Ria Forner1, Ingmar Voogt2, Bart Steensma3, Kyungmin Nam3, Mark Gosselink3, Debra Rivera4, William T Clarke5,6, Aidin Alihaghnejad2, Arjan Hendriks3, and Dennis Klomp1
1UMC Utrecht, Utrecht, Netherlands, 2Wavetronica B.V., Utrecht, Netherlands, 3University Medical Center Utrecht, Utrecht, Netherlands, 4Eindhoven University of Technology, Eindhoven, Netherlands, 5Wellcome Centre for Integrative Neuroimaging, FMRIB, Nuffield, United Kingdom, 6Department of Clinical Neurosciences, University of Oxford, Oxford, United Kingdom
Synopsis
A novel coil design with a 31P birdcage and a 1H dipole array is presented for the purpose of fMRS applications. This design allows for free line-of-sight for fMRI and fMRS visual stimulation via mirrors and despite a lower fill-factor performs comparably to a smaller dual-tuned birdcage. The matching of both frequencies is adequate for a range of human head circumferences from 52cm through 57cm. The 31P birdcage performance is not significantly degraded by presence of 1H dipoles when compared to a conventional birdcage dual-tuning strategy with Foster networks.
Introduction
31P-MRS gives information about concentrations of key high-energy phosphate metabolites and their rate of creation and use in vivo. Changes in metabolism in the brain are implicated in neurological and psychiatric conditions.
With the development of ultra-high field systems dynamic (functional) in vivo 31P spectroscopy(1) is practicable. Transcranial direct current stimulation (tDCS) is a non-invasive brain stimulation technique producing changes in cortical excitability and firing rates-markers of metabolic activity(2). In this work, a 31P head coil for 7T is developed to be compatible with tDCS equipment and functional brain activation via visual stimulation.
Unlike previous head coils, (3,4), for the purposes of image registration, B0 shimming and f0 determination, the simultaneous use of a 1H coil is imperative. This results in a penalty for dual-tuning in the range of 10%-30% of the SNR as compared to a single-tuned coil(5,6,7,8,9,10,11,12).Methods
This 1H/31P head coil consists of a single-tuned 31P birdcage, with a larger-than-usual radius to accommodate mirrors for allowing visual stimuli for fMRI studies (Fig. 1). Taking advantage of symmetry and to minimise coupling, four meandered proton dipoles(13,14) are placed in line with the inner endring-edges but between the legs of the birdcage, and without overlapping with the end rings.
As a comparison, a 1H/31P dual-tuned birdcage with diameter 24cm is tested with protocols identical to the novel coil.
Simulations
Simulations are first performed for both constituent coils in isolation before the combined setup is simulated (Fig. 2). The simulations are performed in a 2L tissue simulating phantom (σ=1.079S/m; μr=1; εr=78), and in male and female human body models (Duke and Ella, ITIS foundation, Zurich) with the software Sim4Life (Zurich Medtech).The effect of two coils on each other is quantified in terms of the difference in B1+ and the SAR values as compared to the single-frequency setups. The simulations for B1+ and 10g averaged pSAR are normalised to 1W of total input power. This significantly reduces the coupling to the other coil and by only using 4 dipoles, it is possible to preserve symmetry and thus homogeneity of the birdcage while also leaving the line-of-sight open for subjects.
Bench
To address the coupling between the dipoles and the birdcage, an iterative approach to tuning is used. First, the birdcage coil is built with capacitor values to tune it to within 10MHz of the target frequency (120.3MHz). The proton dipoles are then introduced and the phosphorus coil is re-tuned. Finally the dipoles and the birdcage are fine-tuned in the presence of a realistic load and human heads. The bench performance compared to a dual-tuned birdcage coil built in-house(15). Bench measurements made using a network analyser (Fig. 3.) give sufficient confidence in the suitability of the coil towards scanner testing. No decoupling circuitry is necessary (S21 of -8dB to -12dB).
Scanner
Phantom safety scans are performed before the first subject scans. The coil is located using a low SNR, fast localising protocol. Thereafter, the B0 and B1 shimming is performed so as to enable f0 determination as the inhomogeneity on the B field may cause the phosphorus spectra to become indeterminate. Identical B1 maps are acquired for both coils in phantoms and in vivo.The 31P performance is quantified by looking at the power needed to achieve a given flip-angle in comparison to a known reference coil. In this case, we step the flip-angle from 40 degrees in steps of 20 degrees to determine the peak of the sinusoidal envelope. Subsequently, the same protocol is repeated on the reference dual-tuned birdcage coil.Results
See figure 2 for bench results
1H
Simulations
With a simulated 10g average of 0.7W/Kg from simulations, a maximum input power of 3W/ channel can be used before local SAR exceeds 10 W/kg. With a safety factor of 2, average power is limited to 1.5W/channel.
Scanner
B1 maps have similar amplitude for both coils invivo and in the phantom (~12uT)- however, the shimmed dipole-array is more homogeneous than the dual-tuned birdcage
31P
Scanner
Both coils reach the 90 degree(ref) flip-angle at about the same flip-angle setting with all other parameters maintained.Discussion
The presence of the 1H dipole array and 31P birdcage detunes both coils, which necessitates iterative re-tuning.
While a similar 1H B1 of 12uT is reached in the phantom and in vivo with both, the novel and comparison coils, the dipole array shows a more homogeneous excitation due to phase-shimming on 4 channels. The 31P performance of both coils is also similar, with the smaller, dual-tuned coil outperforming the larger novel coil by a factor of 15% in a phantom.Conclusion
Despite having a larger diameter than the reference coil, the novel coil achieves similar B1+ efficiency for both frequencies. This indicates inherently better decoupling between the two frequencies as a result of coil geometry. Shimming the four proton channels gives more homogeneous 1H excitation.
The large gap between coil and shield facilitates the use of a mirror and thus the ability to provide visual cues to the subject with minimum interference to the symmetry of the coil. The relatively large coil size could also permit the use of EEG caps or tDCS (trans-cranial direct current stimulation16) for other neuro studies(17,18 )Acknowledgements
This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 801075, 'NICI' References
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