Two major challenges for MRI of short-T2 tissues are creating large gradient strengths and avoiding signal contamination from hardware parts, in particular the RF coils. In this work, to enable short-T2 MRI with a dedicated insert gradient coil, an RF birdcage coil was designed with a) minimized background signal and b) optimized B1 field to prevent aliasing associated with the limited monotonic range of the gradient.
Introduction
Two major challenges for MRI of short-T2 tissues are creating large gradient strengths and avoiding signal contamination from hardware parts, in particular the RF coils [1] [2]. In this work, to enable short-T2 MRI with a dedicated insert gradient coil, an RF birdcage coil was designed with minimized background signal and optimized B1 field to prevent aliasing associated with the limited monotonic range of the gradient [3].A high-pass birdcage electrically designed by using FDTD-simulations (Sim4Life, ZMT, Zurich, Switzerland) was constructed based on two quartz glass cylinders assembled with PTFE plates (fig. 1a). 16 legs made from copper tubes as well as capacitors with micro-strip outlines were directly screwed to the endring elements. A conductive textile was used as shield (Holland Shielding Systems BV, Dordrecht, the Netherlands). After assembling, the coil was cleaned with acetone.
The RF coil with an outer diameter of 32 cm fits into an insert gradient installed in a 3T human whole body scanner (Philips Achieva, Philips Medical Systems, Best, the Netherlands) with a field distribution along the z direction as shown in fig. 1b. Imaging was performed with the short-T2 3D zero-echo-time (ZTE) technique employing a custom-built spectrometer [4] and a symmetrically biased T/R switch [5]. The field of view defined for the insert gradient is indicated in fig. 1c.
As expected intrinsic image contrast of ZTE images of a humans head is poor. Signal intensity of tissues with short T2 relaxation time constants is usually much lower than the one of other components. Nevertheless, in the presented in vivo images short T2 signal was detected. In ZTE images field inhomogeneity due to susceptibility differences does not cause unwanted signal dephasing nor image distortions, which explains the reduction of artifacts close to the nasal sinuses.
In this study, image quality of in vivo ZTE images was limited by the flip angle which can be achieved with block RF pulses short enough to reconstruct the gap in k-space center algebraically. This challenge could be faced by using power efficient excitation pulses such as sweep pulses [6], [7] in combination with other techniques to fill the gap such as PETRA [8] or WASPI [9].
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