Alexei Ouriadov1,2, Dante PI Capaldi1,2, David McCormack3, and Grace Parraga1,2,3
1Robarts Research Institute, London, ON, Canada, 2Department of Medical Biophysics, Western University, London, ON, Canada, 3Division of Respirology, Department of Medicine, Western University, London, ON, Canada
Synopsis
Hyperpolarized gas pulmonary MRI
provides physiologically relevant biomarkers of obstructive lung disease
including emphysema, bronchopulmonary dysplasia, congenital lobar emphysema and
alpha-1 antitrypsin deficiency. Recently, a stretched-exponential-model
combined with under-sampling in the
imaging and diffusion directions was proposed for the evaluation of
hyperpolarized gas multiple b-value diffusion-weighted MRI. The major
advantage of this method is the possibility to significantly speed up the data
acquisition using acceleration factors between 7 and 10. We
hypothesize that this method can be extended to provide whole lung hyperpolarized gas MRI-based
emphysema biomarkers including static-ventilation, T2* ADC and morphometry maps with high spatial image
resolution.
Purpose
Hyperpolarized
gas pulmonary MRI1,2
provides physiologically relevant biomarkers of obstructive lung disease
including emphysema, bronchopulmonary dysplasia, congenital lobar emphysema and
alpha-1 antitrypsin deficiency.3-5 Recently,
a stretched-exponential-model6 combined with under-sampling in the imaging
and diffusion directions7 was proposed for the evaluation of hyperpolarized
gas multiple b-value diffusion-weighted MRI. The major advantage of this
method is the possibility to significantly speed up the data acquisition using
acceleration factors (AF) between 7 and 10.7 This
is potentially more rapid than the compressed-sensing methods recently
published for diffusion-weighted MRI6,8 and achieves high spatial resolution images. This approach provides a way to generate four
non-zero b-values for diffusion-weighted 129Xe MRI. We hypothesize that a previous method7 can be extended to provide whole lung hyperpolarized
gas MRI-based emphysema biomarkers including static-ventilation, T2*,9-11 ADC and morphometry maps with high spatial image
resolution. Therefore, in this
proof-of-concept evaluation, our objective was to develop this approach and generate
emphysema biomarkers in a small group of ex-smokers with emphysema.Methods
As shown
in Table 1, three ex-smokers with emphysema provided a written informed consent to an ethics-board
approved study protocol and underwent spirometry, plethysmography, CT, and
3He MRI twice within 33 months. Imaging was performed at 3.0T (MR750, GEHC, WI) using
whole-body gradients (5G/cm maximum) and a commercial, rigid linear
human RF coil (Rapid Biomedical, Germany). For Visit-1 in a single breath-hold, five interleaved
acquisitions (TE=4.1msec, TR=6.0msec, reconstructed matrix size=128x128, number
of slices=15; slice thickness=15mm, and
FOV=40x40cm2) with and without diffusion sensitization were acquired
for a given line of k-space to ensure that RF depolarization (4o
constant-flip-angle was used).
The diffusion-sensitization gradient pulse ramp up/down time=500μs,
constant time=460μs and diffusion time (Δ)=1.46ms resulted in images acquired at five different
b-values: 0, 1.6, 3.2, 4.8 and 6.4s/cm2. For Visit-2 this sequence was accelerated (AF=7) by under-sampling in
the imaging and diffusion direction .7 Additionally, a short-TE (TE=1.3ms) b=0 image was
used to generate the static-ventilation
image. A 7.4o constant-flip-angle
(120 [20 per b-value] RF pulses per slice) was used while the matrix size was
128x128x15, FOV=40x40cm2, slice thickness=15mm, six b-values and
duration of a single breath-hold whole lung scan was 12sec. The Visit-1 data were retrospectively under-sampled
in both imaging and diffusion directions ensuring AF=7 to validate the
reconstruction method.7 The ADC (b=0/b=1.6s/cm2) and morphometry maps (mean-airway-length-scale
((LmD)6,8), mean-linear-intercept (Lm)12,13) were generated as previously described7,12 and compared with corresponding maps calculated for the fully-sampled
k-spaces. The Visit-2 data were
reconstructed as previously described,7 and static-ventilation (short-TE image), T2*
(TE1/TE2=1.3ms/4.1ms), ADC and morphometry (LmD/Lm) maps were generated. The diffusion-weighted data were corrected using
regional T2* values
to improve signal-to-noise before generating the diffusion-based
biomarkers. Results
Figure 1 shows representative centre
slice ADC/ADCA, LmD/LmDA and Lm/LmA (
where Aindicates under-sampled) maps for the three subjects
(Visit-1) while Table 2 shows mean estimates and SNR
values obtained for b=0/b=6.4s/cm2 images and static-ventilation image (Visit-1). For the Visit-1
subgroup, mean differences of 2.7%, 1.0% and 1.0% were
observed between fully-sampled and under-sampled (AF=1/AF=7)
k-space ADC, LmD and Lm values, respectively. Figure 2 shows representative centre slice static-ventilation, T2*,
ADC, LmD and Lm maps for three COPD subjects (Visit-2) reconstructed from the originally under-sampled
k-space (AF=7). Table 2 shows mean
estimates of T2* ADC, LmD and Lm
and the SNR values for b=0/b=6.4s/cm2 images (after T2* correction) and static-ventilation image (uncorrected) used
to calculate ventilation-defect-percent3 (VDP).Discussion and Conclusion
In this proof-of-concept study we showed that
the differences in ADC/LmD/Lm estimates from fully-sampled and retrospectively under-sampled k-space were similar
to those observed with accelerated 3He multi-b diffusion-weighted
MRI.7 Thus, VDP/T2*/ADC/morphometry estimates
obtained for Visit-2 can be considered as a reliable. Table 2 indicates that ADC/morphometry
estimates obtained for a small group of subjects during two visits were
reasonably close. Diffusion-weighting MRI
biomarkers suggested emphysema progression over the past 33 months for participant
COPD-3. The T2*-results suggested that T2* values were in the 4-8ms
interval for severe emphysema patients. Likely, T2*
estimates depend on alveolar surface-to-volume ratio and, therefore, can be
potentially used as biomarker. Another important role of T2* mapping is a signal correction. The
SNR of static ventilation images (35-40) was more than adequate for the
calculation of VDP and now can be generated alongside ADC values in a single
rapid breath-hold.3Acknowledgements
A. Ouriadov was funded in part by a fellowship
from the Alpha-1 Foundation (USA).References
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