Alireza Akbari1,2, Lanette J Friesen-Waldner1, Timothy RH Regnault3,4, and Charles A McKenzie1,2
1Medical Biophysics, Western University, London, ON, Canada, 2Robarts Research Institute, Western University, London, ON, Canada, 3Obstetrics and Gynaecology, Western University, London, ON, Canada, 4Physiology and Pharmacology, Western University, London, ON, Canada
Synopsis
In this work we demonstrate
high-resolution bipolar water-fat imaging sequence produces same fat
quantification as compared to conventional unipolar water-fat imaging sequence
under the same scan time. Images of resolved boundaries in bipolar Proton
Density Fat Fraction (PDFF) maps are presented. Fat quantifications of the same
regions of interest drawn on bipolar and unipolar PDFF were compared and
statistical analysis was performed to evaluate the similarity of the two
methods.
INTRODUCTON
Guinea
pigs are suitable animal model for studying obesity as they accumulate adipose
deposits in a similar manner as humans.1
However, quantifying adipose tissue in guinea pigs is challenging, as the fat
tissue volume is much smaller than humans due to their small body size. Hence,
to quantify fat tissue, high-resolution images are required to reduce partial
volume effects and minimize segmentation errors.2
Conventional water-fat imaging based on quantitative IDEAL3 uses several unipolar gradient echoes that are acquired
over multiple repetition times (TRs) to achieve optimal echo-spacing. However,
a bipolar water-fat imaging sequence would require fewer numbers of TRs to
acquire the requisite gradient echoes with optimal echo-spacing, leading to a
more time-efficient sequence.4 In
this work, we investigate how a high-resolution bipolar sequence would perform
in quantifying fat in vivo compared to a conventional unipolar sequence
with the same scan time.METHODS
Four guinea pigs were scanned using a 3T MR scanner (Discovery
MR 750, GE Healthcare, Waukesha, WI) and 32-channel cardiac coil. The unipolar
imaging parameters were as follows: echo train length (ETL)=3, TR/TE1/ΔTE =
~11.0/1.6/1.3 ms, slice thickness=0.9 mm and acquisition matrix = 276 x 182 x
88 corresponding to voxel dimensions = 0.94 x 0.86 x 0.9 mm3(= 0.728
mm3). The bipolar imaging parameters were set to: ETL=6, TR/TE1/ΔTE
= ~12.2/1.8/1.6 ms, slice thickness=0.7 and acquisition matrix = 276 x 278 x
112 resulting in voxel dimensions = 0.94 x 0.56 x 0.7 mm3(= 0.368 mm3).
The rest of the imaging parameters: FOV=26 cm x 15.6 cm, flip angle=3 °,
BW=142.86 KHz, NEX=3 were kept the same for both sequences. The scan time for
unipolar and bipolar sequences were kept as close to identical as possible (10:57
and 11:18, respectively) to facilitate comparison. Conjugate-gradient SENSE5 and Max-IDEAL6
were used in the water-fat image reconstruction. The reconstructed matrix size
for unipolar and bipolar images were 512x512x88 and 512x512x112, respectively. Proton
Density Fat Fraction (PDFF) maps were calculated for both the unipolar- and
bipolar-acquired images and were used for all the image analyses as they
provide a quantitative measurement of fat.
To assess the partial volume improvement in bipolar PDFF
maps a region of interest (ROI) was drawn on the boundary between visceral and
subcutaneous fat where the boundary was clearly identifiable on the bipolar
PDFF images. The ROI was subsequently applied to the same volume on the unipolar
PDFF maps. The mean PDFF were computed and an unpaired two-tailed t-test was
performed to determine whether the bipolar sequence would perform differently in
resolving the boundaries as compared to unipolar sequence. Fat quantification
was performed by drawing ROIs on sections of visceral (either thoracic or
abdominal) fat in the unipolar PDFF maps and their corresponding volumes on
bipolar PDFF maps. All ROI analyses were performed using 3D-Slicer
(www.slicer.org). To assess the level of agreement (i.e., identical fat
quantification results) between unipolar and bipolar measurements of PDFF, a
one-sample t-test was performed on the PDFF measurements difference values. These
difference scores were tested against a value of 0, which would indicate that
the measurements were identical.RESULTS
Figure
1 shows that the bipolar sequence achieved higher resolution compared to
unipolar in approximately the same scan time. Figure 2 reports higher fat fraction measured
in the boundary between visceral and subcutaneous fat in unipolar PDFF maps as
compared to the same regions in bipolar PDFF maps (p<0.001). The measured fat fractions were the same per
region between unipolar and bipolar images, and are reported in Table 1. The
t-test for difference (unipolar minus bipolar) against 0 for fat volume was not
significant (p=0.314), indicating the results were statistically similar.DISCUSSION
Our
results indicate that the bipolar sequence performs like unipolar in terms of
quantifying fat in vivo as indicated in table 1 while doubling the image
resolution. Higher resolution helps delineate fat tissue where the boundary
between the fat and other tissues may be unclear due to partial volume effects,
as is demonstrated in Figure 1. The results from figure 2 indicate the boundaries
between subcutaneous and visceral fat in unipolar PDFF maps suffer from partial
volume effects as their mean fat fraction are higher compared to the same
regions in bipolar PDFF maps. Therefore, the high-resolution bipolar sequence
would be ideal for both manual and automated segmentation to produce more
accurate quantitative results.CONCLUSION
We
have demonstrated that high-resolution bipolar water-fat imaging reduces
partial volume effects without compromising the ability in quantifying fat as compared
to conventional unipolar water-fat imaging under the same imaging time.Acknowledgements
No acknowledgement found.References
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