Merlijn C.E. van der Plas1,2, Kirsten Koolstra3, Martijn Nagtegaal2, Emiel Hartsema2, Lena Vaclavu2, Sophie Schmid2, Leoni Petitclerc2, Peter Bornert4, and Matthias van Osch2
1University Medical Center Utrecht, Utrecht, Netherlands, 2C.J. Gorter Center for high field MRI, Leiden University Medical Center, Leiden, Netherlands, 3Phillips, Best, Netherlands, 4Phillips, Hamburg, Germany
Synopsis
Keywords: Arterial spin labelling, Perfusion
In this study, a framework was set up for
the simultaneous acquisition of 4D MRA and perfusion ASL data while maintaining
whole brain coverage. A Hadamard-8 preparation was combined with a 3D Stack of
Spirals readout which resulted in 7 timepoints. By combining these two
techniques we were able to obtain both angiography and perfusion from a single
dataset. By improving the efficiency of the sampling scheme i.e. using variable
density spirals, the total scan time could be reduced further while improving
the SNR during the perfusion phase, albeit at the expense of the quality of the
4D MRA.
Introduction
The combination of 4D angiographic and
perfusion information can provide essential insight into the hemodynamic
condition of the brain. Recently, ASL was combined with a single slice radial
readout to simultaneously obtain high temporal and high spatial resolution 2D
angiography and low spatial resolution perfusion images1,2. Compared
to radial trajectories, spiral trajectories are more efficient regarding
k-space coverage and are even more flexible, since the sampling density can be
varied3. Especially for the simultaneous acquisition of angiography
and perfusion data, a variable density spiral could be of interest, since the
center of k-space can be oversampled to improve the SNR of the perfusion
images. On the other hand, the outer part of k-space can easily be
undersampled, as angiographic images are well-known to be sparse4.
The aim of this study was to
simultaneously acquire 4D ASL angiographic and perfusion images from a single
dataset while maintaining whole brain coverage and improve SNR during the
perfusion phase. Therefore, we combined a time-encoded pseudo-continuous
arterial spin labeling (te-pCASL) preparation with a (uniform or variable
density) 3D Stack of Spirals (SoS) readout.Methods
Three healthy volunteers (age 25-28 y.o., 3f) were scanned using a 32-channel
head coil on a 3T-scanner (Ingenia-CX, Philips). All volunteers provided
informed consent and the study was approved by the local IRB.
A Hadamard-8 matrix, which was used as
the temporal resolution source, was followed by a segmented 3D SoS turbo-field echo
spiral readout block having a golden angle feature, played out after a post-labeling-delay (PLD) of
280 ms (Figure 1). Two Frequency Offset Corrected Inversion (FOCI) pulses at 1815 and 3135 ms were used for background
suppression. Three different spiral trajectories were used to acquire three datasets:
uniform density spiral and a variable density spiral with R=2 or R=3 (Figure 2) using 19 kz phase-encodings employing a flip-angle-sweep to
maintain constant signal (TR/TE 31/1.85 ms, acquisition matrix 256).
An offline reconstruction in Python (V3.6
and V3.7), using the SigPy package, was employed. Sampling density correction
was applied before the adjoint non-uniform Fast Fourier Transform5 and final coil combination by using a sum-of-squares approach. For the
angiography an oversampling factor of 1.1 along the z-direction was used. For
the perfusion phase an oversampling factor of 1.6 was used, because fold-in
artefacts are more evident in the perfusion images than in the 4D MRA images.
Since for perfusion imaging a low spatial resolution is preferred to enhance
SNR, only the densely sampled center of k-space was included in the perfusion
reconstructions (Figure 2).
To compare the SNR between the different acquired
datasets, all scans were repeated once. Temporal SNR for the perfusion data was
calculated as follows: tSNR=(mean signal over time)/(std over time) within the
gray matter (GM).Results
Figure 3 shows the maximum intensity projection
(MIP) for the angiographic phase (A) and the perfusion phase (B) for a
representative subject for all three datasets. The labeled blood is captured
flowing into and through the Circle of Willis while later time points show the
blood traversing the vasculature towards the tissue. The rightmost images show
the MIP of the sum of all four timepoints of the angiographic phase. The second
and third row show the angiographic phase for the undersampled datasets. For
the fully sampled dataset the labeled blood is visible further down the
vascular tree and the signal intensity is higher. The perfusion phase is
reconstructed at a lower spatial resolution leading to an increased SNR as when
reconstructed at the high resolution of the angiography images.
The GM tSNR showed an increase for the variable
density scans compared to a uniform spiral (Table 1). The data with R=3 showed
the highest tSNR, since for this dataset the center of k-space was oversampled
the most, resulting in a higher percentage of k-space points being
included for the perfusion reconstruction.
The two repeats of the variable density
spiral with R=3 were averaged to increase SNR (Figure 4). The total scan time
for this dataset was 5 min 54 sec and especially in the perfusion phase, an
increase in image quality can be observed compared to the fully sampled dataset.Discussion and Conclusion
In this study, a framework was set up for
the simultaneous acquisition of 4D MRA and perfusion ASL data while maintaining
whole brain coverage. By combing te-pCASL with a 3D SoS readout, which resulted in 7
timepoints, both angiography and perfusion were obtained from a single dataset. Using variable density spirals, the total scan time could be reduced further
while improving the SNR during the perfusion phase, albeit at the expense of
the quality of the 4D MRA.
It was checked whether a conjugate phase
reconstruction6,7 would improve the quality of the images, however,
since B0 inhomogeneities were small (within 30 Hz), this was not the case. In
addition, for the perfusion reconstruction only the densely sampled center of
k-space was used, which resulted in a very short acquisition window of 2.3 ms
per spiral.
Further optimization of the exact spiral
trajectories, the use of concurrent magnetic field monitoring to characterize
the effective trajectories, as well as improved reconstruction approaches would
be logical next steps8. Acknowledgements
This work is part of the research programme Innovational Research Incentives Scheme Vici with project number 016.160.351, which is financed by the Netherlands Organisation for Scientific Research (NWO).References
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