Shih-Han Hung1, Meng-Chieh Liao1, Cheng-Ping Chien1, Wen-Chau Wu2, and Hsiao-Wen Chung3
1Graduate Institute of Biomedical Electronics and Bioinformatics, National Taiwan University, Taipei, Taiwan, 2Graduate Institute of Oncology, National Taiwan University, Taipei, Taiwan, 3Electrical Engineering, National Taiwan University, Taipei, Taiwan
Synopsis
A new scheme was proposed to analyze intravoxel
ihcoherent motion MR imaging data of the liver. The method integrated the
combined use of single- and bi-exponential signal decaying models to deal with
regions with absence of prominent vasculature, and the removal of data obtained
at b-values less than 15s/mm2 to avoid contamination from large
vessels. Results from ten healthy subjects scanned twice at 3T showed
substantially improved reproducibility in the pseudo-diffusion coefficient D*,
while those of the true diffusion coefficient and the profusion fraction were
unaltered. Using our scheme the estimated D* mostly fall within 38 to 85x10-3 mm2/s.Introduction
Intravoxel incoherent motion (IVIM) MR imaging
has been emerging as a potentially plausible technique that can quantitatively
assess both water molecular diffusion and capillary blood perfusion
noninvasively in human liver
1. To date, however, the numerical
values reported for the pseudo-diffusion coefficient that reflects liver
perfusion, D*, vary to a great extent from 27 to 190mm
2/s
2-4. It is hypothesized
that modeling of the signal decaying behavior plays a role in D*
quantification, in addition to effects of respiratory motion
5. In
this study, therefore, we aim to increase the reproducibility of D*
measurements via proper selection of the signal decaying model and the
b-values. Results on 10 healthy subjects scanned twice showed substantial
improvements in inter-scan reproducibility in D*.
Theory
Derivation of liver D* using IVIM imaging is
based on fitting of the signals as a function of b-values using the
bi-exponential decaying model: S
b = S
0 [ f*e
-bD* + (1-f)*e
-bD ], where S
b and S
0 are the signal intensities at a
specific b value and b=0, respectively, D the true diffusion coefficient, and f
the fraction of blood flow in the region of interest (ROI). At least two
problems could cause fitting uncertainty. First, in the absence of prominent
vasculature, single exponential model suffices, and over-fitting may result
when using bi-exponential model. Second, the presence of large vessels may
dominate the data at b-values less than 15s/mm
2, leading to D*
over-estimation
6. To solve these issues, we first restricted curve
fitting using data with b>15s/mm
2, followed by the combined use
of single- and bi-exponential models for fitting, for which the one exhibiting
smaller residual fitting error was chosen for the region of interest.
Materials and Methods
All experiments, IRB approved, were carried out
on a Siemens 3T scanner with a torso array for signal receiving. Image data at
sixteen b-values (0, 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 150, 200, 400,
600 and 800 s/mm
2) were obtained from ten healthy young subjects
using respiratory-triggered spin-echo EPI with diffusion sensitizing gradients. Each subject was scanned twice on the same day with
re-positioning to examine inter-scan reproducibility. Scanning parameters were:
FOV=310x310 or 410x410mm,
TE/TR=75/2000ms, thickness=7mm,
matrix size=112x112, NEX=6. For estimations of IVIM parameters, circular ROIs at
about 1cm diameter
were placed on the right hepatic lobe (Fig.1). Curve fitting to derive D* was
performed using the proposed scheme described above, with the consistency
between two measurements of the identical subjects analyzed using the
Bland-Altman plot, and compared with conventional fitting results using solely
the bi-exponential model. All data processing was carried out with
self-designed Matlab scripts.
Results
Figures 2 and 3 show the Bland-Altman plots for
D and D*, respectively. The proposed scheme yielded similar level of
reproducibility around 19% imprecision (Fig.2a)
to that using the conventional bi-exponential model for the true diffusion
coefficient D (Fig.2b) and for the perfusion fraction f (not shown). On the
other hand, D* reproducibility was improved substantially from 104% imprecision
using conventional bi-exponential model (Fig.3a) to 39% imprecision using the proposed scheme
(Fig.3b). With our method, D* for the ten subjects mostly fall within the range of 38 to 85x10
-3 mm
2/s.
Discussions and Conclusion
Prominent inconsistency in the numerical values for
liver D* has been found in past reports employing IVIM imaging
2-4, 6.
Results from our study suggest that such phenomena may have originated, at
least in part, from inappropriate use of the signal model for curve fitting.
Our proposed scheme yielded substantially improved inter-scan D*
reproducibility on repeated scans, while precisions in D and f were unaltered.
The method may find potential in clinical evaluation of liver perfusion using
IVIM MR imaging.
Acknowledgements
No acknowledgement found.References
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