Bart W.J. Philips1, Stephan Orzada2, Ansje Fortuin1, Marnix C. Maas1, and Tom W.J. Scheenen1,2
1Radiology and Nuclear Medicine, Radboud University Medical Centre, Nijmegen, Netherlands, 2Erwin L. Hahn Institute for Magnetic Resonance Imaging, Essen, Germany
Synopsis
MRI of the
pelvis at a high spatial resolution has potential to assess lymph node status
in oncological diseases. We propose to use spectrally selective 3D gradient echo imaging
in combination with TIAMO at 7 Tesla to improve upon spatial resolution using
the SNR increase that ultra high field MRI provides. The method is shown to robustly
obtain homogeneous, large FOV body imaging of the pelvic lymph nodes with a
spatial resolution of 0.66x0.66x0.66 mm3, both
for T2* weighted as well as lipid selective imaging.Introduction
Pelvic lymph
node (LN) imaging is an important tool for regional staging in different types
of cancer [1]. Because these LNs are often small and assessment of their status
is based on morphological characteristics, high resolution MRI could aid in improving
the detection of LN metastases. Ultra high magnetic field potentially offers high
NMR sensitivity, but suffers from radiofrequency (RF) transmit field
inhomogeneities. This is detrimental for lymph node imaging, as it may cause lymph
node metastases to be missed due to local signal intensity losses. In this
abstract we propose to use the time interleaved acquisition of modes (TIAMO)
technique to overcome the homogeneity issues, such that the high signal to
noise ratio (SNR) of ultra high field MRI can be exploited to image LNs over the
whole pelvis with a high spatial resolution. The larger chemical shift
dispersion between water and lipids on 7 Tesla is used to enable short water or
fat selective excitation pulses, avoiding the fat/water chemical shift
displacement artifact in gradient echo (GRE) imaging. This results in T2*
weighted (T2*W) and lipid (similar to T1 weighted) images to assess lymph nodes with two
different types of imaging contrast [2]. In addition, a multi GRE sequence is
used, to enable the calculation of images at arbitrary echo times (TEs), providing
flexibility in T2* contrast [3].
Methods
All measurements were performed on a 7T whole
body MR system (Siemens Magnetom, Erlangen, Germany) with an 8 channel
1H
transceiver body-array coil with meander-type microstrip elements [4]. TIAMO
was used in all measurements and a phase and amplitude shimming algorithm was
applied to optimize the two complementary TIAMO acquisition modes for root sum of
squares homogeneity [5,6].
A 3D GRE sequence was used with a 970 μs
excitation block pulse (Figure 1A) to obtain lipid images. The duration of the
excitation pulse was chosen such that the zero crossing of the frequency
profile of the pulse was at the water resonance frequency, so only lipid tissue
was excited. The images were acquired with a TR of 5.2 ms, TE of 2.09 ms and a
voxel size of 0.66x0.66x0.66 mm
3 (FOV
210x210x169 mm
3, matrix 320x320x256, phase oversampling 50%, GRAPPA acceleration of
2 in phase encoding and 2 in 3D direction) with 2 alternating TIAMO modes as averages
and an acquisition time of 2:51 min.
A 3D multi-GRE T2*W sequence was also performed with the same excitation pulse,
except now centered on the water frequency (Figure 1B) while not exciting lipid
resonances. The TR was 14 ms and the TEs were 2.1, 4.19, 6.21, 8.3 and 10.32
ms. The additional imaging parameters were the same as in the lipid selective
sequence, resulting in an acquisition time of 8:23 min. The calculated echo
time images were based on a linear least squares fit to the logarithmically
transformed signal data. The imaging protocol was tested in 6 healthy male volunteers
(age 25-41).
Results
Homogeneous
images with high SNR were obtained in all volunteers, both in lipid-selective
and T2*W water selective sequences; Figure 2 shows coronal images of 3 different volunteers. In
a different volunteer the transversal,
sagittal and coronal imaging of a mesorectal LN of 2 mm diameter is shown
(Figure 3). The LN is clearly distinguishable with dark signal intensity in the lipid images and
bright signal intensity in the T2*W images. Figure 4 shows a comparison of T2*W
images acquired with TIAMO and with phase-only B1 shimming optimized for
homogeneity. The image with only B1 shimming shows a dark area near the left
iliac vein, conceiling the LN that is visible in the TIAMO image (red circle). In
Figure 5 the measured image at a TE of 8.3 ms is compared to the
computed TE image at a TE of 8.0 ms. Additionally, a computed TE=0
ms image is shown. The contrast in the computed echo time image at 8.0 ms is similar
to that in the acquired image and is clearly different than the contrast in the
more proton density weighted TE=0 ms image. Next to that, the SNR in the
computed echo time image is increased compared to the acquired image.
Discussion and conclusion
With the
proposed measurement setup and protocol we were able to obtain high resolution
homogeneous GRE images of the pelvis at 7 Tesla with reliable visualization of
pelvic LNs over a large FOV. Because of the spectrally selective excitation no substantial chemical shift artifact was present in the images. Moreover, the multi-echo
T2*W imaging approach enables flexible echo time imaging through calculated
echo time images, while maximizing SNR efficiency.
Acknowledgements
Dutch Cancer Society [2014-6624], ERC Grant
agreement [243115]References
[1] Wu et al. Eur J Radiol. 2011;80(2):582-9. [2] Heesakkers et al. Lancet Oncol
2008; 9: 850–56. [3] Riederer et al. Radiol. 1984:153;203-206 [4] Orzada et al.
ISMRM (2009);p.2999. [5] Orzada et al. MRM(2010);64(2):327-33. [6] Orzada
et al. MRM (2012);67(4):1033-41.