming to reduce equipment costs, is to be able to cope with imperfect hardware performance. Even when using current clinical systems, calibration is often required to reduce image artifacts; an example is the impact of eddy-currents in spiral readouts. Here we controlled for this effect by determining the gradient impulse response function (GIRF) using an open source calibration pulse sequence, demonstrating the impact of the GIRF and its correction both through simulation and in real phantom data. This implementation will contribute towards the development of open source tools for spiral imaging. |
3332 | Correct K-space coordinates and gradient coupled $$$B_0$$$ variation for Spiral imaging using the current monitor | |
Tzu-Cheng Chao1, Jürgen Rahmer2, Sandeep Ganji3, Guruprasad Krishnamoorthy3, Peter Börnert2, and James G. Pipe1 | ||
1Department of Radiology, Mayo Clinic, Rochester, MN, United States, 2Philips Research, Hamburg, Germany, 3Philips Healthcare, Gainesville, FL, United States |
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Error from inaccurate eddy current assessment has been a critical issue in spiral imaging. A model is established to estimate both the gradient field and its induced B0 variation from the measured current of the gradient amplifier. The correction improves the geometric consistency between both spiral-in and spiral-out images. The results suggest that the present work have potential to improve quality of spiral imaging. |
3333 | On the predictability of B0 maps at ultra-high fields using deep learning | |
Vidya Prasad1, Sharun S Thazhackal1, Ashvin Srinivasan1, Suja Saraswathy1, Jaladhar Neelavalli2, and Umesh Rudrapatna2 | ||
1Philips Research, Philips, Bangalore, India, 2Philips Healthcare, Philips, Bangalore, India |
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UHF-MRI offers increased scanning sensitivity, but suffers from pronounced B0 inhomogeneities. B0 maps are essential for shimming and reconstruction at UHFs, but suffer from scanning overhead and low measurement confidence. Predicting B0 maps from survey scans can effectively address these issues. We assessed predictability of brain B0 maps at 7T and 11.7T using deep learning on a large synthetic B0 map dataset created from 540 CT images. We found that deep learning can predict 1) spherical harmonics for shimming and 2) the complete B0 maps. Our results indicate that B0 predictions work as effectively as acquiring B0 maps for shimming. |
3334 | A new route of ultrahigh field MRI shimming: hybrid superconducting matrix coil and multi-order spherical harmonics room-temperature shim coils | |
Yaohui Wang1,2, Qiuliang Wang1,2, Yang Liu1, Jigang Zhao1, Hui Wang1, Junsheng Cheng1, and Feng Liu3 | ||
1Institute of Electrical Engineering, Chinese Academy of Sciences, Beijing, China, 2University of Chinese Academy of Sciences, Beijing, China, 3School of Information Technology and Electrical Engineering, The University of Queensland, Brisbane, Australia |
||
A new route for ultrahigh field MRI shimming was proposed which utilized hybrid superconducting matrix coil and multi-order room-temperature shim coils. The proposed scheme was aimed to create a stable and accurate shimming solution for high homogeneous magnetic field magnet. A real 9.4T whole-body MRI magnetic field profile was used to validate the shimming strategy and a remarkable effect was achieved. Therefore, the new shimming method deserves to generalize to ultrahigh field MRI system. |
3335 | Eight channel B0 shim array as add-on for ultra-high field systems | |
Jan Ole Pedersen1, Esben Thade Petersen2,3, Jason Stockmann4, and Vincent O. Boer2 | ||
1Philips Healthcare, Copenhagen, Denmark, 2Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital, Hvidovre, Denmark, 3Section for Magnetic Resonance, DTU Health Tech, Technical University of Denmark, Kgs Lyngby, Denmark, 4Athinoula A Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Charlestown, MA, United States |
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We have simulated and manufactured a shim coil array specifically designed to address fronto-temporal B0 inhomogeneities at 7T. The shim array is driven by an open-source amplifier, and facilitates slice-wise dynamic shimming. Complexity and costs are purposely kept low to allow manufacturing without prior expertise in electronics design and without access to extensive electronics manufacturing facilities. |
3336 | Studies of the static field homogeneity artefacts induced by the diamagnetism of HTS coils and solution to avoid them | |
Aimé Labbé1, Rose-Marie Dubuisson1, Jean-Christophe Ginefri1, Cornelis J van des Beek2, Luc Darrasse1, and Marie Poirier-Quinot1 | ||
1Université Paris-Saclay, CEA, CNRS, Inserm, BioMaps, Orsay, France, 2Université Paris-Saclay, CNRS Center for Nanoscience and Nanotechnology, Palaiseau, France |
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High-Temperature Superconducting (HTS) radiofrequency coils can improve sensitivity by more than an order of magnitude, but their propensity to warp the magnetic field as a result superconducting diamagnetism could cause image degradation. We report on the observation of these B0 artefacts. They are shown to be predominant at lower working temperatures of the HTS coil (60 K) and negligible at 80 K and can be avoided altogether by cooling the HTS coil in B0. We also propose a phenomenological model of these field perturbations. This work studies and solves an important issue in the integration of HTS coil in MRI. |
3337 | Bloch-Siegert |B1+|-Selective Excitation Pulses | |
Jonathan B Martin1, Christopher E Vaughn1, Mark A Griswold2, and William A Grissom1 | ||
1Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 2Radiology, Case Western Reserve University, Cleveland, OH, United States |
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We present a new class of pulses which utilize the Bloch-Siegert shift to localize a |B1+| selective excitation. The summation of a far-off-resonant pulse inducing a |B1+|-dependent Bloch-Siegert shift and a frequency-selective excitation pulse excites spins depending on the strength of transmit field that they experience. The passband of the pulse can be shifted by adjusting the frequency modulation of each of the component pulses. We verify the ability of the new pulse to produce a selective excitation in simulation and on a scanner. |
3338 | B1+ Homogenization in 3D Liver MRI at 7 Tesla Using Eight-Channel Parallel Transmission: Kt-points vs. Phase Shimming | |
Bobby Runderkamp1, Thomas Roos2, Wietske van der Zwaag2, Matthan Caan3, Gustav Strijkers3, and Aart Nederveen1 | ||
1Radiology and Nuclear Medicine, Amsterdam UMC, Amsterdam, Netherlands, 2Spinoza Center for Neuroimaging, Amsterdam, Netherlands, 3Department of Biomedical Engineering and Physics, Amsterdam UMC, Amsterdam, Netherlands |
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Abdominal MRI at ultra-high field benefits from increased SNR but is challenged by high B1+-inhomogeneity. We use eight-channel parallel transmission to homogenize B1+ signal in 7T liver MRI and compare CP-transmission against phase shimming and a kt-points pulse. Increased signal homogeneity was obtained with the kt-points pulse and phase shimming compared to CP-transmission for small volunteers. Combining the kt-points pulse with a compressed sensing reconstruction facilitated single breath-hold high-resolution liver MRI. With improved B1-mapping and kt-point optimization, kt-points is expected to also improve homogeneity in larger volunteers, and to outperform phase shimming in achieving homogeneous signal in 7T liver MRI. |
3339 | Magnitude Least Squares RF Shimming with Singular Vector Minibatching | |
Jonathan B Martin1, Benjamin M Hardy2, and William A Grissom1 | ||
1Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 2Physics and Astronomy, Vanderbilt University, Nashville, TN, United States |
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Magnitude-least squares optimization is widely used to design RF shims that produce homogeneous B1+ fields at high field strengths, but the MLS optimization problem is non-convex and prone to becoming stuck in local minima corresponding to unacceptable voids in the shimmed field. We describe a simple, improved Gerchberg-Saxton algorithm for MLS RF shimming in which randomly selected subsets of the B1+ map matrix's singular vectors are used in each shim update. Shims are then refined using conventional GS. Simulations of 8- and 30-channel head coils at 7T verify the method's robustness, and demonstrate advantages over conventional RF shim design techniques. |
3340 | A universal framework to build digital reference objects for evaluation of quantitative MRI analysis with multiple measurements | |
Henry Szu-Meng Chen1, Brian A Taylor1, Joshua P Yung1, Ping Hou1, R. Jason Stafford1, and Ho-Ling A Liu1 | ||
1Imaging Physics, MD Anderson Cancer Center, Houston, TX, United States |
||
We propose a framework to easily design and generate digital reference object (DRO) s that conforms with DICOM standard for testing quantitative MRI analysis. The method focuses on using existing phantom scan as the basis and allows user to customize the phantom’s geometry and signal model. We generated a number of DRO for T2* and DSC quantitation and analyzed them with two different software as proof-of-concept. |
3341
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Robust real-time 3D motion estimation with MR-MOTUS on an MR-LINAC: a multi-subject validation study | |
Niek RF Huttinga1, Tom Bruijnen1, Cornelis AT van den Berg1, and Alessandro Sbrizzi1 | ||
1Department of Radiotherapy, Computational Imaging Group for MR therapy & Diagnostics, University Medical Center Utrecht, Utrecht, Netherlands |
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In this work we tighten the gap towards clinical application of MR-MOTUS for real-time tracking of non-rigid 3D respiratory motion-fields during MR-guided radiotherapy. The framework is extended from an experimental setting on a conventional 1.5T MR-scanner, to a practical setting on an MR-LINAC: multi-coil and free-breathing data acquisitions, and the possibility for validation at high temporal resolution. 3D motion-field reconstructions are performed in 160ms/dynamic, for a total of five volunteers. Validations show that spatially realistic motion-fields are reconstructed that have 0.94$$$\pm$$$0.018 temporal correlation with a conventional respiratory-motion surrogate, while satisfying the clinical latency requirement of 5Hz for MR-guided radiotherapy. |
3342 | Investigation of respiration-induced changes of the scattering matrix by EM simulations and a breathing body model | |
Natalie Schön1, Frank Seifert1, Gregory J. Metzger2, Bernd Ittermann1, and Sebastian Schmitter1,2 | ||
1Physikalisch-Technische Bundesanstalt (PTB), Braunschweig and Berlin, Germany, Berlin, Germany, 2Center for Magnetic Resonance Research, University of Minnesota, Minneapolis, MN, United States |
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Respiratory motion is a fundamental challenge for thorax MR imaging, particular at ultra-high fields. Recent in-vivo studies have shown that the coil's time-dependent scattering matrix (S-Matrix) can be used for respiration gating to minimize those artefacts. Here, we present electromagnetic simulations of the respiration-induced changes of the transmit RF coil’s S-matrix. Analysing the impact of breathing patterns (conventional, chest, abdominal) illustrates the combined effects of chest/diaphragm motion. The type of respiratory motion and RF coil geometry, position and element type are shown to impact the S-Matrix with implications on coil performance, respiratory triggering, power monitoring and RF pulse design. |
3343 | Using gradient-readout, fast spectroscopic imaging and a 3D multi-echo GRE acquisition for scanner Quality Assurance (QA) | |
Claudiu Schirda1 | ||
1Radiology, University of Pittsburgh School of Medicine, Pittsburgh, PA, United States |
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We propose using a gradient readout, fast MRSI acquisition and a support or stand-alone 3D multi-echo, 3-point Dixon GRE scan for MRI scanner and coil quality assurance (QA). The fast MRSI acquisition with the support 3D GRE scan uses the BRAINO phantom, takes less than 10 minutes and could be used for 1 to 3 months QA. A modified (with an increased FOV), stand-alone 3D GRE scan, takes 3-minutes, could be used either with a spherical or cylindrical phantom and is proposed for daily QA, in addition to the manufacturer EPI-based stability scan. Fully automated reconstruction programs provided at github.com/FastMRSI. |
3344 | A New Representation of the Gradient System Transfer Function Using a Practical Algorithm of Finite Impulse Response Filters | |
Hidenori Takeshima1 | ||
1Advanced Technology Research Department, Research and Development Center, Canon Medical Systems Corporation, Kanagawa, Japan |
||
This work proposes a new representation of the gradient system transfer function (GSTF) based on finite impulse response (FIR) filters. FIR filters can represent arbitrary gradient functions but are not used because of their computational complexity. The proposed method represents the GSTF as a set of average coefficients and their durations. Input signals are represented as sums of signals for the same durations. On an update step, only two signals are accessed for each duration. Therefore, as confirmed experimentally, the proposed method can process arbitrary gradient functions in acceptable computational time, without using infinite impulse response (IIR) filters. |
3345 | Cube set for the quantification of 3-dimensional spatial resolution in MR- micro imaging and microscopy (a = 128 - 4 µm) using 2-photon lithography | |
Andreas Georg Berg1,2, Stefan Hengsbach3, and Klaus Bade3 | ||
1Center for Medical Physics and Biomedical Engineering High field MR-Center, Medical University of Vienna, Vienna, Austria, 2High-Field MR-Center (MRCE), Medical Universits of Vienna, Vienna, Austria, 3Karlsruhe Nano Micro Facility (KNMF), Karlsruhe Institute of Technology (KIT), Leopoldshafen-Eggenstein, Germany |
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Quality-control for systematic improvements in 3D-isotropic spatial resolution of the MR-imaging system up to the microscopic range becomes increasingly relevant not only for preclinical imaging but also for High-Field-MR human scanners. The design of a prototype phantom, comprising a set of 3D-cubes and an exemplary MR-microscopic evaluation is presented. The extraordinary challenges on accurate bar-width-to-cavity ratios for the cube range from periodicity a=128µm down to a=4µm are dealt with using 2-photon-lithography as manufacturing technology. The spatial resolution for 3D isotropic imaging can be checked qualitatively and quantitatively by interpolation of the Modulation-Transfer-Function demonstrated on a 3D-GRE sequence as an example. |
3346 | En Route to multiphasic anthropomorphic MR phantoms: An additive manufacturing approach applying silicone 3D-printing techniques | |
Wolfgang Kilian1, Rüdiger Brühl1, Yasser Abdulhadi1, and Bernd Ittermann1 | ||
1Physikalisch-Technische Bundesanstalt (PTB), Berlin, Germany |
||
Stable and well characterized anthropomorphic MR-phantoms for quantitative MRI of T1 and T2 measurements are still lacking. We investigate the potential application of additive manufacturing of silicone to produce multi-compartment MR-phantoms with well characterized relaxation properties. Various two-component silicone types with different mixture ratios were investigated. Additionally, the influence of admixing colors to modulate relaxation times was studied. First bi-phasic test samples were designed, produced by different commercial 3D printing sources, and characterized. |
3347 | En route to multiphasic anthropomorphic MR phantoms: A new mold-based approach applying gel-based preparation to real MR-datasets geometries | |
Adriano Troia1, Umberto Zanovello1, Luca Zilberti1, Matteo Cencini2, Michela Tosetti2,3, David Kilian4, Martina Capozza5, Wolfgang Kilian6, and Tuğba Dışpınar Gezer7 | ||
1INRIM, Turin, Italy, 2IRCCS Stella Maris, Pisa, Italy, 3IMAGO7 Foundation, Pisa, Italy, 4Centre for Translational Bone, Joint and Soft Tissue Research, Faculty of Medicine and University Hospital TUD, Dresden, Germany, 5Department of Molecular Biotechnology and Health Sciences UNITO, Turin, Italy, 6Physikalisch-Technische Bundesanstalt, Braunschweig, Germany, 7National Metrology Institute, TUBITAK, Istanbul, Turkey |
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Anthropomorphic phantoms for MRI imaging are rapidly evolving also thanks to the increase of 3D printing technologies. Their realization may represent an important support for the implementation of advanced quantitative imaging technique such as Magnetic Resonance Fingerprinting (MRF)or Electrical Properties Tomography (EPT). Even if formulations of gel based tissue-mimicking materials have been widely explored, generally they lacked in achieving the simultaneous tuning of electrical and relaxation properties of the mimicked tissues. In this study, customized moulds of white and grey matter are combined to realize brain-like gel phantoms in which relaxation times, conductivity and permittivity have been measured. |
3348 | A Method for Alignment of an Augmented Reality Display of Brain MRI With The Patient’s Head | |
Christoph Leuze1, Supriya Sathyanarayana1, Bruce L Daniel1, and Jennifer A McNab1 | ||
1Radiology, Stanford University, Stanford, CA, United States |
||
We present a method for alignment of augmented reality display of brain MRI with the patient’s real-world head with potential applications to an AR-neuronavigation system that relies on a see-through display. |
3349 | Specialized Computational Methods for Denoising, B1 Correction, and Kinetic Modeling in Hyperpolarized 13C MR EPSI Studies of Liver Tumors | |
Philip Meng-en Lee1, Hsin-Yu Chen1, Jeremy W Gordon1, Zihan Zhu1, Peder EZ Larson1, Nicholas Dwork1, Mark Van Criekinge1, Lucas Carvajal1, Michael A Ohliger1, Zhen J Wang1, Duan Xu1, John Kurhanewicz1, Robert A Bok1, Rahul Aggarwal2, Pamela N Munster2, and Daniel B Vigneron1 | ||
1Department of Radiology & Biomedical Imaging, University of California, San Francisco, San Francisco, CA, United States, 2Department of Medicine, University of California, San Francisco, San Francisco, CA, United States |
||
The inhomogeneous B1 excitation profile of 13C surface transmit/receive coils provides high SNR near the surface, but results in a spatially-varying B1+. For accurately quantifying the pyruvate to lactate conversion rate (kPL), the flip angle needs to be corrected based on the B1 excitation profile. Simultaneously, random noise in hyperpolarized spectral data obscures peaks of downstream metabolites. In this work, we developed and tested a specialized computational pipeline incorporating denoising and a B1 excitation field correction method that improved quantitative kinetic rate analyses of hyperpolarized 13C MRSI scans of liver tumor patients acquired with a T/R 13C surface coil. |
3350 | A magnetic susceptibility phantom with large range of negative/positive values for quantitative validations | |
Alexey Dimov1, Kelly Gillen1, and Yi Wang1 | ||
1Radiology, Weill Cornell Medicine, New York, NY, United States |
||
A magnetic susceptibility phantom with a large range of negative to positive susceptibility values relative to water is demonstrated for validating quantitative susceptibility mapping (QSM) and related quantitative MRI techniques. The phantom consists of vials with various concentrations of paramagnetic Gadolinium contrast agent (Gd) and diamagnetic calcium chloride (CaCl2) solutions. Compared to previously reported phantoms, this phantom is easy to construct and highly stable and has minimal effects of unwanted air bubbles. |
3351 | 3D Printed MRI Knee Phantom for Imaging Safety and Protocol Studies at Ultrahigh Fields | |
Leo Konst Marecki1, Eric Konst Marecki1, and Xiaoliang Zhang1 | ||
1Biomedical Engineering, SUNY University at Buffalo, Buffalo, NY, United States |
||
Most utilized phantoms for determining the SAR compose of a uniform material to determine the properties of each coil and the exposure time to remain below the FDA guidelines and ensure patient safety. Accurate modeling of the tissue permittivity, conductivity, and geometry will provide more accurate methods to measure the SAR of each organ for a variety of RF coil systems. Our results showed that utilizing 3D printed Nylon containers and Polyvinylpyrrolidone (PVP), NaCl, and water solutions can be used to model the geometry and tissue characteristics of the human knee. |
3352 | Development of an anthropomorphic torso and left ventricle phantom for flow and respiratory motion simulation | |
Tito Körner1, Stefan Wampl1, Marcos Wolf1, Martin Meyerspeer1, Maxim Zaitsev1,2, Wolfgang Birkfellner1, and Albrecht Schmid1 | ||
1High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria, 2Medical Physics, Department of Radiology, University Medical Center Freiburg, Freiburg, Germany |
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Development of motion compensation strategies is challenging, especially when involving volunteer measurements due to high demands to subject compliance and low reproducability. In this work a human shaped torso phantom, capeable of simulating respiratory motion of a left ventricle phantom including blood flow simulation is presented. A tracking algorithm is applied in postprocessing to acquired images containing simulated respiratory motion. Comparison to motion tracking data from an external sensor show good agreement proving the setup to be an environment with high reproducability and hence ideal for the purpose to develop and evaluate motion compensation strategies. |
3353 | 3D printed head-shaped phantom with lipid layer and brain-mimicking metabolites for 7 Tesla MRI and MRSI | |
Rita Schmidt1,2, Ghil Jona3, and Edna Furman-Haran2,3 | ||
1Neurobiology, Weizmann Institute of Science, Rehovot, Israel, 2The Azrieli National Institute for Human Brain Imaging and Research, Weizmann Institute of Science, Rehovot, Israel, 3Life Sciences Core Facilities, Weizmann Institute of Science, Rehovot, Israel |
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Moving to ultra-high fields (≥7T), the inhomogeneity of both RF and static magnetic fields increases, which motivates to design a realistic head-shaped phantom. In this study, a 3D-printed head-shaped phantom with brain mimicking metabolites and lipid layer examined for 7T MRI and MRSI. The phantom was designed to resemble the brain with respect to B0 and B1 distributions, metabolites and lipid layer. We examined it for 1H MRS and MRSI, especially in the lipid layer vicinity. We also demonstrated in EPI that the Fat Suppression pulse flip angle can be optimized to minimize the lipid artifact and reduce the SAR. |
3354 | Oil-in-water emulsions for tissue simulation in magnetic resonance imaging: Determination of MR-properties of emulsifiers | |
Victor Fritz1, Petros Martirosian1, Jürgen Machann1,2, Rolf Daniels3, and Fritz Schick1 | ||
1Section on Experimental Radiology, University of Tübingen, Tübingen, Germany, 2Institute for Diabetes Research and Metabolic Diseases of the Helmholtz Centre Munich at the University of Tübingen, Tübingen, Germany, 3Institute of Pharmaceutical Technology, University of Tübingen, Tübingen, Germany |
||
The aim of this work was to develop stable and homogeneous oil-in-water emulsions for tissue simulation in MRI. For this purpose, three different emulsifiers (polysorbate 60, sodium dodecyl sulfate (SDS), and soy lecithin) were examined for their stabilizing ability. In addition, their potential impact on the MR-measurements was investigated. Sufficient stability can be achieved using both emulsifier, polysorbate and lecithin. Emulsions stabilized by SDS showed a visually lower stability. Due to its sufficient stabilizing ability, promising relaxometric properties (r1,lecithin=0,11wt%-1s-1, r2,lecithin =0,62wt%-1s-1), and no additional spectral resonances, lecithin is suggested as the preferred emulsifier for use in MRI. |
3355 | 1:1 Scale Agar-Agar Paramagnetic Phantom for Brain and Cervical Spine MRI | |
Elif Aygun1,2, Ahmet Rahmetullah Cagil1,2, and Emine Ulku Saritas1,2,3 | ||
1Department of Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey, 2National Magnetic Resonance Research Center (UMRAM), Bilkent University, Ankara, Turkey, 3Neuroscience Graduate Program, Bilkent University, Ankara, Turkey |
||
Phantoms doped with paramagnetic materials are commonly used for quality assessment of MRI protocols and image reconstruction techniques. These phantoms are typically prepared using cylindrical containers and mimic the T1 /T2 characteristics of human tissue. In this work, we propose a 1:1 scale human head and neck agar-agar phantom prepared using a 3D human model. The phantom mimics human tissue characteristics while incorporating the skull and cervical vertebrae. The MRI images show that the phantom closely matches human anatomy, and the susceptibility artifacts in EPI images successfully mimic those seen during in vivo imaging of the brain and spine. |
3356 | MRI System Phantom: assessing the MR visible thermometer, scanner geometric distortion corrections, and effect of fill conductivity | |
Stephen E Russek1, Kathryn E Keenan1, Karl F Stupic1, Teryn S Wilkes2, Ramesh Karki3, and Todor Karaulanov4 | ||
1NIST, Boulder, CO, United States, 2Intermountain Neuroimaging Consortium, University of Colorado, Boulder, CO, United States, 3University of Colorado Anschutz, Radiological Sciences, Aurora, CO, United States, 4CaliberMRI, Inc., Boulder, CO, United States |
||
Using the MRI system phantom we demonstrate the utility of the embedded MR-readable thermometer to measure and correct for temperature variations, demonstrate the use of the fiducial array to characterize scanner geometric distortions and the efficacy of software distortion corrections, and finally look at the effect of the electromagnetic properties of the phantom fill on quantitative measurements. |
3357 | A novel MRI phantom to study the fluid dynamics of the glymphatic system: a proof-of-concept study | |
Endre Grøvik1,2, Elisabeth Lysvik1, Robin Bugge1, Kyrre Emblem1, Trine Hjørnevik1, Svein-Are Vatnehol1, and Tryggve Storås1 | ||
1Oslo University Hospital, Oslo, Norway, 2University of South-Eastern Norway, Drammen, Norway |
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The proposed glymphatic system is hypothesized to be a waste-clearance system of the cerebrospinal fluid (CSF) through the perivascular and interstitial spaces of the brain. The details of this system, and its contribution to the delivery of nutrients and eliminating waste products, are yet to be established. Here we present a tailored MRI phantom to simulate the fluid dynamics of the CSF in the perivascular space. This glymphatic ultra-slow flow phantom facilitates testing of MRI flow measurements in a controlled environment, enabling optimization of MRI scan parameters to allow accurate measurements of glymphatic flow in the human brain. |
3358
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Reaching low-gadolinium concentration detection through sequences optimization on a dedicated phantom | |
Emilie Poirion1, Corentine Marie2, Marine Boudot de La Motte3, Chloé Dupont4, Jean-Claude Sadik1, and Julien Savatovsky1 | ||
1Hospital Foundation A. de Rothschild, Imaging department, Paris, France, PARIS, France, 2Sorbonne University, Paris Brain Institute, Paris, France, Paris, France, 3Hospital Foundation Rothschild,Neurology department, Paris, France, Paris, France, 4Hospital Foundation A. de Rothschild, Pharmaceutical department, Paris, France, PARIS, France |
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Gadolinium-enhanced imaging provides valuable information in clinical practice for the diagnosis of several diseases. Conventional sequences fail to detect low concentrations of gadolinium, such as those encountered in abnormal meninges. We designed a phantom containing 16 diluted gadobutrol tubes to compare and optimize sequences, based on normalized signal and contrast-to-noise ratio, for each gadolinium concentration. We performed a preliminary study comparing T1, FLAIR and FLAIR with optimized parameters on this phantom. The optimized FLAIR sequence shows an efficient detection of low concentrations, with a higher CNR than other sequences. Preliminary in-vivo experiment shows promising results for leptomeningeal abnomalities detection. |
3359 | Commercially available astriction cotton as a anisotropic DTI phantom: Comparisons with a hand-bundled fibers and a glass capillary plate | |
Koji Sakai1, Yasuhiko Tachibana2, Toshiaki Nakagawa3, Hiroyasu Ikeno3, Takayuki Obata2, and Kei Yamada1 | ||
1Kyoto Prefectural University of Medicine, Kyoto, Japan, 2National Institute of Radiological Sciences, Chiba, Japan, 3Kyoto Prefectural University of Medicine Hospital, Kyoto, Japan |
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We compared DTI measures among three different anisotropic diffusion phantoms: a commercially available astriction cotton; a glass capillary plate; a hand-bundled polyethylene fibers. The purpose of this study was to examine whether the cotton is useful as an anisotropic diffusion phantom. Differences in ADC and FA were evaluated by comparing coefficients of variation (CVs). No significant difference was seen for the largest eigen value: 2.06 - 2.14 x 10-3 mm2/sec. Clear differences in FA were seen among the three DTI phantoms (p = 0.0079). CVs from five acquisitions for ADC and FA from every phantoms were all less than 2%. |
3360 | OpenCV based RF field mapping for MR coil assessment | |
Egor Kretov1, Zhao Kaixuan 1,2, Charles Grassin3, and Thoralf Niendorf1 | ||
1Max Delbrück Center for Molecular Medicine, Berlin, Germany, 2School of Biomedical Engineering, Southern Medical University, Guangzhou, China, 3Independent Researcher, Paris, France |
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This work presents a cost-effective near-field RF mapping approach for accurate tracking of a field probe. The method is based on the OpenCV library. It serves as a practical tool for the rapid assessment and characterization of MR coils and arrays. The only equipment required for the setup is a field probe, a regular webcam, and a paper QR code label, which renders this technique highly accessible and easy-to-use. |
3361 | A Simple Device for Real-Time Detection of Head and Body Movements in a Mock Scanner, for Screening and Training Subjects | |
Fadi Ayad1 and Amir Shmuel2 | ||
1Biomedical Engineering, McGill University, Montreal, QC, Canada, 2McConnell Brain Imaging Centre, Montreal Neurological Institute, Montreal, QC, Canada |
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Head and body movements introduce artifacts in structural, diffusion, and functional MRI. With the advent of imaging at ultra-high field, head and body movements limit our capacity to obtain high-resolution, high-quality data. We have developed a small wearable device for acquiring data on head and body movements and transmitting it wirelessly to a computer for real-time analysis while a subject is trained in a mock MRI scanner. This device works in parallel to an in-bore camera used for movement detection, to support subject screening and training to remain still in preparation for MRI. |
3362 | 3-plane Localizer-aided Background Removal in Magnetic Resonance (MR) Images Using Deep Learning | |
Apoorva Agarwal1, Megha Goel1, and Jignesh Dholakia1 | ||
1GE Healthcare, Bengaluru, India |
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This study presents a new Deep-Learning (DL) based strategy for background computation in MR images. 3-plane Localizer scans have been used for background-subtraction in all subsequent scans of same MR Examination. This is accomplished by obtaining foreground-background masks for Localizer images using U-Net model and applying Image Resampling techniques on the obtained mask to compute background for subsequent scans. Comparison with existing algorithms demonstrates that proposed method prevails in accuracy, effectiveness and provides improved visual contrast. It can also be used universally across anatomies and MR pulse-sequences as opposed to other methods requiring anatomy/sequence-specific tuning and adaptive parameter adjustments. |
3363 | Phantom Experiments for Optimal Soft Gating Parameter in Free-Breathing Hepatobiliary Phase MRI with KWIC Reconstruction | |
Tomohiro Noda1, Keitaro Sofue2, Ryuji Shimada1, Yuichiro Somiya1, Shintaro Horii1, Yoshiko Ueno2, Naoki Yoshida1, Yu Ueda3, Akiko Kusaka1, and Takamichi Murakami2 | ||
1Center of Radiology and Radiation Oncology, Kobe University Hospital, Kobe, Japan, 2Department of Radiology, Kobe University Graduate School of Medicine, Kobe, Japan, 3Philips Japan MR Clinical Science, Tokyo, Japan |
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In free-breathing radial k-space sampling with KWIC reconstruction, soft gating method can be adopted to reduce motion artifacts. We investigated optimal soft gating parameters for free-breathing hepatobiliary phase MRI. A programmable respiratory motion phantom with varying motion distance of 10, 20, 30 mm was imaged using six values of soft gating factor (SGF). Image contrast and sharpness were analyzed by calculating contrast ratio (CR) and full width at half maximum (FWHM). The CR and FWHM were not inferior compared with the reference standard images in any of the motion distances when the SGF was set at more than 1.4. |
3364 | A phantom-based method for MRI relaxation time mapping data validation and harmonization | |
Davide Cicolari1, Domenico Lizio2, Patrizia Pedrotti3, Monica Teresa Moioli2, Alessandro Lascialfari1, Manuel Mariani1, and Alberto Torresin2,4 | ||
1Department of Physics, University of Pavia, Pavia, Italy, 2Department of Medical Physics, ASST Grande Ospedale Metropolitano Niguarda, Milan, Italy, 3Department of Cardiology, ASST Grande Ospedale Metropolitano Niguarda, Milan, Italy, 4Department of Physics, University of Milan, Milan, Italy |
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A method for the MRI relaxation time measurement validation and harmonization is proposed: it relies on a phantom composed of vials filled with different concentrations of MnCl2 aqueous solutions, whose relaxation times are characterized as a function of both concentration and temperature, employing NMR techniques. The accuracy and the precision of fast mapping sequences developed for cardiac applications are better quantified through, respectively, the phantom characterization and the SD maps analysis. Scan-dependent recalibrations of the relaxation time maps can be performed relying on the ground-truth NMR values of the phantom, aiming to clinical intra- and inter-center harmonization. |
4005 | Development and Evaluation of an MR-safe Interventional Catheter with Tunable MR Visibility and Radiopacity | |
Bridget F Kilbride1, Caroline D Jordan2, Andrew Chu3, Dave Barry3, Kerstin Mueller4, Sinyeob Ahn4, Teri Moore5, Mark W Wilson5, and Steven W Hetts5 | ||
1Radiology and Biomedical Imaging, University of California San Francisco, San Francisco, CA, United States, 2Texas A&M University, Houston, TX, United States, 3Penumbra, Inc., Alameda, CA, United States, 4Siemens Medical Solutions, Malvern, PA, United States, 5University of California San Francisco, San Francisco, CA, United States |
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Interventional MRI catheter-based procedures are greatly limited by current devices and their safety profiles, and next-generation MR-safe devices are still in development. We designed and evaluated a polymeric catheter concept that is both safe and visible in MRI and X-ray environments. All imaging was done in a two-room hybrid angio-MR suite to demonstrate compatibility with next-generation image-guided procedures. In a phantom, we acquired GRE and TSE sequences at 3T and imaged on a clinical biplane angiographic system to quantitate MRI visibility and radiopacity, respectively. The catheters exhibited promising tracking characteristics under MRI and X-ray on a polymer-based catheter. |
4006 | Optimized passive marker device visibility for MRI-guided endovascular interventions at 3T: a pulsatile flow phantom study | |
Han Nijsink1, Kristian G. Overduin1, Sytse F. De Jong1, Paul J.A. Borm2, Torben Pätz3, Dennis G.H. Bosboom4, Michiel C. Warlé1, and Jurgen J. Fütterer1 | ||
1Radboudumc, Nijmegen, Netherlands, 2Nano4Imaging, Düsseldorf, Germany, 3Fraunhover MEVIS, Bremen, Germany, 4Soteria Medical B.V., Arnhem, Netherlands |
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MRI-guidance for endovascular interventions is only eligible with clearly visible endovascular devices. Hence, we quantitatively and qualitatively evaluated marker visibility and artifact size of passive marker guidewires for different MRI sequence types, MRI parameters and marker concentrations at 3T MRI using a pulsatile flow phantom. Artifact size was positively correlated with TE and marker concentration and was significantly larger for bSSFP images compared to GRE images. The GRE images outperformed the bSSFP images in the quantitative image quality assessment. In conclusion, markers were adequately visible in GRE images and artifact visibility can be optimized by adjusting TE and marker concentration. |
4007 | MRI Needle Tracking with Phase-only Cross-Correlation (POCC) in the Presence of Susceptibility Artifacts | |
Andreas Reichert1 and Michael Bock1 | ||
1Department of Radiology, Medical Physics, Medical Center – University of Freiburg, Faculty of Medicine, University of Freiburg, Freiburg, Germany |
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The phase-only cross correlation (POCC) algorithm can be used to accurately detect the orientation of a passive needle guide in needle interventions. A POCC sequence continuously visualizes the planned needle pathway during needle guide movement. The insertion of a needle into the needle guide, however, degrades the POCC detection because of susceptibility artifacts. In this work, susceptibility artifacts of a needle are measured and simulated, and a potential integration integrated into the POCC algorithm is evaluated. |
4008 | 4-DoF Needle-Guide Manipulator System for Interactive Real-Time MRI-Guided Prostate Interventions | |
Junichi Tokuda1,2, Pedro Moreira1,2, Amanda Aleong3, Franklin King1, John P Grimble4, Kemal Tuncali1,2, Ravi Seethamraju5, Gerald Moran6, Himanshu Bhat5, Nick V Iftimia4, and Jesung Park4 | ||
1Radiology, Brigham and Women's Hospital, Boston, MA, United States, 2Harvard Medical School, Boston, MA, United States, 3University of Toronto, Toronto, ON, Canada, 4Physical Science Inc., Andover, MA, United States, 5Siemens Medical Solutions USA Inc., Boston, MA, United States, 6Siemens Healthcare Ltd., Oakville, ON, Canada |
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Accurate needle placement is crucial for MRI-guided targeted prostate biopsy. However, needle placement accuracy is often affected by the deviation of the needle caused by the anatomical structures on the needle path. To avoid anatomical structures that are likely to cause significant needle deviation, we developed a 4-degree-of-freedom (DoF) needle-guide manipulator system named “Smart Template”. The Smart Template allows physicians to insert a needle accurately to the target while monitoring the needle through interactive real-time MRI. We performed a preliminary evaluation of the device to test the feasibility of needle placement using Smart Template. |
4009 | An MR-Tracked Metallic injection needle for Distancing Radiation-sources from Sensitive tissues: Construct and Initial testing in Swine | |
Ehud Jeruham Schmidt1, Marc Morcos2, Anthony Gunderman3, Junichi Tokuda4, Ravi Teja Seethamraju5, Luca Neri1, Carmen Kut2, Henry R. Halperin1, Akila Ninette Viswanathan2, and Yue Chen3 | ||
1Medicine (Cardiology), Johns Hopkins School of Medicine, Baltimore, MD, United States, 2Radiation Oncology, Johns Hopkins School of Medicine, Baltimore, MD, United States, 3Mechanical Engineering, University of Arkansas, Fayetteville, AR, United States, 4Radiology, Brigham and Women's Hospital, Boston, MA, United States, 5Siemens Medical Solutions, Boston, MA, United States |
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A metallic actively-tracked injection needle was constructed for purposes of reducing dose to normal tissues surrounding irradiated tumors in cervical cancer and prostate cancer radiation therapy. Hydrogel is injected into tissue or anatomic cavities between the tumor and normal tissues, increasing the distance from the radiation source. The needle was tested in a gynecological phantom and in swine. It provided 1.2x1.2x1.2mm3 targeting precision @16 frames-per-second navigation, supporting rapid navigation speeds currently possible only under X-ray or Ultrasound guidance. The injected topology over time was visualized during injection, allowing creation of more uniform dose-shielding regions. |
4010 | Attenuation of the dark band artifact in MR-guided focused ultrasound using an ultra-flexible high-sensitivity head coil | |
Isabelle Saniour1, Fraser Robb2, Victor Taracila2, Henning U. Voss1, Michael G. Kaplitt3, J. Levi Chazen1, and Simone Angela Winkler1 | ||
1Department of Radiology, Weill Cornell Medicine, New York, NY, United States, 2MR Engineering, GE Healthcare, Aurora, OH, United States, 3Department of Neurological Surgery, Weill Cornell Medicine, New york, NY, United States |
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Transcranial magnetic resonance guided focused ultrasound (MRgFUS) has shown dramatic success in the treatment of various neurodegenerative diseases. However, black band artifacts arise in MR images due to the high-permittivity water bath and the metallically lined helmet-shaped transducer together with the vendor-installed body coil. In this work, we present electromagnetic simulations of a very thin, flexible, and acoustic transparent head coil design (FUS-Flex). Simulations show a signal-to-noise-ratio (SNR) increase of 3.5× and 5× compared to a body coil with and without the transducer, respectively, and an attenuation of the black band artifact in the regions of interest. |
4011 | MR guided Focused Ultrasound as a Non-Invasive Surgical Treatment of Lung Cancer | |
Jaime Mata1, Lauren Powlovich2, David Moore2, and Linda Martin1 | ||
1University of Virginia, Charlottesville, VA, United States, 2Focused Ultrasound Foundation, Charlottesville, VA, United States |
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Malignant lung cancer carries a poor prognosis with a 5-year survival rate of about 18%. This new method proposes an innovative minimally invasive procedure for the transcutaneous ablation of lung tumor masses with complete removal or significant debulking of the masses. This new procedure could increase lung cancer survival rates and at the same time decrease morbidity and side effects associated with current treatment therapies. It will also provide a viable treatment for a large group of patients that cannot tolerate resection surgery, radiotherapy and chemotherapy, or who have had prior radiation and cannot have additional radiation to that region. |
4012 | Comparison of Diffusion Tractography and fMRI-based Targeting for MRgFUS Treatment of Essential Tremor | |
Kristin Quah1, Jonathan Samuel Goodman2, Gustavo Loo Kang Chau3, Kim Butts Pauly4, Pejman Ghanouni4, Gary Glover4, and Jennifer McNab4 | ||
1Electrical Engineering, Stanford University, Stanford, CA, United States, 2Biophysics, Stanford University, Stanford, CA, United States, 3Bioengineering, Stanford University, Stanford, CA, United States, 4Radiology, Stanford University, Stanford, CA, United States |
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Probabilistic diffusion tractography and fMRI are two alternative methods for targeting the ventral intermediate nucleus of the thalamus in patients with essential tremor (ET) for treatment with transcranial magnetic resonance imaging-guided focused ultrasound (tcMRgFUS). In this study, three ET subjects underwent MRgFUS thalamotomy with traditional targeting using anatomic landmarks. Tractography and fMRI targeting were compared retrospectively to determine how they relate to one another and to the targets selected by the surgeon. Two of the three subjects showed a consistent spatial relationship between fMRI, tractography and anatomical targets. |
4013 | Comparison of birdcage resonator designs for clinical MR-guided radiotherapy | |
Kilian A. Dietrich1,2, Sebastian Klüter2, Benjamin R. Knowles1, Jürgen Debus2,3, Markus E. Ladd1,3, and Tanja Platt1 | ||
1Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Radiation Oncology, University Hospital, Heidelberg, Germany, 3Faculty of Medicine, Heidelberg University, Heidelberg, Germany |
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Electromagnetic field simulations were performed at 0.345T and 1.5T to find an advantageous RF coil design for typical scanners in MR-guided therapy. Hence, different birdcage coil designs were characterized and compared with one another with respect to their corresponding transmit and receive field characteristics. |
4014 | Feasibility of free breathing real-time cine-MRI for MR-guided Cardiac Radioablation on the Unity MR-linac | |
Osman Akdag1, Stefano Mandija1, Pim Borman1, Eveline Alberts2, and Martin Fast1 | ||
1Radiotherapy, University Medical Center Utrecht, Utrecht, Netherlands, 2Philips Healthcare, Best, Netherlands |
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Stereotactic arrhythmia radioablation (STAR) is a novel non-invasive treatment technique for ventricular tachycardia patients, refractory to conventional catheter ablation. Here, we investigate the feasibility of integrating real-time, free-breathing, cardiac cine-MRI into the STAR radiotherapy workflow. As a first step towards MRI-guided STAR treatments, we test our imaging approach on a diagnostic 1.5T MRI-simulator (Philips, Ingenia), and on a 1.5T Elekta Unity MR-linac. Our results indicate the feasibility of acquiring real-time, free-breathing, cine MRI images on both systems at 14Hz, enabling real-time motion assessment and delivery adaptation without additional cardiac imaging hardware. |
4015 | Clinical evaluation of 4DMRI for lung cancer radiation treatment planning | |
Jonathan Goodwin1,2, Satomi Higuchi1, Laura O'Connor1,2, Amy Zafara1, Kate Skehan1, Terry Perkins3, Sanjiv Gupta1, Peter Greer1,2, Jane Ludbrook1,2, and John Simpson1,2 | ||
1Calvary Mater Hospital, Newcastle, Australia, 2Univeristy of Newcastle, Newcastle, Australia, 3Blacktown Cancer & Haematology Centre, Blacktown, Australia |
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4D-CT is routinely acquired for lung cancer treatment planning to visualise the extent of tumour motion, to determine the appropriate treatment target volume. However, it can be unreliable in cases of irregular breathing, is susceptible to image artefact in regions close to the diaphragm, and shows generally poor soft tissue contrast. In this study we evaluated an alternative self-navigating 4D-MRI approach in terms of motion detection accuracy, measured tumour volume, and dosimetric differences observed with respect to patients’ existing lung cancer treatment plans. |
4016 | MR SIGnature MAtching (MRSIGMA) with retrospective self-validation for real-time volumetric tumor motion imaging | |
Nathanael Kim1, Kathryn Tringale2, Christopher Crane2, Neelam Tyagi1, and Ricardo Otazo1,3 | ||
1Medical Physics, Memorial Sloan Kettering Cancer Center, New York, NY, United States, 2Radiation Oncology, Memorial Sloan Kettering Cancer Center, New York, NY, United States, 3Radiology, Memorial Sloan Kettering Cancer Center, New York, NY, United States |
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MRSIGMA is a promising real-time volumetric imaging for MRI-guided adaptive radiotherapy using a MR-Linac system. However, the lack of a real-time 3D reference image acquired with similar temporal resolution introduces significant challenges for in vivo validation. This work proposes a retrospective self-validation for MRSIGMA, where the same data used for real-time imaging are used to create a non-real-time reference. MRSIGMA with self-validation is tested in patients with liver tumors using quantitative metrics defined on the tumor and nearby organs-at-risk structures. |
4017 | Investigation of A Fast-volumetric Four-dimensional Magnetic Resonance Imaging Technique for Abdominal Radiotherapy Tumor Motion Management | |
Tian Li1, Haonan Xiao1, Ge Ren1, Weiwei Liu2, Yibao Zhang2, Hao Wu2, Weihu Wang2, and Jing Cai1 | ||
1Department of Health Technology and Informatics, The Hong Kong Polytechnic University, Hong Kong, Hong Kong, 2Key Laboratory of Carcinogenesis and Translational Research (Ministry of Education/Beijing), Department of Radiation Oncology, Beijing Cancer Hospital & Institute, Peking University Cancer Hospital & Institute, Beijing, China, Beijing, China |
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Motion management plays an important role in abdominal cancer radiotherapy. Current motion measurement method using 2D Cine MRI is inefficient. However, there is no commercial four-dimensional MRI available for motion management. In this study, we aim to investigate a fast-volumetric four-dimensional MRI technique using commercial sequence for tumor motion management in liver cancer patient. Our preliminary results shown that the commercially available TWIST-VIBE 4D-MRI sequence is capable of measuring liver tumor motion accurately with an acceptable tumor contrast. |
4018 | Subject-specific positional probability volume mapping for internal target volume determination in Radiotherapy | |
Oi Lei Wong1, Jing Yuan1, Darren MC Poon2, Yi Hang Zhou1, Siu Ki Yu1, and Kin Yin Cheung1 | ||
1Medical Physics and Research, Hong Kong Sanatorium, Hong Kong, Hong Kong, 2Comprehensive Oncology Center, Hong Kong Sanatorium, Hong Kong, Hong Kong |
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A novel ITV determination technique based on the volume of positional probability distribution (PPV) generated by volumetric 4DMRI was proposed and verified on cancer patients. For large targets, both PPV and 4D-CT generated ITV were similar with relatively large DSC. For small targets, however, relatively small DSC was observed, where poor tumor visibility in 4D-CT may be the cause. |
4019 | Promising results using synthetic CT for 2D and 3D patient positioning in head and neck radiotherapy | |
Emilia Palmér1, Fredrik Nordström1,2, Anna Karlsson1,2, Karin Petruson3, Maria Ljungberg1,2, and Maja Sohlin1,2 | ||
1Department of Radiation Physics, Institute of Clinical Sciences, Sahlgrenska Academy, University of Gothenburg, Gothenburg, Sweden, 2Department of Medical Physics and Biomedical Engineering, Sahlgrenska University Hospital, Gothenburg, Sweden, 3Department of Oncology and Radiotherapy, Institute of Clinical Sciences, Sahlgrenska Academy, University of Gothenburg, Gothenburg, Sweden |
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In an MRI-only radiotherapy workflow, in addition to enabling absorbed dose calculation the generated synthetic CT (sCT) must also be valid for patient positioning at treatment course. To evaluate MRI-only patient positioning for head and neck cancer patients, fourteen 3D cone beam CTs were retrospectively registered to CT and sCT. Further, original Digital Reconstructed radiographs originating from the CT and synthetic Digital Reconstructed radiographs originating from the sCT, were retrospectively registered to orthogonal projections. The small mean difference between the registrations showed that sCT could replace the CT for both 3D and 2D head and neck radiotherapy patient positioning. |
4020 | Damping acoustic noise for MRI in Radiotherapy Settings | |
Erik R Huijing1, Femke Wetzels1, Edwin Versteeg1, Koenraad Rhebergen1, Simon Woodings1, Dennis Klomp1, Marielle Philippens1, Nico van den Berg2, and Stefano Mandija3 | ||
1UMC Utrecht, Utrecht, Netherlands, 2Computational Imaging Group for MR Diagnostic & Therapy, UMC Utrecht, Utrecht, Netherlands, 3Computational Imaging Group for MR Diagnostic & Therapy, University Medical Center Utrecht, Utrecht, Netherlands |
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We present two hoods for acoustic noise damping for MRI in Radiotherapy. This is especially relevant for brain and head-and-neck patients who are scanned repetitively inside immobilization masks, which prevent wearing all the required earing protection devices. The hoods show good noise damping (average at least 10 dB attenuation) and minimal radiation dose attenuation (<1%), making them suitable also for MR-linac systems. Subjective results from a survey on 15 volunteers show that the hoods are well tolerated and do not increase significantly the feeling of claustrophobia. |
4021 | UTE-MRI complements CT in bone characterization for improved proton therapy dose calculation | |
Xin Miao1, Raanan Marants2, Thomas Benkert3, Evangelia Kaza2, Jeremy Bredfeldt2, and Atchar Sudhyadhom2 | ||
1Siemens Medical Solutions USA Inc., Boston, MA, United States, 2Department of Radiation Oncology, Dana-Farber/Brigham and Women's Cancer Center, Boston, MA, United States, 3Siemens Healthcare GmbH, Erlangen, Germany |
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CT-based proton therapy dose calculation suffers from significant uncertainties that critically limit clinical efficacy. Previous works demonstrated improved proton range calculation by combining quantitative MRI with CT. This study extends those works into bone, a challenging region for tissue characterization. CT and a novel UTE MRI technique were used to investigate their complimentary information for bone characterization. Both phantom and in vivo experiments showed that combining UTE-MRI and CT measurements achieved accurate classification of bone types. Understanding of bone types can have significant implications on the determination of bone tissue composition and, ultimately, accuracy of radiation delivery in proton therapy. |
4022
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Magnetic Resonance Guided Percutaneous Cryoablation of Extra-abdominal Desmoid Tumors: An Institutional Experience | |
Ali Agely1, Vipul Sheth1, Pejman Ghanouni1, and Ryan L. Brunsing1 | ||
1Radiology, Stanford University, Palo Alto, CA, United States |
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Desmoid tumors are challenging to control with chemotherapy, surgery, or radiation. This retrospective review evaluated patients with extra-abdominal desmoid tumors treated with MR-guided cryoablation at our institution over two years. The primary endpoint was tumor volume change before and 3 months after cryoablation; the secondary endpoint was the change in health status assessed at the same interval. Our study demonstrates MR-guided cryoablation results in the reduction of both tumor size and improvement in health status scores. No severe adverse events occurred. We conclude that MR-guided cryoablation is an effective and safe treatment option for desmoid tumors. |
4023 | PET/MRI Assessment of 90Yttrium Prostate Localization and Acute Response Following Intra-arterial Radioembolization in A Canine Model | |
Weiguo Li1,2, Kathleen Harris1, Amrutha Mylarapu1, Malcolm Burks1, Simone Raiter1, Vanessa Louise Gates1, Andrew Gordon1, Robert Lewandowski1, Riad Salem1, and Samdeep Mouli1 | ||
1Radiology, Northwestern University, Chicago, IL, United States, 2Bioengineering, University of Illinois at Chicago, Chicago, IL, United States |
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Local-regional therapy of prostate cancer with 90Yttrium (90Y) radioembolization is a novel radiotherapy approach that delivers high-dose radiation therapy with minimal non-target radiation. However, currently no accurate way exists to evaluate radiation effects noninvasively following embolization. In this study, we sought to apply PET/MRI to assess biodistribution of 90Y and estimate effects of treatment following 90Y prostate artery radioembolization in a dog prostate model. |
4024 | Improved therapy planning for eye tumours: a tumour geometry comparison between MRI and conventional ultrasound | |
L. Klaassen1,2, M.G. Jaarsma-Coes1,2, T.A. Ferreira2, T.H.K. Vu1, M. Marinkovic1, C.R.N. Rasch3, G.P.M. Luyten1, and J.W.M. Beenakker1,2 | ||
1Department of Ophthalmology, LUMC, Leiden, Netherlands, 2Department of Radiology, LUMC, Leiden, Netherlands, 3Department of Radiotherapy, LUMC, Leiden, Netherlands |
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Ocular magnetic resonance imaging, enabling 3D tumour imaging and providing better soft tissue contrast than conventional ultrasound, is increasingly used for uveal melanoma. The aim of this research was to determine the difference in geometrical tumour measurements between ultrasound and MRI. For this purpose, tumour prominence and largest basal diameter were calculated automatically based on MR imaging and compared to the US measurements. Differences >0.5mm were observed in 55% of prominence measurements and 80% of LBD measurements. Furthermore, automatically measuring tumour geometry based on 3D MR imaging lead to the discovery of inconsistencies in measurement definitions within and across disciplines. |
4025 | Low-Field Point-of-Care MRI: Automated Estimates of Brain Midline Shift Correlate With Clinical Outcomes in Stroke | |
Prantik Kundu1, Sadegh M. Salehi1, Bradley A. Cahn2, Mercy H. Mazurek2, Matthew M. Yuen2, Jo Schlemper1, Barbara Gordon-Kundu2, Rafael O'Halloran1, Michal Sofka1, and Kevin N. Sheth2 | ||
1Hyperfine Research Inc., Guilford, CT, United States, 2Yale University School of Medicine, New Haven, CT, United States |
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Low-field (64 mT) point-of-care (POC)-MRI was acquired at the bedside from patients with ischemic and hemorrhagic stroke in the neurointensive care unit at a major academic medical center (n=128). An AI system was trained to quantify brain midline shift (MLS), a standard neuroradiological marker of brain injury from POC-MRI, using anatomical annotations from independent neuroradiologists. A cross-validation experiment showed that AI estimates of MLS from POC-MRI were associated with stroke severity and disability at subsequent discharge. AI estimates of MLS greater than 1.5 mm were positively predictive of poor discharge outcome in the full sample and in ischemic stroke. |
4026 | Reliability of brain volumetrics in low-field portable MRI | |
Thomas Campbell Arnold1, Ramya Muthukrishnan2, Steven N Baldassano1, Samantha By3, Brian Welch3, Brian Litt1,4, and Joel M. Stein5 | ||
1Bioengineering, University of Pennsylvania, Philadelphia, PA, United States, 2Computer Science, University of Pennsylvania, Philadelphia, PA, United States, 3Hyperfine Research, Guilford, CT, United States, 4Neurology, Perelman School of Medicine, Philadelphia, PA, United States, 5Radiology, Perelman School of Medicine, Philadelphia, PA, United States |
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A growing body of literature demonstrates the value of MRI-based volumetric measures in diagnosing and treating neurodegenerative disorders. However, clinicians cannot offer biomarker screening for at-risk patients due to MRI systems’ high cost and limited access. Low-field MRI scanners offer a potential method for collecting low-cost images that could be analyzed for longitudinal biomarker changes or used in population-level studies. Here we examine the reliability of volumetric measurements made on a low-field MRI system. We compare the variability of 6 tissue volumes collected over 40 scans for 3T and 64mT systems, as well as the overlap between volume segmentations. |
4027 | Feasibility of human in vivo skeletal muscle and cardiac proton spectroscopy at 0.75T | |
Sophie M. Peereboom1, Christian Guenthner1, Mohammed M. Albannay1, and Sebastian Kozerke1 | ||
1Institute for Biomedical Engineering, University and ETH Zurich, Zurich, Switzerland |
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Proton MR spectroscopy can assess cardiac triglyceride levels. Although spectral separation and thermal polarization decrease at lower field strength, increased T2* and T2 values, decreased T1 values, decreased echo times and the possibility to decrease receiver bandwidth are clear advantages compared to higher fields. In this work the feasibility of in vivo skeletal muscle and cardiac proton spectroscopy at 0.75T is demonstrated. For this purpose, a clinical 3T Philips Achieva scanner was ramped down to a field strength of 0.75T. Results are compared to spectra acquired at 1.5T and 3T and simulations confirm experimental findings. |
4028 | Novel Technique for Assessment of Patellar Tracking During Weight-Bearing Knee Flexion Using Dynamic Upright MRI | |
Neeraj Kulkarni1, John Greenhalgh1, Robert Wolf1, David Chu1, Rachel Caffrey2, Brianna Elizabeth Damadian1, and Raymond Damadian1 | ||
1FONAR Corporation, Melville, NY, United States, 2Lehigh University, Bethlehem, PA, United States |
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Despite decades of imaging research focused on the knee, little attention has been paid to dynamic, weight-bearing knee MRI emulating the physiologic condition of the joint. Here, we utilize dynamic imaging in alternating axial and sagittal planes to capture the patellofemoral joint of one volunteer performing one cycle of knee flexion/extension. Our findings indicate that it is possible to characterize patellar tracking in both axial and sagittal planes utilizing fast imaging sequences (<2 minutes) on mid-field upright MRI. Additionally, it is possible to quantify the patellofemoral kinematics on these images using patellar flexion angle and anteroposterior patellar translation. |
4029 | A Novel Dedicated 0.35T Open Neonatal-Infant Brain MRI system | |
Mao Sheng1, ZhongChang Miao2, Jian Bao3, Renjie Zong3, SiSeung Kim3, Huiyao Zhang3, and Bing Keong Li3 | ||
1Department of Radiology, Children’s Hospital of Soochow University, Suzhou, China, 2Department of Radiology, The First People’s Hospital of Lianyungang, Jiangsu Province, China, 3Jiangsu LiCi Medical Device Co., Ltd, Lianyungang, China |
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A dedicated 0.35T Neonatal-Infant Brain MRI system is developed to investigate the effectiveness and safeness for neonatal and infant patients. 66 volunteers from 0-12 months are recruited to undergo a clinical trial and it is found that low field brain images displayed high grey-white tissue contrast, which is notably helpful for clinical diagnosis. The newly developed system also has very low acoustic noise and that most of the volunteer showed no sign of temperature raise. Low field MRI system therefore has the potential to be a effective and safer alternative MRI system for neonatal and infant patients. |
4030 | In vivo human imaging on a 47.5mT open MRI system with active Electromagnetic Interference (EMI) mitigation using an electrode | |
Sai Abitha Srinivas1,2, Stephen Cauley3,4, Jason P Stockmann3,4, Charlotte R Sappo1,2, Christopher E Vaughn1,2, Lawrence L Wald3,4,5, William A Grissom1,2,6,7, and Clarissa Zimmermann Cooley3,4 | ||
1Vanderbilt University Institute of imaging science, Nashville, TN, United States, 2Department of Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 3Harvard Medical School, Boston, MA, United States, 4Dept. of Radiology, Massachusetts General Hospital, Athinoula A Martinos Center for Biomedical Imaging, Boston, MA, United States, 5Harvard-MIT Division of Health Sciences and Technology, Cambridge, MA, United States, 6Department of Electrical Engineering, Vanderbilt University, Nashville, TN, United States, 7Department of Radiology, Vanderbilt University, Nashville, TN, United States |
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Low-field MRI scanners can operate outside MR safe rooms, but their image quality is adversely affected due to the presence of electromagnetic interference signals which can severely obscure the images. We demonstrate a generalized dynamic model that can handle time-varying external interference sources by using simultaneously acquired data from multiple EMI detectors - specifically from an electrode, traditional RF pick up coils and the primary MR coil - in-vivo, in real world EMI settings on a 47.5mT permanent magnet open MRI system. |
4031 | Design of a portable, low-field magnetic resonance sensor for clinical measurement of volemic status | |
Sydney Sherman1,2 and Michael Cima2,3 | ||
1Health Science and Technology, Massachusetts Institute of Technology, Cambridge, MA, United States, 2Koch Institute for Integrative Cancer Research, Cambridge, MA, United States, 3Massachusetts Institute of Technology, Cambridge, MA, United States |
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A low-field portable MR-based sensor was designed for the acquisition of clinical T2 relaxometry measurements in skeletal muscle. A range of low-field permanent magnet array configurations were modeled with varying sensitive region depths and homogeneous volumes; an optimization score for each design was calculated. The optimal design has a sensitive region 15-20mm from the surface of the magnet, making it capable of acquiring measurements deep into the leg such that the measurement is fully localized to skeletal muscle. The exclusion of subcutaneous fat tissue in the sensitive region will improve sensitivity to fluid shifts within the skeletal muscle. |
4032 | In vivo hypoxia monitoring using a novel single sided NMR device | |
Dion G Thomas1, Freya G Harrison2, Paul D Teal3, Petrik Galvosas1,4, Mary J Berry2,5, Sergei Obruchkov6, and Yu-Chieh Tzeng2 | ||
1School of Chemical and Physical Sciences, Victoria University of Wellington, Wellington, New Zealand, 2Centre for Translational Physiology, University of Otago, Wellington, New Zealand, 3School of Engineering and Computer Science, Victoria University of Wellington, Wellington, New Zealand, 4MacDiarmid Institute for Advanced Materials and Nanotechnology, Wellington, New Zealand, 5Department of Paediatrics and Child Health, University of Otago, Wellington, New Zealand, 6Robinson Research Institute, Victoria University of Wellington, Wellington, New Zealand |
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In this study, we investigate how a low field single-sided NMR device can be used to monitor brain tissue properties in-vivo. This device produces a B0 field with a sweet spot in the brain, which defines the region of tissue that is measured. An ovine model of brain hypoxia was developed, to allow tissue oxygenation to be controlled. We observed that the T2 decreased during hypoxia, recovering once normal oxygenation levels were re-established. These results shows that single-sided NMR devices have the potential to be used for real-time monitoring applications. |
4033 | Zero-Dead-Time Earth’s Field NMR Using Two-Photon Excitation | |
Victor Han1 and Chunlei Liu1,2 | ||
1Electrical Engineering and Computer Sciences, University of California, Berkeley, Berkeley, CA, United States, 2Helen Wills Neuroscience Institute, University of California, Berkeley, Berkeley, CA, United States |
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Two-photon excitation allows for excitation at half of the Larmor frequency. In Earth’s magnetic field, this corresponds to a Larmor frequency of about 2 kHz and an excitation frequency of about 1 kHz. By transmitting at 1 kHz and receiving at 2 kHz, we could transmit and receive at the same time by using filters to protect the receiver. While some harmonic distortion prevented us from fully separating the transmitted from the received signal during excitation, the always connected and unsaturated receive circuitry allowed us to eliminate receiver dead time, which can be quite long at low frequencies. |
4034 | An axial gradient coil with improved linearity for Halbach-based MR systems | |
Bart de Vos1, Thomas O'Reilly1, Wouter Teeuwisse1, Rob Remis2, and Andrew Webb1 | ||
1C.J. Gorter Center for High Field MRI, Leiden University Medical Center, Leiden, Netherlands, 2Circuits and Systems, Delft University of Technology, Delft, Netherlands |
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We reduced image artifacts and increased the attainable axial field-of-view by designing a highly linear x-gradient coil for Halbach array-based MR systems. A truncated sum of sinusoidal basis function is used for the current density. Higher order modes combined with specifying the target field inside a volume lead to a stable solution of the inverse source problem. The coil was installed on our 50 mT system and resulted in a 150% increase in linear DSV with respect to our previously designed gradient coil. Whole-brain three-dimensional images have been acquired using turbo spin echo sequences in less than 10 minutes. |
4035 | A Linear Gradient Solenoid for Slice-Selective Brain Imaging using B1+-Selective RF Pulses | |
Matthew Wilcox1,2, Sai Abitha Srinivas1,2, Christopher E Vaughn1,2, Charlotte R. Sappo1,2, and William A. Grissom1,2,3,4 | ||
1Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 2Institute of Imaging Science, Vanderbilt University, Nashville, TN, United States, 3Radiology, Vanderbilt University, Nashville, TN, United States, 4Electrical Engineering, Vanderbilt University, Nashville, TN, United States |
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Despite drawbacks including production of acoustic noise and peripheral nerve simulation, long switching times, bulkiness, and high costs, use of B0 gradient coils is ubiquitous in conventional MR imaging. Replacement of B0 encoding with B1+ encoding alleviates these concerns and allows the use of hardware which is lower-cost, more compact, and silent. As a first step towards realizing a full B1+ encoding coil system, this work demonstrates an RF z-gradient solenoid coil developed for brain imaging on a 47.5 mT system. The coil performance is evaluated in simulation, bench, and scanner experiments and slice-selection using B1+-selective pulses is demonstrated. |
4036 | Target-field optimized quadrature RF coils for wrist imaging on a 76 mT Halbach-based MR system | |
Bart de Vos1, Thomas O'Reilly1, Wouter Teeuwisse1, Rob Remis2, and Andrew Webb1 | ||
1C.J. Gorter Center for High Field MRI, Leiden University Medical Center, Leiden, Netherlands, 2Circuits and Systems, Delft University of Technology, Delft, Netherlands |
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We describe a design method for quadrature RF coils for Halbach based magnets using a target field approach. The resulting current densities corresponding to these coils make them inherently decoupled. We constructed a coil pair for a newly built 76 mT system and imaged the wrist of a volunteer. The images showed a 33% SNR improvement over a linear coil, in close agreement with simulations. |
4037 | Design and testing of a four-channel receive array coil on a 50 mT permanent magnet system. | |
Javad Parsa1, Thomas O'Reilly1, Bart de Vos1, and Andrew Webb1 | ||
1Leiden University Medical Center, Leiden, Netherlands |
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An integrated transmit coil and four-element receive array has been simulated, constructed, characterized and tested on a low field MRI system operating at 2.15 MHz. Using a combination of loops and butterfly coils neighbouring inter-element coupling is below -18 dB, with directly opposite coils ~-9 dB, and <-17 dB coupling for all receive coils to the transmit coil. Images of a phantom have been acquired with a simple sum-of-squares reconstruction. |
4038 | Dipole position sensors integrated in receiver array for motion detection and correction | |
Ed Boskamp1, Mike Twieg1, and Rafael O'Halloran1 | ||
1Hyperfine, Guilford, CT, United States |
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MRI is sensitive to patient motion. There are a number of pulse sequence techniques like navigators and propeller to prevent motion artifacts. We are introducing a sensitive sensor based technique to detect motion and pose without touching the patient. The sensors are a number of miniaturized dipole resonators integrated into the receiver array. Motion corrupted lines in k space are flagged and rescanned, or when motion is between a limited number of poses, the data can be binned and combined before the recon process. |
4039 | B0-shimming methodology for affordable, compact, and homogeneous low-field MR magnets | |
Konstantin Wenzel1, Hazem Alhamwey1, Tom O'Reilly2, Layla Riemann1, and Lukas Winter1 | ||
1Physikalisch-Technische Bundesanstalt (PTB), Braunschweig and Berlin, Germany, 2Leiden University Medical Center (LUMC), Leiden, Netherlands |
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In this work, B0-shimming techniques are investigated allowing the construction of simple, low-cost, and homogeneous Halbach-based low-field MR magnets. The techniques are applied to build a desktop MR magnet at B0=0.1T and can be easily scaled to magnet designs of larger diameter. The presented shimming approach improved B0 homogeneity by a factor of ~8 from 5448ppm to 682ppm in a 2D target region. All design files and code concerning this work will be made available open source on www.opensourceimaging.org. |
4040 | The Development of a Digital-twin of a Permanent-Magnet-Array (PMA)-Based Portable MRI System | |
Shao Ying Huang1, Yi-Dan Chen1, Ting-Ou Liang2, Yan Hao Koh1, and Wenwei Yu3 | ||
1Singapore University of Technology and Design, Singapore, Singapore, 2Zhejiang University, Hangzhou, China, 3Chiba University, Chiba, Japan |
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This abstract presents the development of a digital-twin of a permanent-magnet-array-based portable MRI system. It is to guide the design, optimization, hardware debug and calibration, and evaluation of such a system at both a sub-system level and a system level. Meanwhile, it facilitates the development of a sub-system without building the whole system. It consists of the simulators for magnet array, RF coil, gradient coils, pulse sequence, k-space analysis, image reconstruction, and image quality evaluation. |
4041 | The design of a low-weight homogenous Halbach helmet for imaging the adult brain. | |
Thomas O'Reilly1 and Andrew Webb1 | ||
1C.J. Gorter Center for High Field MRI, Leiden University Medical Center, Leiden, Netherlands |
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Arrays of permanent magnets have shown promise as a relatively light weight, low cost, sustainable way of generating magnetic fields suitable for MRI. In this work we show the design of a new homogenous helmet shaped, Halbach-array based magnet optimized for imaging the adult head. The magnet has a mean magnetic field strength of 59.7 mT and a homogeneity of 1313 ppm over a brain sized 25x20x15 cm3 ellipsoid. By truncating one side of the magnet the weight of the system has been reduced compared to symmetric designs while increasing the obtained field strength. |
4042 | The role of non-random magnet rotations on main field homogeneity of permanent magnet assemblies | |
Thomas O'Reilly1 and Andrew Webb1 | ||
1C.J. Gorter Center for High Field MRI, Leiden University Medical Center, Leiden, Netherlands |
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Arrays of permanent magnets are an attractive approach to designing magnets for low field MRI systems as they are affordable, easy to handle and offer great flexibility in magnet designs. However, translating designs from simulations to realised systems is challenging. The difference between the two is often attributed to imperfections in the individual magnets that make up the permanent magnet array. Here we show that non-random errors in the magnet rotations due to imperfect magnet holders can be the dominant cause of this discrepancy and if the imperfections are known they can easily be corrected for during manufacturing. |
4043 | Triple-ring permanent magnet design for ultra-low-field MRI systems | |
Yang Gao1,2, Alex T. L. Leong1,2, Yilong Liu1,2, and Ed X. Wu1,2 | ||
1Laboratory of Biomedical Imaging and Signal Processing, The University of Hong Kong, Hong Kong SAR, China, 2Department of Electrical and Electronic Engineering, The University of Hong Kong, Hong Kong SAR, China |
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MRI has impacted modern healthcare tremendously. However, MRI accessibility is low and extremely inhomogeneous globally. The recent shift in prioritizing MRI’s value has seen the emergence in developing point-of-care systems at ultra-low-field (<0.1T), particularly the use of permanent magnets for its light-weight, low power and low cost benefits. However, fundamentally, a relatively strong and uniform magnetic field is still desired for ultra-low-field MRI systems. Here, we propose a triple-ring permanent magnet design that aims to preserve and improve upon the fundamental field homogeneity requirements of MR imaging at ultra-low-field, without sacrificing the flexibility to perform both body and head imaging. |
4044 | Educational Tabletop MRI system using the Open-Source Console for Real-time Acquisition (OCRA) | |
Marcus Prier1,2, David Schote1,2, Ivan Fomin1,2, Thomas Witzel3, Georg Rose1,2, and Oliver Speck1,2 | ||
1Otto-von-Guericke University, Magdeburg, Germany, 2Research Campus STIMULATE, Magdeburg, Germany, 3Q Bio Inc, San Carlos, CA, United States |
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A Tabletop MRI system was developed that merges the Marinos Center Tabletop and OCRA projects, and is improved in many aspects compared to the original system. The proposed system includes a fully functional MRI console with a customizable GUI and microcontroller server. The hardware was extended with an optimized magnet design with passive shimming, active TR switches with reverse bias and RFPA noise blanking, and a low cost and fast response 4 channel gradient amplifier. It can be used for educational purposes and student courses in medical engineering. |
4242 | Exploration of the Surgical Placement of the Local Pituitary Coil for Microadenomas | |
Jiahao Lin1,2, Siyuan Liu2, Rock Hadley3, Marvin Bergsneider4, Giyarpuram N Prashant4, Sophie Peeters4, Robert Candler2,5, and Kyunghyun Sung1 | ||
1Department of Radiological Sciences, David Geffen School of Medicine, University of California, Los Angeles, LOS ANGELES, CA, United States, 2Department of Electrical and Computer Engineering, University of California, Los Angeles, LOS ANGELES, CA, United States, 3Department of Radiology, University of Utah, Salt Lake City, UT, United States, 4Department of Neurosurgery, University of California, Los Angeles, LOS ANGELES, CA, United States, 5California NanoSystems Institute, Los Angeles, CA, United States |
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We construct an agar phantom to examine the SNR variation as the coil plane rotates from 0° to 90°, respect to B0. Our local pituitary coil has improved SNR with a factor, ranged from 3.3 to 4.2, compared to the commercial Siemens head coil as long as the surgical positioning of the coil to be within 0° and 70° with respect to the B0 field. |
4243 | Toward automatic lesion transmurality assessment using machine learning: a proof of concept in preclinical EP studies under MRI-guidance | |
Valéry Ozenne1,2,3,4, Pierre Bour2,3,4, Marylène Delcey2,3,4, Nicolas Cedilnik5, Maxime Sermesant5, and Bruno Quesson2,3,4 | ||
1Centre de Résonance Magnétique des Systèmes Biologiques, UMR 5536, CNRS, Bordeaux, France, 2IHU Liryc, Electrophysiology and Heart Modeling Institute, Fondation Bordeaux Université, Bordeaux, France, 3Univ. Bordeaux, Centre de recherche Cardio-Thoracique de Bordeaux, U1045, Bordeaux, France, 4INSERM, Centre de recherche Cardio-Thoracique de Bordeaux, U1045, Bordeaux, France, 5Université Côte d’Azur, Inria, Epione, Sophia Antipolis, France |
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MR-guidance of electrophysiological (EP) procedures requires manual segmentation of the cardiac cavities either at the beginning of the procedure to produce the roadmap volume or after radiofrequency ablation (RFA) to assess the lesion transmurality in post ablation images. The purpose of this work is to evaluate the feasibility of automatic in-line segmentation in the context of routine preclinical EP studies. |
4244 | Towards Catheter-based Intra-Arterial Spin Labeling for Perfusion Measurements | |
Kevin Waescher1, Simon Reiss1, Ali Caglar Özen1,2, Thomas Lottner1, and Michael Bock1 | ||
1Dept. of Radiology, Medical Physics, Medical Center University of Freiburg, Faculty of Medicine, University of Freiburg, Freiburg, Germany, 2German Consortium for Translational Cancer Research Partner Site Freiburg, German Cancer Research Center (DKFZ), Heidelberg, Germany |
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MR-guided catheterization with injection of Gd-based contrast agent allows for quantitative perfusion measurement of the myocardium in coronary interventions. However, Gd is contraindicated in patients with impaired renal function, and it changes the relaxation times in the target organ after injection, so that a characterization of the target tissue becomes difficult. In this study, we provide a different solution to quantify perfusion using arterial spin labelling with a catheter based coil. The results show that ASL using a local catheter based labelling coil provides an alternative technique for perfusion measurements during cardiovascular interventions without exogenous contrast agents. |
4245 | Prototype Platform for Real-time MR-guided Brain Clot Evacuation | |
Robert Moskwa1, Azam Ahmed2, and Walter Block1 | ||
1Medical Physics, University of Wisconsin-Madison, Madison, WI, United States, 2Neurological Surgery, University of Wisconsin-Madison, Madison, WI, United States |
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The international Phase III MISTIE Trial, which used CT-image guidance to position a catheter at the site of intracerebral hemorrhage (ICH) failed to meet its clinical endpoint for all patients. The Trial concluded that improved guidance was needed to help a wider set of neurosurgeons. MR-guidance of ICH evacuation could meet these needs. We present an MR-guidance prototype to provide neurosurgeons with a real-time interface with similar viewpoints as commonly used in stereotactic operating room settings. The MR-guidance prototype shows potential to be a reliable tool to assist as monitoring and guiding tools and lysing drugs during clot-evacuation procedures. |
4246 | PETRA subtraction-based MRA to assess middle-cerebral-artery stenosis before and after treatment with angioplasty | |
Feifei Zhang1, Yuncai Ran1, Shujian Li1, Jinxia Zhu2, Xuemei Gao1, Jingliang Cheng1, and Chengcheng Zhu3 | ||
1The first Affiliated Hospital of Zhengzhou University, Zhengzhou, China, Zhengzhou, China, 2MR Collaboration, Siemens Healthcare Ltd., Beijing, China, Beijing, China, 3Department of Radiology, University of Washington, Seattle, Seattle, WA, United States |
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This study investigated the feasibility of PETRA-MRA to evaluate stent angioplasty of middle-cerebral-artery stenosis before and after treatment. PETRA-MRA was shown to significantly reduce susceptibility artifacts induced by metallic devices, decrease the phase dispersion of labeled flow, and increase the signal intensity within the stent. Compared to TOF-MRA, PETRA-MRA has better consistency with DSA in image quality and stenosis measurement, especially for follow-up assessments after stent angioplasty. |
4247 | Deep Learning-Based Needle Tracking Trained on Bloch-Simulated Data and Evaluated on Clinical Real-Time bSSFP Images | |
Ralf Vogel1,2, Dieter Ritter2, Jonathan Weine2,3, Jonas Faust2,4, Elodie Breton5, Julien Garnon5,6, Afshin Gangi5,6, Andreas Maier1, and Florian Maier2 | ||
1Pattern Recognition Lab, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany, 2Siemens Healthcare, Erlangen, Germany, 3TU Dortmund, Dortmund, Germany, 4Universität Heidelberg, Heidelberg, Germany, 5ICube UMR7357, University of Strasbourg, CNRS, FMTS, Strasbourg, France, 6Imagerie Interventionnelle, Hôpitaux Universitaires de Strasbourg, Strasbourg, France |
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Recently, Deep Learning-based methods were used to track the position and orientation of needles in MR images in real-time. Synthetic training data can be generated in large amounts, without data privacy restrictions, and without the need of animal experiments. Therefore, we have simulated the image acquisition using virtual human phantoms containing randomly placed metallic needles in a Bloch simulator. The synthetic images were used to train a U-net to predict the position and orientation of the needle within the susceptibility artifacts of clinical images in less than $$$90\,\text{ms}$$$. |
4248 | Deep Learning-based MR-only Radiation Therapy Planning for Head&Neck and Pelvis | |
Florian Wiesinger1, Sandeep Kaushik1, Mathias Engström2, Mika Vogel1, Graeme McKinnon3, Maelene Lohezic1, Vanda Czipczer4, Bernadett Kolozsvári4, Borbála Deák-Karancsi4, Renáta Czabány4, Bence Gyalai4, Dorottya Hajnal4, Zsófia Karancsi4, Steven F. Petit5, Juan A. Hernandez Tamames5, Marta E. Capala5, Gerda M. Verduijn5, Jean-Paul Kleijnen5, Hazel Mccallum6, Ross Maxwell6, Jonathan J. Wyatt6, Rachel Pearson6, Katalin Hideghéty7, Emőke Borzasi7, Zsófia Együd7, Renáta Kószó7, Viktor Paczona7, Zoltán Végváry7, Suryanarayanan Kaushik3, Xinzeng Wang3, Cristina Cozzini1, and László Ruskó4 | ||
1GE Healthcare, Munich, Germany, 2GE Healthcare, Stockholm, Sweden, 3GE Healthcare, Waukesha, WI, United States, 4GE Healthcare, Budapest, Hungary, 5Erasmus MC, Rotterdam, Netherlands, 6Newcastle University, Newcastle, United Kingdom, 7University of Szeged, Szeged, Hungary |
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MR imaging offers unique advantages for Radiation Therapy Planning (RTP) via excellent soft-tissue contrast for the delineation of the tumor target volume and surrounding organs-at-risk (OARs). Remaining challenges include absent CT information (required for accurate dose calculation) and time-consuming manual tumor and OAR contouring. Here we describe the application of Deep Learning for MR-only RTP in terms of synthetic CT conversion and automated OAR delineation. Exemplary results are illustrated from an ongoing MR-only RTP study in head&neck and pelvis. |
4249 | Neural network based denoising of high temporal resolution cine images for tumor tracking in MR-guided radiotherapy | |
Florian Friedrich1,2, Juliane Hörner-Rieber3, Peter Bachert1,2, Mark E. Ladd1,2,4, and Benjamin R. Knowles1 | ||
1Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Department of Physics and Astronomy, Heidelberg University, Heidelberg, Germany, 3Department of Radiation Oncology, University Hospital of Heidelberg, Heidelberg, Germany, 4Faculty of Medicine, Heidelberg University, Heidelberg, Germany |
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MR-linac systems allow for real-time tumor position updates. Higher temporal resolution imaging through k-space undersampling allows for an increased number of position updates, however iterative reconstructions may negate the decrease in acquisition time and undersampling artifacts may impact tracking stability. In this study a fast method to denoise and suppress image artifact using a U-net is presented. Undersampled Cartesian and radial cine images were acquired from a patient with a liver tumor on an MR-linac. Tumor tracking stability was assessed. Denoising was found to improve tracking stability and has potential in high temporal resolution cine imaging on MR-linac systems. |
4250 | Towards higher accuracy mapping of MRI to electron density using a 3D deep CNN for MRI-only radiotherapy treatment planning | |
Jessica E Scholey1, Abhejit Rajagopal2, Elena Grace Vasquez3, Atchar Sudhyadhom4, and Peder Eric Zufall Larson2 | ||
1Department of Radiation Oncology, University of California, San Francisco, San Francisco, CA, United States, 2Department of Radiology, University of California, San Francisco, San Francisco, CA, United States, 3Department of Physics, University of California, Berkeley, Berkeley, CA, United States, 4Department of Radiation Oncology, Harvard Medical School, Boston, MA, United States |
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We implemented a novel approach of using MRI to synthesize CT datasets acquired at MV photon energies for more accurate electron density mapping in radiotherapy treatment planning. We used a 3D deep convolutional neural network and demonstrated clinical proof-of-concept by evaluating the dosimetric impact of using synthetic datasets in a test radiotherapy treatment plan. The proposed method produced mean MAE of 72.8±17.3 HU and SSIM of 0.82 in the test dataset. The dose distributions computed on the test case produced 100% gamma passing rate (computed at 3%/3mm) indicating that synthetic MV images may be used for clinical treatment planning. |
4251 | Multi-Task MR Simulation for Abdominal Radiation Treatment Planning: Technical Development | |
Junzhou Chen1,2, Pei Han1,2, Fei Han3, Zhehao Hu1,2, Nan Wang1,2, Wensha Yang4, Anthony G Christodoulou1,2, Debiao Li1,2, and Zhaoyang Fan1,2,5 | ||
1Biomedical Imaging Research Institute, Cedars-Sinai Medical Center, Los Angeles, CA, United States, 2Department of Bioengineering, University of California, Los Angeles, Los Angeles, CA, United States, 3Siemens Medical Solutions USA, Inc., Los Angeles, CA, United States, 4Department of Radiation Oncology, University of Southern California, Los Angeles, CA, United States, 5Department of Radiology, University of Southern California, Los Angeles, CA, United States |
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MRI can provide superior soft tissue contrasts for radiation therapy planning. However, radiation planning in the abdomen is especially difficult because respiratory motion can cause misregistration across separate scans with different contrast weightings due to inconsistent breath holds or poor patient compliance. While some studies have produced volumetric and motion-resolved images, they are all limited to a single contrast which is suboptimal for radiation planning. To address these issues, we present a free-breathing MR imaging platform that produces multi-contrast and motion-resolved volumetric images using MR-multitasking, dedicated for radiation therapy planning, and under a 9:30 mins scan time. |
4252 | Image quality comparisons of novel and commercial coil setups in MRI for head and neck radiotherapy simulation | |
Evangelia Kaza1, Jeffrey P Guenette2, Christian V Guthier1, Steven Hatch3, Alexander Marques3, Lisa Singer1, and Jonathan D Schoenfeld1 | ||
1Radiation Oncology, Brigham and Women’s Hospital, Dana-Farber Cancer Institute, Harvard Medical School, Boston, MA, United States, 2Division of Neuroradiology, Brigham and Women’s Hospital, Dana-Farber Cancer Institute, Harvard Medical School, Boston, MA, United States, 3Radiation Oncology, Brigham and Women’s Hospital, Dana-Farber Cancer Institute, Boston, MA, United States |
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Quality characteristics of healthy volunteer head images (SNR, CNR, artifact size) were compared between two flexible coil arrangements encompassing radiotherapy immobilization masks relative to a gold standard diagnostic Head/Neck20 coil that cannot accommodate the masks. The novel arrangement of two UltraFlexLarge18 coils provided higher SNR ratios and was more spacious than the commercially recommended arrangement of two FlexLarge4 coils. Artifact size and CNR ratios were similar for the two coil setups. Clinical application of the UltraFlexLarge18 coil arrangement would be advantageous for head and neck radiotherapy MRI simulations due to higher SNR and increased patient comfort. |
4253 | Real-Time B0 Correction in a MRI Guided Radiotherapy System | |
Austen Curcuru1, Deshan Yang1,2, and Michael Gach1,2,3 | ||
1Biomedical Engineering, Washinton University in Saint Louis, Saint Louis, MO, United States, 2Radiation Oncology, Washinton University in Saint Louis, Saint Louis, MO, United States, 3Radiology, Washinton University in Saint Louis, Saint Louis, MO, United States |
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MRI linear accelerator hybrid systems use balanced steady state free precession sequences (bSSFP) during radiotherapy due to the sequence’s high signal to noise ratio and rapid acquisition times. However, bSSFP sequences are highly sensitive to off-resonance effects.1 As a result, the position and velocity of the radiotherapy gantry can cause imaging artifacts that can impact tumor tracking and cause fluctuations in the main magnetic field that can result in radiotherapy/MRI isocenter misalignments. Sequence parameters were adjusted during the sequence run time to reduce these issues by integrating a navigator into the bSSFP sequence and measuring B0 variations in real-time. |
4254 | Respiratory Motion Detection and Reconstruction Using CAPTURE and Deep Learning for a 0.35T MRI-LINAC System: An Initial Study | |
Sihao Chen1, Cihat Eldeniz1, Weijie Gan1, Ulugbek Kamilov1, Deshan Yang1, Michael Gach1, and Hongyu An1 | ||
1Washington University in St. Louis, Saint Louis, MO, United States |
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Magnetic Resonance Imaging Guided Linear Accelerator (MRI-LINAC) combines an MRI system with a linear accelerator radiotherapy system to treat patients. The MRI-LINAC uses MR to track organ or lesion motion and gates the radiation beam accordingly. In this study, we demonstrate the combination of a T1-weighted self-navigated respiratory motion detection method (CAPTURE) with a deep learning 4D reconstruction (Phase2Phase, P2P) method to derive the 3D deformable respiratory motion field from data acquired on a 0.35 T ViewRay MRI-LINAC system. This initial study demonstrated promising results despite the low SNR at this field strength. |
4255 | Joint Radial Trajectory Correction for Fast T2* Mapping on an MR-Linac | |
Wajiha Bano1,2, Will Holmes1,2, Mohammad Golbabaee3, Alison Tree1,2, Uwe Oelfke1,2, and Andreas Wetscherek1,2 | ||
1Joint Department of Physics, The Institute of Cancer Research, London, United Kingdom, 2The Royal Marsden NHS Foundation Trust, London, United Kingdom, 3Computer Science Department, The University of Bath, Bath, United Kingdom |
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Measuring T2* relaxation during the course of MR-guided radiotherapy can characterize tumour hypoxia, which is associated with treatment resistance. T2* mapping with radial trajectories allows for efficient coverage of k-space but is susceptible to errors arising from gradient delays. We propose a method that jointly estimates gradient delays and T2* using model-based reconstruction. Using the numerical phantom and the in-vivo prostate data we demonstrated that the proposed approach performs better for different noise levels for both fully sampled and undersampled datasets. This will allow better integration of T2* mapping for hypoxia imaging into an MR-linac treatment work flow. |
4256 | Diffusion changes in prostate cancer patients undergoing radiation treatment on an MR-Linac system: Preliminary findings | |
Colleen Bailey1,2, Rachel W Chan1, Jay Detsky3,4, Danny Vesprini3,4, and Angus Z Lau1,2 | ||
1Odette Cancer Centre, Sunnybrook Research Institute, Toronto, ON, Canada, 2Medical Biophysics, University of Toronto, Toronto, ON, Canada, 3Department of Radiation Oncology, Sunnybrook Health Sciences Centre, Toronto, ON, Canada, 4Department of Radiation Oncology, University of Toronto, Toronto, ON, Canada |
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Eight prostate cancer patients undergoing radiation treatment were scanned on an MR-Linac with conventional ADC and high-b diffusion protocols at each of five treatment fractions. With the system’s weaker gradients and longer echo times, 6/8 patients had visible lesions at the maximum b-value of 2000 s/mm2. Fits to the VERDICT model demonstrated higher intracellular fraction in the lesion, inversely correlated with ADC. In three patients, ADC increased starting at the third treatment time point; a fourth patient exhibited a transient ADC increase. Future work will correlate these changes with biochemical recurrence to test their relevance as a biomarker. |
4257 | MRI-based tumor localisation after tantalum clip placement for proton beam therapy planning of uveal melanoma | |
Myriam Jaarsma-Coes1,2, Teresa Ferreira1, Marina Marinkovic2, Khanh Vu2, Gre Luyten2, Coen Rasch3, Berit Verbist1, and Jan-Willem Beenakker1,2 | ||
1Radiology, Leiden University Medical Center, Leiden, Netherlands, 2Ophthalmology, Leiden University Medical Center, Leiden, Netherlands, 3Radiotherapy, Leiden University Medical Center, Leiden, Netherlands |
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For proton beam therapy (PBRT) of Uveal Melanoma, tantalum clips are surgically sutured on the outside of the eye to mark the tumour edge. To aid in the 3D clip localisation and modelling of the tumor, a dedicated MRI protocol was developed and evaluated. In 51% of the clips, the MRI and per-operative measurements differed less than 1.0mm. In 28% of the clips the discrepancy between the MRI and peroperative measurement was attributed to the complex tumor geometry or anterior tumor localisation. For the majority of the patients MRI added valuable information to the peroperative measurements, improving PBRT planning. |
4258 | Deep learning based synthetic CT skull for transcranial MRgFUS interventions using 3D V-net–Transfer learning implications | |
Pan Su1,2, Sijia Guo2,3, Steven Roys2,3, Florian Maier4, Thomas Benkert4, Himanshu Bhat1, Elias R. Melhem2, Dheeraj Gandhi2, Rao P. Gullapalli2,3, and Jiachen Zhuo2,3 | ||
1Siemens Medical Solutions USA, Inc., Malvern, PA, United States, 2Department of Diagnostic Radiology and Nuclear Medicine, University of Maryland, School of Medicine, Baltimore, MD, United States, 3Center for Metabolic Imaging and Therapeutics (CMIT), University of Maryland Medical Center, Baltimore, MD, United States, 4Siemens Healthcare GmbH, Erlangen, Germany |
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Transcranial MRI-guided focused ultrasound (tcMRgFUS) is a promising technique for treating multiple diseases. It is desirable to simplify the clinical workflow of tcMRgFUS treatment planning. Previously, feasibility of leveraging deep learning to generate synthetic CT skull from ultra-short echo time (UTE) MRI has been demonstrated for tcMRgFUS planning. In this study, 3D V-Net was used for skull estimation, by taking advantage of 3D volumetric images. Furthermore, feasibility of applying pre-trained model in new dataset was studied, demonstrating the possibility of generalization across various sequences/protocols and scanners. |
4259 | FMRI of Post High-Frequency Focused Ultrasound Ablation of ViM Shows Reduced Ipsilateral Thalamic and Cortical Motor Activation | |
Anna Crawford1, Mark Lowe1, Sean Nagel2, Daniel Lockwood1, Emmanuel Obusez1, Andre Machado2, and Stephen Jones1 | ||
1Imaging Institute, Cleveland Clinic Foundation, Cleveland, OH, United States, 2Neurological Institute, Cleveland Clinic Foundation, Cleveland, OH, United States |
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High Intensity Focused Ultrasound (HIFU) in now entering clinical practice, for example to treat essential tremor (ET) by creating small lesions in the thalamus. Due to small size of treatment lesions, treatment success depends critically on targeting, which is classically done using measurements and landmarks. We explore an alternative method using functional imaging to guide targeting and assess efficacy, specifically using 7T task-related fMRI. We present preliminary data of the patterns of BOLD activation in a set of patients before and after HIFU. |
4260 | Comparison of Automated Thalamic Segmentation Techniques: Applications in MRgFUS Planning | |
Kain Kyle1, Jerome Maller2, Yael Barnett3, Stephen Tisch3, Benjamin Jonker3, Michael Barnett1, Arkiev D'Souza1, and Chenyu Wang1 | ||
1University of Sydney, Sydney, Australia, 2GE Healthcare, Sydney, Australia, 3St Vincent's Hospital Sydney, Sydney, Australia |
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Investigation of thalamic segmentation tools FreeSurfer and THOMAS for use in MRgFUS planning. |
4261 | Reduced-FOV 3D MR-ARFI with a joint reconstruction for localizing the focused ultrasound beam in neuromodulation | |
Huiwen Luo1,2, Michelle K. Sigona1,2, Li Min Chen2,3, Charles F. Caskey2,3, and William A. Grissom1,2,3 | ||
1Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 2Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 3Radiology and Radiological Sciences, Vanderbilt University Medical Center, Nashville, TN, United States |
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Magnetic resonance acoustic radiation force imaging (MR-ARFI) can be used to localize the focal spot in MR-guided focused ultrasound (FUS) by encoding the ultrasound-induced displacements into the phase of an MR image. A two-minute reduced-FOV 3D MR-ARFI scan with a joint image reconstruction method at 3 Tesla is proposed to image and localize the entire focus in FUS neuromodulation with a low FUS duty-cycle of 0.85%. In this work the reduced FOV MR-ARFI pulse sequence is demonstrated and the proposed k-space undersampling with joint sparse difference image reconstruction to achieve a two-minute scan time is validated. |
4262 | A compact and clonable ultrasound-based sensor system to monitor physiological motion | |
Bruno Madore1, Cheng-Chieh Cheng2, and Frank Preiswerk3 | ||
1Radiology, Brigham and Women's Hospital, Harvard Medical School, Boston, MA, United States, 2Computer Science and Engineering, National Sun Yat-sen University, Kaohsiung, Taiwan, 3Amazon Robotics, Westborough, MA, United States |
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Physiological motion continues to be a problem in MRI and PET, as it can cause blurring and other types of artifacts. We developed a compact, clonable ultrasound-based sensor system that monitors internal motion directly. Alternative means of motion monitoring often involve hardware (including the scanner itself) that is attached to floors, walls and/or ceilings and thus cannot follow the patient from one room to another, from one procedure to the next. The present sensors attach to the skin, they can follow the patient, and as such they may help link different procedures in ways that take internal motion into account. |
4263 | Acoustically transparent and low-profile head coil for high precision magnetic resonance guided focused ultrasound at 3 T | |
Isabelle Saniour1, Fraser Robb2, Victor Taracila2, Jana Vincent2, Henning U. Voss1, Michael G. Kaplitt3, J. Levi Chazen1, and Simone Angela Winkler1 | ||
1Weill Cornell Medicine, New York, NY, United States, 2MR Engineering, GE Healthcare, Aurora, OH, United States, 3Department of Neurological Surgery, Weill Cornell Medicine, New York, NY, United States |
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Magnetic resonance guided focused ultrasound (MRgFUS) is a non-invasive therapeutic modality for neurodegenerative diseases that allows real-time imaging of the targeted regions. However, MR image quality is poor and severely limits the technology due to the use of the body coil for focal targeting. Acoustic simulations demonstrated an acoustic transparency (signal loss <1%) of the coil when used for thalamic sonication. In vivo results showed increase of the SNR over the body coil by a factor of 7.3 and 7.6 in a brain image with and without the presence of the transducer, respectively. |
4264 | A dedicated 3-ch breast coil for Microwave Tomography at 3T | |
Xiaoyu Yang1, Thomas Eastlake1, Tsinghua Zheng1, Shireen Geimer2, Timothy Raynolds2, Paul Meaney2, and Keith Paulsen2 | ||
1Innovation, Quality Electrodynamics, LLC, Mayfield Village, OH, United States, 2Thayer School of Engineering, Dartmouth College, Hanover, NH, United States |
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MR breast imaging has high sensitivity but not high specificity. Microwave Tomography (MT) provides complimentary permittivity information that may improve specificity. MT has poor spatial resolution. Combining MR and MT may address both spatial and specificity issues. Previous MT and MR work demonstrated the MT-MR combination potential. However, there is no dedicated MR coil available for MT-MR combination. The only available coils are the whole-body coil or a single-loop coil that have poor MR image quality. A dedicated 3-ch MRI coil is proposed here for superior MRI imaging quality which enables the next step MT-MR volunteer evaluation. |
4265 | A Dedicated Multichannel Head Coil Array for PET Insert on 3 T MRI | |
Jo Lee1,2, Ziru Sang1,2, Yongfeng Yang1,2, Xiaoliang Zhang3, and Ye Li1,2 | ||
1Paul C. Lauterbur Research Center for Biomedical Imaging, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, 2Shenzhen Key Laboratory for MRI, Shenzhen, China, 3Department of Biomedical Engineering, State University of New York, Buffalo, NY, United States |
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Simultaneous positron emission tomography/ magnetic resonance imaging(PET/MR) provides advantages in clinical and research applications of human’s brain. The two systems, MRI and PET, can work complementary to provide more information for medical diagnosis. As most research and clinical institutes already have MRI systems, an insert PET and matched MRI coil would be a more economical choice than a PET/MR system. In this study, we designed and built a dedicated quadrature birdcage/47Rx head coil array for PET insert on human’s brain study. The flip-angle maps and SNR performances were measured through a dedicated phantom. Anatomical images were scanned on a volunteer. |
4266 | Vector Modulator Based Automated Active Compensation of Direct Feedthrough in Magnetic Particle Imaging | |
Bilal Tasdelen1,2, Mustafa Utkur1,2, Ergin Atalar1,2, and Emine Ulku Saritas1,2 | ||
1Department of Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey, 2National Magnetic Resonance Research Center (UMRAM), Ankara, Turkey |
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In magnetic particle imaging (MPI), simultaneous excitation and signal acquisition leads to direct feedthrough interference. While this interference can be mitigated up to some extent with passive compensation, its time-varying nature necessitates active compensation methods to achieve the sensitivity levels needed for applications such as stem cell tracking. We have recently proposed an active compensation technique for MRI, which uses a vector modulator and a lookup-table-based algorithm for reducing the direct feedthrough in the analog domain. Here, we adapt this technique to MPI, demonstrating a successful recovery of the fundamental frequency and a significant increase in detection sensitivity. |
4267 | Interventional Magnetic Particle Imaging Open-bore Scanner Design | |
Michael Seeg1, Martin Rueckert1, Stefan Herz2, Thomas Kampf1,3, Thorsten Bley2, Volker Behr1, and Patrick Vogel1 | ||
1Experimental Physics V, Julius-Maximilians-University, Wuerzburg, Germany, 2Department of Diagnostic and Interventional Radiology, University Hospital, Wuerzburg, Germany, 3Department of Diagnostic and Interventional Neuroradiology, University Hospital, Wuerzburg, Germany |
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X-ray-guided endovascular interventions are important treatment approaches for many cardiovascular diseases such as myocardial infarction, stroke or occlusive peripheral arterial disease. However, they pose the risk of radiation exposure to patients and staff. Magnetic particle imaging may provide a radiation-free alternative for diagnostic and image guided treatment. A new open bore scanner concept, based on a traveling field free line and super paramagnetic iron oxide tracers is developed especially for interventional treatments. Due to the open design the scanner provides good accessibility to the patient. |
4268 | MR safe electromagnetic direct current motor | |
Lorne W Hofstetter1, J Rock Hadley1, Robb Merrill1, and Dennis L Parker1 | ||
1Department of Radiology and Imaging Sciences, University of Utah, Salt Lake City, UT, United States |
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Combining the unparalleled soft-tissue imaging capabilities of MR imaging with the precision of robotic-assisted surgeries has the potential to revolutionize image-guided surgical interventions. However, strong magnetic fields generated by the MR system prevent the use of conventional robotic servo motor technologies. Here we present a direct current electromagnetic motor design that uses the electromagnetic interaction between the MR B0 field and currents in the rotor windings to generate rotational mechanical actuation. The motor stall torque and interactions caused by simultaneous motor operation and MR imaging are characterized. This new motor may be useful for robotic assisted interventions performed under MR-guidance. |
4269 | Real-time electric field estimation in transcranial magnetic stimulation using deep learning and magnetic resonance imaging | |
Guoping Xu1,2, Yogesh Rathi2,3, Joan A Camprodon3,4, and Lipeng Ning2,3 | ||
1Wuhan Institute of Technology, Wuhan, China, 2Brigham and Women's Hospital, Boston, MA, United States, 3Harvard Medical School, Boston, MA, United States, 4Massachusetts General Hospital, Boston, MA, United States |
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Transcranial magnetic stimulation (TMS) is an effective treatment approach for mental disorders. Accurate and rapid prediction of TMS-evoked electric field (E-field) in brain tissue is important for accurate targeting and to understand the mechanism of treatment response. The standard method for E-field prediction is based on physical modeling which usually takes long computational time. In this work, we introduce a method based on deep neural networks (DNNs) for real-time E-field prediction. We show that the trained DNN can predict high-precision whole-brain E-field in 0.24 seconds. Moreover, diffusion-MRI based tissue conductivity tensor can improve the prediction accuracy of E-field. |
4270 | A wearable “RF-EEG Cap” for full head coverage concurrent TMS/EEG/fMRI experiments at 3T: a feasibility study | |
Lucia Navarro de Lara1,2, Padmavathi Sundaram 1,2, Lena Nohava3, Elmar Laistler3, Mohammad Daneshzand1,2, Lawrence Wald1,2, Jason Stockmann1,2, and Aapo Nummenmaa1,2 | ||
1Martinos Center - MGH, Charlestown, MA, United States, 2Harvard Medical School, Boston, MA, United States, 3High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria |
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To enable concurrent non-invasive stimulation (TMS) and whole-head multimodal imaging (EEG-fMRI), we propose to apply flexible RF coil technology to build a first-of-its-kind TMS compatible integrated multimodal imaging array, the “RF-EEG cap”. The proposed system allows unrestricted positioning of the TMS coil across the entire scalp. We built a 2-channel prototype and conducted a feasibility study analyzing the effects of a TMS coil and EEG-electrodes on the imaging quality (SNR/B0 maps), the in-bore EEG data quality and EPI timeseries stability. Our results indicate that the flexible coaxial RF technology is a feasible choice to build the proposed “RF-EEG Cap”. |
4271 | Quantification of HD-EEG net attenuation on 18F-FDG static PET: a phantom and human brain study | |
Erica Silvestri1,2,3, Marco Castellaro1,4, Alessandra Zorz5, Andrea Bettinelli 1,5, Cristina Campi6, Marta Paiusco5, Diego Cecchin2,7, and Alessandra Bertoldo1,2 | ||
1Department of Information Engineering, University of Padova, Padova, Italy, 2Padova Neuroscience Center, University of Padova, Padova, Italy, 3Department of Neuroscience, University of Padova, Padova, Italy, 4Department of Neurosciences, Biomedicine and Movement Sciences, University of Verona, Verona, Italy, 5Department of Medical Physics, Veneto Institute of Oncology IOV - IRCCS, Padova, Italy, 6Department of Math, University of Padova, Padova, Italy, 7Department of Medicine, Unit of Nuclear Medicine, University of Padova, Padova, Italy |
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Simultaneous trimodal EEG-PET-MR imaging can be a tool to delve deeper in the healthy human brain functioning. One of the aspects scarcely investigated is the interplay between HD-EEG net and PET signal detection and reconstruction. In this work, we assess the impact of HD-EEG on both attenuation corrected (AC) and non-attenuation corrected (NAC) PET images. We found that HD-EEG net attenuates PET signal in NAC images in both phantom and human brain, respectively of 3.01%(±3.69%) and of 0.53%(±5.89%). AC images show an opposite behaviour: attenuation correction factor tends to be overestimated in CT- and UTE-derived UMAP obtained with HD-EEG net. |
4272 | Triggering pulse generation by non-contact monitoring of heart rate using an antenna with 600 MHz resonance | |
Kazuya Okamoto1, Takafumi Ohishi2, Sojuro Kato1, Ryuichi Nanaumi3, Kenji Oyama3, and Kazuhiko Fukutani3 | ||
1Advanced MRI Development PJ Team, Canon Medical Systems Corp., Kawasaki, Japan, 2Advanced Technology Research Department, Research and Development Center, Canon Medical Systems Corp., Kawasaki, Japan, 3Medical Products Technology Development Center, R&D Headquarters, Canon Inc., Tokyo, Japan |
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New non-contact cardiac and respiratory gating method have been developed, which includes an antenna monitoring heart and respiration movement, and independent triggering pulse generation unit with signal processing software. The resonance frequency of the dipole antenna was tuned to around 550MHz on the chest. The triggering pulse generation unit detected and digitized the S11 signals from the antenna. IIR filter removed the low frequency component and a template matching technique was used to seek the triggering points at the inflection point of filtered waveform. As a result, the prospective gating cardiac imaging was successfully performed for volunteers. |
4273 | MRI data transmission via fifth-generation (5G) cellular networks | |
Nicolai Spicher1, Ramon Barakat1, and Thomas Martin Deserno1 | ||
1Peter L. Reichertz Institute for Medical Informatics, TU Braunschweig and Hannover Medical School, Braunschweig, Germany |
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In the last years, research in MRI has expanded towards portable technology, e.g., trailer units carrying conventional scanners or bedside scanners with low-field strengh. The increased portability and shift away from the centralized hospital environment requires wireless data transmission with appropriate data rates to unfold its full potential. In this work, we made use of current fifth-generation (5G) cellular networks for transmitting DICOM data. We demonstrate the potential of reaching more than 50 Mbit/s upload speed using consumer-grade hard- and software. This holds great potential for cellular transmission of data from portable scanners, allowing to increase access to MRI technology. |
4274 | Test Bed for High Speed Serial Wireless MRI Data Studies | |
Audrey Chan1, Fraser Robb2, John Pauly3, Shreyas Vasanawala4, and Greig Cameron Scott5 | ||
1Victoria University of Wellington, Wellington, New Zealand, 2GE Healthcare, Aurora, OH, United States, 3Stanford University, Stanford, CA, United States, 4Radiology, Stanford University, Stanford, CA, United States, 5Electrical Engineering, Stanford University, Stanford, CA, United States |
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We developed a test system to perform pseudo-random binary sequence (PRBS) generation and clock/data recovery to assess high speed serial link performance of wireless and optical signal integrity for MRI data interfacing. We demonstrate applications using up to 1Gbps signal rates and show impairments for wireless amplitude shift keyed data transmission, as well as plastic fiber optical interfacing. |
4275 | Wireless Powered Frequency Encoding of Locally Detected MR Images for Remote Signal Transmission | |
Wei Qian1 and Chunqi Qian1 | ||
1Michigan State University, East Lansing, MI, United States |
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With a compact and batteryless design, the wireless powered parametric oscillator can simultaneously down-convert and frequency encode locally detected MR signals, and wirelessly transmit them to remotely coupled external receivers, thus maintaining superior sensitivity of localized detectors over larger distance separations. |
4276 | Single board computer as a satellite-linked, deep learning capable pocket MR workstation: a feasibility study | |
Keerthi Sravan Ravi1,2, John Thomas Vaughan Jr.2, and Sairam Geethanath2 | ||
1Biomedical Engineering, Columbia University, New York, NY, United States, 2Columbia Magnetic Resonance Research Center, New York, NY, United States |
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This work shows the feasibility of employing a Raspberry Pi (RPi) single-board computer as a deep learning capable MR workstation. RPi’s ability to run a Tensorflow-Lite optimized brain tumour segmentation model is demonstrated. A comparison of data upload across fixed broadband, cellular broadband (LTE, 3G) and satellite terminal methods of internet access is presented. Finally, the setup described in this work is compared with a conventional fixed MRI workstation and a portable MRI workstation. |
4277 | STAR MRI With Non-Magnetic, Integrated Circulator based on Switched Transmission Lines | |
Aravind Nagulu1, Ahmed Kord1, Gehua Tong1, Michael Garwood2, Lance DelaBarre2, Djaudat Idiyatullin2, SungMin Sohn3, J. Thomas Vaughan1, and Harish Krishnaswamy1 | ||
1Columbia University, New York, NY, United States, 2University of Minnesota, Minneapolis, MN, United States, 3Arizona State Univeristy, Tempe, AZ, United States |
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Traditional MRI employs time division duplexing between the receiver (RX) and transmitter (TX) to avoid RX saturation from TX self-interference. Large switching time between the TX and RX modes demands large TX power and constricts the imaging to tissues with large relaxation times. In this work, we propose a magnetic-free, switch-transmission line circulator which is fully compatible with MRI systems and achieve simultaneous transmit and receive (STAR) MRI. |
4278 | A 5.7mW 1.5T Silicon Germanium Pre-Amp, and its Effects on Image Distortion | |
Christopher Vassos1, Fraser Robb2, Shreyas Vasanawala3, John Pauly1, and Greig Scott1 | ||
1Electrical Engineering, Stanford University, Stanford, CA, United States, 2GE Healthcare, Aurora, OH, United States, 3Radiology, Stanford University, Stanford, CA, United States |
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A 5.7mW Silicon Germanium Pre-Amplifier was constructed, characterized, and its potential impact on image quality demonstrated. The amplifier demonstrates significant power savings relative to current implementations at the cost of increased device non-linearity and decreased input impedance. A benchtop measurement setup was constructed to simulate coils signals in conjunction with a physical receive chain. Measured image distortion began at peak input powers of -25dBm. This corresponds to high bandwidth, high dynamic range imaging sequences. For small coil sizes this distortion may not play a role, reducing the power barrier to wireless receive arrays. |
4279 | Hybrid Pair Ratio Adjustable Power Splitter using off-shelf components and easy-to-replace microstrip phase shifter | |
Yue Zhu1,2, William A Grissom1,2,3,4, John C Gore1,2,3,4, and Xinqiang Yan1,2 | ||
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University, Nashville, TN, United States, 3Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 4Electrical and Computer Engineering, Vanderbilt University, Nashville, TN, United States |
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A low loss ratio adjustable power splitter (RAPS) was designed with a Wilkinson Splitter, a pair of transmission lines, and a hybrid coupler. There are some potential issues with the previous RAPS: 1. Build a high-performance RAPS circuit with lumped elements is challenging and laborious at 298 MHz. 2. The 100-Ohm RF decoupling resistor poses a safety hazard to the patient. In this abstract, the Wilkinson splitter was replaced with a hybrid coupler, and the adjustable transmission lines are replaced with printed microstrip lines to mitigate the problems mentioned above. |
4280 | High Speed Serial ASK Signal Integrity for Wireless MRI | |
Greig Cameron Scott1, Audrey Chan2, Wonje Lee3, Fraser Robb4, John Pauly5, and Shreyas Vasanawala6 | ||
1Electrical Engineering, Stanford University, Stanford, CA, United States, 2Victoria University of Wellington, Wellington, New Zealand, 3Pediatric Radiology, Stanford University, Stanford, CA, United States, 4GE Healthcare, Aurora, OH, United States, 5Stanford University, Stanford, CA, United States, 6Radiology, Stanford University, Stanford, CA, United States |
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A major challenge of wireless MRI is how to implement the data link. Here, progress is made using amplitude shift keyed diode ring modulators, serializer/deserializer components and clock/data recovery to demonstrate bit rate transmissions up to 600 Mbps. High gain biquad reflector antennas and UWB antennas are compared for carriers between 3 and 5 GHz. These prototypes also demonstrate bandwidth limitations and electrodynamic interactions in a birdcage test bore on wireless signal integrity. Even if dedicated wireless ICs are not possible, we believe components exist to make an easily integrated modulator for MRI wireless data transmission. |
4281 | A Sip in the Bore: How to Make Coffee with an MRI System | |
Michael Bock1, Thomas Lottner1, and Ali Caglar Özen1,2 | ||
1Radiology - Medical Physics, University Medical Center, Medical Faculty, University Freiburg, Freiburg, Germany, 2German Consortium for Translational Cancer Research (DKTK), Freiburg, Germany |
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Energy harvesting of the RF fields has been proposed to power small milliwatt RF amplifiers. In this work we demonstrate that the time-varying gradient fields can deliver much higher power levels up to a kW which we used to energize a conventional drip coffee machine. A large pick-up coil was designed in which voltages of 100-200V were induced by rapidly oscillating gradients. The coil was connected to a commercial coffee machine in the magnet, and coffee was prepared in and with the MRI in just 5min. |