Brandon Zanette1, Yonni Friedlander1,2, Samal Munidasa1,2, and Giles Santyr1,2
1Translational Medicine, The Hospital for Sick Children, Toronto, ON, Canada, 2Medical Biophysics, University of Toronto, Toronto, ON, Canada
Synopsis
Hyperpolarized 129Xe MRI is an
emergent tool for the quantification of ventilation defects in the lungs. 129Xe
is typically imaged with 2D gradient recalled echo (2D-GRE) which may require lengthy breath-holds (up to 16s) to image the lung. This may be problematic in
subjects who are not able to comply with these breath-hold constraints.
Non-Cartesian spiral imaging samples k-space more efficiently, reducing the
acquisition duration. In this work a 3D stack-of-spirals (3D-SoS) imaging
sequence was developed and tested in healthy adults alongside conventional
2D-GRE for hyperpolarized 129Xe ventilation mapping, showing equivalent
ventilation defect percent quantification in a ~2 s scan.
Introduction
MRI
with hyperpolarized (HP) 129Xe gas is a promising approach for imaging lung diseases
such as asthma, cystic fibrosis, and COPD among others1–4. The spatial distribution of inhaled
xenon gas in the airspaces is typically evaluated with slice-selective 2D
gradient recalled echo (2D-GRE) imaging and compared to 1H thoracic cavity scans, yielding measures of
ventilation defect percent (VDP). Though widely available and straight forward
to implement, 2D-GRE imaging typically requires long breath-hold durations (up
to 16s) due to the Cartesian nature of k-space acquisition. Such long breath
holds can be difficult for subjects to perform, especially for very sick and/or
younger patients. Non-Cartesian methods such as spirals acquire k-space data
more efficiently, reducing overall scan duration5. More recently, these have
allowed for dynamic 129Xe ventilation acquisitions6,7 or 3D isotropic imaging8. Nevertheless, these methods
generally remain under-utilized for this application.
In
this work, HP 129Xe ventilation mapping is performed in healthy volunteers
using a 3D stack-of-spirals (3D-SoS) acquisition and compared to a conventional
2D-GRE approach. The ventilation maps are compared on the basis of SNR and VDP.
The effect of shortening the 3D-SoS readout duration is also investigated.Methods
Four
healthy participants (2 males, 2 females, mean age=27±5 years) were imaged in
accordance with institutional ethics approval at The Hospital for Sick Children. Imaging was
performed on a clinical 3T system (Magnetom Prisma, Siemens Healthcare, Erlangen, Germany) with a flexible
transmit/receive 129Xe chest coil (Clinical MR Solutions, Brookfield, WI). 2D-GRE
and 3D-SoS images were acquired with equivalent in-plane spatial resolutions (3.9×3.9mm2), slice thickness (18.0mm), and number of slices (8-10 depending on participant). Despite equivalent resolutions, 3D-SoS scan
duration was approximately 6-7 times faster (from 12-14s for 2D-GRE to ~2s for
3D-SoS, depending on slice coverage). Sequence parameters are shown in
Table 1. Additionally, a 3D-SoS acquisition with a shortened readout was
performed in one subject. Isotopically enriched 129Xe was polarized to 28±9%
using commercial polarizers (Models 9810 or 9820, Polarean, Durham, NC). Images
were reconstructed in MATLAB (MathWorks, Natick, MA). 3D-SoS images were
reconstructed using a non-uniform FFT9. A 9×9 pixel ROI assessed mean
signal in the right-medial portion of the lung in a slice approximately halfway
through the thorax in the anterior-posterior direction. An equal sized ROI measured
the standard deviation of background noise in the same slice. SNR was
calculated and scaled by polarization at the time of imaging. VDP was
calculated as previously described10,11.Results
Figures
1a and 1b shows 129Xe ventilation maps acquired with 2D-GRE and 3D-SoS in a
representative subject respectively. 3D-SoS maps had image quality comparable
to 2D-GRE shown by the composite images in Figure 1c. 3D-SoS demonstrated
slight blurring near the lung boundaries, presumably due to the relatively long
readout window and/or presence of off-resonance effects. However, it is shown that
this blurring can be reduced with the use of a shortened readout duration
(Figure 2). Scaled SNR was measured to be
slightly higher in the case of 2D-GRE compared to 3D-SoS (52±14 and 32±9
respectively). Nevertheless, VDP values measured across all subjects with
2D-GRE and 3D-SoS were very similar (0.06±0.02% and 0.03±0.01% respectively)
with no significant difference between VDP distributions acquired with either
approach (P>0.05, paired t-test), consistent with lack of any pulmonary
disease in these healthy subjects.Discussion
In this work, a 3D-SoS k-space acquisition is
applied to 129Xe ventilation mapping in a group of healthy adult participants,
yielding image quality and VDP accuracy comparable to a conventional 2D-GRE. 3D-SoS
SNR was slightly lower than 2D-GRE, predominantly driven by increased
background noise. This may be improved in future through optimizations of the non-Cartesian
reconstruction or filtering in k-space (e.g. Hamming, Fermi) which was not done
in this study. Furthermore, the 2D-GRE images were reconstructed with
zero-padding during Fourier transformation (due to partial echo undersampling) to
match matrix sizes. This may have the effect of artificially suppressing
background noise and should be accounted for in the future. Despite this, VDP values measured between approaches were not significantly different
confirming that 3D-SoS provides similar ventilation information without introducing
additional artifacts compared to 2D-GRE in this participant subset. The small VDP
variations between approaches, though not statistically significant, may be
caused by differences in image quality as described above or inherent misregistrations
between the approaches, since each used a separate breath-hold. The main
advantage of 3D-SoS was that data was acquired 6-7 times faster than 2D-GRE.
This has potential for applications in subjects who normally would be unable to
perform lengthy xenon MRI breath-holds. Furthermore, the reduction in scan time
has the potential to be traded for higher spatial resolution, dynamic
acquisitions with high temporal resolution, or wash-in/out ventilation data in
a multi-breath fashion, that may otherwise be difficult to achieve with 2D-GRE.
Further reductions in acquisition duration may be achievable with accelerated
imaging techniques such as parallel imaging and compressed sensing12. Future work will involve optimizing the spiral
acquisition/reconstruction to further improve image quality, as well as testing
in patient populations to confirm quantification of VDP is in agreement with
2D-GRE.Conclusion
3D
Stack-of-spirals imaging provides acquisition of accurate hyperpolarized 129Xe ventilation
images comparable to 2D-GRE in approximately 1/7 the total scan time, enabling
shortened breath-hold durations. Acknowledgements
The
authors thank Dr. Marcus Couch, Elaine Stirrat, Daniel Li, Krzysztof Kowalik,
Ruth Weiss, and Tammy Rayner for assistance with imaging experiments. The
authors acknowledge the Ontario Research Fund (ORF), Canadian Institute of
Health Research (CIHR), and Natural Sciences and Engineering Research Council
of Canada (NSERC) as sources of funding. References
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