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RF coils

The radiofrequency (RF) coil is the closest instrument to the subject under examination in MRI. It is the final component in the transmit chain—determining the uniformity of flip angle and power efficiency—and the first component in the receive chain—determining the image quality. The RF coil is a series resonant circuit, wherein the inductor is a distributed component capable of generating and detecting near-field oscillating magnetic fields. During transmission, the RF coil generates an oscillating magnetic field orthogonal to the static magnetic field, tipping the bulk magnetisation of the sample and the receiver RF coil detects this signal before it decays. 

The oscillating magnetic field interacts with the bulk magnetisation of the sample only when the frequency is the same as the Larmor frequency. Different nuclei have discrete Larmor frequencies according to their gyromagnetic ratios:

Nucleus	Gyromagnetic Ratio  (MHz / T)
1H	42.6
3He	-32.4
13C	10.7
19F	40.1
129Xe	-11.8

Detection of each nuclei requires dedicated multi-tuned RF coils, or sets of coils that resonate at multiple frequencies, thereby imposing RF engineering challenges to enable multinuclear MR capabilities whilst electrically isolating resonant circuits and minimising losses. Resolving these challenges by designing novel RF circuits, components and multinuclear RF coils is the primary focus of engineering research at the POLARIS group - with an intent to apply such technology in the clinical setting. 

X-nuclei RF coils 

There are few commercially available RF coils for X-nuclear (non-¹H) applications, especially when the anatomy of interest is specific, for example brain, lungs, breast and kidneys. In addition, x-nuclei typically resonate at much lower frequencies compared to ¹H, which adds additional challenges to circumvent poor sample loading and filling factor. As such, X-nuclei RF coils often need to be developed in house for specific needs.

Featured Example: ¹²⁹Xe Brain coils

Two birdcage transmit-receive RF coils at 1.5 T and 3.0 T were developed for MR imaging and spectroscopy of inhaled hyperpolarised ¹²⁹Xe in the brain. Using these RF coils, we were able to .

Furthermore, a four channel receiver RF coil was developed in house with superior grade copper, and we were able to . We were also able to show that in a than those seen by contemporary imaging methods. 

Multinuclear RF Coils

There are many approaches to build multinuclear RF coils: 

1. a common resonant structure that resonates at multiple resonant frequencies
2. switchable RF coils using actively-controlled switches 
3. multiple RF coils resonating at different resonance frequencies, and that are electrically isolated
4. using meta-materials

At POLARIS, we have investigated the theory of trap circuits—passive parallel resonant circuits used in series with the RF coil—and we were able to with an arbitrary number of traps. We have demonstrated , and in a breath hold at the same lung inflation state. In addition, we have compared the use of . ¹⁹F is another emerging imaging agent for lung MRI, and the key engineering challenge is the proximity of the resonance frequency to that of protons. We recently proposed an 8 channel distributed transmitter-receiver RF coil with 6 additional receive only channels as the .

People, Projects & Publications

People

Professor Jim Wild

Professor of Magnetic Resonance Physics, Executive Director of Insigneo Institute
Clinical Medicine, School of Medicine and Population Health

Email

j.m.wild@sheffield.ac.uk

Telephone

+44 114 215 9141

Open staff member portrait in a modal window

Mr Oliver Rodgers

Senior Engineering Technician
Clinical Medicine, School of Medicine and Population Health

Email

O.Rodgers@sheffield.ac.uk

Telephone

+44 114 215 9614

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Mr Ryan Munro

Research Engineering Technician
Clinical Medicine, School of Medicine and Population Health

Email

r.munro@sheffield.ac.uk

Telephone

+44 114 215 9595

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Current Projects / Grants

We have ongoing projects in the development of:

• High-density RF coils for multinuclear MRI of the lungs, brain and kidney, e.g.
  • 6 channel ¹²⁹Xe brain RF coil for 3.0 T
  • 8 channel dual-tuned ¹H-¹²⁹Xe RF coil for 1.5/3.0 T
• Novel circuit components for multinuclear MRI 

Our work in MR hardware engineering is / has been supported by the National Institute for Health Research (NIHR), Medical Research Council (MRC), Global Challenges Research Fund (GCRF), BRC grant awards, a studentship from the Natural Sciences and Engineering Research Council of Canada (NSERC), University of ºù«Ӱҵ faculty scholarships, and collaborative funding from the Memorial Sloan Kettering Cancer Center (MSKCC). Current main grants include:

• 04/2015—03/2023. . MRC - Resources and infrastructure Research Grant. PI: Wild
• 06/2016—05/2024. Xenon gas recycling project. PI: Wild

Past Projects / Grants

• 11/2013—10/2018. . NIHR - Research Professorship. PI: Wild
• 10/2012—09/2016. Hyperpolarised 129Xe Magnetic Resonance Imaging Techniques for Assessment of Human Lung Function. . PI: Wild
• 10/2006—10/2011. . EPSRC - Advanced Fellowship. PI: Wild

Collaborators

We work closely with the following MR industry partners:

• GE Healthcare
• Clinical MR Solutions
• Philips
• PulseTeq
• Voxelgrids

Key Publications

• Maunder A, Rao M, Robb F & Wild JM (2020) . Magnetic Resonance in Medicine, 84(4), 2262-2277

• Maunder A, Rao M, Robb F & Wild JM (2018) . Magnetic Resonance in Medicine, 80(4), 1746-1753

• Rao M, Stewart NJ, Griffiths PD, Norquay G, Wild JM (2017) . Radiology, 286(2)

• Rao M, Stewart NJ, Norquay G, Griffiths PD & Wild JM (2016) . Magnetic Resonance in Medicine, 75(6), 2227-2234

• Rao M & Wild J (2016) . Magnetic Resonance in Medicine, 75(4), 1841-1848

• Rao M, Robb F & Wild JM (2015) . Magnetic Resonance in Medicine, 74(1), 291-299