Seong-Eun Kim1, J Scott Scott McNalley1, Adam de Havenon 2, Dennis L Parker1, and Gerald S Treiman 3
1UCAIR, Department of Radiology and Imaging Sciences, University of Utah, Salt Lake City, UT, United States, 2Department of Neurology, University of Utah, Salt Lake City, UT, United States, 3Department of Veterans Affairs, VASLCHCS, Salt Lake City, UT, United States
Synopsis
Large artery atherosclerotic disease
is one of the most common causes of ischemic stroke. Post-contrast plaque
enhancement (PPE), which may result from endothelial dysfunction or be secondary
to intraplaque inflammation, is a vulnerable plaque feature that correlates
with increased stroke risk independent of stenosis. Although PPE can be
detected with vessel wall MRI better quantitative methods to measure PPE are
needed. This work presents a new 3D high resolution T1 mapping technique
for accurate T1 quantification of contrast uptake within vulnerable large
artery plaque.
Purpose
Large artery atherosclerotic disease is one of
the most common causes of ischemic stroke in the world1,2. Post-contrast
plaque enhancement (PPE), which may result from endothelial dysfunction (breakdown
along the intima) or be secondary to intraplaque inflammation and adventitial
neovessel rupture, is a vulnerable plaque feature that correlates with
increased stroke risk independent of stenosis3-6. Although PPE can be
detected with vessel wall MRI (vwMRI) better quantitative methods to measure
PPE are needed. Currently, T1 weighted signal intensity increase has
been used to estimate uptake of paramagnetic contrasts such as Gadolinium(Gd)7. However, this relative signal intensity increase not only reflects
contrast uptake but depends also on tissue and sequence parameters. It is well
known that 1/T1 (R1) is directly related to the uptake of
contrast agent on the tissue over time8. This work presents a new 3D
high resolution T1 mapping technique for accurate T1 quantification
of contrast uptake within vulnerable large artery plaque. Methods
The 3D multi-shot(ms) Spin-Stimulated Echo(STE) EPI
sequence was implemented with a segmented 3D ms EPI sequence (see Fig 1). For
reduced field of view imaging, the slice selection gradients of the last two 90O
pulses (Gps) was applied in the phase encoding direction. For
perfect 90o RF pulses, the measured T1 is: $$$\frac{1}{T_{1}(\overrightarrow{r})}=\frac{lnS_{SE}(\overrightarrow{r})-lnS_{STE} (\overrightarrow{r}) }{TM}$$$ where SSE, SSTE are signal intensity of SE
and STE, respectively. For non perfect 90o RF pulses (B1
inhomogeneity), the STE signal becomes: $$$S_{STE}(\overrightarrow{r})=S_{SE}(\overrightarrow{r})*g(\overrightarrow{r})*e^{-\frac{TM}{T_{1}}}$$$ where $$$g(\overrightarrow{r})$$$ is B1 mapping. For
small TM / T1, $$$g(\overrightarrow{r})\cong \frac{S_{STE}}{S_{SE}}$$$. To validate the T1 measurement, 3D ms-STE EPI was performed on
a cylindrical phantom filled with a solution of MnCl2 (T1 ~1200ms) with imaging parameters: TE/TM/TR= 20.2/ 250/ 500ms, in plane resolution
=0.5x0.5 mm2, slice thickness =1.0mm, 48 slices/slab, etl=17. Scan
time was 3:20 min. With IRB approved informed consent, the 3D ms-STE EPI
acquisition was performed on two human subjects with known large artery
atherosclerosis before and after Gd administration with same imaging parameters
used on the phantom. We also performed the 3D DANTE T1w SPACE imaging. All
scans were performed on a 3T MRI system with composite head and neck coils.
R1 (1/ T1) and T1 maps were calculated and
displayed using software written in Python. Results
The phantom study results are shown in the Fig 2. R1
(a) and T1 (b) maps with B1 correction were more
uniform across the phantom compared to R1(c) and T1 (d) maps
without correction. The almost complete elimination of B1
inhomogeneity using the proposed B1 correction is also demonstrated
by the plots in Fig 2d. Fig 3 shows 3D DANTE T1w SPACE images (a) and R1
maps (b) in a left internal carotid artery atherosclerotic plaque before and
after contrast. The R1 value of the plaque was elevated from 1.75±0.84/s
(white arrow, pre contrast) to 3.02±0.98/s (red arrow, post contrast), indicating active contrast uptake within the
plaque. Fig 4 shows the 3D DANTE T1w SPACE (a), R1 (b) and T1
maps (c) of intracranial atherosclerotic plaque in the right vertebral artery pre
and post contrast. The post T1w image shows PPE within the vertebral artery
plaque (red arrow). The mean R1 (white arrow on b) and T1 (white
arrow on c) before contrast were 1.11±0.78/s and 895.45±22.25ms, respectively. The post R1 in
the plaque (red arrow on b) was increased to 3.07±1.02/s and the post T1 (red arrow on c)
was decreased to 325±99.24ms. Discussion
The resultant T1
measurement obtained using 3D ms-STE EPI agreed well with true T1 values
of the phantom. B1 correction
using the determined ($$$g(\overrightarrow{r})$$$) is robust and experimentally measurable using our
sequence. By limiting acquisition to the desired region of interest, the
reduced FOV technique can acquire the desired region in less scan time. The difference
between pre and post R1 maps can provide quantification of contrast
uptake, which may be more predictive of plaque vulnerability and a better
metric to monitor treatment effects compared to visual inspection. T1
measured using 3D ms-STE EPI may decrease with a lower TM/T1 ratio
because there would be not enough changes in the T1 decay with short
TM. However, because the T1 of muscle or vessel wall are estimated
to be less than 1 sec at 3T and the T1 of plaque components such as intraplaque
hemorrhage may be much lower, a TM of 250 ms may be suitable for T1 mapping
for atherosclerotic plaque. Conclusion
3D me-STE EPI allows quantification of contrast uptake of atherosclerotic
plaque. This may provide important information for clinicians and investigators
interested in quantifying plaque vulnerability and monitoring treatment effects.Acknowledgements
Supported by R01 HL127582, Siemens Medical Solutions, The
Ben B. and Iris M. Margolis Foundation, and the Clinical Merit Review Grant
from the Veterans Administration health Care SystemReferences
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