Very low field MRI setup for brain imaging
Reina AYDE1 and Claude Fermon1

1SPEC, CEA, CNRS, Université Paris-Saclay, Gif-sur-Yvette, France

Synopsis

Mixed sensors are at present competitive with classical tuned coils for the detection of MRI signals on a very low field range. A very low field head MRI system is developed without pre-polarization technique nor magnetic shielding room. Homogeneity of the system and gradients were characterized. A homogeneity of 115 ppm was achieved in a quasi-open configuration. Linearity of the gradients was verified. The amplitude of each gradient was 100 times lower than at high field but sufficiently high to achieve a resolution of 2 mm x 2 mm x 2 mm.

Target audience

MRI engineers, researchers, radiologist and all medical center interested in a low field MRI setup.

Purpose

Very low field Magnetic Resonance (VLF MRI) is a complementary imaging modality of conventional MRI1. VLF MRI based on inductive coils has many advantages: It is a low cost MRI (<50 000$), light weight, transportable (<100 Kg) silent and applicable to patients with metallic implants and pacemakers, claustrophobics and premature babies. Moreover, a new kind of image contrast appears at this range of field that could help in depicting cancer2-3. However, VLF MRI is inherently limited in signal-to-noise Ratio (SNR) and requires important averaging time to obtain images with sufficient SNR for a relevant diagnosis. Many methods were employed in order to improve NMR signal and/or detectivity, i.e., Pre-polarization method4 and/or the use of SQUID or atomic magnetometers5-6. Our laboratory has developed Nitrogen cooled superconducting-magnetoresistive hybrid sensors7 competitive to low Tc SQUIDs above 100kHz. These sensors are untuned and can be coupled through low resistive room temperature flux transformers to a room temperature antenna presenting a high filling factor. They are very robust and accept strong RF pulses with a very short recovery time compared to tuned RF coils, which allow measurements of broad signals. We have already proved the efficiency of using these sensors on a small VLF MRI setup8. In the present work, a VLF whole head MRI system is developed and characterized in order to study the effectiveness of mixed sensors in such a simple clinical system without employing pre-polarization technique or magnetic shielding room.

Method

A VLF MRI setup and a spectrometer were constructed (figure 1). An adjusted three coils Maxwell configuration is adopted to generate the main magnetic field. Coils are designed in order to minimize enclose feelings of claustrophobes (cylinder diameter of 83 cm). Inductive coils are water cooled providing an adjustable magnetic field up to 12 mT. Experiments are usually done at B0=8 mT (353 kHz). Double split saddle coils are used to generate gradient fields along frequency and phase (X and Y) directions and circular Maxwell coils are used to generate the gradient field along Z direction. Gradient coils are used not only for 3D imaging but also for correcting external inhomogeneity (shimming). To test the homogeneity of the static field, we used a container of 200x200x200 mm3 volume filled with doped water (T1 ≈ 120 ms; T2 ≈ 70 ms) simulating the average relaxation time of a brain. A 90â—¦ pulse is applied to obtain a Free Induction Decay (FID). The NMR time-domain signal is Fourier transformed to obtain the magnitude of the resulting spectrum. To test gradients linearity, we have imaged a sample, presented in figure 3a, filled with same doped water. The linearity of the gradients is directly measured on the image profile. We performed 1D images along X and Y directions. Then the position of the signal with the actual position of doped water in the phantom are compared. We have used, for these measurements a tuned coil (Q = 50) placed around the sample.

Results

The Fourier transform of the FID signal is presented in figure 2. Achieved homogeneity is about 115 ppm for 200x200x200 mm3 volume.

Then, gradients linearity was verified. We obtained around 3% of error along both X and Y directions (figure 3). Adjustable gradients strength was also studied. A gradient of 500 µT/m was sufficient to get a 2 mm resolution.

Discussion

Homogeneity of 115 ppm gives the resolution bandwidth (1 point = 40 Hz). Thus, a bandwidth of only 4 kHz will be sufficient for imaging a 200 mm length sample. This fact will compensate partially the loss in SNR due to low polarization at low field. In another hand, although gradients strength allows a good image resolution, those gradients (less than 1 mT/m) imply longer readout sequence limiting the possibility of reducing time’s sequences.

Conclusion

A VLF MRI brain setup was constructed with an adjustable main magnetic field (<12 mT). A field homogeneity of 115 ppm was achieved on a 200x200x200 mm3 volume with this simple and open configuration. Future work will focus on reducing 3D imaging time sequence in order to be ready to combine mixed sensors with brain VLF MRI setup.

Acknowledgements

We acknowledge the Technosanté program support.

References

[1] Sarracanie M, LaPierre C, Salameh N, David E. J. Waddington D, Witzel T, Rosen M, Low-Cost High-Performance MRI. Sci. Rep. 2015; 5:15177. [2] Lee S, Mößle M, Myers W, Kelso N, Trabesinger A, Pines A and Clarke J, SQUID-detected MRI at 132 µT withT1-weighted contrast established at 10 mT-300 mT. Magnetic Resonance in Medicine 2005; 53(1):9-14. [3] Busch S, Hatridge M, Mößle M, Myers W, Wong T, Mück M, Chew K, Kuchinsky K, Simko J, and Clarke J. Measurements of T1-relaxation in ex vivo prostate tissue at 132 mT. Magn Reson Med. 2012;67(4):1138-45. [4] Macovski A and Conolly S, Novel approaches to low-cost MRI. Magnetic Resonance in Medicine, 1993; 30: 221-230. [5] Espy M. A. et al. Progress toward a deployable SQUID-Based Ultra-Low Field MRI system for anatomical imaging. IEEE Transactions on Applied Superconductivity, 2015; 25:1-5. [6] Xu S, Rochester S M, Yashchuk V V, Donaldson M H, and Budker D, Construction and applications of an atomic magnetic gradiometer based on nonlinear magneto-optical rotation. Review of Scientific Instruments 2006; 77: 083106. [7] Pannetier M, Fermon C, Le Goff G, Simola J, Kerr E. Femtotesla magnetic field measurement with magnetoresistive sensors. Science 2004; 304(5677):1648–1650. [8] Herreros Q, Dyvorne H, Campiglio P, Jasmin-Lebras G, Demonti A, Pannetier-Lecoeur M, and Fermon C, Very low field magnetic resonance imaging with spintronic sensors, REVIEW OF SCIENTIFIC INSTRUMENTS 2013; 84: 095116.

Figures

Photo of VLF MRI brain setup

Fourier transform of a FID of a 200x200x200 mm3 container filled with doped water with shimming in black, without shimming in red.

Figure 3: a) Schematic representation of the sample. Frequency profile of the sample along b) X and c) Y directions.



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)
3557