Alex K. Smith1,2, Richard D. Dortch1,2,3, Samantha By1,2, Robert L. Barry2, Chris R. Thompson2, Kristen George-Durrett2, Bailey D. Lyttle2, and Seth A. Smith1,2,3
1Department of Biomedical Engineering, Vanderbilt University, Nashville, TN, United States, 2Vanderbilt University Institute of Imaging Science, Vanderbilt University, Nashville, TN, United States, 3Department of Radiology and Radiological Sciences, Vanderbilt University, Nashville, TN, United States
Synopsis
The spinal
cord is responsible for mediating neurologic function, and in particular, the
lumbar cord is integral to lower extremity function. However, lumbar cord quantitative MRI studies
have been limited due to its size, location, and composition. A single-point quantitative magnetization
transfer was recently developed, but has not been applied to the lumbar
cord. Therefore, we have implemented an
assessment of qMT at the thoracolumbar bulge to characterize the MT effect in
the thoracolumbar cord in healthy volunteers.Purpose
The spinal cord (SC) is responsible for
mediating neurologic function between the brain and peripheral nervous system,
and is somatotopically organized: sensory information is conveyed through the
dorsal columns, while the lateral columns convey a significant fraction of motor
function. Therefore, even small SC
lesions (e.g. multiple sclerosis [MS]) can result in severe neurological
impairment. In particular, the lumbar cord is integral to lower extremity
function: its characterization can significantly improve diagnosis and prognosis
of neurodegenerative disease. However, lumbar cord quantitative MRI studies
have been limited due to its size (~1cm), location, and composition: it is
located directly below the lungs, quickly diminishes in size through the conus
medularis and cauda equine, and has significantly less white matter per volume
than its cervical counterpart.
A
single-point quantitative magnetization transfer (qMT) was recently developed
in the brain1 and cervical SC2 that provides rapid, high-resolution
indices that relate to grey matter (GM) and white matter (WM) myelin content. However, qMT has not been studied in the
lumbar cord; therefore we have implemented for the first time an assessment of
qMT at the thoracolumbar bulge to accurately characterize the MT effects
observed in the WM and GM of the thoracolumbar cord in healthy volunteers.
Methods
Two
healthy volunteers (one male, ages 25 and 26 years) were imaged using a 3.0T
Achieva whole body scanner (Philips, The Netherlands). A two-channel transmit body coil was used for
excitation and a six-channel spine array was used for signal reception. For each volunteer, a transverse volume
between T11 and L2 was selected from a total spine T2-weighted survey image. qMT data were acquired over this volume using
a 3D MT-prepared spoiled gradient echo sequence3. MT-preparation
used a 20 ms single-lobe sinc-Gauss pulse, saturation flip angle (αMT) of 820 ̊, and
offset frequencies (∆ω) of 2.5 and 100 kHz.
Additional imaging parameters included: TR/TE=50/2.7 ms, excitation flip
angle (α)=6 ̊, FOV=150×150×70 mm3, resolution = 0.65×0.65×5 mm3,
and 2 signal averages. B1+ was measured
in the same volume using the actual flip angle imaging method (TR1/TR2= 30/130
ms, α= 60°)4; ∆B0 from gradient echo phase images acquired (∆TE=2.3
ms)5; and T1 using a multiple flip angle acquisition (TR/TE=20/4.6
ms, α = 5, 10, 15, 20, 25, 30°). A high-resolution (0.65×0.65×3 mm3,
2 mm gap) multi-echo gradient echo (mFFE) anatomical image was also acquired
for registration (TR/TE/∆TE = 700/8.0/9.3 ms, α = 33°). Total scan time to acquire anatomical, T1, B1+,
∆B0, and MT data was ≈22 minutes.
Prior
to data fitting, all images were co-registered to the mFFE image using the
FLIRT package from FSL6. Normalized
(to ∆ω = 100 kHz data) signal intensities were then fitted1 to a
two-pool model of the MT effect to find the macromolecular to free pool size
ratio (PSR), while fixing the qMT parameters, kmf, T2fR1f,
and T2m, to their respective values derived from the cervical cord2,
and using the T1, B1+, and ∆B0 field maps to correct for fitting errors associated
with field inhomogeneities/T1 variations.
Results
Figure
1 displays the mFFE (left panel) and PSR (right panels) for a single slice at T12
in each volunteer. WM displays higher PSR than GM, while GM is a significant
fraction of the total cord volume. Of
particular note are the dorsal horns protruding from the cord into the cerebrospinal
fluid which are the start of the dorsal nerve roots. The lumbar PSR data agrees well with
established values
2, as the mean PSR in each volunteer was found to
be (WM = 0.18±0.04,0.21±0.05, GM = 0.13±0.03,0.15±0.03). Table 1 displays the mean PSR for each
volunteer for the dorsal column (DC), lateral column (LC), WM (DC+LC), and GM.
Discussion
The
PSR for WM and GM in the lumbar cord is suspected to be similar to cervical
cord PSR; healthy cervical PSR values in the WM and GM were found to be 0.19±0.01
and 0.15±0.01, respectively
2.
In particular, note the ability to identify the dorsal nerve roots extending
into the CSF beginning in Fig. 1, which are difficult to visualize at lower
resolutions. The integrity of these nerve
roots is paramount for assessing neural function; therefore, the ability to
accurately quantify the PSR in the SC, nerve roots and GM may have important
implications for demyelinating diseases such as MS.
Conclusions
These results demonstrate the first study of high-resolution
qMT and derived PSR maps of the healthy thoracolumbar cord. Future work involves collecting additional
healthy controls, assessing the similarity of the constraints to cervical cord
estimates, and evaluation in patient populations.
Acknowledgements
Funding provided by: NMSS RG-1501-02840,
NIH/NCI R25 CA136440, NIH/NIBIB R21 NS087465-01, NIH/NIBIB R01 EY023240 01A1.
The authors wish to thank Clair Kurtenbach and Leslie McIntosh for their invaluable help with data collection, as well as Philips Medical Systems.
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