Naoki Ohno1, Tosiaki Miyati1, Genki Nambu1, Daichi Tanaka1, Yuki Makino1, Noam Alperin2, Yu Ueda3, Marc Van Cauteren3, Toshifumi Gabata1, and Satoshi Kobayashi1
1Kanazawa University, Kanazawa, Japan, 2University of Miami, Miami, FL, United States, 3Philips Japan, Tokyo, Japan
Synopsis
Keywords: Diffusion/other diffusion imaging techniques, Diffusion/other diffusion imaging techniques
Diffusion
imaging with phase-contrast (DIP) can quantitatively evaluate regional cerebral
blood flow (rCBF), in which total CBF (tCBF) from phase-contrast magnetic
resonance imaging (PC-MRI) converts the brain’s perfusion-related diffusion
parameters into rCBF values. However, it is sensitive to bulk motion (i.e.,
brain pulsation), potentially causing an overestimation of DIP-derived rCBF
values. To overcome this issue, we propose a motion-compensated DIP (MC-DIP) that
incorporates motion-compensated diffusion gradients. DIP with second-order
motion-compensated diffusion gradients (2nd-MC-DIP) improved the fitting
accuracy of the biexponential analysis and showed the ability to quantitatively
evaluate rCBF in gray and white matter.
INTRODUCTION
The perfusion-related diffusion parameter in intravoxel incoherent motion
analysis is closely associated with regional cerebral blood flow (rCBF).1,2
However, it is only a semiquantitative relative value of rCBF, making absolute
rCBF quantification challenging. To overcome this issue, diffusion imaging with
phase-contrast (DIP) was developed, in which total CBF (tCBF) from
phase-contrast magnetic resonance imaging (PC-MRI) converts the brain’s
perfusion-related diffusion parameters into rCBF values.3 However,
it is sensitive to bulk motion (i.e., brain pulsation), which potentially causes
artificial intravoxel phase dispersion and signal loss.4 This may
cause overestimation of perfusion-related diffusion parameters and DIP-derived
rCBF values. Therefore, we propose a motion-compensated DIP (MC-DIP)
incorporating motion-compensated diffusion gradients to reduce the bulk motion
effects on rCBF quantification.MATERIALS AND METHODS
Nine males and two
females (mean age, 23.9 years) were scanned on 3.0T MRI. Single-shot diffusion
echo-planar imaging of the brain was performed with motion-uncompensated gradients
(non-MC) and first- and second-order motion-compensated diffusion gradients (1st-MC
and 2nd-MC, respectively; Figure 1). Transverse diffusion-weighted images of
the whole brain were obtained with multiple b values (0, 10, 20, 30, 50, 100,
200, 400, 600, 800, and 1000 s/mm2). Voxel-wise estimations of the
perfusion-related diffusion coefficient (D*), perfusion fraction (F),
multiplication of D*and F (FD*), and restricted diffusion coefficient were
conducted using bi-exponential function. Parameter estimation was performed by using
a stepwise approach to improve the robustness of the analysis.2 The
fitting procedure was performed using MATLAB with the Levenberg-Marquardt nonlinear least-squares algorithm. The normalized
root-mean-square error (nRMSE) was calculated to evaluate the goodness-of-fit of the biexponential
model for the measured data from each diffusion gradient scheme. A smaller nRMSE indicates a better fitting
quality.
PC-MRI with retrospective peripheral gating was
performed to obtain the tCBF. The transverse imaging plane was set at the
mid-C2 level perpendicular to the internal carotid arteries (ICAs) and
vertebral arteries (VAs). We obtained velocity-mapped phase images, delineated
the lumen boundaries of the ICAs and VAs on the phase images, and determined the
volumetric flow rates within the lumen. Then, the tCBF was calculated as the
sum of the volumetric flow rates of the four lumens (i.e., ICAs and VAs on both
sides). Using tCBF, FD* values in the brain were converted into absolute rCBF
in units of mL/100 g/min (Figure 2).
Reference
rCBF values were obtained using three-dimensional gradient and spin-echo pulsed
continuous arterial spin labeling (ASL). rCBF values obtained using ASL and DIP
with 2nd-MC, 1st-MC, and non-MC were measured in gray and white matter (GM and
WM, respectively). We evaluated the correlations between the DIP with each MC
scheme and ASL using Spearman’s correlation coefficient, and compared the nRMSE
between the MC methods using Friedman’s test. Statistical significance was set
at P < 0.05.RESULTS AND DISCUSSION
Figure 3 shows the representative rCBF images from the same subject
obtained using each method. The rCBF images obtained with the 2nd-MC-DIP showed
better GM-WM contrast and fewer artifacts than the 1st-MC- and non-MC-DIP
images. The 2nd-MC-DIP had a significantly lower nRMSE in the WM than the 1st-MC-
and non-MC-DIP (Figure 4). The nRMSE for the 2nd-MC-DIP was also significantly
lower in the GM than that for the non-MC-DIP. These results indicate that 2nd-MC
diffusion gradients can improve the fitting accuracy of the biexponential
function by reducing the bulk motion effect more efficiently.5
Figure 5 shows scatter
plots of rCBF in GM and WM obtained using each DIP method and ASL. We observed
significant positive correlations of rCBF in the GM between DIP with each MC
method and ASL. Moreover, we found a significant positive correlation of rCBF
in the WM between the 2nd-MC-DIP and ASL, indicating the ability of 2nd-MC-DIP
to quantify rCBF values in the GM and WM. In contrast, there was no significant
correlation between 1st-MC- or non-MC-DIP and ASL. This lack of correlation
might be attributed to the lower fitting accuracy in the 1st-MC- and
non-MC-DIP, as shown by the results of nRMSE in the WM.CONCLUSION
The 2nd-MC-DIP reduced the bulk motion effect on
the biexponential diffusion analysis and enabled the robust quantification of
rCBF.Acknowledgements
This study was supported by JSPS KAKENHI (grant number 18KK0450 and
22K07794).References
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