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A 35Cl ToRo Resonator System for Preclinical MRI/MRS at 9.4T
Matthias Malzacher1, Ruomin Hu1, Jorge Chacon-Caldera1, Andreas Neubauer1, and Lothar R Schad1

1Computer Assisted Clinical Medicine,Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany

Synopsis

Chloride (Cl-) is next to the cations Na+ and K+ the most abundant non-organic anion in the mammals. Assessment of chlorine’s (35Cl) concentration in tissue could provide further insights into tissue viability in addition to tissue sodium concentration. Yet, low Signal-to-Noise ratio (SNR) is challenging for the RF hardware components. To overcome these challenges, a Transmit-only-Receive-only (ToRo) system for 35Cl MRI/MRS at 9.4T was developed comprised of an actively-decoupled linearly-driven 16 leg low-pass Birdcage transmitter coil combined with two different receiver coils. Substantial SNR gain was reached using receive-only elements compared to the Birdcage coil in TxRx mode.

Purpose

Chloride (Cl-) is next to the cations Na+ and K+ the most abundant non-organic anion in the mammals1. Assessment of chlorine’s (35Cl) concentration in tissue could provide further insights into tissue viability in addition to tissue sodium concentration. Furthermore, information regarding physiological processes that involve diverse chlorine channels can be found by evaluating the 35Cl signal of cells in a controlled living environment2. Yet, low Signal-to-Noise ratio (SNR) is challenging for the RF hardware components. For example, special imaging/spectroscopy techniques, such as Triple-Quantum-Filtering3, require homogenous transmission and high receiver sensitivity. To overcome these challenges, a Transmit-only-Receive-only (ToRo) system for 35Cl MRI/MRS at 9.4T was developed and evaluated in simulations and measurements.

Methods

The 35Cl ToRo resonator system is comprised of a transmission (Tx) coil and two different reception (Rx) configurations. EM fields of the coils were calculated using FEM simulations (CST AG, Darmstadt, Germany). Measurements were performed at a 9.4T preclinical MR scanner (Bruker BioSpec 94/20, Ettlingen, Germany).

Tx coil: A linearly driven 16 rung low-pass birdcage (BC) coil was developed to excite the 35Cl nucleus. The BC was tuned to 39.2 MHz (35Cl resonance frequency at 9.4T) with tuning capacitors arranged alternately to increase B1+-field homogeneity. Balancing of the coil was done using a separated ground ring4. Active decoupling was implemented by shortening 4 rung capacitors of the BC (Figure 1 and 2a). The BC was shielded using a “Swiss roll” configuration made of copper foil and an FR4 dielectric. B1+-field homogeneity was evaluated in simulation and measurement using a spherical phantom (diameter=48mm) filled with 18% saline solution.
Measurement sequence: 2D UTE, TE/TR/FA=0.33ms/100ms/80°, matrix=80x80, FoV=60x60mm², slice=20mm, Projections=252, TRA=4ms, Avg=4 and TA=1:40min. Simulation and measurement results were compared using a calibration factor5.


Rx coils: Two different configurations of Rx only coils (denominated Rx Loop and Rx Loop+BF) were developed for measurement and in simulation. Rx Loop was made using a doubled winded silver conductor (diameter=27mm, thickness=2mm) (Figure 2b). Rx Loop+BF consisted of a doubled winded loop and a butterfly coil made of copper tape (width=3mm)(Figure2c-e). All Rx coils were equipped with a cable trap, a low noise preamplifier and actively decoupling unit. Simulation and measurements were performed using two vials(length=28mm, diameter=6mm) filled with 0.9% saline solution.
Measurement sequence: 2D UTE, TE/TR/FA =0.62ms/30ms/72°, matrix=80x80, FoV=80x80mm², slice=8mm, Projections=252, TRA=4ms, Avg=64, TA=8min.

Results

Tx coil: A decoupling of 40dB was achieved by shortening 4 tuning capacitors using PIN diodes. The results of the homogeneity simulations and measurements are depicted in Figure 3. Simulated and measured SNR show resemblance. Yet, the simulated SNR was overestimated. Good homogeneity was accomplished in axial, coronal and sagittal plane over the whole sensitivity volume.

Rx coils: The simulation and measurement results of the BC coil in TxRx mode and the BC coil combined with the different Rx coils are shown in Figure 4. B1--fields increased using the Rx coils for signal reception instead of the volume resonator as expected. The respective SNR measurements revealed the same SNR gain of the Rx coils compared to the BC. The two vials can be well separated using the Rx only coils whereas the vials can hardly be seen using the BC coil in TxRx mode. The noise level of the Rx Loop+BF coil is higher compared to the Rx Loop coil, probably due to coil coupling.

Discussion

By using a BC coil for excitation of the 35Cl nucleus good homogeneity was achieved over a large volume. The extension of the BC coil with Rx only elements increased the SNR performance dramatically. No significant SNR gain was achieved using two receiver channels. The improvement of the Rx coils will be in the scope of future works.

Conclusion

SNR gain using a ToRo setup for 35Cl MRI at 9.4T was achieved. Using this RF resonator system it is now possible to design studies with animals and cells in a controlled living environment.

Acknowledgements

No acknowledgement found.

References

[1] Baier S, Krämer P, Grudzenski S, et al. Chlorine and sodium chemical shift imaging during acute stroke in a rat model at 9.4 Tesla. Magn Reson Mater Phy.2014;27(1):71-79.
[2] Neubauer A, Ruttorf M, Kalaycian R, et al. 23Na Magnetic Resonance Spectroscopic Imaging (MRSI) on a High-Density 3d-cell culture on chip (3D-KITChip). ISMRM.2014;22:1278
[3] Gottwald E, Neubauer A, Schad LR. Tracking Cellular Functions by Exploiting the Paramagnetic Properties of X-Nuclei, Assessment of Cellular and Organ Function and Dysfunction using Direct and Derived MRI Methodologies, Dr. Christakis Constantinides (Ed.), InTech,2016.
[4] Streif JU, Lanz T, Griswold M, et al. A coil combination for magnetic resonance perfusion imaging of mice in vivo at 7 T. Rev Sci Instrum.2003:74(5):2843-2848.
[5] Stumpf C, Rehner R, Martius S, et al. Calibration of electromagnetic field simulations of MR coil arrays for accurate quantitative comparison with the measured image SNR. ISMRM.2012.20:2684.

Figures

Figure1: Section of the electric circuit diagram of the Tx BC coil. Ct: capacitors to tune the BC to the desired frequency. Cm: variable matching capacitor for adaption to different loads. Cdc: DC block capacitors. LRF: RF block inductors.

Figure 2: a) TX BC coil without shield. b) Rx loop coil. c) Rx Loop+BF coil with d) the upper and e) the lower part of the Rx Loop+BF coil.

Figure 3: Simulation and measurement results using the BC coil in TxRx mode using a spherical phantom (diameter=48mm) filled with 18% saline solution.

Figure 4: Simulated B1--fields and measured SNR results using the small vials load and the different resonator combinations. Significant SNR gain was reached using the Rx coils.

Proc. Intl. Soc. Mag. Reson. Med. 25 (2017)
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