Mingyan Li1, Aurelien Destruel1, Ewald Weber1, Aiman Al-Najjar2, Shekhar Chandra1, Feng Liu1, Craig Engstrom3, and Stuart Crozier1
1School of Information Technology and Electrical Engineering, The University of Queensland, Brisbane, Australia, 2Centre for Advanced Imaging, The University of Queensland, Brisbane, Australia, 3School of Human Movement and Nutrition Sciences, The University of Queensland, Brisbane, Australia
Synopsis
High-resolution prostate imaging for
both 3T and 7T MRI are challenging, given the deep location of this exocrine
gland which accentuates technical issues related to the reduced electromagnetic
penetration and B1 inhomogeneity. In this work, high-resolution (0.3 x 0.3mm
in-plane) non-interpolated T2w-TSE prostate images from a healthy volunteer were acquired at 3T using
a commercial 18-channel body matrix and 32-channel spine coil and an 8-channel
prototype coil at 7T at 15 slices and 11 slices, respectively. Compared with standard
clinical prostate imaging at 3T, the 7T prostate images provided higher SNR and
better differentiation of various zones of the prostate.
INTRODUCTION
The prostate is a multi-gland organ located
deep within the pelvic region. High resolution prostate imaging is challenging
for both 3T and 7T for a variety of reasons. At 7T, the wavelength is only
about 11cm inside of the human body 1, leading to reduced field penetration for
visualisation of the prostate. In addition, the prominent wavelength effect produces
destructive and constructive interferences that may cause signal void in/around
the prostate. Although the wavelength effect is not problematic at 3T, the
whole-body coil is distant from the patient, resulting in reduced transmit
efficiency. In addition, standard commercial receive-only body coil array generally
only activate a few elements for imaging the prostate, which undermines the potential
signal-to-noise ratio (SNR) improvement. In previous works that using
non-invasive surface coil array 2-4, images with 0.8 x 0.8 mm in-place resolution were
normally acquired. High resolution (0.35 x 0.35 mm) prostate image was also achievable
5 but with only one slice mainly due to
the high SAR. In this work, we acquired high resolution (0.3 x 0.3mm
in-plane, non-interpolated) T2 weighted Turbo Spin Echo (T2w-TSE) prostate images at 15 slices
and 11 slices at 3T and 7T MRI. The results demonstrated the advantage of 7T
prostate imaging with higher SNR and clearer differentiation of different zones of the prostate. METHODS
The 7T prostate images were acquired on
a 7T research system Magnetom (Siemens Healthcare, Erlangen, Germany) with an 8-element
prototype radiofrequency parallel transmission (pTx) coil, which is a modified version of the previous work 6. The 3T prostate
images were acquired from a 3T Magnetom Prisma fit (Siemens
Healthcare, Erlangen, Germany) using an 18-channel receive-only body coil (anterior)
and 32-channel receive-only spine coil (posterior). Both scanners are located
at the Centre for Advanced Imaging, The University of Queensland. All prostate
images were acquired from the same healthy, 29-year-old volunteer. Axial and
coronal images were collected with an in-plane resolution of 0.3 x 0.3mm (non-interpolated) and a
slice thickness of 3mm. Sequence parameters are listed in Table I. A configuration
of the coil and patient setup for 7T in the transverse plan is shown in Figure
1. Four coil elements of the prototype coil array were positioned over the
anterior and posterior surfaces of the pelvis. A custom designed phase-only B1
shimming code was implemented to improve the B1 uniformity and
amplitude in the prostate region 7, and included constraints based on virtual observation
points 8 to limit the 10g-averaged specific
absorption rate (SAR10g) 9. The B1 maps were acquired
with a system provided turbo-FLASH sequence 10. Participant informed consent form was obtained and all protocols were approved by the institutional review board. RESULTS
As shown in the Figure 2 (a) for the 7T
setup, the default all zero phases caused destructive interference (dark bands)
over the prostate region (red ellipse). However, after applying the optimised phases
calculated from the custom B1 shimming algorithm, the B1
was constructively formed at the selected prostate region (Figure 2 (b)) which
provided enhanced signal. Because different transmit and receive coils were
used and the pre-scan normalisation was adopted to remove the transmit sensitivity
at 3T, a direct quantitative SNR comparison at 3T and 7T is very challenging.
However, visual comparison in Figure 3 shows that the 7T prostate images have lower
noise and clearer boundaries than those acquired at 3T for both axial and
coronal planes. The peripheral zone and central gland in 7T images are better differentiated
than those in 3T images, which have ambiguous and blurry boundaries. Although
dark bands are seen on the urinary bladder at 7T, they are not super-imposed on
the prostate as per B1 map shown in Figure 2. DISCUSSION AND CONCLUSION
It is noteworthy that although we
acquired fewer slices at 7T, the maximum SAR10g was not reached,
indicating the potential of acquiring more slices. In this work, high
resolution non-interpolated (0.3 x 0.3mm in-plane) T2w-TSE prostate images were acquired at
multiple slices for both at both 3T and 7T MRI. Compared with a standard
clinical setup for prostate imaging at 3T, the 7T prostate images provided
higher image quality and better differentiation of various zones of the
prostate. In future work, the T2w -TSE sequence will be optimised for better
contrast and DWI images will be acquired for comparison at both 3T and 7T MRI. Acknowledgements
No acknowledgement found.References
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