Chang Gao1,2,3, Peng Hu1,2, Brian Dale4, Marcel D. Nickel5, Stephan A.R. Kannengiesser5, Berthold Kiefer5, Vibhas Deshpande6, and Xiaodong Zhong3
1Department of Radiological Sciences, David Geffen School of Medicine, University of California, Los Angeles, CA, United States, 2Physics and Biology in Medicine Inter-departmental Graduate Program, David Geffen School of Medicine, University of California, Los Angeles, CA, United States, 3MR R&D Collaborations, Siemens Healthcare, Los Angeles, CA, United States, 4MR Training, Siemens Healthcare, Cary, NC, United States, 5MR Application Development, Siemens Healthcare GmbH, Erlangen, Germany, 6MR R&D Collaborations, Siemens Healthcare, Austin, TX, United States
Synopsis
Accurate quantification of proton-density fat fraction
(PDFF) and R2* requires appropriate compensation of various confounding
factors. A stability study was performed to investigate the impacts of
different protocols and imaging parameters using both breath-hold Cartesian and
free breathing radial sequences on a standardized phantom and a group of 5 same
normal subjects at both 1.5T and 3T. This study revealed that flip angle, TE
mode and coil usage were important protocol parameters to investigate further
in larger patient population.
INTRODUCTION
Accurate proton-density fat fraction (PDFF) and R2*
quantification typically requires simultaneous measurement of these two
biomarkers and appropriate compensation of various confounding factors.1-5
Liver PDFF and R2* quantification is commonly based on breath-hold multi-echo
gradient-echo acquisitions with the Cartesian sampling. Recently, the
stack-of-radial sampling was demonstrated to be more robust to motion6
and validated for free-breathing fat quantification7 and R2*
quantification.8,9 Moreover, standardized phantoms became
commercially available for fat and R2* quantification.10
In this work, we performed a preliminary study to evaluate
the stability of fat and R2* quantification using both breath-hold Cartesian
and free-breathing stack-of-radial sequences on a standardized phantom and a
group of the same normal subjects at both 1.5T and 3T.METHODS
Imaging Sequences and
Protocols
A free-breathing multi-echo stack-of-radial prototype
sequence with gradient delay correction and self-gating motion compensation was
utilized.8,9 A breath-hold Cartesian prototype sequence was performed as a reference standard.11
Imaging protocols and parameters are shown in Table 1. Raw data of all acquisitions were saved and
reconstructed offline using the prototype reconstruction program of these
sequences.8,9,11
Phantom Validation
A standardized PDFF/R2* phantom (Calimetrix, Madison,
Wisconsin, USA) was scanned on a 1.5T and a 3T scanner (MAGNETOM AvantoFit and Prisma, respectively, Siemens Healthcare,
Erlangen, Germany) at the scanner room temperature with the anterior 18‐channel
flexible array and the table‐mounted spine array. The phantom
consists of 7 cylindrical glass vials and the other 8 vials presenting varying
ranges of R2* and PDFF values, respectively.
PDFF and R2* were fitted using a fat spectrum modeling
adjusted according to the manufacturer suggestion.10 For regions
with very high iron concentrations (>500 s-1), R2* was calculated
using an automatic algorithm of mono-exponential fitting without considering
fat. PDFF or R2* values were measured as mean ± standard deviation (SD) within
the circular regions of interest (ROIs) placed inside the vials.
In-vivo Validation
In vivo study was approved by the Institutional Review Board
with written informed consent obtained from each subject. A group of the same 5
normal subjects were scanned using the same 1.5T and 3T scanners and coils as
in the phantom experiment.
The mean and SD of PDFF and R2* were measured by placing one
ROI on one mid-liver slice and avoiding large
hepatic vessels and severe imaging artifacts. Linear
mixed-effects modeling was performed using R 3.5.112 and the lme4
package13 for statistical analysis. Data were grouped by field
strength. Clustering effects were addressed by treating the volunteer as a
random effect. The fixed effects included all variables in Table 1 as main
effects, and an interaction between bandwidth and TE mode. The dependent
variables were PDFF mean, PDFF SD, R2* mean and R2* SD.RESULTS AND DISCUSSION
Figures 1 and 2 show PDFF and R2* results of the phantom,
respectively. Measured PDFF values of all different conditions were consistent
with the reference values. Measured R2* values were also consistent with the
reference, except some underestimated values of the vials with high
iron concentrations. The R2* values of MinTE protocols tended to match the
reference values more closely, mostly due to the SNR.
Statistical analysis of the in-vivo results is shown in
Table 2. Flip angle did not impact R2*, but introduced T1 biases into PDFF
results, consistent with previous findings.14 Pixel size and slice
thickness did not affect PDFF or R2* mean; however, larger voxels were
associated with lower SD, mostly attributed to SNR. Using
MinTE instead of OppInTE showed biases in PDFF mean and R2* SD. Bandwidth had
minimal impact on PDFF or R2* mean, but showed influences on PDFF and R2* SDs
at 1.5 T. Gradient mode exhibited no obvious impacts, nor did shimming, likely
because the quantification methods in this study had more magnitude-fitting
characteristics.8,9,11
Using only the body coil reduced PDFF mean at 3T with a low significance, but
increased R2* SD particularly at 3T. The acquisition and reconstruction modes
had little impact on PDFF, but had strong impacts on R2*. Specifically, Ungated
radial reconstruction introduced positive biases (relative to Cartesian) in R2*
mean at both field strengths, and Gated40 radial reconstruction corrected those
biases. All radial sequences and reconstructions tended to impact PDFF and R2*
SDs, likely due to noise or streaking artifacts. Generally, it is recommended
to use either a breath-hold Cartesian or a gated free-breathing radial
acquisition with the OppInTE mode.
One limitation of this study is the relatively small PDFF
and R2* ranges of the in-vivo subjects. Due to the scan time limit, the
protocol of this study cannot be directly applied on clinical patients.
However, this preliminary study revealed factors which pose significant influences
on PDFF and R2* quantification, such as the TE mode and the flip angle, to be
investigated in patient populations with wide PDFF and R2* ranges. The
reduction of the factors to investigate is critical for the extension of this
work in patients.CONCLUSION
This study investigated the stability of breath-hold and
free-breathing liver fat and R2* quantification on a standardized phantom and a
group of normal subjects at 1.5T and 3T. This study revealed that flip
angle, TE mode and coil usage were important protocol parameters to investigate
further in larger patient population.Acknowledgements
No acknowledgement found.References
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