Matthijs de Buck 1, Peter Jezzard1, and Aaron Hess2
1Wellcome Centre for Integrative Neuroimaging, FMRIB Division, Nuffield Department of Clinical Neurosciences, University of Oxford, Oxford, United Kingdom, 2Oxford Centre for Clinical Magnetic Resonance Research, Department of Cardiovascular Medicine, University of Oxford, Oxford, United Kingdom
Synopsis
3D TOF-MRA at 7T can be greatly accelerated
using compressed sensing reconstruction of undersampled acquisitions, but the
achieved reconstruction quality depends on the undersampling pattern. In this
work, optimal parameters for variable-density Poisson disk undersampling were
established. For all acceleration factors, optimal reconstructions were
achieved by using small fully-sampled calibration areas of 12x12 lines and a
polynomial order of around 2. The optimal undersampling parameters were the
same for all acceleration factors, but the importance of using optimized
undersampling parameters was found to increase for higher acceleration factors.
Introduction
Time-of-flight (TOF) magnetic resonance
angiography (MRA) is a common clinical technique for visualisation of the
intracranial vasculature. High spatial resolution MRA can visualize small and
highly tortuous vessels such as the lenticulostriate arteries1,
which are implicated in up to a third of symptomatic strokes2. In order
to achieve practical scan times, compressed sensing (CS) reconstruction can be
used to iteratively reconstruct highly undersampled data3. However,
the accuracy of CS reconstructions depends on the undersampling patterns being
used.
Cartesian undersampling trajectories in 3D are
commonly designed using two-dimensional undersampling masks covering the two phase-encode
directions, with each sampled point representing a continuously sampled line in
the frequency-encode direction (kx). Undersampling masks are often
generated using pseudo-random variable-density Poisson disks4 with a
fully-sampled auto-calibration region in the centre of k-space5-9.
Variable-density Poisson-disk undersampling distributions are characterized by
three parameters: the undersampling factor (equivalent to the acceleration
factor, R), the polynomial order of the sampling density variation (pp), and
the size of the fully-sampled auto-calibration region: see Figure 1. Although
the reconstruction quality depends on those undersampling parameters, no conclusive
information is available about their optimal values for 3D TOF-MRA at 7T.
In this work, optimal 3D TOF-MRA undersampling
parameters were established for various acceleration factors at 7T through
reconstruction of retrospectively undersampled data. The results were
subsequently validated using additional prospectively undersampled acquisitions
that adopted the optimized parameters.Methods
Data were acquired using a 3D gradient-echo
non-contrast-enhanced TOF-MRA sequence on a Siemens (Erlangen, Germany)
Magnetom 7T scanner using a 1Tx, 32-channel Rx head-coil (Nova Medical,
Wilmington, Massachusetts). Two healthy subjects were scanned to generate the
data used for initial optimization, comprising 4 slabs with a total
field-of-view of 220x174x60mm and resolution of 0.34mm isotropic. Further
sequence parameters were: TR/TE 14ms/5.61ms, flip angle 20o,
bandwidth 118 Hz/pixel, and a total acquisition time of 27 minutes for a fully-sampled
acquisition. For validation of the retrospective optimization results, further prospectively
undersampled and fully-sampled datasets were acquired from three additional healthy
subjects.
Coil sensitivities were estimated using
ESPIRiT10, and compressed sensing was implemented using the
BART-toolbox12,13 (v0.4.02) using FISTA11
with l1 wavelet-regularization. Reconstructions were performed using λ=0.07 in
the wavelet domain with 20 iterations, which yielded consistently good
reconstruction results for various undersampled datasets in an initial
reconstruction parameter optimization.
The quality of the different undersampled
reconstructions, relative to the fully sampled reconstructions, was
quantitatively assessed using the intracranial vessel-masked structural
similarity index (SSIM), which has been found previously to correlate well with
visual evaluation by radiologists14.Results
Figure 2 shows fully-sampled
reconstructions and the corresponding vessel masks for the four slabs that are
used for all retrospectively undersampled reconstructions.
The results of undersampling parameter
optimization are shown in Figure 3, which indicates an optimal set of
undersampling parameters at calib = 12 (i.e. 12x12 calibration lines) with a polynomial order of approximately
2. This result is particularly evident for higher acceleration factors.
Figures 4 and 5 show reconstructions from fully-sampled
data and prospectively undersampled data, using both (i) those ‘optimal’
undersampling parameters and (ii) calibration region sizes based on values
found in the literature5 (representative data is shown from a single
subject). Results are shown for an acceleration factor of 7.2 (which was
previously found to be “a reasonable trade-off between scan time and image
quality”5), and a higher acceleration factor of 15. Discussion
Although differences in the reconstruction
accuracy for different sets of parameters are visible for all acceleration
factors in Figure 3, the relative importance of using the optimal parameters
increases with higher acceleration factors. For all acceleration factors the
combination of 12x12 calibration lines with a polynomial order of about 2 consistently yielded the best reconstruction accuracy. This optimal calibration
region size is considerably smaller than values found in the literature, and
makes it possible to spend more scan time acquiring high spatial frequency-data.
Figures 4 and 5 show a clear reduction in
the number of visible vessels both for optimized and literature-based
acquisition parameters at higher acceleration. However, the vessel visibility
and sharpness is consistently superior when using optimized undersampling
parameters. This improvement can be achieved without increasing scan time or
reconstruction time, and without additional technical requirements.
The data used in this work were acquired
using a relatively simple protocol. Alternative protocols may result in changes
to the acquired contrasts. However, the optimal undersampling parameters were
found to be consistent for volumes with high differences in vascular
characteristics and visibility (Figure 2). When acquiring data at different
resolutions, the optimal polynomial order could change accordingly but the
required calibration region size for accurate coil sensitivity estimation is
expected to remain consistent. Although 32-channel receive coils are most commonly
used in 7T MRI, it remains unclear how the results presented here would
translate to different coil configurations.Conclusion
Optimal undersampling parameters for 3D MRA at
7T using compressed sensing reconstruction were established. For all acceleration
factors, optimal reconstructions were achieved by using a fully-sampled
calibration area of 12x12 lines and a polynomial order of around 2. Although
the optimal undersampling parameters were the same for all acceleration
factors, the importance of using optimized undersampling parameters was found
to increase for higher acceleration factors.Acknowledgements
MdB receives financial support from Siemens Healthineers and the Dunhill Medical Trust.References
[1] J. Hendrikse,
J. J. Zwanenburg, F. Visser, T. Takahara, and P. Luijten, “Noninvasive
depiction of the lenticulostriate arteries with time-of-flight MR angiography
at 7.0 T,” Cerebrovasc. Dis., vol. 26, no. 6, pp. 624–629, 2008.
[2] S. M.
Greenberg, “Small Vessels, Big Problems,” N. Engl. J. Med., vol. 354,
no. 14, pp. 1451–1453, 2006.
[3] M. Lustig, D.
Donoho, and J. M. Pauly, “Sparse MRI: The application of compressed sensing for
rapid MR imaging,” Magn. Reson. Med., vol. 58, no. 6, pp. 1182–1195,
2007.
[4] B. Deka and S.
Datta, “A Practical Under-Sampling Pattern for Compressed Sensing MRI,” Lect.
Notes Electr. Eng., vol. 347, pp. 115–125, 2015.
[5] C. R. Meixner et
al., “High resolution time-of-flight MR-angiography at 7 T exploiting VERSE
saturation, compressed sensing and segmentation,” Magn. Reson. Imaging,
vol. 63, no. August, pp. 193–204, 2019.
[6] T. Yamamoto et
al., “Magnetic resonance angiography with compressed sensing: An evaluation
of moyamoya disease,” PLoS One, vol. 13, no. 1, pp. 1–11, 2018.
[7] S. Rapacchi et
al., “High spatial and temporal resolution dynamic contrast-enhanced
magnetic resonance angiography using compressed sensing with magnitude image
subtraction,” Magn. Reson. Med., vol. 71, no. 5, pp. 1771–1783, 2014.
[8] K. G.
Hollingsworth, “Reducing acquisition time in clinical MRI by data undersampling
and Compressed Sensing reconstruction,” Phys. Med. Biol., vol. 60, no.
21, pp. R297–R322, 2015.
[9] M. H. Moghari,
M. Uecker, S. Roujol, M. Sabbagh, T. Geva, and A. J. Powell, “Accelerated
whole-heart MR angiography using a variable-density poisson-disc undersampling
pattern and compressed sensing reconstruction,” Magn. Reson. Med., vol.
79, no. 2, pp. 761–769, 2018.
[10] M. Uecker et
al., “ESPIRiT - An eigenvalue approach to autocalibrating parallel MRI:
Where SENSE meets GRAPPA,” Magn. Reson. Med., vol. 71, no. 3, pp.
990–1001, 2014.
[11] A. Beck and M.
Teboulle, “A Fast Iterative Shrinkage-Thresholding Algorithm,” Soc. Ind.
Appl. Math. J. Imaging Sci., vol. 2, no. 1, pp. 183–202, 2009.
[12] BART Toolbox
for Computational Magnetic Resonance Imaging, DOI: 10.5281/zenodo.592960.
[13] J. I. Tamir, F.
Ong, J. Y. Cheng, M. Uecker, and M. Lustig, “Generalized Magnetic Resonance
Image Reconstruction using The Berkeley Advanced Reconstruction Toolbox,” Proc.
ISMRM 2016 Data Sampl. Image Reconstr. Work., vol. 2486, 2016.
[14] T. Akasaka et
al., “Optimization of regularization parameters in compressed sensing of
magnetic resonance angiography: Can statistical image metrics mimic radiologists’
perception?,” PLoS One, vol. 11, no. 1, pp. 1–14, 2016.