Publications by authors named "Fraser J L Robb"

The concept of a 2D cylindrical High Pass Ladder (2D c-HPL) is used in the development of this ultra high radio frequency (UHRF) volumetric head coil for 7T tuned at the Larmor frequency of 298 MHz. The architecture of the 2D c-HPL helps to overcome the challenges associated with non-uniform magnetic field distribution. The prototype consists of an individual resonating array of inductance-capacitance (LC) elements and each component is tuned to the precise frequency.

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Lack of a body-sized, bore-mounted, radiofrequency (RF) body coil for ultrahigh field (UHF) magnetic resonance imaging (MRI) is one of the major drawbacks of UHF, hampering the clinical potential of the technology. Transmit field (B ) nonuniformity and low specific absorption rate (SAR) efficiencies in UHF MRI are two challenges to be overcome. To address these problems, and ultimately provide a pathway for the full clinical potential of the modality, we have designed and simulated two-dimensional cylindrical high-pass ladder (2D c-HPL) architectures for clinical bore-size dimensions, and demonstrated a simplified proof of concept with a head-sized prototype at 7 T.

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  • Magnetic resonance guided focused ultrasound (MRgFUS) is a non-invasive treatment method for neurodegenerative diseases that combines MRI imaging and ultrasound technology to target specific brain regions effectively.
  • The development of a new 8-channel, flexible head coil called FUS-Flex enhances MRI signal quality by significantly increasing the signal-to-noise ratio (SNR) compared to standard body coils.
  • Initial tests show that the FUS-Flex coil not only improves MRI image quality but also allows for more precise targeting and better monitoring of temperatures during MRgFUS procedures, potentially improving patient outcomes.
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  • HP C-MRI is a new imaging technique that helps differentiate aggressive prostate cancer from less serious types by analyzing lactate production after injecting hyperpolarised [1-C]pyruvate.
  • The study found that HP C-MRI primarily measures metabolic activity in the cancer's epithelial cells rather than the surrounding stroma, correlating MRI results with the expression of key metabolic enzymes and transporters.
  • This method was also validated through comparisons with existing data on tumours, showing consistent metabolic patterns that can help in identifying clinically significant disease based on cellular differences.
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The purpose of this study is to investigate feasibility of estimating the specific absorption rate (SAR) in MRI in real time. To this goal, SAR maps are predicted from 3T- and 7T-simulated magnetic resonance (MR) images in 10 realistic human body models via a convolutional neural network. Two-dimensional (2-D) U-Net architectures with varying contraction layers and different convolutional filters were designed to estimate the SAR distribution in realistic body models.

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Magnetic resonance imaging systems rely on signal detection via radiofrequency coil arrays which, ideally, need to provide both bendability and form-fitting stretchability to conform to the imaging volume. However, most commercial coils are rigid and of fixed size with a substantial mean offset distance of the coil from the anatomy, which compromises the spatial resolution and diagnostic image quality as well as patient comfort. Here, we propose a soft and stretchable receive coil concept based on liquid metal and ultra-stretchable polymer that conforms closely to a desired anatomy.

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Purpose: To deploy clinically, a combined parallel imaging compressed sensing method with coil compression that achieves a rapid image reconstruction, and assess its clinical performance in contrast-enhanced abdominal pediatric MRI.

Materials And Methods: With Institutional Review Board approval and informed patient consent/assent, 29 consecutive pediatric patients were recruited. Dynamic contrast-enhanced MRI was acquired on a 3 Tesla scanner using a dedicated 32-channel pediatric coil and a three-dimensional SPGR sequence, with pseudo-random undersampling at a high acceleration (R = 7.

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