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Self-shielded and self-decoupled transmit RF array for 7T head imaging
Xinqiang Yan1,2, Yue Zhu1,2, and Ming Lu1,2
1Vanderbilt University Institute of Imaging Science, Nashville, TN, United States, 2Department of Radiology and Radiological Sciences, Vanderbilt University Medical Center, Nashville, TN, United States

Synopsis

Transmit (Tx) array with multiple independent coil elements is a well-recognized approach to addressing the B1 inhomogeneity and high local SAR issues at ultrahigh fields. However, Tx arrays typically have a lighter loading and more severe coil coupling. We designed a self-shielded and self-decoupled 2x8 Tx array with high inter-element isolation for 7T head imaging. Each Tx element is based on the corner-fed self-decoupled coil. Four coil elements were constructed to prove the concept is viable. The coil elements are highly decoupled (inter element response < -15 dB) while maintaining good tuning/matching characteristics (power reflection < -20 dB).

Introduction

Transmit (Tx) array with multiple independent coil elements is a well-recognized approach to addressing the B1 inhomogeneity and high local SAR issues at ultrahigh fields [1]–[14]. Due to the space restriction, Tx arrays are typically placed outside the receive (Rx) array, several centimeters away from the tissue, leading to a lighter loading and more severe coil coupling. At the same time, the standard preamp decoupling in the Rx array is not feasible for Tx coils. Therefore, Tx arrays usually require special decoupling methods that increase the hardware complexity and cost, especially for multi-row Tx arrays with strong coupling from elements in the same rows and columns. Therefore, a simple Tx array design is preferred to simplify hardware fabrication and reduce failure costs and risk. We designed and constructed a self-shielded and self-decoupled 2x8 Tx array with high inter-element isolation for 7T head imaging. Unlike conventional Tx arrays, this coil array is easy to build/reproduce because individual coil blocks could be easily assembled without worrying about coil coupling.

Methods

The modular Tx element is based on the corner-fed self-decoupled coil [15]. As currents along the two arm conductors are not equal in magnitude, B1 fields of the coil differ when fed at the top left or top right corner. In this work, the coil was fed at the top-left corner to benefit the B1+ field. Figure 1 shows how the B1+ and B1- changed when the feed board changed from the top left corner to the top right corner.
The Tx array was designed to be mounted on a 29-cm-diameter acrylic tube (Figure 2a). Each coil has a length/width of 13/9 cm and was made from 10-mm-width copper tape (Figure 2b). The detailed circuit schematic of each Tx coil is shown in Figure 2c. The frequency tuning and impedance matching were realized by trimmer capacitors (from 1.5 pF to 10 pF) instead of inductors. Each coil was individually shielded to avoid its crosstalk with the outer environment. To realize self-decoupling for both circumferential and axial directions, the coil conductor has a 1.7-mm gap at the centrosymmetric position to the feed port. An active detune circuit was employed to disable the Tx coil during the receive phase. A 2x2 coil array was built and bench-tested on a cuboid phantom placed 5 cm below.

Results and Discussion

Figure 3a shows the constructed four self-shielded and self-decoupled coils (2x2 layout, with the shield on/off). Figures 3b plotted the measured S-parameters versus frequency, and Figure 3c depicted the S-matrix at the desired frequency (298 MHz, Larmor frequency of 7T). The inter-element isolation between the adjacent element in the same row (S12 and S34), adjacent elements in different rows (S14 and S23), and diagonal elements (S13 and S24) are ~ -18/-18 dB, ~ -24/-15 dB, and ~-24/-15 dB, respectively. Figure 4a shows each coil's measured quality factors (Q-) in both unloaded and loaded scenarios. The measured ratios between unloaded and loaded Q-factors range from 1.79 to 2.16, with an average of 1.92. Figure 4b depicted the detune performance measured with a double-pick-up probe. The detune could achieve <-20 dB for each coil, indicating a neglectable effect on the receive performance when a separate receive array is used.

Conclusion

A 16-channel double-row self-shielded and self-decoupled Tx coil array was designed, initially constructed, and tested. The self-decoupling approach eliminates additional decoupling methods, and the individual modular shield eliminates the need for a whole RF shield. This design is easy to build/reproduce, providing a much simpler approach to constructing highly-decoupled multi-row detunable Tx arrays for human imaging at ultrahigh fields.

Acknowledgements

This project is supported by NIH EB R21 029639.

References

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Figures

Figure 1 Simulated axial B1+ and B1- maps in a 19-cm-diameter cylindrical phantom demonstrate the difference between the top left corner-fed and top right corner-fed coils. Simulations were performed using Ansys HFSS and Ansys Designer (Pittsburgh, PA).

Figure 2 a) The 3D model of the 2x8 self-shielded self-decoupled Tx coil array for 7T head imaging. The shields on the top row are removed for illustration purposes. b) A single self-shielded self-decoupled Tx coil with the feed port located on the top left and an open circuit at the bottom right. c) Circuit diagram of a single coil with component values illustrated.

Figure 3 a) Photo of four Tx coils in the 2x2 arrangement (left: without shield, right: with shield). b) S-parameter plots of these four coils. The solid lines represent the matching/tuning curves, while the opaque lines show the coupling curves. c) Summary of the S-parameter at 298 MHz (1H frequency at 7 T).

Figure 4 a) Coils’ Q factors with/without a phantom load. b) Coils’ detune performance indicated by the resonate peak change of a double pick-up probe. The good detune performance of < -20 dB indicates Tx coils would be well disabled in the receive phase and have no impact on the receive coils.

Proc. Intl. Soc. Mag. Reson. Med. 30 (2022)
4501
DOI: https://doi.org/10.58530/2022/4501