Dielectric Materials & Resonators
Sebastian Aussenhofer

Synopsis

This session explains the source of dielectric effects in MRI. It is furthermore explained how the dielectric effects can be used to improve image and spectra quality.

HIGHLIGHTS

· dielectric materials can improve magnetic resonance imaging

· high field mri coils can be build from water with very little effort

· modes of dielectric materials for cylinders can easily be estimated

TARGET AUDIENCE researchers and engineers working in the field of high and ultra high field MRI. OUTCOME This talk will inform you about dielectrics, their effects on MRI and how to use them to improve imaging. After this talk you should have a general understanding about dielectrics. You will be able to build a simple microscopy coil for your ultrahigh field mri just using destilled water, a bucket and a pickup probe made from ordinary coaxial wire. You will understand how to use dielectric bags to homogeneize your RF field and thus improving data quality on 3.0, 7.0 Tesla and even higher field strength experiments. PURPOSE Why do we need Dielectric Materials and Resonators? Since the introduction of 3.0 Tesla mri wavelength effects in the human body can no longer be neglected as the high field strength also means a higher frequency is needed for the B1 field (1). However this leads to decreased homogeneity in the body trunk at higher field strength due to the shorter wavelength. Already in standart clinical applications on 3.0 T this effect leads to areas of local signal voids and thus uneven image brightness for example in breast and abdominal imaging (2). Dielectric resonators are interesting alternatives to lumped element mri volume coils especially at higher field strengths (3) and can also be used as surface coils (4). We can summarize the main challenges in high field MRI as: · Inhomogeneous B1+ · Increased SAR · Shading artifacts · Areas of poor contrast This leads to poor image quality (figure 1) already at 3T in the abdomen and in the head also visible in the head.

RESULTS

Due to the decreased wavelength of the B1 radio wave at higher field strength the wave becomes so short that we get standing wave patterns inside the human body. This effect can be clearly shown with an electromagnetic field simulation in the human head for different field strength (figure 2).

However the wavelength is not the only variable leading to this undesired artifacts. One can also clearly show with electromagnetic simulation that the dielectric constant εr of the object in which the wave is traveling has a major impact.

We can combine this knowledge to produce a secondary B1 field by using a bag filled with a high dielectric that „fills up“ the lateral voids in the head if positioned right.

It is then possible to design pads with the right shape and dielectric constant to improve the B1 field in a selected region in our sample with the help of electromagnetic simulations (figure 5) for example targeted for imaging of the inner ear.

METHODS

How to make and use high dielectric bags to improve imaging.

The production of high dielectric bags is very simple: the bag that usually contains a slurry made from a high dielectrics ceramics power such as barium titanat (BaTiO3) gets mixed with water, preferably this should be deuterized if you do not want to see your bag later on the image, and then put into a sealable plastic bag. The application is also simple: for the head at 7 Tesla for example one places the bags just around the backside of the head approximatley from ear to ear (7). On 3 Tesla cardiac and abdominal imaging, one simply puts the bag suspine on the patients chest beneath the coil (see figure 1).

Once one realises the effect of dielectrics on mri, especially the central brightning in the head, one can assume that it also be possible to use this standing wave effects in dielectric materials to ones advantage and build a resonator based on this principle. Indeed this is possible and has been first shown by Wen et al. (8). The feasibilty of these resonators has been shown also at ultra high fields by Neuberger et al. (9) Further designs have been presented in recent years by dutch groups (3,4,10–13).

CONCLUSION

Relevance to clinical practice

Understanding dielectric materials, their properties and how they interact with modern MR systems is an important part of ultra high field mri. The usage of high dielectric bags helps easily to improve image and data quality while reducing SAR. It is now already used on a routine basis at 3 Tesla (14) and for research studies at 7 Tesla field strengh.The principle of how these dielectric bags work has been understood and concerns about negative influence on SAR have been neglected in previous studies (15).

Relevance to future research

Dielectric materials will continue to be an interesting topic in the future of MRI. The basic concept has been addressed (5,16,17) and one can anticipate ongoing improvement of dielectric pad composition and geometry for example by using a target field simulation approach. The integration of dielectric materials in selected coils for ultra high field MRI seems to be the next logical step. Different pads for different body geometries might be required to get optimal results. Future work will show if there is a „one size fits all“ solution or those pads should be more personalized for maximum benefits in contrast-to-noise ratio, homogeneity of B1 and the reduction of the specific absorption rate. Dielectric materials can be used to build novel RF coils (8,12,13) for MRI. The intuitive way to build a simple dielectric resonator from destilled water (8,10) for example for microscopy experiments makes them a usefull skill for researchers working on high Field MRI systems. The high radio frequency nature of ultra high field MRI systems allows for a multitude of new concepts for novel resonators designs for volume and surface coils and has also found its way into traveling wave MRI (11).

Acknowledgements

No acknowledgement found.

References

1. Machann J, Schlemmer H-P, Schick F. Technical challenges and opportunities of whole-body magnetic resonance imaging at 3T. Phys. Med. 2008;24:63–70. doi: 10.1016/j.ejmp.2008.01.011.

2. Dietrich O, Reiser MF, Schoenberg SO. Artifacts in 3-Tesla MRI?: Physical background and reduction strategies. 2008:1–9.

3. Aussenhofer SA, Webb AG. High-permittivity solid ceramic resonators for high-field human MRI. NMR Biomed. 2013. doi: 10.1002/nbm.2990.

4. Aussenhofer SA, Webb AG. An eight-channel transmit/receive array of TE01 mode high permittivity ceramic resonators for human imaging at 7T. J. Magn. Reson. 2014;243:122–9. doi: 10.1016/j.jmr.2014.04.001.

5. Webb AG. Dielectric Materials in Magnetic Resonance. Concepts Magn. Reson. Part A 2011;38A:148–184. doi: 10.1002/cmr.a.

6. Brink WM, van der Jagt AM a, Versluis MJ, Verbist BM, Webb AG. High permittivity dielectric pads improve high spatial resolution magnetic resonance imaging of the inner ear at 7 T. Invest. Radiol. 2014;49:271–7. doi: 10.1097/RLI.0000000000000026.

7. Snaar JEM, Teeuwisse WM, Versluis MJ, van Buchem MA, Kan HE, Smith NB, Webb AG. Improvements in high-field localized MRS of the medial temporal lobe in humans using new deformable high-dielectric materials. NMR Biomed. 2011;24:873–9. doi: 10.1002/nbm.1638.

8. Wen H, Jaffer FA, Denison TJ, Duewell S, Chesnick AS, Balaban RS. The evaluation of dielectric resonators containing H2O or D2O as RF coils for high-field MR imaging and spectroscopy. J. Magn. Reson. B 1996;110:117–23.

9. Neuberger T, Tyagi V, Semouchkina E, Lanagan M, Baker A, Haines K, Webb AG. Design of a Ceramic Dielectric Resonator for NMR Microimaging at 14 . 1 Tesla. :109–114. doi: 10.1002/cmr.b.

10. Aussenhofer SA., Webb AG. Design and evaluation of a detunable water-based quadrature HEM(11) mode dielectric resonator as a new type of volume coil for high field MRI. Magn. Reson. Med. 2012;68:1325–31. doi: 10.1002/mrm.24451.

11. Andreychenko A., Bluemink JJ, Raaijmakers a. JE, Lagendijk JJW, Luijten PR, van den Berg CAT. Improved RF performance of travelling wave MR with a high permittivity dielectric lining of the bore. Magn. Reson. Med. 2012;000:n/a–n/a. doi: 10.1002/mrm.24512.

12. Bluemink JJ, Koning W, CAT van den B. Torus-shaped dielectric resonator for 7T musculoskeletal imaging. In: Vol. 20. ; 2012. p. 540.

13. Koning W, Bluemink JJ, Langenhuizen EAJ, Raaijmakers AJ, Andreychenko A, van den Berg CAT, Luijten PR, Zwanenburg JJM, Klomp DWJ. High-resolution MRI of the carotid arteries using a leaky waveguide transmitter and a high-density receive array at 7 T. Magn. Reson. Med. 2012;000:1–8. doi: 10.1002/mrm.24345.

14. Franklin KM, Dale BM, Merkle EM. Improvement in B1-inhomogeneity artifacts in the abdomen at 3T MR imaging using a radiofrequency cushion. J. Magn. Reson. Imaging [Internet] 2008;27:1443–7. doi: 10.1002/jmri.21164.

15. Brink WM, Webb AG. High permittivity pads reduce specific absorption rate, improve B 1 homogeneity, and increase contrast-to-noise ratio for functional cardiac MRI at 3 T. Magn. Reson. Med. 2014;71:1632–1640. doi: 10.1002/mrm.24778.

16. Teeuwisse WM, Brink WM, Haines KN, Webb AG. Simulations of high permittivity materials for 7 T neuroimaging and evaluation of a new barium titanate-based dielectric. Magn. Reson. Med. 2012;67:912–8. doi: 10.1002/mrm.24176.

17. Yang QX, Wang J, Wang J, Collins CM, Wang C, Smith MB. Reducing SAR and enhancing cerebral signal-to-noise ratio with high permittivity padding at 3 T. Magn. Reson. Med. 2011;65:358–62. doi: 10.1002/mrm.22695.

Figures

Figure 1 Image artifacts due to wavelength effects on 3.0 T (left) showing shading in abdominal imaging anterior and posterior and at 7.0 T heag imaging (right) showing central brightning while poor lateral signal.

Figure 2 Simulated gradient-echo images, assuming a low tip-angle excitation, as a function of field strength using a birdcage coil with ideal current distributions in the rungs. Figure courtesy of A. Webb (5).

Figure 3 Influence of the dielectric constant on a elliptical phantoms. The B1 field is given using a birdcage coil with ideal current distributions in the rungs. Figure courtesy of W. Brink.

Figure 4 A secondary B field can be created by putting a dielectric material lateral to the head. The B1 field produced by the transmit coil will cause a current to flow in the dielectric material thus creating a secondary B field

Figure 5 Improving the B1 field for imaging of the inner ear. Simulation data is shown for a human head with and without pads. Image courtesty of W. Brink (6).

Figure 6 Imaging of the inner ear at 3.0 T without dielectric pads (left) and with dielectric pads (right) showing a dramatic improvement in image quality. Image courtesty of W. Brink (6).

Figure 7 Putting a dielectric bag on the chest to improve cardiac imaging at 3.0 T



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)