Hyungseok Jang1, Michael Carl2, Yajun Ma1, Yanjun Chen1, Saeed Jerban1, Eric Y Chang1,3, and Jiang Du1
1Department of Radiology, University of California San Diego, San Diego, CA, United States, 2GE Healthcare, San Diego, CA, United States, 3Radiology Service, VA San Diego Healthcare System, San Diego, CA, United States
Synopsis
Due to very low proton density and rapid signal
decay (T2*<300µs at 3T), it is challenging to directly image myelin in the white
matter of the brain using MRI. The literature demonstrates that direct myelin
imaging is feasible using inversion recovery (IR) preparation followed by dual
echo ultrashort echo time (UTE) MRI, allowing direct capture of the
rapidly-decaying myelin signal with greatly improved dynamic range. In this study, we show the efficacy of IR
prepared Pointwise Encoding Time Reduction with Radial Acquisition (IR-PETRA)
for direct myelin imaging in the human brain.
Introduction
Due to very low proton density and rapid signal
decay (T2*<300µs at 3T), it is challenging to directly image myelin in white
matter of the brain with MRI. Recent studies have shown that direct myelin
imaging is feasible using inversion recovery (IR) preparation followed by dual
echo ultrashort echo time (UTE) MRI, allowing direct capture of the
rapidly-decaying myelin signal with greatly improved dynamic range1–4. In this study, we explore the efficacy of IR
prepared Pointwise Encoding Time Reduction with Radial Acquisition (IR-PETRA) for
direct myelin imaging in the human brain.Methods
To directly image myelin in MRI, the following
strategies are applied: First, an adiabatic IR pulse preparation is applied to
provide robust suppression of signals from the long T2 components in white
matter, which are mainly water. Second, dual echo imaging is performed to
suppress the remaining long T2 gray matter signal by subtracting the second
echo from the first one. Since the primary short T2 tissue in white matter is
myelin, the remaining signal reflects myelin content. Figure 1-a shows typical
inversion recovery curves for tissues in the human brain (i.e., myelin, white
matter, and gray matter). After the adiabatic inversion preparation, UTE imaging
is performed, as shown in Figure 1-b. Note that multiple spokes are acquired
after each IR preparation to reduce the scan time, centered on the optimal inversion
time (TI) adjusted to invert and null the longitudinal magnetizations of long
T2 white matter. For the imaging, dual echo PETRA5 is performed as illustrated
in Figure 1-c, where single point imaging (SPI) encoding6 is utilized to acquire the
missing central k-space data due to RF coil deadtime during UTE imaging as
shown in Figure 1-d. Note that the second echo (TE2) is also acquired using SPI—despite
the fact that there is no RF deadtime and therefore no missing k-space data—in
order to keep the sampling pattern consistent between the UTE and TE2,
therefore achieving a more reliable subtraction image. To evaluate the
feasibility and efficacy of IR-PETRA for direct myelin imaging, we performed a
phantom experiment with a GE resolution phantom, performed ex vivo imaging with a cadaveric brain (56-year old female donor),
and performed in vivo imaging with three
healthy volunteers (36-, 30-, and, 36-year
old males). The experiments were performed on a 3T GE-MR750 scanner using a
12-ch receive-only HNU coil. The imaging parameters for the phantom experiment are
as follows: a hard pulse with flip angle (FA)=4° (pulse width=20µs), readout
BW=±31.25kHz, matrix size=200x200x40, FOV=220x220x160mm3, inter-spoke
TR=8ms, TE=28µs/2.4ms, # of SPI encoding=544, # of radial frequency encoding=16944,
and scan time=2min 10sec. The ex vivo
experiment was performed with the parameters matched above, except for the
following parameters: adiabatic inversion pulse applied (Silber Hoult pulse,
pulse width=8.64ms), TR=1000ms, TI=310ms, TE=28µs/3.5ms, # of radial frequency
encoding=33856, # of spokes per IR preparation=16, inter-spoke TR=10ms, and
scan time=35min 54sec. In vivo
experiment was performed using the same parameters as in the ex vivo experiment except for TI=325ms, TE=28µs/2.4ms,
# of radial frequency encoding=16944, # of spokes per IR=30, inter-spoke
TR=8ms, and scan time=11min 18sec. All images were reconstructed using online reconstruction
based on GE Orchestra-SDK (v1.7.1).Results
Figure 2 shows the dual echo PETRA images obtained
with a GE resolution phantom. As demonstrated, there are no imaging artifacts manifested
in either the UTE or TE2 images with the given imaging parameters, which
assures the quality of the dual echo PETRA images without IR. Figure 3 shows selected
slices from IR-PETRA imaging of the ex vivo
cadaveric brain. As seen in the UTE image, myelin signal is selectively detected
with long T2 white matter signal suppressed near-completely, verified by the
fact that no signal remains in the white matter region in the second echo
(myelin signal already decayed to near-zero). By subtracting the second echo
from UTE, a highly specific myelin image is obtained, as shown in Figure 3. Figure
4 shows images from the in vivo
experiment, which shows the myelin image with high contrast.Discussion and Conclusion
In this study, we demonstrated the feasibility and
efficacy of IR prepared dual echo PETRA for direct myelin imaging. We showed high
contrast myelin contrast with the ex vivo
and in vivo protocols, which suggests
potential for IR-PETRA to image myelin for in
vivo applications such as multiple sclerosis (MS) and traumatic brain
injury (TBI). In future work, we will compare IR-PETRA with other possible approaches
such as radial UTE, cones UTE, zero echo time (ZTE) imaging, and ramped hybrid encoding (RHE)7 in myelin imaging in MS and
TBI.Acknowledgements
The authors acknowledge research support from GE Healthcare, NIH (R01NS092650), and VA Clinical Science and Rehabilitation R&D Awards (I01CX001388 and I01RX002604).References
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