Shu-Fu Shih1,2, Sophia X. Cui3, Xiaodong Zhong3, Bilal Tasdelen4, Ecrin Yagiz4, Krishna S. Nayak4, and Holden H. Wu1,2
1Department of Radiological Sciences, University of California Los Angeles, Los Angeles, CA, United States, 2Department of Bioengineering, University of California Los Angeles, Los Angeles, CA, United States, 3Siemens Medical Solutions USA, Inc., Los Angeles, CA, United States, 4Ming Hsieh Department of Electrical and Computer Engineering, University of Southern California, Los Angeles, CA, United States
Synopsis
MRI proton-density fat fraction (PDFF) is used for
non-invasive diagnosis of fatty liver disease, and has been validated at 1.5T
and 3T field strengths. There is renewed interest in lower field strengths,
such as 0.55T, because of potential advantages such as lower hardware/siting costs
and a larger bore diameter. This study investigated PDFF quantification at
0.55T and validated PDFF quantification at 0.55T using Cartesian and Radial
Dixon techniques in a reference phantom, and demonstrated the feasibility of in
vivo free-breathing radial liver PDFF quantification in healthy subjects at
0.55T.
Introduction
MRI proton-density fat fraction (PDFF) is a biomarker for non-invasive
diagnosis of fatty liver disease. PDFF quantification using chemical-shift-encoded
“Dixon” MRI has been validated at 1.5T and 3T1-3.
In addition to conventional PDFF quantification using breath-holding (BH) Cartesian
acquisition3,
recent work2
has demonstrated that radial techniques for PDFF enable free-breathing (FB) scans
with larger volumetric coverage.
There is renewed interest in lower field
strength MRI (e.g., 0.55T)4-9 because
of its potential advantages such as lower hardware/siting costs and a larger
bore diameter. These could improve access to MRI for populations with obesity
and at risk for fatty liver disease. Previous works have investigated
qualitative abdominal imaging7 and iron quantification8 at 0.55T. Three-point Dixon water/fat separation at
0.75T was explored using a spiral sequence with BH acquisition9, but free-breathing PDFF quantification has not been
investigated. There are several challenges in adapting Dixon-based PDFF
quantification techniques from current clinical field strengths to lower ones.
First, the already low image signal-to-noise ratio (SNR) at lower field becomes exacerbated
when a small flip angle (FA) is used to reduce T1 bias in PDFF10. Second, the smaller fat/water frequency difference results
in longer out-of-phase (TEop=6.47ms) and in-phase (TEin=12.94ms)
echo times. This increases scan time and limits parameter choices.
In this work, we investigated Cartesian and Radial Dixon techniques
for PDFF quantification at 0.55T, demonstrating accurate PDFF quantification in
a reference phantom and feasibility of FB radial liver PDFF quantification in
healthy subjects.Methods
Scanner and Sequences: Experiments were performed
using a whole-body 0.55T MRI system (prototype MAGNETOM Aera, Siemens
Healthineers, Erlangen, Germany) equipped with high-performance shielded
gradients (45 mT/m amplitude, 200 T/m/s slew rate). We used (1) a conventional
multi-echo gradient-echo 3D Cartesian sequence (“Cartesian Dixon”)3,
and (2) a prototype multi-echo gradient-echo 3D stack-of-radial technique with golden-angle
ordering (“Radial Dixon”)2.
Phantom Study:
We scanned a PDFF phantom (Calimetrix, Madison, WI) with 7 compartments of
known PDFF (0%, 5%, 10%, 20%, 30%, 40%, and 100%). Sequence parameters are in Table 1a.
In Vivo Study: 2 healthy subjects were scanned under
an IRB-approved protocol, after providing written informed consent. Sequence
parameters are in Table 1b. We chose TE1=2.17ms and echo
spacing=2.15ms, which achieved TEop=6.47ms and TEin=12.92ms
in the 3rd and 6th echoes. FA=5° and FA=10° were tested in both sequences. To reduce BH
time in Cartesian Dixon, parallel imaging (acceleration factor R=4) was
used.
Fitting Algorithms: The multi-echo images were fitted
to a multi-peak fat model with single effective R2* using a
multi-step adaptive fitting method3 and a time-domain signal-dephasing fat model11.
For phantom experiments, a vendor-provided fat model was used12.
This fitting method uses images from in-phase and out-of-phase for initial estimates
of fat/water. We chose 2 echo times near TEop=6.47ms and TEin=12.49ms
for this initial step.
Analysis: In
phantoms, we compared PDFF measurements from Cartesian and Radial Dixon with
reference values in regions of interest (ROI). We used Pearson’s correlation
coefficients for linear relationship evaluation and used Lin’s concordance coefficient
to evaluate agreement with the reference. For in vivo scans, 5-cm2
ROIs were drawn in the liver while avoiding large vessels and mean PDFF values
were reported.Results
Figure 1 demonstrates close agreement between PDFF
measurements from Cartesian and Radial Dixon versus reference with concordance
coefficients ρc>0.997. Figures 2 and 3
show results from 2 healthy subjects. Low SNR in BH Cartesian Dixon led to
errors in PDFF. FB Radial Dixon achieved larger volumetric coverage and
sufficient SNR for PDFF quantification. Figure 4 shows that using FA=10° increased image SNR versus FA=5°. However, BH Cartesian with
FA=10° still suffered from low SNR and parallel
imaging artifacts that led to errors in PDFF. FB Radial Dixon using FA=10° had slightly increased PDFF compared with FA=5°, potentially due to
uncorrected T1 bias.Discussion
Compared with previous studies on abdominal MRI at 0.55T7,8,
we demonstrated quantitative fat MRI at 0.55T. The challenge of low SNR at
lower field can potentially be mitigated by using non-Cartesian techniques9,13
that are more SNR-efficient and/or enable FB acquisition of more data without
BH limitations. FB Radial Dixon at 0.55T can especially benefit patients with a
larger body habitus in terms of the larger volumetric coverage and potentially
larger bore size.
There are some limitations in this work. First, we did not compare
all parameter combinations. We chose TEs that at least included the first in-phase
and out-of-phase echo times. Using shorter TEs with more robust fitting
algorithms may shorten the acquisition time. Second, we observed increased PDFF
as FA increased, but the FA choice that balances the trade-off between SNR and T1
bias needs further investigation. Third, the in vivo sample size is small, and
did not include the spectrum of clinical PDFF and underlying obesity status. PDFF
accuracy in subjects with fatty liver disease will be studied in the future.Conclusion
We validated PDFF quantification at 0.55T using Cartesian
and Radial Dixon techniques. We demonstrated the feasibility of in vivo free-breathing
radial liver PDFF quantification at 0.55T.Acknowledgements
We acknowledge grant support from the National Science
Foundation (#1828736) and the National Institutes of Health (R01DK124417), and
research support from Siemens Medical Solutions USA, Inc.References
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