Christian R. Meixner1, Sebastian Schmitter2,3, Jürgen Herrler4, Arnd Dörfler4, Michael Uder1, and Armin M. Nagel1,3
1Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany, 2Physikalisch-Technische Bundesanstalt (PTB), Braunschweig und Berlin, Germany, 3Division of Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 4Institute of Neuro-Radiology, Friedrich-Alexander Universität Erlangen-Nürnberg, Erlangen, Germany
Synopsis
4D-angiography exploiting pseudo-continuous arterial spin labeling at 7T
suffers from specific absorption rate constraints, low B1+
efficiency for the labeling and B1+ inhomogeneity in the
readout. In this work, we propose a B1+-phase shim
trading B1+ homogeneity and transmit efficiency for the labeling
combined with a dynamic transmission 2-spoke excitation readout. In volunteer measurements,
the proposed approach outperformed the standard circular polarized mode by an
increased vessel intensity and more vessel conspicuity.
Introduction:
4D angiography was shown to be
feasible at 7T using pulsed arterial spin labeling (PASL)1,2.
With pseudo-continuous arterial spin labeling (pcASL) a higher arterial signal was
demonstrated at 1.5T compared to PASL3. However, at 7T, pcASL suffers from specific absorption rate (SAR) constraints,
low B1+ efficiency for the labeling and B1+
inhomogeneity in the readout. This might lead to long acquisition times and
poor contrast in the angiography images. To counteract high SAR values,
Variable-Rate Selective Excitation (VERSE) pulses for the labeling scheme show
a significant impact4. The efficiency of B1+ in the labeling could be
improved by phase-only shimming5 as well as B1+ phase/amplitude shimming4. To overcome inhomogeneity in slice-selective small flip angle gradient
echo sequences, multiple spokes are widely used6.
In this work, we combine a B1+
phase shim trading B1+ homogeneity and transmit efficiency
applied to VERSEd pcASL labeling pulses as well as 2-spoke excitation for the
readout in a 4D angiography sequence at 7T. This method was compared to the standard
circular polarized (CP) mode for labeling and readout.Methods:
All measurements were performed on
a 7T MR system (MAGNETOM Terra, Siemens Healthcare GmbH, Erlangen, Germany)
using a 32-channel Rx/8Tx head-coil (Nova Medical, Wilmington, Massachusetts,
USA) and carried out in accordance with the institutional guidelines and with
approval of the local Ethics Committee (Friedrich-Alexander University (FAU)
Erlangen-Nürnberg, Germany). An unbalanced pCASL labeling scheme (TPulse=500μs,
TGap=1200μs, Gmax=4.2mT/m, Gave=0.6mT/m,
labeling duration=300ms) was modified with VERSE pulses7
(50% amplitude reduction, GVERSE,max=10mT/m). For the readout a segmented
spoiled turbo flash (TFL) readout was used (isotropic resolution 1mm3,
52 slices, PAT=3, partial fourier=6/8, TE=2.07ms, nominal flip angle=8°, echo
spacing=4.7ms, TR=1600ms). The post labeling delay (PLD) was varied from
100:150:550ms. After each labeling 31 segments of the readout train were
applied, resulting in a temporal resolution of 145.7ms and a total acquisition
time of 4:40min per time-point.
For the parallel transmission (pTx)
pulse calculations, relative B1+ maps8 as well as B0 maps were acquired. Additional time-of-flight
(TOF) images were achieved at the labeling plane for the hybrid B1+
shim and the shim values were calculated by minimizing the cost function $$$cost=0.3\cdot CoV^{2} + 0.7\cdot\eta^{2}$$$,
with $$$CoV=\frac{std\left(\left|\sum_{c=1}^C B_{1,c}^{+}(r)\right|\right)}{mean\left(\left|\sum_{c=1}^C B_{1,c}^{+}(r)\right|\right)}$$$ and $$$\eta = mean\left(\frac{\left|\sum_{c=1}^C B_{1,c}^{+}(r)\right|}{\sum_{c=1}^C \left|B_{1,c}^{+}(r)\right|}\right)$$$ (compare Fig.1a).
The readout pTx pulses consists of two 0.9ms long Sinc-shaped spokes placed by
an iterative fourier spoke placement9.
The complex weights for each spoke pulse were calculated by minimizing $$$cost=\parallel\left|Ab\right| - \left|m\right|\parallel^{2} + \lambda\parallel b \parallel^{2}$$$ with the desired magnetization pattern m, b the complex weights of each RF channel and spoke in
Volt, A the system
matrix containing the excitation trajectory as well as B1+,
B0 maps, and the regularization factor for the RF energy $$$\parallel b \parallel^{2}$$$.
A magnitude-least-squares (MLS) algorithm was used for the optimization10
(compare Fig.1b).
Additionally, a 1mm3 isotropic
TOF sequence was obtained at the same position (4 slabs à 20 slices, PAT=2,
TE=3.57ms, flip angle=17°, TR=19ms).
In
total 3 subjects (mean age: 26.7±0.5years) were measured with the hybrid B1+
shim for the labeling and the 2-spokes excitation for the readout (referred as 'full pTx') compared to the sequence in the CP-mode. The 4D-pcASL images
underwent postprocessing using SPM12 (Wellcome Trust Centre for Neuroimaging)11 and the FMRIB
Software Library (FSL)12. To evaluate the
data transversal maximum intensity projections (MIPs) of the 4D-pcASL as well
as of the TOF images were created and filtered by a 2D-Frangi filter (Gaussian
kernel σ=1.0, thresholds to control sensitivity α=0.4, β=0.3 and c=40). The
4D-pcASL filtered MIPs were co-registered to the TOF and masked by the filtered
MIPs of the TOF. Those masked 4D-pcASL images were used for signal evaluation
in the vessels and vessel length determination by processing via Fiji ImageJ as
described in a previous work13 (compare Fig.2).Results:
Fig.3a presents the signal intensity of the vessels at the different PLD
time-points. Compared to the CP-mode, the full pTx sequence that includes the
hybrid B1+ shim for the labeling and 2-spoke pTx for
readout shows higher signal in the vessels at all time-points. The measured vessel
length (Fig.3b) remains constant for the first three time-points (100-400ms), however
with a PLD=550ms the measured vessel length for the full pTx mode increases. An
example for all time-points of one subject is given in Fig.4.
There, the higher signal intensity of the full pTx sequence compared to the
CP-mode can also be observed as well as an increasing number of small vessels can be
depicted at later time-points (red arrows).Discussion and Conclusion:
The
combination of B1+-shimming for the labeling and 2-spoke
dynamic pTx for the readout in 4D-pcASL MRI sequences promises great advantage
over conventional CP-mode at 7T. While the higher and more homogenous
distribution of the flip angles increases the vessels’ signal intensities, the
B1+-shimmed labeling pulse strengthens this effect and
yields even more vessel conspicuity, especially at later time-points.Acknowledgements
No acknowledgement found.References
1. Cong, F. et al. Noncontrast-enhanced time-resolved 4D dynamic intracranial
MR angiography at 7T: A feasibility study. J
Magn Reson Imaging 48, 111-120,
doi:10.1002/jmri.25923 (2018).
2. Metzger, G. J. et al.
In Proceedings of the 21st Annual Meeting of ISMRM, Salt Lake City,
USA, 2013.
3. Koktzoglou, I.,
Gupta, N. & Edelman, R. R. Nonenhanced extracranial carotid MR angiography
using arterial spin labeling: improved performance with pseudocontinuous
tagging. J Magn Reson Imaging 34, 384-394, doi:10.1002/jmri.22628
(2011).
4. Tong, Y.,
Jezzard, P., Okell, T. W. & Clarke, W. T. Improving PCASL at ultra-high
field using a VERSE-guided parallel transmission strategy. Magn Reson Med, doi:10.1002/mrm.28173 (2020).
5. Li X, W. D., Wu
X, Van de Moortele PF, Ugurbil K, Metzger GJ. In Proceedings of the 26th Annual Meeting of ISMRM, Paris, France, 2018.
6. Padormo, F., Beqiri,
A., Hajnal, J. V. & Malik, S. J. Parallel transmission for ultrahigh-field
imaging. NMR Biomed 29, 1145-1161, doi:10.1002/nbm.3313
(2016).
7. Schmitter, S. et al. Contrast enhancement in TOF
cerebral angiography at 7 T using saturation and MT pulses under SAR
constraints: impact of VERSE and sparse pulses. Magn Reson Med 68,
188-197, doi:10.1002/mrm.23226 (2012).
8. Fautz
HP, Vogel M, Gross P, Kerr A, Zhu Y. B1 mapping of coil arrays for parallel
transmission. In Proceedings of the 22nd Annual Meeting of ISMRM,
Toronto, Canada, 2008.
9. Saekho, S., Yip,
C. Y., Noll, D. C., Boada, F. E. & Stenger, V. A. Fast-kz three-dimensional
tailored radiofrequency pulse for reduced B1 inhomogeneity. Magn Reson Med 55, 719-724, doi:10.1002/mrm.20840 (2006).
10. Paige, C. C. &
Saunders, M. A. LSQR: An algorithm for sparse linear equations and sparse least
squares. ACM Transactions on Mathematical
Software 8, 43-71 (1982).
11. Wang, Z. et al. Empirical optimization of ASL
data analysis using an ASL data processing toolbox: ASLtbx. Magnetic resonance imaging 26, 261-269,
doi:10.1016/j.mri.2007.07.003 (2008).
12 Jenkinson, M.,
Beckmann, C. F., Behrens, T. E., Woolrich, M. W. & Smith, S. M. Fsl. NeuroImage 62, 782-790, doi:10.1016/j.neuroimage.2011.09.015 (2012).
13. Meixner, C. R. et al. High resolution time-of-flight
MR-angiography at 7T exploiting VERSE saturation, compressed sensing and
segmentation. Magnetic resonance imaging,
doi:10.1016/j.mri.2019.08.014 (2019).