Jo-Hua Peng1, Chun-Jung Juan1,2,3, Yi-Jui Liu4, Ruey-Hwang Chou5, Hing-Chiu Chang6, Chang-Hsien Liou2,7, Szu-Hsien Chou1,2, Yen-Ting Wu1,2, Bai-Wen Wu2, and Hsu-Hsia Peng1
1Department of Biomedical Engineering and Environmental Sciences, National Tsing Hua University, Hsinchu, Taiwan, 2Department of Medical Imaging, China Medical University Hsinchu Hospital, Hsinchu, Taiwan, 3Department of Radiology, School of Medicine, China Medical University, Taichung, Taiwan, 4Department of Automatic Control Engineering, Feng Chia University, Taichung, Taiwan, 5Institute of Cancer Biology, China Medical University, Taichung, Taiwan, 6Department of Biomedical Engineering, Chinese University of Hong Kong, Sha Tin, Hong Kong, 7Institute of Nuclear Engineering and Science, National Tsing Hua University, Hsinchu, Taiwan
Synopsis
ADC estimations are still known to be influenced
by the content of fat. Fat suppression is normally applied in order to avoid
the ADC measurement with fat contamination. The aim of this study was to evaluate
the fat effect on ADC measurement by EP-DWI and PROP-DWI combined with
different fat suppression techniques using a fat-water phantom with different
fat fractions. Our results suggest that the ADC measurement is affected by the
fat fraction and the MR sequences but not the fat suppression methods in EP-DWI.
Introduction
Diffusion-weighted
imaging (DWI) is a MR imaging that can measure proton diffusion information by
calculating apparent diffusion coefficient (ADC) in tissue. Although single-shot
echo-planar diffusion-weighted imaging (EP-DWI) is most commonly used for
diffusion measurement currently, it is susceptible to artifacts such as N/2
ghost artifacts, chemical shift artifacts, and geometric distortion. Fast spin
echo DWI with periodically rotated overlapping parallel lines with enhanced
reconstruction (PROP-DWI) was introduced to eliminate signal pile-up and
geometric warping associated with the EP-DWI1. ADC has been regarded as a tumor
biomarker which is sensitive to biophysiological conditions such as cell
organization, cell density, microstructure, and microcirculation2. However,
ADC estimations based on fast spin-echo imaging are still known to be
influenced by the content of fat in the breast3 and parotid tumor4. Therefore,
fat suppression is necessary in order to avoid the contamination of fat on the
ADC measurement. Three fat suppression methods, water excitation (WE), chemical
shift selective (CHESS), and short tau inversion recovery (STIR), are usually
used to eliminate the fat effect for ADC measurement. Quality assessment and
quality control of MR imaging using a quantitative phantom is important to
ensure the accuracy and precision of measurement5. The aim of this study was
to design a fat fractions (FF) phantom containing
different fat fractions to quantify the ADC measured
by EP-DWI and PROP-DWI combined with different fat suppression techniques.Materials and Methods
Phantom design: Six phantoms with fat fractions of 10%, 20%, 30%, 40%, 50%, and 100%
were made respectively using mixed proper weights of soybean oil and water with
the emulsifying agent (Trion X-100)6 and coagulant (agarose)7.
MRI scans: All images were
performed by a 1.5 Tesla MR scanner (GE Signa MR450w, GE Healthcare). IDEAL IQ sequence
was applied to verify the fat fraction of phantom8. The IDEAL IQ method was a three-dimensional fast spoiled gradient-echo
(3D-FSPGR) sequence employing a six-echo acquisition (1.1ms-6.38ms) with the
imaging parameters including TR, 19.6ms; FOV, 210×210mm; matrix size, 128×128; pixel
bandwidth, 90.91 kHz; flip angle, 5; and slice thickness, 10mm. EP-DWIs with fat
suppression by WE, CHESS, and STIR were performed, respectively, in axial plane
with the scanning parameters including TR, 4000 ms; TE, 78 ms; TI, 105 ms (STIR);
b, 0 and 1000 $$$s/mm^{2}$$$ in three orthogonal bipolar diffusion gradients; NEX,
4; matrix size, 128 × 128; FOV, 210 × 210 mm; and section thickness, 10 mm. PROP-DWIs
with three fat suppression, no fat saturation (no sat), fat saturation (fat
sat), and classic fat saturation (fat cla. sat), were separately performed in
the axial plane with the protocol parameters in the following, TR = 4000 ms, TE
=85 ms, b = 0 and 1000 $$$s/mm^{2}$$$ in three orthogonal bipolar diffusion gradients, NEX=4,
matrix size 128 x 128, FOV 210 x 210 mm, section thickness = 10 mm. Data processing: Proton density fat fraction (PDFF) maps were automatically
produced by the MRI scanner. ADC maps were generated via pixel-by-pixel
computation from $$$b_{0}$$$ and $$$b_{1000}$$$ images based on a
mono-exponential model using a formula of $$$SI_{b1000}=SI_{b0}\times
e^{-bD}$$$. A slice containing the
largest cross-sectional area of the phantom was chosen for ROI selection to
circle whole tube in every DWI and IDEAL IQ scans. Then the values of mean and standard
deviations were calculated for the analysis. Linear regression analysis was
used to evaluate the relationship among the fat and ADC measures.Result
Five
cylinders containing solidified agarose-based emulsions with fat fraction of 10%, 20%, 30%, 40%, and 50% from left
to right, respectively, were demonstrated (Fig.1a). Microscopic images of 10% (Fig.
1b) and 50% (Fig. 1c) FF tubes show the distribution and arrangement of fat droplets
and water in the emulsion. Scatter plot shows high linearity (slope 1.05) and
small bias (–0.17 %) of fat fractions on PDFF maps vs. phantoms (Fig. 2). ADCs at different phantom
FFs with respect to different pulse sequences and fat suppression methods were
shown on Fig. 3. Linear regression analysis reveals the linear relationship of
ADCs between fat suppression (EP-DWI and PROP-DWI) and non-fat suppression (PROP-DWI)
in Fig. 4. Fig. 5 illustrates b=0 and b=1000 $$$s/mm^{2}$$$ images of the 100% FF phantom scanned by EP-DWI and PROP-DWI using the
different methods of fat suppression.Discussion and Conclusion
The
ADC offset from fat suppression to non-fat suppression was obviously observed
in Fig. 3. Due to the characteristics of tiny diffusion in oil9, the ADC is
lower in non-fat suppression compared with fat suppression and is negatively
proportional to the fat fraction of phantom. The
ADC measured in fat-saturated PROP-DWI was higher than in non-fat-saturated PROP-DWI,
similar to previous study10. Although the fat signal was better suppressed by
STIR than by WE and CHESS in EP-DWI, the ADCs were not related to the three fat
suppression methods in EP-DWI. The effect of fat suppression was similar between
fat sat and fat cla. sat in PROP-DWI, but the ADC was divergent at high fat
fraction. Our results suggest that the ADC measurement is affected by the fat fraction
and the MR sequences but not the fat suppression methods in EP-DWI in the
phantom study.Acknowledgements
No acknowledgement found.References
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